|total||5.332 (kb)||5.335 (kb)||1.001||−||1.169 (b)||2.941 (b)|
|elastic||3.668 (b)||4.099 (b)||1.117||−||954.4 (mb)||2.121 (b)|
|capture||54.02 (μb)||54.06 (μb)||1.001||222.7 (μb)||35.21 (μb)||39.22 (μb)|
|(n,p)||5.328 (kb)||5.331 (kb)||1.001||2.383 (kb)||139.8 (mb)||817.0 (mb)|
|(n,d)||( E-thr = 4.362 MeV )||74.07 (mb)||2.647 (mb)|
These cross sections are calculated from JENDL-4.0 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).
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 :