| 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 | // $Id: G4ContinuousGainOfEnergy.cc,v 1.4 2009/11/20 10:31:20 ldesorgh Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 28 | //
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| 29 | #include "G4ContinuousGainOfEnergy.hh"
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| 30 | #include "G4Step.hh"
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| 31 | #include "G4ParticleDefinition.hh"
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| 32 | #include "G4VEmModel.hh"
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| 33 | #include "G4VEmFluctuationModel.hh"
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| 34 | #include "G4VParticleChange.hh"
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| 35 | #include "G4UnitsTable.hh"
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| 36 | #include "G4AdjointCSManager.hh"
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| 37 | #include "G4LossTableManager.hh"
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| 38 |
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| 39 |
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| 40 | ///////////////////////////////////////////////////////
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| 41 | //
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| 42 | G4ContinuousGainOfEnergy::G4ContinuousGainOfEnergy(const G4String& name,
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| 43 | G4ProcessType type): G4VContinuousProcess(name, type)
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| 44 | {
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| 45 |
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| 46 |
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| 47 | linLossLimit=0.05;
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| 48 | lossFluctuationArePossible =true;
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| 49 | lossFluctuationFlag=true;
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| 50 | is_integral = false;
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| 51 |
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| 52 | //Will be properly set in SetDirectParticle()
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| 53 | IsIon=false;
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| 54 | massRatio =1.;
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| 55 | chargeSqRatio=1.;
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| 56 | preStepChargeSqRatio=1.;
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| 57 |
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| 58 |
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| 59 |
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| 60 |
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| 61 |
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| 62 | }
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| 63 |
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| 64 | ///////////////////////////////////////////////////////
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| 65 | //
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| 66 | G4ContinuousGainOfEnergy::~G4ContinuousGainOfEnergy()
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| 67 | {
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| 68 |
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| 69 | }
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| 70 | ///////////////////////////////////////////////////////
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| 71 | //
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| 72 |
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| 73 | void G4ContinuousGainOfEnergy::PreparePhysicsTable(
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| 74 | const G4ParticleDefinition& )
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| 75 | {//theDirectEnergyLossProcess->PreparePhysicsTable(part);
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| 76 |
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| 77 | ;
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| 78 | }
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| 79 |
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| 80 | ///////////////////////////////////////////////////////
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| 81 | //
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| 82 |
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| 83 | void G4ContinuousGainOfEnergy::BuildPhysicsTable(const G4ParticleDefinition&)
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| 84 | {//theDirectEnergyLossProcess->BuildPhysicsTable(part);
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| 85 | ;
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| 86 | }
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| 87 |
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| 88 | ///////////////////////////////////////////////////////
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| 89 | //
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| 90 | void G4ContinuousGainOfEnergy::SetDirectParticle(G4ParticleDefinition* p)
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| 91 | {theDirectPartDef=p;
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| 92 | if (theDirectPartDef->GetParticleType()== "nucleus") {
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| 93 | IsIon=true;
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| 94 | massRatio = proton_mass_c2/theDirectPartDef->GetPDGMass();
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| 95 | G4double q=theDirectPartDef->GetPDGCharge();
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| 96 | chargeSqRatio=q*q;
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| 97 |
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| 98 |
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| 99 | }
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| 100 |
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| 101 | }
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| 102 |
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| 103 | ///////////////////////////////////////////////////////
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| 104 | //
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| 105 | //
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| 106 | G4VParticleChange* G4ContinuousGainOfEnergy::AlongStepDoIt(const G4Track& track,
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| 107 | const G4Step& step)
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| 108 | {
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| 109 |
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| 110 | //Caution in this method the step length should be the true step length
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| 111 | // A problem is that this is compute by the multiple scattering that does not know the energy at the end of the adjoint step. This energy is used during the
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| 112 | //Forward sim. Nothing we can really do against that at this time. This is inherent to the MS method
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| 113 | //
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| 114 |
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| 115 |
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| 116 |
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| 117 | aParticleChange.Initialize(track);
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| 118 |
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| 119 | // Get the actual (true) Step length
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| 120 | //----------------------------------
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| 121 | G4double length = step.GetStepLength();
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| 122 | G4double degain = 0.0;
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| 123 |
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| 124 |
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| 125 |
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| 126 | // Compute this for weight change after continuous energy loss
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| 127 | //-------------------------------------------------------------
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| 128 | G4double DEDX_before = theDirectEnergyLossProcess->GetDEDX(preStepKinEnergy, currentCouple);
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| 129 |
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| 130 |
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| 131 |
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| 132 | // For the fluctuation we generate a new dynamic particle with energy =preEnergy+egain
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| 133 | // and then compute the fluctuation given in the direct case.
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| 134 | //-----------------------------------------------------------------------
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| 135 | G4DynamicParticle* dynParticle = new G4DynamicParticle();
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| 136 | *dynParticle = *(track.GetDynamicParticle());
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| 137 | dynParticle->SetDefinition(theDirectPartDef);
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| 138 | G4double Tkin = dynParticle->GetKineticEnergy();
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| 139 | G4double Tkin1=Tkin*0.001;
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| 140 |
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| 141 | size_t n=1;
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| 142 | if (is_integral ) n=10;
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| 143 | n=1;
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| 144 | G4double dlength= length/n;
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| 145 | for (size_t i=0;i<n;i++) {
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| 146 | G4double factor_dE=1.;
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| 147 | if (Tkin != preStepKinEnergy && IsIon) {
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| 148 | chargeSqRatio = currentModel->GetChargeSquareRatio(theDirectPartDef,currentMaterial,Tkin);
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| 149 | theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,chargeSqRatio);
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| 150 |
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| 151 | }
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| 152 |
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| 153 | G4double r = theDirectEnergyLossProcess->GetRange(Tkin, currentCouple);
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| 154 | if( dlength <= linLossLimit * r ) {
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| 155 | degain = DEDX_before*dlength;
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| 156 | G4double degain1 = dlength*theDirectEnergyLossProcess->GetDEDX(Tkin1, currentCouple);
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| 157 | factor_dE=1.+(degain1-degain)/(Tkin1-Tkin);
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| 158 | }
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| 159 | else {
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| 160 | G4double x = r + dlength;
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| 161 | //degain = theDirectEnergyLossProcess->GetKineticEnergy(x,currentCouple) - theDirectEnergyLossProcess->GetKineticEnergy(r,currentCouple);
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| 162 | G4double E = theDirectEnergyLossProcess->GetKineticEnergy(x,currentCouple);
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| 163 | if (IsIon){
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| 164 | chargeSqRatio = currentModel->GetChargeSquareRatio(theDirectPartDef,currentMaterial,E);
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| 165 | theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,chargeSqRatio);
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| 166 | G4double x1= theDirectEnergyLossProcess->GetRange(E, currentCouple);
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| 167 | while (std::abs(x-x1)>0.01*x) {
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| 168 | E = theDirectEnergyLossProcess->GetKineticEnergy(x,currentCouple);
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| 169 | chargeSqRatio = currentModel->GetChargeSquareRatio(theDirectPartDef,currentMaterial,E);
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| 170 | theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,chargeSqRatio);
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| 171 | x1= theDirectEnergyLossProcess->GetRange(E, currentCouple);
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| 172 |
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| 173 | }
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| 174 | }
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| 175 | G4double r1 = theDirectEnergyLossProcess->GetRange(Tkin1, currentCouple);
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| 176 | G4double x1 = r1 + dlength;
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| 177 | G4double E1 = theDirectEnergyLossProcess->GetKineticEnergy(x1,currentCouple);
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| 178 | factor_dE=(E1-E)/(Tkin1-Tkin);
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| 179 | degain=E-Tkin;
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| 180 |
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| 181 |
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| 182 |
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| 183 | }
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| 184 | //G4cout<<degain<<G4endl;
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| 185 | G4double tmax = currentModel->MaxSecondaryKinEnergy(dynParticle);
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| 186 | tmax = std::min(tmax,currentTcut);
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| 187 |
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| 188 |
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| 189 | dynParticle->SetKineticEnergy(Tkin+degain);
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| 190 |
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| 191 | // Corrections, which cannot be tabulated for ions
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| 192 | //----------------------------------------
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| 193 | G4double esecdep=0;//not used in most models
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| 194 | currentModel->CorrectionsAlongStep(currentCouple, dynParticle, degain,esecdep, dlength);
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| 195 |
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| 196 | // Sample fluctuations
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| 197 | //-------------------
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| 198 |
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| 199 |
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| 200 | G4double deltaE =0.;
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| 201 | if (lossFluctuationFlag ) {
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| 202 | deltaE = currentModel->GetModelOfFluctuations()->
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| 203 | SampleFluctuations(currentMaterial,dynParticle,tmax,dlength,degain)-degain;
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| 204 | }
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| 205 |
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| 206 | G4double egain=degain+deltaE;
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| 207 | if (egain <=0) egain=degain;
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| 208 | Tkin+=egain;
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| 209 | dynParticle->SetKineticEnergy(Tkin);
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| 210 | }
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| 211 |
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| 212 |
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| 213 |
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| 214 |
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| 215 |
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| 216 | delete dynParticle;
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| 217 |
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| 218 | if (IsIon){
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| 219 | chargeSqRatio = currentModel->GetChargeSquareRatio(theDirectPartDef,currentMaterial,Tkin);
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| 220 | theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,chargeSqRatio);
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| 221 |
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| 222 | }
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| 223 |
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| 224 | G4double DEDX_after = theDirectEnergyLossProcess->GetDEDX(Tkin, currentCouple);
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| 225 |
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| 226 |
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| 227 | G4double weight_correction=DEDX_after/DEDX_before;
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| 228 |
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| 229 |
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| 230 | aParticleChange.ProposeEnergy(Tkin);
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| 231 |
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| 232 | //we still need to register in the particleChange the modification of the weight of the particle
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| 233 | G4double new_weight=weight_correction*track.GetWeight();
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| 234 | aParticleChange.SetParentWeightByProcess(false);
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| 235 | aParticleChange.ProposeParentWeight(new_weight);
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| 236 |
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| 237 |
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| 238 | return &aParticleChange;
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| 239 |
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| 240 | }
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| 241 | ///////////////////////////////////////////////////////
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| 242 | //
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| 243 | void G4ContinuousGainOfEnergy::SetLossFluctuations(G4bool val)
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| 244 | {
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| 245 | if(val && !lossFluctuationArePossible) return;
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| 246 | lossFluctuationFlag = val;
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| 247 | }
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| 248 | ///////////////////////////////////////////////////////
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| 249 | //
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| 250 |
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| 251 |
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| 252 |
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| 253 | G4double G4ContinuousGainOfEnergy::GetContinuousStepLimit(const G4Track& track,
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| 254 | G4double , G4double , G4double& )
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| 255 | {
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| 256 | G4double x = DBL_MAX;
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| 257 | x=.1*mm;
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| 258 |
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| 259 |
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| 260 | DefineMaterial(track.GetMaterialCutsCouple());
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| 261 |
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| 262 | preStepKinEnergy = track.GetKineticEnergy();
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| 263 | preStepScaledKinEnergy = track.GetKineticEnergy()*massRatio;
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| 264 | currentModel = theDirectEnergyLossProcess->SelectModelForMaterial(preStepScaledKinEnergy,currentCoupleIndex);
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| 265 | G4double emax_model=currentModel->HighEnergyLimit();
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| 266 | if (IsIon) {
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| 267 | chargeSqRatio = currentModel->GetChargeSquareRatio(theDirectPartDef,currentMaterial,preStepKinEnergy);
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| 268 | preStepChargeSqRatio = chargeSqRatio;
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| 269 | theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,preStepChargeSqRatio);
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| 270 | }
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| 271 |
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| 272 |
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| 273 | G4double maxE =1.1*preStepKinEnergy;
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| 274 | /*if (preStepKinEnergy< 0.05*MeV) maxE =2.*preStepKinEnergy;
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| 275 | else if (preStepKinEnergy< 0.1*MeV) maxE =1.5*preStepKinEnergy;
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| 276 | else if (preStepKinEnergy< 0.5*MeV) maxE =1.25*preStepKinEnergy;*/
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| 277 |
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| 278 | if (preStepKinEnergy < currentTcut) maxE = std::min(currentTcut,maxE);
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| 279 |
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| 280 | maxE=std::min(emax_model*1.001,maxE);
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| 281 |
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| 282 | G4double r = theDirectEnergyLossProcess->GetRange(preStepKinEnergy, currentCouple);
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| 283 |
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| 284 | if (IsIon) {
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| 285 | G4double chargeSqRatioAtEmax = currentModel->GetChargeSquareRatio(theDirectPartDef,currentMaterial,maxE);
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| 286 | theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,chargeSqRatioAtEmax);
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| 287 | }
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| 288 |
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| 289 | G4double r1 = theDirectEnergyLossProcess->GetRange(maxE, currentCouple);
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| 290 |
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| 291 | if (IsIon) theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,preStepChargeSqRatio);
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| 292 |
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| 293 |
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| 294 |
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| 295 | x=r1-r;
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| 296 | x=std::max(r1-r,0.001*mm);
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| 297 |
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| 298 | return x;
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| 299 |
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| 300 |
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| 301 | }
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| 302 | #include "G4EmCorrections.hh"
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| 303 | ///////////////////////////////////////////////////////
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| 304 | //
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| 305 |
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| 306 | void G4ContinuousGainOfEnergy::SetDynamicMassCharge(const G4Track& ,G4double energy)
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| 307 | {
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| 308 |
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| 309 | G4double ChargeSqRatio= G4LossTableManager::Instance()->EmCorrections()->EffectiveChargeSquareRatio(theDirectPartDef,currentMaterial,energy);
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| 310 | if (theDirectEnergyLossProcess) theDirectEnergyLossProcess->SetDynamicMassCharge(massRatio,ChargeSqRatio);
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| 311 | }
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