| MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
|---|---|---|---|---|---|---|---|
| 1 | (n,total) | 6.367 (b) | 6.865 (b) | 1.078 | − | 5.699 (b) | 6.979 (b) |
| 2 | (n,elastic) | 3.871 (b) | 4.367 (b) | 1.128 | − | 3.423 (b) | 5.083 (b) |
| 4 | (n,inelastic) | ( E-thr = 80.01 keV ) | 482.4 (mb) | 1.837 (b) | |||
| 16 | (n,2n) | ( E-thr = 7.993 MeV ) | 1.789 (b) | 3.781 (mb) | |||
| 17 | (n,3n) | ( E-thr = 14.40 MeV ) | − | 10.81 (μb) | |||
| 22 | (n,na) | ( E-thr = 663.1 keV ) | 19.73 (μb) | 8.533 (nb) | |||
| 28 | (n,np) | ( E-thr = 8.574 MeV ) | 2.630 (μb) | 9.141 (nb) | |||
| 32 | (n,nd) | ( E-thr = 13.75 MeV ) | 0.000 (b) | 5.055e-12 (b) | |||
| 102 | (n,γ) | 2.497 (b) | 2.498 (b) | 1.000 | 63.94 (b) | 1.019 (mb) | 54.32 (mb) |
| 103 | (n,p) | ( E-thr = 2.686 MeV ) | 1.813 (mb) | 512.8 (nb) | |||
| 104 | (n,d) | ( E-thr = 6.249 MeV ) | 65.43 (μb) | 33.52 (nb) | |||
| 105 | (n,t) | ( E-thr = 7.530 MeV ) | 5.061 (μb) | 7.371 (nb) | |||
| 107 | (n,a) | 0.000 (b) | 0.000 (b) | − | 4.086 (μb) | 1.683 (mb) | 549.8 (nb) |
|
These cross sections are calculated from JENDL-3.2 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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