$Rev:: 532 $ $Date:: 2011-12-05#$ 1 0 0 0 4.811200+4 1.109420+2 1 0 99 14843 1451 1 0.000000+0 0.000000+0 0 0 0 64843 1451 2 1.000000+0 2.000000+7 1 0 10 74843 1451 3 0.000000+0 0.000000+0 0 0 134 494843 1451 4 48-Cd-112 IRMM,UA,ANLEVAL-OCT10 I.Sirakov,S.Kopecky+,J.McCabe+ 4843 1451 5 DIST-... 20111222 4843 1451 6 ----ENDF/B-VII.1 MATERIAL 4843 4843 1451 7 -----INCIDENT NEUTRON DATA 4843 1451 8 ------ENDF-6 FORMAT 4843 1451 9 ==================================================================4843 1451 10 The present resolved resonance evaluation is a result of a 4843 1451 11 consistent analysis of available experimental information on Cd 4843 1451 12 isotopes together with simultaneous resonance optimization of 4843 1451 13 natural-Cd transmission and capture data measured at GELINA. The 4843 1451 14 R-matrix code REFIT has been used for resonance analysis. 4843 1451 15 Resolved resonance parameters in MF=2 are REFIT (v.2008) output 4843 1451 16 parameters translated into ENDF-6 Reich-Moore format (LRU=1,LRF=3)4843 1451 17 The code REFEND (v.July 2008) has been used for the translation 4843 1451 18 (format-conversion). The REFIT cross-sections are preserved in 4843 1451 19 ENDF provided that NJOY-compatible channel- and scattering-radius 4843 1451 20 options have been chosen by the REFIT evaluator. Conversion below 4843 1451 21 is rigorous/exact because of such compatibility. 4843 1451 22 A full description of the resolved resonance evaluation 4843 1451 23 performed at the EC-JRC-IRMM, Geel, Belgium, is given in Ref.1. 4843 1451 24 Reference: 4843 1451 25 1) S.Kopecky et al. Private Communication. 4843 1451 26 ==================================================================4843 1451 27 4843 1451 28 The remaining part of the evaluation (above the RRR) is the 4843 1451 29 ENDF/B-VII.0 file, which description has been left below intact 4843 1451 30 (including the description of the replaced RRR evaluation in 4843 1451 31 order to be temporarily used for comparison). 4843 1451 32 4843 1451 33 ============================================================== 4843 1451 34 File produced by WPEC Subgroup 23 in 2004-2005 4843 1451 35 - WPEC: NEA Working Party on Evaluation Cooperation 4843 1451 36 - SG23: International library of fission product evaluations 4843 1451 37 4843 1451 38 4843 1451 39 File obtained by merging: &&4843 1451 40 - Resolved Resonances (MLBW) <11.5 keV : Ref.1 &&4843 1451 41 - Unresolved Resonances 11.5 keV - 100 keV : ENDF/B-VI &&4843 1451 42 - Fast neutron region >100 keV : ENDF/B-VI &&4843 1451 43 &&4843 1451 44 Calculated thermal cross sections & resonance integrals: &&4843 1451 45 --------------------------------------------- &&4843 1451 46 Reaction Cross section Res. integral &&4843 1451 47 (barn) (barn) &&4843 1451 48 Total 7.2611E+00 - &&4843 1451 49 Elastic 5.0654E+00 - &&4843 1451 50 Capture 2.1957E+00 1.33E+01 &&4843 1451 51 --------------------------------------------- &&4843 1451 52 4843 1451 53 Corrected threshold energy secondary energy distributions 4843 1451 54 in MF=5. 4843 1451 55 4843 1451 56 Reference: 4843 1451 57 1) S.F.Mughabghab: Atlas of Neutron Resonances, to be 4843 1451 58 published by Elsevier, 2006 (5-th edition of BNL-325) 4843 1451 59 ============================================================== 4843 1451 60 4843 1451 61 ENDF/B-VI MOD 4 Revision (R.Q. Wright, ORNL, V. McLane, NNDC, 4843 1451 62 August, 1996) 4843 1451 63 File 1 comments added 4843 1451 64 File 3, MT=4 Obsolete code deleted 4843 1451 65 4843 1451 66 **************************************************************** 4843 1451 67 4843 1451 68 ENDF/B-VI MOD 3 (J. McCabe, A.B. Smith, J.W. Whalen, ANL, 4843 1451 69 August, 1994) 4843 1451 70 4843 1451 71 Comprehensive neutronic evaluated files for the naturally- 4843 1451 72 occurring isotopes of cadmium are deduced from the experimental 4843 1451 73 data and nuclear models. Particular attention is given to those 4843 1451 74 processes relevant to fuel-cycle and fisson-product applications.4843 1451 75 Some discrepancies with the previous evaluation are very large 4843 1451 76 (e.g., as much as 100%), and the differences have the potential 4843 1451 77 for a pronounced effect on applications usage. The present files4843 1451 78 are comprehensive, including many important processes that are 4843 1451 79 not represented in the previous evaluation. See Ref.1 for 4843 1451 80 complete documentation. 4843 1451 81 The resonance region evaluation was carried over from the 4843 1451 82 previous evaluation, see following. 4843 1451 83 4843 1451 84 REFERENCE 4843 1451 85 1. J. McCabe, A.B. Smith, J.W. Whalen, Report ANL/NDM-129 (1993) 4843 1451 86 Argonne National Laboratory. 4843 1451 87 4843 1451 88 *****************************************************************4843 1451 89 4843 1451 90 ENDF/B-VI MOD 2 Revision (R.Q. Wright, ORNL, December 1991) 4843 1451 91 See ANS Transactions, volume 68, part A, page 468 4843 1451 92 4843 1451 93 The ENDF/B-V evaluation used the SLBW formalism in the 4843 1451 94 resolved resonance range and did not have unresolved resonance 4843 1451 95 parameters. 4843 1451 96 4843 1451 97 Resolved resonance range (1.0E-5 eV to 7.35 keV) 4843 1451 98 ------------------------------------------------ 4843 1451 99 The MLBW formalism is used for this evaluation. The highest 4843 1451 100 energy resonance included is 11455 eV. The resolved resonance 4843 1451 101 parameters are taken from ref. 1 and from table 5 of ref. 2. 4843 1451 102 Upper limit of the resolved resonance range is 7350 eV. This 4843 1451 103 evaluation has 64 s-wave and 54 p-wave resonances including 24 4843 1451 104 s-wave resonances above 7350 eV. The bound level at -125 eV has 4843 1451 105 a gamma-n0 of 93.91 meV and gamma-gamma of 83 meV (ref. 1). The 4843 1451 106 bound level accounts for about 95% of the thermal capture cross 4843 1451 107 section. The elastic cross section at thermal is 6.31 barns. 4843 1451 108 4843 1451 109 Unresolved resonance range (7.35 to 100 keV) 4843 1451 110 -------------------------------------------- 4843 1451 111 The unresolved resonance range fit is based on the average 4843 1451 112 capture cross sections from ref. 3. 4843 1451 113 The unresolved resonance parameters are based on: 4843 1451 114 D0 = 190 eV, S0 = 0.5, S1 = 4.4, AND S2 = 1.5 4843 1451 115 D1 = 75 eV, SG0 = 4.05, SG1 = 12.0 4843 1451 116 4843 1451 117 File 3: 4843 1451 118 ------- 4843 1451 119 Total, elastic, and capture are set to zero in the resolved 4843 1451 120 and unresolved resonance ranges (1.0E-5 eV to 100 keV). 4843 1451 121 4843 1451 122 2200 m/s capture cross section, barns 4843 1451 123 (from resonance parameters) = 2.195 4843 1451 124 4843 1451 125 computed resonance integral = 13.50 4843 1451 126 4843 1451 127 REFERENCES 4843 1451 128 4843 1451 129 1. S.F. Mughabghab, M. Divadeenam, and N.E. Holden, Neutron 4843 1451 130 Cross Sections, vol 1A, Academic Press, New York (1981). 4843 1451 131 2. Musgrove et al., Neutron-capture resonance parameters and 4843 1451 132 cross sections for the even-A isotopes of cadmium, J. of 4843 1451 133 Physics, part G 4 (5), 771 (1978). 4843 1451 134 3. Musgrove et al., 1978 Harwell Conf. on Neutron Physics and 4843 1451 135 Nucl. Data, table V, page 449. (1978). Values are mult. by 4843 1451 136 a factor of 1.0069 (see Nucl.Sci.Eng. 82, p. 230). 4843 1451 137 4843 1451 138 1 451 187 14843 1451 139 2 151 174 14843 1451 140 3 1 24 04843 1451 141 3 2 24 04843 1451 142 3 4 20 04843 1451 143 3 16 7 04843 1451 144 3 17 5 04843 1451 145 3 22 8 04843 1451 146 3 28 7 04843 1451 147 3 32 5 04843 1451 148 3 33 4 04843 1451 149 3 51 11 04843 1451 150 3 52 9 04843 1451 151 3 53 9 04843 1451 152 3 54 9 04843 1451 153 3 55 9 04843 1451 154 3 56 9 04843 1451 155 3 57 8 04843 1451 156 3 58 8 04843 1451 157 3 91 15 04843 1451 158 3 102 13 04843 1451 159 3 103 9 04843 1451 160 3 104 8 04843 1451 161 3 105 7 04843 1451 162 3 106 6 04843 1451 163 3 107 10 04843 1451 164 4 2 96 04843 1451 165 4 16 2 04843 1451 166 4 17 2 04843 1451 167 4 22 2 04843 1451 168 4 28 2 04843 1451 169 4 32 2 04843 1451 170 4 33 2 04843 1451 171 4 51 2 04843 1451 172 4 52 2 04843 1451 173 4 53 2 04843 1451 174 4 54 2 04843 1451 175 4 55 2 04843 1451 176 4 56 2 04843 1451 177 4 57 2 04843 1451 178 4 58 2 04843 1451 179 4 91 2 04843 1451 180 5 16 75 14843 1451 181 5 17 34 14843 1451 182 5 22 64 14843 1451 183 5 28 75 14843 1451 184 5 32 31 14843 1451 185 5 33 31 14843 1451 186 5 91 212 04843 1451 187 0.000000+0 0.000000+0 0 0 0 04843 1 099999 0.000000+0 0.000000+0 0 0 0 04843 0 0 0 4.811200+4 1.109420+2 0 0 1 04843 2151 1 4.811200+4 1.000000+0 0 0 2 04843 2151 2 1.000000-5 1.150000+4 1 3 0 14843 2151 3 0.000000+0 0.000000+0 1 0 2 44843 2151 4 1.109420+2 6.600000-1 0 0 252 424843 2151 5 -1.216363+1 5.000000-1 3.439000-3 7.600000-2 0.000000+0 0.000000+04843 2151 6 6.678000+1 5.000000-1 8.476000-3 6.280000-2 0.000000+0 0.000000+04843 2151 7 2.265090+2 5.000000-1 2.057000-2 5.590000-2 0.000000+0 0.000000+04843 2151 8 4.431000+2 5.000000-1 6.131000-2 6.160000-2 0.000000+0 0.000000+04843 2151 9 7.377380+2 5.000000-1 3.538000-1 6.740000-2 0.000000+0 0.000000+04843 2151 10 9.092200+2 5.000000-1 2.770000-1 6.870000-2 0.000000+0 0.000000+04843 2151 11 1.116124+3 5.000000-1 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