| 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: G4AdjointeIonisationModel.cc,v 1.2 2009/11/20 10:31:20 ldesorgh Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-04-beta-01 $
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| 28 | //
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| 29 | #include "G4AdjointeIonisationModel.hh"
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| 30 | #include "G4AdjointCSManager.hh"
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| 31 |
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| 32 |
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| 33 | #include "G4Integrator.hh"
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| 34 | #include "G4TrackStatus.hh"
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| 35 | #include "G4ParticleChange.hh"
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| 36 | #include "G4AdjointElectron.hh"
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| 37 | #include "G4Gamma.hh"
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| 38 | #include "G4AdjointGamma.hh"
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| 39 |
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| 40 |
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| 41 | ////////////////////////////////////////////////////////////////////////////////
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| 42 | //
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| 43 | G4AdjointeIonisationModel::G4AdjointeIonisationModel():
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| 44 | G4VEmAdjointModel("Inv_eIon_model")
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| 45 |
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| 46 | {
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| 47 |
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| 48 | UseMatrix =true;
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| 49 | UseMatrixPerElement = true;
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| 50 | ApplyCutInRange = true;
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| 51 | UseOnlyOneMatrixForAllElements = true;
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| 52 | CS_biasing_factor =1.;
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| 53 | WithRapidSampling = false;
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| 54 |
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| 55 | theAdjEquivOfDirectPrimPartDef =G4AdjointElectron::AdjointElectron();
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| 56 | theAdjEquivOfDirectSecondPartDef=G4AdjointElectron::AdjointElectron();
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| 57 | theDirectPrimaryPartDef=G4Electron::Electron();
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| 58 | second_part_of_same_type=true;
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| 59 | }
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| 60 | ////////////////////////////////////////////////////////////////////////////////
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| 61 | //
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| 62 | G4AdjointeIonisationModel::~G4AdjointeIonisationModel()
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| 63 | {;}
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| 64 | ////////////////////////////////////////////////////////////////////////////////
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| 65 | //
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| 66 | void G4AdjointeIonisationModel::SampleSecondaries(const G4Track& aTrack,
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| 67 | G4bool IsScatProjToProjCase,
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| 68 | G4ParticleChange* fParticleChange)
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| 69 | {
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| 70 |
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| 71 |
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| 72 | const G4DynamicParticle* theAdjointPrimary =aTrack.GetDynamicParticle();
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| 73 |
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| 74 | //Elastic inverse scattering
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| 75 | //---------------------------------------------------------
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| 76 | G4double adjointPrimKinEnergy = theAdjointPrimary->GetKineticEnergy();
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| 77 | G4double adjointPrimP =theAdjointPrimary->GetTotalMomentum();
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| 78 |
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| 79 | if (adjointPrimKinEnergy>HighEnergyLimit*0.999){
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| 80 | return;
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| 81 | }
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| 82 |
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| 83 | //Sample secondary energy
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| 84 | //-----------------------
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| 85 | G4double projectileKinEnergy;
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| 86 | if (!WithRapidSampling ) { //used by default
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| 87 | projectileKinEnergy = SampleAdjSecEnergyFromCSMatrix(adjointPrimKinEnergy, IsScatProjToProjCase);
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| 88 |
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| 89 | CorrectPostStepWeight(fParticleChange,
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| 90 | aTrack.GetWeight(),
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| 91 | adjointPrimKinEnergy,
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| 92 | projectileKinEnergy,
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| 93 | IsScatProjToProjCase); //Caution !!!this weight correction should be always applied
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| 94 | }
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| 95 | else { //only for test at the moment
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| 96 |
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| 97 | G4double Emin,Emax;
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| 98 | if (IsScatProjToProjCase) {
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| 99 | Emin=GetSecondAdjEnergyMinForScatProjToProjCase(adjointPrimKinEnergy,currentTcutForDirectSecond);
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| 100 | Emax=GetSecondAdjEnergyMaxForScatProjToProjCase(adjointPrimKinEnergy);
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| 101 | }
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| 102 | else {
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| 103 | Emin=GetSecondAdjEnergyMinForProdToProjCase(adjointPrimKinEnergy);
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| 104 | Emax=GetSecondAdjEnergyMaxForProdToProjCase(adjointPrimKinEnergy);
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| 105 | }
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| 106 | projectileKinEnergy = Emin*std::pow(Emax/Emin,G4UniformRand());
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| 107 |
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| 108 |
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| 109 |
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| 110 | lastCS=lastAdjointCSForScatProjToProjCase;
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| 111 | if ( !IsScatProjToProjCase) lastCS=lastAdjointCSForProdToProjCase;
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| 112 |
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| 113 | G4double new_weight=aTrack.GetWeight();
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| 114 | G4double used_diffCS=lastCS*std::log(Emax/Emin)/projectileKinEnergy;
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| 115 | G4double needed_diffCS=adjointPrimKinEnergy/projectileKinEnergy;
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| 116 | if (!IsScatProjToProjCase) needed_diffCS *=DiffCrossSectionPerVolumePrimToSecond(currentMaterial,projectileKinEnergy,adjointPrimKinEnergy);
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| 117 | else needed_diffCS *=DiffCrossSectionPerVolumePrimToScatPrim(currentMaterial,projectileKinEnergy,adjointPrimKinEnergy);
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| 118 | new_weight*=needed_diffCS/used_diffCS;
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| 119 | fParticleChange->SetParentWeightByProcess(false);
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| 120 | fParticleChange->SetSecondaryWeightByProcess(false);
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| 121 | fParticleChange->ProposeParentWeight(new_weight);
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| 122 |
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| 123 |
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| 124 | }
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| 125 |
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| 126 |
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| 127 |
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| 128 | //Kinematic:
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| 129 | //we consider a two body elastic scattering for the forward processes where the projectile knock on an e- at rest and gives
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| 130 | // him part of its energy
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| 131 | //----------------------------------------------------------------------------------------
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| 132 |
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| 133 | G4double projectileM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
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| 134 | G4double projectileTotalEnergy = projectileM0+projectileKinEnergy;
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| 135 | G4double projectileP2 = projectileTotalEnergy*projectileTotalEnergy - projectileM0*projectileM0;
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| 136 |
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| 137 |
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| 138 |
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| 139 | //Companion
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| 140 | //-----------
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| 141 | G4double companionM0 = theAdjEquivOfDirectPrimPartDef->GetPDGMass();
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| 142 | if (IsScatProjToProjCase) {
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| 143 | companionM0=theAdjEquivOfDirectSecondPartDef->GetPDGMass();
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| 144 | }
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| 145 | G4double companionTotalEnergy =companionM0+ projectileKinEnergy-adjointPrimKinEnergy;
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| 146 | G4double companionP2 = companionTotalEnergy*companionTotalEnergy - companionM0*companionM0;
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| 147 |
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| 148 |
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| 149 | //Projectile momentum
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| 150 | //--------------------
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| 151 | G4double P_parallel = (adjointPrimP*adjointPrimP + projectileP2 - companionP2)/(2.*adjointPrimP);
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| 152 | G4double P_perp = std::sqrt( projectileP2 - P_parallel*P_parallel);
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| 153 | G4ThreeVector dir_parallel=theAdjointPrimary->GetMomentumDirection();
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| 154 | G4double phi =G4UniformRand()*2.*3.1415926;
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| 155 | G4ThreeVector projectileMomentum = G4ThreeVector(P_perp*std::cos(phi),P_perp*std::sin(phi),P_parallel);
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| 156 | projectileMomentum.rotateUz(dir_parallel);
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| 157 |
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| 158 |
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| 159 |
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| 160 | if (!IsScatProjToProjCase ){ //kill the primary and add a secondary
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| 161 | fParticleChange->ProposeTrackStatus(fStopAndKill);
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| 162 | fParticleChange->AddSecondary(new G4DynamicParticle(theAdjEquivOfDirectPrimPartDef,projectileMomentum));
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| 163 | //G4cout<<"projectileMomentum "<<projectileMomentum<<G4endl;
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| 164 | }
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| 165 | else {
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| 166 | fParticleChange->ProposeEnergy(projectileKinEnergy);
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| 167 | fParticleChange->ProposeMomentumDirection(projectileMomentum.unit());
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| 168 | }
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| 169 |
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| 170 |
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| 171 |
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| 172 |
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| 173 | }
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| 174 | ////////////////////////////////////////////////////////////////////////////////
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| 175 | //
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| 176 | //The implementation here is correct for energy loss process, for the photoelectric and compton scattering the method should be redefine
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| 177 | G4double G4AdjointeIonisationModel::DiffCrossSectionPerAtomPrimToSecond(
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| 178 | G4double kinEnergyProj,
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| 179 | G4double kinEnergyProd,
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| 180 | G4double Z,
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| 181 | G4double )
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| 182 | {
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| 183 | G4double dSigmadEprod=0;
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| 184 | G4double Emax_proj = GetSecondAdjEnergyMaxForProdToProjCase(kinEnergyProd);
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| 185 | G4double Emin_proj = GetSecondAdjEnergyMinForProdToProjCase(kinEnergyProd);
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| 186 |
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| 187 |
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| 188 | if (kinEnergyProj>Emin_proj && kinEnergyProj<=Emax_proj){ //the produced particle should have a kinetic energy smaller than the projectile
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| 189 | dSigmadEprod=Z*DiffCrossSectionMoller(kinEnergyProj,kinEnergyProd);
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| 190 | }
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| 191 | return dSigmadEprod;
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| 192 |
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| 193 |
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| 194 |
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| 195 | }
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| 196 |
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| 197 | //////////////////////////////////////////////////////////////////////////////
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| 198 | //
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| 199 | G4double G4AdjointeIonisationModel::DiffCrossSectionMoller(G4double kinEnergyProj,G4double kinEnergyProd){
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| 200 | G4double electron_mass_c2=0.51099906*MeV;
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| 201 | G4double energy = kinEnergyProj + electron_mass_c2;
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| 202 | G4double x = kinEnergyProd/kinEnergyProj;
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| 203 | G4double gam = energy/electron_mass_c2;
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| 204 | G4double gamma2 = gam*gam;
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| 205 | G4double beta2 = 1.0 - 1.0/gamma2;
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| 206 |
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| 207 | G4double g = (2.0*gam - 1.0)/gamma2;
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| 208 | G4double y = 1.0 - x;
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| 209 | G4double fac=twopi_mc2_rcl2/electron_mass_c2;
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| 210 | G4double dCS = fac*( 1.-g + ((1.0 - g*x)/(x*x)) + ((1.0 - g*y)/(y*y)))/(beta2*(gam-1));
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| 211 | return dCS/kinEnergyProj;
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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 |
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