| MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fis. Spec. Average |
|---|---|---|---|---|---|---|---|
| 1 | (n,total) | 13.66 (b) | 14.64 (b) | 1.072 | − | 4.875 (b) | 6.437 (b) |
| 2 | (n,elastic) | 2.906 (b) | 3.282 (b) | 1.129 | − | 2.731 (b) | 4.209 (b) |
| 4 | (n,inelastic) | ( E-threshold = 105.0 keV ) | 499.4 (mb) | 2.117 (b) | |||
| 16 | (n,2n) | ( E-threshold = 9.567 MeV ) | 1.601 (b) | 855.5 (μb) | |||
| 17 | (n,3n) | ( E-threshold = 17.42 MeV ) | − | 62.51 (nb) | |||
| 22 | (n,na) | ( E-threshold = 1.017 MeV ) | 246.6 (μb) | 96.76 (nb) | |||
| 28 | (n,np) | ( E-threshold = 5.020 MeV ) | 6.559 (mb) | 5.717 (μb) | |||
| 32 | (n,nd) | ( E-threshold = 12.32 MeV ) | 3.1e-16 (b) | 310.4 (pb) | |||
| 33 | (n,nt) | ( E-threshold = 13.26 MeV ) | 6.2e-21 (b) | 1.383 (pb) | |||
| 41 | (n,2np) | ( E-threshold = 14.56 MeV ) | − | 45.33 (pb) | |||
| 102 | (n,γ) | 10.64 (b) | 10.65 (b) | 1.001 | 1.158 (kb) | 972.0 (μb) | 110.0 (mb) |
| 103 | (n,p) | 1.000 (μb) | 1.001 (μb) | 1.001 | 2.576 (mb) | 27.20 (mb) | 307.0 (μb) |
| 104 | (n,d) | ( E-threshold = 2.778 MeV ) | 2.053 (mb) | 468.2 (nb) | |||
| 105 | (n,t) | ( E-threshold = 6.013 MeV ) | 11.89 (μb) | 8.801 (nb) | |||
| 106 | (n,He-3) | ( E-threshold = 5.473 MeV ) | 207.0 (pb) | 6.144 (pb) | |||
| 107 | (n,a) | 85.03 (nb) | 85.08 (nb) | 1.001 | 127.0 (μb) | 3.659 (mb) | 7.936 (μb) |
| 111 | (n,2p) | ( E-threshold = 6.306 MeV ) | 1.050 (nb) | 2.718 (pb) | |||
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These cross sections are calculated from JENDL-5 at 300K using with LINEAR, RECENT and SIGMA1 codes of PREPRO. For more detail, please click here.
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), (pb) → 10−12(b), (fb) → 10−15(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.
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