| 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 | // $Id: G4LowEnergyBremsstrahlung.cc,v 1.74 2009/06/11 15:47:08 mantero Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-03-cand-01 $
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| 28 | //
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| 29 | // --------------------------------------------------------------
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| 30 | //
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| 31 | // File name: G4LowEnergyBremsstrahlung
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| 32 | //
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| 33 | // Author: Alessandra Forti, Vladimir Ivanchenko
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| 34 | //
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| 35 | // Creation date: March 1999
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| 36 | //
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| 37 | // Modifications:
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| 38 | // 18.04.2000 V.L.
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| 39 | // - First implementation of continuous energy loss.
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| 40 | // 17.02.2000 Veronique Lefebure
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| 41 | // - correct bug : the gamma energy was not deposited when the gamma was
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| 42 | // not produced when its energy was < cutForLowEnergySecondaryPhotons
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| 43 | //
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| 44 | // Added Livermore data table construction methods A. Forti
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| 45 | // Modified BuildMeanFreePath to read new data tables A. Forti
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| 46 | // Modified PostStepDoIt to insert sampling with with EEDL data A. Forti
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| 47 | // Added SelectRandomAtom A. Forti
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| 48 | // Added map of the elements A. Forti
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| 49 | // 20.09.00 update printout V.Ivanchenko
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| 50 | // 24.04.01 V.Ivanchenko remove RogueWave
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| 51 | // 29.09.2001 V.Ivanchenko: major revision based on design iteration
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| 52 | // 10.10.2001 MGP Revision to improve code quality and consistency with design
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| 53 | // 18.10.2001 MGP Revision to improve code quality
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| 54 | // 28.10.2001 VI Update printout
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| 55 | // 29.11.2001 VI New parametrisation
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| 56 | // 30.07.2002 VI Fix in restricted energy loss
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| 57 | // 21.01.2003 VI Cut per region
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| 58 | // 21.02.2003 V.Ivanchenko Energy bins for spectrum are defined here
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| 59 | // 28.02.03 V.Ivanchenko Filename is defined in the constructor
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| 60 | // 24.03.2003 P.Rodrigues Changes to accommodate new angular generators
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| 61 | // 20.05.2003 MGP Removed memory leak related to angularDistribution
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| 62 | // 06.11.2003 MGP Improved user interface to select angular distribution model
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| 63 | //
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| 64 | // --------------------------------------------------------------
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| 65 |
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| 66 | #include "G4LowEnergyBremsstrahlung.hh"
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| 67 | #include "G4eBremsstrahlungSpectrum.hh"
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| 68 | #include "G4BremsstrahlungCrossSectionHandler.hh"
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| 69 | #include "G4VBremAngularDistribution.hh"
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| 70 | #include "G4ModifiedTsai.hh"
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| 71 | #include "G4Generator2BS.hh"
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| 72 | #include "G4Generator2BN.hh"
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| 73 | #include "G4VDataSetAlgorithm.hh"
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| 74 | #include "G4LogLogInterpolation.hh"
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| 75 | #include "G4VEMDataSet.hh"
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| 76 | #include "G4EnergyLossTables.hh"
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| 77 | #include "G4UnitsTable.hh"
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| 78 | #include "G4Electron.hh"
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| 79 | #include "G4Gamma.hh"
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| 80 | #include "G4ProductionCutsTable.hh"
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| 81 |
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| 82 |
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| 83 | G4LowEnergyBremsstrahlung::G4LowEnergyBremsstrahlung(const G4String& nam)
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| 84 | : G4eLowEnergyLoss(nam),
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| 85 | crossSectionHandler(0),
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| 86 | theMeanFreePath(0),
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| 87 | energySpectrum(0)
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| 88 | {
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| 89 | cutForPhotons = 0.;
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| 90 | verboseLevel = 0;
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| 91 | generatorName = "tsai";
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| 92 | angularDistribution = new G4ModifiedTsai("TsaiGenerator"); // default generator
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| 93 | // angularDistribution->PrintGeneratorInformation();
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| 94 | TsaiAngularDistribution = new G4ModifiedTsai("TsaiGenerator");
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| 95 |
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| 96 |
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| 97 | G4cout << G4endl;
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| 98 | G4cout << "*******************************************************************************" << G4endl;
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| 99 | G4cout << "*******************************************************************************" << G4endl;
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| 100 | G4cout << " The class G4LowEnergyBremsstrahlung is NOT SUPPORTED ANYMORE. " << G4endl;
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| 101 | G4cout << " It will be REMOVED with the next major release of Geant4. " << G4endl;
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| 102 | G4cout << " Please consult: https://twiki.cern.ch/twiki/bin/view/Geant4/LoweProcesses" << G4endl;
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| 103 | G4cout << "*******************************************************************************" << G4endl;
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| 104 | G4cout << "*******************************************************************************" << G4endl;
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| 105 | G4cout << G4endl;
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| 106 | }
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| 107 |
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| 108 | /*
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| 109 | G4LowEnergyBremsstrahlung::G4LowEnergyBremsstrahlung(const G4String& nam, G4VBremAngularDistribution* distribution)
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| 110 | : G4eLowEnergyLoss(nam),
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| 111 | crossSectionHandler(0),
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| 112 | theMeanFreePath(0),
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| 113 | energySpectrum(0),
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| 114 | angularDistribution(distribution)
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| 115 | {
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| 116 | cutForPhotons = 0.;
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| 117 | verboseLevel = 0;
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| 118 |
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| 119 | angularDistribution->PrintGeneratorInformation();
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| 120 |
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| 121 | TsaiAngularDistribution = new G4ModifiedTsai("TsaiGenerator");
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| 122 | }
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| 123 | */
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| 124 |
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| 125 | G4LowEnergyBremsstrahlung::~G4LowEnergyBremsstrahlung()
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| 126 | {
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| 127 | if(crossSectionHandler) delete crossSectionHandler;
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| 128 | if(energySpectrum) delete energySpectrum;
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| 129 | if(theMeanFreePath) delete theMeanFreePath;
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| 130 | delete angularDistribution;
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| 131 | delete TsaiAngularDistribution;
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| 132 | energyBins.clear();
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| 133 | }
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| 134 |
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| 135 |
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| 136 | void G4LowEnergyBremsstrahlung::BuildPhysicsTable(const G4ParticleDefinition& aParticleType)
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| 137 | {
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| 138 | if(verboseLevel > 0) {
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| 139 | G4cout << "G4LowEnergyBremsstrahlung::BuildPhysicsTable start"
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| 140 | << G4endl;
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| 141 | }
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| 142 |
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| 143 | cutForSecondaryPhotons.clear();
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| 144 |
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| 145 | // Create and fill BremsstrahlungParameters once
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| 146 | if( energySpectrum != 0 ) delete energySpectrum;
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| 147 | energyBins.clear();
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| 148 | for(size_t i=0; i<15; i++) {
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| 149 | G4double x = 0.1*((G4double)i);
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| 150 | if(i == 0) x = 0.01;
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| 151 | if(i == 10) x = 0.95;
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| 152 | if(i == 11) x = 0.97;
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| 153 | if(i == 12) x = 0.99;
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| 154 | if(i == 13) x = 0.995;
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| 155 | if(i == 14) x = 1.0;
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| 156 | energyBins.push_back(x);
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| 157 | }
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| 158 | const G4String dataName("/brem/br-sp.dat");
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| 159 | energySpectrum = new G4eBremsstrahlungSpectrum(energyBins,dataName);
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| 160 |
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| 161 | if(verboseLevel > 0) {
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| 162 | G4cout << "G4LowEnergyBremsstrahlungSpectrum is initialized"
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| 163 | << G4endl;
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| 164 | }
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| 165 |
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| 166 | // Create and fill G4CrossSectionHandler once
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| 167 |
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| 168 | if( crossSectionHandler != 0 ) delete crossSectionHandler;
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| 169 | G4VDataSetAlgorithm* interpolation = new G4LogLogInterpolation();
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| 170 | G4double lowKineticEnergy = GetLowerBoundEloss();
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| 171 | G4double highKineticEnergy = GetUpperBoundEloss();
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| 172 | G4int totBin = GetNbinEloss();
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| 173 | crossSectionHandler = new G4BremsstrahlungCrossSectionHandler(energySpectrum, interpolation);
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| 174 | crossSectionHandler->Initialise(0,lowKineticEnergy, highKineticEnergy, totBin);
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| 175 | crossSectionHandler->LoadShellData("brem/br-cs-");
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| 176 |
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| 177 | if (verboseLevel > 0) {
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| 178 | G4cout << GetProcessName()
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| 179 | << " is created; Cross section data: "
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| 180 | << G4endl;
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| 181 | crossSectionHandler->PrintData();
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| 182 | G4cout << "Parameters: "
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| 183 | << G4endl;
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| 184 | energySpectrum->PrintData();
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| 185 | }
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| 186 |
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| 187 | // Build loss table for Bremsstrahlung
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| 188 |
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| 189 | BuildLossTable(aParticleType);
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| 190 |
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| 191 | if(verboseLevel > 0) {
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| 192 | G4cout << "The loss table is built"
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| 193 | << G4endl;
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| 194 | }
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| 195 |
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| 196 | if (&aParticleType==G4Electron::Electron()) {
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| 197 |
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| 198 | RecorderOfElectronProcess[CounterOfElectronProcess] = (*this).theLossTable;
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| 199 | CounterOfElectronProcess++;
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| 200 | PrintInfoDefinition();
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| 201 |
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| 202 | } else {
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| 203 |
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| 204 | RecorderOfPositronProcess[CounterOfPositronProcess] = (*this).theLossTable;
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| 205 | CounterOfPositronProcess++;
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| 206 | }
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| 207 |
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| 208 | // Build mean free path data using cut values
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| 209 |
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| 210 | if( theMeanFreePath != 0 ) delete theMeanFreePath;
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| 211 | theMeanFreePath = crossSectionHandler->
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| 212 | BuildMeanFreePathForMaterials(&cutForSecondaryPhotons);
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| 213 |
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| 214 | if(verboseLevel > 0) {
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| 215 | G4cout << "The MeanFreePath table is built"
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| 216 | << G4endl;
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| 217 | }
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| 218 |
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| 219 | // Build common DEDX table for all ionisation processes
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| 220 |
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| 221 | BuildDEDXTable(aParticleType);
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| 222 |
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| 223 | if(verboseLevel > 0) {
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| 224 | G4cout << "G4LowEnergyBremsstrahlung::BuildPhysicsTable end"
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| 225 | << G4endl;
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| 226 | }
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| 227 |
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| 228 | }
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| 229 |
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| 230 |
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| 231 | void G4LowEnergyBremsstrahlung::BuildLossTable(const G4ParticleDefinition& )
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| 232 | {
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| 233 | // Build table for energy loss due to soft brems
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| 234 | // the tables are built for *MATERIALS* binning is taken from LowEnergyLoss
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| 235 |
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| 236 | G4double lowKineticEnergy = GetLowerBoundEloss();
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| 237 | G4double highKineticEnergy = GetUpperBoundEloss();
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| 238 | size_t totBin = GetNbinEloss();
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| 239 |
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| 240 | // create table
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| 241 |
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| 242 | if (theLossTable) {
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| 243 | theLossTable->clearAndDestroy();
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| 244 | delete theLossTable;
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| 245 | }
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| 246 | const G4ProductionCutsTable* theCoupleTable=
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| 247 | G4ProductionCutsTable::GetProductionCutsTable();
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| 248 | size_t numOfCouples = theCoupleTable->GetTableSize();
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| 249 | theLossTable = new G4PhysicsTable(numOfCouples);
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| 250 |
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| 251 | // Clean up the vector of cuts
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| 252 | cutForSecondaryPhotons.clear();
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| 253 |
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| 254 | // Loop for materials
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| 255 |
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| 256 | for (size_t j=0; j<numOfCouples; j++) {
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| 257 |
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| 258 | // create physics vector and fill it
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| 259 | G4PhysicsLogVector* aVector = new G4PhysicsLogVector(lowKineticEnergy,
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| 260 | highKineticEnergy,
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| 261 | totBin);
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| 262 |
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| 263 | // get material parameters needed for the energy loss calculation
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| 264 | const G4MaterialCutsCouple* couple = theCoupleTable->GetMaterialCutsCouple(j);
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| 265 | const G4Material* material= couple->GetMaterial();
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| 266 |
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| 267 | // the cut cannot be below lowest limit
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| 268 | G4double tCut = (*(theCoupleTable->GetEnergyCutsVector(0)))[j];
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| 269 | tCut = std::min(highKineticEnergy, tCut);
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| 270 | cutForSecondaryPhotons.push_back(tCut);
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| 271 |
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| 272 | const G4ElementVector* theElementVector = material->GetElementVector();
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| 273 | size_t NumberOfElements = material->GetNumberOfElements() ;
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| 274 | const G4double* theAtomicNumDensityVector =
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| 275 | material->GetAtomicNumDensityVector();
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| 276 | if(verboseLevel > 1) {
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| 277 | G4cout << "Energy loss for material # " << j
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| 278 | << " tCut(keV)= " << tCut/keV
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| 279 | << G4endl;
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| 280 | }
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| 281 |
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| 282 | // now comes the loop for the kinetic energy values
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| 283 | for (size_t i = 0; i<totBin; i++) {
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| 284 |
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| 285 | G4double lowEdgeEnergy = aVector->GetLowEdgeEnergy(i);
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| 286 | G4double ionloss = 0.;
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| 287 |
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| 288 | // loop for elements in the material
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| 289 | for (size_t iel=0; iel<NumberOfElements; iel++ ) {
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| 290 | G4int Z = (G4int)((*theElementVector)[iel]->GetZ());
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| 291 | G4double e = energySpectrum->AverageEnergy(Z, 0.0, tCut, lowEdgeEnergy);
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| 292 | G4double cs= crossSectionHandler->FindValue(Z, lowEdgeEnergy);
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| 293 | ionloss += e * cs * theAtomicNumDensityVector[iel];
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| 294 | if(verboseLevel > 1) {
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| 295 | G4cout << "Z= " << Z
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| 296 | << "; tCut(keV)= " << tCut/keV
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| 297 | << "; E(keV)= " << lowEdgeEnergy/keV
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| 298 | << "; Eav(keV)= " << e/keV
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| 299 | << "; cs= " << cs
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| 300 | << "; loss= " << ionloss
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| 301 | << G4endl;
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| 302 | }
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| 303 | }
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| 304 | aVector->PutValue(i,ionloss);
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| 305 | }
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| 306 | theLossTable->insert(aVector);
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| 307 | }
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| 308 | }
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| 309 |
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| 310 |
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| 311 | G4VParticleChange* G4LowEnergyBremsstrahlung::PostStepDoIt(const G4Track& track,
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| 312 | const G4Step& step)
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| 313 | {
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| 314 | aParticleChange.Initialize(track);
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| 315 |
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| 316 | const G4MaterialCutsCouple* couple = track.GetMaterialCutsCouple();
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| 317 | G4double kineticEnergy = track.GetKineticEnergy();
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| 318 | G4int index = couple->GetIndex();
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| 319 | G4double tCut = cutForSecondaryPhotons[index];
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| 320 |
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| 321 | // Control limits
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| 322 | if(tCut >= kineticEnergy)
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| 323 | return G4VContinuousDiscreteProcess::PostStepDoIt(track, step);
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| 324 |
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| 325 | G4int Z = crossSectionHandler->SelectRandomAtom(couple, kineticEnergy);
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| 326 |
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| 327 | G4double tGamma = energySpectrum->SampleEnergy(Z, tCut, kineticEnergy, kineticEnergy);
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| 328 | G4double totalEnergy = kineticEnergy + electron_mass_c2;
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| 329 | G4double finalEnergy = kineticEnergy - tGamma; // electron/positron final energy
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| 330 | G4double theta = 0;
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| 331 |
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| 332 | if((kineticEnergy < 1*MeV && kineticEnergy > 1*keV && generatorName == "2bn")){
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| 333 | theta = angularDistribution->PolarAngle(kineticEnergy,finalEnergy,Z);
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| 334 | }else{
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| 335 | theta = TsaiAngularDistribution->PolarAngle(kineticEnergy,finalEnergy,Z);
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| 336 | }
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| 337 |
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| 338 | G4double phi = twopi * G4UniformRand();
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| 339 | G4double dirZ = std::cos(theta);
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| 340 | G4double sinTheta = std::sqrt(1. - dirZ*dirZ);
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| 341 | G4double dirX = sinTheta*std::cos(phi);
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| 342 | G4double dirY = sinTheta*std::sin(phi);
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| 343 |
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| 344 | G4ThreeVector gammaDirection (dirX, dirY, dirZ);
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| 345 | G4ThreeVector electronDirection = track.GetMomentumDirection();
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| 346 |
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| 347 | //
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| 348 | // Update the incident particle
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| 349 | //
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| 350 | gammaDirection.rotateUz(electronDirection);
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| 351 |
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| 352 | // Kinematic problem
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| 353 | if (finalEnergy < 0.) {
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| 354 | tGamma += finalEnergy;
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| 355 | finalEnergy = 0.0;
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| 356 | }
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| 357 |
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| 358 | G4double momentum = std::sqrt((totalEnergy + electron_mass_c2)*kineticEnergy);
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| 359 |
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| 360 | G4double finalX = momentum*electronDirection.x() - tGamma*gammaDirection.x();
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| 361 | G4double finalY = momentum*electronDirection.y() - tGamma*gammaDirection.y();
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| 362 | G4double finalZ = momentum*electronDirection.z() - tGamma*gammaDirection.z();
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| 363 |
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| 364 | aParticleChange.SetNumberOfSecondaries(1);
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| 365 | G4double norm = 1./std::sqrt(finalX*finalX + finalY*finalY + finalZ*finalZ);
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| 366 | aParticleChange.ProposeMomentumDirection(finalX*norm, finalY*norm, finalZ*norm);
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| 367 | aParticleChange.ProposeEnergy( finalEnergy );
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| 368 |
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| 369 | // create G4DynamicParticle object for the gamma
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| 370 | G4DynamicParticle* aGamma= new G4DynamicParticle (G4Gamma::Gamma(),
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| 371 | gammaDirection, tGamma);
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| 372 | aParticleChange.AddSecondary(aGamma);
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| 373 |
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| 374 | return G4VContinuousDiscreteProcess::PostStepDoIt(track, step);
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| 375 | }
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| 376 |
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| 377 |
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| 378 | void G4LowEnergyBremsstrahlung::PrintInfoDefinition()
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| 379 | {
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| 380 | G4String comments = "Total cross sections from EEDL database.";
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| 381 | comments += "\n Gamma energy sampled from a parameterised formula.";
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| 382 | comments += "\n Implementation of the continuous dE/dx part.";
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| 383 | comments += "\n At present it can be used for electrons ";
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| 384 | comments += "in the energy range [250eV,100GeV].";
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| 385 | comments += "\n The process must work with G4LowEnergyIonisation.";
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| 386 |
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| 387 | G4cout << G4endl << GetProcessName() << ": " << comments << G4endl;
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| 388 | }
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| 389 |
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| 390 | G4bool G4LowEnergyBremsstrahlung::IsApplicable(const G4ParticleDefinition& particle)
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| 391 | {
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| 392 | return ( (&particle == G4Electron::Electron()) );
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| 393 | }
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| 394 |
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| 395 |
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| 396 | G4double G4LowEnergyBremsstrahlung::GetMeanFreePath(const G4Track& track,
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| 397 | G4double,
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| 398 | G4ForceCondition* cond)
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| 399 | {
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| 400 | *cond = NotForced;
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| 401 | G4int index = (track.GetMaterialCutsCouple())->GetIndex();
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| 402 | const G4VEMDataSet* data = theMeanFreePath->GetComponent(index);
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| 403 | G4double meanFreePath = data->FindValue(track.GetKineticEnergy());
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| 404 | return meanFreePath;
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|---|
| 405 | }
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| 406 |
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| 407 | void G4LowEnergyBremsstrahlung::SetCutForLowEnSecPhotons(G4double cut)
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|---|
| 408 | {
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|---|
| 409 | cutForPhotons = cut;
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|---|
| 410 | }
|
|---|
| 411 |
|
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| 412 | void G4LowEnergyBremsstrahlung::SetAngularGenerator(G4VBremAngularDistribution* distribution)
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|---|
| 413 | {
|
|---|
| 414 | angularDistribution = distribution;
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|---|
| 415 | angularDistribution->PrintGeneratorInformation();
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|---|
| 416 | }
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|---|
| 417 |
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|---|
| 418 | void G4LowEnergyBremsstrahlung::SetAngularGenerator(const G4String& name)
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|---|
| 419 | {
|
|---|
| 420 | if (name == "tsai")
|
|---|
| 421 | {
|
|---|
| 422 | delete angularDistribution;
|
|---|
| 423 | angularDistribution = new G4ModifiedTsai("TsaiGenerator");
|
|---|
| 424 | generatorName = name;
|
|---|
| 425 | }
|
|---|
| 426 | else if (name == "2bn")
|
|---|
| 427 | {
|
|---|
| 428 | delete angularDistribution;
|
|---|
| 429 | angularDistribution = new G4Generator2BN("2BNGenerator");
|
|---|
| 430 | generatorName = name;
|
|---|
| 431 | }
|
|---|
| 432 | else if (name == "2bs")
|
|---|
| 433 | {
|
|---|
| 434 | delete angularDistribution;
|
|---|
| 435 | angularDistribution = new G4Generator2BS("2BSGenerator");
|
|---|
| 436 | generatorName = name;
|
|---|
| 437 | }
|
|---|
| 438 | else
|
|---|
| 439 | {
|
|---|
| 440 | G4Exception("G4LowEnergyBremsstrahlung::SetAngularGenerator - generator does not exist");
|
|---|
| 441 | }
|
|---|
| 442 |
|
|---|
| 443 | angularDistribution->PrintGeneratorInformation();
|
|---|
| 444 | }
|
|---|
| 445 |
|
|---|