ENTRY F1490 20231128 F095F1490 0 1 SUBENT F1490001 20231128 F095F1490 1 1 BIB 12 38 F1490 1 2 TITLE Proton induced reactions on 114Sn and 120Sn targets F1490 1 3 at energies up to 18 MeV F1490 1 4 AUTHOR (G.H.Hovhannisyan,T.M.Bakhshiyan,G.V.Martirosyan, F1490 1 5 R.K.Dallakyan,A.R.Balabekyan) F1490 1 6 INSTITUTE (4ARMJSU,4ARMJER) F1490 1 7 (4ARMARM) Institute of Applied Problems of Physics, F1490 1 8 Yerevan, Armenia F1490 1 9 REFERENCE (J,EPJ/A,59,161,2023) F1490 1 10 #doi:10.1140/epja/s10050-023-01071-y F1490 1 11 FACILITY (CYCLO,4ARMJER) Cyclotron C18/18 F1490 1 12 SAMPLE Stack of enriched 114Sn and 120Sn foils were used. F1490 1 13 The stack was composed of 6 blocks of natCu-114Sn- F1490 1 14 natCu-120Sn layers where tin foils were 20 to 40 mu-m F1490 1 15 thick and copper foils were 20 mu-m thick. F1490 1 16 DETECTOR (HPGE) High-purity germanium detector GEM15P4-70 was F1490 1 17 used. The energy resolution of the HPGe detector was F1490 1 18 1.66 keV FWHM at 1332.5 keV peak of 60Co, and 0.618 keVF1490 1 19 FWHM at 122 keV peak of 57Co. F1490 1 20 METHOD (ACTIV) Irradiation was 5 min long with a collimated F1490 1 21 1 mu-A proton beam of the same diameter as the F1490 1 22 target. The measurements were performed periodically F1490 1 23 during several days, with the first measurement done F1490 1 24 40 min after the end of irradiation (to allow F1490 1 25 short-lived isotope cross-section measurements). F1490 1 26 (STTA,EDEG) F1490 1 27 MONITOR (29-CU-63(P,N)30-ZN-63,,SIG) F1490 1 28 (29-CU-63(P,2N)30-ZN-62,,SIG) F1490 1 29 ERR-ANALYS The proton energy uncertainties were calculated using F1490 1 30 SRIM-2013 code and also include uncertainties from the F1490 1 31 primary beam energy (0.2 MeV) and target thickness (5%)F1490 1 32 (ERR-T) Resulting cross section uncertainties add F1490 1 33 uncertainties from the following sources in quadrature:F1490 1 34 (ERR-S,0.5,16.) Statistical errors on counts F1490 1 35 (ERR-1,,7.) Uncertainty in the flux F1490 1 36 (ERR-2) Uncertainty in detector efficiency F1490 1 37 (ERR-3) Uncertainty in target thickness F1490 1 38 STATUS (APRVD) Entry was approved by Dr. G.H.Hovhannisyan F1490 1 39 HISTORY (20231128C) F1490 1 40 ENDBIB 38 0 F1490 1 41 COMMON 2 3 F1490 1 42 ERR-2 ERR-3 F1490 1 43 PER-CENT PER-CENT F1490 1 44 4. 5. F1490 1 45 ENDCOMMON 3 0 F1490 1 46 ENDSUBENT 45 0 F1490 199999 SUBENT F1490002 20231128 F095F1490 2 1 BIB 5 10 F1490 2 2 REACTION (50-SN-114(P,A)49-IN-111,,SIG) F1490 2 3 DECAY-DATA (49-IN-111-G,2.805D,DG,171.28,0.907, F1490 2 4 DG,245.39,0.941) F1490 2 5 SAMPLE (50-SN-114,ENR=0.632) F1490 2 6 COMMENT *By authors* Reaction cross sections were measured on F1490 2 7 a 114Sn target with an enrichment of 63.2%. The data F1490 2 8 presented are corrected for 100% enrichment. F1490 2 9 The contribution of 111In(p,2p)111(m+g)In can be F1490 2 10 neglected. F1490 2 11 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 2 12 ENDBIB 10 0 F1490 2 13 NOCOMMON 0 0 F1490 2 14 DATA 4 6 F1490 2 15 EN EN-ERR DATA ERR-T F1490 2 16 MEV MEV MB MB F1490 2 17 17.34 0.89 7.98 0.72 F1490 2 18 15.79 0.81 6.59 0.59 F1490 2 19 14.13 0.72 3.96 0.38 F1490 2 20 12.13 0.64 2.52 0.23 F1490 2 21 10.52 0.54 1.30 0.19 F1490 2 22 8.46 0.50 0.54 0.09 F1490 2 23 ENDDATA 8 0 F1490 2 24 ENDSUBENT 23 0 F1490 299999 SUBENT F1490003 20231128 F095F1490 3 1 BIB 5 7 F1490 3 2 REACTION (50-SN-114(P,A)49-IN-111-M,,SIG) F1490 3 3 DECAY-DATA (49-IN-111-M,7.7MIN,DG,537.22,0.87) F1490 3 4 SAMPLE (50-SN-114,ENR=0.632) F1490 3 5 COMMENT *By authors* Reaction cross sections were measured on F1490 3 6 a 114Sn target with an enrichment of 63.2%. The data F1490 3 7 presented are corrected for 100% enrichment. F1490 3 8 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 3 9 ENDBIB 7 0 F1490 3 10 NOCOMMON 0 0 F1490 3 11 DATA 4 1 F1490 3 12 EN EN-ERR DATA ERR-T F1490 3 13 MEV MEV MB MB F1490 3 14 17.34 0.89 0.58 0.11 F1490 3 15 ENDDATA 3 0 F1490 3 16 ENDSUBENT 15 0 F1490 399999 SUBENT F1490004 20231128 F095F1490 4 1 BIB 5 9 F1490 4 2 REACTION (50-SN-114(P,X)50-SN-113,CUM,SIG) F1490 4 3 DECAY-DATA (50-SN-113-G,115.1D,DG,391.71,0.6497) F1490 4 4 SAMPLE (50-SN-114,ENR=0.632) F1490 4 5 COMMENT *By authors* Reaction cross sections were measured on F1490 4 6 a 114Sn target with an enrichment of 63.2%. The data F1490 4 7 presented are corrected for 100% enrichment. F1490 4 8 Contributions of other Sn isotopes contained in the F1490 4 9 target to the 113Sn production can be neglected. F1490 4 10 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 4 11 ENDBIB 9 0 F1490 4 12 NOCOMMON 0 0 F1490 4 13 DATA 4 4 F1490 4 14 EN EN-ERR DATA ERR-T F1490 4 15 MEV MEV MB MB F1490 4 16 17.34 0.89 281. 25. F1490 4 17 15.79 0.81 138. 13. F1490 4 18 14.13 0.72 26.49 2.91 F1490 4 19 12.13 0.64 2.65 0.50 F1490 4 20 ENDDATA 6 0 F1490 4 21 ENDSUBENT 20 0 F1490 499999 SUBENT F1490005 20231128 F095F1490 5 1 BIB 5 10 F1490 5 2 REACTION (50-SN-114(P,2N)51-SB-113,,SIG) F1490 5 3 DECAY-DATA (51-SB-113,6.67MIN,DG,332.4,0.148) F1490 5 4 SAMPLE (50-SN-114,ENR=0.632) F1490 5 5 COMMENT *By authors* Reaction cross sections were measured on F1490 5 6 a 114Sn target with an enrichment of 63.2%. The data F1490 5 7 presented are corrected for 100% enrichment. F1490 5 8 The contribution of the side reaction F1490 5 9 112Sn(p,gamma)113Sb does not exceed the uncertainty F1490 5 10 of measured cross section. F1490 5 11 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 5 12 ENDBIB 10 0 F1490 5 13 NOCOMMON 0 0 F1490 5 14 DATA 4 1 F1490 5 15 EN EN-ERR DATA ERR-T F1490 5 16 MEV MEV MB MB F1490 5 17 17.34 0.89 21.58 4.10 F1490 5 18 ENDDATA 3 0 F1490 5 19 ENDSUBENT 18 0 F1490 599999 SUBENT F1490006 20231128 F095F1490 6 1 BIB 5 8 F1490 6 2 REACTION (50-SN-120(P,N)51-SB-120-M,,SIG) F1490 6 3 DECAY-DATA (51-SB-120-M,5.76D,DG,197.3,0.87, F1490 6 4 DG,1023.1,0.994) F1490 6 5 SAMPLE (50-SN-120,ENR=0.996) F1490 6 6 COMMENT *By authors* The purity of the 120Sn target used in theF1490 6 7 experiments is 99.6%, making the contributions of F1490 6 8 other tin isotopes to product yields negligibly small. F1490 6 9 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 6 10 ENDBIB 8 0 F1490 6 11 NOCOMMON 0 0 F1490 6 12 DATA 4 6 F1490 6 13 EN EN-ERR DATA ERR-T F1490 6 14 MEV MEV MB MB F1490 6 15 16.57 0.85 23.34 2.59 F1490 6 16 14.97 0.77 39.66 3.58 F1490 6 17 13.27 0.69 49.08 4.42 F1490 6 18 11.48 0.61 71.56 10.73 F1490 6 19 9.51 0.51 46.78 7.03 F1490 6 20 7.31 0.41 14.56 2.18 F1490 6 21 ENDDATA 8 0 F1490 6 22 ENDSUBENT 21 0 F1490 699999 SUBENT F1490007 20231128 F095F1490 7 1 BIB 5 8 F1490 7 2 REACTION (50-SN-120(P,N)51-SB-120-G,,SIG) F1490 7 3 DECAY-DATA (51-SB-120-G,15.89MIN,DG,703.8,0.00149, F1490 7 4 DG,988.6,0.00063) F1490 7 5 SAMPLE (50-SN-120,ENR=0.996) F1490 7 6 COMMENT *By authors* The purity of the 120Sn target used in theF1490 7 7 experiments is 99.6%, making the contributions of F1490 7 8 other tin isotopes to product yields negligibly small. F1490 7 9 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 7 10 ENDBIB 8 0 F1490 7 11 NOCOMMON 0 0 F1490 7 12 DATA 4 4 F1490 7 13 EN EN-ERR DATA ERR-T F1490 7 14 MEV MEV MB MB F1490 7 15 16.57 0.85 108. 15. F1490 7 16 14.97 0.77 131. 18. F1490 7 17 13.27 0.69 215. 20. F1490 7 18 11.48 0.61 551. 55. F1490 7 19 ENDDATA 6 0 F1490 7 20 ENDSUBENT 19 0 F1490 799999 SUBENT F1490008 20231128 F095F1490 8 1 BIB 5 7 F1490 8 2 REACTION (50-SN-120(P,A)49-IN-117-M,,SIG) F1490 8 3 DECAY-DATA (49-IN-117-M,116.2MIN,DG,315.302,0.191) F1490 8 4 SAMPLE (50-SN-120,ENR=0.996) F1490 8 5 COMMENT *By authors* The purity of the 120Sn target used in theF1490 8 6 experiments is 99.6%, making the contributions of F1490 8 7 other tin isotopes to product yields negligibly small. F1490 8 8 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 8 9 ENDBIB 7 0 F1490 8 10 NOCOMMON 0 0 F1490 8 11 DATA 4 5 F1490 8 12 EN EN-ERR DATA ERR-T F1490 8 13 MEV MEV MB MB F1490 8 14 16.57 0.85 1.20 0.22 F1490 8 15 14.97 0.77 1.10 0.11 F1490 8 16 13.27 0.69 0.76 0.07 F1490 8 17 11.48 0.61 0.50 0.05 F1490 8 18 9.51 0.51 0.17 0.03 F1490 8 19 ENDDATA 7 0 F1490 8 20 ENDSUBENT 19 0 F1490 899999 SUBENT F1490009 20231128 F095F1490 9 1 BIB 5 7 F1490 9 2 REACTION (50-SN-120(P,A)49-IN-117-G,,SIG) F1490 9 3 DECAY-DATA (49-IN-117-G,43.2MIN,DG,552.9,1.) F1490 9 4 SAMPLE (50-SN-120,ENR=0.996) F1490 9 5 COMMENT *By authors* The purity of the 120Sn target used in theF1490 9 6 experiments is 99.6%, making the contributions of F1490 9 7 other tin isotopes to product yields negligibly small. F1490 9 8 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Tbl. 3 F1490 9 9 ENDBIB 7 0 F1490 9 10 NOCOMMON 0 0 F1490 9 11 DATA 4 5 F1490 9 12 EN EN-ERR DATA ERR-T F1490 9 13 MEV MEV MB MB F1490 9 14 16.57 0.85 5.22 0.46 F1490 9 15 14.97 0.77 3.52 0.33 F1490 9 16 13.27 0.69 1.82 0.16 F1490 9 17 11.48 0.61 1.08 0.11 F1490 9 18 9.51 0.51 0.46 0.09 F1490 9 19 ENDDATA 7 0 F1490 9 20 ENDSUBENT 19 0 F1490 999999 SUBENT F1490010 20231128 F095F1490 10 1 BIB 5 13 F1490 10 2 REACTION (50-SN-120(P,N)51-SB-120-M/G,,SIG/RAT) F1490 10 3 DECAY-DATA (51-SB-120-G,15.89MIN,DG,703.8,0.00149, F1490 10 4 DG,988.6,0.00063) F1490 10 5 (51-SB-120-M,5.76D,DG,197.3,0.87, F1490 10 6 DG,1023.1,0.994) F1490 10 7 SAMPLE (50-SN-120,ENR=0.996) F1490 10 8 COMMENT *By authors* The purity of the 120Sn target used in theF1490 10 9 experiments is 99.6%, making the contributions of F1490 10 10 other tin isotopes to product yields negligibly small. F1490 10 11 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Data F1490 10 12 were received from authors, the same on Fig. 8. F1490 10 13 (DEP,F1490006) 120mSb production cross section F1490 10 14 (DEP,F1490007) 120gSb production cross section F1490 10 15 ENDBIB 13 0 F1490 10 16 NOCOMMON 0 0 F1490 10 17 DATA 4 4 F1490 10 18 EN EN-ERR DATA ERR-T F1490 10 19 MEV MEV NO-DIM NO-DIM F1490 10 20 16.57 0.85 0.216111 0.038419 F1490 10 21 14.97 0.77 0.302748 0.049773 F1490 10 22 13.27 0.69 0.228279 0.029556 F1490 10 23 11.48 0.61 0.129873 0.023394 F1490 10 24 ENDDATA 6 0 F1490 10 25 ENDSUBENT 24 0 F1490 1099999 SUBENT F1490011 20231128 F095F1490 11 1 BIB 5 11 F1490 11 2 REACTION (50-SN-120(P,A)49-IN-117-G/M,,SIG/RAT) F1490 11 3 DECAY-DATA (49-IN-117-G,43.2MIN,DG,552.9,1.) F1490 11 4 (49-IN-117-M,116.2MIN,DG,315.302,0.191) F1490 11 5 SAMPLE (50-SN-120,ENR=0.996) F1490 11 6 COMMENT *By authors* The purity of the 120Sn target used in theF1490 11 7 experiments is 99.6%, making the contributions of F1490 11 8 other tin isotopes to product yields negligibly small. F1490 11 9 STATUS (TABLE,,G.H.Hovhannisyan+,J,EPJ/A,59,161,2023) Data F1490 11 10 were received from authors, the same on Fig. 9. F1490 11 11 (DEP,F1490008) 117mIn production cross section F1490 11 12 (DEP,F1490009) 117gIn production cross section F1490 11 13 ENDBIB 11 0 F1490 11 14 NOCOMMON 0 0 F1490 11 15 DATA 4 5 F1490 11 16 EN EN-ERR DATA ERR-T F1490 11 17 MEV MEV NO-DIM NO-DIM F1490 11 18 16.57 0.85 4.35 0.884845 F1490 11 19 14.97 0.77 3.2 0.438634 F1490 11 20 13.27 0.69 2.394737 0.304912 F1490 11 21 11.48 0.61 2.16 0.308312 F1490 11 22 9.51 0.51 2.705882 0.712946 F1490 11 23 ENDDATA 7 0 F1490 11 24 ENDSUBENT 23 0 F1490 1199999 ENDENTRY 11 0 F149099999999