| 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: G4PEEffectModel.cc,v 1.8 2009/04/09 18:41:18 vnivanch Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-03 $
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| 28 | //
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| 29 | // -------------------------------------------------------------------
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| 30 | //
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| 31 | // GEANT4 Class file
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| 32 | //
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| 33 | //
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| 34 | // File name: G4PEEffectModel
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| 35 | //
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| 36 | // Author: Vladimir Ivanchenko on base of Michel Maire code
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| 37 | //
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| 38 | // Creation date: 21.03.2005
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| 39 | //
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| 40 | // Modifications:
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| 41 | //
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| 42 | // 04.12.05 : SetProposedKineticEnergy(0.) for the killed photon (mma)
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| 43 | // 20.02.09 : Added initialisation of deexcitation flag and method
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| 44 | // CrossSectionPerVolume instead of mfp (V.Ivanchenko)
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| 45 | //
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| 46 | // Class Description:
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| 47 | //
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| 48 | // -------------------------------------------------------------------
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| 49 | //
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| 50 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 51 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 52 |
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| 53 | #include "G4PEEffectModel.hh"
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| 54 | #include "G4Electron.hh"
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| 55 | #include "G4Gamma.hh"
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| 56 | #include "Randomize.hh"
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| 57 | #include "G4DataVector.hh"
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| 58 | #include "G4ParticleChangeForGamma.hh"
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| 59 |
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| 60 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 61 |
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| 62 | using namespace std;
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| 63 |
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| 64 | G4PEEffectModel::G4PEEffectModel(const G4ParticleDefinition*,
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| 65 | const G4String& nam)
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| 66 | : G4VEmModel(nam),isInitialized(false)
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| 67 | {
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| 68 | theGamma = G4Gamma::Gamma();
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| 69 | theElectron = G4Electron::Electron();
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| 70 | fminimalEnergy = 1.0*eV;
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| 71 | }
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| 72 |
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| 73 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 74 |
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| 75 | G4PEEffectModel::~G4PEEffectModel()
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| 76 | {}
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| 77 |
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| 78 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 79 |
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| 80 | void G4PEEffectModel::Initialise(const G4ParticleDefinition*,
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| 81 | const G4DataVector&)
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| 82 | {
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| 83 | // always false before the run
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| 84 | SetDeexcitationFlag(false);
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| 85 |
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| 86 | if (isInitialized) return;
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| 87 | fParticleChange = GetParticleChangeForGamma();
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| 88 | isInitialized = true;
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| 89 | }
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| 90 |
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| 91 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.....
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| 92 |
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| 93 | G4double G4PEEffectModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*,
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| 94 | G4double energy,
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| 95 | G4double Z, G4double,
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| 96 | G4double, G4double)
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| 97 | {
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| 98 | G4double* SandiaCof = G4SandiaTable::GetSandiaCofPerAtom((G4int)Z, energy);
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| 99 |
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| 100 | G4double energy2 = energy*energy;
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| 101 | G4double energy3 = energy*energy2;
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| 102 | G4double energy4 = energy2*energy2;
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| 103 |
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| 104 | return SandiaCof[0]/energy + SandiaCof[1]/energy2 +
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| 105 | SandiaCof[2]/energy3 + SandiaCof[3]/energy4;
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| 106 | }
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| 107 |
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| 108 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 109 |
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| 110 | G4double G4PEEffectModel::CrossSectionPerVolume(const G4Material* material,
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| 111 | const G4ParticleDefinition*,
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| 112 | G4double energy,
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| 113 | G4double, G4double)
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| 114 | {
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| 115 | G4double* SandiaCof =
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| 116 | material->GetSandiaTable()->GetSandiaCofForMaterial(energy);
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| 117 |
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| 118 | G4double energy2 = energy*energy;
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| 119 | G4double energy3 = energy*energy2;
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| 120 | G4double energy4 = energy2*energy2;
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| 121 |
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| 122 | return SandiaCof[0]/energy + SandiaCof[1]/energy2 +
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| 123 | SandiaCof[2]/energy3 + SandiaCof[3]/energy4;
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| 124 | }
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| 125 |
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| 126 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 127 |
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| 128 | void G4PEEffectModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
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| 129 | const G4MaterialCutsCouple* couple,
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| 130 | const G4DynamicParticle* aDynamicPhoton,
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| 131 | G4double,
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| 132 | G4double)
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| 133 | {
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| 134 | const G4Material* aMaterial = couple->GetMaterial();
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| 135 |
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| 136 | G4double energy = aDynamicPhoton->GetKineticEnergy();
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| 137 | G4ParticleMomentum PhotonDirection = aDynamicPhoton->GetMomentumDirection();
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| 138 |
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| 139 | // select randomly one element constituing the material.
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| 140 | const G4Element* anElement = SelectRandomAtom(aMaterial,theGamma,energy);
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| 141 |
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| 142 | //
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| 143 | // Photo electron
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| 144 | //
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| 145 |
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| 146 | // Select atomic shell
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| 147 | G4int nShells = anElement->GetNbOfAtomicShells();
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| 148 | G4int i = 0;
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| 149 | while ((i<nShells) && (energy<anElement->GetAtomicShell(i))) i++;
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| 150 |
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| 151 | // no shell available
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| 152 | if (i == nShells) return;
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| 153 |
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| 154 | G4double bindingEnergy = anElement->GetAtomicShell(i);
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| 155 | G4double ElecKineEnergy = energy - bindingEnergy;
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| 156 |
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| 157 | if (ElecKineEnergy > fminimalEnergy)
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| 158 | {
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| 159 | // direction of the photo electron
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| 160 | //
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| 161 | G4double cosTeta = ElecCosThetaDistribution(ElecKineEnergy);
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| 162 | G4double sinTeta = sqrt(1.-cosTeta*cosTeta);
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| 163 | G4double Phi = twopi * G4UniformRand();
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| 164 | G4double dirx = sinTeta*cos(Phi),diry = sinTeta*sin(Phi),dirz = cosTeta;
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| 165 | G4ThreeVector ElecDirection(dirx,diry,dirz);
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| 166 | ElecDirection.rotateUz(PhotonDirection);
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| 167 | //
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| 168 | G4DynamicParticle* aParticle = new G4DynamicParticle (
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| 169 | theElectron,ElecDirection, ElecKineEnergy);
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| 170 | fvect->push_back(aParticle);
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| 171 | }
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| 172 |
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| 173 | fParticleChange->SetProposedKineticEnergy(0.);
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| 174 | fParticleChange->ProposeTrackStatus(fStopAndKill);
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| 175 | fParticleChange->ProposeLocalEnergyDeposit(bindingEnergy);
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| 176 | }
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| 177 |
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| 178 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 179 |
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| 180 | G4double G4PEEffectModel::ElecCosThetaDistribution(G4double kineEnergy)
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| 181 | {
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| 182 | // Compute Theta distribution of the emitted electron, with respect to the
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| 183 | // incident Gamma.
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| 184 | // The Sauter-Gavrila distribution for the K-shell is used.
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| 185 | //
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| 186 | G4double costeta = 1.;
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| 187 | G4double gamma = 1. + kineEnergy/electron_mass_c2;
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| 188 | if (gamma > 5.) return costeta;
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| 189 | G4double beta = sqrt(gamma*gamma-1.)/gamma;
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| 190 | G4double b = 0.5*gamma*(gamma-1.)*(gamma-2);
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| 191 |
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| 192 | G4double rndm,term,greject,grejsup;
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| 193 | if (gamma < 2.) grejsup = gamma*gamma*(1.+b-beta*b);
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| 194 | else grejsup = gamma*gamma*(1.+b+beta*b);
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| 195 |
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| 196 | do { rndm = 1.-2*G4UniformRand();
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| 197 | costeta = (rndm+beta)/(rndm*beta+1.);
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| 198 | term = 1.-beta*costeta;
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| 199 | greject = (1.-costeta*costeta)*(1.+b*term)/(term*term);
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| 200 | } while(greject < G4UniformRand()*grejsup);
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| 201 |
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| 202 | return costeta;
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| 203 | }
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| 204 |
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| 205 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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