| [968] | 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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| [991] | 26 | // $Id: G4LivermorePhotoElectricModel.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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| [968] | 28 | //
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| 29 |
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| 30 | #include "G4LivermorePhotoElectricModel.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 | G4LivermorePhotoElectricModel::G4LivermorePhotoElectricModel(const G4ParticleDefinition*,
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| 39 | const G4String& nam)
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| [991] | 40 | :G4VEmModel(nam),isInitialised(false)
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| [968] | 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 | SetLowEnergyLimit(lowEnergyLimit);
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| 45 | SetHighEnergyLimit(highEnergyLimit);
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| 46 |
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| 47 | G4cout << "Livermore Compton is constructed " << G4endl
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| 48 | << "Energy range: "
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| 49 | << lowEnergyLimit / keV << " keV - "
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| 50 | << highEnergyLimit / GeV << " GeV"
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| 51 | << G4endl;
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| 52 |
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| 53 | verboseLevel= 0;
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| 54 | // Verbosity scale:
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| 55 | // 0 = nothing
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| 56 | // 1 = warning for energy non-conservation
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| 57 | // 2 = details of energy budget
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| 58 | // 3 = calculation of cross sections, file openings, sampling of atoms
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| 59 | // 4 = entering in methods
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| 60 | }
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| 61 |
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| 62 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 63 |
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| 64 | G4LivermorePhotoElectricModel::~G4LivermorePhotoElectricModel()
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| 65 | {
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| [991] | 66 | delete meanFreePathTable;
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| 67 | delete crossSectionHandler;
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| 68 | delete shellCrossSectionHandler;
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| 69 | delete ElectronAngularGenerator;
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| [968] | 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 G4LivermorePhotoElectricModel::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 G4LivermorePhotoElectricModel::Initialise()" << G4endl;
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| 79 |
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| [991] | 80 | InitialiseElementSelectors(particle,cuts);
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| 81 |
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| [968] | 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 << "G4LivermorePhotoElectricModel: low energy limit increased from " <<
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| 87 | LowEnergyLimit()/eV << " eV to " << lowEnergyLimit << " eV" <<
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| 88 | G4endl;
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| 89 | SetLowEnergyLimit(lowEnergyLimit);
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| 90 | }
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| 91 |
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| 92 | if (HighEnergyLimit() > highEnergyLimit)
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| 93 | {
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| 94 | G4cout << "G4LivermorePhotoElectricModel: high energy limit decreased from " <<
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| 95 | HighEnergyLimit()/GeV << " GeV to " << highEnergyLimit << " GeV"
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| 96 | << G4endl;
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| 97 | SetHighEnergyLimit(highEnergyLimit);
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| 98 | }
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| 99 |
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| 100 | // Read data tables for all materials
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| 101 |
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| 102 | crossSectionHandler = new G4CrossSectionHandler();
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| 103 | crossSectionHandler->Clear();
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| 104 | G4String crossSectionFile = "phot/pe-cs-";
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| 105 | crossSectionHandler->LoadData(crossSectionFile);
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| 106 |
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| 107 | meanFreePathTable = 0;
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| 108 | meanFreePathTable = crossSectionHandler->BuildMeanFreePathForMaterials();
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| 109 |
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| 110 | shellCrossSectionHandler = new G4CrossSectionHandler();
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| 111 | shellCrossSectionHandler->Clear();
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| 112 | G4String shellCrossSectionFile = "phot/pe-ss-cs-";
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| 113 | shellCrossSectionHandler->LoadShellData(shellCrossSectionFile);
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| 114 |
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| 115 | // SI - Buggy default ?
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| 116 | //generatorName = "geant4.6.2";
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| 117 | //ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorSimple("GEANTSimpleGenerator"); // default generator
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| 118 |
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| 119 | //
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| 120 |
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| 121 | if (verboseLevel > 2)
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| 122 | G4cout << "Loaded cross section files for Livermore PhotoElectric model" << G4endl;
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| 123 |
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| 124 | G4cout << "Livermore PhotoElectric model is initialized " << G4endl
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| 125 | << "Energy range: "
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| 126 | << LowEnergyLimit() / keV << " keV - "
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| 127 | << HighEnergyLimit() / GeV << " GeV"
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| 128 | << G4endl;
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| 129 |
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| 130 | if(isInitialised) return;
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| 131 |
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| 132 | if(pParticleChange)
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| 133 | fParticleChange = reinterpret_cast<G4ParticleChangeForGamma*>(pParticleChange);
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| 134 | else
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| 135 | fParticleChange = new G4ParticleChangeForGamma();
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| 136 |
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| 137 | isInitialised = true;
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| 138 | }
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| 139 |
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| 140 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 141 |
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| 142 | G4double G4LivermorePhotoElectricModel::ComputeCrossSectionPerAtom(
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| 143 | const G4ParticleDefinition*,
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| 144 | G4double GammaEnergy,
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| 145 | G4double Z, G4double,
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| 146 | G4double, G4double)
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| 147 | {
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| 148 | if (verboseLevel > 3)
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| 149 | G4cout << "Calling ComputeCrossSectionPerAtom() of G4LivermorePhotoElectricModel" << G4endl;
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| 150 |
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| 151 | G4double cs = crossSectionHandler->FindValue(G4int(Z), GammaEnergy);
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| 152 | return cs;
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| 153 | }
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| 154 |
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| 155 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 156 |
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| 157 | void G4LivermorePhotoElectricModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect,
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| 158 | const G4MaterialCutsCouple* couple,
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| 159 | const G4DynamicParticle* aDynamicGamma,
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| 160 | G4double,
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| 161 | G4double)
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| 162 | {
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| 163 |
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| 164 | // Fluorescence generated according to:
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| 165 | // J. Stepanek ,"A program to determine the radiation spectra due to a single atomic
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| 166 | // subshell ionisation by a particle or due to deexcitation or decay of radionuclides",
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| 167 | // Comp. Phys. Comm. 1206 pp 1-1-9 (1997)
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| 168 |
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| 169 | if (verboseLevel > 3)
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| 170 | G4cout << "Calling SampleSecondaries() of G4LivermorePhotoElectricModel" << G4endl;
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| 171 |
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| 172 | G4double photonEnergy = aDynamicGamma->GetKineticEnergy();
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| 173 |
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| 174 | if (photonEnergy <= lowEnergyLimit)
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| 175 | {
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| 176 | fParticleChange->ProposeTrackStatus(fStopAndKill);
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| 177 | fParticleChange->SetProposedKineticEnergy(0.);
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| 178 | fParticleChange->ProposeLocalEnergyDeposit(photonEnergy);
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| [991] | 179 | // SI - IS THE FOLLOWING RETURN NECESSARY ?
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| [968] | 180 | return ;
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| 181 | }
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| 182 |
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| 183 | G4ThreeVector photonDirection = aDynamicGamma->GetMomentumDirection(); // Returns the normalized direction of the momentum
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| 184 |
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| 185 | // Select randomly one element in the current material
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| 186 | G4int Z = crossSectionHandler->SelectRandomAtom(couple,photonEnergy);
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| 187 |
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| 188 | // Select the ionised shell in the current atom according to shell cross sections
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| 189 | size_t shellIndex = shellCrossSectionHandler->SelectRandomShell(Z,photonEnergy);
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| 190 |
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| 191 | // Retrieve the corresponding identifier and binding energy of the selected shell
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| 192 | const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance();
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| 193 | const G4AtomicShell* shell = transitionManager->Shell(Z,shellIndex);
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| 194 | G4double bindingEnergy = shell->BindingEnergy();
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| 195 | G4int shellId = shell->ShellId();
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| 196 |
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| 197 | // Create lists of pointers to DynamicParticles (photons and electrons)
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| 198 | // (Is the electron vector necessary? To be checked)
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| 199 | std::vector<G4DynamicParticle*>* photonVector = 0;
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| 200 | std::vector<G4DynamicParticle*> electronVector;
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| 201 |
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| 202 | G4double energyDeposit = 0.0;
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| 203 |
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| 204 | // Primary outcoming electron
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| 205 | G4double eKineticEnergy = photonEnergy - bindingEnergy;
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| 206 |
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| 207 | // There may be cases where the binding energy of the selected shell is > photon energy
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| 208 | // In such cases do not generate secondaries
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| 209 | if (eKineticEnergy > 0.)
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| 210 | {
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| 211 | // SI - Removed safety
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| 212 |
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| 213 | // Generate the electron only if with large enough range w.r.t. cuts and safety
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| 214 | //G4double safety = aStep.GetPostStepPoint()->GetSafety();
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| 215 |
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| 216 | //if (rangeTest->Escape(G4Electron::Electron(),couple,eKineticEnergy,safety))
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| 217 | {
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| 218 |
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| 219 | // Calculate direction of the photoelectron
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| 220 | G4ThreeVector gammaPolarization = aDynamicGamma->GetPolarization();
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| 221 | G4ThreeVector electronDirection = ElectronAngularGenerator->GetPhotoElectronDirection(photonDirection,eKineticEnergy,gammaPolarization,shellId);
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| 222 |
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| 223 | // The electron is created ...
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| 224 | G4DynamicParticle* electron = new G4DynamicParticle (G4Electron::Electron(),
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| 225 | electronDirection,
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| 226 | eKineticEnergy);
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| 227 | electronVector.push_back(electron);
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| 228 | }
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| 229 | /*else
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| 230 | {
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| 231 | energyDeposit += eKineticEnergy;
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| 232 | }*/
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| 233 | }
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| 234 | else
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| 235 | {
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| 236 | bindingEnergy = photonEnergy;
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| 237 | }
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| 238 |
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| 239 | G4int nElectrons = electronVector.size();
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| 240 | size_t nTotPhotons = 0;
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| 241 | G4int nPhotons=0;
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| 242 | const G4ProductionCutsTable* theCoupleTable=
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| 243 | G4ProductionCutsTable::GetProductionCutsTable();
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| 244 |
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| 245 | size_t index = couple->GetIndex();
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| 246 | G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[index];
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| 247 | cutg = std::min(cutForLowEnergySecondaryPhotons,cutg);
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| 248 |
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| 249 | G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[index];
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| 250 | cute = std::min(cutForLowEnergySecondaryPhotons,cute);
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| 251 |
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| 252 | G4DynamicParticle* aPhoton;
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| 253 |
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| 254 | // Generation of fluorescence
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| 255 | // Data in EADL are available only for Z > 5
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| 256 | // Protection to avoid generating photons in the unphysical case of
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| 257 | // shell binding energy > photon energy
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| 258 | if (Z > 5 && (bindingEnergy > cutg || bindingEnergy > cute))
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| 259 | {
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| 260 | photonVector = deexcitationManager.GenerateParticles(Z,shellId);
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| 261 | nTotPhotons = photonVector->size();
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| 262 | for (size_t k=0; k<nTotPhotons; k++)
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| 263 | {
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| 264 | aPhoton = (*photonVector)[k];
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| 265 | if (aPhoton)
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| 266 | {
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| 267 | G4double itsCut = cutg;
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| 268 | if(aPhoton->GetDefinition() == G4Electron::Electron()) itsCut = cute;
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| 269 | G4double itsEnergy = aPhoton->GetKineticEnergy();
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| 270 |
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| 271 | if (itsEnergy > itsCut && itsEnergy <= bindingEnergy)
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| 272 | {
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| 273 | nPhotons++;
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| 274 | // Local energy deposit is given as the sum of the
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| 275 | // energies of incident photons minus the energies
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| 276 | // of the outcoming fluorescence photons
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| 277 | bindingEnergy -= itsEnergy;
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| 278 |
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| 279 | }
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| 280 | else
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| 281 | {
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| 282 | delete aPhoton;
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| 283 | (*photonVector)[k] = 0;
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| 284 | }
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| 285 | }
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| 286 | }
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| 287 | }
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| 288 |
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| 289 | energyDeposit += bindingEnergy;
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| 290 |
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| 291 | // Final state
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| 292 |
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| 293 | for (G4int l = 0; l<nElectrons; l++ )
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| 294 | {
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| 295 | aPhoton = electronVector[l];
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| 296 | if(aPhoton) {
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| 297 | fvect->push_back(aPhoton);
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| 298 | }
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| 299 | }
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| 300 | for ( size_t ll = 0; ll < nTotPhotons; ll++)
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| 301 | {
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| 302 | aPhoton = (*photonVector)[ll];
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| 303 | if(aPhoton) {
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| 304 | fvect->push_back(aPhoton);
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| 305 | }
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| 306 | }
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| 307 |
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| 308 | delete photonVector;
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| 309 |
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| 310 | if (energyDeposit < 0)
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| 311 | {
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| 312 | G4cout << "WARNING - "
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| 313 | << "G4LowEnergyPhotoElectric::PostStepDoIt - Negative energy deposit"
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| 314 | << G4endl;
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| 315 | energyDeposit = 0;
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| 316 | }
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| 317 |
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| 318 | // kill incident photon
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| 319 | fParticleChange->ProposeMomentumDirection( 0., 0., 0. );
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| 320 | fParticleChange->SetProposedKineticEnergy(0.);
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| 321 | fParticleChange->ProposeTrackStatus(fStopAndKill);
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| 322 | fParticleChange->ProposeLocalEnergyDeposit(energyDeposit);
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| 323 | }
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| 324 |
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| 325 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 326 |
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| 327 | void G4LivermorePhotoElectricModel::SetCutForLowEnSecPhotons(G4double cut)
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| 328 | {
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| 329 | cutForLowEnergySecondaryPhotons = cut;
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| 330 | deexcitationManager.SetCutForSecondaryPhotons(cut);
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| 331 | }
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| 332 |
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| 333 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 334 |
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| 335 | void G4LivermorePhotoElectricModel::SetCutForLowEnSecElectrons(G4double cut)
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| 336 | {
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| 337 | cutForLowEnergySecondaryElectrons = cut;
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| 338 | deexcitationManager.SetCutForAugerElectrons(cut);
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| 339 | }
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| 340 |
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| 341 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 342 |
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| 343 | void G4LivermorePhotoElectricModel::ActivateAuger(G4bool val)
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| 344 | {
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| 345 | deexcitationManager.ActivateAugerElectronProduction(val);
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| 346 | }
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| 347 |
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| 348 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 349 |
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| 350 | void G4LivermorePhotoElectricModel::SetAngularGenerator(G4VPhotoElectricAngularDistribution* distribution)
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| 351 | {
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| 352 | ElectronAngularGenerator = distribution;
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| 353 | ElectronAngularGenerator->PrintGeneratorInformation();
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| 354 | }
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| 355 |
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| 356 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 357 |
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| 358 | void G4LivermorePhotoElectricModel::SetAngularGenerator(const G4String& name)
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| 359 | {
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| 360 | if (name == "default")
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| 361 | {
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| 362 | delete ElectronAngularGenerator;
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| 363 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorSimple("GEANT4LowEnergySimpleGenerator");
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| 364 | generatorName = name;
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| 365 | }
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| 366 | else if (name == "standard")
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| 367 | {
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| 368 | delete ElectronAngularGenerator;
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| 369 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorSauterGavrila("GEANT4SauterGavrilaGenerator");
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| 370 | generatorName = name;
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| 371 | }
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| 372 | else if (name == "polarized")
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| 373 | {
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| 374 | delete ElectronAngularGenerator;
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| 375 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorPolarized("GEANT4LowEnergyPolarizedGenerator");
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| 376 | generatorName = name;
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| 377 | }
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| 378 | else
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| 379 | {
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| 380 | G4Exception("G4LowEnergyPhotoElectric::SetAngularGenerator - generator does not exist");
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| 381 | }
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| 382 |
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| 383 | ElectronAngularGenerator->PrintGeneratorInformation();
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| 384 | }
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| 385 |
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| 386 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 387 |
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| 388 | G4double G4LivermorePhotoElectricModel::GetMeanFreePath(const G4Track& track,
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| 389 | G4double, // previousStepSize
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| 390 | G4ForceCondition*)
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| 391 | {
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| 392 | const G4DynamicParticle* photon = track.GetDynamicParticle();
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| 393 | G4double energy = photon->GetKineticEnergy();
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| 394 | G4Material* material = track.GetMaterial();
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| 395 | // size_t materialIndex = material->GetIndex();
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| 396 |
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| 397 | G4double meanFreePath = DBL_MAX;
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| 398 |
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| 399 | // if (energy > highEnergyLimit)
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| 400 | // meanFreePath = meanFreePathTable->FindValue(highEnergyLimit,materialIndex);
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| 401 | // else if (energy < lowEnergyLimit) meanFreePath = DBL_MAX;
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| 402 | // else meanFreePath = meanFreePathTable->FindValue(energy,materialIndex);
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| 403 |
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| 404 | G4double cross = shellCrossSectionHandler->ValueForMaterial(material,energy);
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| 405 | if(cross > 0.0) meanFreePath = 1.0/cross;
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| 406 |
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| 407 | return meanFreePath;
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| 408 | }
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| 409 |
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