| MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fis. Spec. Average |
|---|---|---|---|---|---|---|---|
| 1 | (n,total) | 13.95 (b) | 15.60 (b) | 1.119 | − | 3.581 (b) | 4.296 (b) |
| 2 | (n,elastic) | 4.740 (b) | 5.351 (b) | 1.129 | − | 1.926 (b) | 2.891 (b) |
| 4 | (n,inelastic) | ( E-threshold = 50.19 keV ) | 373.1 (mb) | 1.332 (b) | |||
| 16 | (n,2n) | ( E-threshold = 7.972 MeV ) | 1.195 (b) | 1.263 (mb) | |||
| 22 | (n,na) | ( E-threshold = 5.590 MeV ) | 190.8 (μb) | 70.18 (nb) | |||
| 24 | (n,2na) | ( E-threshold = 13.10 MeV ) | 4.5e-21 (b) | 378.0 (fb) | |||
| 28 | (n,np) | ( E-threshold = 9.210 MeV ) | 12.40 (mb) | 2.100 (μb) | |||
| 32 | (n,nd) | ( E-threshold = 14.95 MeV ) | − | 48.78 (pb) | |||
| 41 | (n,2np) | ( E-threshold = 17.20 MeV ) | − | 4.625 (pb) | |||
| 102 | (n,γ) | 8.968 (b) | 8.973 (b) | 1.001 | 174.7 (b) | 1.036 (mb) | 67.39 (mb) |
| 103 | (n,p) | 9.000 (nb) | 9.005 (nb) | 1.001 | 24.06 (mb) | 66.74 (mb) | 3.846 (mb) |
| 104 | (n,d) | ( E-threshold = 6.957 MeV ) | 1.391 (mb) | 280.6 (nb) | |||
| 105 | (n,t) | ( E-threshold = 8.613 MeV ) | 1.864 (μb) | 4.307 (nb) | |||
| 106 | (n,He-3) | ( E-threshold = 8.746 MeV ) | 24.13 (pb) | 8.748 (pb) | |||
| 107 | (n,a) | 2.526 (μb) | 2.527 (μb) | 1.001 | 1.372 (mb) | 7.778 (mb) | 137.6 (μb) |
| 111 | (n,2p) | ( E-threshold = 6.524 MeV ) | 28.58 (μb) | 5.535 (nb) | |||
| 112 | (n,pa) | ( E-threshold = 5.490 MeV ) | 510.9 (pb) | 9.378 (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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