ENTRY F1459 20220315 F088F145900000001 SUBENT F1459001 20220315 F088F145900100001 BIB 11 27 F145900100002 TITLE Experimental study of alpha-particle induced F145900100003 reactions on natural erbium for the production of F145900100004 Auger-emitters 167Tm, 165Er and 169Yb F145900100005 AUTHOR (E.S.Kormazeva,I.A.Khomenko,V.N.Unezhev,R.A.Aliev) F145900100006 REFERENCE (J,ARI,177,109919,2021) F145900100007 #doi:10.1016/j.apradiso.2021.109919 F145900100008 INSTITUTE (4RUSKUR) F145900100009 FACILITY (ISOCY,4RUSKUR) U-150 isochronous cyclotron F145900100010 SAMPLE Erbium targets of natural isotopic composition were F145900100011 used. Mechanically stable and visually homogeneous F145900100012 samples with a thickness of 5-11 mg/cm2 were F145900100013 obtained. The spot diameter was 20 mm. The target was F145900100014 covered with ~9 mu-m aluminum foil. Three stacks of F145900100015 foils were prepared, each consisted of ten erbium F145900100016 targets and aluminum degraders with a thickness of F145900100017 ~20 and ~30 mu-m interposed between them. F145900100018 DETECTOR (HPGE) Gamma spectrometer with an ORTEC GEM 35P4 high F145900100019 purity germanium detector with energy resolution 850 eVF145900100020 for the 122 keV line and 1.8 keV for the 1330 keV F145900100021 line was used. F145900100022 METHOD (ACTIV) The irradiation time was ~ 0.5 h at a beam F145900100023 current of 200-400 nA. F145900100024 (STTA,EDEG,GSPEC) F145900100025 MONITOR (13-AL-27(A,X)11-NA-24,,SIG) F145900100026 (13-AL-27(A,X)11-NA-22,,SIG) F145900100027 STATUS (APRVD) Entry was approved by Dr. E.S. Kormazeva F145900100028 HISTORY (20220315C) F145900100029 ENDBIB 27 0 F145900100030 NOCOMMON 0 0 F145900100031 ENDSUBENT 30 0 F145900199999 SUBENT F1459002 20220315 F088F145900200001 BIB 4 17 F145900200002 REACTION (68-ER-0(A,X)69-TM-165,CUM,SIG) F145900200003 DECAY-DATA (69-TM-165,30.6HR,DG,218.9,0.0334, F145900200004 DG,242.9,0.355, F145900200005 DG,297.4,0.127, F145900200006 DG,346.9,0.0310, F145900200007 DG,356.5,0.0275, F145900200008 DG,389.4,0.0282, F145900200009 DG,564.2,0.0231, F145900200010 DG,806.4,0.095, F145900200011 DG,1184.5,0.0295) F145900200012 ERR-ANALYS (ERR-T) The uncertainties of the cross sections were F145900200013 determined by taking the sum in quadrature of all F145900200014 individual linear contributions: F145900200015 (ERR-1) uncertainty of target thickness; F145900200016 (ERR-2) uncertainty of beam current; F145900200017 (ERR-3,1.,30.) uncertainty of isotopes. F145900200018 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900200019 ENDBIB 17 0 F145900200020 COMMON 2 3 F145900200021 ERR-1 ERR-2 F145900200022 PER-CENT PER-CENT F145900200023 10. 10. F145900200024 ENDCOMMON 3 0 F145900200025 DATA 4 24 F145900200026 EN EN-ERR DATA ERR-T F145900200027 MEV MEV MB MB F145900200028 16.6 2.8 0.2 0.1 F145900200029 21.0 2.2 0.7 0.1 F145900200030 24.9 2.0 0.8 0.1 F145900200031 28.3 1.6 0.8 0.3 F145900200032 31.7 1.3 3.8 0.8 F145900200033 33.4 1.5 6.8 2.6 F145900200034 35.0 1.0 13.9 2.3 F145900200035 36.8 1.7 9.3 1.7 F145900200036 37.4 1.3 15.6 2.1 F145900200037 39.1 1.5 13.2 4.6 F145900200038 41.0 1.2 17.1 3.2 F145900200039 41.3 1.4 15.8 4.4 F145900200040 44.1 1.4 13.1 3.1 F145900200041 44.8 1.0 17.3 2.2 F145900200042 46.5 1.1 12.0 3.0 F145900200043 48.5 0.9 14.9 3.1 F145900200044 48.9 1.0 11.9 3.4 F145900200045 51.3 0.9 32.1 3.3 F145900200046 52.0 0.8 44.9 6.1 F145900200047 54.2 0.8 83.8 8.7 F145900200048 55.6 0.6 108.5 12.4 F145900200049 56.6 0.6 142.8 12.1 F145900200050 59.0 0.6 238.8 31.3 F145900200051 59.1 0.6 173.3 16.8 F145900200052 ENDDATA 26 0 F145900200053 ENDSUBENT 52 0 F145900299999 SUBENT F1459003 20220315 F088F145900300001 BIB 6 22 F145900300002 REACTION (68-ER-0(A,X)69-TM-166,,SIG) F145900300003 REL-REF (D,E2618008,M.Saito+,J,ARI,154,108874,2019) F145900300004 ANALYSIS (DECAY) Separation to 166Tm and 166Yb production F145900300005 contribution. F145900300006 DECAY-DATA (69-TM-166-G,7.7HR,DG,80.6,0.115,DG,215.2,0.053, F145900300007 DG,594.4,0.035, F145900300008 DG,672.2,0.062, F145900300009 DG,674.8,0.026, F145900300010 DG,691.3,0.075, F145900300011 DG,705.3,0.111, F145900300012 DG,778.8,0.191, F145900300013 DG,785.9,0.100, F145900300014 DG,875.7,0.041, F145900300015 DG,1176.7,0.096, F145900300016 DG,1273.5,0.150) F145900300017 ERR-ANALYS (ERR-T) The uncertainties of the cross sections were F145900300018 determined by taking the sum in quadrature of all F145900300019 individual linear contributions: F145900300020 (ERR-1) uncertainty of target thickness; F145900300021 (ERR-2) uncertainty of beam current; F145900300022 (ERR-3,1.,30.) uncertainty of isotopes. F145900300023 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900300024 ENDBIB 22 0 F145900300025 COMMON 2 3 F145900300026 ERR-1 ERR-2 F145900300027 PER-CENT PER-CENT F145900300028 10. 10. F145900300029 ENDCOMMON 3 0 F145900300030 DATA 4 20 F145900300031 EN EN-ERR DATA ERR-T F145900300032 MEV MEV MB MB F145900300033 25.0 2.1 0.1 0.0 F145900300034 29.8 1.8 0.3 0.1 F145900300035 33.4 1.5 0.4 0.4 F145900300036 36.8 1.7 0.7 0.1 F145900300037 37.4 1.3 0.9 0.1 F145900300038 39.1 1.5 1.3 0.2 F145900300039 41.0 1.2 1.4 0.3 F145900300040 41.3 1.4 1.3 0.4 F145900300041 44.1 1.4 2.0 0.6 F145900300042 44.8 1.0 2.2 0.7 F145900300043 46.5 1.1 4.1 0.6 F145900300044 48.5 0.9 7.3 1.0 F145900300045 48.9 1.0 9.2 1.2 F145900300046 51.3 0.9 13.3 1.5 F145900300047 52.0 0.8 13.8 1.7 F145900300048 54.2 0.8 20.8 1.8 F145900300049 55.6 0.6 20.8 2.7 F145900300050 56.6 0.6 25.4 2.0 F145900300051 59.0 0.6 34.8 4.4 F145900300052 59.1 0.6 25.9 2.1 F145900300053 ENDDATA 22 0 F145900300054 ENDSUBENT 53 0 F145900399999 SUBENT F1459004 20220315 F088F145900400001 BIB 6 22 F145900400002 REACTION (68-ER-0(A,X)70-YB-166,,SIG) F145900400003 ANALYSIS (DECAY) Separation to 166Tm and 166Yb production F145900400004 contribution. F145900400005 RAD-DET (69-TM-166-G,DG) F145900400006 DECAY-DATA (69-TM-166-G,7.7HR,DG,80.6,0.115,DG,215.2,0.053, F145900400007 DG,594.4,0.035, F145900400008 DG,672.2,0.062, F145900400009 DG,674.8,0.026, F145900400010 DG,691.3,0.075, F145900400011 DG,705.3,0.111, F145900400012 DG,778.8,0.191, F145900400013 DG,785.9,0.100, F145900400014 DG,875.7,0.041, F145900400015 DG,1176.7,0.096, F145900400016 DG,1273.5,0.150) F145900400017 ERR-ANALYS (ERR-T) The uncertainties of the cross sections were F145900400018 determined by taking the sum in quadrature of all F145900400019 individual linear contributions: F145900400020 (ERR-1) uncertainty of target thickness; F145900400021 (ERR-2) uncertainty of beam current; F145900400022 (ERR-3,1.,30.) uncertainty of isotopes. F145900400023 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900400024 ENDBIB 22 0 F145900400025 COMMON 2 3 F145900400026 ERR-1 ERR-2 F145900400027 PER-CENT PER-CENT F145900400028 10. 10. F145900400029 ENDCOMMON 3 0 F145900400030 DATA 4 25 F145900400031 EN EN-ERR DATA ERR-T F145900400032 MEV MEV MB MB F145900400033 21.0 2.2 1.1 0.2 F145900400034 24.9 2.0 11.1 2.7 F145900400035 25.0 2.1 10.1 1.5 F145900400036 28.3 1.6 18.0 4.3 F145900400037 29.8 1.8 15.3 2.5 F145900400038 31.7 1.3 16.2 2.2 F145900400039 33.4 1.5 14.2 2.1 F145900400040 35.0 1.0 9.3 2.3 F145900400041 36.8 1.7 6.8 1.9 F145900400042 37.4 1.3 8.5 1.5 F145900400043 39.1 1.5 18.7 3.6 F145900400044 41.0 1.2 68.4 9.5 F145900400045 41.3 1.4 65.3 10.7 F145900400046 44.1 1.4 137.0 18.4 F145900400047 44.8 1.0 213.6 28.1 F145900400048 46.5 1.1 252.0 30.2 F145900400049 48.5 0.9 338.2 42.0 F145900400050 48.9 1.0 305.5 32.3 F145900400051 51.3 0.9 340.9 35.3 F145900400052 52.0 0.8 363.5 43.1 F145900400053 54.2 0.8 356.2 33.0 F145900400054 55.6 0.6 305.1 36.1 F145900400055 56.6 0.6 321.8 27.5 F145900400056 59.0 0.6 364.9 53.0 F145900400057 59.1 0.6 266.4 23.9 F145900400058 ENDDATA 27 0 F145900400059 ENDSUBENT 58 0 F145900499999 SUBENT F1459005 20220315 F088F145900500001 BIB 4 9 F145900500002 REACTION (68-ER-0(A,X)69-TM-167,CUM,SIG) F145900500003 DECAY-DATA (69-TM-167,9.25D,DG,207.8,0.42,DG,531.5,0.0161) F145900500004 ERR-ANALYS (ERR-T) The uncertainties of the cross sections were F145900500005 determined by taking the sum in quadrature of all F145900500006 individual linear contributions: F145900500007 (ERR-1) uncertainty of target thickness; F145900500008 (ERR-2) uncertainty of beam current; F145900500009 (ERR-3,1.,30.) uncertainty of isotopes. F145900500010 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900500011 ENDBIB 9 0 F145900500012 COMMON 2 3 F145900500013 ERR-1 ERR-2 F145900500014 PER-CENT PER-CENT F145900500015 10. 10. F145900500016 ENDCOMMON 3 0 F145900500017 DATA 4 27 F145900500018 EN EN-ERR DATA ERR-T F145900500019 MEV MEV MB MB F145900500020 11.3 4.1 0.6 0.1 F145900500021 16.6 2.8 2.0 0.2 F145900500022 21.0 2.2 5.9 0.6 F145900500023 24.9 2.0 5.0 0.5 F145900500024 25.0 2.1 3.3 0.5 F145900500025 28.3 1.6 28.6 2.7 F145900500026 29.8 1.8 44.6 6.0 F145900500027 31.7 1.3 228.5 18.5 F145900500028 33.4 1.5 276.7 37.0 F145900500029 35.0 1.0 454.1 33.0 F145900500030 36.8 1.7 292.9 42.1 F145900500031 37.4 1.3 426.1 54.9 F145900500032 39.1 1.5 463.0 66.1 F145900500033 41.0 1.2 513.3 65.2 F145900500034 41.3 1.4 489.5 69.9 F145900500035 44.1 1.4 402.2 50.3 F145900500036 44.8 1.0 439.7 53.0 F145900500037 46.5 1.1 420.5 47.2 F145900500038 48.5 0.9 405.6 47.8 F145900500039 48.9 1.0 379.4 36.7 F145900500040 51.3 0.9 382.9 35.7 F145900500041 52.0 0.8 371.9 41.3 F145900500042 54.2 0.8 390.1 31.1 F145900500043 55.6 0.6 327.2 35.0 F145900500044 56.6 0.6 363.7 27.0 F145900500045 59.0 0.6 394.9 42.2 F145900500046 59.1 0.6 307.8 22.6 F145900500047 ENDDATA 29 0 F145900500048 ENDSUBENT 47 0 F145900599999 SUBENT F1459006 20220315 F088F145900600001 BIB 4 9 F145900600002 REACTION (68-ER-0(A,X)70-YB-167,,SIG) F145900600003 DECAY-DATA (70-YB-167,17.5MIN,DG,143.5,0.0211,DG,176.,0.237) F145900600004 ERR-ANALYS (ERR-T) The uncertainties of the cross sections were F145900600005 determined by taking the sum in quadrature of all F145900600006 individual linear contributions: F145900600007 (ERR-1) uncertainty of target thickness; F145900600008 (ERR-2) uncertainty of beam current; F145900600009 (ERR-3,1.,30.) uncertainty of isotopes. F145900600010 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900600011 ENDBIB 9 0 F145900600012 COMMON 2 3 F145900600013 ERR-1 ERR-2 F145900600014 PER-CENT PER-CENT F145900600015 10. 10. F145900600016 ENDCOMMON 3 0 F145900600017 DATA 4 10 F145900600018 EN EN-ERR DATA ERR-T F145900600019 MEV MEV MB MB F145900600020 36.8 1.7 214.1 37.8 F145900600021 39.1 1.5 266.8 41.8 F145900600022 41.3 1.4 303.6 49.1 F145900600023 44.1 1.4 217.5 30.8 F145900600024 46.5 1.1 273.8 38.3 F145900600025 48.9 1.0 249.0 30.8 F145900600026 51.3 0.9 258.7 34.0 F145900600027 54.2 0.8 232.9 19.8 F145900600028 56.6 0.6 225.5 19.8 F145900600029 59.1 0.6 183.7 21.9 F145900600030 ENDDATA 12 0 F145900600031 ENDSUBENT 30 0 F145900699999 SUBENT F1459007 20220315 F088F145900700001 BIB 4 15 F145900700002 REACTION (68-ER-0(A,X)69-TM-168,,SIG) F145900700003 DECAY-DATA (69-TM-168,93.1D,DG,198.3,0.545, F145900700004 DG,447.5,0.240, F145900700005 DG,631.7,0.0926, F145900700006 DG,720.4,0.122, F145900700007 DG,741.4,0.128, F145900700008 DG,816.0,0.51, F145900700009 DG,821.1,0.120) F145900700010 ERR-ANALYS (DATA-ERR) The uncertainties of the cross sections wereF145900700011 determined by taking the sum in quadrature of all F145900700012 individual linear contributions: F145900700013 (ERR-1) uncertainty of target thickness; F145900700014 (ERR-2) uncertainty of beam current; F145900700015 (ERR-3,1.,30.) uncertainty of isotopes. F145900700016 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900700017 ENDBIB 15 0 F145900700018 COMMON 2 3 F145900700019 ERR-1 ERR-2 F145900700020 PER-CENT PER-CENT F145900700021 10. 10. F145900700022 ENDCOMMON 3 0 F145900700023 DATA 4 21 F145900700024 EN EN-ERR DATA DATA-ERR F145900700025 MEV MEV MB MB F145900700026 25.0 2.1 2.4 1.0 F145900700027 28.3 1.6 4.9 1.3 F145900700028 29.8 1.8 4.3 0.7 F145900700029 31.7 1.3 9.1 0.9 F145900700030 33.4 1.5 11.2 2.1 F145900700031 35.0 1.0 16.9 2.0 F145900700032 36.8 1.7 9.9 1.9 F145900700033 37.4 1.3 19.0 3.1 F145900700034 39.1 1.5 19.5 10.2 F145900700035 41.0 1.2 20.0 3.2 F145900700036 41.3 1.4 23.1 9.9 F145900700037 44.1 1.4 22.5 7.4 F145900700038 44.8 1.0 25.7 3.1 F145900700039 46.5 1.1 31.3 11.7 F145900700040 48.5 0.9 35.2 5.5 F145900700041 48.9 1.0 36.3 15.1 F145900700042 51.3 0.9 38.2 15.5 F145900700043 52.0 0.8 34.5 4.0 F145900700044 54.2 0.8 43.4 18.0 F145900700045 56.6 0.6 44.7 18.6 F145900700046 59.1 0.6 39.9 15.7 F145900700047 ENDDATA 23 0 F145900700048 ENDSUBENT 47 0 F145900799999 SUBENT F1459008 20220315 F088F145900800001 BIB 4 13 F145900800002 REACTION (68-ER-0(A,X)70-YB-169,,SIG) F145900800003 DECAY-DATA (70-YB-169-G,32.02D,DG,109.8,0.174, F145900800004 DG,130.5,0.114, F145900800005 DG,177.2,0.223, F145900800006 DG,198.0,0.359, F145900800007 DG,307.7,0.101) F145900800008 ERR-ANALYS (DATA-ERR) The uncertainties of the cross sections wereF145900800009 determined by taking the sum in quadrature of all F145900800010 individual linear contributions: F145900800011 (ERR-1) uncertainty of target thickness; F145900800012 (ERR-2) uncertainty of beam current; F145900800013 (ERR-3,1.,30.) uncertainty of isotopes. F145900800014 STATUS (TABLE)Tbl.2 from Applied Rad.Isotopes, 177,109919,2021F145900800015 ENDBIB 13 0 F145900800016 COMMON 2 3 F145900800017 ERR-1 ERR-2 F145900800018 PER-CENT PER-CENT F145900800019 10. 10. F145900800020 ENDCOMMON 3 0 F145900800021 DATA 4 24 F145900800022 EN EN-ERR DATA DATA-ERR F145900800023 MEV MEV MB MB F145900800024 16.6 2.8 7.1 1.0 F145900800025 21.0 2.2 123.7 12.3 F145900800026 24.9 2.0 239.0 24.2 F145900800027 25.0 2.1 196.2 27.5 F145900800028 28.3 1.6 303.2 39.3 F145900800029 29.8 1.8 261.3 38.2 F145900800030 31.7 1.3 374.5 35.7 F145900800031 33.4 1.5 371.3 65.7 F145900800032 35.0 1.0 390.8 44.1 F145900800033 36.8 1.7 263.3 65.3 F145900800034 37.4 1.3 357.2 51.4 F145900800035 39.1 1.5 260.6 63.7 F145900800036 41.0 1.2 223.1 38.6 F145900800037 41.3 1.4 193.4 48.1 F145900800038 44.1 1.4 108.5 29.3 F145900800039 44.8 1.0 158.4 37.7 F145900800040 46.5 1.1 105.3 24.0 F145900800041 48.5 0.9 140.3 20.3 F145900800042 48.9 1.0 112.3 24.9 F145900800043 51.3 0.9 131.1 27.2 F145900800044 52.0 0.8 178.2 25.5 F145900800045 54.2 0.8 156.8 38.1 F145900800046 56.6 0.6 129.2 41.7 F145900800047 59.1 0.6 109.1 21.9 F145900800048 ENDDATA 26 0 F145900800049 ENDSUBENT 48 0 F145900899999 SUBENT F1459009 20220221 F088F145900900001 BIB 5 15 F145900900002 REACTION (68-ER-0(A,X)69-TM-165,CUM,TTY,,EOB,DERIV) F145900900003 ANALYSIS (INTEF) F145900900004 DECAY-DATA (69-TM-165,30.6HR,DG,218.9,0.0334, F145900900005 DG,242.9,0.355, F145900900006 DG,297.4,0.127, F145900900007 DG,346.9,0.0310, F145900900008 DG,356.5,0.0275, F145900900009 DG,389.4,0.0282, F145900900010 DG,564.2,0.0231, F145900900011 DG,806.4,0.095, F145900900012 DG,1184.5,0.0295) F145900900013 ERR-ANALYS (ERR-1) uncertainty of detector efficiency; F145900900014 (ERR-2,1.,10.) uncertainty of photopeak area; F145900900015 (ERR-3) uncertainty of nuclear data. F145900900016 STATUS (TABLE) Table 3 of Applied Rad.Isotopes,177,109919,2021F145900900017 ENDBIB 15 0 F145900900018 COMMON 2 3 F145900900019 ERR-1 ERR-3 F145900900020 PER-CENT PER-CENT F145900900021 10. 3. F145900900022 ENDCOMMON 3 0 F145900900023 DATA 4 1 F145900900024 EN-MAX EN-MIN TIME-IRRD DATA F145900900025 MEV MEV HR MBQ/MUA F145900900026 60. 40. 0.5 4.6 F145900900027 ENDDATA 3 0 F145900900028 ENDSUBENT 27 0 F145900999999 SUBENT F1459010 20220221 F088F145901000001 BIB 5 8 F145901000002 REACTION (68-ER-0(A,X)69-TM-167,CUM,TTY,,EOB,DERIV) F145901000003 Impurities, % of EOB: 168Tm -0.78, 166Tm - 76. F145901000004 ANALYSIS (INTEF) F145901000005 DECAY-DATA (69-TM-167,9.25D,DG,207.8,0.42,DG,531.5,0.0161) F145901000006 ERR-ANALYS (ERR-1) uncertainty of detector efficiency; F145901000007 (ERR-2,1.,10.) uncertainty of photopeak area; F145901000008 (ERR-3) uncertainty of nuclear data. F145901000009 STATUS (TABLE) Table 4 of Applied Rad.Isotopes,177,109919,2021F145901000010 ENDBIB 8 0 F145901000011 COMMON 2 3 F145901000012 ERR-1 ERR-3 F145901000013 PER-CENT PER-CENT F145901000014 10. 3. F145901000015 ENDCOMMON 3 0 F145901000016 DATA 4 1 F145901000017 EN-MAX EN-MIN TIME-IRRD DATA F145901000018 MEV MEV HR MBQ/MUA F145901000019 60. 30. 0.5 5.4 F145901000020 ENDDATA 3 0 F145901000021 ENDSUBENT 20 0 F145901099999 SUBENT F1459011 20220221 F088F145901100001 BIB 5 11 F145901100002 REACTION (68-ER-0(A,X)70-YB-169,,TTY,,EOB,DERIV) F145901100003 ANALYSIS (INTEF) F145901100004 DECAY-DATA (70-YB-169-G,32.02D,DG,109.8,0.174, F145901100005 DG,130.5,0.114, F145901100006 DG,177.2,0.223, F145901100007 DG,198.0,0.359, F145901100008 DG,307.7,0.101) F145901100009 ERR-ANALYS (ERR-1) uncertainty of detector efficiency; F145901100010 (ERR-2,1.,10.) uncertainty of photopeak area; F145901100011 (ERR-3) uncertainty of nuclear data. F145901100012 STATUS (TABLE) Table 5 of Applied Rad.Isotopes,177,109919,2021F145901100013 ENDBIB 11 0 F145901100014 COMMON 2 3 F145901100015 ERR-1 ERR-3 F145901100016 PER-CENT PER-CENT F145901100017 10. 3. F145901100018 ENDCOMMON 3 0 F145901100019 DATA 4 1 F145901100020 EN-MAX EN-MIN TIME-IRRD DATA F145901100021 MEV MEV HR MBQ/MUA F145901100022 60. 20. 0.5 1.0 F145901100023 ENDDATA 3 0 F145901100024 ENDSUBENT 23 0 F145901199999 ENDENTRY 11 0 F145999999999