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G4C13GEMProbability.cc
Go to the documentation of this file. Or view the newest version in sPHENIX GitHub for file G4C13GEMProbability.cc
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25 //
26 //
27 // Hadronic Process: Nuclear De-excitations
28 // by V. Lara (Nov 1999)
29 //
30 
31 #include "G4C13GEMProbability.hh"
32 #include "G4SystemOfUnits.hh"
33 
35  G4GEMProbability(13,6,1.0/2.0) // A,Z,Spin
36 {
37 
38  ExcitEnergies.push_back(3089.443*keV);
39  ExcitSpins.push_back(1.0/2.0);
40  ExcitLifetimes.push_back(1.04e-15*s);
41 
42  ExcitEnergies.push_back(3684.507*keV);
43  ExcitSpins.push_back(3.0/2.0);
44  ExcitLifetimes.push_back(1.04e-15*s);
45 
46  ExcitEnergies.push_back( 3853.807*keV);
47  ExcitSpins.push_back(5.0/2.0);
48  ExcitLifetimes.push_back(7.5e-12*s);
49 
50  ExcitEnergies.push_back(6864*keV);
51  ExcitSpins.push_back(5.0/2.0);
52  ExcitLifetimes.push_back(fPlanck/(6*keV));
53 
54  ExcitEnergies.push_back(7492*keV);
55  ExcitSpins.push_back(7.0/2.0);
56  ExcitLifetimes.push_back(fPlanck/(5*keV));
57 
58  ExcitEnergies.push_back(7547*keV);
59  ExcitSpins.push_back(5.0/2.0);
60  ExcitLifetimes.push_back(fPlanck/(1.2*keV));
61 
62  ExcitEnergies.push_back(7677*keV);
63  ExcitSpins.push_back(3.0/2.0);
64  ExcitLifetimes.push_back(fPlanck/(70*keV));
65 
66  ExcitEnergies.push_back(8.2E3*keV);
67  ExcitSpins.push_back(3.0/2.0);
68  ExcitLifetimes.push_back(fPlanck/(1000*keV));
69 
70  ExcitEnergies.push_back(8860*keV);
71  ExcitSpins.push_back(1.0/2.0);
72  ExcitLifetimes.push_back(fPlanck/(150*keV));
73 
74  ExcitEnergies.push_back(9498*keV);
75  ExcitSpins.push_back(3.0/2.0);
76  ExcitLifetimes.push_back(fPlanck/(5*keV));
77 
78  ExcitEnergies.push_back(9897*keV);
79  ExcitSpins.push_back(3.0/2.0);
80  ExcitLifetimes.push_back(fPlanck/(26*keV));
81 
82  ExcitEnergies.push_back(10753*keV);
83  ExcitSpins.push_back(7.0/2.0);
84  ExcitLifetimes.push_back(fPlanck/(55*keV));
85 
86  ExcitEnergies.push_back(10818*keV);
87  ExcitSpins.push_back(5.0/2.0);
88  ExcitLifetimes.push_back(fPlanck/(24*keV));
89 
90  ExcitEnergies.push_back(10996*keV);
91  ExcitSpins.push_back(1.0/2.0);
92  ExcitLifetimes.push_back(fPlanck/(37*keV));
93 
94  ExcitEnergies.push_back(11080*keV);
95  ExcitSpins.push_back(1.0/2.0);
96  ExcitLifetimes.push_back(fPlanck/(4*keV));
97 
98  ExcitEnergies.push_back(11851*keV);
99  ExcitSpins.push_back(3.0/2.0);
100  ExcitLifetimes.push_back(fPlanck/(68*keV));
101 
102  ExcitEnergies.push_back(11970*keV);
103  ExcitSpins.push_back(5.0/2.0);
104  ExcitLifetimes.push_back(fPlanck/(200*keV));
105 
106  ExcitEnergies.push_back(12106*keV);
107  ExcitSpins.push_back(9.0/2.0);
108  ExcitLifetimes.push_back(fPlanck/(81*keV));
109 
110  ExcitEnergies.push_back(12400*keV);
111  ExcitSpins.push_back(7.0/2.0);
112  ExcitLifetimes.push_back(fPlanck/(150*keV));
113 
114  ExcitEnergies.push_back(13280*keV);
115  ExcitSpins.push_back(3.0/2.0);
116  ExcitLifetimes.push_back(fPlanck/(340*keV));
117 
118  ExcitEnergies.push_back(13410*keV);
119  ExcitSpins.push_back(9.0/2.0);
120  ExcitLifetimes.push_back(fPlanck/(35*keV));
121 
122  ExcitEnergies.push_back(13560*keV);
123  ExcitSpins.push_back(5.0/2.0);
124  ExcitLifetimes.push_back(fPlanck/(500*keV));
125 
126  ExcitEnergies.push_back(13760*keV);
127  ExcitSpins.push_back(3.0/2.0);
128  ExcitLifetimes.push_back(fPlanck/(300*keV));
129 
130  ExcitEnergies.push_back(14120*keV);
131  ExcitSpins.push_back(5.0/2.0);
132  ExcitLifetimes.push_back(fPlanck/(200*keV));
133 
134  ExcitEnergies.push_back(14.39E3*keV);
135  ExcitSpins.push_back(5.0/2.0);
136  ExcitLifetimes.push_back(fPlanck/(260*keV));
137 
138  ExcitEnergies.push_back(14940*keV);
139  ExcitSpins.push_back(3.0/2.0);
140  ExcitLifetimes.push_back(fPlanck/(380*keV));
141 
142  ExcitEnergies.push_back(15108.2*keV);
143  ExcitSpins.push_back(3.0/2.0);
144  ExcitLifetimes.push_back(fPlanck/(5*keV));
145 
146  ExcitEnergies.push_back(19500*keV);
147  ExcitSpins.push_back(5.0/2.0);
148  ExcitLifetimes.push_back(fPlanck/(450*keV));
149 
150 }
151 
153 {}