[1058] | 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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[1192] | 26 | // $Id: G4LivermoreIonisationModel.cc,v 1.7 2009/10/23 09:30:08 pandola Exp $ |
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[1196] | 27 | // GEANT4 tag $Name: geant4-09-03-cand-01 $ |
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[1058] | 28 | // |
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| 29 | // Author: Luciano Pandola |
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| 30 | // |
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| 31 | // History: |
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| 32 | // -------- |
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| 33 | // 12 Jan 2009 L Pandola Migration from process to model |
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| 34 | // 03 Mar 2009 L Pandola Bug fix (release memory in the destructor) |
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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 | // - simplify sampling of deexcitation by using cut in energy |
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| 39 | // - set activation of Auger "false" |
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| 40 | // - remove initialisation of element selectors |
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| 41 | // 19 May 2009 L Pandola Explicitely set to zero pointers deleted in |
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| 42 | // Initialise(), since they might be checked later on |
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[1192] | 43 | // 23 Oct 2009 L Pandola |
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| 44 | // - atomic deexcitation managed via G4VEmModel::DeexcitationFlag() is |
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| 45 | // set as "true" (default would be false) |
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[1058] | 46 | // |
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| 47 | |
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| 48 | #include "G4LivermoreIonisationModel.hh" |
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| 49 | #include "G4ParticleDefinition.hh" |
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| 50 | #include "G4MaterialCutsCouple.hh" |
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| 51 | #include "G4ProductionCutsTable.hh" |
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| 52 | #include "G4DynamicParticle.hh" |
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| 53 | #include "G4Element.hh" |
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| 54 | #include "G4AtomicTransitionManager.hh" |
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| 55 | #include "G4AtomicDeexcitation.hh" |
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| 56 | #include "G4AtomicShell.hh" |
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| 57 | #include "G4Gamma.hh" |
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| 58 | #include "G4Electron.hh" |
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| 59 | #include "G4CrossSectionHandler.hh" |
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| 60 | #include "G4ProcessManager.hh" |
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| 61 | #include "G4VEMDataSet.hh" |
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| 62 | #include "G4EMDataSet.hh" |
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| 63 | #include "G4eIonisationCrossSectionHandler.hh" |
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| 64 | #include "G4eIonisationSpectrum.hh" |
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| 65 | #include "G4VDataSetAlgorithm.hh" |
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| 66 | #include "G4SemiLogInterpolation.hh" |
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| 67 | #include "G4ShellVacancy.hh" |
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| 68 | #include "G4VDataSetAlgorithm.hh" |
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| 69 | #include "G4LogLogInterpolation.hh" |
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| 70 | #include "G4CompositeEMDataSet.hh" |
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| 71 | |
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| 72 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 73 | |
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| 74 | |
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| 75 | G4LivermoreIonisationModel::G4LivermoreIonisationModel(const G4ParticleDefinition*, |
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| 76 | const G4String& nam) |
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| 77 | :G4VEmModel(nam),isInitialised(false),crossSectionHandler(0), |
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| 78 | energySpectrum(0),shellVacancy(0) |
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| 79 | { |
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| 80 | fIntrinsicLowEnergyLimit = 10.0*eV; |
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| 81 | fIntrinsicHighEnergyLimit = 100.0*GeV; |
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| 82 | fNBinEnergyLoss = 360; |
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| 83 | // SetLowEnergyLimit(fIntrinsicLowEnergyLimit); |
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| 84 | SetHighEnergyLimit(fIntrinsicHighEnergyLimit); |
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| 85 | // |
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| 86 | verboseLevel = 0; |
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| 87 | // |
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[1192] | 88 | //By default: use deexcitation, not auger |
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| 89 | SetDeexcitationFlag(true); |
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[1058] | 90 | ActivateAuger(false); |
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[1192] | 91 | |
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[1058] | 92 | // |
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| 93 | // Notice: the fluorescence along step is generated only if it is |
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| 94 | // set by the PROCESS (e.g. G4eIonisation) via the command |
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| 95 | // process->ActivateDeexcitation(true); |
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| 96 | // |
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| 97 | } |
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| 98 | |
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| 99 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 100 | |
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| 101 | G4LivermoreIonisationModel::~G4LivermoreIonisationModel() |
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| 102 | { |
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| 103 | if (energySpectrum) delete energySpectrum; |
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| 104 | if (crossSectionHandler) delete crossSectionHandler; |
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| 105 | if (shellVacancy) delete shellVacancy; |
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| 106 | } |
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| 107 | |
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| 108 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 109 | |
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| 110 | void G4LivermoreIonisationModel::Initialise(const G4ParticleDefinition* particle, |
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| 111 | const G4DataVector& cuts) |
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| 112 | { |
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| 113 | //Check that the Livermore Ionisation is NOT attached to e+ |
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| 114 | if (particle != G4Electron::Electron()) |
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| 115 | { |
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| 116 | G4cout << "ERROR: Livermore Ionisation Model is applicable only to electrons" << G4endl; |
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| 117 | G4cout << "It cannot be registered to " << particle->GetParticleName() << G4endl; |
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| 118 | G4Exception(); |
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| 119 | } |
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| 120 | |
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| 121 | //Read energy spectrum |
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| 122 | if (energySpectrum) |
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| 123 | { |
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| 124 | delete energySpectrum; |
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| 125 | energySpectrum = 0; |
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| 126 | } |
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| 127 | energySpectrum = new G4eIonisationSpectrum(); |
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| 128 | if (verboseLevel > 0) |
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| 129 | G4cout << "G4VEnergySpectrum is initialized" << G4endl; |
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| 130 | |
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| 131 | //Initialize cross section handler |
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| 132 | if (crossSectionHandler) |
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| 133 | { |
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| 134 | delete crossSectionHandler; |
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| 135 | crossSectionHandler = 0; |
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| 136 | } |
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| 137 | |
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| 138 | G4VDataSetAlgorithm* interpolation = new G4SemiLogInterpolation(); |
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| 139 | crossSectionHandler = new G4eIonisationCrossSectionHandler(energySpectrum,interpolation, |
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| 140 | LowEnergyLimit(),HighEnergyLimit(), |
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| 141 | fNBinEnergyLoss); |
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| 142 | crossSectionHandler->Clear(); |
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| 143 | crossSectionHandler->LoadShellData("ioni/ion-ss-cs-"); |
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| 144 | //This is used to retrieve cross section values later on |
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| 145 | crossSectionHandler->BuildMeanFreePathForMaterials(&cuts); |
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| 146 | |
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| 147 | //Fluorescence data |
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| 148 | transitionManager = G4AtomicTransitionManager::Instance(); |
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| 149 | if (shellVacancy) delete shellVacancy; |
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| 150 | shellVacancy = new G4ShellVacancy(); |
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| 151 | InitialiseFluorescence(); |
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| 152 | |
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| 153 | if (verboseLevel > 0) |
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| 154 | { |
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| 155 | G4cout << "Livermore Ionisation model is initialized " << G4endl |
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| 156 | << "Energy range: " |
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| 157 | << LowEnergyLimit() / keV << " keV - " |
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| 158 | << HighEnergyLimit() / GeV << " GeV" |
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| 159 | << G4endl; |
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| 160 | } |
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| 161 | |
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| 162 | if (verboseLevel > 1) |
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| 163 | { |
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| 164 | G4cout << "Cross section data: " << G4endl; |
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| 165 | crossSectionHandler->PrintData(); |
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| 166 | G4cout << "Parameters: " << G4endl; |
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| 167 | energySpectrum->PrintData(); |
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| 168 | } |
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| 169 | |
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| 170 | if(isInitialised) return; |
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| 171 | fParticleChange = GetParticleChangeForLoss(); |
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| 172 | isInitialised = true; |
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| 173 | } |
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| 174 | |
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| 175 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 176 | |
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| 177 | G4double G4LivermoreIonisationModel::MinEnergyCut(const G4ParticleDefinition*, |
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| 178 | const G4MaterialCutsCouple*) |
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| 179 | { |
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| 180 | return 250.*eV; |
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| 181 | } |
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| 182 | |
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| 183 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 184 | |
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| 185 | G4double G4LivermoreIonisationModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*, |
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| 186 | G4double energy, |
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| 187 | G4double Z, G4double, |
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| 188 | G4double cutEnergy, |
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| 189 | G4double) |
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| 190 | { |
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| 191 | G4int iZ = (G4int) Z; |
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| 192 | if (!crossSectionHandler) |
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| 193 | { |
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| 194 | G4cout << "G4LivermoreIonisationModel::ComputeCrossSectionPerAtom" << G4endl; |
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| 195 | G4cout << "The cross section handler is not correctly initialized" << G4endl; |
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| 196 | G4Exception(); |
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| 197 | } |
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| 198 | |
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| 199 | //The cut is already included in the crossSectionHandler |
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| 200 | G4double cs = |
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| 201 | crossSectionHandler->GetCrossSectionAboveThresholdForElement(energy,cutEnergy,iZ); |
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| 202 | |
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| 203 | if (verboseLevel > 1) |
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| 204 | { |
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| 205 | G4cout << "G4LivermoreIonisationModel " << G4endl; |
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| 206 | G4cout << "Cross section for delta emission > " << cutEnergy/keV << " keV at " << |
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| 207 | energy/keV << " keV and Z = " << iZ << " --> " << cs/barn << " barn" << G4endl; |
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| 208 | } |
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| 209 | return cs; |
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| 210 | } |
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| 211 | |
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| 212 | |
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| 213 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 214 | |
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| 215 | G4double G4LivermoreIonisationModel::ComputeDEDXPerVolume(const G4Material* material, |
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| 216 | const G4ParticleDefinition* , |
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| 217 | G4double kineticEnergy, |
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| 218 | G4double cutEnergy) |
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| 219 | { |
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| 220 | G4double sPower = 0.0; |
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| 221 | |
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| 222 | const G4ElementVector* theElementVector = material->GetElementVector(); |
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| 223 | size_t NumberOfElements = material->GetNumberOfElements() ; |
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| 224 | const G4double* theAtomicNumDensityVector = |
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| 225 | material->GetAtomicNumDensityVector(); |
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| 226 | |
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| 227 | // loop for elements in the material |
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| 228 | for (size_t iel=0; iel<NumberOfElements; iel++ ) |
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| 229 | { |
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| 230 | G4int iZ = (G4int)((*theElementVector)[iel]->GetZ()); |
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| 231 | G4int nShells = transitionManager->NumberOfShells(iZ); |
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| 232 | for (G4int n=0; n<nShells; n++) |
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| 233 | { |
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| 234 | G4double e = energySpectrum->AverageEnergy(iZ, 0.0,cutEnergy, |
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| 235 | kineticEnergy, n); |
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| 236 | G4double cs= crossSectionHandler->FindValue(iZ,kineticEnergy, n); |
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| 237 | sPower += e * cs * theAtomicNumDensityVector[iel]; |
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| 238 | } |
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| 239 | G4double esp = energySpectrum->Excitation(iZ,kineticEnergy); |
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| 240 | sPower += esp * theAtomicNumDensityVector[iel]; |
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| 241 | } |
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| 242 | |
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| 243 | if (verboseLevel > 2) |
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| 244 | { |
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| 245 | G4cout << "G4LivermoreIonisationModel " << G4endl; |
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| 246 | G4cout << "Stopping power < " << cutEnergy/keV << " keV at " << |
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| 247 | kineticEnergy/keV << " keV = " << sPower/(keV/mm) << " keV/mm" << G4endl; |
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| 248 | } |
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| 249 | |
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| 250 | return sPower; |
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| 251 | } |
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| 252 | |
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| 253 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 254 | |
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| 255 | void G4LivermoreIonisationModel::SampleSecondaries(std::vector<G4DynamicParticle*>* fvect, |
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| 256 | const G4MaterialCutsCouple* couple, |
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| 257 | const G4DynamicParticle* aDynamicParticle, |
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| 258 | G4double cutE, |
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| 259 | G4double maxE) |
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| 260 | { |
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| 261 | |
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| 262 | G4double kineticEnergy = aDynamicParticle->GetKineticEnergy(); |
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| 263 | |
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| 264 | if (kineticEnergy <= fIntrinsicLowEnergyLimit) |
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| 265 | { |
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| 266 | fParticleChange->SetProposedKineticEnergy(0.); |
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| 267 | fParticleChange->ProposeLocalEnergyDeposit(kineticEnergy); |
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| 268 | return ; |
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| 269 | } |
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| 270 | |
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| 271 | // Select atom and shell |
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| 272 | G4int Z = crossSectionHandler->SelectRandomAtom(couple, kineticEnergy); |
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| 273 | G4int shell = crossSectionHandler->SelectRandomShell(Z, kineticEnergy); |
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| 274 | const G4AtomicShell* atomicShell = |
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| 275 | (G4AtomicTransitionManager::Instance())->Shell(Z, shell); |
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| 276 | G4double bindingEnergy = atomicShell->BindingEnergy(); |
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| 277 | G4int shellId = atomicShell->ShellId(); |
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| 278 | |
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| 279 | // Sample delta energy using energy interval for delta-electrons |
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| 280 | G4double energyMax = |
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| 281 | std::min(maxE,energySpectrum->MaxEnergyOfSecondaries(kineticEnergy)); |
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| 282 | G4double energyDelta = energySpectrum->SampleEnergy(Z, cutE, energyMax, |
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| 283 | kineticEnergy, shell); |
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| 284 | |
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| 285 | if (energyDelta == 0.) //nothing happens |
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| 286 | return; |
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| 287 | |
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| 288 | // Transform to shell potential |
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| 289 | G4double deltaKinE = energyDelta + 2.0*bindingEnergy; |
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| 290 | G4double primaryKinE = kineticEnergy + 2.0*bindingEnergy; |
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| 291 | |
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| 292 | // sampling of scattering angle neglecting atomic motion |
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| 293 | G4double deltaMom = std::sqrt(deltaKinE*(deltaKinE + 2.0*electron_mass_c2)); |
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| 294 | G4double primaryMom = std::sqrt(primaryKinE*(primaryKinE + 2.0*electron_mass_c2)); |
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| 295 | |
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| 296 | G4double cost = deltaKinE * (primaryKinE + 2.0*electron_mass_c2) |
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| 297 | / (deltaMom * primaryMom); |
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| 298 | if (cost > 1.) cost = 1.; |
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| 299 | G4double sint = std::sqrt(1. - cost*cost); |
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| 300 | G4double phi = twopi * G4UniformRand(); |
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| 301 | G4double dirx = sint * std::cos(phi); |
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| 302 | G4double diry = sint * std::sin(phi); |
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| 303 | G4double dirz = cost; |
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| 304 | |
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| 305 | // Rotate to incident electron direction |
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| 306 | G4ThreeVector primaryDirection = aDynamicParticle->GetMomentumDirection(); |
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| 307 | G4ThreeVector deltaDir(dirx,diry,dirz); |
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| 308 | deltaDir.rotateUz(primaryDirection); |
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| 309 | //Updated components |
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| 310 | dirx = deltaDir.x(); |
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| 311 | diry = deltaDir.y(); |
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| 312 | dirz = deltaDir.z(); |
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| 313 | |
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| 314 | // Take into account atomic motion del is relative momentum of the motion |
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| 315 | // kinetic energy of the motion == bindingEnergy in V.Ivanchenko model |
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| 316 | cost = 2.0*G4UniformRand() - 1.0; |
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| 317 | sint = std::sqrt(1. - cost*cost); |
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| 318 | phi = twopi * G4UniformRand(); |
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| 319 | G4double del = std::sqrt(bindingEnergy *(bindingEnergy + 2.0*electron_mass_c2)) |
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| 320 | / deltaMom; |
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| 321 | dirx += del* sint * std::cos(phi); |
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| 322 | diry += del* sint * std::sin(phi); |
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| 323 | dirz += del* cost; |
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| 324 | |
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| 325 | // Find out new primary electron direction |
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| 326 | G4double finalPx = primaryMom*primaryDirection.x() - deltaMom*dirx; |
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| 327 | G4double finalPy = primaryMom*primaryDirection.y() - deltaMom*diry; |
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| 328 | G4double finalPz = primaryMom*primaryDirection.z() - deltaMom*dirz; |
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| 329 | |
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| 330 | //Ok, ready to create the delta ray |
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| 331 | G4DynamicParticle* theDeltaRay = new G4DynamicParticle(); |
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| 332 | theDeltaRay->SetKineticEnergy(energyDelta); |
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| 333 | G4double norm = 1.0/std::sqrt(dirx*dirx + diry*diry + dirz*dirz); |
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| 334 | dirx *= norm; |
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| 335 | diry *= norm; |
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| 336 | dirz *= norm; |
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| 337 | theDeltaRay->SetMomentumDirection(dirx, diry, dirz); |
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| 338 | theDeltaRay->SetDefinition(G4Electron::Electron()); |
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| 339 | fvect->push_back(theDeltaRay); |
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| 340 | |
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| 341 | //This is the amount of energy available for fluorescence |
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| 342 | G4double theEnergyDeposit = bindingEnergy; |
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| 343 | |
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| 344 | // fill ParticleChange |
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| 345 | // changed energy and momentum of the actual particle |
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| 346 | G4double finalKinEnergy = kineticEnergy - energyDelta - theEnergyDeposit; |
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| 347 | if(finalKinEnergy < 0.0) |
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| 348 | { |
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| 349 | theEnergyDeposit += finalKinEnergy; |
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| 350 | finalKinEnergy = 0.0; |
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| 351 | } |
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| 352 | else |
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| 353 | { |
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| 354 | G4double norm = 1.0/std::sqrt(finalPx*finalPx+finalPy*finalPy+finalPz*finalPz); |
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| 355 | finalPx *= norm; |
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| 356 | finalPy *= norm; |
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| 357 | finalPz *= norm; |
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| 358 | fParticleChange->ProposeMomentumDirection(finalPx, finalPy, finalPz); |
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| 359 | } |
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| 360 | fParticleChange->SetProposedKineticEnergy(finalKinEnergy); |
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| 361 | |
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| 362 | // deexcitation may be active per G4Region |
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| 363 | if(DeexcitationFlag() && Z > 5) |
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| 364 | { |
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| 365 | G4ProductionCutsTable* theCoupleTable = |
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| 366 | G4ProductionCutsTable::GetProductionCutsTable(); |
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| 367 | // Retrieve cuts for gammas |
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| 368 | G4double cutG = (*theCoupleTable->GetEnergyCutsVector(0))[couple->GetIndex()]; |
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| 369 | if(theEnergyDeposit > cutG || theEnergyDeposit > cutE) |
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| 370 | { |
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| 371 | deexcitationManager.SetCutForSecondaryPhotons(cutG); |
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| 372 | deexcitationManager.SetCutForAugerElectrons(cutE); |
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| 373 | std::vector<G4DynamicParticle*>* secondaryVector = |
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| 374 | deexcitationManager.GenerateParticles(Z, shellId); |
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| 375 | G4DynamicParticle* aSecondary; |
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| 376 | |
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| 377 | if (secondaryVector) |
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| 378 | { |
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| 379 | for (size_t i = 0; i<secondaryVector->size(); i++) |
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| 380 | { |
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| 381 | aSecondary = (*secondaryVector)[i]; |
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| 382 | //Check if it is a valid secondary |
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| 383 | if (aSecondary) |
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| 384 | { |
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| 385 | G4double e = aSecondary->GetKineticEnergy(); |
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| 386 | if (e < theEnergyDeposit) |
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| 387 | { |
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| 388 | theEnergyDeposit -= e; |
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| 389 | fvect->push_back(aSecondary); |
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| 390 | } |
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| 391 | else |
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| 392 | { |
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| 393 | delete aSecondary; |
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| 394 | (*secondaryVector)[i] = 0; |
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| 395 | } |
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| 396 | } |
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| 397 | } |
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| 398 | } |
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| 399 | } |
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| 400 | } |
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| 401 | |
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| 402 | if (theEnergyDeposit < 0) |
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| 403 | { |
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| 404 | G4cout << "G4LivermoreIonisationModel: Negative energy deposit: " |
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| 405 | << theEnergyDeposit/eV << " eV" << G4endl; |
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| 406 | theEnergyDeposit = 0.0; |
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| 407 | } |
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| 408 | |
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| 409 | //Assign local energy deposit |
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| 410 | fParticleChange->ProposeLocalEnergyDeposit(theEnergyDeposit); |
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| 411 | |
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| 412 | if (verboseLevel > 1) |
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| 413 | { |
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| 414 | G4cout << "-----------------------------------------------------------" << G4endl; |
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| 415 | G4cout << "Energy balance from G4LivermoreIonisation" << G4endl; |
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| 416 | G4cout << "Incoming primary energy: " << kineticEnergy/keV << " keV" << G4endl; |
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| 417 | G4cout << "-----------------------------------------------------------" << G4endl; |
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| 418 | G4cout << "Outgoing primary energy: " << finalKinEnergy/keV << " keV" << G4endl; |
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| 419 | G4cout << "Delta ray " << energyDelta/keV << " keV" << G4endl; |
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| 420 | G4cout << "Fluorescence: " << (bindingEnergy-theEnergyDeposit)/keV << " keV" << G4endl; |
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| 421 | G4cout << "Local energy deposit " << theEnergyDeposit/keV << " keV" << G4endl; |
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| 422 | G4cout << "Total final state: " << (finalKinEnergy+energyDelta+bindingEnergy+ |
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| 423 | theEnergyDeposit)/keV << " keV" << G4endl; |
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| 424 | G4cout << "-----------------------------------------------------------" << G4endl; |
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| 425 | } |
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| 426 | return; |
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| 427 | } |
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| 428 | |
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| 429 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 430 | |
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| 431 | |
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| 432 | void G4LivermoreIonisationModel::SampleDeexcitationAlongStep(const G4Material* theMaterial, |
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| 433 | const G4Track& theTrack, |
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| 434 | G4double& eloss) |
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| 435 | { |
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| 436 | //No call if there is no deexcitation along step |
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| 437 | if (!DeexcitationFlag()) return; |
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| 438 | |
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| 439 | //This method gets the energy loss calculated "Along the Step" and |
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| 440 | //(including fluctuations) and produces explicit fluorescence/Auger |
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| 441 | //secondaries. The eloss value is updated. |
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| 442 | G4double energyLossBefore = eloss; |
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| 443 | if (verboseLevel > 2) |
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| 444 | G4cout << "Energy loss along step before deexcitation : " << energyLossBefore/keV << |
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| 445 | " keV" << G4endl; |
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| 446 | |
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| 447 | G4double incidentEnergy = theTrack.GetDynamicParticle()->GetKineticEnergy(); |
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| 448 | |
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| 449 | G4ProductionCutsTable* theCoupleTable = |
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| 450 | G4ProductionCutsTable::GetProductionCutsTable(); |
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| 451 | const G4MaterialCutsCouple* couple = theTrack.GetMaterialCutsCouple(); |
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| 452 | size_t index = couple->GetIndex(); |
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| 453 | G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[index]; |
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| 454 | G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[index]; |
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| 455 | |
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| 456 | //Notice: in LowEnergyIonisation, fluorescence is always generated above 250 eV |
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| 457 | //not above the tracking cut. |
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| 458 | //G4double cutForLowEnergySecondaryParticles = 250.0*eV; |
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| 459 | |
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| 460 | std::vector<G4DynamicParticle*>* deexcitationProducts = |
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| 461 | new std::vector<G4DynamicParticle*>; |
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| 462 | |
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| 463 | if(eloss > cute || eloss > cutg) |
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| 464 | { |
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| 465 | const G4AtomicTransitionManager* transitionManager = |
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| 466 | G4AtomicTransitionManager::Instance(); |
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| 467 | deexcitationManager.SetCutForSecondaryPhotons(cutg); |
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| 468 | deexcitationManager.SetCutForAugerElectrons(cute); |
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| 469 | |
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| 470 | size_t nElements = theMaterial->GetNumberOfElements(); |
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| 471 | const G4ElementVector* theElementVector = theMaterial->GetElementVector(); |
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| 472 | |
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| 473 | std::vector<G4DynamicParticle*>* secVector = 0; |
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| 474 | G4DynamicParticle* aSecondary = 0; |
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| 475 | //G4ParticleDefinition* type = 0; |
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| 476 | G4double e; |
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| 477 | G4ThreeVector position; |
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| 478 | G4int shell, shellId; |
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| 479 | |
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| 480 | // sample secondaries |
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| 481 | G4double eTot = 0.0; |
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| 482 | std::vector<G4int> n = |
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| 483 | shellVacancy->GenerateNumberOfIonisations(couple, |
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| 484 | incidentEnergy,eloss); |
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| 485 | for (size_t i=0; i<nElements; i++) |
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| 486 | { |
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| 487 | G4int Z = (G4int)((*theElementVector)[i]->GetZ()); |
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| 488 | size_t nVacancies = n[i]; |
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| 489 | G4double maxE = transitionManager->Shell(Z, 0)->BindingEnergy(); |
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| 490 | if (nVacancies > 0 && Z > 5 && (maxE > cute || maxE > cutg)) |
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| 491 | { |
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| 492 | for (size_t j=0; j<nVacancies; j++) |
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| 493 | { |
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| 494 | shell = crossSectionHandler->SelectRandomShell(Z, incidentEnergy); |
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| 495 | shellId = transitionManager->Shell(Z, shell)->ShellId(); |
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| 496 | G4double maxEShell = |
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| 497 | transitionManager->Shell(Z, shell)->BindingEnergy(); |
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| 498 | if (maxEShell > cute || maxEShell > cutg ) |
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| 499 | { |
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| 500 | secVector = deexcitationManager.GenerateParticles(Z, shellId); |
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| 501 | if (secVector) |
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| 502 | { |
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| 503 | for (size_t l = 0; l<secVector->size(); l++) { |
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| 504 | aSecondary = (*secVector)[l]; |
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| 505 | if (aSecondary) |
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| 506 | { |
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| 507 | e = aSecondary->GetKineticEnergy(); |
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| 508 | if ( eTot + e <= eloss ) |
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| 509 | { |
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| 510 | eTot += e; |
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| 511 | deexcitationProducts->push_back(aSecondary); |
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| 512 | } |
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| 513 | else |
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| 514 | { |
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| 515 | delete aSecondary; |
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| 516 | } |
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| 517 | } |
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| 518 | } |
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| 519 | delete secVector; |
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| 520 | } |
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| 521 | } |
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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 | |
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| 527 | size_t nSecondaries = deexcitationProducts->size(); |
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| 528 | if (nSecondaries > 0) |
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| 529 | { |
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| 530 | fParticleChange->SetNumberOfSecondaries(nSecondaries); |
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| 531 | const G4StepPoint* preStep = theTrack.GetStep()->GetPreStepPoint(); |
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| 532 | const G4StepPoint* postStep = theTrack.GetStep()->GetPostStepPoint(); |
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| 533 | G4ThreeVector r = preStep->GetPosition(); |
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| 534 | G4ThreeVector deltaR = postStep->GetPosition(); |
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| 535 | deltaR -= r; |
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| 536 | G4double t = preStep->GetGlobalTime(); |
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| 537 | G4double deltaT = postStep->GetGlobalTime(); |
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| 538 | deltaT -= t; |
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| 539 | G4double time, q; |
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| 540 | G4ThreeVector position; |
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| 541 | |
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| 542 | for (size_t i=0; i<nSecondaries; i++) |
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| 543 | { |
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| 544 | G4DynamicParticle* part = (*deexcitationProducts)[i]; |
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| 545 | if (part) |
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| 546 | { |
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| 547 | G4double eSecondary = part->GetKineticEnergy(); |
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| 548 | eloss -= eSecondary; |
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| 549 | if (eloss > 0.) |
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| 550 | { |
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| 551 | q = G4UniformRand(); |
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| 552 | time = deltaT*q + t; |
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| 553 | position = deltaR*q; |
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| 554 | position += r; |
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| 555 | G4Track* newTrack = new G4Track(part, time, position); |
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| 556 | pParticleChange->AddSecondary(newTrack); |
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| 557 | } |
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| 558 | else |
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| 559 | { |
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| 560 | eloss += eSecondary; |
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| 561 | delete part; |
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| 562 | part = 0; |
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| 563 | } |
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| 564 | } |
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| 565 | } |
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| 566 | } |
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| 567 | delete deexcitationProducts; |
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| 568 | |
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| 569 | if (verboseLevel > 2) |
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| 570 | G4cout << "Energy loss along step after deexcitation : " << eloss/keV << |
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| 571 | " keV" << G4endl; |
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| 572 | } |
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| 573 | |
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| 574 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 575 | |
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| 576 | void G4LivermoreIonisationModel::InitialiseFluorescence() |
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| 577 | { |
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| 578 | G4DataVector* ksi = 0; |
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| 579 | G4DataVector* energyVector = 0; |
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| 580 | size_t binForFluo = fNBinEnergyLoss/10; |
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| 581 | |
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| 582 | G4PhysicsLogVector* eVector = new G4PhysicsLogVector(LowEnergyLimit(),HighEnergyLimit(), |
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| 583 | binForFluo); |
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| 584 | const G4ProductionCutsTable* theCoupleTable= |
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| 585 | G4ProductionCutsTable::GetProductionCutsTable(); |
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| 586 | size_t numOfCouples = theCoupleTable->GetTableSize(); |
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| 587 | |
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| 588 | // Loop on couples |
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| 589 | for (size_t m=0; m<numOfCouples; m++) |
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| 590 | { |
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| 591 | const G4MaterialCutsCouple* couple = theCoupleTable->GetMaterialCutsCouple(m); |
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| 592 | const G4Material* material= couple->GetMaterial(); |
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| 593 | |
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| 594 | const G4ElementVector* theElementVector = material->GetElementVector(); |
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| 595 | size_t NumberOfElements = material->GetNumberOfElements() ; |
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| 596 | const G4double* theAtomicNumDensityVector = |
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| 597 | material->GetAtomicNumDensityVector(); |
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| 598 | |
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| 599 | G4VDataSetAlgorithm* interp = new G4LogLogInterpolation(); |
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| 600 | G4VEMDataSet* xsis = new G4CompositeEMDataSet(interp, 1., 1.); |
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| 601 | //loop on elements |
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| 602 | G4double energyCut = (*(theCoupleTable->GetEnergyCutsVector(1)))[m]; |
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| 603 | for (size_t iel=0; iel<NumberOfElements; iel++ ) |
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| 604 | { |
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| 605 | G4int iZ = (G4int)((*theElementVector)[iel]->GetZ()); |
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| 606 | energyVector = new G4DataVector(); |
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| 607 | ksi = new G4DataVector(); |
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| 608 | //Loop on energy |
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| 609 | for (size_t j = 0; j<binForFluo; j++) |
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| 610 | { |
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| 611 | G4double energy = eVector->GetLowEdgeEnergy(j); |
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| 612 | G4double cross = 0.; |
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| 613 | G4double eAverage= 0.; |
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| 614 | G4int nShells = transitionManager->NumberOfShells(iZ); |
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| 615 | |
---|
| 616 | for (G4int n=0; n<nShells; n++) |
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| 617 | { |
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| 618 | G4double e = energySpectrum->AverageEnergy(iZ, 0.0,energyCut, |
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| 619 | energy, n); |
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| 620 | G4double pro = energySpectrum->Probability(iZ, 0.0,energyCut, |
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| 621 | energy, n); |
---|
| 622 | G4double cs= crossSectionHandler->FindValue(iZ, energy, n); |
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| 623 | eAverage += e * cs * theAtomicNumDensityVector[iel]; |
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| 624 | cross += cs * pro * theAtomicNumDensityVector[iel]; |
---|
| 625 | if(verboseLevel > 1) |
---|
| 626 | { |
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| 627 | G4cout << "Z= " << iZ |
---|
| 628 | << " shell= " << n |
---|
| 629 | << " E(keV)= " << energy/keV |
---|
| 630 | << " Eav(keV)= " << e/keV |
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| 631 | << " pro= " << pro |
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| 632 | << " cs= " << cs |
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| 633 | << G4endl; |
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| 634 | } |
---|
| 635 | } |
---|
| 636 | |
---|
| 637 | G4double coeff = 0.0; |
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| 638 | if(eAverage > 0.) |
---|
| 639 | { |
---|
| 640 | coeff = cross/eAverage; |
---|
| 641 | eAverage /= cross; |
---|
| 642 | } |
---|
| 643 | |
---|
| 644 | if(verboseLevel > 1) |
---|
| 645 | { |
---|
| 646 | G4cout << "Ksi Coefficient for Z= " << iZ |
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| 647 | << " E(keV)= " << energy/keV |
---|
| 648 | << " Eav(keV)= " << eAverage/keV |
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| 649 | << " coeff= " << coeff |
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| 650 | << G4endl; |
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| 651 | } |
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| 652 | energyVector->push_back(energy); |
---|
| 653 | ksi->push_back(coeff); |
---|
| 654 | } |
---|
| 655 | G4VEMDataSet* p = new G4EMDataSet(iZ,energyVector,ksi,interp,1.,1.); |
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| 656 | xsis->AddComponent(p); |
---|
| 657 | } |
---|
| 658 | if(verboseLevel>0) xsis->PrintData(); |
---|
| 659 | shellVacancy->AddXsiTable(xsis); |
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| 660 | } |
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| 661 | } |
---|
| 662 | |
---|
| 663 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 664 | |
---|
| 665 | void G4LivermoreIonisationModel::ActivateAuger(G4bool val) |
---|
| 666 | { |
---|
[1192] | 667 | if (!DeexcitationFlag() && val) |
---|
| 668 | { |
---|
| 669 | G4cout << "WARNING - G4LivermoreIonisationModel" << G4endl; |
---|
| 670 | G4cout << "The use of the Atomic Deexcitation Manager is set to false " << G4endl; |
---|
| 671 | G4cout << "Therefore, Auger electrons will be not generated anyway" << G4endl; |
---|
| 672 | } |
---|
[1058] | 673 | deexcitationManager.ActivateAugerElectronProduction(val); |
---|
[1192] | 674 | if (verboseLevel > 1) |
---|
| 675 | G4cout << "Auger production set to " << val << G4endl; |
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[1058] | 676 | } |
---|
| 677 | |
---|