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: G4Mg26GEMProbability.cc,v 1.4 2006/06/29 20:22:37 gunter Exp $ |
---|
28 | // GEANT4 tag $Name: $ |
---|
29 | // |
---|
30 | // Hadronic Process: Nuclear De-excitations |
---|
31 | // by V. Lara (Nov 1999) |
---|
32 | // |
---|
33 | |
---|
34 | |
---|
35 | #include "G4Mg26GEMProbability.hh" |
---|
36 | |
---|
37 | G4Mg26GEMProbability::G4Mg26GEMProbability() : |
---|
38 | G4GEMProbability(26,12,0.0) // A,Z,Spin |
---|
39 | { |
---|
40 | |
---|
41 | ExcitEnergies.push_back(1808.68*keV); |
---|
42 | ExcitSpins.push_back(2.0); |
---|
43 | ExcitLifetimes.push_back(485.0e-3*picosecond); |
---|
44 | |
---|
45 | ExcitEnergies.push_back(2938.36*keV); |
---|
46 | ExcitSpins.push_back(2.0); |
---|
47 | ExcitLifetimes.push_back(139.0e-3*picosecond); |
---|
48 | |
---|
49 | ExcitEnergies.push_back(3588.3*keV); |
---|
50 | ExcitSpins.push_back(0.0); |
---|
51 | ExcitLifetimes.push_back(6.6e-6*picosecond); |
---|
52 | |
---|
53 | ExcitEnergies.push_back(3940.5*keV); |
---|
54 | ExcitSpins.push_back(3.0); |
---|
55 | ExcitLifetimes.push_back(6.2e-5*picosecond); |
---|
56 | |
---|
57 | ExcitEnergies.push_back(4318.4*keV); |
---|
58 | ExcitSpins.push_back(4.0); |
---|
59 | ExcitLifetimes.push_back(201.0e-3*picosecond); |
---|
60 | |
---|
61 | ExcitEnergies.push_back(4331.9*keV); |
---|
62 | ExcitSpins.push_back(2.0); |
---|
63 | ExcitLifetimes.push_back(55.0e-3*picosecond); |
---|
64 | |
---|
65 | ExcitEnergies.push_back(4349.8*keV); |
---|
66 | ExcitSpins.push_back(3.0); |
---|
67 | ExcitLifetimes.push_back(104.0e-3*picosecond); |
---|
68 | |
---|
69 | ExcitEnergies.push_back(4834.3*keV); |
---|
70 | ExcitSpins.push_back(2.0); |
---|
71 | ExcitLifetimes.push_back(35.0e-3*picosecond); |
---|
72 | |
---|
73 | ExcitEnergies.push_back(4900.3*keV); |
---|
74 | ExcitSpins.push_back(4.0); |
---|
75 | ExcitLifetimes.push_back(49.0e-3*picosecond); |
---|
76 | |
---|
77 | ExcitEnergies.push_back(4972.2*keV); |
---|
78 | ExcitSpins.push_back(0.0); |
---|
79 | ExcitLifetimes.push_back(444.0e-3*picosecond); |
---|
80 | |
---|
81 | ExcitEnergies.push_back(5290.8*keV); |
---|
82 | ExcitSpins.push_back(2.0); |
---|
83 | ExcitLifetimes.push_back(69.0e-3*picosecond); |
---|
84 | |
---|
85 | ExcitEnergies.push_back(5473.9*keV); |
---|
86 | ExcitSpins.push_back(4.0); |
---|
87 | ExcitLifetimes.push_back(24.0e-3*picosecond); |
---|
88 | |
---|
89 | ExcitEnergies.push_back(5690.1*keV); |
---|
90 | ExcitSpins.push_back(1.0); |
---|
91 | ExcitLifetimes.push_back(49.0e-3*picosecond); |
---|
92 | |
---|
93 | ExcitEnergies.push_back(5715.5*keV); |
---|
94 | ExcitSpins.push_back(4.0); |
---|
95 | ExcitLifetimes.push_back(94.0e-3*picosecond); |
---|
96 | |
---|
97 | ExcitEnergies.push_back(6256.0*keV); |
---|
98 | ExcitSpins.push_back(0.0); |
---|
99 | ExcitLifetimes.push_back(52.0e-3*picosecond); |
---|
100 | |
---|
101 | ExcitEnergies.push_back(6621.0*keV); |
---|
102 | ExcitSpins.push_back(3.0); |
---|
103 | ExcitLifetimes.push_back(69.0e-3*picosecond); |
---|
104 | |
---|
105 | ExcitEnergies.push_back(6744.0*keV); |
---|
106 | ExcitSpins.push_back(2.0); |
---|
107 | ExcitLifetimes.push_back(55.0e-3*picosecond); |
---|
108 | |
---|
109 | ExcitEnergies.push_back(6877.7*keV); |
---|
110 | ExcitSpins.push_back(3.0); |
---|
111 | ExcitLifetimes.push_back(83.0e-3*picosecond); |
---|
112 | |
---|
113 | } |
---|
114 | |
---|
115 | |
---|
116 | G4Mg26GEMProbability::G4Mg26GEMProbability(const G4Mg26GEMProbability &) : G4GEMProbability() |
---|
117 | { |
---|
118 | throw G4HadronicException(__FILE__, __LINE__, "G4Mg26GEMProbability::copy_constructor meant to not be accessable"); |
---|
119 | } |
---|
120 | |
---|
121 | |
---|
122 | |
---|
123 | |
---|
124 | const G4Mg26GEMProbability & G4Mg26GEMProbability:: |
---|
125 | operator=(const G4Mg26GEMProbability &) |
---|
126 | { |
---|
127 | throw G4HadronicException(__FILE__, __LINE__, "G4Mg26GEMProbability::operator= meant to not be accessable"); |
---|
128 | return *this; |
---|
129 | } |
---|
130 | |
---|
131 | |
---|
132 | G4bool G4Mg26GEMProbability::operator==(const G4Mg26GEMProbability &) const |
---|
133 | { |
---|
134 | return false; |
---|
135 | } |
---|
136 | |
---|
137 | G4bool G4Mg26GEMProbability::operator!=(const G4Mg26GEMProbability &) const |
---|
138 | { |
---|
139 | return true; |
---|
140 | } |
---|
141 | |
---|
142 | |
---|
143 | |
---|