MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
---|---|---|---|---|---|---|---|
1 | (n,total) | 11.23 (b) | 12.01 (b) | 1.069 | − | 4.537 (b) | 5.613 (b) |
2 | (n,elastic) | 6.002 (b) | 6.775 (b) | 1.129 | − | 2.818 (b) | 3.952 (b) |
4 | (n,inelastic) | ( E-thr = 128.5 keV ) | 161.6 (mb) | 1.566 (b) | |||
16 | (n,2n) | ( E-thr = 6.874 MeV ) | 1.527 (b) | 8.553 (mb) | |||
17 | (n,3n) | ( E-thr = 16.65 MeV ) | − | 517.8 (nb) | |||
22 | (n,na) | ( E-thr = 2.857 MeV ) | 623.6 (μb) | 141.8 (nb) | |||
28 | (n,np) | ( E-thr = 9.319 MeV ) | 231.0 (μb) | 86.51 (nb) | |||
32 | (n,nd) | ( E-thr = 13.82 MeV ) | 0.000 (b) | 248.5e-12 (b) | |||
102 | (n,γ) | 5.232 (b) | 5.238 (b) | 1.001 | 100.9 (b) | 1.002 (mb) | 82.60 (mb) |
103 | (n,p) | ( E-thr = 850.6 keV ) | 21.31 (mb) | 35.61 (μb) | |||
104 | (n,d) | ( E-thr = 6.985 MeV ) | 680.2 (μb) | 150.8 (nb) | |||
105 | (n,t) | ( E-thr = 7.575 MeV ) | 11.42 (μb) | 10.64 (nb) | |||
106 | (n,He-3) | ( E-thr = 8.926 MeV ) | 15.91e-15 (b) | 3.879e-12 (b) | |||
107 | (n,a) | 0.000 (b) | 0.000 (b) | − | 465.8 (μb) | 5.513 (mb) | 58.79 (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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