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: G4AblaDataDefs.hh,v 1.6 2007/12/03 19:36:06 miheikki Exp $ |
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27 | // Translation of INCL4.2/ABLA V3 |
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28 | // Pekka Kaitaniemi, HIP (translation) |
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29 | // Christelle Schmidt, IPNL (fission code) |
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30 | // Alain Boudard, CEA (contact person INCL/ABLA) |
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31 | // Aatos Heikkinen, HIP (project coordination) |
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32 | |
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33 | // Data structures needed by ABLA evaporation code. |
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34 | |
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35 | #ifndef G4AblaDataDefs_hh |
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36 | #define G4AblaDataDefs_hh 1 |
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37 | |
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38 | // ABLA |
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39 | |
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40 | class G4Nevent { |
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41 | public: |
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42 | G4Nevent() {}; |
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43 | ~G4Nevent() {}; |
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44 | |
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45 | G4int ii; |
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46 | }; |
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47 | |
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48 | // ABLA |
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49 | #define PACESIZEROWS 500 |
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50 | #define PACESIZECOLS 500 |
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51 | /** |
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52 | * Masses. |
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53 | */ |
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54 | |
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55 | class G4Pace { |
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56 | |
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57 | public: |
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58 | G4Pace() {}; |
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59 | |
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60 | ~G4Pace() {}; |
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61 | |
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62 | G4double dm[PACESIZEROWS][PACESIZECOLS]; |
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63 | }; |
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64 | |
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65 | #define EC2SUBROWS 154 |
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66 | #define EC2SUBCOLS 99 |
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67 | /** |
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68 | * |
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69 | */ |
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70 | |
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71 | class G4Ec2sub { |
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72 | public: |
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73 | G4Ec2sub() {}; |
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74 | |
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75 | ~G4Ec2sub() {}; |
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76 | |
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77 | G4double ecnz[EC2SUBROWS][EC2SUBCOLS]; |
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78 | }; |
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79 | |
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80 | class G4Ald { |
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81 | public: |
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82 | /** |
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83 | * |
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84 | */ |
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85 | G4Ald() {}; |
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86 | ~G4Ald() {}; |
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87 | |
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88 | G4double av,as,ak,optafan; |
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89 | }; |
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90 | |
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91 | class G4Ablamain { |
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92 | public: |
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93 | G4Ablamain() {}; |
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94 | ~G4Ablamain() {}; |
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95 | |
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96 | G4double ap,zp,at,zt,eap,beta,bmaxnuc,crtot,crnuc,r_0, r_p,r_t,pi,bfpro,snpro,sppro,shell; |
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97 | G4int imax, inum; |
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98 | }; |
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99 | |
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100 | #define ECLDROWS 154 |
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101 | #define ECLDCOLS 99 |
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102 | /** |
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103 | * Shell corrections and deformations. |
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104 | */ |
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105 | |
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106 | class G4Ecld { |
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107 | |
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108 | public: |
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109 | G4Ecld() {}; |
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110 | ~G4Ecld() {}; |
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111 | |
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112 | /** |
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113 | * Ground state shell correction frldm for a spherical ground state. |
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114 | */ |
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115 | G4double ecgnz[ECLDROWS][ECLDCOLS]; |
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116 | |
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117 | /** |
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118 | * Shell correction for the saddle point (now: == 0). |
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119 | */ |
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120 | G4double ecfnz[ECLDROWS][ECLDCOLS]; |
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121 | |
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122 | /** |
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123 | * Difference between deformed ground state and ldm value. |
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124 | */ |
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125 | G4double vgsld[ECLDROWS][ECLDCOLS]; |
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126 | |
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127 | /** |
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128 | * Alpha ground state deformation (this is not beta2!) |
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129 | * beta2 = std::sqrt(5/(4pi)) * alpha |
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130 | */ |
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131 | G4double alpha[ECLDROWS][ECLDCOLS]; |
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132 | }; |
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133 | |
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134 | class G4Fiss { |
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135 | /** |
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136 | * Options and parameters for fission channel. |
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137 | */ |
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138 | |
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139 | public: |
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140 | G4Fiss() {}; |
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141 | ~G4Fiss() {}; |
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142 | |
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143 | G4double akap,bet,homega,koeff,ifis; |
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144 | G4int optshp, optxfis,optles,optcol; |
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145 | }; |
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146 | |
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147 | #define FBROWS 101 |
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148 | #define FBCOLS 161 |
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149 | /** |
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150 | * Fission barriers. |
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151 | */ |
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152 | |
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153 | class G4Fb { |
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154 | |
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155 | public: |
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156 | G4Fb() {}; |
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157 | ~G4Fb() {;} |
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158 | |
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159 | // G4double efa[FBROWS][FBCOLS]; |
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160 | G4double efa[FBCOLS][FBROWS]; |
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161 | }; |
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162 | |
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163 | /** |
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164 | * Options |
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165 | */ |
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166 | |
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167 | class G4Opt { |
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168 | |
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169 | public: |
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170 | G4Opt() {}; |
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171 | ~G4Opt() {}; |
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172 | |
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173 | G4int optemd,optcha; |
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174 | G4double eefac; |
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175 | }; |
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176 | |
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177 | #define EENUCSIZE 2002 |
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178 | #define XHESIZE 50 |
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179 | class G4Eenuc { |
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180 | public: |
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181 | G4Eenuc() {}; |
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182 | ~G4Eenuc() {}; |
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183 | |
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184 | G4double she[EENUCSIZE],xhe[XHESIZE][EENUCSIZE]; |
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185 | }; |
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186 | |
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187 | #define EMDPARSIZE 1000 |
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188 | /** |
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189 | * Energies widths and cross sections for em excitation. |
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190 | */ |
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191 | |
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192 | class G4Emdpar { |
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193 | |
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194 | public: |
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195 | G4Emdpar() {}; |
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196 | ~G4Emdpar() {}; |
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197 | |
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198 | G4double egdr,egqr,fwhmgdr,fwhmgqr,cremde1,cremde2; |
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199 | G4double ae1[EMDPARSIZE],be1[EMDPARSIZE],ce1[EMDPARSIZE],ae2[EMDPARSIZE]; |
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200 | G4double be2[EMDPARSIZE],ce2[EMDPARSIZE],sre1[EMDPARSIZE],sre2[EMDPARSIZE]; |
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201 | G4double xre1[EMDPARSIZE],xre2[EMDPARSIZE],ds1,ds2; |
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202 | }; |
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203 | |
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204 | //#define VOLANTSIZE 200 |
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205 | #define VOLANTSIZE 2000 |
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206 | /** |
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207 | * Evaporation and fission output data. |
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208 | */ |
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209 | |
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210 | class G4Volant { |
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211 | |
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212 | public: |
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213 | G4Volant() {}; |
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214 | ~G4Volant() {}; |
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215 | |
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216 | void dump() |
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217 | { |
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218 | G4cout <<"i \t ACV \t ZPCV \t PCV" << G4endl; |
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219 | for(G4int i = 0; i <= iv; i++) { |
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220 | G4cout << "volant" << i << "\t" << acv[i] << " \t " << zpcv[i] << " \t " << pcv[i] << G4endl; |
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221 | } |
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222 | } |
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223 | |
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224 | G4double acv[VOLANTSIZE],zpcv[VOLANTSIZE],pcv[VOLANTSIZE],xcv[VOLANTSIZE]; |
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225 | G4double ycv[VOLANTSIZE],zcv[VOLANTSIZE]; |
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226 | G4int iv; |
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227 | }; |
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228 | |
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229 | #endif |
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