ENTRY O2429 20230117 O093O242900000001
SUBENT O2429001 20230117 O093O242900100001
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