ENTRY E2629 20191216 E124E262900000001 SUBENT E2629001 20191216 E124E262900100001 BIB 13 30 E262900100002 TITLE Activation cross sections of dysprosium-157,159 and E262900100003 terbium-160 radioisotopes from the deuteron-induced E262900100004 reactions on terbium-159 up to 24 MeV E262900100005 AUTHOR (D.Ichinkhorloo, M.Aikawa, Ts.Zolbadral, Y.Komori, E262900100006 H.Haba) E262900100007 INSTITUTE (2JPNHOK) Faculty of Science E262900100008 (3MGLNUM) Nuclear Research Center E262900100009 (2JPNHOK) Graduate School of Biomedical Science and E262900100010 Engineering E262900100011 (2JPNIPC) Nishina Center for Accelerator-Based Science E262900100012 REFERENCE (J,NIM/B,461,102,2019) E262900100013 MONITOR (22-TI-0(D,X)23-V-48,,SIG) E262900100014 MONIT-REF (,A.Hermanne+,J,NDS,148,338,2018) E262900100015 INC-SOURCE Beam intensity is 94.3 nA. E262900100016 SAMPLE - Target is natural. E262900100017 - Chemical-form of target is element. E262900100018 - Physical-form of target is solid. E262900100019 - Target-thickness is 20.56 mg/cm2. E262900100020 METHOD (ACTIV,GSPEC,STTA) E262900100021 FACILITY (ISOCY,2JPNIPC) AVF cyclotron E262900100022 DETECTOR (HPGE) E262900100023 ERR-ANALYS (ERR-T) Total uncertainty E262900100024 (ERR-1) target thickness E262900100025 (ERR-2) target purity E262900100026 (ERR-3) beam intensity E262900100027 (ERR-4) detector efficiency E262900100028 (ERR-5,2.3,5.7) gamma-ray intensity (2.3-5.7%) E262900100029 (ERR-6) peak fitting E262900100030 (ERR-S,0.4,7.0) Statistical uncertainty (0.4-7.0%) E262900100031 HISTORY (20191007C) Ichinko E262900100032 ENDBIB 30 0 E262900100033 COMMON 5 3 E262900100034 ERR-6 ERR-1 ERR-2 ERR-3 ERR-4 E262900100035 PER-CENT PER-CENT PER-CENT PER-CENT PER-CENT E262900100036 3. 2. 1. 5. 6. E262900100037 ENDCOMMON 3 0 E262900100038 ENDSUBENT 37 0 E262900199999 SUBENT E2629002 20191216 E124E262900200001 BIB 3 4 E262900200002 REACTION (65-TB-159(D,2N)66-DY-159,,SIG) E262900200003 DECAY-DATA (66-DY-159,144.4D,DG,58.0,0.227) E262900200004 STATUS (TABLE) Table 2 and Fig.2 of Nucl. Instrum. Methods B E262900200005 461 (2019) 102. E262900200006 ENDBIB 4 0 E262900200007 NOCOMMON 0 0 E262900200008 DATA 4 15 E262900200009 EN EN-ERR DATA ERR-T E262900200010 MEV MEV MB MB E262900200011 23.7 0.2 149.3 16.7 E262900200012 22.8 0.2 169.6 18.2 E262900200013 21.9 0.2 170.9 18.4 E262900200014 21.0 0.2 187.0 20.1 E262900200015 20.1 0.2 222.4 23.6 E262900200016 19.1 0.2 262.8 27.8 E262900200017 18.1 0.2 306.3 32.3 E262900200018 17.1 0.3 407.4 42.8 E262900200019 15.9 0.3 460.3 48.3 E262900200020 14.8 0.3 592.6 61.9 E262900200021 13.6 0.3 662.3 69.1 E262900200022 12.3 0.3 604.0 63.1 E262900200023 10.8 0.4 477.0 50.0 E262900200024 9.3 0.4 237.8 25.2 E262900200025 7.5 0.5 47.2 5.66 E262900200026 ENDDATA 17 0 E262900200027 ENDSUBENT 26 0 E262900299999 SUBENT E2629003 20191216 E124E262900300001 BIB 3 4 E262900300002 REACTION (65-TB-159(D,4N)66-DY-157,,SIG) E262900300003 DECAY-DATA (66-DY-157,8.14HR,DG,326.336,0.93) E262900300004 STATUS (TABLE) Table 2 and Fig.3 of Nucl. Instrum. Methods B E262900300005 461 (2019) 102. E262900300006 ENDBIB 4 0 E262900300007 NOCOMMON 0 0 E262900300008 DATA 4 4 E262900300009 EN EN-ERR DATA ERR-T E262900300010 MEV MEV MB MB E262900300011 23.7 0.2 122.5 11.3 E262900300012 22.8 0.2 50.0 4.6 E262900300013 21.9 0.2 11.8 1.1 E262900300014 21.0 0.2 1.0 0.1 E262900300015 ENDDATA 6 0 E262900300016 ENDSUBENT 15 0 E262900399999 SUBENT E2629004 20191216 E124E262900400001 BIB 3 4 E262900400002 REACTION (65-TB-159(D,P)65-TB-160,,SIG) E262900400003 DECAY-DATA (65-TB-160,72.3D,DG,298.5783,0.261) E262900400004 STATUS (TABLE) Table 2 and Fig.4 of Nucl. Instrum. Methods B E262900400005 461 (2019) 102. E262900400006 ENDBIB 4 0 E262900400007 NOCOMMON 0 0 E262900400008 DATA 4 17 E262900400009 EN EN-ERR DATA ERR-T E262900400010 MEV MEV MB MB E262900400011 23.7 0.2 84.9 7.6 E262900400012 22.8 0.2 86.4 7.8 E262900400013 21.9 0.2 91.7 8.2 E262900400014 21.0 0.2 97.4 8.8 E262900400015 20.1 0.2 105.5 9.5 E262900400016 19.1 0.2 115.6 10.4 E262900400017 18.1 0.3 122.8 11.0 E262900400018 17.0 0.3 140.7 12.6 E262900400019 15.9 0.3 146.7 13.2 E262900400020 14.8 0.3 164.6 14.8 E262900400021 13.6 0.3 185.9 16.7 E262900400022 12.3 0.3 188.1 16.9 E262900400023 10.8 0.4 200.3 18.0 E262900400024 9.3 0.4 157.4 14.1 E262900400025 7.5 0.5 59.1 5.3 E262900400026 5.5 0.6 4.4 0.4 E262900400027 2.6 1.1 1.1 0.1 E262900400028 ENDDATA 19 0 E262900400029 ENDSUBENT 28 0 E262900499999 ENDENTRY 4 0 E262999999999