65FE 65MN B- DECAY (91.9 MS) 2013OL06 25NDS 202505
65FE H TYP=FUL$AUT=Jun Chen$CIT=NDS 202, 59 (2025)$CUT=25-Feb-2025$
65FE DB EAV,LOGFT$FROM BetaShape v2.4 (Jun-2024) 2023MO21.
65FE DG CC$FROM BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr.
65FE dL E$Least-squares fitting is done by GLSC (version 15-Aug-2024)
65FE c Adapted from the XUNDL dataset for 2013Ol06 compiled by B. Singh
65FE2c (McMaster), on November 25, 2013
65FE c 2013Ol06: {+65}Mn source was produced in bombardment of UC{-x}/graphite
65FE2c target by 1.4-GeV pulsed protons at the ISOLDE-CERN facility. Reaction
65FE3c products were diffused out of the target, ionized by selective
65FE4c resonant ionization using RILIS, mass separated by General Purpose
65FE5c Separator (GPS) and implanted into a thin Al foil. |b particles were
65FE6c detected with a fast-timing plastic scintillator and |g rays were
65FE7c detected with two LaBr{-3}(Ce) and two HPGe detectors. Measured E|g,
65FE8c I|g,|g|g-coin, |b|g(t), |b|g|g(t). Deduced levels, J, |p, T{-1/2},
65FE9c decay branching ratios, log {Ift}, |g-ray transition strengths.
65FEac Comparisons with available data and large-scale shell-model
65FEbc calculations with the Lenzi-Nowacki-Poves-Sieja (LNPS) interaction.
65FE c 2005GaZR (thesis): {+65}Mn source was produced by fragmentation of a
65FE2c 61.8 MeV/nucleon {+76}Ge beam on a {+58}Ni target at GANIL. Measured
65FE3c E|g, I|g. Deduced levels, J, |p, decay branching ratios, log {Ift}.
65FE4c Report 5 transitions.
65FE cB $The decay scheme is considered fairly complete by the evaluator,
65FE2cB considering possibly a small amount of missing transitions. See
65FE3cB comments for 393.6-keV isomeric level
65FE cB IB$Deduced by the evaluator from intensity balance. Values from
65FE2cB 2013Ol06 are higher by |?12% and given under comments
65FE cG E,RI$From 2013Ol06
65FE cG RI(A)$From |g|g-coin data (2013Ol06)
65FE cG E(D),RI(D)$Doublet. Intensities for separate components obtained
65FE2cG from |g|g-coin spectra with gates on 374.1|g and 405.6|g
65FE cL E$From a least-squares fit to |g-ray energies. 796.9|g from
65FE2cL 1367 level was not included in the fit due to its poor energy
65FE3cL agreement.
65FE cL J$From Adopted Levels. Assignments up to 1367 level from 2013Ol06 are
65FE2cL given under comments if different
65FE cL T$From |b|g(t) for 364, 456 and 561 levels and from |b|g|g(t) for other
65FE2cL levels in 2013Ol06, unless otherwise stated. The same values are
65FE3cL adopted in Adopted Levels
65FE cL T(B)$From Adopted Levels
65FE cL T(D)$Limit is estimated by 2013Ol06 for levels used as semi-prompt
65FE2cL reference in time-response calibrations of the fast-timing detectors
65MN P 0 (5/2-) 91.9 MS 9 10251 6
65MN cP J,T$From Adopted Levels of {+65}Mn. Adopted T{-1/2} is from |b-delayed
65MN2cP 363.7|g(t) in the decay of {+65}Mn in 2013Ol06, where a value of 92.0
65MN3cP ms {I13} is also reported using five other |g transitions 455.6|g,
65MN4cP 569.1|g, 683.3|g, 725.2|g and 1002.9|g. Other: 92 ms {I1} (2005GaZR).
65MN5cP See Adopted Levels of {+65}Mn for more measurements of T{-1/2} of
65MN6cP {+65}Mn.
65MN cP QP$ From 2021Wa16
65FE N 0.539 19 0.539 19 1.0 1.0
65FE cN NR,NT$Deduced by 2013Ol06 from %I(|b decay of g.s.)+%I(|b decay of
65FE2cN isomer)+%|b{+-}n=100, where %|b{+-}n=7.9 {I12} (relative intensity=14.6
65FE3cN {I21}) and relative I(|b decay of g.s.)=163.61 {I61} from |g
65FE4cN intensities in {+65}Co only from the |b{+-} decay of {+65}Fe g.s. and
65FE5cN relative I(|b decay of isomer)=7.3 {I10} from |g intensities in {+65}Co
65FE6cN only from the |b{+-} decay of this isomer, relative to
65FE7cN I|g(363.7|g)=100.
65FE PN 5
65FE G 501.3 5 0.2 1
65FE2 G %IG=0.11 6
65FE G 1051.5 5 0.2 1
65FE2 G %IG=0.11 6
65FE L 0.0 (1/2-) 0.805 S 10 B
65FE B 8.8 LT 7.8 GT ?
65FES B EAV=4806.3 29
65FE cB IB$estimated by 2013Ol06 from the difference between the total
65FE2cB intensities of |g transitions to {+65}Co g.s. from the decay of {+65}Fe
65FE3cB g.s. (equivalent to total feedings to levels in {+65}Co since no direct
65FE4cB g.s. feeding) and |g transitions to {+65}Fe ground state. If g.s. J|p
65FE5cB is 5/2- for {+65}Mn and 1/2- for {+65}Fe, then no |b feeding is
65FE6cB expected.
65FE L 363.62 5 (3/2-) 93 PS 3
65FE B 37.4 15 4.74 2
65FES B EAV=4629.8 29
65FE cB IB$42 {I5} (2013Ol06)
65FE G 363.7 1 100 [M1,E2] 0.0027 13 C
65FES G KC=0.0024 11$LC=2.3E-4 11$MC=3.2E-5 15
65FES G NC=1.4E-6 7
65FE2 G %IG=54
65FE L 393.65 17 (9/2+) 1.12 S 15 BM1
65FE2 L %B-=100
65FE cL $No direct |b feeding is expected from (5/2-) parent state. Indirect
65FE2cL feeding through 215.8|g from 609.5 level is 1.56% {I12}. 2013Ol06
65FE3cL report a total relative |b decay intensity of this isomer=7.9 {I10}
65FE4cL relative to I|g(364.7|g)=100, from intensities of |g transitions only
65FE5cL from the |b decay of this iosmer. This is equivalent to %I(|b decay of
65FE6cL isomer)=3.94 {I54} per 100 {+65}Fe decays, greater than 1.56% indirect
65FE7cL feeding above, which may indicate there are missing transitions that
65FE8cL feed this isomer.
65FE G 393.7 0.15 LT [M4] 0.0521 7 ?
65FES G KC=0.0463 6$LC=0.00505 7$MC=0.000697 10
65FES G NC=2.98E-5 4
65FE2 G %IG LT 0.081
65FE cG E,RI$393.7|g with implied M4 multipolarity is not seen, upper limit of
65FE2cG intensity established by 2013Ol06 as <0.15 relative to 100 for 363.7|g
65FE L 397.56 7 (5/2+) 420 NS 13 BM2
65FE cL T$other: 437 ns {I55} from 2013Ol06
65FE B 0.79 LT 6.4 GT ?
65FES B EAV=4613.2 29
65FE cB IB$0.1 {I6} (2013Ol06)
65FE G 33.9 2 1.9 5 [E1] 1.127 25 4 1
65FES G K/T=0.477 6$L/T=0.0467 12$M/T=0.00631 16
65FES G N/T=0.000255 6
65FES G KC=1.014 23$LC=0.0994 23$MC=0.01343 30
65FES G NC=0.000542 12
65FE cG TI$from time-delayed component of the 363.7|g
65FE cG RI$from I(|g+ce) and total conversion coefficient
65FE G 397.6 0.15 LT [M2] 0.00417 6 ?
65FES G KC=0.00374 5$LC=0.000370 5$MC=5.10E-5 7
65FES G NC=2.325E-6 33
65FE2 G %IG LT 0.081
65FE cG E,RI$397.6|g with implied M2 multipolarity is not seen, upper limit of
65FE2cG intensity established by 2013Ol06 as <0.15 relative to 100 for 363.7|g
65FE L 455.59 5 (5/2-) 350 PS 10
65FE B 7.1 13 5.4 1
65FES B EAV=4585.0 29
65FE cB IB$8.1 {I11} (2013Ol06)
65FE G 92.0 1 0.8 1 [M1] 0.0439 6 C
65FES G KC=0.0394 6$LC=0.00391 6$MC=0.000539 8
65FES G NC=2.428E-5 35
65FE2 G %IG=0.43 6
65FE G 455.6 1 24.4 18 [E2] 1.84E-3 3 C
65FES G KC=0.001652 23$LC=0.0001600 22$MC=2.199E-5 31
65FES G NC=9.93E-7 14
65FE2 G %IG=13.2 11
65FE L 560.74 6 (3/2,5/2-) 390 PS 30
65FE cL T$from Table IV and text of 2013Ol06, uncertainty is listed as 50 ps
65FE2cL in authors' level-scheme figure 7 and table II
65FE B 1.14 22 6.2 1
65FES B EAV=4533.8 29
65FE cB IB$1.5 {I2} (2013Ol06)
65FE G 163.1 1 0.7 1 [M1,E1] 0.0096920 C
65FES G KC=0.00872 18$LC=0.000843 25$MC=0.000116 4
65FES G NC=5.25E-6 20
65FE2 G %IG=0.38 6
65FE G 197.6 3 1.4 1 [M1,E1] 0.0057 4 AC
65FES G KC=0.00514 33$LC=0.00050 4$MC=6.8E-5 5
65FES G NC=3.10E-6 25
65FE2 G %IG=0.76 6
65FE G 560.8 1 2.7 2 [D,E2] C
65FE2 G %IG=1.46 12
65FE L 569.05 6 (3/2,5/2-) 12 PS LT
65FE cL J$(1/2,3/2) proposed in 2013Ol06 by excluding E2 and M2 for 569|g to
65FE2cL (1/2-) ground state. However, E2 cannot be completely ruled out based
65FE3cL on RUL=300 for B(E2)W.u., which would only require a T{-1/2}>1.9 ps
65FE4cL that overlaps with the limit of <12 ps proposed in 2013Ol06.
65FE B 0.8 4 6.4 +3-2
65FES B EAV=4529.9 29
65FE cB IB$0.9 {I4} (2013Ol06)
65FE G 205.3 2 0.3 1 [D,E2] C
65FE2 G %IG=0.16 6
65FE G 569.1 1 8.4 6 [D,E2] C
65FE2 G %IG=4.5 4
65FE L 609.45 14 (7/2+)
65FE B 0.92 19 6.3 1
65FES B EAV=4510.4 29
65FE cB IB$1.0 {I1} (2013Ol06)
65FE G 215.8 1 2.9 2 C
65FE2 G %IG=1.56 12
65FE L 683.26 5 (3/2,5/2-) 24 PS 12
65FE cL T$from Table IV and text of 2013Ol06, uncertainty is listed as 10 ps
65FE2cL in authors' level-scheme figure 7
65FE B 1.9 4 6.0 1
65FES B EAV=4474.3 29
65FE cB IB$2.1 {I3} (2013Ol06)
65FE G 114.5 3 0.2 1 [D,E2] AC
65FE2 G %IG=0.11 6
65FE G 227.7 1 2.5 2 [D,E2] C
65FE2 G %IG=1.35 12
65FE G 319.7 1 4.4 3 [D,E2] C
65FE2 G %IG=2.37 18
65FE G 683.3 1 3.6 3 [D,E2] @C
65FEF G FLAG=D
65FE2 G %IG=1.94 18
65FE L 894.72 7 (7/2-) 27 PS LT
65FE B 1.19 24 6.1 1
65FES B EAV=4371.0 29
65FE cB IB$1.4 {I2} (2013Ol06)
65FE G 439.2 1 3.5 3 [M1,E2] 0.0015 6 C
65FES G KC=0.0013 5$LC=1.3E-4 5$MC=1.8E-5 7
65FES G NC=8.1E-7 31
65FE2 G %IG=1.89 18
65FE G 531.1 1 1.1 1 [E2] 1.12E-3 2 C
65FES G KC=0.001013 14$LC=9.77E-5 14$MC=1.344E-5 19
65FES G NC=6.10E-7 9
65FE2 G %IG=0.59 6
65FE L 1057.29 6 (3/2-,5/2-) 8 PS LT D
65FE B 2.64 22 5.74 4
65FES B EAV=4292.1 29
65FE cB IB$2.9 {I2} (2013Ol06)
65FE G 374.1 1 1.0 1 [D,E2] C
65FE2 G %IG=0.54 6
65FE G 488.3 2 0.2 1 [D,E2] C
65FE2 G %IG=0.11 6
65FE G 601.7 1 0.9 1 [M1,E2] C
65FES G CC=6.1E-4 16$KC=5.5E-4 14$LC=5.3E-5 14$MC=7.3E-6 19
65FES G NC=3.3E-7 9
65FE2 G %IG=0.49 6
65FE G 659.7 1 0.8 1 [E1] C
65FES G CC=0.0002038 29$KC=0.0001838 26$LC=1.747E-5 24$MC=2.404E-6 34
65FES G NC=1.111E-7 16
65FE2 G %IG=0.43 6
65FE G 693.7 1 2.2 2 [M1,E2] C
65FES G CC=0.00042 9$KC=0.00038 8$LC=3.6E-5 8$MC=5.0E-6 11
65FES G NC=2.3E-7 5
65FE2 G %IG=1.19 12
65FE G 1057.2 1 0.7 1 [M1,E2]
65FES G CC=0.000156 16$KC=0.000140 14$LC=1.34E-5 14$MC=1.84E-6 19
65FES G NC=8.5E-8 8
65FE2 G %IG=0.38 6
65FE L 1088.80 5 (3/2-,5/2-) 8 PS LT D
65FE B 18.9 12 4.88 3
65FES B EAV=4276.5 29
65FE cB IB$20.7 {I9} (2013Ol06)
65FE G 405.6 1 1.8 1 [D,E2] C
65FE2 G %IG=0.97 7
65FE G 519.8 1 4.3 3 [D,E2] C
65FE2 G %IG=2.32 18
65FE G 528.1 1 0.9 1 [D,E2] C
65FE2 G %IG=0.49 6
65FE G 633.2 1 2.2 2 [M1,E2] C
65FES G CC=0.00053 13$KC=0.00048 12$LC=4.6E-5 11$MC=6.3E-6 16
65FES G NC=2.9E-7 7
65FE2 G %IG=1.19 12
65FE G 691.5 5 0.4 LT [E1] C
65FES G CC=0.0001831 26$KC=0.0001652 23$LC=1.570E-5 22$MC=2.160E-6 30
65FES G NC=9.99E-8 14
65FE2 G %IG=0.11 11
65FE cG E,RI$|g observed only in delayed coincidence of 363.7|g
65FE G 725.2 1 8.8 7 [M1,E2] C
65FES G CC=0.00038 7$KC=0.00034 7$LC=3.2E-5 6$MC=4.5E-6 9
65FES G NC=2.1E-7 4
65FE2 G %IG=4.7 4
65FE G 1088.6 1 16.9 13 [M1,E2]
65FES G CC=0.000146 14$KC=0.000132 12$LC=1.25E-5 12$MC=1.73E-6 17
65FES G NC=8.0E-8 7
65FE2 G %IG=9.1 8
65FE L 1228.19 21 (3/2,5/2,7/2)
65FE B 0.22 6 6.8 +2-1
65FES B EAV=4208.7 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE G 772.6 2 0.4 1 C
65FE2 G %IG=0.22 6
65FE L 1366.62 6 (5/2-) 8 PS LT D
65FE B 5.77 35 5.34 4
65FES B EAV=4141.0 29
65FE cB IB$6.3 {I3} (2013Ol06)
65FE G 472.0 1 0.9 1 [M1,E2] 0.0012 4 C
65FES G KC=0.0011 4$LC=1.0E-4 4$MC=1.4E-5 5
65FES G NC=6.5E-7 23
65FE2 G %IG=0.49 6
65FE G 683.3 1 2.6 2 [D,E2] @C
65FEF G FLAG=D
65FES G CC=0.00044 9$KC=0.00039 8$LC=3.8E-5 8$MC=5.2E-6 11
65FES G NC=2.4E-7 5
65FE2 G %IG=1.40 12
65FE G 757.2 2 0.2 1 [E1] C
65FES G CC=0.0001499 21$KC=0.0001352 19$LC=1.284E-5 18$MC=1.768E-6 25
65FES G NC=8.19E-8 11
65FE2 G %IG=0.11 6
65FE G 796.9 1 0.5 1 [D,E2] AC
65FEF G FL=569.05
65FE2 G %IG=0.27 6
65FE cG E$poor fit, level-energy difference=797.57
65FE G 805.9 2 0.3 1 [D,E2] C
65FES G CC=0.00029 5$KC=0.00026 4$LC=2.5E-5 4$MC=3.4E-6 6
65FES G NC=1.59E-7 26
65FE2 G %IG=0.16 6
65FE G 911.1 2 0.3 1 [M1,E2] C
65FES G CC=0.000217 29$KC=0.000196 26$LC=1.87E-5 25$MC=2.57E-6 34
65FES G NC=1.19E-7 15
65FE2 G %IG=0.16 6
65FE G 969.1 1 0.8 1 [E1] C
65FES G CC=9.02E-5 13$KC=8.14E-5 11$LC=7.72E-6 11$MC=1.063E-6 15
65FES G NC=4.93E-8 7
65FE2 G %IG=0.43 6
65FE G 1002.9 1 4.8 4 [M1,E2] C
65FES G CC=0.000175 19$KC=0.000158 17$LC=1.50E-5 17$MC=2.07E-6 23
65FES G NC=9.6E-8 10
65FE2 G %IG=2.59 24
65FE G 1366.2 4 0.3 1 [E2]
65FES G CC=0.0001415 20$KC=8.72E-5 12$LC=8.28E-6 12$MC=1.141E-6 16
65FES G NC=5.30E-8 7$IPC=4.49E-5 6
65FE2 G %IG=0.16 6
65FE L 1372.36 11 (3/2+,5/2,7/2)
65FE B 0.27 9 6.7 +2-1
65FES B EAV=4138.5 29
65FE cB IB$0.3 {I1} (2013Ol06)
65FE G 763.0 3 0.2 1 C
65FE2 G %IG=0.11 6
65FE G 811.6 1 0.3 1 C
65FE2 G %IG=0.16 6
65FE L 1449.1 4 (1/2+,3/2,5/2-)
65FE B 0.22 6 6.7 +2-1
65FES B EAV=4101.0 29
65FE cB IB$0.3 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(1449)=3/2 and 5/2-; for J=1/2+, it
65FE2cB should be 9.0 {I+2-1} for 1st forbidden unique.
65FE G 1449.1 4 0.4 1
65FE2 G %IG=0.22 6
65FE L 1457.2 5 (3/2,5/2,7/2)
65FE B 0.43 7 6.4 1
65FES B EAV=4097.1 29
65FE cB IB$0.5 {I1} (2013Ol06)
65FE G 1001.6 5 0.8 1 AC
65FE2 G %IG=0.43 6
65FE L 1472.0 6 (1/2,3/2,5/2-)
65FE B 0.11 LT 7.0 GT
65FES B EAV=4089.8 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE G 1472.0 6 0.1 1
65FE2 G %IG=0.05 5
65FE L 1530.0 5
65FE B 0.11 6 7.0 +3-2
65FES B EAV=4061.5 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE G 1132.4 5 0.2 1 C
65FE2 G %IG=0.11 6
65FE cG RI$from Table I of 2013Ol06; 0.3 listed in authors' level-scheme
65FE2cG figure 7
65FE L 1558.86 7 (3/2-,5/2-)
65FE B 2.21 19 5.71 4
65FES B EAV=4047.4 29
65FE cB IB$2.4 {I1} (2013Ol06)
65FE G 875.7 1 0.8 1 C
65FE2 G %IG=0.43 6
65FE G 989.7 1 0.7 1 C
65FE2 G %IG=0.38 6
65FE G 1103.2 1 1.4 1 C
65FE2 G %IG=0.76 6
65FE G 1161.5 3 0.5 1 C
65FE2 G %IG=0.27 6
65FE G 1195.2 2 0.6 1 C
65FE2 G %IG=0.32 6
65FE G 1559.4 4 0.1 1
65FE2 G %IG=0.05 5
65FE L 1674.2 7 (1/2,3/2,5/2-)
65FE B 0.11 LT 7.0 GT
65FES B EAV=3991.3 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE G 1674.2 7 0.1 1
65FE2 G %IG=0.05 5
65FE L 1693.67 10 (3/2-,5/2-)
65FE B 1.24 12 5.93 5
65FES B EAV=3981.6 29
65FE cB IB$1.3 {I1} (2013Ol06)
65FE G 1124.6 5 0.2 1 AC
65FE2 G %IG=0.11 6
65FE G 1296.2 2 0.6 1 C
65FE2 G %IG=0.32 6
65FE G 1330.0 1 1.2 1 C
65FE2 G %IG=0.65 6
65FE G 1693.7 4 0.3 1
65FE2 G %IG=0.16 6
65FE L 1732.51 15 (5/2-)
65FE B 1.24 13 5.92 5
65FES B EAV=3962.6 29
65FE cB IB$1.4 {I1} (2013Ol06)
65FE G 837.6 5 0.6 1 AC
65FE2 G %IG=0.32 6
65FE G 1123.0 2 0.6 1 C
65FE2 G %IG=0.32 6
65FE G 1163.6 3 0.2 1 AC
65FE2 G %IG=0.11 6
65FE G 1368.9 3 0.6 1 C
65FE2 G %IG=0.32 6
65FE G 1732.5 4 0.3 1
65FE2 G %IG=0.16 6
65FE L 1853.34 16 (3/2-,5/2,7/2)
65FE B 1.08 17 6.0 1
65FES B EAV=3904.1 29
65FE cB IB$1.2 {I1} (2013Ol06)
65FE G 796.4 4 0.9 2 C
65FE2 G %IG=0.49 11
65FE cG RI$from Table I of 2013Ol06; uncertainty is listed as 0.1 in authors'
65FE2cG level-scheme figure 7
65FE G 958.5 2 0.9 1 C
65FE2 G %IG=0.49 6
65FE G 1397.8 3 0.2 1 C
65FE2 G %IG=0.11 6
65FE L 2001.93 16 (3/2+,5/2,7/2)
65FE B 0.59 12 6.2 1
65FES B EAV=3831.4 29
65FE cB IB$0.7 {I1} (2013Ol06)
65FE G 1318.7 2 0.6 1 C
65FE2 G %IG=0.32 6
65FE G 1392.4 4 0.2 1 C
65FE2 G %IG=0.11 6
65FE cG RI$from Table I of 2013Ol06; 0.3 listed in authors' level-scheme
65FE2cG figure 7
65FE G 1432.8 3 0.3 1 C
65FE2 G %IG=0.16 6
65FE L 2301.3 8 (1/2,3/2,5/2-)
65FE B 0.11 LT 6.8 GT
65FES B EAV=3685.7 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE G 2301.3 8 0.1 1
65FE2 G %IG=0.05 5
65FE L 2341.5 7 (1/2,3/2,5/2-)
65FE B 0.11 LT 6.8 GT
65FES B EAV=3666.2 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE G 2341.4 7 0.1 1
65FE2 G %IG=0.05 5
65FE L 2520.18 41 (1/2+:7/2)
65FE B 0.22 6 6.5 +2-1
65FES B EAV=3579.0 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(2520)=3/2,5/2,7/2; for J=1/2+, it
65FE2cB should be 8.6 {I+2-1} for 1st forbidden unique.
65FE G 1951.1 4 0.4 1 C
65FE2 G %IG=0.22 6
65FE L 2639.0 8 (1/2,3/2,5/2-)
65FE B 0.11 LT 6.7 GT
65FES B EAV=3521.0 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE G 2638.9 8 0.1 1
65FE2 G %IG=0.05 5
65FE L 2690.5 8 (1/2+,3/2,5/2-)
65FE B 0.11 6 6.7 +3-2
65FES B EAV=3496.1 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(2691)=3/2,5/2-; for J=1/2+, it
65FE2cB should be 8.9 {I+3-2} for 1st forbidden unique.
65FE G 2690.4 8 0.2 1
65FE2 G %IG=0.11 6
65FE cG RI$from Table I of 2013Ol06; 0.1 listed in authors' level-scheme
65FE2cG figure 7
65FE L 2780.3 8 (1/2+,3/2,5/2-)
65FE B 0.11 6 6.7 +3-2
65FES B EAV=3452.3 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(2780)=3/2,5/2-; for J=1/2+, it
65FE2cB should be 8.8 {I+3-2} for 1st forbidden unique.
65FE G 2780.2 8 0.2 1
65FE2 G %IG=0.11 6
65FE L 2839.9 8 (1/2+,3/2,5/2-)
65FE B 0.16 6 6.5 2
65FES B EAV=3423.0 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(2840)=3/2,5/2-; for J=1/2+, it
65FE2cB should be 8.6 {I2} for 1st forbidden unique.
65FE G 2839.8 8 0.3 1
65FE2 G %IG=0.16 6
65FE L 2898.5 8 (1/2+:7/2-)
65FE B 0.16 6 6.5 2
65FES B EAV=3394.8 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(2899)=3/2,5/2,7/2-; for J=1/2+, it
65FE2cB should be 8.6 {I2} for 1st forbidden unique.
65FE G 2534.8 8 0.3 1 C
65FE2 G %IG=0.16 6
65FE L 2932.49 41 (3/2,5/2,7/2)
65FE B 0.32 7 6.2 1
65FES B EAV=3378.2 29
65FE cB IB$0.4 {I1} (2013Ol06)
65FE G 2371.7 4 0.6 1 C
65FE2 G %IG=0.32 6
65FE L 3013.5 5 (3/2,5/2-)
65FE B 0.43 9 6.1 1
65FES B EAV=3338.7 29
65FE cB IB$0.5 {I1} (2013Ol06)
65FE G 2444.8 7 0.3 1 C
65FE2 G %IG=0.16 6
65FE cG RI$from Table I of 2013Ol06; 0.6 listed in authors' level-scheme
65FE2cG figure 7
65FE G 3013.1 6 0.5 1
65FE2 G %IG=0.27 6
65FE cG E$from Table I of 2013Ol06; 3013.5 listed in authors' level-scheme
65FE2cG figure 7
65FE L 3245.1 7 (3/2,5/2,7/2)
65FE B 0.22 6 6.3 +2-1
65FES B EAV=3225.7 29
65FE cB IB$0.3 {I1} (2013Ol06)
65FE G 2561.8 7 0.4 1 C
65FE2 G %IG=0.22 6
65FE L 3306.1 9 (1/2+,3/2,5/2-)
65FE B 0.16 6 6.4 2
65FES B EAV=3196.0 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(3306)=3/2,5/2-; for J=1/2+, it
65FE2cB should be 8.5 {I2} for 1st forbidden unique.
65FE G 3306.0 9 0.3 1
65FE2 G %IG=0.16 6
65FE L 3374.0 8 (1/2+,3/2,5/2-)
65FE B 0.11 6 6.5 +3-2
65FES B EAV=3162.9 29
65FE cB IB$0.1 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(3374)=3/2,5/2-; for J=1/2+, it
65FE2cB should be 8.5 {I+3-2} for 1st forbidden unique.
65FE G 3373.9 8 0.2 1
65FE2 G %IG=0.11 6
65FE L 3399.3 5 (1/2+:7/2-)
65FE B 0.16 6 6.4 2
65FES B EAV=3150.7 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(3399)=3/2,5/2,7/2-; for J=1/2+, it
65FE2cB should be 8.4 {I2} for 1st forbidden unique.
65FE G 3035.6 5 0.3 1 C
65FE2 G %IG=0.16 6
65FE L 3421.0 9 (1/2+,3/2,5/2-)
65FE B 0.16 6 6.4 2
65FES B EAV=3140.0 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE cB LOGFT$calculated as allowed for J(3421)=3/2,5/2-; for J=1/2+, it
65FE2cB should be 8.4 {I2} for 1st forbidden unique.
65FE G 3420.9 9 0.3 1
65FE2 G %IG=0.16 6
65FE L 4095.84 41 (3/2-,5/2-,7/2-)
65FE B 0.32 7 5.9 1
65FES B EAV=2811.3 29
65FE cB IB$0.3 {I1} (2013Ol06)
65FE G 3535.0 4 0.6 1 C
65FE2 G %IG=0.32 6
65FE L 4438.4 9 (3/2,5/2-)
65FE B 0.16 6 6.0 2
65FES B EAV=2644.9 29
65FE cB IB$0.2 {I1} (2013Ol06)
65FE G 4438.2 9 0.3 1
65FE2 G %IG=0.16 6
65FE L 4320+X R
65FE cL E$x<5931 {I5} from Q(|b{+-})({+65}Mn)-S(n)({+65}Fe), where
65FE2cL Q(|b{+-})=10251 {I6} and S(n)=4320 {I7} from 2021Wa16. This represents
65FE3cL a range of unobserved levels that subsequently decay to {+64}Fe via
65FE4cL one-neutron emission.
65FE B 7.9 12 4.4
65FE cB IB$from adopted %|b{+-}n=7.9 {I12} for {+65}Mn decay, deduced by
65FE2cB 2013Ol06 based on their measured intensity of 1345.8|g in {+64}Ni from
65FE3cB the decay chain of {+65}Mn |b{+-}n decay to {+64}Fe, then |b{+-} decay
65FE4cB to {+64}Co, then |b{+-} decay to {+64}Ni, and %I|g(1345.8|g)=7.54
65FE5cB deduced by 2013Ol06 using data in 2012Pa39 for {+64}Co |b{+-} decay.
65FES B EAV=2702.3