[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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[1315] | 26 | // $Id: G4LivermorePhotoElectricModel.cc,v 1.11 2010/03/26 09:32:50 pandola Exp $ |
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| 27 | // GEANT4 tag $Name: geant4-09-04-beta-cand-01 $ |
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[968] | 28 | // |
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[1055] | 29 | // |
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| 30 | // Author: Sebastien Inserti |
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| 31 | // 30 October 2008 |
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| 32 | // |
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| 33 | // History: |
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| 34 | // -------- |
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| 35 | // 15 Apr 2009 V Ivanchenko Cleanup initialisation and generation of secondaries: |
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| 36 | // - apply internal high-energy limit only in constructor |
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| 37 | // - do not apply low-energy limit (default is 0) |
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| 38 | // - remove GetMeanFreePath method and table |
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| 39 | // - simplify sampling of deexcitation by using cut in energy |
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| 40 | // - added protection against numerical problem in energy sampling |
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| 41 | // - use G4ElementSelector |
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[1192] | 42 | // 23 Oct 2009 L Pandola |
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| 43 | // - atomic deexcitation managed via G4VEmModel::DeexcitationFlag() is |
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| 44 | // set as "true" (default would be false) |
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[1315] | 45 | // 15 Mar 2010 L Pandola |
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| 46 | // - removed methods to set explicitely fluorescence cuts. |
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| 47 | // Main cuts from G4ProductionCutsTable are always used |
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| 48 | // |
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[968] | 49 | |
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| 50 | #include "G4LivermorePhotoElectricModel.hh" |
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| 51 | |
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| 52 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 53 | |
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| 54 | using namespace std; |
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| 55 | |
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| 56 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 57 | |
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| 58 | G4LivermorePhotoElectricModel::G4LivermorePhotoElectricModel(const G4ParticleDefinition*, |
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| 59 | const G4String& nam) |
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[1055] | 60 | :G4VEmModel(nam),isInitialised(false),meanFreePathTable(0), |
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| 61 | crossSectionHandler(0),shellCrossSectionHandler(0),ElectronAngularGenerator(0) |
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[968] | 62 | { |
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[1055] | 63 | lowEnergyLimit = 250 * eV; |
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[968] | 64 | highEnergyLimit = 100 * GeV; |
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[1055] | 65 | // SetLowEnergyLimit(lowEnergyLimit); |
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[968] | 66 | SetHighEnergyLimit(highEnergyLimit); |
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[1315] | 67 | |
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[968] | 68 | verboseLevel= 0; |
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| 69 | // Verbosity scale: |
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| 70 | // 0 = nothing |
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| 71 | // 1 = warning for energy non-conservation |
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| 72 | // 2 = details of energy budget |
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| 73 | // 3 = calculation of cross sections, file openings, sampling of atoms |
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| 74 | // 4 = entering in methods |
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[1315] | 75 | |
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| 76 | //Set atomic deexcitation by default |
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| 77 | SetDeexcitationFlag(true); |
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| 78 | ActivateAuger(false); |
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| 79 | |
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[1055] | 80 | if(verboseLevel>0) { |
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| 81 | G4cout << "Livermore PhotoElectric is constructed " << G4endl |
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| 82 | << "Energy range: " |
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| 83 | << lowEnergyLimit / eV << " eV - " |
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| 84 | << highEnergyLimit / GeV << " GeV" |
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| 85 | << G4endl; |
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| 86 | } |
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[968] | 87 | } |
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| 88 | |
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| 89 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 90 | |
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| 91 | G4LivermorePhotoElectricModel::~G4LivermorePhotoElectricModel() |
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| 92 | { |
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[1055] | 93 | if (crossSectionHandler) delete crossSectionHandler; |
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| 94 | if (shellCrossSectionHandler) delete shellCrossSectionHandler; |
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| 95 | if (ElectronAngularGenerator) delete ElectronAngularGenerator; |
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[968] | 96 | } |
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| 97 | |
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| 98 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 99 | |
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[1055] | 100 | void |
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| 101 | G4LivermorePhotoElectricModel::Initialise(const G4ParticleDefinition*, |
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| 102 | const G4DataVector&) |
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[968] | 103 | { |
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| 104 | if (verboseLevel > 3) |
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| 105 | G4cout << "Calling G4LivermorePhotoElectricModel::Initialise()" << G4endl; |
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| 106 | |
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[1055] | 107 | if (crossSectionHandler) |
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[968] | 108 | { |
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[1055] | 109 | crossSectionHandler->Clear(); |
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| 110 | delete crossSectionHandler; |
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[968] | 111 | } |
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[1055] | 112 | |
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| 113 | if (shellCrossSectionHandler) |
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[968] | 114 | { |
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[1055] | 115 | shellCrossSectionHandler->Clear(); |
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| 116 | delete shellCrossSectionHandler; |
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[968] | 117 | } |
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[1055] | 118 | |
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[968] | 119 | // Read data tables for all materials |
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| 120 | |
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| 121 | crossSectionHandler = new G4CrossSectionHandler(); |
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| 122 | crossSectionHandler->Clear(); |
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| 123 | G4String crossSectionFile = "phot/pe-cs-"; |
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| 124 | crossSectionHandler->LoadData(crossSectionFile); |
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| 125 | |
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| 126 | shellCrossSectionHandler = new G4CrossSectionHandler(); |
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| 127 | shellCrossSectionHandler->Clear(); |
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| 128 | G4String shellCrossSectionFile = "phot/pe-ss-cs-"; |
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| 129 | shellCrossSectionHandler->LoadShellData(shellCrossSectionFile); |
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| 130 | |
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[1315] | 131 | // default generator |
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[1055] | 132 | ElectronAngularGenerator = |
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| 133 | new G4PhotoElectricAngularGeneratorSauterGavrila("GEANTSauterGavrilaGenerator"); |
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[968] | 134 | |
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[1055] | 135 | // |
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[968] | 136 | if (verboseLevel > 2) |
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| 137 | G4cout << "Loaded cross section files for Livermore PhotoElectric model" << G4endl; |
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| 138 | |
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[1055] | 139 | // InitialiseElementSelectors(particle,cuts); |
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[968] | 140 | |
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[1055] | 141 | if (verboseLevel > 0) { |
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| 142 | G4cout << "Livermore PhotoElectric model is initialized " << G4endl |
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| 143 | << "Energy range: " |
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| 144 | << LowEnergyLimit() / eV << " eV - " |
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| 145 | << HighEnergyLimit() / GeV << " GeV" |
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| 146 | << G4endl; |
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| 147 | } |
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| 148 | |
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[968] | 149 | if(isInitialised) return; |
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[1055] | 150 | fParticleChange = GetParticleChangeForGamma(); |
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[968] | 151 | isInitialised = true; |
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| 152 | } |
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| 153 | |
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| 154 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 155 | |
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| 156 | G4double G4LivermorePhotoElectricModel::ComputeCrossSectionPerAtom( |
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| 157 | const G4ParticleDefinition*, |
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| 158 | G4double GammaEnergy, |
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| 159 | G4double Z, G4double, |
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| 160 | G4double, G4double) |
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| 161 | { |
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| 162 | if (verboseLevel > 3) |
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[1055] | 163 | G4cout << "Calling ComputeCrossSectionPerAtom() of G4LivermorePhotoElectricModel" |
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| 164 | << G4endl; |
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[968] | 165 | |
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[1055] | 166 | if (GammaEnergy < lowEnergyLimit || GammaEnergy > highEnergyLimit) |
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| 167 | return 0; |
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| 168 | |
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[968] | 169 | G4double cs = crossSectionHandler->FindValue(G4int(Z), GammaEnergy); |
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| 170 | return cs; |
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| 171 | } |
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| 172 | |
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| 173 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 174 | |
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[1055] | 175 | void |
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| 176 | G4LivermorePhotoElectricModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect, |
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| 177 | const G4MaterialCutsCouple* couple, |
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| 178 | const G4DynamicParticle* aDynamicGamma, |
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| 179 | G4double, |
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| 180 | G4double) |
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[968] | 181 | { |
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| 182 | |
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| 183 | // Fluorescence generated according to: |
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| 184 | // J. Stepanek ,"A program to determine the radiation spectra due to a single atomic |
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| 185 | // subshell ionisation by a particle or due to deexcitation or decay of radionuclides", |
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| 186 | // Comp. Phys. Comm. 1206 pp 1-1-9 (1997) |
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| 187 | |
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| 188 | if (verboseLevel > 3) |
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| 189 | G4cout << "Calling SampleSecondaries() of G4LivermorePhotoElectricModel" << G4endl; |
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| 190 | |
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| 191 | G4double photonEnergy = aDynamicGamma->GetKineticEnergy(); |
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| 192 | |
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[1055] | 193 | // kill incident photon |
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| 194 | fParticleChange->SetProposedKineticEnergy(0.); |
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| 195 | fParticleChange->ProposeTrackStatus(fStopAndKill); |
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| 196 | |
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| 197 | // low-energy gamma is absorpted by this process |
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[968] | 198 | if (photonEnergy <= lowEnergyLimit) |
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| 199 | { |
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| 200 | fParticleChange->ProposeLocalEnergyDeposit(photonEnergy); |
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[1055] | 201 | return; |
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[968] | 202 | } |
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| 203 | |
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[1055] | 204 | // Returns the normalized direction of the momentum |
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| 205 | G4ThreeVector photonDirection = aDynamicGamma->GetMomentumDirection(); |
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[968] | 206 | |
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| 207 | // Select randomly one element in the current material |
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[1055] | 208 | // G4int Z = crossSectionHandler->SelectRandomAtom(couple,photonEnergy); |
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| 209 | const G4ParticleDefinition* particle = aDynamicGamma->GetDefinition(); |
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| 210 | const G4Element* elm = SelectRandomAtom(couple->GetMaterial(),particle,photonEnergy); |
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| 211 | G4int Z = (G4int)elm->GetZ(); |
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[968] | 212 | |
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| 213 | // Select the ionised shell in the current atom according to shell cross sections |
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| 214 | size_t shellIndex = shellCrossSectionHandler->SelectRandomShell(Z,photonEnergy); |
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| 215 | |
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| 216 | // Retrieve the corresponding identifier and binding energy of the selected shell |
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| 217 | const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); |
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| 218 | const G4AtomicShell* shell = transitionManager->Shell(Z,shellIndex); |
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| 219 | G4double bindingEnergy = shell->BindingEnergy(); |
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| 220 | G4int shellId = shell->ShellId(); |
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| 221 | |
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| 222 | // Primary outcoming electron |
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| 223 | G4double eKineticEnergy = photonEnergy - bindingEnergy; |
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| 224 | |
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| 225 | // There may be cases where the binding energy of the selected shell is > photon energy |
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| 226 | // In such cases do not generate secondaries |
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| 227 | if (eKineticEnergy > 0.) |
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| 228 | { |
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[1055] | 229 | // Calculate direction of the photoelectron |
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| 230 | G4ThreeVector gammaPolarization = aDynamicGamma->GetPolarization(); |
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| 231 | G4ThreeVector electronDirection = |
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| 232 | ElectronAngularGenerator->GetPhotoElectronDirection(photonDirection, |
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| 233 | eKineticEnergy, |
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| 234 | gammaPolarization, |
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| 235 | shellId); |
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[968] | 236 | |
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[1055] | 237 | // The electron is created ... |
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| 238 | G4DynamicParticle* electron = new G4DynamicParticle (G4Electron::Electron(), |
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| 239 | electronDirection, |
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| 240 | eKineticEnergy); |
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| 241 | fvect->push_back(electron); |
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[968] | 242 | } |
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| 243 | else |
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| 244 | { |
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| 245 | bindingEnergy = photonEnergy; |
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| 246 | } |
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| 247 | |
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[1055] | 248 | // deexcitation |
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| 249 | if(DeexcitationFlag() && Z > 5) { |
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[968] | 250 | |
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[1055] | 251 | const G4ProductionCutsTable* theCoupleTable= |
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| 252 | G4ProductionCutsTable::GetProductionCutsTable(); |
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[968] | 253 | |
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[1055] | 254 | size_t index = couple->GetIndex(); |
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| 255 | G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[index]; |
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| 256 | G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[index]; |
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[968] | 257 | |
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[1055] | 258 | // Generation of fluorescence |
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| 259 | // Data in EADL are available only for Z > 5 |
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| 260 | // Protection to avoid generating photons in the unphysical case of |
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| 261 | // shell binding energy > photon energy |
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| 262 | if (bindingEnergy > cutg || bindingEnergy > cute) |
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| 263 | { |
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| 264 | G4DynamicParticle* aPhoton; |
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| 265 | deexcitationManager.SetCutForSecondaryPhotons(cutg); |
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| 266 | deexcitationManager.SetCutForAugerElectrons(cute); |
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| 267 | |
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| 268 | std::vector<G4DynamicParticle*>* photonVector = |
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| 269 | deexcitationManager.GenerateParticles(Z,shellId); |
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| 270 | size_t nTotPhotons = photonVector->size(); |
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| 271 | for (size_t k=0; k<nTotPhotons; k++) |
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| 272 | { |
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| 273 | aPhoton = (*photonVector)[k]; |
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| 274 | if (aPhoton) |
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| 275 | { |
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| 276 | G4double itsEnergy = aPhoton->GetKineticEnergy(); |
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| 277 | if (itsEnergy <= bindingEnergy) |
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| 278 | { |
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| 279 | // Local energy deposit is given as the sum of the |
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| 280 | // energies of incident photons minus the energies |
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| 281 | // of the outcoming fluorescence photons |
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| 282 | bindingEnergy -= itsEnergy; |
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| 283 | fvect->push_back(aPhoton); |
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| 284 | } |
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| 285 | else |
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| 286 | { |
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| 287 | // abnormal case of energy non-conservation |
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| 288 | delete aPhoton; |
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| 289 | (*photonVector)[k] = 0; |
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| 290 | } |
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| 291 | } |
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| 292 | } |
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| 293 | delete photonVector; |
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[968] | 294 | } |
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[1055] | 295 | } |
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| 296 | // excitation energy left |
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| 297 | fParticleChange->ProposeLocalEnergyDeposit(bindingEnergy); |
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[968] | 298 | } |
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| 299 | |
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| 300 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 301 | |
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[1315] | 302 | void G4LivermorePhotoElectricModel::ActivateAuger(G4bool augerbool) |
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[968] | 303 | { |
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[1315] | 304 | if (!DeexcitationFlag() && augerbool) |
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| 305 | { |
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| 306 | G4cout << "WARNING - G4PenelopePhotoElectricModel" << G4endl; |
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| 307 | G4cout << "The use of the Atomic Deexcitation Manager is set to false " << G4endl; |
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| 308 | G4cout << "Therefore, Auger electrons will be not generated anyway" << G4endl; |
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| 309 | } |
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| 310 | deexcitationManager.ActivateAugerElectronProduction(augerbool); |
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| 311 | if (verboseLevel > 1) |
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| 312 | G4cout << "Auger production set to " << augerbool << G4endl; |
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[968] | 313 | } |
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| 314 | |
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| 315 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 316 | |
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[1055] | 317 | void |
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| 318 | G4LivermorePhotoElectricModel::SetAngularGenerator(G4VPhotoElectricAngularDistribution* dist) |
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[968] | 319 | { |
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[1055] | 320 | ElectronAngularGenerator = dist; |
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[968] | 321 | ElectronAngularGenerator->PrintGeneratorInformation(); |
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| 322 | } |
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| 323 | |
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| 324 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 325 | |
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| 326 | void G4LivermorePhotoElectricModel::SetAngularGenerator(const G4String& name) |
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| 327 | { |
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| 328 | if (name == "default") |
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| 329 | { |
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| 330 | delete ElectronAngularGenerator; |
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[1055] | 331 | ElectronAngularGenerator = |
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| 332 | new G4PhotoElectricAngularGeneratorSimple("GEANT4LowEnergySimpleGenerator"); |
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[968] | 333 | generatorName = name; |
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| 334 | } |
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| 335 | else if (name == "standard") |
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| 336 | { |
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| 337 | delete ElectronAngularGenerator; |
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[1055] | 338 | ElectronAngularGenerator = |
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| 339 | new G4PhotoElectricAngularGeneratorSauterGavrila("GEANT4SauterGavrilaGenerator"); |
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[968] | 340 | generatorName = name; |
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| 341 | } |
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| 342 | else if (name == "polarized") |
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| 343 | { |
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| 344 | delete ElectronAngularGenerator; |
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[1055] | 345 | ElectronAngularGenerator = |
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| 346 | new G4PhotoElectricAngularGeneratorPolarized("GEANT4LowEnergyPolarizedGenerator"); |
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[968] | 347 | generatorName = name; |
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| 348 | } |
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| 349 | else |
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| 350 | { |
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| 351 | G4Exception("G4LowEnergyPhotoElectric::SetAngularGenerator - generator does not exist"); |
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| 352 | } |
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| 353 | |
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| 354 | ElectronAngularGenerator->PrintGeneratorInformation(); |
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| 355 | } |
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| 356 | |
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