ENTRY E2729 20230122 E272900000001 SUBENT E2729001 20230122 20230412 E272900100001 BIB 14 28 E272900100002 TITLE Production cross sections of samarium-153 and -145 via E272900100003 alpha-particle-induced reactions on natural neodymium E272900100004 AUTHOR (M.Aikawa, M.Sakaguchi, N.Ukon, Y.Komori, H.Haba, E272900100005 N.Otuka, S.Takacs) E272900100006 INSTITUTE (2JPNHOK,2JPNIPC,3ZZZIAE,3HUNDEB) E272900100007 (2JPNJPN) Advanced Clinical Research Center, Fukushima E272900100008 Medical University, Fukushima E272900100009 REFERENCE (J,ARI,187,110345,2022) E272900100010 MONITOR (22-TI-0(A,X)24-CR-51,,SIG) E272900100011 MONIT-REF (,A.Hermanne+,J,NDS,148,338,2018) E272900100012 (,S.M.Qaim+,R,IAEA-TECDOC-1211,2001) E272900100013 INC-SOURCE Beam intensity is 205 to 209 nA. E272900100014 SAMPLE - Chemical-form of target is element. E272900100015 - Physical-form of target is solid. E272900100016 - Target-thickness is 16.3 mg/cm2. E272900100017 METHOD (ACTIV) Irradiated for 33 min E272900100018 (GSPEC) E272900100019 FACILITY (ISOCY,2JPNIPC) AVF cyclotron E272900100020 DETECTOR (HPGE) E272900100021 ERR-ANALYS (ERR-T) Total uncertainty E272900100022 (ERR-1) beam intensity E272900100023 (ERR-2) gamma-ray intensity E272900100024 (ERR-3) detector efficiency E272900100025 (ERR-4) target thickness E272900100026 (ERR-5) target purity E272900100027 (ERR-S,0.4,5.5) Statistical uncertainty (0.4-5.5%) E272900100028 COMMENT EN-RSL: total energy loss in the target foils E272900100029 HISTORY (20220703C) MA E272900100030 ENDBIB 28 0 E272900100031 COMMON 5 3 E272900100032 ERR-1 ERR-2 ERR-3 ERR-4 ERR-5 E272900100033 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT E272900100034 5. 0.8 5. 2. 1. E272900100035 ENDCOMMON 3 0 E272900100036 ENDSUBENT 35 0 E272900199999 SUBENT E2729002 20230122 20230412 E272900200001 BIB 3 4 E272900200002 REACTION (60-ND-0(A,X)62-SM-153,CUM,SIG) E272900200003 DECAY-DATA (62-SM-153,46.284HR,DG,103.18012,0.2925) E272900200004 STATUS (TABLE) Tables 4-5 of Appl. Radiat. Isot. 187 (2022) E272900200005 110345. E272900200006 ENDBIB 4 0 E272900200007 NOCOMMON 0 0 E272900200008 DATA 5 10 E272900200009 EN EN-ERR EN-RSL DATA ERR-T E272900200010 MEV MEV MEV MB MB E272900200011 23.0 0.3 2.1 0.93 0.07 E272900200012 22.6 0.3 2.1 0.92 0.07 E272900200013 21.0 0.3 2.2 0.99 0.07 E272900200014 20.6 0.3 2.2 0.96 0.07 E272900200015 18.8 0.3 2.4 1.21 0.09 E272900200016 18.3 0.3 2.4 1.21 0.09 E272900200017 16.4 0.4 2.6 1.12 0.08 E272900200018 15.9 0.4 2.6 1.02 0.08 E272900200019 13.8 0.5 3.0 0.27 0.02 E272900200020 13.3 0.5 3.0 0.17 0.01 E272900200021 ENDDATA 12 0 E272900200022 ENDSUBENT 21 0 E272900299999 SUBENT E2729003 20230122 20230412 E272900300001 BIB 3 4 E272900300002 REACTION (60-ND-0(A,X)62-SM-145,,SIG) E272900300003 DECAY-DATA (62-SM-145,340.D,DG,61.2265,0.1215) E272900300004 STATUS (TABLE) Tables 4-5 of Appl. Radiat. Isot. 187 (2022) E272900300005 110345. E272900300006 ENDBIB 4 0 E272900300007 NOCOMMON 0 0 E272900300008 DATA 5 8 E272900300009 EN EN-ERR EN-RSL DATA ERR-T E272900300010 MEV MEV MEV MB MB E272900300011 23.0 0.3 2.1 168. 13. E272900300012 22.6 0.3 2.1 169. 13. E272900300013 21.0 0.3 2.2 171. 13. E272900300014 20.6 0.3 2.2 168. 13. E272900300015 18.8 0.3 2.4 102. 8. E272900300016 18.3 0.3 2.4 94. 7. E272900300017 16.4 0.4 2.6 22. 2. E272900300018 15.9 0.4 2.6 19. 2. E272900300019 ENDDATA 10 0 E272900300020 ENDSUBENT 19 0 E272900399999 ENDENTRY 3 0 E272999999999