ENTRY F1490 20231128 F149000000001 SUBENT F1490001 20231128 20240316 F149000100001 BIB 12 38 F149000100002 TITLE Proton induced reactions on 114Sn and 120Sn targets F149000100003 at energies up to 18 MeV F149000100004 AUTHOR (G.H.Hovhannisyan,T.M.Bakhshiyan,G.V.Martirosyan, F149000100005 R.K.Dallakyan,A.R.Balabekyan) F149000100006 INSTITUTE (4ARMJSU,4ARMJER) F149000100007 (4ARMARM) Institute of Applied Problems of Physics, F149000100008 Yerevan, Armenia F149000100009 REFERENCE (J,EPJ/A,59,161,2023) F149000100010 #doi:10.1140/epja/s10050-023-01071-y F149000100011 FACILITY (CYCLO,4ARMJER) Cyclotron C18/18 F149000100012 SAMPLE Stack of enriched 114Sn and 120Sn foils were used. F149000100013 The stack was composed of 6 blocks of natCu-114Sn- F149000100014 natCu-120Sn layers where tin foils were 20 to 40 mu-m F149000100015 thick and copper foils were 20 mu-m thick. F149000100016 DETECTOR (HPGE) High-purity germanium detector GEM15P4-70 was F149000100017 used. The energy resolution of the HPGe detector was F149000100018 1.66 keV FWHM at 1332.5 keV peak of 60Co, and 0.618 keVF149000100019 FWHM at 122 keV peak of 57Co. F149000100020 METHOD (ACTIV) Irradiation was 5 min long with a collimated F149000100021 1 mu-A proton beam of the same diameter as the F149000100022 target. The measurements were performed periodically F149000100023 during several days, with the first measurement done F149000100024 40 min after the end of irradiation (to allow F149000100025 short-lived isotope cross-section measurements). F149000100026 (STTA,EDEG) F149000100027 MONITOR (29-CU-63(P,N)30-ZN-63,,SIG) F149000100028 (29-CU-63(P,2N)30-ZN-62,,SIG) F149000100029 ERR-ANALYS The proton energy uncertainties were calculated using F149000100030 SRIM-2013 code and also include uncertainties from the F149000100031 primary beam energy (0.2 MeV) and target thickness (5%)F149000100032 (ERR-T) Resulting cross section uncertainties add F149000100033 uncertainties from the following sources in quadrature:F149000100034 (ERR-S,0.5,16.) Statistical errors on counts F149000100035 (ERR-1,,7.) Uncertainty in the flux F149000100036 (ERR-2) Uncertainty in detector efficiency F149000100037 (ERR-3) Uncertainty in target thickness F149000100038 STATUS (APRVD) Entry was approved by Dr. G.H.Hovhannisyan F149000100039 HISTORY (20231128C) F149000100040 ENDBIB 38 0 F149000100041 COMMON 2 3 F149000100042 ERR-2 ERR-3 F149000100043 PER-CENT PER-CENT F149000100044 4. 5. F149000100045 ENDCOMMON 3 0 F149000100046 ENDSUBENT 45 0 F149000199999 SUBENT F1490002 20231128 20240316 F149000200001 BIB 5 10 F149000200002 REACTION (50-SN-114(P,A)49-IN-111,,SIG) F149000200003 DECAY-DATA (49-IN-111-G,2.805D,DG,171.28,0.907, F149000200004 DG,245.39,0.941) F149000200005 SAMPLE (50-SN-114,ENR=0.632) F149000200006 COMMENT *By authors* Reaction cross sections were measured on F149000200007 a 114Sn target with an enrichment of 63.2%. The data F149000200008 presented are corrected for 100% enrichment. F149000200009 The contribution of 111In(p,2p)111(m+g)In can be F149000200010 neglected. F149000200011 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000200012 ENDBIB 10 0 F149000200013 NOCOMMON 0 0 F149000200014 DATA 4 6 F149000200015 EN EN-ERR DATA ERR-T F149000200016 MEV MEV MB MB F149000200017 17.34 0.89 7.98 0.72 F149000200018 15.79 0.81 6.59 0.59 F149000200019 14.13 0.72 3.96 0.38 F149000200020 12.13 0.64 2.52 0.23 F149000200021 10.52 0.54 1.30 0.19 F149000200022 8.46 0.50 0.54 0.09 F149000200023 ENDDATA 8 0 F149000200024 ENDSUBENT 23 0 F149000299999 SUBENT F1490003 20231128 20240316 F149000300001 BIB 5 7 F149000300002 REACTION (50-SN-114(P,A)49-IN-111-M,,SIG) F149000300003 DECAY-DATA (49-IN-111-M,7.7MIN,DG,537.22,0.87) F149000300004 SAMPLE (50-SN-114,ENR=0.632) F149000300005 COMMENT *By authors* Reaction cross sections were measured on F149000300006 a 114Sn target with an enrichment of 63.2%. The data F149000300007 presented are corrected for 100% enrichment. F149000300008 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000300009 ENDBIB 7 0 F149000300010 NOCOMMON 0 0 F149000300011 DATA 4 1 F149000300012 EN EN-ERR DATA ERR-T F149000300013 MEV MEV MB MB F149000300014 17.34 0.89 0.58 0.11 F149000300015 ENDDATA 3 0 F149000300016 ENDSUBENT 15 0 F149000399999 SUBENT F1490004 20231128 20240316 F149000400001 BIB 5 9 F149000400002 REACTION (50-SN-114(P,X)50-SN-113,CUM,SIG) F149000400003 DECAY-DATA (50-SN-113-G,115.1D,DG,391.71,0.6497) F149000400004 SAMPLE (50-SN-114,ENR=0.632) F149000400005 COMMENT *By authors* Reaction cross sections were measured on F149000400006 a 114Sn target with an enrichment of 63.2%. The data F149000400007 presented are corrected for 100% enrichment. F149000400008 Contributions of other Sn isotopes contained in the F149000400009 target to the 113Sn production can be neglected. F149000400010 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000400011 ENDBIB 9 0 F149000400012 NOCOMMON 0 0 F149000400013 DATA 4 4 F149000400014 EN EN-ERR DATA ERR-T F149000400015 MEV MEV MB MB F149000400016 17.34 0.89 281. 25. F149000400017 15.79 0.81 138. 13. F149000400018 14.13 0.72 26.49 2.91 F149000400019 12.13 0.64 2.65 0.50 F149000400020 ENDDATA 6 0 F149000400021 ENDSUBENT 20 0 F149000499999 SUBENT F1490005 20231128 20240316 F149000500001 BIB 5 10 F149000500002 REACTION (50-SN-114(P,2N)51-SB-113,,SIG) F149000500003 DECAY-DATA (51-SB-113,6.67MIN,DG,332.4,0.148) F149000500004 SAMPLE (50-SN-114,ENR=0.632) F149000500005 COMMENT *By authors* Reaction cross sections were measured on F149000500006 a 114Sn target with an enrichment of 63.2%. The data F149000500007 presented are corrected for 100% enrichment. F149000500008 The contribution of the side reaction F149000500009 112Sn(p,gamma)113Sb does not exceed the uncertainty F149000500010 of measured cross section. F149000500011 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000500012 ENDBIB 10 0 F149000500013 NOCOMMON 0 0 F149000500014 DATA 4 1 F149000500015 EN EN-ERR DATA ERR-T F149000500016 MEV MEV MB MB F149000500017 17.34 0.89 21.58 4.10 F149000500018 ENDDATA 3 0 F149000500019 ENDSUBENT 18 0 F149000599999 SUBENT F1490006 20231128 20240316 F149000600001 BIB 5 8 F149000600002 REACTION (50-SN-120(P,N)51-SB-120-M,,SIG) F149000600003 DECAY-DATA (51-SB-120-M,5.76D,DG,197.3,0.87, F149000600004 DG,1023.1,0.994) F149000600005 SAMPLE (50-SN-120,ENR=0.996) F149000600006 COMMENT *By authors* The purity of the 120Sn target used in theF149000600007 experiments is 99.6%, making the contributions of F149000600008 other tin isotopes to product yields negligibly small. F149000600009 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000600010 ENDBIB 8 0 F149000600011 NOCOMMON 0 0 F149000600012 DATA 4 6 F149000600013 EN EN-ERR DATA ERR-T F149000600014 MEV MEV MB MB F149000600015 16.57 0.85 23.34 2.59 F149000600016 14.97 0.77 39.66 3.58 F149000600017 13.27 0.69 49.08 4.42 F149000600018 11.48 0.61 71.56 10.73 F149000600019 9.51 0.51 46.78 7.03 F149000600020 7.31 0.41 14.56 2.18 F149000600021 ENDDATA 8 0 F149000600022 ENDSUBENT 21 0 F149000699999 SUBENT F1490007 20231128 20240316 F149000700001 BIB 5 8 F149000700002 REACTION (50-SN-120(P,N)51-SB-120-G,,SIG) F149000700003 DECAY-DATA (51-SB-120-G,15.89MIN,DG,703.8,0.00149, F149000700004 DG,988.6,0.00063) F149000700005 SAMPLE (50-SN-120,ENR=0.996) F149000700006 COMMENT *By authors* The purity of the 120Sn target used in theF149000700007 experiments is 99.6%, making the contributions of F149000700008 other tin isotopes to product yields negligibly small. F149000700009 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000700010 ENDBIB 8 0 F149000700011 NOCOMMON 0 0 F149000700012 DATA 4 4 F149000700013 EN EN-ERR DATA ERR-T F149000700014 MEV MEV MB MB F149000700015 16.57 0.85 108. 15. F149000700016 14.97 0.77 131. 18. F149000700017 13.27 0.69 215. 20. F149000700018 11.48 0.61 551. 55. F149000700019 ENDDATA 6 0 F149000700020 ENDSUBENT 19 0 F149000799999 SUBENT F1490008 20231128 20240316 F149000800001 BIB 5 7 F149000800002 REACTION (50-SN-120(P,A)49-IN-117-M,,SIG) F149000800003 DECAY-DATA (49-IN-117-M,116.2MIN,DG,315.302,0.191) F149000800004 SAMPLE (50-SN-120,ENR=0.996) F149000800005 COMMENT *By authors* The purity of the 120Sn target used in theF149000800006 experiments is 99.6%, making the contributions of F149000800007 other tin isotopes to product yields negligibly small. F149000800008 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000800009 ENDBIB 7 0 F149000800010 NOCOMMON 0 0 F149000800011 DATA 4 5 F149000800012 EN EN-ERR DATA ERR-T F149000800013 MEV MEV MB MB F149000800014 16.57 0.85 1.20 0.22 F149000800015 14.97 0.77 1.10 0.11 F149000800016 13.27 0.69 0.76 0.07 F149000800017 11.48 0.61 0.50 0.05 F149000800018 9.51 0.51 0.17 0.03 F149000800019 ENDDATA 7 0 F149000800020 ENDSUBENT 19 0 F149000899999 SUBENT F1490009 20231128 20240316 F149000900001 BIB 5 7 F149000900002 REACTION (50-SN-120(P,A)49-IN-117-G,,SIG) F149000900003 DECAY-DATA (49-IN-117-G,43.2MIN,DG,552.9,1.) F149000900004 SAMPLE (50-SN-120,ENR=0.996) F149000900005 COMMENT *By authors* The purity of the 120Sn target used in theF149000900006 experiments is 99.6%, making the contributions of F149000900007 other tin isotopes to product yields negligibly small. F149000900008 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F149000900009 ENDBIB 7 0 F149000900010 NOCOMMON 0 0 F149000900011 DATA 4 5 F149000900012 EN EN-ERR DATA ERR-T F149000900013 MEV MEV MB MB F149000900014 16.57 0.85 5.22 0.46 F149000900015 14.97 0.77 3.52 0.33 F149000900016 13.27 0.69 1.82 0.16 F149000900017 11.48 0.61 1.08 0.11 F149000900018 9.51 0.51 0.46 0.09 F149000900019 ENDDATA 7 0 F149000900020 ENDSUBENT 19 0 F149000999999 SUBENT F1490010 20231128 20240316 F149001000001 BIB 5 13 F149001000002 REACTION (50-SN-120(P,N)51-SB-120-M/G,,SIG/RAT) F149001000003 DECAY-DATA (51-SB-120-G,15.89MIN,DG,703.8,0.00149, F149001000004 DG,988.6,0.00063) F149001000005 (51-SB-120-M,5.76D,DG,197.3,0.87, F149001000006 DG,1023.1,0.994) F149001000007 SAMPLE (50-SN-120,ENR=0.996) F149001000008 COMMENT *By authors* The purity of the 120Sn target used in theF149001000009 experiments is 99.6%, making the contributions of F149001000010 other tin isotopes to product yields negligibly small. F149001000011 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Data F149001000012 were received from authors, the same on Fig. 8. F149001000013 (DEP,F1490006) 120mSb production cross section F149001000014 (DEP,F1490007) 120gSb production cross section F149001000015 ENDBIB 13 0 F149001000016 NOCOMMON 0 0 F149001000017 DATA 4 4 F149001000018 EN EN-ERR DATA ERR-T F149001000019 MEV MEV NO-DIM NO-DIM F149001000020 16.57 0.85 0.216111 0.038419 F149001000021 14.97 0.77 0.302748 0.049773 F149001000022 13.27 0.69 0.228279 0.029556 F149001000023 11.48 0.61 0.129873 0.023394 F149001000024 ENDDATA 6 0 F149001000025 ENDSUBENT 24 0 F149001099999 SUBENT F1490011 20231128 20240316 F149001100001 BIB 5 11 F149001100002 REACTION (50-SN-120(P,A)49-IN-117-G/M,,SIG/RAT) F149001100003 DECAY-DATA (49-IN-117-G,43.2MIN,DG,552.9,1.) F149001100004 (49-IN-117-M,116.2MIN,DG,315.302,0.191) F149001100005 SAMPLE (50-SN-120,ENR=0.996) F149001100006 COMMENT *By authors* The purity of the 120Sn target used in theF149001100007 experiments is 99.6%, making the contributions of F149001100008 other tin isotopes to product yields negligibly small. F149001100009 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Data F149001100010 were received from authors, the same on Fig. 9. F149001100011 (DEP,F1490008) 117mIn production cross section F149001100012 (DEP,F1490009) 117gIn production cross section F149001100013 ENDBIB 11 0 F149001100014 NOCOMMON 0 0 F149001100015 DATA 4 5 F149001100016 EN EN-ERR DATA ERR-T F149001100017 MEV MEV NO-DIM NO-DIM F149001100018 16.57 0.85 4.35 0.884845 F149001100019 14.97 0.77 3.2 0.438634 F149001100020 13.27 0.69 2.394737 0.304912 F149001100021 11.48 0.61 2.16 0.308312 F149001100022 9.51 0.51 2.705882 0.712946 F149001100023 ENDDATA 7 0 F149001100024 ENDSUBENT 23 0 F149001199999 ENDENTRY 11 0 F149099999999