- Hard Probes
- Heavy Flavor
- Abstracts, Presentations and Proceedings
- HF PWG QM2011 analysis topics
- HF PWG Preliminary plots
- Heavy Quark Physics in Nucleus-Nucleus Collisions Workshop at UCLA
- NPE Analyses
- PicoDst production requests
- Upsilon Analysis
- Combinatorial background subtraction for e+e- signals
- Estimating Acceptance Uncertainty due to unknown Upsilon Polarization
- Estimating Drell-Yan contribution from NLO calculation.
- Response to PRD referee comments on Upsilon Paper
- Upsilon Analysis in d+Au 2008
- Upsilon Analysis in p+p 2009
- Upsilon Paper: pp, d+Au, Au+Au
- Using Pythia 8 to get b-bbar -> e+e-
- Varying the Continuum Contribution to the Dielectron Mass Spectrum
- WWW
- Jet-like correlations
- Other Groups
- Peripheral Collisions
- Spin
Code to run with STAR HF Tune
Updated on Thu, 2009-09-17 12:28. Originally created by calderon on 2009-09-17 12:28.
Under:
// main00.cc
// Modified from the main01.cc
// which is a part of the PYTHIA event generator.
// Copyright (C) 2008 Torbjorn Sjostrand.
// PYTHIA is licenced under the GNU GPL version 2, see COPYING for details.
// Please respect the MCnet Guidelines, see GUIDELINES for details.
// This is a simple test program.
#include "Pythia.h"
#include "Basics.h"
#include "TROOT.h"
#include "TFile.h"
#include "TH1.h"
bool isBHadron(int id) {
// This snippet is meant to capture all B hadrons
// as given in the PDG.
if (id<0) id*=-1;
if (id<500) return false;
return (fmod(id/100,5.)==0.0 || id/1000==5);
}
using namespace Pythia8;
double myRapidity(Vec4& p) {
return 0.5*log(p.pPlus()/p.pMinus());
}
int main() {
// Initialize root
TROOT root("Manuel's ROOT Session","PYTHIA Histograms");
// Generator. Process selection. LHC initialization. Histogram.
Pythia pythia;
// Shorthand for some public members of pythia (also static ones).
//Event& event = pythia.event;
ParticleDataTable& pdt = pythia.particleData;
// The cmnd file below contains
// the Pythia Tune parameters
// the processes that are turned on
// and the PDFs used
// for the pythia run.
pythia.readFile("main00.cmnd");
UserHooks *oniumUserHook = new SuppressSmallPT();
pythia.setUserHooksPtr(oniumUserHook);
cout << "Mass of b quark " << ParticleDataTable::mass(5) << endl;
cout << "Mass of b bar " << ParticleDataTable::mass(-5) << endl;
// Extract settings to be used in the main program.
int nEvent = pythia.mode("Main:numberOfEvents");
int nList = pythia.mode("Main:numberToList");
int nShow = pythia.mode("Main:timesToShow");
int nAllowErr = pythia.mode("Main:timesAllowErrors");
bool showCS = pythia.flag("Main:showChangedSettings");
bool showSett = pythia.flag("Main:showAllSettings");
bool showStat = pythia.flag("Main:showAllStatistics");
bool showCPD = pythia.flag("Main:showChangedParticleData");
pythia.init();
if (showSett) pythia.settings.listAll();
if (showCS) pythia.settings.listChanged();
if (showCPD) pdt.listChanged();
Hist mult("charged multiplicity", 100, -0.5, 799.5);
TH1D* multHist = new TH1D("multHist","Multiplicity",100,-0.5,99.5);
TH1D* bquarkPt = new TH1D("bquarkPt","bquarkPt",100,0,50);
TH1D* bbarquarkPt = new TH1D("bbarquarkPt","bbar quark Pt",100,0,50);
TH1D* B0mesonPt = new TH1D("BOmesonPt","B0mesonPt",100,0,50);
TH1D* B0barmesonPt = new TH1D("BObarmesonPt","B0bar meson Pt",100,0,50);
TH1D* BplusmesonPt = new TH1D("BplusmesonPt","BplusmesonPt",100,0,50);
TH1D* BminusmesonPt = new TH1D("BminusmesonPt","Bminus meson Pt",100,0,50);
TH1D* BplusmesonPtCDFrap = new TH1D("BplusmesonPtCDFrap","BplusmesonPt |y|<1",100,0,50);
TH1D* BminusmesonPtCDFrap = new TH1D("BminusmesonPtCDFrap","Bminus meson Pt |y|<1",100,0,50);
TH1D* electronFrombPt = new TH1D("electronFrombPt","electrons from b",100,0,30);
TH1D* positronFrombPt = new TH1D("positronFrombPt","positrons from b",100,0,30);
TH1D* epluseminusMinv = new TH1D("epluseminusMinv","e+ e- Inv. Mass",300,0,30);
TH1D* epluseminusRapidity = new TH1D("epluseminusRapidity","e+ e- y",80,-4,4);
TH1D* epluseminusMinvMidRap = new TH1D("epluseminusMinvMidRap","e+ e- Inv. Mass |y|<0.5",300,0,30);
// Begin event loop. Generate event. Skip if error. List first one.
int nPace = max(1,nEvent/nShow);
int nErrors(0);
for (int iEvent = 0; iEvent < nEvent; ++iEvent) {
if (!pythia.next()) {
++nErrors;
if (nErrors>=nAllowErr) {
cout << "Reached error limit : " << nErrors << endl;
cout << "Bailing out! " << endl;
break;
}
continue;
}
if (iEvent%nPace == 0) cout << " Now begin event " << iEvent << endl;
if (iEvent < nList) {pythia.info.list(); pythia.event.list();}
// Find number of all final charged particles and fill histogram.
// Find the b (id = 5) and bbar (id = -5), find their daughters,
// if daughters include electron (id = 11) and positron (id=-11), calculate their
// invariant mass
// Status flags:
// 21 incoming particles of hardest subprocess
// 23 outgoing particles of hardest subprocess
// 81-89 primary hadrons produced by hadronization process (B mesons, e.g.)
// 91-99 particles produced in decay process or by B-E effects (e.g. the electrons)
int nCharged = 0;
int indexBQuark(0), indexBbarQuark(0);
for (int i = 0; i < pythia.event.size(); ++i) {
if (pythia.event[i].isFinal() && pythia.event[i].isCharged()) {
++nCharged;
}
Particle& theParticle = pythia.event[i];
if (theParticle.id() == 5 ) {
indexBQuark = i;
//cout << "Mother 1, Mother 2 = " << theParticle.mother1() << ", " << theParticle.mother2() << endl;
}
if (theParticle.id() == -5) {
indexBbarQuark = i;
//cout << "Mother 1, Mother 2 = " << theParticle.mother1() << ", " << theParticle.mother2() << endl;
}
} // particle loop
cout << "Found b quark at index " << indexBQuark << endl;
cout << "Found bbar quark at index " << indexBbarQuark << endl;
bquarkPt->Fill(pythia.event[indexBQuark].pT());
bbarquarkPt->Fill(pythia.event[indexBbarQuark].pT());
mult.fill( nCharged );
multHist->Fill(nCharged);
//cout << "Event " << iEvent << ", Nch= " << nCharged << endl;
//Find hadronization products of b and bbar.
int bQuarkDaughter1 = pythia.event[indexBQuark].daughter1();//first daughter index
int bQuarkDaughter2 = pythia.event[indexBQuark].daughter2();//last daughter index
int bbarQuarkDaughter1 = pythia.event[indexBbarQuark].daughter1();
int bbarQuarkDaughter2 = pythia.event[indexBbarQuark].daughter2();
// Obtain the two hadrons from the fragmentation process
// Use the PDG id's for this. All B mesons id's are of the form xx5xx, and
// all B baryons are of the form 5xxx.
// So we obtain the id, (make it positive if needed) and then test
// to see if it is a meson with fmod(currId/100,5)==0.0
// to see if it is a baryon with currId/1000==5
int HadronFromBQuark(0), HadronFromBbarQuark(0);
if (bQuarkDaughter1<bQuarkDaughter2) {
cout << "Daughters of b Quark" << endl;
for (int j=bQuarkDaughter1; j<=bQuarkDaughter2; ++j) {
if (isBHadron(pythia.event[j].id())) {
cout << "Fragmentation: b -> " << pythia.event[j].name() << endl;
cout << " id " << pythia.event[j].id() << " at index " << j << endl;
HadronFromBQuark = j;
}
}
}
if (bbarQuarkDaughter1<bbarQuarkDaughter2) {
cout << "Daughters of bbar Quark" << endl;
for (int k=bbarQuarkDaughter1; k<=bbarQuarkDaughter2; ++k) {
if (isBHadron(pythia.event[k].id())) {
cout << "Fragmentation : bbar -> " << pythia.event[k].name() << endl;
cout << " id " << pythia.event[k].id() << " at index " << k << endl;
HadronFromBbarQuark = k;
}
}
}
// Search the daughters of the hadrons until electrons and positrons are found
// if there are any from a semileptonic decay of a beauty hadron
// Start with the b quark, the b-bar quark loop comes after this
int Daughter(HadronFromBQuark), electronIndex(0), positronIndex(0);
while (Daughter!=0) {
cout << "Checking " << pythia.event[Daughter].name() << " for e+/e- daughters" << endl;
if (pythia.event[Daughter].id()==-511) {
// This is a Bbar0, enter its pT
cout << "Filling Bbar0 pT" << endl;
B0barmesonPt->Fill(pythia.event[Daughter].pT());
}
if (pythia.event[Daughter].id()==511) {
// This is a B0, enter its pT
cout << "Filling Bbar0 pT" << endl;
B0mesonPt->Fill(pythia.event[Daughter].pT());
}
Vec4 daughterVec4 = pythia.event[Daughter].p();
double daughterRap = myRapidity(daughterVec4);
if (pythia.event[Daughter].id()==-521) {
// This is a Bminus, enter its pT
cout << "Filling Bminus pT" << endl;
BminusmesonPt->Fill(pythia.event[Daughter].pT());
if (fabs(daughterRap)<1.0) {
BminusmesonPtCDFrap->Fill(pythia.event[Daughter].pT());
}
}
if (pythia.event[Daughter].id()==521) {
// This is a Bplus, enter its pT
cout << "Filling Bplus pT" << endl;
BplusmesonPt->Fill(pythia.event[Daughter].pT());
if (fabs(daughterRap)<1.0) {
BplusmesonPtCDFrap->Fill(pythia.event[Daughter].pT());
}
}
int nextDaughter1 = pythia.event[Daughter].daughter1();
int nextDaughter2 = pythia.event[Daughter].daughter2();
// search for electron or positron
for (int iDaughter = nextDaughter1; iDaughter<=nextDaughter2; ++iDaughter) {
if (pythia.event[iDaughter].id()==11) {
cout << "Found electron" << endl;
cout << pythia.event[iDaughter].name() << endl;
electronIndex=iDaughter;
electronFrombPt->Fill(pythia.event[electronIndex].pT());
break;
}
if (pythia.event[iDaughter].id()==-11) {
cout << "Found positron" << endl;
cout << pythia.event[iDaughter].name() << endl;
positronIndex=iDaughter;
positronFrombPt->Fill(pythia.event[positronIndex].pT());
break;
}
}// loop over daughters to check for e+e-
// If we get here, that means there were no electrons nor positrons.
// Set the Daughter index to zero now.
Daughter = 0;
// If any of the daughters is still a beauty-hadron, we can try again
// and reset the Daughter index, but only if one of the daughters contains a
// b quark.
for (int jDaughter = nextDaughter1; jDaughter<=nextDaughter2; ++jDaughter) {
if (isBHadron(pythia.event[jDaughter].id())) {
//One of the daughters is a beauty hadron.
Daughter = jDaughter;
}
}// loop over daughters to check for another b hadron
}// end of search for electrons in all the daughters of the b quark
// Now search among the daughters of the bbar quark
Daughter=HadronFromBbarQuark;
while (Daughter!=0) {
cout << "Checking " << pythia.event[Daughter].name() << " for e+/e- daughters" << endl;
if (pythia.event[Daughter].id()==-511) {
// This is a Bbar0, enter its pT
cout << "Filling Bbar0 pT" << endl;
B0barmesonPt->Fill(pythia.event[Daughter].pT());
}
if (pythia.event[Daughter].id()==511) {
// This is a B0, enter its pT
cout << "Filling B0 pT" << endl;
B0mesonPt->Fill(pythia.event[Daughter].pT());
}
Vec4 daughterVec4 = pythia.event[Daughter].p();
double daughterRap = myRapidity(daughterVec4);
if (pythia.event[Daughter].id()==-521) {
// This is a Bminus, enter its pT
cout << "Filling Bminus pT" << endl;
BminusmesonPt->Fill(pythia.event[Daughter].pT());
if (fabs(daughterRap)<1.0) {
BminusmesonPtCDFrap->Fill(pythia.event[Daughter].pT());
}
}
if (pythia.event[Daughter].id()==521) {
// This is a Bplus, enter its pT
cout << "Filling Bplus pT" << endl;
BplusmesonPt->Fill(pythia.event[Daughter].pT());
if (fabs(daughterRap)<1.0) {
BplusmesonPtCDFrap->Fill(pythia.event[Daughter].pT());
}
}
int nextDaughter1 = pythia.event[Daughter].daughter1();
int nextDaughter2 = pythia.event[Daughter].daughter2();
// search for electron or positron
for (int iDaughter = nextDaughter1; iDaughter<=nextDaughter2; ++iDaughter) {
//cout << "daughter is a " << pythia.event[iDaughter].name() << endl;
if (pythia.event[iDaughter].id()==11) {
cout << "Found electron" << endl;
cout << pythia.event[iDaughter].name() << endl;
electronIndex=iDaughter;
electronFrombPt->Fill(pythia.event[electronIndex].pT());
break;
}
if (pythia.event[iDaughter].id()==-11) {
cout << "Found positron" << endl;
cout << pythia.event[iDaughter].name() << endl;
positronIndex=iDaughter;
positronFrombPt->Fill(pythia.event[positronIndex].pT());
break;
}
}// loop over daughters to check for e+e-
// If we get here, that means there were no electrons nor positrons.
// Set the Daughter index to zero now.
Daughter = 0;
// If any of the daughters is still a beauty-hadron, we can try again
// and reset the Daughter index, but only if one of the daughters contains a
// b quark.
for (int jDaughter = nextDaughter1; jDaughter<=nextDaughter2; ++jDaughter) {
if (isBHadron(pythia.event[jDaughter].id())) {
//One of the daughters is a beauty hadron.
Daughter = jDaughter;
}
}// loop over daughters to check for another b hadron
}//end of search for electron among daughters of bbar quark
if (electronIndex!=0 && positronIndex!=0) {
cout << "Found an e+e- pair from bbar" << endl;
cout << "Ele 4-mom = " << pythia.event[electronIndex].p() << endl;
cout << "Pos 4-mom = " << pythia.event[positronIndex].p() << endl;
Vec4 epluseminus(pythia.event[electronIndex].p()+pythia.event[positronIndex].p());
epluseminusMinv->Fill(epluseminus.mCalc());
double epluseminusRap = 0.5*log((epluseminus.e()+epluseminus.pz())/(epluseminus.e()-epluseminus.pz()));
epluseminusRapidity->Fill(epluseminusRap);
if (fabs(epluseminusRap)<0.5) epluseminusMinvMidRap->Fill(epluseminus.mCalc());
}
else {
cout << "No e+e- pair in event" << endl;
}
// End of event loop. Statistics. Histogram. Done.
}// event loop
if (showStat) pythia.statistics();
//cout << mult << endl;
//Write Output ROOT hisotgram into ROOT file
TFile* outFile = new TFile("pythiaOutputHistosTest.root","RECREATE");
multHist->Write();
bquarkPt->Write();
bbarquarkPt->Write();
B0mesonPt->Write();
B0barmesonPt->Write();
BplusmesonPt->Write();
BminusmesonPt->Write();
BplusmesonPtCDFrap->Write();
BminusmesonPtCDFrap->Write();
electronFrombPt->Write();
positronFrombPt->Write();
epluseminusMinv->Write();
epluseminusRapidity->Write();
epluseminusMinvMidRap->Write();
outFile->Close();
return 0;
}
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