TAPE 134 134 0 0 0 6.214400+4 1.426800+2 1 0 0 26225 1451 1 0.000000+0 0.000000+0 0 0 0 66225 1451 2 1.000000+0 0.000000+0 0 0 10 66225 1451 3 0.000000+0 0.000000+0 0 0 124 136225 1451 4 62-SM-144 ORNL,HEDL EVAL-FEB80 R.Q. WRIGHT, F.M.MANN 6225 1451 5 DIST-APR95 REV1-OCT94 950516 6225 1451 6 ----ENDF/B-VI MATERIAL 6255 REVISION 1 6225 1451 7 -----INCIDENT NEUTRON DATA 6225 1451 8 ------ENDF-6 FORMAT 6225 1451 9 6225 1451 10 CHANGES FOR ENDF/B-VI (R. Q. WRIGHT, OCTOBER 1994) 6225 1451 11 6225 1451 12 Resolved resonance range: 6225 1451 13 6225 1451 14 The previous evaluation did not have resonance paramters. 6225 1451 15 The revised evaluation has a resolved resonance range from 6225 1451 16 0.4 to 12 keV. The resolved resonance parameters are based on 6225 1451 17 data from reference 1. The MLBW formalism is used for this 6225 1451 18 evaluation. The highest resonance included is 39.117 keV. 6225 1451 19 The principal source for the resolved resonance parameters in 6225 1451 20 this evaluation is Table II of Reference 1 which has 18 s-wave 6225 1451 21 and 56 p-wave resonances. An additional 26 s-wave resonances 6225 1451 22 and 2 p-wave resonances have been included from Table III of 6225 1451 23 Reference 1. These additional resonances are above the cutoff 6225 1451 24 and are only used to calculate the cross sections below 12 keV. 6225 1451 25 The scattering radius, R = 5.617 fm. 6225 1451 26 6225 1451 27 Unresolved resonance range: 6225 1451 28 6225 1451 29 The unresolved resonance range is 12 to 80 keV. The average 6225 1451 30 gamma-width for s-wave is 0.074 eV; D0 = 670 eV, S0 = 3.6e-4. 6225 1451 31 The average gamma-width for both p-wave and d-wave is 0.089 eV; 6225 1451 32 S1 = 1.0e-4, S2 = 2.4e-4. The scattering radius, R = 5.617 fm. 6225 1451 33 6225 1451 34 FILE 3 Changes: 6225 1451 35 6225 1451 36 FILE 3 Cross Sections are revised below 400 eV. The low energy 6225 1451 37 elastic cross section is calculated from the resolved resonance 6225 1451 38 parameters. The low energy capture is 1/V up to 400 eV with a 6225 1451 39 thermal value of 1.64 barns (Ref. 2). The elastic cross section 6225 1451 40 has been set to zero in the resolved resonance range but for the 6225 1451 41 capture a small 1/V background has been used. 6225 1451 42 6225 1451 43 Changes above 80 keV: 6225 1451 44 6225 1451 45 Total cross section above 1 MeV is based on the Sm-148 total 6225 1451 46 of Shamu et al. (Refs. 3 and 4). (N,2N) cross section is based 6225 1451 47 on measured data as shown in Ref. 4. (N,2N) was not included 6225 1451 48 in the previous evaluation but was included in the inelastic. 6225 1451 49 The inelastic above 11 MeV is revised to account for the (N,2N) 6225 1451 50 being included as a separate reaction. MT = 91 also revised to 6225 1451 51 be the same as MT = 4. Capture is based on Table IV of Ref. 1 6225 1451 52 for the energy range 80-500 keV. Extension to 20 MeV is based 6225 1451 53 on shape of Sm-154 capture. Elastic = Total - Nonelastic. 6225 1451 54 6225 1451 55 MF = 4, MT = 2 used data from Sm-152, MAT 6249 6225 1451 56 MF = 4, MT = 16 assumed to be isotropic 6225 1451 57 MF = 5, MT = 16 used data from Sm-152, MAT 6249 6225 1451 58 6225 1451 59 AVERAGE CAPTURE CROSS SECTIONS: 6225 1451 60 6225 1451 61 The average capture cross sections, flat weighting, calculated 6225 1451 62 with NJOY, using this evaluation are compared with the measured 6225 1451 63 values from reference 1 for the energy range 6 to 500 keV in 6225 1451 64 Table 1, below. 6225 1451 65 6225 1451 66 Table 1. Sm-144 Average Capture (mb) 6225 1451 67 6225 1451 68 Energy (keV) Measured Calculated 6225 1451 69 6225 1451 70 6 - 8 130 113.7 6225 1451 71 8 -10 143 134.9 6225 1451 72 10 -12 176 163.5 6225 1451 73 12 -15 185 124.2 6225 1451 74 15 -20 120 108.7 6225 1451 75 20 -30 84 91.8 6225 1451 76 30 -40 77 79.8 6225 1451 77 40 -60 73 70.3 6225 1451 78 60 -80 65 62.7 6225 1451 79 80-100 57 56.4 6225 1451 80 100-150 49.1 49.2 6225 1451 81 150-200 48.2 48.2 6225 1451 82 200-300 45.0 45.0 6225 1451 83 300-400 40.9 41.0 6225 1451 84 400-500 41.7 41.5 6225 1451 85 6225 1451 86 6225 1451 87 2200 M/S CROSS SECTIONS, BARNS 6225 1451 88 TOTAL = 2.813 BARNS 6225 1451 89 ELASTIC = 1.173 BARNS 6225 1451 90 CAPTURE = 1.640 BARNS 6225 1451 91 6225 1451 92 CAPTURE RESONANCE INTEGRAL = 1.861 BARNS 6225 1451 93 6225 1451 94 For the previous evaluation the thermal capture cross section 6225 1451 95 was 0.7 barns and the capture resonance integral 30.1 barns. 6225 1451 96 The revised values represent a change of 134 percent for the 6225 1451 97 thermal capture and -93.8 percent for the capture resonance 6225 1451 98 integral. The measured values from Ref. 2 are 1.64 +/- 0.10 6225 1451 99 barns for the thermal capture and 2.38 +/- 0.17 barns for the 6225 1451 100 capture resonance integral. 6225 1451 101 6225 1451 102 REFERENCES 6225 1451 103 6225 1451 104 1. R. L. Macklin, N. W. Hill, J. A. Harvey, and G. L. Tweed, 6225 1451 105 "Neutron capture and total cross sections of Sm-144", 6225 1451 106 Physical Review C, Volume 48, Number 3 (September 1993). 6225 1451 107 2. C. W. Alexander, J. Halperin, J. B. Knauer, R. L. Walker, 6225 1451 108 "The Thermal Neutron Capture Cross Sections and Resonance 6225 1451 109 Integrals of Sm-144 and Sm-145," Nuclear Science and Eng. 6225 1451 110 95, 194-199 (1987). 6225 1451 111 3. R. E. Shamu et al. "Effects of deformation on Neutron 6225 1451 112 Total Cross Sections of Even-A Nd and Sm Isotopes," PR/C 6225 1451 113 22, 1857 (November 1980). 6225 1451 114 4. V. McLane, C. L. Dunford, and P. F. Rose, Neutron Cross 6225 1451 115 Sections, Vol. 2, Academic Press, New York (1988). 6225 1451 116 6225 1451 117 *********** ENDF/B-V COMMENTS FOLLOW: 6225 1451 118 6225 1451 119 ENDF/B-V MATERIAL CONVERTED TO ENDF-6 FORMAT BY NNDC 6225 1451 120 * * * * * * *6225 1451 121 MF=2, MT=251 SCATTERING RADIUS ONLY 6225 1451 122 MF=3 CROSS SECTIONS ARE FROM HAUSER-FESHBACH CALCULATIONS 6225 1451 123 USING THE MOLDAUER POTENTIAL 6225 1451 124 LOW ENERGY DATA DETERMINED FROM THERMAL CROSS SECTION 6225 1451 125 USING A 1.0/V TAIL 6225 1451 126 MF=4 ISOTROPIC ANGULAR DISTRIBUTIONS 6225 1451 127 MF=5 EVAPORATION TEMPERATURES FROM 3.2*SQRT(E/AWR) 6225 1451 128 1 451 141 16225 1451 129 2 151 173 16225 1451 130 3 1 34 16225 1451 131 3 2 34 16225 1451 132 3 4 17 16225 1451 133 3 16 10 16225 1451 134 3 91 17 16225 1451 135 3 102 34 16225 1451 136 4 2 51 16225 1451 137 4 16 2 16225 1451 138 4 91 2 06225 1451 139 5 16 9 06225 1451 140 5 91 8 06225 1451 141 0.000000+0 0.000000+0 0 0 0 06225 1 0 142 0.000000+0 0.000000+0 0 0 0 06225 0 0 143 6.214400+4 1.426800+2 0 0 1 06225 2151 144 6.214400+4 1.000000+0 0 0 2 06225 2151 145 4.000000+2 1.200000+4 1 2 0 06225 2151 146 0.000000+0 5.617000-1 0 0 2 06225 2151 147 1.426800+2 0.000000+0 0 0 264 446225 2151 148 1.6219E+03 5.0000E-01 8.8990E-01 8.2400E-01 6.5900E-02 0.0000E+006225 2151 149 1.6930E+03 5.0000E-01 6.7558E+00 6.6930E+00 6.2800E-02 0.0000E+006225 2151 150 2.5846E+03 5.0000E-01 6.5693E+00 6.5100E+00 5.9300E-02 0.0000E+006225 2151 151 3.0431E+03 5.0000E-01 1.1464E+01 1.1360E+01 1.0430E-01 0.0000E+006225 2151 152 4.0420E+03 5.0000E-01 1.4443E+01 1.4370E+01 7.2600E-02 0.0000E+006225 2151 153 4.4873E+03 5.0000E-01 2.7436E+00 2.6800E+00 6.3600E-02 0.0000E+006225 2151 154 4.6391E+03 5.0000E-01 7.8571E+01 7.8450E+01 1.2100E-01 0.0000E+006225 2151 155 5.5674E+03 5.0000E-01 9.2990E+00 9.2500E+00 4.9000E-02 0.0000E+006225 2151 156 6.1607E+03 5.0000E-01 7.5740E-01 7.0000E-01 5.7400E-02 0.0000E+006225 2151 157 7.4832E+03 5.0000E-01 4.7100E-01 4.0000E-01 7.1000E-02 0.0000E+006225 2151 158 8.0859E+03 5.0000E-01 2.9999E+01 2.9920E+01 7.9000E-02 0.0000E+006225 2151 159 8.8917E+03 5.0000E-01 5.0489E+01 5.0400E+01 8.9000E-02 0.0000E+006225 2151 160 9.8872E+03 5.0000E-01 4.1300E-01 3.1000E-01 1.0300E-01 0.0000E+006225 2151 161 1.0386E+04 5.0000E-01 3.2183E+01 3.2100E+01 8.3000E-02 0.0000E+006225 2151 162 1.0905E+04 5.0000E-01 1.0160E+00 9.4000E-01 7.6000E-02 0.0000E+006225 2151 163 1.1280E+04 5.0000E-01 1.8350E+00 1.7000E+00 1.3500E-01 0.0000E+006225 2151 164 1.1503E+04 5.0000E-01 1.3686E+02 1.3680E+02 6.4000E-02 0.0000E+006225 2151 165 1.1917E+04 5.0000E-01 3.1320E+00 3.0700E+00 6.2000E-02 0.0000E+006225 2151 166 1.3574E+04 5.0000E-01 1.8874E+01 1.8800E+01 7.4000E-02 0.0000E+006225 2151 167 1.4055E+04 5.0000E-01 2.0974E+01 2.0900E+01 7.4000E-02 0.0000E+006225 2151 168 1.4818E+04 5.0000E-01 1.5017E+02 1.5010E+02 7.4000E-02 0.0000E+006225 2151 169 1.5336E+04 5.0000E-01 1.8074E+01 1.8000E+01 7.4000E-02 0.0000E+006225 2151 170 1.6704E+04 5.0000E-01 3.7474E+01 3.7400E+01 7.4000E-02 0.0000E+006225 2151 171 1.7059E+04 5.0000E-01 1.4074E+01 1.4000E+01 7.4000E-02 0.0000E+006225 2151 172 1.8065E+04 5.0000E-01 2.2674E+01 2.2600E+01 7.4000E-02 0.0000E+006225 2151 173 1.8763E+04 5.0000E-01 1.6740E+00 1.6000E+00 7.4000E-02 0.0000E+006225 2151 174 1.8881E+04 5.0000E-01 4.6740E+00 4.6000E+00 7.4000E-02 0.0000E+006225 2151 175 1.9507E+04 5.0000E-01 1.2457E+02 1.2450E+02 7.4000E-02 0.0000E+006225 2151 176 1.9901E+04 5.0000E-01 6.0740E+00 6.0000E+00 7.4000E-02 0.0000E+006225 2151 177 2.0803E+04 5.0000E-01 2.1740E+00 2.1000E+00 7.4000E-02 0.0000E+006225 2151 178 2.1597E+04 5.0000E-01 1.5740E+00 1.5000E+00 7.4000E-02 0.0000E+006225 2151 179 2.2058E+04 5.0000E-01 2.6740E+00 2.6000E+00 7.4000E-02 0.0000E+006225 2151 180 2.2647E+04 5.0000E-01 2.5374E+01 2.5300E+01 7.4000E-02 0.0000E+006225 2151 181 2.3003E+04 5.0000E-01 3.1874E+01 3.1800E+01 7.4000E-02 0.0000E+006225 2151 182 2.3550E+04 5.0000E-01 2.2274E+01 2.2200E+01 7.4000E-02 0.0000E+006225 2151 183 2.4494E+04 5.0000E-01 1.0717E+02 1.0710E+02 7.4000E-02 0.0000E+006225 2151 184 2.5327E+04 5.0000E-01 1.3174E+01 1.3100E+01 7.4000E-02 0.0000E+006225 2151 185 2.9068E+04 5.0000E-01 3.0274E+01 3.0200E+01 7.4000E-02 0.0000E+006225 2151 186 2.9716E+04 5.0000E-01 1.0767E+02 1.0760E+02 7.4000E-02 0.0000E+006225 2151 187 3.1280E+04 5.0000E-01 5.3074E+01 5.3000E+01 7.4000E-02 0.0000E+006225 2151 188 3.4378E+04 5.0000E-01 1.9574E+01 1.9500E+01 7.4000E-02 0.0000E+006225 2151 189 3.4914E+04 5.0000E-01 2.0274E+01 2.0200E+01 7.4000E-02 0.0000E+006225 2151 190 3.8410E+04 5.0000E-01 1.3074E+01 1.3000E+01 7.4000E-02 0.0000E+006225 2151 191 3.9117E+04 5.0000E-01 4.8374E+01 4.8300E+01 7.4000E-02 0.0000E+006225 2151 192 1.426800+2 0.000000+0 1 0 348 586225 2151 193 7.510000+2 5.000000-1 8.380000-2 3.800000-3 8.000000-2 0.000000+06225 2151 194 1.023000+3 5.000000-1 1.120000-1 1.800000-2 9.400000-2 0.000000+06225 2151 195 1.186900+3 5.000000-1 1.300000-1 8.000000-2 5.000000-2 0.000000+06225 2151 196 1.262500+3 5.000000-1 9.290000-2 3.900000-3 8.900000-2 0.000000+06225 2151 197 1.602500+3 5.000000-1 1.163000-1 1.330000-2 1.030000-1 0.000000+06225 2151 198 1.895100+3 5.000000-1 8.800000-2 1.400000-2 7.400000-2 0.000000+06225 2151 199 1.982300+3 5.000000-1 1.706000-1 1.060000-1 6.460000-2 0.000000+06225 2151 200 2.071100+3 5.000000-1 8.800000-2 8.000000-3 8.000000-2 0.000000+06225 2151 201 2.279100+3 5.000000-1 1.750000-1 5.200000-2 1.230000-1 0.000000+06225 2151 202 2.824700+3 5.000000-1 1.600000-1 3.600000-2 1.240000-1 0.000000+06225 2151 203 3.154200+3 5.000000-1 1.020000-1 1.600000-2 8.600000-2 0.000000+06225 2151 204 3.411800+3 5.000000-1 1.150000-1 2.600000-2 8.900000-2 0.000000+06225 2151 205 3.777000+3 5.000000-1 1.051000-1 8.100000-3 9.700000-2 0.000000+06225 2151 206 3.875700+3 5.000000-1 9.400000-2 5.000000-3 8.900000-2 0.000000+06225 2151 207 3.881300+3 5.000000-1 9.730000-2 8.300000-3 8.900000-2 0.000000+06225 2151 208 4.295200+3 5.000000-1 1.360000-1 4.800000-2 8.800000-2 0.000000+06225 2151 209 4.480700+3 5.000000-1 9.640000-2 7.400000-3 8.900000-2 0.000000+06225 2151 210 4.534100+3 5.000000-1 1.094000-1 1.540000-2 9.400000-2 0.000000+06225 2151 211 4.744300+3 5.000000-1 1.070000-1 4.500000-2 6.200000-2 0.000000+06225 2151 212 4.902600+3 5.000000-1 2.200000-1 1.440000-1 7.600000-2 0.000000+06225 2151 213 5.193600+3 5.000000-1 1.875000-1 9.000000-2 9.750000-2 0.000000+06225 2151 214 5.820000+3 5.000000-1 3.402000-1 2.220000-1 1.182000-1 0.000000+06225 2151 215 5.984700+3 5.000000-1 1.420000-1 5.300000-2 8.900000-2 0.000000+06225 2151 216 6.062100+3 5.000000-1 9.900000-2 1.000000-2 8.900000-2 0.000000+06225 2151 217 6.394400+3 5.000000-1 1.150000-1 2.500000-2 9.000000-2 0.000000+06225 2151 218 6.549600+3 5.000000-1 2.870000-1 1.870000-1 1.000000-1 0.000000+06225 2151 219 6.904800+3 5.000000-1 4.290000-1 3.100000-1 1.190000-1 0.000000+06225 2151 220 7.145800+3 5.000000-1 1.020000-1 4.200000-2 6.000000-2 0.000000+06225 2151 221 7.313500+3 5.000000-1 1.590000-1 7.000000-2 8.900000-2 0.000000+06225 2151 222 7.326300+3 5.000000-1 1.445000-1 5.600000-2 8.850000-2 0.000000+06225 2151 223 7.722400+3 5.000000-1 1.240000-1 3.500000-2 8.900000-2 0.000000+06225 2151 224 7.759400+3 5.000000-1 9.830000-2 9.300000-3 8.900000-2 0.000000+06225 2151 225 7.848500+3 5.000000-1 9.660000-2 7.600000-3 8.900000-2 0.000000+06225 2151 226 8.009700+3 5.000000-1 1.940000-1 1.400000-1 5.400000-2 0.000000+06225 2151 227 8.266300+3 5.000000-1 9.650000-2 7.500000-3 8.900000-2 0.000000+06225 2151 228 8.304600+3 5.000000-1 8.730000-2 7.300000-3 8.000000-2 0.000000+06225 2151 229 8.441800+3 5.000000-1 9.460000-2 5.600000-3 8.900000-2 0.000000+06225 2151 230 8.495600+3 1.500000+0 2.070000-1 1.250000-1 8.200000-2 0.000000+06225 2151 231 8.590000+3 5.000000-1 2.170000-1 1.300000-1 8.700000-2 0.000000+06225 2151 232 8.729700+3 5.000000-1 9.800000-2 9.000000-3 8.900000-2 0.000000+06225 2151 233 9.036000+3 5.000000-1 9.510000-2 6.100000-3 8.900000-2 0.000000+06225 2151 234 9.598000+3 5.000000-1 1.550000-1 6.700000-2 8.800000-2 0.000000+06225 2151 235 9.812100+3 5.000000-1 2.900000-1 2.000000-1 9.000000-2 0.000000+06225 2151 236 1.015300+4 1.500000+0 1.490000-1 6.100000-2 8.800000-2 0.000000+06225 2151 237 1.020800+4 5.000000-1 1.052000-1 1.520000-2 9.000000-2 0.000000+06225 2151 238 1.030900+4 5.000000-1 4.210000-1 3.500000-1 7.100000-2 0.000000+06225 2151 239 1.051200+4 5.000000-1 2.170000-1 1.300000-1 8.700000-2 0.000000+06225 2151 240 1.056500+4 5.000000-1 1.130000-1 2.400000-2 8.900000-2 0.000000+06225 2151 241 1.064600+4 5.000000-1 1.052000-1 1.520000-2 9.000000-2 0.000000+06225 2151 242 1.069600+4 5.000000-1 1.025000-1 1.250000-2 9.000000-2 0.000000+06225 2151 243 1.079200+4 5.000000-1 1.690000-1 8.000000-2 8.900000-2 0.000000+06225 2151 244 1.133300+4 5.000000-1 1.025000-1 1.250000-2 9.000000-2 0.000000+06225 2151 245 1.141300+4 5.000000-1 1.095000-1 1.950000-2 9.000000-2 0.000000+06225 2151 246 1.159100+4 5.000000-1 1.530000-1 6.400000-2 8.900000-2 0.000000+06225 2151 247 1.173500+4 5.000000-1 1.470000-1 5.800000-2 8.900000-2 0.000000+06225 2151 248 1.180800+4 1.500000+0 1.520000-1 6.100000-2 9.100000-2 0.000000+06225 2151 249 1.301700+4 1.500000+0 4.240000-1 3.350000-1 8.900000-2 0.000000+06225 2151 250 1.429200+4 1.500000+0 2.790000-1 1.900000-1 8.900000-2 0.000000+06225 2151 251 1.200000+4 8.000000+4 2 2 0 06225 2151 252 0.000000+0 5.617000-1 0 0 3 06225 2151 253 1.426800+2 0.000000+0 0 0 1 06225 2151 254 5.000000-1 0.000000+0 2 0 66 106225 2151 255 0.000000+0 0.000000+0 0.000000+0 1.000000+0 0.000000+0 0.000000+06225 2151 256 1.200000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 257 1.600000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 258 2.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 259 2.500000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 260 3.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 261 4.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 262 5.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 263 6.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 264 7.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 265 8.000000+4 6.700000+2 0.000000+0 2.412000-1 7.400000-2 0.000000+06225 2151 266 1.426800+2 0.000000+0 1 0 2 06225 2151 267 5.000000-1 0.000000+0 2 0 66 106225 2151 268 0.000000+0 0.000000+0 0.000000+0 1.000000+0 0.000000+0 0.000000+06225 2151 269 1.200000+4 6.700000+2 0.000000+0 6.700000-2 8.900000-2 0.000000+06225 2151 270 1.600000+4 6.700000+2 0.000000+0 6.700000-2 8.900000-2 0.000000+06225 2151 271 2.000000+4 6.700000+2 0.000000+0 6.700000-2 8.900000-2 0.000000+06225 2151 272 2.500000+4 6.700000+2 0.000000+0 6.700000-2 8.900000-2 0.000000+06225 2151 273 3.000000+4 6.700000+2 0.000000+0 6.700000-2 8.900000-2 0.000000+06225 2151 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