| [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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| [961] | 26 | // $Id: G4eplusPolarizedAnnihilation.cc,v 1.8 2008/10/30 22:34:23 schaelic Exp $
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| [1337] | 27 | // GEANT4 tag $Name: geant4-09-04-beta-01 $
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| [819] | 28 | //
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| 29 | // -------------------------------------------------------------------
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| 30 | //
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| 31 | // GEANT4 Class file
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| 32 | //
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| 33 | //
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| 34 | // File name: G4eplusPolarizedAnnihilation
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| 35 | //
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| 36 | // Author: A. Schaelicke on base of Vladimir Ivanchenko / Michel Maire code
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| 37 | //
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| 38 | // Creation date: 02.07.2006
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| 39 | //
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| 40 | // Modifications:
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| 41 | // 26-07-06 modified cross section (P. Starovoitov)
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| 42 | // 21-08-06 interface updated (A. Schaelicke)
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| 43 | // 11-06-07, add PostStepGetPhysicalInteractionLength (A.Schalicke)
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| 44 | // 02-10-07, enable AtRest (V.Ivanchenko)
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| 45 | //
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| 46 | //
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| 47 | // Class Description:
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| 48 | //
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| 49 | // Polarized process of e+ annihilation into 2 gammas
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| 50 | //
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| 51 |
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| 52 | //
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| 53 | // -------------------------------------------------------------------
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| 54 | //
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| 55 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 56 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 57 |
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| 58 | #include "G4eplusPolarizedAnnihilation.hh"
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| 59 | #include "G4MaterialCutsCouple.hh"
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| 60 | #include "G4Gamma.hh"
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| 61 | #include "G4PhysicsVector.hh"
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| 62 | #include "G4PhysicsLogVector.hh"
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| 63 |
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| 64 |
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| 65 | #include "G4PolarizedAnnihilationModel.hh"
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| 66 | #include "G4PhysicsTableHelper.hh"
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| 67 | #include "G4ProductionCutsTable.hh"
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| 68 | #include "G4PolarizationManager.hh"
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| 69 | #include "G4PolarizationHelper.hh"
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| 70 | #include "G4StokesVector.hh"
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| 71 |
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| 72 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 73 |
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| 74 | G4eplusPolarizedAnnihilation::G4eplusPolarizedAnnihilation(const G4String& name)
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| 75 | : G4VEmProcess(name), isInitialised(false),
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| 76 | theAsymmetryTable(NULL),
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| 77 | theTransverseAsymmetryTable(NULL)
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| 78 | {
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| 79 | enableAtRestDoIt = true;
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| [961] | 80 | SetProcessSubType(fAnnihilation);
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| [819] | 81 | }
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| 82 |
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| 83 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 84 |
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| 85 | G4eplusPolarizedAnnihilation::~G4eplusPolarizedAnnihilation()
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| 86 | {
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| 87 | if (theAsymmetryTable) {
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| 88 | theAsymmetryTable->clearAndDestroy();
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| 89 | delete theAsymmetryTable;
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| 90 | }
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| 91 | if (theTransverseAsymmetryTable) {
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| 92 | theTransverseAsymmetryTable->clearAndDestroy();
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| 93 | delete theTransverseAsymmetryTable;
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| 94 | }
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| 95 | }
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| 96 |
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| 97 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 98 |
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| 99 | void G4eplusPolarizedAnnihilation::InitialiseProcess(const G4ParticleDefinition*)
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| 100 | {
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| 101 | if(!isInitialised) {
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| 102 | isInitialised = true;
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| 103 | // SetVerboseLevel(3);
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| 104 | SetBuildTableFlag(true);
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| 105 | SetStartFromNullFlag(false);
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| 106 | SetSecondaryParticle(G4Gamma::Gamma());
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| 107 | G4double emin = 0.1*keV;
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| 108 | G4double emax = 100.*TeV;
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| 109 | SetLambdaBinning(120);
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| 110 | SetMinKinEnergy(emin);
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| 111 | SetMaxKinEnergy(emax);
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| 112 | emModel = new G4PolarizedAnnihilationModel();
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| 113 | emModel->SetLowEnergyLimit(emin);
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| 114 | emModel->SetHighEnergyLimit(emax);
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| 115 | AddEmModel(1, emModel);
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| 116 | }
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| 117 | }
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| 118 |
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| 119 |
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| 120 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 121 |
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| 122 | // for polarization
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| 123 |
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| 124 | G4double G4eplusPolarizedAnnihilation::GetMeanFreePath(const G4Track& track,
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| 125 | G4double previousStepSize,
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| 126 | G4ForceCondition* condition)
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| 127 | {
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| 128 | G4double mfp = G4VEmProcess::GetMeanFreePath(track, previousStepSize, condition);
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| 129 |
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| 130 | if (theAsymmetryTable) {
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| 131 |
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| 132 | G4Material* aMaterial = track.GetMaterial();
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| 133 | G4VPhysicalVolume* aPVolume = track.GetVolume();
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| 134 | G4LogicalVolume* aLVolume = aPVolume->GetLogicalVolume();
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| 135 |
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| 136 | // G4Material* bMaterial = aLVolume->GetMaterial();
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| 137 | G4PolarizationManager * polarizationManger = G4PolarizationManager::GetInstance();
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| 138 |
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| 139 | const G4bool volumeIsPolarized = polarizationManger->IsPolarized(aLVolume);
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| 140 | G4StokesVector electronPolarization = polarizationManger->GetVolumePolarization(aLVolume);
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| 141 |
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| 142 | if (!volumeIsPolarized || mfp == DBL_MAX) return mfp;
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| 143 |
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| 144 | // *** get asymmetry, if target is polarized ***
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| 145 | const G4DynamicParticle* aDynamicPositron = track.GetDynamicParticle();
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| 146 | const G4double positronEnergy = aDynamicPositron->GetKineticEnergy();
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| 147 | const G4StokesVector positronPolarization = track.GetPolarization();
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| 148 | const G4ParticleMomentum positronDirection0 = aDynamicPositron->GetMomentumDirection();
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| 149 |
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| 150 | if (verboseLevel>=2) {
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| 151 |
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| 152 | G4cout << " Mom " << positronDirection0 << G4endl;
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| 153 | G4cout << " Polarization " << positronPolarization << G4endl;
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| 154 | G4cout << " MaterialPol. " << electronPolarization << G4endl;
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| 155 | G4cout << " Phys. Volume " << aPVolume->GetName() << G4endl;
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| 156 | G4cout << " Log. Volume " << aLVolume->GetName() << G4endl;
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| 157 | G4cout << " Material " << aMaterial << G4endl;
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| 158 | }
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| 159 |
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| 160 | G4bool isOutRange;
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| 161 | G4int idx= CurrentMaterialCutsCoupleIndex();
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| 162 | G4double lAsymmetry = (*theAsymmetryTable)(idx)->
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| 163 | GetValue(positronEnergy, isOutRange);
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| 164 | G4double tAsymmetry = (*theTransverseAsymmetryTable)(idx)->
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| 165 | GetValue(positronEnergy, isOutRange);
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| 166 |
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| 167 | G4double polZZ = positronPolarization.z()*
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| 168 | electronPolarization*positronDirection0;
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| 169 | G4double polXX = positronPolarization.x()*
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| 170 | electronPolarization*G4PolarizationHelper::GetParticleFrameX(positronDirection0);
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| 171 | G4double polYY = positronPolarization.y()*
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| 172 | electronPolarization*G4PolarizationHelper::GetParticleFrameY(positronDirection0);
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| 173 |
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| 174 | G4double impact = 1. + polZZ*lAsymmetry + (polXX + polYY)*tAsymmetry;
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| 175 |
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| 176 | mfp *= 1. / impact;
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| 177 |
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| 178 | if (verboseLevel>=2) {
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| 179 | G4cout << " MeanFreePath: " << mfp / mm << " mm " << G4endl;
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| 180 | G4cout << " Asymmetry: " << lAsymmetry << ", " << tAsymmetry << G4endl;
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| 181 | G4cout << " PolProduct: " << polXX << ", " << polYY << ", " << polZZ << G4endl;
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| 182 | }
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| 183 | }
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| 184 |
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| 185 | return mfp;
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| 186 | }
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| 187 |
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| 188 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 189 |
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| 190 | G4double G4eplusPolarizedAnnihilation::PostStepGetPhysicalInteractionLength(
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| 191 | const G4Track& track,
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| 192 | G4double previousStepSize,
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| 193 | G4ForceCondition* condition)
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| 194 | {
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| 195 | G4double mfp = G4VEmProcess::PostStepGetPhysicalInteractionLength(track, previousStepSize, condition);
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| 196 |
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| 197 | if (theAsymmetryTable) {
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| 198 |
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| 199 | G4Material* aMaterial = track.GetMaterial();
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| 200 | G4VPhysicalVolume* aPVolume = track.GetVolume();
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| 201 | G4LogicalVolume* aLVolume = aPVolume->GetLogicalVolume();
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| 202 |
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| 203 | // G4Material* bMaterial = aLVolume->GetMaterial();
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| 204 | G4PolarizationManager * polarizationManger = G4PolarizationManager::GetInstance();
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| 205 |
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| 206 | const G4bool volumeIsPolarized = polarizationManger->IsPolarized(aLVolume);
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| 207 | G4StokesVector electronPolarization = polarizationManger->GetVolumePolarization(aLVolume);
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| 208 |
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| 209 | if (!volumeIsPolarized || mfp == DBL_MAX) return mfp;
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| 210 |
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| 211 | // *** get asymmetry, if target is polarized ***
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| 212 | const G4DynamicParticle* aDynamicPositron = track.GetDynamicParticle();
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| 213 | const G4double positronEnergy = aDynamicPositron->GetKineticEnergy();
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| 214 | const G4StokesVector positronPolarization = track.GetPolarization();
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| 215 | const G4ParticleMomentum positronDirection0 = aDynamicPositron->GetMomentumDirection();
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| 216 |
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| 217 | if (verboseLevel>=2) {
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| 218 |
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| 219 | G4cout << " Mom " << positronDirection0 << G4endl;
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| 220 | G4cout << " Polarization " << positronPolarization << G4endl;
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| 221 | G4cout << " MaterialPol. " << electronPolarization << G4endl;
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| 222 | G4cout << " Phys. Volume " << aPVolume->GetName() << G4endl;
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| 223 | G4cout << " Log. Volume " << aLVolume->GetName() << G4endl;
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| 224 | G4cout << " Material " << aMaterial << G4endl;
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| 225 | }
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| 226 |
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| 227 | G4bool isOutRange;
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| 228 | G4int idx= CurrentMaterialCutsCoupleIndex();
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| 229 | G4double lAsymmetry = (*theAsymmetryTable)(idx)->
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| 230 | GetValue(positronEnergy, isOutRange);
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| 231 | G4double tAsymmetry = (*theTransverseAsymmetryTable)(idx)->
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| 232 | GetValue(positronEnergy, isOutRange);
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| 233 |
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| 234 | G4double polZZ = positronPolarization.z()*
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| 235 | electronPolarization*positronDirection0;
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| 236 | G4double polXX = positronPolarization.x()*
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| 237 | electronPolarization*G4PolarizationHelper::GetParticleFrameX(positronDirection0);
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| 238 | G4double polYY = positronPolarization.y()*
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| 239 | electronPolarization*G4PolarizationHelper::GetParticleFrameY(positronDirection0);
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| 240 |
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| 241 | G4double impact = 1. + polZZ*lAsymmetry + (polXX + polYY)*tAsymmetry;
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| 242 |
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| 243 | mfp *= 1. / impact;
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| 244 |
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| 245 | if (verboseLevel>=2) {
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| 246 | G4cout << " MeanFreePath: " << mfp / mm << " mm " << G4endl;
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| 247 | G4cout << " Asymmetry: " << lAsymmetry << ", " << tAsymmetry << G4endl;
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| 248 | G4cout << " PolProduct: " << polXX << ", " << polYY << ", " << polZZ << G4endl;
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| 249 | }
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| 250 | }
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| 251 |
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| 252 | return mfp;
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| 253 | }
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| 254 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 255 |
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| 256 | void G4eplusPolarizedAnnihilation::BuildPhysicsTable(const G4ParticleDefinition& pd)
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| 257 | {
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| 258 | G4VEmProcess::BuildPhysicsTable(pd);
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| 259 | BuildAsymmetryTable(pd);
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| 260 | }
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| 261 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 262 |
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| 263 | void G4eplusPolarizedAnnihilation::PreparePhysicsTable(const G4ParticleDefinition& pd)
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| 264 | {
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| 265 | G4VEmProcess::PreparePhysicsTable(pd);
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| 266 | theAsymmetryTable = G4PhysicsTableHelper::PreparePhysicsTable(theAsymmetryTable);
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| 267 | theTransverseAsymmetryTable = G4PhysicsTableHelper::PreparePhysicsTable(theTransverseAsymmetryTable);
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| 268 | }
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| 269 |
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| 270 | void G4eplusPolarizedAnnihilation::BuildAsymmetryTable(const G4ParticleDefinition& part)
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| 271 | {
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| 272 | // Access to materials
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| 273 | const G4ProductionCutsTable* theCoupleTable=
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| 274 | G4ProductionCutsTable::GetProductionCutsTable();
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| 275 | size_t numOfCouples = theCoupleTable->GetTableSize();
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| 276 | G4cout<<" annih-numOfCouples="<<numOfCouples<<"\n";
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| 277 | for(size_t i=0; i<numOfCouples; ++i) {
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| 278 | G4cout<<"annih- "<<i<<"/"<<numOfCouples<<"\n";
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| 279 | if (!theAsymmetryTable) break;
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| 280 | G4cout<<"annih- "<<theAsymmetryTable->GetFlag(i)<<"\n";
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| 281 | if (theAsymmetryTable->GetFlag(i)) {
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| 282 | G4cout<<" building pol-annih ... \n";
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| 283 |
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| 284 | // create physics vector and fill it
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| 285 | const G4MaterialCutsCouple* couple = theCoupleTable->GetMaterialCutsCouple(i);
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| 286 |
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| 287 | // use same parameters as for lambda
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| 288 | G4PhysicsVector* aVector = LambdaPhysicsVector(couple);
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| 289 | G4PhysicsVector* tVector = LambdaPhysicsVector(couple);
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| 290 |
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| 291 | for (G4int j = 0 ; j < LambdaBinning() ; ++j ) {
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| 292 | G4double lowEdgeEnergy = aVector->GetLowEdgeEnergy(j);
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| 293 | G4double tasm=0.;
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| 294 | G4double asym = ComputeAsymmetry(lowEdgeEnergy, couple, part, 0., tasm);
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| 295 | aVector->PutValue(j,asym);
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| 296 | tVector->PutValue(j,tasm);
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| 297 | }
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| 298 |
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| 299 | G4PhysicsTableHelper::SetPhysicsVector(theAsymmetryTable, i, aVector);
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| 300 | G4PhysicsTableHelper::SetPhysicsVector(theTransverseAsymmetryTable, i, tVector);
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| 301 | }
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| 302 | }
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| 303 |
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| 304 | }
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| 305 |
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| 306 |
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| 307 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 308 |
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| 309 | G4double G4eplusPolarizedAnnihilation::ComputeAsymmetry(G4double energy,
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| 310 | const G4MaterialCutsCouple* couple,
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| 311 | const G4ParticleDefinition& aParticle,
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| 312 | G4double cut,
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| 313 | G4double &tAsymmetry)
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| 314 | {
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| 315 | G4double lAsymmetry = 0.0;
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| 316 | tAsymmetry = 0.0;
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| 317 |
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| 318 | // calculate polarized cross section
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| 319 | theTargetPolarization=G4ThreeVector(0.,0.,1.);
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| 320 | emModel->SetTargetPolarization(theTargetPolarization);
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| 321 | emModel->SetBeamPolarization(theTargetPolarization);
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| 322 | G4double sigma2=emModel->CrossSection(couple,&aParticle,energy,cut,energy);
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| 323 |
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| 324 | // calculate transversely polarized cross section
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| 325 | theTargetPolarization=G4ThreeVector(1.,0.,0.);
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| 326 | emModel->SetTargetPolarization(theTargetPolarization);
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| 327 | emModel->SetBeamPolarization(theTargetPolarization);
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| 328 | G4double sigma3=emModel->CrossSection(couple,&aParticle,energy,cut,energy);
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| 329 |
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| 330 | // calculate unpolarized cross section
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| 331 | theTargetPolarization=G4ThreeVector();
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| 332 | emModel->SetTargetPolarization(theTargetPolarization);
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| 333 | emModel->SetBeamPolarization(theTargetPolarization);
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| 334 | G4double sigma0=emModel->CrossSection(couple,&aParticle,energy,cut,energy);
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| 335 |
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| 336 | // determine assymmetries
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| 337 | if (sigma0>0.) {
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| 338 | lAsymmetry=sigma2/sigma0-1.;
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| 339 | tAsymmetry=sigma3/sigma0-1.;
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| 340 | }
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| 341 | return lAsymmetry;
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| 342 |
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| 343 | }
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| 344 |
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| 345 |
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| 346 |
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| 347 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 348 |
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| 349 | void G4eplusPolarizedAnnihilation::PrintInfo()
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| 350 | {
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| 351 | G4cout << " Polarized model for annihilation into 2 photons"
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| 352 | << G4endl;
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| 353 | }
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| 354 |
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| 355 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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| 356 |
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| 357 | G4VParticleChange* G4eplusPolarizedAnnihilation::AtRestDoIt(const G4Track& aTrack,
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| 358 | const G4Step& )
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| 359 | //
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| 360 | // Performs the e+ e- annihilation when both particles are assumed at rest.
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| 361 | // It generates two back to back photons with energy = electron_mass.
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| 362 | // The angular distribution is isotropic.
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| 363 | // GEANT4 internal units
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| 364 | //
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| 365 | // Note : Effects due to binding of atomic electrons are negliged.
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| 366 | {
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| 367 | fParticleChange.InitializeForPostStep(aTrack);
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| 368 |
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| 369 | fParticleChange.SetNumberOfSecondaries(2);
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| 370 |
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| 371 | G4double cosTeta = 2.*G4UniformRand()-1. , sinTeta = std::sqrt(1.-cosTeta*cosTeta);
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| 372 | G4double phi = twopi * G4UniformRand();
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| 373 | G4ThreeVector direction (sinTeta*std::cos(phi), sinTeta*std::sin(phi), cosTeta);
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| 374 | fParticleChange.AddSecondary( new G4DynamicParticle (G4Gamma::Gamma(),
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| 375 | direction, electron_mass_c2) );
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| 376 | fParticleChange.AddSecondary( new G4DynamicParticle (G4Gamma::Gamma(),
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| 377 | -direction, electron_mass_c2) );
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| 378 | // Kill the incident positron
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| 379 | //
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| 380 | fParticleChange.ProposeTrackStatus(fStopAndKill);
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| 381 | return &fParticleChange;
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| 382 | }
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| 383 |
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| 384 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo....
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