ENTRY O2470 20200823 O080O247000000001 SUBENT O2470001 20200823 O080O247000100001 BIB 12 30 O247000100002 TITLE Measurement of the 43Sc production cross-section with O247000100003 a deuteron beam O247000100004 AUTHOR (T.S.Carzaniga,N.P.Van Der Meulen,R.Hasler,C.Kottler, O247000100005 P.Peier,A.Turler,E.Vermeulen,C.Vockenhuber,S.Braccini) O247000100006 INSTITUTE (2SWTUBE,2SWTPSI,2SWTETH) O247000100007 (2SWTSWT) Federal Institute of Metrology METAS, O247000100008 Bern-Wabern, Switzerland O247000100009 REFERENCE (J,ARI,145,205,2019) O247000100010 #doi:10.1016/j.apradiso.2018.12.031 O247000100011 FACILITY (VDGT,2SWTETH) O247000100012 SAMPLE (20-CA-42,ENR=0.8080) +- 0.008 42CaCO3 powder O247000100013 Target isotope composition: O247000100014 40Ca - 17.79%, 43CA - 0.39%, 44Ca - 0.97, O247000100015 46Ca less than 0.01%, 48Ca less that 0.05 O247000100016 The mass of the target ranges from 0.15 to 0.5 mg and O247000100017 the thickness of the targets is in the order of 15 um. O247000100018 INC-SPECT The accelerated deuterium beam had an energy spread O247000100019 of 1 keV. The value of the beam energy was known with O247000100020 an uncertainty of 1%. The entry, exit and mean energy O247000100021 of the deuteron beam in the target was computed via O247000100022 SRIM simulations and used to evaluate the beam energy O247000100023 and its uncertainty. O247000100024 METHOD (ACTIV,GSPEC) O247000100025 Irradiation time - 5 min. O247000100026 Gamma spectrum measurement time of few hours. O247000100027 (STTA,BCINT) O247000100028 MONITOR (28-NI-0(D,X)29-CU-61,,SIG) O247000100029 MONIT-REF (,A.Hermanne+,J,NDS,148,338,2018) O247000100030 DECAY-MON (29-CU-61,3.339HR,DG,282.956,0.122) O247000100031 HISTORY (20200823C) VS O247000100032 ENDBIB 30 0 O247000100033 NOCOMMON 0 0 O247000100034 ENDSUBENT 33 0 O247000199999 SUBENT O2470002 20200823 O080O247000200001 BIB 4 7 O247000200002 REACTION (28-NI-0(D,X)29-CU-61,,SIG) O247000200003 DECAY-DATA (29-CU-61,3.339HR,DG,282.956,0.122) O247000200004 ERR-ANALYS (ERR-T) Total uncertainty is dominated by the O247000200005 uncertainty on the mass of the Nickel foil. O247000200006 (ERR-1) Uncertainty on the mass of the Nickel foil - O247000200007 20%. O247000200008 STATUS (TABLE) Table A1 of Appl.Radiat.Isot.145(2019)205 O247000200009 ENDBIB 7 0 O247000200010 COMMON 1 3 O247000200011 ERR-1 O247000200012 PER-CENT O247000200013 20. O247000200014 ENDCOMMON 3 0 O247000200015 DATA 4 9 O247000200016 EN EN-ERR DATA ERR-T O247000200017 MEV MEV MB MB O247000200018 7.5 0.17 86. 17. O247000200019 7.0 0.18 88. 18. O247000200020 6.5 0.19 70. 14. O247000200021 6.0 0.20 69. 14. O247000200022 5.5 0.22 48. 10. O247000200023 5.0 0.24 55. 11. O247000200024 4.5 0.26 38. 8. O247000200025 4.0 0.28 20. 4. O247000200026 3.5 0.32 7. 2. O247000200027 ENDDATA 11 0 O247000200028 ENDSUBENT 27 0 O247000299999 SUBENT O2470003 20200823 O080O247000300001 BIB 4 9 O247000300002 REACTION (20-CA-42(D,N)21-SC-43,,SIG) O247000300003 DECAY-DATA (21-SC-43,3.891HR,DG,372.9,0.172) O247000300004 ERR-ANALYS (ERR-T) Total uncertainty determined from: O247000300005 (ERR-1,,7.) sample mass O247000300006 (ERR-2) flatness of the beam - 5% O247000300007 (ERR-3) detector efficiency calibration - 5% O247000300008 (ERR-S,,4.) the biggest uncertainty on the neat peak O247000300009 area O247000300010 STATUS (TABLE) Table A2 of Appl.Radiat.Isot.145(2019)205 O247000300011 ENDBIB 9 0 O247000300012 COMMON 2 3 O247000300013 ERR-2 ERR-3 O247000300014 PER-CENT PER-CENT O247000300015 5. 5. O247000300016 ENDCOMMON 3 0 O247000300017 DATA 4 9 O247000300018 EN EN-ERR DATA ERR-T O247000300019 MEV MEV MB MB O247000300020 7.1 0.2 178. 23. O247000300021 6.6 0.2 207. 27. O247000300022 6.1 0.2 176. 20. O247000300023 5.5 0.2 189. 24. O247000300024 5.0 0.2 159. 20. O247000300025 4.5 0.2 180. 24. O247000300026 3.9 0.3 123. 16. O247000300027 3.4 0.3 62. 7. O247000300028 2.8 0.3 34. 5. O247000300029 ENDDATA 11 0 O247000300030 ENDSUBENT 29 0 O247000399999 ENDENTRY 3 0 O247099999999