| MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
|---|---|---|---|---|---|---|---|
| 1 | (n,total) | 5.076 (b) | 5.725 (b) | 1.128 | − | 3.569 (b) | 4.777 (b) |
| 2 | (n,elastic) | 5.031 (b) | 5.681 (b) | 1.129 | − | 1.870 (b) | 3.760 (b) |
| 4 | (n,inelastic) | ( E-thr = 662.8 keV ) | 410.8 (mb) | 1.015 (b) | |||
| 16 | (n,2n) | ( E-thr = 9.390 MeV ) | 1.284 (b) | 929.8 (μb) | |||
| 17 | (n,3n) | ( E-thr = 16.17 MeV ) | − | 231.0 (nb) | |||
| 22 | (n,na) | ( E-thr = 8.257 MeV ) | 0.000 (b) | 408.2e-12 (b) | |||
| 28 | (n,np) | ( E-thr = 12.50 MeV ) | 0.000 (b) | 7.838 (nb) | |||
| 102 | (n,γ) | 44.21 (mb) | 44.24 (mb) | 1.000 | 709.8 (mb) | 665.3 (μb) | 1.578 (mb) |
| 103 | (n,p) | ( E-thr = 6.568 MeV ) | 3.103 (mb) | 814.2 (nb) | |||
| 104 | (n,d) | ( E-thr = 10.25 MeV ) | 538.8 (nb) | 31.61 (nb) | |||
| 105 | (n,t) | ( E-thr = 12.46 MeV ) | 0.000 (b) | 72.63e-12 (b) | |||
| 106 | (n,He-3) | ( E-thr = 15.12 MeV ) | − | 94.18e-21 (b) | |||
| 107 | (n,a) | ( E-thr = 2.489 MeV ) | 42.70 (μb) | 20.67 (nb) | |||
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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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