| 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 | // $Id: G4LowEnergyPhotoElectric.cc,v 1.56 2006/06/29 19:40:23 gunter Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-02 $
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| 29 | //
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| 30 | // Author: A. Forti
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| 31 | // Maria Grazia Pia (Maria.Grazia.Pia@cern.ch)
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| 32 | //
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| 33 | // History:
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| 34 | // --------
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| 35 | // October 1998 - low energy modifications by Alessandra Forti
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| 36 | // Added Livermore data table construction methods A. Forti
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| 37 | // Modified BuildMeanFreePath to read new data tables A. Forti
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| 38 | // Added EnergySampling method A. Forti
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| 39 | // Modified PostStepDoIt to insert sampling with EPDL97 data A. Forti
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| 40 | // Added SelectRandomAtom A. Forti
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| 41 | // Added map of the elements A. Forti
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| 42 | // 10.04.2000 VL
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| 43 | // - Correcting Fluorescence transition probabilities in order to take into account
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| 44 | // non-radiative transitions. No Auger electron simulated yet: energy is locally deposited.
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| 45 | // 17.02.2000 Veronique Lefebure
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| 46 | // - bugs corrected in fluorescence simulation:
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| 47 | // . when final use of binding energy: no photon was ever created
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| 48 | // . no Fluorescence was simulated when the photo-electron energy
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| 49 | // was below production threshold.
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| 50 | //
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| 51 | // 07-09-99, if no e- emitted: edep=photon energy, mma
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| 52 | // 24.04.01 V.Ivanchenko remove RogueWave
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| 53 | // 12.08.2001 MGP Revised according to a design iteration
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| 54 | // 16.09.2001 E. Guardincerri Added fluorescence generation
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| 55 | // 06.10.2001 MGP Added protection to avoid negative electron energies
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| 56 | // when binding energy of selected shell > photon energy
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| 57 | // 18.04.2001 V.Ivanchenko Fix problem with low energy gammas from fluorescence
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| 58 | // MeanFreePath is calculated by crosSectionHandler directly
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| 59 | // 31.05.2002 V.Ivanchenko Add path of Fluo + Auger cuts to AtomicDeexcitation
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| 60 | // 14.06.2002 V.Ivanchenko By default do not cheak range of e-
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| 61 | // 21.01.2003 V.Ivanchenko Cut per region
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| 62 | // 10.05.2004 P.Rodrigues Changes to accommodate new angular generators
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| 63 | // 20.01.2006 A.Trindade Changes to accommodate polarized angular generator
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| 64 | //
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| 65 | // --------------------------------------------------------------
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| 66 |
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| 67 | #include "G4LowEnergyPhotoElectric.hh"
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| 68 |
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| 69 | #include "G4VPhotoElectricAngularDistribution.hh"
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| 70 | #include "G4PhotoElectricAngularGeneratorSimple.hh"
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| 71 | #include "G4PhotoElectricAngularGeneratorSauterGavrila.hh"
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| 72 | #include "G4PhotoElectricAngularGeneratorPolarized.hh"
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| 73 |
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| 74 | #include "G4ParticleDefinition.hh"
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| 75 | #include "G4Track.hh"
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| 76 | #include "G4Step.hh"
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| 77 | #include "G4ForceCondition.hh"
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| 78 | #include "G4Gamma.hh"
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| 79 | #include "G4Electron.hh"
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| 80 | #include "G4DynamicParticle.hh"
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| 81 | #include "G4VParticleChange.hh"
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| 82 | #include "G4ThreeVector.hh"
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| 83 | #include "G4VCrossSectionHandler.hh"
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| 84 | #include "G4CrossSectionHandler.hh"
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| 85 | #include "G4VEMDataSet.hh"
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| 86 | #include "G4CompositeEMDataSet.hh"
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| 87 | #include "G4VDataSetAlgorithm.hh"
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| 88 | #include "G4LogLogInterpolation.hh"
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| 89 | #include "G4VRangeTest.hh"
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| 90 | #include "G4RangeNoTest.hh"
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| 91 | #include "G4AtomicTransitionManager.hh"
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| 92 | #include "G4AtomicShell.hh"
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| 93 | #include "G4ProductionCutsTable.hh"
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| 94 |
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| 95 | G4LowEnergyPhotoElectric::G4LowEnergyPhotoElectric(const G4String& processName)
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| 96 | : G4VDiscreteProcess(processName), lowEnergyLimit(250*eV), highEnergyLimit(100*GeV),
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| 97 | intrinsicLowEnergyLimit(10*eV),
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| 98 | intrinsicHighEnergyLimit(100*GeV),
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| 99 | cutForLowEnergySecondaryPhotons(250.*eV),
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| 100 | cutForLowEnergySecondaryElectrons(250.*eV)
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| 101 | {
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| 102 | if (lowEnergyLimit < intrinsicLowEnergyLimit ||
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| 103 | highEnergyLimit > intrinsicHighEnergyLimit)
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| 104 | {
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| 105 | G4Exception("G4LowEnergyPhotoElectric::G4LowEnergyPhotoElectric - energy limit outside intrinsic process validity range");
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| 106 | }
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| 107 |
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| 108 | crossSectionHandler = new G4CrossSectionHandler();
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| 109 | shellCrossSectionHandler = new G4CrossSectionHandler();
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| 110 | meanFreePathTable = 0;
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| 111 | rangeTest = new G4RangeNoTest;
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| 112 | generatorName = "geant4.6.2";
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| 113 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorSimple("GEANTSimpleGenerator"); // default generator
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| 114 |
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| 115 |
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| 116 | if (verboseLevel > 0)
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| 117 | {
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| 118 | G4cout << GetProcessName() << " is created " << G4endl
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| 119 | << "Energy range: "
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| 120 | << lowEnergyLimit / keV << " keV - "
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| 121 | << highEnergyLimit / GeV << " GeV"
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| 122 | << G4endl;
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| 123 | }
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| 124 | }
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| 125 |
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| 126 | G4LowEnergyPhotoElectric::~G4LowEnergyPhotoElectric()
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| 127 | {
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| 128 | delete crossSectionHandler;
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| 129 | delete shellCrossSectionHandler;
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| 130 | delete meanFreePathTable;
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| 131 | delete rangeTest;
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| 132 | delete ElectronAngularGenerator;
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| 133 | }
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| 134 |
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| 135 | void G4LowEnergyPhotoElectric::BuildPhysicsTable(const G4ParticleDefinition& )
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| 136 | {
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| 137 |
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| 138 | crossSectionHandler->Clear();
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| 139 | G4String crossSectionFile = "phot/pe-cs-";
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| 140 | crossSectionHandler->LoadData(crossSectionFile);
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| 141 |
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| 142 | shellCrossSectionHandler->Clear();
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| 143 | G4String shellCrossSectionFile = "phot/pe-ss-cs-";
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| 144 | shellCrossSectionHandler->LoadShellData(shellCrossSectionFile);
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| 145 |
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| 146 | delete meanFreePathTable;
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| 147 | meanFreePathTable = crossSectionHandler->BuildMeanFreePathForMaterials();
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| 148 | }
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| 149 |
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| 150 | G4VParticleChange* G4LowEnergyPhotoElectric::PostStepDoIt(const G4Track& aTrack,
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| 151 | const G4Step& aStep)
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| 152 | {
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| 153 | // Fluorescence generated according to:
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| 154 | // J. Stepanek ,"A program to determine the radiation spectra due to a single atomic
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| 155 | // subshell ionisation by a particle or due to deexcitation or decay of radionuclides",
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| 156 | // Comp. Phys. Comm. 1206 pp 1-1-9 (1997)
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| 157 |
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| 158 | aParticleChange.Initialize(aTrack);
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| 159 |
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| 160 | const G4DynamicParticle* incidentPhoton = aTrack.GetDynamicParticle();
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| 161 | G4double photonEnergy = incidentPhoton->GetKineticEnergy();
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| 162 | if (photonEnergy <= lowEnergyLimit)
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| 163 | {
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| 164 | aParticleChange.ProposeTrackStatus(fStopAndKill);
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| 165 | aParticleChange.ProposeEnergy(0.);
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| 166 | aParticleChange.ProposeLocalEnergyDeposit(photonEnergy);
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| 167 | return G4VDiscreteProcess::PostStepDoIt(aTrack,aStep);
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| 168 | }
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| 169 |
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| 170 | G4ThreeVector photonDirection = incidentPhoton->GetMomentumDirection(); // Returns the normalized direction of the momentum
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| 171 |
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| 172 | // Select randomly one element in the current material
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| 173 | const G4MaterialCutsCouple* couple = aTrack.GetMaterialCutsCouple();
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| 174 | G4int Z = crossSectionHandler->SelectRandomAtom(couple,photonEnergy);
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| 175 |
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| 176 | // Select the ionised shell in the current atom according to shell cross sections
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| 177 | size_t shellIndex = shellCrossSectionHandler->SelectRandomShell(Z,photonEnergy);
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| 178 |
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| 179 | // Retrieve the corresponding identifier and binding energy of the selected shell
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| 180 | const G4AtomicTransitionManager* transitionManager = G4AtomicTransitionManager::Instance();
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| 181 | const G4AtomicShell* shell = transitionManager->Shell(Z,shellIndex);
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| 182 | G4double bindingEnergy = shell->BindingEnergy();
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| 183 | G4int shellId = shell->ShellId();
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| 184 |
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| 185 | // Create lists of pointers to DynamicParticles (photons and electrons)
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| 186 | // (Is the electron vector necessary? To be checked)
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| 187 | std::vector<G4DynamicParticle*>* photonVector = 0;
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| 188 | std::vector<G4DynamicParticle*> electronVector;
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| 189 |
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| 190 | G4double energyDeposit = 0.0;
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| 191 |
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| 192 | // Primary outcoming electron
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| 193 | G4double eKineticEnergy = photonEnergy - bindingEnergy;
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| 194 |
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| 195 | // There may be cases where the binding energy of the selected shell is > photon energy
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| 196 | // In such cases do not generate secondaries
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| 197 | if (eKineticEnergy > 0.)
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| 198 | {
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| 199 | // Generate the electron only if with large enough range w.r.t. cuts and safety
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| 200 | G4double safety = aStep.GetPostStepPoint()->GetSafety();
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| 201 |
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| 202 | if (rangeTest->Escape(G4Electron::Electron(),couple,eKineticEnergy,safety))
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| 203 | {
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| 204 |
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| 205 | // Calculate direction of the photoelectron
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| 206 | G4ThreeVector gammaPolarization = incidentPhoton->GetPolarization();
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| 207 | G4ThreeVector electronDirection = ElectronAngularGenerator->GetPhotoElectronDirection(photonDirection,eKineticEnergy,gammaPolarization,shellId);
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| 208 |
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| 209 | // The electron is created ...
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| 210 | G4DynamicParticle* electron = new G4DynamicParticle (G4Electron::Electron(),
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| 211 | electronDirection,
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| 212 | eKineticEnergy);
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| 213 | electronVector.push_back(electron);
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| 214 | }
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| 215 | else
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| 216 | {
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| 217 | energyDeposit += eKineticEnergy;
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| 218 | }
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| 219 | }
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| 220 | else
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| 221 | {
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| 222 | bindingEnergy = photonEnergy;
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| 223 | }
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| 224 |
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| 225 | G4int nElectrons = electronVector.size();
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| 226 | size_t nTotPhotons = 0;
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| 227 | G4int nPhotons=0;
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| 228 | const G4ProductionCutsTable* theCoupleTable=
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| 229 | G4ProductionCutsTable::GetProductionCutsTable();
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| 230 |
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| 231 | size_t index = couple->GetIndex();
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| 232 | G4double cutg = (*(theCoupleTable->GetEnergyCutsVector(0)))[index];
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| 233 | cutg = std::min(cutForLowEnergySecondaryPhotons,cutg);
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| 234 |
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| 235 | G4double cute = (*(theCoupleTable->GetEnergyCutsVector(1)))[index];
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| 236 | cute = std::min(cutForLowEnergySecondaryPhotons,cute);
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| 237 |
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| 238 | G4DynamicParticle* aPhoton;
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| 239 |
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| 240 | // Generation of fluorescence
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| 241 | // Data in EADL are available only for Z > 5
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| 242 | // Protection to avoid generating photons in the unphysical case of
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| 243 | // shell binding energy > photon energy
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| 244 | if (Z > 5 && (bindingEnergy > cutg || bindingEnergy > cute))
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| 245 | {
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| 246 | photonVector = deexcitationManager.GenerateParticles(Z,shellId);
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| 247 | nTotPhotons = photonVector->size();
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| 248 | for (size_t k=0; k<nTotPhotons; k++)
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| 249 | {
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| 250 | aPhoton = (*photonVector)[k];
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| 251 | if (aPhoton)
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| 252 | {
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| 253 | G4double itsCut = cutg;
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| 254 | if(aPhoton->GetDefinition() == G4Electron::Electron()) itsCut = cute;
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| 255 | G4double itsEnergy = aPhoton->GetKineticEnergy();
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| 256 |
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| 257 | if (itsEnergy > itsCut && itsEnergy <= bindingEnergy)
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| 258 | {
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| 259 | nPhotons++;
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| 260 | // Local energy deposit is given as the sum of the
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| 261 | // energies of incident photons minus the energies
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| 262 | // of the outcoming fluorescence photons
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| 263 | bindingEnergy -= itsEnergy;
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| 264 |
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| 265 | }
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| 266 | else
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| 267 | {
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| 268 | delete aPhoton;
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| 269 | (*photonVector)[k] = 0;
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| 270 | }
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| 271 | }
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| 272 | }
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| 273 | }
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| 274 |
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| 275 | energyDeposit += bindingEnergy;
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| 276 |
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| 277 | G4int nSecondaries = nElectrons + nPhotons;
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| 278 | aParticleChange.SetNumberOfSecondaries(nSecondaries);
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| 279 |
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| 280 | for (G4int l = 0; l<nElectrons; l++ )
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| 281 | {
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| 282 | aPhoton = electronVector[l];
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| 283 | if(aPhoton) {
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| 284 | aParticleChange.AddSecondary(aPhoton);
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| 285 | }
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| 286 | }
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| 287 | for ( size_t ll = 0; ll < nTotPhotons; ll++)
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| 288 | {
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| 289 | aPhoton = (*photonVector)[ll];
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| 290 | if(aPhoton) {
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| 291 | aParticleChange.AddSecondary(aPhoton);
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| 292 | }
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| 293 | }
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| 294 |
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| 295 | delete photonVector;
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| 296 |
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| 297 | if (energyDeposit < 0)
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| 298 | {
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| 299 | G4cout << "WARNING - "
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| 300 | << "G4LowEnergyPhotoElectric::PostStepDoIt - Negative energy deposit"
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| 301 | << G4endl;
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| 302 | energyDeposit = 0;
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| 303 | }
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| 304 |
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| 305 | // Kill the incident photon
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| 306 | aParticleChange.ProposeMomentumDirection( 0., 0., 0. );
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| 307 | aParticleChange.ProposeEnergy( 0. );
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| 308 |
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| 309 | aParticleChange.ProposeLocalEnergyDeposit(energyDeposit);
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| 310 | aParticleChange.ProposeTrackStatus( fStopAndKill );
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| 311 |
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| 312 | // Reset NbOfInteractionLengthLeft and return aParticleChange
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| 313 | return G4VDiscreteProcess::PostStepDoIt( aTrack, aStep );
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| 314 | }
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| 315 |
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| 316 | G4bool G4LowEnergyPhotoElectric::IsApplicable(const G4ParticleDefinition& particle)
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| 317 | {
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| 318 | return ( &particle == G4Gamma::Gamma() );
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| 319 | }
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| 320 |
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| 321 | G4double G4LowEnergyPhotoElectric::GetMeanFreePath(const G4Track& track,
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| 322 | G4double, // previousStepSize
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| 323 | G4ForceCondition*)
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| 324 | {
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| 325 | const G4DynamicParticle* photon = track.GetDynamicParticle();
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| 326 | G4double energy = photon->GetKineticEnergy();
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| 327 | G4Material* material = track.GetMaterial();
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| 328 | // size_t materialIndex = material->GetIndex();
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| 329 |
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| 330 | G4double meanFreePath = DBL_MAX;
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| 331 |
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| 332 | // if (energy > highEnergyLimit)
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| 333 | // meanFreePath = meanFreePathTable->FindValue(highEnergyLimit,materialIndex);
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| 334 | // else if (energy < lowEnergyLimit) meanFreePath = DBL_MAX;
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| 335 | // else meanFreePath = meanFreePathTable->FindValue(energy,materialIndex);
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| 336 |
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| 337 | G4double cross = shellCrossSectionHandler->ValueForMaterial(material,energy);
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| 338 | if(cross > 0.0) meanFreePath = 1.0/cross;
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| 339 |
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| 340 | return meanFreePath;
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| 341 | }
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| 342 |
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| 343 | void G4LowEnergyPhotoElectric::SetCutForLowEnSecPhotons(G4double cut)
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| 344 | {
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| 345 | cutForLowEnergySecondaryPhotons = cut;
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| 346 | deexcitationManager.SetCutForSecondaryPhotons(cut);
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| 347 | }
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| 348 |
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| 349 | void G4LowEnergyPhotoElectric::SetCutForLowEnSecElectrons(G4double cut)
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| 350 | {
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| 351 | cutForLowEnergySecondaryElectrons = cut;
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| 352 | deexcitationManager.SetCutForAugerElectrons(cut);
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| 353 | }
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| 354 |
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| 355 | void G4LowEnergyPhotoElectric::ActivateAuger(G4bool val)
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| 356 | {
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| 357 | deexcitationManager.ActivateAugerElectronProduction(val);
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| 358 | }
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| 359 |
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| 360 | void G4LowEnergyPhotoElectric::SetAngularGenerator(G4VPhotoElectricAngularDistribution* distribution)
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| 361 | {
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| 362 | ElectronAngularGenerator = distribution;
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| 363 | ElectronAngularGenerator->PrintGeneratorInformation();
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| 364 | }
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| 365 |
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| 366 | void G4LowEnergyPhotoElectric::SetAngularGenerator(const G4String& name)
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| 367 | {
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| 368 | if (name == "default")
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| 369 | {
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| 370 | delete ElectronAngularGenerator;
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| 371 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorSimple("GEANT4LowEnergySimpleGenerator");
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| 372 | generatorName = name;
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| 373 | }
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| 374 | else if (name == "standard")
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| 375 | {
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| 376 | delete ElectronAngularGenerator;
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| 377 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorSauterGavrila("GEANT4SauterGavrilaGenerator");
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| 378 | generatorName = name;
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| 379 | }
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| 380 | else if (name == "polarized")
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| 381 | {
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| 382 | delete ElectronAngularGenerator;
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| 383 | ElectronAngularGenerator = new G4PhotoElectricAngularGeneratorPolarized("GEANT4LowEnergyPolarizedGenerator");
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| 384 | generatorName = name;
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| 385 | }
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| 386 | else
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| 387 | {
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| 388 | G4Exception("G4LowEnergyPhotoElectric::SetAngularGenerator - generator does not exist");
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| 389 | }
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| 390 |
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| 391 | ElectronAngularGenerator->PrintGeneratorInformation();
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| 392 | }
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