| [807] | 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | // Rich advanced example for Geant4
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| 27 | // HpdSiEnergyLoss.cc for Rich of LHCb
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| 28 | // History:
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| 29 | // Created: Sajan Easo (Sajan.Easo@cern.ch)
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| 30 | // Revision: Patricia Mendez (Patricia.Mendez@cern.ch)
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| 31 | /////////////////////////////////////////////////////////////////////////////
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| 32 | #include "HpdSiEnergyLoss.hh"
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| 33 | #include "G4Material.hh"
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| 34 | #include "Randomize.hh"
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| 35 | #include "RichTbMaterialParameters.hh"
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| 36 | #include "RichTbAnalysisManager.hh"
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| 37 |
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| 38 | HpdSiEnergyLoss::HpdSiEnergyLoss(const G4String& materialName,
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| 39 | const G4String& processName)
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| 40 | : G4VEnergyLoss(processName),
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| 41 | MinKineticEnergy(1.*eV),MipEnergy(30000.0*eV),
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| 42 | finalRangeforStep(0.15*mm) {
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| 43 | ElossMaterialName= materialName;
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| 44 |
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| 45 | const G4MaterialTable* theMaterialTable = G4Material::GetMaterialTable();
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| 46 | G4int numberOfMat = G4Material::GetNumberOfMaterials();
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| 47 |
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| 48 | G4int iMat=0;
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| 49 | for(iMat=0;iMat<numberOfMat;iMat++) {
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| 50 | if ( materialName == (*theMaterialTable)[iMat]->GetName()){
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| 51 | fMatIndex=(*theMaterialTable)[iMat]->GetIndex();
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| 52 | break;
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| 53 | }
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| 54 |
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| 55 | }
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| 56 | if(iMat >= numberOfMat ) {
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| 57 | G4Exception("Invalid material Name in HpdSiEnergyLoss constructor" );
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| 58 | }
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| 59 | }
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| 60 |
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| 61 | HpdSiEnergyLoss::~HpdSiEnergyLoss() { }
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| 62 |
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| 63 | G4bool HpdSiEnergyLoss::IsApplicable(const G4ParticleDefinition&
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| 64 | aParticleType) {
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| 65 | return(aParticleType.GetPDGCharge()!= 0.);
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| 66 | }
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| 67 |
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| 68 | G4double HpdSiEnergyLoss::GetContinuousStepLimit(const G4Track& track,
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| 69 | G4double,
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| 70 | G4double,
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| 71 | G4double& ){
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| 72 |
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| 73 | G4double RangeForStep = finalRangeforStep;
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| 74 |
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| 75 | if( fMatIndex != G4int(track.GetMaterial() -> GetIndex()) ) {
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| 76 | RangeForStep = DBL_MAX;
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| 77 | }
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| 78 |
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| 79 | return RangeForStep;
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| 80 | }
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| 81 |
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| 82 | G4double HpdSiEnergyLoss::GetMeanFreePath(const G4Track&,
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| 83 | G4double,
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| 84 | G4ForceCondition* condition) {
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| 85 | // return infinity so that it does nothing.
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| 86 | *condition = NotForced;
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| 87 | return DBL_MAX;
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| 88 |
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| 89 | }
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| 90 |
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| 91 | G4VParticleChange* HpdSiEnergyLoss::PostStepDoIt(const G4Track& aTrack,
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| 92 | const G4Step& aStep) {
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| 93 | // Do nothing
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| 94 | aParticleChange.Initialize(aTrack) ;
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| 95 | return G4VContinuousDiscreteProcess::PostStepDoIt(aTrack,aStep);
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| 96 |
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| 97 | }
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| 98 |
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| 99 | G4VParticleChange* HpdSiEnergyLoss::AlongStepDoIt(const G4Track& aTrack,
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| 100 | const G4Step&) {
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| 101 |
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| 102 |
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| 103 | #ifdef G4ANALYSIS_USE
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| 104 | RichTbAnalysisManager * analysis = RichTbAnalysisManager::getInstance();
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| 105 | #endif
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| 106 |
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| 107 |
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| 108 | aParticleChange.Initialize(aTrack);
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| 109 | G4int aMaterialIndex = aTrack.GetMaterial()->GetIndex();
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| 110 | if(fMatIndex != aMaterialIndex ) {
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| 111 | return &aParticleChange;
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| 112 | }
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| 113 |
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| 114 | const G4DynamicParticle* aParticle = aTrack.GetDynamicParticle();
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| 115 | G4double aKinEnergyInit = aParticle->GetKineticEnergy();
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| 116 | G4double Eloss, aKinEnergyFinal;
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| 117 | if(aKinEnergyInit < MinKineticEnergy ) { Eloss=0.0 ; }
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| 118 | else if( aKinEnergyInit < MipEnergy ) {Eloss= aKinEnergyInit ;}
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| 119 | else { Eloss = MipEnergy; }
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| 120 |
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| 121 | aKinEnergyFinal=aKinEnergyInit-Eloss;
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| 122 |
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| 123 |
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| 124 | //In the G4example the backscattering is implemented in
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| 125 | //an adhoc manner as done below. It simply causes an
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| 126 | // efficiency loss.
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| 127 |
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| 128 | G4double bckratio;
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| 129 | if( SignalToNoiseInData > 0.0 ){
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| 130 | bckratio = NsigmaInPedCut/ SignalToNoiseInData ;
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| 131 |
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| 132 | }
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| 133 | G4double Effs = 1.0 - backscaprob * bckratio;
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| 134 | G4double Randbsk = G4UniformRand();
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| 135 | if(Randbsk <= Effs && Eloss > 0.0 ) {
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| 136 | aParticleChange.ProposeLocalEnergyDeposit(Eloss);
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| 137 |
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| 138 | #ifdef G4ANALYSIS_USE
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| 139 |
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| 140 | analysis->bumpNumHitInSi();
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| 141 |
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| 142 | #endif
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| 143 |
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| 144 | // G4StepPoint* pPreStepPoint = aStep.GetPreStepPoint();
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| 145 | // G4String tpreVol = pPreStepPoint -> GetPhysicalVolume()->GetName();
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| 146 | // G4int tpreVP = pPreStepPoint -> GetPhysicalVolume()->GetCopyNo();
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| 147 | }
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| 148 | if (aKinEnergyFinal <= MinKineticEnergy ) {
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| 149 | aParticleChange.ProposeTrackStatus(fStopAndKill);
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| 150 |
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| 151 | }else {
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| 152 | aParticleChange.ProposeEnergy(aKinEnergyFinal);
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| 153 |
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| 154 | }
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| 155 | return &aParticleChange;
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| 156 |
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| 157 | }
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| 158 |
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| 159 |
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| 160 |
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| 161 |
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| 162 |
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| 163 |
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| 164 |
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| 165 |
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