1 | // |
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2 | // ******************************************************************** |
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3 | // * License and Disclaimer * |
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6 | // * the Geant4 Collaboration. It is provided under the terms and * |
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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: G4ExcitationHandler.hh,v 1.8 2008/09/19 13:32:54 ahoward Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-03-cand-01 $ |
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29 | // |
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30 | // Hadronic Process: Nuclear De-excitations |
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31 | // by V. Lara (May 1998) |
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32 | // |
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33 | // Modif (03 September 2008) by J. M. Quesada for external choice of inverse |
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34 | // cross section option |
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35 | // |
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36 | // Modif (30 June 1998) by V. Lara: |
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37 | // -Using G4ParticleTable and therefore G4IonTable |
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38 | // it can return all kind of fragments produced in |
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39 | // deexcitation |
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40 | // -It uses default algorithms for: |
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41 | // Evaporation: G4StatEvaporation |
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42 | // MultiFragmentation: G4DummyMF (a dummy one) |
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43 | // Fermi Breakup model: G4StatFermiBreakUp |
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44 | // |
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45 | // Modif (03 September 2008) by J. M. Quesada for external choice of inverse |
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46 | // cross section option |
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47 | // JMQ (06 September 2008) Also external choices have been added for |
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48 | // superimposed Coulomb barrier (if useSICBis set true, by default is false) |
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49 | |
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50 | #ifndef G4ExcitationHandler_h |
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51 | #define G4ExcitationHandler_h 1 |
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52 | |
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53 | #include "G4VMultiFragmentation.hh" |
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54 | #include "G4VFermiBreakUp.hh" |
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55 | #include "G4VEvaporation.hh" |
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56 | #include "G4VPhotonEvaporation.hh" |
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57 | #include "G4Fragment.hh" |
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58 | #include "G4DynamicParticle.hh" |
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59 | #include "G4ReactionProductVector.hh" |
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60 | #include "G4ReactionProduct.hh" |
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61 | #include "G4ParticleTypes.hh" |
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62 | #include "G4ParticleTable.hh" |
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63 | // needed for default models |
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64 | #include "G4Evaporation.hh" |
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65 | #include "G4StatMF.hh" |
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66 | #include "G4FermiBreakUp.hh" |
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67 | #include "G4PhotonEvaporation.hh" |
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68 | #include "G4IonConstructor.hh" |
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69 | |
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70 | //#define debug |
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71 | |
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72 | class G4ExcitationHandler |
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73 | { |
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74 | public: |
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75 | G4ExcitationHandler(); |
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76 | ~G4ExcitationHandler(); |
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77 | private: |
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78 | G4ExcitationHandler(const G4ExcitationHandler &right); |
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79 | |
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80 | const G4ExcitationHandler & operator=(const G4ExcitationHandler &right); |
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81 | G4bool operator==(const G4ExcitationHandler &right) const; |
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82 | G4bool operator!=(const G4ExcitationHandler &right) const; |
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83 | |
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84 | |
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85 | public: |
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86 | G4ReactionProductVector * BreakItUp(const G4Fragment &theInitialState) const; |
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87 | |
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88 | void SetEvaporation(G4VEvaporation *const value); |
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89 | |
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90 | void SetMultiFragmentation(G4VMultiFragmentation *const value); |
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91 | |
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92 | void SetFermiModel(G4VFermiBreakUp *const value); |
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93 | |
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94 | void SetPhotonEvaporation(G4VPhotonEvaporation * const value); |
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95 | |
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96 | void SetMaxZForFermiBreakUp(G4int aZ); |
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97 | void SetMaxAForFermiBreakUp(G4int anA); |
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98 | void SetMaxAandZForFermiBreakUp(G4int anA,G4int aZ); |
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99 | void SetMinEForMultiFrag(G4double anE); |
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100 | |
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101 | // for inverse cross section choice |
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102 | inline void SetOPTxs(G4int opt) { OPTxs = opt;} |
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103 | // for superimposed Coulomb Barrir for inverse cross sections |
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104 | inline void UseSICB(){useSICB=true;} |
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105 | |
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106 | private: |
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107 | |
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108 | G4ReactionProductVector * Transform(G4FragmentVector * theFragmentVector) const; |
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109 | |
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110 | const G4VEvaporation * GetEvaporation() const; |
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111 | |
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112 | const G4VMultiFragmentation * GetMultiFragmentation() const; |
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113 | |
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114 | const G4VFermiBreakUp * GetFermiModel() const; |
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115 | |
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116 | const G4VPhotonEvaporation * GetPhotonEvaporation() const; |
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117 | |
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118 | G4int GetMaxZ() const; |
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119 | G4int GetMaxA() const; |
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120 | G4double GetMinE() const; |
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121 | |
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122 | #ifdef debug |
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123 | void CheckConservation(const G4Fragment & aFragment, |
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124 | G4FragmentVector * Result) const; |
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125 | #endif |
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126 | private: |
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127 | |
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128 | G4VEvaporation *theEvaporation; |
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129 | |
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130 | G4VMultiFragmentation *theMultiFragmentation; |
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131 | |
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132 | G4VFermiBreakUp *theFermiModel; |
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133 | |
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134 | G4VPhotonEvaporation * thePhotonEvaporation; |
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135 | |
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136 | G4int maxZForFermiBreakUp; |
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137 | G4int maxAForFermiBreakUp; |
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138 | G4double minEForMultiFrag; |
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139 | |
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140 | G4ParticleTable *theTableOfParticles; |
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141 | |
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142 | G4bool MyOwnEvaporationClass; |
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143 | G4bool MyOwnMultiFragmentationClass; |
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144 | G4bool MyOwnFermiBreakUpClass; |
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145 | G4bool MyOwnPhotonEvaporationClass; |
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146 | |
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147 | G4int OPTxs; |
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148 | G4bool useSICB; |
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149 | |
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150 | struct DeleteFragment |
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151 | { |
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152 | template<typename T> |
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153 | void operator()(const T* ptr) const |
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154 | { |
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155 | delete ptr; |
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156 | } |
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157 | }; |
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158 | |
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159 | |
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160 | }; |
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161 | |
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162 | |
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163 | |
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164 | inline const G4VEvaporation * G4ExcitationHandler::GetEvaporation() const |
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165 | { |
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166 | return theEvaporation; |
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167 | } |
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168 | |
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169 | inline void G4ExcitationHandler::SetEvaporation(G4VEvaporation *const value) |
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170 | { |
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171 | if (theEvaporation != 0 && MyOwnEvaporationClass) delete theEvaporation; |
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172 | MyOwnEvaporationClass = false; |
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173 | theEvaporation = value; |
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174 | } |
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175 | |
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176 | inline const G4VMultiFragmentation * G4ExcitationHandler::GetMultiFragmentation() const |
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177 | { |
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178 | return theMultiFragmentation; |
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179 | } |
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180 | |
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181 | inline void G4ExcitationHandler::SetMultiFragmentation(G4VMultiFragmentation *const value) |
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182 | { |
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183 | if (theMultiFragmentation != 0 && MyOwnMultiFragmentationClass) delete theMultiFragmentation; |
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184 | MyOwnMultiFragmentationClass = false; |
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185 | theMultiFragmentation = value; |
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186 | } |
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187 | |
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188 | inline const G4VFermiBreakUp * G4ExcitationHandler::GetFermiModel() const |
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189 | { |
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190 | return theFermiModel; |
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191 | } |
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192 | |
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193 | inline void G4ExcitationHandler::SetFermiModel(G4VFermiBreakUp *const value) |
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194 | { |
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195 | if (theFermiModel != 0 && MyOwnFermiBreakUpClass) delete theFermiModel; |
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196 | MyOwnFermiBreakUpClass = false; |
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197 | theFermiModel = value; |
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198 | } |
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199 | |
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200 | |
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201 | inline const G4VPhotonEvaporation * G4ExcitationHandler::GetPhotonEvaporation() const |
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202 | { |
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203 | return thePhotonEvaporation; |
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204 | } |
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205 | |
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206 | inline void G4ExcitationHandler::SetPhotonEvaporation(G4VPhotonEvaporation *const value) |
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207 | { |
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208 | if (thePhotonEvaporation != 0 && MyOwnPhotonEvaporationClass) delete thePhotonEvaporation; |
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209 | MyOwnPhotonEvaporationClass = false; |
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210 | thePhotonEvaporation = value; |
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211 | } |
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212 | |
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213 | inline void G4ExcitationHandler::SetMaxZForFermiBreakUp(G4int aZ) |
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214 | { |
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215 | maxZForFermiBreakUp = aZ; |
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216 | } |
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217 | |
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218 | inline void G4ExcitationHandler::SetMaxAForFermiBreakUp(G4int anA) |
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219 | { |
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220 | maxAForFermiBreakUp = anA; |
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221 | } |
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222 | |
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223 | inline void G4ExcitationHandler::SetMaxAandZForFermiBreakUp(G4int anA, G4int aZ) |
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224 | { |
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225 | maxAForFermiBreakUp = anA; |
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226 | maxZForFermiBreakUp = aZ; |
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227 | } |
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228 | |
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229 | inline void G4ExcitationHandler::SetMinEForMultiFrag(G4double anE) |
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230 | { |
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231 | minEForMultiFrag = anE; |
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232 | } |
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233 | |
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234 | inline G4int G4ExcitationHandler::GetMaxZ() const |
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235 | { |
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236 | return maxZForFermiBreakUp; |
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237 | } |
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238 | |
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239 | inline G4int G4ExcitationHandler::GetMaxA() const |
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240 | { |
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241 | return maxAForFermiBreakUp; |
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242 | } |
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243 | |
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244 | inline G4double G4ExcitationHandler::GetMinE() const |
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245 | { |
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246 | return minEForMultiFrag; |
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247 | } |
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248 | |
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249 | |
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250 | #endif |
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