| 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: G4LivermoreRayleighModel.cc,v 1.1 2008/10/30 14:16:35 sincerti Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-02 $
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| 28 | //
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| 29 |
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| 30 | #include "G4LivermoreRayleighModel.hh"
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| 31 |
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| 32 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 33 |
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| 34 | using namespace std;
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| 35 |
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| 36 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 37 |
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| 38 | G4LivermoreRayleighModel::G4LivermoreRayleighModel(const G4ParticleDefinition*,
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| 39 | const G4String& nam)
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| 40 | :G4VEmModel(nam),isInitialised(false)
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| 41 | {
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| 42 | lowEnergyLimit = 250 * eV; // SI - Could be 10 eV ?
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| 43 | highEnergyLimit = 100 * GeV;
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| 44 |
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| 45 | SetLowEnergyLimit(lowEnergyLimit);
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| 46 | SetHighEnergyLimit(highEnergyLimit);
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| 47 | //
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| 48 | verboseLevel= 0;
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| 49 | // Verbosity scale:
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| 50 | // 0 = nothing
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| 51 | // 1 = warning for energy non-conservation
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| 52 | // 2 = details of energy budget
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| 53 | // 3 = calculation of cross sections, file openings, sampling of atoms
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| 54 | // 4 = entering in methods
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| 55 |
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| 56 | G4cout << "Livermore Rayleigh is constructed " << G4endl
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| 57 | << "Energy range: "
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| 58 | << lowEnergyLimit / keV << " keV - "
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| 59 | << highEnergyLimit / GeV << " GeV"
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| 60 | << G4endl;
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| 61 | }
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| 62 |
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| 63 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 64 |
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| 65 | G4LivermoreRayleighModel::~G4LivermoreRayleighModel()
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| 66 | {
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| 67 | delete meanFreePathTable;
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| 68 | delete crossSectionHandler;
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| 69 | delete formFactorData;
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| 70 | }
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| 71 |
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| 72 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 73 |
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| 74 | void G4LivermoreRayleighModel::Initialise(const G4ParticleDefinition* particle,
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| 75 | const G4DataVector& cuts)
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| 76 | {
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| 77 | if (verboseLevel > 3)
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| 78 | G4cout << "Calling G4LivermoreRayleighModel::Initialise()" << G4endl;
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| 79 |
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| 80 | InitialiseElementSelectors(particle,cuts);
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| 81 |
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| 82 | // Energy limits
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| 83 |
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| 84 | if (LowEnergyLimit() < lowEnergyLimit)
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| 85 | {
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| 86 | G4cout << "G4LivermoreRayleighModel: low energy limit increased from " <<
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| 87 | LowEnergyLimit()/eV << " eV to " << lowEnergyLimit << " eV" << G4endl;
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| 88 | SetLowEnergyLimit(lowEnergyLimit);
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| 89 | }
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| 90 |
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| 91 | if (HighEnergyLimit() > highEnergyLimit)
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| 92 | {
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| 93 | G4cout << "G4LivermoreRayleighModel: high energy limit decreased from " <<
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| 94 | HighEnergyLimit()/GeV << " GeV to " << highEnergyLimit << " GeV" << G4endl;
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| 95 | SetHighEnergyLimit(highEnergyLimit);
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| 96 | }
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| 97 |
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| 98 | // Data are read for all materials
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| 99 |
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| 100 | crossSectionHandler = new G4CrossSectionHandler;
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| 101 | crossSectionHandler->Clear();
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| 102 | G4String crossSectionFile = "rayl/re-cs-";
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| 103 | crossSectionHandler->LoadData(crossSectionFile);
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| 104 |
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| 105 | meanFreePathTable = 0;
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| 106 | meanFreePathTable = crossSectionHandler->BuildMeanFreePathForMaterials();
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| 107 |
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| 108 | G4VDataSetAlgorithm* ffInterpolation = new G4LogLogInterpolation;
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| 109 | G4String formFactorFile = "rayl/re-ff-";
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| 110 | formFactorData = new G4CompositeEMDataSet(ffInterpolation,1.,1.);
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| 111 | formFactorData->LoadData(formFactorFile);
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| 112 |
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| 113 | //
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| 114 |
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| 115 | if (verboseLevel > 2)
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| 116 | G4cout << "Loaded cross section files for Livermore Rayleigh model" << G4endl;
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| 117 |
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| 118 | G4cout << "Livermore Rayleigh model is initialized " << G4endl
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| 119 | << "Energy range: "
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| 120 | << LowEnergyLimit() / keV << " keV - "
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| 121 | << HighEnergyLimit() / GeV << " GeV"
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| 122 | << G4endl;
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| 123 |
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| 124 | if(isInitialised) return;
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| 125 |
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| 126 | if(pParticleChange)
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| 127 | fParticleChange = reinterpret_cast<G4ParticleChangeForGamma*>(pParticleChange);
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| 128 | else
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| 129 | fParticleChange = new G4ParticleChangeForGamma();
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| 130 |
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| 131 | isInitialised = true;
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| 132 |
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| 133 | }
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| 134 |
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| 135 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 136 |
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| 137 | G4double G4LivermoreRayleighModel::ComputeCrossSectionPerAtom(
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| 138 | const G4ParticleDefinition*,
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| 139 | G4double GammaEnergy,
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| 140 | G4double Z, G4double,
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| 141 | G4double, G4double)
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| 142 | {
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| 143 | if (verboseLevel > 3)
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| 144 | G4cout << "Calling CrossSectionPerAtom() of G4LivermoreRayleighModel" << G4endl;
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| 145 |
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| 146 | G4double cs = crossSectionHandler->FindValue(G4int(Z), GammaEnergy);
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| 147 | return cs;
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| 148 | }
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| 149 |
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| 150 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 151 |
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| 152 | void G4LivermoreRayleighModel::SampleSecondaries(std::vector<G4DynamicParticle*>* /*fvect*/,
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| 153 | const G4MaterialCutsCouple* couple,
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| 154 | const G4DynamicParticle* aDynamicGamma,
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| 155 | G4double,
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| 156 | G4double)
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| 157 | {
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| 158 | if (verboseLevel > 3)
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| 159 | G4cout << "Calling SampleSecondaries() of G4LivermoreRayleighModel" << G4endl;
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| 160 |
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| 161 | G4double photonEnergy0 = aDynamicGamma->GetKineticEnergy();
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| 162 |
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| 163 | if (photonEnergy0 <= lowEnergyLimit)
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| 164 | {
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| 165 | fParticleChange->ProposeTrackStatus(fStopAndKill);
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| 166 | fParticleChange->SetProposedKineticEnergy(0.);
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| 167 | fParticleChange->ProposeLocalEnergyDeposit(photonEnergy0);
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| 168 | // SI - IS THE FOLLOWING RETURN NECESSARY ?
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| 169 | return ;
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| 170 | }
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| 171 |
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| 172 | G4ParticleMomentum photonDirection0 = aDynamicGamma->GetMomentumDirection();
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| 173 |
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| 174 | // Select randomly one element in the current material
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| 175 | G4int Z = crossSectionHandler->SelectRandomAtom(couple,photonEnergy0);
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| 176 |
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| 177 | // Sample the angle of the scattered photon
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| 178 |
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| 179 | G4double wlPhoton = h_Planck*c_light/photonEnergy0;
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| 180 |
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| 181 | G4double gReject,x,dataFormFactor;
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| 182 | G4double randomFormFactor;
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| 183 | G4double cosTheta;
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| 184 | G4double sinTheta;
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| 185 | G4double fcostheta;
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| 186 |
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| 187 | do
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| 188 | {
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| 189 | do
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| 190 | {
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| 191 | cosTheta = 2. * G4UniformRand() - 1.;
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| 192 | fcostheta = ( 1. + cosTheta*cosTheta)/2.;
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| 193 | } while (fcostheta < G4UniformRand());
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| 194 |
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| 195 | G4double sinThetaHalf = std::sqrt((1. - cosTheta) / 2.);
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| 196 | x = sinThetaHalf / (wlPhoton/cm);
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| 197 | if (x > 1.e+005)
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| 198 | dataFormFactor = formFactorData->FindValue(x,Z-1);
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| 199 | else
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| 200 | dataFormFactor = formFactorData->FindValue(0.,Z-1);
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| 201 | randomFormFactor = G4UniformRand() * Z * Z;
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| 202 | sinTheta = std::sqrt(1. - cosTheta*cosTheta);
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| 203 | gReject = dataFormFactor * dataFormFactor;
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| 204 |
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| 205 | } while( gReject < randomFormFactor);
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| 206 |
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| 207 | // Scattered photon angles. ( Z - axis along the parent photon)
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| 208 | G4double phi = twopi * G4UniformRand() ;
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| 209 | G4double dirX = sinTheta*std::cos(phi);
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| 210 | G4double dirY = sinTheta*std::sin(phi);
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| 211 | G4double dirZ = cosTheta;
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| 212 |
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| 213 | // Update G4VParticleChange for the scattered photon
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| 214 | G4ThreeVector photonDirection1(dirX, dirY, dirZ);
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| 215 | photonDirection1.rotateUz(photonDirection0);
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| 216 | fParticleChange->ProposeMomentumDirection(photonDirection1);
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| 217 |
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| 218 | fParticleChange->SetProposedKineticEnergy(photonEnergy0);
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| 219 | }
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| 220 |
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| 221 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 222 |
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| 223 | G4double G4LivermoreRayleighModel::GetMeanFreePath(const G4Track& track,
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| 224 | G4double, // previousStepSize
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| 225 | G4ForceCondition*)
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| 226 | {
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| 227 | const G4DynamicParticle* photon = track.GetDynamicParticle();
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| 228 | G4double energy = photon->GetKineticEnergy();
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| 229 | const G4MaterialCutsCouple* couple = track.GetMaterialCutsCouple();
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| 230 | size_t materialIndex = couple->GetIndex();
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| 231 |
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| 232 | G4double meanFreePath;
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| 233 | if (energy > highEnergyLimit) meanFreePath = meanFreePathTable->FindValue(highEnergyLimit,materialIndex);
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| 234 | else if (energy < lowEnergyLimit) meanFreePath = DBL_MAX;
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| 235 | else meanFreePath = meanFreePathTable->FindValue(energy,materialIndex);
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| 236 | return meanFreePath;
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| 237 | }
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| 238 |
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