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2 | // ******************************************************************** |
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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 | } |
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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; |
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390 | } |
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391 | |
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392 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo.... |
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393 | |
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394 | const G4IonisParamMat& G4IonisParamMat::operator=(const G4IonisParamMat& right) |
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395 | { |
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396 | if (this != &right) |
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397 | { |
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398 | fMaterial = right.fMaterial; |
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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]; |
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404 | fShellCorrectionVector[1] = right.fShellCorrectionVector[1]; |
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405 | fShellCorrectionVector[2] = right.fShellCorrectionVector[2]; |
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406 | fTaul = right.fTaul; |
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407 | fCdensity = right.fCdensity; |
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408 | fMdensity = right.fMdensity; |
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409 | fAdensity = right.fAdensity; |
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410 | fX0density = right.fX0density; |
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411 | fX1density = right.fX1density; |
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412 | fF1fluct = right.fF1fluct; |
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413 | fF2fluct = right.fF2fluct; |
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414 | fEnergy1fluct = right.fEnergy1fluct; |
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415 | fLogEnergy1fluct = right.fLogEnergy1fluct; |
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416 | fEnergy2fluct = right.fEnergy2fluct; |
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417 | fLogEnergy2fluct = right.fLogEnergy2fluct; |
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418 | fEnergy0fluct = right.fEnergy0fluct; |
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419 | fRateionexcfluct = right.fRateionexcfluct; |
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420 | } |
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421 | return *this; |
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422 | } |
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423 | |
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424 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo.... |
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425 | |
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426 | G4int G4IonisParamMat::operator==(const G4IonisParamMat& right) const |
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427 | { |
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428 | return (this == (G4IonisParamMat*) &right); |
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429 | } |
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430 | |
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431 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo.... |
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432 | |
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433 | G4int G4IonisParamMat::operator!=(const G4IonisParamMat& right) const |
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434 | { |
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435 | return (this != (G4IonisParamMat*) &right); |
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436 | } |
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437 | |
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438 | //....oooOO0OOooo........oooOO0OOooo........oooOO0OOooo.... ....oooOO0OOooo.... |
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439 | |
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