ENTRY F1204 20131007 F052F120400000001 SUBENT F1204001 20131007 F052F120400100001 BIB 6 7 F120400100002 TITLE Neutron single-particle states in Nd-143 and Sm-145. F120400100003 AUTHOR (P.R.Christensen,B.Herskind,R.R.Borchers,L.Westgaard) F120400100004 INSTITUTE (2DENNBI,1USAWIS,2SWDSWR) F120400100005 REFERENCE (J,NP/A,102,481,1967) F120400100006 #doi:10.1016/0375-9474(67)90387-9 F120400100007 FACILITY (VDGT,2DENNBI) F120400100008 HISTORY (20131007C) F120400100009 ENDBIB 7 0 F120400100010 COMMON 1 3 F120400100011 EN F120400100012 MEV F120400100013 12. F120400100014 ENDCOMMON 3 0 F120400100015 ENDSUBENT 14 0 F120400199999 SUBENT F1204002 20131007 F052F120400200001 BIB 6 14 F120400200002 REACTION (60-ND-142(D,EL)60-ND-142,,DA,,RTH) F120400200003 DETECTOR (MAGSP,SILI,SOLST) The elastically scattered particles F120400200004 were detected in a 2 mm thick Si(Li) counter after F120400200005 being analysed in a high resolution, magnetic F120400200006 spectrograph. The solid state counter was placed in theF120400200007 focal plane of the spectrograph and had a slit opening F120400200008 sufficiently large to cover the whole elastic group. F120400200009 SAMPLE Evaporated targets of a thickness of approximately F120400200010 100 mu-g/cm2 of Nd-142 (>97%) supported by a thin F120400200011 carbon film were used. F120400200012 METHOD (BCINT) F120400200013 ERR-ANALYS (ANG-ERR-D) Angle digitizing error F120400200014 (ERR-DIG) Data digitizing error F120400200015 STATUS (CURVE) Fig.1 F120400200016 ENDBIB 14 0 F120400200017 COMMON 2 3 F120400200018 ANG-ERR-D ERR-DIG F120400200019 ADEG PER-CENT F120400200020 0.34 0.78 F120400200021 ENDCOMMON 3 0 F120400200022 DATA 2 20 F120400200023 ANG DATA F120400200024 ADEG NO-DIM F120400200025 19.70 1.0085 F120400200026 24.90 1.0366 F120400200027 29.67 1.0131 F120400200028 34.86 0.9573 F120400200029 40.03 0.8177 F120400200030 45.21 0.7183 F120400200031 50.16 0.6034 F120400200032 55.13 0.5638 F120400200033 59.67 0.5123 F120400200034 65.51 0.4978 F120400200035 70.26 0.4349 F120400200036 74.78 0.3757 F120400200037 79.96 0.3227 F120400200038 89.89 0.2709 F120400200039 99.86 0.2631 F120400200040 110.00 0.2136 F120400200041 119.94 0.1743 F120400200042 130.33 0.1665 F120400200043 139.64 0.1581 F120400200044 150.24 0.1436 F120400200045 ENDDATA 22 0 F120400200046 ENDSUBENT 45 0 F120400299999 SUBENT F1204003 20131007 F052F120400300001 BIB 6 14 F120400300002 REACTION (62-SM-144(D,EL)62-SM-144,,DA,,RTH) F120400300003 DETECTOR (MAGSP,SILI,SOLST) The elastically scattered particles F120400300004 were detected in a 2 mm thick Si(Li) counter after F120400300005 being analysed in a high resolution, magnetic F120400300006 spectrograph. The solid state counter was placed in theF120400300007 focal plane of the spectrograph and had a slit opening F120400300008 sufficiently large to cover the whole elastic group. F120400300009 SAMPLE Evaporated targets of a thickness of approximately F120400300010 100 mu-g/cm2 of Sm-144 (>94%) supported by a thin F120400300011 carbon film were used. F120400300012 METHOD (BCINT) F120400300013 ERR-ANALYS (ANG-ERR-D) Angle digitizing error F120400300014 (ERR-DIG) Data digitizing error F120400300015 STATUS (CURVE) Fig.2 F120400300016 ENDBIB 14 0 F120400300017 COMMON 2 3 F120400300018 ANG-ERR-D ERR-DIG F120400300019 ADEG PER-CENT F120400300020 0.55 0.84 F120400300021 ENDCOMMON 3 0 F120400300022 DATA 2 9 F120400300023 ANG DATA F120400300024 ADEG NO-DIM F120400300025 19.41 1.0122 F120400300026 29.40 1.0182 F120400300027 39.39 0.8113 F120400300028 54.60 0.5389 F120400300029 64.37 0.4811 F120400300030 89.56 0.2742 F120400300031 99.11 0.2681 F120400300032 120.18 0.1812 F120400300033 149.92 0.1547 F120400300034 ENDDATA 11 0 F120400300035 ENDSUBENT 34 0 F120400399999 SUBENT F1204004 20131007 F052F120400400001 BIB 5 14 F120400400002 REACTION (62-SM-144(D,P)62-SM-145,PAR,DA) F120400400003 DETECTOR (SILI,SIBAR) A 30 cm scattering chamber equipped with aF120400400004 horizontal turntable with a 2 mm thick Li(Si) counter F120400400005 was used. The turntable was constructed in such a way F120400400006 that the counter could be cooled. Another detector, a F120400400007 0.8 mm thick surface barrier counter, was placed at a F120400400008 fixed angle, 90 degr., and served as a monitor by F120400400009 recording the elastically scattered deuterons. F120400400010 SAMPLE The targets were self-supporting, metallic foils of F120400400011 Sm-144 (> 94%)with a thickness of approximately F120400400012 1 mg/cm2. F120400400013 ERR-ANALYS (ANG-ERR-D) Angle digitizing error F120400400014 (ERR-DIG) Data digitizing error F120400400015 STATUS (CURVE) Fig.4 F120400400016 ENDBIB 14 0 F120400400017 COMMON 3 3 F120400400018 EN-RSL ANG-ERR-D ERR-DIG F120400400019 KEV ADEG PER-CENT F120400400020 45. 0.36 1.84 F120400400021 ENDCOMMON 3 0 F120400400022 DATA 3 84 F120400400023 E-LVL ANG DATA F120400400024 KEV ADEG MB/SR F120400400025 0. 27.80 1.1032 F120400400026 0. 44.11 1.6832 F120400400027 0. 48.63 1.8649 F120400400028 0. 58.70 1.3897 F120400400029 0. 68.78 1.0356 F120400400030 0. 78.95 0.8973 F120400400031 0. 88.21 0.7511 F120400400032 0. 99.22 0.5998 F120400400033 0. 108.79 0.4028 F120400400034 0. 118.44 0.3108 F120400400035 0. 128.18 0.2789 F120400400036 0. 138.78 0.2361 F120400400037 0. 148.05 0.2023 F120400400038 894. 29.35 2.0784 F120400400039 894. 45.29 2.8497 F120400400040 894. 49.85 3.1498 F120400400041 894. 60.24 1.6127 F120400400042 894. 70.05 1.3911 F120400400043 894. 80.11 0.8625 F120400400044 894. 91.01 0.4814 F120400400045 894. 100.17 0.3039 F120400400046 894. 110.35 0.2281 F120400400047 894. 120.00 0.1516 F120400400048 894. 129.97 0.0804 F120400400049 894. 140.14 0.0604 F120400400050 894. 150.37 0.0494 F120400400051 1110. 27.72 0.0991 F120400400052 1110. 38.52 0.0739 F120400400053 1110. 43.06 0.1044 F120400400054 1110. 47.41 0.0973 F120400400055 1110. 57.91 0.0970 F120400400056 1110. 87.66 0.0949 F120400400057 1110. 116.39 0.0673 F120400400058 1110. 136.48 0.0616 F120400400059 1110. 146.84 0.0449 F120400400060 1425. 28.03 0.0824 F120400400061 1425. 37.85 0.1320 F120400400062 1425. 43.09 0.1288 F120400400063 1425. 47.23 0.2115 F120400400064 1425. 57.63 0.1635 F120400400065 1425. 87.65 0.1033 F120400400066 1425. 116.89 0.0852 F120400400067 1425. 137.77 0.0613 F120400400068 1425. 147.43 0.0670 F120400400069 1610. 38.34 1.7424 F120400400070 1610. 43.63 1.4595 F120400400071 1610. 48.64 1.6141 F120400400072 1610. 58.78 0.5572 F120400400073 1610. 89.21 0.2066 F120400400074 1610. 118.93 0.0506 F120400400075 1610. 139.04 0.0199 F120400400076 1610. 149.31 0.0361 F120400400077 1660. 39.64 0.6406 F120400400078 1660. 44.40 0.4758 F120400400079 1660. 49.73 0.8654 F120400400080 1660. 59.48 0.3381 F120400400081 1660. 89.65 0.1737 F120400400082 1660. 119.65 0.0340 F120400400083 1660. 139.87 0.0328 F120400400084 1660. 149.12 0.0238 F120400400085 1788. 38.58 0.0389 F120400400086 1788. 47.86 0.0826 F120400400087 1788. 88.90 0.0362 F120400400088 1788. 148.83 0.0263 F120400400089 1855. 39.63 0.0714 F120400400090 1855. 49.26 0.1055 F120400400091 1855. 89.08 0.0094 F120400400092 1855. 149.04 0.0018 F120400400093 1880. 39.01 0.3036 F120400400094 1880. 49.65 0.2746 F120400400095 1880. 89.77 0.1271 F120400400096 1880. 149.38 0.0470 F120400400097 1978. 39.40 0.6826 F120400400098 1978. 44.33 0.6730 F120400400099 1978. 49.83 0.7419 F120400400100 1978. 59.78 0.4929 F120400400101 1978. 89.24 0.2446 F120400400102 1978. 148.81 0.0737 F120400400103 2000. 40.20 0.6937 F120400400104 2000. 44.09 0.5502 F120400400105 2000. 49.61 0.7496 F120400400106 2000. 59.59 0.4495 F120400400107 2000. 90.67 0.3529 F120400400108 2000. 149.80 0.1102 F120400400109 ENDDATA 86 0 F120400400110 ENDSUBENT 109 0 F120400499999 SUBENT F1204005 20131007 F052F120400500001 BIB 5 14 F120400500002 REACTION (60-ND-142(D,P)60-ND-143,PAR,DA) F120400500003 DETECTOR (SILI,SIBAR) A 30 cm scattering chamber equipped with aF120400500004 horizontal turntable with a 2 mm thick Li(Si) counter F120400500005 was used. The turntable was constructed in such a way F120400500006 that the counter could be cooled. Another detector, a F120400500007 0.8 mm thick surface barrier counter, was placed at a F120400500008 fixed angle, 90 degr., and served as a monitor by F120400500009 recording the elastically scattered deuterons. F120400500010 SAMPLE The targets were self-supporting, metallic foils of F120400500011 Nd-142 (> 97%) with a thickness of approximately F120400500012 1 mg/cm2. F120400500013 ERR-ANALYS (ANG-ERR-D) Angle digitizing error F120400500014 (ERR-DIG) Data digitizing error F120400500015 STATUS (CURVE) Fig.7 F120400500016 ENDBIB 14 0 F120400500017 COMMON 3 3 F120400500018 EN-RSL ANG-ERR-D ERR-DIG F120400500019 KEV ADEG PER-CENT F120400500020 45. 0.25 1.34 F120400500021 ENDCOMMON 3 0 F120400500022 DATA 3 203 F120400500023 E-LVL ANG DATA F120400500024 KEV ADEG MB/SR F120400500025 0. 29.51 1.9768 F120400500026 0. 39.05 2.0152 F120400500027 0. 44.49 2.0108 F120400500028 0. 48.99 1.8944 F120400500029 0. 53.50 1.8265 F120400500030 0. 58.91 1.7401 F120400500031 0. 63.38 1.5653 F120400500032 0. 68.78 1.4572 F120400500033 0. 78.58 1.0998 F120400500034 0. 88.96 1.0100 F120400500035 0. 98.76 0.7535 F120400500036 0. 109.39 0.5006 F120400500037 0. 118.35 0.4194 F120400500038 0. 124.18 0.3770 F120400500039 0. 129.12 0.3470 F120400500040 0. 138.97 0.2839 F120400500041 0. 148.83 0.2351 F120400500042 740. 29.68 2.3643 F120400500043 740. 40.07 2.2990 F120400500044 740. 44.63 2.4341 F120400500045 740. 49.56 2.2629 F120400500046 740. 54.87 1.8472 F120400500047 740. 59.34 1.6975 F120400500048 740. 65.14 1.5047 F120400500049 740. 69.27 1.6315 F120400500050 740. 79.43 1.1003 F120400500051 740. 89.15 0.7599 F120400500052 740. 98.88 0.5248 F120400500053 740. 109.62 0.4325 F120400500054 740. 118.98 0.3483 F120400500055 740. 124.43 0.3558 F120400500056 740. 129.65 0.2551 F120400500057 740. 138.93 0.1783 F120400500058 740. 149.22 0.1487 F120400500059 1226. 28.34 0.0216 F120400500060 1226. 42.78 0.0841 F120400500061 1226. 47.42 0.1244 F120400500062 1226. 53.20 0.1132 F120400500063 1226. 57.71 0.1212 F120400500064 1226. 62.67 0.1312 F120400500065 1226. 77.04 0.1451 F120400500066 1226. 87.70 0.1135 F120400500067 1226. 97.47 0.0919 F120400500068 1226. 106.85 0.0856 F120400500069 1226. 117.17 0.0894 F120400500070 1226. 126.52 0.0776 F120400500071 1226. 136.34 0.0714 F120400500072 1226. 146.14 0.0619 F120400500073 1305. 29.53 1.1096 F120400500074 1305. 39.56 1.2549 F120400500075 1305. 44.56 1.2965 F120400500076 1305. 49.88 1.1006 F120400500077 1305. 54.74 0.9026 F120400500078 1305. 59.61 0.7576 F120400500079 1305. 64.56 0.7219 F120400500080 1305. 70.44 0.7286 F120400500081 1305. 79.82 0.5965 F120400500082 1305. 89.50 0.3831 F120400500083 1305. 99.30 0.2994 F120400500084 1305. 109.67 0.2782 F120400500085 1305. 119.88 0.2028 F120400500086 1305. 124.28 0.1664 F120400500087 1305. 129.13 0.1349 F120400500088 1305. 138.98 0.1143 F120400500089 1305. 148.86 0.1014 F120400500090 1405. 41.81 0.1650 F120400500091 1405. 46.35 0.2078 F120400500092 1405. 50.83 0.2100 F120400500093 1405. 56.66 0.2147 F120400500094 1405. 61.11 0.1911 F120400500095 1405. 76.34 0.1885 F120400500096 1405. 86.14 0.1528 F120400500097 1405. 96.40 0.1298 F120400500098 1405. 106.24 0.1223 F120400500099 1405. 116.09 0.1207 F120400500100 1405. 126.32 0.0903 F120400500101 1405. 136.15 0.0822 F120400500102 1405. 146.41 0.0706 F120400500103 1555. 39.46 0.5581 F120400500104 1555. 44.82 0.4913 F120400500105 1555. 49.46 0.5753 F120400500106 1555. 54.73 0.4366 F120400500107 1555. 59.24 0.4212 F120400500108 1555. 64.15 0.3708 F120400500109 1555. 70.08 0.3917 F120400500110 1555. 78.97 0.2869 F120400500111 1555. 89.37 0.2761 F120400500112 1555. 99.18 0.2092 F120400500113 1555. 108.93 0.1429 F120400500114 1555. 118.80 0.1200 F120400500115 1555. 123.42 0.1374 F120400500116 1555. 129.19 0.1129 F120400500117 1555. 138.67 0.1051 F120400500118 1555. 149.33 0.0726 F120400500119 1740. 43.35 0.0554 F120400500120 1740. 46.97 0.0674 F120400500121 1740. 52.38 0.0830 F120400500122 1740. 57.32 0.0921 F120400500123 1740. 62.70 0.0931 F120400500124 1740. 77.40 0.0598 F120400500125 1740. 87.71 0.0633 F120400500126 1740. 98.45 0.0596 F120400500127 1740. 108.32 0.0624 F120400500128 1740. 117.69 0.0518 F120400500129 1740. 127.51 0.0445 F120400500130 1740. 137.33 0.0365 F120400500131 1740. 148.49 0.0292 F120400500132 1851. 43.52 0.0743 F120400500133 1851. 48.48 0.6982 F120400500134 1851. 53.79 0.5545 F120400500135 1851. 59.22 0.5402 F120400500136 1851. 64.14 0.4781 F120400500137 1851. 78.96 0.3693 F120400500138 1851. 89.29 0.3071 F120400500139 1851. 98.62 0.2186 F120400500140 1851. 108.43 0.1612 F120400500141 1851. 118.38 0.1530 F120400500142 1851. 128.73 0.1335 F120400500143 1851. 138.62 0.1138 F120400500144 1851. 148.89 0.0859 F120400500145 1911. 28.94 0.6396 F120400500146 1911. 43.78 0.5311 F120400500147 1911. 48.78 0.5420 F120400500148 1911. 53.29 0.5231 F120400500149 1911. 59.12 0.4716 F120400500150 1911. 64.50 0.4350 F120400500151 1911. 78.74 0.2919 F120400500152 1911. 88.24 0.2811 F120400500153 1911. 99.46 0.2391 F120400500154 1911. 109.22 0.1739 F120400500155 1911. 119.11 0.1531 F120400500156 1911. 129.04 0.1441 F120400500157 1911. 139.82 0.1239 F120400500158 1911. 149.08 0.0853 F120400500159 2016. 53.56 0.1124 F120400500160 2016. 58.99 0.1108 F120400500161 2016. 63.53 0.1106 F120400500162 2016. 79.22 0.0782 F120400500163 2016. 89.16 0.0722 F120400500164 2016. 98.99 0.0538 F120400500165 2016. 109.21 0.0358 F120400500166 2016. 119.14 0.0327 F120400500167 2016. 129.03 0.0273 F120400500168 2016. 139.42 0.0252 F120400500169 2016. 149.80 0.0229 F120400500170 2127. 29.70 0.3045 F120400500171 2127. 44.66 0.3173 F120400500172 2127. 54.88 0.2366 F120400500173 2127. 59.74 0.1971 F120400500174 2127. 65.14 0.1897 F120400500175 2127. 80.26 0.1251 F120400500176 2127. 89.64 0.1040 F120400500177 2127. 99.35 0.0705 F120400500178 2127. 110.01 0.0519 F120400500179 2127. 119.49 0.0499 F120400500180 2127. 129.28 0.0390 F120400500181 2127. 138.60 0.0291 F120400500182 2183. 28.84 0.2587 F120400500183 2183. 44.19 0.2256 F120400500184 2183. 54.53 0.1857 F120400500185 2183. 59.07 0.1876 F120400500186 2183. 62.69 0.1852 F120400500187 2183. 79.74 0.1256 F120400500188 2183. 89.69 0.1193 F120400500189 2183. 98.67 0.0994 F120400500190 2183. 109.38 0.0684 F120400500191 2183. 119.71 0.0549 F120400500192 2183. 129.68 0.0541 F120400500193 2183. 139.62 0.0502 F120400500194 2183. 149.88 0.0354 F120400500195 2250. 44.17 0.4868 F120400500196 2250. 54.48 0.4218 F120400500197 2250. 58.88 0.3472 F120400500198 2250. 79.51 0.2635 F120400500199 2250. 89.36 0.2235 F120400500200 2250. 99.05 0.1498 F120400500201 2250. 109.35 0.1257 F120400500202 2250. 118.75 0.1089 F120400500203 2250. 129.01 0.0866 F120400500204 2250. 138.43 0.0767 F120400500205 2250. 149.06 0.0537 F120400500206 2319. 43.61 0.2563 F120400500207 2319. 59.32 0.2087 F120400500208 2319. 64.69 0.1897 F120400500209 2319. 79.42 0.1391 F120400500210 2319. 89.10 0.0899 F120400500211 2319. 99.38 0.0733 F120400500212 2319. 109.61 0.0558 F120400500213 2319. 119.49 0.0500 F120400500214 2319. 128.75 0.0339 F120400500215 2319. 138.69 0.0334 F120400500216 2319. 148.83 0.0218 F120400500217 2363. 44.94 0.4669 F120400500218 2363. 58.30 0.3492 F120400500219 2363. 64.59 0.3281 F120400500220 2363. 79.77 0.2480 F120400500221 2363. 90.36 0.1729 F120400500222 2363. 99.59 0.1193 F120400500223 2363. 108.97 0.1018 F120400500224 2363. 118.32 0.0829 F120400500225 2363. 129.45 0.0643 F120400500226 2363. 138.75 0.0487 F120400500227 2363. 148.91 0.0352 F120400500228 ENDDATA 205 0 F120400500229 ENDSUBENT 228 0 F120400599999 SUBENT F1204006 20131007 F052F120400600001 BIB 4 12 F120400600002 REACTION (62-SM-144(D,P)62-SM-145,PAR,DA) F120400600003 DETECTOR (SILI,SIBAR) A 30 cm scattering chamber equipped with aF120400600004 horizontal turntable with a 2 mm thick Li(Si) counter F120400600005 was used. The turntable was constructed in such a way F120400600006 that the counter could be cooled. Another detector, a F120400600007 0.8 mm thick surface barrier counter, was placed at a F120400600008 fixed angle, 90 degr., and served as a monitor by F120400600009 recording the elastically scattered deuterons. F120400600010 SAMPLE The targets were self-supporting, metallic foils of F120400600011 Sm-144 (> 94%)with a thickness of approximately F120400600012 1 mg/cm2. F120400600013 STATUS (TABLE) Tbl.2 p.485 F120400600014 ENDBIB 12 0 F120400600015 COMMON 2 3 F120400600016 ANG EN-RSL F120400600017 ADEG KEV F120400600018 50. 45. F120400600019 ENDCOMMON 3 0 F120400600020 DATA 2 18 F120400600021 E-LVL DATA F120400600022 MEV MB/SR F120400600023 0. 1.83 F120400600024 0.894 2.12 F120400600025 1.110 0.10 F120400600026 1.426 0.21 F120400600027 1.610 1.47 F120400600028 1.660 0.44 F120400600029 1.788 0.08 F120400600030 1.855 0.11 F120400600031 1.880 0.28 F120400600032 1.978 0.76 F120400600033 2.000 0.76 F120400600034 2.130 0.20 F120400600035 2.155 0.19 F120400600036 2.431 0.18 F120400600037 2.690 0.20 F120400600038 2.974 0.12 F120400600039 3.090 0.35 F120400600040 3.132 0.47 F120400600041 ENDDATA 20 0 F120400600042 ENDSUBENT 41 0 F120400699999 SUBENT F1204007 20131007 F052F120400700001 BIB 4 12 F120400700002 REACTION (60-ND-142(D,P)60-ND-143,PAR,DA) F120400700003 DETECTOR (SILI,SIBAR) A 30 cm scattering chamber equipped with aF120400700004 horizontal turntable with a 2 mm thick Li(Si) counter F120400700005 was used. The turntable was constructed in such a way F120400700006 that the counter could be cooled. Another detector, a F120400700007 0.8 mm thick surface barrier counter, was placed at a F120400700008 fixed angle, 90 degr., and served as a monitor by F120400700009 recording the elastically scattered deuterons. F120400700010 SAMPLE The targets were self-supporting, metallic foils of F120400700011 Nd-142 (> 97%) with a thickness of approximately F120400700012 1 mg/cm2. F120400700013 STATUS (TABLE) Tbl.3 p.490 F120400700014 ENDBIB 12 0 F120400700015 COMMON 1 3 F120400700016 EN-RSL F120400700017 KEV F120400700018 45. F120400700019 ENDCOMMON 3 0 F120400700020 DATA 3 20 F120400700021 ANG E-LVL DATA F120400700022 ADEG MEV MB/SR F120400700023 45. 0. 2.05 F120400700024 45. 0.740 2.47 F120400700025 45. 1.226 0.09 F120400700026 45. 1.305 1.31 F120400700027 45. 1.405 0.17 F120400700028 45. 1.555 0.50 F120400700029 45. 1.740 0.06 F120400700030 45. 1.851 0.75 F120400700031 45. 1.911 0.55 F120400700032 45. 2.127 0.32 F120400700033 45. 2.183 0.23 F120400700034 45. 2.250 0.49 F120400700035 45. 2.319 0.26 F120400700036 45. 2.363 0.46 F120400700037 45. 2.416 0.02 F120400700038 45. 2.459 0.01 F120400700039 45. 2.496 0.11 F120400700040 45. 2.529 0.55 F120400700041 45. 2.552 0.24 F120400700042 55. 2.016 0.11 F120400700043 ENDDATA 22 0 F120400700044 ENDSUBENT 43 0 F120400799999 SUBENT F1204008 20131007 F052F120400800001 BIB 4 9 F120400800002 REACTION (60-ND-143(D,INL)60-ND-143,PAR,DA) F120400800003 DETECTOR (MAGSP,PLATE) Photographic plates placed along the F120400800004 focal plane of the high resolution, magnetic F120400800005 spectrograph at three different angles 90, 125 and 150 F120400800006 degr. were used. F120400800007 SAMPLE An evaporated target of enriched Nd-143 (>91%) F120400800008 supported by a thin carbon backing was used. The F120400800009 thickness of the target was approximately 100 mu-g/cm2.F120400800010 STATUS (TABLE) Tbl.3 p.490 F120400800011 ENDBIB 9 0 F120400800012 NOCOMMON 0 0 F120400800013 DATA 3 57 F120400800014 ANG E-LVL DATA F120400800015 ADEG MEV MU-B/SR F120400800016 90. 0. 35500. F120400800017 90. 0.740 93.1 F120400800018 90. 1.226 95.5 F120400800019 90. 1.405 31.3 F120400800020 90. 1.432 87.1 F120400800021 90. 1.506 12.9 F120400800022 90. 1.555 21.4 F120400800023 90. 1.607 12.4 F120400800024 90. 1.740 21.2 F120400800025 90. 1.801 25.8 F120400800026 90. 1.851 21.6 F120400800027 90. 1.911 5.4 F120400800028 90. 1.995 26.1 F120400800029 90. 2.016 38.0 F120400800030 90. 2.074 19.8 F120400800031 90. 2.090 47.1 F120400800032 90. 2.127 2.3 F120400800033 90. 2.183 3.8 F120400800034 90. 2.250 54.0 F120400800035 125. 0.000 8890. F120400800036 125. 0.740 43.2 F120400800037 125. 1.226 51.6 F120400800038 125. 1.305 11. F120400800039 125. 1.405 17. F120400800040 125. 1.432 36.3 F120400800041 125. 1.506 9.4 F120400800042 125. 1.555 11.7 F120400800043 125. 1.607 9.8 F120400800044 125. 1.740 7.8 F120400800045 125. 1.801 15.2 F120400800046 125. 1.851 12.9 F120400800047 125. 1.911 9.5 F120400800048 125. 1.995 39. F120400800049 125. 2.016 46.7 F120400800050 125. 2.074 13.5 F120400800051 125. 2.090 33.7 F120400800052 125. 2.250 40.9 F120400800053 150. 0.000 5440. F120400800054 150. 0.740 41.8 F120400800055 150. 1.226 49.4 F120400800056 150. 1.305 17.6 F120400800057 150. 1.405 14. F120400800058 150. 1.432 38.1 F120400800059 150. 1.506 15.2 F120400800060 150. 1.555 26.9 F120400800061 150. 1.607 6.9 F120400800062 150. 1.740 4.2 F120400800063 150. 1.801 15.3 F120400800064 150. 1.851 11.4 F120400800065 150. 1.911 7.7 F120400800066 150. 1.995 20.5 F120400800067 150. 2.016 22.2 F120400800068 150. 2.074 12.5 F120400800069 150. 2.090 33.6 F120400800070 150. 2.127 4.8 F120400800071 150. 2.183 3.3 F120400800072 150. 2.250 39.8 F120400800073 ENDDATA 59 0 F120400800074 ENDSUBENT 73 0 F120400899999 ENDENTRY 8 0 F120499999999