[1197] | 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 | |
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| 27 | #include "G4LivermorePolarizedPhotoElectricModel.hh" |
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| 28 | |
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| 29 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 30 | |
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| 31 | using namespace std; |
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| 32 | |
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| 33 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 34 | |
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| 35 | G4LivermorePolarizedPhotoElectricModel::G4LivermorePolarizedPhotoElectricModel(const G4ParticleDefinition*, |
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| 36 | const G4String& nam) |
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| 37 | :G4VEmModel(nam),isInitialised(false),meanFreePathTable(0),crossSectionHandler(0), shellCrossSectionHandler(0) |
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| 38 | { |
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| 39 | lowEnergyLimit = 250 * eV; // SI - Could be 10 eV ? |
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| 40 | highEnergyLimit = 100 * GeV; |
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| 41 | SetLowEnergyLimit(lowEnergyLimit); |
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| 42 | SetHighEnergyLimit(highEnergyLimit); |
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| 43 | |
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| 44 | verboseLevel= 0; |
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| 45 | // Verbosity scale: |
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| 46 | // 0 = nothing |
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| 47 | // 1 = warning for energy non-conservation |
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| 48 | // 2 = details of energy budget |
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| 49 | // 3 = calculation of cross sections, file openings, sampling of atoms |
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| 50 | // 4 = entering in methods |
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| 51 | |
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| 52 | G4cout << "Livermore Polarized PhotoElectric is constructed " << G4endl |
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| 53 | << "Energy range: " |
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| 54 | << lowEnergyLimit / keV << " keV - " |
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| 55 | << highEnergyLimit / GeV << " GeV" |
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| 56 | << G4endl; |
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| 57 | |
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| 58 | } |
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| 59 | |
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| 60 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 61 | |
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| 62 | G4LivermorePolarizedPhotoElectricModel::~G4LivermorePolarizedPhotoElectricModel() |
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| 63 | { |
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| 64 | if (meanFreePathTable) delete meanFreePathTable; |
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| 65 | if (crossSectionHandler) delete crossSectionHandler; |
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| 66 | if (shellCrossSectionHandler) delete shellCrossSectionHandler; |
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| 67 | } |
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| 68 | |
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| 69 | |
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| 70 | |
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| 71 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 72 | |
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| 73 | void G4LivermorePolarizedPhotoElectricModel::Initialise(const G4ParticleDefinition* particle, |
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| 74 | const G4DataVector& cuts) |
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| 75 | { |
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| 76 | if (verboseLevel > 3) |
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| 77 | G4cout << "Calling G4LivermorePolarizedPhotoElectricModel::Initialise()" << G4endl; |
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| 78 | |
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| 79 | if (crossSectionHandler) |
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| 80 | { |
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| 81 | crossSectionHandler->Clear(); |
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| 82 | delete crossSectionHandler; |
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| 83 | } |
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| 84 | |
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| 85 | if (shellCrossSectionHandler) |
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| 86 | { |
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| 87 | shellCrossSectionHandler->Clear(); |
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| 88 | delete shellCrossSectionHandler; |
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| 89 | } |
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| 90 | |
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| 91 | |
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| 92 | // Energy limits |
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| 93 | |
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| 94 | if (LowEnergyLimit() < lowEnergyLimit) |
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| 95 | { |
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| 96 | G4cout << "G4LivermorePolarizedPhotoElectricModel: low energy limit increased from " << |
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| 97 | LowEnergyLimit()/eV << " eV to " << lowEnergyLimit << " eV" << G4endl; |
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| 98 | SetLowEnergyLimit(lowEnergyLimit); |
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| 99 | } |
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| 100 | |
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| 101 | if (HighEnergyLimit() > highEnergyLimit) |
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| 102 | { |
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| 103 | G4cout << "G4LivermorePolarizedPhotoElectricModel: high energy limit decreased from " << |
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| 104 | HighEnergyLimit()/GeV << " GeV to " << highEnergyLimit << " GeV" << G4endl; |
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| 105 | SetHighEnergyLimit(highEnergyLimit); |
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| 106 | } |
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| 107 | |
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| 108 | // Reading of data files - all materials are read |
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| 109 | |
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| 110 | crossSectionHandler = new G4CrossSectionHandler; |
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| 111 | crossSectionHandler->Clear(); |
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| 112 | G4String crossSectionFile = "phot/pe-cs-"; |
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| 113 | crossSectionHandler->LoadData(crossSectionFile); |
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| 114 | |
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| 115 | meanFreePathTable = 0; |
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| 116 | meanFreePathTable = crossSectionHandler->BuildMeanFreePathForMaterials(); |
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| 117 | |
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| 118 | shellCrossSectionHandler = new G4CrossSectionHandler(); |
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| 119 | shellCrossSectionHandler->Clear(); |
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| 120 | G4String shellCrossSectionFile = "phot/pe-ss-cs-"; |
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| 121 | shellCrossSectionHandler->LoadShellData(shellCrossSectionFile); |
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| 122 | |
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| 123 | |
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| 124 | // |
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| 125 | if (verboseLevel > 2) |
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| 126 | G4cout << "Loaded cross section files for Livermore Polarized PhotoElectric model" << G4endl; |
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| 127 | |
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| 128 | InitialiseElementSelectors(particle,cuts); |
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| 129 | |
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| 130 | G4cout << "Livermore Polarized PhotoElectric model is initialized " << G4endl |
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| 131 | << "Energy range: " |
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| 132 | << LowEnergyLimit() / keV << " keV - " |
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| 133 | << HighEnergyLimit() / GeV << " GeV" |
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| 134 | << G4endl; |
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| 135 | |
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| 136 | // |
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| 137 | |
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| 138 | if(isInitialised) return; |
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| 139 | |
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| 140 | if(pParticleChange) |
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| 141 | fParticleChange = reinterpret_cast<G4ParticleChangeForGamma*>(pParticleChange); |
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| 142 | else |
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| 143 | fParticleChange = new G4ParticleChangeForGamma(); |
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| 144 | |
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| 145 | isInitialised = true; |
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| 146 | } |
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| 147 | |
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| 148 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 149 | |
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| 150 | G4double G4LivermorePolarizedPhotoElectricModel::ComputeCrossSectionPerAtom( |
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| 151 | const G4ParticleDefinition*, |
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| 152 | G4double GammaEnergy, |
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| 153 | G4double Z, G4double, |
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| 154 | G4double, G4double) |
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| 155 | { |
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| 156 | if (verboseLevel > 3) |
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| 157 | G4cout << "Calling ComputeCrossSectionPerAtom() of G4LivermorePolarizedPhotoElectricModel" << G4endl; |
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| 158 | |
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| 159 | G4double cs = crossSectionHandler->FindValue(G4int(Z), GammaEnergy); |
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| 160 | return cs; |
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| 161 | } |
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| 162 | |
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| 163 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 164 | |
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| 165 | void G4LivermorePolarizedPhotoElectricModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect, |
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| 166 | const G4MaterialCutsCouple* couple, |
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| 167 | const G4DynamicParticle* aDynamicGamma, |
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| 168 | G4double, |
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| 169 | G4double) |
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| 170 | { |
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| 171 | |
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| 172 | // Fluorescence generated according to: |
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| 173 | // J. Stepanek ,"A program to determine the radiation spectra due to a single atomic |
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| 174 | // subshell ionisation by a particle or due to deexcitation or decay of radionuclides", |
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| 175 | // Comp. Phys. Comm. 1206 pp 1-1-9 (1997) |
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| 176 | |
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| 177 | if (verboseLevel > 3) |
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| 178 | G4cout << "Calling SampleSecondaries() of G4LivermorePolarizedPhotoElectricModel" << G4endl; |
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| 179 | |
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| 180 | G4double photonEnergy = aDynamicGamma->GetKineticEnergy(); |
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| 181 | // Within energy limit? |
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| 182 | |
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| 183 | if(photonEnergy <= lowEnergyLimit) |
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| 184 | { |
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| 185 | fParticleChange->ProposeTrackStatus(fStopAndKill); |
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| 186 | fParticleChange->SetProposedKineticEnergy(0.); |
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| 187 | fParticleChange->ProposeLocalEnergyDeposit(photonEnergy); |
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| 188 | return; |
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| 189 | } |
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| 190 | |
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| 191 | |
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| 192 | G4ThreeVector gammaPolarization0 = aDynamicGamma->GetPolarization(); |
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| 193 | |
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| 194 | // Protection: a polarisation parallel to the |
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| 195 | // direction causes problems; |
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| 196 | // in that case find a random polarization |
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| 197 | |
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| 198 | G4ThreeVector photonDirection = aDynamicGamma->GetMomentumDirection(); |
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| 199 | |
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| 200 | // Make sure that the polarization vector is perpendicular to the |
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| 201 | // gamma direction. If not |
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| 202 | |
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| 203 | if(!(gammaPolarization0.isOrthogonal(photonDirection, 1e-6))||(gammaPolarization0.mag()==0)) |
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| 204 | { // only for testing now |
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| 205 | gammaPolarization0 = GetRandomPolarization(photonDirection); |
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| 206 | } |
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| 207 | else |
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| 208 | { |
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| 209 | if ( gammaPolarization0.howOrthogonal(photonDirection) != 0) |
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| 210 | { |
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| 211 | gammaPolarization0 = GetPerpendicularPolarization(photonDirection, gammaPolarization0); |
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| 212 | } |
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| 213 | } |
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| 214 | |
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| 215 | // End of Protection |
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| 216 | |
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| 217 | // G4double E0_m = photonEnergy / electron_mass_c2 ; |
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| 218 | |
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| 219 | // Select randomly one element in the current material |
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| 220 | |
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| 221 | G4int Z = crossSectionHandler->SelectRandomAtom(couple,photonEnergy); |
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| 222 | |
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| 223 | // Select the ionised shell in the current atom according to shell cross sections |
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| 224 | |
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| 225 | size_t shellIndex = shellCrossSectionHandler->SelectRandomShell(Z,photonEnergy); |
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| 226 | |
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| 227 | const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance(); |
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| 228 | const G4AtomicShell* shell = transitionManager->Shell(Z,shellIndex); |
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| 229 | G4double bindingEnergy = shell->BindingEnergy(); |
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| 230 | G4int shellId = shell->ShellId(); |
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| 231 | |
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| 232 | // Create lists of pointers to DynamicParticles (photons and electrons) |
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| 233 | // (Is the electron vector necessary? To be checked) |
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| 234 | std::vector<G4DynamicParticle*>* photonVector = 0; |
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| 235 | std::vector<G4DynamicParticle*> electronVector; |
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| 236 | |
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| 237 | G4double energyDeposit = 0.0; |
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| 238 | |
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| 239 | // Primary outgoing electron |
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| 240 | |
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| 241 | G4double eKineticEnergy = photonEnergy - bindingEnergy; |
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| 242 | |
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| 243 | |
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| 244 | if (eKineticEnergy > 0.) |
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| 245 | { |
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| 246 | |
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| 247 | G4double costheta = SetCosTheta(eKineticEnergy); |
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| 248 | G4double sintheta = sqrt(1. - costheta*costheta); |
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| 249 | G4double phi = SetPhi(photonEnergy,eKineticEnergy,costheta); |
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| 250 | G4double dirX = sintheta*cos(phi); |
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| 251 | G4double dirY = sintheta*sin(phi); |
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| 252 | G4double dirZ = costheta; |
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| 253 | G4ThreeVector electronDirection(dirX, dirY, dirZ); |
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| 254 | SystemOfRefChange(photonDirection, electronDirection, gammaPolarization0); |
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| 255 | G4DynamicParticle* electron = new G4DynamicParticle (G4Electron::Electron(), |
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| 256 | electronDirection, |
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| 257 | eKineticEnergy); |
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| 258 | electronVector.push_back(electron); |
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| 259 | } |
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| 260 | else |
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| 261 | { |
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| 262 | bindingEnergy = photonEnergy; |
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| 263 | } |
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| 264 | |
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| 265 | |
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| 266 | G4int nElectrons = electronVector.size(); |
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| 267 | size_t nTotPhotons = 0; |
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| 268 | G4int nPhotons=0; |
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| 269 | |
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| 270 | const G4ProductionCutsTable* theCoupleTable= |
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| 271 | G4ProductionCutsTable::GetProductionCutsTable(); |
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| 272 | size_t index = couple->GetIndex(); |
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| 273 | G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[index]; |
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| 274 | cutg = std::min(cutForLowEnergySecondaryPhotons,cutg); |
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| 275 | |
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| 276 | G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[index]; |
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| 277 | cute = std::min(cutForLowEnergySecondaryPhotons,cute); |
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| 278 | |
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| 279 | G4DynamicParticle* aPhoton; |
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| 280 | |
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| 281 | // Generation of fluorescence |
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| 282 | // Data in EADL are available only for Z > 5 |
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| 283 | // Protection to avoid generating photons in the unphysical case of |
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| 284 | // shell binding energy > photon energy |
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| 285 | if (Z > 5 && (bindingEnergy > cutg || bindingEnergy > cute)) |
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| 286 | { |
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| 287 | photonVector = deexcitationManager.GenerateParticles(Z,shellId); |
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| 288 | nTotPhotons = photonVector->size(); |
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| 289 | for (size_t k=0; k<nTotPhotons; k++) |
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| 290 | { |
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| 291 | aPhoton = (*photonVector)[k]; |
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| 292 | if (aPhoton) |
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| 293 | { |
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| 294 | G4double itsCut = cutg; |
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| 295 | if(aPhoton->GetDefinition() == G4Electron::Electron()) itsCut = cute; |
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| 296 | |
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| 297 | G4double itsEnergy = aPhoton->GetKineticEnergy(); |
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| 298 | |
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| 299 | if (itsEnergy > itsCut && itsEnergy <= bindingEnergy) |
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| 300 | { |
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| 301 | nPhotons++; |
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| 302 | // Local energy deposit is given as the sum of the |
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| 303 | // energies of incident photons minus the energies |
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| 304 | // of the outcoming fluorescence photons |
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| 305 | bindingEnergy -= itsEnergy; |
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| 306 | |
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| 307 | } |
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| 308 | else |
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| 309 | { |
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| 310 | delete aPhoton; |
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| 311 | (*photonVector)[k] = 0; |
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| 312 | } |
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| 313 | } |
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| 314 | } |
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| 315 | } |
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| 316 | energyDeposit += bindingEnergy; |
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| 317 | // Final state |
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| 318 | |
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| 319 | for (G4int l = 0; l<nElectrons; l++ ) |
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| 320 | { |
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| 321 | aPhoton = electronVector[l]; |
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| 322 | if(aPhoton) { |
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| 323 | fvect->push_back(aPhoton); |
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| 324 | } |
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| 325 | } |
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| 326 | for ( size_t ll = 0; ll < nTotPhotons; ll++) |
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| 327 | { |
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| 328 | aPhoton = (*photonVector)[ll]; |
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| 329 | if(aPhoton) { |
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| 330 | fvect->push_back(aPhoton); |
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| 331 | } |
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| 332 | } |
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| 333 | |
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| 334 | delete photonVector; |
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| 335 | |
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| 336 | if (energyDeposit < 0) |
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| 337 | { |
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| 338 | G4cout << "WARNING - " |
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| 339 | << "G4LowEnergyPhotoElectric::PostStepDoIt - Negative energy deposit" |
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| 340 | << G4endl; |
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| 341 | energyDeposit = 0; |
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| 342 | } |
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| 343 | |
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| 344 | // kill incident photon |
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| 345 | fParticleChange->ProposeMomentumDirection( 0., 0., 0. ); |
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| 346 | fParticleChange->SetProposedKineticEnergy(0.); |
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| 347 | fParticleChange->ProposeTrackStatus(fStopAndKill); |
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| 348 | fParticleChange->ProposeLocalEnergyDeposit(energyDeposit); |
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| 349 | |
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| 350 | } |
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| 351 | |
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| 352 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 353 | |
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| 354 | void G4LivermorePolarizedPhotoElectricModel::SetCutForLowEnSecPhotons(G4double cut) |
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| 355 | { |
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| 356 | cutForLowEnergySecondaryPhotons = cut; |
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| 357 | deexcitationManager.SetCutForSecondaryPhotons(cut); |
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| 358 | } |
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| 359 | |
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| 360 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 361 | |
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| 362 | void G4LivermorePolarizedPhotoElectricModel::SetCutForLowEnSecElectrons(G4double cut) |
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| 363 | { |
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| 364 | cutForLowEnergySecondaryElectrons = cut; |
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| 365 | deexcitationManager.SetCutForAugerElectrons(cut); |
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| 366 | } |
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| 367 | |
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| 368 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 369 | |
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| 370 | void G4LivermorePolarizedPhotoElectricModel::ActivateAuger(G4bool val) |
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| 371 | { |
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| 372 | deexcitationManager.ActivateAugerElectronProduction(val); |
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| 373 | } |
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| 374 | |
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| 375 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 376 | |
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| 377 | |
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| 378 | G4double G4LivermorePolarizedPhotoElectricModel::SetCosTheta(G4double energyE) |
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| 379 | |
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| 380 | { |
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| 381 | G4double rand1,rand2,onemcost,greject; |
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| 382 | G4double masarep = 510.99906*keV; |
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| 383 | |
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| 384 | G4double gamma = 1. + energyE/masarep; |
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| 385 | G4double gamma2 = gamma*gamma; |
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| 386 | |
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| 387 | G4double beta = sqrt((gamma2 - 1.)/gamma2); |
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| 388 | |
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| 389 | G4double alfa = 1./beta - 1.; |
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| 390 | |
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| 391 | G4double g1 = 0.5*beta*gamma*(gamma-1.)*(gamma-2.); |
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| 392 | |
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| 393 | G4double alfap2 = alfa+2.; |
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| 394 | |
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| 395 | G4double grejectmax = 2.*(g1+1./alfa); |
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| 396 | |
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| 397 | do |
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| 398 | { |
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| 399 | rand1 = G4UniformRand(); |
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| 400 | onemcost = 2.*alfa*(2.*rand1 + alfap2 * sqrt(rand1))/ |
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| 401 | (alfap2*alfap2 - 4.*rand1); |
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| 402 | greject = (2. - onemcost)*(g1+1./(alfa+onemcost)); |
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| 403 | rand2 = G4UniformRand(); |
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| 404 | } |
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| 405 | while (rand2*grejectmax > greject); |
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| 406 | G4double cosTheta = 1. - onemcost; |
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| 407 | return cosTheta; |
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| 408 | } |
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| 409 | |
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| 410 | |
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| 411 | |
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| 412 | G4double G4LivermorePolarizedPhotoElectricModel::SetPhi(G4double Ph_energy, |
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| 413 | G4double E_energy, |
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| 414 | G4double costheta) |
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| 415 | { |
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| 416 | G4double epsilon = E_energy/electron_mass_c2; |
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| 417 | G4double k = Ph_energy/electron_mass_c2; |
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| 418 | G4double gamma = 1. + epsilon; |
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| 419 | G4double gamma2 = gamma*gamma; |
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| 420 | G4double beta = sqrt((gamma2 - 1.)/gamma2); |
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| 421 | |
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| 422 | G4double d = (2./(k*gamma*(1-beta*costheta))-1)*(1/k); |
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| 423 | |
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| 424 | G4double norm_factor = 1 +2*d; |
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| 425 | |
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| 426 | G4double rnd1; |
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| 427 | G4double rnd2; |
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| 428 | G4double phi, phiprob; |
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| 429 | |
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| 430 | do |
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| 431 | { |
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| 432 | rnd1 =G4UniformRand(); |
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| 433 | rnd2 =G4UniformRand(); |
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| 434 | phi = rnd1*twopi; |
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| 435 | phiprob = 1 +2*d*cos(phi)*cos(phi); |
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| 436 | } |
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| 437 | while (rnd2*norm_factor > phiprob); |
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| 438 | return phi; |
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| 439 | } |
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| 440 | |
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| 441 | |
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| 442 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 443 | |
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| 444 | G4ThreeVector G4LivermorePolarizedPhotoElectricModel::SetPerpendicularVector(G4ThreeVector& a) |
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| 445 | { |
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| 446 | G4double dx = a.x(); |
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| 447 | G4double dy = a.y(); |
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| 448 | G4double dz = a.z(); |
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| 449 | G4double x = dx < 0.0 ? -dx : dx; |
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| 450 | G4double y = dy < 0.0 ? -dy : dy; |
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| 451 | G4double z = dz < 0.0 ? -dz : dz; |
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| 452 | if (x < y) { |
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| 453 | return x < z ? G4ThreeVector(-dy,dx,0) : G4ThreeVector(0,-dz,dy); |
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| 454 | }else{ |
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| 455 | return y < z ? G4ThreeVector(dz,0,-dx) : G4ThreeVector(-dy,dx,0); |
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| 456 | } |
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| 457 | } |
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| 458 | |
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| 459 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 460 | |
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| 461 | G4ThreeVector G4LivermorePolarizedPhotoElectricModel::GetRandomPolarization(G4ThreeVector& direction0) |
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| 462 | { |
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| 463 | G4ThreeVector d0 = direction0.unit(); |
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| 464 | G4ThreeVector a1 = SetPerpendicularVector(d0); //different orthogonal |
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| 465 | G4ThreeVector a0 = a1.unit(); // unit vector |
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| 466 | |
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| 467 | G4double rand1 = G4UniformRand(); |
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| 468 | |
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| 469 | G4double angle = twopi*rand1; // random polar angle |
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| 470 | G4ThreeVector b0 = d0.cross(a0); // cross product |
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| 471 | |
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| 472 | G4ThreeVector c; |
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| 473 | |
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| 474 | c.setX(std::cos(angle)*(a0.x())+std::sin(angle)*b0.x()); |
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| 475 | c.setY(std::cos(angle)*(a0.y())+std::sin(angle)*b0.y()); |
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| 476 | c.setZ(std::cos(angle)*(a0.z())+std::sin(angle)*b0.z()); |
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| 477 | |
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| 478 | G4ThreeVector c0 = c.unit(); |
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| 479 | |
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| 480 | return c0; |
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| 481 | |
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| 482 | } |
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| 483 | |
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| 484 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 485 | |
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| 486 | G4ThreeVector G4LivermorePolarizedPhotoElectricModel::GetPerpendicularPolarization |
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| 487 | (const G4ThreeVector& gammaDirection, const G4ThreeVector& gammaPolarization) const |
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| 488 | { |
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| 489 | |
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| 490 | // |
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| 491 | // The polarization of a photon is always perpendicular to its momentum direction. |
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| 492 | // Therefore this function removes those vector component of gammaPolarization, which |
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| 493 | // points in direction of gammaDirection |
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| 494 | // |
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| 495 | // Mathematically we search the projection of the vector a on the plane E, where n is the |
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| 496 | // plains normal vector. |
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| 497 | // The basic equation can be found in each geometry book (e.g. Bronstein): |
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| 498 | // p = a - (a o n)/(n o n)*n |
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| 499 | |
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| 500 | return gammaPolarization - gammaPolarization.dot(gammaDirection)/gammaDirection.dot(gammaDirection) * gammaDirection; |
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| 501 | } |
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| 502 | |
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| 503 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 504 | |
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| 505 | |
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| 506 | void G4LivermorePolarizedPhotoElectricModel::SystemOfRefChange |
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| 507 | (G4ThreeVector& direction0,G4ThreeVector& direction1, |
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| 508 | G4ThreeVector& polarization0) |
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| 509 | { |
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| 510 | // direction0 is the original photon direction ---> z |
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| 511 | // polarization0 is the original photon polarization ---> x |
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| 512 | // need to specify y axis in the real reference frame ---> y |
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| 513 | G4ThreeVector Axis_Z0 = direction0.unit(); |
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| 514 | G4ThreeVector Axis_X0 = polarization0.unit(); |
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| 515 | G4ThreeVector Axis_Y0 = (Axis_Z0.cross(Axis_X0)).unit(); // to be confirmed; |
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| 516 | |
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| 517 | G4double direction_x = direction1.getX(); |
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| 518 | G4double direction_y = direction1.getY(); |
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| 519 | G4double direction_z = direction1.getZ(); |
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| 520 | |
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| 521 | direction1 = (direction_x*Axis_X0 + direction_y*Axis_Y0 + direction_z*Axis_Z0).unit(); |
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| 522 | |
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| 523 | } |
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| 524 | |
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| 525 | |
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| 526 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 527 | |
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| 528 | G4double G4LivermorePolarizedPhotoElectricModel::GetMeanFreePath(const G4Track& track, |
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| 529 | G4double, |
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| 530 | G4ForceCondition*) |
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| 531 | { |
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| 532 | |
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| 533 | const G4DynamicParticle* photon = track.GetDynamicParticle(); |
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| 534 | G4double energy = photon->GetKineticEnergy(); |
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| 535 | G4Material* material = track.GetMaterial(); |
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| 536 | // size_t materialIndex = material->GetIndex(); |
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| 537 | |
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| 538 | G4double meanFreePath = DBL_MAX; |
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| 539 | |
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| 540 | // if (energy > highEnergyLimit) |
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| 541 | // meanFreePath = meanFreePathTable->FindValue(highEnergyLimit,materialIndex); |
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| 542 | // else if (energy < lowEnergyLimit) meanFreePath = DBL_MAX; |
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| 543 | // else meanFreePath = meanFreePathTable->FindValue(energy,materialIndex); |
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| 544 | |
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| 545 | G4double cross = shellCrossSectionHandler->ValueForMaterial(material,energy); |
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| 546 | if(cross > 0.0) meanFreePath = 1.0/cross; |
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| 547 | |
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| 548 | return meanFreePath; |
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| 549 | |
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| 550 | |
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| 551 | } |
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| 552 | |
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| 553 | |
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