ENTRY O2429 20230117 O242900000001 SUBENT O2429001 20230117 20231011 O242900100001 BIB 11 31 O242900100002 TITLE First isomeric yield ratio measurements by direct ion O242900100003 counting and implications for the angular momentum of O242900100004 the primary fission fragments O242900100005 AUTHOR (V.Rakopoulos,M.Lantz,A.Solders,A.Al-Adili,A.Mattera, O242900100006 L.Canete,T.Eronen,D.Gorelov,A.Jokinen,A.Kankainen, O242900100007 V.S.Kolhinen,I.D.Moore,D.A.Nesterenko,H.Penttila, O242900100008 I.Pohjalainen,S.Rinta-Antila,V.Simutkin,M.Vilen, O242900100009 A.Voss,S.Pomp) O242900100010 INSTITUTE (2SWDUPP,2SF JYV) O242900100011 REFERENCE (J,PR/C,98,024612,2018) O242900100012 #doi:10.1103/PhysRevC.98.024612 O242900100013 (J,EPJ/CS,146,04054,2017) - prelim.results O242900100014 FACILITY (CYCLO,2SF JYV) 25 MeV proton beam from the K130 O242900100015 cyclotron at the University of Jyvaskyla. O242900100016 INC-SOURCE (ISOL) IGISOL-3 and IGISOL-4 Ion Guide Isotope O242900100017 Separator On-Line (IGISOL) facility and O242900100018 DETECTOR (MAGSP) JYFLTRAP double Penning trap mass spectrometer O242900100019 using just the first (purification trap) of the two O242900100020 traps and employing the sideband cooling technique. O242900100021 (MCPLT) O242900100022 METHOD (ASEP) The obtained spectra are Penning trap cyclotron O242900100023 frequency spectra, inversely proportional to mass. O242900100024 (TOF) TOF depends on the mass and charge of the ions. O242900100025 ANALYSIS The isomeric yield ratio is defined as the high-spin O242900100026 state yield over the total yield of the isotope. O242900100027 ERR-ANALYS (DATA-ERR) The given uncertainties include the O242900100028 statistical uncertainties and the uncertainties due O242900100029 to the radioactive decay loss correction. O242900100030 HISTORY (20190521C) VS O242900100031 (20200827U) SD: STATUS updated in Subents 002,006. O242900100032 (20230117U) SD: Ref. EPJ/CS,146 added. O242900100033 ENDBIB 31 0 O242900100034 COMMON 1 3 O242900100035 EN O242900100036 MEV O242900100037 25. O242900100038 ENDCOMMON 3 0 O242900100039 ENDSUBENT 38 0 O242900199999 SUBENT O2429002 20200827 O079O242900200001 BIB 5 7 O242900200002 REACTION (92-U-0(P,F)32-GE-81-G/T,IND,FY/RAT) O242900200003 SAMPLE natU target with thickness of 14 mg/cm2 O242900200004 LEVEL-PROP (32-GE-81-G,E-LVL=0.,SPIN=4.5,PARITY=+1.) O242900200005 (32-GE-81-M,E-LVL=679.1,SPIN=0.5,PARITY=+1.) O242900200006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900200007 (COREL,O2395002) Data from PI-ICR method O242900200008 HISTORY (20200827U) SD: STATUS updated O242900200009 ENDBIB 7 0 O242900200010 NOCOMMON 0 0 O242900200011 DATA 2 1 O242900200012 DATA DATA-ERR O242900200013 NO-DIM NO-DIM O242900200014 0.97 0.01 O242900200015 ENDDATA 3 0 O242900200016 ENDSUBENT 15 0 O242900299999 SUBENT O2429003 20190523 O070O242900300001 BIB 4 5 O242900300002 REACTION (92-U-0(P,F)39-Y-96-M/T,IND,FY/RAT) O242900300003 SAMPLE natU target with thickness of 14 mg/cm2 O242900300004 LEVEL-PROP (39-Y-96-G,E-LVL=0.,SPIN=0.,PARITY=-1.) O242900300005 (39-Y-96-M,E-LVL=1540.,SPIN=8.,PARITY=+1.) O242900300006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900300007 ENDBIB 5 0 O242900300008 NOCOMMON 0 0 O242900300009 DATA 2 1 O242900300010 DATA DATA-ERR O242900300011 NO-DIM NO-DIM O242900300012 0.55 0.01 O242900300013 ENDDATA 3 0 O242900300014 ENDSUBENT 13 0 O242900399999 SUBENT O2429004 20190523 O070O242900400001 BIB 4 5 O242900400002 REACTION (92-U-0(P,F)39-Y-97-M/T,IND,FY/RAT) O242900400003 SAMPLE natU target with thickness of 14 mg/cm2 O242900400004 LEVEL-PROP (39-Y-97-G,E-LVL=0.,SPIN=0.5,PARITY=-1.) O242900400005 (39-Y-97-M,E-LVL=667.5,SPIN=4.5,PARITY=+1.) O242900400006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900400007 ENDBIB 5 0 O242900400008 NOCOMMON 0 0 O242900400009 DATA 2 1 O242900400010 DATA DATA-ERR O242900400011 NO-DIM NO-DIM O242900400012 0.73 0.02 O242900400013 ENDDATA 3 0 O242900400014 ENDSUBENT 13 0 O242900499999 SUBENT O2429005 20190523 O070O242900500001 BIB 4 5 O242900500002 REACTION (92-U-0(P,F)50-SN-128-M/T,IND,FY/RAT) O242900500003 SAMPLE natU target with thickness of 14 mg/cm2 O242900500004 LEVEL-PROP (50-SN-128-G,E-LVL=0.,SPIN=0.,PARITY=+1.) O242900500005 (50-SN-128-M,E-LVL=2091.5,SPIN=7.,PARITY=-1.) O242900500006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900500007 ENDBIB 5 0 O242900500008 NOCOMMON 0 0 O242900500009 DATA 2 1 O242900500010 DATA DATA-ERR O242900500011 NO-DIM NO-DIM O242900500012 0.58 0.02 O242900500013 ENDDATA 3 0 O242900500014 ENDSUBENT 13 0 O242900599999 SUBENT O2429006 20200827 O079O242900600001 BIB 5 7 O242900600002 REACTION (92-U-0(P,F)51-SB-129-M/T,IND,FY/RAT) O242900600003 SAMPLE natU target with thickness of 14 mg/cm2 O242900600004 LEVEL-PROP (51-SB-129-G,E-LVL=0.,SPIN=3.5,PARITY=+1.) O242900600005 (51-SB-129-M,E-LVL=1851.3,SPIN=9.5,PARITY=-1.) O242900600006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900600007 (COREL,O2395013) Data from PI-ICR method O242900600008 HISTORY (20200827U) SD: STATUS updated O242900600009 ENDBIB 7 0 O242900600010 NOCOMMON 0 0 O242900600011 DATA 2 1 O242900600012 DATA DATA-ERR O242900600013 NO-DIM NO-DIM O242900600014 0.47 0.04 O242900600015 ENDDATA 3 0 O242900600016 ENDSUBENT 15 0 O242900699999 SUBENT O2429007 20190523 O070O242900700001 BIB 4 5 O242900700002 REACTION (92-U-0(P,F)50-SN-130-M/T,IND,FY/RAT) O242900700003 SAMPLE natU target with thickness of 14 mg/cm2 O242900700004 LEVEL-PROP (50-SN-130-G,E-LVL=0.,SPIN=0.,PARITY=+1.) O242900700005 (50-SN-130-M,E-LVL=1946.9,SPIN=7.,PARITY=-1.) O242900700006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900700007 ENDBIB 5 0 O242900700008 NOCOMMON 0 0 O242900700009 DATA 2 1 O242900700010 DATA DATA-ERR O242900700011 NO-DIM NO-DIM O242900700012 0.54 0.02 O242900700013 ENDDATA 3 0 O242900700014 ENDSUBENT 13 0 O242900799999 SUBENT O2429008 20190521 O070O242900800001 BIB 4 5 O242900800002 REACTION (90-TH-232(P,F)32-GE-81-M/T,IND,FY/RAT) O242900800003 SAMPLE Th-232 target with thickness of 15 mg/cm2 O242900800004 LEVEL-PROP (32-GE-81-G,E-LVL=0.,SPIN=4.5,PARITY=+1.) O242900800005 (32-GE-81-M,E-LVL=679.1,SPIN=0.5,PARITY=+1.) O242900800006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900800007 ENDBIB 5 0 O242900800008 NOCOMMON 0 0 O242900800009 DATA 2 1 O242900800010 DATA DATA-ERR O242900800011 NO-DIM NO-DIM O242900800012 0.92 0.02 O242900800013 ENDDATA 3 0 O242900800014 ENDSUBENT 13 0 O242900899999 SUBENT O2429009 20190523 O070O242900900001 BIB 4 5 O242900900002 REACTION (90-TH-232(P,F)39-Y-96-M/T,IND,FY/RAT) O242900900003 SAMPLE Th-232 target with thickness of 15 mg/cm2 O242900900004 LEVEL-PROP (39-Y-96-G,E-LVL=0.,SPIN=0.,PARITY=-1.) O242900900005 (39-Y-96-M,E-LVL=1540.,SPIN=8.,PARITY=+1.) O242900900006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242900900007 ENDBIB 5 0 O242900900008 NOCOMMON 0 0 O242900900009 DATA 2 1 O242900900010 DATA DATA-ERR O242900900011 NO-DIM NO-DIM O242900900012 0.61 0.02 O242900900013 ENDDATA 3 0 O242900900014 ENDSUBENT 13 0 O242900999999 SUBENT O2429010 20190523 O070O242901000001 BIB 4 5 O242901000002 REACTION (90-TH-232(P,F)39-Y-97-M/T,IND,FY/RAT) O242901000003 SAMPLE Th-232 target with thickness of 15 mg/cm2 O242901000004 LEVEL-PROP (39-Y-97-G,E-LVL=0.,SPIN=0.5,PARITY=-1.) O242901000005 (39-Y-97-M,E-LVL=667.5,SPIN=4.5,PARITY=+1.) O242901000006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242901000007 ENDBIB 5 0 O242901000008 NOCOMMON 0 0 O242901000009 DATA 2 1 O242901000010 DATA DATA-ERR O242901000011 NO-DIM NO-DIM O242901000012 0.78 0.02 O242901000013 ENDDATA 3 0 O242901000014 ENDSUBENT 13 0 O242901099999 SUBENT O2429011 20190523 O070O242901100001 BIB 4 5 O242901100002 REACTION (90-TH-232(P,F)50-SN-128-M/T,IND,FY/RAT) O242901100003 SAMPLE Th-232 target with thickness of 15 mg/cm2 O242901100004 LEVEL-PROP (50-SN-128-G,E-LVL=0.,SPIN=0.,PARITY=+1.) O242901100005 (50-SN-128-M,E-LVL=2091.5,SPIN=7.,PARITY=-1.) O242901100006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242901100007 ENDBIB 5 0 O242901100008 NOCOMMON 0 0 O242901100009 DATA 2 1 O242901100010 DATA DATA-ERR O242901100011 NO-DIM NO-DIM O242901100012 0.46 0.01 O242901100013 ENDDATA 3 0 O242901100014 ENDSUBENT 13 0 O242901199999 SUBENT O2429012 20190523 O070O242901200001 BIB 4 5 O242901200002 REACTION (90-TH-232(P,F)51-SB-129-M/T,IND,FY/RAT) O242901200003 SAMPLE Th-232 target with thickness of 15 mg/cm2 O242901200004 LEVEL-PROP (51-SB-129-G,E-LVL=0.,SPIN=3.5,PARITY=+1.) O242901200005 (51-SB-129-M,E-LVL=1851.3,SPIN=9.5,PARITY=-1.) O242901200006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242901200007 ENDBIB 5 0 O242901200008 NOCOMMON 0 0 O242901200009 DATA 2 1 O242901200010 DATA DATA-ERR O242901200011 NO-DIM NO-DIM O242901200012 0.46 0.01 O242901200013 ENDDATA 3 0 O242901200014 ENDSUBENT 13 0 O242901299999 SUBENT O2429013 20190523 O070O242901300001 BIB 4 5 O242901300002 REACTION (90-TH-232(P,F)50-SN-130-M/T,IND,FY/RAT) O242901300003 SAMPLE Th-232 target with thickness of 15 mg/cm2 O242901300004 LEVEL-PROP (50-SN-130-G,E-LVL=0.,SPIN=0.,PARITY=+1.) O242901300005 (50-SN-130-M,E-LVL=1946.9,SPIN=7.,PARITY=-1.) O242901300006 STATUS (TABLE) Table II of Phys.Rev.C98(2018)024612 O242901300007 ENDBIB 5 0 O242901300008 NOCOMMON 0 0 O242901300009 DATA 2 1 O242901300010 DATA DATA-ERR O242901300011 NO-DIM NO-DIM O242901300012 0.38 0.01 O242901300013 ENDDATA 3 0 O242901300014 ENDSUBENT 13 0 O242901399999 ENDENTRY 13 0 O242999999999