1 /**************************************************************************
2 * Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. *
4 * Author: The ALICE Off-line Project. *
5 * Contributors are mentioned in the code where appropriate. *
7 * Permission to use, copy, modify and distribute this software and its *
8 * documentation strictly for non-commercial purposes is hereby granted *
9 * without fee, provided that the above copyright notice appears in all *
10 * copies and that both the copyright notice and this permission notice *
11 * appear in the supporting documentation. The authors make no claims *
12 * about the suitability of this software for any purpose. It is *
13 * provided "as is" without express or implied warranty. *
14 **************************************************************************/
18 // Class to generate correlated Heavy Flavor hadron pairs (one or several pairs
19 // per event) using paramtrized kinematics of quark pairs from some generator
20 // and quark fragmentation functions.
21 // Is a generalisation of AliGenParam class for correlated pairs of hadrons.
22 // In this version quark pairs and fragmentation functions are obtained from
23 // ~2.10^6 Pythia6.214 events generated with kCharmppMNRwmi & kBeautyppMNRwmi,
24 // CTEQ5L PDF and Pt_hard = 2.76 GeV/c for p-p collisions at 7, 10 and 14 TeV,
25 // and with kCharmppMNR (Pt_hard = 2.10 GeV/c) & kBeautyppMNR (Pt_hard = 2.75 GeV/c),
26 // CTEQ4L PDF for Pb-Pb at 3.94 TeV, for p-Pb & Pb-p at 8.8 TeV.
27 // Decays are performed by Pythia.
28 // Author: S. Grigoryan, LPC Clermont-Fd & YerPhI, Smbat.Grigoryan@cern.ch
29 // July 07: added quarks in the stack (B. Vulpescu)
30 // April 09: added energy choice between 10 and 14 TeV (S. Grigoryan)
31 // Sept 09: added hadron pair composition probabilities via 2D histo (X.M. Zhang)
32 // Oct 09: added energy choice between 7, 10, 14 TeV (for p-p), 4 TeV (for Pb-Pb),
33 // 9 TeV (for p-Pb) and -9 TeV (for Pb-p) (S. Grigoryan)
34 // April 10: removed "static" from definition of some variables (B. Vulpescu)
35 // May 11: added Flag for transportation of background particles while using
36 // SetForceDecay() function (L. Manceau)
37 // June 11: added modifications allowing the setting of cuts on HF-hadron children.
38 // Quarks, hadrons and decay particles are loaded in the stack outside the loop
39 // of HF-hadrons, when the cuts on their children are satisfied (L. Manceau)
40 // Oct 11: added Pb-Pb at 2.76 TeV (S. Grigoryan)
42 //-------------------------------------------------------------------------
43 // How it works (for the given flavor and p-p energy):
45 // 1) Reads QQbar kinematical grid (TTree) from the Input file and generates
46 // quark pairs according to the weights of the cells.
47 // It is a 5D grid in y1,y2,pt1,pt2 and deltaphi, with occupancy weights
48 // of the cells obtained from Pythia (see details in GetQuarkPair).
49 // 2) Reads "soft" and "hard" fragmentation functions (12 2D-histograms each,
50 // for 12 pt bins) from the Input file, applies to quarks and produces hadrons
51 // (only lower states, with proportions of species obtained from Pythia).
52 // Fragmentation functions are the same for all hadron species and depend
53 // on 2 variables - light cone energy-momentum fractions:
54 // z1=(E_H + Pz_H)/(E_Q + Pz_Q), z2=(E_H - Pz_H)/(E_Q - Pz_Q).
55 // "soft" & "hard" FFs correspond to "slower" & "faster" quark of a pair
56 // (see details in GetHadronPair). Fragmentation does not depend on p-p energy.
57 // 3) Decays the hadrons and saves all the particles in the event stack in the
58 // following order: HF hadron from Q, then its decay products, then HF hadron
59 // from Qbar, then its decay productes, then next HF hadon pair (if any)
60 // in the same way, etc...
61 // 4) It is fast, e.g., generates the same number of events with a beauty pair
62 // ~15 times faster than AliGenPythia with kBeautyppMNRwmi (w/o tracking)
64 // An Input file for each quark flavor and p-p energy is in EVGEN/dataCorrHF/
65 // One can use also user-defined Input files.
67 // More details could be found in my presentation at DiMuonNet Workshop, Dec 2006:
68 // http://www-dapnia.cea.fr/Sphn/Alice/DiMuonNet.
70 //-------------------------------------------------------------------------
73 // add the following typical lines in Config.C
75 if (!strcmp(option,"corr")) {
76 // An example for correlated charm or beauty hadron pair production at 14 TeV
78 // AliGenCorrHF *gener = new AliGenCorrHF(1, 4, 14); // for charm, 1 pair per event
79 AliGenCorrHF *gener = new AliGenCorrHF(1, 5, 14); // for beauty, 1 pair per event
81 gener->SetMomentumRange(0,9999);
82 gener->SetCutOnChild(0); // 1/0 means cuts on children enable/disable
83 gener->SetChildThetaRange(171.0,178.0);
84 gener->SetOrigin(0,0,0); //vertex position
85 gener->SetSigma(0,0,0); //Sigma in (X,Y,Z) (cm) on IP position
86 gener->SetForceDecay(kSemiMuonic);
87 gener->SetTrackingFlag(0);
91 // and in aliroot do e.g. gAlice->Run(10,"Config.C") to produce 10 events.
92 // One can include AliGenCorrHF in an AliGenCocktail generator.
93 //--------------------------------------------------------------------------
95 #include <Riostream.h>
97 #include <TClonesArray.h>
98 #include <TDatabasePDG.h>
101 #include <TLorentzVector.h>
103 #include <TParticle.h>
104 #include <TParticlePDG.h>
108 #include <TVirtualMC.h>
109 #include <TVector3.h>
111 #include "AliGenCorrHF.h"
113 #include "AliConst.h"
114 #include "AliDecayer.h"
117 #include "AliGenEventHeader.h"
119 ClassImp(AliGenCorrHF)
123 <img src="picts/AliGenCorrHF.gif">
127 Double_t AliGenCorrHF::fgdph[19] = {0, 10, 20, 30, 40, 50, 60, 70, 80, 90, 100, 110, 120, 130, 140, 150, 160, 170, 180};
128 Double_t AliGenCorrHF::fgy[31] = {-10,-7, -6.5, -6, -5.5, -5, -4.5, -4, -3.5, -3, -2.5, -2,- 1.5, -1, -0.5, 0, 0.5, 1, 1.5, 2, 2.5, 3, 3.5, 4, 4.5, 5, 5.5, 6, 6.5, 7, 10};
129 Double_t AliGenCorrHF::fgpt[51] = {0, 0.5, 1, 1.5, 2, 2.5, 3, 3.5, 4, 4.5, 5, 5.5, 6, 6.6, 7.2, 7.8, 8.4, 9, 9.6, 10.3, 11.1, 12, 13, 14, 15, 16, 17, 18, 19, 20.1, 21.5, 23, 24.5, 26, 27.5, 29.1, 31, 33, 35, 37, 39.2, 42, 45, 48, 51, 55.2, 60, 65, 71, 81, 100};
130 Int_t AliGenCorrHF::fgnptbins = 12;
131 Double_t AliGenCorrHF::fgptbmin[12] = {0, 0.5, 1, 1.5, 2, 2.5, 3, 4, 5, 6, 7, 9};
132 Double_t AliGenCorrHF::fgptbmax[12] = {0.5, 1, 1.5, 2, 2.5, 3, 4, 5, 6, 7, 9, 100};
134 //____________________________________________________________
135 AliGenCorrHF::AliGenCorrHF():
146 // Default constructor
149 //____________________________________________________________
150 AliGenCorrHF::AliGenCorrHF(Int_t npart, Int_t idquark, Int_t energy):
162 // Constructor using particle number, quark type, energy & default InputFile
166 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPP7PythiaMNRwmi.root";
167 else if (fEnergy == 10)
168 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPP10PythiaMNRwmi.root";
169 else if (fEnergy == 14)
170 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPP14PythiaMNRwmi.root";
171 else if (fEnergy == 3)
172 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPbPb276PythiaMNR.root";
173 else if (fEnergy == 4)
174 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPbPb394PythiaMNR.root";
175 else if (fEnergy == 9 || fEnergy == -9)
176 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPPb88PythiaMNR.root";
177 else fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/BeautyPbPb394PythiaMNR.root";
182 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPP7PythiaMNRwmi.root";
183 else if (fEnergy == 10)
184 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPP10PythiaMNRwmi.root";
185 else if (fEnergy == 14)
186 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPP14PythiaMNRwmi.root";
187 else if (fEnergy == 3)
188 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPbPb276PythiaMNR.root";
189 else if (fEnergy == 4)
190 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPbPb394PythiaMNR.root";
191 else if (fEnergy == 9 || fEnergy == -9)
192 fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPPb88PythiaMNR.root";
193 else fFileName = "$ALICE_ROOT/EVGEN/dataCorrHF/CharmPbPb394PythiaMNR.root";
196 fTitle= "Generator for correlated pairs of HF hadrons";
199 for (Int_t i=0; i<5; i++) fChildSelect[i]=0;
202 SetChildMomentumRange();
205 SetChildThetaRange();
208 //___________________________________________________________________
209 AliGenCorrHF::AliGenCorrHF(char* tname, Int_t npart, Int_t idquark, Int_t energy):
221 // Constructor using particle number, quark type, energy & user-defined InputFile
223 if (fQuark != 5) fQuark = 4;
224 fName = "UserDefined";
225 fTitle= "Generator for correlated pairs of HF hadrons";
228 for (Int_t i=0; i<5; i++) fChildSelect[i]=0;
231 SetChildMomentumRange();
234 SetChildThetaRange();
237 //____________________________________________________________
238 AliGenCorrHF::~AliGenCorrHF()
244 //____________________________________________________________
245 void AliGenCorrHF::Init()
248 AliInfo(Form("Number of HF-hadron pairs = %d",fNpart));
249 AliInfo(Form(" QQbar kinematics and fragm. functions from: %s",fFileName.Data() ));
250 fFile = TFile::Open(fFileName.Data());
251 if(!fFile->IsOpen()){
252 AliError(Form("Could not open file %s",fFileName.Data() ));
255 ComputeIntegral(fFile);
257 fParentWeight = 1./fNpart; // fNpart is number of HF-hadron pairs
259 // particle decay related initialization
261 if (gMC) fDecayer = gMC->GetDecayer();
262 fDecayer->SetForceDecay(fForceDecay);
268 //____________________________________________________________
269 void AliGenCorrHF::Generate()
272 // Generate fNpart of correlated HF hadron pairs per event
273 // in the the desired theta and momentum windows (phi = 0 - 2pi).
276 // Reinitialize decayer
278 fDecayer->SetForceDecay(fForceDecay);
281 Float_t polar[2][3]; // Polarisation of the parent particle (for GEANT tracking)
282 Float_t origin0[2][3]; // Origin of the generated parent particle (for GEANT tracking)
283 Float_t pt, pl, ptot; // Transverse, logitudinal and total momenta of the parent particle
284 Float_t phi, theta; // Phi and theta spherical angles of the parent particle momentum
285 Float_t p[2][3]; // Momenta
286 Int_t nt, i, j, ihad, ipa, ipa0, ipa1, ihadron[2], iquark[2];
287 Float_t wgtp[2], wgtch[2], random[6];
288 Float_t pq[2][3], pc[3]; // Momenta of the two quarks
289 Double_t tanhy2, qm = 0;
291 Double_t dphi=0, ptq[2], yq[2], pth[2], plh[2], ph[2], phih[2], phiq[2];
293 Int_t** pSelected = new Int_t* [2];
294 Int_t** trackIt = new Int_t* [2];
296 for (i=0; i<2; i++) {
305 for (j=0; j<3; j++) polar[i][j]=0;
308 // same quarks mass as in the fragmentation functions
309 if (fQuark == 4) qm = 1.20;
312 TClonesArray *particleshad1 = new TClonesArray("TParticle",1000);
313 TClonesArray *particleshad2 = new TClonesArray("TParticle",1000);
315 TList *particleslist = new TList();
316 particleslist->Add(particleshad1);
317 particleslist->Add(particleshad2);
319 TDatabasePDG *pDataBase = TDatabasePDG::Instance();
321 // Calculating vertex position per event
323 for (j=0;j<3;j++) origin0[i][j]=fOrigin[j];
324 if (fVertexSmear==kPerEvent) {
326 for (j=0;j<3;j++) origin0[i][j]=fVertex[j];
334 // Generating fNpart HF-hadron pairs
337 while (ipa<2*fNpart) {
339 GetQuarkPair(fFile, fgIntegral, yq[0], yq[1], ptq[0], ptq[1], dphi);
341 GetHadronPair(fFile, fQuark, yq[0], yq[1], ptq[0], ptq[1], ihadron[0], ihadron[1], plh[0], plh[1], pth[0], pth[1]);
343 if (fEnergy == 9 || fEnergy == -9) { // boost particles from c.m.s. to ALICE lab frame
344 Double_t dyBoost = 0.47;
345 Double_t beta = TMath::TanH(dyBoost);
346 Double_t gamma = 1./TMath::Sqrt((1.-beta)*(1.+beta));
347 Double_t gb = gamma * beta;
350 plh[0] = gb * TMath::Sqrt(plh[0]*plh[0] + pth[0]*pth[0]) + gamma * plh[0];
351 plh[1] = gb * TMath::Sqrt(plh[1]*plh[1] + pth[1]*pth[1]) + gamma * plh[1];
360 // Cuts from AliGenerator
363 theta=TMath::ATan2(pth[0],plh[0]);
364 if (theta<fThetaMin || theta>fThetaMax) continue;
365 theta=TMath::ATan2(pth[1],plh[1]);
366 if (theta<fThetaMin || theta>fThetaMax) continue;
369 ph[0]=TMath::Sqrt(pth[0]*pth[0]+plh[0]*plh[0]);
370 if (ph[0]<fPMin || ph[0]>fPMax) continue;
371 ph[1]=TMath::Sqrt(pth[1]*pth[1]+plh[1]*plh[1]);
372 if (ph[1]<fPMin || ph[1]>fPMax) continue;
374 // Add the quarks in the stack
376 phiq[0] = Rndm()*k2PI;
378 phiq[1] = phiq[0] + dphi*kDegrad;
380 phiq[1] = phiq[0] - dphi*kDegrad;
382 if (phiq[1] > k2PI) phiq[1] -= k2PI;
383 if (phiq[1] < 0 ) phiq[1] += k2PI;
390 TVector2 qvect1 = TVector2();
391 TVector2 qvect2 = TVector2();
392 qvect1.SetMagPhi(ptq[0],phiq[0]);
393 qvect2.SetMagPhi(ptq[1],phiq[1]);
394 pq[0][0] = qvect1.Px();
395 pq[0][1] = qvect1.Py();
396 pq[1][0] = qvect2.Px();
397 pq[1][1] = qvect2.Py();
400 tanhy2 = TMath::TanH(yq[0]);
402 pq[0][2] = TMath::Sqrt((ptq[0]*ptq[0]+qm*qm)*tanhy2/(1-tanhy2));
403 pq[0][2] = TMath::Sign((Double_t)pq[0][2],yq[0]);
404 tanhy2 = TMath::TanH(yq[1]);
406 pq[1][2] = TMath::Sqrt((ptq[1]*ptq[1]+qm*qm)*tanhy2/(1-tanhy2));
407 pq[1][2] = TMath::Sign((Double_t)pq[1][2],yq[1]);
409 // Here we assume that |phi_H1 - phi_H2| = |phi_Q1 - phi_Q2| = dphi
410 // which is a good approximation for heavy flavors in Pythia
411 // ... moreover, same phi angles as for the quarks ...
418 for (ihad = 0; ihad < 2; ihad++) {
424 fChildWeight=(fDecayer->GetPartialBranchingRatio(ihadron[ihad]))*fParentWeight;
425 wgtp[ihad]=fParentWeight;
426 wgtch[ihad]=fChildWeight;
427 TParticlePDG *particle = pDataBase->GetParticle(ihadron[ihad]);
428 Float_t am = particle->Mass();
432 ptot=TMath::Sqrt(pt*pt+pl*pl);
434 p[ihad][0]=pt*TMath::Cos(phi);
435 p[ihad][1]=pt*TMath::Sin(phi);
438 if(fVertexSmear==kPerTrack) {
442 fOrigin[j]+fOsigma[j]*TMath::Cos(2*random[2*j]*TMath::Pi())*
443 TMath::Sqrt(-2*TMath::Log(random[2*j+1]));
447 // Looking at fForceDecay :
448 // if fForceDecay != none Primary particle decays using
449 // AliPythia and children are tracked by GEANT
451 // if fForceDecay == none Primary particle is tracked by GEANT
452 // (In the latest, make sure that GEANT actually does all the decays you want)
454 if (fForceDecay != kNoDecay) {
455 // Using lujet to decay particle
456 Float_t energy=TMath::Sqrt(ptot*ptot+am*am);
457 TLorentzVector pmom(p[ihad][0], p[ihad][1], p[ihad][2], energy);
458 fDecayer->Decay(ihadron[ihad],&pmom);
460 // select decay particles
462 np[ihad]=fDecayer->ImportParticles((TClonesArray *)particleslist->At(ihad));
464 // Selecting GeometryAcceptance for particles fPdgCodeParticleforAcceptanceCut;
466 if (fGeometryAcceptance)
467 if (!CheckAcceptanceGeometry(np[ihad],(TClonesArray*)particleslist->At(ihad))) continue;
469 trackIt[ihad] = new Int_t [np[ihad]];
470 pSelected[ihad] = new Int_t [np[ihad]];
471 Int_t* pFlag = new Int_t [np[ihad]];
473 for (i=0; i<np[ihad]; i++) {
475 pSelected[ihad][i] = 0;
479 TParticle* iparticle = 0;
482 for (i = 1; i<np[ihad] ; i++) {
483 trackIt[ihad][i] = 1;
485 (TParticle *) ((TClonesArray *) particleslist->At(ihad))->At(i);
486 Int_t kf = iparticle->GetPdgCode();
487 Int_t ks = iparticle->GetStatusCode();
490 ipF = iparticle->GetFirstDaughter();
491 ipL = iparticle->GetLastDaughter();
492 if (ipF > 0) for (j=ipF-1; j<ipL; j++) pFlag[j]=1;
496 // flag decay products of particles with long life-time (c tau > .3 mum)
498 Double_t lifeTime = fDecayer->GetLifetime(kf);
499 if (lifeTime > (Double_t) fMaxLifeTime) {
500 ipF = iparticle->GetFirstDaughter();
501 ipL = iparticle->GetLastDaughter();
502 if (ipF > 0) for (j=ipF-1; j<ipL; j++) pFlag[j]=1;
504 trackIt[ihad][i] = 0;
505 pSelected[ihad][i] = 1;
510 if ((ChildSelected(TMath::Abs(kf)) || fForceDecay == kAll || fSelectAll) && trackIt[ihad][i])
513 pc[0]=iparticle->Px();
514 pc[1]=iparticle->Py();
515 pc[2]=iparticle->Pz();
516 //printf("px %f py %f pz %f\n",pc[0],pc[1],pc[2]);
517 Bool_t childok = KinematicSelection(iparticle, 1);
519 pSelected[ihad][i] = 1;
526 pSelected[ihad][i] = 1;
528 } // if child selection
530 } // decay particle loop
531 } // if decay products
533 if ((fCutOnChild && ncsel[ihad] >0) || !fCutOnChild) ipa1++;
535 if (pFlag) delete[] pFlag;
537 } // kinematic selection
538 else // nodecay option, so parent will be tracked by GEANT (pions, kaons, eta, omegas, baryons)
541 PushTrack(fTrackIt,-1,ihadron[ihad],p[ihad],origin0[ihad],polar[ihad],0,kPPrimary,nt,wgtp[ihad]);
550 if (pSelected[ihad]) delete pSelected[ihad];
551 if (trackIt[ihad]) delete trackIt[ihad];
552 particleshad1->Clear();
553 particleshad2->Clear();
555 }//go out of loop and generate new pair if at least one hadron is rejected
556 } // hadron pair loop
561 if(fForceDecay != kNoDecay){
562 for(ihad=0;ihad<2;ihad++){
564 //load tracks in the stack if both hadrons of the pair accepted
565 LoadTracks(iquark[ihad],pq[ihad],ihadron[ihad],p[ihad],np[ihad],
566 (TClonesArray *)particleslist->At(ihad),origin0[ihad],
567 polar[ihad],wgtp[ihad],wgtch[ihad],nt,ncsel[ihad],
568 pSelected[ihad],trackIt[ihad]);
570 if (pSelected[ihad]) delete pSelected[ihad];
571 if (trackIt[ihad]) delete trackIt[ihad];
574 particleshad1->Clear();
575 particleshad2->Clear();
578 } // while (ipa<2*fNpart) loop
580 SetHighWaterMark(nt);
582 AliGenEventHeader* header = new AliGenEventHeader("CorrHF");
583 header->SetPrimaryVertex(fVertex);
584 header->SetNProduced(fNprimaries);
588 delete particleshad1;
589 delete particleshad2;
590 delete particleslist;
595 //____________________________________________________________________________________
596 void AliGenCorrHF::IpCharm(TH2F *hProbHH, Int_t &pdg3, Int_t &pdg4)
598 // Composition of a lower state charm hadron pair from a ccbar quark pair
599 Int_t pdgH[] = {411, 421, 431, 4122, 4132, 4232, 4332};
602 hProbHH->GetRandom2(id3, id4);
603 pdg3 = pdgH[(Int_t)TMath::Floor(id3)];
604 pdg4 = -1*pdgH[(Int_t)TMath::Floor(id4)];
609 void AliGenCorrHF::IpBeauty(TH2F *hProbHH, Int_t &pdg3, Int_t &pdg4)
611 // Composition of a lower state beauty hadron pair from a bbbar quark pair
612 // B-Bbar mixing will be done by Pythia at their decay point
613 Int_t pdgH[] = {511, 521, 531, 5122, 5132, 5232, 5332};
616 hProbHH->GetRandom2(id3, id4);
617 pdg3 = pdgH[(Int_t)TMath::Floor(id3)];
618 pdg4 = -1*pdgH[(Int_t)TMath::Floor(id4)];
620 if ( (pdg3== 511) || (pdg3== 521) || (pdg3== 531) ) pdg3 *= -1;
621 if ( (pdg4==-511) || (pdg4==-521) || (pdg4==-531) ) pdg4 *= -1;
626 //____________________________________________________________________________________
627 Double_t AliGenCorrHF::ComputeIntegral(TFile* fG) // needed by GetQuarkPair
629 // Read QQbar kinematical 5D grid's cell occupancy weights
630 Int_t cell[6]; // cell[6]={wght,iy1,iy2,ipt1,ipt2,idph}
631 TTree* tG = (TTree*) fG->Get("tGqq");
632 tG->GetBranch("cell")->SetAddress(&cell);
633 Int_t nbins = tG->GetEntries();
635 // delete previously computed integral (if any)
636 if(fgIntegral) delete [] fgIntegral;
638 fgIntegral = new Double_t[nbins+1];
641 for(bin=0;bin<nbins;bin++) {
643 fgIntegral[bin+1] = fgIntegral[bin] + cell[0];
645 // Normalize integral to 1
646 if (fgIntegral[nbins] == 0 ) {
649 for (bin=1;bin<=nbins;bin++) fgIntegral[bin] /= fgIntegral[nbins];
651 return fgIntegral[nbins];
655 //____________________________________________________________________________________
656 void AliGenCorrHF::GetQuarkPair(TFile* fG, Double_t* fInt, Double_t &y1, Double_t &y2, Double_t &pt1, Double_t &pt2, Double_t &dphi)
657 // modification of ROOT's TH3::GetRandom3 for 5D
659 // Read QQbar kinematical 5D grid's cell coordinates
660 Int_t cell[6]; // cell[6]={wght,iy1,iy2,ipt1,ipt2,idph}
661 TTree* tG = (TTree*) fG->Get("tGqq");
662 tG->GetBranch("cell")->SetAddress(&cell);
663 Int_t nbins = tG->GetEntries();
665 gRandom->RndmArray(6,rand);
666 Int_t ibin = TMath::BinarySearch(nbins,fInt,rand[0]);
668 y1 = fgy[cell[1]] + (fgy[cell[1]+1]-fgy[cell[1]])*rand[1];
669 y2 = fgy[cell[2]] + (fgy[cell[2]+1]-fgy[cell[2]])*rand[2];
670 pt1 = fgpt[cell[3]] + (fgpt[cell[3]+1]-fgpt[cell[3]])*rand[3];
671 pt2 = fgpt[cell[4]] + (fgpt[cell[4]+1]-fgpt[cell[4]])*rand[4];
672 dphi = fgdph[cell[5]]+ (fgdph[cell[5]+1]-fgdph[cell[5]])*rand[5];
675 //____________________________________________________________________________________
676 void AliGenCorrHF::GetHadronPair(TFile* fG, Int_t idq, Double_t y1, Double_t y2, Double_t pt1, Double_t pt2, Int_t &id3, Int_t &id4, Double_t &pz3, Double_t &pz4, Double_t &pt3, Double_t &pt4)
678 // Generate a hadron pair
679 void (*fIpParaFunc)(TH2F *, Int_t &, Int_t &);//Pointer to hadron pair composition function
680 fIpParaFunc = IpCharm;
681 Double_t mq = 1.2; // c & b quark masses (used in AliPythia)
683 fIpParaFunc = IpBeauty;
690 Double_t pz1, pz2, e1, e2, mh, ptemp, rand[2];
692 TH2F *h2h[12], *h2s[12], *hProbHH; // hard & soft fragmentation and HH-probability functions
693 for (Int_t ipt = 0; ipt<fgnptbins; ipt++) {
694 snprintf(tag,100, "h2h_pt%d",ipt);
695 h2h[ipt] = (TH2F*) fG->Get(tag);
696 snprintf(tag,100, "h2s_pt%d",ipt);
697 h2s[ipt] = (TH2F*) fG->Get(tag);
701 for (Int_t ipt = 0; ipt<fgnptbins; ipt++) {
702 if(pt1 >= fgptbmin[ipt] && pt1 < fgptbmax[ipt])
703 h2h[ipt]->GetRandom2(z11, z21);
704 if(pt2 >= fgptbmin[ipt] && pt2 < fgptbmax[ipt])
705 h2h[ipt]->GetRandom2(z12, z22);
709 if (TMath::Abs(y1) > TMath::Abs(y2)) {
710 for (Int_t ipt = 0; ipt<fgnptbins; ipt++) {
711 if(pt1 >= fgptbmin[ipt] && pt1 < fgptbmax[ipt])
712 h2h[ipt]->GetRandom2(z11, z21);
713 if(pt2 >= fgptbmin[ipt] && pt2 < fgptbmax[ipt])
714 h2s[ipt]->GetRandom2(z12, z22);
718 for (Int_t ipt = 0; ipt<fgnptbins; ipt++) {
719 if(pt1 >= fgptbmin[ipt] && pt1 < fgptbmax[ipt])
720 h2s[ipt]->GetRandom2(z11, z21);
721 if(pt2 >= fgptbmin[ipt] && pt2 < fgptbmax[ipt])
722 h2h[ipt]->GetRandom2(z12, z22);
726 gRandom->RndmArray(2,rand);
727 ptemp = TMath::Sqrt(pt1*pt1 + mq*mq);
728 pz1 = ptemp*TMath::SinH(y1);
729 e1 = ptemp*TMath::CosH(y1);
730 ptemp = TMath::Sqrt(pt2*pt2 + mq*mq);
731 pz2 = ptemp*TMath::SinH(y2);
732 e2 = ptemp*TMath::CosH(y2);
734 hProbHH = (TH2F*)fG->Get("hProbHH");
735 fIpParaFunc(hProbHH, id3, id4);
736 mh = TDatabasePDG::Instance()->GetParticle(id3)->Mass();
737 ptemp = z11*z21*(e1*e1-pz1*pz1) - mh*mh;
738 if (idq==5) pt3 = pt1; // an approximation at low pt, try better
739 else pt3 = rand[0]; // pt3=pt1 gives less D-hadrons at low pt
740 if (ptemp > 0) pt3 = TMath::Sqrt(ptemp);
741 if (pz1 > 0) pz3 = (z11*(e1 + pz1) - z21*(e1 - pz1)) / 2;
742 else pz3 = (z21*(e1 + pz1) - z11*(e1 - pz1)) / 2;
743 e1 = TMath::Sqrt(pz3*pz3 + pt3*pt3 + mh*mh);
745 mh = TDatabasePDG::Instance()->GetParticle(id4)->Mass();
746 ptemp = z12*z22*(e2*e2-pz2*pz2) - mh*mh;
747 if (idq==5) pt4 = pt2; // an approximation at low pt, try better
749 if (ptemp > 0) pt4 = TMath::Sqrt(ptemp);
750 if (pz2 > 0) pz4 = (z12*(e2 + pz2) - z22*(e2 - pz2)) / 2;
751 else pz4 = (z22*(e2 + pz2) - z12*(e2 - pz2)) / 2;
752 e2 = TMath::Sqrt(pz4*pz4 + pt4*pt4 + mh*mh);
754 // small corr. instead of using Frag. Func. depending on yQ (in addition to ptQ)
755 Float_t ycorr = 0.2, y3, y4;
756 gRandom->RndmArray(2,rand);
757 y3 = 0.5 * TMath::Log((e1 + pz3 + 1.e-13)/(e1 - pz3 + 1.e-13));
758 y4 = 0.5 * TMath::Log((e2 + pz4 + 1.e-13)/(e2 - pz4 + 1.e-13));
759 if(TMath::Abs(y3)<ycorr && TMath::Abs(y4)<ycorr && rand[0]>0.5) {
760 ptemp = TMath::Sqrt((e1-pz3)*(e1+pz3));
761 y3 = 4*(1 - 2*rand[1]);
762 pz3 = ptemp*TMath::SinH(y3);
768 //____________________________________________________________________________________
769 void AliGenCorrHF::LoadTracks(Int_t iquark, Float_t *pq,
770 Int_t iPart, Float_t *p,
771 Int_t np, TClonesArray *particles,
772 Float_t *origin0, Float_t *polar,
773 Float_t wgtp, Float_t wgtch,
774 Int_t &nt, Int_t ncsel, Int_t *pSelected,
778 Int_t* pParent = new Int_t[np];
779 Float_t pc[3], och[3];
782 for(i=0;i<np;i++) pParent[i]=-1;
784 if ((fCutOnChild && ncsel >0) || !fCutOnChild){
787 PushTrack(0, -1, iquark, pq, origin0, polar, 0, kPPrimary, nt, wgtp);
791 PushTrack(0, ntq, iPart, p, origin0, polar, 0, kPDecay, nt, wgtp);
797 for (i = 1; i < np; i++) {
800 TParticle* iparticle = (TParticle *) particles->At(i);
801 Int_t kf = iparticle->GetPdgCode();
802 Int_t jpa = iparticle->GetFirstMother()-1;
804 och[0] = origin0[0]+iparticle->Vx()/10;
805 och[1] = origin0[1]+iparticle->Vy()/10;
806 och[2] = origin0[2]+iparticle->Vz()/10;
807 pc[0] = iparticle->Px();
808 pc[1] = iparticle->Py();
809 pc[2] = iparticle->Pz();
812 iparent = pParent[jpa];
817 PushTrack(fTrackIt*trackIt[i], iparent, kf,
819 0, kPDecay, nt, wgtch);
827 if (pParent) delete[] pParent;