ENTRY 10852 20210827 14911085200000001 SUBENT 10852001 20210827 14911085200100001 BIB 13 45 1085200100002 TITLE Gamma-Ray Production and Inferred Inelastic Neutron 1085200100003 Cross Sections for Nickel Isotopes 1085200100004 AUTHOR (S.Traiforos,A.Mittler,W.A.Schier,B.K.Barnes, 1085200100005 L.E.Beghian,P.Harihar) 1085200100006 REFERENCE (J,NSE,72,191,1979) 1085200100007 #doi:10.13182/NSE79-A19463 1085200100008 (J,BAP,23,636(KL6),1978) Preliminary results. 1085200100009 INSTITUTE (1USALTI) 1085200100010 FACILITY (ACCEL,1USALTI) 1085200100011 INC-SOURCE (P-T) The T(p,n)3He reaction provided neutron bursts 1085200100012 in this pulsed beam experiment. The neutron energy 1085200100013 spread was due both to target thickness effects on 1085200100014 the protons and the effect of reaction kinematics 1085200100015 caused by the sample's subtended solid angle. The two 1085200100016 effects summed in quadrature gave an estimated 1085200100017 neutron energy spread of ~100 keV. 1085200100018 INC-SPECT Neutron energy spread 100 keV due to target thickness 1085200100019 and reaction kinematics caused by subtended solid angle1085200100020 of the sample. 1085200100021 SAMPLE Cylinder of natural nickel, 5-cm high by 2.5-cm 1085200100022 diameter. 1085200100023 METHOD (TOF) 1085200100024 DETECTOR (GELI) 40 cubic centimeter GeLi detector calibrated 1085200100025 with standard sources. 1085200100026 (LONGC) Long counter for neutron flux normalization 1085200100027 proton recoil detector for neutron flux normalization. 1085200100028 CORRECTION Data corrected for 1085200100029 - dead time 1085200100030 - small dc current in beam 1085200100031 - neutron attenuation 1085200100032 - gamma attenuation 1085200100033 - neutron multiple scattering 1085200100034 - non parallel neutron flux 1085200100035 - angular variation of n-source 1085200100036 ERR-ANALYS (DATA-ERR) Typical uncertainties in data are 1085200100037 (ERR-1) detector efficiency, +- 6 percent 1085200100038 (ERR-2) finite sample correction, +- 4 percent 1085200100039 (ERR-3) calculated conversion factors, +- 2 percent 1085200100040 HISTORY (19800609C) 1085200100041 (20210827A) BP: Updated to new date formats, lower 1085200100042 case. Corrections according last EXFOR rules and 1085200100043 Dict. Updated entry, added doi, digitized data, 1085200100044 deleted subentries 2-5, 14 (unobtainable data) per an 1085200100045 NRDC decision for data sets that were published 1085200100046 before 2000 (C32 of WP2022-01). Added subentry 15. 1085200100047 ENDBIB 45 0 1085200100048 COMMON 4 3 1085200100049 EN-RSL ERR-1 ERR-2 ERR-3 1085200100050 KEV PER-CENT PER-CENT PER-CENT 1085200100051 100. 6.0 4.0 2.0 1085200100052 ENDCOMMON 3 0 1085200100053 ENDSUBENT 52 0 1085200199999 NOSUBENT 10852002 20210827 14911085200200001 NOSUBENT 10852003 20210827 14911085200300001 NOSUBENT 10852004 20210827 14911085200400001 NOSUBENT 10852005 20210827 14911085200500001 SUBENT 10852006 20210827 14911085200600001 BIB 3 3 1085200600002 REACTION (28-NI-58(N,X)0-G-0,PAR,DA) 1085200600003 STATUS (CURVE) Fig. 4, page 196 of Nucl.Sci.Eng.72,191,1979. 1085200600004 HISTORY (20210827A) BP: Digitized data. 1085200600005 ENDBIB 3 0 1085200600006 COMMON 1 3 1085200600007 ANG 1085200600008 ADEG 1085200600009 125.0 1085200600010 ENDCOMMON 3 0 1085200600011 DATA 4 102 1085200600012 E EN DATA DATA-ERR 1085200600013 KEV MEV MB/SR MB/SR 1085200600014 961.0 3.479 0.640 1085200600015 961.0 3.573 2.485 0.283 1085200600016 961.0 3.670 3.418 1085200600017 961.0 3.775 4.285 1085200600018 961.0 3.881 4.523 1085200600019 1005.0 2.685 1.586 1085200600020 1005.0 2.774 2.670 0.318 1085200600021 1005.0 2.871 3.346 1085200600022 1005.0 2.967 3.932 1085200600023 1005.0 3.088 4.245 1085200600024 1005.0 3.184 5.193 1085200600025 1005.0 3.281 5.553 1085200600026 1005.0 3.394 6.817 1085200600027 1005.0 3.490 6.362 1085200600028 1005.0 3.587 8.712 1085200600029 1005.0 3.699 8.031 1085200600030 1005.0 3.796 10.064 1.222 1085200600031 1005.0 3.885 11.057 1085200600032 1321.0 2.884 3.755 1085200600033 1321.0 2.988 7.421 1.071 1085200600034 1321.0 3.093 9.569 1085200600035 1321.0 3.197 11.092 1085200600036 1321.0 3.293 12.436 1085200600037 1321.0 3.396 11.994 1085200600038 1321.0 3.484 12.356 1085200600039 1321.0 3.588 12.361 1085200600040 1321.0 3.684 11.919 1085200600041 1321.0 3.787 11.657 1.250 1085200600042 1321.0 3.891 11.840 1085200600043 1448.0 2.960 2.482 1085200600044 1448.0 3.063 8.684 1.033 1085200600045 1448.0 3.167 14.023 1085200600046 1448.0 3.275 14.449 1085200600047 1448.0 3.366 15.910 1085200600048 1448.0 3.474 15.043 1085200600049 1448.0 3.572 17.797 1085200600050 1448.0 3.673 16.154 1085200600051 1448.0 3.781 16.493 1.810 1085200600052 1448.0 3.865 16.920 1085200600053 1454.0 1.568 13.205 1085200600054 1454.0 1.657 26.740 4.052 1085200600055 1454.0 1.770 35.327 1085200600056 1454.0 1.978 40.335 1085200600057 1454.0 2.178 45.791 1085200600058 1454.0 2.394 48.098 1085200600059 1454.0 2.490 47.221 1085200600060 1454.0 2.586 50.849 1085200600061 1454.0 2.690 54.929 4.947 1085200600062 1454.0 2.802 57.661 1085200600063 1454.0 2.890 62.638 1085200600064 1454.0 2.994 60.862 1085200600065 1454.0 3.098 60.889 1085200600066 1454.0 3.202 64.969 1085200600067 1454.0 3.298 67.246 1085200600068 1454.0 3.402 70.876 1085200600069 1454.0 3.498 71.350 1085200600070 1454.0 3.602 74.079 1085200600071 1454.0 3.697 70.500 1085200600072 1454.0 3.801 72.328 1085200600073 1454.0 3.889 76.405 7.660 1085200600074 1488.0 2.989 0.344 1085200600075 1488.0 3.100 0.758 0.404 1085200600076 1488.0 3.199 0.845 1085200600077 1488.0 3.296 1.036 1085200600078 1488.0 3.397 0.987 1085200600079 1488.0 3.490 0.895 1085200600080 1488.0 3.581 1.058 1085200600081 1488.0 3.680 1.135 1085200600082 1488.0 3.867 0.960 0.436 1085200600083 1488.0 3.955 1.282 1085200600084 1584.0 3.176 1.653 1085200600085 1584.0 3.288 3.062 1085200600086 1584.0 3.400 3.310 0.455 1085200600087 1584.0 3.496 4.037 1085200600088 1584.0 3.592 4.627 1085200600089 1584.0 3.680 4.035 1085200600090 1584.0 3.776 4.147 1085200600091 1584.0 3.880 5.169 0.683 1085200600092 1810.0 3.376 0.560 1085200600093 1810.0 3.507 1.237 1085200600094 1810.0 3.593 1.916 0.416 1085200600095 1810.0 3.693 2.090 1085200600096 1810.0 3.808 2.373 1085200600097 1810.0 3.910 3.336 1085200600098 1810.0 3.977 2.722 1085200600099 2077.0 3.689 0.659 1085200600100 2077.0 3.778 1.230 1085200600101 2077.0 3.879 1.065 0.307 1085200600102 2077.0 3.964 0.977 1085200600103 3038.0 3.200 0.902 0.364 1085200600104 3038.0 3.304 2.242 1085200600105 3038.0 3.496 1.944 1085200600106 3038.0 3.592 2.398 1085200600107 3038.0 3.688 2.260 0.478 1085200600108 3038.0 3.792 3.191 1085200600109 3254.0 3.354 1.042 1085200600110 3254.0 3.503 2.596 1085200600111 3254.0 3.590 3.538 1085200600112 3254.0 3.689 3.514 0.877 1085200600113 3254.0 3.813 4.280 1085200600114 3254.0 3.907 5.375 1085200600115 3254.0 3.991 5.198 1085200600116 ENDDATA 104 0 1085200600117 ENDSUBENT 116 0 1085200699999 SUBENT 10852007 20210827 14911085200700001 BIB 3 3 1085200700002 REACTION (28-NI-60(N,X)0-G-0,PAR,DA) 1085200700003 STATUS (CURVE) Fig. 5, page 197 of Nucl.Sci.Eng.72,191,1979. 1085200700004 HISTORY (20210827A) BP: Digitized data. 1085200700005 ENDBIB 3 0 1085200700006 COMMON 1 3 1085200700007 ANG 1085200700008 ADEG 1085200700009 125.0 1085200700010 ENDCOMMON 3 0 1085200700011 DATA 4 116 1085200700012 E EN DATA DATA-ERR 1085200700013 KEV MEV MB/SR MB/SR 1085200700014 467.0 2.765 1.971 0.412 1085200700015 467.0 2.877 3.109 1085200700016 467.0 2.973 4.143 1085200700017 467.0 3.082 6.105 1085200700018 467.0 3.182 5.696 1085200700019 467.0 3.286 6.576 1085200700020 467.0 3.375 6.939 1085200700021 467.0 3.479 7.974 1085200700022 467.0 3.571 7.204 0.618 1085200700023 467.0 3.676 7.877 1085200700024 467.0 3.776 7.365 1085200700025 467.0 3.874 7.523 1085200700026 827.0 2.361 9.374 1085200700027 827.0 2.472 13.091 1085200700028 827.0 2.541 14.545 1085200700029 827.0 2.566 15.677 1085200700030 827.0 2.678 15.354 1.616 1085200700031 827.0 2.780 18.101 1085200700032 827.0 2.882 21.333 1085200700033 827.0 2.985 20.525 1085200700034 827.0 3.088 20.687 1085200700035 827.0 3.191 23.111 1085200700036 827.0 3.293 24.081 1085200700037 827.0 3.388 22.949 1085200700038 827.0 3.499 26.182 1085200700039 827.0 3.593 25.859 1085200700040 827.0 3.679 25.212 1085200700041 827.0 3.790 25.051 1085200700042 827.0 3.893 24.404 1.939 1085200700043 953.0 2.469 2.347 1085200700044 953.0 2.558 4.337 1085200700045 953.0 2.674 5.102 0.408 1085200700046 953.0 2.773 5.612 1085200700047 953.0 2.890 5.408 1085200700048 953.0 2.998 4.796 1085200700049 953.0 3.097 5.918 1085200700050 953.0 3.196 6.327 1085200700051 953.0 3.297 5.510 1085200700052 953.0 3.406 4.490 1085200700053 953.0 3.488 5.510 1085200700054 953.0 3.588 4.745 1085200700055 953.0 3.688 5.306 1085200700056 953.0 3.796 5.102 1085200700057 953.0 3.888 4.592 0.510 1085200700058 953.0 3.971 4.286 1085200700059 1174.0 2.593 1.645 1085200700060 1174.0 2.691 3.181 1085200700061 1174.0 2.789 4.310 1.430 1085200700062 1174.0 2.902 6.052 1085200700063 1174.0 2.984 6.771 1085200700064 1174.0 3.114 5.657 1085200700065 1174.0 3.187 9.029 1085200700066 1174.0 3.301 8.935 1085200700067 1174.0 3.390 10.981 1085200700068 1174.0 3.504 13.233 1085200700069 1174.0 3.602 13.546 4.083 1085200700070 1174.0 3.691 14.878 1085200700071 1174.0 3.789 13.966 1085200700072 1174.0 3.894 14.381 1085200700073 1332.0 1.328 3.342 1085200700074 1332.0 1.449 23.983 1085200700075 1332.0 1.553 39.331 1085200700076 1332.0 1.639 37.214 1085200700077 1332.0 1.750 40.919 1085200700078 1332.0 1.965 51.504 1085200700079 1332.0 2.172 57.326 1085200700080 1332.0 2.369 65.264 1085200700081 1332.0 2.465 80.083 1085200700082 1332.0 2.550 80.613 1085200700083 1332.0 2.584 76.379 1085200700084 1332.0 2.679 75.320 5.822 1085200700085 1332.0 2.782 84.317 1085200700086 1332.0 2.885 86.434 1085200700087 1332.0 2.988 88.022 1085200700088 1332.0 3.108 84.317 1085200700089 1332.0 3.195 99.136 1085200700090 1332.0 3.298 100.724 1085200700091 1332.0 3.401 100.195 1085200700092 1332.0 3.504 110.780 1085200700093 1332.0 3.598 104.429 1085200700094 1332.0 3.710 103.900 1085200700095 1332.0 3.813 103.370 8.468 1085200700096 1332.0 3.898 98.607 1085200700097 1792.0 3.293 3.996 1085200700098 1792.0 3.390 6.334 1085200700099 1792.0 3.496 8.051 1085200700100 1792.0 3.593 7.021 1.190 1085200700101 1792.0 3.691 7.649 1085200700102 1792.0 3.805 8.434 1085200700103 1792.0 3.902 10.616 1085200700104 1986.0 3.568 2.480 1085200700105 1986.0 3.656 2.240 1085200700106 1986.0 3.752 2.827 1.307 1085200700107 1986.0 3.848 2.853 1085200700108 1986.0 3.960 2.747 1085200700109 2062.0 3.587 1.446 1085200700110 2062.0 3.677 2.196 1085200700111 2062.0 3.791 2.920 1085200700112 2062.0 3.880 3.214 0.830 1085200700113 2062.0 3.985 3.911 1085200700114 2159.000 2.303 0.646 1085200700115 2159.000 2.397 0.646 1085200700116 2159.000 2.500 2.424 1085200700117 2159.000 2.602 2.424 1085200700118 2159.000 2.705 1.616 1.131 1085200700119 2159.000 2.808 3.232 1085200700120 2159.000 3.005 3.394 1085200700121 2159.000 3.117 3.556 1085200700122 2159.000 3.202 3.879 1085200700123 2159.000 3.331 4.040 1085200700124 2159.000 3.417 3.717 1085200700125 2159.000 3.519 4.687 1085200700126 2159.000 3.622 4.687 1085200700127 2159.000 3.733 5.010 1085200700128 2159.000 3.905 4.364 2.101 1085200700129 2159.000 3.999 4.364 1085200700130 ENDDATA 118 0 1085200700131 ENDSUBENT 130 0 1085200799999 SUBENT 10852008 20210827 14911085200800001 BIB 3 3 1085200800002 REACTION (28-NI-62(N,X)0-G-0,PAR,DA) 1085200800003 STATUS (CURVE) Fig. 5, page 197 of Nucl.Sci.Eng.72,191,1979. 1085200800004 HISTORY (20210827A) BP: Digitized data. 1085200800005 ENDBIB 3 0 1085200800006 COMMON 1 3 1085200800007 ANG 1085200800008 ADEG 1085200800009 125.0 1085200800010 ENDCOMMON 3 0 1085200800011 DATA 4 8 1085200800012 E EN DATA DATA-ERR 1085200800013 KEV MEV MB/SR MB/SR 1085200800014 1173.0 1.345 22.795 3.608 1085200800015 1173.0 1.466 32.667 1085200800016 1173.0 1.571 34.798 1085200800017 1173.0 1.754 58.629 1085200800018 1173.0 1.980 62.901 1085200800019 1173.0 2.174 64.060 1085200800020 1173.0 2.386 55.436 1085200800021 1173.0 2.588 56.084 6.201 1085200800022 ENDDATA 10 0 1085200800023 ENDSUBENT 22 0 1085200899999 SUBENT 10852009 20210827 14911085200900001 BIB 3 3 1085200900002 REACTION (28-NI-64(N,X)0-G-0,PAR,DA) 1085200900003 STATUS (CURVE) Fig. 5, page 197 of Nucl.Sci.Eng.72,191,1979. 1085200900004 HISTORY (20210827A) BP: Digitized data. 1085200900005 ENDBIB 3 0 1085200900006 COMMON 1 3 1085200900007 ANG 1085200900008 ADEG 1085200900009 125.0 1085200900010 ENDCOMMON 3 0 1085200900011 DATA 4 20 1085200900012 E EN DATA DATA-ERR 1085200900013 KEV MEV MB/SR MB/SR 1085200900014 1348.0 1.794 34.821 1085200900015 1348.0 1.985 53.760 26.020 1085200900016 1348.0 2.171 50.759 1085200900017 1348.0 2.309 47.742 1085200900018 1348.0 2.389 50.319 1085200900019 1348.0 2.492 60.046 1085200900020 1348.0 2.575 46.807 1085200900021 1348.0 2.679 49.902 1085200900022 1348.0 2.782 62.181 1085200900023 1348.0 2.889 49.460 1085200900024 1348.0 2.984 65.307 1085200900025 1348.0 3.088 66.871 25.515 1085200900026 1348.0 3.178 60.778 1085200900027 1348.0 3.292 53.672 1085200900028 1348.0 3.394 73.603 1085200900029 1348.0 3.482 78.223 1085200900030 1348.0 3.569 89.986 1085200900031 1348.0 3.674 89.510 1085200900032 1348.0 3.763 88.008 1085200900033 1348.0 3.858 98.243 1085200900034 ENDDATA 22 0 1085200900035 ENDSUBENT 34 0 1085200999999 SUBENT 10852010 20210915 14911085201000001 BIB 4 17 1085201000002 REACTION (28-NI-58(N,X)0-G-0,PAR,SIG) 1085201000003 ANALYSIS Total cross sections were deduced from the 125 deg 1085201000004 gamma-ray production cross sections. In the 1085201000005 conversion of 125-deg gamma-ray production cross 1085201000006 sections, dsigma/dOmega (125 deg) , to total gamma 1085201000007 ray production cross sections preparatory to the 1085201000008 inference of neutron excitation functions, an 1085201000009 integral of the gamma radiation over all angles must 1085201000010 be taken. The result can be expressed as sigmaT = 1085201000011 4*pi*(dsigma/dOmega 125 deg) M. The factor M takes 1085201000012 into account the fourth-order Legendre polynomial's 1085201000013 effect on the 125-deg cross section. (The 1085201000014 second-order Legendre polynomial is zero at this 1085201000015 angle.) 1085201000016 STATUS (DEP,10852006) 1085201000017 (CURVE) Fig. 6, page 199 of J,NSE,72,191,1979. 1085201000018 HISTORY (20210827A) BP: Digitized data. 1085201000019 ENDBIB 17 0 1085201000020 NOCOMMON 0 0 1085201000021 DATA 4 89 1085201000022 E EN DATA DATA-ERR 1085201000023 KEV MEV MB MB 1085201000024 1454.0 1.551 154.860 1085201000025 1454.0 1.653 301.195 1085201000026 1454.0 1.745 412.897 1085201000027 1454.0 1.939 470.940 1085201000028 1454.0 2.153 536.711 1085201000029 1454.0 2.337 579.351 1085201000030 1454.0 2.449 571.862 1085201000031 1454.0 2.520 595.068 1085201000032 1454.0 2.561 629.756 1085201000033 1454.0 2.663 641.479 57.691 1085201000034 1454.0 2.765 672.433 1085201000035 1454.0 2.867 672.618 1085201000036 1454.0 2.959 576.632 1085201000037 1454.0 3.061 457.589 1085201000038 1454.0 3.153 396.219 1085201000039 1454.0 3.255 369.481 1085201000040 1454.0 3.367 377.377 1085201000041 1454.0 3.449 377.525 1085201000042 1454.0 3.541 335.384 1085201000043 1454.0 3.653 316.357 1085201000044 1454.0 3.755 320.388 1085201000045 1454.0 3.847 316.709 76.866 1085201000046 2459.0 2.675 16.505 1085201000047 2459.0 2.768 31.068 1085201000048 2459.0 2.870 40.777 9.709 1085201000049 2459.0 2.973 46.602 1085201000050 2459.0 3.075 50.485 1085201000051 2459.0 3.168 62.136 1085201000052 2459.0 3.260 68.932 1085201000053 2459.0 3.383 82.524 1085201000054 2459.0 3.556 73.786 1085201000055 2459.0 3.667 57.282 1085201000056 2459.0 3.760 70.874 1085201000057 2459.0 3.853 81.553 16.505 1085201000058 2775.0 2.872 44.330 1085201000059 2775.0 2.974 81.120 17.894 1085201000060 2775.0 3.086 108.433 1085201000061 2775.0 3.179 126.281 1085201000062 2775.0 3.291 144.120 1085201000063 2775.0 3.383 136.706 1085201000064 2775.0 3.476 144.028 1085201000065 2775.0 3.578 141.872 1085201000066 2775.0 3.670 135.510 1085201000067 2775.0 3.791 135.450 1085201000068 2775.0 3.874 134.356 14.737 1085201000069 2902.0 3.000 28.646 26.550 1085201000070 2902.0 3.073 44.716 1085201000071 2902.0 3.165 104.803 1085201000072 2902.0 3.257 92.926 1085201000073 2902.0 3.358 115.983 1085201000074 2902.0 3.459 115.284 1085201000075 2902.0 3.560 135.546 1085201000076 2902.0 3.661 104.105 1085201000077 2902.0 3.761 125.764 1085201000078 2902.0 3.862 96.419 49.607 1085201000079 2942.0 2.986 42.130 1085201000080 2942.0 3.053 94.746 1085201000081 2942.0 3.161 106.485 1085201000082 2942.0 3.250 129.311 1085201000083 2942.0 3.352 121.660 1085201000084 2942.0 3.454 112.622 1085201000085 2942.0 3.543 133.371 1085201000086 2942.0 3.643 143.035 1085201000087 2942.0 3.848 120.805 51.941 1085201000088 2942.0 3.943 165.793 1085201000089 3038.0 3.154 36.278 9.622 1085201000090 3038.0 3.244 60.807 1085201000091 3038.0 3.346 64.384 1085201000092 3038.0 3.447 71.454 1085201000093 3038.0 3.548 82.891 1085201000094 3038.0 3.650 73.368 1085201000095 3038.0 3.742 86.544 1085201000096 3038.0 3.842 99.727 13.115 1085201000097 3240.0 3.488 8.348 1085201000098 3240.0 3.556 34.435 1085201000099 3240.0 3.650 46.435 1085201000100 3240.0 3.762 58.435 5.739 1085201000101 3240.0 3.863 61.565 1085201000102 3264.0 3.342 22.957 1085201000103 3264.0 3.464 48.696 1085201000104 3264.0 3.559 68.870 1085201000105 3264.0 3.650 69.565 1085201000106 3264.0 3.762 80.000 1085201000107 3264.0 3.866 108.522 13.913 1085201000108 3264.0 3.957 100.174 1085201000109 3532.0 3.647 8.341 1085201000110 3532.0 3.756 15.848 1085201000111 3532.0 3.855 12.350 3.667 1085201000112 3532.0 3.955 10.337 1085201000113 ENDDATA 91 0 1085201000114 ENDSUBENT 113 0 1085201099999 SUBENT 10852011 20210827 14911085201100001 BIB 4 17 1085201100002 REACTION (28-NI-60(N,X)0-G-0,PAR,SIG) 1085201100003 ANALYSIS Total cross sections were deduced from the 125 deg 1085201100004 gamma-ray production cross sections. In the 1085201100005 conversion of 125-deg gamma-ray production cross 1085201100006 sections, dsigma/dOmega (125 deg) , to total gamma 1085201100007 ray production cross sections preparatory to the 1085201100008 inference of neutron excitation functions, an 1085201100009 integral of the gamma radiation over all angles must 1085201100010 be taken. The result can be expressed as sigmaT = 1085201100011 4*pi*(dsigma/dOmega 125 deg) M. The factor M takes 1085201100012 into account the fourth-order Legendre polynomial's 1085201100013 effect on the 125-deg cross section. (The 1085201100014 second-order Legendre polynomial is zero at this 1085201100015 angle.) 1085201100016 STATUS (DEP,10852007) 1085201100017 (CURVE) Fig. 7, page 200 of J,NSE,72,191,1979. 1085201100018 HISTORY (20210827A) BP: Digitized data. 1085201100019 ENDBIB 17 0 1085201100020 NOCOMMON 0 0 1085201100021 DATA 4 97 1085201100022 E EN DATA DATA-ERR 1085201100023 KEV MEV MB MB 1085201100024 1332.0 1.430 265.670 1085201100025 1332.0 1.527 438.285 34.592 1085201100026 1332.0 1.634 420.618 1085201100027 1332.0 1.749 459.133 1085201100028 1332.0 1.929 579.574 1085201100029 1332.0 2.151 652.309 1085201100030 1332.0 2.357 647.269 1085201100031 1332.0 2.447 755.053 1085201100032 1332.0 2.538 724.471 1085201100033 1332.0 2.564 642.230 1085201100034 1332.0 2.663 607.295 86.451 1085201100035 1332.0 2.770 654.486 1085201100036 1332.0 2.878 606.551 1085201100037 1332.0 2.976 623.503 1085201100038 1332.0 3.084 575.568 1085201100039 1332.0 3.182 683.323 1085201100040 1332.0 3.281 644.064 1085201100041 1332.0 3.389 604.777 1085201100042 1332.0 3.488 626.053 1085201100043 1332.0 3.588 543.554 1085201100044 1332.0 3.696 499.943 1085201100045 1332.0 3.779 465.065 108.128 1085201100046 1332.0 3.887 391.186 1085201100047 2159.0 2.368 131.425 1085201100048 2159.0 2.449 195.474 1085201100049 2159.0 2.546 229.784 1085201100050 2159.0 2.670 217.359 17.019 1085201100051 2159.0 2.768 232.522 1085201100052 2159.0 2.874 258.346 1085201100053 2159.0 2.973 235.216 1085201100054 2159.0 3.073 216.340 1085201100055 2159.0 3.170 261.288 1085201100056 2159.0 3.269 259.432 1085201100057 2159.0 3.376 236.325 1085201100058 2159.0 3.474 274.890 1085201100059 2159.0 3.572 281.544 1085201100060 2159.0 3.679 264.818 1085201100061 2159.0 3.753 267.149 40.511 1085201100062 2159.0 3.877 254.724 1085201100063 2285.0 2.454 29.915 1085201100064 2285.0 2.560 52.980 1085201100065 2285.0 2.650 63.904 8.908 1085201100066 2285.0 2.748 71.644 1085201100067 2285.0 2.863 66.633 1085201100068 2285.0 2.979 60.984 1085201100069 2285.0 3.077 74.469 1085201100070 2285.0 3.175 77.741 1085201100071 2285.0 3.274 68.249 1085201100072 2285.0 3.365 56.198 1085201100073 2285.0 3.480 68.419 1085201100074 2285.0 3.579 59.565 1085201100075 2285.0 3.677 64.115 1085201100076 2285.0 3.776 62.920 1085201100077 2285.0 3.875 56.619 13.430 1085201100078 2285.0 3.974 50.956 1085201100079 2506.0 2.557 28.502 1085201100080 2506.0 2.669 36.393 1085201100081 2506.0 2.773 50.258 12.803 1085201100082 2506.0 2.867 70.952 1085201100083 2506.0 2.955 82.223 1085201100084 2506.0 3.080 65.321 1085201100085 2506.0 3.179 106.558 1085201100086 2506.0 3.269 103.288 1085201100087 2506.0 3.362 129.114 1085201100088 2506.0 3.456 156.652 1085201100089 2506.0 3.561 160.252 48.799 1085201100090 2506.0 3.656 175.813 1085201100091 2506.0 3.747 166.555 1085201100092 2506.0 3.860 170.169 1085201100093 2626.0 2.765 40.419 1085201100094 2626.0 2.865 61.008 10.258 1085201100095 2626.0 2.990 80.755 1085201100096 2626.0 3.083 117.596 1085201100097 2626.0 3.181 111.661 1085201100098 2626.0 3.289 127.977 1085201100099 2626.0 3.388 134.877 1085201100100 2626.0 3.479 152.894 1085201100101 2626.0 3.576 139.260 1085201100102 2626.0 3.676 153.004 1085201100103 2626.0 3.781 141.941 16.270 1085201100104 2626.0 3.888 145.423 1085201100105 3124.0 3.281 53.536 1085201100106 3124.0 3.364 89.517 1085201100107 3124.0 3.488 112.686 1085201100108 3124.0 3.587 96.485 18.837 1085201100109 3124.0 3.686 105.951 1085201100110 3124.0 3.785 117.985 1085201100111 3124.0 3.901 147.994 1085201100112 3318.0 3.554 30.418 1085201100113 3318.0 3.644 28.065 1085201100114 3318.0 3.745 35.392 17.423 1085201100115 3318.0 3.841 35.190 1085201100116 3318.0 3.939 34.129 1085201100117 3394.0 3.548 23.676 1085201100118 3394.0 3.652 32.432 1085201100119 3394.0 3.747 43.135 1085201100120 3394.0 3.836 47.351 12.000 1085201100121 ENDDATA 99 0 1085201100122 ENDSUBENT 121 0 1085201199999 SUBENT 10852012 20210827 14911085201200001 BIB 4 17 1085201200002 REACTION (28-NI-62(N,X)0-G-0,PAR,SIG) 1085201200003 ANALYSIS Total cross sections were deduced from the 125 deg 1085201200004 gamma-ray production cross sections. In the 1085201200005 conversion of 125-deg gamma-ray production cross 1085201200006 sections, dsigma/dOmega (125 deg) , to total gamma 1085201200007 ray production cross sections preparatory to the 1085201200008 inference of neutron excitation functions, an 1085201200009 integral of the gamma radiation over all angles must 1085201200010 be taken. The result can be expressed as sigmaT = 1085201200011 4*pi*(dsigma/dOmega 125 deg) M. The factor M takes 1085201200012 into account the fourth-order Legendre polynomial's 1085201200013 effect on the 125-deg cross section. (The 1085201200014 second-order Legendre polynomial is zero at this 1085201200015 angle.) 1085201200016 STATUS (DEP,10852008) 1085201200017 (CURVE) Fig. 7, page 200 of J,NSE,72,191,1979. 1085201200018 HISTORY (20210827A) BP: Digitized data. 1085201200019 ENDBIB 17 0 1085201200020 NOCOMMON 0 0 1085201200021 DATA 4 8 1085201200022 E EN DATA DATA-ERR 1085201200023 KEV MEV MB MB 1085201200024 1173.0 1.329 265.017 43.010 1085201200025 1173.0 1.442 368.564 1085201200026 1173.0 1.539 390.346 1085201200027 1173.0 1.737 683.389 1085201200028 1173.0 1.948 735.601 1085201200029 1173.0 2.143 753.360 1085201200030 1173.0 2.331 706.581 1085201200031 1173.0 2.543 659.872 81.695 1085201200032 ENDDATA 10 0 1085201200033 ENDSUBENT 32 0 1085201299999 SUBENT 10852013 20210827 14911085201300001 BIB 4 17 1085201300002 REACTION (28-NI-64(N,X)0-G-0,PAR,SIG) 1085201300003 ANALYSIS Total cross sections were deduced from the 125 deg 1085201300004 gamma-ray production cross sections. In the 1085201300005 conversion of 125-deg gamma-ray production cross 1085201300006 sections, dsigma/dOmega (125 deg) , to total gamma 1085201300007 ray production cross sections preparatory to the 1085201300008 inference of neutron excitation functions, an 1085201300009 integral of the gamma radiation over all angles must 1085201300010 be taken. The result can be expressed as sigmaT = 1085201300011 4*pi*(dsigma/dOmega 125 deg) M. The factor M takes 1085201300012 into account the fourth-order Legendre polynomial's 1085201300013 effect on the 125-deg cross section. (The 1085201300014 second-order Legendre polynomial is zero at this 1085201300015 angle.) 1085201300016 STATUS (DEP,10852009) 1085201300017 (CURVE) Fig. 7, page 200 of J,NSE,72,191,1979. 1085201300018 HISTORY (20210827A) BP: Digitized data. 1085201300019 ENDBIB 17 0 1085201300020 NOCOMMON 0 0 1085201300021 DATA 4 14 1085201300022 E EN DATA DATA-ERR 1085201300023 KEV MEV MB MB 1085201300024 1348.0 1.747 380.672 200.023 1085201300025 1348.0 1.953 615.865 1085201300026 1348.0 2.157 582.958 1085201300027 1348.0 2.272 541.043 1085201300028 1348.0 2.360 601.109 1085201300029 1348.0 2.472 703.859 1085201300030 1348.0 2.564 563.947 1085201300031 1348.0 2.669 594.319 1085201300032 1348.0 2.763 752.292 1085201300033 1348.0 2.872 595.451 1085201300034 1348.0 2.966 783.207 1085201300035 1348.0 3.087 813.670 1085201300036 1348.0 3.187 724.861 1085201300037 1348.0 3.286 636.053 297.929 1085201300038 ENDDATA 16 0 1085201300039 ENDSUBENT 38 0 1085201399999 NOSUBENT 10852014 20210827 14911085201400001 SUBENT 10852015 20210915 14911085201500001 BIB 4 12 1085201500002 REACTION (28-NI-0(N,INL)28-NI-0,,SIG) 1085201500003 ANALYSIS Values presented here as natural cross sections 1085201500004 include all the inferred neutron inelastic cross 1085201500005 sections of significance in all nickel isotopes with 1085201500006 the exception of that from the 1.19% abundant 61Ni 1085201500007 component. 1085201500008 STATUS (DEP,10852006) 1085201500009 (DEP,10852007) 1085201500010 (DEP,10852008) 1085201500011 (DEP,10852009) 1085201500012 (CURVE) Fig. 8, page 201 of J,NSE,72,191,1979. 1085201500013 HISTORY (20210827C) BP: Digitized data. 1085201500014 ENDBIB 12 0 1085201500015 NOCOMMON 0 0 1085201500016 DATA 3 23 1085201500017 EN DATA DATA-ERR 1085201500018 MEV MB MB 1085201500019 1.442 80.007 1085201500020 1.541 230.859 1085201500021 1.636 340.248 1085201500022 1.741 421.310 26.146 1085201500023 1.943 507.054 1085201500024 2.140 570.970 1085201500025 2.347 624.008 30.463 1085201500026 2.452 659.261 1085201500027 2.535 681.349 1085201500028 2.553 703.224 1085201500029 2.664 714.496 1085201500030 2.760 778.076 43.689 1085201500031 2.870 822.070 1085201500032 2.957 841.992 1085201500033 3.073 820.558 1085201500034 3.159 890.652 74.167 1085201500035 3.270 904.106 1085201500036 3.362 943.676 1085201500037 3.471 1009.483 1085201500038 3.568 1014.166 82.893 1085201500039 3.666 981.765 1085201500040 3.767 1017.002 1085201500041 3.869 988.979 78.530 1085201500042 ENDDATA 25 0 1085201500043 ENDSUBENT 42 0 1085201599999 ENDENTRY 15 0 1085299999999