1 | // |
---|
2 | // ******************************************************************** |
---|
3 | // * License and Disclaimer * |
---|
4 | // * * |
---|
5 | // * The Geant4 software is copyright of the Copyright Holders of * |
---|
6 | // * the Geant4 Collaboration. It is provided under the terms and * |
---|
7 | // * conditions of the Geant4 Software License, included in the file * |
---|
8 | // * LICENSE and available at http://cern.ch/geant4/license . These * |
---|
9 | // * include a list of copyright holders. * |
---|
10 | // * * |
---|
11 | // * Neither the authors of this software system, nor their employing * |
---|
12 | // * institutes,nor the agencies providing financial support for this * |
---|
13 | // * work make any representation or warranty, express or implied, * |
---|
14 | // * regarding this software system or assume any liability for its * |
---|
15 | // * use. Please see the license in the file LICENSE and URL above * |
---|
16 | // * for the full disclaimer and the limitation of liability. * |
---|
17 | // * * |
---|
18 | // * This code implementation is the result of the scientific and * |
---|
19 | // * technical work of the GEANT4 collaboration. * |
---|
20 | // * By using, copying, modifying or distributing the software (or * |
---|
21 | // * any work based on the software) you agree to acknowledge its * |
---|
22 | // * use in resulting scientific publications, and indicate your * |
---|
23 | // * acceptance of all terms of the Geant4 Software license. * |
---|
24 | // ******************************************************************** |
---|
25 | // |
---|
26 | // |
---|
27 | // $Id: G4ProtonEvaporationProbability.cc,v 1.4 2006/06/29 20:10:43 gunter Exp $ |
---|
28 | // GEANT4 tag $Name: geant4-09-01-patch-02 $ |
---|
29 | // |
---|
30 | // Hadronic Process: Nuclear De-excitations |
---|
31 | // by V. Lara (Nov 1999) |
---|
32 | // |
---|
33 | |
---|
34 | |
---|
35 | #include "G4ProtonEvaporationProbability.hh" |
---|
36 | |
---|
37 | G4ProtonEvaporationProbability::G4ProtonEvaporationProbability() : |
---|
38 | G4EvaporationProbability(1,1,2) // A,Z,Gamma |
---|
39 | { |
---|
40 | std::vector<G4double>::size_type NumExcitedStatesEnergy = 31+1; |
---|
41 | std::vector<G4int>::size_type NumExcitedStatesSpin = 31+1; |
---|
42 | ExcitEnergies.reserve(NumExcitedStatesEnergy); |
---|
43 | ExcitSpins.reserve(NumExcitedStatesSpin); |
---|
44 | ExcitEnergies.insert(ExcitEnergies.begin(),NumExcitedStatesEnergy,0.0); |
---|
45 | ExcitSpins.insert(ExcitSpins.begin(),NumExcitedStatesSpin,0); |
---|
46 | |
---|
47 | |
---|
48 | |
---|
49 | ExcitEnergies[15] = 5.96*MeV; |
---|
50 | ExcitEnergies[17] = 1.74*MeV; |
---|
51 | ExcitEnergies[18] = 4.44*MeV; |
---|
52 | ExcitEnergies[19] = 1.67*MeV; |
---|
53 | ExcitEnergies[20] = 4.32*MeV; |
---|
54 | ExcitEnergies[22] = 3.68*MeV; |
---|
55 | ExcitEnergies[23] = 6.69*MeV; |
---|
56 | ExcitEnergies[25] = 3.95*MeV; |
---|
57 | ExcitEnergies[26] = 6.32*MeV; |
---|
58 | ExcitEnergies[27] = 0.30*MeV; |
---|
59 | ExcitEnergies[28] = 6.18*MeV; |
---|
60 | ExcitEnergies[29] = 6.92*MeV; |
---|
61 | ExcitEnergies[30] = 3.06*MeV; |
---|
62 | ExcitEnergies[31] = 3.57*MeV; |
---|
63 | |
---|
64 | |
---|
65 | ExcitSpins[15] = 8; |
---|
66 | ExcitSpins[17] = 1; |
---|
67 | ExcitSpins[18] = 6; |
---|
68 | ExcitSpins[19] = 5; |
---|
69 | ExcitSpins[20] = 6; |
---|
70 | ExcitSpins[22] = 4; |
---|
71 | ExcitSpins[23] = 8; |
---|
72 | ExcitSpins[25] = 3; |
---|
73 | ExcitSpins[26] = 4; |
---|
74 | ExcitSpins[27] = 7; |
---|
75 | ExcitSpins[28] = 4; |
---|
76 | ExcitSpins[29] = 5; |
---|
77 | ExcitSpins[30] = 2; |
---|
78 | ExcitSpins[31] = 10; |
---|
79 | |
---|
80 | SetExcitationEnergiesPtr(&ExcitEnergies); |
---|
81 | SetExcitationSpinsPtr(&ExcitSpins); |
---|
82 | |
---|
83 | } |
---|
84 | |
---|
85 | G4ProtonEvaporationProbability::G4ProtonEvaporationProbability(const G4ProtonEvaporationProbability &) : G4EvaporationProbability() |
---|
86 | { |
---|
87 | throw G4HadronicException(__FILE__, __LINE__, "G4ProtonEvaporationProbability::copy_constructor meant to not be accessable"); |
---|
88 | } |
---|
89 | |
---|
90 | const G4ProtonEvaporationProbability & G4ProtonEvaporationProbability:: |
---|
91 | operator=(const G4ProtonEvaporationProbability &) |
---|
92 | { |
---|
93 | throw G4HadronicException(__FILE__, __LINE__, "G4ProtonEvaporationProbability::operator= meant to not be accessable"); |
---|
94 | return *this; |
---|
95 | } |
---|
96 | |
---|
97 | |
---|
98 | G4bool G4ProtonEvaporationProbability::operator==(const G4ProtonEvaporationProbability &) const |
---|
99 | { |
---|
100 | return false; |
---|
101 | } |
---|
102 | |
---|
103 | G4bool G4ProtonEvaporationProbability::operator!=(const G4ProtonEvaporationProbability &) const |
---|
104 | { |
---|
105 | return true; |
---|
106 | } |
---|
107 | |
---|
108 | G4double G4ProtonEvaporationProbability::CCoeficient(const G4double aZ) const |
---|
109 | { |
---|
110 | // Data comes from |
---|
111 | // Dostrovsky, Fraenkel and Friedlander |
---|
112 | // Physical Review, vol 116, num. 3 1959 |
---|
113 | // |
---|
114 | // const G4int size = 5; |
---|
115 | // G4double Zlist[5] = { 10.0, 20.0, 30.0, 50.0, 70.0}; |
---|
116 | // G4double Cp[5] = { 0.50, 0.28, 0.20, 0.15, 0.10}; |
---|
117 | G4double C = 0.0; |
---|
118 | |
---|
119 | if (aZ >= 70) { |
---|
120 | C = 0.10; |
---|
121 | } else { |
---|
122 | C = ((((0.15417e-06*aZ) - 0.29875e-04)*aZ + 0.21071e-02)*aZ - 0.66612e-01)*aZ + 0.98375; |
---|
123 | } |
---|
124 | |
---|
125 | return C; |
---|
126 | |
---|
127 | } |
---|