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: G4He3GEMProbability.cc,v 1.4 2006/06/29 20:22:15 gunter Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-02-ref-02 $ |
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29 | // |
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30 | // Hadronic Process: Nuclear De-excitations |
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31 | // by V. Lara (Nov 1999) |
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32 | // |
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33 | |
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34 | |
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35 | #include "G4He3GEMProbability.hh" |
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36 | |
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37 | G4He3GEMProbability::G4He3GEMProbability() : |
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38 | G4GEMProbability(3,2,1.0/2.0) // A,Z,Gamma |
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39 | { |
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40 | SetExcitationEnergiesPtr(&ExcitEnergies); |
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41 | SetExcitationSpinsPtr(&ExcitSpins); |
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42 | SetExcitationLifetimesPtr(&ExcitLifetimes); |
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43 | } |
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44 | |
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45 | |
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46 | G4He3GEMProbability::G4He3GEMProbability(const G4He3GEMProbability &) : G4GEMProbability() |
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47 | { |
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48 | throw G4HadronicException(__FILE__, __LINE__, "G4He3GEMProbability::copy_constructor meant to not be accessable"); |
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49 | } |
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50 | |
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51 | |
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52 | |
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53 | |
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54 | const G4He3GEMProbability & G4He3GEMProbability:: |
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55 | operator=(const G4He3GEMProbability &) |
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56 | { |
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57 | throw G4HadronicException(__FILE__, __LINE__, "G4He3GEMProbability::operator= meant to not be accessable"); |
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58 | return *this; |
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59 | } |
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60 | |
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61 | |
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62 | G4bool G4He3GEMProbability::operator==(const G4He3GEMProbability &) const |
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63 | { |
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64 | return false; |
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65 | } |
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66 | |
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67 | G4bool G4He3GEMProbability::operator!=(const G4He3GEMProbability &) const |
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68 | { |
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69 | return true; |
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70 | } |
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71 | |
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72 | |
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73 | G4double G4He3GEMProbability::CCoeficient(const G4double aZ) const |
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74 | { |
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75 | // Data comes from |
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76 | // Dostrovsky, Fraenkel and Friedlander |
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77 | // Physical Review, vol 116, num. 3 1959 |
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78 | // |
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79 | // const G4int size = 5; |
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80 | // G4double Zlist[5] = { 10.0, 20.0, 30.0, 50.0, 70.0}; |
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81 | // G4double Calpha[5] = { 0.10, 0.10, 0.10, 0.08, 0.06}; |
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82 | // C for He3 is equal to C for alpha times 4/3 |
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83 | G4double C = 0.0; |
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84 | |
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85 | |
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86 | if (aZ <= 30) { |
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87 | C = 0.10; |
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88 | } else if (aZ <= 50) { |
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89 | C = 0.1 + -((aZ-50.)/20.)*0.02; |
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90 | } else if (aZ < 70) { |
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91 | C = 0.08 + -((aZ-70.)/20.)*0.02; |
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92 | } else { |
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93 | C = 0.06; |
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94 | } |
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95 | return C*(4.0/3.0); |
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96 | } |
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97 | |
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