MT | Reaction | 0.0253-eV | Maxwellian Average |
g-factor | Resonance Integral |
14-MeV | Fiss. Spec. Average |
---|---|---|---|---|---|---|---|
1 | (n,total) | 6.370 (b) | 7.126 (b) | 1.119 | − | 3.842 (b) | 4.946 (b) |
2 | (n,elastic) | 5.890 (b) | 6.646 (b) | 1.128 | − | 2.400 (b) | 3.733 (b) |
4 | (n,inelastic) | ( E-thr = 153.1 keV ) | 408.2 (mb) | 1.184 (b) | |||
16 | (n,2n) | ( E-thr = 10.61 MeV ) | 986.5 (mb) | 276.8 (μb) | |||
17 | (n,3n) | ( E-thr = 19.55 MeV ) | − | 67.52e-12 (b) | |||
22 | (n,na) | ( E-thr = 6.683 MeV ) | 41.87 (μb) | 40.07 (nb) | |||
28 | (n,np) | ( E-thr = 7.104 MeV ) | 23.02 (mb) | 17.69 (μb) | |||
32 | (n,nd) | ( E-thr = 15.41 MeV ) | − | 51.53e-12 (b) | |||
102 | (n,γ) | 480.2 (mb) | 480.2 (mb) | 1.000 | 8.723 (b) | 1.009 (mb) | 26.36 (mb) |
103 | (n,p) | 0.000 (b) | 0.000 (b) | − | 4.449 (mb) | 16.91 (mb) | 410.1 (μb) |
104 | (n,d) | ( E-thr = 4.766 MeV ) | 959.9 (μb) | 240.1 (nb) | |||
105 | (n,t) | ( E-thr = 9.156 MeV ) | 1.940 (μb) | 11.54 (nb) | |||
106 | (n,He-3) | ( E-thr = 10.11 MeV ) | 19.99e-15 (b) | 4.688e-12 (b) | |||
107 | (n,a) | 0.000 (b) | 0.000 (b) | − | 99.82 (μb) | 5.623 (mb) | 4.835 (μb) |
These cross sections are calculated from JENDL-3.3 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 :
|