ENTRY E2589 20230406 E258900000001 SUBENT E2589001 20230406 20231011 E258900100001 BIB 13 25 E258900100002 TITLE Activation cross sections of deuteron-induced E258900100003 reactions on niobium up to 24 MeV E258900100004 AUTHOR (M.Aikawa, Y.Komori, H.Haba) E258900100005 INSTITUTE (2JPNHOK,2JPNIPC) E258900100006 REFERENCE (J,NIM/B,436,217,2018) E258900100007 MONITOR (22-TI-0(D,X)23-V-48,,SIG) E258900100008 MONIT-REF (,S.M.Qaim+,R,IAEA-TECDOC-1211,2001) E258900100009 INC-SOURCE Beam intensity is 200.3 nA. E258900100010 SAMPLE - Chemical-form of target is element. E258900100011 - Physical-form of target is solid. E258900100012 - Target-thickness is 27.11 mg/cm2. E258900100013 METHOD (ACTIV) Irradiated for 30 min E258900100014 (GSPEC) E258900100015 FACILITY (ISOCY,2JPNIPC) AVF cyclotron E258900100016 DETECTOR (HPGE) E258900100017 ERR-ANALYS (ERR-T) Total uncertainty E258900100018 (ERR-1) beam intensity E258900100019 (ERR-2) target thickness E258900100020 (ERR-3) target purity E258900100021 (ERR-4) detector efficiency E258900100022 (ERR-5,,1.1) gamma-ray intensity (<1.1%) E258900100023 (ERR-6) peak fitting E258900100024 (ERR-S,,23.1) Statistical uncertainty (<23.1%) E258900100025 HISTORY (20181008C) MA E258900100026 (20230406A) MA. REACTION in 002 was modified. E258900100027 ENDBIB 25 0 E258900100028 COMMON 5 3 E258900100029 ERR-6 ERR-1 ERR-2 ERR-3 ERR-4 E258900100030 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT E258900100031 3. 5. 1. 1. 5. E258900100032 ENDCOMMON 3 0 E258900100033 ENDSUBENT 32 0 E258900199999 SUBENT E2589002 20230406 20231011 E258900200001 BIB 4 5 E258900200002 REACTION (41-NB-93(D,2N)42-MO-93-M,,SIG) E258900200003 DECAY-DATA (42-MO-93-M,6.85HR,DG,263.049,0.574) E258900200004 STATUS (TABLE) Table 2 of Nucl. Instrum. Methods B 436 (2018) E258900200005 217 E258900200006 HISTORY (20230406A) MA. SF3: X -> 2N E258900200007 ENDBIB 5 0 E258900200008 NOCOMMON 0 0 E258900200009 DATA 4 15 E258900200010 EN EN-ERR DATA ERR-T E258900200011 MEV MEV MB MB E258900200012 22.7 0.4 64.5 5.3 E258900200013 22.1 0.4 70.6 5.8 E258900200014 21.5 0.4 81.5 6.7 E258900200015 19.6 0.4 100.3 8.2 E258900200016 19.0 0.5 108.3 8.9 E258900200017 18.3 0.5 114.4 9.4 E258900200018 16.2 0.5 113.2 9.3 E258900200019 15.4 0.5 107.3 8.8 E258900200020 14.6 0.6 98.6 8.1 E258900200021 12.1 0.6 62.8 5.1 E258900200022 11.2 0.7 48.7 4.0 E258900200023 10.2 0.7 33.6 2.7 E258900200024 6.8 0.9 0.94 0.08 E258900200025 5.3 1.1 0.016 0.001 E258900200026 3.5 1.4 0.0038 0.0003 E258900200027 ENDDATA 17 0 E258900200028 ENDSUBENT 27 0 E258900299999 SUBENT E2589003 20181106 E118E258900300001 BIB 3 4 E258900300002 REACTION (41-NB-93(D,X)41-NB-92-M,,SIG) E258900300003 DECAY-DATA (41-NB-92-M,10.15D,DG,934.44,0.9915) E258900300004 STATUS (TABLE) Table 2 of Nucl. Instrum. Methods B 436 (2018) E258900300005 217 E258900300006 ENDBIB 4 0 E258900300007 NOCOMMON 0 0 E258900300008 DATA 4 12 E258900300009 EN EN-ERR DATA ERR-T E258900300010 MEV MEV MB MB E258900300011 22.7 0.4 53.9 4.4 E258900300012 22.1 0.4 45.6 3.8 E258900300013 21.5 0.4 41.2 3.4 E258900300014 19.6 0.4 24.0 2.0 E258900300015 19.0 0.5 16.4 1.4 E258900300016 18.3 0.5 13.9 1.2 E258900300017 16.2 0.5 7.0 0.6 E258900300018 15.4 0.5 6.5 0.6 E258900300019 14.6 0.6 5.5 0.5 E258900300020 12.1 0.6 3.9 0.4 E258900300021 11.2 0.7 3.3 0.3 E258900300022 10.2 0.7 2.4 0.3 E258900300023 ENDDATA 14 0 E258900300024 ENDSUBENT 23 0 E258900399999 SUBENT E2589004 20181106 E118E258900400001 BIB 3 4 E258900400002 REACTION (41-NB-93(D,X)40-ZR-89-G,M+,SIG) E258900400003 DECAY-DATA (40-ZR-89-G,78.41HR,DG,909.15,0.9904) E258900400004 STATUS (TABLE) Table 2 of Nucl. Instrum. Methods B 436 (2018) E258900400005 217 E258900400006 ENDBIB 4 0 E258900400007 NOCOMMON 0 0 E258900400008 DATA 4 5 E258900400009 EN EN-ERR DATA ERR-T E258900400010 MEV MEV MB MB E258900400011 22.7 0.4 9.1 0.7 E258900400012 22.1 0.4 6.4 0.6 E258900400013 21.5 0.4 4.5 0.4 E258900400014 19.6 0.4 0.83 0.11 E258900400015 19.0 0.5 0.36 0.09 E258900400016 ENDDATA 7 0 E258900400017 ENDSUBENT 16 0 E258900499999 ENDENTRY 4 0 E258999999999