| [819] | 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| [1315] | 26 | // $Id: G4PAIModel.cc,v 1.52 2010/06/03 07:28:39 grichine Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-04-beta-cand-01 $
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| [1055] | 28 | //
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| 29 | // -------------------------------------------------------------------
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| 30 | //
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| 31 | // GEANT4 Class
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| [819] | 32 | // File name: G4PAIModel.cc
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| 33 | //
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| [1315] | 34 | // Author: Vladimir.Grichine@cern.ch on base of Vladimir Ivanchenko model interface
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| [819] | 35 | //
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| 36 | // Creation date: 05.10.2003
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| 37 | //
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| 38 | // Modifications:
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| 39 | //
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| 40 | // 17.08.04 V.Grichine, bug fixed for Tkin<=0 in SampleSecondary
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| 41 | // 16.08.04 V.Grichine, bug fixed in massRatio for DEDX, CrossSection, SampleSecondary
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| 42 | // 08.04.05 Major optimisation of internal interfaces (V.Ivantchenko)
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| [1196] | 43 | // 26.07.09 Fixed logic to work with several materials (V.Ivantchenko)
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| [819] | 44 | //
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| 45 |
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| 46 | #include "G4Region.hh"
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| 47 | #include "G4PhysicsLogVector.hh"
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| 48 | #include "G4PhysicsFreeVector.hh"
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| 49 | #include "G4PhysicsTable.hh"
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| 50 | #include "G4ProductionCutsTable.hh"
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| 51 | #include "G4MaterialCutsCouple.hh"
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| 52 | #include "G4MaterialTable.hh"
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| 53 | #include "G4SandiaTable.hh"
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| 54 | #include "G4OrderedTable.hh"
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| 55 |
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| 56 | #include "G4PAIModel.hh"
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| 57 | #include "Randomize.hh"
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| 58 | #include "G4Electron.hh"
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| 59 | #include "G4Positron.hh"
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| 60 | #include "G4Poisson.hh"
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| 61 | #include "G4Step.hh"
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| 62 | #include "G4Material.hh"
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| 63 | #include "G4DynamicParticle.hh"
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| 64 | #include "G4ParticleDefinition.hh"
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| 65 | #include "G4ParticleChangeForLoss.hh"
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| 66 |
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| 67 | ////////////////////////////////////////////////////////////////////////
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| 68 |
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| 69 | using namespace std;
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| 70 |
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| 71 | G4PAIModel::G4PAIModel(const G4ParticleDefinition* p, const G4String& nam)
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| 72 | : G4VEmModel(nam),G4VEmFluctuationModel(nam),
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| 73 | fVerbose(0),
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| 74 | fLowestGamma(1.005),
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| 75 | fHighestGamma(10000.),
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| 76 | fTotBin(200),
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| 77 | fMeanNumber(20),
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| 78 | fParticle(0),
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| 79 | fHighKinEnergy(100.*TeV),
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| 80 | fTwoln10(2.0*log(10.0)),
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| 81 | fBg2lim(0.0169),
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| 82 | fTaulim(8.4146e-3)
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| 83 | {
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| 84 | if(p) SetParticle(p);
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| 85 |
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| 86 | fElectron = G4Electron::Electron();
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| 87 | fPositron = G4Positron::Positron();
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| 88 |
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| 89 | fPAItransferTable = 0;
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| 90 | fPAIdEdxTable = 0;
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| 91 | fSandiaPhotoAbsCof = 0;
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| 92 | fdEdxVector = 0;
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| 93 | fLambdaVector = 0;
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| 94 | fdNdxCutVector = 0;
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| 95 |
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| 96 | isInitialised = false;
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| 97 | }
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| 98 |
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| 99 | ////////////////////////////////////////////////////////////////////////////
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| 100 |
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| 101 | G4PAIModel::~G4PAIModel()
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| 102 | {
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| 103 | // G4cout << "PAI: start destruction" << G4endl;
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| 104 | if(fParticleEnergyVector) delete fParticleEnergyVector;
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| 105 | if(fdEdxVector) delete fdEdxVector ;
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| 106 | if(fLambdaVector) delete fLambdaVector;
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| 107 | if(fdNdxCutVector) delete fdNdxCutVector;
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| 108 |
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| 109 | if( fPAItransferTable )
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| 110 | {
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| 111 | fPAItransferTable->clearAndDestroy();
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| 112 | delete fPAItransferTable ;
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| 113 | }
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| 114 | if( fPAIdEdxTable )
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| 115 | {
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| 116 | fPAIdEdxTable->clearAndDestroy();
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| 117 | delete fPAIdEdxTable ;
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| 118 | }
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| 119 | if(fSandiaPhotoAbsCof)
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| 120 | {
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| 121 | for(G4int i=0;i<fSandiaIntervalNumber;i++)
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| 122 | {
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| 123 | delete[] fSandiaPhotoAbsCof[i];
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| 124 | }
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| 125 | delete[] fSandiaPhotoAbsCof;
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| 126 | }
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| 127 | //G4cout << "PAI: end destruction" << G4endl;
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| 128 | }
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| 129 |
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| 130 | ///////////////////////////////////////////////////////////////////////////////
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| 131 |
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| 132 | void G4PAIModel::SetParticle(const G4ParticleDefinition* p)
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| 133 | {
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| 134 | if(fParticle == p) return;
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| 135 | fParticle = p;
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| 136 | fMass = fParticle->GetPDGMass();
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| 137 | fSpin = fParticle->GetPDGSpin();
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| 138 | G4double q = fParticle->GetPDGCharge()/eplus;
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| 139 | fChargeSquare = q*q;
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| 140 | fLowKinEnergy = 0.2*MeV*fMass/proton_mass_c2;
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| 141 | fRatio = electron_mass_c2/fMass;
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| 142 | fQc = fMass/fRatio;
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| 143 | }
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| 144 |
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| 145 | ////////////////////////////////////////////////////////////////////////////
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| 146 |
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| 147 | void G4PAIModel::Initialise(const G4ParticleDefinition* p,
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| 148 | const G4DataVector&)
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| 149 | {
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| [1315] | 150 | G4cout<<"G4PAIModel::Initialise for "<<p->GetParticleName()<<G4endl;
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| [819] | 151 | if(isInitialised) return;
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| 152 | isInitialised = true;
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| 153 |
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| 154 | SetParticle(p);
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| 155 | fLowestKineticEnergy = fMass*(fLowestGamma - 1.0);
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| 156 | fHighestKineticEnergy = fMass*(fHighestGamma - 1.0);
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| 157 |
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| 158 | fParticleEnergyVector = new G4PhysicsLogVector(fLowestKineticEnergy,
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| 159 | fHighestKineticEnergy,
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| 160 | fTotBin);
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| 161 |
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| [1055] | 162 | fParticleChange = GetParticleChangeForLoss();
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| [819] | 163 |
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| 164 | // Prepare initialization
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| 165 | const G4ProductionCutsTable* theCoupleTable =
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| 166 | G4ProductionCutsTable::GetProductionCutsTable();
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| 167 | const G4MaterialTable* theMaterialTable = G4Material::GetMaterialTable();
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| 168 | size_t numOfMat = G4Material::GetNumberOfMaterials();
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| 169 | size_t numRegions = fPAIRegionVector.size();
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| 170 |
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| 171 | for(size_t iReg = 0; iReg < numRegions; ++iReg) // region loop
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| 172 | {
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| 173 | const G4Region* curReg = fPAIRegionVector[iReg];
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| 174 | for(size_t jMat = 0; jMat < numOfMat; ++jMat) // region material loop
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| 175 | {
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| 176 | fMaterial = (*theMaterialTable)[jMat];
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| 177 | fCutCouple = theCoupleTable->GetMaterialCutsCouple( fMaterial,
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| 178 | curReg->GetProductionCuts() );
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| [1055] | 179 | //G4cout << "Reg <" <<curReg->GetName() << "> mat <"
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| 180 | // << fMaterial->GetName() << "> fCouple= "
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| [1196] | 181 | // << fCutCouple<<" " << p->GetParticleName() <<G4endl;
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| [819] | 182 | if( fCutCouple ) {
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| 183 | fMaterialCutsCoupleVector.push_back(fCutCouple);
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| 184 |
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| [1196] | 185 | fPAItransferTable = new G4PhysicsTable(fTotBin+1);
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| 186 | fPAIdEdxTable = new G4PhysicsTable(fTotBin+1);
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| 187 |
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| [819] | 188 | fDeltaCutInKinEnergy =
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| 189 | (*theCoupleTable->GetEnergyCutsVector(1))[fCutCouple->GetIndex()];
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| 190 |
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| 191 | //ComputeSandiaPhotoAbsCof();
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| 192 | BuildPAIonisationTable();
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| 193 |
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| 194 | fPAIxscBank.push_back(fPAItransferTable);
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| 195 | fPAIdEdxBank.push_back(fPAIdEdxTable);
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| 196 | fdEdxTable.push_back(fdEdxVector);
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| 197 |
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| 198 | BuildLambdaVector();
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| 199 | fdNdxCutTable.push_back(fdNdxCutVector);
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| 200 | fLambdaTable.push_back(fLambdaVector);
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| 201 | }
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| 202 | }
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| 203 | }
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| 204 | }
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| 205 |
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| 206 | //////////////////////////////////////////////////////////////////
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| 207 |
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| [1055] | 208 | void G4PAIModel::InitialiseMe(const G4ParticleDefinition*)
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| 209 | {}
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| 210 |
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| 211 | //////////////////////////////////////////////////////////////////
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| 212 |
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| [819] | 213 | void G4PAIModel::ComputeSandiaPhotoAbsCof()
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| 214 | {
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| 215 | G4int i, j, numberOfElements ;
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| 216 | static const G4MaterialTable* theMaterialTable = G4Material::GetMaterialTable();
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| 217 |
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| 218 | G4SandiaTable thisMaterialSandiaTable(fMatIndex) ;
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| 219 | numberOfElements = (*theMaterialTable)[fMatIndex]->
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| 220 | GetNumberOfElements();
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| 221 | G4int* thisMaterialZ = new G4int[numberOfElements] ;
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| 222 |
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| 223 | for(i=0;i<numberOfElements;i++)
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| 224 | {
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| 225 | thisMaterialZ[i] =
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| 226 | (G4int)(*theMaterialTable)[fMatIndex]->GetElement(i)->GetZ() ;
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| 227 | }
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| 228 | fSandiaIntervalNumber = thisMaterialSandiaTable.SandiaIntervals
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| 229 | (thisMaterialZ,numberOfElements) ;
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| 230 |
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| 231 | fSandiaIntervalNumber = thisMaterialSandiaTable.SandiaMixing
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| 232 | ( thisMaterialZ ,
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| 233 | (*theMaterialTable)[fMatIndex]->GetFractionVector() ,
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| 234 | numberOfElements,fSandiaIntervalNumber) ;
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| 235 |
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| 236 | fSandiaPhotoAbsCof = new G4double*[fSandiaIntervalNumber] ;
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| 237 |
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| 238 | for(i=0;i<fSandiaIntervalNumber;i++) fSandiaPhotoAbsCof[i] = new G4double[5] ;
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| 239 |
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| 240 | for( i = 0 ; i < fSandiaIntervalNumber ; i++ )
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| 241 | {
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| 242 | fSandiaPhotoAbsCof[i][0] = thisMaterialSandiaTable.GetPhotoAbsorpCof(i+1,0) ;
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| 243 |
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| 244 | for( j = 1; j < 5 ; j++ )
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| 245 | {
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| 246 | fSandiaPhotoAbsCof[i][j] = thisMaterialSandiaTable.
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| 247 | GetPhotoAbsorpCof(i+1,j)*
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| 248 | (*theMaterialTable)[fMatIndex]->GetDensity() ;
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| 249 | }
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| 250 | }
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| 251 | // delete[] thisMaterialZ ;
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| 252 | }
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| 253 |
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| 254 | ////////////////////////////////////////////////////////////////////////////
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| 255 | //
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| 256 | // Build tables for the ionization energy loss
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| 257 | // the tables are built for MATERIALS
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| 258 | // *********
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| 259 |
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| 260 | void G4PAIModel::BuildPAIonisationTable()
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| 261 | {
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| 262 | G4double LowEdgeEnergy , ionloss ;
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| 263 | G4double tau, Tmax, Tmin, Tkin, deltaLow, gamma, bg2 ;
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| 264 |
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| 265 | fdEdxVector = new G4PhysicsLogVector( fLowestKineticEnergy,
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| 266 | fHighestKineticEnergy,
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| 267 | fTotBin);
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| 268 | G4SandiaTable* sandia = fMaterial->GetSandiaTable();
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| 269 |
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| 270 | Tmin = sandia->GetSandiaCofForMaterialPAI(0,0)*keV;
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| 271 | deltaLow = 100.*eV; // 0.5*eV ;
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| 272 |
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| [1196] | 273 | for (G4int i = 0 ; i <= fTotBin ; i++) //The loop for the kinetic energy
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| [819] | 274 | {
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| 275 | LowEdgeEnergy = fParticleEnergyVector->GetLowEdgeEnergy(i) ;
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| 276 | tau = LowEdgeEnergy/fMass ;
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| 277 | gamma = tau +1. ;
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| 278 | // G4cout<<"gamma = "<<gamma<<endl ;
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| 279 | bg2 = tau*( tau + 2. );
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| 280 | Tmax = MaxSecondaryEnergy(fParticle, LowEdgeEnergy);
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| 281 | // Tmax = std::min(fDeltaCutInKinEnergy, Tmax);
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| 282 | Tkin = Tmax ;
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| 283 |
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| 284 | if ( Tmax < Tmin + deltaLow ) // low energy safety
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| 285 | Tkin = Tmin + deltaLow ;
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| 286 |
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| 287 | fPAIySection.Initialize(fMaterial, Tkin, bg2);
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| 288 |
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| 289 | // G4cout<<"ionloss = "<<ionloss*cm/keV<<" keV/cm"<<endl ;
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| 290 | // G4cout<<"n1 = "<<protonPAI.GetIntegralPAIxSection(1)*cm<<" 1/cm"<<endl ;
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| 291 | // G4cout<<"protonPAI.GetSplineSize() = "<<
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| 292 | // protonPAI.GetSplineSize()<<G4endl<<G4endl ;
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| 293 |
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| 294 | G4int n = fPAIySection.GetSplineSize();
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| 295 | G4PhysicsFreeVector* transferVector = new G4PhysicsFreeVector(n) ;
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| 296 | G4PhysicsFreeVector* dEdxVector = new G4PhysicsFreeVector(n);
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| 297 |
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| 298 | for( G4int k = 0 ; k < n; k++ )
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| 299 | {
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| 300 | transferVector->PutValue( k ,
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| 301 | fPAIySection.GetSplineEnergy(k+1),
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| 302 | fPAIySection.GetIntegralPAIySection(k+1) ) ;
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| 303 | dEdxVector->PutValue( k ,
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| 304 | fPAIySection.GetSplineEnergy(k+1),
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| 305 | fPAIySection.GetIntegralPAIdEdx(k+1) ) ;
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| 306 | }
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| 307 | ionloss = fPAIySection.GetMeanEnergyLoss() ; // total <dE/dx>
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| 308 |
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| 309 | if ( ionloss < DBL_MIN) ionloss = DBL_MIN;
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| 310 | fdEdxVector->PutValue(i,ionloss) ;
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| 311 |
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| 312 | fPAItransferTable->insertAt(i,transferVector) ;
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| 313 | fPAIdEdxTable->insertAt(i,dEdxVector) ;
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| 314 |
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| 315 | } // end of Tkin loop
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| 316 | }
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| 317 |
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| 318 | ///////////////////////////////////////////////////////////////////////
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| 319 | //
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| 320 | // Build mean free path tables for the delta ray production process
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| 321 | // tables are built for MATERIALS
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| 322 | //
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| 323 |
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| 324 | void G4PAIModel::BuildLambdaVector()
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| 325 | {
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| 326 | fLambdaVector = new G4PhysicsLogVector( fLowestKineticEnergy,
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| 327 | fHighestKineticEnergy,
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| 328 | fTotBin ) ;
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| 329 | fdNdxCutVector = new G4PhysicsLogVector( fLowestKineticEnergy,
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| 330 | fHighestKineticEnergy,
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| 331 | fTotBin ) ;
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| 332 | if(fVerbose > 1)
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| 333 | {
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| 334 | G4cout<<"PAIModel DeltaCutInKineticEnergyNow = "
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| 335 | <<fDeltaCutInKinEnergy/keV<<" keV"<<G4endl;
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| 336 | }
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| [1196] | 337 | for (G4int i = 0 ; i <= fTotBin ; i++ )
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| [819] | 338 | {
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| 339 | G4double dNdxCut = GetdNdxCut(i,fDeltaCutInKinEnergy) ;
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| [1196] | 340 | //G4cout << "i= " << i << " x= " << dNdxCut << G4endl;
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| 341 | if(dNdxCut < 0.0) dNdxCut = 0.0;
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| 342 | // G4double lambda = dNdxCut <= DBL_MIN ? DBL_MAX: 1.0/dNdxCut ;
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| 343 | G4double lambda = DBL_MAX;
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| 344 | if(dNdxCut > 0.0) lambda = 1.0/dNdxCut;
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| [819] | 345 |
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| 346 | fLambdaVector->PutValue(i, lambda) ;
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| 347 | fdNdxCutVector->PutValue(i, dNdxCut) ;
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| 348 | }
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| 349 | }
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| 350 |
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| 351 | ///////////////////////////////////////////////////////////////////////
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| 352 | //
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| 353 | // Returns integral PAI cross section for energy transfers >= transferCut
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| 354 |
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| 355 | G4double
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| 356 | G4PAIModel::GetdNdxCut( G4int iPlace, G4double transferCut)
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| 357 | {
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| 358 | G4int iTransfer;
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| 359 | G4double x1, x2, y1, y2, dNdxCut;
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| 360 | // G4cout<<"iPlace = "<<iPlace<<"; "<<"transferCut = "<<transferCut<<G4endl;
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| 361 | // G4cout<<"size = "<<G4int((*fPAItransferTable)(iPlace)->GetVectorLength())
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| 362 | // <<G4endl;
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| 363 | for( iTransfer = 0 ;
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| 364 | iTransfer < G4int((*fPAItransferTable)(iPlace)->GetVectorLength()) ;
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| 365 | iTransfer++)
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| 366 | {
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| 367 | if(transferCut <= (*fPAItransferTable)(iPlace)->GetLowEdgeEnergy(iTransfer))
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| 368 | {
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| 369 | break ;
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| 370 | }
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| 371 | }
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| 372 | if ( iTransfer >= G4int((*fPAItransferTable)(iPlace)->GetVectorLength()) )
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| 373 | {
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| 374 | iTransfer = (*fPAItransferTable)(iPlace)->GetVectorLength() - 1 ;
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| 375 | }
|
|---|
| 376 | y1 = (*(*fPAItransferTable)(iPlace))(iTransfer-1) ;
|
|---|
| 377 | y2 = (*(*fPAItransferTable)(iPlace))(iTransfer) ;
|
|---|
| [1196] | 378 | if(y1 < 0.0) y1 = 0.0;
|
|---|
| 379 | if(y2 < 0.0) y2 = 0.0;
|
|---|
| [819] | 380 | // G4cout<<"y1 = "<<y1<<"; "<<"y2 = "<<y2<<G4endl;
|
|---|
| 381 | x1 = (*fPAItransferTable)(iPlace)->GetLowEdgeEnergy(iTransfer-1) ;
|
|---|
| 382 | x2 = (*fPAItransferTable)(iPlace)->GetLowEdgeEnergy(iTransfer) ;
|
|---|
| 383 | // G4cout<<"x1 = "<<x1<<"; "<<"x2 = "<<x2<<G4endl;
|
|---|
| 384 |
|
|---|
| 385 | if ( y1 == y2 ) dNdxCut = y2 ;
|
|---|
| 386 | else
|
|---|
| 387 | {
|
|---|
| 388 | // if ( x1 == x2 ) dNdxCut = y1 + (y2 - y1)*G4UniformRand() ;
|
|---|
| [1055] | 389 | // if ( std::abs(x1-x2) <= eV ) dNdxCut = y1 + (y2 - y1)*G4UniformRand() ;
|
|---|
| 390 | if ( std::abs(x1-x2) <= eV ) dNdxCut = y1 + (y2 - y1)*0.5 ;
|
|---|
| [819] | 391 | else dNdxCut = y1 + (transferCut - x1)*(y2 - y1)/(x2 - x1) ;
|
|---|
| 392 | }
|
|---|
| 393 | // G4cout<<""<<dNdxCut<<G4endl;
|
|---|
| [1196] | 394 | if(dNdxCut < 0.0) dNdxCut = 0.0;
|
|---|
| [819] | 395 | return dNdxCut ;
|
|---|
| 396 | }
|
|---|
| 397 | ///////////////////////////////////////////////////////////////////////
|
|---|
| 398 | //
|
|---|
| 399 | // Returns integral dEdx for energy transfers >= transferCut
|
|---|
| 400 |
|
|---|
| 401 | G4double
|
|---|
| 402 | G4PAIModel::GetdEdxCut( G4int iPlace, G4double transferCut)
|
|---|
| 403 | {
|
|---|
| 404 | G4int iTransfer;
|
|---|
| 405 | G4double x1, x2, y1, y2, dEdxCut;
|
|---|
| [1196] | 406 | //G4cout<<"iPlace = "<<iPlace<<"; "<<"transferCut = "<<transferCut<<G4endl;
|
|---|
| [819] | 407 | // G4cout<<"size = "<<G4int((*fPAIdEdxTable)(iPlace)->GetVectorLength())
|
|---|
| 408 | // <<G4endl;
|
|---|
| 409 | for( iTransfer = 0 ;
|
|---|
| 410 | iTransfer < G4int((*fPAIdEdxTable)(iPlace)->GetVectorLength()) ;
|
|---|
| 411 | iTransfer++)
|
|---|
| 412 | {
|
|---|
| 413 | if(transferCut <= (*fPAIdEdxTable)(iPlace)->GetLowEdgeEnergy(iTransfer))
|
|---|
| 414 | {
|
|---|
| 415 | break ;
|
|---|
| 416 | }
|
|---|
| 417 | }
|
|---|
| 418 | if ( iTransfer >= G4int((*fPAIdEdxTable)(iPlace)->GetVectorLength()) )
|
|---|
| 419 | {
|
|---|
| 420 | iTransfer = (*fPAIdEdxTable)(iPlace)->GetVectorLength() - 1 ;
|
|---|
| 421 | }
|
|---|
| 422 | y1 = (*(*fPAIdEdxTable)(iPlace))(iTransfer-1) ;
|
|---|
| 423 | y2 = (*(*fPAIdEdxTable)(iPlace))(iTransfer) ;
|
|---|
| [1196] | 424 | if(y1 < 0.0) y1 = 0.0;
|
|---|
| 425 | if(y2 < 0.0) y2 = 0.0;
|
|---|
| 426 | //G4cout<<"y1 = "<<y1<<"; "<<"y2 = "<<y2<<G4endl;
|
|---|
| [819] | 427 | x1 = (*fPAIdEdxTable)(iPlace)->GetLowEdgeEnergy(iTransfer-1) ;
|
|---|
| 428 | x2 = (*fPAIdEdxTable)(iPlace)->GetLowEdgeEnergy(iTransfer) ;
|
|---|
| [1196] | 429 | //G4cout<<"x1 = "<<x1<<"; "<<"x2 = "<<x2<<G4endl;
|
|---|
| [819] | 430 |
|
|---|
| 431 | if ( y1 == y2 ) dEdxCut = y2 ;
|
|---|
| 432 | else
|
|---|
| 433 | {
|
|---|
| 434 | // if ( x1 == x2 ) dEdxCut = y1 + (y2 - y1)*G4UniformRand() ;
|
|---|
| [1055] | 435 | // if ( std::abs(x1-x2) <= eV ) dEdxCut = y1 + (y2 - y1)*G4UniformRand() ;
|
|---|
| 436 | if ( std::abs(x1-x2) <= eV ) dEdxCut = y1 + (y2 - y1)*0.5 ;
|
|---|
| [819] | 437 | else dEdxCut = y1 + (transferCut - x1)*(y2 - y1)/(x2 - x1) ;
|
|---|
| 438 | }
|
|---|
| [1196] | 439 | //G4cout<<""<<dEdxCut<<G4endl;
|
|---|
| 440 | if(dEdxCut < 0.0) dEdxCut = 0.0;
|
|---|
| [819] | 441 | return dEdxCut ;
|
|---|
| 442 | }
|
|---|
| 443 |
|
|---|
| 444 | //////////////////////////////////////////////////////////////////////////////
|
|---|
| 445 |
|
|---|
| [1055] | 446 | G4double G4PAIModel::ComputeDEDXPerVolume(const G4Material*,
|
|---|
| 447 | const G4ParticleDefinition* p,
|
|---|
| 448 | G4double kineticEnergy,
|
|---|
| 449 | G4double cutEnergy)
|
|---|
| [819] | 450 | {
|
|---|
| 451 | G4int iTkin,iPlace;
|
|---|
| [1055] | 452 |
|
|---|
| 453 | //G4double cut = std::min(MaxSecondaryEnergy(p, kineticEnergy), cutEnergy);
|
|---|
| 454 | G4double cut = cutEnergy;
|
|---|
| 455 |
|
|---|
| [819] | 456 | G4double massRatio = fMass/p->GetPDGMass();
|
|---|
| 457 | G4double scaledTkin = kineticEnergy*massRatio;
|
|---|
| 458 | G4double charge = p->GetPDGCharge();
|
|---|
| [1055] | 459 | G4double charge2 = charge*charge;
|
|---|
| 460 | const G4MaterialCutsCouple* matCC = CurrentCouple();
|
|---|
| [819] | 461 |
|
|---|
| [1196] | 462 | size_t jMat = 0;
|
|---|
| 463 | for(;jMat < fMaterialCutsCoupleVector.size(); ++jMat )
|
|---|
| [819] | 464 | {
|
|---|
| 465 | if( matCC == fMaterialCutsCoupleVector[jMat] ) break;
|
|---|
| 466 | }
|
|---|
| [1196] | 467 | //G4cout << "jMat= " << jMat
|
|---|
| 468 | // << " jMax= " << fMaterialCutsCoupleVector.size()
|
|---|
| 469 | // << " matCC: " << matCC;
|
|---|
| 470 | //if(matCC) G4cout << " mat: " << matCC->GetMaterial()->GetName();
|
|---|
| 471 | // G4cout << G4endl;
|
|---|
| 472 | if(jMat == fMaterialCutsCoupleVector.size()) return 0.0;
|
|---|
| [819] | 473 |
|
|---|
| 474 | fPAIdEdxTable = fPAIdEdxBank[jMat];
|
|---|
| 475 | fdEdxVector = fdEdxTable[jMat];
|
|---|
| [1196] | 476 | for(iTkin = 0 ; iTkin <= fTotBin ; iTkin++)
|
|---|
| [819] | 477 | {
|
|---|
| 478 | if(scaledTkin < fParticleEnergyVector->GetLowEdgeEnergy(iTkin)) break ;
|
|---|
| 479 | }
|
|---|
| [1196] | 480 | //G4cout << "E= " << scaledTkin << " iTkin= " << iTkin
|
|---|
| 481 | // << " " << fdEdxVector->GetVectorLength()<<G4endl;
|
|---|
| [819] | 482 | iPlace = iTkin - 1;
|
|---|
| 483 | if(iPlace < 0) iPlace = 0;
|
|---|
| [1196] | 484 | else if(iPlace >= fTotBin) iPlace = fTotBin-1;
|
|---|
| [1055] | 485 | G4double dEdx = charge2*( (*fdEdxVector)(iPlace) - GetdEdxCut(iPlace,cut) );
|
|---|
| [819] | 486 | if( dEdx < 0.) dEdx = 0.;
|
|---|
| 487 | return dEdx;
|
|---|
| 488 | }
|
|---|
| 489 |
|
|---|
| 490 | /////////////////////////////////////////////////////////////////////////
|
|---|
| 491 |
|
|---|
| [1055] | 492 | G4double G4PAIModel::CrossSectionPerVolume( const G4Material*,
|
|---|
| 493 | const G4ParticleDefinition* p,
|
|---|
| 494 | G4double kineticEnergy,
|
|---|
| 495 | G4double cutEnergy,
|
|---|
| 496 | G4double maxEnergy )
|
|---|
| [819] | 497 | {
|
|---|
| 498 | G4int iTkin,iPlace;
|
|---|
| [1055] | 499 | G4double tmax = std::min(MaxSecondaryEnergy(p, kineticEnergy), maxEnergy);
|
|---|
| 500 | if(tmax <= cutEnergy) return 0.0;
|
|---|
| [819] | 501 | G4double massRatio = fMass/p->GetPDGMass();
|
|---|
| 502 | G4double scaledTkin = kineticEnergy*massRatio;
|
|---|
| 503 | G4double charge = p->GetPDGCharge();
|
|---|
| 504 | G4double charge2 = charge*charge, cross, cross1, cross2;
|
|---|
| [1055] | 505 | const G4MaterialCutsCouple* matCC = CurrentCouple();
|
|---|
| [819] | 506 |
|
|---|
| [1196] | 507 | size_t jMat = 0;
|
|---|
| 508 | for(;jMat < fMaterialCutsCoupleVector.size(); ++jMat )
|
|---|
| [819] | 509 | {
|
|---|
| 510 | if( matCC == fMaterialCutsCoupleVector[jMat] ) break;
|
|---|
| 511 | }
|
|---|
| [1196] | 512 | if(jMat == fMaterialCutsCoupleVector.size()) return 0.0;
|
|---|
| [819] | 513 |
|
|---|
| 514 | fPAItransferTable = fPAIxscBank[jMat];
|
|---|
| 515 |
|
|---|
| [1196] | 516 | for(iTkin = 0 ; iTkin <= fTotBin ; iTkin++)
|
|---|
| [819] | 517 | {
|
|---|
| 518 | if(scaledTkin < fParticleEnergyVector->GetLowEdgeEnergy(iTkin)) break ;
|
|---|
| 519 | }
|
|---|
| 520 | iPlace = iTkin - 1;
|
|---|
| 521 | if(iPlace < 0) iPlace = 0;
|
|---|
| [1196] | 522 | else if(iPlace >= fTotBin) iPlace = fTotBin-1;
|
|---|
| [819] | 523 |
|
|---|
| [1196] | 524 | //G4cout<<"iPlace = "<<iPlace<<"; tmax = "
|
|---|
| [819] | 525 | // <<tmax<<"; cutEnergy = "<<cutEnergy<<G4endl;
|
|---|
| 526 | cross1 = GetdNdxCut(iPlace,tmax) ;
|
|---|
| [1196] | 527 | //G4cout<<"cross1 = "<<cross1<<G4endl;
|
|---|
| [819] | 528 | cross2 = GetdNdxCut(iPlace,cutEnergy) ;
|
|---|
| [1196] | 529 | //G4cout<<"cross2 = "<<cross2<<G4endl;
|
|---|
| [819] | 530 | cross = (cross2-cross1)*charge2;
|
|---|
| [1196] | 531 | //G4cout<<"cross = "<<cross<<G4endl;
|
|---|
| 532 | if( cross < DBL_MIN) cross = 0.0;
|
|---|
| [819] | 533 | // if( cross2 < DBL_MIN) cross2 = DBL_MIN;
|
|---|
| 534 |
|
|---|
| 535 | // return cross2;
|
|---|
| 536 | return cross;
|
|---|
| 537 | }
|
|---|
| 538 |
|
|---|
| 539 | ///////////////////////////////////////////////////////////////////////////
|
|---|
| 540 | //
|
|---|
| 541 | // It is analog of PostStepDoIt in terms of secondary electron.
|
|---|
| 542 | //
|
|---|
| 543 |
|
|---|
| 544 | void G4PAIModel::SampleSecondaries(std::vector<G4DynamicParticle*>* vdp,
|
|---|
| 545 | const G4MaterialCutsCouple* matCC,
|
|---|
| 546 | const G4DynamicParticle* dp,
|
|---|
| 547 | G4double tmin,
|
|---|
| 548 | G4double maxEnergy)
|
|---|
| 549 | {
|
|---|
| [1196] | 550 | size_t jMat = 0;
|
|---|
| 551 | for(;jMat < fMaterialCutsCoupleVector.size(); ++jMat )
|
|---|
| [819] | 552 | {
|
|---|
| 553 | if( matCC == fMaterialCutsCoupleVector[jMat] ) break;
|
|---|
| 554 | }
|
|---|
| [1196] | 555 | if(jMat == fMaterialCutsCoupleVector.size()) return;
|
|---|
| [819] | 556 |
|
|---|
| 557 | fPAItransferTable = fPAIxscBank[jMat];
|
|---|
| 558 | fdNdxCutVector = fdNdxCutTable[jMat];
|
|---|
| 559 |
|
|---|
| 560 | G4double tmax = std::min(MaxSecondaryKinEnergy(dp), maxEnergy);
|
|---|
| 561 | if( tmin >= tmax && fVerbose > 0)
|
|---|
| 562 | {
|
|---|
| 563 | G4cout<<"G4PAIModel::SampleSecondary: tmin >= tmax "<<G4endl;
|
|---|
| 564 | }
|
|---|
| 565 | G4ThreeVector direction= dp->GetMomentumDirection();
|
|---|
| 566 | G4double particleMass = dp->GetMass();
|
|---|
| 567 | G4double kineticEnergy = dp->GetKineticEnergy();
|
|---|
| 568 |
|
|---|
| 569 | G4double massRatio = fMass/particleMass;
|
|---|
| 570 | G4double scaledTkin = kineticEnergy*massRatio;
|
|---|
| 571 | G4double totalEnergy = kineticEnergy + particleMass;
|
|---|
| 572 | G4double pSquare = kineticEnergy*(totalEnergy+particleMass);
|
|---|
| 573 |
|
|---|
| 574 | G4double deltaTkin = GetPostStepTransfer(scaledTkin);
|
|---|
| 575 |
|
|---|
| 576 | // G4cout<<"G4PAIModel::SampleSecondaries; deltaKIn = "<<deltaTkin/keV<<" keV "<<G4endl;
|
|---|
| 577 |
|
|---|
| 578 | if( deltaTkin <= 0. && fVerbose > 0)
|
|---|
| 579 | {
|
|---|
| 580 | G4cout<<"G4PAIModel::SampleSecondary e- deltaTkin = "<<deltaTkin<<G4endl;
|
|---|
| 581 | }
|
|---|
| 582 | if( deltaTkin <= 0.) return;
|
|---|
| 583 |
|
|---|
| 584 | if( deltaTkin > tmax) deltaTkin = tmax;
|
|---|
| 585 |
|
|---|
| 586 | G4double deltaTotalMomentum = sqrt(deltaTkin*(deltaTkin + 2. * electron_mass_c2 ));
|
|---|
| 587 | G4double totalMomentum = sqrt(pSquare);
|
|---|
| 588 | G4double costheta = deltaTkin*(totalEnergy + electron_mass_c2)
|
|---|
| 589 | /(deltaTotalMomentum * totalMomentum);
|
|---|
| 590 |
|
|---|
| 591 | if( costheta > 0.99999 ) costheta = 0.99999;
|
|---|
| 592 | G4double sintheta = 0.0;
|
|---|
| 593 | G4double sin2 = 1. - costheta*costheta;
|
|---|
| 594 | if( sin2 > 0.) sintheta = sqrt(sin2);
|
|---|
| 595 |
|
|---|
| 596 | // direction of the delta electron
|
|---|
| 597 | G4double phi = twopi*G4UniformRand();
|
|---|
| 598 | G4double dirx = sintheta*cos(phi), diry = sintheta*sin(phi), dirz = costheta;
|
|---|
| 599 |
|
|---|
| 600 | G4ThreeVector deltaDirection(dirx,diry,dirz);
|
|---|
| 601 | deltaDirection.rotateUz(direction);
|
|---|
| 602 | deltaDirection.unit();
|
|---|
| 603 |
|
|---|
| 604 | // primary change
|
|---|
| 605 | kineticEnergy -= deltaTkin;
|
|---|
| 606 | G4ThreeVector dir = totalMomentum*direction - deltaTotalMomentum*deltaDirection;
|
|---|
| 607 | direction = dir.unit();
|
|---|
| 608 | fParticleChange->SetProposedKineticEnergy(kineticEnergy);
|
|---|
| 609 | fParticleChange->SetProposedMomentumDirection(direction);
|
|---|
| 610 |
|
|---|
| 611 | // create G4DynamicParticle object for e- delta ray
|
|---|
| 612 | G4DynamicParticle* deltaRay = new G4DynamicParticle;
|
|---|
| 613 | deltaRay->SetDefinition(G4Electron::Electron());
|
|---|
| 614 | deltaRay->SetKineticEnergy( deltaTkin ); // !!! trick for last steps /2.0 ???
|
|---|
| 615 | deltaRay->SetMomentumDirection(deltaDirection);
|
|---|
| 616 |
|
|---|
| 617 | vdp->push_back(deltaRay);
|
|---|
| 618 | }
|
|---|
| 619 |
|
|---|
| 620 |
|
|---|
| 621 | ///////////////////////////////////////////////////////////////////////
|
|---|
| 622 | //
|
|---|
| 623 | // Returns post step PAI energy transfer > cut electron energy according to passed
|
|---|
| 624 | // scaled kinetic energy of particle
|
|---|
| 625 |
|
|---|
| 626 | G4double
|
|---|
| 627 | G4PAIModel::GetPostStepTransfer( G4double scaledTkin )
|
|---|
| 628 | {
|
|---|
| 629 | // G4cout<<"G4PAIModel::GetPostStepTransfer"<<G4endl ;
|
|---|
| 630 |
|
|---|
| 631 | G4int iTkin, iTransfer, iPlace ;
|
|---|
| 632 | G4double transfer = 0.0, position, dNdxCut1, dNdxCut2, E1, E2, W1, W2, W ;
|
|---|
| 633 |
|
|---|
| [1196] | 634 | for(iTkin=0;iTkin<=fTotBin;iTkin++)
|
|---|
| [819] | 635 | {
|
|---|
| 636 | if(scaledTkin < fParticleEnergyVector->GetLowEdgeEnergy(iTkin)) break ;
|
|---|
| 637 | }
|
|---|
| 638 | iPlace = iTkin - 1 ;
|
|---|
| 639 | // G4cout<<"from search, iPlace = "<<iPlace<<G4endl ;
|
|---|
| 640 | if(iPlace < 0) iPlace = 0;
|
|---|
| [1196] | 641 | else if(iPlace >= fTotBin) iPlace = fTotBin-1;
|
|---|
| [819] | 642 | dNdxCut1 = (*fdNdxCutVector)(iPlace) ;
|
|---|
| 643 | // G4cout<<"dNdxCut1 = "<<dNdxCut1<<G4endl ;
|
|---|
| 644 |
|
|---|
| 645 |
|
|---|
| 646 | if(iTkin == fTotBin) // Fermi plato, try from left
|
|---|
| 647 | {
|
|---|
| 648 | position = dNdxCut1*G4UniformRand() ;
|
|---|
| 649 |
|
|---|
| 650 | for( iTransfer = 0;
|
|---|
| 651 | iTransfer < G4int((*fPAItransferTable)(iPlace)->GetVectorLength()); iTransfer++ )
|
|---|
| 652 | {
|
|---|
| 653 | if(position >= (*(*fPAItransferTable)(iPlace))(iTransfer)) break ;
|
|---|
| 654 | }
|
|---|
| 655 | transfer = GetEnergyTransfer(iPlace,position,iTransfer);
|
|---|
| 656 | }
|
|---|
| 657 | else
|
|---|
| 658 | {
|
|---|
| 659 | dNdxCut2 = (*fdNdxCutVector)(iPlace+1) ;
|
|---|
| 660 | // G4cout<<"dNdxCut2 = "<<dNdxCut2<<G4endl ;
|
|---|
| 661 | if(iTkin == 0) // Tkin is too small, trying from right only
|
|---|
| 662 | {
|
|---|
| 663 | position = dNdxCut2*G4UniformRand() ;
|
|---|
| 664 |
|
|---|
| 665 | for( iTransfer = 0;
|
|---|
| 666 | iTransfer < G4int((*fPAItransferTable)(iPlace+1)->GetVectorLength()); iTransfer++ )
|
|---|
| 667 | {
|
|---|
| 668 | if(position >= (*(*fPAItransferTable)(iPlace+1))(iTransfer)) break ;
|
|---|
| 669 | }
|
|---|
| 670 | transfer = GetEnergyTransfer(iPlace+1,position,iTransfer);
|
|---|
| 671 | }
|
|---|
| 672 | else // general case: Tkin between two vectors of the material
|
|---|
| 673 | {
|
|---|
| 674 | E1 = fParticleEnergyVector->GetLowEdgeEnergy(iTkin - 1) ;
|
|---|
| 675 | E2 = fParticleEnergyVector->GetLowEdgeEnergy(iTkin) ;
|
|---|
| 676 | W = 1.0/(E2 - E1) ;
|
|---|
| 677 | W1 = (E2 - scaledTkin)*W ;
|
|---|
| 678 | W2 = (scaledTkin - E1)*W ;
|
|---|
| 679 |
|
|---|
| 680 | position = ( dNdxCut1*W1 + dNdxCut2*W2 )*G4UniformRand() ;
|
|---|
| 681 |
|
|---|
| 682 | // G4cout<<position<<"\t" ;
|
|---|
| 683 |
|
|---|
| 684 | G4int iTrMax1, iTrMax2, iTrMax;
|
|---|
| 685 |
|
|---|
| 686 | iTrMax1 = G4int((*fPAItransferTable)(iPlace)->GetVectorLength());
|
|---|
| 687 | iTrMax2 = G4int((*fPAItransferTable)(iPlace+1)->GetVectorLength());
|
|---|
| 688 |
|
|---|
| 689 | if (iTrMax1 >= iTrMax2) iTrMax = iTrMax2;
|
|---|
| 690 | else iTrMax = iTrMax1;
|
|---|
| 691 |
|
|---|
| 692 |
|
|---|
| 693 | for( iTransfer = 0; iTransfer < iTrMax; iTransfer++ )
|
|---|
| 694 | {
|
|---|
| 695 | if( position >=
|
|---|
| 696 | ( (*(*fPAItransferTable)(iPlace))(iTransfer)*W1 +
|
|---|
| 697 | (*(*fPAItransferTable)(iPlace+1))(iTransfer)*W2) ) break ;
|
|---|
| 698 | }
|
|---|
| 699 | transfer = GetEnergyTransfer(iPlace,position,iTransfer);
|
|---|
| 700 | }
|
|---|
| 701 | }
|
|---|
| 702 | // G4cout<<"PAImodel PostStepTransfer = "<<transfer/keV<<" keV"<<G4endl ;
|
|---|
| 703 | if(transfer < 0.0 ) transfer = 0.0 ;
|
|---|
| 704 | // if(transfer < DBL_MIN ) transfer = DBL_MIN;
|
|---|
| 705 |
|
|---|
| 706 | return transfer ;
|
|---|
| 707 | }
|
|---|
| 708 |
|
|---|
| 709 | ///////////////////////////////////////////////////////////////////////
|
|---|
| 710 | //
|
|---|
| 711 | // Returns random PAI energy transfer according to passed
|
|---|
| 712 | // indexes of particle kinetic
|
|---|
| 713 |
|
|---|
| 714 | G4double
|
|---|
| 715 | G4PAIModel::GetEnergyTransfer( G4int iPlace, G4double position, G4int iTransfer )
|
|---|
| 716 | {
|
|---|
| 717 | G4int iTransferMax;
|
|---|
| 718 | G4double x1, x2, y1, y2, energyTransfer;
|
|---|
| 719 |
|
|---|
| 720 | if(iTransfer == 0)
|
|---|
| 721 | {
|
|---|
| 722 | energyTransfer = (*fPAItransferTable)(iPlace)->GetLowEdgeEnergy(iTransfer);
|
|---|
| 723 | }
|
|---|
| 724 | else
|
|---|
| 725 | {
|
|---|
| 726 | iTransferMax = G4int((*fPAItransferTable)(iPlace)->GetVectorLength());
|
|---|
| 727 |
|
|---|
| 728 | if ( iTransfer >= iTransferMax ) iTransfer = iTransferMax - 1;
|
|---|
| 729 |
|
|---|
| 730 | y1 = (*(*fPAItransferTable)(iPlace))(iTransfer-1);
|
|---|
| 731 | y2 = (*(*fPAItransferTable)(iPlace))(iTransfer);
|
|---|
| 732 |
|
|---|
| 733 | x1 = (*fPAItransferTable)(iPlace)->GetLowEdgeEnergy(iTransfer-1);
|
|---|
| 734 | x2 = (*fPAItransferTable)(iPlace)->GetLowEdgeEnergy(iTransfer);
|
|---|
| 735 |
|
|---|
| 736 | if ( x1 == x2 ) energyTransfer = x2;
|
|---|
| 737 | else
|
|---|
| 738 | {
|
|---|
| 739 | if ( y1 == y2 ) energyTransfer = x1 + (x2 - x1)*G4UniformRand();
|
|---|
| 740 | else
|
|---|
| 741 | {
|
|---|
| 742 | energyTransfer = x1 + (position - y1)*(x2 - x1)/(y2 - y1);
|
|---|
| 743 | }
|
|---|
| 744 | }
|
|---|
| 745 | }
|
|---|
| 746 | return energyTransfer;
|
|---|
| 747 | }
|
|---|
| 748 |
|
|---|
| 749 | ///////////////////////////////////////////////////////////////////////
|
|---|
| 750 |
|
|---|
| 751 | G4double G4PAIModel::SampleFluctuations( const G4Material* material,
|
|---|
| 752 | const G4DynamicParticle* aParticle,
|
|---|
| 753 | G4double&,
|
|---|
| 754 | G4double& step,
|
|---|
| 755 | G4double&)
|
|---|
| 756 | {
|
|---|
| [1196] | 757 | size_t jMat = 0;
|
|---|
| 758 | for(;jMat < fMaterialCutsCoupleVector.size(); ++jMat )
|
|---|
| [819] | 759 | {
|
|---|
| 760 | if( material == fMaterialCutsCoupleVector[jMat]->GetMaterial() ) break;
|
|---|
| 761 | }
|
|---|
| [1196] | 762 | if(jMat == fMaterialCutsCoupleVector.size()) return 0.0;
|
|---|
| [819] | 763 |
|
|---|
| 764 | fPAItransferTable = fPAIxscBank[jMat];
|
|---|
| 765 | fdNdxCutVector = fdNdxCutTable[jMat];
|
|---|
| 766 |
|
|---|
| [1196] | 767 | G4int iTkin, iTransfer, iPlace;
|
|---|
| [819] | 768 | G4long numOfCollisions=0;
|
|---|
| 769 |
|
|---|
| [1196] | 770 | //G4cout<<"G4PAIModel::SampleFluctuations"<<G4endl ;
|
|---|
| 771 | //G4cout<<"in: "<<fMaterialCutsCoupleVector[jMat]->GetMaterial()->GetName()<<G4endl;
|
|---|
| [819] | 772 | G4double loss = 0.0, charge2 ;
|
|---|
| 773 | G4double stepSum = 0., stepDelta, lambda, omega;
|
|---|
| 774 | G4double position, E1, E2, W1, W2, W, dNdxCut1, dNdxCut2, meanNumber;
|
|---|
| 775 | G4bool numb = true;
|
|---|
| 776 | G4double Tkin = aParticle->GetKineticEnergy() ;
|
|---|
| 777 | G4double MassRatio = fMass/aParticle->GetDefinition()->GetPDGMass() ;
|
|---|
| 778 | G4double charge = aParticle->GetDefinition()->GetPDGCharge() ;
|
|---|
| 779 | charge2 = charge*charge ;
|
|---|
| 780 | G4double TkinScaled = Tkin*MassRatio ;
|
|---|
| 781 |
|
|---|
| [1196] | 782 | for(iTkin=0;iTkin<=fTotBin;iTkin++)
|
|---|
| [819] | 783 | {
|
|---|
| 784 | if(TkinScaled < fParticleEnergyVector->GetLowEdgeEnergy(iTkin)) break ;
|
|---|
| 785 | }
|
|---|
| 786 | iPlace = iTkin - 1 ;
|
|---|
| 787 | if(iPlace < 0) iPlace = 0;
|
|---|
| [1196] | 788 | else if(iPlace >= fTotBin) iPlace = fTotBin - 1;
|
|---|
| 789 | //G4cout<<"from search, iPlace = "<<iPlace<<G4endl ;
|
|---|
| [819] | 790 | dNdxCut1 = (*fdNdxCutVector)(iPlace) ;
|
|---|
| [1196] | 791 | //G4cout<<"dNdxCut1 = "<<dNdxCut1<<G4endl ;
|
|---|
| [819] | 792 |
|
|---|
| 793 | if(iTkin == fTotBin) // Fermi plato, try from left
|
|---|
| 794 | {
|
|---|
| 795 | meanNumber =((*(*fPAItransferTable)(iPlace))(0)-dNdxCut1)*step*charge2;
|
|---|
| 796 | if(meanNumber < 0.) meanNumber = 0. ;
|
|---|
| 797 | // numOfCollisions = RandPoisson::shoot(meanNumber) ;
|
|---|
| 798 | // numOfCollisions = G4Poisson(meanNumber) ;
|
|---|
| 799 | if( meanNumber > 0.) lambda = step/meanNumber;
|
|---|
| 800 | else lambda = DBL_MAX;
|
|---|
| 801 | while(numb)
|
|---|
| 802 | {
|
|---|
| 803 | stepDelta = CLHEP::RandExponential::shoot(lambda);
|
|---|
| 804 | stepSum += stepDelta;
|
|---|
| 805 | if(stepSum >= step) break;
|
|---|
| 806 | numOfCollisions++;
|
|---|
| 807 | }
|
|---|
| [1196] | 808 | //G4cout<<"##1 numOfCollisions = "<<numOfCollisions<<G4endl ;
|
|---|
| [819] | 809 |
|
|---|
| 810 | while(numOfCollisions)
|
|---|
| 811 | {
|
|---|
| 812 | position = dNdxCut1+
|
|---|
| 813 | ((*(*fPAItransferTable)(iPlace))(0)-dNdxCut1)*G4UniformRand() ;
|
|---|
| 814 |
|
|---|
| 815 | for( iTransfer = 0;
|
|---|
| 816 | iTransfer < G4int((*fPAItransferTable)(iPlace)->GetVectorLength()); iTransfer++ )
|
|---|
| 817 | {
|
|---|
| 818 | if(position >= (*(*fPAItransferTable)(iPlace))(iTransfer)) break ;
|
|---|
| 819 | }
|
|---|
| 820 | omega = GetEnergyTransfer(iPlace,position,iTransfer);
|
|---|
| [1196] | 821 | //G4cout<<"G4PAIModel::SampleFluctuations, omega = "<<omega/keV<<" keV; "<<"\t";
|
|---|
| [819] | 822 | loss += omega;
|
|---|
| 823 | numOfCollisions-- ;
|
|---|
| 824 | }
|
|---|
| 825 | }
|
|---|
| 826 | else
|
|---|
| 827 | {
|
|---|
| 828 | dNdxCut2 = (*fdNdxCutVector)(iPlace+1) ;
|
|---|
| [1196] | 829 | //G4cout<<"dNdxCut2 = "<<dNdxCut2<< " iTkin= "<<iTkin<<" iPlace= "<<iPlace<<G4endl;
|
|---|
| [819] | 830 |
|
|---|
| 831 | if(iTkin == 0) // Tkin is too small, trying from right only
|
|---|
| 832 | {
|
|---|
| 833 | meanNumber =((*(*fPAItransferTable)(iPlace+1))(0)-dNdxCut2)*step*charge2;
|
|---|
| 834 | if( meanNumber < 0. ) meanNumber = 0. ;
|
|---|
| 835 | // numOfCollisions = CLHEP::RandPoisson::shoot(meanNumber) ;
|
|---|
| 836 | // numOfCollisions = G4Poisson(meanNumber) ;
|
|---|
| [1196] | 837 | if( meanNumber > 0.) lambda = step/meanNumber;
|
|---|
| 838 | else lambda = DBL_MAX;
|
|---|
| 839 | while(numb)
|
|---|
| 840 | {
|
|---|
| 841 | stepDelta = CLHEP::RandExponential::shoot(lambda);
|
|---|
| 842 | stepSum += stepDelta;
|
|---|
| 843 | if(stepSum >= step) break;
|
|---|
| 844 | numOfCollisions++;
|
|---|
| 845 | }
|
|---|
| [819] | 846 |
|
|---|
| [1196] | 847 | //G4cout<<"##2 numOfCollisions = "<<numOfCollisions<<G4endl ;
|
|---|
| [819] | 848 |
|
|---|
| 849 | while(numOfCollisions)
|
|---|
| 850 | {
|
|---|
| 851 | position = dNdxCut2+
|
|---|
| 852 | ((*(*fPAItransferTable)(iPlace+1))(0)-dNdxCut2)*G4UniformRand();
|
|---|
| 853 |
|
|---|
| 854 | for( iTransfer = 0;
|
|---|
| 855 | iTransfer < G4int((*fPAItransferTable)(iPlace+1)->GetVectorLength()); iTransfer++ )
|
|---|
| 856 | {
|
|---|
| 857 | if(position >= (*(*fPAItransferTable)(iPlace+1))(iTransfer)) break ;
|
|---|
| 858 | }
|
|---|
| 859 | omega = GetEnergyTransfer(iPlace,position,iTransfer);
|
|---|
| [1196] | 860 | //G4cout<<omega/keV<<"\t";
|
|---|
| [819] | 861 | loss += omega;
|
|---|
| 862 | numOfCollisions-- ;
|
|---|
| 863 | }
|
|---|
| 864 | }
|
|---|
| 865 | else // general case: Tkin between two vectors of the material
|
|---|
| 866 | {
|
|---|
| 867 | E1 = fParticleEnergyVector->GetLowEdgeEnergy(iTkin - 1) ;
|
|---|
| 868 | E2 = fParticleEnergyVector->GetLowEdgeEnergy(iTkin) ;
|
|---|
| 869 | W = 1.0/(E2 - E1) ;
|
|---|
| 870 | W1 = (E2 - TkinScaled)*W ;
|
|---|
| 871 | W2 = (TkinScaled - E1)*W ;
|
|---|
| 872 |
|
|---|
| [1196] | 873 | //G4cout << fPAItransferTable->size() << G4endl;
|
|---|
| 874 | //G4cout<<"(*(*fPAItransferTable)(iPlace))(0) = "<<
|
|---|
| [819] | 875 | // (*(*fPAItransferTable)(iPlace))(0)<<G4endl ;
|
|---|
| [1196] | 876 | //G4cout<<"(*(*fPAItransferTable)(iPlace+1))(0) = "<<
|
|---|
| [819] | 877 | // (*(*fPAItransferTable)(iPlace+1))(0)<<G4endl ;
|
|---|
| 878 |
|
|---|
| 879 | meanNumber=( ((*(*fPAItransferTable)(iPlace))(0)-dNdxCut1)*W1 +
|
|---|
| 880 | ((*(*fPAItransferTable)(iPlace+1))(0)-dNdxCut2)*W2 )*step*charge2;
|
|---|
| 881 | if(meanNumber<0.0) meanNumber = 0.0;
|
|---|
| 882 | // numOfCollisions = RandPoisson::shoot(meanNumber) ;
|
|---|
| 883 | // numOfCollisions = G4Poisson(meanNumber) ;
|
|---|
| [1196] | 884 | if( meanNumber > 0.) lambda = step/meanNumber;
|
|---|
| 885 | else lambda = DBL_MAX;
|
|---|
| 886 | while(numb)
|
|---|
| 887 | {
|
|---|
| 888 | stepDelta = CLHEP::RandExponential::shoot(lambda);
|
|---|
| 889 | stepSum += stepDelta;
|
|---|
| 890 | if(stepSum >= step) break;
|
|---|
| 891 | numOfCollisions++;
|
|---|
| 892 | }
|
|---|
| [819] | 893 |
|
|---|
| [1196] | 894 | //G4cout<<"##3 numOfCollisions = "<<numOfCollisions<<endl ;
|
|---|
| [819] | 895 |
|
|---|
| 896 | while(numOfCollisions)
|
|---|
| 897 | {
|
|---|
| 898 | position = dNdxCut1*W1 + dNdxCut2*W2 +
|
|---|
| 899 | ( ( (*(*fPAItransferTable)(iPlace))(0)-dNdxCut1 )*W1 +
|
|---|
| 900 | dNdxCut2+
|
|---|
| 901 | ( (*(*fPAItransferTable)(iPlace+1))(0)-dNdxCut2 )*W2 )*G4UniformRand();
|
|---|
| 902 |
|
|---|
| 903 | // G4cout<<position<<"\t" ;
|
|---|
| 904 |
|
|---|
| 905 | for( iTransfer = 0;
|
|---|
| 906 | iTransfer < G4int((*fPAItransferTable)(iPlace)->GetVectorLength()); iTransfer++ )
|
|---|
| 907 | {
|
|---|
| 908 | if( position >=
|
|---|
| 909 | ( (*(*fPAItransferTable)(iPlace))(iTransfer)*W1 +
|
|---|
| 910 | (*(*fPAItransferTable)(iPlace+1))(iTransfer)*W2) )
|
|---|
| 911 | {
|
|---|
| 912 | break ;
|
|---|
| 913 | }
|
|---|
| 914 | }
|
|---|
| 915 | omega = GetEnergyTransfer(iPlace,position,iTransfer);
|
|---|
| 916 | // G4cout<<omega/keV<<"\t";
|
|---|
| 917 | loss += omega;
|
|---|
| 918 | numOfCollisions-- ;
|
|---|
| 919 | }
|
|---|
| 920 | }
|
|---|
| 921 | }
|
|---|
| [1196] | 922 | //G4cout<<"PAIModel AlongStepLoss = "<<loss/keV<<" keV, on step = "
|
|---|
| [819] | 923 | // <<step/mm<<" mm"<<G4endl ;
|
|---|
| 924 | if(loss > Tkin) loss=Tkin;
|
|---|
| 925 | if(loss < 0. ) loss = 0.;
|
|---|
| 926 | return loss ;
|
|---|
| 927 |
|
|---|
| 928 | }
|
|---|
| 929 |
|
|---|
| 930 | //////////////////////////////////////////////////////////////////////
|
|---|
| 931 | //
|
|---|
| 932 | // Returns the statistical estimation of the energy loss distribution variance
|
|---|
| 933 | //
|
|---|
| 934 |
|
|---|
| 935 |
|
|---|
| 936 | G4double G4PAIModel::Dispersion( const G4Material* material,
|
|---|
| 937 | const G4DynamicParticle* aParticle,
|
|---|
| 938 | G4double& tmax,
|
|---|
| 939 | G4double& step )
|
|---|
| 940 | {
|
|---|
| 941 | G4double loss, sumLoss=0., sumLoss2=0., sigma2, meanLoss=0.;
|
|---|
| 942 | for(G4int i = 0 ; i < fMeanNumber; i++)
|
|---|
| 943 | {
|
|---|
| 944 | loss = SampleFluctuations(material,aParticle,tmax,step,meanLoss);
|
|---|
| 945 | sumLoss += loss;
|
|---|
| 946 | sumLoss2 += loss*loss;
|
|---|
| 947 | }
|
|---|
| 948 | meanLoss = sumLoss/fMeanNumber;
|
|---|
| 949 | sigma2 = meanLoss*meanLoss + (sumLoss2-2*sumLoss*meanLoss)/fMeanNumber;
|
|---|
| 950 | return sigma2;
|
|---|
| 951 | }
|
|---|
| 952 |
|
|---|
| [1055] | 953 | /////////////////////////////////////////////////////////////////////
|
|---|
| [819] | 954 |
|
|---|
| [1055] | 955 | G4double G4PAIModel::MaxSecondaryEnergy( const G4ParticleDefinition* p,
|
|---|
| 956 | G4double kinEnergy)
|
|---|
| 957 | {
|
|---|
| 958 | G4double tmax = kinEnergy;
|
|---|
| 959 | if(p == fElectron) tmax *= 0.5;
|
|---|
| 960 | else if(p != fPositron) {
|
|---|
| 961 | G4double mass = p->GetPDGMass();
|
|---|
| 962 | G4double ratio= electron_mass_c2/mass;
|
|---|
| 963 | G4double gamma= kinEnergy/mass + 1.0;
|
|---|
| 964 | tmax = 2.0*electron_mass_c2*(gamma*gamma - 1.) /
|
|---|
| 965 | (1. + 2.0*gamma*ratio + ratio*ratio);
|
|---|
| 966 | }
|
|---|
| 967 | return tmax;
|
|---|
| 968 | }
|
|---|
| 969 |
|
|---|
| 970 | ///////////////////////////////////////////////////////////////
|
|---|
| 971 |
|
|---|
| 972 | void G4PAIModel::DefineForRegion(const G4Region* r)
|
|---|
| 973 | {
|
|---|
| 974 | fPAIRegionVector.push_back(r);
|
|---|
| 975 | }
|
|---|
| 976 |
|
|---|
| [819] | 977 | //
|
|---|
| 978 | //
|
|---|
| 979 | /////////////////////////////////////////////////
|
|---|
| 980 |
|
|---|
| 981 |
|
|---|
| 982 |
|
|---|
| 983 |
|
|---|
| 984 |
|
|---|
| 985 |
|
|---|