MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
---|---|---|---|---|---|---|---|
1 | (n,total) | 88.53 (b) | 89.36 (b) | 1.009 | − | 5.321 (b) | 6.860 (b) |
2 | (n,elastic) | 4.474 (b) | 5.018 (b) | 1.122 | − | 2.587 (b) | 4.156 (b) |
4 | (n,inelastic) | ( E-thr = 93.71 keV ) | 620.4 (mb) | 2.628 (b) | |||
16 | (n,2n) | ( E-thr = 7.669 MeV ) | 2.104 (b) | 6.326 (mb) | |||
17 | (n,3n) | ( E-thr = 14.09 MeV ) | − | 6.512 (μb) | |||
22 | (n,na) | 0.000 (b) | 0.000 (b) | − | 383.2e-12 (b) | 72.05 (μb) | 24.36 (nb) |
28 | (n,np) | ( E-thr = 7.386 MeV ) | 48.98 (μb) | 39.11 (nb) | |||
32 | (n,nd) | ( E-thr = 12.26 MeV ) | 0.000 (b) | 39.36e-12 (b) | |||
102 | (n,γ) | 84.05 (b) | 84.35 (b) | 1.004 | 1.915 (kb) | 1.746 (mb) | 68.44 (mb) |
103 | (n,p) | ( E-thr = 1.326 MeV ) | 6.375 (mb) | 2.752 (μb) | |||
104 | (n,d) | ( E-thr = 5.149 MeV ) | 709.3 (μb) | 176.2 (nb) | |||
105 | (n,t) | ( E-thr = 5.969 MeV ) | 21.97 (μb) | 10.66 (nb) | |||
106 | (n,He-3) | ( E-thr = 5.843 MeV ) | 0.000 (b) | 195.8e-15 (b) | |||
107 | (n,a) | 0.000 (b) | 0.000 (b) | − | 16.08 (μb) | 1.315 (mb) | 1.017 (μb) |
These cross sections are calculated from JENDL-4.0 at 300K.
The background color of each cell noted a cross section means the order of the cross-section value.
The unit of cross section, (b), means barns, and SI prefixes are used as following.
(kb) → 103(b), (mb) → 10−3(b),
(μb) → 10−6(b), (nb) → 10−9(b).
MT is a number that defines a reaction type. For the relation between MT and reaction type, please see here or refer to the manual of ENDF formats.
Maxwellian Average :
where T denotes the temperature, and kB the Boltzmann constant.
The upper and lower limits of integration, EL and EU
are set to 10−5 eV and 10 eV, respectively.
Resonance Integral :
with EL = 0.5 eV and EU = 10 MeV.
U-235 Thermal Fission-Neutron Spectrum Average (Fiss. Spec. Average) :
with EL = 10−5 eV and EU = 20 MeV.
The parameters a and b are 0.988 MeV and 2.249 MeV−1, respectively.
Westcott g-factor :
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