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 | // Hadronic Process: Nuclear De-excitations |
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28 | // by V. Lara |
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29 | |
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30 | inline G4FermiIntegerPartition::G4FermiIntegerPartition() |
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31 | : total(0), enableNull(false) |
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32 | { |
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33 | } |
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34 | |
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35 | inline G4FermiIntegerPartition::~G4FermiIntegerPartition() |
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36 | { |
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37 | } |
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38 | |
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39 | inline G4FermiIntegerPartition::G4FermiIntegerPartition(const G4FermiIntegerPartition& right) |
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40 | : total(right.total), enableNull(right.enableNull), partition(right.partition) |
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41 | { |
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42 | } |
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43 | |
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44 | |
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45 | inline const G4FermiIntegerPartition& |
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46 | G4FermiIntegerPartition::operator=(const G4FermiIntegerPartition& right) |
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47 | { |
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48 | total=right.total; |
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49 | enableNull=right.enableNull; |
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50 | partition=right.partition; |
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51 | return *this; |
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52 | } |
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53 | |
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54 | inline G4bool G4FermiIntegerPartition:: |
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55 | operator==(const G4FermiIntegerPartition& right) |
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56 | { |
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57 | return (total == right.total && |
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58 | enableNull == enableNull && |
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59 | partition == right.partition); |
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60 | } |
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61 | |
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62 | inline G4bool G4FermiIntegerPartition:: |
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63 | operator!=(const G4FermiIntegerPartition& right) |
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64 | { |
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65 | return (total != right.total || |
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66 | enableNull != right.enableNull || |
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67 | partition != right.partition); |
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68 | } |
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69 | |
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70 | inline std::vector<G4int> G4FermiIntegerPartition:: |
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71 | GetPartition() const |
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72 | { |
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73 | return partition; |
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74 | } |
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75 | |
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76 | inline void G4FermiIntegerPartition:: |
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77 | EnableNull(const G4bool v) |
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78 | { |
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79 | enableNull=v; |
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80 | return; |
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81 | } |
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82 | |
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83 | #ifdef G4FermiIntegerPartition_debug |
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84 | |
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85 | inline G4int G4FermiIntegerPartition::GetSum() |
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86 | { |
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87 | return std::accumulate(partition.begin(), partition.end(), 0); |
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88 | } |
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89 | |
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90 | #endif |
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91 | |
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