MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
---|---|---|---|---|---|---|---|
1 | (n,total) | 16.45 (b) | 17.14 (b) | 1.042 | − | 4.394 (b) | 5.784 (b) |
2 | (n,elastic) | 5.395 (b) | 6.088 (b) | 1.129 | − | 2.330 (b) | 4.389 (b) |
4 | (n,inelastic) | ( E-thr = 663.8 keV ) | 531.7 (mb) | 1.337 (b) | |||
16 | (n,2n) | ( E-thr = 10.01 MeV ) | 1.493 (b) | 701.0 (μb) | |||
17 | (n,3n) | ( E-thr = 17.40 MeV ) | − | 41.91 (nb) | |||
22 | (n,na) | ( E-thr = 2.902 MeV ) | 432.5 (μb) | 157.0 (nb) | |||
28 | (n,np) | ( E-thr = 9.001 MeV ) | 1.718 (mb) | 580.9 (nb) | |||
32 | (n,nd) | ( E-thr = 16.03 MeV ) | − | 499.7e-15 (b) | |||
102 | (n,γ) | 11.06 (b) | 11.05 (b) | 0.999 | 39.18 (b) | 929.2 (μb) | 55.87 (mb) |
103 | (n,p) | ( E-thr = 2.129 MeV ) | 31.63 (mb) | 35.64 (μb) | |||
104 | (n,d) | ( E-thr = 6.756 MeV ) | 1.185 (mb) | 359.6 (nb) | |||
105 | (n,t) | ( E-thr = 9.718 MeV ) | 802.0 (nb) | 7.879 (nb) | |||
106 | (n,He-3) | ( E-thr = 7.759 MeV ) | 2.917e-12 (b) | 604.7e-15 (b) | |||
107 | (n,a) | 0.000 (b) | 0.000 (b) | − | 142.7 (μb) | 6.996 (mb) | 9.349 (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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