source: trunk/source/processes/hadronic/models/de_excitation/gem_evaporation/src/G4F17GEMProbability.cc @ 1340

Last change on this file since 1340 was 1340, checked in by garnier, 14 years ago

update ti head
File size: 10.4 KB
Line 
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: G4F17GEMProbability.cc,v 1.6 2009/09/15 12:54:17 vnivanch Exp $
28// GEANT4 tag $Name: geant4-09-03-ref-09 $
29//
30// Hadronic Process: Nuclear De-excitations
31// by V. Lara (Nov 1999)
32//
33
34
35#include "G4F17GEMProbability.hh"
36
37G4F17GEMProbability::G4F17GEMProbability() :
38  G4GEMProbability(17,9,5.0/2.0) // A,Z,Spin
39{
40
41  ExcitEnergies.push_back(495.33*keV);
42  ExcitSpins.push_back(1.0/2.0);
43  ExcitLifetimes.push_back(286.0*picosecond);
44
45  ExcitEnergies.push_back(3104.0*keV);
46  ExcitSpins.push_back(1.0/2.0);
47  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(19.0*keV));
48
49  ExcitEnergies.push_back(3857.0*keV);
50  ExcitSpins.push_back(5.0/2.0);
51  ExcitLifetimes.push_back(4.2e-3*picosecond);
52
53  ExcitEnergies.push_back(3857.0*keV);
54  ExcitSpins.push_back(5.0/2.0);
55  ExcitLifetimes.push_back(4.2e-3*picosecond);
56
57  ExcitEnergies.push_back(4696.0*keV);
58  ExcitSpins.push_back(3.0/2.0);
59  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(225.0*keV));
60
61  ExcitEnergies.push_back(5103.0*keV);
62  ExcitSpins.push_back(3.0/2.0);
63  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1530.0*keV));
64
65  ExcitEnergies.push_back(5521.0*keV);
66  ExcitSpins.push_back(3.0/2.0);
67  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(68.0*keV));
68
69  ExcitEnergies.push_back(5672.0*keV);
70  ExcitSpins.push_back(7.0/2.0);
71  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(40.0*keV));
72
73  ExcitEnergies.push_back(5682.0*keV);
74  ExcitSpins.push_back(1.0/2.0);
75  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.6*keV));
76
77  ExcitEnergies.push_back(5817.0*keV);
78  ExcitSpins.push_back(3.0/2.0);
79  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(180.0*keV));
80
81  ExcitEnergies.push_back(6036.0*keV);
82  ExcitSpins.push_back(1.0/2.0);
83  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV));
84
85  ExcitEnergies.push_back(6556.0*keV);
86  ExcitSpins.push_back(1.0/2.0);
87  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(200.0*keV));
88
89  ExcitEnergies.push_back(6699.0*keV);
90  ExcitSpins.push_back(3.0/2.0);
91  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.0*keV));
92
93  ExcitEnergies.push_back(6774.0*keV);
94  ExcitSpins.push_back(3.0/2.0);
95  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(4.5*keV));
96
97  ExcitEnergies.push_back(7027.0*keV);
98  ExcitSpins.push_back(5.0/2.0);
99  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(3.8*keV));
100
101  ExcitEnergies.push_back(7356.0*keV);
102  ExcitSpins.push_back(3.0/2.0);
103  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(10.0*keV));
104
105  ExcitEnergies.push_back(7479.0*keV);
106  ExcitSpins.push_back(3.0/2.0);
107  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(795.0*keV));
108
109  ExcitEnergies.push_back(7546.0*keV);
110  ExcitSpins.push_back(7.0/2.0);
111  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV));
112
113  ExcitEnergies.push_back(7750.0*keV);
114  ExcitSpins.push_back(1.0/2.0);
115  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(179.0*keV));
116
117  ExcitEnergies.push_back(8075.0*keV);
118  ExcitSpins.push_back(5.0/2.0);
119  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(100.0*keV));
120
121  ExcitEnergies.push_back(8200.0*keV);
122  ExcitSpins.push_back(3.0/2.0);
123  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(700.0*keV));
124
125  ExcitEnergies.push_back(8383.0*keV);
126  ExcitSpins.push_back(5.0/2.0);
127  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(11.0*keV));
128
129  ExcitEnergies.push_back(8416.0*keV);
130  ExcitSpins.push_back(7.0/2.0);
131  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(45.0*keV));
132
133  ExcitEnergies.push_back(8750.0*keV);
134  ExcitSpins.push_back(5.0/2.0);
135  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(170.0*keV));
136
137  ExcitEnergies.push_back(8760.0*keV);
138  ExcitSpins.push_back(3.0/2.0);
139  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90.0*keV));
140
141  ExcitEnergies.push_back(8970.0*keV);
142  ExcitSpins.push_back(7.0/2.0);
143  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(165.0*keV));
144
145  ExcitEnergies.push_back(9270.0*keV);
146  ExcitSpins.push_back(3.0/2.0);
147  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(140.0*keV));
148
149  ExcitEnergies.push_back(9910.0*keV);
150  ExcitSpins.push_back(9.0/2.0);
151  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(90.0*keV));
152
153  ExcitEnergies.push_back(10040.0*keV);
154  ExcitSpins.push_back(7.0/2.0);
155  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(280.0*keV));
156
157  ExcitEnergies.push_back(10400.0*keV);
158  ExcitSpins.push_back(5.0/2.0);
159  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(160.0*keV));
160
161  ExcitEnergies.push_back(10499.0*keV);
162  ExcitSpins.push_back(7.0/2.0);
163  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(165.0*keV));
164
165  ExcitEnergies.push_back(10.91E3*keV);
166  ExcitSpins.push_back(1.0/2.0);
167  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(560.0*keV));
168
169  ExcitEnergies.push_back(11193.1*keV);
170  ExcitSpins.push_back(1.0/2.0);
171  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(0.20*keV));
172
173  ExcitEnergies.push_back(12250.0*keV);
174  ExcitSpins.push_back(3.0/2.0);
175  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV));
176
177  ExcitEnergies.push_back(12355.0*keV);
178  ExcitSpins.push_back(1.0/2.0);
179  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(190.0*keV));
180
181  ExcitEnergies.push_back(12500.0*keV);
182  ExcitSpins.push_back(7.0/2.0);
183  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(660.0*keV));
184
185  ExcitEnergies.push_back(12550.0*keV);
186  ExcitSpins.push_back(3.0/2.0);
187  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.83*keV));
188
189  ExcitEnergies.push_back(13061.0*keV);
190  ExcitSpins.push_back(5.0/2.0);
191  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.0*keV));
192
193  ExcitEnergies.push_back(13080.0*keV);
194  ExcitSpins.push_back(1.0/2.0);
195  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2.0*keV));
196
197  ExcitEnergies.push_back(13130.0*keV);
198  ExcitSpins.push_back(5.0/2.0);
199  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(520.0*keV));
200
201  ExcitEnergies.push_back(13781.0*keV);
202  ExcitSpins.push_back(5.0/2.0);
203  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(12.0*keV));
204
205  ExcitEnergies.push_back(14000.0*keV);
206  ExcitSpins.push_back(7.0/2.0);
207  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(260.0*keV));
208
209  ExcitEnergies.push_back(14176.0*keV);
210  ExcitSpins.push_back(3.0/2.0);
211  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(30.0*keV));
212
213  ExcitEnergies.push_back(14304.0*keV);
214  ExcitSpins.push_back(7.0/2.0);
215  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(19.3*keV));
216
217  ExcitEnergies.push_back(14380.0*keV);
218  ExcitSpins.push_back(5.0/2.0);
219  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(610.0*keV));
220
221  ExcitEnergies.push_back(14.71E3*keV);
222  ExcitSpins.push_back(1.0/2.0);
223  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(470.0*keV));
224
225  ExcitEnergies.push_back(14809.0*keV);
226  ExcitSpins.push_back(1.0/2.0);
227  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(190.0*keV));
228
229  ExcitEnergies.push_back(17100.0*keV);
230  ExcitSpins.push_back(5.0/2.0);
231  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1500.0*keV));
232
233  ExcitEnergies.push_back(19420.0*keV);
234  ExcitSpins.push_back(5.0/2.0);
235  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(300.0*keV));
236
237  ExcitEnergies.push_back(20250.0*keV);
238  ExcitSpins.push_back(7.0/2.0);
239  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(350.0*keV));
240
241  ExcitEnergies.push_back(20900.0*keV);
242  ExcitSpins.push_back(9.0/2.0);
243  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV));
244
245  ExcitEnergies.push_back(21010.0*keV);
246  ExcitSpins.push_back(1.0/2.0);
247  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(280.0*keV));
248
249  ExcitEnergies.push_back(21800.0*keV);
250  ExcitSpins.push_back(9.0/2.0);
251  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(400.0*keV));
252
253  ExcitEnergies.push_back(22700.0*keV);
254  ExcitSpins.push_back(7.0/2.0);
255  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV));
256
257  ExcitEnergies.push_back(23800.0*keV);
258  ExcitSpins.push_back(7.0/2.0);
259  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(600.0*keV));
260
261  ExcitEnergies.push_back(25400.0*keV);
262  ExcitSpins.push_back(7.0/2.0);
263  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1500.0*keV));
264
265  ExcitEnergies.push_back(27200.0*keV);
266  ExcitSpins.push_back(5.0/2.0);
267  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(1500.0*keV));
268
269  ExcitEnergies.push_back(28900.0*keV);
270  ExcitSpins.push_back(5.0/2.0);
271  ExcitLifetimes.push_back(hbar_Planck*std::log(2.0)/(2000.0*keV));
272
273}
274
275
276G4F17GEMProbability::G4F17GEMProbability(const G4F17GEMProbability &) : G4GEMProbability()
277{
278  throw G4HadronicException(__FILE__, __LINE__, "G4F17GEMProbability::copy_constructor meant to not be accessable");
279}
280
281
282
283
284const G4F17GEMProbability & G4F17GEMProbability::
285operator=(const G4F17GEMProbability &)
286{
287  throw G4HadronicException(__FILE__, __LINE__, "G4F17GEMProbability::operator= meant to not be accessable");
288  return *this;
289}
290
291
292G4bool G4F17GEMProbability::operator==(const G4F17GEMProbability &) const
293{
294  return false;
295}
296
297G4bool G4F17GEMProbability::operator!=(const G4F17GEMProbability &) const
298{
299  return true;
300}
301
302
303
Note: See TracBrowser for help on using the repository browser.