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G4O17GEMProbability.cc
Go to the documentation of this file.
1
//
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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: G4O17GEMProbability.cc 74869 2013-10-23 09:26:17Z gcosmo $
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//
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// Hadronic Process: Nuclear De-excitations
29
// by V. Lara (Nov 1999)
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//
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32
#include "
G4O17GEMProbability.hh
"
33
#include "
G4PhysicalConstants.hh
"
34
#include "
G4SystemOfUnits.hh
"
35
#include "
G4Log.hh
"
36
37
G4O17GEMProbability::G4O17GEMProbability
() :
38
G4GEMProbability
(17,9,5.0/2.0)
// A,Z,Spin
39
{
40
41
ExcitEnergies
.push_back(870.81*
keV
);
42
ExcitSpins
.push_back(1.0/2.0);
43
ExcitLifetimes
.push_back(179.2*
picosecond
);
44
45
ExcitEnergies
.push_back(3055.2*
keV
);
46
ExcitSpins
.push_back(1.0/2.0);
47
ExcitLifetimes
.push_back(83.0E-3*
picosecond
);
48
49
ExcitEnergies
.push_back(3841.0*
keV
);
50
ExcitSpins
.push_back(5.0/2.0);
51
ExcitLifetimes
.push_back(17.0E-3*
picosecond
);
52
53
ExcitEnergies
.push_back(4553.0*
keV
);
54
ExcitSpins
.push_back(3.0/2.0);
55
ExcitLifetimes
.push_back(
fPlanck
/(40.0*
keV
));
56
57
ExcitEnergies
.push_back(5086.0*
keV
);
58
ExcitSpins
.push_back(3.0/2.0);
59
ExcitLifetimes
.push_back(
fPlanck
/(95.0*
keV
));
60
61
ExcitEnergies
.push_back(5380.0*
keV
);
62
ExcitSpins
.push_back(3.0/2.0);
63
ExcitLifetimes
.push_back(
fPlanck
/(28.0*
keV
));
64
65
ExcitEnergies
.push_back(5698.0*
keV
);
66
ExcitSpins
.push_back(7.0/2.0);
67
ExcitLifetimes
.push_back(
fPlanck
/(3.4*
keV
));
68
69
ExcitEnergies
.push_back(5870.0*
keV
);
70
ExcitSpins
.push_back(3.0/2.0);
71
ExcitLifetimes
.push_back(
fPlanck
/(6.6*
keV
));
72
73
ExcitEnergies
.push_back(5940.0*
keV
);
74
ExcitSpins
.push_back(1.0/2.0);
75
ExcitLifetimes
.push_back(
fPlanck
/(32.0*
keV
));
76
77
ExcitEnergies
.push_back(6357.0*
keV
);
78
ExcitSpins
.push_back(1.0/2.0);
79
ExcitLifetimes
.push_back(
fPlanck
/(124.0*
keV
));
80
81
ExcitEnergies
.push_back(7168.7*
keV
);
82
ExcitSpins
.push_back(5.0/2.0);
83
ExcitLifetimes
.push_back(
fPlanck
/(1.5*
keV
));
84
85
ExcitEnergies
.push_back(7202.0*
keV
);
86
ExcitSpins
.push_back(3.0/2.0);
87
ExcitLifetimes
.push_back(
fPlanck
/(280.0*
keV
));
88
89
ExcitEnergies
.push_back(7383.1*
keV
);
90
ExcitSpins
.push_back(5.0/2.0);
91
ExcitLifetimes
.push_back(
fPlanck
/(0.6*
keV
));
92
93
ExcitEnergies
.push_back(7386.0*
keV
);
94
ExcitSpins
.push_back(5.0/2.0);
95
ExcitLifetimes
.push_back(
fPlanck
/(0.9*
keV
));
96
97
ExcitEnergies
.push_back(7560.0*
keV
);
98
ExcitSpins
.push_back(3.0/2.0);
99
ExcitLifetimes
.push_back(
fPlanck
/(500.0*
keV
));
100
101
ExcitEnergies
.push_back(7577.0*
keV
);
102
ExcitSpins
.push_back(7.0/2.0);
103
ExcitLifetimes
.push_back(
fPlanck
/(1.0*
keV
));
104
105
ExcitEnergies
.push_back(7690.0*
keV
);
106
ExcitSpins
.push_back(7.0/2.0);
107
ExcitLifetimes
.push_back(
fPlanck
/(18.0*
keV
));
108
109
ExcitEnergies
.push_back(7956.0*
keV
);
110
ExcitSpins
.push_back(1.0/2.0);
111
ExcitLifetimes
.push_back(
fPlanck
/(90.0*
keV
));
112
113
ExcitEnergies
.push_back(7990.0*
keV
);
114
ExcitSpins
.push_back(1.0/2.0);
115
ExcitLifetimes
.push_back(
fPlanck
/(270.0*
keV
));
116
117
ExcitEnergies
.push_back(8070.0*
keV
);
118
ExcitSpins
.push_back(3.0/2.0);
119
ExcitLifetimes
.push_back(
fPlanck
/(85.0*
keV
));
120
121
ExcitEnergies
.push_back(8180.0*
keV
);
122
ExcitSpins
.push_back(1.0/2.0);
123
ExcitLifetimes
.push_back(
fPlanck
/(69.0*
keV
));
124
125
ExcitEnergies
.push_back(8200.0*
keV
);
126
ExcitSpins
.push_back(3.0/2.0);
127
ExcitLifetimes
.push_back(
fPlanck
/(60.0*
keV
));
128
129
ExcitEnergies
.push_back(8352.0*
keV
);
130
ExcitSpins
.push_back(1.0/2.0);
131
ExcitLifetimes
.push_back(
fPlanck
/(9.0*
keV
));
132
133
ExcitEnergies
.push_back(8410.0*
keV
);
134
ExcitSpins
.push_back(5.0/2.0);
135
ExcitLifetimes
.push_back(
fPlanck
/(4.0*
keV
));
136
137
ExcitEnergies
.push_back(8474.0*
keV
);
138
ExcitSpins
.push_back(7.0/2.0);
139
ExcitLifetimes
.push_back(
fPlanck
/(7.0*
keV
));
140
141
ExcitEnergies
.push_back(8508.0*
keV
);
142
ExcitSpins
.push_back(5.0/2.0);
143
ExcitLifetimes
.push_back(
hbar_Planck
*
G4Log
(2.0)/(5.0*
keV
));
144
145
ExcitEnergies
.push_back(8700.0*
keV
);
146
ExcitSpins
.push_back(3.0/2.0);
147
ExcitLifetimes
.push_back(
fPlanck
/(50.0*
keV
));
148
149
ExcitEnergies
.push_back(8898.0*
keV
);
150
ExcitSpins
.push_back(3.0/2.0);
151
ExcitLifetimes
.push_back(
fPlanck
/(101.0*
keV
));
152
153
ExcitEnergies
.push_back(8972.0*
keV
);
154
ExcitSpins
.push_back(7.0/2.0);
155
ExcitLifetimes
.push_back(
fPlanck
/(21.0*
keV
));
156
157
ExcitEnergies
.push_back(9148.0*
keV
);
158
ExcitSpins
.push_back(1.0/2.0);
159
ExcitLifetimes
.push_back(
fPlanck
/(4.0*
keV
));
160
161
ExcitEnergies
.push_back(9187.0*
keV
);
162
ExcitSpins
.push_back(7.0/2.0);
163
ExcitLifetimes
.push_back(
fPlanck
/(3.0*
keV
));
164
165
ExcitEnergies
.push_back(9201.0*
keV
);
166
ExcitSpins
.push_back(5.0/2.0);
167
ExcitLifetimes
.push_back(
fPlanck
/(5.5*
keV
));
168
169
ExcitEnergies
.push_back(9422.0*
keV
);
170
ExcitSpins
.push_back(3.0/2.0);
171
ExcitLifetimes
.push_back(
fPlanck
/(120.0*
keV
));
172
173
ExcitEnergies
.push_back(9493.0*
keV
);
174
ExcitSpins
.push_back(5.0/2.0);
175
ExcitLifetimes
.push_back(
hbar_Planck
*
G4Log
(2.0)/(15.0*
keV
));
176
177
ExcitEnergies
.push_back(9720.0*
keV
);
178
ExcitSpins
.push_back(7.0/2.0);
179
ExcitLifetimes
.push_back(
fPlanck
/(16.0*
keV
));
180
181
ExcitEnergies
.push_back(9775.0*
keV
);
182
ExcitSpins
.push_back(3.0/2.0);
183
ExcitLifetimes
.push_back(
fPlanck
/(25.0*
keV
));
184
185
ExcitEnergies
.push_back(9977.0*
keV
);
186
ExcitSpins
.push_back(5.0/2.0);
187
ExcitLifetimes
.push_back(
fPlanck
/(80.0*
keV
));
188
189
ExcitEnergies
.push_back(10178.0*
keV
);
190
ExcitSpins
.push_back(7.0/2.0);
191
ExcitLifetimes
.push_back(
fPlanck
/(40.0*
keV
));
192
193
ExcitEnergies
.push_back(10337.0*
keV
);
194
ExcitSpins
.push_back(5.0/2.0);
195
ExcitLifetimes
.push_back(
fPlanck
/(150.0*
keV
));
196
197
ExcitEnergies
.push_back(10490.0*
keV
);
198
ExcitSpins
.push_back(5.0/2.0);
199
ExcitLifetimes
.push_back(
fPlanck
/(75.0*
keV
));
200
201
ExcitEnergies
.push_back(10773.0*
keV
);
202
ExcitSpins
.push_back(1.0/2.0);
203
ExcitLifetimes
.push_back(
fPlanck
/(80.0*
keV
));
204
205
ExcitEnergies
.push_back(10910.0*
keV
);
206
ExcitSpins
.push_back(5.0/2.0);
207
ExcitLifetimes
.push_back(
fPlanck
/(57.0*
keV
));
208
209
ExcitEnergies
.push_back(11076.0*
keV
);
210
ExcitSpins
.push_back(1.0/2.0);
211
ExcitLifetimes
.push_back(
fPlanck
/(5.0*
keV
));
212
213
ExcitEnergies
.push_back(12946.0*
keV
);
214
ExcitSpins
.push_back(1.0/2.0);
215
ExcitLifetimes
.push_back(
fPlanck
/(6.0*
keV
));
216
217
ExcitEnergies
.push_back(14980.0*
keV
);
218
ExcitSpins
.push_back(5.0/2.0);
219
ExcitLifetimes
.push_back(
fPlanck
/(150.0*
keV
));
220
221
ExcitEnergies
.push_back(21.7E3*
keV
);
222
ExcitSpins
.push_back(5.0/2.0);
223
ExcitLifetimes
.push_back(
fPlanck
/(750.0*keV));
224
225
ExcitEnergies
.push_back(22.1E3*keV);
226
ExcitSpins
.push_back(7.0/2.0);
227
ExcitLifetimes
.push_back(
fPlanck
/(750.0*keV));
228
229
ExcitEnergies
.push_back(22.5E3*keV);
230
ExcitSpins
.push_back(3.0/2.0);
231
ExcitLifetimes
.push_back(
fPlanck
/(1000.0*keV));
232
233
ExcitEnergies
.push_back(23.0E3*keV);
234
ExcitSpins
.push_back(1.0/2.0);
235
ExcitLifetimes
.push_back(
fPlanck
/(400.0*keV));
236
}
237
238
G4O17GEMProbability::~G4O17GEMProbability
()
239
{}
G4GEMProbability
Definition:
G4GEMProbability.hh:54
python.hepunit.hbar_Planck
hbar_Planck
Definition:
hepunit.py:264
G4GEMProbability::ExcitLifetimes
std::vector< G4double > ExcitLifetimes
Definition:
G4GEMProbability.hh:132
picosecond
static constexpr double picosecond
Definition:
G4SIunits.hh:161
G4GEMProbability::ExcitSpins
std::vector< G4double > ExcitSpins
Definition:
G4GEMProbability.hh:129
G4Log.hh
G4GEMProbability::ExcitEnergies
std::vector< G4double > ExcitEnergies
Definition:
G4GEMProbability.hh:126
G4PhysicalConstants.hh
G4Log
G4double G4Log(G4double x)
Definition:
G4Log.hh:230
G4O17GEMProbability::G4O17GEMProbability
G4O17GEMProbability()
Definition:
G4O17GEMProbability.cc:37
G4O17GEMProbability::~G4O17GEMProbability
~G4O17GEMProbability()
Definition:
G4O17GEMProbability.cc:238
G4O17GEMProbability.hh
G4SystemOfUnits.hh
keV
static constexpr double keV
Definition:
G4SIunits.hh:216
G4GEMProbability::fPlanck
G4double fPlanck
Definition:
G4GEMProbability.hh:123
source
geant4.10.03.p03
source
processes
hadronic
models
de_excitation
gem_evaporation
src
G4O17GEMProbability.cc
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