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9.6.p02
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geant4_9_6_p02
source
processes
hadronic
models
de_excitation
gem_evaporation
src
G4N13GEMProbability.cc
Go to the documentation of this file.
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//
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// ********************************************************************
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// * License and Disclaimer *
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// * *
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// * The Geant4 software is copyright of the Copyright Holders of *
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// * the Geant4 Collaboration. It is provided under the terms and *
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// * conditions of the Geant4 Software License, included in the file *
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// * LICENSE and available at http://cern.ch/geant4/license . These *
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// * include a list of copyright holders. *
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// * *
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// * Neither the authors of this software system, nor their employing *
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// * institutes,nor the agencies providing financial support for this *
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// * work make any representation or warranty, express or implied, *
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// * regarding this software system or assume any liability for its *
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// * use. Please see the license in the file LICENSE and URL above *
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// * for the full disclaimer and the limitation of liability. *
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// * *
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// * This code implementation is the result of the scientific and *
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// * technical work of the GEANT4 collaboration. *
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// * By using, copying, modifying or distributing the software (or *
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// * any work based on the software) you agree to acknowledge its *
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// * use in resulting scientific publications, and indicate your *
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// * acceptance of all terms of the Geant4 Software license. *
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// ********************************************************************
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//
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// $Id$
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//
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// Hadronic Process: Nuclear De-excitations
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// by V. Lara (Nov 1999)
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//
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#include "
G4N13GEMProbability.hh
"
33
#include "
G4SystemOfUnits.hh
"
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G4N13GEMProbability::G4N13GEMProbability
() :
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G4GEMProbability
(13,7,1.0/2.0)
// A,Z,Spin
37
{
38
ExcitEnergies
.push_back(2365.3*
keV
);
39
ExcitSpins
.push_back(1.0/2.0);
40
ExcitLifetimes
.push_back(
fPlanck
/(33*
keV
));
41
42
ExcitEnergies
.push_back(3511*
keV
);
43
ExcitSpins
.push_back(3.0/2.0);
44
ExcitLifetimes
.push_back(
fPlanck
/(66*
keV
));
45
46
ExcitEnergies
.push_back(3547*
keV
);
47
ExcitSpins
.push_back(5.0/2.0);
48
ExcitLifetimes
.push_back(
fPlanck
/(47*
keV
));
49
50
ExcitEnergies
.push_back(6364*
keV
);
51
ExcitSpins
.push_back(5.0/2.0);
52
ExcitLifetimes
.push_back(
fPlanck
/(11*
keV
));
53
54
ExcitEnergies
.push_back(6885*
keV
);
55
ExcitSpins
.push_back(3.0/2.0);
56
ExcitLifetimes
.push_back(
fPlanck
/(115*
keV
));
57
58
ExcitEnergies
.push_back(7155*
keV
);
59
ExcitSpins
.push_back(7.0/2.0);
60
ExcitLifetimes
.push_back(
fPlanck
/(9.0*
keV
));
61
62
ExcitEnergies
.push_back(7376*
keV
);
63
ExcitSpins
.push_back(5.0/2.0);
64
ExcitLifetimes
.push_back(
fPlanck
/(75*
keV
));
65
66
ExcitEnergies
.push_back(8000*
keV
);
67
ExcitSpins
.push_back(3.0/2.0);
68
ExcitLifetimes
.push_back(
fPlanck
/(1500*
keV
));
69
70
ExcitEnergies
.push_back(8918*
keV
);
71
ExcitSpins
.push_back(1.0/2.0);
72
ExcitLifetimes
.push_back(
fPlanck
/(230*
keV
));
73
74
ExcitEnergies
.push_back(9476*
keV
);
75
ExcitSpins
.push_back(3.0/2.0);
76
ExcitLifetimes
.push_back(
fPlanck
/(30*
keV
));
77
78
ExcitEnergies
.push_back(10.25E3*
keV
);
79
ExcitSpins
.push_back(3.0/2.0);
80
ExcitLifetimes
.push_back(
fPlanck
/(270*keV));
81
82
ExcitEnergies
.push_back(10360*keV);
83
ExcitSpins
.push_back(5.0/2.0);
84
ExcitLifetimes
.push_back(
fPlanck
/(30*keV));
85
86
ExcitEnergies
.push_back(10360*keV);
87
ExcitSpins
.push_back(7.0/2.0);
88
ExcitLifetimes
.push_back(
fPlanck
/(76*keV));
89
90
ExcitEnergies
.push_back(11530*keV);
91
ExcitSpins
.push_back(5.0/2.0);
92
ExcitLifetimes
.push_back(
fPlanck
/(430*keV));
93
94
ExcitEnergies
.push_back(11700*keV);
95
ExcitSpins
.push_back(5.0/2.0);
96
ExcitLifetimes
.push_back(
fPlanck
/(115*keV));
97
98
ExcitEnergies
.push_back(11740*keV);
99
ExcitSpins
.push_back(3.0/2.0);
100
ExcitLifetimes
.push_back(
fPlanck
/(250*keV));
101
102
ExcitEnergies
.push_back(11740*keV);
103
ExcitSpins
.push_back(3.0/2.0);
104
ExcitLifetimes
.push_back(
fPlanck
/(530*keV));
105
106
ExcitEnergies
.push_back(11878*keV);
107
ExcitSpins
.push_back(3.0/2.0);
108
ExcitLifetimes
.push_back(
fPlanck
/(380*keV));
109
110
ExcitEnergies
.push_back(12130*keV);
111
ExcitSpins
.push_back(7.0/2.0);
112
ExcitLifetimes
.push_back(
fPlanck
/(250*keV));
113
114
ExcitEnergies
.push_back(13.5E3*keV);
115
ExcitSpins
.push_back(3.0/2.0);
116
ExcitLifetimes
.push_back(
fPlanck
/(6500*keV));
117
118
ExcitEnergies
.push_back(14040*keV);
119
ExcitSpins
.push_back(3.0/2.0);
120
ExcitLifetimes
.push_back(
fPlanck
/(155*keV));
121
122
ExcitEnergies
.push_back(15065.1*keV);
123
ExcitSpins
.push_back(3.0/2.0);
124
ExcitLifetimes
.push_back(
fPlanck
/(1.10*keV));
125
126
ExcitEnergies
.push_back(15.3E3*keV);
127
ExcitSpins
.push_back(3.0/2.0);
128
ExcitLifetimes
.push_back(
fPlanck
/(350*keV));
129
130
ExcitEnergies
.push_back(16020*keV);
131
ExcitSpins
.push_back(7.0/2.0);
132
ExcitLifetimes
.push_back(
fPlanck
/(130*keV));
133
134
ExcitEnergies
.push_back(18230*keV);
135
ExcitSpins
.push_back(1.0/2.0);
136
ExcitLifetimes
.push_back(
fPlanck
/(300*keV));
137
138
ExcitEnergies
.push_back(18406*keV);
139
ExcitSpins
.push_back(3.0/2.0);
140
ExcitLifetimes
.push_back(
fPlanck
/(66*keV));
141
142
ExcitEnergies
.push_back(18961*keV);
143
ExcitSpins
.push_back(7.0/2.0);
144
ExcitLifetimes
.push_back(
fPlanck
/(23*keV));
145
146
ExcitEnergies
.push_back(19830*keV);
147
ExcitSpins
.push_back(5.0/2.0);
148
ExcitLifetimes
.push_back(
fPlanck
/(1000*keV));
149
150
ExcitEnergies
.push_back(19880*keV);
151
ExcitSpins
.push_back(3.0/2.0);
152
ExcitLifetimes
.push_back(
fPlanck
/(520*keV));
153
154
ExcitEnergies
.push_back(20.9E3*keV);
155
ExcitSpins
.push_back(5.0/2.0);
156
ExcitLifetimes
.push_back(
fPlanck
/(1100*keV));
157
158
ExcitEnergies
.push_back(22.4E3*keV);
159
ExcitSpins
.push_back(5.0/2.0);
160
ExcitLifetimes
.push_back(
fPlanck
/(2000*keV));
161
}
162
163
G4N13GEMProbability::~G4N13GEMProbability
()
164
{}
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