MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
---|---|---|---|---|---|---|---|
1 | (n,total) | 3.641 (kb) | 3.649 (kb) | 1.002 | − | 6.018 (b) | 8.293 (b) |
2 | (n,elastic) | 9.319 (b) | 10.52 (b) | 1.129 | − | 2.833 (b) | 4.497 (b) |
4 | (n,inelastic) | ( E-thr = 60.24 keV ) | 299.4 (mb) | 1.516 (b) | |||
16 | (n,2n) | ( E-thr = 5.197 MeV ) | 326.5 (mb) | 15.77 (mb) | |||
17 | (n,3n) | ( E-thr = 11.74 MeV ) | 55.17 (mb) | 7.740 (μb) | |||
18 | (n,fission) | 3.362 (kb) | 3.366 (kb) | 1.001 | 1.460 (kb) | 2.496 (b) | 2.224 (b) |
19 | (n,f) | 3.362 (kb) | 3.366 (kb) | 1.001 | 1.460 (kb) | 1.578 (b) | 2.217 (b) |
20 | (n,nf) | ( E-thr = 2.500 MeV ) | 813.8 (mb) | 7.428 (mb) | |||
21 | (n,2nf) | ( E-thr = 7.500 MeV ) | 107.7 (mb) | 19.61 (μb) | |||
37 | (n,4n) | ( E-thr = 17.30 MeV ) | − | 846.9e-12 (b) | |||
38 | (n,3nf) | ( E-thr = 14.50 MeV ) | − | 2.711 (nb) | |||
102 | (n,γ) | 270.1 (b) | 270.3 (b) | 1.001 | 116.3 (b) | 673.8 (μb) | 38.85 (mb) |
456 | νp | 4.000 | − | − | − | 7.500 | − |
455 | νd | 2.733e-3 | − | − | − | 1.885e-3 | − |
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 :
νp,
νd
: numbers of prompt and delayed neutrons per fission.
|