Nuclide | MAT | Numerical Data*1 | Comments | Figures*2) | Sig. table |
92-U-230 | 9213 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-231 | 9216 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-232 | 9219 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-233 | 9222 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-234 | 9225 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-235 | 9228 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-236 | 9231 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-237 | 9234 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-238 | 9237 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
92-U-240 | 9243 | original, 0K, 300K u20 | comment | Fig1 Fig2 Fig3 Fig4 | table |
*1) u20: Data up to 20 MeV. *2) Fig1, Fig2 and Fig3 are made from pointwise files at 300 K. Fig1 : Total, elastic and inelastic scattering, capture and fission cross sections Fig2 : Same as Fig1 but the cross sections are averaged in 70 energy group intervals Fig3 : Threshold reaction cross sections Fig4 : Number of prompt and delayed neutrons per fission |