[968] | 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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[1347] | 26 | // $Id: G4PenelopeRayleighModel.cc,v 1.8 2010/11/26 11:51:11 pandola Exp $ |
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| 27 | // GEANT4 tag $Name: geant4-09-04-ref-00 $ |
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[968] | 28 | // |
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| 29 | // Author: Luciano Pandola |
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| 30 | // |
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| 31 | // History: |
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| 32 | // -------- |
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| 33 | // 14 Oct 2008 L Pandola Migration from process to model |
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[1055] | 34 | // 17 Apr 2009 V Ivanchenko Cleanup initialisation and generation of secondaries: |
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| 35 | // - apply internal high-energy limit only in constructor |
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| 36 | // - do not apply low-energy limit (default is 0) |
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| 37 | // 19 May 2009 L Pandola Explicitely set to zero pointers deleted in |
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| 38 | // PrepareConstants(), since they might be checked later on |
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[1315] | 39 | // 18 Dec 2009 L Pandola Added a dummy ComputeCrossSectionPerAtom() method issueing a |
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| 40 | // warning if users try to access atomic cross sections via |
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| 41 | // G4EmCalculator |
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[968] | 42 | // |
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| 43 | |
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| 44 | #include "G4PenelopeRayleighModel.hh" |
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| 45 | #include "G4ParticleDefinition.hh" |
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| 46 | #include "G4MaterialCutsCouple.hh" |
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| 47 | #include "G4ProductionCutsTable.hh" |
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| 48 | #include "G4DynamicParticle.hh" |
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| 49 | #include "G4PhysicsTable.hh" |
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| 50 | #include "G4ElementTable.hh" |
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| 51 | #include "G4Element.hh" |
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| 52 | #include "G4PenelopeIntegrator.hh" |
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| 53 | |
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| 54 | |
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| 55 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 56 | |
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| 57 | |
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| 58 | G4PenelopeRayleighModel::G4PenelopeRayleighModel(const G4ParticleDefinition*, |
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| 59 | const G4String& nam) |
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| 60 | :G4VEmModel(nam),samplingFunction_x(0),samplingFunction_xNoLog(0), |
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| 61 | theMaterial(0), |
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| 62 | isInitialised(false) |
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| 63 | { |
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| 64 | fIntrinsicLowEnergyLimit = 100.0*eV; |
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| 65 | fIntrinsicHighEnergyLimit = 100.0*GeV; |
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[1055] | 66 | // SetLowEnergyLimit(fIntrinsicLowEnergyLimit); |
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[968] | 67 | SetHighEnergyLimit(fIntrinsicHighEnergyLimit); |
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| 68 | // |
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| 69 | verboseLevel= 0; |
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| 70 | // Verbosity scale: |
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| 71 | // 0 = nothing |
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| 72 | // 1 = warning for energy non-conservation |
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| 73 | // 2 = details of energy budget |
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| 74 | // 3 = calculation of cross sections, file openings, sampling of atoms |
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| 75 | // 4 = entering in methods |
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| 76 | |
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| 77 | PrepareConstants(); |
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| 78 | } |
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| 79 | |
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| 80 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 81 | |
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| 82 | G4PenelopeRayleighModel::~G4PenelopeRayleighModel() |
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| 83 | { |
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| 84 | std::map <const G4Material*,G4DataVector*>::iterator i; |
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| 85 | for(i=SamplingTable.begin(); i != SamplingTable.end(); i++) { |
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| 86 | delete (*i).second; |
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| 87 | } |
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| 88 | if (samplingFunction_x) delete samplingFunction_x; |
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| 89 | if (samplingFunction_xNoLog) delete samplingFunction_xNoLog; |
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| 90 | } |
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| 91 | |
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| 92 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 93 | |
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| 94 | void G4PenelopeRayleighModel::Initialise(const G4ParticleDefinition* , |
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| 95 | const G4DataVector& ) |
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| 96 | { |
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| 97 | if (verboseLevel > 3) |
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| 98 | G4cout << "Calling G4PenelopeRayleighModel::Initialise()" << G4endl; |
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| 99 | |
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| 100 | |
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[1055] | 101 | if (verboseLevel > 0) { |
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| 102 | G4cout << "Penelope Rayleigh model is initialized " << G4endl |
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| 103 | << "Energy range: " |
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| 104 | << LowEnergyLimit() / keV << " keV - " |
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| 105 | << HighEnergyLimit() / GeV << " GeV" |
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| 106 | << G4endl; |
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| 107 | } |
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[968] | 108 | |
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| 109 | if(isInitialised) return; |
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[1055] | 110 | fParticleChange = GetParticleChangeForGamma(); |
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[968] | 111 | isInitialised = true; |
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| 112 | } |
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| 113 | |
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| 114 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 115 | |
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[1055] | 116 | G4double |
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| 117 | G4PenelopeRayleighModel::CrossSectionPerVolume(const G4Material* material, |
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| 118 | const G4ParticleDefinition* p, |
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| 119 | G4double ekin, |
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| 120 | G4double, |
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| 121 | G4double) |
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[968] | 122 | { |
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| 123 | // Penelope model to calculate the Rayleigh scattering inverse mean |
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| 124 | // free path. |
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| 125 | // |
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| 126 | // The basic method is from |
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| 127 | // M. Born, Atomic physics, Ed. Blackie and Sons (1969) |
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| 128 | // using numerical approximations developed in |
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| 129 | // J. Baro' et al., Radiat. Phys. Chem. 44 (1994) 531 |
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| 130 | // Data used for the form factor used in the calculation (numerical integral of |
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| 131 | // dSigma/dOmega) are been derived by fitting the atomic forn factor tables |
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| 132 | // tabulated in |
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| 133 | // J.H. Hubbel et al., J. Phys. Chem. Ref. Data 4 (1975) 471; erratum ibid. |
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| 134 | // 6 (1977) 615. |
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| 135 | // The numerical integration of the differential cross section dSigma/dOmega, |
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| 136 | // which is implemented in the DifferentialCrossSection() method, is performed |
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| 137 | // by 20-point Gaussian method (managed by G4PenelopeIntegrator). |
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| 138 | // |
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| 139 | |
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| 140 | if (verboseLevel > 3) |
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| 141 | G4cout << "Calling CrossSectionPerVolume() of G4PenelopeRayleighModel" << G4endl; |
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| 142 | SetupForMaterial(p, material, ekin); |
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| 143 | |
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| 144 | //Assign local variable "material" to private member "theMaterial", because |
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| 145 | //this information is necessary to calculate the cross section |
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| 146 | theMaterial = material; |
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| 147 | |
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| 148 | G4int nElements = material->GetNumberOfElements(); |
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| 149 | const G4ElementVector* elementVector = material->GetElementVector(); |
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| 150 | |
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| 151 | G4int maxZ=0; |
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| 152 | for (G4int i=0; i<nElements; i++) |
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| 153 | { |
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| 154 | G4int Z = (G4int) (*elementVector)[i]->GetZ(); |
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| 155 | if (Z>maxZ) |
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| 156 | maxZ = Z; |
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| 157 | } |
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| 158 | |
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| 159 | G4double ec=std::min(ekin,0.5*maxZ); |
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| 160 | factorE = 849.3315*(ec/electron_mass_c2)*(ec/electron_mass_c2); |
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| 161 | G4double cs=0; |
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| 162 | // |
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| 163 | //Integrate the Differential Cross Section dSigma/dCosTheta between -1 and 1. |
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| 164 | // |
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| 165 | G4PenelopeIntegrator<G4PenelopeRayleighModel,G4double(G4PenelopeRayleighModel::*)(G4double)> |
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| 166 | theIntegrator; |
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| 167 | cs = |
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| 168 | theIntegrator.Calculate(this,&G4PenelopeRayleighModel::DifferentialCrossSection, |
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| 169 | -1.0,0.90,1e-06); |
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| 170 | cs += theIntegrator.Calculate(this,&G4PenelopeRayleighModel::DifferentialCrossSection, |
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| 171 | 0.90,0.9999999,1e-06); |
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| 172 | cs = cs*(ec/ekin)*(ec/ekin)*pi*classic_electr_radius*classic_electr_radius; |
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| 173 | // |
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| 174 | // Here cs represents the cross section per molecule for materials defined with chemical |
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| 175 | // formulas and the average cross section per atom in compounds (defined with the mass |
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| 176 | // fraction) |
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| 177 | // |
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| 178 | const G4int* stechiometric = material->GetAtomsVector(); |
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| 179 | //This is the total density of atoms in the material |
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| 180 | G4double atomDensity = material->GetTotNbOfAtomsPerVolume(); |
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| 181 | G4double moleculeDensity = 0; |
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| 182 | |
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| 183 | //Default case: the material is a compound. In this case, cs is the average cross section |
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| 184 | // _per_atom_ and one has to multiply for the atom density. |
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| 185 | G4double cross = atomDensity*cs; |
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| 186 | G4bool isAMolecule = false; |
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| 187 | |
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| 188 | //Alternative case: the material is a molecule. In this case cs is the cross section |
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| 189 | // _per_molecule_ and one has to multiply for the molecule density |
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| 190 | if (stechiometric) |
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| 191 | { |
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| 192 | //Calculate the total number of atoms per molecule |
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| 193 | G4int atomsPerMolecule = 0; |
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| 194 | for (G4int k=0;k<nElements;k++) |
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[1315] | 195 | { |
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[968] | 196 | atomsPerMolecule += stechiometric[k]; |
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[1315] | 197 | if (verboseLevel > 2) |
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| 198 | { |
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| 199 | G4cout << "Element: " << (G4int) (*elementVector)[k]->GetZ() << " has " << |
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| 200 | stechiometric[k] << " atoms/molecule" << G4endl; |
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| 201 | } |
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| 202 | } |
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[968] | 203 | if (atomsPerMolecule) |
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| 204 | { |
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| 205 | isAMolecule = true; |
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| 206 | if (verboseLevel > 3) |
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| 207 | { |
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| 208 | G4cout << "Material " << material->GetName() << " is a molecule composed by " << |
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| 209 | atomsPerMolecule << " atoms" << G4endl; |
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| 210 | } |
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| 211 | moleculeDensity = atomDensity/((G4double) atomsPerMolecule); |
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| 212 | cross = cs*moleculeDensity; |
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| 213 | } |
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| 214 | } |
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[1315] | 215 | |
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[968] | 216 | if (verboseLevel > 2) |
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| 217 | { |
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| 218 | if (isAMolecule) |
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| 219 | { |
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| 220 | G4cout << "Rayleigh cross section at " << ekin/keV << " keV for material " << |
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| 221 | material->GetName() << " (molecule) = " << cs/barn << " barn/molecule." << G4endl; |
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| 222 | G4cout << "Mean free path: " << (1./cross)/mm << " mm" << G4endl; |
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| 223 | } |
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| 224 | else |
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| 225 | { |
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| 226 | G4cout << "Rayleigh cross section at " << ekin/keV << " keV for material " << |
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| 227 | material->GetName() << " (compound) = " << cs/barn << " barn/atom." << G4endl; |
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| 228 | G4cout << "Mean free path: " << (1./cross)/mm << " mm" << G4endl; |
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| 229 | } |
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| 230 | } |
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| 231 | return cross; |
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| 232 | } |
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| 233 | |
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[1315] | 234 | |
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| 235 | //This is a dummy method. Never inkoved by the tracking, it just issues |
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| 236 | //a warning if one tries to get Cross Sections per Atom via the |
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| 237 | //G4EmCalculator. |
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| 238 | G4double G4PenelopeRayleighModel::ComputeCrossSectionPerAtom(const G4ParticleDefinition*, |
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| 239 | G4double, |
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| 240 | G4double, |
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| 241 | G4double, |
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| 242 | G4double, |
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| 243 | G4double) |
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| 244 | { |
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| 245 | G4cout << "*** G4PenelopeRayleighModel -- WARNING ***" << G4endl; |
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| 246 | G4cout << "Penelope Rayleigh model does not calculate cross section _per atom_ " << G4endl; |
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| 247 | G4cout << "so the result is always zero. For physics values, please invoke " << G4endl; |
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| 248 | G4cout << "GetCrossSectionPerVolume() or GetMeanFreePath() via the G4EmCalculator" << G4endl; |
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| 249 | return 0; |
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| 250 | } |
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| 251 | |
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| 252 | |
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[968] | 253 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 254 | |
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| 255 | void G4PenelopeRayleighModel::SampleSecondaries(std::vector<G4DynamicParticle*>* , |
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[1055] | 256 | const G4MaterialCutsCouple* couple, |
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| 257 | const G4DynamicParticle* aDynamicGamma, |
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| 258 | G4double, |
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| 259 | G4double) |
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[968] | 260 | { |
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| 261 | // Penelope model to sample the Rayleigh scattering final state. |
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| 262 | // |
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| 263 | // The angular deflection of the scattered photon is sampled according to the |
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| 264 | // differential cross section dSigma/dOmega used for the numerical integration, |
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| 265 | // and implemented in the DifferentialCrossSection() method. See comments in |
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| 266 | // method CrossSectionPerVolume() for more details on the original references |
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| 267 | // of the model. |
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| 268 | // |
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| 269 | |
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| 270 | if (verboseLevel > 3) |
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| 271 | G4cout << "Calling SamplingSecondaries() of G4PenelopeRayleighModel" << G4endl; |
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[1055] | 272 | |
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[968] | 273 | G4double photonEnergy0 = aDynamicGamma->GetKineticEnergy(); |
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| 274 | |
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[1055] | 275 | if (photonEnergy0 <= fIntrinsicLowEnergyLimit) |
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| 276 | { |
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[968] | 277 | fParticleChange->ProposeTrackStatus(fStopAndKill); |
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| 278 | fParticleChange->SetProposedKineticEnergy(0.); |
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| 279 | fParticleChange->ProposeLocalEnergyDeposit(photonEnergy0); |
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| 280 | return ; |
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[1055] | 281 | } |
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[968] | 282 | |
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| 283 | G4ParticleMomentum photonDirection0 = aDynamicGamma->GetMomentumDirection(); |
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| 284 | |
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| 285 | // Sampling inizialitation (build internal table) |
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| 286 | theMaterial = couple->GetMaterial(); |
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| 287 | InitialiseSampling(); |
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| 288 | |
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| 289 | G4DataVector* samplingFunction_y = SamplingTable.find(theMaterial)->second; |
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| 290 | |
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| 291 | // Sample the angle of the scattered photon |
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| 292 | G4double x2max = 2.0*std::log(41.2148*photonEnergy0/electron_mass_c2); |
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| 293 | G4int jm=0; |
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| 294 | G4int asize = samplingFunction_x->size(); |
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| 295 | if (x2max < (*samplingFunction_x)[1]) |
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| 296 | jm=0; |
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| 297 | else if(x2max>(*samplingFunction_x)[asize-2]) |
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| 298 | jm=asize-2; |
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| 299 | else |
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| 300 | { |
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| 301 | //spacing in the logTable |
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| 302 | G4double logScalingFactor = (*samplingFunction_x)[1]-(*samplingFunction_x)[0]; |
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| 303 | jm=(G4int) ((x2max-(*samplingFunction_x)[0])/logScalingFactor); |
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| 304 | } |
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| 305 | |
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| 306 | G4double rumax = (*samplingFunction_y)[jm]+((*samplingFunction_y)[jm+1]-(*samplingFunction_y)[jm])* |
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| 307 | (x2max-(*samplingFunction_x)[jm])/((*samplingFunction_x)[jm+1]-(*samplingFunction_x)[jm]); |
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| 308 | G4double cosTheta=0; |
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| 309 | G4double rejectionValue = 0; |
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| 310 | do{ |
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| 311 | G4double ru = rumax + std::log(G4UniformRand()); |
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| 312 | G4int j=0; |
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| 313 | G4int ju=jm+1; |
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| 314 | do{ |
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| 315 | G4int jt=(j+ju)/2; //bipartition |
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| 316 | if (ru > (*samplingFunction_y)[jt]) |
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| 317 | j=jt; |
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| 318 | else |
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| 319 | ju=jt; |
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| 320 | }while ((ju-j)>1); |
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| 321 | G4double x2rat = 0; |
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| 322 | G4double denomin = (*samplingFunction_y)[j+1]-(*samplingFunction_y)[j]; |
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| 323 | if (denomin > 1e-12) |
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| 324 | { |
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| 325 | x2rat = (*samplingFunction_x)[j]+(((*samplingFunction_x)[j+1]-(*samplingFunction_x)[j])* |
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| 326 | (ru-(*samplingFunction_y)[j])/denomin)-x2max; |
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| 327 | } |
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| 328 | else |
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| 329 | { |
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| 330 | x2rat = (*samplingFunction_x)[j]-x2max; |
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| 331 | } |
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| 332 | cosTheta = 1.0-2.0*std::exp(x2rat); |
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| 333 | rejectionValue = 0.5*(1.0+cosTheta*cosTheta); |
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| 334 | }while (G4UniformRand() > rejectionValue); |
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| 335 | |
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| 336 | G4double sinTheta = std::sqrt(1-cosTheta*cosTheta); |
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| 337 | |
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| 338 | // Scattered photon angles. ( Z - axis along the parent photon) |
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| 339 | G4double phi = twopi * G4UniformRand() ; |
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| 340 | G4double dirX = sinTheta*std::cos(phi); |
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| 341 | G4double dirY = sinTheta*std::sin(phi); |
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| 342 | G4double dirZ = cosTheta; |
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| 343 | |
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| 344 | // Update G4VParticleChange for the scattered photon |
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| 345 | G4ThreeVector photonDirection1(dirX, dirY, dirZ); |
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| 346 | |
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| 347 | photonDirection1.rotateUz(photonDirection0); |
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| 348 | fParticleChange->ProposeMomentumDirection(photonDirection1) ; |
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| 349 | fParticleChange->SetProposedKineticEnergy(photonEnergy0) ; |
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| 350 | |
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| 351 | return; |
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| 352 | } |
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| 353 | |
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| 354 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 355 | |
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| 356 | G4double G4PenelopeRayleighModel::DifferentialCrossSection(G4double cosTheta) |
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| 357 | { |
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| 358 | //Differential cross section for Rayleigh scattering |
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| 359 | G4double x2 = factorE*(1-cosTheta); |
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| 360 | G4double gradx = (1+cosTheta*cosTheta)*MolecularFormFactor(x2); |
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| 361 | return gradx; |
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| 362 | } |
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| 363 | |
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| 364 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
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| 365 | |
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| 366 | G4double G4PenelopeRayleighModel::MolecularFormFactor(G4double x2) |
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| 367 | { |
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| 368 | //Squared molecular form factor (additivity rule) |
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| 369 | const G4int ntot=95; |
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| 370 | G4double RA1[ntot] = {0.0e0, 3.9265e+0, 4.3100e+1, 5.2757e+1, 2.5021e+1, |
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| 371 | 1.2211e+1, 9.3229e+0, 3.2455e+0, 2.4197e+0, 1.5985e+0, |
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| 372 | 3.0926e+1, 1.5315e+1, 7.7061e+0, 3.9493e+0, 2.2042e+0, |
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| 373 | 1.9453e+1, 1.9354e+1, 8.0374e+0, 8.3779e+1, 5.7370e+1, |
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| 374 | 5.2310e+1, 4.7514e+1, 4.3785e+1, 4.2048e+1, 3.6972e+1, |
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| 375 | 3.3849e+1, 3.1609e+1, 2.8763e+1, 2.7217e+1, 2.4263e+1, |
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| 376 | 2.2403e+1, 1.8606e+1, 1.5143e+1, 1.4226e+1, 1.1792e+1, |
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| 377 | 9.7574e+0, 1.2796e+1, 1.2854e+1, 1.2368e+1, 1.0208e+1, |
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| 378 | 8.2823e+0, 7.4677e+0, 7.6028e+0, 6.1090e+0, 5.5346e+0, |
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| 379 | 4.2340e+0, 4.0444e+0, 4.2905e+0, 4.7950e+0, 5.1112e+0, |
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| 380 | 5.2407e+0, 5.2153e+0, 5.1639e+0, 4.8814e+0, 5.8054e+0, |
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| 381 | 6.6724e+0, 6.5104e+0, 6.3364e+0, 6.2889e+0, 6.3028e+0, |
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| 382 | 6.3853e+0, 6.3475e+0, 6.5779e+0, 6.8486e+0, 7.0993e+0, |
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| 383 | 7.6122e+0, 7.9681e+0, 8.3481e+0, 6.3875e+0, 8.0042e+0, |
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| 384 | 8.0820e+0, 7.6940e+0, 7.1927e+0, 6.6751e+0, 6.1623e+0, |
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| 385 | 5.8335e+0, 5.5599e+0, 4.6551e+0, 4.4327e+0, 4.7601e+0, |
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| 386 | 5.2872e+0, 5.6084e+0, 5.7680e+0, 5.8041e+0, 5.7566e+0, |
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| 387 | 5.6541e+0, 6.3932e+0, 6.9313e+0, 7.0027e+0, 6.8796e+0, |
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| 388 | 6.4739e+0, 6.2405e+0, 6.0081e+0, 5.5708e+0, 5.3680e+0}; |
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| 389 | |
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| 390 | |
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| 391 | G4double RA2[ntot] = {0.0e0, 1.3426e-1, 9.4875e+1,-1.0896e+2,-4.5494e+1, |
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| 392 | -1.9572e+1,-1.2382e+1,-3.6827e+0,-2.4542e+0,-1.4453e+0, |
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| 393 | 1.3401e+2, 7.9717e+1, 6.2164e+1, 4.0300e+1, 3.1682e+1, |
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| 394 | -1.3639e+1,-1.5950e+1,-5.1523e+0, 1.8351e+2, 1.2205e+2, |
---|
| 395 | 1.0007e+2, 8.5632e+1, 7.9145e+1, 6.3675e+1, 6.2954e+1, |
---|
| 396 | 5.6601e+1, 5.4171e+1, 4.8752e+1, 3.8062e+1, 3.9933e+1, |
---|
| 397 | 4.8343e+1, 4.2137e+1, 3.4617e+1, 2.9430e+1, 2.4010e+1, |
---|
| 398 | 1.9744e+1, 4.0009e+1, 5.1614e+1, 5.0456e+1, 3.9088e+1, |
---|
| 399 | 2.6824e+1, 2.2953e+1, 2.4773e+1, 1.6893e+1, 1.4548e+1, |
---|
| 400 | 9.7226e+0, 1.0192e+1, 1.1153e+1, 1.3188e+1, 1.4733e+1, |
---|
| 401 | 1.5644e+1, 1.5939e+1, 1.5923e+1, 1.5254e+1, 2.0748e+1, |
---|
| 402 | 2.6901e+1, 2.7032e+1, 2.4938e+1, 2.1528e+1, 2.0362e+1, |
---|
| 403 | 1.9474e+1, 1.8238e+1, 1.7898e+1, 1.9174e+1, 1.9023e+1, |
---|
| 404 | 1.8194e+1, 1.8504e+1, 1.8955e+1, 1.4276e+1, 1.7558e+1, |
---|
| 405 | 1.8651e+1, 1.7984e+1, 1.6793e+1, 1.5469e+1, 1.4143e+1, |
---|
| 406 | 1.3149e+1, 1.2255e+1, 9.2352e+0, 8.6067e+0, 9.7460e+0, |
---|
| 407 | 1.1749e+1, 1.3281e+1, 1.4326e+1, 1.4920e+1, 1.5157e+1, |
---|
| 408 | 1.5131e+1, 1.9489e+1, 2.3649e+1, 2.4686e+1, 2.4760e+1, |
---|
| 409 | 2.1519e+1, 2.0099e+1, 1.8746e+1, 1.5943e+1, 1.4880e+1}; |
---|
| 410 | |
---|
| 411 | G4double RA3[ntot] = {0.0e0, 2.2648e+0, 1.0579e+3, 8.6177e+2, 2.4422e+2, |
---|
| 412 | 7.8788e+1, 3.8293e+1, 1.2564e+1, 6.9091e+0, 3.7926e+0, |
---|
| 413 | 0.0000e+0, 0.0000e+0, 1.6759e-9, 1.3026e+1, 3.0569e+0, |
---|
| 414 | 1.5521e+2, 1.2815e+2, 4.7378e+1, 9.2802e+2, 4.7508e+2, |
---|
| 415 | 3.6612e+2, 2.7582e+2, 2.1008e+2, 1.5903e+2, 1.2322e+2, |
---|
| 416 | 9.2898e+1, 7.1345e+1, 5.1651e+1, 3.8474e+1, 2.7410e+1, |
---|
| 417 | 1.9126e+1, 1.0889e+1, 5.3479e+0, 8.2223e+0, 5.0837e+0, |
---|
| 418 | 2.8905e+0, 2.7457e+0, 6.7082e-1, 0.0000e+0, 0.0000e+0, |
---|
| 419 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, |
---|
| 420 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, |
---|
| 421 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, |
---|
| 422 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 1.7264e-1, 2.7322e-1, |
---|
| 423 | 3.9444e-1, 4.5648e-1, 6.2286e-1, 7.2468e-1, 8.4296e-1, |
---|
| 424 | 1.1698e+0, 1.2994e+0, 1.4295e+0, 0.0000e+0, 8.1570e-1, |
---|
| 425 | 6.9349e-1, 4.9536e-1, 3.1211e-1, 1.5931e-1, 2.9512e-2, |
---|
| 426 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, |
---|
| 427 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, |
---|
| 428 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, |
---|
| 429 | 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0, 0.0000e+0}; |
---|
| 430 | |
---|
| 431 | G4double RA4[ntot] = {1.1055e1,6.3519e0,4.7367e+1, 3.9402e+1, 2.2896e+1, |
---|
| 432 | 1.3979e+1, 1.0766e+1, 6.5252e+0, 5.1631e+0, 4.0524e+0, |
---|
| 433 | 2.7145e+1, 1.8724e+1, 1.4782e+1, 1.1608e+1, 9.7750e+0, |
---|
| 434 | 1.6170e+1, 1.5249e+1, 9.1916e+0, 5.4499e+1, 4.1381e+1, |
---|
| 435 | 3.7395e+1, 3.3815e+1, 3.1135e+1, 2.8273e+1, 2.6140e+1, |
---|
| 436 | 2.3948e+1, 2.2406e+1, 2.0484e+1, 1.8453e+1, 1.7386e+1, |
---|
| 437 | 1.7301e+1, 1.5388e+1, 1.3411e+1, 1.2668e+1, 1.1133e+1, |
---|
| 438 | 9.8081e+0, 1.3031e+1, 1.4143e+1, 1.3815e+1, 1.2077e+1, |
---|
| 439 | 1.0033e+1, 9.2549e+0, 9.5338e+0, 7.9076e+0, 7.3263e+0, |
---|
| 440 | 5.9996e+0, 6.0087e+0, 6.2660e+0, 6.7914e+0, 7.1501e+0, |
---|
| 441 | 7.3367e+0, 7.3729e+0, 7.3508e+0, 7.1465e+0, 8.2731e+0, |
---|
| 442 | 9.3745e+0, 9.3508e+0, 8.9897e+0, 8.4566e+0, 8.2690e+0, |
---|
| 443 | 8.1398e+0, 7.9183e+0, 7.9123e+0, 8.1677e+0, 8.1871e+0, |
---|
| 444 | 8.1766e+0, 8.2881e+0, 8.4227e+0, 7.0273e+0, 8.0002e+0, |
---|
| 445 | 8.1440e+0, 7.9104e+0, 7.5685e+0, 7.1970e+0, 6.8184e+0, |
---|
| 446 | 6.5469e+0, 6.3056e+0, 5.4844e+0, 5.2832e+0, 5.5889e+0, |
---|
| 447 | 6.0919e+0, 6.4340e+0, 6.6426e+0, 6.7428e+0, 6.7636e+0, |
---|
| 448 | 6.7281e+0, 7.5729e+0, 8.2808e+0, 8.4400e+0, 8.4220e+0, |
---|
| 449 | 7.8662e+0, 7.5993e+0, 7.3353e+0, 6.7829e+0, 6.5520e+0}; |
---|
| 450 | |
---|
| 451 | G4double RA5[ntot] = {0.0e0, 4.9828e+0, 5.5674e+1, 3.0902e+1, 1.1496e+1, |
---|
| 452 | 4.8936e+0, 2.5506e+0, 1.2236e+0, 7.4698e-1, 4.7042e-1, |
---|
| 453 | 4.7809e+0, 4.6315e+0, 4.3677e+0, 4.9269e+0, 2.6033e+0, |
---|
| 454 | 9.6229e+0, 7.2592e+0, 4.1634e+0, 1.3999e+1, 8.6975e+0, |
---|
| 455 | 6.9630e+0, 5.4681e+0, 4.2653e+0, 3.2848e+0, 2.7354e+0, |
---|
| 456 | 2.1617e+0, 1.7030e+0, 1.2826e+0, 9.7080e-1, 7.2227e-1, |
---|
| 457 | 5.0874e-1, 3.1402e-1, 1.6360e-1, 3.2918e-1, 2.3570e-1, |
---|
| 458 | 1.5868e-1, 1.5146e-1, 9.7662e-2, 7.3151e-2, 6.4206e-2, |
---|
| 459 | 4.8945e-2, 4.3189e-2, 4.4368e-2, 3.3976e-2, 3.0466e-2, |
---|
| 460 | 2.4477e-2, 3.7202e-2, 3.7093e-2, 3.8161e-2, 3.8576e-2, |
---|
| 461 | 3.8403e-2, 3.7806e-2, 3.4958e-2, 3.6029e-2, 4.3087e-2, |
---|
| 462 | 4.7069e-2, 4.6452e-2, 4.2486e-2, 4.1517e-2, 4.1691e-2, |
---|
| 463 | 4.2813e-2, 4.2294e-2, 4.5287e-2, 4.8462e-2, 4.9726e-2, |
---|
| 464 | 5.5097e-2, 5.6568e-2, 5.8069e-2, 1.2270e-2, 3.8006e-2, |
---|
| 465 | 3.5048e-2, 3.0050e-2, 2.5069e-2, 2.0485e-2, 1.6151e-2, |
---|
| 466 | 1.4631e-2, 1.4034e-2, 1.1978e-2, 1.1522e-2, 1.2375e-2, |
---|
| 467 | 1.3805e-2, 1.4954e-2, 1.5832e-2, 1.6467e-2, 1.6896e-2, |
---|
| 468 | 1.7166e-2, 1.9954e-2, 2.2497e-2, 2.1942e-2, 2.1965e-2, |
---|
| 469 | 2.0005e-2, 1.8927e-2, 1.8167e-2, 1.6314e-2, 1.5522e-2}; |
---|
| 470 | |
---|
| 471 | G4double x=std::sqrt(x2); |
---|
| 472 | G4double gradx1=0.0; |
---|
| 473 | |
---|
| 474 | G4int nElements = theMaterial->GetNumberOfElements(); |
---|
| 475 | const G4ElementVector* elementVector = theMaterial->GetElementVector(); |
---|
| 476 | const G4int* stechiometric = theMaterial->GetAtomsVector(); |
---|
| 477 | const G4double* vector_of_atoms = theMaterial->GetVecNbOfAtomsPerVolume(); |
---|
| 478 | const G4double tot_atoms = theMaterial->GetTotNbOfAtomsPerVolume(); |
---|
| 479 | for (G4int i=0;i<nElements;i++) |
---|
| 480 | { |
---|
| 481 | G4int Z = (G4int) (*elementVector)[i]->GetZ(); |
---|
| 482 | if (Z>ntot) Z=95; |
---|
| 483 | G4double denomin = 1.+x2*(RA4[Z-1]+x2*RA5[Z-1]); |
---|
| 484 | G4double fa=Z*(1+x2*(RA1[Z-1]+x*(RA2[Z-1]+x*RA3[Z-1])))/(denomin*denomin); |
---|
| 485 | if (Z>10 && fa>2.0) |
---|
| 486 | { |
---|
| 487 | G4double k1=0.3125; |
---|
| 488 | G4double k2=2.426311e-02; |
---|
| 489 | G4double Pa=(Z-k1)*fine_structure_const; |
---|
| 490 | G4double Pg=std::sqrt(1-(Pa*Pa)); |
---|
| 491 | G4double Pq=k2*x/Pa; |
---|
| 492 | G4double fb=std::sin(2.0*Pg*std::atan(Pq))/(Pg*Pq*std::pow((1+Pq*Pq),Pg)); |
---|
| 493 | fa=std::max(fa,fb); |
---|
| 494 | } |
---|
| 495 | if (stechiometric && stechiometric[i]!=0) |
---|
| 496 | gradx1 += stechiometric[i]*(fa*fa); //sum on the molecule |
---|
| 497 | else |
---|
| 498 | gradx1 += (vector_of_atoms[i]/tot_atoms)*(fa*fa); //weighted mean |
---|
| 499 | } |
---|
| 500 | return gradx1; |
---|
| 501 | } |
---|
| 502 | |
---|
| 503 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... |
---|
| 504 | |
---|
| 505 | void G4PenelopeRayleighModel::InitialiseSampling() |
---|
| 506 | { |
---|
| 507 | if (!samplingFunction_x || !samplingFunction_xNoLog) |
---|
| 508 | { |
---|
| 509 | G4cout << "G4PenelopeRayleighModel::InitialiseSampling(), something wrong" << G4endl; |
---|
[1347] | 510 | G4cout << "It looks like G4PenelopeRayleighModel::PrepareConstants() has not been called" |
---|
| 511 | << G4endl; |
---|
[968] | 512 | G4Exception(); |
---|
[1347] | 513 | return; |
---|
[968] | 514 | } |
---|
| 515 | if (!SamplingTable.count(theMaterial)) //material not defined yet |
---|
| 516 | { |
---|
| 517 | G4double XlowInte = 0.; |
---|
| 518 | G4double XhighInte=(*samplingFunction_xNoLog)[0]; |
---|
| 519 | //material not inizialized yet: initialize it now |
---|
| 520 | G4DataVector* samplingFunction_y = new G4DataVector(); |
---|
| 521 | G4PenelopeIntegrator<G4PenelopeRayleighModel,G4double(G4PenelopeRayleighModel::*)(G4double)> |
---|
| 522 | theIntegrator; |
---|
| 523 | G4double sum = theIntegrator.Calculate(this,&G4PenelopeRayleighModel::MolecularFormFactor, |
---|
| 524 | XlowInte,XhighInte,1e-10); |
---|
| 525 | samplingFunction_y->push_back(sum); |
---|
| 526 | for (G4int i=1;i<nPoints;i++) |
---|
| 527 | { |
---|
| 528 | XlowInte=(*samplingFunction_xNoLog)[i-1]; |
---|
| 529 | XhighInte=(*samplingFunction_xNoLog)[i]; |
---|
| 530 | sum += theIntegrator.Calculate(this, |
---|
| 531 | &G4PenelopeRayleighModel::MolecularFormFactor, |
---|
| 532 | XlowInte,XhighInte,1e-10); |
---|
| 533 | samplingFunction_y->push_back(sum); |
---|
| 534 | } |
---|
| 535 | for (G4int i=0;i<nPoints;i++) |
---|
| 536 | (*samplingFunction_y)[i]=std::log((*samplingFunction_y)[i]); |
---|
| 537 | |
---|
| 538 | // |
---|
| 539 | /* |
---|
| 540 | G4String nnn = theMaterial->GetName()+".ntab"; |
---|
| 541 | std::ofstream file(nnn); |
---|
| 542 | for (size_t k=0;k<samplingFunction_x->size();k++) |
---|
| 543 | file << (*samplingFunction_x)[k] << " " << (*samplingFunction_y)[k] << G4endl; |
---|
| 544 | file.close(); |
---|
| 545 | */ |
---|
| 546 | // |
---|
| 547 | SamplingTable[theMaterial] = samplingFunction_y; |
---|
| 548 | } |
---|
| 549 | } |
---|
| 550 | |
---|
| 551 | void G4PenelopeRayleighModel::PrepareConstants() |
---|
| 552 | { |
---|
| 553 | if (verboseLevel > 3) |
---|
| 554 | G4cout << "Calling G4PenelopeRayleighModel::PrepareConstants()" << G4endl; |
---|
| 555 | nPoints=241; |
---|
| 556 | Xlow=1e-04; |
---|
| 557 | Xhigh=1e06; |
---|
| 558 | if (samplingFunction_x) |
---|
[1055] | 559 | { |
---|
| 560 | delete samplingFunction_x; |
---|
| 561 | samplingFunction_x = 0; |
---|
| 562 | } |
---|
[968] | 563 | if (samplingFunction_xNoLog) |
---|
[1055] | 564 | { |
---|
| 565 | delete samplingFunction_xNoLog; |
---|
| 566 | samplingFunction_xNoLog = 0; |
---|
| 567 | } |
---|
| 568 | |
---|
[968] | 569 | samplingFunction_x = new G4DataVector(); |
---|
| 570 | samplingFunction_xNoLog = new G4DataVector(); |
---|
| 571 | |
---|
| 572 | G4double scalingFactor = std::pow((Xhigh/Xlow),((1/((G4double)(nPoints-1))))); |
---|
| 573 | G4double logScalingFactor=(1/((G4double)(nPoints-1)))*std::log(Xhigh/Xlow); |
---|
| 574 | //Logarithmic table between log(Xlow) and log(Xhigh) |
---|
| 575 | samplingFunction_x->push_back(std::log(Xlow)); |
---|
| 576 | //Table between Xlow and Xhigh with log spacement: needed for InitialiseSampling() |
---|
| 577 | samplingFunction_xNoLog->push_back(Xlow); |
---|
| 578 | |
---|
| 579 | for (G4int i=1;i<nPoints;i++) |
---|
| 580 | { |
---|
| 581 | G4double nextx = (*samplingFunction_x)[i-1]+logScalingFactor; |
---|
| 582 | samplingFunction_x->push_back(nextx); |
---|
| 583 | nextx = (*samplingFunction_xNoLog)[i-1]*scalingFactor; |
---|
| 584 | samplingFunction_xNoLog->push_back(nextx); |
---|
| 585 | } |
---|
| 586 | } |
---|