1 | // |
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2 | // ******************************************************************** |
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10 | // * * |
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15 | // * use. Please see the license in the file LICENSE and URL above * |
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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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22 | // * use in resulting scientific publications, and indicate your * |
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24 | // ******************************************************************** |
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25 | // |
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26 | // |
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27 | // $Id: G4CameronTruranHilfShellCorrections.cc,v 1.6 2009/11/30 10:33:33 gcosmo Exp $ |
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28 | // GEANT4 tag $Name: geant4-09-03-ref-09 $ |
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29 | // |
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30 | // Hadronic Process: Nuclear De-excitations |
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31 | // by V. Lara |
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32 | |
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33 | #include "G4CameronTruranHilfShellCorrections.hh" |
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34 | |
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35 | |
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36 | // Data comes from: |
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37 | // J.W. Truran, A.G.W. Cameron, and E. Hilf, |
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38 | // Proc. Int. Conf. on the Properties of Nuclei Far From the Beta-Stability, |
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39 | // Leysin, Switzerland, August 31 - September 4, 1970, Vol.1, p. 275 |
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40 | // S(Z) |
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41 | const G4double G4CameronTruranHilfShellCorrections::ShellZTable |
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42 | [G4CameronTruranHilfShellCorrections::ZTableSize] = { // 93 from Z = 10 to Z = 102 |
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43 | 2.349, 1.936, 1.596, 1.061, 0.341,-0.040, 0.565, 1.065, 1.536, |
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44 | 1.972, 1.855, 2.043, 1.931, 1.652, 1.347, 0.973, 0.579, 0.159, |
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45 | -0.487,-0.192, 0.443, 0.932, 1.387, 1.810, 1.969, 2.067, 2.064, |
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46 | 1.825, 1.539, 1.251, 0.957, 1.128, 1.007, 0.603, 0.013,-0.635, |
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47 | -1.258,-1.905,-2.562,-3.266,-4.099,-3.615,-3.171,-2.814,-2.337, |
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48 | -1.778,-1.220,-0.694,-0.181, 0.323, 0.624, 0.841, 0.904, 0.906, |
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49 | 0.930, 0.919, 0.934, 0.941, 0.978, 0.982, 1.083, 1.201, 1.281, |
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50 | 1.189, 0.963, 0.781, 0.738, 0.696, 0.119,-0.619,-1.265,-1.898, |
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51 | -2.431,-1.326,-0.268, 0.737, 1.451, 2.138, 2.307, 2.221, 2.041, |
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52 | 1.827, 1.239, 0.747, 0.214,-0.263,-0.778,-1.272,-1.800,-2.302, |
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53 | -2.846,-3.499,-3.042 |
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54 | }; |
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55 | // S(N) |
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56 | const G4double G4CameronTruranHilfShellCorrections::ShellNTable |
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57 | [G4CameronTruranHilfShellCorrections::NTableSize] = { // 146 from N = 10 to N = 155 |
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58 | 2.439, 1.829, 1.419, 0.746,-0.082,-0.832,-0.960,-1.006,-1.045, |
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59 | -1.114,-0.900,-0.081, 0.334, 0.064,-0.639,-1.363,-2.138,-2.987, |
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60 | -4.042,-4.001,-3.582,-3.120,-2.677,-2.259,-1.778,-1.315,-0.944, |
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61 | -0.599,-0.285,-0.020, 0.121, 0.140, 0.149,-0.001,-0.230,-0.604, |
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62 | -1.010,-1.570,-2.466,-3.489,-4.552,-4.214,-3.375,-2.526,-1.725, |
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63 | -0.923,-0.164, 0.601, 1.316, 1.947, 2.482, 2.971, 3.398, 3.737, |
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64 | 3.979, 4.183, 4.374, 4.517, 4.605, 4.539, 4.375, 4.043, 3.672, |
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65 | 3.250, 2.776, 2.254, 1.715, 1.151, 0.463,-0.237,-1.031,-1.850, |
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66 | -2.722,-1.663,-0.724, 0.035, 0.786, 1.587, 2.145, 2.669, 2.680, |
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67 | 2.488, 2.243, 1.969, 1.778, 1.663, 1.487, 1.325, 1.148, 0.962, |
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68 | 0.843, 0.727, 0.574, 0.436, 0.320, 0.264, 0.397, 0.507, 0.405, |
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69 | 0.346, 0.369, 0.397, 0.403, 0.379, 0.184,-0.226,-0.737,-1.305, |
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70 | -1.950,-2.565,-3.126,-3.721,-4.393,-5.082,-5.921,-6.712,-6.853, |
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71 | -5.592,-4.413,-3.333,-2.413,-1.582,-0.966,-0.421,-0.123, 0.228, |
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72 | 0.543, 0.874, 1.059, 1.181, 1.186, 1.029, 1.029, 1.153, 1.227, |
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73 | 1.330, 1.449, 1.596, 1.712, 1.851, 1.949, 2.044, 2.155, 2.307, |
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74 | 2.621, 3.096 |
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75 | }; |
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76 | |
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77 | G4CameronTruranHilfShellCorrections* G4CameronTruranHilfShellCorrections::theInstance = 0; |
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78 | |
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79 | |
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80 | G4CameronTruranHilfShellCorrections::G4CameronTruranHilfShellCorrections() |
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81 | {;} |
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82 | |
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83 | G4CameronTruranHilfShellCorrections::~G4CameronTruranHilfShellCorrections() |
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84 | {;} |
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85 | |
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86 | G4CameronTruranHilfShellCorrections* G4CameronTruranHilfShellCorrections::GetInstance() |
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87 | { |
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88 | static G4CameronTruranHilfShellCorrections theCorrections; |
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89 | if (!theInstance) { theInstance = &theCorrections; } |
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90 | return theInstance; |
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91 | } |
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