2-He-3 ENDF/B-VII.1 Processed by Red Cullen using PREPRO2012 7100 0 0 0 2003.00000 2.98903200 0 0 0 0 225 1451 1 0.0 0.0 0 0 0 6 225 1451 2 1.00000000 20000000.0 1 0 10 7 225 1451 3 120000000. 0.0 1 0 216 8 225 1451 4 2-He- 3 LANL EVAL-MAY90 G.Hale,D.Dodder,P.Young 225 1451 5 DIST-DEC06 20111222 225 1451 6 ----ENDF/B-VII.1 MATERIAL 225 225 1451 7 -----INCIDENT NEUTRON DATA 225 1451 8 ------ENDF-6 FORMAT 225 1451 9 225 1451 10 225 1451 11 **************************************************************** 225 1451 12 ENDF/B-VII.1 225 1451 13 **************************************************************** 225 1451 14 225 1451 15 New capture cross sections were evaluated with the EDA code. 225 1451 16 The ENDF/B-VI evaluation is strictly 1/v, going through a low 225 1451 17 thermal value, whereas the data indicate a higher thermal value, 225 1451 18 and resonance structure around 2 MeV. This fit also had data in 225 1451 19 the 4He(gamma,n) direction that indicated a much higher cross 225 1451 20 section in the MeV region, and that is the reason why the new 225 1451 21 evaluation looks overshooting the experimental 3He(n,g) data 225 1451 22 in the MeV region. The differences in the new and old capture 225 1451 23 cross sections was added to the total cross sections. 225 1451 24 225 1451 25 G. Hale (Apr. 2011) 225 1451 26 225 1451 27 **************************************************************** 225 1451 28 225 1451 29 ENDF/B-VII CONVERTED FROM ENDF/B-VI BY NNDC OCT 2004 225 1451 30 225 1451 31 **************************************************************** 225 1451 32 225 1451 33 MOD1 OF ENDF/B-VI 225 1451 34 225 1451 35 THE ONLY REVISION MADE FOR MOD1 OF ENDF/B-VI WAS TO ADD THE 225 1451 36 COMMENTS BELOW ON THE STANDARDS COVARIANCES. THE DESCRIPTION 225 1451 37 OF THE ENDF/B-VI EVALUATION IS GIVEN BELOW. 225 1451 38 225 1451 39 ***************************************************************** 225 1451 40 225 1451 41 ---------------------------------------------------------------- 225 1451 42 HE-3 FREE ATOM EVALUATION 225 1451 43 ENDF/B-VI DESCRIPTION 225 1451 44 ---------------------------------------------------------------- 225 1451 45 225 1451 46 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 225 1451 47 225 1451 48 this file transfered from l.stewart's endf/b-iii evaluation with 225 1451 49 modifications only in the 3he(n,p) and the elastic cross sections 225 1451 50 below 5 MeV, and the total cross section below 0.1 MeV. 225 1451 51 * * * * * * * 225 1451 52 * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * * 225 1451 53 * * 225 1451 54 * cross section standard he-3 (n,p) * 225 1451 55 * * 225 1451 56 * the he-3 (n,p) cross section for this material is recommended 225 1451 57 * as a standard for neutron energies from thermal to 50 kev 225 1451 58 * * 225 1451 59 * * * * * * * 225 1451 60 225 1451 61 225 1451 62 mf=1 225 1451 63 225 1451 64 mt=451, atomic mass=3.0160 225 1451 65 225 1451 66 mf=2 225 1451 67 225 1451 68 mt=151, scattering length=0.2821e-12 cm. 225 1451 69 225 1451 70 mf=3 225 1451 71 225 1451 72 mt= 1, total cross sections --- from .00001 ev to 200 kev 225 1451 73 mt1 taken as sum mt2+mt102+mt103. from 200 kev to 20 225 1451 74 mev, mt1 evaluated using experimental data from ref.6. 225 1451 75 225 1451 76 mt= 2, elastic scattering cross sections --- from .00001 ev 225 1451 77 to 200 kev, mt2 taken approximately from r-matrix 225 1451 78 analysis described below. above 200 kev, obtained 225 1451 79 from mt2=mt1-mt102-mt103-mt104. note two reactions 225 1451 80 missing from this evaluation, namely n,n-prime,p and 225 1451 81 n,2n,2p. exp. data at 15 mev indicates non-zero 225 1451 82 cross sections for these. included in mt2 this eval. 225 1451 83 225 1451 84 mt=102, radiative capture cross sections --- thermal value 225 1451 85 taken from ref.17, with assumption of 1/v energy 225 1451 86 energy variation at all other energies. 225 1451 87 225 1451 88 mt=103, n-p cross sections --- below 5 mev taken from an 225 1451 89 r-matrix calculation of the four-body reactions 225 1451 90 by hale and dodder. 3he(n,p) data included were 225 1451 91 from refs. 5,13,14, and 15. for energies in the 225 1451 92 5-20 mev range, data were used as follows - 225 1451 93 ref.4 - 5.8 mev to 11. mev 225 1451 94 ref.10- 5.0 mev to 11. mev 225 1451 95 ref.12- 5.0 mev to 12. mev 225 1451 96 ref.16- 14. mev 225 1451 97 data extrapolated to 20. mev. 225 1451 98 225 1451 99 mt=104, n-d cross sections --- threshold=4.36147mev 225 1451 100 q=-3.2684 mev. evaluation from a detailed balance 225 1451 101 calculation(ref.13) and experimental data(ref.11). 225 1451 102 225 1451 103 mt=251, average value of cosine of elastic scattering angle, 225 1451 104 laboratory system. obtained from data mf=4,mt=2. 225 1451 105 225 1451 106 mt=252, values of xi, obtained from data mf=4,mt=2 225 1451 107 225 1451 108 mt=253, values of gamma,obtained from data mf=4,mt=2 225 1451 109 225 1451 110 mf=4 225 1451 111 225 1451 112 mt= 2, angular distribution of secondary neutrons from 225 1451 113 elastic scatter. evaluated from experimental data 225 1451 114 from refs.2,7,9,11,16,17 covering incident energies 225 1451 115 as follows - 225 1451 116 incident energy references 225 1451 117 1.e-5ev (isotropic) 225 1451 118 0.5 mev (isotropic) 225 1451 119 1.0 mev 9 225 1451 120 2.0 mev 9 225 1451 121 2.6 mev 11 225 1451 122 3.5 mev 9 225 1451 123 5.0 mev 11 225 1451 124 6.0 mev 9,7(from p+t elastic scatt) 225 1451 125 8.0 mev 11,7(from p+t elastic scatt) 225 1451 126 14.5 mev 16,17(from p+t elastic scatt) 225 1451 127 17.5 mev 11 225 1451 128 20.0 mev 2(from p+t elastic scatt) 225 1451 129 225 1451 130 references 225 1451 131 225 1451 132 1. r.batchelor,r.aves,and t.h.r.skyrme,rev.sci.instr.26,1037 225 1451 133 (1955). 225 1451 134 2. r.a.vanetsian and e.d.fenchenko,soviet journal of atomic 225 1451 135 energy 2,141(1957). 225 1451 136 3. j.n.bradbury and l.stewart,bull.am.phys.soc.3,417(1958) 225 1451 137 4. g.f.bogdanov,n.a.vlasov,c.p.kalinin,b.v.rybakov,l.n. 225 1451 138 samoilov,and v.a.sidorov,jetp(ussr)36,633(1959). 225 1451 139 5. j.h.gibbons and r.l.macklin,phys.rev.114,571(1959). 225 1451 140 6. los alamos physics and cryogenics groups,nucl.phys.12, 225 1451 141 291(1959). 225 1451 142 7. j.e.brolley,jr.,t.m.putnam,l.rosen,and l.stewart,phys. 225 1451 143 rev.159,777(1967). 225 1451 144 8. j.e.perry,private communication to stewart(1960) 225 1451 145 9. j.d.seagrave,l.cranberg,and j.e.simmons,phys.rev.119, 225 1451 146 1981(1960) 225 1451 147 10. m.d.goldberg,j.d.anderson,j.p.stoering,and c.wong,phys. 225 1451 148 rev.122,1510(1961). 225 1451 149 11. a.r.sayers,k.w.jones,and c.s.wu,phys.rev.122,1853(1961). 225 1451 150 12. w.e.wilson,r.l.walter,and d.b.fossan,nucl.phys.27,421 225 1451 151 (1961). 225 1451 152 13. j.als-nielsen and o.dietrich,phys.rev.133,b925(1964). 225 1451 153 14. r.l.macklin and j.h.gibbons,proceedings of the internatl. 225 1451 154 conf.on the study of nucl.struct.with neuts.,antwerp(1965) 225 1451 155 15. j.h.gibbons,private communication to stewart(1966). 225 1451 156 16. b.antolkovic,g.paic,p.tomas,and r.rendic,phys.rev.159, 225 1451 157 777(1967). 225 1451 158 17. l.rosen and w.leland,private communication(1967) 225 1451 159 18. s.mughabghab et al., neut.cross sect., vol.1, neut.reson. 225 1451 160 parameters and thermal cross sect., academic pr.(1981). 225 1451 161 225 1451 162 **************************************************************** 225 1451 163 225 1451 164 STANDARDS COVARIANCES 225 1451 165 225 1451 166 Phase 1 reviewers of the ENDF/B-VI standards cross sections have 225 1451 167 expressed the concern that the uncertainties resulting from the 225 1451 168 combination of R-matrix and simultaneous evaluations might have 225 1451 169 led to uncertainties that are too small. As a result, the 225 1451 170 Standards Subcommittee produced (at the May, 1990 CSEWG meeting) 225 1451 171 a set of expanded covariance estimates for the standard cross 225 1451 172 section reactions. These uncertainties are estimates such that 225 1451 173 if a modern day experiment were performed on a given standard 225 1451 174 cross section using the best techniques, approximately 2/3 of 225 1451 175 the results should fall within these expanded uncertainties. The 225 1451 176 expanded uncertainties for the He-3(n,p) cross section are as 225 1451 177 follows: 225 1451 178 225 1451 179 Energy Range Estimated Uncertainty 225 1451 180 (keV) (percent) 225 1451 181 225 1451 182 1.0E-08 - 0.1 0.3 225 1451 183 0.1 - 1.0 0.7 225 1451 184 1.0 - 10. 2.0 225 1451 185 10. - 50. 5.0 225 1451 186 **************************************************************** 225 1451 187 225 1451 188 ***************** Program LINEAR (VERSION 2012-1) *************** 225 1451 189 For All Data Greater than 1.0000E-10 barns in Absolute Value 225 1451 190 Data Linearized to Within an Accuracy of .010000000 per-cent 225 1451 191 ***************** Program SIGMA1 (VERSION 2012-1) *************** 225 1451 192 Data Doppler Broadened to 1200.00000 Kelvin 225 1451 193 For All Data Greater than 1.0000E-10 barns in Absolute Value 225 1451 194 Data Linearized Using Energy Dependent Uncertainty 225 1451 195 Energy Accuracy 225 1451 196 (eV) (per-cent) 225 1451 197 ----------- ----------- 225 1451 198 1.00000000 .010000000 225 1451 199 2.00000000 .100000000 225 1451 200 ***************** Program SIGMA1 (VERSION 2012-1) *************** 225 1451 201 Data Doppler Broadened to 120000000. Kelvin 225 1451 202 For All Data Greater than 1.0000E-10 barns in Absolute Value 225 1451 203 Data Linearized to Within an Accuracy of .500000000 per-cent 225 1451 204 ***************** Program FIXUP (Version 2012-1) **************** 225 1451 205 Corrected ZA/AWR in All Sections-----------------------------Yes 225 1451 206 Corrected Thresholds-----------------------------------------No 225 1451 207 Extended Cross Sections to 20 MeV----------------------------No 225 1451 208 Allow Cross Section Deletion---------------------------------No 225 1451 209 Allow Cross Section Reconstruction---------------------------Yes 225 1451 210 Make All Cross Sections Non-Negative-------------------------Yes 225 1451 211 Delete Energies Not in Ascending Order-----------------------Yes 225 1451 212 Deleted Duplicate Points-------------------------------------Yes 225 1451 213 Check for Ascending MAT/MF/MT Order--------------------------Yes 225 1451 214 Check for Legal MF/MT Numbers--------------------------------Yes 225 1451 215 Allow Creation of Missing Sections---------------------------Yes 225 1451 216 Allow Insertion of Energy Points-----------------------------No 225 1451 217 Uniform Energy Grid for ALL MT-------------------------------No 225 1451 218 Delete Section if Cross Section =0 at All Energies-----------Yes 225 1451 219 **************** Program DICTIN (VERSION 2012-1) **************** 225 1451 220 1 451 228 0 225 1451 221 2 151 4 0 225 1451 222 3 1 118 0 225 1451 223 3 2 42 0 225 1451 224 3 102 41 0 225 1451 225 3 103 49 0 225 1451 226 3 104 42 0 225 1451 227 4 2 100 0 225 1451 228 225 1 0 229 225 0 0 230 2003.00000 2.98903200 0 0 1 0 225 2151 231 2003.00000 1.00000000 0 0 1 0 225 2151 232 .025000000 1000000.00 0 0 0 0 225 2151 233 .500000000 .513226500 0 0 0 0 225 2151 234 225 2 0 235 225 0 0 236 2003.00000 2.98903200 0 0 0 0 225 3 1 237 0.0 0.0 0 0 1 345 225 3 1 238 345 2 225 3 1 239 1.00000E-5 308094.090 1.25126E-5 275428.590 1.56566E-5 246226.422 225 3 1 240 1.95905E-5 220120.402 2.45129E-5 196782.258 3.06721E-5 175918.524 225 3 1 241 3.83789E-5 157266.859 4.80221E-5 140592.725 6.00883E-5 125686.455 225 3 1 242 7.51862E-5 112360.615 9.40778E-5 100447.639 1.17716E-4 89797.7302 225 3 1 243 1.47294E-4 80276.9723 1.84303E-4 71765.6471 2.30612E-4 64156.7303 225 3 1 244 2.88556E-4 57354.5449 3.61060E-4 51273.5574 4.51781E-4 45837.3031 225 3 1 245 5.65297E-4 40977.4247 7.07336E-4 36632.8123 8.85063E-4 32748.8349 225 3 1 246 .001107447 29276.6540 .001385708 26172.6090 .001733885 23397.6684 225 3 1 247 .002169547 20916.9388 .002714674 18699.2260 .003396773 16716.6456 225 3 1 248 .004250257 14944.2777 .005318191 13359.8231 .006654457 11943.3568 225 3 1 249 .008326477 10677.0692 .010418616 9545.03798 .013036432 8533.02789 225 3 1 250 .016312009 7628.32052 .020410618 6819.53339 .025241880 6132.27878 225 3 1 251 .025300000 6125.23110 .031656962 5475.80591 .039611195 4895.23840 225 3 1 252 .049564035 4376.22371 .062017658 3912.23764 .077600420 3497.44551 225 3 1 253 .097098559 3126.63155 .121495864 2795.13271 .152023317 2498.78152 225 3 1 254 .190221199 2233.85062 .238016807 1997.00897 .297821698 1785.27849 225 3 1 255 .372653364 1595.99678 .466287482 1426.78373 .583448419 1275.51149 225 3 1 256 .730047600 1140.27818 .913481777 1019.38306 1.14300623 911.306052 225 3 1 257 1.43020176 814.688164 1.78955899 728.314455 2.23920951 651.098852 225 3 1 258 2.80184070 582.070402 3.50584047 520.361120 4.38672956 465.195062 225 3 1 259 5.48895375 415.878531 6.86812644 371.791419 8.59383463 332.379346 225 3 1 260 10.7531500 297.146737 13.4550220 265.650559 16.8357754 237.494769 225 3 1 261 16.9545367 236.788149 21.0659881 212.325323 21.3631912 211.061992 225 3 1 262 26.3590980 189.825735 26.9195404 188.125711 32.9821722 169.735569 225 3 1 263 33.2148317 169.189516 33.9193752 167.666073 41.2693820 151.773073 225 3 1 264 41.8516187 150.799615 42.7414603 149.428027 51.6388635 135.713713 225 3 1 265 52.7367998 134.406054 53.8554376 133.176947 64.6138153 121.356152 225 3 1 266 66.4498454 119.798427 67.8626901 118.691863 80.8488965 108.520840 225 3 1 267 83.7327755 106.777948 85.5088910 105.786372 101.163258 97.0467955 225 3 1 268 105.505643 95.1774537 108.012563 94.1798603 126.581873 86.7904668 225 3 1 269 132.946590 84.8388926 136.098857 83.9448157 158.387253 77.6231624 225 3 1 270 167.516429 75.6294871 171.496787 74.8248743 198.184159 69.4301338 225 3 1 271 211.085751 67.4236061 216.090757 66.7025833 247.980567 62.1085273 225 3 1 272 265.973961 60.1158112 272.293769 59.4670496 310.288985 55.5666409 225 3 1 273 335.151088 53.6062682 345.518025 52.8480134 388.253223 49.7222911 225 3 1 274 422.299761 47.8112736 438.433483 46.9706214 485.807013 44.5022103 225 3 1 275 532.135642 42.6515127 560.232386 41.6098044 607.872492 39.8435113 225 3 1 276 675.235634 37.9313449 715.902728 36.8596868 760.608546 35.6816006 225 3 1 277 856.817559 33.7439120 921.236882 32.5375780 951.721568 31.9667134 225 3 1 278 1087.22984 30.0308970 1190.85428 28.6535029 1193.76848 28.6240200 225 3 1 279 1389.26745 26.6461636 1490.07227 25.6969001 1557.83588 25.2126620 225 3 1 280 1787.73507 23.5698050 1864.47276 23.0587313 2061.61512 22.0660244 225 3 1 281 2316.71847 20.7814563 2332.94636 20.7051235 2786.31732 19.0996229 225 3 1 282 2919.13018 18.6292993 3023.25552 18.3472281 3652.60050 16.7821393 225 3 1 283 3872.58392 16.3662147 3972.90280 16.1765409 4570.36499 15.1356034 225 3 1 284 5331.85245 14.1342198 5344.90031 14.1183267 5718.73003 13.6629790 225 3 1 285 7105.86271 12.3926094 7307.77894 12.2511194 8427.32674 11.5342984 225 3 1 286 8829.02448 11.2771005 10372.7225 10.5294860 10970.5888 10.2610559 225 3 1 287 13630.9413 9.36757246 15462.6703 8.90056159 16818.6163 8.58018401 225 3 1 288 20751.7477 7.87959937 25426.5597 7.24592787 25604.6649 7.22330759 225 3 1 289 31372.7089 6.66779532 37467.6566 6.21632743 38438.2523 6.14443297 225 3 1 290 44842.6089 5.77516519 47097.3592 5.65592191 57302.9102 5.23790696 225 3 1 291 62042.7629 5.08503334 69719.9072 4.83742360 71198.7857 4.79931345 225 3 1 292 84827.5496 4.49321311 96462.1768 4.28717675 102485.929 4.18050263 225 3 1 293 108393.046 4.09659238 123826.293 3.90919257 149602.961 3.66436603 225 3 1 294 158613.028 3.59681296 163869.738 3.55740065 180754.376 3.45337428 225 3 1 295 218381.648 3.27792497 236456.850 3.21366488 239207.453 3.20388603 225 3 1 296 265702.879 3.13330871 327839.046 3.01762797 357460.394 2.97791589 225 3 1 297 379801.279 2.94796416 446185.193 2.88907475 540412.355 2.82105262 225 3 1 298 550528.200 2.81374994 604232.460 2.79051739 738838.898 2.77861094 225 3 1 299 761349.830 2.78095869 788862.331 2.79043929 898938.278 2.82836962 225 3 1 300 950000.000 2.85258733 1080125.64 2.92700111 1400005.67 3.10992501 225 3 1 301 1480693.65 3.15606574 1500000.00 3.16276108 1521311.58 3.16864766 225 3 1 302 1740391.92 3.21356236 1777308.61 3.22113045 1785478.42 3.22104499 225 3 1 303 2023688.11 3.19240915 2100562.85 3.17573923 2175383.15 3.15951437 225 3 1 304 2200000.00 3.15345747 2655280.73 3.04143457 2894001.23 2.98269521 225 3 1 305 3047301.94 2.92705487 3220568.71 2.87151561 3332453.65 2.83565180 225 3 1 306 3363323.13 2.82575680 3434700.34 2.80287732 3470388.94 2.79143759 225 3 1 307 3488233.24 2.78571772 3497155.39 2.78285778 3502731.74 2.78107032 225 3 1 308 3508308.08 2.77928286 3513884.43 2.77749540 3519460.78 2.77570794 225 3 1 309 3525037.12 2.77392048 3530613.47 2.77213302 3536189.81 2.77034557 225 3 1 310 3541766.15 2.76855811 3547342.50 2.76677065 3552918.84 2.76498319 225 3 1 311 3555392.49 2.76419028 3558495.19 2.76330981 3564071.53 2.76172740 225 3 1 312 3569647.87 2.76014499 3575224.22 2.75856257 3580800.56 2.75698015 225 3 1 313 3586376.90 2.75539774 3591953.25 2.75381532 3597529.59 2.75223291 225 3 1 314 3603105.94 2.75065049 3609797.55 2.74875159 3616489.16 2.74685270 225 3 1 315 3623180.77 2.74495380 3629872.39 2.74305490 3636564.00 2.74115600 225 3 1 316 3643255.61 2.73925711 3649947.22 2.73735821 3656638.84 2.73545931 225 3 1 317 3663330.46 2.73356041 3670022.07 2.73166152 3676713.68 2.72976262 225 3 1 318 3683405.30 2.72786373 3690096.91 2.72596484 3696788.52 2.72406595 225 3 1 319 3703480.13 2.72216706 3711287.01 2.71995169 3719093.90 2.71773632 225 3 1 320 3726900.78 2.71552095 3734707.66 2.71330559 3742514.54 2.71109024 225 3 1 321 3750321.42 2.70887488 3758128.30 2.70665954 3765935.18 2.70444420 225 3 1 322 3773742.06 2.70222887 3781548.95 2.70001355 3789355.83 2.69779824 225 3 1 323 3798277.98 2.69526648 3807200.14 2.69273473 3816122.29 2.69020301 225 3 1 324 3825044.44 2.68767133 3833966.59 2.68513967 3842888.74 2.68260806 225 3 1 325 3851810.89 2.68007650 3860733.04 2.67754499 3869655.19 2.67501355 225 3 1 326 3878577.34 2.67248219 3887499.49 2.66995091 3896421.64 2.66741974 225 3 1 327 3905343.79 2.66488869 3916496.47 2.66172507 3927649.16 2.65856169 225 3 1 328 3938801.85 2.65539861 3949954.55 2.65223587 3961107.23 2.64907353 225 3 1 329 3972259.92 2.64591166 3983412.61 2.64275032 3994565.30 2.63958959 225 3 1 330 4007948.52 2.63579766 4021331.75 2.63200689 4034714.97 2.62821750 225 3 1 331 4048098.20 2.62442967 4061481.42 2.62064363 4077095.18 2.61622917 225 3 1 332 4092708.96 2.61181788 4093335.46 2.61164102 4108322.72 2.60784569 225 3 1 333 4123936.48 2.60389579 4141780.78 2.59938725 4159625.08 2.59488545 225 3 1 334 4179699.92 2.58982992 4197544.22 2.58534496 4219849.59 2.57975165 225 3 1 335 4242154.98 2.57417393 4264460.35 2.56861308 4291226.80 2.56196387 225 3 1 336 4317993.25 2.55534212 4349220.78 2.54765308 4385343.53 2.53880924 225 3 1 337 4424880.79 2.52919314 4467277.63 2.51895712 4518298.63 2.50674580 225 3 1 338 4569474.27 2.49462052 4626931.55 2.48116411 4660514.94 2.47340875 225 3 1 339 4691409.97 2.46627430 4760306.50 2.45061288 4809336.34 2.43965940 225 3 1 340 4861190.99 2.42914692 4865382.33 2.42830649 5161325.60 2.36449671 225 3 1 341 5401299.11 2.31192929 5468138.21 2.29700041 5476821.32 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