| MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fis. Spec. Average |
|---|---|---|---|---|---|---|---|
| 1 | (n,total) | 4.436 (b) | 4.720 (b) | 1.064 | − | 2.538 (b) | 3.698 (b) |
| 2 | (n,elastic) | 2.183 (b) | 2.465 (b) | 1.129 | − | 1.149 (b) | 3.190 (b) |
| 4 | (n,inelastic) | ( E-threshold = 105.0 keV ) | 386.7 (mb) | 423.7 (mb) | |||
| 16 | (n,2n) | ( E-threshold = 13.63 MeV ) | 1.557 (mb) | 1.073 (μb) | |||
| 22 | (n,na) | ( E-threshold = 8.575 MeV ) | 153.1 (μb) | 274.1 (nb) | |||
| 28 | (n,np) | ( E-threshold = 9.019 MeV ) | 553.5 (mb) | 137.4 (μb) | |||
| 44 | (n,n2p) | ( E-threshold = 15.70 MeV ) | − | 21.64 (pb) | |||
| 102 | (n,γ) | 2.253 (b) | 2.255 (b) | 1.001 | 1.215 (b) | 994.5 (μb) | 4.479 (mb) |
| 103 | (n,p) | 0.000 (b) | 0.000 (b) | − | 495.5 (mb) | 343.7 (mb) | 78.47 (mb) |
| 104 | (n,d) | ( E-threshold = 6.753 MeV ) | 6.285 (mb) | 3.031 (μb) | |||
| 105 | (n,t) | ( E-threshold = 12.66 MeV ) | 71.08 (pb) | 983.2 (pb) | |||
| 106 | (n,He-3) | ( E-threshold = 7.839 MeV ) | 3.604 (μb) | 886.4 (pb) | |||
| 107 | (n,a) | 0.000 (b) | 0.000 (b) | − | 17.16 (mb) | 84.79 (mb) | 871.8 (μb) |
| 108 | (n,2a) | ( E-threshold = 8.247 MeV ) | 3.579 (fb) | 6.379 (pb) | |||
| 111 | (n,2p) | ( E-threshold = 7.614 MeV ) | 10.84 (mb) | 2.285 (μb) | |||
| 112 | (n,pa) | ( E-threshold = 8.835 MeV ) | 172.5 (nb) | 26.84 (nb) | |||
| 115 | (n,pd) | ( E-threshold = 13.44 MeV ) | 1.8e-20 (b) | 568.3 (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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