| 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 | //
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| 27 | // $Id: G4IonisParamMat.cc,v 1.20 2007/09/27 14:05:47 vnivanch Exp $
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| 28 | // GEANT4 tag $Name: geant4-09-01-patch-02 $
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| 29 | //
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| 30 | //
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| 31 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 32 |
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| 33 | // 09-07-98, data moved from G4Material, M.Maire
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| 34 | // 18-07-98, bug corrected in ComputeDensityEffect() for gas
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| 35 | // 16-01-01, bug corrected in ComputeDensityEffect() E100eV (L.Urban)
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| 36 | // 08-02-01, fShellCorrectionVector correctly handled (mma)
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| 37 | // 28-10-02, add setMeanExcitationEnergy (V.Ivanchenko)
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| 38 | // 06-09-04, factor 2 to shell correction term (V.Ivanchenko)
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| 39 | // 10-05-05, add a missing coma in FindMeanExcitationEnergy() - Bug#746 (mma)
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| 40 | // 27-09-07, add computation of parameters for ions (V.Ivanchenko)
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| 41 |
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| 42 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 43 |
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| 44 | #include "G4IonisParamMat.hh"
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| 45 | #include "G4Material.hh"
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| 46 | #include "G4NistManager.hh"
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| 47 |
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| 48 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 49 |
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| 50 | G4IonisParamMat::G4IonisParamMat(G4Material* material)
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| 51 | : fMaterial(material)
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| 52 | {
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| 53 | ComputeMeanParameters();
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| 54 | ComputeDensityEffect();
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| 55 | ComputeFluctModel();
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| 56 | ComputeIonParameters();
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| 57 | }
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| 58 |
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| 59 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 60 |
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| 61 | // Fake default constructor - sets only member data and allocates memory
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| 62 | // for usage restricted to object persistency
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| 63 |
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| 64 | G4IonisParamMat::G4IonisParamMat(__void__&)
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| 65 | : fMaterial(0), fShellCorrectionVector(0)
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| 66 | {
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| 67 | }
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| 68 |
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| 69 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 70 |
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| 71 | void G4IonisParamMat::ComputeMeanParameters()
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| 72 | {
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| 73 | // compute mean excitation energy and shell correction vector
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| 74 |
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| 75 | fTaul = (*(fMaterial->GetElementVector()))[0]->GetIonisation()->GetTaul();
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| 76 |
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| 77 | fMeanExcitationEnergy = 0.;
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| 78 | fLogMeanExcEnergy = 0.;
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| 79 |
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| 80 |
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| 81 | for (size_t i=0; i < fMaterial->GetNumberOfElements(); i++) {
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| 82 | fLogMeanExcEnergy +=
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| 83 | (fMaterial->GetVecNbOfAtomsPerVolume())[i]
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| 84 | *((*(fMaterial->GetElementVector()))[i]->GetZ())
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| 85 | *std::log((*(fMaterial->GetElementVector()))[i]->GetIonisation()
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| 86 | ->GetMeanExcitationEnergy());
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| 87 | }
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| 88 |
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| 89 | fLogMeanExcEnergy /= fMaterial->GetTotNbOfElectPerVolume();
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| 90 | fMeanExcitationEnergy = std::exp(fLogMeanExcEnergy);
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| 91 |
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| 92 | fShellCorrectionVector = new G4double[3]; //[3]
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| 93 |
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| 94 | for (G4int j=0; j<=2; j++)
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| 95 | {
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| 96 | fShellCorrectionVector[j] = 0.;
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| 97 |
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| 98 | for (size_t k=0; k<fMaterial->GetNumberOfElements(); k++) {
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| 99 | fShellCorrectionVector[j] += (fMaterial->GetVecNbOfAtomsPerVolume())[k]
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| 100 | *((*(fMaterial->GetElementVector()))[k]->GetIonisation()
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| 101 | ->GetShellCorrectionVector()[j]);
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| 102 | }
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| 103 | fShellCorrectionVector[j] *= 2.0/fMaterial->GetTotNbOfElectPerVolume();
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| 104 | }
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| 105 | }
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| 106 |
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| 107 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 108 |
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| 109 | void G4IonisParamMat::ComputeDensityEffect()
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| 110 | {
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| 111 | // Compute parameters for the density effect correction in DE/Dx formula.
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| 112 | // The parametrization is from R.M. Sternheimer, Phys. Rev.B,3:3681 (1971)
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| 113 |
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| 114 | const G4double Cd2 = 4*pi*hbarc_squared*classic_electr_radius;
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| 115 | const G4double twoln10 = 2.*std::log(10.);
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| 116 |
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| 117 | G4int icase;
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| 118 |
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| 119 | fCdensity = 1. + std::log(fMeanExcitationEnergy*fMeanExcitationEnergy
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| 120 | /(Cd2*fMaterial->GetTotNbOfElectPerVolume()));
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| 121 |
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| 122 | //
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| 123 | // condensed materials
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| 124 | //
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| 125 | G4State State = fMaterial->GetState();
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| 126 |
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| 127 | if ((State == kStateSolid)||(State == kStateLiquid)) {
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| 128 |
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| 129 | const G4double E100eV = 100.*eV;
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| 130 | const G4double ClimiS[] = {3.681 , 5.215 };
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| 131 | const G4double X0valS[] = {1.0 , 1.5 };
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| 132 | const G4double X1valS[] = {2.0 , 3.0 };
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| 133 |
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| 134 | if(fMeanExcitationEnergy < E100eV) icase = 0;
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| 135 | else icase = 1;
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| 136 |
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| 137 | if(fCdensity < ClimiS[icase]) fX0density = 0.2;
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| 138 | else fX0density = 0.326*fCdensity-X0valS[icase];
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| 139 |
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| 140 | fX1density = X1valS[icase] ; fMdensity = 3.0;
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| 141 |
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| 142 | //special: Hydrogen
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| 143 | if ((fMaterial->GetNumberOfElements()==1)&&(fMaterial->GetZ()==1.)) {
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| 144 | fX0density = 0.425; fX1density = 2.0; fMdensity = 5.949;
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| 145 | }
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| 146 | }
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| 147 |
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| 148 | //
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| 149 | // gases
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| 150 | //
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| 151 | if (State == kStateGas) {
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| 152 |
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| 153 | const G4double ClimiG[] = { 10. , 10.5 , 11. , 11.5 , 12.25 , 13.804};
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| 154 | const G4double X0valG[] = { 1.6 , 1.7 , 1.8 , 1.9 , 2.0 , 2.0 };
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| 155 | const G4double X1valG[] = { 4.0 , 4.0 , 4.0 , 4.0 , 4.0 , 5.0 };
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| 156 |
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| 157 | icase = 5;
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| 158 | fX0density = 0.326*fCdensity-2.5 ; fX1density = 5.0 ; fMdensity = 3. ;
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| 159 | while((icase > 0)&&(fCdensity < ClimiG[icase])) icase-- ;
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| 160 | fX0density = X0valG[icase] ; fX1density = X1valG[icase] ;
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| 161 |
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| 162 | //special: Hydrogen
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| 163 | if ((fMaterial->GetNumberOfElements()==1)&&(fMaterial->GetZ()==1.)) {
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| 164 | fX0density = 1.837; fX1density = 3.0; fMdensity = 4.754;
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| 165 | }
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| 166 |
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| 167 | //special: Helium
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| 168 | if ((fMaterial->GetNumberOfElements()==1)&&(fMaterial->GetZ()==2.)) {
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| 169 | fX0density = 2.191; fX1density = 3.0; fMdensity = 3.297;
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| 170 | }
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| 171 |
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| 172 | // change parameters if the gas is not in STP.
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| 173 | // For the correction the density(STP) is needed.
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| 174 | // Density(STP) is calculated here :
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| 175 |
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| 176 | G4double Density = fMaterial->GetDensity();
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| 177 | G4double Pressure = fMaterial->GetPressure();
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| 178 | G4double Temp = fMaterial->GetTemperature();
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| 179 |
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| 180 | G4double DensitySTP = Density*STP_Pressure*Temp/(Pressure*STP_Temperature);
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| 181 |
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| 182 | G4double ParCorr = std::log(Density/DensitySTP);
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| 183 |
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| 184 | fCdensity -= ParCorr;
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| 185 | fX0density -= ParCorr/twoln10;
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| 186 | fX1density -= ParCorr/twoln10;
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| 187 | }
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| 188 |
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| 189 | G4double Xa = fCdensity/twoln10;
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| 190 | fAdensity = twoln10*(Xa-fX0density)
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| 191 | /std::pow((fX1density-fX0density),fMdensity);
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| 192 | }
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| 193 |
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| 194 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 195 |
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| 196 | void G4IonisParamMat::ComputeFluctModel()
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| 197 | {
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| 198 | // compute parameters for the energy loss fluctuation model
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| 199 |
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| 200 | // need an 'effective Z' ?????
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| 201 | G4double Zeff = 0.;
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| 202 | for (size_t i=0;i<fMaterial->GetNumberOfElements();i++)
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| 203 | Zeff += (fMaterial->GetFractionVector())[i]
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| 204 | *((*(fMaterial->GetElementVector()))[i]->GetZ());
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| 205 |
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| 206 | if (Zeff > 2.) fF2fluct = 2./Zeff ;
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| 207 | else fF2fluct = 0.;
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| 208 |
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| 209 | fF1fluct = 1. - fF2fluct;
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| 210 | fEnergy2fluct = 10.*Zeff*Zeff*eV;
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| 211 | fLogEnergy2fluct = std::log(fEnergy2fluct);
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| 212 | fLogEnergy1fluct = (fLogMeanExcEnergy - fF2fluct*fLogEnergy2fluct)
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| 213 | /fF1fluct;
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| 214 | fEnergy1fluct = std::exp(fLogEnergy1fluct);
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| 215 | fEnergy0fluct = 10.*eV;
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| 216 | fRateionexcfluct = 0.4;
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| 217 | }
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| 218 |
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| 219 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 220 |
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| 221 | void G4IonisParamMat::ComputeIonParameters()
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| 222 | {
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| 223 | // compute parameters for ion transport
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| 224 | // The aproximation from:
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| 225 | // J.F.Ziegler, J.P. Biersack, U. Littmark
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| 226 | // The Stopping and Range of Ions in Matter,
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| 227 | // Vol.1, Pergamon Press, 1985
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| 228 | // Fast ions or hadrons
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| 229 |
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| 230 | static G4double vFermi[92] = {
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| 231 | 1.0309, 0.15976, 0.59782, 1.0781, 1.0486, 1.0, 1.058, 0.93942, 0.74562, 0.3424,
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| 232 | 0.45259, 0.71074, 0.90519, 0.97411, 0.97184, 0.89852, 0.70827, 0.39816, 0.36552, 0.62712,
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| 233 | 0.81707, 0.9943, 1.1423, 1.2381, 1.1222, 0.92705, 1.0047, 1.2, 1.0661, 0.97411,
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| 234 | 0.84912, 0.95, 1.0903, 1.0429, 0.49715, 0.37755, 0.35211, 0.57801, 0.77773, 1.0207,
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| 235 | 1.029, 1.2542, 1.122, 1.1241, 1.0882, 1.2709, 1.2542, 0.90094, 0.74093, 0.86054,
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| 236 | 0.93155, 1.0047, 0.55379, 0.43289, 0.32636, 0.5131, 0.695, 0.72591, 0.71202, 0.67413,
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| 237 | 0.71418, 0.71453, 0.5911, 0.70263, 0.68049, 0.68203, 0.68121, 0.68532, 0.68715, 0.61884,
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| 238 | 0.71801, 0.83048, 1.1222, 1.2381, 1.045, 1.0733, 1.0953, 1.2381, 1.2879, 0.78654,
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| 239 | 0.66401, 0.84912, 0.88433, 0.80746, 0.43357, 0.41923, 0.43638, 0.51464, 0.73087, 0.81065,
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| 240 | 1.9578, 1.0257} ;
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| 241 |
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| 242 | static G4double lFactor[92] = {
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| 243 | 1.0, 1.0, 1.1, 1.06, 1.01, 1.03, 1.04, 0.99, 0.95, 0.9,
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| 244 | 0.82, 0.81, 0.83, 0.88, 1.0, 0.95, 0.97, 0.99, 0.98, 0.97,
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| 245 | 0.98, 0.97, 0.96, 0.93, 0.91, 0.9, 0.88, 0.9, 0.9, 0.9,
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| 246 | 0.9, 0.85, 0.9, 0.9, 0.91, 0.92, 0.9, 0.9, 0.9, 0.9,
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| 247 | 0.9, 0.88, 0.9, 0.88, 0.88, 0.9, 0.9, 0.88, 0.9, 0.9,
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| 248 | 0.9, 0.9, 0.96, 1.2, 0.9, 0.88, 0.88, 0.85, 0.9, 0.9,
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| 249 | 0.92, 0.95, 0.99, 1.03, 1.05, 1.07, 1.08, 1.1, 1.08, 1.08,
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| 250 | 1.08, 1.08, 1.09, 1.09, 1.1, 1.11, 1.12, 1.13, 1.14, 1.15,
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| 251 | 1.17, 1.2, 1.18, 1.17, 1.17, 1.16, 1.16, 1.16, 1.16, 1.16,
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| 252 | 1.16, 1.16} ;
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| 253 |
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| 254 | // get elements in the actual material,
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| 255 | const G4ElementVector* theElementVector = fMaterial->GetElementVector() ;
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| 256 | const G4double* theAtomicNumDensityVector =
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| 257 | fMaterial->GetAtomicNumDensityVector() ;
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| 258 | const G4int NumberOfElements = fMaterial->GetNumberOfElements() ;
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| 259 |
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| 260 | // loop for the elements in the material
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| 261 | // to find out average values Z, vF, lF
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| 262 | G4double z = 0.0, vF = 0.0, lF = 0.0, norm = 0.0 ;
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| 263 |
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| 264 | if( 1 == NumberOfElements ) {
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| 265 | z = fMaterial->GetZ() ;
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| 266 | G4int iz = G4int(z) - 1 ;
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| 267 | if(iz < 0) iz = 0 ;
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| 268 | else if(iz > 91) iz = 91 ;
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| 269 | vF = vFermi[iz] ;
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| 270 | lF = lFactor[iz] ;
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| 271 |
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| 272 | } else {
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| 273 | for (G4int iel=0; iel<NumberOfElements; iel++)
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| 274 | {
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| 275 | const G4Element* element = (*theElementVector)[iel] ;
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| 276 | G4double z2 = element->GetZ() ;
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| 277 | const G4double weight = theAtomicNumDensityVector[iel] ;
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| 278 | norm += weight ;
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| 279 | z += z2 * weight ;
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| 280 | G4int iz = G4int(z2) - 1 ;
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| 281 | if(iz < 0) iz = 0 ;
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| 282 | else if(iz > 91) iz =91 ;
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| 283 | vF += vFermi[iz] * weight ;
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| 284 | lF += lFactor[iz] * weight ;
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| 285 | }
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| 286 | z /= norm ;
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| 287 | vF /= norm ;
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| 288 | lF /= norm ;
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| 289 | }
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| 290 | fZeff = z;
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| 291 | fLfactor = lF;
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| 292 | fFermiEnergy = 25.*keV*vF*vF;
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| 293 | }
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| 294 |
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| 295 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 296 |
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| 297 | void G4IonisParamMat::SetMeanExcitationEnergy(G4double value)
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| 298 | {
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| 299 | if(value == fMeanExcitationEnergy || value <= 0.0) return;
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| 300 |
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| 301 | if (G4NistManager::Instance()->GetVerbose() > 0)
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| 302 | G4cout << "G4Material: Mean excitation energy is changed for "
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| 303 | << fMaterial->GetName()
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| 304 | << " Iold= " << fMeanExcitationEnergy/eV
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| 305 | << "eV; Inew= " << value/eV << " eV;"
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| 306 | << G4endl;
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| 307 |
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| 308 | fMeanExcitationEnergy = value;
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| 309 | fLogMeanExcEnergy = std::log(value);
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| 310 | ComputeDensityEffect();
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| 311 | ComputeFluctModel();
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| 312 | }
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| 313 |
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| 314 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 315 |
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| 316 | G4double G4IonisParamMat::FindMeanExcitationEnergy(const G4String& chFormula)
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| 317 | {
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| 318 |
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| 319 | // The data on mean excitation energy for compaunds
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| 320 | // from "Stopping Powers for Electrons and Positrons"
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| 321 | // ICRU Report N#37, 1984 (energy in eV)
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| 322 |
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| 323 | const size_t numberOfMolecula = 79 ;
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| 324 |
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| 325 | static G4String name[numberOfMolecula] = {
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| 326 |
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| 327 | // gas
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| 328 | "NH_3", "C_4H_10", "CO_2", "C_2H_6", "C_7H_16",
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| 329 | "C_6H_14", "CH_4", "NO", "N_2O", "C_8H_18",
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| 330 | "C_5H_12", "C_3H_8", "H_2O-Gas",
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| 331 |
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| 332 | // liquid
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| 333 | "C_3H_6O", "C_6H_5NH_2", "C_6H_6", "C_4H_9OH", "CCl_4",
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| 334 | "C_6H_5Cl", "CHCl_3", "C_6H_12", "C_6H_4Cl_2", "C_4Cl_2H_8O",
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| 335 | "C_2Cl_2H_4", "(C_2H_5)_2O", "C_2H_5OH", "C_3H_5(OH)_3","C_7H_16",
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| 336 | "C_6H_14", "CH_3OH", "C_6H_5NO_2","C_5H_12", "C_3H_7OH",
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| 337 | "C_5H_5N", "C_8H_8", "C_2Cl_4", "C_7H_8", "C_2Cl_3H",
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| 338 | "H_2O", "C_8H_10",
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| 339 |
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| 340 | //solid
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| 341 | "C_5H_5N_5", "C_5H_5N_5O", "(C_6H_11NO)-nylon", "C_25H_52",
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| 342 | "(C_2H_4)-Polyethylene", "(C_5H_8O-2)-Polymethil_Methacrylate",
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| 343 | "(C_8H_8)-Polystyrene", "A-150-tissue", "Al_2O_3", "CaF_2",
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| 344 | "LiF", "Photo_Emulsion", "(C_2F_4)-Teflon", "SiO_2"
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| 345 |
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| 346 | } ;
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| 347 |
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| 348 | static G4double meanExcitation[numberOfMolecula] = {
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| 349 |
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| 350 | 53.7, 48.3, 85.0, 45.4, 49.2,
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| 351 | 49.1, 41.7, 87.8, 84.9, 49.5,
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| 352 | 48.2, 47.1, 71.6,
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| 353 |
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| 354 | 64.2, 66.2, 63.4, 59.9, 166.3,
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| 355 | 89.1, 156.0, 56.4, 106.5, 103.3,
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| 356 | 111.9, 60.0, 62.9, 72.6, 54.4,
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| 357 | 54.0, 67.6, 75.8, 53.6, 61.1,
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| 358 | 66.2, 64.0, 159.2, 62.5, 148.1,
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| 359 | 75.0, 61.8,
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| 360 |
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| 361 | 71.4, 75.0, 63.9, 48.3, 57.4,
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| 362 | 74.0, 68.7, 65.1, 145.2, 166.,
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| 363 | 94.0, 331.0, 99.1, 139.2
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| 364 |
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| 365 | } ;
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| 366 |
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| 367 | G4double x = fMeanExcitationEnergy;
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| 368 |
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| 369 | for(size_t i=0; i<numberOfMolecula; i++) {
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| 370 | if(chFormula == name[i]) {
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| 371 | x = meanExcitation[i]*eV;
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| 372 | break;
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| 373 | }
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| 374 | }
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| 375 | return x;
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| 376 | }
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| 377 |
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| 378 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 379 |
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| 380 | G4IonisParamMat::~G4IonisParamMat()
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| 381 | {
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| 382 | if (fShellCorrectionVector) delete [] fShellCorrectionVector;
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| 383 | }
|
|---|
| 384 |
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| 385 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 386 |
|
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| 387 | G4IonisParamMat::G4IonisParamMat(const G4IonisParamMat& right)
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| 388 | {
|
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| 389 | *this = right;
|
|---|
| 390 | }
|
|---|
| 391 |
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| 392 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
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| 393 |
|
|---|
| 394 | const G4IonisParamMat& G4IonisParamMat::operator=(const G4IonisParamMat& right)
|
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| 395 | {
|
|---|
| 396 | if (this != &right)
|
|---|
| 397 | {
|
|---|
| 398 | fMaterial = right.fMaterial;
|
|---|
| 399 | fMeanExcitationEnergy = right.fMeanExcitationEnergy;
|
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| 400 | fLogMeanExcEnergy = right.fLogMeanExcEnergy;
|
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| 401 | if (fShellCorrectionVector) delete [] fShellCorrectionVector;
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| 402 | fShellCorrectionVector = new G4double[3];
|
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| 403 | fShellCorrectionVector[0] = right.fShellCorrectionVector[0];
|
|---|
| 404 | fShellCorrectionVector[1] = right.fShellCorrectionVector[1];
|
|---|
| 405 | fShellCorrectionVector[2] = right.fShellCorrectionVector[2];
|
|---|
| 406 | fTaul = right.fTaul;
|
|---|
| 407 | fCdensity = right.fCdensity;
|
|---|
| 408 | fMdensity = right.fMdensity;
|
|---|
| 409 | fAdensity = right.fAdensity;
|
|---|
| 410 | fX0density = right.fX0density;
|
|---|
| 411 | fX1density = right.fX1density;
|
|---|
| 412 | fF1fluct = right.fF1fluct;
|
|---|
| 413 | fF2fluct = right.fF2fluct;
|
|---|
| 414 | fEnergy1fluct = right.fEnergy1fluct;
|
|---|
| 415 | fLogEnergy1fluct = right.fLogEnergy1fluct;
|
|---|
| 416 | fEnergy2fluct = right.fEnergy2fluct;
|
|---|
| 417 | fLogEnergy2fluct = right.fLogEnergy2fluct;
|
|---|
| 418 | fEnergy0fluct = right.fEnergy0fluct;
|
|---|
| 419 | fRateionexcfluct = right.fRateionexcfluct;
|
|---|
| 420 | }
|
|---|
| 421 | return *this;
|
|---|
| 422 | }
|
|---|
| 423 |
|
|---|
| 424 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
|
|---|
| 425 |
|
|---|
| 426 | G4int G4IonisParamMat::operator==(const G4IonisParamMat& right) const
|
|---|
| 427 | {
|
|---|
| 428 | return (this == (G4IonisParamMat*) &right);
|
|---|
| 429 | }
|
|---|
| 430 |
|
|---|
| 431 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
|
|---|
| 432 |
|
|---|
| 433 | G4int G4IonisParamMat::operator!=(const G4IonisParamMat& right) const
|
|---|
| 434 | {
|
|---|
| 435 | return (this != (G4IonisParamMat*) &right);
|
|---|
| 436 | }
|
|---|
| 437 |
|
|---|
| 438 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo....
|
|---|
| 439 |
|
|---|