ENTRY V0006 20210414 V039V000600000001 SUBENT V0006001 20210414 V039V000600100001 BIB 9 48 V000600100002 TITLE Fast neutron cross-sections for curium-244 V000600100003 AUTHOR (H.Fernandez Gianotti) V000600100004 INSTITUTE (3ARGCNE) V000600100005 REFERENCE (J,NSE,65,164,1978) Total,capture & fission sig in fig.V000600100006 (W,FERNANDEZ GIANOTTI,19761012) V000600100007 Preprint from Fernandez Gianotti 1976/10/12. V000600100008 INDC(ARG)-9,197701 was coded, but no relevant report V000600100009 is given in this report. V000600100010 METHOD Evaluation V000600100011 ANALYSIS Calculation with the combined code ABACUS-NEARREX by V000600100012 Caner and Gitter, TNSD-R/424,(1971). This computer V000600100013 code was the developed from the V000600100014 - ABACUS-2 (Optical model code), BNL-6562 (1962), V000600100015 and the V000600100016 - NEARREX (Statistical model code), ANL-6978 (1964). V000600100017 The following set of optical parameters based on recentV000600100018 experimental results, was used, i.e. V000600100019 Vre = 42.915 - 0.833*E V000600100020 Vim = 6.204 - 0.120*E V000600100021 Vso = 7.5 MeV V000600100022 r0 = 1.32 fm V000600100023 a = 0.47 fm, b = 1.0 fm V000600100024 alpha = 0.178 for E greater than 1.0 MeV, V000600100025 and the level scheme of V000600100026 Dzepelov, Schemy Raspada Radioaktivnych Jader A = 100V000600100027 Mockba, 1963, V000600100028 was adopted. V000600100029 The statistical parameters used in calculation, were V000600100030 obtained by fitting the available experimental data V000600100031 for fission cross-section, V000600100032 for neutron energy (E) between 0.001 and 0.7 MeV, V000600100033 Q = 1 and (nuf) = 1. AND V000600100034 for neutron energy(E) between 0.75 and 3.5 MeV, V000600100035 Q = 0.75 and (nuf) = 4. V000600100036 where Q is a measure of nuclear level overlap and V000600100037 (nuf) is a degree of freedom for statistical V000600100038 fluctuation correction factor in the fission cross- V000600100039 section calculation. V000600100040 COMMENT There are quite few experimental cross-section data V000600100041 except for fission. A consistent group of calculated V000600100042 total, elastic, differential elastic, inelastic, V000600100043 radiative capture and fission neutron cross-sections V000600100044 is presented. V000600100045 STATUS (APRVD) Proof-read by Fernandez Gianotti (1977-02-15) V000600100046 HISTORY (19761122C) KO. V000600100047 (20110119A) On. REFERENCE: R,INDC(ARG)-9,197701 deletedV000600100048 (20190617U) On. REFERENCE: J,NSE,65,164,1978 added. V000600100049 (20210414A) On. Major revision in 004 and 006. V000600100050 ENDBIB 48 0 V000600100051 NOCOMMON 0 0 V000600100052 ENDSUBENT 51 0 V000600199999 SUBENT V0006002 20110119 V028V000600200001 BIB 4 11 V000600200002 REACTION (96-CM-244(N,TOT),,SIG,,,EVAL) V000600200003 COMMENT Calculation by the optical model part of the ABACUS- V000600200004 NEARREX code. V000600200005 Comparison is done with the following results by V000600200006 A.Prince, GEMP 411 (1966), V000600200007 C.L.Dunford and H.Alter, NAA-SR-12271 (1967), V000600200008 ENDF-LLL, UCRL 50400-VOL 15 (1976). V000600200009 STATUS (TABLE) Table 1 of priv.comm.by Fernandez Gianotti, V000600200010 76/10/12, Corresponding to Fig 1, ibid. V000600200011 HISTORY (19761012R) V000600200012 (20110119U) On. STATUS: TABLE added V000600200013 ENDBIB 11 0 V000600200014 NOCOMMON 0 0 V000600200015 DATA 2 60 V000600200016 EN DATA V000600200017 MEV B V000600200018 .001 16.79 V000600200019 .0015 15.74 V000600200020 .002 15.12 V000600200021 .0025 14.71 V000600200022 .003 14.42 V000600200023 .0035 14.19 V000600200024 .004 14.01 V000600200025 .0045 13.87 V000600200026 .005 13.75 V000600200027 .0055 13.65 V000600200028 .006 13.56 V000600200029 .0065 13.49 V000600200030 .007 13.42 V000600200031 .0075 13.37 V000600200032 .008 13.32 V000600200033 .0085 13.27 V000600200034 .009 13.23 V000600200035 .0095 13.19 V000600200036 .01 13.16 V000600200037 .015 12.94 V000600200038 .02 12.83 V000600200039 .025 12.70 V000600200040 .03 12.70 V000600200041 .035 12.66 V000600200042 .04 12.63 V000600200043 .045 12.60 V000600200044 .05 12.56 V000600200045 .055 12.53 V000600200046 .06 12.50 V000600200047 .065 12.46 V000600200048 .07 12.43 V000600200049 .075 12.39 V000600200050 .08 12.38 V000600200051 .085 12.35 V000600200052 .09 12.31 V000600200053 .095 12.27 V000600200054 .1 12.23 V000600200055 .15 11.80 V000600200056 .2 11.32 V000600200057 .25 10.83 V000600200058 .3 10.34 V000600200059 .35 9.98 V000600200060 .4 9.57 V000600200061 .45 9.19 V000600200062 .5 8.84 V000600200063 .55 8.52 V000600200064 .6 8.39 V000600200065 .65 7.98 V000600200066 .7 7.75 V000600200067 .75 7.55 V000600200068 .8 7.38 V000600200069 .85 7.23 V000600200070 .9 7.10 V000600200071 .95 6.98 V000600200072 1.0 6.89 V000600200073 1.5 7.90 V000600200074 2.0 7.79 V000600200075 2.5 7.86 V000600200076 3.0 8.00 V000600200077 3.5 8.06 V000600200078 ENDDATA 62 0 V000600200079 ENDSUBENT 78 0 V000600299999 SUBENT V0006003 20110119 V028V000600300001 BIB 4 12 V000600300002 REACTION (96-CM-244(N,EL)96-CM-244,,SIG,,,EVAL) V000600300003 COMMENT Calculation by the optical model part of the ABACUS- V000600300004 NEAREX code and by the statistical theory for the V000600300005 compound elastic cross-section. V000600300006 Comparison is done with the following results by V000600300007 A.Prince, GEMP 411 (1966), V000600300008 C.L.Dunford and H.Alter, NAA-SR-12271 (1967), V000600300009 ENDF-LLL, UCRL 50400-VOL 15 (1976). V000600300010 STATUS (TABLE) Table 1 of priv.comm.by Fernandez Gianotti, V000600300011 76/10/12, Corresponding to Fig 2, ibid. V000600300012 HISTORY (19761012R) V000600300013 (20110119U) On. STATUS: TABLE added V000600300014 ENDBIB 12 0 V000600300015 NOCOMMON 0 0 V000600300016 DATA 2 60 V000600300017 EN DATA V000600300018 MEV B V000600300019 .001 13.55 V000600300020 .0015 13.17 V000600300021 .002 12.91 V000600300022 .0025 12.73 V000600300023 .003 12.58 V000600300024 .0035 12.47 V000600300025 .004 12.37 V000600300026 .0045 12.29 V000600300027 .005 12.23 V000600300028 .0055 12.17 V000600300029 .006 12.13 V000600300030 .0065 12.08 V000600300031 .007 12.05 V000600300032 .0075 12.02 V000600300033 .008 11.99 V000600300034 .0085 11.97 V000600300035 .009 11.95 V000600300036 .0095 11.93 V000600300037 .01 11.91 V000600300038 .015 11.83 V000600300039 .02 11.82 V000600300040 .025 11.83 V000600300041 .03 11.84 V000600300042 .035 11.85 V000600300043 .04 11.86 V000600300044 .045 11.86 V000600300045 .05 11.82 V000600300046 .055 11.70 V000600300047 .06 11.71 V000600300048 .065 11.69 V000600300049 .07 11.58 V000600300050 .075 11.52 V000600300051 .08 11.46 V000600300052 .085 11.46 V000600300053 .09 11.34 V000600300054 .095 11.28 V000600300055 .1 11.22 V000600300056 .15 10.61 V000600300057 .2 10.03 V000600300058 .25 9.47 V000600300059 .3 8.93 V000600300060 .35 8.41 V000600300061 .4 7.93 V000600300062 .45 7.45 V000600300063 .5 7.0 V000600300064 .55 6.58 V000600300065 .6 6.18 V000600300066 .65 5.80 V000600300067 .7 5.48 V000600300068 .75 5.17 V000600300069 .8 4.91 V000600300070 .85 4.63 V000600300071 .9 4.49 V000600300072 .95 4.43 V000600300073 1.0 4.19 V000600300074 1.5 4.81 V000600300075 2.0 4.60 V000600300076 2.5 4.63 V000600300077 3.0 4.70 V000600300078 3.5 4.71 V000600300079 ENDDATA 62 0 V000600300080 ENDSUBENT 79 0 V000600399999 SUBENT V0006004 20210414 V039V000600400001 BIB 5 12 V000600400002 REACTION (96-CM-244(N,EL)96-CM-244,,DA,,,EVAL) V000600400003 ANALYSIS Calculation by the optical model part of the ABACUS- V000600400004 NEAREX code and by the statistical theory for the V000600400005 compound elastic cross-section. V000600400006 COMMENT Comparison is done with the following results by V000600400007 A.Prince, GEMP 411 (1966), V000600400008 ENDF-LLL, UCRL 50400-VOL 15 (1976). V000600400009 STATUS (TABLE) Table 3 of priv.comm.by Fernandez Gianotti, V000600400010 76/10/12, Corresponding to Figs 3-4, ibid. V000600400011 HISTORY (19761012R) V000600400012 (20110119U) On. STATUS: TABLE added V000600400013 (20210414A) On. Vector common formalism cancelled. V000600400014 ENDBIB 12 0 V000600400015 NOCOMMON 0 0 V000600400016 DATA 3 252 V000600400017 EN COS DATA V000600400018 MEV NO-DIM B/SR V000600400019 0.05 1.0 1.18 V000600400020 0.05 0.9 1.14 V000600400021 0.05 0.8 1.09 V000600400022 0.05 0.7 1.06 V000600400023 0.05 0.6 1.02 V000600400024 0.05 0.5 0.99 V000600400025 0.05 0.4 0.96 V000600400026 0.05 0.3 0.94 V000600400027 0.05 0.2 0.92 V000600400028 0.05 0.1 0.90 V000600400029 0.05 0.0 0.88 V000600400030 0.05 -0.1 0.87 V000600400031 0.05 -0.2 0.86 V000600400032 0.05 -0.3 0.86 V000600400033 0.05 -0.4 0.85 V000600400034 0.05 -0.5 0.85 V000600400035 0.05 -0.6 0.86 V000600400036 0.05 -0.7 0.86 V000600400037 0.05 -0.8 0.87 V000600400038 0.05 -0.9 0.89 V000600400039 0.05 -1.0 0.90 V000600400040 0.1 1.0 1.32 V000600400041 0.1 0.9 1.24 V000600400042 0.1 0.8 1.18 V000600400043 0.1 0.7 1.12 V000600400044 0.1 0.6 1.06 V000600400045 0.1 0.5 1.01 V000600400046 0.1 0.4 0.96 V000600400047 0.1 0.3 0.81 V000600400048 0.1 0.2 0.81 V000600400049 0.1 0.1 0.84 V000600400050 0.1 0.0 0.81 V000600400051 0.1 -0.1 0.79 V000600400052 0.1 -0.2 0.77 V000600400053 0.1 -0.3 0.75 V000600400054 0.1 -0.4 0.74 V000600400055 0.1 -0.5 0.73 V000600400056 0.1 -0.6 0.74 V000600400057 0.1 -0.7 0.73 V000600400058 0.1 -0.8 0.74 V000600400059 0.1 -0.9 0.75 V000600400060 0.1 -1.0 0.76 V000600400061 0.2 1.0 1.49 V000600400062 0.2 0.9 1.38 V000600400063 0.2 0.8 1.27 V000600400064 0.2 0.7 1.17 V000600400065 0.2 0.6 1.08 V000600400066 0.2 0.5 1.00 V000600400067 0.2 0.4 0.92 V000600400068 0.2 0.3 0.85 V000600400069 0.2 0.2 0.79 V000600400070 0.2 0.1 0.73 V000600400071 0.2 0.0 0.68 V000600400072 0.2 -0.1 0.64 V000600400073 0.2 -0.2 0.61 V000600400074 0.2 -0.3 0.58 V000600400075 0.2 -0.4 0.55 V000600400076 0.2 -0.5 0.54 V000600400077 0.2 -0.6 0.52 V000600400078 0.2 -0.7 0.52 V000600400079 0.2 -0.8 0.52 V000600400080 0.2 -0.9 0.52 V000600400081 0.2 -1.0 0.54 V000600400082 0.3 1.0 1.57 V000600400083 0.3 0.9 1.42 V000600400084 0.3 0.8 1.28 V000600400085 0.3 0.7 1.16 V000600400086 0.3 0.6 1.04 V000600400087 0.3 0.5 0.94 V000600400088 0.3 0.4 0.85 V000600400089 0.3 0.3 0.77 V000600400090 0.3 0.2 0.69 V000600400091 0.3 0.1 0.63 V000600400092 0.3 0.0 0.57 V000600400093 0.3 -0.1 0.52 V000600400094 0.3 -0.2 0.48 V000600400095 0.3 -0.3 0.45 V000600400096 0.3 -0.4 0.42 V000600400097 0.3 -0.5 0.40 V000600400098 0.3 -0.6 0.39 V000600400099 0.3 -0.7 0.38 V000600400100 0.3 -0.8 0.38 V000600400101 0.3 -0.9 0.38 V000600400102 0.3 -1.0 0.39 V000600400103 0.4 1.0 1.62 V000600400104 0.4 0.9 1.42 V000600400105 0.4 0.8 1.25 V000600400106 0.4 0.7 1.09 V000600400107 0.4 0.6 0.96 V000600400108 0.4 0.5 0.85 V000600400109 0.4 0.4 0.75 V000600400110 0.4 0.3 0.67 V000600400111 0.4 0.2 0.59 V000600400112 0.4 0.1 0.53 V000600400113 0.4 0.0 0.48 V000600400114 0.4 -0.1 0.43 V000600400115 0.4 -0.2 0.40 V000600400116 0.4 -0.3 0.36 V000600400117 0.4 -0.4 0.34 V000600400118 0.4 -0.5 0.31 V000600400119 0.4 -0.6 0.30 V000600400120 0.4 -0.7 0.29 V000600400121 0.4 -0.8 0.28 V000600400122 0.4 -0.9 0.28 V000600400123 0.4 -1.0 0.29 V000600400124 0.5 1.0 1.63 V000600400125 0.5 0.9 1.38 V000600400126 0.5 0.8 1.18 V000600400127 0.5 0.7 1.01 V000600400128 0.5 0.6 0.86 V000600400129 0.5 0.5 0.75 V000600400130 0.5 0.4 0.65 V000600400131 0.5 0.3 0.57 V000600400132 0.5 0.2 0.51 V000600400133 0.5 0.1 0.45 V000600400134 0.5 0.0 0.41 V000600400135 0.5 -0.1 0.37 V000600400136 0.5 -0.2 0.33 V000600400137 0.5 -0.3 0.30 V000600400138 0.5 -0.4 0.28 V000600400139 0.5 -0.5 0.25 V000600400140 0.5 -0.6 0.24 V000600400141 0.5 -0.7 0.22 V000600400142 0.5 -0.8 0.21 V000600400143 0.5 -0.9 0.20 V000600400144 0.5 -1.0 0.21 V000600400145 0.6 1.0 1.63 V000600400146 0.6 0.9 1.33 V000600400147 0.6 0.8 1.09 V000600400148 0.6 0.7 0.90 V000600400149 0.6 0.6 0.76 V000600400150 0.6 0.5 0.64 V000600400151 0.6 0.4 0.55 V000600400152 0.6 0.3 0.48 V000600400153 0.6 0.2 0.43 V000600400154 0.6 0.1 0.38 V000600400155 0.6 0.0 0.35 V000600400156 0.6 -0.1 0.32 V000600400157 0.6 -0.2 0.29 V000600400158 0.6 -0.3 0.26 V000600400159 0.6 -0.4 0.24 V000600400160 0.6 -0.5 0.21 V000600400161 0.6 -0.6 0.19 V000600400162 0.6 -0.7 0.17 V000600400163 0.6 -0.8 0.15 V000600400164 0.6 -0.9 0.14 V000600400165 0.6 -1.0 0.14 V000600400166 0.7 1.0 1.63 V000600400167 0.7 0.9 1.30 V000600400168 0.7 0.8 1.05 V000600400169 0.7 0.7 0.85 V000600400170 0.7 0.6 0.70 V000600400171 0.7 0.5 0.59 V000600400172 0.7 0.4 0.50 V000600400173 0.7 0.3 0.44 V000600400174 0.7 0.2 0.39 V000600400175 0.7 0.1 0.35 V000600400176 0.7 0.0 0.32 V000600400177 0.7 -0.1 0.30 V000600400178 0.7 -0.2 0.27 V000600400179 0.7 -0.3 0.25 V000600400180 0.7 -0.4 0.22 V000600400181 0.7 -0.5 0.20 V000600400182 0.7 -0.6 0.17 V000600400183 0.7 -0.7 0.15 V000600400184 0.7 -0.8 0.13 V000600400185 0.7 -0.9 0.12 V000600400186 0.7 -1.0 0.12 V000600400187 0.8 1.0 1.67 V000600400188 0.8 0.9 1.24 V000600400189 0.8 0.8 0.92 V000600400190 0.8 0.7 0.70 V000600400191 0.8 0.6 0.54 V000600400192 0.8 0.5 0.44 V000600400193 0.8 0.4 0.37 V000600400194 0.8 0.3 0.33 V000600400195 0.8 0.2 0.30 V000600400196 0.8 0.1 0.29 V000600400197 0.8 0.0 0.27 V000600400198 0.8 -0.1 0.26 V000600400199 0.8 -0.2 0.24 V000600400200 0.8 -0.3 0.22 V000600400201 0.8 -0.4 0.20 V000600400202 0.8 -0.5 0.17 V000600400203 0.8 -0.6 0.13 V000600400204 0.8 -0.7 0.10 V000600400205 0.8 -0.8 0.08 V000600400206 0.8 -0.9 0.06 V000600400207 0.8 -1.0 0.07 V000600400208 1.0 1.0 1.83 V000600400209 1.0 0.9 1.21 V000600400210 1.0 0.8 0.80 V000600400211 1.0 0.7 0.53 V000600400212 1.0 0.6 0.37 V000600400213 1.0 0.5 0.29 V000600400214 1.0 0.4 0.25 V000600400215 1.0 0.3 0.23 V000600400216 1.0 0.2 0.24 V000600400217 1.0 0.1 0.24 V000600400218 1.0 0.0 0.25 V000600400219 1.0 -0.1 0.25 V000600400220 1.0 -0.2 0.23 V000600400221 1.0 -0.3 0.21 V000600400222 1.0 -0.4 0.18 V000600400223 1.0 -0.5 0.15 V000600400224 1.0 -0.6 0.11 V000600400225 1.0 -0.7 0.07 V000600400226 1.0 -0.8 0.04 V000600400227 1.0 -0.9 0.04 V000600400228 1.0 -1.0 0.08 V000600400229 1.5 1.0 3.63 V000600400230 1.5 0.9 1.99 V000600400231 1.5 0.8 1.03 V000600400232 1.5 0.7 0.52 V000600400233 1.5 0.6 0.27 V000600400234 1.5 0.5 0.18 V000600400235 1.5 0.4 0.16 V000600400236 1.5 0.3 0.18 V000600400237 1.5 0.2 0.19 V000600400238 1.5 0.1 0.20 V000600400239 1.5 0.0 0.19 V000600400240 1.5 -0.1 0.18 V000600400241 1.5 -0.2 0.15 V000600400242 1.5 -0.3 0.12 V000600400243 1.5 -0.4 0.09 V000600400244 1.5 -0.5 0.07 V000600400245 1.5 -0.6 0.06 V000600400246 1.5 -0.7 0.06 V000600400247 1.5 -0.8 0.08 V000600400248 1.5 -0.9 0.12 V000600400249 1.5 -1.0 0.18 V000600400250 3.0 1.0 6.78 V000600400251 3.0 0.9 2.42 V000600400252 3.0 0.8 0.67 V000600400253 3.0 0.7 0.12 V000600400254 3.0 0.6 0.44 V000600400255 3.0 0.5 0.10 V000600400256 3.0 0.4 0.17 V000600400257 3.0 0.3 0.20 V000600400258 3.0 0.2 0.19 V000600400259 3.0 0.1 0.15 V000600400260 3.0 0.0 0.11 V000600400261 3.0 -0.1 0.07 V000600400262 3.0 -0.2 0.04 V000600400263 3.0 -0.3 0.02 V000600400264 3.0 -0.4 0.02 V000600400265 3.0 -0.5 0.02 V000600400266 3.0 -0.6 0.04 V000600400267 3.0 -0.7 0.05 V000600400268 3.0 -0.8 0.05 V000600400269 3.0 -0.9 0.04 V000600400270 3.0 -1.0 0.02 V000600400271 ENDDATA 254 0 V000600400272 ENDSUBENT 271 0 V000600499999 SUBENT V0006005 20110119 V028V000600500001 BIB 4 11 V000600500002 REACTION (96-CM-244(N,INL)96-CM-244,,SIG,,,EVAL) V000600500003 COMMENT Calculation by the optical model part of the ABACUS- V000600500004 NEARREX code. V000600500005 Comparison is done with the following results by V000600500006 A.Prince, GEMP 411 (1966), V000600500007 C.L.Dunford and H.Alter, NAA-SR-12271 (1967), V000600500008 ENDF-LLL, UCRL 50400-VOL 15 (1976). V000600500009 STATUS (TABLE) Table 1 of priv.comm.by Fernandez Gianotti, V000600500010 76/10/12, Corresponding to Fig 5, ibid. V000600500011 HISTORY (19761012R) V000600500012 (20110119U) On. STATUS: TABLE added V000600500013 ENDBIB 11 0 V000600500014 NOCOMMON 0 0 V000600500015 DATA 2 34 V000600500016 EN DATA V000600500017 MEV B V000600500018 .05 .08 V000600500019 .055 .15 V000600500020 .06 .23 V000600500021 .065 .29 V000600500022 .07 .35 V000600500023 .075 .40 V000600500024 .08 .46 V000600500025 .085 .51 V000600500026 .09 .55 V000600500027 .095 .59 V000600500028 .1 .62 V000600500029 .15 .87 V000600500030 .2 .99 V000600500031 .25 1.06 V000600500032 .3 1.08 V000600500033 .35 1.19 V000600500034 .4 1.21 V000600500035 .45 1.22 V000600500036 .5 1.22 V000600500037 .55 1.21 V000600500038 .6 1.19 V000600500039 .65 1.16 V000600500040 .7 .94 V000600500041 .75 .90 V000600500042 .8 .87 V000600500043 .85 .86 V000600500044 .9 .87 V000600500045 .95 .88 V000600500046 1.0 .90 V000600500047 1.5 1.27 V000600500048 2.0 1.53 V000600500049 2.5 1.73 V000600500050 3.0 1.91 V000600500051 3.5 2.07 V000600500052 ENDDATA 36 0 V000600500053 ENDSUBENT 52 0 V000600599999 SUBENT V0006006 20210414 V039V000600600001 BIB 4 8 V000600600002 REACTION (96-CM-244(N,INL)96-CM-244,PAR,SIG,,,EVAL) V000600600003 COMMENT Comparison has been made with the result by V000600600004 A.Prince, GEMP 411 (1966). V000600600005 STATUS (TABLE) Table 2 of priv.comm.by Fernandez Gianotti, V000600600006 76/10/12, Corresponding to Fig 6, ibid. V000600600007 HISTORY (19761012R) V000600600008 (20110119U) On. STATUS: TABLE added V000600600009 (20210414A) On. Vector common formalism cancelled. V000600600010 ENDBIB 8 0 V000600600011 NOCOMMON 0 0 V000600600012 DATA 3 77 V000600600013 E-LVL EN DATA V000600600014 KEV MEV B V000600600015 43. .05 .082 V000600600016 43. .055 .157 V000600600017 43. .06 .229 V000600600018 43. .065 .245 V000600600019 43. .07 .354 V000600600020 43. .075 .408 V000600600021 43. .08 .467 V000600600022 43. .085 .513 V000600600023 43. .09 .554 V000600600024 43. .095 .593 V000600600025 43. .1 .628 V000600600026 43. .15 .873 V000600600027 43. .20 .997 V000600600028 43. .25 1.060 V000600600029 43. .3 1.086 V000600600030 43. .35 1.142 V000600600031 43. .4 1.145 V000600600032 43. .45 1.124 V000600600033 43. .5 1.098 V000600600034 43. .55 1.062 V000600600035 43. .60 1.021 V000600600036 43. .65 .976 V000600600037 43. .7 .763 V000600600038 43. .75 .722 V000600600039 43. .8 .683 V000600600040 43. .85 .657 V000600600041 43. .9 .649 V000600600042 43. .95 .632 V000600600043 43. 1.0 .629 V000600600044 43. 1.5 .793 V000600600045 43. 2.0 .829 V000600600046 43. 2.5 .819 V000600600047 43. 3.0 .857 V000600600048 43. 3.5 .756 V000600600049 142. .25 .001 V000600600050 142. .3 .002 V000600600051 142. .35 .050 V000600600052 142. .4 .068 V000600600053 142. .45 .101 V000600600054 142. .5 .124 V000600600055 142. .55 .148 V000600600056 142. .60 .169 V000600600057 142. .65 .188 V000600600058 142. .7 .180 V000600600059 142. .75 .180 V000600600060 142. .8 .190 V000600600061 142. .85 .203 V000600600062 142. .9 .219 V000600600063 142. .95 .236 V000600600064 142. 1.0 .256 V000600600065 142. 1.5 .419 V000600600066 142. 2.0 .534 V000600600067 142. 2.5 .608 V000600600068 142. 3.0 .642 V000600600069 142. 3.5 .688 V000600600070 296. .65 .001 V000600600071 296. .7 .002 V000600600072 296. .75 .003 V000600600073 296. .8 .004 V000600600074 296. .85 .007 V000600600075 296. .9 .009 V000600600076 296. .95 .012 V000600600077 296. 1.0 .015 V000600600078 296. 1.5 .056 V000600600079 296. 2.0 .118 V000600600080 296. 2.5 .177 V000600600081 296. 3.0 .235 V000600600082 296. 3.5 .287 V000600600083 503. 2.0 .008 V000600600084 503. 2.5 .020 V000600600085 503. 3.0 .032 V000600600086 503. 3.5 .057 V000600600087 1042. 1.5 .005 V000600600088 1042. 2.0 .045 V000600600089 1042. 2.5 .100 V000600600090 1042. 3.0 .153 V000600600091 1042. 3.5 .287 V000600600092 ENDDATA 79 0 V000600600093 ENDSUBENT 92 0 V000600699999 SUBENT V0006007 20110119 V028V000600700001 BIB 4 17 V000600700002 REACTION (96-CM-244(N,G)96-CM-245,,SIG,,,EVAL) V000600700003 COMMENT The ABACUS-NEARREX computed the cross-sections and V000600700004 (n,gamma n') competition was neglected. V000600700005 The following parameters were used, V000600700006 radiation width = 37 milli-eV, V000600700007 mean level spacing, D = 13.7 eV, V000600700008 excitation nuclear energy, u = 5.7 MeV, V000600700009 level density parameter, a = 28.94 (1/(MeV)), V000600700010 spin density, sigma = 4. V000600700011 Comparison has been done with the following results by V000600700012 A.Prince, GEMP 411 (1966), V000600700013 C.L.Dunford and H.Alter, NAA-SR-12271 (1967), V000600700014 ENDF-LLL, UCRL 50400-VOL 15 (1976). V000600700015 STATUS (TABLE) Table 1 of priv.comm.by Fernandez Gianotti, V000600700016 76/10/12, Corresponding to Fig 7, ibid. V000600700017 HISTORY (19761012R) V000600700018 (20110119U) On. STATUS: TABLE added V000600700019 ENDBIB 17 0 V000600700020 NOCOMMON 0 0 V000600700021 DATA 2 54 V000600700022 EN DATA V000600700023 MEV B V000600700024 .001 3.07 V000600700025 .0015 2.44 V000600700026 .002 2.10 V000600700027 .0025 1.89 V000600700028 .003 1.74 V000600700029 .0035 1.64 V000600700030 .004 1.56 V000600700031 .0045 1.49 V000600700032 .005 1.44 V000600700033 .0055 1.40 V000600700034 .006 1.36 V000600700035 .0065 1.33 V000600700036 .007 1.30 V000600700037 .0075 1.28 V000600700038 .008 1.25 V000600700039 .0085 1.23 V000600700040 .009 1.21 V000600700041 .0095 1.19 V000600700042 .01 1.18 V000600700043 .015 1.04 V000600700044 .02 .95 V000600700045 .025 .87 V000600700046 .03 .81 V000600700047 .035 .76 V000600700048 .04 .71 V000600700049 .045 .67 V000600700050 .05 .61 V000600700051 .055 .56 V000600700052 .06 .52 V000600700053 .065 .48 V000600700054 .07 .45 V000600700055 .075 .43 V000600700056 .08 .42 V000600700057 .085 .40 V000600700058 .09 .38 V000600700059 .095 .36 V000600700060 .1 .35 V000600700061 .15 .27 V000600700062 .2 .23 V000600700063 .25 .22 V000600700064 .3 .20 V000600700065 .35 .21 V000600700066 .4 .21 V000600700067 .45 .20 V000600700068 .5 .20 V000600700069 .55 .20 V000600700070 .6 .19 V000600700071 .65 .19 V000600700072 .7 .16 V000600700073 .75 .15 V000600700074 .8 .15 V000600700075 .85 .16 V000600700076 .9 .17 V000600700077 .95 .19 V000600700078 ENDDATA 56 0 V000600700079 ENDSUBENT 78 0 V000600799999 SUBENT V0006008 20110119 V028V000600800001 BIB 4 23 V000600800002 REACTION (96-CM-244(N,F),,SIG,,,EVAL) V000600800003 COMMENT ABACUS-NEARREX code was used with the following V000600800004 information, V000600800005 The fission width of the Hill-Wheeler type, V000600800006 The value of the curvature of the potential barrier V000600800007 peak of 0.61 MeV and the fission threshold of 740 keV,V000600800008 and the number of the fission channels with given V000600800009 angular momentum and parity was taken from Caner and V000600800010 Yiftah, IA-1243.(FOR PU-240) V000600800011 Comparison has been made with the following results by V000600800012 A.Prince, GEMP 411 (1966), V000600800013 C.L.Dunford and H.Alter, NAA-SR-12271 (1967), V000600800014 ENDF-LLL, UCRL 50400-VOL 15 (1976), V000600800015 M.S.Moore et al.,Phys.Rev. C3(1971)1656,and Nucl.Data V000600800016 for Reactors, Helsinki 1970, Vol. 1(1970) P.527, V000600800017 (experiment) V000600800018 R.R.Fullwood et al.,2nd Conf.on Nucl.Cross-Sections V000600800019 and Techn.,Washington (1968) p.567, (experiment) V000600800020 Koontz et al, ibid (1968) p.597. (experiment) V000600800021 STATUS (TABLE) Table 1 of priv.comm.by Fernandez Gianotti, V000600800022 76/10/12, Corresponding to Fig 8, ibid. V000600800023 HISTORY (19761012R) V000600800024 (20110119U) On. STATUS: TABLE added V000600800025 ENDBIB 23 0 V000600800026 NOCOMMON 0 0 V000600800027 DATA 2 60 V000600800028 EN DATA V000600800029 MEV B V000600800030 .001 .16 V000600800031 .0015 .13 V000600800032 .002 .11 V000600800033 .0025 .10 V000600800034 .003 .09 V000600800035 .0035 .09 V000600800036 .004 .08 V000600800037 .0045 .08 V000600800038 .005 .08 V000600800039 .0055 .08 V000600800040 .006 .08 V000600800041 .0065 .08 V000600800042 .007 .08 V000600800043 .0075 .07 V000600800044 .008 .07 V000600800045 .0085 .07 V000600800046 .009 .07 V000600800047 .0095 .07 V000600800048 .01 .07 V000600800049 .015 .06 V000600800050 .02 .06 V000600800051 .025 .06 V000600800052 .03 .06 V000600800053 .035 .06 V000600800054 .04 .05 V000600800055 .045 .05 V000600800056 .05 .05 V000600800057 .055 .05 V000600800058 .06 .04 V000600800059 .065 .04 V000600800060 .07 .04 V000600800061 .075 .04 V000600800062 .08 .04 V000600800063 .085 .04 V000600800064 .09 .04 V000600800065 .095 .04 V000600800066 .1 .04 V000600800067 .15 .05 V000600800068 .2 .06 V000600800069 .25 .08 V000600800070 .3 .11 V000600800071 .35 .16 V000600800072 .4 .23 V000600800073 .45 .31 V000600800074 .5 .41 V000600800075 .55 .53 V000600800076 .6 .67 V000600800077 .65 .81 V000600800078 .7 1.17 V000600800079 .75 1.32 V000600800080 .8 1.43 V000600800081 .85 1.51 V000600800082 .9 1.56 V000600800083 .95 1.59 V000600800084 1.0 1.60 V000600800085 1.5 1.81 V000600800086 2.0 1.65 V000600800087 2.5 1.51 V000600800088 3.0 1.38 V000600800089 3.5 1.27 V000600800090 ENDDATA 62 0 V000600800091 ENDSUBENT 90 0 V000600899999 ENDENTRY 8 0 V000699999999