JEFF-3.0 file header. Release April 2002 6.315400+4 1.526000+2 1 0 2 06334 1451 1 0.000000+0 1.000000+0 0 0 0 66334 1451 2 1.000000+0 2.000000+7 7 0 10 306334 1451 3 0.000000+0 0.000000+0 0 0 218 376334 1451 4 63-EU-154 ORNL,BNL EVAL-MAY89 R.Q.WRIGHT, H.TAKAHASHI 6334 1451 5 DIST-APR02 6334 1451 6 ----JEFF-30 MATERIAL 6334 6334 1451 7 -----INCIDENT NEUTRON DATA 6334 1451 8 ------ENDF-6 FORMAT 6334 1451 9 6334 1451 10 ***************************** JEFF-3.0 ***********************6334 1451 11 6334 1451 12 DATA TAKEN FROM :- ENDF/B-VI rel.7 (DIST-APR00) 6334 1451 13 6334 1451 14 ******************************************************************6334 1451 15 6334 1451 16 6334 1451 17 ENDF/B-VI MOD 2 Revision, March 1998, R.Q. Wright (ORNL) 6334 1451 18 6334 1451 19 MF=2 RESONANCE PARAMETERS (Revised) 6334 1451 20 A negative level at -0.71 eV is added and the parameters for 6334 1451 21 the first positive resonance at 0.19 eV are revised. The 6334 1451 22 parameters for this resonance are now very nearly the same as 6334 1451 23 those of Anufriev [27]. 6334 1451 24 The revised thermal cross sections are as follows: 6334 1451 25 6334 1451 26 2200 m/sec cross sections (barns) 6334 1451 27 total 1853.14 6334 1451 28 elastic 6.65 6334 1451 29 capture 1846.49 6334 1451 30 Capture resonance integral = 1357 barns 6334 1451 31 6334 1451 32 The thermal capture cross section in the revised evaluation is 6334 1451 33 in good agreement with the measured value of Sekine [28], 6334 1451 34 1840 +/- 90 barns. 6334 1451 35 6334 1451 36 *****************************************************************6334 1451 37 6334 1451 38 ENDF/B-VI MOD 1 Evaluation, May 1989, R.Q. Wright (ORNL) 6334 1451 39 ENDF/B-V material converted to ENDF-6 format by NNDC 6334 1451 40 6334 1451 41 The ENDF/B-V evaluation, MAT 1293, has been revised below 6334 1451 42 10 keV. 6334 1451 43 6334 1451 44 MF= 2 RESONANCE PARAMETERS 6334 1451 45 RESOLVED RESONANCE PARAMETERS, are revised, taken from 6334 1451 46 Mughabghab [26] and are used to delfine the total, elastic, 6334 1451 47 and capture cross sections for energies between 0.00001 and 6334 1451 48 27.8 eV. A MLBW formalism is used. The original resonance 6334 1451 49 parameters in the energy range 27.8 to 63.0 eV are modified 6334 1451 50 as follows. 6334 1451 51 E0 same as ENDF/B-V (MAT 1293) 6334 1451 52 GN = GN/(2.0*G) (to keep same value of 2G*GN) 6334 1451 53 GG = GG*1.3125 (to get average width= 0.126) 6334 1451 54 GT = GN+GG 6334 1451 55 6334 1451 56 Average reduced neutron width = 4.44540E-04 6334 1451 57 Average gamma width = 1.25926E-01 6334 1451 58 Strength function = 2.19309E-04 6334 1451 59 6334 1451 60 UNRESOLVED RESONANCE RANGE, UPPER LIMIT IS 10 KEV 6334 1451 61 The unresolved resonance parameters are based on the data 6334 1451 62 of Mughabghab [26]. 6334 1451 63 Average gamma width = 0.1260 EV 6334 1451 64 D0 (Maughabghab 0.92 EV) = 0.9752 EV 6334 1451 65 S0 (not given in Mughabghab) = 2.5709E-04 6334 1451 66 6334 1451 67 MF= 3 SMOOTH CROSS SECTIONS 6334 1451 68 Elastic and capture backgrounds are zero below 10 keV. 6334 1451 69 MT= 1 Total cross section was revised by small amounts at 21 6334 1451 70 points between 8.7 and 11.8 MeV to agree with the sum of the 6334 1451 71 partial cross sections. 6334 1451 72 MT= 2 Elastic cross section at 10 keV was reduced to 13.8 6334 1451 73 barns. 6334 1451 74 MT=102 Capture cross section at 30 keV is 2920 mb (unchanged). 6334 1451 75 6334 1451 76 **************************************************************** 6334 1451 77 6334 1451 78 ENDF/B-V MAT 1293 Translation, December 1978, F. Mann and 6334 1451 79 R. Schenter (HEDL) 6334 1451 80 6334 1451 81 **************************************************************** 6334 1451 82 6334 1451 83 ENDF/B-IV MAT Evaluation, December 1973, H. Takahashi (BNL) 6334 1451 84 6334 1451 85 Almost no experimental data are available for 154Eu, so the 6334 1451 86 evaluations was mostly carried out by nuclear model calculations.6334 1451 87 6334 1451 88 MT= 2 RESONANCE PARAMETERS 6334 1451 89 Replaced in ENDF/B-VI. 6334 1451 90 6334 1451 91 MT= 3 SMOOTH CROSS SECTIONS 6334 1451 92 MT= 1 Total cross section 6334 1451 93 Between 10 keV and 2.5 MeV, the total cross sections were 6334 1451 94 calculated using ABACUS-2 [6] Optical Model code. The 6334 1451 95 Optical Model parameters used in the calculation will be 6334 1451 96 shown in a later section. Above 2.5 MeV, the total cross 6334 1451 97 sections were assumed to be the same as the experimental 6334 1451 98 values of natural europium measured by Foster [7]. 6334 1451 99 MT= 2 Elastic scattering cross sections 6334 1451 100 The elastic scattering cross sections in the energy higher 6334 1451 101 than the unresolved resonance energy were obtained by 6334 1451 102 substructing the non elastic cross section from the evaluated 6334 1451 103 total cross section. 6334 1451 104 MT= 3 Nonelastic scattering cross section 6334 1451 105 The nonelastic scattering cross section was calculated by 6334 1451 106 summing up all cross sections except the elastic scattering 6334 1451 107 cross section. 6334 1451 108 MT= 4,51,52...,91 Inelastic scattering cross sections 6334 1451 109 The inelastic scattering cross sections are given as total 6334 1451 110 (MT=4), discrete level excitation cross section (MT=51...) for6334 1451 111 the first 5 levels and continuum level excitation cross 6334 1451 112 section (MT=91). The level scheme for these discrete level is 6334 1451 113 taken from Refs. [9,10,11,12,13]. 6334 1451 114 Since no experimental data are available for the individual 6334 1451 115 level excitation cross sections, they were calculated using 6334 1451 116 COMNUC-3 [14] for energies up to 3 MeV. Above 3 MeV, 6334 1451 117 inelastic scattering is mostly the excitation of the 6334 1451 118 continuum of levels, so that the inelastic scattering cross 6334 1451 119 section for discrete level excitation above this energy was 6334 1451 120 neglected and the inelastic scattering cross section for 6334 1451 121 continuum level excitation was calculated by the Cascade 6334 1451 122 calculation using GROGI-3 [15]. The level density parameters 6334 1451 123 for the continuum of levels were taken from Cook's data [17] 6334 1451 124 for the deformed nuclei using the Gilbert-Cameron formula [18]6334 1451 125 MT= 16,17 (n,2n), (n,3n) cross sections 6334 1451 126 These cross sections were calculated by using GROGI-3. The 6334 1451 127 Optical Model parameters described in the later section were 6334 1451 128 used. 6334 1451 129 MT=102 Radiative capture cross section 6334 1451 130 The radiative capture cross sections at low energy range were 6334 1451 131 calculated from the File 2 resonance parameters and are given 6334 1451 132 as smooth cross sections. The cross sections between 100 eV 6334 1451 133 and 10 keV are presented as unresolved resonance parameters. 6334 1451 134 For energy higher than 10 keV, the cross sections were 6334 1451 135 calculated using COMNUC-3. The calculation was done similarly6334 1451 136 to the ones for Eu151 and Eu153 [7], that is, Moldauer's 6334 1451 137 Q value was assumed to be zero, and the correlation correction6334 1451 138 factor due to the degrees of freedom associated with open 6334 1451 139 channels was taken into account. From 3 MeV to 20 MeV, the 6334 1451 140 capture cross section was obtained by GROGI-3 for the compound6334 1451 141 process, by Cvelbar's formula [21] based on Lane-Lynn [22] 6334 1451 142 and Brown's [23] formula for the direct and semi-direct 6334 1451 143 reaction. 6334 1451 144 MT=103,28 (n,p) and (n,n',p) cross sections 6334 1451 145 No experimental values were available, so that we calculated 6334 1451 146 these by nuclear model codes. For (n,p) reaction, the semi- 6334 1451 147 empirical Statistical Model code THRESH [20] was used. But 6334 1451 148 the evaluation [7] of Eu151 and Eu153 indicated that the 6334 1451 149 cross sections around 14 MeV calculated by this code were 6334 1451 150 small compared to the experimental values. thus, the 6334 1451 151 calculated cross sections were normalized by the factors 6334 1451 152 obtained for Eu151. The (n,n'p) cross sections were 6334 1451 153 calculated using GROGI-3. 6334 1451 154 MT=104,105,107 (n,d), (n,t), (n,He3) reaction cross sections 6334 1451 155 The cross sections calculated by THRESH were adopted. 6334 1451 156 MT=107,22 (n,alpha) and (n,n'd) cross sections 6334 1451 157 These cross sections were obtained in a similar manner to the 6334 1451 158 (n,p) and (n,n'p) reactions. 6334 1451 159 6334 1451 160 MT= 4 ANGULAR DISTRIBUTION OF SECONDARY NEUTRONS 6334 1451 161 MT= 2 Elastic scattering 6334 1451 162 Calculated by ABACUS-2 (NABAK PDP-10 version) [6]. The 6334 1451 163 Legendre coefficients calculated by CHAD (NUCHAD in PDP-10 6334 1451 164 version) [24] were given. Since the elastic scattering due 6334 1451 165 to the nuclear compound process is small in the energy range 6334 1451 166 above 3 MeV, the elastic angular distribution of was 6334 1451 167 calculated by taking only the shape elastic scattering into 6334 1451 168 account above 3 MeV. 6334 1451 169 MT= 51,...,91,16,17,22,23 Inelastic scattering,(n,2n),(n,3n), 6334 1451 170 (n,n'p), and (n,n'alpha) 6334 1451 171 Assumed to be isotropic in the center-of-mass system. 6334 1451 172 6334 1451 173 MT= 5 ENERGY DISTRIBUTION OF SECONDARY NEUTRONS 6334 1451 174 MT= 16,16,91 (n,2n),(n,3n),(n,n') 6334 1451 175 Energy distributions of neutron were assumed to be 6334 1451 176 Maxwellian. The effective temperatures were obtained by the 6334 1451 177 Weiskopf formula [25]. 6334 1451 178 6334 1451 179 **************************************************************** 6334 1451 180 6334 1451 181 REFERENCES 6334 1451 182 1. J.L. Cook, report AAEC/TM-549 (1969) 6334 1451 183 2. D.W. Barr and J.H. Devaney, report LA-3643 (1967) 6334 1451 184 3. R.J. Hayden et. al., Phys.Rev. 75, 1500 (1949) 6334 1451 185 4. W.H. Walker, Chalk River report AECL-3037, Part I (1969) 6334 1451 186 5. S.F. Mughabghab and D. Garber, report BNL-325, 3rd Ed., 6334 1451 187 Vol.1 (1973) 6334 1451 188 6. E.H. Auerbach, report BNL-6562 (1962) 6334 1451 189 7. H. Takahashi, report BNL-19455 (1974) [ENDF-213] 6334 1451 190 8. D.G. Foster Jr. and D.W. Glasgow, Phys.Rev.C 3, 576 (1971) 6334 1451 191 9. T. Lewis and R. Graetzer, Nucl.Phys. A162, 145 (1971) 6334 1451 192 10. A. Faessler and H.G. Wahsweiler, Nucl.Phys. 59, 202 (1964) 6334 1451 193 11. L.V. Groshev et al., Nucl.Data Table A5, 1 (1968) 6334 1451 194 12. D.J. Horen et al., "Nuclear Level Scheme A=45 through A=257,"6334 1451 195 to be published in Nucl.Data Tables 6334 1451 196 13. C. Lederer, J. Hollander and I. Perlman, Table of Isotopes, 6334 1451 197 6th Ed. (1967) 6334 1451 198 14. C. Dunford, report AI-AEC-12931 (1970) and private 6334 1451 199 communication (COMNUC-3 code) (1971) 6334 1451 200 15. H. Takahashi, GROGI-III, modified from GROGI-2. (1 7) 6334 1451 201 16. J. Gilat, report BNL-50246 (1970) 6334 1451 202 17. J.L. Cook, H. Ferguson and A.R. de L. Musgrove, report 6334 1451 203 AAEC/TM-392 (1967) 6334 1451 204 18. A. Gilbert and A.G.W. Cameron, Can.J.Phys. 43, 1446 (1965) 6334 1451 205 19. T. Tamura, Rev.Mod.Phys. 37, 679 (1965) 6334 1451 206 20. S. Pearlstein, J.Nucl.En. 27, 81 (1973) 6334 1451 207 21. F. Cvelbar et al., NIJS report T-529 (1968) 6334 1451 208 22. A.M. Lane and J.E. Lynn, Peaceful Uses of Atomic Energy, 6334 1451 209 Proc. Conf., Geneva, 1958, Vol.15 (United Nations, 1958) p.386334 1451 210 23. G.E. Brown, Nucl.Phys. 57, 339 (1964) 6334 1451 211 24. R.F. Berland, Atomics Int. report NAA-SR-11231 (1965) 6334 1451 212 25. A. Weinberg and E. Wigner, The Physical Theory of Reactors 6334 1451 213 (U. of Chicago Press, 1959) 6334 1451 214 26. S.F. Mughabghab, Neutron Cross Sections, Vol. 1, Part B, 6334 1451 215 Z=61-100 (Academic Press 1984) 6334 1451 216 27. V.A. Anufriev et al., Sov.At.En. 46, 182 (1979); translated 6334 1451 217 from At.En. 46, 158 (1979). [Data from EXFOR40484] 6334 1451 218 28. T. Sekine, S. Ichikawa and S. Baba, Appl.Rad.Isotopes 38, 6334 1451 219 513 (1987) 6334 1451 220 6334 1451 221 ************************ C O N T E N T S *********************** 6334 1451 222 1 451 259 06334 1451 223 2 151 75 06334 1451 224 3 1 56 06334 1451 225 3 2 35 06334 1451 226 3 4 24 06334 1451 227 3 16 9 06334 1451 228 3 17 5 06334 1451 229 3 22 7 06334 1451 230 3 28 7 06334 1451 231 3 51 17 06334 1451 232 3 52 15 06334 1451 233 3 53 14 06334 1451 234 3 54 13 06334 1451 235 3 55 11 06334 1451 236 3 91 16 06334 1451 237 3 102 26 16334 1451 238 3 103 16 06334 1451 239 3 104 12 06334 1451 240 3 105 11 06334 1451 241 3 106 5 06334 1451 242 3 107 15 06334 1451 243 4 2 271 06334 1451 244 4 16 10 06334 1451 245 4 17 10 06334 1451 246 4 22 10 06334 1451 247 4 28 10 06334 1451 248 4 51 10 06334 1451 249 4 52 10 06334 1451 250 4 53 10 06334 1451 251 4 54 10 06334 1451 252 4 55 10 06334 1451 253 4 91 10 06334 1451 254 5 16 7 06334 1451 255 5 17 7 06334 1451 256 5 22 7 06334 1451 257 5 28 7 06334 1451 258 5 91 7 06334 1451 259 0.000000+0 0.000000+0 0 0 0 06334 1 099999 0.000000+0 0.000000+0 0 0 0 06334 0 0 0 6.315400+4 1.526000+2 0 0 1 06334 2151 1 6.315400+4 1.000000+0 0 0 2 06334 2151 2 1.000000-5 6.300000+1 1 2 0 06334 2151 3 3.000000+0 8.800000-1 0 0 1 06334 2151 4 1.526000+2 0.000000+0 0 0 360 606334 2151 5 -7.100000-1 2.500000+0 1.264160-1 4.160000-4 1.260000-1 0.000000+06334 2151 6 1.900000-1 3.500000+0 1.600595-1 5.950000-5 1.600000-1 0.000000+06334 2151 7 8.570000-1 2.500000+0 1.260560-1 5.600000-5 1.260000-1 0.000000+06334 2151 8 1.368000+0 3.500000+0 1.353456-1 3.456250-4 1.350000-1 0.000000+06334 2151 9 3.510000+0 3.500000+0 1.151663-1 1.662500-4 1.150000-1 0.000000+06334 2151 10 4.140000+0 2.500000+0 1.296417-1 6.416666-4 1.290000-1 0.000000+06334 2151 11 5.200000+0 3.500000+0 1.403587-1 3.587500-4 1.400000-1 0.000000+06334 2151 12 5.620000+0 2.500000+0 1.273033-1 3.033333-4 1.270000-1 0.000000+06334 2151 13 6.650000+0 3.500000+0 1.260228-1 2.275000-5 1.260000-1 0.000000+06334 2151 14 6.820000+0 3.500000+0 1.520500-1 1.050000-3 1.510000-1 0.000000+06334 2151 15 9.320000+0 2.500000+0 1.081500-1 3.150000-3 1.050000-1 0.000000+06334 2151 16 9.480000+0 3.500000+0 1.125750-1 1.575000-3 1.110000-1 0.000000+06334 2151 17 1.070000+1 3.500000+0 1.083413-1 3.412500-4 1.080000-1 0.000000+06334 2151 18 1.095000+1 2.500000+0 1.146533-1 6.533334-4 1.140000-1 0.000000+06334 2151 19 1.254000+1 3.500000+0 1.748662-1 8.662500-4 1.740000-1 0.000000+06334 2151 20 1.368000+1 2.500000+0 1.167350-1 7.350000-4 1.160000-1 0.000000+06334 2151 21 1.597000+1 3.500000+0 1.003325-1 3.325000-4 1.000000-1 0.000000+06334 2151 22 2.107000+1 2.500000+0 1.359000-1 4.900000-3 1.310000-1 0.000000+06334 2151 23 2.217000+1 3.500000+0 1.444500-1 2.450000-3 1.420000-1 0.000000+06334 2151 24 2.510000+1 2.500000+0 1.198667-1 1.866667-3 1.180000-1 0.000000+06334 2151 25 2.730000+1 3.500000+0 9.555125-2 5.512500-4 9.500000-2 0.000000+06334 2151 26 2.827100+1 2.500000+0 1.307729-1 8.353567-4 1.299375-1 0.000000+06334 2151 27 2.877900+1 3.500000+0 1.243259-1 9.509500-4 1.233750-1 0.000000+06334 2151 28 2.962700+1 3.500000+0 1.288930-1 2.892925-3 1.260001-1 0.000000+06334 2151 29 2.975100+1 3.500000+0 1.260644-1 6.423375-5 1.260001-1 0.000000+06334 2151 30 3.006000+1 2.500000+0 1.261720-1 1.718267-4 1.260001-1 0.000000+06334 2151 31 3.051800+1 3.500000+0 1.221206-1 1.370425-3 1.207501-1 0.000000+06334 2151 32 3.149000+1 2.500000+0 1.529095-1 4.597017-3 1.483125-1 0.000000+06334 2151 33 3.196000+1 2.500000+0 1.492289-1 7.478917-3 1.417500-1 0.000000+06334 2151 34 3.271600+1 3.500000+0 1.574720-1 1.284500-3 1.561875-1 0.000000+06334 2151 35 3.327300+1 2.500000+0 1.336325-1 7.632333-3 1.260001-1 0.000000+06334 2151 36 3.350800+1 3.500000+0 1.248073-1 1.196562-4 1.246876-1 0.000000+06334 2151 37 3.526000+1 3.500000+0 1.269128-1 9.127125-4 1.260001-1 0.000000+06334 2151 38 3.607700+1 2.500000+0 1.123201-1 7.576217-4 1.115625-1 0.000000+06334 2151 39 3.682000+1 3.500000+0 1.351642-1 1.289225-3 1.338750-1 0.000000+06334 2151 40 3.782900+1 3.500000+0 1.172684-1 1.489338-2 1.023750-1 0.000000+06334 2151 41 3.854000+1 2.500000+0 1.410393-1 3.226767-3 1.378125-1 0.000000+06334 2151 42 3.878200+1 3.500000+0 1.254451-1 3.382575-3 1.220625-1 0.000000+06334 2151 43 3.950000+1 2.500000+0 1.608558-1 8.605800-3 1.522500-1 0.000000+06334 2151 44 4.129500+1 2.500000+0 1.152008-1 2.325633-3 1.128751-1 0.000000+06334 2151 45 4.246500+1 3.500000+0 1.165747-1 2.387087-3 1.141876-1 0.000000+06334 2151 46 4.327600+1 3.500000+0 1.326475-1 1.397463-3 1.312500-1 0.000000+06334 2151 47 4.471800+1 2.500000+0 1.267358-1 7.356650-4 1.260001-1 0.000000+06334 2151 48 4.582600+1 3.500000+0 1.261585-1 1.583663-4 1.260001-1 0.000000+06334 2151 49 4.673000+1 2.500000+0 1.263224-1 3.222333-4 1.260001-1 0.000000+06334 2151 50 4.881000+1 3.500000+0 1.458901-1 6.765150-3 1.391250-1 0.000000+06334 2151 51 4.939800+1 3.500000+0 1.374297-1 2.242188-3 1.351875-1 0.000000+06334 2151 52 5.048100+1 2.500000+0 1.284646-1 2.464467-3 1.260001-1 0.000000+06334 2151 53 5.110600+1 3.500000+0 1.145622-1 1.687087-3 1.128751-1 0.000000+06334 2151 54 5.295700+1 3.500000+0 1.263425-1 3.423350-4 1.260001-1 0.000000+06334 2151 55 5.339600+1 2.500000+0 9.684501-2 7.595000-3 8.925001-2 0.000000+06334 2151 56 5.441200+1 3.500000+0 1.400781-1 2.265638-3 1.378125-1 0.000000+06334 2151 57 5.528400+1 2.500000+0 1.268179-1 8.177166-4 1.260001-1 0.000000+06334 2151 58 5.606400+1 3.500000+0 1.056326-1 1.945125-3 1.036875-1 0.000000+06334 2151 59 5.683800+1 2.500000+0 1.274238-1 1.423683-3 1.260001-1 0.000000+06334 2151 60 5.776700+1 3.500000+0 1.349810-1 1.948100-2 1.155000-1 0.000000+06334 2151 61 5.800800+1 3.500000+0 1.263606-1 3.604475-4 1.260001-1 0.000000+06334 2151 62 5.906600+1 2.500000+0 1.274520-1 1.451917-3 1.260001-1 0.000000+06334 2151 63 5.921500+1 3.500000+0 1.273624-1 1.362287-3 1.260001-1 0.000000+06334 2151 64 5.973200+1 2.500000+0 1.460025-1 1.606500-2 1.299375-1 0.000000+06334 2151 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