|1||(n,total)||4.247 (b)||4.706 (b)||1.108||−||801.5 (mb)||2.538 (b)|
|2||(n,elastic)||4.246 (b)||4.705 (b)||1.108||−||624.4 (mb)||2.532 (b)|
|16||(n,2n)||( E-thr = 3.339 MeV )||177.2 (mb)||5.276 (mb)|
|102||(n,γ)||550.0 (μb)||550.2 (μb)||1.000||279.9 (μb)||9.512 (μb)||7.072 (μb)|
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 :