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G4N16GEMProbability.cc
Go to the documentation of this file. Or view the newest version in sPHENIX GitHub for file G4N16GEMProbability.cc
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25 //
26 //
27 // Hadronic Process: Nuclear De-excitations
28 // by V. Lara (Nov 1999)
29 //
30 
31 #include "G4N16GEMProbability.hh"
32 #include "G4SystemOfUnits.hh"
33 
34 G4N16GEMProbability::G4N16GEMProbability() :
35  G4GEMProbability(16,7,2.0) // A,Z,Spin
36 {
37  ExcitEnergies.push_back(120.42*keV);
38  ExcitSpins.push_back(0.0);
39  ExcitLifetimes.push_back(5.25e-6*s);
40 
41  ExcitEnergies.push_back(298.22*keV);
42  ExcitSpins.push_back(0.0);
43  ExcitLifetimes.push_back(9.13e-11*s);
44 
45  ExcitEnergies.push_back(397.27*keV);
46  ExcitSpins.push_back(1.0);
47  ExcitLifetimes.push_back(4.5e-12*s);
48 
49  ExcitEnergies.push_back( 3355*keV);
50  ExcitSpins.push_back(1.0);
51  ExcitLifetimes.push_back(fPlanck/(15*keV));
52 
53  ExcitEnergies.push_back( 3519*keV);
54  ExcitSpins.push_back(2.0);
55  ExcitLifetimes.push_back(fPlanck/(3*keV));
56 
57  ExcitEnergies.push_back( 3960*keV);
58  ExcitSpins.push_back(3.0);
59  ExcitLifetimes.push_back(fPlanck/(2*keV));
60 
61  ExcitEnergies.push_back( 4319*keV);
62  ExcitSpins.push_back(1.0);
63  ExcitLifetimes.push_back(fPlanck/(20*keV));
64 
65  ExcitEnergies.push_back( 4387*keV);
66  ExcitSpins.push_back(1.0);
67  ExcitLifetimes.push_back(fPlanck/(82*keV));
68 
69  ExcitEnergies.push_back( 4760*keV);
70  ExcitSpins.push_back(1.0);
71  ExcitLifetimes.push_back(fPlanck/(250*keV));
72 
73  ExcitEnergies.push_back( 4776*keV);
74  ExcitSpins.push_back(2.0);
75  ExcitLifetimes.push_back(fPlanck/(59*keV));
76 
77  ExcitEnergies.push_back( 5050*keV);
78  ExcitSpins.push_back(2.0);
79  ExcitLifetimes.push_back(fPlanck/(19*keV));
80 
81  ExcitEnergies.push_back( 5130*keV);
82  ExcitSpins.push_back(2.0);
83  ExcitLifetimes.push_back(fPlanck/(7*keV));
84 
85  ExcitEnergies.push_back( 5150*keV);
86  ExcitSpins.push_back(3.0);
87  ExcitLifetimes.push_back(fPlanck/(7*keV));
88 
89  ExcitEnergies.push_back( 5232*keV);
90  ExcitSpins.push_back(3.0);
91  ExcitLifetimes.push_back(fPlanck/(4*keV));
92 
93  ExcitEnergies.push_back( 5240*keV);
94  ExcitSpins.push_back(1.0);
95  ExcitLifetimes.push_back(fPlanck/(260*keV));
96 
97  ExcitEnergies.push_back( 5250*keV);
98  ExcitSpins.push_back(2.0);
99  ExcitLifetimes.push_back(fPlanck/(320*keV));
100 
101  ExcitEnergies.push_back( 5518*keV);
102  ExcitSpins.push_back(3.0);
103  ExcitLifetimes.push_back(fPlanck/(7*keV));
104 
105  ExcitEnergies.push_back( 5730*keV);
106  ExcitSpins.push_back(5.0);
107  ExcitLifetimes.push_back(fPlanck/(7*keV));
108 
109  ExcitEnergies.push_back( 6009*keV);
110  ExcitSpins.push_back(1.0);
111  ExcitLifetimes.push_back(fPlanck/(270*keV));
112 
113  ExcitEnergies.push_back( 6168*keV);
114  ExcitSpins.push_back(4.0);
115  ExcitLifetimes.push_back(fPlanck/(7*keV));
116 
117  ExcitEnergies.push_back( 6373*keV);
118  ExcitSpins.push_back(3.0);
119  ExcitLifetimes.push_back(fPlanck/(30*keV));
120 
121  ExcitEnergies.push_back( 6513*keV);
122  ExcitSpins.push_back(2.0);
123  ExcitLifetimes.push_back(fPlanck/(34*keV));
124 
125  ExcitEnergies.push_back( 6840*keV);
126  ExcitSpins.push_back(2.0);
127  ExcitLifetimes.push_back(fPlanck/(140*keV));
128 
129  ExcitEnergies.push_back( 7020*keV);
130  ExcitSpins.push_back(1.0);
131  ExcitLifetimes.push_back(fPlanck/(22*keV));
132 
133  ExcitEnergies.push_back( 7250*keV);
134  ExcitSpins.push_back(2.0);
135  ExcitLifetimes.push_back(fPlanck/(17*keV));
136 
137  ExcitEnergies.push_back( 7573*keV);
138  ExcitSpins.push_back(3.0);
139  ExcitLifetimes.push_back(fPlanck/(7*keV));
140 
141  ExcitEnergies.push_back( 7877*keV);
142  ExcitSpins.push_back(4.0);
143  ExcitLifetimes.push_back(fPlanck/(100*keV));
144 
145  ExcitEnergies.push_back( 8365*keV);
146  ExcitSpins.push_back(1.0);
147  ExcitLifetimes.push_back(fPlanck/(18*keV));
148 
149  ExcitEnergies.push_back( 8490*keV);
150  ExcitSpins.push_back(1.0);
151  ExcitLifetimes.push_back(fPlanck/(50*keV));
152 
153  ExcitEnergies.push_back( 8720*keV);
154  ExcitSpins.push_back(1.0);
155  ExcitLifetimes.push_back(fPlanck/(40*keV));
156 
157  ExcitEnergies.push_back( 9160*keV);
158  ExcitSpins.push_back(2.0);
159  ExcitLifetimes.push_back(fPlanck/(100*keV));
160 
161  ExcitEnergies.push_back( 9459*keV);
162  ExcitSpins.push_back(2.0);
163  ExcitLifetimes.push_back(fPlanck/(100*keV));
164 
165  ExcitEnergies.push_back( 9928*keV);
166  ExcitSpins.push_back(0.0);
167  ExcitLifetimes.push_back(fPlanck/(12*keV));
168 
169  ExcitEnergies.push_back(10055*keV);
170  ExcitSpins.push_back(3.0);
171  ExcitLifetimes.push_back(fPlanck/(30*keV));
172 
173  ExcitEnergies.push_back(10270*keV);
174  ExcitSpins.push_back(2.0);
175  ExcitLifetimes.push_back(fPlanck/(165*keV));
176 
177  ExcitEnergies.push_back(10710*keV);
178  ExcitSpins.push_back(2.0);
179  ExcitLifetimes.push_back(fPlanck/(120*keV));
180 
181  ExcitEnergies.push_back(11620*keV);
182  ExcitSpins.push_back(3.0);
183  ExcitLifetimes.push_back(fPlanck/(220*keV));
184 
185  ExcitEnergies.push_back(11701*keV);
186  ExcitSpins.push_back(2.0);
187  ExcitLifetimes.push_back(fPlanck/(12*keV));
188 
189  ExcitEnergies.push_back(14410*keV);
190  ExcitSpins.push_back(3.0);
191  ExcitLifetimes.push_back(fPlanck/(180*keV));
192 }
193 
194 G4N16GEMProbability::~G4N16GEMProbability()
195 {}