/************************************************************************** * Copyright(c) 1998-1999, ALICE Experiment at CERN, All rights reserved. * * * * Author: The ALICE Off-line Project. * * Contributors are mentioned in the code where appropriate. * * * * Permission to use, copy, modify and distribute this software and its * * documentation strictly for non-commercial purposes is hereby granted * * without fee, provided that the above copyright notice appears in all * * copies and that both the copyright notice and this permission notice * * appear in the supporting documentation. The authors make no claims * * about the suitability of this software for any purpose. It is * * provided "as is" without express or implied warranty. * **************************************************************************/ /* $Id$ */ /////////////////////////////////////////////////////////////////////////////// // // // Transition Radiation Detector version 1 -- slow simulator // // // //Begin_Html /* */ //End_Html // // // // /////////////////////////////////////////////////////////////////////////////// #include #include #include #include #include #include #include #include "AliConst.h" #include "AliLog.h" #include "AliMC.h" #include "AliRun.h" #include "AliTRDgeometry.h" #include "AliTRDhit.h" #include "AliTRDsim.h" #include "AliTRDv1.h" ClassImp(AliTRDv1) //_____________________________________________________________________________ AliTRDv1::AliTRDv1():AliTRD() { // // Default constructor // fSensSelect = 0; fSensPlane = -1; fSensChamber = -1; fSensSector = -1; fSensSectorRange = 0; fDeltaE = NULL; fDeltaG = NULL; fTR = NULL; fTRon = kFALSE; fStepSize = 0.1; fTypeOfStepManager = 1; } //_____________________________________________________________________________ AliTRDv1::AliTRDv1(const char *name, const char *title) :AliTRD(name, title) { // // Standard constructor for Transition Radiation Detector version 1 // fSensSelect = 0; fSensPlane = -1; fSensChamber = -1; fSensSector = -1; fSensSectorRange = 0; fDeltaE = NULL; fDeltaG = NULL; fTR = NULL; fTRon = kTRUE; fStepSize = 0.1; fTypeOfStepManager = 1; SetBufferSize(128000); } //_____________________________________________________________________________ AliTRDv1::AliTRDv1(const AliTRDv1 &trd):AliTRD(trd) { // // Copy constructor // ((AliTRDv1 &) trd).Copy(*this); } //_____________________________________________________________________________ AliTRDv1::~AliTRDv1() { // // AliTRDv1 destructor // if (fDeltaE) delete fDeltaE; if (fDeltaG) delete fDeltaG; if (fTR) delete fTR; } //_____________________________________________________________________________ AliTRDv1 &AliTRDv1::operator=(const AliTRDv1 &trd) { // // Assignment operator // if (this != &trd) ((AliTRDv1 &) trd).Copy(*this); return *this; } //_____________________________________________________________________________ void AliTRDv1::Copy(TObject &trd) const { printf("void AliTRDv1::Copy(TObject &trd) const\n"); // // Copy function // ((AliTRDv1 &) trd).fSensSelect = fSensSelect; ((AliTRDv1 &) trd).fSensPlane = fSensPlane; ((AliTRDv1 &) trd).fSensChamber = fSensChamber; ((AliTRDv1 &) trd).fSensSector = fSensSector; ((AliTRDv1 &) trd).fSensSectorRange = fSensSectorRange; ((AliTRDv1 &) trd).fTypeOfStepManager = fTypeOfStepManager; ((AliTRDv1 &) trd).fStepSize = fStepSize; ((AliTRDv1 &) trd).fTRon = fTRon; fDeltaE->Copy(*((AliTRDv1 &) trd).fDeltaE); fDeltaG->Copy(*((AliTRDv1 &) trd).fDeltaG); fTR->Copy(*((AliTRDv1 &) trd).fTR); } //_____________________________________________________________________________ void AliTRDv1::CreateGeometry() { // // Create the GEANT geometry for the Transition Radiation Detector - Version 1 // This version covers the full azimuth. // // Check that FRAME is there otherwise we have no place where to put the TRD AliModule* frame = gAlice->GetModule("FRAME"); if (!frame) return; // Define the chambers AliTRD::CreateGeometry(); } //_____________________________________________________________________________ void AliTRDv1::CreateMaterials() { // // Create materials for the Transition Radiation Detector version 1 // AliTRD::CreateMaterials(); } //_____________________________________________________________________________ void AliTRDv1::CreateTRhit(Int_t det) { // // Creates an electron cluster from a TR photon. // The photon is assumed to be created a the end of the radiator. The // distance after which it deposits its energy takes into account the // absorbtion of the entrance window and of the gas mixture in drift // volume. // // PDG code electron const Int_t kPdgElectron = 11; // Ionization energy const Float_t kWion = 23.53; // Maximum number of TR photons per track const Int_t kNTR = 50; TLorentzVector mom, pos; // Create TR at the entrance of the chamber if (gMC->IsTrackEntering()) { // Create TR only for electrons Int_t iPdg = gMC->TrackPid(); if (TMath::Abs(iPdg) != kPdgElectron) return; Float_t eTR[kNTR]; Int_t nTR; // Create TR photons gMC->TrackMomentum(mom); Float_t pTot = mom.Rho(); fTR->CreatePhotons(iPdg,pTot,nTR,eTR); if (nTR > kNTR) { AliFatal(Form("Boundary error: nTR = %d, kNTR = %d",nTR,kNTR)); } // Loop through the TR photons for (Int_t iTR = 0; iTR < nTR; iTR++) { Float_t energyMeV = eTR[iTR] * 0.001; Float_t energyeV = eTR[iTR] * 1000.0; Float_t absLength = 0; Float_t sigma = 0; // Take the absorbtion in the entrance window into account Double_t muMy = fTR->GetMuMy(energyMeV); sigma = muMy * fFoilDensity; if (sigma > 0.0) { absLength = gRandom->Exp(1.0/sigma); if (absLength < AliTRDgeometry::MyThick()) continue; } else { continue; } // The absorbtion cross sections in the drift gas // Gas-mixture (Xe/CO2) Double_t muXe = fTR->GetMuXe(energyMeV); Double_t muCO = fTR->GetMuCO(energyMeV); sigma = (0.85 * muXe + 0.15 * muCO) * fGasDensity * fTR->GetTemp(); // The distance after which the energy of the TR photon // is deposited. if (sigma > 0.0) { absLength = gRandom->Exp(1.0/sigma); if (absLength > (AliTRDgeometry::DrThick() + AliTRDgeometry::AmThick())) { continue; } } else { continue; } // The position of the absorbtion Float_t posHit[3]; gMC->TrackPosition(pos); posHit[0] = pos[0] + mom[0] / pTot * absLength; posHit[1] = pos[1] + mom[1] / pTot * absLength; posHit[2] = pos[2] + mom[2] / pTot * absLength; // Create the charge Int_t q = ((Int_t) (energyeV / kWion)); // Add the hit to the array. TR photon hits are marked // by negative charge AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber(),det,posHit,-q,kTRUE); } } } //_____________________________________________________________________________ void AliTRDv1::Init() { // // Initialise Transition Radiation Detector after geometry has been built. // AliTRD::Init(); AliDebug(1,"Slow simulator\n"); if (fSensSelect) { if (fSensPlane >= 0) AliInfo(Form("Only plane %d is sensitive")); if (fSensChamber >= 0) AliInfo(Form("Only chamber %d is sensitive",fSensChamber)); if (fSensSector >= 0) { Int_t sens1 = fSensSector; Int_t sens2 = fSensSector + fSensSectorRange; sens2 -= ((Int_t) (sens2 / AliTRDgeometry::Nsect())) * AliTRDgeometry::Nsect(); AliInfo(Form("Only sectors %d - %d are sensitive\n",sens1,sens2-1)); } } // Switch on TR simulation as default if (!fTRon) { AliInfo("TR simulation off"); } else { fTR = new AliTRDsim(); } // First ionization potential (eV) for the gas mixture (90% Xe + 10% CO2) const Float_t kPoti = 12.1; // Maximum energy (50 keV); const Float_t kEend = 50000.0; // Ermilova distribution for the delta-ray spectrum Float_t poti = TMath::Log(kPoti); Float_t eEnd = TMath::Log(kEend); // Ermilova distribution for the delta-ray spectrum fDeltaE = new TF1("deltae" ,Ermilova ,poti,eEnd,0); // Geant3 distribution for the delta-ray spectrum fDeltaG = new TF1("deltag",IntSpecGeant,2.421257,28.536469,0); AliDebug(1,"+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++"); } //_____________________________________________________________________________ void AliTRDv1::SetSensPlane(Int_t iplane) { // // Defines the hit-sensitive plane (0-5) // if ((iplane < 0) || (iplane > 5)) { AliWarning(Form("Wrong input value:%d",iplane)); AliWarning("Use standard setting"); fSensPlane = -1; fSensSelect = 0; return; } fSensSelect = 1; fSensPlane = iplane; } //_____________________________________________________________________________ void AliTRDv1::SetSensChamber(Int_t ichamber) { // // Defines the hit-sensitive chamber (0-4) // if ((ichamber < 0) || (ichamber > 4)) { AliWarning(Form("Wrong input value: %d",ichamber)); AliWarning("Use standard setting"); fSensChamber = -1; fSensSelect = 0; return; } fSensSelect = 1; fSensChamber = ichamber; } //_____________________________________________________________________________ void AliTRDv1::SetSensSector(Int_t isector) { // // Defines the hit-sensitive sector (0-17) // SetSensSector(isector,1); } //_____________________________________________________________________________ void AliTRDv1::SetSensSector(Int_t isector, Int_t nsector) { // // Defines a range of hit-sensitive sectors. The range is defined by // (0-17) as the starting point and as the number // of sectors to be included. // if ((isector < 0) || (isector > 17)) { AliWarning(Form("Wrong input value : %d",isector)); AliWarning("Use standard setting"); fSensSector = -1; fSensSectorRange = 0; fSensSelect = 0; return; } if ((nsector < 1) || (nsector > 18)) { AliWarning(Form("Wrong input value : %d",nsector)); AliWarning("Use standard setting"); fSensSector = -1; fSensSectorRange = 0; fSensSelect = 0; return; } fSensSelect = 1; fSensSector = isector; fSensSectorRange = nsector; } //_____________________________________________________________________________ void AliTRDv1::StepManager() { // // Slow simulator. Every charged track produces electron cluster as hits // along its path across the drift volume. // switch (fTypeOfStepManager) { case 0 : StepManagerErmilova(); break; // 0 is Ermilova case 1 : StepManagerGeant(); break; // 1 is Geant case 2 : StepManagerFixedStep(); break; // 2 is fixed step default : AliWarning("Not a valid Step Manager."); } } //_____________________________________________________________________________ void AliTRDv1::SelectStepManager(Int_t t) { // // Selects a step manager type: // 0 - Ermilova // 1 - Geant3 // 2 - Fixed step size // /* if (t == 1) { AliWarning("Sorry, Geant parametrization step manager is not implemented yet. Please ask K.Oyama for detail."); } */ fTypeOfStepManager = t; AliInfo(Form("Step Manager type %d was selected",fTypeOfStepManager)); } //_____________________________________________________________________________ void AliTRDv1::StepManagerGeant() { // // Slow simulator. Every charged track produces electron cluster as hits // along its path across the drift volume. The step size is set acording // to Bethe-Bloch. The energy distribution of the delta electrons follows // a spectrum taken from Geant3. // Int_t pla = 0; Int_t cha = 0; Int_t sec = 0; Int_t det = 0; Int_t iPdg; Int_t qTot; Float_t hits[3]; Float_t charge; Float_t aMass; Double_t pTot = 0; Double_t eDelta; Double_t betaGamma, pp; Double_t stepSize=0; Bool_t drRegion = kFALSE; Bool_t amRegion = kFALSE; TString cIdCurrent; TString cIdSensDr = "J"; TString cIdSensAm = "K"; Char_t cIdChamber[3]; cIdChamber[2] = 0; TLorentzVector pos, mom; const Int_t kNplan = AliTRDgeometry::Nplan(); const Int_t kNcham = AliTRDgeometry::Ncham(); const Int_t kNdetsec = kNplan * kNcham; const Double_t kBig = 1.0E+12; // Infinitely big const Float_t kWion = 23.53; // Ionization energy const Float_t kPTotMaxEl = 0.002; // Maximum momentum for e+ e- g // Minimum energy for the step size adjustment const Float_t kEkinMinStep = 1.0e-5; // energy threshold for production of delta electrons const Float_t kECut = 1.0e4; // Parameters entering the parametrized range for delta electrons const float ra=5.37E-4, rb=0.9815, rc=3.123E-3; // Gas density -> To be made user adjustable ! const float rho=0.004945 ; //[0.85*0.00549+0.15*0.00186 (Xe-CO2 85-15)] // Plateau value of the energy-loss for electron in xenon // taken from: Allison + Comb, Ann. Rev. Nucl. Sci. (1980), 30, 253 //const Double_t kPlateau = 1.70; // the averaged value (26/3/99) const Float_t kPlateau = 1.55; const Float_t kPrim = 19.34; // dN1/dx|min for the gas mixture (90% Xe + 10% CO2) // First ionization potential (eV) for the gas mixture (90% Xe + 10% CO2) const Float_t kPoti = 12.1; const Int_t kPdgElectron = 11; // PDG code electron // Set the maximum step size to a very large number for all // neutral particles and those outside the driftvolume gMC->SetMaxStep(kBig); // Use only charged tracks if (( gMC->TrackCharge() ) && (!gMC->IsTrackStop() ) && (!gMC->IsTrackDisappeared())) { // Inside a sensitive volume? drRegion = kFALSE; amRegion = kFALSE; cIdCurrent = gMC->CurrentVolName(); if (cIdSensDr == cIdCurrent[1]) { drRegion = kTRUE; } if (cIdSensAm == cIdCurrent[1]) { amRegion = kTRUE; } if (drRegion || amRegion) { // The hit coordinates and charge gMC->TrackPosition(pos); hits[0] = pos[0]; hits[1] = pos[1]; hits[2] = pos[2]; // The sector number (0 - 17) // The numbering goes clockwise and starts at y = 0 Float_t phi = kRaddeg*TMath::ATan2(pos[0],pos[1]); if (phi < 90.) phi = phi + 270.; else phi = phi - 90.; sec = ((Int_t) (phi / 20)); // The plane and chamber number cIdChamber[0] = cIdCurrent[2]; cIdChamber[1] = cIdCurrent[3]; Int_t idChamber = (atoi(cIdChamber) % kNdetsec); cha = kNcham - ((Int_t) idChamber / kNplan) - 1; pla = ((Int_t) idChamber % kNplan); // Check on selected volumes Int_t addthishit = 1; if (fSensSelect) { if ((fSensPlane >= 0) && (pla != fSensPlane )) addthishit = 0; if ((fSensChamber >= 0) && (cha != fSensChamber)) addthishit = 0; if (fSensSector >= 0) { Int_t sens1 = fSensSector; Int_t sens2 = fSensSector + fSensSectorRange; sens2 -= ((Int_t) (sens2 / AliTRDgeometry::Nsect())) * AliTRDgeometry::Nsect(); if (sens1 < sens2) { if ((sec < sens1) || (sec >= sens2)) addthishit = 0; } else { if ((sec < sens1) && (sec >= sens2)) addthishit = 0; } } } // Add this hit if (addthishit) { // The detector number det = fGeometry->GetDetector(pla,cha,sec); // Special hits only in the drift region if (drRegion) { // Create a track reference at the entrance and // exit of each chamber that contain the // momentum components of the particle if (gMC->IsTrackEntering() || gMC->IsTrackExiting()) { gMC->TrackMomentum(mom); AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber()); } if (gMC->IsTrackEntering() && !gMC->IsNewTrack()) { // determine if hit belong to primary track fPrimaryTrackPid=gAlice->GetMCApp()->GetCurrentTrackNumber(); //determine track length when entering the detector fTrackLength0=gMC->TrackLength(); } // Create the hits from TR photons if (fTR) CreateTRhit(det); } // Calculate the energy of the delta-electrons // modified by Alex Bercuci (A.Bercuci@gsi.de) on 26.01.06 // take into account correlation with the underlying GEANT tracking // mechanism. see // http://www-linux.gsi.de/~abercuci/Contributions/TRD/index.html // determine the most significant process (last on the processes list) // which caused this hit TArrayI processes; gMC->StepProcesses(processes); int nofprocesses=processes.GetSize(), pid; if(!nofprocesses) pid=0; else pid= processes[nofprocesses-1]; // generate Edep according to GEANT parametrisation eDelta =TMath::Exp(fDeltaG->GetRandom()) - kPoti; eDelta=TMath::Max(eDelta,0.0); float pr_range=0.; float range=gMC->TrackLength()-fTrackLength0; // merge GEANT tracker information with localy cooked one if(gAlice->GetMCApp()->GetCurrentTrackNumber()==fPrimaryTrackPid) { // printf("primary pid=%d eDelta=%f\n",pid,eDelta); if(pid==27){ if(eDelta>=kECut){ pr_range=ra*eDelta*.001*(1.-rb/(1.+rc*eDelta*0.001))/rho; if(pr_range>=(3.7-range)) eDelta*=.1; } } else if(pid==1){ if(eDelta=((AliTRDgeometry::DrThick() + AliTRDgeometry::AmThick())-range)) eDelta*=.05; else eDelta*=.5; } } else eDelta=0.; } else eDelta=0.; // Generate the electron cluster size if(eDelta==0.) qTot=0; else qTot = ((Int_t) (eDelta / kWion) + 1); // Create a new dEdx hit AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber(),det,hits,qTot, drRegion); // Calculate the maximum step size for the next tracking step // Produce only one hit if Ekin is below cutoff aMass = gMC->TrackMass(); if ((gMC->Etot() - aMass) > kEkinMinStep) { // The energy loss according to Bethe Bloch iPdg = TMath::Abs(gMC->TrackPid()); if ( (iPdg != kPdgElectron) || ((iPdg == kPdgElectron) && (pTot < kPTotMaxEl))) { gMC->TrackMomentum(mom); pTot = mom.Rho(); betaGamma = pTot / aMass; pp = BetheBlochGeant(betaGamma); // Take charge > 1 into account charge = gMC->TrackCharge(); if (TMath::Abs(charge) > 1) pp = pp * charge*charge; } else { // Electrons above 20 Mev/c are at the plateau pp = kPrim * kPlateau; } Int_t nsteps = 0; do {nsteps = gRandom->Poisson(pp);} while(!nsteps); stepSize = 1./nsteps; gMC->SetMaxStep(stepSize); } } } } } //_____________________________________________________________________________ void AliTRDv1::StepManagerErmilova() { // // Slow simulator. Every charged track produces electron cluster as hits // along its path across the drift volume. The step size is set acording // to Bethe-Bloch. The energy distribution of the delta electrons follows // a spectrum taken from Ermilova et al. // Int_t pla = 0; Int_t cha = 0; Int_t sec = 0; Int_t det = 0; Int_t iPdg; Int_t qTot; Float_t hits[3]; Double_t random[1]; Float_t charge; Float_t aMass; Double_t pTot = 0; Double_t eDelta; Double_t betaGamma, pp; Double_t stepSize; Bool_t drRegion = kFALSE; Bool_t amRegion = kFALSE; TString cIdCurrent; TString cIdSensDr = "J"; TString cIdSensAm = "K"; Char_t cIdChamber[3]; cIdChamber[2] = 0; TLorentzVector pos, mom; const Int_t kNplan = AliTRDgeometry::Nplan(); const Int_t kNcham = AliTRDgeometry::Ncham(); const Int_t kNdetsec = kNplan * kNcham; const Double_t kBig = 1.0E+12; // Infinitely big const Float_t kWion = 23.53; // Ionization energy const Float_t kPTotMaxEl = 0.002; // Maximum momentum for e+ e- g // energy threshold for production of delta electrons //const Float_t kECut = 1.0e4; // Parameters entering the parametrized range for delta electrons //const float ra=5.37E-4, rb=0.9815, rc=3.123E-3; // Gas density -> To be made user adjustable ! //const float rho=0.004945 ; //[0.85*0.00549+0.15*0.00186 (Xe-CO2 85-15)] // Minimum energy for the step size adjustment const Float_t kEkinMinStep = 1.0e-5; // Plateau value of the energy-loss for electron in xenon // taken from: Allison + Comb, Ann. Rev. Nucl. Sci. (1980), 30, 253 //const Double_t kPlateau = 1.70; // the averaged value (26/3/99) const Float_t kPlateau = 1.55; const Float_t kPrim = 48.0; // dN1/dx|min for the gas mixture (90% Xe + 10% CO2) // First ionization potential (eV) for the gas mixture (90% Xe + 10% CO2) const Float_t kPoti = 12.1; const Int_t kPdgElectron = 11; // PDG code electron // Set the maximum step size to a very large number for all // neutral particles and those outside the driftvolume gMC->SetMaxStep(kBig); // Use only charged tracks if (( gMC->TrackCharge() ) && (!gMC->IsTrackStop() ) && (!gMC->IsTrackDisappeared())) { // Inside a sensitive volume? drRegion = kFALSE; amRegion = kFALSE; cIdCurrent = gMC->CurrentVolName(); if (cIdSensDr == cIdCurrent[1]) { drRegion = kTRUE; } if (cIdSensAm == cIdCurrent[1]) { amRegion = kTRUE; } if (drRegion || amRegion) { // The hit coordinates and charge gMC->TrackPosition(pos); hits[0] = pos[0]; hits[1] = pos[1]; hits[2] = pos[2]; // The sector number (0 - 17) // The numbering goes clockwise and starts at y = 0 Float_t phi = kRaddeg*TMath::ATan2(pos[0],pos[1]); if (phi < 90.) phi = phi + 270.; else phi = phi - 90.; sec = ((Int_t) (phi / 20)); // The plane and chamber number cIdChamber[0] = cIdCurrent[2]; cIdChamber[1] = cIdCurrent[3]; Int_t idChamber = (atoi(cIdChamber) % kNdetsec); cha = kNcham - ((Int_t) idChamber / kNplan) - 1; pla = ((Int_t) idChamber % kNplan); // Check on selected volumes Int_t addthishit = 1; if (fSensSelect) { if ((fSensPlane >= 0) && (pla != fSensPlane )) addthishit = 0; if ((fSensChamber >= 0) && (cha != fSensChamber)) addthishit = 0; if (fSensSector >= 0) { Int_t sens1 = fSensSector; Int_t sens2 = fSensSector + fSensSectorRange; sens2 -= ((Int_t) (sens2 / AliTRDgeometry::Nsect())) * AliTRDgeometry::Nsect(); if (sens1 < sens2) { if ((sec < sens1) || (sec >= sens2)) addthishit = 0; } else { if ((sec < sens1) && (sec >= sens2)) addthishit = 0; } } } // Add this hit if (addthishit) { // The detector number det = fGeometry->GetDetector(pla,cha,sec); // Special hits only in the drift region if (drRegion) { // Create a track reference at the entrance and // exit of each chamber that contain the // momentum components of the particle if (gMC->IsTrackEntering() || gMC->IsTrackExiting()) { gMC->TrackMomentum(mom); AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber()); } // Create the hits from TR photons if (fTR) CreateTRhit(det); } // Calculate the energy of the delta-electrons eDelta = TMath::Exp(fDeltaE->GetRandom()) - kPoti; eDelta = TMath::Max(eDelta,0.0); // Generate the electron cluster size if(eDelta==0.) qTot=0; else qTot = ((Int_t) (eDelta / kWion) + 1); // Create a new dEdx hit if (drRegion) { AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber() ,det,hits,qTot, kTRUE); } else { AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber() ,det,hits,qTot,kFALSE); } // Calculate the maximum step size for the next tracking step // Produce only one hit if Ekin is below cutoff aMass = gMC->TrackMass(); if ((gMC->Etot() - aMass) > kEkinMinStep) { // The energy loss according to Bethe Bloch iPdg = TMath::Abs(gMC->TrackPid()); if ( (iPdg != kPdgElectron) || ((iPdg == kPdgElectron) && (pTot < kPTotMaxEl))) { gMC->TrackMomentum(mom); pTot = mom.Rho(); betaGamma = pTot / aMass; pp = kPrim * BetheBloch(betaGamma); // Take charge > 1 into account charge = gMC->TrackCharge(); if (TMath::Abs(charge) > 1) pp = pp * charge*charge; } else { // Electrons above 20 Mev/c are at the plateau pp = kPrim * kPlateau; } if (pp > 0) { do gMC->GetRandom()->RndmArray(1, random); while ((random[0] == 1.) || (random[0] == 0.)); stepSize = - TMath::Log(random[0]) / pp; gMC->SetMaxStep(stepSize); } } } } } } //_____________________________________________________________________________ void AliTRDv1::StepManagerFixedStep() { // // Slow simulator. Every charged track produces electron cluster as hits // along its path across the drift volume. The step size is fixed in // this version of the step manager. // Int_t pla = 0; Int_t cha = 0; Int_t sec = 0; Int_t det = 0; Int_t qTot; Float_t hits[3]; Double_t eDep; Bool_t drRegion = kFALSE; Bool_t amRegion = kFALSE; TString cIdCurrent; TString cIdSensDr = "J"; TString cIdSensAm = "K"; Char_t cIdChamber[3]; cIdChamber[2] = 0; TLorentzVector pos, mom; const Int_t kNplan = AliTRDgeometry::Nplan(); const Int_t kNcham = AliTRDgeometry::Ncham(); const Int_t kNdetsec = kNplan * kNcham; const Double_t kBig = 1.0E+12; const Float_t kWion = 23.53; // Ionization energy const Float_t kEkinMinStep = 1.0e-5; // Minimum energy for the step size adjustment // Set the maximum step size to a very large number for all // neutral particles and those outside the driftvolume gMC->SetMaxStep(kBig); // If not charged track or already stopped or disappeared, just return. if ((!gMC->TrackCharge()) || gMC->IsTrackStop() || gMC->IsTrackDisappeared()) return; // Inside a sensitive volume? cIdCurrent = gMC->CurrentVolName(); if (cIdSensDr == cIdCurrent[1]) drRegion = kTRUE; if (cIdSensAm == cIdCurrent[1]) amRegion = kTRUE; if ((!drRegion) && (!amRegion)) return; // The hit coordinates and charge gMC->TrackPosition(pos); hits[0] = pos[0]; hits[1] = pos[1]; hits[2] = pos[2]; // The sector number (0 - 17) // The numbering goes clockwise and starts at y = 0 Float_t phi = kRaddeg*TMath::ATan2(pos[0],pos[1]); if (phi < 90.) phi += 270.; else phi -= 90.; sec = ((Int_t) (phi / 20.)); // The plane and chamber number cIdChamber[0] = cIdCurrent[2]; cIdChamber[1] = cIdCurrent[3]; Int_t idChamber = (atoi(cIdChamber) % kNdetsec); cha = kNcham - ((Int_t) idChamber / kNplan) - 1; pla = ((Int_t) idChamber % kNplan); // Check on selected volumes Int_t addthishit = 1; if(fSensSelect) { if ((fSensPlane >= 0) && (pla != fSensPlane )) addthishit = 0; if ((fSensChamber >= 0) && (cha != fSensChamber)) addthishit = 0; if (fSensSector >= 0) { Int_t sens1 = fSensSector; Int_t sens2 = fSensSector + fSensSectorRange; sens2 -= ((Int_t) (sens2 / AliTRDgeometry::Nsect())) * AliTRDgeometry::Nsect(); if (sens1 < sens2) { if ((sec < sens1) || (sec >= sens2)) addthishit = 0; } else { if ((sec < sens1) && (sec >= sens2)) addthishit = 0; } } } if (!addthishit) return; det = fGeometry->GetDetector(pla,cha,sec); // The detector number Int_t trkStat = 0; // 0: InFlight 1:Entering 2:Exiting // Special hits only in the drift region if (drRegion) { // Create a track reference at the entrance and exit of each // chamber that contain the momentum components of the particle if (gMC->IsTrackEntering()) { gMC->TrackMomentum(mom); AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber()); trkStat = 1; } if (gMC->IsTrackExiting()) { gMC->TrackMomentum(mom); AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber()); trkStat = 2; } // Create the hits from TR photons if (fTR) CreateTRhit(det); } // Calculate the charge according to GEANT Edep // Create a new dEdx hit eDep = TMath::Max(gMC->Edep(),0.0) * 1.0e+09; qTot = (Int_t) (eDep / kWion); AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber() ,det,hits,qTot,drRegion); // Set Maximum Step Size // Produce only one hit if Ekin is below cutoff if ((gMC->Etot() - gMC->TrackMass()) < kEkinMinStep) return; gMC->SetMaxStep(fStepSize); } //_____________________________________________________________________________ Double_t AliTRDv1::BetheBloch(Double_t bg) { // // Parametrization of the Bethe-Bloch-curve // The parametrization is the same as for the TPC and is taken from Lehrhaus. // // This parameters have been adjusted to averaged values from GEANT const Double_t kP1 = 7.17960e-02; const Double_t kP2 = 8.54196; const Double_t kP3 = 1.38065e-06; const Double_t kP4 = 5.30972; const Double_t kP5 = 2.83798; // This parameters have been adjusted to Xe-data found in: // Allison & Cobb, Ann. Rev. Nucl. Sci. (1980), 30, 253 //const Double_t kP1 = 0.76176E-1; //const Double_t kP2 = 10.632; //const Double_t kP3 = 3.17983E-6; //const Double_t kP4 = 1.8631; //const Double_t kP5 = 1.9479; // Lower cutoff of the Bethe-Bloch-curve to limit step sizes const Double_t kBgMin = 0.8; const Double_t kBBMax = 6.83298; //const Double_t kBgMin = 0.6; //const Double_t kBBMax = 17.2809; //const Double_t kBgMin = 0.4; //const Double_t kBBMax = 82.0; if (bg > kBgMin) { Double_t yy = bg / TMath::Sqrt(1. + bg*bg); Double_t aa = TMath::Power(yy,kP4); Double_t bb = TMath::Power((1./bg),kP5); bb = TMath::Log(kP3 + bb); return ((kP2 - aa - bb)*kP1 / aa); } else { return kBBMax; } } //_____________________________________________________________________________ Double_t AliTRDv1::BetheBlochGeant(Double_t bg) { // // Return dN/dx (number of primary collisions per centimeter) // for given beta*gamma factor. // // Implemented by K.Oyama according to GEANT 3 parametrization shown in // A.Andronic's webpage: http://www-alice.gsi.de/trd/papers/dedx/dedx.html // This must be used as a set with IntSpecGeant. // Double_t arr_g[20] = { 1.100000, 1.200000, 1.300000, 1.500000, 1.800000, 2.000000, 2.500000, 3.000000, 4.000000, 7.000000, 10.000000, 20.000000, 40.000000, 70.000000, 100.000000, 300.000000, 600.000000, 1000.000000, 3000.000000, 10000.000000 }; Double_t arr_nc[20] = { 75.009056, 45.508083, 35.299252, 27.116327, 22.734999, 21.411915, 19.934095, 19.449375, 19.344431, 20.185553, 21.027925, 22.912676, 24.933352, 26.504053, 27.387468, 29.566597, 30.353779, 30.787134, 31.129285, 31.157350 }; // betagamma to gamma Double_t g = TMath::Sqrt( 1. + bg*bg ); // Find the index just before the point we need. int i; for( i = 0 ; i < 18 ; i++ ) if( arr_g[i] < g && arr_g[i+1] > g ) break; // Simple interpolation. Double_t pp = ((arr_nc[i+1] - arr_nc[i]) / (arr_g[i+1]-arr_g[i])) * (g-arr_g[i]) + arr_nc[i]; return pp; //arr_nc[8]; } //_____________________________________________________________________________ void AliTRDv1::Stepping() { // Stepping info // --- cout << "X(cm) " << "Y(cm) " << "Z(cm) " << "KinE(MeV) " << "dE(MeV) " << "Step(cm) " << "TrackL(cm) " << "Volume " << "Process " << endl; // Position // Double_t x, y, z; gMC->TrackPosition(x, y, z); cout << setw(8) << setprecision(3) << x << " " << setw(8) << setprecision(3) << y << " " << setw(8) << setprecision(3) << z << " "; // Kinetic energy // Double_t px, py, pz, etot; gMC->TrackMomentum(px, py, pz, etot); Double_t ekin = etot - gMC->TrackMass(); cout << setw(9) << setprecision(4) << ekin*1e03 << " "; // Energy deposit // cout << setw(9) << setprecision(4) << gMC->Edep()*1e03 << " "; // Step length // cout << setw(8) << setprecision(3) << gMC->TrackStep() << " "; // Track length // cout << setw(8) << setprecision(3) << gMC->TrackLength() << " "; // Volume // if (gMC->CurrentVolName() != 0) cout << setw(4) << gMC->CurrentVolName() << " "; else cout << setw(4) << "None" << " "; // Process // TArrayI processes; Int_t nofProcesses = gMC->StepProcesses(processes); for(int ip=0;ip 0); pos2--; if (pos2 > kNv) pos2 = kNv - 1; pos1 = pos2 - 1; // Differentiate between the sampling points dnde = (vye[pos1] - vye[pos2]) / (vxe[pos2] - vxe[pos1]); return dnde; } //_____________________________________________________________________________ Double_t IntSpecGeant(Double_t *x, Double_t *) { // // Integrated spectrum from Geant3 // const Int_t npts = 83; Double_t arre[npts] = { 2.421257, 2.483278, 2.534301, 2.592230, 2.672067, 2.813299, 3.015059, 3.216819, 3.418579, 3.620338, 3.868209, 3.920198, 3.978284, 4.063923, 4.186264, 4.308605, 4.430946, 4.553288, 4.724261, 4.837736, 4.999842, 5.161949, 5.324056, 5.486163, 5.679688, 5.752998, 5.857728, 5.962457, 6.067185, 6.171914, 6.315653, 6.393674, 6.471694, 6.539689, 6.597658, 6.655627, 6.710957, 6.763648, 6.816338, 6.876198, 6.943227, 7.010257, 7.106285, 7.252151, 7.460531, 7.668911, 7.877290, 8.085670, 8.302979, 8.353585, 8.413120, 8.483500, 8.541030, 8.592857, 8.668865, 8.820485, 9.037086, 9.253686, 9.470286, 9.686887, 9.930838, 9.994655, 10.085822, 10.176990, 10.268158, 10.359325, 10.503614, 10.627565, 10.804637, 10.981709, 11.158781, 11.335854, 11.593397, 11.781165, 12.049404, 12.317644, 12.585884, 12.854123, 14.278421, 16.975889, 20.829416, 24.682943, 28.536469 }; /* Double_t arrdndx[npts] = { 19.344431, 18.664679, 18.136106, 17.567745, 16.836426, 15.677382, 14.281277, 13.140237, 12.207677, 11.445510, 10.697049, 10.562296, 10.414673, 10.182341, 9.775256, 9.172330, 8.240271, 6.898587, 4.808303, 3.889751, 3.345288, 3.093431, 2.897347, 2.692470, 2.436222, 2.340029, 2.208579, 2.086489, 1.975535, 1.876519, 1.759626, 1.705024, 1.656374, 1.502638, 1.330566, 1.200697, 1.101168, 1.019323, 0.943867, 0.851951, 0.755229, 0.671576, 0.570675, 0.449672, 0.326722, 0.244225, 0.188225, 0.149608, 0.121529, 0.116289, 0.110636, 0.103490, 0.096147, 0.089191, 0.079780, 0.063927, 0.047642, 0.036341, 0.028250, 0.022285, 0.017291, 0.016211, 0.014802, 0.013533, 0.012388, 0.011352, 0.009803, 0.008537, 0.007039, 0.005829, 0.004843, 0.004034, 0.003101, 0.002564, 0.001956, 0.001494, 0.001142, 0.000873, 0.000210, 0.000014, 0.000000, 0.000000, 0.000000 }; */ // Differentiate // dnde = (arrdndx[i-1] - arrdndx[i]) / (arre[i] - arre[i-1]); Double_t arrdnde[npts] = { 10.960000, 10.960000, 10.359500, 9.811340, 9.1601500, 8.206670, 6.919630, 5.655430, 4.6221300, 3.777610, 3.019560, 2.591950, 2.5414600, 2.712920, 3.327460, 4.928240, 7.6185300, 10.966700, 12.225800, 8.094750, 3.3586900, 1.553650, 1.209600, 1.263840, 1.3241100, 1.312140, 1.255130, 1.165770, 1.0594500, 0.945450, 0.813231, 0.699837, 0.6235580, 2.260990, 2.968350, 2.240320, 1.7988300, 1.553300, 1.432070, 1.535520, 1.4429900, 1.247990, 1.050750, 0.829549, 0.5900280, 0.395897, 0.268741, 0.185320, 0.1292120, 0.103545, 0.0949525, 0.101535, 0.1276380, 0.134216, 0.123816, 0.104557, 0.0751843, 0.0521745, 0.0373546, 0.0275391, 0.0204713, 0.0169234, 0.0154552, 0.0139194, 0.0125592, 0.0113638, 0.0107354, 0.0102137, 0.00845984, 0.00683338, 0.00556836, 0.00456874, 0.0036227, 0.00285991, 0.00226664, 0.00172234, 0.00131226, 0.00100284, 0.000465492, 7.26607e-05, 3.63304e-06, 0.0000000, 0.0000000 }; Int_t i; Double_t energy = x[0]; for( i = 0 ; i < npts ; i++ ) if( energy < arre[i] ) break; if( i == 0 ) AliErrorGeneral("AliTRDv1","Given energy value is too small or zero"); return arrdnde[i]; }