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 ////////////////////////////////////////////////////////////////////////////
20 // Transition Radiation Detector version 1 -- slow simulator //
22 ////////////////////////////////////////////////////////////////////////////
27 #include <TLorentzVector.h>
31 #include <TVirtualMC.h>
32 #include <TGeoManager.h>
39 #include "AliTRDgeometry.h"
40 #include "AliTRDhit.h"
41 #include "AliTRDsim.h"
46 //_____________________________________________________________________________
51 ,fTypeOfStepManager(0)
59 // Default constructor
64 //_____________________________________________________________________________
65 AliTRDv1::AliTRDv1(const char *name, const char *title)
69 ,fTypeOfStepManager(2)
77 // Standard constructor for Transition Radiation Detector version 1
80 SetBufferSize(128000);
84 //_____________________________________________________________________________
88 // AliTRDv1 destructor
108 //_____________________________________________________________________________
109 void AliTRDv1::AddAlignableVolumes() const
112 // Create entries for alignable volumes associating the symbolic volume
113 // name with the corresponding volume path. Needs to be syncronized with
114 // eventual changes in the geometry.
120 TString vpStr = "ALIC_1/B077_1/BSEGMO";
121 TString vpApp1 = "_1/BTRD";
122 TString vpApp2 = "_1";
123 TString vpApp3 = "/UTR1_1/UTS1_1/UTI1_1/UT";
125 TString snStr = "TRD/sm";
126 TString snApp1 = "/st";
127 TString snApp2 = "/pl";
131 // The symbolic names are: TRD/sm00
135 for (Int_t isect = 0; isect < AliTRDgeometry::Nsect(); isect++) {
144 symName += Form("%02d",isect);
146 gGeoManager->SetAlignableEntry(symName.Data(),volPath.Data());
151 // The readout chambers
152 // The symbolic names are: TRD/sm00/st0/pl0
156 for (Int_t isect = 0; isect < AliTRDgeometry::Nsect(); isect++) {
157 for (Int_t icham = 0; icham < AliTRDgeometry::Ncham(); icham++) {
158 for (Int_t iplan = 0; iplan < AliTRDgeometry::Nplan(); iplan++) {
160 Int_t idet = AliTRDgeometry::GetDetectorSec(iplan,icham);
168 volPath += Form("%02d",idet);
172 symName += Form("%02d",isect);
178 gGeoManager->SetAlignableEntry(symName.Data(),volPath.Data());
186 //_____________________________________________________________________________
187 void AliTRDv1::CreateGeometry()
190 // Create the GEANT geometry for the Transition Radiation Detector - Version 1
191 // This version covers the full azimuth.
194 // Check that FRAME is there otherwise we have no place where to put the TRD
195 AliModule* frame = gAlice->GetModule("FRAME");
197 AliError("TRD needs FRAME to be present\n");
201 // Define the chambers
202 AliTRD::CreateGeometry();
206 //_____________________________________________________________________________
207 void AliTRDv1::CreateMaterials()
210 // Create materials for the Transition Radiation Detector version 1
213 AliTRD::CreateMaterials();
217 //_____________________________________________________________________________
218 void AliTRDv1::CreateTRhit(Int_t det)
221 // Creates an electron cluster from a TR photon.
222 // The photon is assumed to be created a the end of the radiator. The
223 // distance after which it deposits its energy takes into account the
224 // absorbtion of the entrance window and of the gas mixture in drift
229 const Float_t kWion = 23.53;
231 // Maximum number of TR photons per track
232 const Int_t kNTR = 50;
241 gMC->TrackMomentum(mom);
242 Float_t pTot = mom.Rho();
243 fTR->CreatePhotons(11,pTot,nTR,eTR);
245 AliFatal(Form("Boundary error: nTR = %d, kNTR = %d",nTR,kNTR));
248 // Loop through the TR photons
249 for (Int_t iTR = 0; iTR < nTR; iTR++) {
251 Float_t energyMeV = eTR[iTR] * 0.001;
252 Float_t energyeV = eTR[iTR] * 1000.0;
253 Float_t absLength = 0.0;
256 // Take the absorbtion in the entrance window into account
257 Double_t muMy = fTR->GetMuMy(energyMeV);
258 sigma = muMy * fFoilDensity;
260 absLength = gRandom->Exp(1.0/sigma);
261 if (absLength < AliTRDgeometry::MyThick()) {
269 // The absorbtion cross sections in the drift gas
270 // Gas-mixture (Xe/CO2)
271 Double_t muXe = fTR->GetMuXe(energyMeV);
272 Double_t muCO = fTR->GetMuCO(energyMeV);
273 sigma = (0.85 * muXe + 0.15 * muCO) * fGasDensity * fTR->GetTemp();
275 // The distance after which the energy of the TR photon
278 absLength = gRandom->Exp(1.0/sigma);
279 if (absLength > (AliTRDgeometry::DrThick()
280 + AliTRDgeometry::AmThick())) {
288 // The position of the absorbtion
290 gMC->TrackPosition(pos);
291 posHit[0] = pos[0] + mom[0] / pTot * absLength;
292 posHit[1] = pos[1] + mom[1] / pTot * absLength;
293 posHit[2] = pos[2] + mom[2] / pTot * absLength;
296 Int_t q = ((Int_t) (energyeV / kWion));
298 // Add the hit to the array. TR photon hits are marked
299 // by negative charge
300 AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber()
304 ,gMC->TrackTime()*1.0e06
311 //_____________________________________________________________________________
312 void AliTRDv1::Init()
315 // Initialise Transition Radiation Detector after geometry has been built.
320 AliDebug(1,"Slow simulator\n");
322 // Switch on TR simulation as default
324 AliInfo("TR simulation off");
327 fTR = new AliTRDsim();
330 // First ionization potential (eV) for the gas mixture (90% Xe + 10% CO2)
331 const Float_t kPoti = 12.1;
332 // Maximum energy (50 keV);
333 const Float_t kEend = 50000.0;
334 // Ermilova distribution for the delta-ray spectrum
335 Float_t poti = TMath::Log(kPoti);
336 Float_t eEnd = TMath::Log(kEend);
338 // Ermilova distribution for the delta-ray spectrum
339 fDeltaE = new TF1("deltae" ,Ermilova ,poti,eEnd,0);
341 // Geant3 distribution for the delta-ray spectrum
342 fDeltaG = new TF1("deltag",IntSpecGeant,2.421257,28.536469,0);
344 AliDebug(1,"+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++");
348 //_____________________________________________________________________________
349 void AliTRDv1::StepManager()
352 // Slow simulator. Every charged track produces electron cluster as hits
353 // along its path across the drift volume.
356 switch (fTypeOfStepManager) {
358 StepManagerErmilova();
364 StepManagerFixedStep();
367 AliWarning("Not a valid Step Manager.");
372 //_____________________________________________________________________________
373 void AliTRDv1::SelectStepManager(Int_t t)
376 // Selects a step manager type:
379 // 2 - Fixed step size
382 fTypeOfStepManager = t;
383 AliInfo(Form("Step Manager type %d was selected",fTypeOfStepManager));
387 //_____________________________________________________________________________
388 void AliTRDv1::StepManagerGeant()
391 // Slow simulator. Every charged track produces electron cluster as hits
392 // along its path across the drift volume. The step size is set acording
393 // to Bethe-Bloch. The energy distribution of the delta electrons follows
394 // a spectrum taken from Geant3.
396 // Version by A. Bercuci
414 Double_t stepSize = 0;
416 Bool_t drRegion = kFALSE;
417 Bool_t amRegion = kFALSE;
424 TString cIdSensDr = "J";
425 TString cIdSensAm = "K";
426 Char_t cIdChamber[3];
434 const Int_t kNplan = AliTRDgeometry::Nplan();
435 const Int_t kNcham = AliTRDgeometry::Ncham();
436 const Int_t kNdetsec = kNplan * kNcham;
438 const Double_t kBig = 1.0e+12; // Infinitely big
439 const Float_t kWion = 23.53; // Ionization energy
440 const Float_t kPTotMaxEl = 0.002; // Maximum momentum for e+ e- g
442 // Minimum energy for the step size adjustment
443 const Float_t kEkinMinStep = 1.0e-5;
444 // energy threshold for production of delta electrons
445 const Float_t kECut = 1.0e4;
446 // Parameters entering the parametrized range for delta electrons
447 const Float_t kRa = 5.37e-4;
448 const Float_t kRb = 0.9815;
449 const Float_t kRc = 3.123e-3;
450 // Gas density -> To be made user adjustable !
451 // [0.85*0.00549+0.15*0.00186 (Xe-CO2 85-15)]
452 const Float_t kRho = 0.004945 ;
454 // Plateau value of the energy-loss for electron in xenon
455 // The averaged value (26/3/99)
456 const Float_t kPlateau = 1.55;
457 // dN1/dx|min for the gas mixture (90% Xe + 10% CO2)
458 const Float_t kPrim = 19.34;
459 // First ionization potential (eV) for the gas mixture (90% Xe + 10% CO2)
460 const Float_t kPoti = 12.1;
462 const Int_t kPdgElectron = 11;
464 // Set the maximum step size to a very large number for all
465 // neutral particles and those outside the driftvolume
466 gMC->SetMaxStep(kBig);
468 // Use only charged tracks
469 if (( gMC->TrackCharge() ) &&
470 (!gMC->IsTrackDisappeared())) {
472 // Inside a sensitive volume?
475 cIdCurrent = gMC->CurrentVolName();
476 if (cIdSensDr == cIdCurrent[1]) {
479 if (cIdSensAm == cIdCurrent[1]) {
482 if (drRegion || amRegion) {
484 // The hit coordinates and charge
485 gMC->TrackPosition(pos);
490 // The sector number (0 - 17), according to standard coordinate system
491 cIdPath = gGeoManager->GetPath();
492 cIdSector[0] = cIdPath[21];
493 cIdSector[1] = cIdPath[22];
494 sec = atoi(cIdSector);
496 // The plane and chamber number
497 cIdChamber[0] = cIdCurrent[2];
498 cIdChamber[1] = cIdCurrent[3];
499 Int_t idChamber = (atoi(cIdChamber) % kNdetsec);
500 cha = ((Int_t) idChamber / kNplan);
501 pla = ((Int_t) idChamber % kNplan);
503 // The detector number
504 det = fGeometry->GetDetector(pla,cha,sec);
506 // Special hits only in the drift region
508 (gMC->IsTrackEntering())) {
510 // Create a track reference at the entrance of each
511 // chamber that contains the momentum components of the particle
512 gMC->TrackMomentum(mom);
513 AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber());
515 // Create the hits from TR photons if electron/positron is
516 // entering the drift volume
518 (TMath::Abs(gMC->TrackPid()) == kPdgElectron)) {
523 else if ((amRegion) &&
524 (gMC->IsTrackExiting())) {
526 // Create a track reference at the exit of each
527 // chamber that contains the momentum components of the particle
528 gMC->TrackMomentum(mom);
529 AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber());
533 // Calculate the energy of the delta-electrons
534 // modified by Alex Bercuci (A.Bercuci@gsi.de) on 26.01.06
535 // take into account correlation with the underlying GEANT tracking
537 // http://www-linux.gsi.de/~abercuci/Contributions/TRD/index.html
539 // determine the most significant process (last on the processes list)
540 // which caused this hit
541 gMC->StepProcesses(processes);
542 Int_t nofprocesses = processes.GetSize();
548 pid = processes[nofprocesses-1];
551 // Generate Edep according to GEANT parametrisation
552 eDelta = TMath::Exp(fDeltaG->GetRandom()) - kPoti;
553 eDelta = TMath::Max(eDelta,0.0);
554 Float_t prRange = 0.0;
555 Float_t range = gMC->TrackLength() - fTrackLength0;
556 // merge GEANT tracker information with locally cooked one
557 if (gAlice->GetMCApp()->GetCurrentTrackNumber() == fPrimaryTrackPid) {
559 if (eDelta >= kECut) {
560 prRange = kRa * eDelta * 0.001
561 * (1.0 - kRb / (1.0 + kRc * eDelta * 0.001)) / kRho;
562 if (prRange >= (3.7 - range)) {
568 if (eDelta < kECut) {
572 prRange = kRa * eDelta * 0.001
573 * (1.0 - kRb / (1.0 + kRc * eDelta * 0.001)) / kRho;
574 if (prRange >= ((AliTRDgeometry::DrThick()
575 + AliTRDgeometry::AmThick()) - range)) {
591 // Generate the electron cluster size
594 qTot = ((Int_t) (eDelta / kWion) + 1);
596 // Create a new dEdx hit
597 AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber()
601 ,gMC->TrackTime()*1.0e06
606 // Calculate the maximum step size for the next tracking step
607 // Produce only one hit if Ekin is below cutoff
608 aMass = gMC->TrackMass();
609 if ((gMC->Etot() - aMass) > kEkinMinStep) {
611 // The energy loss according to Bethe Bloch
612 iPdg = TMath::Abs(gMC->TrackPid());
613 if ((iPdg != kPdgElectron) ||
614 ((iPdg == kPdgElectron) &&
615 (pTot < kPTotMaxEl))) {
616 gMC->TrackMomentum(mom);
618 betaGamma = pTot / aMass;
619 pp = BetheBlochGeant(betaGamma);
620 // Take charge > 1 into account
621 charge = gMC->TrackCharge();
622 if (TMath::Abs(charge) > 1) {
623 pp = pp * charge*charge;
627 // Electrons above 20 Mev/c are at the plateau
628 pp = kPrim * kPlateau;
633 nsteps = gRandom->Poisson(pp);
635 stepSize = 1.0 / nsteps;
636 gMC->SetMaxStep(stepSize);
646 //_____________________________________________________________________________
647 void AliTRDv1::StepManagerErmilova()
650 // Slow simulator. Every charged track produces electron cluster as hits
651 // along its path across the drift volume. The step size is set acording
652 // to Bethe-Bloch. The energy distribution of the delta electrons follows
653 // a spectrum taken from Ermilova et al.
674 Bool_t drRegion = kFALSE;
675 Bool_t amRegion = kFALSE;
682 TString cIdSensDr = "J";
683 TString cIdSensAm = "K";
684 Char_t cIdChamber[3];
690 const Int_t kNplan = AliTRDgeometry::Nplan();
691 const Int_t kNcham = AliTRDgeometry::Ncham();
692 const Int_t kNdetsec = kNplan * kNcham;
694 const Double_t kBig = 1.0e+12; // Infinitely big
695 const Float_t kWion = 23.53; // Ionization energy
696 const Float_t kPTotMaxEl = 0.002; // Maximum momentum for e+ e- g
698 // Minimum energy for the step size adjustment
699 const Float_t kEkinMinStep = 1.0e-5;
701 // Plateau value of the energy-loss for electron in xenon
702 // The averaged value (26/3/99)
703 const Float_t kPlateau = 1.55;
704 // dN1/dx|min for the gas mixture (90% Xe + 10% CO2)
705 const Float_t kPrim = 48.0;
706 // First ionization potential (eV) for the gas mixture (90% Xe + 10% CO2)
707 const Float_t kPoti = 12.1;
709 const Int_t kPdgElectron = 11;
711 // Set the maximum step size to a very large number for all
712 // neutral particles and those outside the driftvolume
713 gMC->SetMaxStep(kBig);
715 // Use only charged tracks
716 if (( gMC->TrackCharge() ) &&
717 (!gMC->IsTrackDisappeared())) {
719 // Inside a sensitive volume?
722 cIdCurrent = gMC->CurrentVolName();
723 if (cIdSensDr == cIdCurrent[1]) {
726 if (cIdSensAm == cIdCurrent[1]) {
729 if (drRegion || amRegion) {
731 // The hit coordinates and charge
732 gMC->TrackPosition(pos);
737 // The sector number (0 - 17), according to standard coordinate system
738 cIdPath = gGeoManager->GetPath();
739 cIdSector[0] = cIdPath[21];
740 cIdSector[1] = cIdPath[22];
741 sec = atoi(cIdSector);
743 // The plane and chamber number
744 cIdChamber[0] = cIdCurrent[2];
745 cIdChamber[1] = cIdCurrent[3];
746 Int_t idChamber = (atoi(cIdChamber) % kNdetsec);
747 cha = ((Int_t) idChamber / kNplan);
748 pla = ((Int_t) idChamber % kNplan);
750 // The detector number
751 det = fGeometry->GetDetector(pla,cha,sec);
753 // Special hits only in the drift region
755 (gMC->IsTrackEntering())) {
757 // Create a track reference at the entrance of each
758 // chamber that contains the momentum components of the particle
759 gMC->TrackMomentum(mom);
760 AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber());
762 // Create the hits from TR photons if electron/positron is
763 // entering the drift volume
765 (TMath::Abs(gMC->TrackPid()) == kPdgElectron)) {
770 else if ((amRegion) &&
771 (gMC->IsTrackExiting())) {
773 // Create a track reference at the exit of each
774 // chamber that contains the momentum components of the particle
775 gMC->TrackMomentum(mom);
776 AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber());
780 // Calculate the energy of the delta-electrons
781 eDelta = TMath::Exp(fDeltaE->GetRandom()) - kPoti;
782 eDelta = TMath::Max(eDelta,0.0);
784 // Generate the electron cluster size
787 qTot = ((Int_t) (eDelta / kWion) + 1);
789 // Create a new dEdx hit
791 AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber()
795 ,gMC->TrackTime()*1.0e06
799 AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber()
803 ,gMC->TrackTime()*1.0e06
809 // Calculate the maximum step size for the next tracking step
810 // Produce only one hit if Ekin is below cutoff
811 aMass = gMC->TrackMass();
812 if ((gMC->Etot() - aMass) > kEkinMinStep) {
814 // The energy loss according to Bethe Bloch
815 iPdg = TMath::Abs(gMC->TrackPid());
816 if ((iPdg != kPdgElectron) ||
817 ((iPdg == kPdgElectron) &&
818 (pTot < kPTotMaxEl))) {
819 gMC->TrackMomentum(mom);
821 betaGamma = pTot / aMass;
822 pp = kPrim * BetheBloch(betaGamma);
823 // Take charge > 1 into account
824 charge = gMC->TrackCharge();
825 if (TMath::Abs(charge) > 1) {
826 pp = pp * charge*charge;
830 // Electrons above 20 Mev/c are at the plateau
831 pp = kPrim * kPlateau;
836 gMC->GetRandom()->RndmArray(1,random);
838 while ((random[0] == 1.0) ||
840 stepSize = - TMath::Log(random[0]) / pp;
841 gMC->SetMaxStep(stepSize);
852 //_____________________________________________________________________________
853 void AliTRDv1::StepManagerFixedStep()
856 // Slow simulator. Every charged track produces electron cluster as hits
857 // along its path across the drift volume. The step size is fixed in
858 // this version of the step manager.
862 const Int_t kPdgElectron = 11;
873 Bool_t drRegion = kFALSE;
874 Bool_t amRegion = kFALSE;
881 TString cIdSensDr = "J";
882 TString cIdSensAm = "K";
883 Char_t cIdChamber[3];
889 const Int_t kNplan = AliTRDgeometry::Nplan();
890 const Int_t kNcham = AliTRDgeometry::Ncham();
891 const Int_t kNdetsec = kNplan * kNcham;
893 const Double_t kBig = 1.0e+12;
895 const Float_t kWion = 23.53; // Ionization energy
896 const Float_t kEkinMinStep = 1.0e-5; // Minimum energy for the step size adjustment
898 // Set the maximum step size to a very large number for all
899 // neutral particles and those outside the driftvolume
900 gMC->SetMaxStep(kBig);
902 // If not charged track or already stopped or disappeared, just return.
903 if ((!gMC->TrackCharge()) ||
904 gMC->IsTrackDisappeared()) {
908 // Inside a sensitive volume?
909 cIdCurrent = gMC->CurrentVolName();
911 if (cIdSensDr == cIdCurrent[1]) {
914 if (cIdSensAm == cIdCurrent[1]) {
923 // The hit coordinates and charge
924 gMC->TrackPosition(pos);
929 // The sector number (0 - 17), according to standard coordinate system
930 cIdPath = gGeoManager->GetPath();
931 cIdSector[0] = cIdPath[21];
932 cIdSector[1] = cIdPath[22];
933 sec = atoi(cIdSector);
935 // The plane and chamber number
936 cIdChamber[0] = cIdCurrent[2];
937 cIdChamber[1] = cIdCurrent[3];
938 Int_t idChamber = (atoi(cIdChamber) % kNdetsec);
939 cha = ((Int_t) idChamber / kNplan);
940 pla = ((Int_t) idChamber % kNplan);
942 // The detector number
943 det = fGeometry->GetDetector(pla,cha,sec);
945 // 0: InFlight 1:Entering 2:Exiting
948 // Special hits only in the drift region
950 (gMC->IsTrackEntering())) {
952 // Create a track reference at the entrance of each
953 // chamber that contains the momentum components of the particle
954 gMC->TrackMomentum(mom);
955 AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber());
958 // Create the hits from TR photons if electron/positron is
959 // entering the drift volume
961 (TMath::Abs(gMC->TrackPid()) == kPdgElectron)) {
966 else if ((amRegion) &&
967 (gMC->IsTrackExiting())) {
969 // Create a track reference at the exit of each
970 // chamber that contains the momentum components of the particle
971 gMC->TrackMomentum(mom);
972 AddTrackReference(gAlice->GetMCApp()->GetCurrentTrackNumber());
977 // Calculate the charge according to GEANT Edep
978 // Create a new dEdx hit
979 eDep = TMath::Max(gMC->Edep(),0.0) * 1.0e+09;
980 qTot = (Int_t) (eDep / kWion);
983 AddHit(gAlice->GetMCApp()->GetCurrentTrackNumber()
987 ,gMC->TrackTime()*1.0e06
991 // Set Maximum Step Size
992 // Produce only one hit if Ekin is below cutoff
993 if ((gMC->Etot() - gMC->TrackMass()) < kEkinMinStep) {
996 gMC->SetMaxStep(fStepSize);
1000 //_____________________________________________________________________________
1001 Double_t AliTRDv1::BetheBloch(Double_t bg)
1004 // Parametrization of the Bethe-Bloch-curve
1005 // The parametrization is the same as for the TPC and is taken from Lehrhaus.
1008 // This parameters have been adjusted to averaged values from GEANT
1009 const Double_t kP1 = 7.17960e-02;
1010 const Double_t kP2 = 8.54196;
1011 const Double_t kP3 = 1.38065e-06;
1012 const Double_t kP4 = 5.30972;
1013 const Double_t kP5 = 2.83798;
1015 // Lower cutoff of the Bethe-Bloch-curve to limit step sizes
1016 const Double_t kBgMin = 0.8;
1017 const Double_t kBBMax = 6.83298;
1020 Double_t yy = bg / TMath::Sqrt(1.0 + bg*bg);
1021 Double_t aa = TMath::Power(yy,kP4);
1022 Double_t bb = TMath::Power((1.0/bg),kP5);
1023 bb = TMath::Log(kP3 + bb);
1024 return ((kP2 - aa - bb) * kP1 / aa);
1032 //_____________________________________________________________________________
1033 Double_t AliTRDv1::BetheBlochGeant(Double_t bg)
1036 // Return dN/dx (number of primary collisions per centimeter)
1037 // for given beta*gamma factor.
1039 // Implemented by K.Oyama according to GEANT 3 parametrization shown in
1040 // A.Andronic's webpage: http://www-alice.gsi.de/trd/papers/dedx/dedx.html
1041 // This must be used as a set with IntSpecGeant.
1046 Double_t arrG[20] = { 1.100000, 1.200000, 1.300000, 1.500000
1047 , 1.800000, 2.000000, 2.500000, 3.000000
1048 , 4.000000, 7.000000, 10.000000, 20.000000
1049 , 40.000000, 70.000000, 100.000000, 300.000000
1050 , 600.000000, 1000.000000, 3000.000000, 10000.000000 };
1052 Double_t arrNC[20] = { 75.009056, 45.508083, 35.299252, 27.116327
1053 , 22.734999, 21.411915, 19.934095, 19.449375
1054 , 19.344431, 20.185553, 21.027925, 22.912676
1055 , 24.933352, 26.504053, 27.387468, 29.566597
1056 , 30.353779, 30.787134, 31.129285, 31.157350 };
1058 // Betagamma to gamma
1059 Double_t g = TMath::Sqrt(1.0 + bg*bg);
1061 // Find the index just before the point we need.
1062 for (i = 0; i < 18; i++) {
1063 if ((arrG[i] < g) &&
1069 // Simple interpolation.
1070 Double_t pp = ((arrNC[i+1] - arrNC[i]) / (arrG[i+1] - arrG[i]))
1071 * (g - arrG[i]) + arrNC[i];
1077 //_____________________________________________________________________________
1078 Double_t Ermilova(Double_t *x, Double_t *)
1081 // Calculates the delta-ray energy distribution according to Ermilova.
1082 // Logarithmic scale !
1092 const Int_t kNv = 31;
1094 Float_t vxe[kNv] = { 2.3026, 2.9957, 3.4012, 3.6889, 3.9120
1095 , 4.0943, 4.2485, 4.3820, 4.4998, 4.6052
1096 , 4.7005, 5.0752, 5.2983, 5.7038, 5.9915
1097 , 6.2146, 6.5221, 6.9078, 7.3132, 7.6009
1098 , 8.0064, 8.5172, 8.6995, 8.9872, 9.2103
1099 , 9.4727, 9.9035, 10.3735, 10.5966, 10.8198
1102 Float_t vye[kNv] = { 80.0, 31.0, 23.3, 21.1, 21.0
1103 , 20.9, 20.8, 20.0, 16.0, 11.0
1104 , 8.0, 6.0, 5.2, 4.6, 4.0
1105 , 3.5, 3.0, 1.4, 0.67, 0.44
1106 , 0.3, 0.18, 0.12, 0.08, 0.056
1107 , 0.04, 0.023, 0.015, 0.011, 0.01
1112 // Find the position
1117 dpos = energy - vxe[pos2++];
1126 // Differentiate between the sampling points
1127 dnde = (vye[pos1] - vye[pos2]) / (vxe[pos2] - vxe[pos1]);
1133 //_____________________________________________________________________________
1134 Double_t IntSpecGeant(Double_t *x, Double_t *)
1137 // Integrated spectrum from Geant3
1140 const Int_t npts = 83;
1141 Double_t arre[npts] = { 2.421257, 2.483278, 2.534301, 2.592230
1142 , 2.672067, 2.813299, 3.015059, 3.216819
1143 , 3.418579, 3.620338, 3.868209, 3.920198
1144 , 3.978284, 4.063923, 4.186264, 4.308605
1145 , 4.430946, 4.553288, 4.724261, 4.837736
1146 , 4.999842, 5.161949, 5.324056, 5.486163
1147 , 5.679688, 5.752998, 5.857728, 5.962457
1148 , 6.067185, 6.171914, 6.315653, 6.393674
1149 , 6.471694, 6.539689, 6.597658, 6.655627
1150 , 6.710957, 6.763648, 6.816338, 6.876198
1151 , 6.943227, 7.010257, 7.106285, 7.252151
1152 , 7.460531, 7.668911, 7.877290, 8.085670
1153 , 8.302979, 8.353585, 8.413120, 8.483500
1154 , 8.541030, 8.592857, 8.668865, 8.820485
1155 , 9.037086, 9.253686, 9.470286, 9.686887
1156 , 9.930838, 9.994655, 10.085822, 10.176990
1157 , 10.268158, 10.359325, 10.503614, 10.627565
1158 , 10.804637, 10.981709, 11.158781, 11.335854
1159 , 11.593397, 11.781165, 12.049404, 12.317644
1160 , 12.585884, 12.854123, 14.278421, 16.975889
1161 , 20.829416, 24.682943, 28.536469 };
1163 Double_t arrdnde[npts] = { 10.960000, 10.960000, 10.359500, 9.811340
1164 , 9.1601500, 8.206670, 6.919630, 5.655430
1165 , 4.6221300, 3.777610, 3.019560, 2.591950
1166 , 2.5414600, 2.712920, 3.327460, 4.928240
1167 , 7.6185300, 10.966700, 12.225800, 8.094750
1168 , 3.3586900, 1.553650, 1.209600, 1.263840
1169 , 1.3241100, 1.312140, 1.255130, 1.165770
1170 , 1.0594500, 0.945450, 0.813231, 0.699837
1171 , 0.6235580, 2.260990, 2.968350, 2.240320
1172 , 1.7988300, 1.553300, 1.432070, 1.535520
1173 , 1.4429900, 1.247990, 1.050750, 0.829549
1174 , 0.5900280, 0.395897, 0.268741, 0.185320
1175 , 0.1292120, 0.103545, 0.0949525, 0.101535
1176 , 0.1276380, 0.134216, 0.123816, 0.104557
1177 , 0.0751843, 0.0521745, 0.0373546, 0.0275391
1178 , 0.0204713, 0.0169234, 0.0154552, 0.0139194
1179 , 0.0125592, 0.0113638, 0.0107354, 0.0102137
1180 , 0.00845984, 0.00683338, 0.00556836, 0.00456874
1181 , 0.0036227, 0.00285991, 0.00226664, 0.00172234
1182 , 0.00131226, 0.00100284, 0.000465492, 7.26607e-05
1183 , 3.63304e-06, 0.0000000, 0.0000000 };
1186 Double_t energy = x[0];
1188 for (i = 0; i < npts; i++) {
1189 if (energy < arre[i]) {
1195 AliErrorGeneral("AliTRDv1::IntSpecGeant","Given energy value is too small or zero");