ENDF/B-VI REVISION 2 TAPE 101 101 0 1.904100+4 4.060990+1 0 0 0 01931 1451 1 0.000000+0 0.000000+0 0 0 0 61931 1451 2 1.000000+0 0.000000+0 0 0 10 61931 1451 3 0.000000+0 0.000000+0 0 0 19 51931 1451 4 19-K - 41 HEDL EVAL-JAN79 MANN 1931 1451 5 DIST-JAN90 900123 1931 1451 6 ----ENDF/B-VI MATERIAL 1931 1931 1451 7 -----INCIDENT NEUTRON DATA 1931 1451 8 ------ENDF-6 FORMAT 1931 1451 9 ENDF/B-V MATERIAL CONVERTED TO ENDF-6 FORMAT BY NNDC 1931 1451 10 * * * * * * *1931 1451 11 MF= 3, MT= 103 SMOOTH (N,P) CROSS SECTION 1931 1451 12 THE EVALUATION IS BASED ON A NUCLEAR MODEL CALCULATION 1931 1451 13 CONSISTING OF HAUSER-FESHBACH AND PRE-EQUILIBRIUM COMPONENTS. THE1931 1451 14 EVALUATION IS IN GOOD AGREEMENT WITH THE DATA OF BASS ET AL 1931 1451 15 (EANDG(E)-57(1965)P. 1). FOR (N,P)AR-41, FILE 3 MUST BE 1931 1451 16 MULTIPLIED BY QUANTITIES IN FILE 9. 1931 1451 17 MF= 9, MT= 103 (N,P) FRACTION 1931 1451 18 THE EVALUATION IS BASED ON A NUCLEAR MODEL CALCULATION UP 1931 1451 19 TO 16 MEV AND THEREAFTER FOLLOWS THE CROSS SECTIONS MEASURED BY 1931 1451 20 BORMANN ET AL (NUCL. PHYS. A130(1969)195, WHICH ARE A FACTOR OF 2 1931 1451 21 LOWER THAN CALCULATIONS AT 18 MEV. AT LOWER ENERGIES THE 1931 1451 22 AGREEMENT IS GOOD. 1931 1451 23 1 451 28 01931 1451 24 2 151 4 01931 1451 25 3 103 8 01931 1451 26 8 103 4 01931 1451 27 9 103 6 01931 1451 28 0.000000+0 0.000000+0 0 0 0 01931 1 0 29 0.000000+0 0.000000+0 0 0 0 01931 0 0 30 1.904100+4 4.060990+1 0 0 1 01931 2151 31 1.904100+4 1.000000+0 0 0 1 01931 2151 32 1.000000-5 1.000000+6 0 0 0 01931 2151 33 1.500000+0 5.040000-1 0 0 0 01931 2151 34 0.000000+0 0.000000+0 0 0 0 01931 2 0 35 0.000000+0 0.000000+0 0 0 0 01931 0 0 36 1.904100+4 4.060990+1 0 0 0 01931 3103 37 -1.709600+6-1.709600+6 0 0 1 141931 3103 38 14 2 1931 3103 39 1.751000+6 0.000000+0 3.000000+6 4.000000-5 4.000000+6 3.100000-31931 3103 40 5.000000+6 1.330000-2 6.000000+6 1.900000-2 7.000000+6 2.130000-21931 3103 41 8.000000+6 2.860000-2 9.000000+6 3.670000-2 1.000000+7 4.800000-21931 3103 42 1.200000+7 6.660000-2 1.400000+7 8.560000-2 1.600000+7 1.021000-11931 3103 43 1.800000+7 1.174000-1 2.000000+7 1.309000-1 1931 3103 44 0.000000+0 0.000000+0 0 0 0 01931 3 0 45 0.000000+0 0.000000+0 0 0 0 01931 0 0 46 1.904100+4 4.060990+1 0 0 1 01931 8103 47 1.804100+4 0.000000+0 9 0 12 18401931 8103 48 6.577201+3 1.000000+0 1.904100+4 9.917000-1 1.198300+6 1.020000+01931 8103 49 6.577201+3 1.000000+0 1.904100+4 7.800000-3 2.492000+6 1.000000+01931 8103 50 0.000000+0 0.000000+0 0 0 0 01931 8 0 51 0.000000+0 0.000000+0 0 0 0 01931 0 0 52 1.904100+4 4.060990+1 0 0 1 01931 9103 53 -1.709600+6-1.709600+6 0 0 1 71931 9103 54 7 2 1931 9103 55 1.751000+6 1.000000+0 1.000000+7 1.000000+0 1.200000+7 8.700000-11931 9103 56 1.400000+7 6.300000-1 1.600000+7 4.400000-1 1.800000+7 3.100000-11931 9103 57 2.000000+7 2.300000-1 1931 9103 58 0.000000+0 0.000000+0 0 0 0 01931 9 0 59 0.000000+0 0.000000+0 0 0 0 01931 0 0 60 0.000000+0 0.000000+0 0 0 0 0 0 0 0 61 -1 0 0 0