| 1 | //
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| 2 | // ********************************************************************
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| 3 | // * License and Disclaimer *
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| 4 | // * *
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| 5 | // * The Geant4 software is copyright of the Copyright Holders of *
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| 6 | // * the Geant4 Collaboration. It is provided under the terms and *
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| 7 | // * conditions of the Geant4 Software License, included in the file *
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| 8 | // * LICENSE and available at http://cern.ch/geant4/license . These *
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| 9 | // * include a list of copyright holders. *
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| 10 | // * *
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| 11 | // * Neither the authors of this software system, nor their employing *
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| 12 | // * institutes,nor the agencies providing financial support for this *
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| 13 | // * work make any representation or warranty, express or implied, *
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| 14 | // * regarding this software system or assume any liability for its *
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| 15 | // * use. Please see the license in the file LICENSE and URL above *
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| 16 | // * for the full disclaimer and the limitation of liability. *
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| 17 | // * *
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| 18 | // * This code implementation is the result of the scientific and *
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| 19 | // * technical work of the GEANT4 collaboration. *
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| 20 | // * By using, copying, modifying or distributing the software (or *
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| 21 | // * any work based on the software) you agree to acknowledge its *
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| 22 | // * use in resulting scientific publications, and indicate your *
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| 23 | // * acceptance of all terms of the Geant4 Software license. *
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| 24 | // ********************************************************************
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| 25 | //
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| 26 | // $Id: G4CrossSectionChargeIncreasePartial.cc,v 1.2 2008/07/14 20:47:34 sincerti Exp $
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| 27 | // GEANT4 tag $Name: geant4-09-02 $
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| 28 |
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| 29 | #include "G4CrossSectionChargeIncreasePartial.hh"
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| 30 |
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| 31 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 32 |
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| 33 | G4CrossSectionChargeIncreasePartial::G4CrossSectionChargeIncreasePartial()
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| 34 | {
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| 35 | //ALPHA+
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| 36 |
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| 37 | f0[0][0]=1.;
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| 38 | a0[0][0]=2.25;
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| 39 | a1[0][0]=-0.75;
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| 40 | b0[0][0]=-32.10;
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| 41 | c0[0][0]=0.600;
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| 42 | d0[0][0]=2.40;
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| 43 | x0[0][0]=4.60;
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| 44 |
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| 45 | x1[0][0]=-1.;
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| 46 | b1[0][0]=-1.;
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| 47 |
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| 48 | numberOfPartialCrossSections[0]=1;
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| 49 |
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| 50 | //HELIUM
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| 51 |
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| 52 | f0[0][1]=1.;
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| 53 | a0[0][1]=2.25;
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| 54 | a1[0][1]=-0.75;
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| 55 | b0[0][1]=-30.93;
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| 56 | c0[0][1]=0.590;
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| 57 | d0[0][1]=2.35;
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| 58 | x0[0][1]=4.29;
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| 59 |
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| 60 | f0[1][1]=1.;
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| 61 | a0[1][1]=2.25;
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| 62 | a1[1][1]=-0.75;
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| 63 | b0[1][1]=-32.61;
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| 64 | c0[1][1]=0.435;
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| 65 | d0[1][1]=2.70;
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| 66 | x0[1][1]=4.45;
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| 67 |
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| 68 | x1[0][1]=-1.;
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| 69 | b1[0][1]=-1.;
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| 70 |
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| 71 | x1[1][1]=-1.;
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| 72 | b1[1][1]=-1.;
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| 73 |
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| 74 | numberOfPartialCrossSections[1]=2;
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| 75 | }
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| 76 |
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| 77 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 78 |
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| 79 | G4CrossSectionChargeIncreasePartial::~G4CrossSectionChargeIncreasePartial()
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| 80 | {}
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| 81 |
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| 82 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 83 |
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| 84 | G4double G4CrossSectionChargeIncreasePartial::CrossSection(G4double k, G4int index,
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| 85 | const G4ParticleDefinition* particleDefinition)
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| 86 | {
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| 87 |
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| 88 | G4int particleTypeIndex = 0;
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| 89 | G4DNAGenericIonsManager *instance;
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| 90 | instance = G4DNAGenericIonsManager::Instance();
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| 91 |
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| 92 | if (particleDefinition == instance->GetIon("alpha+")) particleTypeIndex=0;
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| 93 | if (particleDefinition == instance->GetIon("helium")) particleTypeIndex=1;
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| 94 |
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| 95 | //
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| 96 | // sigma(T) = f0 10 ^ y(log10(T/eV))
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| 97 | //
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| 98 | // / a0 x + b0 x < x0
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| 99 | // |
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| 100 | // y(x) = < a0 x + b0 - c0 (x - x0)^d0 x0 <= x < x1
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| 101 | // |
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| 102 | // \ a1 x + b1 x >= x1
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| 103 | //
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| 104 | //
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| 105 | // f0, a0, a1, b0, b1, c0, d0, x0, x1 are parameters that change for protons and helium (0, +, ++)
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| 106 | //
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| 107 | // f0 has been added to the code in order to manage partial (shell-dependent) cross sections (if no shell dependence is present. f0=1. Sum of f0 over the considered shells should give 1)
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| 108 | //
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| 109 | // From Rad. Phys. and Chem. 59 (2000) 255-275, M. Dingfelder et al.
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| 110 | // Inelastic-collision cross sections of liquid water for interactions of energetic proton
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| 111 | //
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| 112 |
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| 113 | if (x1[index][particleTypeIndex]<x0[index][particleTypeIndex])
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| 114 | {
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| 115 | //
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| 116 | // if x1 < x0 means that x1 and b1 will be calculated with the following formula (this piece of code is run on all alphas and not on protons)
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| 117 | //
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| 118 | // x1 = x0 + ((a0 - a1)/(c0 * d0)) ^ (1 / (d0 - 1))
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| 119 | //
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| 120 | // b1 = (a0 - a1) * x1 + b0 - c0 * (x1 - x0) ^ d0
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| 121 | //
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| 122 |
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| 123 | x1[index][particleTypeIndex]=x0[index][particleTypeIndex] + std::pow((a0[index][particleTypeIndex] - a1[index][particleTypeIndex]) / (c0[index][particleTypeIndex] * d0[index][particleTypeIndex]), 1. / (d0[index][particleTypeIndex] - 1.));
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| 124 | b1[index][particleTypeIndex]=(a0[index][particleTypeIndex] - a1[index][particleTypeIndex]) * x1[index][particleTypeIndex] + b0[index][particleTypeIndex] - c0[index][particleTypeIndex] * std::pow(x1[index][particleTypeIndex] - x0[index][particleTypeIndex], d0[index][particleTypeIndex]);
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| 125 | }
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| 126 |
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| 127 | G4double x(std::log10(k/eV));
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| 128 | G4double y;
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| 129 |
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| 130 | if (x<x0[index][particleTypeIndex])
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| 131 | y=a0[index][particleTypeIndex] * x + b0[index][particleTypeIndex];
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| 132 | else if (x<x1[index][particleTypeIndex])
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| 133 | y=a0[index][particleTypeIndex] * x + b0[index][particleTypeIndex] - c0[index][particleTypeIndex] * std::pow(x - x0[index][particleTypeIndex], d0[index][particleTypeIndex]);
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| 134 | else
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| 135 | y=a1[index][particleTypeIndex] * x + b1[index][particleTypeIndex];
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| 136 |
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| 137 | return f0[index][particleTypeIndex] * std::pow(10., y)*m*m;
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| 138 |
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| 139 | }
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| 140 |
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| 141 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 142 |
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| 143 | G4int G4CrossSectionChargeIncreasePartial::RandomSelect(G4double k,
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| 144 | const G4ParticleDefinition* particleDefinition)
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| 145 | {
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| 146 |
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| 147 | G4int particleTypeIndex = 0;
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| 148 | G4DNAGenericIonsManager *instance;
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| 149 | instance = G4DNAGenericIonsManager::Instance();
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| 150 |
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| 151 | if (particleDefinition == instance->GetIon("hydrogen")) return 0;
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| 152 | if (particleDefinition == instance->GetIon("alpha+")) particleTypeIndex=0;
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| 153 | if (particleDefinition == instance->GetIon("helium")) particleTypeIndex=1;
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| 154 |
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| 155 | const G4int n = numberOfPartialCrossSections[particleTypeIndex];
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| 156 | G4double* values(new G4double[n]);
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| 157 | G4double value = 0;
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| 158 | G4int i = n;
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| 159 |
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| 160 | while (i>0)
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| 161 | {
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| 162 | i--;
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| 163 | values[i]=CrossSection(k, i, particleDefinition);
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| 164 | value+=values[i];
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| 165 | }
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| 166 |
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| 167 | value*=G4UniformRand();
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| 168 |
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| 169 | i=n;
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| 170 | while (i>0)
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| 171 | {
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| 172 | i--;
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| 173 |
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| 174 | if (values[i]>value)
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| 175 | break;
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| 176 |
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| 177 | value-=values[i];
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| 178 | }
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| 179 |
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| 180 | delete[] values;
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| 181 |
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| 182 | return i;
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| 183 | }
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| 184 |
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| 185 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo........oooOO0OOooo......
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| 186 |
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| 187 | G4double G4CrossSectionChargeIncreasePartial::Sum(G4double k, const G4ParticleDefinition* particleDefinition)
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| 188 | {
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| 189 | G4int particleTypeIndex = 0;
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| 190 | G4DNAGenericIonsManager *instance;
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| 191 | instance = G4DNAGenericIonsManager::Instance();
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| 192 |
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| 193 | if (particleDefinition == instance->GetIon("alpha+")) particleTypeIndex=0;
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| 194 | if (particleDefinition == instance->GetIon("helium")) particleTypeIndex=1;
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| 195 |
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| 196 | G4double totalCrossSection = 0.;
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| 197 |
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| 198 | for (G4int i=0; i<numberOfPartialCrossSections[particleTypeIndex]; i++)
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| 199 | {
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| 200 | totalCrossSection += CrossSection(k,i,particleDefinition);
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| 201 | }
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| 202 | return totalCrossSection;
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| 203 | }
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| 204 |
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