# LEVEL

level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$487.4|g D+Q, |DJ=1 to 3/2-; L(d,{+3}He)=3 from 0+ 
T$from <0.1 ns from |b|g(t) in |b{+-} decay (4.140 h) and >23 ps from measured width in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=0 from 3/2- 
T$from DSAM in Coulomb excitation. Others: 22 ps {I+12-9} from B(E2)|^=0.0080 {I13} in Coulomb excitation with adopted branching and |d=-0.37 {I6} for 512|g; >4.7 ps from measured width in (|g,|g'), both in disagreement with DSAM value from Coulomb excitation. Either level T{-1/2} or |d(E2/M1) may be in error if B(E2) values from Coulomb excitation are considered correct. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$3/2 from |g excitation function in (n,n'|g); L(p,|a)=1 from 0+ 
T$weighted average of 0.24 ps {I16} from DSAM in Coulomb excitation and 0.67 ps {I6} from width in (|g,|g') 
$B(E2)|^: unweighted average of 0.0020 {I3} from Coulomb excitation and 0.00056 {I33} in (e,e') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=3 from 0+; 964.7|g M1+E2 to 3/2-. J|p=7/2(-) assigned in ({+7}Li,|a2n|g) is inconsistent; Mult=Q with |DJ=2 for 453|g to 3/2- and 965|g to 3/2- in ({+7}Li,|a2n|g) could imply a different level with close energy. 
T$from measured width in (|g,|g'). Others: 2.2 ps {I+14-9} from adopted B(E2)|^=0.022 {I6}, |d=+1.3 {I3} and branching=76.5% {I15} for 964.7|g; >0.76 ps from DSAM in Coulomb excitation 
$B(E2)|^: unweighted average of 0.032 {I5} (1972An17) and 0.024 {I13} (2010Di14) in Coulomb excitation, and 0.0112 {I37} in (e,e') 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$595.9|g E2, |DJ=2 to 3/2-; 620.1|g M1+E2 to 5/2- 
T$from B(E2)|^ in Coulomb excitation (1972An17), and adopted branching=2.05% {I9} for 1107.3|g. Other: >0.21 ps from DSAM in {+68}Zn(|a,p|g); <0.1 ns from |b|g(t) in |b{+-} decay (4.140 h) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
J$L(d,{+3}He)=1 from 0+; spin=1/2 from |g excitation function in (n,n'|g) 
T$from measured width in (|g,|g'). Other: 0.13 ps {I+8-4} from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$1395.3|g E2, |DJ=2 to 3/2-; L(d,{+3}He)=3 from 0+ 
T$weighted average of 0.76 ps {I5} from DSAM in Coulomb excitation and 1.1 ps {I3} from measured width in (|g,|g'). Other: 1.00 ps {I+21-15} from measured B(E2)|^ in Coulomb excitation and adopted branching=44.8% {I7} for 1395.3|g; 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J$|DJ=2, Q 1010.9|g to 5/2-; 952.4|g from 7/2+; 1010.9|g not M2 since it would require an isomeric T{-1/2}>1.5 ns, inconsistent with the observation of very strong prompt 1010.9|g in ({+7}Li,|a2n|g) J=5/2,7/2 proposed in (n,n'|g), possibly on the basis of excitation functions and |g(|q), is in disagreement. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=0 from 3/2- 
T$from DSAM in (n,n'|g). Other: >13 fs from measured width in (|g,|g') 
$B(E2)|^ from (e,e') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$L({+3}He,d)=0 from 0+. Note that L({+3}He,d)=1+3 has also been suggested by 1974Ze01 for 1713 {I15} group. While it is inconsistent with L=0, but it may be a doublet with the other member possibly associated with 1719.6, (5/2)- level. 
T$from measured width in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$1719.6|g M1+E2 to 3/2-; 527.7|g from 7/2+ cannot be M2 from RUL. (5/2) also from |g(|q) in (n,n'|g). See also comment for 1699 level for possible doublet in ({+3}He,d) 
T$weighted average of 0.10 ps {I+5-2} from DSAM in (n,n'|g) and 0.16 ps {I5} from measured width in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$(11/2)- assigned in ({+7}Li,|a2n|g) with J(964)=7/2(-); evaluators assign (9/2-) from |DJ=2, Q |g to 964, 5/2- 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$(3/2) from excitation function in (n,n'|g); 546.6|g to 7/2- favors |p=-. But |p=(+) from L(t,p)=(3) from 3/2- is in disagreement, which could indicate different level in (t,p) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: FS
level_comment:
J$log| {Ift}=6.0 for |b{+-} decay from 1/2- state; L(t,p)=2 
T$T{-1/2}/(2J+1)=25.7 fs {I45} from measured width gives: 51 fs {I9} if J=1/2; 103 fs {I18} if J=3/2 from (|g,|g'). The adopted value of 82 fs {I40} is selected to cover the ranges of both possible T{-1/2} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$spin=7/2 from |g excitation function in (n,n'|g); 753.4|g M1+E2 to 9/2+; L(t,p)=3 from 3/2-. log| {Ift}=5.99 from 9/2+ rules out 5/2 
T$from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$L({+3}He,d)=1 from 0+; spin=1/2 from excitation function in (n,n'|g); also supported by log {Ift}=4.9 from 1/2- parent 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$weighted average of 2529 {I10} from (t,p) and 2516 {I30} from ({+3}He,d) 
J$L({+3}He,d)=1 from 0+. But L(t,p)=(4) from 3/2- seems in disagreement 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2-)
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(23/2-) in ({+7}Li,|a2n|g); evaluators assign (21/2-) from |g to 3909, (17/2-) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$S'=0.17 {I6} 
E$IAR of 1261 level in {+71}Zn 
$E(p)|?5071, |G{-p}=0.6 keV {I2} 
E$ data indicate other weak resonances may be present 


level_energy_unit: KEV
level_comment:
E$doublet; other member of the doublet is probably the level at 1475 with J|p=5/2- thus requiring L=3. 
S$2.90-3.60 (for L=4, J=9/2+), 0.29 (for L=(2), J=(5/2+)) component 
S$ 5.3, L=4(+1) (1974Ze01) 


level_energy_unit: KEV
level_comment:
$L=1+3 in 1974Ze01, implying a doublet, is in disagreement. 
S$0.9 for L=3 or 0.1 for L=1 (1974Ze01) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$B(E2)|^: from 1972An17. Other: 0.0087 {I35} from measured B(E2)(W.u.)=5 {I2} (2010Di14) 
T$other: 22 ps {I+12-9} from B(E2)|^=0.0080 {I13}, adopted branching of 91.98% {I23} for 511|g, and adopted |d(511.6|g)=-0.37 {I6} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^=0.032 {I5}, adopted branching=76.5% {I15} and adopted |d=1.3 {I3}. Other: >0.76 ps (DSAM,1974Iv03) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^=0.0029 {I5} and adopted branching=2.05% {I9} for 1107|g. Other: >0.21 ps (DSAM,1974Iv03) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$others: 1.00 ps {I+21-15} from B(E2)|^=0.0096 {I14} and adopted branching=44.8% {I7}; 0.32 ps from DSAM (1973AnZX) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$values from this dataset: <0.1 ns (1967Li01), <0.5 ns (1969Co20) 
$|m=0.95 {I5} (1975BeYD), but no details are provided 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
J$from level-scheme Fig. 1 in 2021Zh44, 1/2- as J|p of initial level in authors' Table 1 for 487.5|g, 5/2- as J|p of final level for 620|g and 1010|g 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: H
level_comment:
J$spin from atomic-beam measurement (1960Ch13), parity from |b|g directional correlations, {+72}Ga |b{+-} decay. For |b{+-} decay to 2+ states in {+72}Ge, anisotropy of |b|g(|q) shows |b{+-} transition is of forbidden nature. 
T$weighted average of 14.1 h {i2} (1939Sa02), 14.25 h {i20} (1943Ma03), 14.08 h {i2} (1950Bi20), 14.25 h {i10} (1950Si02), 14.12 h {i2} (1961Wy01) and 14.3 h {i3} (1974BaZB) 
MOMM1$Atomic beam (1962Eh02, 2005St24). 
MOME2$Atomic beam, recalculated to include polarization correction (1972St38, 2005St24). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$spin from dipole radiation to 3- g.s. and from 1+ states at 161 and 208; parity from L(d,{+3}He)=3. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: MS
level_comment:
J$from (M2) |g to 2- and d |g's from 1+ states, lack of |b{+-} feeding and no |g to 3- g.s. 
T$from 1972Br53, {+71}Ga(n,|g). Other: 35 ms {i6} from {+72}Zn |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: H
level_comment:
J$ from Adopted Levels of {+72}Ga in ENSDF database 
T$ Measured by 2012Kr07 from decay curves for 630, 834, 894, 1051, 2202, 2491 and 2508-keV |g rays for at least two half-lives, and for three different samples. Final result is based on weighted average of 18 data points. Systematic and fitting uncertainties are included. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|d<r{+2}>({+71}Ga,{+72}Ga)=+0.161 fm{+2} {I8}(stat) {I26}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+72}Ga)=+23 MHz {I3}(stat) {I2}(syst) (2012Pr11) 
J$from {+72}Ga Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: H
level_comment:
J$From Adopted Levels of {+72}Ga in ENSDF database. 
T$From 2016Ak04, average of 13.4 h {I8} from 630|g(t), 13.9 h {I2} from 834|g(t), and 12 h {I2} from 2201|g(t). Systematic and fitting uncertainties are included. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$Capture rate to excited states (feeding g.s.)=0.026|*10{+6} s{+-1} {I7}, corresponding to a percentage is 0.40% {I11} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: h
level_comment:
T$Measured decay curves for 630 and 834 keV |g-rays. Final value taken from weighted average for three different samples (2024Do05). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
$|d<r{+2}>({+71}Ga,{+73}Ga)=+0.243 fm{+2} {I4}(stat) {I42}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+73}Ga)=+15.5 MHz {I15}(stat) {I40}(syst) (2012Pr11) 
J$spin from collinear laser spectroscopy (2010Ch16, observation of only three lines in the hyperfine spectrum gives unambiguous 1/2 assignment); parity from allowed |b{+-} decay (log| {Ift}=5.3 to 1/2-, 1132 level in {+73}Ge. Considering J{+|p}(g.s.)=3/2- for neighboring odd-A Ga isotopes, the anomalous J{+|p}(g.s.)=1/2- of {+73}Ga suggests a changing shell structure from N=42 onwards and strong influence of |pf{-5/2} orbital in the g.s. wave function. Previously adopted J{+|p}(g.s.)=3/2-, based on L-transfers in (t,p) and (d,{+3}He), corresponds to an almost degenerate level (2010Ch16), a conclusion also supported by 2010Di14 in Coulomb excitation. 
T$from 1976Fo07. Others: 4.91 h {I5} (1970Wa21), 4.85 h {I10} (1958Yt22), 1960Ku04, 1973McZP. 
MOMM1$from collinear laser spectroscopy (2010Ch16). Note that in 2016St14 evaluation, Q=+0.209 {I2} from 2010Ch16 is incorrectly listed. 


level_energy_unit: KEV
level_energy_info: ;ERR=LT;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: MS
level_lifetime_info: ;ERR=LT;ISO=M
level_comment:
E$from <0.3 keV, deduced by 2017Ve05 in the study of {+73}Zn decay. Other estimates: 0.4 keV {I4} (2010Di14, Coulomb excitation); 0.075-1 keV (2010Ch16, 0.075 keV limit from assumption of T{-1/2}>200 ms based on their experimental conditions, and by assuming same B(M1) as for 3/2- to 1/2- transition in {+71}Ga; 1 keV cited by 2010Ch16 from theoretical estimate in 2009St12, but perusal of 2009St12 suggests a possibility of 1/2- g.s. and a closely-spaced 3/2- but does not give the spacing of 1 keV); 9 keV (2011Ji08, shell-model calculations, 1/2- g.s. is reproduced) 
T$expected to be <200 ms, as a 3/2- level is not seen in the hyperfine structure study by 2010Ch16 who mention that due to slow release of Ga from their ion source and the accumulation time in the cooler, the half-life of the 3/2- state would have to be >200 ms to be observed in their study, assuming equal production of 1/2- and 3/2- states. 
J$L(t,p)=0 from 3/2-; L(d,{+3}He)=1 from 0+ together with vector analyzing power 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$5/2-,7/2- from L(d,{+3}He)=3; 7/2- is ruled out by population in Coulomb excitation (2010Di14); J=5/2 is also from measured polarization asymmetry in 2008KaZT in (d,{+3}He) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=3 from 0+ and L(t,p)=2 from 3/2-. J{+|p}=7/2- from measured polarization asymmetry in 2008KaZT in (d,{+3}He). Direct population of the 496-keV state via Coulomb excitation from 1/2- ground state, however, limits the spin of this state to be 5/2- (2010Di14) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$proposed by 2010Di14 in Coulomb excitation based on observed population compatible with single-step Coulomb excitation from 1/2- g.s.; L(t,p)=4 from 3/2- for a level at 1396 {I3} 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E$weighted average of 1578 {I3} from (t,p) and 1576 {I6} from (|a,p) 
J$from comparisons of measured |s(|q) in {+70}Zn(|a,p) with those for states of known J|p in {+68}Zn(|a,p) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
E$weighted average of 1771 {I3} from (t,p) and 1777 {I7} from (d,{+3}He) 
J$L(d,{+3}He)=(3) from 0+ and L(t,p)=2 from 3/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$L(d,{+3}He)=1 from 0+ and L(t,p)=2 from 3/2-. But 5/2 preferred from cross section in (|a,p) for a level at 1939 {I8} 


level_energy_unit: KEV
level_energy_info: ;ERR=LT;ERR=?
level_spin_parity: 3/2-
level_comment:
E$from Adopted Levels, where almost degenerate 1/2- g.s. and first excited 3/2- level are given. 2008KaZT and 1978Ro14 assigned L=1 to the g.s. but this L-transfer and the vector analyzing power measurement in 2008KaZT suggest that this level corresponds to the 3/2-, <0.3 keV level, instead, and that 1/2- g.s. is not populated in this reaction 
J$vector analyzing power=-0.094 {I8} (2008KaZT) gives 3/2- 
S$other: 1.33 (1978Ro14) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$5/2-,7/2- is adopted in Adopted Levels, with 5/2- from direct population the 496-keV state via Coulomb excitation from 1/2- g.s. 
S$from 1978Ro14 for J=7/2. Other: 0.32 for J=5/2 (1978Ro14) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$existence of a level near the 1/2- g.s. is deduced from the observed Doppler-broadening of 199.2|g from the 199.2, 5/2- level, which restricts the lifetime of the 5/2- level considerably smaller than 3.5 ns (maximum time-of-flight between target and detector), consistent with the lifetime=3.3 ps from Weisskopf estimate for a pure 199-keV M1 transition to a level with J|p between 3/2- and 7/2- but not with 13 ns {I2} from measured B(E2)(W.u.)=11 {I2} for the assumption of a pure E2 to 1/2- g.s. 
E$the energy of this level is estimated by 2010Di14 as 0.4 keV {I4} from adopted E|g=496.07 {I12} from 496 level and E|g=218.08 {I11} and 278.5 {I3} cascade adding to 496.5 {I4}. Energy is 0.15 keV {I15} in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$The population of this state by Coulomb excitation from 1/2- g.s. can only take place by a two-step process (2010Di14) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$proposed by 2010Di14 from observed population compatible with single-step Coulomb excitation from 1/2- g.s. A two-step excitation would require unreasonably large B(E2) values between this state and 3/2- and 5/2- states leading to strong |g-decay branches to these states which however are not observed (2010Di14) 
T$2.0 ps {I+6-5} from B(E2)(W.u.)=3.0 {I7} if 1395|g to 1/2- g.s. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: MIN
level_comment:
$|d<r{+2}>({+71}Ga,{+74}Ga)=+0.223 fm{+2} {I5}(stat) {I45}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+74}Ga)=-32 MHz {I2}(stat) {I6}(syst) (2012Pr11) 
J$from hyperfine structure measurements by 2011Ma45, J=1 is ruled out by the number of atomic transitions and selection rules. J=2,3,4 possibilities were analyzed and reduced |h{+2} considered for the fitting of the hyperfine spectrum. For {+74}Ga, J=3 is the most likely choice, but J=4 could not be completely ruled out. Spins higher than 4 gave poorer match to the observed spectra. Negative parity is suggested by the comparison of measured and theoretical magnetic dipole moments and electric quadrupole moments. Additional arguments in favor of J=3: log| {Ift}=7.9 to 2+ and 4+ levels in {+74}Ge. Systematics suggest 3-, 2-, 0+ for the 0, 56.5 and 59.6 levels, respectively, as for example in {+72}Ga. Shell-model calculations by 2012Sr01 using JUN45 interaction support 3- for ground state, with also reasonable agreement of theoretical and experimental static quadrupole moments. The 4- state in these calculations is at about 225 keV excitation. 
MOMM1,MOME2$from hyperfine structure measurements (2011Ma45). The values are for J=3. For J=4, |m=0.000 {I75}, Q=+0.604 {I42} (2011Ma45) 
T$from |g-decay curves in {+74}Ga |b{+-} decay; unweighted average of 8.00 min {I5} (1975Ta03) and 8.25 min {I5} (1971Ca06). Others: 1967Vi08, 8 min (1962Ei02), 7.7 min {I4} (1960Ma12), 8.0 min {I1} (1959Yt23), 7.8 min {I2} (1958Ei02), 8 min {I1} (1958Le26), |?8 min (1956Mo39) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
J$dipole transition to (3-); |g from 1+; systematics of neighboring nuclides support negative parity 
T from |g|g(t) (1977Va01) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$ No |b{+-} branch observed (1974Va08). An upper limit is suggested as 50% (1974Va08) 
E$from observation of sum peak. See {+74}Ga IT decay (1974Va08) 
J$|g to (2); positive parity is suggested by the systematics of neighboring nuclides; long lifetime of this level is consistent with this assignment. 
T$from {+74}Ga IT decay (1974Va08) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$Capture rate to excited states (feeding g.s.)=0.026|*10{+6} s{+-1} {I6}, corresponding to a percentage is 0.40% {I9} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_comment:
J$ spin from hyperfine structure (2010Ch16) using collinear laser spectroscopy at ISOLDE, CERN; parity from analyzing powers in (pol d,{+3}He) 
T$from 1974Gr29. Others: 130 s {I6} (1974Ch22), 120 s {I12} (1960Mo01) 90 s {I30} (1960Yt01). 
MOMM1,MOME2$ hyperfine structure (2010Ch16) using collinear laser spectroscopy at ISOLDE, CERN 
$ 2012Pr11: charge radii of Ga isotopes measured relative to that {+71}Ga; Collinear laser spectroscopy technique at ISOLDE-CERN facility 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|d<r{+2}>({+71}Ga,{+75}Ga)=+0.285 fm{+2} {I4}(stat) {I58}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+75}Ga)=-45.3 MHz {I16}(stat) {I70}(syst) (2012Pr11) 
J$from {+75}Ga Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
MOMM1$ Deduced from the measured A(5{Is}{+2}{IS}{-1/2},{+75}Ga)=+971.7 {I12} MHz in 2017Fa09 and A(5{Is}{+2}{IS}{-1/2},{+71}Ga)=+1358.2 {I16} MHz (2010Ch16), relative to |m({+71}Ga)=+2.56227 {I2} (2005St24) and J({+71}Ga)=3/2. 
MOME2$ Deduced from the measured B(4{Ip}{+2}{IP}{-3/2},{+75}Ga)=-107 {I2} MHz in 2017Fa09 and B(4{Ip}{+2}{IP}{-3/2},{+71}Ga)=+39 {I2} MHz (2010Ch16), relative to Q({+71}Ga)=+0.107 {I1} (2008Py02). 
J$Directly measured using the hyperfine structure analysis in 2017Fa09. |p from |m and the proposed mixed |pp{-3/2} and |pf{-5/2} configuration (by compilers). 
$Isotope shift |d|n=-44 {I4} MHz, measured relative to {+71}Ga. 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_lifetime_unit: S
level_comment:
$Mean-square charge radius <r{+2}>({+71}Ga,{+76}Ga)=+0.276 {I5} {I64} (2012Pr11), first uncertainty is statistical, second is systematic 
J$from laser hyperfine spectroscopy (2011Ma45), J=1 is ruled out by the number of atomic transitions and selection rules. J=2,3,4 are analyzed and reduced |h{+2} considered for the fitting of the hyperfine spectrum; J=2 is the most likely assignment. Spins higher than J=3 give poor match to the observed spectra. Negative parity is suggested by the comparison of measured and theoretical magnetic dipole moments and electric quadrupole moments. J|p=2- is also supported by 2016Do05 in comparison of their TAS data with their theoretical shell-model calculations, although a definite conclusion about J|p is not made due to the presence of several states in a narrow range in the theoretical level energy spectrum 
T$weighted average (NRM) of 30.6 s {I3} (2016Do05, from decay curve for implanted activity in the counting system and TAS detector); 32.6 s {I6} (1985Ta01, from decay curve of 546|g+563|g); 29.8 s {I4} (1974Gr29) (from integral |b spectrum; previous measurements at the same laboratory: 23.9 s {I19} (1981Ru07), 30 s (1972MaWL) and 29.0 s {I3} (1970OsZZ)); 32 s {I3} (1961Ta08, from integral |b{+-} spectrum above 3.2 MeV). Weighted average is 30.6 s {I5} but with reduced |h{+2}=5.1 as compared to |h{+2}=2.6 at 95% confidence level. Others: 27.1 s {I2} (1971Ca39, from |g-ray spectrum in the range 300-800 keV); 42 s (1966Se04, method not known) seem discrepant. 
MOMM1,MOME2$Laser Resonance Spectroscopy (LRS) (2011Ma45) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J$log {Ift}=4.7 from 0+ 
T$34 ns {I1}(stat) {I8}(syst) from 2022Ch09, weighted average of 33.9 ns {I11} from (|g rays in coin with the 199|g)(199|g)(t) and 30 ns {I4} from |b|g(t) in {+76}Zn |b{+-} decay. 
$Structure of this isomeric state is proposed by 2022Ch09 as a highly-mixed state of negative-parity proton configurations coupled to 1/2- neutron configurations 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
T$34 ns {I1}(stat) {I8}(syst) from 2022Ch09, weighted average of 33.9 ns {I11} from (|g rays in coin with the 199|g)(199|g)(t) and 30 ns {I4} from |b|g(t). Evaluators combined statistical and systematic uncertainties in quadrature 
$Structure of this isomeric state is proposed as a highly-mixed state of negative-parity proton configurations coupled to 1/2- neutron configurations (2022Ch09) 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: S
level_comment:
$Measured |d<r{+2}>({+71}Ga,{+77}Ga)=+0.308 fm{+2} {I4}(stat) {I74}(syst) (2012Pr11) 
$Measured isotope shift |d|n({+71}Ga,{+77}Ga)=-109.4 MHz {I15}(stat) {I110}(syst) (2012Pr11) 
J$spin from hyperfine structure and collinear laser spectroscopy; parity from dominant configuration=|pf{-5/2}{+3} (2010Ch16) deduced from magnetic dipole moment. Proposed configuration=|pf{-5/2}{+2}~#|pp{-3/2}) (2011Ma45) 
MOMM1,MOME2$ collinear laser spectroscopy (2010Ch16). See also 2017Ne04 review article. Measured |m=+2.020 {I3} by 2010Ch16 is re-evaluated to |m=+2.018 {I3} 
T$from 1977Al17. Other: 17.1 s {I15} (1968Wi11) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: S
level_comment:
J$log| {If{+1u}t}<8.5 to (2+) and (4+); 2205|g from 1+ 
T$from 1974Gr29 in {+78}Ga |b{+-} decay (milking experiment). Others: 5.9 s {I25} (1980Le22: from the decay curve for the 619|g in {+78}Ga |b{+-} decay), 4.8 s {I13} (1972De43), 4.9 s (1970OsZZ), |?4 s (1968Wi11). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT;ISO=M
level_comment:
T$ from time correlations between implanted {+78}Ga nuclei and |g-ray events (c.m. Folden III et al., Phys. Rev. C 79, 064318 (2009)). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$ from time correlations between implanted {+78}Ga nuclei and |g-ray events (c.m. Folden III et al., Phys. Rev. C 79, 064318 (2009)) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_lifetime_unit: NS
level_comment:
T$from |g-ray decay curve (2010Da06,1999DaZQ). 
$ Isomeric transitions of 46.1, 157.5 and 217.8 are reported 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_comment:
J$ from present measurements, J=1 is ruled out by the number of atomic transitions and selection rules. J=2,3,4 possibilities are analyzed and reduced |h{+2} considered for the fitting of the hyperfine spectrum. For {+78}Ga, J=2 is the most likely assignment. Spins higher than J=3 give poorer match to the observed spectra. Negative parity is suggested by the comparison of measured and theoretical magnetic dipole moments and electric quadrupole moments 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_comment:
$|d<r{+2}>({+71}Ga,{+78}Ga)=+0.270 fm{+2} {I5}(stat) {I78}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+78}Ga)=-160 MHz {I2}(stat) {I13}(syst) (2012Pr11) 
J$from 2011Ma45: Phys. Rev. C84, 024303. J|p=(3+) in {+78}Ga Adopted Levels in ENSDF database needs revision 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: S
level_comment:
$|d<r{+2}>({+71}Ga,{+79}Ga)=+0.290 fm{+2} {I5}(stat) {I87}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+79}Ga)=-186.2 MHz {I19}(stat) {I140}(syst) (2012Pr11) 
$Theoretical T{-1/2}=1.76 s, %|b{+-}n=0.06 (2003Mo09) 
$Theoretical T{-1/2}=119 s, %|b{+-}n=1.0 (2016Ma12) 
$%|b{+-}n: weighted average given by 1993Ru01 of the following values: 0.113 {I11} (1993Ru01), 0.055 {I12} (1986Wa17), 0.098 {I16} (1980Lu04). The uncertainty given by 1986Wa17 is 0.004 and that by 1980Lu04 is 0.010. 1993Ru01 seem to have increased these uncertainties in obtaining weighted average. Other: 0.10 {I1} (1984Ma39,compilation) 
J$spin measured in 2010Ch16 from hyperfine structure using collinear laser spectroscopy. Parity from probable p{-3/2} configuration. The g.s. and 5.4 are too close to assign p{-3/2} and f{-5/2} uniquely, but some evidence of |b{+-} feeding from g.s. to (1/2-) in {+79}Ge (log| {Ift}=5.8) favors negative parity for g.s. 
T$from weighted average of 2.847 s {I3} (1991Kr15, neutron counting), 2.88 s {I2} (1993Ru01, neutron and |b), and 2.85 s {I1} (1986Wa17). Others: 2.63 s {I20} (1982FoZZ,1981Ho24), 2.9 s {I5} (given by 1977Al17 from an unpublished work from their laboratory), 2.63 s {I9} (1976Ru01), 3.00 s {I9} (1974Gr29, authors also give 2.8 s 2 from decay curve for a 490|g from a work to be published by the same group), 2.86 s {I4} (1970OsZZ) 
MOMM1,MOME2$collinear laser spectroscopy (2010Ch16) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
MOMM1$ Deduced from the measured A(5{Is}{+2}{IS}{-1/2},{+79}Ga)=+550.2 {I112} MHz in 2017Fa09 and A(5{Is}{+2}{IS}{-1/2},{+71}Ga)=+1358.2 {I16} MHz (2010Ch16), relative to |m({+71}Ga)=+2.56227 {I2} (2005St24) and J({+71}Ga)=3/2. 
MOME2$ Deduced from the measured B(4{Ip}{+2}{IP}{-3/2},{+79}Ga)=+49 {I12} MHz in 2017Fa09 and B(4{Ip}{+2}{IP}{-3/2},{+71}Ga)=+39 {I2} MHz (2010Ch16), relative to Q({+71}Ga)=+0.107 {I1} (2008Py02). 
J$Directly measured using the hyperfine structure analysis in 2017Fa09. |p from |m and the proposed mixed |pp{-3/2} and |pf{-5/2} configuration (by compiler). 
$Isotope shift |d|n=-173 {I11} MHz, measured relative to {+71}Ga. 


level_energy_unit: KEV
level_spin_parity: 6(-)
level_lifetime_unit: S
level_comment:
$|d<r{+2}>(charge)({+71}Ga,{+80}Ga)=+0.242 fm{+2} {I91} (2012Pr11); 0.010 fm{+2} is statistical uncertainty, 0.091 fm{+2} is systematic 
$|d|n(IS)({+71}Ga,{+80}Ga)=-239 MHz {I16} (2012Pr11); 4 MHz is statistical uncertainty, 16 MHz is systematic 
E$shell-model predictions suggest 6- to be the g.s. 
J$spin from hyperfine structure (2010Ch50), parity from shell-model predictions and comparison with measured moments 
T$measured by 2013Ve03 from decay curves for many |g rays. Others: much greater than 200 ms (2010Ch50), 1.65 s {I1} (1993Ru01), 1.706 s {I10} (1991Kr15), 1.67 s {I10} (1982FoZZ), 1.7 s (1981Gi17), 1.66 s {I2} (1976Ru01) 1.7 s {I2} (1974Gr29). All measured values prior to 1994 are most likely for a combined mixture of the 1.9-s, 6(-) and 1.3-s, 3(-) activities. See detailed discussion in 2013Ve03 
%B-N$ weighted average of 0.97 {I6} (1993Ru01), 0.69 {I8} (1986Wa17), 0.84 {I6} (1980Lu04). Here all of %|b{+-}n is assigned to g.s., but most likely it is for a mixture of the 1.9-s and 1.3-s activities. Other measurements: 1986ReZU and 1986ReZS (same group as 1986Wa17); 1982Ru01, 1981Ho07, 1977Ru09 (also 1977Ru10) (same group as 1980Lu04) Compilation and other analyses of %|b{+-}n values: 1989BrZI, 1984Ma39, 1984Ha58, 1984KoYR, 1979RuZQ. 
MOMM1,MOME2$from collinear laser spectroscopic technique (2010Ch50). For any spin value, magnitudes of moments are: |m=0.123 to 0.182 {I4} or <0.055 {I4}; Q<0.050 {I12} or Q=0.182 {I11} to 0.510 {I28} (2010Ch50) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$%|b{+-}n=0.86 {i7} assigned to the ground state decay is most likely for a mixture of the two activities of 1.9 s and 1.3 s 
$|d<r{+2}>(charge)({+71}Ga,{+80}Ga)=+0.260 fm{+2} {I92} (2012Pr11); 0.007 fm{+2} is statistical uncertainty, 0.092 fm{+2} is systematic 
$|d|n(IS)({+71}Ga,{+80}Ga)=-232.0 MHz {I160} (2012Pr11); 2.5 MHz is statistical uncertainty, 16.0 MHz is systematic 
E$from 2014Li32 
J$spin from hyperfine structure (2010Ch50), parity from shell-model considerations and comparison with measured moments. Nordheim's rule also suggests 3-. J|p=3+ with configuration= |pf{-5/2}~#|n p{-1/2} is suggested by 1987Wi13. 
T$measured by 2013Ve03 from decay curves for many |g rays. See also comment for half-life of g.s. 
MOMM1,MOME2$from collinear laser spectroscopic technique (2010Ch50). 


level_energy_unit: KEV
level_spin_parity: 6(-)
level_comment:
MOMM1$ Deduced from the measured A(4{Ip}{+2}{IP}{-3/2},{+80}Ga)=+1.4 {I7} MHz in 2017Fa09, A(5{Is}{+2}{IS}{-1/2},{+71}Ga)=+1358.2 {I16} MHz (2010Ch16), A(5{Is}{+2}{IS}{-1/2})/ A(4{Ip}{+2}{IP}{-3/2})=+5.592 {I9} (2010Ch16), relative to |m({+71}Ga)=+2.56227 {I2} (2005St24) and J({+71}Ga)=3/2. 
MOME2$ Deduced from the measured B(4{Ip}{+2}{IP}{-3/2},{+80}Ga)=+186 {I7} MHz in 2017Fa09 and B(4{Ip}{+2}{IP}{-3/2},{+71}Ga)=+39 {I2} MHz (2010Ch16), relative to Q({+71}Ga)=+0.107 {I1} (2008Py02). 
$Isotope shift |d|n=-230 {I4} MHz, measured relative to {+71}Ga. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3(-)
level_comment:
MOMM1$ Deduced from the measured A(4{Ip}{+2}{IP}{-3/2},{+80}Ga)=-68.0 {I2} MHz in 2017Fa09, A(5{Is}{+2}{IS}{-1/2},{+71}Ga)=+1358.2 {I16} MHz (2010Ch16), A(5{Is}{+2}{IS}{-1/2})/ A(4{Ip}{+2}{IP}{-3/2})=+5.592 {I9} (2010Ch16), relative to |m({+71}Ga)=+2.56227 {I2} (2005St24) and J({+71}Ga)=3/2. 
MOME2$ Deduced from the measured B(4{Ip}{+2}{IP}{-3/2},{+80}Ga)=+132 {I3} MHz in 2017Fa09 and B(4{Ip}{+2}{IP}{-3/2},{+71}Ga)=+39 {I2} MHz (2010Ch16), relative to Q({+71}Ga)=+0.107 {I1} (2008Py02). 
$Isotope shift |d|n=-224 {I4} MHz, measured relative to {+71}Ga. 


level_energy_unit: KEV
level_spin_parity: 6(-)
level_lifetime_unit: S
level_comment:
$|d<r{+2}>({+71}Ga,{+80}Ga)=+0.242 fm{+2} {I10}(stat) {I91}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+80}Ga)=-239 MHz {I4}(stat) {I16}(syst) (2012Pr11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$|d<r{+2}>({+71}Ga,{+80}Ga)=+0.260 fm{+2} {I7}(stat) {I92}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+80}Ga)=-232.0 MHz {I25}(stat) {I160}(syst) (2012Pr11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
T$2020Pa26 determine T{-1/2}=1.70 s {I3} which they determine is mainly due to the 3- half life, but does contain a contribution from the ground state. 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_lifetime_unit: S
level_comment:
$|d<r{+2}>({+71}Ga,{+81}Ga)=+0.242 fm{+2} {I4}(stat) {I99}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+81}Ga)=-271.8 MHz {I15}(stat) {I170}(syst) (2012Pr11) 
J$ 5/2 from collinear laser spectroscopy measurements reported in 2010Ch16. Parity from shell-model configuration. Anomalous g.s. spins of {+81}Ga and change in sign of Q{-2} suggest a changing shell structure from N=42 onwards and strong influence of |pf{-5/2} orbital in the g.s. wave function (2010Ch16). 
T weighted average of 1.221 s {I5} (delayed-n activity, 1991Kr15) and 1.211 s {I6} (1993Ru01), 1.23 s {I1} (1976Ru01), 1.23 s {I10} (1982FoZZ), 1.22 s {I1} (1986Wa17), 1.2 s {I2} (quoted value in 1976Ru01 from Ref. 14), 1.25 s {I3} (2020Pa26). Weighted average: 1.219 s {I34} Uncertainty from 1991Kr15 - the lowest from the input values. Others: 0.959 s {I+37-29} (2010Ho12) is a discrepant value, 2.2 s (1975Al11). All from decay curve fitting including |b-, n, and coincidence growth measurements. 
%|b{+-}n is from simultaneous measurement of n-emission rate and |b{+-} decay rate. Average of: 10.6% {I8} (1986Wa17 - 4% statistical and 7% systematic uncertainty); 12.2% {I10} (revised/recommended value (1984Ma39) based on 12.0% {I9} (1980Lu04) and overall consistency of data from different laboratories); 12.9% {I8} (1993Ru01), and 11.2% {I26} (2019To09). Other: 12.7% {I12} (deduced by evaluator using I|g(216)/|I{-p}=2.9 {I2} (1981Ho07) and %I|g(216 in {+81}Ga |b- decay)=36.7 {I24}). 
MOMM1$From 2010Ch16, 2019StZV - Collinear Laser Spectroscopy. Other: +1.747 {I8} (2017Fa09). 
MOME2$From 2010Ch16, 2021StZZ - Collinear Laser Spectroscopy. Other: -0.033 {I13} (2017Fa09). 


level_energy_unit: KEV
level_comment:
E,J$level not reported in ({+238}U,f|g). Spin parity 9/2- from shell model calculations in ({+82}Se,x|g). In ({+238}U,f|g) 9/2- has been reported at 1340.7 keV. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$if beta feeding to this level from (1/2+,3/2+) in {+81}Zn |b- decay is true, then it might be a different level or spin parity should be considered with caution. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: PS
level_comment:
$Configuration: |p(p{-3/2}){+2} (2007Ve08) 
T$measured by the absolute comparison using parallel transitions, also see the footnote. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$from S(n)=6476 {I4} ({+81}Ga) and x<4952 {I7} [from Q(|b{+-}) ({+81}Zn=11428 {I6})-S(n)({+81}Ga) (2021Wa16)]. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
$%|b{+-}n: From 2016Te09. Others: 1986Wa17, 1980Lu04 
J$From Laser spectroscopy work in 2012Ch51. This assignment is tentative since J|p=1-,3- were not ruled out. 
T$Weighted average of 0.602 s {I6} (1986Wa17), 0.599 s {I2} (1991Kr15), 0.610 s {I+83-72} (2010Ho12), 0.592 s {I9} (2015Et01), 0.604 s {I11} (2016Te09). Other: 1976Ru01 
T$2016Te09 value from growth curve for (delayed) neutron activity assigned purely to {+82}Ga |b{+-}n decay. Uncertainty is from the fit to the neutron activity curve. (In 2016Te09 radioactive ion beam of {+82}Ga at 30 keV was produced in photofission of {+238}U using UC{-x} pellets containing about 60 g of {+238}U) 
T$2015Et01 value from fit to {+82}Ge (first 2+ to g.s.) 1348-keV gamma activity in a 2-s beam on/off cycles. {+82}Ga nuclides obtained from {+238}U(e,F), E=50 MeV 
T$2010Ho12 value from measurement of time sequence of decay type events correlated with the implanted nuclei (of {+82}Ga) in Si detectors (2010Ho12) using method of maximum likelihood analysis with input parameters including |b-detection efficiency, background, half-lives of daughter and granddaughter nuclei and experimental or theoretical values of %|b{+-}n of all nuclei involved. 2010Ho10 used {+9}Be({+86}Kr,X) E=140 MeV/nucleon 
MOMM1$Using U(n,X) reaction; deduced from the measured hyperfine parameters in 2017Fa09 and 2010Ch16, relative to |m({+71}Ga)=+2.56227 {I2} (2005St24) and J({+71}Ga)=3/2. 
MOME2$Using U(n,x) reaction; deduced from the measured hyperine parameters 2017Fa09 and 2010Ch16, relative to Q({+71}Ga)=+0.107 {I1} (2008Py02). 
$Other: |m=+0.459 {I4}, Q=+0.197 {I13} (2012Ch51) using U(p,x). 2012Ch51 also give corresponding values for J=1 and 3. For J=1, |m=+0.364 {I3}, +0.019 {I4} and Q=+0.117 {I9}, -0.549 {I29} for two sets of hyperfine parameters A and B. For J=3, |m=+0.510 {I4}, Q=+0.271 {i17} 
$|d<r{+2}>({+71}Ga,{+82}Ga)=+0.447 fm{+2} {I23}(stat) {I120}(syst) (2012Pr11) 
$Isotope shift |d|n({+71}Ga,{+82}Ga)=-222 MHz {I9}(stat) {I19}(syst) (2012Pr11) measured relative to {+71}Ga. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$J|p=(2-,3-) in 2016Al10. J|p=3- is not likely, as it would imply a possible M2 multipolarity for the 2943.8-keV |g ray from the 2973.6-keV level competing with an E1 transition 
T$Estimated in 2016Al10. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
T$From 2016Al10. Other: 0.98 |ms {I+10-9} (2012Ka36) from |g(t) in Be({+238}U,F|g); <500 ns (2009Fo05) from time correlations between implanted {+82}Ga nuclei and |g-ray events in {+9}Be({+238}U,X). 
J$possible E2 |g to (2-) g.s.; no |b feeding from {+82}Zn 0+ parent 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
J$2016Al10 assigned firm 2- by citing the laser spectroscopy work of 2012Ch51; however, this assignment is tentative as J=1 and 3 were not ruled out, and the parity is based only on a comparison of measured magnetic moment with shell-model predictions. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$From Adopted Levels. 2016Al10 assign firm 2- by citing the laser spectroscopy work of 2012Ch51 but evaluators note that the assignment of J=2 was tentative in this work, while J=1 and 3 were not totally ruled out, and that the parity is based only from a comparison of measured magnetic moment with shell-model predictions. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$possible E2 |g to (2-) g.s.; no |b feeding from {+82}Zn 0+ parent 
T$measured by 2016Al10. No details are provided but the measurement is probably from delayed coincidence data. This value is compared to 98 ns {I+10-9} from 2012Ka36 (Phys. Rev. C86, 054319) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from comparison of absolute intensities of most intense |g rays from nuclei in the |b{+-}n branch to the number of ions deposited; weighted average of %|b{+-}n=64 {I3} and 61 {I4} (2009Wi03). Others: 14.9 {I18} (1993Ru01), 54 {I7} (1986Wa17), 43 {I7} (1980Lu04). Uncertainty of 1986Wa17 does not include that of the neutron-efficiency detection. 2002Pf04 compilation adopted %|b{+-}n=39 {I10}. 
J$3/2- from systematics (2012Au07), 1/2- in calculations of 1997Mo25. 
T$weighted average of values from |g(t): 0.317 s {I17} (1348|g in {+82}Ge), 0.319 s {I24} (1238|g in {+83}Ge) (2006Pe20), and from |b{+-}-delayed neutron activity: 0.307 s {I7} (1993Ru01), 0.308 s {I1} (1991Kr15), 0.31 s {I1} (1986Wa17), 0.31 s {I1} (1980Lu04). Other: 0.31 s {I1} (1976Ru01) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from the sum of the neutron intensity distribution normalized to the total number of decays observed (2016Ma50). 
T$from the Adopted Levels of {+83}Ga in the ENSDF database, 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
T$measured by 2016Al10 from grow-in and decay curve for |b-gated 1348|g from {+83}Ga |b{+-}n decay. Another value of 307 ms {I19} was obtained from the grow-in and decay of 1238|g from {+83}Ga |b{+-} decay. These values can be compared with 308.1 ms {I10} in {+83}Ga Adopted Levels in the ENSDF database (Dec 2014 update) 
J$5/2- given in Fig. 10 of 2016Al10 is from shell-model calculations (see Fig. 15 in 2016Al10) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n from neutron and |b activity measurement (2017Ve01). This value can be compared with 62.8 {I25} in {+83}Ga Adopted Levels in the ENSDF database (Dec 2014 update); and 56 {I7} in 2016Ma50 (Phys. Rev. Lett. 117, 092502). 
J$(5/2-) from systematics (2017Au03: NUBASE-2016) 
T$measured by 2017Ve01 from grow-in curve for (delayed) neutron activity assigned purely to {+83}Ga |b{+-}n decay. Uncertainty is from the fit to the neutron activity curve. This value can be compared with 308.1 ms {I10} in {+83}Ga Adopted Levels in the ENSDF database (Dec 2014 update), and 309 ms {I6} (2016Al10: Phys. Rev. C 93, 044325; from decay curve for 1348-keV |g ray in {+82}Ge emitted by the |b{+-}n decay of {+83}Ga) 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: MS
level_comment:
%B-N$weighted average of 44 {I4} (2019Yo03, from sum of neutron intensity distribution normalized to the total number of decays observed, systematic uncertainty included); 53 {I20} (2017Ve01, from neutron and |b activity measurement, also 51 {I28} in 2014TeZY); 40 {I7} (2016Ma50, from sum of the neutron intensity distribution normalized to the total number of decays observed); 74 {I14} (2010Wi03, from |b|g-coin data, 80 {I15} in 2009Gr06, 47 {I10} in 2008WiZZ); 70 {I15} (1991Kr15, from neutron measurement) 
%B-2N$from 2019Yo03, sum of the two-neutron intensity distribution normalized to the total number of decays observed. 
T$unweighted average of 97.6 ms {I12} (2019Yo03, from binned maximum likelihood fitting of |bn(t) as 1n spectra including contributions from parent, daughter, |b1n, and |b2n daughter and a linear background); and 92.7 ms {I7} (2014XuZZ, |b|g-coin, also 91.2 ms {I83} from analysis of |b-decay curve). Others: 84 ms {I7} (2013Ko32, from evaluator's weighted average of measured half-lives for eight |g rays) 76 ms {I48} (2009Le26, from decay curve for 247.8|g, 75 ms {I33} in 2009Ve11); 70 ms {I35} (2006Pe20, from decay curve for |g rays); 85 ms {I10} (1991Kr15, neutron-decay curve) 
J$0- assigned by 2009Le26 based on configuration of |p1f{-5/2}{+3}~#|n2d{-5/2}{+3} and Paar model. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from (implants)(1n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 37.0 {I4}(stat) {I11}(syst); uncertainties added in quadrature. Authors' %|b{+-}n value is weighted average of two measurements: 38.2 {I21} in one run and 37.0 {I4} in the second run. 
%B-2N$from (implants)(2n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 1.88 {I6}(stat) {I11}(syst); uncertainties added in quadrature. Authors' %|b{+-}2n value is weighted average of two measurements: 1.91 {I17} in one run and 1.87 {I7} in the second run. 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b{+-}1n, and |b{+-}2n daughter as well as a linear background (2023Yo04). Quoted T{-1/2} are from |b{+-}(neutron) correlated decay curves, as 1n spectra have a smaller component from decays of descendant nuclei than the 0n spectra and greater statistics than the 2n spectra (2023Yo04). Authors' T{-1/2} value is weighted average of two measurements: 95.0 ms {I25} in one run and 97.6 ms {I12} in the second run. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$Delayed-neutron is expected to be the dominant decay mode as suggested by the observation of a strong 624|g in {+84}Ge, and from theoretical values of %|b{+-}n=94, %|b{+-}2n=6 (1997Mo25); total delayed-neutron decay=100% (2005Bo19) 
E$it is assumed that the observed {+85}Ga fragments are associated with the g.s. 
J$proposed in 2013Ko31 based on systematics of neighboring Ga nuclei, and agreement of experimental and theoretical half-lives from CQRPA calculations; probable f{-5/2} orbital. Others: 3/2- (syst,2012Au07), 1/2- (predicted,1997Mo25) 
T$measured value from decay curves of five |g rays (2013Mi19). Others: 93 ms {I7} (2012Ma37, from gates on 107.8- and 624.3-keV |g rays from decay of {+85}Ga), <100 ms, estimated in 2010Wi03 from observation of events due to 624-keV |g ray (in {+84}Ge from delayed neutron decay of {+85}Ga) in the first 190 ms after implantation. 


level_energy_unit: KEV
level_spin_parity: (-)
level_lifetime_unit: MS
level_comment:
%B-N$from detected neutrons versus cycle time as shown in authors' Fig. 4a, together with fitting of the resultant curve with the network of daughter isotopes originating from the decay of {+85}Ga. 
%B-2N$estimated by 2018Mi03 from non-observation of |g rays belonging to {+83}Ge and no evidence for simultaneous emission of two neutrons. 
J$Odd proton likely to be in {If} or {Ip} orbital of {Ifpg} shells (2018Mi03) 
T$From {+85}Ga Adopted Levels in the ENSDF database (Dec 2013 update). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from the sum of the neutron intensity distribution normalized to the total number of decays observed (2019Yo03). Uncertainty is systematic, which is the dominant contribution (2019Yo03). 
%B-2N$from the sum of the two neutron intensity distribution normalized to the total number of decays observed (2019Yo03). 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b1n, and |b2n daughter as well as a linear background (2019Yo03). Quoted T{-1/2} are from |bn(t) as 1n spectra have a smaller component from decays of descendant nuclei than 0n spectra and greater statistics than 2n spectra (2019Yo03). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from (implants)(1n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 75.8 {I18}(stat) {I24}(syst); uncertainties added in quadrature. Authors' %|b{+-}n value is weighted average of two measurements: 73 {I4} in one run and 76.4 {I18} in the second run. 
%B-2N$from (implants)(2n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 1.58 {I13}(stat) {I9}(syst); uncertainties added in quadrature. Authors' %|b{+-}2n value is weighted average of two measurements: 1.8 {I3} in one run and 1.53 {I14} in the second run. 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b{+-}1n, and |b{+-}2n daughter as well as a linear background (2023Yo04). Quoted T{-1/2} are from |b{+-}(neutron) correlated decay curves, as 1n spectra have a smaller component from decays of descendant nuclei than the 0n spectra and greater statistics than the 2n spectra (2023Yo04). Authors' T{-1/2} value is weighted average of two measurements: 101 ms {I4} in one run and 95.3 ms {I10} in the second run. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$measured value from decay curves of five |g rays (2013Mi19). Theoretical values vary from 26 to 128 ms (2013Mi19) 
%B-N,%B-2N$from measurement by 2013Mi19, 2014Gr03. Theoretical values vary from 20 to 61 for %|b{+-}n, and 12 to 44 for %|b{+-}2n (2013Mi19). Other theoretical values: %|b{+-}n=60.6 (1997Mo25), 67.2, 100 (2002Pf04); %|b{+-}2n=13.3 (1997Mo25). Systematic (KHF) value of %|b{+-}n=42.4 (2002Pf04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from the sum of the one neutron intensity distribution normalized to the total number of decays observed (2019Yo03). Reported value is 74 {I2} (stat) {I8} (syst) (2019Yo03); uncertainty added in quadrature 
%B-2N$from the sum of the two neutron intensity distribution normalized to the total number of decays observed (2019Yo03). Reported value is 16.2 {I9} (stat) {I6} (syst). 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b1n, and |b2n daughter as well as a linear background (2019Yo03). Quoted T{-1/2} are from |bn(t) as 1n spectra have a smaller component from decays of descendant nuclei than 0n spectra and greater statistics than 2n spectra (2019Yo03). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from (implants)(1n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 59.5 {I21}(stat) {I18}(syst); uncertainties added in quadrature. Authors' %|b{+-}n value is weighted average of two measurements: 57 {I6} in one run and 59.9 {I23} in the second run. 
%B-2N$from (implants)(2n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 14.7 {I9}(stat) {I11}(syst); uncertainties added in quadrature. Authors' %|b{+-}2n value is weighted average of two measurements: 17.8 {I22} in one run and 14.1 {I10} in the second run. 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b{+-}1n, and |b{+-}2n daughter as well as a linear background (2023Yo04). Quoted T{-1/2} are from |b{+-}(neutron) correlated decay curves, as 1n spectra have a smaller component from decays of descendant nuclei than the 0n spectra and greater statistics than the 2n spectra (2023Yo04). Authors' T{-1/2} value is weighted average of two measurements: 53 ms {I4} in one run and 51 ms {I2} in the second run. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
T$ lower limit from time-of-flight (2010Oh02), based on private communication from T. Kubo dated 14 July 2010. Actual half-life is predicted to be much longer, as suggested by the calculated values of 70 ms (2005Bo19), 24 ms and 118 ms (2002Pf04), 28.0 ms (1997Mo25). 
$Probability of misidentification of {+87}Ga isotope<0.001% (2010Oh02). 
J$ 3/2- predicted in calculations (1997Mo25) 
$Calculated %|b{+-}n=90.8, %|b{+-}2n=7.4 (1997Mo25). Calculated %|b{+-}n=100 (2002Pf04). More %|b{+-}n calculations are given in 2005Bo19 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Estimated |s=19 pb based on ratio of the measured production rate to the LISE++ simulated production rate and the predicted cross section. The estimated systematic uncertainty is|?50% 
T$ lower limit from time-of-flight, according to private communication from T. Kubo dated 14 July 2010. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from the sum of the one neutron intensity distribution normalized to the total number of decays observed (2019Yo03). Reported value is 81 {I9} (stat) {I8} (syst) (2019Yo03); uncertainty added in quadrature. 
%B-2N$from the sum of the two neutron intensity distribution normalized to the total number of decays observed (2019Yo03). Reported value is 10.2 {I28} (stat) {I5} (syst). 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b1n, and |b2n daughter as well as a linear background (2019Yo03). Quoted T{-1/2} are from |bn(t) as 1n spectra have a smaller component from decays of descendant nuclei than 0n spectra and greater statistics than 2n spectra (2019Yo03). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from (implants)(1n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 72 {I9}(stat) {I2}(syst); uncertainty added in quadrature by compiler. Authors' %|b{+-}n value is weighted average of two measurements: 73 {I31} in one run and 72 {I9} in the second run. 
%B-2N$from (implants)(2n)|b-correlated events and methodology described by 2018Ra27 (Nucl. Instrum. Methods Phys. Res. A911, 79); authors' reported value is 8.7 {I28}(stat) {I5}(syst); uncertainty added in quadrature by compiler. Authors' %|b{+-}2n value is weighted average of two measurements: 18 {I18} in one run and 8.5 {I28} in the second run. 
T$from binned maximum likelihood fitting including contributions from parent, daughter, |b{+-}1n, and |b{+-}2n daughter as well as a linear background (2023Yo04). Quoted T{-1/2} are from |b{+-}(neutron) correlated decay curves, as 1n spectra have a smaller component from decays of descendant nuclei than the 0n spectra and greater statistics than the 2n spectra (2023Yo04). Authors' T{-1/2} value is weighted average of two measurements: 31 ms {I9} in one run and 24 ms {I8} in the second run. 


level_energy_unit: KEV
level_comment:
%B-$decay mode not observed, however, inferred by compiler as only energetically allowed decay mode. 
$75 counts assigned to {+88}Ga by 2024Sh17, which are assumed by the compiler to correspond to the g.s. activity of {+88}Ga 
$Measured production |s=6.6 |* 10{+2} fb (2024Sh17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
$No events could be assigned to {+58}Ge. From comparison with the yields of neighboring nuclides, expected counts were 1.2 {I12} for optimized setting on {+65}Br and 20 {I12} for setting on {+62}Se. 
$Non-observation of {+58}Ge nuclide is consistent with its g.s. being proton-unbound or expected 2p emitter 
T$from the flight time through the BigRIPS separator 
$Production |s<0.076 fb (2016Bl05) based on observation of maximum of one count. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$2p decay mode is likely since S(2p)=2102 {I447} (2017Wa10). However, no evidence for 2p emission is detected by 2016Go26. An upper limit of 0.2% proposed by 2016Go16, assuming all events but one come from |b-delayed decays. 
E$Detected activity is assumed to correspond to the g.s. of {+59}Ge 
T$Measured from |b decay-time curve and fitting (2016Go26) 
J$7/2- proposed from systematic trend (2017Au03); 7/2- neutron orbital in theoretical calculations (1997Mo25). 
$Measured production cross section |s=48 fb {I10} (2016Bl05) is about 3 times larger than the measured value of |s=17 fb {I+13-9}(stat) {I5}(syst) by 2015Ci06. 2016Bl05 attribute this difference due to the difficulty in correctly calculating the transmissions with models. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
T$ limiting value from experimental observation of at least one event combined with expected number of transmitted nuclei based on abrasion-ablation model cross sections and the time of flight (362 ns for {+60}Ge). Actual half-life is expected to be much longer as suggested by systematics value of 30 ms (2003Au02) and calculated value of 82 ms (1997Mo25) for |b decay 
$Production cross sections=0.38 pb {I+27-31} (2005St29), |?5 pb (2007Bl09) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B+P$from 11 protons out of the 19 events which were stopped in the active volume of the detector, four protons out of the eight events in unknown direction, assumed isotropic distribution of proton emission, and proton detection efficiency factor of 50%, deduced decay branch is consistent with 100% delayed one-proton decay (2016Ci01) 
%B+2P$approximate upper limit from non-observation of two-proton events (2016Ci01) 
T$from decay time distributions between the arrival of {+60}Ge ion and emission of a proton from |b-delayed proton emission process, and analysis of this distribution by maximum likelihood method (2016Ci01) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
%ECP$%listed as |ep>62 {i4} (2007Bl09). Other: |?80 (1987Ho01) 
J$T{-z}=-3/2 mirror state of {+61}Cu g.s. 
T$weighted average of 45 ms {I6} (delayed proton timing,2007Bl09) and 40 ms {I15} (1987Ho01,pulsed beam). Other: 36 ms {I21} (2002Lo13, same group as 2007Bl09) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$Measured by 2014Gr10 from |b-decay activity curve correlated with the decay of {+62}Ga daughter decay 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Decay modes from {+62}Ge Adopted Levels in ENSDF database 
$T{-z}=-1 
T$measured by 2014Ro14 from |b{++} decay correlation time spectrum 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$T{-z}=-1 
T$measured by 2017Ku12 from ({+62}Ge implants)|b correlated decay curve. Others: 54 ms {I5} in 2014Ro14 (Nucl. Data Sheets 120, 41, at GANIL); 129 ms {I35} in 2002Lo13 (Phys. Rev. C 66, 025803, at GANIL); 82.9 ms {I14} in 2014Gr10 (Phys. Rev. Lett. 113, 092501, at GSI). Value from 2014Gr10 agrees with that from 2017Ku12, and is also more precise than all the other values. Value of 129 ms {I35} from 2002Lo13 is listed in {+62}Ge Adopted Levels in the ENSDF database (April 2012 update). 
$Total number of {+62}Ge implanted ions=6080 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
J$3/2- from systematics in 2021Ko07; mirror of 3/2- g.s. of {+63}Ga (2019Ru07). Other: 1/2- from theory in 2019Mo01 
T$weighted average of 153.3 ms {I6} (2019Ru07), 153.6 ms {I11} (2020Gi02), 150 ms {I9} (2002Lo13,2002Bl17), 149 ms {I4} (2014Ro14), and 156 ms {I11} (2017Ku12). Other: 95 ms {I+23-20} (1993Wi03,1993Wi18) is discrepant. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$from recoil-distance method (2007St16) in {+12}C({+65}Ge,{+64}Ge); listed in {+12}C({+54}Fe,2n|g),{+54}Fe({+12}C,2n|g) dataset 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
J$|g to 0+; |g from (4+) 
T$from recoil-distance method (2007St16) in {+12}C({+65}Ge,{+64}Ge); listed in {+12}C({+54}Fe,2n|g),{+54}Fe({+12}C,2n|g) dataset 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: PS
level_comment:
E$only one level at this energy is proposed by 2003Fa01, the authors do not confirm two levels near this energy as in 1991En01 
J$|DJ=1, (E1+M2) |g to 4+ 


level_energy_unit: KEV
level_spin_parity: (12)
level_comment:
E$1820|g in {+12}C({+54}Fe,2n|g),{+54}Fe({+12}C,2n|g) (1991En01) is placed from a 6065 level, instead 
J$|DJ=2 |g to (10). Positive parity proposed by 2003Fa01 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E$this level is not confirmed in 2003Fa01, 1047|g is placed from the 3717, (5-) level. Thus this level is omitted in adopted levels 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
T$<0.21 ns (estimate by 1991En01 from nonobservation of expected intensity imbalance at 5- level if |t(mean)|?300 ps) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_comment:
J from allowed log| {Ift} to (1/2)- and 1/2-,3/2- levels and log| {Ift}= 6.3 to 5/2- which rules out J|p=1/2-. 
T 30.9 s {I5}. Weighted mean of 31.2 s {I7} (1973Jo12), 30.0 s {I12} (1974Ro16), 30.8 s {I10} (1976Ha29,1981Ha44), and 30.8 s {I7} (2000Gi11). 
Expected configuration=(|n 2p{-3/2}) (1995He27) 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_comment:
Possible configuration=(|n 1g{-9/2})~#4+ (1995He27). J|p=(15/2-) in 1997So06 
E$E(lev)=3334 if the placement of 1254|g and 1356|g is reversed as 1997So06 
J$15/2- in 1997So06 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 25/2(-)
level_comment:
E$x=5671 (1997So06) based upon 462|g depopulating this level and feeding 5209 level; however 462|g is placed from 5153 level by 1995He27 not reported by 1997So06 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T weighted average of 2.23 h {I10} (1969Bo21), and 2.27 h {I5} (1970De39). Others: |?2.5 h (1950Ho26,1965He08) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J J=4 from |g(|q) (1982So04,1990HeYS), DCO (1982So04); |p=+ from E2 to 2+. 
T from 1980Cl01. T{-1/2}<2 ps from 1979Wa23. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J J=6 from |g(|q) (1979Wa23,1990HeYS); |p=+ from E2 to 4+. DCO measurements support J=6 (1982So04). 
T from 1980Cl01. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J J=5 from |g(|q), |p=- from E1+M2 to 4+ (1980Cl01). |g(|q) (1982So04,1990HeYS) and DCO measurements give J=5 (1982So04). 
T from 1980Cl01. T{-1/2}<2 ps from 1980WaZY. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$J=7 from |g(|q) (1980Cl01,1990HeYS); |p=- from E2 to 5-. Configuration=((|n f{-5/2})(|n g{-9/2}))7- (1990Bo27) 
T$weighted average of 190 ps {I10} (1980Cl01) and 204 ps {I28} (1979Wa23). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from 1990Bo27 in {+64}Zn({+12}C,{+10}Be) 
J$configuration=((|p g{-9/2})(|p d{-5/2}))6+ (1990Bo27) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J J=6 from |g(|q) (1979Wa23,1990HeYS); |p=+ from E2 to 4+. |g(|q) and DCO measurements support J=6 (1982So04). 
T from 1980Cl01. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$J=7 from |g(|q) (1980Cl01,1990HeYS); |p=- from E2 to 5-. Configuration=((|n f{-5/2})(|n g9/))7- (1990Bo27) 
T$weighted average of 190 ps {I10} (1980Cl01) and 204 ps {I28} (1979Wa23). 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
T$from 1980Cl01. Other: 1.2 ps {I+5-3} (1988ZhZX) 
J J=9 from |g(|q) (1990HeYS); |p=(-) favored by |g(|q), T{-1/2}, and systematics (1980Cl01) 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J J=8 from |g(|q) (1990HeYS); |p=(+) from systematics. Configuration=(|n g{-9/2}){++2}{-8+} (1990Bo27) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$956.94 {I8} in Adopted Levels for {+66}Ge in ENSDF database 
$B(E2) deduced by 2013Co23 from Coulomb excitation yields; listed here in e{+2}b{+2} units 
T$deduced by compilers from B(E2)|^=0.1401 {I69} and E|g=956.9 {I1} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_uncertain: S
level_comment:
$B(E2) from 0,0+ deduced by 2013Co23 from Coulomb excitation yields. Level not observed in 2013Co23, thus only an upper limit of B(E2) is given. 
E$from {+66}Ge Adopted Levels in ENSDF database 
T$deduced by compilers from B(E2)|^<0.0050 and listed branching ratios 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
J=1/2 from |g(|q) and |g|g(|q) in {+64}Zn(|a,n|g), |p=- from log| {Ift}=5.61 {I4} to 1/2- 
T weighted average of 18.7 min {I5} (1959Ri35) and 19.0 min {I3} (1969Ba07) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
MOMM1 From {+64}Zn(|a,n|g) 
J=9/2 from |g(|q) and polarization studies in {+57}Fe({+12}C,2n|g); |p=+ from M2 to 5/2-. 
T from 2000Ch07. Others: 110.9 ns {i14} (1979Al04), 70 ns {i7} (1973BeVT), 102 ns {i10} (1978Na10). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: US
level_comment:
T average of 12.8 |ms {I2} (1978Mu05) and 14.6 |ms {I2} (1979Al04) both measured by pulsed beam 
J 5/2 from |g(|q) (1983Mu15) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
G$deduced from the Larmor frequency ratio of |o{-L}({+67}Ge)/|o{-L}({+69}Ge)=0.869 {I9} obtained in TDPAD measurement and the {Ig}({+69}Ge)=-0.2224 {I7} from 1970Ch05 (2020Gr05). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
T$weighted average of 270.82 d {I27} (1981Wa26) and 270.99 d {I19} (1994Sc44). Others: 228 d {I6} (Rudstam thesis, Uppsala University, Sweden) and 275 d {I20} (1956Cr29). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=2 
MOMM1$from transient field method (2011StZZ,2005Le19). 
T$weighted average of 2.15 ps {I14} from DSAM in {+12}C({+64}Zn,{+8}Be|g) and 1.98 ps {I17} from DSAM and RDM in {+58}Ni({+12}C,2p|g),{+64}Zn({+7}Li,p2n|g). Others: 2.1 ps {I7} (1981De03), 3.5 ps {I+21-14} (1977Mo20), and 1.4 ps {I7} (1977Gu08) all from DSAM/RDM in {+58}Ni({+12}C,2p|g),{+64}Zn({+7}Li,p2n|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+12}C({+64}Zn,{+8}Be|g). Others: >3.5 ps (1982Pa03), 3.5 ps {I+21-14} (1977Mo20), and 4.2 ps {I7} (1977Gu08) from {+58}Ni({+12}C,2p|g),{+64}Zn({+7}Li,p2n|g). 
J$E2 1777|g to 0+ g.s. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4 
T$weighted average of 0.90 ps {I14} from {+12}C({+64}Zn,{+8}Be|g) and 0.83 ps {I14} from {+64}Zn({+7}Li,p2n|g). 


level_energy_unit: KEV
level_comment:
E$log {Ift}=6.2 from {+68}As |e decay (J|p=3+) suggests this is a distinct level from the 0+ 3476 {I3}. 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: PS
level_comment:
MOMM1$from recoil into gas perturbed angular correlations (2011StZZ,1986Ba64). Relative to g=0.44 {I2} for the 596 {I2}+ state in {+74}Ge. 
J$J=6 from |g(|q), DCO and yield function; M1(+E2) 234|g to 5-. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$L(p,t)=(7); J=7 from |g(|q), DCO and yield function 
MOMM1$from recoil into gas perturbed angular correlations (2011StZZ,1986Ba64). Relative to g=0.44 {I2} for the 596 {I2}+ state in {+74}Ge. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$J=7 from |g(|q), DCO and yield function; M1+E2 400|g to 7-. L(p,t)=(6) discrepant (but the fit is poor). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
T$the B(E2)(606|g) exceeds RUL by a factor of |?3, suggesting that the T{-1/2} value may be too small 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
MOMM1$from transient field method (2011StZZ,1986Ba64); measured relative to a theoretical value of g=0.4 for the 3696, 6+ state in {+68}Ge 
J$J=8 from |g(|q), DCO and yield function; E2 1141|g to 6+. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
MOMM1$from transient field method (2011StZZ,1986Ba64); measured relative to a theoretical value of g=0.4 for the 3696, 6+ state in {+68}Ge 
J$J=8 from |g(|q), DCO and yield function; E2 1354|g to 6+. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$from crude shell-model calculations (1990Bo27). 
$Configuration:(|pg{-9/2}|pd{-5/2}){-6+} (1990Bo27). 


level_energy_unit: KEV
level_comment:
L$assigned L=2 and (2) by 1972Sh27 and 1972IsZV, respectively. 1977Gu02 claim at least two contaminant peaks at this energy and as such, no L value can be extracted. 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
E$1992He16 invert the order of the 252|g and 983|g and define a level at 3631. Given a single cascade of these two |g's between the 3883 and 2649 levels, the I|g data places the 252|g below the 983|g 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
G$from transient field method (1986Ba64); measured relative to a theoretical value of g=0.4 for the 3696, 6+ state in {+68}Ge 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$reported in 1992He16 and 1996Ch34. 2001Wa02 find no evidence for this level. 
J$1996Ch34 assign J|p=10+. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$1996Ch34 and 1992He16 report a 10025 level decaying by a 1364|g, while 2002WaZU report a 10024 level decaying by an 854|g. Possibly two distinct levels. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.15 ps {I21} from RDM (2012Lu03) and 1.80 ps {I21} from DSAM (1982Pa03). Others: 2.1 ps {I7} (1981De03), 3.5 ps {I+21-14} (1977Mo20), and 1.4 ps {I7} (1977Gu08). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 3.5 ps {I+21-14} (1977Mo20) and 4.2 ps {I7} (1977Gu08). These values are discrepant with the adopted value of 1.80 ps {I14}. 
T$Other: >3.5 ps (1982Pa03) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from DSAM in 1982Pa03. 
T$Others: 0.55 ps {I+28-14} (1983KiZW), 1.0 ps {I3} (1981De03), and 0.8 ps {I+3-2} (1977Mo20). 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: PS
level_comment:
G$from recoil into gas perturbed angular correlations (1982Ba42). Relative to g=0.44 {I2} for the 596, 2+ state in {+74}Ge. Value has been adjusted by evaluator from g=0.096 {I25} determined relative to g=0.47 {I10} for {+74}Ge. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
G$from recoil into gas perturbed angular correlations (1982Ba42). Relative to g=0.44 {I2} for the 596, 2+ state in {+74}Ge. Value has been adjusted by evaluator from g=0.122 {I29} determined relative to g=0.47 {I10} for {+74}Ge. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$d|s/d|W=116 {I35} 
J$from systematic trends and crude shell-model calculations 
$Configuration:(|pf{-5/2}){+2}{-4+}. 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
$d|s/d|W=156 {I47} 
J$from crude shell-model calculations 
$Configuration:(|pf{-5/2}|pg{-9/2}){-7-} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
T$weighted average (by compiler) of 271.14 d {I15} measured with the NaI(Tl) well counter and 271.07 d {I12} with the ionization chamber. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+72,68}=-0.184 {I13} (stat) {I67} (syst) (2024Wa45). Systematic uncertainties are from atomic mass-shift and field-shift factors. 
$R{-ch}=4.036 {I3} (stat) {I8} (syst) (2024Wa45) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: H
level_comment:
MOMM1, MOME2$ from atomic beam measurements . Compiled by 2011StZZ. 
J from atomic beam measurements (1976Fu06); |p from L(p,d)=3. 
T from |b{++} counting in {+69}Ge |e decay (1969Zo01). Others: 39.6 h 5 (1948Mc32), 40.4 h {I3} (1957Nu20), 38.5 h {I5} (1963Sc27) and 35.5 h {I8} (1965Te02), 38.4 h {I8} (1975Bu07) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: US
level_comment:
T weighted average of 5.1 |ms {I2} from {+69}Ge IT decay and 5.1 |ms {I2} from {+69}As |e decay both from delayed coincidences. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_comment:
MOMM1$from g-factor measured by stroboscopic resonance in {+69}Ga(p,n|g) (1970Ch05). Compiled by 2011StZZ 
J from L(p,d)=4 and M2 |g to 5/2- level 
T weighted average of 2.84 |ms {I7} from {+69}Ga(p,n|g) and 2.79 |ms {I6} from {+66}Zn(|a,n|g). Other: 3.2 |ms {I6} from {+69}Ge IT decay 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J 7/2 from |g(|q) in {+69}Ga(p,n|g); |p from E2 to 3/2- level. 
T$From {+66}Zn(|a,n|g). Other: 2.8 ps {I14} in {+69}Ga(p,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J 5/2 from |g(|q) in {+69}Ga(p,n|g); |p from E2 to 1/2- level 
T from DSA in {+69}Ga(p,n|g). Other: >1.7 ps from DSA in {+66}Zn(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J from |g(|q) in {+66}Zn(|a,n|g); |p: M1+E2 |g to 3/2- level 
T$Weighted average of 0.97 ps {I21} from DSA in (HI,xn|g) and 0.55 ps {I14} from DSA in {+69}Ga(p,n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J 11/2 from |g(|q) in (HI,xn|g); |p from M1 to 9/2+ level. 
T weighted average of DSA measurements, 0.50 ps {I11} in {+69}Ga(p,n|g), 0.59 ps {I7} in (HI,xn|g), and 0.49 ps {I+17-11} in {+66}Zn(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J 13/2 from |g(|q) in (HI,xn|g); |p from E2 to 9/2+ level. 
T$Weighted average of DSA measurements, 1.59 ps {I7} in (HI,xn|g) and 1.18 ps {I+35-21} in {+66}Zn(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J 9/2 from |g(|q) in (HI,xn|g); |p from E2 to 5/2- level. 
T$Weighted average of DSA measurements, 0.61 ps {I19} in (HI,xn|g), 0.54 ps {I14} in {+69}Ga(p,n|g), 0.83 ps {I+21-14} and 0.51 ps {I10} in {+66}Zn(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J 1/2,3/2 from |g(|q) in {+69}Ga(p,n|g); M1 to 5/2+ rules out 1/2 and gives |p=+ 
T from DSA in {+66}Zn(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J 3/2,1/2 from |g(|q) of 1452|g in {+69}Ga(p,n|g); excitation function excludes 1/2; |p from L(p,d)=1. 
T from DSA in {+69}Ga(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J 7/2 from |g(|q) in (HI,xn|g); |p=+ from M1 to 5/2+ 
T$Weighted average of DSA measurements, 0.76 ps {I+28-21} in {+66}Zn(|a,n|g), 0.55 ps {I+28-14} in (HI,xn|g); other: 2.1 ps {I14} in {+69}Ga(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J 3/2-,5/2-,7/2- from allowed log| {Ift}=5.83 {I5} in {+69}As |e decay, |g transition to 1/2- level rule out 7/2- 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J 13/2 from |g(|q) in (HI,xn|g); |p from M1 to 11/2+. 
T from (HI,xn|g); other: T{-1/2}>1.4 ps from DSA in {+66}Zn(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J 15/2 from |g(|q) in (HI,xn|g); |p from E2 to 11/2+ level. 
T$From (HI,xn|g). Others: 1.0 ps {I+6-4} and 0.62 ps {I+49-21} from DSA in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_comment:
J 3/2-,5/2-,7/2- from allowed log| {Ift}=5.77 {I5} in {+69}As |e decay from 5/2-; |g to 1/2- rules out 7/2- 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J 17/2 from |g(|q) in (HI,xn|g); |p from E2 to 13/2+ level. 
T$Weighted average of 0.6 ps {I1} in (HI,xn|g) and 0.49 ps {I+28-21} from DSA in {+66}Zn(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$possible separate level in (p,d) since J|p=(3/2+,5/2+) from L(p,d)=(2) for level at 2985 {I5}. 
J 3/2-,5/2-,7/2- from allowed log| {Ift}=5.45 {I5} from 5/2- in {+69}As |e decay |g transition to 9/2+ level rules out 3/2-, 5/2-. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J from L({+3}He,|a)=1; 3/2- favored if analog of {+69}Ga g.s. 
|G|a/|G|<0.01 at 95% confidence level from ({+3}He,t) reaction. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
T 0.90 ps {I+14-21} (1979Al08) and 1.25 ps {I25} (1976Eb02) give unacceptably large transition rates for the 414|g (E2). The T{-1/2} measurements were made by DSA of the 812|g which, however, is a doublet also depopulating the 1210 level. 
J 5/2+ consistent with |g(|q) and side feeding of 1997Be65 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J 5/2 from |g(|q) 822|g (1979Al08); J|p=5/2-; J=3/2,5/2 are possible from side feeding excitation function (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J 5/2,7/2,9/2 from |g(|q) (1979Al08); J|p=7/2+; J=5/2,7/2 are possible from side feeding excitation function (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J 13/2(+) favored from |g(|q) and yield ratio of 668|g (1975Eb05); J=13/2(+),15/2(+) most probable from |g(|q) and yield function of 668|g (1974Fo12); 13/2+ (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
J 11/2+ (1997Be65) 
E inferred from coincidence data showing a 712|g feeding 1407 level (1974Fo12). This level not seen by 1975Eb05. However, since they do see a 712|g, they cannot rule it out (1975Eb05) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J 9/2,11/2 most probable from |g(|q) (1979Al08); J|p=11/2-; J=9/2,11/2 are possible from side feeding excitation function (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
E$two closely spaced levels at 2483.5 {I5} and 2483.6 {I5} deexciting by 1132.9 and 1076.1 |g rays, respectively, were proposed by 1975Eb05 and 1976Eb02. From the variation of the relative intensity of these |g rays 1979Pa13 and 1982Pa03 assign both of them to one level. 
T$from 1133|g. T{-1/2}=0.62 ps +{I49}-{I21} from 1076|g. Authors (1979Al08) treated these two |g's as being from different levels 
J 15/2+ from |g(|q) and yield ratio of 1133|g (1975Eb05) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J (9/2+) assuming 603|g and 596|g to 13/2+ and 5/2+ levels to be E2 (|DJ=2) since these were observed in prompt |g|g coincidences (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J 15/2(+) from |g(|q) and yield ratio of 1669|g (1975Eb05); J=13/2(+),15/2(+) consistent with |g(|q) yield ratio of 1669|g (1974Fo12) 
T$from 1976Eb02; >0.69 ps (1979Al08) at both 14.0 MeV and 16.5 MeV 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$C{+2}S=0.2 {I1} 
This state may be the analog of the ground state of {+69}Ga. 
|G|a/|G|<0.01 at 95% confidence level (1988Ch38) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T corrected for feeding from above. Others: |<0.7 ps (1979Zo02), 1.1 ps {I2} (1997Be65) 
J 11/2+ from |g(|q) of 953|g and linear-polarization data (1979Zo02); same J|p assigned by 1982Pa03 and 1979Pa13 based on |g(|q) and yield data. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T other: 1.7 ps {I+7-4} (1982Pa03) 
J 13/2+ from |g(|q) of 1009|g and linear-polarization data (1979Zo02); same J|p assigned by 1982Pa03 and 1979Pa13 based on |g(|q) and yield data. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T weighted average of 1.0 ps {I3} (1997Be65) and 0.52 ps {I14} (1982Pa03) 
J 9/2(-) from |g(|q) and yield ratio (1982Pa03); 9/2- (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T weighted average of 1.11 ps {I35} (1997Be65), 1.66 ps {I42} (1979Zo02), and 1.87 ps {I49} (1982Pa03) 
J 13/2(+) from |g(|q) and yield ratio (1982Pa03); 13/2 from |g(|q) (1979Zo02); 13/2+ (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J 17/2(+) from |g(|q) and yield ratio (1982Pa03,1979Pa13). Reinvestigation of |g(|q) of 1348|g allowing for Doppler shift gave J=17/2 (1980Zo03). This resolves the discrepancy between 1979Pa13 and 1979Zo02 for the J of this level; 17/2+ (1997Be65) 
T others: 0.2 ps {I1} by RDDS (1997Be65), |<0.5 ps by recoil distance (1979Zo02) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J 15/2 from |g(|q) (1979Pa13); 15/2- (1997Be65) 
T others: 1.5 ps {I+12-4} (1982Pa03), |<0.7 ps by recoil distance (1979Zo02) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T other: 2.4 ps {I5} (1997Be65) 
J 19/2 from |g(|q) (1979Pa13); |p=- from linear polarization (1979Zo02); 19/2- (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
T Weighted average of 3.5 ps {I5} (1997Be65) and 2.9 ps {I3} (1979Zo02) 
J 21/2 from |g(|q) and yield; |p=- from RUL (1979Pa13) 


level_energy_unit: KEV
level_spin_parity: 23/2-
level_lifetime_unit: PS
level_comment:
T other: 12.1 ps {I10} (1997Be65) 
J (23/2) from |g(|q) and yield (1979Pa13); 23/2- most likely from systematics (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 27/2-
level_lifetime_unit: PS
level_comment:
J yield ratio suggests J>25/2; |g(|q) of 1242|g to 23/2 4595 level shows it to be quadrupole; hence J=27/2. J=27/2- from side feeding excitation function and systematics (1997Be65) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: H
level_comment:
T$reported as 38.82 h {I7} (stat) {I4} (syst); compiler combines uncertainties in quadrature. Value is weighted average of 38.68 h {I13} (stat) {I2} (syst), 38.76 h {I23} (stat) {I3} (syst), and 38.90 h {I9} (stat) {I1} (syst), all from combined (574.1|g+871.98|g+1106.77|g)(t) (2021Ha10). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
MOMM1,MOME2$from hyperfine spectroscopy (2020Ka58) 
J$from the Adopted Levels of {+69}Ge in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|d<r{+2}>{+72,69}=-0.244 {I6} (stat) {I62} (syst) (2024Wa45). Systematic uncertainties are from atomic mass-shift and field-shift factors. 
$R{-ch}=4.029 {I2} (stat) {I8} (syst) (2024Wa45) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.179 {I3} in Coulomb excitation. Others: 1.38 ps {I8} from B(E2)=0.169 {I10} from (e,e'), 1.32 ps {I14} from DSAM in {+12}C({+66}Zn, {+8}Be), 1.3 ps {I3} from DSAM in {+68}Zn(|a,2n|g), {+67}Zn(|a,n|g) and >5 ps in ({+7}Li,2n|g) 
J$from 1039.49|g E2 to 0+ 
MOME2$from multiple Coulomb Excitation (2003Su01). 
MOMM1$from weighted average of 0.88 {I8} (2013Gu23, from g-factor using TF), 0.90 {I16} (2007Bo41, from g-factor using TF), 0.86 {I24} (2006Le24, from g-factor using TF), 0.740 {I178} (1987La20, from g-factor using TF), 0.94 {I52} (1984Pa20, from g-factor using TF), 0.94 {I20} (1977Fa07, from g-factor using IMPAC). Others: 0.76 {I16} (1977Fa07), 1.18 {I58} (1969He11); the same data reanalyzed by 1974Hu01 gave |m=1.76 {I42}; the same data reanalyzed by 1977Fa07 according to the latest understanding of the experiment and corrections |m = 0.94 {I20} (from g=0.47 {I10}) (this value is included in the weighted average) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$from electron spectrometer measurement with pulsed-cyclotron beam in (p,p'|g). Others: 2.9 ns {I4} from {+70}Ga |b{+-} decay; 4.8 ns {I7} from B(E2) in Coulomb excitation 
J$L=0 from {+72}Ge(p,t) and {+66}Zn({+6}Li,d); E0 transition to g.s.. The level interpreted as deformed-intruder state (2003Su01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$from 1708|g E2 transition to g.s. 
T$from DSAM in {+12}C({+66}Zn, {+8}Be). Other: 1.1 ps {I+10-4} from (|a,2n|g), (|a,n|g), 4.2 ps {I+26-14} from Coulomb excitation and > 7 ps in {+65}Cu({+7}Li, 2n|g), {+60}Ni({+12}C,2p|g) 
MOME2$from multiple Coulomb Excitation. 
MOMM1$from g-factor measurements using TF in Coulomb excitation. Other: 0.8 {I12} from {+12}C({+66}Zn, {+8}Be) using TF. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+12}C({+66}Zn,{+8}Be). Others: 4 ps {I1} from DSAM in {+65}Cu({+7}Li,2n|g), {+60}Ni({+12}C,2p|g) and 1.7 ps {I4} from Coulomb excitation and 0.8 ps {I2} from DSAM in {+68}Zn(|a.2n|g),{+67}Zn(|a,n|g). 
J$from 1113.60|g E2 to 2+; assumed E2 cascade member 
MOME2$from multiple Coulomb Excitation (2003Su01) 
MOMM1$from g-factor measurements using TF in Coulomb excitation (2013Gu23,2007Bo41). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=2; J|p not consistent with observed log| {Ift}=7.8 from 4+ 
T$Other: >0.4 ps from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.55 ps {I7} in {+12}C({+66}Zn, {+8}Be|g) (from DSAM) and 0.4 ps {I1} in {+65}Cu({+7}Li,2n|g), {+60}Ni({+12}C,2p|g) (from DSAM). Others: 2.3 ps {I5} from {+65}Cu({+7}Li,2n|g), {+60}Ni({+12}C,2p|g) 
J$L(p,t)=3 
$B(E3)=0.073 {I10} in {+70}Ge(e,e'); 0.068 from Coulomb excitation 
MOMM1$from transient field method in Coulomb excitation (2007Bo04) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4; 1098.54|g E2 to 2+. Discrepant with L(|a,|a')=3 for E=2800 keV {I10} which may be a different level. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$others: 2.6 ps {I6} from DSAM in {+65}Cu({+7}Li,2n|g), {+60}Ni({+12}C,2p|g) 
J$from 1143.89|g E2 to 4+; band assignment 


level_energy_unit: KEV
level_spin_parity: (3,4)
level_lifetime_unit: PS
level_comment:
J$log| {Ift}=7.7 {I1} from 4+ in |e decay; J=5 unlikely because of 2333|g to 2+ level 
T$from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: PS
level_comment:
J$J=6 from |g(|q) in {+46}Ti({+28}Si,4p|g), |p from 250|g M1(+E2) to 5- 
T$others: 40 ps {I8} in {+68}Zn(|a,2n|g), {+67}Zn(|a,n|g) and 74 ps {I6} in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 9(-)
level_comment:
J$from 1344.1|g (E2) to 7-, 1273|g from 11(-); inconsistent with (6,7,8) from |g(|q) in ({+7}Li,2n|g) 


level_energy_unit: KEV
level_spin_parity: (10)
level_lifetime_unit: NS
level_comment:
T$from electronic timing in {+68}Zn(|a,2n|g), {+67}Zn(|a,n|g) 
J$T{-1/2} of this level suggests that the 1108|g to 8+ may be M2, suggesting an assignment of J|p=10-. However, level is assigned as side band member based on 8+ in {+64}Ni({+12}C,|a2n|g), suggesting an assignment of J|p=10+. Other: 9+ in {+65}Cu({+7}Li,2n|g), {+60}Ni({+12}C,2p|g). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$weighted average of 2.8 ns {I8} (1958Ke20, using |b|g delayed-coincidence technique) and 3.0 ns {I5} (1958Al01, using delayed |b-e coincidences) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 transition to 0+ g.s. 
T$weighted average of 1.3 ps {I3} (1984Ef01) and 1.5 ps {I10} (1977Mo20) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$E2 transition to 1039.2 level and yield function 
T$weighted average of 0.6 ps {I3} (1984Ef01) and 1.0 ps {I3} (1977Mo20) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$|g(|q) and linear polarization measurement of 1522|g (1978Cl05) 
T$unweighted average of 0.6 ps {I1} (1984Ef01) and 0.3 ps {I1} (1977Mo20) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|g(|q) of 1144|g E2 transition and yield function 
T$weighted average of 0.5 ps {I1} (1977Mo20) and 0.6 ps {I2} (1984Ef01) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$|g(|q) and yield function of 854|g 
T$from 1982Cl02. Others: 3 ps {I+4-2} (1977Mo20), 1.9 ps {I9} (1984Ef01) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: PS
level_comment:
J$J=6 from |g(|q) of 250|g (1976Mo15); parity from M1 transition to J|p=5- level at 3415.7 
T$from 1982Cl02. Other: 40 ps {I8} (1984Ef01) 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: PS
level_comment:
J$|g(|q) of 947|g suggests a 6+ assignment but the yield function does not confirm this 
T$Other: > 3 ps (1977Mo20) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$J=7 from |g(|q) of 288|g and 658|g (1976Mo15); parity from M1 transition to J|p=6- level at 3666.1 keV 
T$weighted average of 17.5 ps {I10} (1982Cl02) and 15 ps {I2} (1984Ef01). 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
J$J from |g(|q) of 344|g and 1003|g; absence of a transition to the 5- level at 3415.7 may indicate a positive parity for this level 


level_energy_unit: KEV
level_spin_parity: (8)+
level_lifetime_unit: PS
level_comment:
J$1134|g E2 transition and yield function 
T$Other: 0.8 ps {I2} from 1977Mo20 which if corrected for the tail of the 1144|g is expected to be less than the reported value. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$J suggested by the |g(|q) of the 896|g; this is not confirmed by the yield function 
T$from 1977Mo20 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: NS
level_comment:
T$from 1976Mo15 
J$the T{-1/2} for this level suggests that the 1109|g may be M2 with an assignment of J|p=10- 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{+2}{-|g0}/|G (MeV)=3.0 {I6} 
S$14 {I2} at 10 MeV 
$I{-s}: Integrated photon scattering cross section = 3.3 eVb {I6} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{+2}{-|g0}/|G (MeV)=11 {I3} 
S$55 {I6} at 10 MeV 
T$|G=|G{-0} 
$I{-s}: Integrated photon scattering cross section = 11.3 evb {I27} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{+2}{-|g0}/|G (MeV)=14 {I5} 
S$31 {I7} at 10 MeV 
T$|G=|G{-0} 
$I{-s}: Integrated photon scattering cross section = 10.6 evb {I34} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=67 {I11} 
$I{-s}: Integrated photon scattering cross section = 40.5 eVb {I68} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g0}{+2}/|G (MeV)=61 {I11} 
$I{-s}: Integrated photon scattering cross section = 35.6 eVb {I65} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g0}{+2}/|G (MeV)=67 {ILT} 
$I{-s}: Integrated photon scattering cross section = 37.8 eVb {I52} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=28 {I16} 
$I{-s}: Integrated photon scattering cross section = 13.9 eVb {I82} 
J$from 4790.4|g E1 to 0+ 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{-|g0}{+2}/|G (MeV)=40 {I10} 
$I{-s}: Integrated photon scattering cross section = 19.2 eVb {I46} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g0}{+2}/|G (MeV)=89 {I25} 
$I{-s}: Integrated photon scattering cross section = 38.8 eVb {I11} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=112 {I21} 
$I{-s}: Integrated photon scattering cross section = 46.6 eVb {I88} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g0}{+2}/|G (MeV)=133 {I22} 
$I{-s}: Integrated photon scattering cross section = 51.2 eVb {I85} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=113 {I18} 
$I{-s}: Integrated photon scattering cross section = 43.0 eVb {I67} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=96 {I30} 
$I{-s}: Integrated photon scattering cross section = 32.0 eVb {I99} 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=149 {I31} 
$I{-s}: Integrated photon scattering cross section = 48.0 eVb {I98} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{-|g0}{+2}/|G (MeV)=147 {I46} 
$I{-s}: Integrated photon scattering cross section = 42.8 eVb {I14} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{-|g0}{+2}/|G (MeV)=133 {I28} 
$I{-s}: Integrated photon scattering cross section = 37.9 eVb {I80} 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=136 {I25} 
$I{-s}: Integrated photon scattering cross section = 36.1 eVb {I67} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{-|g0}{+2}/|G (MeV)=168 {I25} 
$I{-s}: Integrated photon scattering cross section = 44.1 eVb {I66} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=289 {I49} 
$I{-s}: Integrated photon scattering cross section = 74.1 eVb {I13} 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=249 {I60} 
$I{-s}: Integrated photon scattering cross section = 53.8 eVb {I13} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=316 {I60} 
$I{-s}: Integrated photon scattering cross section = 66.0 eVb {I13} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=307 {I66} 
$I{-s}: Integrated photon scattering cross section = 59.0 eVb {I13} 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_comment:
$|G{-|g0}{+2}/|G (MeV)=307 {I86} 
$I{-s}: Integrated photon scattering cross section = 51.5 eVb {I15} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$|G{-|g0}{+2}/|G (MeV)=332 {I78} 
$I{-s}: Integrated photon scattering cross section = 48.5 eVb {I12} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$R=4.07 fm {I2} (1975Kl10), 4.055 fm {I8} (1990Kh03); R is the rms value of the charge distribution 


level_energy_unit: KEV
level_comment:
$J|p=2+ 
E$the 2156 and 2160 levels form a doublet with an estimated separation of 3.4 keV {I5} (1969Hi01) 


level_energy_unit: KEV
level_comment:
$J|p=3-; based on the large |s(p,p') at 10 MeV for the 2565-keV level which suggests that it is the one-phonon octupole level. 
$|b{-3}=0.265 {I20} (1992Ke07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$J|p=(4+) from angular distribution and comparison with angular distribution data on {+72}Ge (1967Kr01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$J|p=4+ assignment by other reaction studies confirmed by the |s(|q) data; but little could be concluded from the fit to the vector analyzing power (VAP) data (1978Sz08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$J|p=4+ shows better overall fit to the |s(|q) and VAP data; however, it is possible that the data have contributions from more than one level (1978Sz08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$J|p=(4+) appears to be most consistent with |s(|q) and VAP data; because of the experimental uncertainties of the data on this weakly excited level, this assignment is tentative (1978Sz08) 


level_energy_unit: KEV
level_comment:
E$this level is possibly the 3139 level in {+74}Ge present as a 3.4% impurity in the {+70}Ge target 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$from 1980Le16. Others: B(E2)=0.179 {I3} (1983Uh01); B(E2)=0.179 {I3}; B(E2)=0.172 {I21} (1962St02) 
G$from weighted average of 0.44 {I4} (2013Gu23, using TF), 0.45 {I8} (2007Bo41, using TF), 0.370 {I89} (1987La20, using TF), 0.468 {I26} (1984Pa20, using TF) and 0.47 {I10} (1977Fa07, using IMPAC). Others: 0.38 {I8} (1977Fa07), 0.59 {I29} (1969He11); the same data reanalyzed by 1974Hu01 gave g=0.88 {I21}; the same data reanalyzed by 1977Fa07 according to the latest understanding of the experiment and corrections give g=0.47 {I10} (this value is included in the weighted average). 
$Q=+0.04 {I3} from multistep Coulomb excitation in 2003Su01; Q=+0.03 {I6} from multistep Coulomb excitation in 1980Le16 and correspond to considering {+70}Ge to be almost spherical; if it is considered as a moderately deformed oblate spheroid the same data give B(E2)=0.178 {I3} and Q=+0.09 {I6}; Q=+0.003 {I100} (1969Si15) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
BE2$Coulomb excitation from 1039.5 to 1215.6 level; weighted average of 0.0158 {I24} (1972Si06) and 0.012 {I3} (1980Le24) 
T$Deduced from B(E2) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$weighted average of +0.39 {I37} and +1.03 {I44} for two targets and two beam energies in 2013Gu23 using TF. 
BE2$for Coulomb excitation from g.s. to 1708.2 level (1980Le24) 
$B(E2)(1040 to 1708)=0.050 {I19}; B(E2)(1216 to 1708)=0.018 {I16} (1980Le24) 
T$from B(E2) for Coulomb excitation from 1039.5 to 1708.2 level with a branching fraction of 0.53 for the 669 transition from adopted |g's. Other: 5.4 ps {I+53 - 18} in 1980Le24 
MOME2$=-0.07 {I4} from multistep Coulomb Excitation in 2003Su01 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
G$weighted average of +0.21 {I63} and +0.22 {I36} for two targets and two beam energies (2013Gu23, using TF) and 0.5 {I2} (2007Bo41, using TF). 
BE2$for Coulomb excitation from 1040 to 2154 level 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3$from 1983Uh01; authors state that large uncertainties in data and possible defects in the first order DWBA do not allow a precise determination of B(E3). Other: 0.043 {I3} (1980Le24) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+72,70}=-0.121 {I6} (stat) {I36} (syst) (2024Wa45). Systematic uncertainties are from atomic mass-shift and field-shift factors. 
$R{-ch}=4.044 {I2} (stat) {I4} (syst) (2024Wa45) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
MOMM1$hyperfine spectroscopy at ISOLDE-CERN (2020Ka58). Others: +0.546 {I5} (atomic beam, 1966Ch02, 1970Be29, 2019StZV) 
J$spin from atomic beam (1963Ch12). Parity from L(d,p)=L(p,d)=1 from 0+ targets 
T$from detection of K X rays and Auger electrons using Ge detector and proportional counters (1985Ha06); the adopted value is the weighted average of six experimental runs covering time span of up to 12 half-lives of {+71}Ge. The quoted value includes statistical and systematic uncertainties. Others: 11.15 d {I15} (1971Ge02), 10.5 d {I4} (1956Ru45), 12.5 d {I1} (1955Bi96), 11 d (1950Ho26), 11.4 d {I1} (1948Mc32), 11 d (1941Se03) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
MOMM1$from DPAD (1968Mo12) 
MOME2$2016St14 evaluated quadrupole moment with reference to measured value for {+73}Ge g.s. by TDPAD method (1993Co17) and using quadrupole interaction frequencies from 1981Vi05. The same value is listed in 2021StZZ compilation 
J$L(d,p)=L(p,d)=3 from 0+; 174.96|g E2 to 1/2- 
T$weighted average of 79 ns {I2} (1968Mo12) in (p,n|g), 88 ns {I4} (1978Ta08) and 73 ns {I11} (1974Iv02) in (n,|g), using |g|g(t) 
$Q(175 level)/Q({+69}Ge,398)=0.22 {I3} (1973HaVW) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$from TDPAD (1970Be29). Value of -1.0413 {I7} in 1970Be29 evaluated to -1.039 {I2} in 2020StZV 
MOME2$from QIR (1975Ri03,1976Br41). Other: 0.28 (1973RiZI) 
J$L(d,p)=L(p,d)=4 from 0+; L+1/2 from analyzing power in (pol d,p); L(p,t)=0 from 9/2+ 
T$from the decay of 175|g in NaI detectors except as noted in IT decay. Value is weighted average of results listed as follows: 20.082 ms {I+71-70} (2014De19, decay curve for 198.4-keV radiation from coincidence summing of 174.95|g and ce of 23.44-keV transition within HPGe detector array GEANIE at LANSC-WNR Los Alamos facility, where the {+71m}Ge activity by {+72}Ge(n,2n) reaction by scattered neutrons incident on the HPGe detector system; statistical and fitting uncertainties were included, in averaging procedure uncertainty was increased to 0.105 ms by evaluators to account for possible systematic uncertainties); 20.48 ms {I18} (Ge(Li) with NaI anti-Compton,1980Jo11); 21.5 ms {I4} (neutron activation of Ge(Li) detector,1974Bu14); 20.4 ms {I4} (1976Ga33); 21.5 ms {I10} (1971Go21); 22.2 ms {I10} (1971Mu14); 20.4 ms {I10} (1970Ru08,1969Ru10); 21.2 ms {I12} (1966Me02); 20.0 ms {I6} (1963Al32); 19.5 ms {I5} (conversion electron detection in anthracene detector, 1962Re09); 20 ms {I1} (1962Mo19); 19.4 ms {I4} (1961Mo06); 20.3 ms {I3} (1961Sc11). Values of 21.87 ms {I7} (1972Br53), and 16 ms {I1} (1959Gl56) were not included in the averaging procedure, as these appear to be outliers. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$391.4|g M1+E2 to 9/2+; spin=5/2,7/2 from |g(|q) in (|a,n|g); 7/2 also favored by excitation function in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$1/2 from |g(|q) and |g|g(|q) in (|a,n|g) and excitation function in (p,n|g); 1/2- from Gamow-Teller excitation in ({+3}He,t). Other: L(p,d)=2 for an uncertain level at 807 {I10} is in disagreement 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$|g rays to 1/2- and 5/2- give (1/2-,3/2,5/2-); possible |e feeding from 5/2- parent (log {Ift}= 9.1) disfavours 1/2-; L(d,p)=(1) from 0+ favors 3/2- 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(p,d)=1 from 0+; L+1/2 from analyzing power in (pol d,p). Excitation function in (p,n|g) gives 3/2-, excludes 1/2- 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$|g|g(|q)(ADO) and |g(lin pol) in (|a,|a3n|g); excitation function in (p,n|g) gives 7/2-, excludes 7/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L(d,p)=2 from 0+; L+1/2 from analyzing power in (pol d,p). L(p,d)=1 for a group at E=1166 {I10} is in disagreement, probably indicating a different level 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$974.2|g E2, |DJ=2 to 9/2+; 1126.6|g from J=17/2 
T$from 0.90 ps {I18} with no side feeding corrections in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g(lin pol) in (|a,n|g); excitation function in (p,n|g) also gives 11/2, excludes 9/2 
T$from 0.90 ps {I18} with no side feeding corrections in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$1212.5|g |DJ=2 to 1/2-; L(p,d)=3 from 0+; excitation function in (p,n|g) gives 3/2-,5/2-, excludes 3/2+,5/2+,7/2+. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$L(d,p)=L(p,d)=1 from 0+; L-1/2 from analyzing power in (pol d,p). Excitation function in (p,n|g) also gives 1/2-, excludes 1/2+,3/2,5/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$1298.5|g D+Q to 1/2-; excitation function in (p,n|g) gives 1/2+,3/2- and excludes 1/2-,3/2+,5/2,7/2; 3/2- from Gamow-Teller excitation in ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$excitation function in (p,n|g) (1993Fe03) gives 1/2-,7/2-, excludes 1/2+,3/2, 5/2,7/2+; |g to 1/2-. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$possible doublet proposed by the evaluators based on very different |g branching ratios observed from 1379 level in |e decay, (|a,n|g), (n,|g) and (p,n|g) reactions. L(d,p)=(2,3) level at 1375 {I3} is associated with this level, rather than the (1/2-) level near this energy, based on spin consideration 
J$log| {Ift}=7.4 from 5/2-; |gs to 5/2- and 7/2+; L(d,p)=(3,2); (L+1/2) from analyzing power in (pol d,p) suggests (5/2+,7/2-); |s(|q) in ({+3}He,t) gives 5/2- 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$excitation function in (p,n|g) gives 5/2-,7/2+, excludes 5/2+, 7/2-, 9/2+; L(d,p)=(3) from 0+ for a group at E=1470. However, L(d,p)=2 from 0+ for a group at E=1474 {I3} is inconsistent, which might indicate a different level 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2-)
level_comment:
J$primary |g from 1/2+ in (n,|g) and |g rays to 5/2+ and 1/2-; excitation function in (p,n|g) gives 1/2+,3/2-, excludes 1/2-,3/2+,5/2. But L(d,p)+(2) from 0+ for a group at E=1539 {I3} is inconsistent 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L(d,p)=2 from 0+; L+1/2 from analyzing power in (pol d,p). However, L(p,d)=3 for a group at 1558 {I2} is in disagreement, which could indicate a different level 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2+)
level_comment:
J$excitation function in (p,n|g) gives 3/2-,5/2-,7/2+, excludes 3/2+,5/2+,7/2-,9/2; |g to 7/2+ disfavors 3/2- 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2-)
level_comment:
E$ this level seems different from the 1629 level, although the energies of the 883.5 and 1632.0 |g rays are close to 881.9 and 1629.1, respectively assigned to the 1629 level. 
J$|g rays to 1/2- and 5/2- 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
J$1/2-,3/2- from L(p,d)=1 for a group at E=2031 {I3} and 3/2+,5/2+ from L(d,p)=2 for a group at E=2028 {I3} are in disagreement, which may indicate two separate levels near this energy. Strong primary |g from 1/2+ in (n,|g) suggests 1/2,3/2 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$from ({+3}He,t). Others: 2041 {I3} from (d,p) and 2045 {I3} from (p,d) 
J$L(d,p)=1 from 0+. Tentative (3/2-,5/2-) from |s(|q) in ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$from ({+3}He,t). Other: 2279 {I3} from (p,d) 
J$L(p,d)=1 from 0+. Tentative (3/2-,5/2-) from |s(|q) in ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$this level is most likely different from the 2276 level due to differences in J|p assignments 
J$L(d,p)=2 from 0+ and L+1/2 from analyzing power in (pol d,p) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$L(p,d)=1 from 0+. Tentative (3/2-,5/2-) from |s(|q) in ({+3}He,t). This level is probably different from 2345 {I3} in (d,p) due to different L-transfers involved 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
E$this level is likely different from the 2435.2, 1/2+ level 
J$tentative assignment from |s(|q) in ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$weighted average of 2896 {I3} from (d,p), 2888 {I1} from ({+3}He,t), and 2889 {I4} from (p,d) 
J$L(p,d)=1 from 0+. Tentative (5/2-) from |s(|q) in ({+3}He,t) 


level_energy_unit: KEV
level_comment:
E$wide bump in the range 2-8 MeV with a total G-T strength=3.2 {i4}. G-T strengths (1991As05) for different energy regions are: 0.17 {i3} for 0-1 MeV, 0.14 {i3} for 1-2 MeV, 0.13 {i3} for 2-3 MeV, 0.35 {i6} for 3-4 MeV, 0.71 {i14} for 4-5 MeV, 0.64 {i15} for 5-6 MeV, 0.55 {i14} for 6-7 MeV, 0.55 {i14} for 7-8 MeV 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from ({+3}He,t) 
J$IAS of 3/2- g.s. in {+71}Ga 
$53% {I9} decay proceeds through neutron decay to 1.22 MeV state in {+70}Ge with subsequent observation of 1040|g in {+70}Ge. 
$The |g decay of IAS to {+71}Ga through single high-energy |g ray or a cascade of two |g rays is determined to be less than 11%(1988Ch25) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$Gamow-Teller giant resonance (GTGR), wide structure from 10-16 MeV, peaking at |?11.75 MeV (2015Fr02,2011Fr15) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2-)
level_lifetime_unit: PS
level_comment:
$431.7, 798.3, 911.4 and 1191.3 |g rays placed by 1972Va17 from this level. The 911|g is not seen by 1990Me01 while others are placed from different levels. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from the Adopted Levels 
E$transitions from this 20-ms isomeric state were not observed in these studies. The level energy is taken from 1971Mu14. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$the 1096.1 and 1096.3 levels reported elsewhere (1974Ma32) are not resolved in experiments with this reaction (1977Ke16) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$13/2+; from |g(|q) and |p from polarization data of 974|g (1974Fo12) confirmed by the |g(|q) and polarization data of 1976Eb02 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$|g(|q) of 1278|g gives a unique assignment of J=11/2 (1974Fo12) 
T$weighted average of 0.52 ps {I10} and 0.57 ps {I11} (1976Eb02) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=1.118 {I2}, g|G{-n}=4.6 eV {I10}, |G{-|g}=0.160 eV {I25}, g|G{-n}|G{|g}/|G=0.155 eV {I25} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=1.474 {I5}, g|G{-n}=0.70 eV {I12}, |G{-|g}=0.150 eV {I25}, g|G{-n}|G{|g}/|G=0.124 eV {I25} 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$possible level reported only in 1968Go02, not in any other reaction or decay. Level not listed in the Adopted Levels 
$d|s/d|W(max)<7 |mb/sr (1968Go02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$510 in 1976Yo04 is composite of 501 and 526 levels; 480 listed in table 2 of 1976Yo04 and in table I of 1968Go02 
S$0.27 (1968Go02) 
$d|s/d|W(max)=600 |mb/sr for 480 level (1968Go02) 


level_energy_unit: KEV
level_comment:
E$level reported only in 1968Go02, not in any other reaction or decay. 
$d|s/d|W(max)=35 mb/sr (1968Go02) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$possible level reported only in 1968Go02, not in any other reaction or decay. Level not listed in the Adopted Levels 
$d|s/d|W(max)<7 mb/sr (1968Go02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$1977Bi08 state that energy is from 1976Yo04 but the latter do not report this level 
L$(2) in 1968Go02 
S$0.021 (1968Go02) 
$d|s/d|W(max)=25 |mb/sr for 730 level (1968Go02) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$level reported only in 1968Go02, not in any other reaction or decay. Level not listed in the Adopted Levels 
$d|s/d|W(max)<7 mb/sr (1968Go02) 


level_energy_unit: KEV
level_comment:
E$level reported only in 1968Go02, not in any other reaction or decay. 
$d|s/d|W(max)=40 mb/sr (1968Go02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J,L,S$from 1976Yo04; no angular distribution data in 1977Bi08 
S$0.029 (1968Go02) 
$d|s/d|W(max)=37 |mb/sr for 1160 level (1968Go02) 


level_energy_unit: KEV
level_spin_parity: (7/2-,5/2+)
level_comment:
E$ possibly a doublet from L=(3,2) 
S,L$0.019 for L=(2) for 1380 group (1968Go02) 
$d|s/d|W(max)=26 |mb/sr for 1380 level (1968Go02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$from VAP data of 1976Yo04 for 1542 group which is identified in 1977Bi08 with their 1556 group 
S$0.493 (1976Yo04), 0.21 (1968Go02) 
$d|s/d|W(max)=280 |mb/sr for 1550 level (1968Go02) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
S$1.53 (1976Yo04), 0.63 for L=(3) (1968Go02) 
J$7/2 was proposed by 1976Yo04 from their VAP data but this assignment has been questioned by 1977Bi08 
$d|s/d|W(max)=160 |mb/sr for 1690 level (1968Go02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$a small peak from the 1006 level in {+77}Ge is also present. S' upper limit with about one-third of observed strength due to 1006 level. 


level_energy_unit: KEV
level_comment:
E$a doublet partly due to 1733 level in {+73}Ge. 
$d|s/d|W(max)=170 |mb/sr for 2350 level (1968Go02) 


level_energy_unit: KEV
level_comment:
E$a doublet partly due to the 2459 level in {+73}Ge. 
$d|s/d|W(max)=380 |mb/sr for 3080 level (1968Go02) 


level_energy_unit: KEV
level_comment:
L$0 in 1977Bi08, but |s(|q) distribution not shown by authors 
$d|s/d|W(max)=260 |mb/sr for 3230 level (1968Go02) 


level_energy_unit: KEV
level_spin_parity: (5/2+,1/2-)
level_comment:
E$a doublet partly due to 2382 level in {+75}Ge 
S,L$0.086 for L=2 (1968Go02) 
$d|s/d|W(max)=180 |mb/sr for 3280 level (1968Go02) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1968Mo12). Other: 84 ns {I2} (thesis by W. Withuhn, Freien University, Berlin (1968); quoted by 1978Ta08) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$20.2 ms (1970Be29) 
G$other: -0.2304 {I5} (1970Be29). 
T$weighted average of 20.3 ms {I3} (1961Sc11) and 19.5 ms {I5} (1962Re09). Value is 20.22 ms {I12} in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$Relative=96 {I4} 
S$at E(p)=2.03 MeV 
J$|g(|q) of 500|g limits it to 1/2 or 3/2; |g(|q) of 247|g to this level excludes 1/2; |p from multipolarity of 500|g (1975On01). Excitation function (1993Fe03) gives 3/2-,5/2-, excludes 1/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$Relative=100 {I3} 
J$5/2 from excitation function and |g(|q). Excitation function (1993Fe03) gives 3/2+,5/2+, excludes 7/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$Relative=55.4 {I20} 
J$7/2+ to 11/2+ from |g(|q) and M1 transition to the 198 {I9}/2+ level, the excitation function favors J=7/2. Excitation function (1993Fe03) gives 5/2-,7/2+, excludes 5/2+,7/2-,9/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
$Relative=82.1 {I23} 
T$from 1999Iv08. Other: 0.46 ps {I+6-5} (2002Ka51) 
J$3/2-,1/2- from excitation function and |g(|q); |p from multipolarity of 708|g. Excitation function (1993Fe03) gives 3/2-,5/2, excludes 1/2- 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
$Relative=57.6 {I12} 
J$|g(|q) gives a unique assignment of 5/2; |p from M1+E2 |g to 500 level. Excitation function (1993Fe03) gives 3/2-,5/2-, excludes 7/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
$Relative=29.3 {I8} 
J$1/2 from |g(|q) and excitation function (1993Fe03). Excitation function (1993Fe03) excludes 3/2-,5/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$Relative=67.8 {I14} 
J$3/2- from |g(|q) and excitation function; |p from M1 transition to 500 level Excitation function (1993Fe03) gives 3/2-, excludes 1/2-,3/2+,5/2 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
$Relative=36.1 {I10} 
T$from 1999Iv08. Other: 0.47 ps {I+15-9} (2002Ka51) 
J$5/2 uniquely determined from |g(|q) of 527|g; negative parity preferred from excitation function. Excitation function (1993Fe03) gives 3/2-,5/2-,7/2+ with a better agreement with 5/2-; excludes 3/2+,5/2+,7/2- 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$Relative=6.25 {I16} 
E$level from 1974Ma32 only 
J$(7/2 to 11/2) from |g(|q) of 839|g; excitation function prefers J=9/2. Excitation function (1993Fe03) gives 9/2-,9/2+, excludes 7/2,11/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$Relative=34.8 {I9} 
J$1/2,3/2 from |g(|q) of 1096|g; excitation function prefers J=3/2. Excitation function (1993Fe03) gives 3/2-, marginally excludes 5/2-; excludes 1/2-,3/2+,5/2+,7/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
$Relative=12.2 {I11} 
T$from Doppler shift for 921|g (2002Ka51); the authors incorrectly assigned 921|g to 3/2- level. 
J$7/2 uniquely determined from |g(|q) of 921|g. Excitation function (1993Fe03) gives 7/2-, excludes 5/2,7/2+,9/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$Relative=37.5 {I12} 
J$3/2,1/2 from |g(|q) of g.s. transition; excitation function favors J=3/2. Excitation function (1993Fe03) gives 3/2,5/2+, excludes 1/2,5/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
$Relative=10.9 {I4} 
J$3/2 to 7/2 from |g(|q); excitation function favors 5/2. Excitation function (1993Fe03) gives 3/2-,5/2+, excludes 3/2+,5/2-,7/2 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
$Relative=20.8 {I6} 
T$from 1999Iv08. Other: 0.31 ps {I+5-4} (2002Ka51) 
J$unique assignment of 5/2 from |g(|q) of both 713|g and 1212|g; excitation function favors negative parity. Excitation function (1993Fe03) gives 3/2-,5/2-, excludes 3/2+,5/2+,7/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$Relative=8.1 {I4} 
T$other: 0.31 ps +5-4 (2002Ka51) 
J$1/2,3/2 from |g(|q) of 1299|g; excitation function favors negative parity. Excitation function (1993Fe03) gives 1/2+,3/2-, excludes 1/2-,3/2+, 5/2,7/2 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
T$0.33 ps +8-6 (2002Ka51) 
J$excitation function (1993Fe03) gives 1/2-, but does not seem to rule out 1/2+ and 7/2 from figure 3 in 1993Fe03, excludes 3/2,5/2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$d|s/d|W(q=0)=0.786 mb/sr {I9} (2015Fr02) 
$Solar neutrino capture rate=109.8 SNU {I13} (2015Fr02) 
$B(>)=0.0891 {I13} (1998Ej03) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$d|s/d|W(q=0)=0.071 mb/sr {I4} (2015Fr02) 
$Solar neutrino capture rate=1.2 SNU {I7} (2015Fr02) 
$B(>)=0.0049 {I18} (1998Ej03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$d|s/d|W(q=0)=0.171 mb/sr {I4} (2015Fr02) 
$Solar neutrino capture rate=2.7 SNU {I2} (2015Fr02) 
$B(>)=0.0208 {I21} (1998Ej03) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$830 in 1998Ej03 
$d|s/d|W(q=0)=0.210 mb/sr {I4} (2015Fr02) 
$Solar neutrino capture rate=0.61 SNU {I7} (2015Fr02) 
$B(>)=0.0237 {I23} (1998Ej03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$d|s/d|W(q=0)=0.184 mb/sr {I4} (2015Fr02) 
$Solar neutrino capture rate=0.33 SNU {I3} (2015Fr02) 
$B(>)=0.0233 {I24} (1998Ej03) 
E$1096 (1984Ko10), 1160 (1998Ej03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$d|s/d|W(q=0)=0.126 mb/sr {I2} (2015Fr02) 
$Solar neutrino capture rate=0.17 SNU {I1} (2015Fr02) 
$B(>)=0.0201 {I23} (1998Ej03) 
E$1299 (1984Ko10), 1360 in 1998Ej03 could be a composite of 1299 and 1378 keV peaks 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$B(Fermi)=0.0900 {I22} (2011Fr15) 
$53% {I9} decay proceeds through neutron decay to 1.22 MeV state in {+70}Ge with subsequent observation of 1040|g in {+70}Ge. 
$The |g decay of IAS to {+71}Ga through single high-energy |g ray or a cascade of two |g rays is determined to be less than 11% (1988Ch25) 
E$from 2011Fr15 and 2015Fr02, with uncertainty estimated as 5 keV by evaluators based on FWHM=45 keV. Other: 8932 {I13} (1988Ch25). 
J$IAS of 3/2- g.s. in {+71}Ga 
$|G from 2011Fr15 
$d|s/d|W(q=0)=9.04 mb/sr {I12} (2011Fr15) 


level_energy_unit: KEV
level_comment:
E$wide bump in the range 2-8 MeV with a total B(>)=3.2 {I4}. B(>) strengths (1991As05) for different energy regions are: 0.17 {I3} for 0-1 MeV, 0.14 {I3} for 1-2 MeV, 0.13 {I3} for 2-3 MeV, 0.35 {I6} for 3-4 MeV, 0.71 {I14} for 4-5 MeV, 0.64 {I15} for 5-6 MeV, 0.55 {I14} for 6-7 MeV, 0.55 {I14} for 7-8 MeV 


level_energy_unit: KEV
level_comment:
L$3+4 for 186 {I5} group (1973Fo01): composite of 174+198 
S$ 3.64 for L=3, 1.93 for L=4 (1973Fo01) 
$d|s/d|W(max)=1.20 mb/sr for 186 doublet 


level_energy_unit: KEV
level_comment:
E,L,S$from 1973Fo01. Level (at 807) is uncertain in 1975ShYV. L=2 is inconsistent with 1/2(-) in Adopted Levels 
$d|s/d|W(max)=0.05 mb/sr 


level_energy_unit: KEV
level_comment:
$ L=2, S=0.03 for 1025 {I7} group (1973Fo01), L+1/2 assumed L=2 is inconsistent with 5/2- in Adopted Levels 
$d|s/d|W(max)=0.05 mb/sr 


level_energy_unit: KEV
level_comment:
E,L,S$from 1973Fo01. Level (E=1169) uncertain in 1975ShYV 
L$ 1+3 for 1166+1207 group (1973Fo01). L=1 is in disagreement with 5/2+ in Adopted Levels 
$d|s/d|W(max)=0.15 mb/sr for 1166+1207 


level_energy_unit: KEV
level_comment:
$L=2, S=0.03 (5/2+ assumed) for 1354 {I10} level (1973Fo01). L=2 is inconsistent with L=0 in (d,p) 
$d|s/d|W(max)=0.05 mb/sr 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from the decay of 175|g in NaI detectors, except as noted. Value is weighted average of results listed as follows: 20.082 ms {I+71-70} (2014De19, in averaging uncertainty increased to 0.105 ms by evaluators to account for possible systematic uncertainties); 20.48 ms {I18} (1980Jo11,Ge(Li) with NaI anti-Compton); 21.5 ms {I4} (1974Bu14,neutron activation of Ge(Li) detector); 20.4 ms {I4} (1976Ga33); 21.5 ms {I10} (1971Go21); 22.2 ms {I10} (1971Mu14); 20.4 ms {I10} (1970Ru08,1969Ru10); 21.2 ms {I12} (1966Me02); 20.0 ms {I6} (1963Al32); 19.5 ms {I5} (1962Re09,conversion electron detection in anthracene detector); 20 ms {I1} (1962Mo19); 19.4 ms {I4} (1961Mo06); 20.3 ms {I3} (1961Sc11). Values of 21.87 ms {I7} (1972Br53), and 16 ms {I1} (1959Gl56) were not included in the averaging procedure, as these appear to be outliers. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$Capture rate to this isomer=0.020|*10{+6} s{+-1} {I3}, corresponding to a percentage is 0.32% {I5} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
T$from fit to summed rate of 1.29-keV and 10.37-keV transitions resulting from |e decay from the atomic L and K shells, respectively (2023Co07) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
T$from fit to decay of 9.2-keV and 10.2-keV transitions resulting from |e decay from the atomic K shells. (2024No04). One absolute measurement was performed and two relative measurements, to {+55}Fe and {+57}Co. Reported value is 11.4683 {I17} (stat) {I82} (syst). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$|d<r{+2}>{+72,71}=-0.223 {I9} (stat) {I43} (syst) (2024Wa45). Systematic uncertainties are from atomic mass-shift and field-shift factors. 
$R{-ch}=4.032 {I2} (stat) {I5} (syst) (2024Wa45) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$from delayed auto-coincidence of a Ge(Li) detector (1984Br24). Others: 0.40 |ms {i11} in {+72}Ga |b{+-} decay; 427 ns {i11} in (n,n'|g); 439 ns {i4} in (p,p'|g); and 404 ns {i45} in (|a,|a'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2) in Coul excitation. Others: 3.3 ps {i4} {+72}Ge(|g,|g'); 2.8 ps {I+21-7} {+70}Zn(|a,2n|g), DSA; 2.9 ps {i2} (e,e'). 
MOMM1$Weighted average of +0.734 {I88}, +0.798 {I66} from transient field IPAC (1987La20, 1984Pa20) and +0.74 {i18} from IMPAC, recalculation (1989Ra17). 
MOME2$Coul excitation reorientation (1980Le16,2005St24). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$from B(E3)=0.061 {i15} (average of (e,e') and Coul ex.) and adopted branching. Other: 0.7 ps {I+7-4} in (|a,2n|g). 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$from L(t,p) and L({+6}Li,d). However, J|p=3- to 6- from L(p,d)=1, and L({+3}He,d)=1+3 not consistent with 0. 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-
level_comment:
$Possible multiplet: L({+3}He,d)=1+3 at 4047 {i3} implies J|p=1+ to 3+; L(p,d)=1+3 at 4047 {i10} implies J|p=3- to 6- 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: US
level_comment:
T$unweighted average of delayed coincidence values: 0.50 |ms {i5} (1948Bo10) and 0.29 |ms {i6} (1949Mc29) 


level_energy_unit: KEV
level_comment:
$Angular distribution not fitted by single L, found sizable L=4 component. (2+) from (p,t) reaction 


level_energy_unit: KEV
level_comment:
|b{-2}=0.190 (harmonic vibrational model, 1989Ro12). |b{-2}R=1.078 (harmonic vibrational model) and -1.136 (asymmetric rotor model) (1988Ba70). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
Q=-0.13 {I6} (1980Le16), g=+0.40 {I3} (1984Pa20). 
G Others: 0.50 {I25}, IMPAC measurement (1969He11); 0.58 {I15}, data of 1969He11 reanalyzed, corrected for decay in flight (1974Hu01); 0.37 {I9}, from reanalysis of 1969He11 data, making use of the linear recoil velocity dependence of the transient field (1977Fa07). 
B(E2)(691-834)=0.132 {I24} (1972Ha37). There is discrepancy in values deduced by two methods. From |b{+-} decay: 0.0255 {I25} (1967Kr01). The 1972Ha37 value is consistent with that derived from branching ratio and B(E2) value of the 834 level. 
B(E2)(0-834)=0.208 {I3} (1980Le16). Others: 0.16 (1956Te26), 0.23 {I2} (1962St02), 0.18 {I2} (1972Sa27), and 0.21 {I3} (1962Er05). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)(0-1464)=0.00095 {I40} (1980Le24). Other: 0.0017 {I5} (1962Ga13). 
B(E2)(834-1464)=0.114 {I13} (1980Le24). 


level_energy_unit: KEV
level_comment:
$|s/|s(g.s.)=2,8 
L$from 1974Ba67 assuming J|p=2+ is known. Not well fitted by DWBA (1977Gu12) 
$|s(3|/)/|s(22|')=0.9 (2007Fr10) 


level_energy_unit: KEV
level_comment:
$|s/|s(g.s.)=0.5 
L$from 1974Ba67. Not well fitted by DWBA (1977Gu12) 
$|s(3|/)/|s(22|')=1.5 (2007Fr10) 


level_energy_unit: KEV
level_comment:
$|s/|s(g.s.)=0.5 
L$not fitted by DWBA (1977Gu12). Shape similar to known J|p=0+ 1481 level in {+74}Ge 
$|s(3|/)/|s(22|')=4 (2007Fr10) 


level_energy_unit: KEV
level_comment:
$1980Re04 observed a level at 3895 with angular distribution not fitted by DWBA, possibly an unresolved multiplet 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$partial half-life for 2|g decay in bare {+72}Ge ions (2024Fr05) 
E$measurement from one Schottky detector (2024Fr05). Other: 695.0 {I32} from measurement in the other Schottky detector. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius: <r{+2}>{+1/2}=4.0632 fm {I14} (2013An02) 
T$>1.8|*10{+23} y for charge non-conserving |b{+-} decay (to {+73}As) (2002Kl09); at 90% confidence limit 
J$spin from microwave spectroscopy (1949To09); parity from L(d,p)=L(p,d)=L({+3}He,|a)=4 from 0+ 
MOMM1$from 1974Sa25 using NMR method. Others: 0.87917 {I12} (1967Lu07), 1954Ak27, 1953Je16. 
MOME2$from 2008Py02 and 2016St14 evaluations: Measurements: -0.285 {I43} (1966Ch02, from hyperfine structure constants in atomic beam method, this value corrected to -0.173 {I26} by 1970Ol02 based on their hyperfine structure study for {+69},{+71},{+75}Ge, and through private communication with authors of 1966Ch02); -0.21 {I10} (1949To09, microwave spectroscopy, also Mays and Townes: Phys. Rev. 81, 940 (1951)). See 1999Ke17 for calculation of nuclear quadrupole moment from microwave data, and 1962Ko22 for theoretical calculation of electric field gradients for {+73}Ge. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: US
level_comment:
J$L(d,p)=2 from 0+; 13.3|g E2 to 9/2+ 
T$weighted average of 2.92 |ms {I2} from |g-(K x ray)(t) in {+73}As |e decay and 2.88 |ms {I7} from delayed-coincidence summing in {+73}Ge IT decay 
MOMM1,MOME2$from 1993Co17 using TDPAC. Other: |m=-0.0941 {I25} (1975Ha37); Q=-0.4 {I3} (1983Pf02, Mossbauer effect) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$L(pol d,p)=1 and analyzing power; 53.44|g M2 to 5/2+ 
T$from delayed |g-ray spectra in {+73}Ge IT decay (1974Bu14). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$68.75|g M1+E2 to 9/2+ and 430.4|g M1+E2 from 7/2+ gives 7/2+ or 9/2+; 9/2+ is ruled out by 799.2|g Q (|DJ=2) from the 868 level which has spin limited in (7/2,11/2) based on its 868.0|g D (|DJ=1) to 9/2+ ground state. This also further determines J=11/2 for 868 level. See also comments for 868 level. 
T$weighted average of 1.86 ns {I10} from Mossbauer |G in (|g,|g):Mossbauer and 1.62 ns {I14} from |g(t) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J$L(p,d)=L({+3}He,|a)=3 from 0+; 5/2 supported by shell model calculation (see 1976Fo07 in {+73}Ga |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$499.0|g M1+E2 (|DJ=1) to 9/2+ and 485.9|g M1+E2 to 5/2+ 
T$2.2 ps {I+38-13} from B(E2)|^=0.0091 {I5} and 499.0|g branching ratio=3.4% according to |eB(E2)|^ ratio with the assumption of |d(E2/M1)=+1.2 {I+5-7} for 499.0|g in 1972Sa27 in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$825.8|g E2 (|DJ=2) to 9/2+; 5/2 is ruled out by |g(|q) in Coulomb excitation 
T$from B(E2)|^=0.077 {I4} in Coulomb excitation for J=13/2 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
J$868.0|g D (|DJ=1) to 9/2+ determines J=7/2 or 11/2; 7/2 is ruled out by 799.2|g Q (|DJ=2) to 68.75 level which has spin limited in (7/2,9/2) based on other evidence; |p=+ from Coulomb excitation from 9/2+. This also further determines J=7/2 for 68.75 level. See also comments for 68.75 level 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)+
level_comment:
J$L(p,p')=2 from 9/2+ gives (5/2 to 13/2)+; 1062.8|g to 7/2+; 1085.5|g from 5/2+; yield in (n,n'|g) supports 7/2 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$weighted average of 1153 {I3} from (p,d) and 1150 {I5} from ({+3}He,|a) 
J$L(p,d)=3 and L({+3}He,|a)=(3) from 0+ 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$L(p,p')=2 from 9/2+; 975.9|g to 3/2- and 784.7|g to 1/2+; but 1/2 from yield in (n,n'|g) is inconsistent 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$log| {Ift}=5.9 {I1} from 3/2- parent; 3/2 from yield in (n,n'|g); primary 5395.9|g from 1/2+ neutron capture state in (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_comment:
J$783.8|g Q (|DJ=2) to 7/2(-) and band assignment. But J=(5/2,7/2) from yield in (n,n'|g) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$742.2|g D+Q (|DJ=1) to 11/2+; 9/2 from yield in (n,n'|g); it corresponds to the L(p,d)=4 component of the L(p,d)=3+4 doublet at 1611 {I7}, and the L=3 component then corresponds to the 1624 {I5} level in ({+3}He,|a) with L=(3) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$from ({+3}He,|a) 
J$L({+3}He,|a)=(3) from 0+; L(p,d)=3 component of the L(p,d)=3+4 doublet at 1611. See also comments for 1610 level 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 1623 {I10} in (pol d,p) and 1635 {I5} in (p,d) 
J$L(pol d,p)=L(p,d)=2 from 0+ and L+1/2 transfer from analyzing power 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$L(pol d,p)=2 from 0+ and L-1/2 transfer from analyzing power; 3/2 also supported by yield in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 15/2(-)
level_comment:
J$834.7|g Q (|DJ=2) to 11/2(-); band assignment; a 2364 {I10} in (p,p') with L(p,p')=3 from 9/2+ could be the same level 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: US
level_comment:
E$from measured E|g=66.59 {I6} for the observed sum-peak 13.06|g+53.53|g and E|g=53.53 {I6} in 1974Bu14. 
T$from delayed-coincidence summing in 1978Ta08 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$from measured E|g=66.59 {I6} for the observed sum-peak 13.06|g+53.53|g (1974Bu14). 
T$from |g(t) in 1974Bu14 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: US
level_comment:
T$weighted average of 2.94 |ms {I3} (2002Mo46), 2.86 |ms {I3} (1993Co17), 2.96 |ms {I9} (1970Ky01), 2.95 |ms {I5} (1970Do01), 2.98 |ms 5 (1971Ra10), 2.95 |ms {I5} (1971Ve04). All values are obtained from measurements of 53.4|g-(K x-ray)(t). Note: 2.96 |ms {I9} from 1970Ky01 is deduced by the evaluators from the average of several measurements with a 3% uncertainty included due to calibration of the delay as indicated by the authors; 1970Ky01 give a weighted average of 2.94 |ms {I3} without taking into account the 3% uncertainty. 
T$values from 1970Ky01: 2.98 s {I3} and 3.04 s {I7} (single channel) from ce(K+L)-(K x-ray)(t), 2.92 s {I3} from ce(L)-(K x-ray)(t), 3.02 s {I4} from (K x-ray)-(K x-ray)(t), 2.79 s {I4} and 3.18 s {I11} (single channel) from 53.4|g-(K x-ray)(t), with quoted uncertainties from fits not including a 3% uncertainty from calibration of the delay. weighted average taking into account the 3% uncertainty gives 2.96 s {I9} with a reduced |h=1.35 
MOMM1,MOME2$from |g-electron and electron-electron perturbed angular correlation (PAC) in 1993Co17. Other: -0.94 {I3} from |g|g PAC in 1975Ha37. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from Adopted Levels. Values from |e decay measurements: 0.57 s {I10} (1970Ky01); 0.54 s {I11}, 0.58 s {I5}, 0.66 s {I12} in Fig.7 of 2008Li25 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_uncertain: ?
level_comment:
E$this level is not reported in any of the measurements in this study. It is placed here by the evaluators based on the facts that there could a doublet around E=500 keV as explained in Adopted Levels and that an unassigned 432.7|g is observed by 1972We10 in coincidence with the 430.2|g that could be also placed from the 932 level and thus matches a level at a different energy other than that of the 499 level on the basis of energy sums. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$others: 67 {I5} (1972Ha74), 67 {I10} (1969He05) 
S$others: 0.32 (1969He05), 0.78 (1972Ha74), 0.72 (1976Yo04) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 356 {I5} from 1973Ka03 and 368 {I10} from 1969He05 could correspond to 352+361 resolved in 1972Ha74. 
S$other: 0.25 (1969He05), 0.59 (1972Ha74) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$other: 512 {I10} (1969He05), 497 {I5} (1972Ha74) 
L$other: 1 from 1969He05 is inconsistent 
S$others: 0.20 for L=1 (1969He05), 0.58 (1972Ha74), 0.72 (1976Yo04) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$others: 562 {I10} (1969He05), 551 {I5} (1972Ha74) 
L$other: 0+2 (1969He05) 
S$others: 0.20 for L=2 (1969He05), 0.054 (1972Ha74) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E$others: 666 {I10} (1969He05), 655 {I5} (1972Ha74) 
S$others: 0.65 (1969He05), 1.62 (1972Ha74), 1.05 (1976Yo04) 


level_energy_unit: KEV
level_comment:
E,J$899, 1/2-, (2J+1)S=0.38 from 1976Yo04 for an unresolved doublet; 899 {5}, (2J+1)S=0.24 from 1973Ka03 could also be a doublet corresponding to 888+904 resolved in 1972Ha74. Other: 904 {I10}, (2J+1)S=0.12 (1969He05) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 1051 {I10} (1969He05), 1036 {10} (1972Ha74) 
S$others: 0.07 (1969He05), 0.16 (1972Ha74), 0.16 (1976Yo04) 


level_energy_unit: KEV
level_comment:
E$others: 1617 {I10} (1969He05), 1595 {I10} (1972Ha74) 
L$other: 0+2 (1969He05) 
S$others: 0.24 for L=2 (1969He05), <0.01 (1972Ha74) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 1646 {I10} (1969He05), 1623 {I10} (1972Ha74) 
S$others: 0.58 (1969He05), 1.13 (1972Ha74), 1.32 (1976Yo04) 


level_energy_unit: KEV
level_comment:
E$others: 1756 {I10} (1969He05), 1733 {I10} (1972Ha74) 
L$other: 0+2 (1969He05) 
S$others: 0.97 for L=2 (1969He05), 0.037 (1972Ha74), 0.45 (1976Yo04) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$other: 1936 {I10} (1969He05), 1911 {I10} (1972Ha74) 
L$other: 1 from 1969He05 is inconsistent 
S$others: 0.48 (1972Ha74), 0.46 (1976Yo04), 0.16 for L=1 (1969He05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 1983 {I10} (1969He05), 1958 {I10} (1972Ha74) 
L$other: 1 from 1969He05 is inconsistent 
S$others: 0.25 (1972Ha74), 0.25 (1976Yo04), 0.10 for L=1 (1969He05) 


level_energy_unit: KEV
level_comment:
E$other: 2024 {I10} (1972Ha74), 2053 {I10} (1969He05) 
L,S$from 1972Ha74. Other: L=1 with (2J+1)=0.06 from 1969He05 is inconsistent 


level_energy_unit: KEV
level_comment:
E$others: 2093 {I10} (1969He05), 2088 {I10} (1972Ha74) 
L,S$from 1972Ha74. Others: (2J+1)S=0.41 (1969He05); L=(0), (2J+1)S=0.098 from 1973Ka03; L=0+2 is also possible (1969He05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 2251 {I10} (1969He05), 2225 {I10} (1972Ha74) 
S$others: 0.17 (1969He05), 0.49 (1972Ha74), 0.35 (1976Yo04) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$other: 2353 {I10} (1969He05), 2321 {I10} (1972Ha74) 
S$others: 0.10 (1969He05), 0.24 (1972Ha74), 0.24 (1976Yo04) 


level_energy_unit: KEV
level_comment:
E$other: 2495 {I10} (1969He05), 2463 {I10} (1972Ha74) 
L$other: 0+2 (1969He05) 
S$others: 0.49 for L=2 (1969He05), 0.065 (1972Ha74), 0.36 (1976Yo04) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 2614 {I10} (1969He05), 2583 {I10} (1972Ha74) 
S$others: 0.20 (1969He05), 0.32 (1972Ha74), 0.48 (1976Yo04) 


level_energy_unit: KEV
level_comment:
E$other: 2726 {I10} (1969He05) 
L$from 1969He05. Other: L=(2) from 1973Ka03 
S$other: 0.05 (1969He05). L=2 is inconsistent with J|p(2678)=1/2-,3/2- in adopted levels 


level_energy_unit: KEV
level_comment:
E$others: 2885 {I10} (1969He05), 2860 {I10} (1972Ha74) 
L$from 1969He05. Other: L=(2) from 1973Ka03 
S$other: 0.08 (1969He05) 


level_energy_unit: KEV
level_comment:
E$other: 2963 {I10} (1969He05), 2931 {I10} (1972Ha74) 
L$other: 0+2 (1969He05) 
S$other: 0.28 for L=2 (1969He05), 0.032 (1972Ha74) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
BE2$others: 0.076 {I14} (1974An21), 0.046 {I7} (1962Ri09), 0.084 (1956Te26) 
T$from |g(t) in 1961Ho05 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
BE2$other: 0.010 {I2} (1974An21) 
J$499|g(|q) allows J=7/2 or 9/2, 486|g(|q) rules out 9/2, |p=+ from Coulomb excitation from 9/2+ (1972Sa27) 
T$2.2 ps {I+38-13} from B(E2)|^=0.0091 {I5} and 499.0|g branching ratio=3.4% according to |eB(E2)|^ ratio with the assumption of |d(E2/M1)=+1.2 {I+5-7} for 499.0|g in 1972Sa27 
$|eB(E2)|^(from g.s.)=0.00031 {I9} (1972Sa27), where |e is the ratio of the observed |g-ray yield to the total de-excitation of the state. 
$|eB(E2)|^(from 13.18 level)=0.0013 {I1} (1972Sa27) 
$|eB(E2)|^(from 68.75 level)=0.0075 {I4} (1972Sa27) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
BE2$others: 0.081 {I13} (1974An21), 0.035 {I9} (1962Va20), 0.062 (1956Te26) 
J$(7/2,13/2) from 825.6|g(|q) with 7/2 is favored, |p=+ from Coulomb excitation from 9/2+ (1972Sa27) 
T$from B(E2)=0.077 {I4} in 1972Sa27 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (+)
level_uncertain: ?
level_comment:
E$from 1962Va20 only. Not adopted in Adopted Levels 
J$|p=+ from Coulomb excitation from 9/2+ (1974An21) 


level_energy_unit: KEV
level_comment:
E$other: possible doublet at 494 {I5} (1973Fo01) 
L,S$other: S=0.08 for L=1, J=1/2-; S=0.12 for L=2, J=5/2 (1973Fo01). 


level_energy_unit: KEV
level_comment:
E,L,S$other: 0.06 for E=557 {I15} with L=2, J=5/2 (1973Fo01), but it is possible that impurity was not subtracted out correctly ( see 1975ShYV) 


level_energy_unit: KEV
level_comment:
E$possible doublet (1975ShYV). Other: 1139 {I5} (1973Fo01) 
L$other: 3 (1973Fo01) 
S$for J=5/2 and 1/2. Other: 0.64 (1973Fo01) 


level_energy_unit: KEV
level_comment:
E,L,S$other: C{+2}S=0.07 for E=1653 {I15} with L=1 and J=3/2 (1973Fo01), but it may be an impurity; see 1975ShYV. 


level_energy_unit: KEV
level_comment:
E,L,S$other: C{+2}S=0.06 for E=1744 {I15} with L=2 and J=5/2 (1973Fo01); the discrepancy in L transfer could be accounted for by the poor statistics and not being resolved from the weak peak of 1756 level (see 1975ShYV) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
MOMM1,MOME2$from hyperfine spectroscopy (2020Ka58). Values are weighted average of the moments extracted from the measured hyperfine parameters and the calculated hyperfine fields of three transitions. (2020Ka58). 
J$from the Adopted Levels of {+73}Ge in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|d<r{+2}>{+72,73}=0.031 {I13} (stat) {I15} (syst) (2024Wa45). Systematic uncertainties are from atomic mass-shift and field-shift factors. 
$R{-ch}=4.063 {I3} (stat) {I2} (syst) (2024Wa45) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$ transient-field PAC (1984Pa20). Others: +0.70 {I4} (1987La20), +0.70 {I24} (1977Fa07). See also 2005St24 compilation 
MOME2$reorientation effect in Coul. ex. (2000To12). Other: -0.25 {I6} (1980Le16,1989Ra17). See also 2005St24 compilation 
$ |b{-2}=0.290, 0.298 from ({+16}O,{+16}O') (1979Fe03,1976Co04) 
$ |b{-2}(from (pol d,d'))=0.28 (1978Sz08), 0.197 {I10} (1985Se05) 
$ |b{-2}(from (p,p'))=0.29 (1982Ta16) 
$ |b{-2}(from (pol p,p'))=0.208 {I10} (1985Se05), 0.27 {I1} (1986MoZR) 
J L=2 in (t,p), (p,p'), (d,d'), (|a,|a') and (d,{+6}Li) 
$ T{-1/2} from B(E2) in Coul. ex. Others: 11.8 ps {I+11-10} (DSA method in (n,n'|g)) (1988DoZU), 13 ps {I2} from (|g,|g') (1956Me13). 2001Ra27 adopted 12.50 ps {I25} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$ transient-field PAC (1984Pa20). See also 2005St24 compilation 
|b{-2}=0.07 from (p,p') (1982Ta16) 
J L=2 in (t,p), (p,p'), (d,d'), (|a,|a'), (p,t) and (d,{+6}Li) 
$ T{-1/2} from DSA method in (n,n'|g). Other: 5.9 ps {I9} from B(E2)'s in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L=4 in (p,p'), (d,d') and (|a,|a') 
$ T{-1/2} from B(E2) in Coul. ex. 
$ |b{-4}=0.02 from (p,p') (1982Ta16), -0.015 {I15} from (pol p,p') (1986MoZR) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J |g|g(|q) in {+74}As |e decay and (|g,|g'). L=0 in (t,p), ({+6}Li,d) and (|a,|a') 
$ T{-1/2} from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (3,4)+
level_comment:
J |g to 2+ and strong primary |g from 4+, 5+. The L=3 group in (d,{+3}He) at 2168 {I10} probably corresponds to this level rather than to the 2165 level of J|p=(1-). L(p,p')=(1) for a doublet E=2165 {I5}, the second component is probably L=4 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J |g's to 0+ and 4+, L=2 in (t,p), (p,p') and (p,t). L=(4) for a 2210 group in (d,d') inconsistent with J|p=2+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$ |b{-3}=0.16 ((p,p'),1982Ta16), 0.15 {I1} ((pol p,p'),1986MoZR) 
$B(E3)(p,p')=0.020 {I7} (2002Ki06,evaluation) 
J L=3 in (t,p), (p,p'), (d,d') and (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$ L(p,t)=4; L(|a,|a')=(4). L(p,p')=(3) inconsistent with J|p=4+, but assignment perturbed by {+70}Ge impurity 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_lifetime_unit: PS
level_comment:
J |g's to 2+ and primaries from thermal capture and from two J|p=4+ neutron resonances gives J|p=3,4+. If L(p,p')=(2+3) for E=2690 {I5} corresponds to this level, then J|p=(3-). L(|a,|a')=(1) for E=2695 {I10} inconsistent with J|p=3,4+ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J |g to 4+ and no feeding from thermal capture and from any of the five neutron resonances studied. L(|a,|a')=(1) for E=2695 {I10} inconsistent with J|p=2+ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
E$it appears that 2833 and 2836 are two different levels the first populated in (n,n'|g) and the second in (n,|g) E=th, although, existence of a doublet near this energy does not seem definitive. The |g rays in both reactions proceed to the same final levels but are about 3 keV different in energy. Also the branching ratios are different in the two reactions. 
J$ L=2 in (t,p) and (p,t) for a probable doublet. L(p,p')=4 for a doublet E=2833 {I5}, the second component is probably L=2 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: PS
level_comment:
J L=1+3 in (d,{+3}He), L=(3,4) in (d,d'), |g to 4+ and primaries from thermal capture and from J|p=4+ neutron resonance. In (p,p'), either the L=(5) assignment for a 3081 group is incorrect or there is a different level near this energy 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J |g's to (2+), (4+) and primaries from thermal capture and from two J|p=4+ neutron resonances. If same as L=3 in (d,p) then J|p=(3-). If same as L=(4) in (d,d') then J|p=(4+) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J L=(6) in (|a,|a'), L=7,6 in (p,t) and L=6+8 or 6+7 in (|a,{+2}He). L(p,p')=(5) inconsistent with J|p 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$|g to 3-; L(p,t)=2; L(p,p')=(2) assuming the same levels are populated in (p,t), (p,p') and (n,|g) E=th 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
E$this level may be the same as 4235.33 seen in 
J$ primary |g's from thermal capture and from J|p=4+ neutron resonance 


level_energy_unit: KEV
level_spin_parity: 4+,5+
level_comment:
J L(d,p)=0. L(p,t)=5 is reported by 1972IsZV for E=5313; however, in the work of 1977Gu12, the 5148 peak is not fit by any single L value 


level_energy_unit: KEV
level_comment:
|b{-2}=0.29 (CCBA), 0.25 (DWBA) (1982Ta16) 
|b{-2}=0.29 (1970Pe09) (DWBA), 0.208 {I10} (CCBA) (1985Se05), 0.27 {I1} (1986MoZR) 


level_energy_unit: KEV
level_comment:
|b{-4}=0.02 (CCBA), 0.07 (DWBA) (1982Ta16), -0.015 {I15} (1986MoZR). 1993Mo05 report an unresolved doublet at 1464 keV. 


level_energy_unit: KEV
level_comment:
L=0 component present but fit to |s(|q) by CCBA is not good (1982Ta16). 1993Mo05 report an unresolved doublet at 1483 keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$ |b{-2}=0.290, 0.298 from ({+16}O,{+16}O') (1979Fe03,1976Co04) 
$ |b{-2}=0.300, 0.298 from ({+18}O,{+18}O') (1979Fe02,1976Co04) 
See also 1981Ra08 for analysis of data for this level 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ <Q{+2}>=0.28 {I4}; <cos3|d>=+0.32 {I12} (2000To12) 
g-factor=+0.350 {I22} (1987La20), +0.433 {I20} (1984Pa20), 0.44 {I22} (1969He11), 0.45 {I10} (1974Hu01), 0.37 {I6} (1977Fa07) 
MOMM1 1977Fa07 and 1974Hu01 reanalyzed data of 1969He11. Evaluators have adjusted values of 1969He11, 1974Hu01 and 1977Fa07 using T{-1/2}=12.41 ps 
MOME2$ others: -0.25 {I6} (1980Le16), -0.25 {I10} (1972Gr37). The values are for constructive interference. For destructive interference values are -0.05 {I6} (1980Le16) and -0.17 {I10} (1972Gr37). Models predict constructive interference (see 1980Le16) 
BE2$weighted average of 0.3045 {I30} (1980Le24,1980Le16) and 0.3036 {I22} (2000To12). Others: 0.32 {i3} (1962St02), 0.30 {i5} (1962Er05), 0.32 {I3} (1960Wi18), 0.25 {I4} (1956Te26), 0.29 {I2} (1972Sa27) 
T$From B(E2)=0.3040 {I22} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ <Q{+2}>=0.08 {I+10-6}; <cos3|d>=-0.15 {I15} (2000To12) 
$B(E2)(from g.s.)=0.0062 {I10} (weighted average of 0.0035 {I15} (2000To12), 0.0065 {i25} (1980Le24),0.0066 {i10} (1962Mc03) and 0.0082 {i16} (1962Ga13)) 
$B(E2) (from 596,2+)=0.058 {I17} (weighted average of 0.051 {I8} (2000To12) and 0.10 {I2} (1980Le24)) 
T$weighted average of 5.7 ps {I9} (from B(E2)=0.0062 {I10}) and 7.4 ps {I22} (from B(E2)(from 596,2+)=0.058 {I17}), using Branching and |d from 'adopted gammas' 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$ from 596,2+; weighted average of 0.144 {I9} (2000To12) and 0.121 {I11} (1980Le24) 
T$From B(E2)=0.135 {I9} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$from B(E2) of 2000To12 
$ <Q{+2}>=0.02 {I+6-2}; <cos3|d>=+0.44 {I24} (2000To12) 
$ B(E2)(from 596,2+)=0.0036 {I26} (2000To12), <0.008 (1980Le24) 


level_energy_unit: KEV
level_comment:
L 3(+1) or 2+4 
Correspondence to 2+, 3005 level (see 'adopted levels') suggests L=3+(1) 
S 0.014, 0.18 if L=(1)+3; 0.27 if L=3 


level_energy_unit: KEV
level_comment:
Not resolved from 1461 level. |s(|q) for 1481 does not agree with L=0 DWBA calculation. See 1982Be45 for cross section of this level 


level_energy_unit: KEV
level_comment:
L from 1980Re04. 1977Gu12 give L=4; however, the peak is contaminated by an impurity. Moreover, the fit to L=4 DWBA curve does not agree at low angles 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$(2J+1)|s(EXPT)/|s(DWBA)=0.03 
E 1460, 1480 levels are unresolved 
L (0+4) for the doublet at 1460, 1480 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
G$average of +0.40 {I3}, +0.33 {I3}, +0.32 {I2}, +0.36 {I2}, +0.37 {I2}, +0.33 {I2} for three targets and five beam energies 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
G$average of +0.42 {I41}, +0.14 {I28}, +0.65 {I22}, +0.79 {I21}, +0.48 {I34}, +0.42 {I34}, +0.64 {I36}, +0.19 {I36} and -0.18 {I36} for four targets and four beam energies 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
G$average of +0.54 {I41}, +0.59 {I25}, +0.62 {I25}, +0.35 {I28}, -0.18 {I34}, +0.07 {I48}, -0.36 {I50} and +0.63 {I36} for three targets and four beam energies 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$0- in Table 1 is likely a typo 
$|d<r{+2}>{+72,74}=0.174 {I6} (stat) {I41} (syst) (2024Wa45). Systematic uncertainties are from atomic mass-shift and field-shift factors. 
$R{-ch}=4.080 {I2} (stat) {I5} (syst) (2024Wa45) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
J$spin from 1970Ol02, 1969OlZY (atomic beam), parity from L(d,p)=1 
MOMM1$atomic beam (1970Ol02) 
T$from |g-spectroscopy followed over 10 half-lives (1968Re04), Others: 78 min {I4} (2011Ra08), 1973ArZI, 1973McZP, 1970Az01 (also 1969Az02), 82.2 min {I12} (1948Mc32), 89 min {I2} (1941Se03), 81 min {I3} (1939Sa02). Activities with half-life of 30 min (1935Am01) and 120 min (Sugden: Nature 135, 469 (1935)) do not seem to belong to {+75}Ge 
$ Earlier value of T{-1/2} from 1968Re04: 79 M 4 (Reynolds, ORNL-867, 24, 30 (1950)) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$L(p,d)=L(d,p)=4 and E3 |g to 1/2- 
T$from 1974Ch22. Others: 46.6 s {I5} (1976Bh04), 48.9 s {I2} (1969Im02), 45.8 s {I31} (1974Bu14), 48 s {I2} (1970Me20), 48 s (1963Ma44), 49 s 2 (1954Bu94), 48 s 2 (1952Sm51), 42 s 2 (A. Flammerfeld, Z. Naturforsch. 7a, 295 (1952)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L=1 in (d,p), (p,d) and (d,t) give 1/2-, 3/2-. Angular correlation measurements in (d,p|g) confirm 3/2- 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L=1 in (p,d), (d,t) and anisotropy of 574.8|g in p|g(|q) in (d,p|g). L({+3}He,|a)=(3), giving (5/2-,7/2-) is in disagreement if 576 group in this reaction is the same level as 574.69 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
J$|g to 3/2-, possible |b feeding from (3/2)-. L(t,p)=3 from 9/2+ and L(p,d)=1 for 2664.4 and/or 2665.0 level 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$a doublet is proposed in (p,d). However, no doublet is seen in (d,p|g) 
J$L(p,d)=1; |g to 7/2+. May be a doublet 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of E(t,p)=3213 {I5} and E(d,p)=3215 {I4} 
J$L(d,p)=2 give 3/2+, 5/2+ but L(t,p)=2 from 9/2+ rules out 3/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from 1974Ch22. Others: 46.6 s {I5} (1976Bh04), 48.9 s {I2} (1969Im02), 45.8 s {I31} (1974Bu14), 48 s {I2} (1970Me20) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$from |g(t) (1982Is07) 
J$T{-1/2}(674 level)<10 ns restricts mult(481|g to 5/2+) to dipole or Q giving J(192 level)=1/2+,3/2,5/2+. ce data of 52.5|g and RUL(M2)|<1 supporting M1+E2 restrict J|p to 5/2+, 7/2+, 9/2+, thus giving J|p(192 level)=5/2+ 


level_energy_unit: KEV
level_comment:
S$for L=1+4, S=0.010 (L=1), 0.37 (L=4). For L=1+3, S=0.007 (L=1), 0.25 (L=3). The authors do not give the specific J values used for the calculation of the above S values 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=2.858 keV {I8}. g|G{-n}=8.2 eV {I20}, |G{-|g}=0.16 eV {I4}, g|G{-n}|G{-|g}/|G=0.16 eV {I4} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=3.051 keV {I12}. g|G{-n}=1.0 eV {I6}, |G{-|g}=0.23 eV {I4}, g|G{-n}|G{-|g}/|G=0.19 eV {I4} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
L,S$from 1976Yo04. 1988BuZV find a doublet with L=2+4 and (2J+1)S=1.97; indicating that the 192,5/2+ level seen in (d,p|g) is also being populated 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
S$0.105 in 2007ScZX 
J$from Adopted Levels. 1976Yo04 report J=9/2+1/2 for the 200+253 doublet. 1983Is07, in (d,p|g) explain the discrepancy for J(253) as being due to the presence of the 192,5/2+ level in the peak observed by 1976Yo04. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$from Adopted Levels. 1976Yo04 report J=3/2, but contribution from 574 {I3}/2- level (not reported in (d,p)) could explain the discrepancy 


level_energy_unit: KEV
level_comment:
L,S$from 1972Ha74. 1988BuZV give L=0+3, (2J+1)S=0.023. 1973Ka03 give L=1 contradicting others (see Adopted Levels). 1976Yo04 report J=3/2, but a possible contribution from the 574 {I3}/2- level (unreported in (d,p)) might explain the discrepancy. 


level_energy_unit: KEV
level_comment:
E,L,S$from 1972Ha74. L=4 in table 7 of 1972Ha74 is a misprint. Figure 7 gives L=2 for the 1534-keV level 


level_energy_unit: KEV
level_comment:
S$0.103 in 2007ScZX 
L$1973Ka03 give L=0 for 2636 level which does not agree with the value in (p,d); perhaps a different level. 1972Ha74 also give L=0 for E=2660 


level_energy_unit: KEV
level_comment:
E$reported by 1988BuZV and 1973Ka03. But the level reported by 1973Ka03 may correspond to 3160 level of 1988BuZV. 1973Ka03 report L=0 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Capture rate to excited states (feeding g.s.)=0.054|*10{+6} s{+-1} {I2}, corresponding to a percentage is 0.86% {I3} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: S
level_comment:
$Capture rate to this isomer=0.047|*10{+6} s{+-1} {I18}, corresponding to a percentage is 0.75% {I21} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.0811 fm {I12} (2013An02 evaluation) 
$Spin 0 is consistent with microwave absorption measurement (1949To09) 
T$for 2|n|b|b decay, from GERDA collaboration (2015Ag06, see also 2015Ag10, 2015Ag01,2013Ag02). Others: 1.5|*10{+21} y {I1} (as recommended in evaluation by 2010Ba07 and 2011Ba28; see values and references therein for input data), 1.43|*10{+21} y {I53} in |b|b decay database at NNDC-BNL, 1.88|*10{+21} y {I8} in 2021Ko07; >7.5|*10{+23} y (2021Ar01); >2.022|*10{+21} y (2023Ag05) 
$T{-1/2} for 0|n|b|b decay mode: >8.3|*10{+25} y (2023Ar02); >5.62|*10{+22} y (2022Da13); >9.0|*10{+25} y (2020Da08); >1.8|*10{+26} (2020Ag05); >4.8|*10{+25} y (2019Al24); >1.9|*10{+25} y (2018Aa02); >8.0|*10{+25} y (2018Ag03,2017Ag04); >2.1|*10{+25} y (2013Ag11, GERDA) at 90% confidence level, authors give T{-1/2}>3.0|*10{+25} y by combining results from measurements by 2001Kl11 and 2002Aa01. 2012Zu07 compilation lists T{-1/2}>1.9|*10{+25} or 2.23|*10{+25} {I+44-31}, both at 90% confidence level. First value is also quoted in article by 2013Ac01. The source reference for the second value needs to be confirmed. 
$T{-1/2} for one Majoron emission 0|n|b|b decay mode, measured T{-1/2}>4.2|*10{+23} y (2015He19, GERDA collaboration) 
$See also 2011Ba28 for a review of experimental half-life measurements for different 2|b decay modes. Consult NSR database at www.nndc.bnl.gov for an extensive list of experimental and theoretical articles on 2|b decay of {+76}Ge 
$2013Ac01: arXiv preprint by A.H. Ackermann, 1212.4067v1, Dec 17, 2012 
$2009Ka06: deduced occupancy of valence neutron and proton orbitals from single-particle transfer reaction studies using {+76}Ge target 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2 from 0+ 
MOMM1$transient-field technique in Coulomb excitation (2019Mc05), measured g{+76}Ge/g{+74}Ge=0.88 {I5} for the first 2+ states. Other: +0.64 {I2} (transient-field technique in Coulomb excitation, 2013Gu23); +0.838 {I46} from |g(|q,H) in Coul. ex. (1984Pa20), +0.67 {I8} (|g(|q,H) in Coul. ex.,1987La20); +0.56 {I12} (IMPAC,1969He11,1974Hu01,1977Fa07). Weighted average (NRM method) of all the four values is 0.67 {I5} 
MOME2$reorientation effect in Coul. ex. (2001To13, previous value from authors was -0.19 {I2} in 2000To12). Other: -0.19 {I6} for constructive interference and -0.03 {I6} for destructive interference (1980Le16), 1972Gr37, 1969Si15. 2016St14 give -0.19 {I6} from 1980Le16 and 2000To12 
$|b{-2}(pol p,p')=0.25 {I1} (1993Mo05). See also other values in (p,p') 
$|b{-2}(pol d,d')=0.197 {I10} (1985Se05) 
$|b{-2}(|a,|a')=0.265 (1988Ba70), deduced from |b{-2}R=1.313 
$|b{-2}(({+16}O,{+16}O'),({+18}O,{+18}O'))=0.26 (Coulomb), 0.23 (nuclear) (1976Co04) 
$|b{-2}(Coul.ex.)=0.267 (1980Le24) 
T$from B(E2)|^=0.276 {I2}, weighted average of 0.277 {I2} (2023Ay02), 0.278 {I3} (1980Le16), 0.27 {I2} (1972Sa27), 0.260 {I5} (1969Si15), 0.263 {I+32-24} (1962St02), 0.29 {I3} (1960Wi18), 0.230 {I35} (1956Te26) from various Coulomb excitation measurements. Other Coulomb excitation measurements with beam energies above the Coulomb barrier: B(E2)|^=0.299 {I27} (2006Pe13), 0.292 {I35} (2005Di05), 0.280 {I42} (1962Er05). Lifetime measurements T{-1/2}=18.4 ps {I21} (2013Lo04,RDM), and 18.2 ps {I21} (1988DoZU,|g|g(t)) are in a good agreement. 
$2008StZT: measured attenuation parameters G{-2} and G{-4}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2 
T$from B(E2) in Coul. ex. and adopted |g branching ratios 
$|b{-2}(pol p,p')=0.058 (1993Mo05,1986MoZR). See (p,p') for other values 
$|b{-2}(|a,|a')=-0.057 (1988Ba70) 
$|b{-2}(coul.ex.)=0.047 (1980Le24) 
MOMM1$transient-field method in Coul. ex. (2013Gu23), measured value of +0.78 {I10} is re-evaluated to +0.64 {I10} in 2020StZV 
MOME2$reorientation effect in Coul. ex. (2001To13) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=4 
T$from B(E2) in Coul. ex. 
$|b{-4}(pol p,p')=0.064 {I11}, 0.024 {I6}, 0.020 {I20}, 0.001 (1993Mo05,1986MoZR), 0.02 ((p,p'),1983Ra32) 
MOMM1$transient-field method in Coul. ex. (2013Gu23), measured value of +1.0 {I7} is re-evaluated to +0.8 {I6} in 2020StZV 
MOME2$reorientation effect in Coul. ex. (2001To13) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=0 
T$from B(E2) in Coul. ex. Other: 1.25 ps {I+62-35} from DSAM in (n,n'|g) 
$Intruder spherical state based on very small value of expectation value of <Q{+2}>=0.01 {I2} deduced by 2001To13 in their Coul. ex. experiment 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|g|g(|q) ({+76}Ge,{+76}Ge'|g); E2 |g to 2+ 
T$from B(E2) in Coul. ex. Other: 1.5 ps {I+10-4} from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 4+; g.s. band member 
T$weighted average of 0.59 ps {I+19-12} from B(E2) in Coul. ex. and 0.26 ps {I+29-10} from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(|a,|a')=3 
T$other: values from B(E1)|_ in Coul. ex. are about 3 fs, which are discrepant 
$|b{-3}(pol p,p')=0.15 {I1} (1993Mo05,1986MoZR). See also other values in (p,p') 
$|b{-3}(|a,|a')=0.11 (1988Ba70) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(|a,|a')=L(p,p')=3 
$2921 level is treated as different from 2920 level since an intense g.s. transition from 2920 level is inconsistent with L(|a,|a')=3 for a 2921 group 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J$E2 |g to 3-, E1 |g to 4+. Also supported by L(t,p)=5 and L(|a,|a')=(5). But L(p,p')=3 suggests 3- 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$|g|g(|q) in (|g,|g'); L(t,p)=L(p,p')=2 with assumed S=1 
$T{-1/2} from DSAM in (n,n'|g) (2015Cr06). Other: 0.06 ps {I+7-4} (1990DoZU) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(|a,|a')=3. Also L(p,p')=0+3 for a doublet. L(t,p)=0,1 and 3,4 also indicates a doublet with J|p=0+ or 1- and 3- or 4+ 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$L(p,p')=0+3 for a doublet and L(t,p)=0,1 and 3,4 for a doublet. L=3 component is associated with the 3312 level 


level_energy_unit: KEV
level_spin_parity: (2+,3)
level_comment:
E,J$L(t,p)=1 or 0 (and L>1); |g from 4+. Probably a doublet with 1- or 0+ for one of the components 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$from (pol |g,|g') data at HIGS-TUNL facility (priv. comm. of Feb 20, 2016 from W. Tornow); also |gs to 0+, 2+ and 3- 
$T{-1/2} from DSAM in (n,n'|g) (2015Cr06) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.28 ps {I+15-8} (1984KoZN) and 0.160 ps {I14} (2017Mu03) 
$B(E3)=0.021 {I7} (2002Ki06 evaluation, from |b{-3} in (p,p')). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$Based on large B(M1) value of 0.24 for 2203.7|g and low B(E2)(W.u.) of 0.33 for the 2766.7|g, and shell-model calculations, this level is identified by 2017Mu03 as a mixed-symmetry state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|s(|q) and VAP data are in agreement with calculations when prolate symmetric rotational model is used 


level_energy_unit: KEV
level_comment:
$G{-2}(W.u.)=2.0 
$|b{-2}R=-0.284 (vibrational model) (1988Ba70). Deduced |b{-2}=-0.057 using R{-0}=1.17 


level_energy_unit: KEV
level_comment:
$G{-3}(W.u.)=11.7 
$|b{-3}R=0.538 (vibrational model) (1988Ba70). Deduced |b{-3}=0.11, using R{-0}=1.17 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 M.E. (0,0+ |) 563,2+)=+0.526 {I2} 
$E2 diagonal M.E. (563,2+ |) 563,2+)=-0.24 {I2} 
BE2$ weighted average of 0.278 {I3} (1980Le24,1980Le16), 0.272 {I+5-4} (2001To13), 0.277 {I2} (2019Ay04) 
BE2$others: 0.272 {I25} (2008AzZZ), 0.292 {I35} (2005Di05), 0.27 {I2} (1972Sa27), 0.260 {I5} (1969Si15), 0.263 {I+32-21} (1962St02), 0.28 {I4} (1962Er05), 0.29 {I3} (1960Wi18), 0.23 {I4} (1956Te26). Weighted average of all the available values gives B(E2)=0.273 {I3}. 2001Ra27 evaluation lists B(E2)=0.268 {I8} and corresponding half-life=18.6 ps {I6} 
$|b{-2}=0.267 (1980Le24) 
$Q=-0.19 {I6} or -0.03 {I6} (1980Le16), -0.14 {I4} (2001To13) 
MOME2$two values correspond to constructive and destructive interference, respectively, with the 1108, 2+ level. Others: Q=-0.15 {I10} or -0.05 {I10} (1972Gr37); -0.18 {I14} or +0.05 {I14} (1969Si15). 
$g factor from transient-field technique in Coulomb excitation, average of +0.39 {I3}, +0.32 {I3}, +0.32 {I1} and +0.31 {I1} for three targets and three beam energies (2013Gu23), 0.334 {I39} (1987La20), +0.419 {I23} (1984Pa20). Method in 1987La20 and 1984Pa20: |g(|q,H) using transient-field technique 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 M.E. (0,0+ |) 1108,2+)=+0.089 {I3} 
$E2 M.E. (563,2+ |) 1108,2+)=+0.535 {I+3-7} 
$M1 M.E. (563,2+ |) 1108,2+)=+0.175 {I+6-8} 
$E2 diagonal M.E. (1108,2+ |) 1108,2+)=+0.26 {I+2-5} 
T$from B(E2)(from 2+,563)=0.064 {I8} (2013Gu23), 0.0572 {I+7-14} (2019Ay04), 0.074 {I9} (1980Le24), 0.058 {I7} (2001To13), weighted average=0.0576 {I+12-14} giving T{-1/2}=10.2 ps {I9}; B(E2)(from 0+,g.s.)=0.0065 {I15} (2013Gu23), 0.0079 {I6} (2019Ay04), 0.0085 {I15} (1980Le24), 0.00475 {I+150-175} (2001To13), weighted average=0.00752 {I60} giving T{-1/2}=9.3 ps {I+13-11}. 
G$average of +0.43 {I33}, +0.29 {I10}, +0.50 {I32}, +0.36 {I10} and +0.44 {I7} for four targets and three beam energies (2013Gu23) 
$Q=+0.28 {I6} (2001To13) 
$|b{-2}=0.047 (1980Le24) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$E2 M.E. (563,2+ |) 1410,4+)=+0.795 {I5} 
$E2 M.E. (1108,2+ |) 1410,4+) =+0.09 {I2} 
$E2 diagonal M.E. (1410,4+ |) 1410,4+)=-0.26 {I+1-7} 
G$average of +0.11 {I56}, +0.26 {I18} and +0.12 {I86} for three targets and three beam energies (2013Gu23) 
$Q=-0.01 {I5} (2001To13) 
T$from B(E2)(from 2+,563): 0.1264 {I16} (2019Ay04), 0.131 {I24} (1980Le24), 0.101 {I11} (2001To13), weighted average=0.1259 {I26} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
$E2 M.E. (563,2+ |) 1539,3+)=+0.082 {I5} 
$M1 M.E. (563,2+ |) 1539,3+)=+0.027 {I3} 
$E2 M.E. (1108,2+ |) 1539,3+)=+0.52 {I+2-4} 
$M1 M.E. (1108,2+ |) 1539,3+)=+0.10 {I1} 
$E2 M.E. (1410,4+ |) 1539,3+)=-0.44 {I+8-5} 
$E2 diagonal M.E. (1539,3+ |) 1539,3+)=+0.13 {I+8-10} 
T$B(E2)(from 563, 2+)=0.00134 {I+17-15} (2019Ay04), B(E2)(from 1410, 4+)=0.022 {I+5-8} (2019Ay04) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$B(E2)(from 563,2+)=0.00128 {I+114-78} (2001To13), 0.00144 {I6} (2023Ay02), weighted average=0.0144 {I6} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$E2 M.E. (563,2+ |) 2020,4+)=-0.220 {I+5-3} 
$E2 M.E. (1108,2+ |) 2020,4+)=+0.472 {I6} 
$E2 M.E. (1410,4+ |) 2020,4+)=+0.61 {I1} 
$M1 M.E. (1410,4+ |) 2020,4+)=+0.447 {I9} 
$E2 M.E. (1539,3+ |) 2020,4+)=+0.64 {I+3-7} 
$M1 M.E. (1539,3+ |) 2020,4+)=+0.26 {I1} 
$E2 diagonal M.E. (2020,4+ |) 2020,4+)=-0.24 {I+8-4} 
T$B(E2)(from 1108,2+)=0.0446 {I+11-12} (2019Ay04), 0.0626 {I+47-43} (2001To13), unweighted average=0.536 {I90} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
$E2 M.E. (1410,4+ |) 2454,6+)=+1.11 {I+3-2} 
$E2 M.E. (2020,4+ |) 2454,6+)=+0.35 {I+5-3} 
$E2 diagonal M.E. (2454,6+ |) 2454,6+)=-0.23 {I+9-4} 
T$B(E2)(from 1410, 4+)=0.137 {I+7-5} (2019Ay04), 0.084 {I4} (2001To13), unweighted average=0.111 {I27} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+
level_comment:
$E2 M.E. (1410,4+ |) 2487,5+)=-0.08 {I+9-5} 
$E2 M.E. (1540,3+ |) 2487,5+)=+0.9 {I+4-6} 
$E2 M.E. (2021,4+ |) 2487,5+)=-0.9 {I+7-2} 
$M1 M.E. (2021,4+ |) 2487,5+)=-0.74 {I+18-6} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$E2 M.E. (0,0+ |) 2504,2+)=+0.061 {I3} 
$E2 M.E. (563,2+ |) 2504,2+)=-0.126 {I+6-4} 
$M1 M.E. (563,2+ |) 2504,2+)=+0.11 {I+6-28} 
$E2 M.E. (1108,2+ |) 2504,2+)=+0.38 {I+1-2} 
$M1 M.E. (1108,2+ |) 2504,2+)=+0.31 {I+4-3} 
$E2 M.E. (1539,3+ |) 2504,2+)=+0.25 {I+2-4} 
$M1 M.E. (1539,3+ |) 2504,2+)=+0.33 {I+2-3} 
$E2 M.E. (1911,0+ |) 2504,2+)=+0.32 {I2} 
$E2 diagonal M.E. (2504,2+ |) 2504,2+)=-0.24 {I+2-16} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$E3 M.E. (0,0+ |) 2692,3-)=+0.12 {I+2-4} 
$E1 M.E. (563,2+ |) 2692,3-)=+0.026 {I1} 
$E1 M.E. (1108,2+ |) 2692,3-)=+0.012 {I1} 
$E1 M.E. (1410,4+ |) 2692,3-)=+0.021 {I2} 
$E2 diagonal M.E. (2692,3- |) 2692,3-)=+0.1 {I+18-15} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$E2 M.E. (563,2+ |) 2733,4+)=-0.064 {I+6-7} 
$E2 M.E. (1108,2+ |) 2733,4+)=+0.60 {I+1-2} 
$E2 M.E. (1410,4+ |) 2733,4+)=+0.04 {I+2-3} 
$M1 M.E. (1410,4+ |) 2733,4+)=+0.9 {I+2-1} 
$E2 M.E. (1539,3+ |) 2733,4+)=+0.35 {I+4-7} 
$M1 M.E. (1539,3+ |) 2733,4+)=+0.69 {I+2-5} 
$E2 diagonal M.E. (2733,4+ |) 2733,4+)=+0.5 {I+1-2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$E2 M.E. (0,0+ |) 2767,2+)=+0.054 {I4} 
$E2 M.E. (563,2+ |) 2767,2+)=+0.022 {I+8-5} 
$M1 M.E. (563,2+ |) 2767,2+)=+0.2 {I+1-4} 
$E2 M.E. (1108,2+ |) 2767,2+)=-0.18 {I2} 
$M1 M.E. (1108,2+ |) 2767,2+)=+0.51 {I+10-5} 
$E2 diagonal M.E. (2767,2+ |) 2767,2+)=-0.12 {I+3-12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_comment:
$E2 M.E. (1410,4+ |) 3033,6+)=-0.186 {I+30-5} 
$E2 M.E. (2021,4+ |) 3033,6+)=+0.49 {I3} 
$E2 M.E. (2454,6+ |) 3033,6+)=+1.2 {I+2-1} 
$E2 M.E. (2487,5+ |) 3033,6+)=-0.74 {I+10-8} 
$E2 diagonal M.E. (3033,6+ |) 3033,6+)=+1.3 {I2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$E2 M.E. (0,0+ |) 3130,2+)=+0.023 {I6} 
$E2 M.E. (563,2+ |) 3130,2+)=-0.048 {I+2-7} 
$M1 M.E. (563,2+ |) 3130,2+)=+1.08 {I+16-6} 
$E2 M.E. (1108,2+ |) 3130,2+)=+0.036 {I+11-7} 
$E2 diagonal M.E. (3130,2+ |) 3130,2+)=-0.2 {I+3-2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4)+
level_comment:
$E2 M.E. (563,2+ |) 3163,4+)=+0.47 {I+7-2} 
$E2 M.E. (1108,2+ |) 3163,4+)=+0.25 {I+2-5} 
$E2 M.E. (1410,4+ |) 3163,4+)=+0.21 {I1} 
$M1 M.E. (1410,4+ |) 3163,4+)=+0.21 {I2} 
$E2 diagonal M.E. (3163,4+ |) 3163,4+)=+0.8 {I2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$this level corresponds to 4611 {I10} level in Adopted Levels, which 2016Do05 included in their analysis 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$this level corresponds to 4936.07 {I20} level in Adopted Levels, which 2016Do05 included in their analysis 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
S$other: 2.1 {I8} from 1995Ju01 
$|G{-0}{+2}/|G=0.0015 eV {I6}. 
$Note there are other transitions from this level in Adopted dataset. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$|G{-0}{+2}/|G=0.0466 eV {I23} at 4 MeV, 0.088 eV {I10} at 10 MeV. |G{-f}=0.068 eV {I3}. 
S$other: 46.0 {I23} from 1995Ju01 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
S$other: 58.6 {I33} from 1995Ju01 
$|G{-0}{+2}/|G=0.069 eV {I4} at 4 MeV, 0.090 eV {I8} at 10 MeV. |G{-f}=0.083 eV {I5}. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
S$other: 29.4 {I26} from 1995Ju01 
$|G{-0}{+2}/|G=0.036 eV {I3} at 4 MeV, 0.058 eV {I16} at 10 MeV. |G{-f}=0.069 eV {I6}. 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
S$other: 3.8 {I14} from 1995Ju01 
$|G{-0}{+2}/|G=0.0053 eV {I20} at 4 MeV, 0.032 eV {I4} at 10 MeV. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$observed feeding is ambiguous. 
S$other: 55 {I9} (1995Ju01) 
$|G{-0}{+2}/|G=0.101 eV {I16}. |G{-f}>0.101 eV. 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
E$level fed by inelastic transitions. 
S$other: 53 {I5} (1995Ju01) 
$|G{-0}{+2}/|G<0.111 eV. |G{-f}<0.111 eV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|b{-2}=0.260 {I18} (1986Ro08,1983Ra32,rotational and vibrational models). Others: |b{-2}=0.250 {I18} (1987Ja05,1983Ra32,DWBA); 0.250 {I19} (1992Ke07); 0.211 {I10} (1985Se05); 0.22 (1970Cu03); 0.26 (1970Pe09); 0.25 {I1} (1993Mo05, 1986MoZR) (vibrational and rotational models). Deformation lengths (|b{-2}R) are also given by 1987Ja05, 1993Mo05 (and 1986MoZR) 
$G{-2}(W.u.)=25.5 {I40} (1992Ke07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|b{-2}=0.075 (DWBA), 0.085 (coupled-channel,vibrational model). Other: |b{-2}=0.067 {I4}, 0.073 {I2} (1986MoZR,vibrational model); 0.032 (1970Cu03) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$|b{-4}=0.07 (DWBA), 0.020 (coupled-channel,vibrational and rotational models). Others: |b{-4}=0.064 {I11}, 0.024 {I6} (1986MoZR, vibrational model); 0.001 (1993Mo05,symmetric rotor model), 0.020 (1986MoZR); 0.0 (1970Cu03) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|b{-3}=0.140 {I10} (DWBA,1983Ra32,1987Ja05); 0.150 {I11} (coupled-channel, 1983Ra32,1986Ro08,1987Ja05,vibrational model). Others: |b{-2}=0.150 {I12} (1992Ke07); 0.14 (1970Cu03); 0.13 (1970Pe09); 0.15 {I1} (1993Mo05,1986MoZR,vibrational model) 
$G{-3}(W.u.)=9.4 {I14} (1992Ke07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|b{-2}(Coulomb)=0.256, |b{-2}(nuclear)=0.228 (from ({+16}O,{+16}O') reaction 1976Co04). Corresponding values from ({+18}O,{+18}O') reaction are 0.262 and 0.231, respectively. 1979Fe03 deduce |b{-2} values from a reanalysis of data from 1976Co04 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$RDDS method (2017Do13). Mean lifetime |t=3.2 ps {I1}, weighted average (by evaluators) of |t=3.5 ps {I2} for unshifted peak, 3.1 ps {I1} for shifted peak, and 3.2 ps {I1} by conventional method 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|s(exp)=43 mb {I12} 
T$from measured B(E2)|_(1109|g)=0.0017 {I5} and adopted branching of 0.41 {I4} for 1109|g from Adopted Levels, Gammas 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
J$octupole transition from 159.7, 1/2- level; log| {Ift}=8.64 (log| {If{+1u}t}=9.87) to 215.5, 3/2- level in {+77}As 
T$from time decay of ten different |g rays from the decay of {+77}Ge followed over |?10 half-lives (2007Li06). Others: 11.248 h {I2} (1995An38), 11.30 h {I1} (1968Re04, earlier reports: 11.30 h {I3} in 1965Em03, 12 h {I1} in ORNL-867, 24 (1950)), 11.3 h {I3} (1957Ly49), |?11 h (1950St02), |?12 h (1941Se03), |?8 h (1939Sa02). Values from 2007Li06, 1995An38 and 1968Re04 present a discrepant set of data, the weighted average giving a reduced |h{+2}=70. The value from 2007Li06 is adopted here as it represents a largest set of measurements (56 spectra, 10 |g rays, followed over 10 half-lives). Weighted average of all three values is 11.238 h {I11} with reduced |h{+2}=72, unweighted average=11.253 h {I26} 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$L(d,p)=1 and Ay(|q) in (pol d,p) 
T$weighted average of 52.9 s {I6} (1974Gr29), 56 s {I2} (1970Me20), 54.0 s {I6} (1970OsZZ), 55.5 s {I10} (1969Im02), 53.5 s {I5} (1968Ma12), 53.6 s {I9} (1957Ly49) and 52 s {I2} (1954Bu94). Others: 59 s {I2} (1965Va12) and 59 s {I2} (1947Ar01) are omitted since these seem discrepant. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$L(|a,{+3}He)=3 dominant with some mixture of L=2; |DJ=1, dipole |g to 7/2+. L=2 component is probably contributed by 505, 5/2+ level 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L(d,p)=2 and Ay(|q) in (pol d,p) 
$There is severe disagreement in gamma-ray branching ratios between the values given here from (n,|g) (2012Me04) and those from {+76}Ge({+13}C,{+12}C|g) (2009Ka22). For example I|g(893)/I|g(880)=1.75 in (n,|g) whereas it is 0.144 in ({+13}C,{+12}C|g). The evaluators adopt branching ratios from the latter work due to better statistics and |g|g coin data using the Gammasphere array. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2)
level_comment:
J$primary |g from 1/2+; gammas to 1/2+ and 5/2+. L(|a,{+3}He)=(3) is inconsistent, which either implies a different level in (|a,{+3}He) or incorrect L-transfer 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2)
level_uncertain: ?
level_comment:
E$ordering of the 2785.11-2782.91 cascade is not established. Reverse ordering gives a level at 3288 keV. Due to the poor energy fit of the 2785|g and 2783|g, level energy uncertainty is inflated by 1 keV 
J$ primary |g from 1/2+; |g to 5/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_uncertain: ?
level_comment:
E$581 level proposed by 1977Al17 not confirmed by 2009Ka22 in {+76}Ge({+13}C,{+12}C|g); 421|g placed as g.s. transition 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$There is severe disagreement in gamma-ray branching ratios between the values given here from (n,|g) (2012Me04) and those from {+76}Ge({+13}C,{+12}C|g) (2009Ka22). For example I|g(893)/I|g(880)=1.75 in (n,|g) whereas it is 0.144 in ({+13}C,{+12}C|g). The evaluators adopt branching ratios from the latter work due to better statistics and |g|g coin data using the Gammasphere array. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2)
level_uncertain: ?
level_comment:
E$ordering of the 2785.11-2782.91 cascade is not established. Reverse ordering gives a level at 3288 keV. Due to the poor energy fit of the 2785|g and 2783|g, level energy uncertainty is inflated by 1 keV 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=0.551 {I1} keV, g|G{-n}=0.35 eV {I8}, |G{-|g}=0.115 eV {I25}, g|G{-n}|G{-|g}/|G=0.087 eV {I25} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$level is Coulomb excited from 0+; L(t,p)=2 
T$weighted average of 15.9 ps {I28} from |b|g|g(t) in |b{+-} decay (1993Ch05) and 11.1 ps {I7} from B(E2)|^=0.222 {I14} (2005Pa23) 


level_energy_unit: KEV
level_comment:
J$L(t,p)=(4,5) suggests (4+,5-), another L(t,p)=(0,4) suggests (0+,4+). The 2330 peak in (t,p) may contain contribution from 2319 level as well 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: S
level_comment:
J$log| {Ift}=5.2 to 3/2- {+79}As g.s. Probable configuration=p{-1/2} 
T$from 1991Kr15. Others: 19.1 s {I3} (1974Gr29); 18.4 s {I10} (1982FoZZ,1981Ho24); 19.1 s (1975Al11); 18.5 s {I5} (1972MaWL); 18.5 s {I2} (1970OsZZ) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$systematics. 7/2+ and 1/2- isomers occur in several odd-mass nuclides in this region 
T$from 1982FoZZ, 1981Ho24. Others: 47 s {I2} (1974KrZG); 41.1 s {I43} (1972De43); 40 s {I4} (1970Va31); 40 s (1977Al17,1972MaWL); 42 s {I2} (1970Ka04) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1974Gr29. Others: 24.5 s {I10} (1982FoZZ), 29 s (1981Gi17), 26.8 s 16 (1981ZeZY), 28 s {I4} (1974KrZG), 24.5 s {I10} (1972De43), 24 s {I1} (1970OsZZ) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$level is Coulomb excited from 0+ g.s.; syst of even-even nuclides 
T$from B(E2)=0.139 {I27} (2005Pa23) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
T$|b|g|g(t) (2005MaZW). Other: >0.4 ns from {+198}Pt({+82}Se,X|g) (1999Ma21) 
$Possibly |ng{-9/2}{+-2} isomer 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
T$estimated by 1999Ma21 from |g-ray yields of N=48 isotones. Short lifetime precluded measurement from timing of (projectile-like fragment)(|g) coin 
$Possibly |ng{-9/2}{+-2} isomer 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ |s(exp)=59 mb {I19} 
T$ from measured B(E2)|_(917|g)=0.0023 {I7} and adopted branching ratio of 0.55 {I3} (from ENSDF database) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$According to discussion on page 4, 2021Se17 propose only one level and the 571.1|g from this level as a single line, not a doublet as proposed in 1981Ho24 and kept in a later study by 2013Ve03 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$<0+||E2||2+>=0.14 {I5}, sign not determined 
$<2{-1}+||E2||2{-2}+> < 0.8, sign not determined 
$<2{-1}+||M1||2{-2}+> < 0.5, sign not determined 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
J shell model systematics for N=49 nuclei 
T from 2022De07, determined in {+81}Ga |b{+-} decay (|g ray time distribution measurement) of purified g.s. selected with the double Penning trap JYFLTRAP for the post-trap decay spectroscopy measurements. 
Isomeric yield (high spin state over total yield) of 0.97 {I1} and 0.92 {I2} for 25-MeV proton-induced fission of {+nat}U and {+232}Th, respectively (2018Ra19). Other isomeric yield: 0.975 {I7} (2019Ra01). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$Level energy held fixed In least-squares adjustment 
%IT<1 (1981Ho24). 
T the latest measured value of T{-1/2}(g.s.)=6.4 s {I2} (2022De07) implies T{-1/2} |> 7.0 s (from 7.6 s {I6} (1981Ho24)) for the isomeric state. 7.6 s {I6} in 1981Ho24 (also in 1982FoZZ), authors were unable to distinguish between two similar (g.s. and isomeric) half-lives in their A=81 multispectrum analysis. Presumably other authors' data also refer to mixtures of the g.s. and isomeric state. Those data are 10.1 s {I8} (1972De43), 8.8 s {I11} (1974KrZG, 1973KrZN), 7.8 s {I2} (1981ZeZY), and 13.4 s (1975Al11). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
J log {Ift}=6.5 (log {If{+1u}t}=8.7) from (5/2-); |g to (9/2+); therefore, J|p=(5/2+,7/2,9/2+). 5/2+ is favored by systematics since B(E2)(W.u.)=0.038, comparable to that for the analogous 5/2+ to 9/2+ transition in {+83}Se. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T from Adopted Levels. In 1981Ho24, 7.6 s {I6} - same value as of the 1st excited state. See the footnote. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E 710 {I310} from difference in measured |b endpoint energies for various |g({+81}As)-gated |b({+81}Ge) spectra for {+81}Ge g.s. and isomeric state decays (1981Al20). 
|g-ray decay intensity <1 per 100 isomeric decays (1981Ho24). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$from S(n)=4827.7 {I29} ({+81}Ge) and x<3836 {I5} [from Q(|b{+-}) ({+81}Ga=8664 {I4})-S(n)({+81}Ge) (2021Wa16)]. 


level_energy_unit: KEV
level_spin_parity: 1/2+&5/2+
level_comment:
E,J$unresolved doublet associated with a 1/2+ state at 679 keV and a 5/2+ at 711 keV (2019Ah05). 
$Spectroscopic factor S: 0.27 {I11} for s{-1/2} and 0.39 {I17} for d{-5/2}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$Based on measured values by 2015Et01. The weighted average value of the 13 values measured by 2015Et01 is 4.04 s {I27}; however, an uncertainty of 0.27 s is considerably lower than the smallest measured T{-1/2} uncertainty and may be smaller than the systematic uncertainty, moreover, the T{-1/2} from the strongest gamma ray of 1092 keV is 5.0 s {I7}. As a result, evaluators adopt a value of 4.0 s {I7}. Others: 4.60 s {I35} (1972De43), 4.5 s {I4} (1981ZeZY) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced from measured B(E2)(up) in Coul. Ex. 
J$Coulomb excited from 0+ ground state. Syst.of even-even nuclides. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(n)({+82}Ge)=7195 {I3} (2017Wa10); x<5289 {I4} from Q(|b{+-})({+82}Ga decay)=12484 {I3} and S(n)({+82}Ga) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$Others: 0.115 {I20} (2005Pa23), |?0.1 (2005Iw03) 
T$deduced from measured B(E2)|^=0.128 {I22} (2010Ga14). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: S
level_comment:
J$L=2 in {+2}H({+82}Ge,p); systematics of N=51 isotones from {+89}Sr to {+95}Ru 
T$from |g(t) of 306-keV |g ray (1988Wi17). Others: 1.9 s {I4}, by periodic milking of the {+83}Se daughter activity (1972De43); |<1.6 s (1974KrZG). 
%B-N$0.02 (systematics, 2012Mc04) and 0.1 (QRPA theory, 2002Pf04). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
$S{-lj}=0.48 {I14} 
$C{+2}{-lj}=4.0 fm{+-1} {I10} 
J$3/2+,5/2+ from L=2; 5/2+ is supported by the systematics of ground states of even Z and N=51 isotones 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(n)({+83}Ge)=3633 {I3} (2012Wa38); x<8086 {I5} from Q(|b{+-})({+83}Ga decay)=11719 {I4} and S(n)({+83}Ge) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$S(n)({+83}Ge)=3633 {I3} (2017Wa10); x<8086 {I5} from Q(|b{+-})({+83}Ga decay)=11719 {I4} and S(n)({+83}Ge) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$%|b{+-}n from 2002Pf04, others: 10.8 {I6} (1993Ru01), 9.5 {I20} (1991Kr15), 9 {I3} (1991Om01) 
T$from 2002Pf04. Others: 0.947 s {I11} (1993Ru01), 0.984 s {I23} (1991Kr15), 0.98 s {I5} (1991Om01), 1.2 s {I3} (1972De43). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
E$ level treated as tentative (evaluators) since |g|g coin evidence for 1046-624 cascade is lacking. In reference 8 quoted by 2009LeZZ, one of the possible assignment of 1046|g is in {+83}Ge nuclide from {+84}Ga delayed neutron decay, although, this possibility is considered as less likely by 2009LeZZ 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$ measured by 2013Ma22 from |b-gated time distribution of |g rays in {+84}As. Weighted average of 936 ms {I22}, 962 ms {I27} and 858 ms {I72} for 100|g, 243|g and 347|g, respectively. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<8627 {I400}. Group of neutron-unbound levels between S(n)({+84}Ge)=5243 {I4} (2012Wa38) and Q(|b{+-})=13870 {I400} 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(n)({+84}Ge)=5243 {I4} (2017Wa10); x<8817 {I200} from Q(|b{+-})({+84}Ga decay)=14060 {I200} and S(n)({+84}Ge) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=13.8 {I+79-98} (2018De35). Unobserved feeding to this level was estimated by 2018De35 as 10% {I10}, based on relative intensities of the 805.4- and 624.3-keV |g rays. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$effective mean lifetime |t=10.3 {I+30-65} (2018De35). Since no feeding correction was applied, T{-1/2}<9.2 ps 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity is associated with the g.s. 
J$from shell-model predictions (2013Ko31). Others: 5/2+ (systematics, 2012Au07), 1/2+ (predicted, 1997Mo25) 
T$measured by 2013Ma22 from |b-gated time distribution of |g rays in {+85}As and {+84}As. Weighted average of 484 ms {I9}, 526 ms {I22}, 549 ms {I24} and 444 ms {I37} for the unresolved 100|g and 102|g, 116|g, 267|g and 395|g, respectively. 2013Ma22 quote weighted averaged value of 494 ms {I8}, but the evaluators obtain 503 ms {I18} using LWM method from the same set of data. Others: 0.535 s {I47} (1991Kr15) and 0.58 s {I5} (1991Om01) are consistent with value from 2013Ma22 but less precise 
$%|b{+-}n value is from neutron and |b intensity measurement (2013AgZY) at JYFL facility using BELEN neutron counter and Si detectors for |b. This value most likely includes |b{+-}2n contribution, although, it is predicted to be negligible in theoretical calculations (1997Mo25) Other: 14% {I3} (1991Kr15) agrees with the value from 2013AgZY 
$ 2013AgZY: contribution to ND-2013 and priv. comm. of April 12, 2013 from J.L. Tain, Valencia University 


level_energy_unit: KEV
level_spin_parity: (+)
level_comment:
%B-N$estimated from reduced |h{+2} plot of %|b{+-}n values for {+85}Ga versus %|b{+-}n values for {+85}Ge, as shown in Fig. 5 of 2018Mi03 
J$odd neutrons likely to be in d{-5/2} orbit (2018Mi03) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<10224 {I300} from Q(|b{+-})({+85}Ga)-S(n)({+85}Ge), where Q(|b{+-})=13270 {I300} from systematics, and S(n)=3046 keV {I5} (2017Wa10) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2013Ma22 from |b-gated time distribution of |g rays in {+86}As and {+85}As. Weighted average of 217 ms {I28}, 242 ms {I56} and 235 ms {I39} for 102.0|g, 111.7|g and the unresolved 116.3|g and 118.9|g, respectively. Theoretical T{-1/2}=195 ms (1997Mo25), 95, 184, 2168 ms (2002Pf04) 
%B-N$estimated from measurements in 2013Mi19. Theoretical %|b{+-}n=7 (1997Mo25), 6.6, 65.6 (2002Pf04). Systematic (KHF) %|b{+-}n=6.0 (2002Pf04) 
T$CALCULATIONS: 1981Al25, 2012Ch48 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_lifetime_info: ;ERR=AP
level_comment:
J from systematics of N=55 nuclides 
T from model calculations and |b decay strength function (1981Al25); other: >150 ns from particle transit time of 300 ns in FRS fragment separator (1995CzZZ, 1997Be12, and 1997Be70). 
%B-N$Calculations in 2005Bo19 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E,J$assuming that the observed events correspond to the ground state 
T$assuming that T{-1/2} has to be of the same order or larger than the time of flight through the separator, which for this experiment was |? 300 ns. T{-1/2} is expected to be much larger, some estimates of the half-life are 66 ms (systematics, 2002Pf04) and 162 ms (QRPA theory, 2003Mo09). 
%B-N$this level is expected to undergo beta delayed neutron emission, some estimates of %|b{+-}n include 17% (systematics, 2002Pf04) and 49% (QRPA theory, 2003Mo09). 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay is possible, followed by delayed neutron emission, thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=15.2 ms, %|b{+-}n=19, %|b{+-}2n=1 (2019Mo01) 
$Theoretical T{-1/2}=27.1 ms, %|b{+-}n=42.2, %|b{+-}2n=0.8 (2016Ma12) 
E$the observed fragments are assumed to belong to g.s. of {+89}Ge 
J$3/2+ proposed from systematics (2021Ko07), and from theoretical calculations (2019Mo01) 
T$half-life of decay of {+89}Ge has not been measured. T{-1/2}>300 ns from time-of-flight of fission fragments (1997Be70,1997Be12). General decreasing trend of half-lives with increasing neutron numbers in neutron-rich isotopes suggests T{-1/2}<60 ms from measured T{-1/2}=954 ms for {+84}Ge, 503 ms for {+85}Ge and 226 ms for {+86}Ge, 103 ms for {+87}Ge, and 61 ms for {+88}Ge. Values for {+84}Ge, {+85}Ge, and {+86}Ge are taken from ENSDF database (October 13, 2021 version), and for {+87}Ge and {+88}Ge from 2014XuZZ thesis, considered as preliminary values. T{-1/2}=60 ms from systematics (2021Ko07). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$measured |s=6 pb (2010Oh02), systematic uncertainty|?50%, based on 3 counts assigned to {+90}Ge. Probability of misidentification of {+90}Ge isotope 0.0043% (2010Oh02). 
T$ >635 ns from time-of-flight through spectrometer (2010Oh02). Actual half-life is expected to be much longer as suggested by the calculated value of 20.3 ms (2019Mo01) 
$calculated %|b{+-}n=42, %|b{+-}2n=1 (2019Mo01). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
J$3/2- from theory in 2019Mo01 and systematics in 2021Ko07. 
T$estimated by 2005St29 from a time-of-flight of 363 ns and an expectation of 340 {+63}As to be observed at the focal plane 
$No events could be assigned to {+63}As, implying that {+63}As is unbound towards proton emission (2005St29). 
$Calculated T{-1/2}(|b decay)=86 ms (2019Mo01) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
${+64}Se is most likely stable towards proton decay, as S(p) is only marginally negative, and a large number of events are assigned to this isotope in A/Q Fig. 1 of 2016Bl05. As only the |b{++} decay has been observed, %|e+%|b{++}=100 is assigned by inference. 
$T{-z}=-1 
E$the observed activity is assumed to correspond to the g.s. of {+64}As 
T$extracted from a fit to measured {+64}As decay curve in 2020Gi02 and 2017GoZT by taking into account the contribution from decay of the {+64}Ge daughter with T{-1/2}=63.7 s {I25}. Others: 72 ms {I6} measured by 2014Ro14 from (fragment)|b{++}-correlated decay curve. Value of 18 ms {I+43-7} measured by 2002Lo13 is in disagreement with those from 2014Ro14 and 2020Gi02 
J$2021Ko07 suggest 0+ from systematics 
$Production |s=0.3 pb {I2} (2007Bl09) in Ni({+70}Ge,X), E=71.6 MeV/nucleon 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|e+%|b{++}: No evidence of ground state proton decay was found by 1993Wi03,1989Ho19. Relativistic mean field model predict stable against p emission (2001Pa02) 
T$weighted average calculated by 2002Lo13 based on their measured value 126 ms {I16} (2002Lo13,2002Bl17), following the fragmentation of primary {+78}Kr beam at 73 MeV/A energy, and T{-1/2}=0.19 s {I+11-7} (1993Wi03,1993Wi18), using analysis of decay spectra. T{-1/2}|?0.9 s for |e+|b{++} branch from gross |b decay theory calculations of 1973Ta30. 


level_energy_unit: KEV
level_comment:
$IAS 
$Decays to {+64}Ge by p, E(p)=3.52 MeV {I2} (weighted average of 2011RoZZ and 1993Ba12). Other: 3.70 MeV {I8} (1995Hu24). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
E,J$calculations using D1S Gogny interactions and shell-model approach using the JUN45 interactions predict oblate-deformed shape 
T$ from Adopted Levels for {+65}As in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
E$the Coulomb energy difference of +76 keV 3 was deduced from the excitation energies of the 5/2{+-} states in {+65}As and {+65}Ge. 
T$from comparison between the observed lineshape of 187|g with Monte-Carlo simulations 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$ This level decays by protons since S(p)({+65}As)=-89 {I85} (2011AuZZ) 
J$ from 2011Ro47; T{-z}=-3/2 
E$a 3.51 MeV {I2} proton peak is observed which is not in coin with |g rays. This proton group depopulates IAS in {+65}As at 3420 keV {I87} 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Decay mode from {+65}As Adopted Levels in ENSDF database 
$T{-z}=-1/2 
T$measured by 2014Ro14 from |b{++} decay correlation time spectrum 


level_energy_unit: KEV
level_spin_parity: [0+]
level_lifetime_unit: MS
level_comment:
T weighted average of 95.77 ms {I28} (1988Bu12) and 95.78 ms {I39} (1978Al23). Others: 93 ms {I5} (1976JaZP), 100 ms {I+70-50} (1993Wi18,1993Wi03), 100 ms {I+60-40} (1993Wi18 using the method of analysis of 1984Sc13), 97 ms {I2} (2002Bl17,2002Lo13) 
J Expected from shell-model (2005Ha30). 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: US
level_comment:
J$J|p=(7,8,9,10+) (1998Gr12) 
T$from 2001Gr07. T{-1/2}=17.5 |ms {I15} (1998Gr12) has been superseded 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$obtained with centroid shift method (2012De05). Value from deduced from mean lifetime |t=1.1 ns {I3} listed in the paper. 
E$ believed to be the predicted oblate shape isomer. 


level_energy_unit: KEV
level_spin_parity: 4
level_comment:
J$ 4+ proposed in text of 2012De05, but no parity listed in authors' level-scheme figure 2 and in table I 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$ weighted average (by 2013Ru10) of 1.16 |ms {I4} from recoil corrected data, and 1.09 |ms {I10} from |b-tagged data (2013Ru10) 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$ weighted average (by 2013Ru10) of 8.10 |ms {I34} from recoil corrected data, and 7.70 |ms {I39} from |b-tagged data (2013Ru10) 


level_energy_unit: KEV
level_spin_parity: [0+]
level_lifetime_unit: MS
level_comment:
$Decay modes and J|p from {+66}As Adopted Levels in ENSDF database 
$T{-z}=0 
T$measured by 2014Ro14 from |b{++} decay correlation time spectrum 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
$B(E2) deduced by 2013Co23 from Coulomb excitation yields; listed here in e{+2}b{+2} units 
$B(E2)=0.1162 {I236}(stat) {I+0-90} (syst, due to <10% branching ratio for (9/2-) to (7/2-) transition) (2013Co23). Compilers have quadratically summed the two uncertainties 
T$deduced by compilers from B(E2)|^, assuming pure E2 for 720 transition. Dominant E2 is suggested by shell-model calculations 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
$B(E2) deduced by 2013Co23 from Coulomb excitation yields; listed here in e{+2}b{+2} units 
$B(E2)(from 0,5/2-)=0.0460 {I70} (stat) {I+50-0} (syst, due to <10% branching ratio for (9/2-) to (7/2-) transition) (2013Co23). Compilers have quadratically summed the two uncertainties 
T$deduced by compilers from B(E2)|^ 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: S
level_comment:
J$2,3,4 from log| {Ift}=5.9 to J=3; log| {Ift}'s to several 2+ states and 4+ states rule out 4 and 2,respectively. |p=+ from 313|g(lin pol) in {+54}Fe({+16}O,np|g). 
T$weighted av of 151.5 s {I9} (1977Pa13) and 151.8 s {I18} (1972Tu07). Other: 159 s {I4} (1971Pa32). 


level_energy_unit: KEV
level_spin_parity: 9(+)
level_lifetime_unit: NS
level_comment:
J$M2 854|g to 7(-). 944|g to 6(-) is inconsistent with J|p, see comment in Adopted Gammas 
T$Other: 37 ns (1986RaZU) 
MOMM1$from g=0.23 {I2} in TDPAD (1986RaZU,2011StZZ). 
$conf=|pg{-9/2}|ng{-9/2} from analysis of systematics in 1998So23. 


level_energy_unit: KEV
level_spin_parity: (6)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
T$from 1986RaZU 
G$from TDPAD (2011StZZ,1986RaZU) 
J$assigned >7 by 1996Pe04 based on excitation function. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
J$5/2 from atomic-beam magnetic resonance (1976He21); |p from log {Ift}=5.50 {I2} in {+69}As |e decay to {+69}Ge g.s. with J|p=5/2- 
T$ weighted average of 15.3 m 2 (1978TeZY) and 15.1 m 3 (1979Su02). Others: 14.9 m 9 (1970Bo19), 15.5 m 10 (1970Mu03), 13.0 m 15 (1971Do01), and 16 m 1 (1974Ro14) 
MOMM1$from NMR on oriented nuclei (2005Go44). Compiled by 2011StZZ. Other: 1.2 {I2} from atomic-beam magnetic resonance-thermal beam (1980Ho02). Compiled by 2011StZZ. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$band member; (M1) 98|g to 5/2- g.s 
T$from pulsed beam delayed coincidences in {+70}Ge(p,2n|g) (1978TeZY) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$1.3 ns {I1} (1976IvZW) 
J$Band member; E1 89.3 |g to 7/2-; M2 1305.6 |g to 5/2- 
MOMM1$from integral perturbed angular distribution. Other: +6 {I2} from recoil into gas or vacuum method (1981Ki07). Compiled by 2011StZZ 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T$From 1998Sk04. Others: 4 ps {I2} (1976IvZW) and 3.5 ps {I6} (1978He13). 1998Sk04 explain discrepancy with value of 1978He13 as due to side feeding 
J$Band member; E2 853.8 |g to 9/2+ 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
J$Tentative spin assignment (13/2+) in {+58}Ni({+14}N,2pn|g) (2009Ba30) based on the suggested presence of a 9/2+ rotational band built on the 2310 level. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 4.9 ps {I9}, 4.7 ps {I19}, and 7.6 ps {I28} from 1978He13, and 6.6 ps {I14} from 1976IvZW. Based on these same data, 1978He13 adopts T{-1/2}< 8 ps to account for possible branching from higher levels 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
J$Tentative assignment (13/2+) in {+58}Ni({+14}N,2pn|g) based on assumption of rotational band built on the 2311 level assigned as J|p=9/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2-
level_comment:
J$Tentative spin assignment (13/2+) by 2009Ba30 based on the suggested presence of a 9/2+ rotational band at 2310 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|> 9/2 from |g(|q). Unable to make |p assignment due to large error from |g linear polarization (2009Ba30). (15/2) from systematics of neighboring nuclides. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MIN
level_comment:
J$J=4 from atomic-beam resonance method (1976He24); |p from shell model agrees with |m. Possible configuration=((|pf{-5/2})(|nf{-5/2})) 
T$weighted average of 53.0 min {I6} (1968De16), 52.5 min {I3} (1968Bo40), and 52 min {I1} (1952Ve09) 
MOMM1,MOME2$from atomic beam resonance method. Values are from 2014StZZ, the original values of |m=+2.1054 {I2} and Q=0.094 from 1980Ho02 are uncorrected for diamagnetic shielding. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$from delayed coincidences in {+58}Ni({+14}N,2p|g) (1987Ba39, 1991Ba43). 
J$from 166.83|g M1 to 4+; 134.63|g M1(+E2) to 2+. 


level_energy_unit: KEV
level_spin_parity: (0)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$from 263.13|g M1 to 1+, excitation function and comparison with Hauser-Feshbach analysis in {+70}Ge(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
T$weighted average of 4.5 ns {I10} from {+70}Ge(p,n|g) (deduced from off-beam I|g in 1979Te06) and 4.0 ns {I4} from {+58}Ni({+14}N,2p|g) (delayed coincidences) (1987Ba39, 1991Ba43). 
J$J=4 from |g(|q) in (p,n|g); |p from 318.60|g E1+M2 to 3+ 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$from 81.19|g D+Q to 4-; Hauser-Feshbach analysis in {+70}Ge(p,n|g). 
T$from delayed |g|g coincidence in {+58}Ni({+14}N,2p|g). Other < 3 ns from {+70}Ge(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 7(-)
level_lifetime_unit: NS
level_comment:
MOMM1$from perturbed angular distribution from an implanted source (1991Ba43) 
J$from 321.1|g E2 to 5(-); based on excitation function and linear polarization measurements in {+58}Ni({+14}N,2p|g). 
T$from delayed coincidences in {+58}Ni({+14}N,2p|g) (1987Ba39, 1991Ba43). 


level_energy_unit: KEV
level_spin_parity: 8(+)
level_lifetime_unit: PS
level_comment:
J$from 788.3|g (E1+M2) to 7(-); J=8 from |g(|q) and excitation function in {+58}Ni({+14}N,2p|g). 
T$from line-shape analysis in {+9}Be({+78}Rb,{+70}As|g) Other: < 2 ns in {+58}Ni({+14}N,2p|g). 


level_energy_unit: KEV
level_spin_parity: 9(+)
level_lifetime_unit: PS
level_comment:
J$from 76.1|g D(+Q) to 8(+); J=9 from |g(|q) and excitation function in {+58}Ni({+14}N,2p|g) 
T$from line-shape analysis in {+9}Be({+78}Rb,{+70}As|g). Other: < 2 ns in {+58}Ni({+14}N,2p|g). 
$Configuration:((|pg{-9/2})(|ng{-9/2})) 


level_energy_unit: KEV
level_spin_parity: 11(+)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+55}Mn({+18}O,3n|g). Other: 0.76 ps {I21} from DSAM in {+58}Ni({+14}N,2p|g),{+56}Fe({+16}O,np|g). 
J$E2 981|g to 9(+); band assignment 


level_energy_unit: KEV
level_spin_parity: 13(+)
level_lifetime_unit: PS
level_comment:
T$other: <0.49 ps from effective lifetime from DSAM in {+58}Ni({+14}N,2p|g),{+56}Fe({+16}O,np|g) 
J$E2 1343|g to 11(+), band assignment 


level_energy_unit: KEV
level_spin_parity: 7(-)
level_lifetime_unit: NS
level_comment:
T$weighted average of 4.4 ns {I1} (1978Fi09) and 5.3 ns {I3} (1987Be39,1991Ba43) 
G$From perturbed |g(|q) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from DSAM in 1997Ga26. Upper limit from effective lifetime of 0.42 ps {I7}, not corrected for sidefeeding. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: H
level_comment:
MOMM1$nuclear magnetic resonance on oriented nuclei (1976He06, 1976He25). Other: 1.64 {I4} (atomic-beam magnetic resonance,1980Ho02). 
MOME2$from Q({+71}As)/Q({+72}As)=+0.25 {I1} (1988Wh03), nuclear orientation with |g ray measurements. 
J$L({+3}He,d)=3 from 0+; log {Ift}=5.9 to 175, 3/2- states in {+71}Ge. 
T$from timing of |g rays (1990Me01). Others: 61 h {I2} (1971Mu14), 64.8 h {I7} (1959Re24), 60 h 3 (1957Be46), 62 h 3 (1955Gr08), 65 h 5 (1954Th36), 59.5 h {I20} (1953St31,timing of conversion electrons), 60 h (1950Ho26). The weighted average of all the values is 65.28 h 12 with reduced |h{+2}=3.0. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: NS
level_comment:
J$E2 |g to 5/2-; L({+3}He,d)=1 for 143+147 doublet. Interacting fermion boson mode calculations (2004Br44) predict 3/2 and 1/2 doublet in close proximity to 5/2 g.s.. 
T$from |g|g(t) in (p,2n|g) (1980Te01). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: NS
level_comment:
J$|DJ=1, M1 |g to 5/2-; L({+3}He,d)=1 for 143+147 doublet. Interacting fermion boson mode calculations (2004Br44) predict 3/2 and 1/2 lying close to 5/2 g.s.. The qp-phonon model calculations of 2003Ho02 predict first excited state of 3/2- at 120 keV. 
T$from |g|g(t), centroid-shift method in {+60}Ni(160,apg) (1985An23). Other: <2 ns in (p,2n|g) (1980Te01). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
J$924.6|g |DJ=1 to 5/2-; excitation function in in-beam |g-ray study favors 7/2 
T$from DSAM in (|a,2n|g),({+12}C,pn|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
MOMM1$g factor=+1.14 {I2} (1971BeWR,time-dependent perturbed angular distribution method, TDPAD). Value of +5.15 {I9} in 1971BeWR re-evaluated to +5.13 {I9} in 2020StZV. 
J$L({+3}He,d)=1+4 for 1000+1007 doublet; |DJ=2, quadrupole |g to 5/2- from |g|g(|q)(DCO) in ({+19}F,|a2p|g). 
T$|g(t) in {+70}Ge(d,n|g) (1971BeWR). 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J$log {Ift}=5.2 from (5/2-) parent; 1098.8|g to (1/2)-. Other: (7/2-) proposed in (|a,2n|g) is inconsistent 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$proposed in (|a,2n|g) based on |g-decay pattern 
T$from RDM in (|a,2n|g),({+12}C,pn|g). 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=2, E2 |g to 5/2-. 
T$from DSAM in ({+19}F,|a2p|g). 
$|g to 1000.2 level was not seen in ({+19}F,|a2p|g), I|g<2%. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 9/2+; 13/2 from excitation function in (|a,2n|g); band assignment 
T$from (|a,2n|g). Other: 4.3 ps {I14} from ({+23}Na,|a2p|g) 
$ Q(transition)=1.90 {I+11-9} (1994Zi01). 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to 9/2+ 
T$from DSAM in (|a,2n|g),({+12}C,pn|g). Other: >1.4 ps from ({+19}F,|a2p|g) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=2, (E2) |g to 9/2-; band assignment 
T$from DSAM in ({+19}F,|a2p|g) and in ({+23}Na,|a2p|g). 
$ Q{-t}<0.98 or <2.0 from ({+19}F,|a2p|g) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 13/2+; band assignment 
T$weighted average of 0.53 ps {I+51-19} from ({+23}Na,|a2p|g), 0.48 ps {I15} from ({+19}F,|a2p|g), and 0.62 ps {I21} from (|a,2n|g) 
$ Q{-t}=2.2 {I+5-3}. 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$|DJ=1, (M1+E2) |g to 13/2+. 
T$from RDM in (|a,2n|g),({+12}C,pn|g). Other: >1.4 ps from DSAM in ({+19}F,|a2p|g). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: PS
level_comment:
$ Q{-t}=2.10 {I+22-16} from ({+19}F,|a2p|g) 
J$|DJ=2, E2 |g to (13/2-); |DJ=1 |g to (15/2-). 
T$from DSAM in (|a,2n|g),({+12}C,pn|g). Other: >1.4 ps from DSAM in ({+23}Na,|a2p|g). 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 17/2+; band assignment 
T$from DSAM in ({+23}Na,|a2p|g). Others: 0.29 ps {I13} from DSAM in ({+19}F,|a2p|g); |<0.7 ps from DSAM in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
$ Q{-t}=2.08 {I+36-23}. 
J$|DJ=2, E2 |g to (15/2-); band assignment 
T$from DSAM in ({+23}Na,|a2p|g). 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (17/2-); band assignment 
T$weighted average of 0.46 ps {I+22-12} from ({+23}Na,|a2p|g) and 0.59 ps {I16} from ({+19}F,|a2p|g) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J$|DJ=1, D |g to (17/2+); negative parity assumed by 1994Zi01 in ({+19}F,|a2p|g), based on likely (E1) for pure dipole transition 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J$|DJ=1, D |g to (17/2+); negative parity assumed by 1994Zi01 in ({+19}F,|a2p|g) in level-scheme Fig. 5 of 1994Zi01, based on likely (E1) for pure dipole transitions. Note that positive parity in Table I of 1994Zi01 seems a misprint 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 21/2+; band assignment 
T$from DSAM in ({+23}Na,|a2p|g). Other: 0.21 ps {I7} from ({+19}F,|a2p|g) 
$ Q{-t}=1.74 {I+39-23}. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|gs to (19/2-) and (21/2-); band assignment 
T$effective half-life from DSAM in ({+23}Na,|a2p|g). 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (21/2-); band assignment 
T$weighted average of 0.21 ps {I6} from ({+23}Na,|a2p|g) and 0.23 ps {I8} from ({+19}F,|a2p|g) 
$ Q{-t}=2.10 {I+34-23} from ({+23}Na,|a2p|g) 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=1 |g to (21/2-); (23/2-) proposed in ({+19}F,|a2p|g) 
T$from DSAM in (|a,2n|g),({+12}C,pn|g). 


level_energy_unit: KEV
level_spin_parity: (29/2-)
level_lifetime_unit: PS
level_comment:
$Q{-t}>1.93. 
J$|DJ=2, E2 |g to (25/2-); band assignment 
T$from DSAM in ({+23}Na,|a2p|g). Other: <0.13 ps from DSAM in (|a,2n|g),({+12}C,pn|g). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
E,J$1980Gu05 conclude that this level energy should be 1343.0 with a J|p=(9/2-) and that it decays by a 418|g instead of the 414|g seen by 1977He08. Neither the 418|g and 414|g are confirmed in later studies by 1994Zi01 and 1999Fo02. Tentative placement of 213|g is also unlikely as with present J|p assignments, it requires high multipolarity 
T$from timing of 418|g (1980Gu05) 


level_energy_unit: KEV
level_spin_parity: (17/2-,19/2-)
level_lifetime_unit: NS
level_comment:
T$a long-lived component with this T{-1/2} was seen by 1976He05 in the analysis of 714|g and 975|g and attributed to the feeding of 2690 level by a 300|g from 2990 level in 1977He08. This has been confirmed by the decay and intensity data on 300, 714 and 975 gammas by 1980Gu05. Other: 0.37 ns {I7} (effective half-life by RDM,1980Gu05) 


level_energy_unit: KEV
level_comment:
J$there are two levels at 143.49 {I7} with J|p=(1/2)- and 147.41 {I4} with J|p=3/2- in Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(max)=6.70 mb/sr for 146 doublet (1974Be54) 
$d|s/d|W(max)=3.28 mb/sr (1968Br11) for 145 {I15} doublet 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.58 mb/sr for L=1, 0.62 mb/sr for L=4 (1974Be54) 
$d|s/d|W(max)=0.50 mb/sr (1968Br11) for 992 {I15} 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$measured mean lifetime |t>2 ps at 145|' for 671.8, from spectra gated above the 671.8 transition 
$Q{-t}<1.96, <0.98 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.76 ps {I+76-28} at 35|' for 974.9|g, from spectra gated above the 974.9 transition 
$Q{-t}=2.1 {I6} 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$measured mean lifetime |t>2 ps at 35|' for 758.1|g; |t=1.40 ps {I+222-59} at 35|' and >2 ps at 145|' for 403.5|g, from spectra gated above the 758.1 and 403.5 transitions 
$Q{-t}<1.62 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=0.73 ps {I+37-20} (in 2011Ka10), as average of measured mean lifetimes |t=0.86 ps {I+117-35} at 35|' and 0.50 ps {I+37-20} at 145|' for 846.0 transition; and |t=0.92 ps {I+38-22} for 442.6 |g-ray at 35|' 
$Q{-t}=1.98 {I+34-37} 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$measured mean lifetime |t>2 ps at 35|'and 145|' for 820.6|g, from spectra gated above the 820.6 transition 
$ Q{-t}<1.96 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
T$averaged mean lifetime |t=0.40 ps {I19} (2011Ka10) of measured mean lifetimes |t=0.57 ps {I+18-13} at 35|' and 0.30 ps {I+11-10} at 145|' for 475.9 transition 
$Q{-t}=2.1 {I+8-4} 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.42 ps {I+16-12} at 35|' for 1100.1|g, from spectra gated above the 1100.1 transition 
$Q{-t}=2.0 {I+4-3} 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$averaged value of mean lifetime |t=0.76 ps {I28} (2011Ka10) from measured mean lifetimes |t=0.96 ps {I+22-15} at 35|' and 0.56 ps {I+22-15} at 145|' for 494.2 |g-ray 
$Q{-t}=1.61 {I+42-23} 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
T$measured mea lifetime |t=0.66 ps {I+32-17} at 145|' for 943.4|g, from spectra gated above the 943.4 transition 
$Q{-t}=2.36 {I+38-42} 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: PS
level_comment:
T$averaged mean lifetime |t=0.31 ps {I+4-3} (2011Ka10) from measured mean lifetimes |t=0.33 ps {I5} at 35|' and 0.30 ps {I+4-3} at 145|' for 1232.8|g 
$Q{-t}=1.72 {I+9-10} 


level_energy_unit: KEV
level_spin_parity: 25/2-
level_lifetime_unit: PS
level_comment:
T$averaged mean lifetime |t=0.31 ps {I8} (2011Ka10) from measured mean lifetimes |t=0.37 ps {I+10-8} at 35|' and 0.26 ps {I+7-6} at 145|' for 1137.5|g 
$Q{-t}=2.10 {I+34-23} 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
T$averaged mean lifetime |t=0.12 ps {I4} (2011Ka10) from measured mean lifetimes |t=0.14 ps {I+7-5} at 35|' and 0.10 ps {I4} at 145|' for 1338.4|g 
$Q{-t}=2.2 {I+5-3} 


level_energy_unit: KEV
level_spin_parity: 29/2-
level_lifetime_unit: PS
level_comment:
T$averaged mean lifetime |t=0.30 ps {I9} (2011Ka10) from measured mean lifetimes |t=0.32 ps {I+10-9} at 35|' and 0.29 ps {I9} at 145|' for 1301.4|g 
$Q{-t}=1.50 {I+29-18} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$from the Adopted Levels 
$Capture rate to excited states (feeding g.s.)=0.061|*10{+6} s{+-1} {I18}, corresponding to a percentage is 0.96% {I28} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: H
level_comment:
MOMM1,MOME2$atomic beam (1989Ra17, 2005St24); recalculated for consistency with the {+75}As standard. 
J$|b{++} first-forbidden unique shape: {+72}As |e decay to 0+, {+72}Ge g.s. 
T$from 1972Em01. Others: 26 h (1947Mi11,1948Mc31), 26.7 h (1950Ho26), 24 h (1965He08). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$from {+72}Ge(p,n|g):set 1; other: 78.4 ns ({+28}Si,3p|g) 
J$E1 |g to g.s. 2-, E2 |g to 1+, |g(|q). 
$|m: TDPAD (1975Be32) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
T$weighted average of 33 ns {I2} ({+72}Ge(p,n|g):set 1), 17 ns {I3} ({+70}Ge(|a,np|g), {+72}Ge(|a,3np|g)), and 20 ns {I6} ({+47}Ti({+28}Si,3p|g)). 
J$E1 |g to 3+, E2 |g to g.s. 2-, |g(|q). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
T$from {+72}Ge(p,n|g):set 1 
J$M1 |g from 3+, |s(E). This choice will have M|g=[M2] for the 318 |g, with a B(M2)(W.u.)=1.70 {I19}, which is marginally higher than the recommended upper limit of 1. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$weighted average of 87 ns {I2} ({+59}Co({+16}O,n2p|g)) and 90 ns {I3} ({+47}Ti({+28}Si,3p|g)) 
J$E2 |g to 5-. 
$|g: TDPAD (1977Ra03) 


level_energy_unit: KEV
level_spin_parity: 4-,5-
level_comment:
E$The gamma rays depopulating this level are taken from {+72}Ge(p,n|g):set 2 and {+69}Ga(|a,n|g). The 530 keV |g was also observed by {+72}Ge(p,n|g):set 1. 
J$M1 |g to 4-. 


level_energy_unit: KEV
level_spin_parity: (2,3)
level_comment:
E$The gamma rays depopulating this level are taken from {+72}Ge(p,n|g):set 2. The 401 keV and 427 |g's were also observed by {+72}Ge(p,n|g):set 1. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.76 ps {I14} (59Co({+19}F,|apn|g)) and 1.7 ps 4({+65}Cu(12Cf,ang)). 
J$E2 |g to 8+, band member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
$ Measured |m is in disagreement with that expected for |p1g{-9/2}~#|n1g{-9/2} configuration. More complex configuration seems involved. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$Capture rate to excited states (feeding g.s.)=0.15|*10{+6} s{+-1} {I3}, corresponding to a percentage is 2.4% {I5} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=3, M1(+E2) |g to 3/2-. 
T$|g(t) in {+73}Se |e decay (7.15 h). 
MOMM1$TDPAC (1963Bo26,1975Re06)). 
MOME2$TDPAC (1992Sc21) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$L({+3}He,d)=4, M2+E3 |g to 5/2- 
T$weighted average of 5.5 |ms {I3} from {+73}Se |e decay (7.15 h), 5.7 |ms {I2} from {+72}Ge(d,n|g) and {+74}Ge(p,2n|g) (both included in (p,n|g) dataset), 6.0 |ms {I12} from (|a,2n|g) 
MOMM1$stroboscopic perturbed angular distribution (PAD) (1970Be23). Other: +5.157 {I32} (1969Qu03,NMR) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$L({+3}He,d)=3; M1+E2 |g to 3/2-; |s(p,n|g) also favors 5/2 but 7/2- in ({+12}C,p2n|g) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$L(p,t)=2 from 3/2- target; L(d,{+3}He)=3 from 0+; 860.56|g E2 (|DJ=2) to 3/2-; |s(p,t) also supports 7/2 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: PS
level_comment:
J$609.22|g E2 (|DJ=2) to 9/2+; band assignment; |s(p,n|g) supports 13/2 
E$1037 level in (p,|g) with proposed J|p=7/2- may be a different level 
T$from {+58}Fe({+18}O,2np|g) by recoil distance (included in (|a,2n|g) dataset). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$doublet in ({+3}He,d) and probably also in (d,{+3}He) 
J$L({+3}He,d)=1+3 from 0+ for a 1073 group and L(d,{+3}He)=1 from 0+ for a 1081 group; |s(p,n|g) supports 3/2 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$L(d,{+3}He)=L({+3}He,d)=1; possible 356|g to 7/2- supports 3/2-, but 789|g to 9/2+ disfavors both 1/2- and 3/2- 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_comment:
E$different from 1293.3 level from probable J values and absence of 784|g in {+71}Ga(|a,2n|g). High |s(p,n) in {+73}Ge(p,n|g) confirms doublet 
J$865.18|g M1,E2 to 9/2+, 256.20|g to (13/2)+; |s(p,n|g) supports 11/2 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
J$900.87|g M1,E2 to 9/2+; |s(p,n|g) supports 7/2+; possible |e feeding from 9/2+. But L({+3}He,d)=1+2 for a 1326 suggests two levels, one with J|p=1/2-,3/2-; the other with J|p=3/2+,5/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J$L({+3}He,d)=1+3 for 1590 doublet; 1333.8|g to 1/2-. The L=1 component in ({+3}He,d) most likely corresponds to the 1592 level 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2-)
level_comment:
J$|gs to 5/2- and (1/2)-; possible |e feeding from 3/2-. The 1971 {I5} level in ({+3}He,d) with L=3 could correspond to 1972.98+1975.40+1977.54 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)
level_comment:
J$1547.45|g to 9/2+ and 700.0|g and 682.25|g to (7/2)+, 5887 |g from (1/2-,3/2,5/2-); possible |e feeding from 9/2+. The 1971 {I5} level in ({+3}He,d) with L=3 could correspond to 1972.98+1975.40+1977.54 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
E$two separate levels around this energy were proposed by 1977He08 in (|a,2n|g) from their placements of 1002.6|g and 1110.4|g from different levels with J{+|p}=(15/2+) assigned to a second level. However, there is no strong evidence to support the existence of two levels and a recent study by 2015Ra20 in ({+12}C,p2n|g) reported that a 1002|g and a 1110|g were from the same level. 
J$1110.4|g Q (|DJ=2) to (9/2-), 1002.6|g D (|DJ=0) to (13/2)+; band assignment in ({+12}C,p2n|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
E$other: a doublet at 8890 from ({+3}He,d) is claimed to be the possible analog of g.s. in {+73}Ge. See ({+3}He,d) for additional levels, which are |?80 keV lower than the corresponding IAS reported in {+72}Ge(p,p'), {+72}Ge(p,|g) and are not adopted here. 
J$L(p,p')=2; IAS of E=13, 5/2+ in {+73}Ge 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
G$from 1963Bo26 using Perturbed Angular Correlation (PAC) 
T$adopted from the same value in 1966Ol04 by delayed coin. Others: 1963Bo16, 1963Bo26. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_comment:
T$values from this dataset: 5.5 |ms {I3} from unweighted average of 6.0 |ms {I2} (1956Ha10), 5.0 |ms {I4} (1963Bo16) and 5.6 |ms {I3} (1969Ma21), all delayed |g|g coin 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$|s(p,p)(mb)=0.084 
E$IAS of 13 level in {+73}Ge 
$E(p)(lab)=3374 
L$any L=4 component corresponding to IAS of {+73}Ge(g.s.) is obscured by the L=2 component 


level_energy_unit: KEV
level_comment:
E$1307 {I10} (1976Sc13) 
S$0.08 for L=2 (1974Be54); 0.02, 0.04 for L=1+2, 0.03, 0.17 for L=1+3 (1976Sc13) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$level proposed by 1975Va03 from neutron tof spectrum. This level is also listed in 2004Si28 with J|p=5/2- 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from DSA of 1019.9|g (1999Bu05) 
T$mean lifetime |t=1022 fs {I132} (2004Si28) from 1002.4|g and 1019.0|g 
J$5/2 (2004Si28) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$from DSA of 1154.3|g (1999Bu05) 
T$mean lifetime |t=1050 fs {I132} (2004Si28) from 643.4|g and 1154.3|g 
J$7/2 (2004Si28) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$5/2,7/2 (2004Si28) 
T$from DSA of 901.0|g (1999Bu05) 
T$mean lifetime |t=312 fs {I+90-60} (2004Si28) from 818.8|g and 901.0|g 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
T$from DSA of 979.4|g (1999Bu05) 
T$mean lifetime |t=142 fs {I18} (2004Si28) from 451.8|g and 979.4|g 
J$5/2 (2004Si28) 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
$CROSS=29 {I7} 
J$3/2- (1979Sz06,1997Ra16) 
$Relative population=0.93 {I9} (1997Ra16), 0.96 {I4} (1979Sz06) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$CROSS=15 {I3} 
J$1/2- (1979Sz06). J|p=5/2- in figure 3 of 1997Ra16 seems a misprint 
$Relative population=0.47 {I7} (1997Ra16), 0.50 {I3} (1979Sz06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_uncertain: ?
level_comment:
$CROSS=6.9 {ILE} 
J$7/2- (1997Ra16) 
$Relative population |<0.22 (1997Ra16), 0.54 {I4} for doublet (1979Sz06) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
$CROSS=5.5 {I13} 
J$7/2- (1979Sz06,1997Ra16) 
$Relative population=0.18 {I7} (1997Ra16), 0.17 {I4} (1979Sz06) 
E$quoted as 894 in 1979Sz06 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$CROSS=6 {I4} 
Decay mode not consistent with that observed in {+73}Ge(p,n|g) 
$Relative population<0.5 (1997Ra16) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E$1178 (1997Ra16) is probably different from 1190 in 1979Sz06 
J$3/2- (1979Sz06) 
$Relative population=0.40 {I3} (1979Sz06) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
$CROSS=30 {I7} 
E,J$1221, 5/2- in 1997Ra16 
$Relative population=0.98 {I3} (1997Ra16), 0.98 {I4} (1979Sz06) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2)
level_comment:
$CROSS=19 {I4} 
J$3/2- (1997Ra16) 
$Relative population=0.61 {I25} (1997Ra16), 0.72 {I4} (1979Sz06) 


level_energy_unit: KEV
level_comment:
$CROSS=4.6 {I15} 
E,J$1556, 5/2+ (1997Ra16) 
$Relative population=0.15 {I8} (1997Ra16), 0.25 {I2} (1979Sz06) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
T$from 1972Em01 and 1962Ei02. Others: 1968Bo25, 1953Wa40, 1948Mc31 
J$log| {Ift} value to 0+ and shape factor of |b{+-}, |b{++} spectra which are characteristic of first-forbidden unique transitions (1971Bo01,1958Gr02,1951Jo06) 
MOMM1$nuclear magnetic resonance (1972Ka35,1976St25). See also 2005St24 compilation 
$Configuration=|pf{-5/2}|ng{-9/2} (1972Ka35) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
J$E1 |g to 2- 
E$198 in (p,d) corresponds to this level rather than 202 level, because L(p,d)=1 gives positive parity. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: NS
level_comment:
MOMM1$TDPAD (time-differential PAD method in (p,n|g)) (1971Ch10,1976Ga23). See also 2005St24 compilation 
J$M1 |g from (3)+ 
T$|g(t) in (p,n|g) (1971Ch10). Others: 25.7 ns {I20} (|gce(t) in (p,n|g), 1976La10); 27 ns {I2} (|g(t) in (|a,pn|g),1976Ga23) 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$M1 |g to 2- 
E$265 in (p,d) and 273 in (|a,d) correspond to any of the 267 or 271 levels, because L(p,d)=4+2 and L({+3}He,d)=1+3 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: NS
level_comment:
T adopted T{-1/2}=26.8 ns {I5} (1971Ch10) (see adopted level) 
g=+0.809 {I10} (1975Be58, differential PAD method) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
T from |g|g(t) (1971Ch10). Other: 25.7 ns {I20} (1976La10,|gce(t)) 
g-factor=+0.809 {I10} (1971Ch10, time differential PAD method) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$Capture rate to excited states (feeding g.s.)=1.1|*10{+6} s{+-1} {I2}, corresponding to a percentage is 17.5% {I32} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
%B-,%EC+%B+$from 'adopted levels, gammas' dataset for {+74}As in ENSDF database 
%B-,%EC+%B+$the measured normalized ratio of counts in the peaks 595.8|g and 634.8|g that follow |e+|b{++} and |b{+-} decay of {+74}As, respectively, as a function of temperature (in K) in germanium environment is: 100.04 % 16 (300 K 1), 100.10 % 9 (76.8 K 5), 99.96 % 9 (5.3 K 1), 99.98 % 30 (1.4 K 2) and 99.98 % 13 (0.31 K 2) 
%B-,%EC+%B+$the measured normalized ratio of counts in the peaks 595.8|g and 634.8|g that follow |e+|b{++} and |b{+-} decay of {+74}As, respectively, as a function of temperature (in K) in tantalum environment is: 99.86 % 9 (300 K 1), 99.82 % 12 (77.0 K 5), 100.07 % 11 (4.1 K 1), 99.95 % 20 (1.2 K 2) and 100.30 % 19 (0.26 K 1) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$ RMS charge radius <r{+2}>{+1/2}=4.0968 fm {I20} (2004An14 evaluation; and 2008 update available at http://cdfe.sinp.msu.ru) 
J$spin from NMR (1952Je05); others: 1954Fl41, 1948Da08, 1932To01. Parity from L({+3}He,d)=L(d,{+3}He)=1 
MOMM1$NMR (1953Ti01,1952Je05) 
MOMM1$ THEORETICAL PREDICTION FROM 75AS(3HE,D) REACTION: 1998Si28 
MOME2$from 1982Ef01 (high resolution, Ge semi detector). Others: +0.30 {I5} (1983Vo15; optical spectroscopy), 0.29 (1962Ko22) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$from L({+3}He,d)=L(d,{+3}He)=1 and |g|g(|q) of (136|g-66|g) in {+75}Se |e decay exclude 3/2- 
T$average of 870 ps {I30} (1969Ho25) and 900 ps {I30} (1967Se01); both delayed coin. Others: 1969Az02, 1970Az01, 1970Si21 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
MOMM1$IPAC (1971BeWK,1973Ch45) 
J$from L(d,{+3}He)=1 and |g|g(|q) of (136|g-265|g) in {+75}Se |e decay exclude 1/2- (non zero A{-2}) 
T$weighted average of 10.9 ps {I7} (1962Me04) and 11.2 ps {I3} (1967La07); see {+75}As(|g,|g') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from |g|g(t) (1989Mo14,1990Mo06). Others: 1973Ch45, 1972Gu03, 1971Ba71, 1970Az01, 1969Ho25, 1969Sh12, 1968Go41, 1967La07, 1967Se01, 1962Va02 
J$from L({+3}He,d)=L(d,{+3}He)=3; |g(|q) of 280|g in Coulomb excitation and M1+E2 |g to 3/2- 
MOMM1,MOME2$TDPAC method (1989Mo14,1990Mo22). Others: |m=+0.81 {I8} IPAC (1971BeWK), 1973Ch45, 1970Az01, 1966Ag01, 1960Ma03 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from 1998Hw05 (correlation counting method). Others: 16.2 ms {I3} (1994Sm09), 16.79 ms {I15} (1980Jo11), 16.9 ms {I6}, 18.2 ms {I10} (1984Br30), 17.53 ms {I8} (1972Br53), 16.5 ms {I3} (1969Ku08), 1969Fa13 (and 1969FaZY), 17.5 ms {I10} (1966Me02), 16.3 ms {I16} (1967Iv04), 15.4 ms {I6} (1966La25), 16.8 ms {I4} (1961Sc09), 15.6 ms {I4} (1961Mo06), 17.0 ms {I10} (1959Gl56), 17.0 ms {I10} (1958Du80), 17.0 ms {I7} (1957Sc11). 1998Hw05 obtain 16.5 ms by analyzing data in the same manner as 1994Sm09. Weighted average of all values is 16.9 ms {I2} 
J$L({+3}He,d)=L(d,{+3}He)=4; E3 |g to 3/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
E$uncertain in {+75}Ge |b{+-} decay(82.78) and {+75}As(|g,|g') 
J$from L({+3}He,d)=L(d,{+3}He)=2 and E2 |g to 9/2+. In 2012Sa41, the authors compare |s(|q) with Hauser-Feshbach calculations and find J=5/2- 
T$from {+75}Se |e decay (1967Se01). Others: 1969Ho25, 1970Az01, 1959Ve22 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=3; L+1/2 from a{-y}(|q) in (pol d,{+3}He). Also |g(|q) of 572 |g in Coul. ex. supports 5/2- 
T$from {+75}As(|g,|g'). Coul. ex. gives 2.4 ps {I6} 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$L(d,{+3}He)=1; L-1/2 from (pol d,{+3}He) 
E$from ({+3}He,d). Level uncertain in ({+3}He,d). 1997Ra16 reported E=585 in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$from L({+3}He,d)=3, (d,{+3}He) and |g(|q) of 822|g in Coul. ex. 
T$from 1981Ca10 by nuclear resonance fluorescence technique. Other: 2.46 ps {I19} from B(E2) and Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_lifetime_unit: PS
level_comment:
J$Coulomb excitation suggest 1/2-, 3/2-, 5/2-, 7/2-. |g to 1/2- rules out J|p=7/2-; |g from 7/2-rules out 1/2 
T$from 1981Ca10 (nuclear resonance fluorescence technique) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$from L(d,{+3}He)=1 and |g(|q) in (n,n'|g). From the comparison of |s(|q) with Hauser-Feshbach calculations, the authors of 2012Sa41 assign J=3/2-,5/2-. 
T$from 1981Ca10 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$L(d,{+3}He)=L({+3}He,d)=1+4 for a 1435 doublet. L+1/2 from (pol d,{+3}He). The L=1 component is most likely associated with 1430.5 level seen in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E$from ({+3}He,d) for a doublet and level uncertain in (p,|g) 
J$L({+3}He,d)=2+4 gives 3/2+,5/2+ and 7/2+,9/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from 1998Hw05 (correlation counting method). Others: 16.2 ms {I3} (1994Sm09), 16.9 ms {I6}, 18.2 ms {I10} (1984Br30), 16.79 ms {I15} (1980Jo11), 17.53 ms {I8} (1972Br53), 16.5 ms {I3} (1969Ku08), 1969Fa13 (and 1969FaZY), 16.3 ms {I16} (1967Iv04), 17.5 ms {I10} (1966Me02), 15.4 ms {I6} (1966La25), 16.8 ms {I4} (1961Sc09), 15.6 ms {I4} (1961Mo06), 17.0 ms {I10} (1959Gl56), 17.0 ms {I10} (1958Du80), 17.0 ms {I7} (1957Sc11). 1998Hw05 obtain 16.5 ms by analyzing data in the same manner as 1994Sm09. Weighted average of all values is 16.9 ms {I2} 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$E(level)'=0 
E$observed by 1978Kl05, 1977Dr01, 1967Co04 
E(p)(lab)=3568 {I3}, IAS of {+75}Ge(g.s.) 


level_energy_unit: KEV
level_comment:
E$1974Be54 report a level at 2252 {I10} with L=(3) and S=0.43. It seems to be the same level as 2210 {I10} of 1976Sc13 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$from 1962Me04 and 1967La07. 1962Me04 report |G(0)=4.03|*10{+-5} eV 11 and obtained T{-1/2}=10.9 ps {I7} using |G(0)/|G=0.96. 1967La07 report |G(0){+2}/|G=3.62|*10{+-5} eV {I20} and use |G(0)/|G=0.97 to get T{-1/2}=11.9 ps {I7}. Our adopted value is |G(0)/|G=0.968 {I1} giving T{-1/2}=11.2 ps {I3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
E$from 1967La07 
T$1967La07 report |G(0){+2}/|G=1.60|*10{+-6} eV {I12} and get T{-1/2}=279 ps {I21} using |G(0)/|G=0.99. From our adopted branching, we get |G=1.68|*10{+-6} and thus T{-1/2}=270 ps {I21} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2(+)
level_lifetime_unit: FS
level_comment:
T$from |G=0.36 eV {I10} and |G(0)=0.041 eV {I11} given by 1969Mo27 
J$from |g(|q) and transition strengths 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$from 1974Mc10 
T$from |g(t) (1972Br53). Others: 1976Ga33 (17.0 ms {I3}), 1966Me02 (17.5 ms {I10}) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
B(E2): weighted average of 0.0161 {I14} (1967Ro14), 0.0153 {I16} (1977An32) 
T$from 1969Sh12 (pulsed-beam technique) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
B(E2): weighted average of 0.045 {I4}, 0.054 {I7} (1977An32) 
J$|g(|q) of 280|g in 1967Ro14 determine uniquely J=5/2. 
T$from pulsed-beam |g(t) (1969Sh12). From measured B(E2), T{-1/2}=0.22 ns {I9} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
B(E2): weighted average of 0.073 {I7} (1967Ro14), 0.074 {I9} (1977An32) 
J$|g(|q) measurements of 1967Ro14 support J=5/2 
T$from B(E2) and |d(572|g)=0.39 {I5} (1967Ro14) and Adopted branching 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
B(E2): weighted average of 0.107 {I10} (1967Ro14), 0.102 {I14} (1977An32) 
T$from B(E2) (1967Ro14) and Adopted branching 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
BE2$0.0024 {I4} listed in 1976AnZJ, but is not given by the authors in their published work 1977An32. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$isotropic result in |g|g(|q) consistent with J=1/2 
T$average of 870 ps {I30} (1969Ho25) and 900 ps {I30} (1967Se01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from |g|g(t) (1989Mo14,1990Mo06). Others: 280 ps {I20} (1969Ho25), 1973Ch45, 1972Gu03, 1971Ba71, 1970Az01, 1969Sh12, 1968Go41, 1967Se01, 1962Va02, 1955Sc09 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from 1998Hw05. Others: 15.6 ms {I9} (1965La15), 17.0 ms {I7} (1957Sc11). See also numerous other experimental values in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$from 1967Se01. Others: 1970Az01, 1.67 ns {I14} (1969Ho25), 1.8 ns {I4} (1959Ve22), 1.5 ns {I4} (1958La10), <10 ns (1958Va02) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
$ The |g-ray branching ratios are used from Adopted Levels, Gammas dataset. The ratios in 2005Ra29 and 1977Pr08, where |g rays from this level are reported, are in severe disagreement with the ones obtained from Coulomb excitation, where this level is very strongly populated. Energies of 249, 542, and 558 gamma rays are also taken from Adopted Gammas, since the evaluators believe that gamma rays reported near these energies in 2005Ra29 and 1977Pr08 are contributed by impurities. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$ unresolved from 265 group, line-fitting procedure used to obtain separate cross sections. 
S$0.12 in 1983Ro08 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
E$ from 2008KaZT, assumed to be unresolved doublet corresponding to 2239.5 and 2228.6 levels in Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_comment:
$Capture rate to this isomer=0.41|*10{+6} s{+-1} {I7}, corresponding a percentage is 6.5% {I11} per muon capture (2019Zi01). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: H
level_comment:
$%|e|?0.027, preliminary measured value from 2014Do08. Others: no |e decay observed: %|e(K)<0.02 (1957Sc23). 1963Ba30, 1954Mu22, 1951Mi16, 1949Ma03, 1948Wu02, and 1947Ba08 searched for positron decays from {+76}As, but none detected and upper limits were suggested. From Q(|e)=921.5 keV (2021Wa16), positron emission is forbidden. 
MOMM1$measured |m=-0.9028 {I10} from nuclear magnetic resonance on oriented nuclei (NMR/ON) followed by |g and |b detection (1999Oh01), sign is from 1958Pi43 measurement. 2019StZV re-evaluated to 0.9023 {I10}. Measured value in 1999Oh01 is consistent with a configuration of 3/2- for protons and 7/2+ for neutrons (1999Oh01). Other configuration= |p1f{-5/2}{++1}~#|n(2p{-1/2},1g{-9/2}{++5}) (1980Ki01). Other: -0.906 {I5} (1958Pi43, nuclear orientation method) 
MOME2$ atomic beam magnetic resonance (1961Ch10). No values given in 2021StZZ and 2016St14 evaluations of quadrupole moments. 
J$spin from atomic-beam method (1961Ch10). Parity from L(d,p)=2 from 3/2- target; and L({+3}He,t)=1 from 0+ target 
T$weighted average of 26.261 h {I16} (2004Un01, ionization chamber), 26.251 h {I11} (2003Li62, from 559|g+564|g timing, weighted average of eight measurements using five Ge detectors). Others: 25.87 h {I5} (1994Mi03, this value seems discrepant by several standard deviations), 26.321 h {I1} (1989Ab22, quoted uncertainty is unrealistically low), 26.32 h {I7} (1972Em01, weighted average of seven different measurements), 26.4 h {I1} (1970Mc01), 26.30 h {I4} (1969Na11), 26.8 h {I1} (1957Wr37), 26.5 h {I2} (1955Dz48), 26.4 h {I2} (1953Hu47), 26.1 h {I3} (1948Ph08), 26.8 h {I2} (1942We01) and 26.3 h {I3} (1940Mi04). Weighted average of all the above measurements (with uncertainty of 0.020 for 1989Ab22) gives 26.263 h {I24} with reduced |h{+2}=9.4, whereas NRM weighted average is 26.266 h {I14} with reduced |h{+2}=2.7. Others: 1967Or04, 1966La22, 1935Am01 


level_energy_unit: KEV
level_spin_parity: (1)+
level_lifetime_unit: US
level_comment:
MOMM1$perturbed angular distribution (PAD) method using {+76}Ge(p,n|g) and {+75}As(d,p|g) reactions (1971BeWJ,1975Re06) 
$Configurations consistent with measured magnetic moment are: |p1f{-5/2}{+1}~#|n2p{-3/2}{+-1} and |p2p{-3/2}{+-1}~#|n2p{-3/2}{+-1} (1975Re06). Measured g factor in 1971BeWJ in agreement with 1+,2+,3+. 
J$L(d,p)=1+3 from 3/2- gives 1+,2+,3+; systematics of neighboring nuclides support 1+. Other: J=2 is proposed in 2015CoZV from (157|g)(426|g)(|q) data from 628,2+ |) 471,3+ |) 44,2+ sequence, in (p,n|g), but details of these data are not available. 
T$weighted average of 1.93 |ms {I6} (1968He15,|g|g(t) in (n,|g),E=thermal) and 1.80 |ms {I4} (1975Re06,|g(t) in (p,n|g)). Other: 2.1 |ms {I3} (1966Tu02,|g(t) in (p,n|g)) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$L(d,p)=1+3 from 3/2-; spin=1 from |s(|q) in ({+3}He,t). Reduced |g intensity in (n,|g),E=2 keV gives 1+, 2+; excitation function in (p,n|g) favors 1+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$E1 |g to 2- and M1+E2 |g to (1)+; spin=1 from |s(|q) in ({+3}He,t). Excitation function in (p,n|g) favors 1+ 
T$2.1 ns from 121|g(t) in (p,n|g) (1966Tu02). This T{-1/2} is for 120 and/or 122 level 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$M1 |g to 2- and L(d,p)=4 from 3/2-; |g(|q) and excitation function in (p,n|g) consistent with 3 or 4 


level_energy_unit: KEV
level_spin_parity: (0,1)+
level_comment:
J$|g to (1)+ is M1 (from (n,|g)) or M1+E2 (from (p,n|g)). Excitation function in (p,n|g) is consistent with 0+,1+. Reduced |g intensities in (n,|g),E=2, 24 keV agree better with 0+ 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
J$E2 (from ce data) |g to 2- and excitation function in (p,n|g). Reduced |g intensities in (n,|g),E=2, 24 keV are consistent with 4- 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
J$M1+E2 |g to (1)+. Reduced |g intensities in (n,|g),E=2, 24 keV give (1,2,3)+. But excitation function of 236|g in (p,n|g) suggests 3- 


level_energy_unit: KEV
level_spin_parity: (3,4)-
level_comment:
J$M1+E2 |g to (4)- and |g from 550 level (J|p=(1-,2-)) also L(d,p)=4 from 3/2- for a 285 {I5} group 


level_energy_unit: KEV
level_spin_parity: (2,3+)
level_comment:
J$dipole |g to (3)- and |g to (1)+; excitation function in (p,n|g) gives 3 or 4. Reduced |g intensities in (n,|g),E=2, 24 keV suggest 0+,3+ and only marginally agree with 2- 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$M1(+E2) |g to 1+ and |g to (3)-; L(d,p)=1+3 from 3/2-. But excitation function in (p,n|g) suggests 3+, 4+ 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$(M1) |g to 2-, |g to (1)+. L(d,p)=3+4 from 3/2- suggests a doublet with opposite parities; |s(|q) in ({+3}He,t) supports 2-; L=4 may (J|p=2- to 6-) may correspond to 364 or 366 level. Excitation function of 242|g and 364|g in (p,n|g) give 3,4. But 364|g in (p,n|g) may be doubly placed. 


level_energy_unit: KEV
level_spin_parity: (2- : 5-)
level_comment:
J$|gs to (3)- and (4)-. J=2,3 are less likely since no primary |gs (from 1-,2-, and (1,2,3+) capture states) are observed 


level_energy_unit: KEV
level_spin_parity: (1,2,3)-
level_comment:
J$|g to (3)-; L(d,p)=2 from 3/2-. Primary |g in (n,|g),E=thermal (from 1-,2- capture state) and reduced |g intensities in (n,|g),E=2, 24 keV disfavor J=4 


level_energy_unit: KEV
level_spin_parity: (2,3,4)-
level_comment:
J$L(d,p)=4 from 3/2-; |g rays to (2)-, (3)-, and (4)-. J=2,3 are less likely since no primary |g rays (from 1-,2-,0+,1+,2+,3+ capture states) are observed 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$(M1) |g to (1)+ and possible |g to 2-. Reduced |g intensities in (n,|g),E=2, 24 keV support 1+,2+ but L(d,p)=0+2 for a 500 {I5} group gives 1-,2-. Level at 0.5 MeV in (d,{+2}He) with proposed 1+,2- is probably a doublet. L({+3}He,t) supports (1+,2-) 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$(M1) |g to (1)+. Reduced |g intensities in (n,|g) E=2, 24 keV give 1+,2+. L(d,p)=1+3 from 3/2- for a 516 {I5} group gives 1+, 2+, 3+ which corresponds to 518 and/or 520 levels 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E$doublet in (d,p) with L=(1+4) from 3/2- 
J$|g rays to (1)+, (2)+ and 2-. Reduced |g intensities in (n,|g), E=2, 24 keV disfavor J=1,2 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$dipole |g to (2)-, |g to (1)-; 306.6|g from 1+. Reduced |g intensities in (n,|g) E=2, 24 keV support 1+, 2+ 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E$639 group in (d,p) is associated with 640 level only due to parity considerations 
J$L(d,p)=0+2 from 3/2- 


level_energy_unit: KEV
level_spin_parity: (1- : 4)
level_comment:
J$L(d,p)=(2) from 3/2- gives 1- to 4-; |g to (3)-. But reduced |g intensities in (n,|g),E=2, 24 keV suggest 0+,3+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$L(d,p)=1+3 from 3/2-; |s(|q) in ({+3}He,t). Reduced |g intensities in (n,|g),E=2, 24 keV give J=(1+,2+) 


level_energy_unit: KEV
level_spin_parity: (LE 3-)
level_comment:
J$0+ and 3- are less likely from |g rays to (2)- and (1)+. If this level corresponds to 928 {I5} group in L(d,p)=1+3 suggests 1+,2+,3+ but (E1) primary |g from 1-,2- gives negative parity 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$L(d,p)=1+3 from 3/2-. Reduced |g intensities in (n,|g),E=2,24 keV support 1+,2+; 1+ from |s(|q) shape for a 1030 group in (d,{+2}He) 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E,J$L(d,p)=0+2 from 3/2- for a 1478 {I10} group suggests 1-,2- for 1474 or 1478 level. Since 1474 level is proposed as 1+ from ({+3}He,t), evaluators assign L(d,p)=0+2 for 1478 level 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
J$L(d,p)=0 from 3/2- for a 1717 {I10} group suggests 1-,2- for 1714, or 1716 level. Since 1716 is assigned 1+ from ({+3}He,t), L(d,p) is associated with 1714 level 


level_energy_unit: KEV
level_spin_parity: (1,2,3+)
level_uncertain: S
level_comment:
E$ S(n)+2 keV neutron resonances, S(n)=7328.50 {I7} (2021Wa16) 
J$ s- or p-wave capture in 3/2- g.s. of {+75}As; |g to 2- 


level_energy_unit: KEV
level_spin_parity: (1,2,3+)
level_uncertain: S
level_comment:
E$S(n)+24 keV neutron resonances, S(n)=7328.50 {I7} (2021Wa16) 
J$ s- or p-wave capture in 3/2- g.s. of {+75}As; |g to 2- 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_uncertain: S
level_comment:
E$systematic uncertainty of 0.08 keV is added in quadrature to the uncertainty of 0.07 keV from least squares fit. This value can be compared with S(n)=7328.50 keV {I7} (2021Wa16) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_lifetime_unit: US
level_comment:
MOMM1$perturbed angular distribution (PAD) method in (p,n|g) reaction, measured g factor=+0.559 {I5} 
T$from 1975Re06 (|g(t) method). Other: 2.1 |ms {I3} (1966Tu02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$based on excitation function of 264|g, 1980Fe04 give J=3 or 4, but 264|g may not deexcite this level (see (n,|g),E=thermal) 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
$Level proposed by (n,|g),E=thermal by placement of 235.6|g from the 280.6 level rather than 235.6 level suggested by 1980Ki01 and 1988FeZU 
J$excitation function of 235|g (1980Ki01) suggests 3- 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2,3+)
level_uncertain: S
level_comment:
E$S(n)+E(n), where E(n)=2 keV and S(n)=7328.50 {I7} (2021Wa16) 
J$s- and/or p-wave capture in 3/2- g.s. of {+75}As 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2,3+)
level_uncertain: S
level_comment:
E$S(n)+E(n), where E(n)=24 keV, S(n)=7328.50 {I7} (2021Wa16) 
J$s- and/or p-wave capture in 3/2- g.s. of {+75}As 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
L$from DWBA fit to measured differential cross section (2017Fr02) 
$d|s/d|W(q{-max})=0.40 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=1.8 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$d|s/d|W(q{-max})=0.064 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=0.28 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (2-,1+)
level_comment:
$d|s/d|W=0.621 mb/sr {I10} 
$d|s/d|W(q{-max})=0.13 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=0.58 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$d|s/d|W=0.071 mb/sr {I2} 
$d|s/d|W(q{-max})=0.024 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=0.1 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$d|s/d|W=0.044 mb/sr {I1} 
$d|s/d|W(q{-max})=0.016 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=0.07 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$d|s/d|W=0.120 mb/sr {I3} 
$d|s/d|W(q{-max})=0.022 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=0.1 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$d|s/d|W=0.254 mb/sr {I5} 
$d|s/d|W(q{-max})=0.03 mb/sr (2017Fr02) 
$Relative spin-dipole M2 transition strength=0.13 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+,2-
level_comment:
$d|s/d|W (mb/sr)=0.087 {I11} 
E$unresolved structure composed of g.s. 2-, 44-keV, 1+ and 86-keV, 1+. The angular distribution suggests that most of the Gamow-Teller strength is in 44 and/or 86 states 
$B(>{++})=0.102 {I13}, M(>{++})=0.32 {I2} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J$L({+3}He,d)=(d,{+3}He)=1; log| {Ift}=7.2 to 5/2- state in {+77}Se 
T$weighted average of 38.83 h 5 (1968Re04), 38.5 {I5} (1959Kj49), 38.7 h 5 (1955Sc36), 38.68 h 9 (1953Bu57), 38.0 h 5 (1953Su04), 39 h 1 (1953Re12). Others: 38 h (1951Tu01), |?40 h (1950St02) 
MOMM1$NMR on oriented nuclei by detecting |b and |g rays (1999Oh01). 1999Oh01 point out that this value is smaller than Schmidt value of +3.79 for p{-3/2} orbital, the deviation may be explained by the core-polarization effects. Calculated value of +1.50 for |p[(2p{-3/2}){+3}(1g{-9/2}){+2}] and +1.92 for |p[(2p{-3/2}){+3}(1f{-5/2}){+2}] favors the former configuration. Measured |m=+1.2946 {I13} by 1999Oh01 is re-evaluated to |m=+1.2940 {I13} by 2019StZV 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=(d,{+3}He)=1; log| {If{+1u}t}=11.0 from 7/2+ rejects 1/2 
T$from |g|g(t) in {+77}Ge decay (1970Dr09) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L({+3}He,d)=(d,{+3}He)=1; log| {If{+1u}t}=10.0 from 7/2+ rejects 1/2 
T$from |g|g(t) in {+77}Ge decay (1970Tu03) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=(d,{+3}He)=3; |g|g(|q) in {+77}Ge decay (1974LeYO) is consistent with J=5/2, not 7/2 
T$from |g|g(t) in {+77}Ge decay (1989Mo14) 
MOMM1$|g|g(|q,H,t) method using 211-264 cascade (1989Mo14,1990Mo22). Others: +0.83 {I7} (1974LiYP,1973Ch42), 1972BeWU. 
MOME2$DPAC method (1990Mo23). Value not listed in 2014StZZ compilation 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$L({+3}He,d)=(d,{+3}He)=4; |g|g(|q) in {+77}Ge decay (1974LeYO) 
T$from 1980Jo11 (time digitized multiscaling). Others: 116 |ms {I4} (1968Io01,1957Sc11), >2 |ms (1997Is13) 
MOMM1$PAD method (1970BeYN). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=(d,{+3}He)=2; |g|g(|q) in {+77}Ge decay (1974LeYO) is consistent with J=5/2, not 3/2 
T$from |b|g(t) in {+77}Ge decay (1974ChXP). Other: 75 ps {I15} (1970Tu03) 
MOMM1$IPAC method (1974Ch31,1974LiYP). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L({+3}He,d)=3; |g|g(|q) in {+77}Ge decay; log| {Ift}=7.2 (log| {If{+1u}t}=8.0) from 7/2+; |g to 9/2+ 
T$from |b|g(t) in {+77}Ge |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$|g|g(|q) in {+77}Ge decay; log| {Ift}=7.9 (log| {If{+1u}t}=8.7) from 7/2+; gammas to 5/2+ and (11/2+) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2-)
level_comment:
J$|g|g(|q) in {+77}Ge decay; gammas to 3/2- and 7/2-; log| {Ift}=7.9 (log| {If{+1u}t}=8.2) from 7/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L({+3}He,d)=2; |g|g(|q) in {+77}Ge decay; |g to 9/2+; log| {Ift}=7.8 (log| {If{+1u}t}=8.4) from 7/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g|g(|q) in {+77}Ge decay; gammas to 9/2+ and 3/2-. Parity from 1085|g to 9/2+ not M2 from RUL 
T$from |b|g(t) in {+77}Ge |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2-)
level_comment:
E$level is weakly populated in (d,{+3}He) 
J$log| {Ift}=7.7 (log| {If{+1u}t}=8.3) from 7/2+; gammas to 3/2- and 7/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$L(d,{+3}He)=1. L=1+3 in ({+3}He,d) indicates a doublet with J|p=1/2-,3/2- and 5/2-,7/2-, respectively 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
J$L({+3}He,d)=4(+0); log| {Ift}=6.8 (log| {If{+1u}t}=7.2) from 7/2+; gammas to 5/2+, 9/2+ and (11/2+). 
E$this level may be a doublet with J|p=(1/2+) from L({+3}He,d)=(0) for the second component 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L(d,{+3}He)=2; |g|g(|q) in {+77}Ge decay; log| {Ift}=6.3 (log| {If{+1u}t}=6.6) from 7/2+; gammas to 1/2+ and 7/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L(d,{+3}He)=2; log| {Ift}=6.6 (log| {If{+1u}t}=6.8) from 7/2+; gammas to 5/2-, 5/2+, 7/2- and (7/2+). 
E$L({+3}He,d)=0+2 suggests a doublet with J|p=1/2+ for one level and 3/2+,5/2+ for the other. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$L(d,{+3}He)=L({+3}He,d)=1; Ay(|q) in (pol d,{+3}He). An uncertain 1411|g to 7/2- implying mult=M3 is unlikely; the placement may be incorrect 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$|g|g(|q) in {+77}Ge decay; log| {Ift}=5.8 (log| {If{+1u}t}=5.7) from 7/2+; gammas to 3/2- and 7/2- 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$|g|g(|q) in {+77}Ge decay; log| {Ift}=6.1 (log| {If{+1u}t}=5.9) from 7/2+; gammas to 3/2-, 9/2+ and (9/2-) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$L({+3}He,d)=4; log| {Ift}=5.84 (log| {If{+1u}t}=5.3) from 7/2+; gammas to 5/2-, 5/2+, 9/2+ and (9/2-) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$ L(d,{+3}He)=1 
E$this level agrees in energy with 2543.88 level populated in |b decay, but probably is a different level due to different J|p assignments 


level_energy_unit: KEV
level_comment:
J$L({+3}He,d)=0+3,4 suggests either a doublet with J|p=1/2+ and 5/2-,7/2- or a single level with J|p=7/2+,9/2+, respectively 


level_energy_unit: KEV
level_comment:
S$0.93 (2008KaZT) combined for 192.6+214.9 unresolved group with L=1 for the doublet; 0.74 for the doublet (1974Be54) 


level_energy_unit: KEV
level_comment:
E$1974Be54 report 1201 {I7} with L=0, (2J+1)C{+2}S=0.04; d|s/d|W(max)=0.18 mb/sr. A level at 1204 with L=0 is also reported in (d,{+3}He). It is possible that the 1194 level is a doublet with two components, one with L=3 and the other with L=0 


level_energy_unit: KEV
level_comment:
E$1974Be54 report 1674 {I7} with L=1 and (2J+1)C{+2}S=0.08; d|s/d|W(max)=0.17 mb/sr. 
S$angle-to-angle ratios of cross sections were used in 2008KaZT to assign separate cross sections to the two components of the doublet. Other: 0.09 for L=1, 0.16 for L=4 (1976Sc13). 


level_energy_unit: KEV
level_comment:
E$partly contributed by {+75}As. 1974Be54 report 1998 {I7} with L=4, (2J+1)C{+2}S=1.17; d|s/d|W(max)=0.16 mb/sr. 
S$0.87 (2008KaZT) for a 1971 group analyzed as L=4 transition 


level_energy_unit: KEV
level_comment:
L$from 2008KaZT and 1974Be54 
S$0.05 (1974Be54), level not in 1976Sc13 
$ d|s/d|W(max)=0.11 mb/sr (1974Be54) 


level_energy_unit: KEV
level_comment:
S$0.05 for L=1, 0.14 for L=4 (1976Sc13). 
E,S,L$1974Be54 report a level at 2637 with L=1+3, (2J+1)C{+2}S=0.03 for L=1 and 0.30 for L=3; d|s/d|W(max)=0.09 mb/sr for L=1 and 0.05 for L=3 


level_energy_unit: KEV
level_comment:
E,L,S$1974Be54 report 3113 {I10} with L=(1), (2J+1)C{+2}S=0.08 which probably corresponds to 3086 level and not 3118; d|s/d|W(max)=0.25 mb/sr 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from |g|g(t) in (1989Mo14). Others: 1973Ch26, 1969Az04 
$g-factor=0.303 {I8} from |g|g(|q,H) using DPAC technique (1989Mo14,1990Mo22). Other: 0.30 {I3} from |g|g(|q,H) using PAC (1973Ch42) 
$Q<0.75 (1990Mo23) from |g|g(|q,H,t) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$from |b|g(t) in {+77}Ge decay (1974ChXP). Others: 1970Tu03, 1969Az04 
$g-factor=+1.01 {I16} from |g|g(|q,H,t) using PAC technique (1974Ch31) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from 1980Jo11 (time digitized multiscaling). Others: 116 |ms {I4} (1968Io01,1957Sc11), >2 |ms (1997Is13) 
MOMM1$from g factor by PAD method (1970BeYN). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(p)(c.m.)=4077 keV {I5}, |G{-|g}=30 keV {I5}; identified as analog of 160 {I5}, 1/2- level in {+77}Ge 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$E(p)(c.m.)=4135 keV {I5} 
$Level-energy difference=218 keV {I5}, relative to the 12070 energy normalized to 160 keV {I5} (level in {+77}Ge); identified as analog of 225, 9/2+ level in {+77}Ge 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E(p)(c.m.)=4433 keV {I3}, |G{-|g}=26 keV {I5} 
$Level-energy difference=516 keV {I3}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 510, 5/2+ level in {+77}Ge 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(p)(c.m.)=4551 keV {I3}, |G{-|g}=27 keV {I5} 
$Level-energy difference=634 keV {I3}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 629, 3/2- level in {+77}Ge 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E(p)(c.m.)=4811 keV {I3}, |G{-|g}=26 keV {I5} 
$Level-energy difference=894 keV {I3}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 884, 5/2+ level in {+77}Ge 


level_energy_unit: KEV
level_comment:
E$12972 in 1978Kl05 is probably a misprint 
$E(p)(c.m.)=4931 keV {I3}, |G{-|g}=42 keV {I5} 
$Level-energy difference=1014 keV {I3}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 1006 or 1021 level in {+77}Ge 


level_energy_unit: KEV
level_comment:
$E(p)(c.m.)=5101 keV {I12}, |G{-|g}=80 keV {I7} 
$Level-energy difference=1184 keV {I12}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 1189 level in {+77}Ge 


level_energy_unit: KEV
level_comment:
$E(p)(c.m.)=5250 keV {I7}, |G{-|g}=56 keV {I5} 
$Level-energy difference=1333 keV {I7}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 1359 or 1386 level in {+77}Ge 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(p)(c.m.)=5446 keV {I10} 
$Level-energy difference=1529 keV {I10}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 1536, 1/2+ level in {+77}Ge 


level_energy_unit: KEV
level_comment:
$E(p)(c.m.)=5704 keV {I10}, |G{-|g}=72 keV {I5} 
$Level-energy difference=1787 keV {I10}, relative to the 12070 energy normalized to 160 keV (level in {+77}Ge); identified as analog of 1777 or 1804 level in {+77}Ge 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
J$L(d,|a)=3. log| {If{+1u}t}=9.64 to 0+ 
T$from timing of decay of {+78}As (1970Mc01). Others: 87 min {I3} (1970Pa05), 91 min {I2} (1959Kj49), 91.2 min {I6} (1953Su04), 88 min {I6} (1953Cu33), 90 min {I2} (1951Sh40) and 1950St02, 1937Sn02. Weighted average of all the listed values is the same as from 1970Mc01 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$in both (t,{+3}He) and (d,|a), it may Be unresolved doublet which implies the population of 293 level as well. 
J$log| {Ift}=4.26 from 0+; L(d,|a)=0+2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=5.27 to 1/2- and 6.85 to 5/2-; L(d,{+3}He)=L(t,|a)=L(|a,p)=1. Probable p{-3/2} orbital 
T$from 1953Cu33. Others: 8.2 min {I2} (1970OsZZ), 9 min {I2} (1961Yt01), 1954Yt03, 9 min (1951Bu25) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$M1+E2 |g to 3/2-; L(d,{+3}He)=1 and probable contribution from p{-3/2} orbital 
E$in (t,|a), 105 {I7} level (L=1) most likely involves p{-3/2} orbital 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$L(d,{+3}He)=L(t,|a)=L(|a,p)=4 and probable contribution from g{-9/2} orbital 
T$from |g(t); weighted average of 1.21 |ms {I1} (1988Gr14) and 1.18 |ms {I4} (2013RuZX). Other: 0.87 |ms {I6} (1998Ho15) is in disagreement 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$L(t,|a)=1 and probable contribution from p{-3/2} orbital 
E$this level is most likely different from 1012 since opposite parities are predicted by log| {Ift} value and L-transfer. Although from energy values levels in (|a,p) and (d,{+3}He) could be 1012 and/or 1016, but it is assumed that a common level is populated in the three reactions 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J$L(d,{+3}He)=L(t,|a)=L(|a,p)=1 and probable contribution from p{-1/2} orbital; |s(|q) shape in (|a,p) 


level_energy_unit: KEV
level_comment:
S$for L=1, value is for p{-3/2}. But J|p=1/2- (p{-1/2}) is suggested from other reaction data (see Adopted Levels) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from weighted average of 1.21 |ms {I1} (1988Gr14) and 1.18 |ms {I4} (2013RuZX). Other: 0.87 |ms {I6} (1998Ho15) is in disagreement 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J$log| {Ift}=4.5 from 0+ 
T$from 1975Kr08. Others: 16 s (1981Gi17), 16.5 s {I3} (1971Mc17), 15.3 s {I2} (1959Me68) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E,T$may be an isomer of few ns since 237|g is not seen in CLARA-PRISMA array in {+238}U({+82}Se,X|g) experiment where a thin target has to be used. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_comment:
J L(d,{+3}He)=1; log {Ift}=6.6 to 5/2- at 623.89 in {+81}Se; 1/2- discarded based on log {Ift}=8.3 {I1} (second-forbidden beta transition: 1/2- to 5/2-). 
T weighted average of 34 s {I2} (1975Kr08), 35.8 s {I16} (1974Ch11), 30 s {I4} (1962Cr08), 33 s {I1} (1960Yt02), 31 s {I2} (1960Mo01). Uncertainty is the lowest input value. Other measurement: 43 s {I1} (1970OsZZ). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J (1/2)- in 2008Ba34. 
J M1+E2 |g to 3/2-; log {Ift}=6.73 from (1/2+) in {+81}Ge |b- decay (6.4 s); |g from (7/2-) at 2197. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J L(d,{+3}He)=1+(3,4); L(|a,t)=(1,3); see also comment on J|p(1042). Origin of L=(3,4) component in (d,{+3}He) is not known. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J M1,E2 |g to 3/2-; L(t,|a)=3; considering connecting |g transitions from (3/2+) at 3136 and 3195 keV levels. 
T from |g|g(t) (1981Ho24 - {+81}Ge |b- decay (6.4 s)). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J L(t,|a)=3, |g to 3/2- and (5/2)-. Levels at 727 {I9} and 738 {I4} in (t,|a) and ({+3}He,d), respectively, may differ from state populated in |b{+-} decay, log {If{+1u}t}=8.4 {I2} from (1/2+) and negligible |b feeding from (9/2+). 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
J L(t,|a)=4. This level must differ from the 758.4 level known from |b{+-} decay unless the reported L(t,|a) (based on |s at only 5 angles) is incorrect. 


level_energy_unit: KEV
level_spin_parity: (5/2-,3/2+)
level_comment:
J |g to 3/2- g.s.; log| {Ift}=6.7 from (1/2+) (log{+1u} {Ift}>8.5); 2207.5|g from (7/2+) 2965.9. Assumed to differ from the 757 level in |b{+-} decay because the reported L(t,|a)=4 is inconsistent with J|p deduced from |b{+-} decay to this 758.4 level. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J 751.5|g connecting this level with the 290 level for which L(t,|a)=1 implies J|p(1042)=(7/2-) and J|p(290)=(3/2)-. Preferred assignment from shell model calculation (2022De07 - {+81}Ge |b{+-} decay (6.4 s)). log {Ift}=6.7 from (9/2+). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: ?
level_comment:
E weighted average of 1613 {I5} from (t,|a) and 1613 {I8} from (d,{+3}He). 
J L(t,|a)=0 based on just 4 data points. This state is not fed in |b{+-} decay from (1/2+) and could only correspond to the 1614 level fed in |b{+-} decay from (9/2+) if L|=0. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J 876|g to (7/2-) 738 and 1144.7|g from (11/2+) 2758, 9/2+ from shell model (2022De07). Indirectly populated in |b{+-} decay from (9/2+). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-,9/2-)
level_comment:
J log {Ift}=8.3 from (9/2+), preferred 5/2- from shell model calculations (2022De07 - {+81}Ge |b- decay (6.4 s) - 5/2- to 11/2-). 1005.7|g to (1/2-,3/2-,5/2-). 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J log {Ift}=4.9 from (9/2+), preferred (9/2+) in shell model calculations (2022De07). (11/2)+ assumed in ({+16}O,x|g). 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2-)
level_comment:
J log| {Ift}=5.9 from (9/2+); 2526.5|g to (5/2)- 336, 2103.9|g to (5/2-,3/2+). Other: (7/2+,9/2+,11/2+) in 2022De07. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-,5/2-)
level_comment:
E this level assigned in {+81}Ge |b- decay (6.4 s) (2022De07). In 1981Ho24, assigned in isomeric {+81}Ge |b- decay (7.6 s). 
J proposed in 2022De07, based on insignificant |b feeding from (9/2+) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-,9/2-)
level_comment:
E this level assigned in {+81}Ge |b- decay (6.4 s) (2022De07). In 1981Ho24, assigned in isomeric {+81}Ge |b- decay (7.6 s). 
J (5/2-,7/2-,9/2-,11/2-) proposed in 2022De07. (1/2,3/2) as of the assignment in 1981Ho24 from isomeric {+81}Ge |b- decay (7.6 s) (1/2+). 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
From total intensity balance I|b=1.0 {I6} gives log {Ift}=6.4 {I3}. For J{+|p}=(13/2+), it should be a negligible branch from (9/2+). 
J (5/2-,7/2-,9/2-,11/2-) in 2022De07, based on log {Ift}=6.2 {I1}. 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2-)
level_comment:
E this level assigned in {+81}Ge |b- decay (6.4 s) (2022De07). In 1981Ho24, assigned in isomeric {+81}Ge |b- decay (7.6 s). 
J (7/2+,9/2+,11/2+) in 2022De07. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
In 1981Ho24, 1352.3|g {I1} placed from this level, absent in their 1980HoZN and not reported in 2022De07. Also 2228.2|g {I5} with I|g=2.4 {I5} (from 2.0 {I4}) is reported in 1980HoZN, 1981Ho24, but not reported in 2022De07. The evaluator avoids to list these E|g. 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+,11/2+)
level_comment:
E this level assigned in {+81}Ge |b- decay (6.4 s) (2022De07). In 1981Ho24, assigned in isomeric {+81}Ge |b- decay (7.6 s). 
J (7/2+,9/2+,11/2+) in 2022De07 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-,9/2-)
level_uncertain: ?
level_comment:
J in 2022De07, this level populated in |b feeding from (9/2+) and proposed J{+|p}=5/2-,7/2-,9/2-,11/2-. No J{+|p} listed here. (1/2,3/2) can be expected if |b feeding from (1/2+). 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2-)
level_uncertain: ?
level_comment:
I|b=4.8 {I19} log {Ift}=5.9 {I2}, less likely for a (7/2+,9/2+) state (Adopted Levels) from (1/2+). 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_uncertain: ?
level_comment:
I|b=6.0 {I24} log {Ift}=5.8 {I2}, less likely for a (7/2+,9/2+) state (Adopted Levels) from (1/2+). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
J$2004Ga44 suggest 2-,5- sequence for the two isomers. Previously adopted 1+ for g.s. is not supported by decay data (2014Mi16). 1092|g from 1+ supports 2- for g.s. 2014Mi16 summarize shell-model calculations suggesting states with J|p=2-,5-,4- 
T from 1975Kr08. Others: 22.6 s {I14} (1972De43), 19.0 s {I15} (1970Va31). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$from 2004Ga44; log| {Ift}=6.2 to (4+); 5- isomers in {+82}Br, {+80}Br, and {+82}Rb. 
T weighted average of 14.0 s {I5} (1975Kr08), 13.7 s {I8} (1970Ka04), and 13.0 s {I6} (1970Va31). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$132.1 {I3} obtained in 2014Mi16 is in agreement with 128 keV {i6} from mass measurement (2008Ha23) 


level_energy_unit: KEV
level_spin_parity: (0-,1-,2-)
level_comment:
E$note that the ordering of the 575.5-516.5 |g cascade is reversed in 2014Mi16, thus defining a level here at 516.6 keV instead of a level at 576 keV as in 2014Mi16 


level_energy_unit: KEV
level_comment:
J$(0-,1) from log| {Ift}=6.13 {I11} from 0+ parent in conflict with decay to (4-); no assignment in 2015Et01 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$it is assumed by the authors that the lowest state in the reaction is the 5- isomer. Authors consider it unlikely that the g.s. as well as the isomer is populated. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
T$weighted average of 14.1 s {I11} (1968De19), 13.3 s {I4} (1969ScZY), 13.3 s {I6} (1974KrZG). 
J$the first two orbitals located above the Z=28 shell closure are |pf5/2 and |pp3/2, thus the low-lying levels are expected to have J|p=3/2-,5/2-. {+85}Br (Z=35) has J|p(g.s.)=3/2-, suggesting that the f5/2 orbital is filled first; therefore, {+83}As(Z=33) should have J|p(g.s.)=5/2-. Non observation of the 306-keV level in {+208}Pb({+18}O,X|g) further suggests the spin of the ground state is higher than that of the 306-keV level. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$from systematics of the |pg{-9/2} single particle levels in N=30-50, Cu, Ga, As, Br and Rb nuclides, in agreement with Shell model calculations. 


level_energy_unit: KEV
level_spin_parity: (11/2+,13/2+)
level_comment:
J$from I(429|g)>I(1341|g), indicating a positive parity and relation to the (9/2+) level at 2779 keV. However, Shell model calculations show this level at 0.5-0.7 MeV higher energy. An increase in collectivity may explain the lowering. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: S
level_comment:
J$strong feeding of 2+, (4+) levels, log| {Ift}=6.4, 6.5, respectively. Negative parity is suggested by shell model. 
T$weighted average of 4.5 s {I2} (1991Om01), 5.3 s {I4} (1975Kr08), 3.24 s 26 (1996WaZX). Others: 5.8 s {I5} (1968De19) and 4.02 s {I3} (1993Ru01). 
$%|b{+-}n from 2002Pf04; others: 0.28 {I4} (1993Ru01), 0.13 {I6} (1973Kr06), 0.06 {I3} (1976NiZZ). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: S
level_comment:
T$ measured by 2013Ma22 from |b-gated time distribution of |g rays in {+84}Se. Weighted average of 3.08 s {I78} and 3.27 s {I87} for 667|g and 1455|g, respectively. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: S
level_comment:
J$from systematics of odd-a neutron-rich As isotopes. 
T$unweighted average of 2.002 s {I13} (1993Ru01), 2.032 s {I12} (1991Kr15) and 2.028 s {I12} (1968To19). Others: 2.08 s 14 (2013Ma22), 2.0 s 1 (1991Om01), 1.90 s {I10} (1978Cr03), 2.08 s {I5} (1976Ru01), 2.05 s {I5} (1973Kr06), 2.15 s {I15} (1967De01), 1969ScZY 
%B-N$weighted average of 64.1 {I14} (2013AgZY) and 59.4 {I24} (1993Ru01). Other values: 39 {I5} (1991Om01), and 58 {I10} (1991Kr15). Earlier measurements of 23 {I3} (1973Kr06) and 22 {I8} (1978Cr03) were based on outdated fission yields. Analysis and evaluation of %|b{+-}n data: 1989BrZI, 1982Ru01, 1977Ru10, 1975Iz03 
$Measured delayed-neutron emission probability or yields: 1993Ru01, 1991Om01, 1991Om02, 1991Kr15, 1979Kr03, 1978Cr03, 1975Kr08, 1973Kr06, 1969ScZY, 1968To18, 1968To19, 1967De01, 1966To02 
$Measured delayed-neutron spectra: 1981ShZS, 1979Kr03, 1976Kr18 (also 1974Fr09), 1976Ru01, 1974Cr06, 1974Sh18, 1973Kr06, 1968To18, 1968To19, 1967De01, 1966To02 
$Calculated delayed neutron spectra: 1979Pr03, 1978Gj01, 1977Sh10, 1972Pa11 
$1981ShZS report following 23 neutron groups from the decay of 85AS with energy (relative intensity): 55.0 10 (32 12), 65.3 13 (33 11), 69.2 14 (44 10), 76.2 15 (20 10), 83.8 16 (41 11), 97.8 19 (86 12), 109.8 22 (84 11), 125.8 25 (20 10), 141.4 28 (53 10), 153 3 (27 9), 172 3 (55 9), 202 4 (37 9), 284 6 (46 9), 412 9 (36 9), 521 11 (100 7), 581 13 (47 9), 726 16 (29 8), 937 23 (52 8), 1584 43 (16 8), 2027 57 (11 7), 2342 68 (20 8), 2812 86 (19 8), 4510 161 (16 7) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: S
level_comment:
$The g.s. of {+85}As is expected to be populated in delayed neutron decay of {+86}Ge 
J,T$from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$as given in Figure 5 of 2015Ma61. J|p=(3/2-) is given in the Adopted Levels for {+85}As in the ENSDF database based on systematics of odd-A neutron rich As isotopes. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$as given by 2017Ko11. J|p=(3/2-) is given in {+85}As Adopted Levels in the ENSDF database (Dec 2013 update) from systematics of odd-A neutron-rich As isotopes. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$measured by 1993Ru01. Others: 0.861 s {I64} (2013Ma22), |?0.9 s (1978Cr03), 0.9 s {I2} (1973Kr06) 
%B-N$measured by 2014Ag12. Others: 33 {I4} (1993Ru01), 3.8 {I+17-10} (1973Kr06), 10.5 {I22} (1978Cr03), 26 {I7} (2002Pf04 compilation). Theoretical %|b{+-}n=12.8 (1997Mo25), 6.6, 65.6 (2002Pf04). Systematic (KHF) %|b{+-}n=6.0 (2002Pf04). Theoretical %|b{+-}2n=0.02 (1997Mo25) 
$1993Ru01 QUOTE REVISED VALUES OF %B-N AS 15 11 (1973Kr06) AND 12 8 (1978Cr03) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
J$from systematics of the odd-mass arsenic isotopes, see the nuclear-data evaluations for A=77 (1997Fa12), 79 (2002Si13), and 81 (2008Ba34). 
T$There have been several measurements of the half life. In 2013Ma22 a proton beam was provided by the Oak Ridge Isochronous Cyclotron (ORIC) at the HRIBF-ORNL facility with a {+238}uc{-x} target. Fission fragment were ionized to charge state +1 then purified using H{-2}S gas, a mass pre-separator and electromagnetic separation. The purified beams were then sent to the Low-energy Radioactive Ion Beam Spectroscopy Station (LeRIBSS) and implanted in a moving tape collector. Measured E|g, I|g, E|b, |b|g-coin, and half-life of the {+87}As g.s. using two plastic scintillation counters and four HPGe detectors. Comparison with the Gross theory of |beta decay, the finite-range droplet model and the continuum quasiparticle random-phase approximation. The half life was measured from a |b-gated time distribution of |g rays in {+87}Se and {+86}Se. In 2012Qu01, a {+136}Xe primary beam, E=120 MeV/nucleon, impinged on a 235 mg/cm{+2} Be target. Experiment performed at the NSCL Coupled Cyclotron Facility. Fragments were separated by the A1900 fragment separator using the B|r-|DE-B|r technique. Beta decays measured in the NSCL |b Counting System (BCS) consisting of four silicon pin detectors, a double sided silicon strip detector and a single sided silicon strip detector. Measured energy loss total kinetic energy, time of flight, and isotopic isotopic half-life. A total of 27 implantions were observed with 12 correlated decay sequences. The value listed in Table I of 2012Qu01 is 1450 ms {i550} (systematic) {I+3900=1100} (statistical) and used the maximum liklihoood method for the T{-1/2} analysis. However, due to the large uncertainties, this was not included in the weighted average. Finally, the Adopted Value is taken from a weighted average of 0.485 s {i40} (1993Ru01), neutron counting measurements, both values, 0.478 s {I 44} and 0.495 {i60} from 2013Ma22 and adopting the smallest uncertainty from that set. Others: |<1.5 s (1967De01), 0.6 s {i3}(1970Kr05), |?0.3 s (1973Kr06) 0.73 s {i6} (1978Cr03), and 1.5 s {I 39-12} from maximum-likelihood method (2012Qu01) 
%B-N from 1993Ru01; others: 44% (14) (1978Cr03) which was re-evaluated to 51% (35) in 1993Ru01 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
E$assuming that the observed events correspond to the ground state 
T$from |b decays correlated with implanation events (2012Qu01). Value given by 2012Qu01 is 200 ms {I5} (syst) {I+200-90} (stat) obtained by analysis using maximum likelihood method applied to 16 implantations and 8 correlated decay sequences. 
%B-N$ this level is expected to undergo beta delayed neutron emission, some estimates of %|b{+-}n include 38% (systematics, 2012Mc04) and 32% (QRPA theory, 2003Mo09). 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay is possible, followed by delayed neutron emission, thus 100% |b{+-} decay is assigned by inference. The |b{+-}3n decay mode is unlikely as Q(|b{+-}3n)=-240 {I300} (syst) 
$Theoretical T{-1/2}=58.9 ms, %|b{+-}n=72, %|b{+-}2n=0 (2019Mo01) 
$Theoretical T{-1/2}=65.9 ms, %|b{+-}n=61.8, %|b{+-}2n=0.2 (2016Ma12) 
E$the observed fragments are assumed to belong to g.s. of {+89}As 
J$5/2- proposed from systematics (2021Ko07), 1/2- in theoretical calculation (2019Mo01) 
T$half-life of decay of {+89}As has not been measured. T{-1/2}>300 ns from time-of-flight of fission fragments (1997Be12), and >150 ns from time-of-flight in 1994Be24. General decreasing trend of half-lives with increasing neutron numbers in neutron-rich isotopes suggests T{-1/2}<200 ms from measured T{-1/2}=945 ms for {+86}As, 484 ms for {+87}As and 200 ms for {+88}As. Values for {+86},{+87},{+88}As are taken from ENSDF database (October 13, 2021 version). T{-1/2}=220 ms from systematics (2021Ko07). 


level_energy_unit: KEV
level_comment:
E$the observed fragments assigned to {+90}As are assumed to correspond to the ground state 
T$>300 ns from time-of-flight in 1997Be70. Actual half-life is expected to be much longer as suggested by the calculated value of 20.5 ms (2019Mo01) 
J$1/2- proton and 3/2+ neutron orbital predicted by 2019Mo01 
$production cross section=21 nb (1997Be70) corresponding to 228 counts assigned to {+90}As 
$Calculated %|b{+-}n=40, %|b{+-}2n=1 (2019Mo01). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E$it is not established to which level the 0.20 |ms isomer decays. It is possible this is the ground state of {+90}As. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_comment:
$Number of implanted fragments=1.1|*10{+4} 
T$from 124.5|g(t) using maximum likelihood method assuming exponential decay component(s) plus a constant background (2012Ka36) 


level_energy_unit: KEV
level_comment:
T lifetime exceeds flight time (unstated) through fragment mass analyzer in experiment of 1997Be70, 1995CzZZ. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed events correspond to the ground-state 
J$3/2- from theory in 2019Mo01 and systematics in 2021Ko07. 
T$measured by 2016Go26 (same T{-1/2} given in 2020Gi02 and 2017GoZT thesis) from correlated decay curve for {+63}Se implants and subsequent decays 
$A total of 348 events were assigned in 2016Go26 to {+63}Se. 
$Production |s=13 fb {I3} (2016Bl05) in {+9}Be({+78}Kr,X), E=345 MeV/nucleon 
$No peak due to protons at an expected 2p-decay energy was observed, upper limit is based on the assignment of at most one count to this decay mode for a total of 189 implants of {+63}Se (2016Go26) 
$Several theoretical calculations as cited in Fig. 1 of 2016Go26 predict negative S(2p) value for {+63}Se, making this nucleus a possible 2p-emitter 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
${+64}Se is most likely stable towards proton decay, as S(p) seems positive and S(2p) is only marginally negative. In addition, a large number of events were assigned to this isotope in A/Q Fig. 1 of 2016Bl05. As no other decay mode is possible, %|e+%|b{++}=100 is assigned by inference. 
T$half-life of {+64}Se has not been measured. 2005St29 suggested >180 ns from 2005St29, based on experimental observation of at least one event combined with expected number of transmitted nuclei based on abrasion-ablation model cross sections and the time of flight (358 ns for {+64}Se). From a systematic trend of half-lives of 33 ms {I4} for {+65}Se, 42 ms {I12} for {+66}Se, 136 ms {I12} for {+67}Se and 35.5 s {I7} for {+68}Se, half-life of {+64}Se is expected to be <40 ms, assuming a decreasing trend as the neutron number decreases. 
$Theoretical T{-1/2}(|b decay)=87 ms (2019Mo01). 2021Ko07 give 30 ms from systematic trend. 
$Production cross section=0.28 pb {I19} (2005St29), 0.38 pb {I24} (2016Bl05) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
T$from 2011RoZZ. Other: 9.6 ms {I+5.3-4.1} (1995Hu24). 
J$from mirror symmetry arguments ({+65}Ga J|p=-3/2) and non observation of p decay to excited states in {+64}Ge which suggests low-spin. 
$2011RoZZ observed 3.51 MeV {I2} proton decay from 3.4 MeV {I9} IAS in {+65}As. %|b{++}=48 {I15} to the IAS. Authors assumed superallowed transition to IAS with log| {Ift}=3.57 {I20}. These results are consistent with those of 1993Ba12. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
$ T{-z}=-3/2 
T$ measured by 2011Ro47 from |b{++} decay correlation time spectrum 
J$ as suggested in 2011Ro47 
%B+P$ from integrating the decay-time spectrum gated on proton spectra above 900 keV (2011Ro47) 
$ A 3.51 MeV {I2} proton peak is observed which is not in coin with |g rays. This proton group depopulates IAS in {+65}As at 3420 keV {I87}. Two weaker peaks are seen at 2.62 MeV {I3} and 3.77 MeV {I3}, the former is consistent with decay to 901.7, 2+ level in {+64}Ge, but this proton group is not seen in coincidence with |g rays. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E,J$calculations using D1S Gogny interactions and shell-model approach using the JUN45 interactions predict oblate-deformed shape 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$the Coulomb energy difference of -28 keV 7 was deduced from the excitation energies of the 2{++} states in {+66}Se and {+66}Ge. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Decay modes from {+66}Se Adopted Levels in ENSDF database 
$T{-z}=-1 
T$measured by 2014Ro14 from |b{++} decay correlation time spectrum 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$T{-z}=-1/2 
$Production |s=0.11 |mb {I5} in {+9}Be({+78}Kr,X),E=140 MeV/nucleon (2005St29), compared with theoretical cross sections 
J$analogy to mirror g.s. state of {+67}As with J|p=(5/2-) 
T$weighted average of 133 ms {I4} (2014Ro14, fragment-|b, and fragment-|g correlations); and 136 ms {I12} (2002Lo13,2002Bl17; previous T{-1/2}=60 ms {I+17-11} in 1995Bl23); and 107 ms {I35} (1994Ba50) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_comment:
T$measured mean lifetime |t=1.5 ns {I6} (2009Or02, time spectra gated above and below the 9/2+ state) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
%ECP$Weighted average of 0.062 {I12} (1977Ma24) and 0.045 {I10} (1988De28) 
J$From the |b-delayed proton emission work of 1977Ma24, J({+69}Se g.s.) =1/2,3/2, or 5/2. Higher J values are ruled out. Given J(39 level) =5/2, |a(exp)(39|g)=28.0 {I25} gives |d(E2/M1)>5. Along with T{-1/2}(39 level)=2.0 |ms {I2}, J(g.s.)=3/2 or 5/2, and for E|g=38.8, one gets B(M1)(W.u.)<2.4x10{+-7}. This is unreasonably small and rules out the J=3/2 or 5/2 alternatives. This argument establishes J=1/2. There is no experimental evidence for |p, but systematics and the available shell model states |p must be negative 
T$from time-sequential proton spectra in {+69}Se |e decay (1977Ma24). Also reported by similar group in 1976Ha22 and 1976Ha29 Other: 27 s 3 from {+69}Se |e decay (1974No08) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$J=9/2 from excit. in ({+32}S,2pn|g). |p=+ from M2-E2 cascade to |p=- gs 
T$From {+40}Ca({+32}S,2pn|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 225 ps {I11} from the lineshape analysis of 161|g and 250 ps {I20} from the lineshape analysis of 251|g (2015Ni01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from weighted average of 2.27 ps {I26} (2014Ni09) and 2.22 ps {I14} (2008Lj01) using recoil distance Doppler shift method. Others: 1.0 ps {I2} from recoil distance Doppler shift method (1986He17) and 1.1 ps {I3} (1975GuYV). 
J$from 944.51|g E2 to 0+ 
MOME2$from nuclear reorientation effect in Coulomb excitation (2007Hu03). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Other: < 5.2 ps effective half-life from recoil distance Doppler shift method (2014Ni09). 
J$from 1600.1|g E2 to 0+. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$(0+) from 1065.8|g Q to 2+ in 1981Ah03. Authors tentatively assigned (0+) for this level based on isotropic angular distribution. Other: (0+) in 1980Wa19, based on the isotropic angular distribution. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$Others: < 3.3 ps, effective half-life from recoil distance Doppler shift method (2014Ni09) and 1.0 ps (1986He17) using recoil distance Doppler shift method deduced from singles data and 2.3 ps {I6} (1975GuYV). 
J$from 1094.4|g E2 to 2+; assumed E2 cascade member. 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$upper limit from effective half-life of 1.29 ps {I40} from recoil distance Doppler shift method (2014Ni09). Other: 4.2 ps {I6} using recoil distance Doppler shift method (1986He17) using singles data. 
J$from 1574.1|g D to 2+; 868.8|g from 5- 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$other: 2.7 ps {I6} from recoil distance Doppler shift method, deduced using singles (1986He17). 
J$from 964.39|g E2 to 4+; assumed E2 cascade member. 


level_energy_unit: KEV
level_comment:
J$(9) from 348.0|g to 8+ suggested in |e decay (2000Pi15) but the placement of the |g transition is uncertain. 


level_energy_unit: KEV
level_spin_parity: (13-)
level_lifetime_unit: NS
level_comment:
T$quoted by 1989My01; generalized centroid-shift method. 
J$from 796.5|g to 12+; 348.0|g to (12+); proposed based on Weisskopf estimates in 1989My01. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_comment:
$2002Ro25 report a 958|g depopulating this level, but no final level was given. As there is no corresponding final level in the Adopted Levels, the 958|g is not adopted here. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Other: 1.0 ps {I2} from recoil distance Doppler shift method (deduced using singles data) in 1986He17. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$Other: 2.7 ps {I6} from recoil distance Doppler shift method, (deduced using singles data) in 1986He17. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13-)
level_lifetime_unit: NS
level_comment:
T$quoted by 1989My01; generalized centroid-shift method 
J$proposed based on Weisskopf estimates in 1989My01. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Q=+ (2007Hu03) 
$Diagonal E2 matrix element=-0.5 is required for agreement of the current measurement with earlier measured lifetime |t=1.5 ps {I3} at 1|s level. This value implies prolate shape. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$total branching fraction that decays through the 2+ level is estimated as 1.3 % {I11} by 2017Mo18 by determining the intensity balance of the 2+ level. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$from E|g. Value of 954 listed in Table I of 2021Wi01 is a misprint 
J$From {+70}Se Adopted Levels in the ENSDF database (July 2016 update). 
$Measured |s=234 mb {I70}(stat) {I43}(syst) for {+197}Au target (2021Wi01) at E({+70}Se)=140 MeV/nucleon 
$Measured |s=15.1 mb {I53}(stat) {I28}(syst) for {+9}Be target (2021Wi01) at E({+70}Se)=140 MeV/nucleon 
$Deduced nuclear deformation length |d{-N}=1.11 fm {I22} (2021Wi01), where uncertainty includes 0.20 fm statistical and 0.10 systematic. 
$Deduced E2 matrix element=0.407 eb {I82} (2021Wi01), where uncertainty includes 0.068 eb statistical, 0.041 eb systematic, and 0.020 eb theoretical 
$Deduced B(E2)=0.1659 e{+2}b{+2} {I659} (2021Wi01), where uncertainty includes 0.0543 e{+2}b{+2} statistical, 0.0336 e{+2}b{+2} systematic, and 0.0164 e{+2}b{+2} theoretical 
T$deduced by compiler from B(E2) value. This value can be compared T{-1/2}=2.23 ps {I14} in {+70}Se Adopted Levels in the ENSDF database (July 2016 update), measured using RDDS method 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$from {+70}Se Adopted Levels in the ENSDF database (July 2016 update); no new T{-1/2} measurement since the 2016 update. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=5.8 to 5/2- and log| {Ift}=5.9 to 3/2-; observed feeding with log| {If{+1u}t}=9.0 to 9/2+ rules out 3/2-. 
T$from |g-decay curve in a well-type NaI detector (1980Te01). Others: 5.6 min {I15} (1971Do01), 4.93 min {I10} (1969Hu13), 5 min {I2} (1957Be43), 4.5 min {I5} (1957At37) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
J$E2 |g to (5/2-); systematic occurrence of low-lying p{-1/2} orbital in neighboring nuclides 
T$from |g|g(t) and |g(x ray)(t) in |e decay 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from 260|g(t) (2000Ch07), {+71}Se formed in fragmentation of {+92}Mo beam at 60 MeV/nucleon with a nickel target at GANIL facility. Other: 19 |ms {I3} from |g|g(t) in |e decay (1982Ha32) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (9/2+), band member. 
T$from DSAM in {+58}Ni({+16}O,2pn|g) (1984EbZZ). Other: >1.4 ps in ({+23}Na,pn|a|g). 
$Q(transition)<1.25 (2012Ho16). 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
$Q(transition)=1.40 {I5} (2012Ho16). 
J$|DJ=(2), (E2) |g to (13/2+), band member. 
T$other: 0.53 ps {I21} from DSAM in {+58}Ni({+16}O,2pn|g) (1984EbZZ). 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: PS
level_comment:
J$|DJ=(2), (E2) |g to (11/2-), band member. 
T$from DSAM in {+58}Ni({+16}O,2pn|g) (1984EbZZ). Other: >1.4 ps in ({+23}Na,pn|a|g). 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
$Q(transition)=2.03 {I3} (2012Ho16). 
J$|DJ=(2), (E2) |g to (15/2-), band member. 
T$other: <0.7 ps from DSAM in {+58}Ni({+16}O,2pn|g) (1984EbZZ). 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J$|DJ=1, dipole |g to (17/2+). 
$Possible 3-qp state formed by coupling of g{-9/2} neutron to 5- state at 3387 keV in {+70}Se (2012Ho16). 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: PS
level_comment:
J$|DJ=(2), (E2) |g to (17/2+), band member. 
T$other: 0.40 ps {I28} from DSAM in {+58}Ni({+16}O,2pn|g) (1984EbZZ). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
T$from |g-decay in a well-type NaI detector. Other: 4.93 min {I10} (1969Hu13). Same value in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
$This level is replaced by 1233 level as the 1233.0|g is now placed from 1233 level to g.s. in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
$This level is replaced by 1379 level as the 1378.8|g is now placed from 1379 level to g.s. in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_comment:
$This level is replaced by 2066 level as the 687.6|g is now placed from 2066 level to 1378 level and the 833.4|g is placed from 1233 level in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_comment:
$This level is replaced by 2976 level as the 909.8|g is now placed from 2976 level to 2066 level in the Adopted Levels 


level_energy_unit: KEV
level_comment:
$This level is replaced by 4039 level as the 1064.2|g is now placed from 4039 level to 2976 level in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.39 ps {I+11-10} from DSAM for 1263.3|g (2012Ho16) 
$Q(transition)=1.63 {I+26-19} 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.77 ps {I+6-5} from DSAM for 1150.5|g (2012Ho16) 
$Q(transition)=1.40 {I5} 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=1.18 ps {I11} from DSAM for 909.6|g (2012Ho16) 
$Q(transition)=2.04 {I+10-9} 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.92 ps {I3} from DSAM for 945.5|g (2012Ho16) 
$Q(transition)=2.03 {I3} 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.43 ps {I+12-9} from DSAM for 1033.6|g (2012Ho16) 
$Q(transition)=2.01 {I+25-23} 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.41 ps {I2} from DSAM for 1186.9|g (2012Ho16) 
$Q(transition)=1.69 {I4} 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.70 ps {I2} from DSAM for 1063.6|g (2012Ho16) 
$Q(transition)=1.70 {I2} 


level_energy_unit: KEV
level_spin_parity: 23/2-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.48 ps {I2} from DSAM for 1077.7|g (2012Ho16) 
$Q(transition)=1.95 {I4} 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.47 ps {I4} from DSAM for 1199.2|g (2012Ho16) 
$Q(transition)=1.46 {I+7-6} 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.57 ps {I5} from DSAM for 1140.7|g (2012Ho16) 
$Q(transition)=1.52 {I+7-6} 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.54 ps {I4} from DSAM for 1202.0|g (2012Ho16) 
$Q(transition)=1.36 {I5} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$unweighted average of delayed coincidence measurements: 19.3 ns 4 from {+70}Ge(|a,2n|g) (1974Dr02) and 15.8 ns {i10} from {+72}Br |e decay (1974Ha04) 


level_energy_unit: KEV
level_comment:
E$may be a doublet: J|p=(2)+ from |g to 0+ and log| {Ift}=6.34 from 3+, J=(3) from |g(|q) in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (26+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E$1991Ch14 observed a 26+ level at 18184 {i3} which decays to the 24+ level. 
J$stretched (E2) |g to 24+. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
E$placed by arguments from |g|g data. 
T$from delayed |g|g between 1062 and 862 |g's (1974Ha04), with the assumption that T{-1/2} of the 862 level is comparatively short 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.91 ps {I21} (2008Lj01), 2.4 ps {i2}, 2.8 ps {i3} (1986He17), 3.3 ps {i4} (1979Ki17), 3.6 ps {i3} (1978He13), 2.0 ps {i4} (1975Lo08) (recoil-distance method); and 4.0 ps {i8} (line-shape analysis, 1976Ha01). Other: 1.80 ps {I7} (1998Sk01). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$T{-1/2} weighted average of 2.29 ps {I14} (2008Lj01), 1.66 ps {i17} and 1.9 ps {i2} (1986He17), 2.6 ps {i3} (1979Ki17), 1.9 ps {i2} (1978He13) (recoil-distance method); and 3.1 ps {i10} (line-shape analysis, 1976Ha01). Other: 1.46 ps {I7} (1998Sk01). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.18 ps {I7} (2008Lj01), 1.8 ps {i3} and 1.5 ps {i2} (1986He17); 1.1 ps {i2} (1979Ki17); and 1.8 ps {i5} (1976Ha01). Other: 0.97 ps {I7} (1998Sk01). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.42 ps {I9} (2001Pa03), 0.55 ps {i10} (1979Ki17), 0.62 ps {i17} (1977Li06) (DSA) and 0.52 ps {i7} (line-shape analysis, 1976Ha01) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.21 ps {I3} (2001Pa03), 0.21 ps {i3} (1979Ki17), 0.28 ps {i8} (1977Li06); and 0.24 ps {i5} (1976Ha01) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$average of 0.15 ps +6-4 (2001pa03), 0.12 ps {i3} (1979Ki17), 0.11 ps {i3} (1977Li06); and 0.17 ps {i3} (l1976Ha01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
MOME2$from spectroscopic quadrupole moment Q=-0.57 {I29} (stat) {I10} (syst) with statistical and systematic uncertainties added in quadrature. It is deduced from the diagonal matrix element=-0.76 {I38} (stat) {I14} (syst) extracted from a GOSIA fit to the measured |g-ray yields, with known matrix elements from literature as constraints in the fit. The negative spectroscopic quadrupole moment indicates that the anticipated transition from prolate to oblate shape in neutron-deficient selenium occurs between {+72}Se and {+70}Se, viewed in the systematics of spectroscopic quadrupole moments for the first excited 2+ states in neighboring Se isotopes 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$measured mean lifetime |t=27.7 ns {I3} from time difference of (379|g+1062|g+1434|g)(ce for 937) (2022Sm02). This value is compared by authors to T{-1/2}=19.3 ns {I4} in 1974Dr02 (Phys. Rev. C9, 948), and 15.8 ns {I10} in 1974Ha04 (Phys. Rev. Lett. 32, 239). A weighted averaged value (using NRM technique) of the three experimental is given by 2022Sm02 as |t=27.7 ns {I4} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
$Strong absorption radius r{-0}=1.028 fm {I23}; rms matter radius <r{+2}>{+1/2}=3.92 fm {I17}, deduced from measured reaction |s{-R} in Si({+73}Se,X),E|?50-60 MeV/nucleon and Glauber model analysis (2004Li29,2005Le43) 
J$spin from NMR and nuclear orientation (1988Be39). Parity from log| {Ift}=5.4 to 9/2+ 
T$weighted average of 7.18 h {I9} (1969Ma21) and 7.08 h {I15} (1976Bo19). Others: 1967Ra08, 1960Ri09, 1955Ha85 
MOMM1$from 2001St31. Others: 0.87 {I5} (1988Be39), 0.85 {I7} (1987Ni13). All measurements used |b-NMR method on oriented nuclei 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$%|e+%IT: from growth and decay of {+73}Se g.s. 
J$|e feeding to 3/2- and 5/2-; E3 |g to 9/2+ and RUL 
T$weighted average of 40.5 min {I17} (1976Bo19), 38.6 min {I22} (1969Ma21). Others: 1960Ri09, 1968Ak03, 1969Mu03, 1970Me20. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$125.6|g M1 (|DJ=1) to 3/2-; 354.3|g M1+E2 from 7/2- 
T$from RDM in ({+16}O,n2p|g). Other: 0.20 ns {I14} from |g-rf in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$192.4|g to 9/2+, 446.9|g Q (|DJ)=2 from 9/2+; RUL gives 5/2+ or 13/2+ since negative parity would require an unreasonably large B(M2) value for 192.4|g; 13/2+ is ruled out by 103.0|g from 7/2+. 
T$|g-rf in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$639.3|g D(+Q) (|DJ=0) to 9/2+; 933.1|g from 13/2+ and RUL forbids 9/2- since it would requires an unreasonably large B(M2); band assignment 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$653.6|g E2 (|DJ=2) to 5/2-, 299.3|g M1+E2 to 7/2-; band assignment 
T$RDM in ({+16}O,n2p|g). Other: 3.9 ps {I7} (RDM in ({+19}F,3pn|g)) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$971.0|g E2 (|DJ=2) to 9/2+ g.s.; band assignment 
T$average of 0.90 ps {I7} (RDM in ({+16}O,n2p|g)), 0.83 ps {I7} (DSAM in (|a,n|g)), 1.3 ps {I3} (RDM in ({+19}F,3pn|g)) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$674.3|g E2 (|DJ=2) to 7/2-, 374.3|g D+Q to 9/2- 
T$from RDM in ({+16}O,n2p|g). Other: 2.5 ps {I3} (RDM in ({+19}F,3pn|g)) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 747.7|g to 9/2-; |DJ=1, M1+E2 373.1|g to 11/2- 
T$weighted average of 1.01 ps {I+17-16} (DSAM in ({+28}Si,|apn|g)), 1.32 ps {I14} (RDM in ({+19}F,3pn|g)), 1.18 ps {I21} (RDM in ({+16}O,n2p|g)), 0.83 ps {I14} (DSAM in (|a,n|g)) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$822.8|g |DJ=2, E2 to 11/2-; 450.0|g to 13/2-; band assignment 
T$DSAM in (|a,n|g). Others: 0.82 ps {I10} (DSAM in ({+28}Si,|apn|g)), 0.8 ps {I4} (RDM in ({+19}F,3pn|g)). Other: |<1.4 ps (RDM in ({+16}O,n2p|g)) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J$1043.9|g |DJ=2, E2 to 13/2+; band assignment 
T$DSAM in ({+19}F,3pn|g). Others: 0.31 ps {I7} (|a,n|g), 0.37 ps {I+4-5} ({+28}Si,|apn|g), |<0.5 ps (RDM in ({+16}O,n2p|g)) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 13/2-, 430.5|g M1+E2 to 15/2-; band assignment 
T$DSAM in ({+19}F,3pn|g). Others: 0.28 ps {I14} (|a,n|g), 0.48 ps {I9} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
J$947.4|g |DJ=(2), (E2) to 15/2-, 517.3|g to 17/2-; band assignment 
T$DSAM in ({+19}F,3pn|g). Others: 0.28 ps {I14} (|a,n|g), 0.36 ps {I+5-7} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: PS
level_comment:
J$1156.1|g |DJ=(2), (E2) to 17/2+; 299.5 |g to (19/2+); band assignment 
T$DSAM in ({+19}F,3pn|g). Others: 0.14 ps {I7} (|a,n|g), 0.18 ps {I4} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: PS
level_comment:
J$1007.9|g |DJ=(2), (E2) to 17/2-; 490.4|g to (19/2-); band assignment 
T$DSAM in ({+19}F,3pn|g). Others: 0.21 ps {I10} (|a,n|g), 0.312 ps {I35} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
J$1061.9|g to (19/2-) and 572.7|g to (21/2-); band assignment 
T$DSAM in ({+19}F,3pn|g). Others: 0.35 ps {I21} (|a,n|g), 0.33 ps {I4} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
J$1214.4|g to (21/2+) and 473.5|g to (23/2+); band assignment 
T$DSAM in ({+19}F,3pn|g). Other: 0.062 ps {I14} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: PS
level_comment:
J$1148.9|g to (21/2-) and 578.0|g to (23/2-); band assignment 
T$DSAM in ({+19}F,3pn|g). Other: 0.187 ps {I+28-21} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
J$1206|g to (23/2-) and 630|g to (25/2-); band assignment 
T$DSAM in ({+19}F,3pn|g). Other: 0.104 ps {I14} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
J$|g's to (25/2+) and (27/2+); band assignment 
T$DSAM in ({+19}F,3pn|g). Other: 0.111 ps {I+21-28} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (29/2-)
level_lifetime_unit: PS
level_comment:
J$|g's to (25/2-) and (27/2-); band assignment 
T$DSAM in ({+19}F,3pn|g). Other: 0.083 ps {I14} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: PS
level_comment:
J$|g's to (27/2-) and (29/2-); band assignment 
T$DSAM in ({+19}F,3pn|g). Other: 0.132 ps {I21} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (33/2+)
level_lifetime_unit: PS
level_comment:
J$1378.1|g to (29/2+); band assignment 
T$effective T{-1/2} (DSAM in ({+19}F,3pn|g)). Other: 0.21 ps {I+3-6} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (33/2-)
level_lifetime_unit: PS
level_comment:
J$|g's to (29/2-) and (31/2-); band assignment 
T$effective T{-1/2} (DSAM in ({+19}F,3pn|g)). Other: 0.159 ps {I28} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_lifetime_unit: PS
level_comment:
J$1428|g to (31/2-); band assignment 
T$effective T{-1/2} (DSAM in ({+19}F,3pn|g)). Other: 0.117 ps {I+21-28} ({+28}Si,|apn|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from Adopted Levels 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
T$reported as 7.180 h {I20} (stat) {I4} (syst); compiler combines uncertainties in quadrature. Value is weighted average of 7.27 h {I7} (stat) {I1} (syst), 7.130 h {I40} (stat) {I3} (syst), 7.150 h {I30} (stat) {I1} (syst), and 7.210 h {I30} (stat) {I1} (syst) all from 361.2|g(t) (2021Ha10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$%(|e)(|b{++})=?, %(|e)(|e)=? (see 1993Hy02 for experimental study of double |b decay) 
$<r{+2}>{+1/2}=4.070 fm {I20} (2004An14) 
J$no hyperfine structure observed in microwave spectroscopy (1950Ge05, 1949St07), consistent with J=0 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$projectile excitation and transient-field technique (1998Sp03). See also 2005St24 compilation 
MOME2$from Coul. ex. (1978Le22). See also 2005St24 compilation 
|b{-2}=0.337 (from ({+16}O,{+14}C)), 0.26 {I4} (from (pol p,p')) 
|bR=1.38 {I14} (from (p,p')) 
J$L(pol p,p')=L(p,t)=2 
T from B(E2)=0.388 {I5} in Coul. ex. other: 7.4 ps 6 (DSA method in in-beam |g). 2001Ra27 adopted 7.08 ps {I15} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$(219|g)(635|g)(|q) in {+74}Br |e (46 min). L(p,p')=L(p,t)=0 
T from B(E2) in Coul. ex. others: 0.83 ns {I14} (|g|g(t) in {+74}Br |e (25.4 min)), 0.52 ns {I6} (centroid-shift in (p,p')) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$projectile excitation and transient-field technique (1998Sp03). See also 2005St24 compilation 
|bR=0.23 {I3} (from (p,p')) 
J$L(p,p')=L(p,t)=2 
T other: 3.3 ps {I15} (Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$projectile excitation and transient-field technique (1998Sp03). See also 2005St24 compilation 
|b{-4}=0.019 {I8} (from (pol p, p')) 
|bR=0.09 {I1} (from (p,p')) 
J$L(p,t)=L(pol p,p')=4 
T from B(E2) in Coul. ex. other: 2.73 ps {I20} (from 1979Ki17 and 1989Ad01, see {+58}Ni({+19}F,3p|g) dataset) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
|b{-3}=0.140 (from ({+16}O,{+14}C)) 
|bR=0.77 {I8} (from (p,p')) 
$B(E3)(Coul. ex.)=0.021 {I5} (2002Ki06,evaluation) 
J$L(p,t)=(pol p,p')=3 


level_energy_unit: KEV
level_spin_parity: (2 : 5)
level_comment:
$L=4 in (p,t) corresponds to 3251 or 3253 level 
J$|g to (3+); absence of |g's to 0+ and 2+ disfavors J|p<4 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T weighted average of 1.2 ps {I6} (1979Ki17), 1.0 ps {I3} (DSA method) (1979Ki17), 1.04 ps {I21}, 0.97 ps {I21} (1989Ad01), 0.53 ps {I11} (DSA method) (1990Co21) and 1.66 ps {I21} (DSA method)(1979Pi05). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.263 ps {I35} (1999Lo17), 0.55 ps {I7} (1979Pi05), 0.67 ps {I7} (1976Ha10), 0.83 ps {I21} (1979Ki17), 0.58 ps {I14}, 0.49 ps {I14} (1989Ad01) and 0.374 ps {I21} (1990Co21) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
T weighted average of 3.6 ps {I4} (1979Ki17), 3.2 ps {I7} (1989Ad01) and 3.5 ps {I14} (DSA method, 1979Pi05) 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
T weighted average of 1.8 ps {I10} (1979Ki17), 1.1 ps {I3} (1989Ad01) and 0.49 ps {I21} (DSA method, 1979Pi05) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.139 ps {I14} (1999Lo17), 0.49 ps {I14} (1979Ki17),0.47 ps {I4} (1976Ha10), 0.37 ps {I7} (1979Pi05), 0.22 ps {I3}, 0.35 ps {I6} (1989Ad01) and 0.243 ps {I21} (1990Co21) 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.83 ps {I56} (1979Ki17), 0.49 ps {I14} (1979Pi05), 0.76 ps {I14} (1989Ad01) and 0.55 ps {I7} (1990Co21) 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: PS
level_comment:
T weighted average of 1.8 ps {I10} (1979Ki17), 1.1 ps {I5} (DSA method, 1979Ki17), 0.42 ps {I14} (DSA method 1979Pi05), 0.58 ps {I10} and 0.9 ps {I3} (1989Ad01) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.062 ps {I21} (1999Lo17), 0.24 ps {I7} (1979Ki17), 0.21 ps {I10} (1979Pi05), 0.28 ps {I4} (1976Ha10), 0.17 ps {I3} (1989Ad01) and 0.111 ps 14 (1990Co21) 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.26 ps {I7} (1999Mu21), 0.24 ps {I7} (1979Ki17), 0.28 ps {I4} (1979Pi05), 0.37 ps {I7}, 0.28 ps {I7} (1989Ad01) and 0.194 ps {I21} (1990Co21) 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.097 ps {I21} (1999Lo17), 0.21 ps {I6} (1979Ki17), 0.24 ps {I10} (1979Pi05), 0.21 ps {I4} (1976Ha10), 0.15 ps {I6}, 0.21 ps {I7} (1989Ad01) and 0.132 ps {I14} (1990Co21) 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_comment:
T DSA method. Weighted average of 0.062 ps {I14} (1999Lo17), 0.09 ps {I5} (1979Ki17), 0.15 ps {I4} and 0.10 ps {I4} (1976Ha10) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2 For constructive interference which is supported by models. For destructive interference Q=-0.14 {I7} (1978Le22) 
B(E2)|^=0.388 {I5} (1978Le22), 0.370 {I15} (1974Ba80). Others: 0.48 {I15} (1970AgZV), 0.44 (1961An07), 0.21 (1956Te26) 
T from B(E2)=0.388 {I5} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)=0.0080 {I5} (1974Ba80) 
BE2 Other: 1962Ga13, 1962Ga10 
T from B(E2)=0.0080 {I5} and adopted branching ratio=0.34 {I3} 


level_energy_unit: KEV
level_comment:
E 1976Or02 report only one level at 2129 {I10} with L=0. It is possible that the group at 2129 corresponds to two separate levels at at 2101 and 2146 


level_energy_unit: KEV
level_comment:
$SUMMED=22.9 
E 1976Or02 report a single level at 3749 {I10} which may correspond to doublet at 3719, 3769 reported by 1977Bo18 
L from 1977Bo18. 1976Or02 give L=(5) for a 3749 {I10} level 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$from 2020Ba08 for the 0|n:2L decay mode for the decay branch of g.s. to g.s. at 90% confidence level. Limits for other decay modes and decay branches were also derived in 2020Ba03 and are listed in the table above. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
J$measured using microwave method (1955Aa06). Parity from L=2 in (d,p), (p,d) and (d,t) 
T$LWM or NRM weighted average of 119.78 d {I7} (revised value in 2012Fi12 from 119.809 d {I66} in 2002Un02; earlier value from NIST 119.80 d {I7}, 1982HoZJ), 119.0 d {I5} (1994Iw04), 119.76 d {I5} (1980Sc07), 119.779 d {I4} (1980Ho17), 120.4 d {I2} (1960Ea02), 119.9 d {I6} (1957Wr37). The uncertainty of 0.004 d given by 1980Ho17 gets increased to 0.04 in the LWM and NRM procedures by adjusting relative weight to 50%. Reduced |h{+2}=2.5 in LWM and 1.7 in NRM. Others: 120 d {I15} (2012Ba12), 115.0 d {I117} (2002He19), 120 d {I1} (1976MaZW), 118.45 d {I25} (1975La16, not included since authors retracted their result), 128 d (1950Co58), 125 d {I5} (Gest and Glendenin, NNES 9, 1924 (1950)), 127 d {I7} (1948Co07), 115 d {I5} (1947Fr08) 
MOMM1$ NMR on oriented nuclei (2001St31). Other: 0.67 {I4} (1974Ca23) 
MOME2$Microwave absorption in gases (1955Aa06). Other: 1988Wh03, measured |g(|q), anisotropy and deduced electric field gradient 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$L=4 in (d,p), (p,d) and (d,t), 133|g to 5/2+ is E2, and |g(|q) in (|a,n|g) 
T$from (p,n|g) in 1974Ag05 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$L=1 in (d,p), (p,d) and (d,t), 287|g to 5/2+ is E1 
T$from average of 1.23 ns {I15} ({+75}Br |e decay), and 1.35 ns {I15} ({+75}As(p,n|g)) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
J$L=1 in (d,p) gives 1/2-,3/2- and |g(|q) in 1991Sa22 ruled out 3/2 
T$from {+75}As(p,n|g) (1968Ri14). Others: 1972Co06, 1974Ag05 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$ on the basis of energies the groups in (p,d) and ({+3}He,|a) can correspond to 1184.188 level also, however if L(d,p)=(1) for an 1187 group suggests that level in (p,d) and ({+3}He,|a) is different from that in (d,p) 
J$L(p,d)=3. Also L({+3}He,|a)=(3) 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2,5/2
level_comment:
J$log| {Ift}=6.3 from 3/2-. L(d,p)=(1) for an uncertain level suggests (1/2-,3/2-). L(d,t)=(1+4) suggests a doublet with J|p=1/2-,3/2- and 7/2+,9/2+. See also comments for 1181.85 level 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_comment:
T$ this value is inconsistent with |d(E2/M1)=-1.5 {I3} which gives B(E2)(W.u.) much larger than RUL=300 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2-)
level_lifetime_unit: PS
level_comment:
J$|g rays to 7/2-, 7/2+ and 3/2- suggest 5/2, 7/2-. log| {Ift}=6.1 from 3/2- supports 5/2 while |g(|q) in (p,n|g) supports 7/2 


level_energy_unit: KEV
level_comment:
E,J$ |g to 13/2+ suggests 9/2+ to 17/2+. This level must be different from 1913, L=(1) level in (p,d) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T$from |b(287|g)(t) using delayed coincidence technique (1969Ra24). Value is 1.29 ns {I15} in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
E$resolved doublet of 286 suggested by authors 
T$from delayed |b|g coincidence with the 287|g (1972Co06). The authors erroneously assigned this half-life to the 286.5 level. Value is 30.0 ns {I4} in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=0.2715 keV {I10}. g|G{-n}=4.5 eV {I2}, |G{-|g}=0.30 eV {I5}, g|G{-n}|G{-|g}/|G=0.28 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=1.0210 keV {I1}. g|G{-n}=2.4 eV {I4}, |G{-|g}=0.30 eV {I5}, g|G{-n}|G{-|g}/|G=0.27 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=1.3750 keV {I7}. g|G{-n}=1.22 eV {I9}, |G{-|g}=0.32 eV {I5}, g|G{-n}|G{-|g}/|G=0.25 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=1.732 keV {I4}. g|G{-n}=9.9 eV {I6}, |G{-|g}=0.27 eV {I6}, g|G{-n}|G{-|g}/|G=0.26 eV {I6} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-n}(lab)=2.303 keV {I24}. g|G{-n}=1.6 eV {I4}, |G{-|g}=0.28 eV {I5}, g|G{-n}|G{-|g}/|G=0.23 eV {I5} 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: NS
level_comment:
T$from |g(t) (1968Ri14). Other: 31 ns {I2} (1974Ag05). 1968Ri14 assigned this T{-1/2} to the 287 level, but it actually corresponds to the 293 level. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$from DSA for 1245.1|g 
J$1991Sa22 propose 3/2,5/2,7/2; but 7/2 is ruled out by a definite |g (see (n,|g)) to (1/2)- 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
T$from DSA for 1491.6|g 
J$ parity from Adopted Levels, based on 906.1|g to 3/2-. Positive parity in 1991Sa22 is in conflict with implied M2 |g to 3/2- 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.1395 fm {I16} (2013An02 evaluation) 
J$microwave absorption method (1950Ge05,1949St07,1933Ra02) consistent with J=0 
$Valence protons in g.s. from transfer reaction measurements (2009Ka06) 
$From (p,t) reactions, 2007Fr10 deduce very similar neutron pair correlations for {+76}Se and {+76}Ge. 
$From ({+3}He,n) reaction, 2013Ro10 deduce no evidence of pairing vibrations for {+76}Se and {+76}Ge, and conclude a simple BCS structure for the ground states of both nuclei 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$from averaged B(E2)|^=0.432 {I+15-6} (2016Pr01 evaluation), based on the following measurements: mean lifetime |t=15.5 ps {I+13-19} (1963Pr04 in (|g,|g')), 13 ps {I2} (1960De08 in (|g,|g')), 33 ps {I22} (1955Co55,|g|g(t)). Coulomb excitation measurements: B(E2)|^=0.419 {I43} (1995Ka29, incident energy above the Coulomb barrier), 0.425 {I9} (1984Zo01, RDM and DSA), 0.423 {I6} (1977Le11), 0.42 {I2} (1974Ba80, superseded by 1977Le11), 0.390 {I40} (1970AgZV), 0.45 {I4} (1962Ga13), 0.480 {I43} (1962St02), 0.42 {I8} (1960An07), 0.43 {I6} (1956Te26). 
MOMM1$transient-field method in Coul. ex. (2019Mc05), with measured g{+76}Se/g{+74}Se=0.96 {I7} for first 2+ states. Others: +0.806 {I46} (1998Sp03,transient-field method in Coul. ex.); +0.81 {I22} (1967Mu10, |g|g(|q,H) in {+76}As |b{+-}), +0.80 {I22} (1969He11, IMPAC in Coul. Ex.) 
MOME2$reorientaton in Coul. ex. (2019He07). Others: -0.34 {I7} (1977Le11, reorientation in Coul. ex.); -0.30 {I5} (1976VoZY) 
$|b{-2}(p,p'): 0.28 {I1} (1993Mo05); 0.310 {I10}, 0.301 {I15} (1984De01); 0.27 {I4}, 0.28 {I4} (1983Ma59); 0.278 {I7}, 0.293 {I7} (1979Ma28); 0.323 (1970He10) 
$|b{-2}(n,n'): 0.28 (1976La12). |b{-2}R=1.52 {I5} (1984Ku09), 1.72 {I5} (1981Br23) 
$|b{-2}(|a,|a'): 0.265, 0.356 (1988Ba35) 
$|b{-2}(Coul. ex.): 0.268 (1977Le11), 0.309 (1974Ba80), 0.319 (1970AgZV) 
$|b{-2}({+16}O,{+14}O): 0.326 (1976Co09) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$from B(E2) in Coul. ex. Otehr: 11 ps {I5} from B(E2) ratios of unresolved 563|g and 559|g (1964By02) in Coul. ex. 
J$E0 transition to 0+. Also |g|g(|q) in {+76}As |b{+-} and {+76}Br |e decay 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field method in Coul. ex. (1998Sp03), measured value of 0.70 {I12} in 1998Sp03 is re-evaluated to 0.61 {I11} in 2020StZV 
MOME2$reorientaton in Coul. ex. (2019He07). 
J$E2 |g to 0+ 
T$from B(E2) in Coul. ex. Other: 3.5 ps {I14} (DSAM in (|a,2n|g)) 
$|b{-2}(p,p')=0.085 {I2} (1993Mo05). |b{-2}(|a,|a')=0.1 (1988Ba35) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field method in Coul. ex. (1998Sp03), measured value of 2.56 {I36} in 1998Sp03 is re-evaluated to 2.2 {I4} in 2020StZV 
MOME2$reorientaton in Coul. ex. (2019He07). 
J$|DJ=2, E2 |g to 2+. Observed anisotropy forbids J=0 
T$from B(E2) in Coul. ex. Others: 0.7 ps {I+5-4} (DSAM in (|a,2n|g)), 1.3 ps {I+5-1} (p,p'|g) 
$|b{-4}(p,p')=0.049 {I10} or 0.012 (1986MoZR), 0.040 (1984De01), 0.014 {I5}, 0.012 {I4} (1983Ma59); |b{-4}(n,n')=0 (1984Ku09) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$M1+E2 |g to 2+; |g rays to 0+ and 4+ and L(p,p')=2 
T$weighted average of 1.18 ps {I+42-24} from DSAM in (n,n'|g) (2019Mu04) and 1.5 ps {I+5-4} from B(E2) for 1229|g in Coul. ex. 
$|b{-2}(|a,|a')=0.07 (1988Ba35) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$from isotropic |g(|q) for 575.3|g and comparison of excitation function data with statistical model calculations using CINDY code in (n,n'|g); spin=0 also from |g|g(|q) in {+76}Br |e decay (2018MoZZ) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 2+ and M1+E2 |g to 4+ 
T$weighted average of 1.8 ps {I4} from DSAM in (|a,2n|g) and 1.6 ps {I2} from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
J$L(p,t)=(0). But L({+3}He,d)=(1+3) from 3/2- suggests (1+,2+,3+) 
E$there may be two separate levels near this energy as indicated by contradictory L(p,t) and L({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 4+; member of rotaional band 
T$weighted average of 0.62 ps {I7} from DSAM in (|a,2n|g) and 0.56 ps {I5} from B(E2) in Coul.ex. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$B(E3)=0.032 {I7} (2002Ki06 evaluation, from Coulomb ex.) 
J$L(d,{+3}He)=4 from 3/2- and L(p,p')=3. Also dipole |g rays to 2+ and 3+; 403|g to 4+ can only be D,E2 from RUL 
T$weighted average of 14 ps {I7} from DSAM in (|a,2n|g) and 8.7 ps {I+15-12} from B(E3) in Coul. ex. and adopted |g branching ratios 
$|b{-3}(p,p')=0.17 {I1} (1993Mo05), 0.15 (1984De01), 0.164 (1979Ma28, 1979Ma41); |b{-3}(|a,|a')=0.183 (1988Ba35); |b{-3}(Coul. ex.)=0.185 (1974Ba80); |b{-3}({+16}O,{+14}O)=0.185 (1976Co09); |b{-3}R(n,n')=0.77 {I5} (1984Ku09). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$(M1) intense 2950|g to 0+; M1+E2 |g to 2+; dipole |g to 0+ from |g(|q) in (|g,|g') 
T$weighted average of 76 fs {I13} from (|g,|g') and 104 fs {I11} from (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_comment:
J$from isotropic |g(|q) for 1815 and 2472 |g rays and comparison of excitation function data with statistical model calculations using CINDY code in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: PS
level_comment:
J$(M1), |DJ=(0) |g to 5- 
T$from DSAM in (n,n'|g). Other: <0.28 ns from (|a,2n|g). Note that the quoted T{-1/2} results in a large reduduced transition strength for any of Mult=E1, M1, or E2 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
J$|gs to 4+ and 1+; |e feeding (log {Ift}=6.4 from 1-). But 0+ proposed in (n,n'|g) from isotropic 2601|g(|q) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: FS
level_comment:
J$|g to 0+ can only be D,E2 from RUL; M1+E2 |g to 2+ 
T$from DSAM in (n,n'|g). Other: 11 fs {I4} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (6,8+)
level_comment:
J$|DJ=0 or 2 |g to 6+ 
T$from DSAM in (|a,2n|g) 1981KiZW give 1.1 ps {I3} but this value is not reported in authors' published work (1984Zo01) 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$|g to 0+; L({+3}He,d)=1+3 for a group at 3295 
E,T$69 fs {I5} for a 3295.28 level in (n,n'|g) could correspond to 3295.70+3297.05 levels in {+76}Br |e decay based on matching of their decaying |g transitions 


level_energy_unit: KEV
level_spin_parity: 1(+),2+
level_lifetime_unit: FS
level_comment:
J$|g to 0+ can only be D,E2 from RUL; L({+3}He,d)=1+3 from 3/2- for a group at 3378 could correspond to 3376.3+3377.2 levels 


level_energy_unit: KEV
level_spin_parity: (2+,3+,4+)
level_lifetime_unit: FS
level_comment:
J$592|g to 3+ can't be pure E1, E2 or M2 based on RUL; |g to 4+. Note that (5+) is proposed in (n,n'|g), but it would require a B(E2)(W.u.)=5.5|*10{+3} {I+7-6} for 592|g, which greatly exceeds RUL=300. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$|e feeding (log {Ift}=6.6) from 1-; |gs to 3+ and 3-; L({+3}He,d)=1+3 from 3/2- for a group at 3467 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$|e feeding (log {Ift}=6.4) from 1-; |g to 0+ can only be D,E2 from RUL; L({+3}He,d)=1+3 from 3/2- for a group at 3598; dipole |g to 0+ in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3+)
level_comment:
J$L({+3}He,d)=1+3 from 3/2- for a group at 3659 and |gs to 1+ and 3+ suggests (1+,2+,3+). But L(p,p')=(4) for a 3655 group suggests (4+) and may indicate a different level 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$L({+3}He,d)=1+3 from 3/2- for a 4729 group gives 1+,2+,3+ and L(p,p')=4 gives 4+. However, J|p=3+ would agree with both if unnatural parity state is populated in (p,p') 


level_energy_unit: KEV
level_comment:
J$|g to 7- suggests (7,8,9) 
T$for a 1287|g, from DSAM 1981KiZW report T{-1/2}=0.6 ps {I1}, but this value is not reported in authors' published work (1984Zo01) 


level_energy_unit: KEV
level_spin_parity: (+)
level_comment:
J$L({+3}He,d)=1+3 from 3/2- allows (1+,2+,3+) but L(p,p')=4 suggests 4+. However, J|p=3+ agrees with both if an unnatural parity state is populated in (p,p') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ 
T$weighted average of 19.2 fs {I32} from (|g,|g') and 17.1 fs {I26} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ 
T$weighted average of 3.90 fs {I29} from (|g,|g') and 4.4 fs {I10} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$evaluators assume that 6242.7 in (pol |g,|g') and 6247.4 in (|g,|g') correspond to the same level 
J$E1 |g to 0+ 
T$other: 4.6 fs {I6} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$evaluators assume that 6250.7 in (pol |g,|g') and 6254.0 in (|g,|g') correspond to the same level 
J$E1 |g to 0+ 
T$weighted average of 5.5 fs {I8} from (|g,|g') and 5.8 fs {I15} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ 
T$weighted average of 2.97 fs {I25} from (|g,|g') and 5.1 fs {I12} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ 
T$unweighted average of 6.6 fs {I13} from (|g,|g') and 2.1 fs {I10} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ 
T$weighted average of 9.6 fs {I16} from (|g,|g') and 10.2 fs {I17} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$evaluators assume that 6970.3 in (pol |g,|g') and 6973.0 in (|g,|g') correspond to the same level 
J$E1 |g to 0+ 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$evaluators assume that 7455.5 in (pol |g,|g') and 7457.6 in (|g,|g') correspond to the same level 
J$E1 |g to 0+ 
T$unweighted average of 5.1 fs {I10} from (|g,|g') and 2.6 fs {I6} from (pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ 
T$weighted average of 1.59 fs {I14} from (|g,|g') and 1.66 fs {I14} from (pol |g,|g') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(lab)=3060, |G=28, IAR of 44, (1)+ level in {+76}As 
$Assignment from 45 level proposed by 1974El07. 1967Fa07 and 1967Co04 incorrectly associated this resonance with {+76}As 2- g.s. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Mean lifetime |t=1700 fs {I+600-350}. This value differs from 9 ps {I+9-3} in 1995Si03 evaluation. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$from isotropic |g(|q) for 575.3|g and comparison of excitation function data with statistical model calculations using CINDY code. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$A |g transition with E|g=238.8 {I5}, I|g=18 reported only by 1977SiZT, not confirmed by 2019Mu04 or in any other study 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$from |g(|q) and comparison of excitation function data with statistical model calculations using CINDY code. 
$A 796|g from this level in 1995Si03 now assigned from 2485 level 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
$Mean lifetime |t=700 fs {I+110-90} 
J$from |g(|q) and comparison of excitation function data with statistical model calculations using CINDY code. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$Mean lifetime |t=1560 fs {I+920-430} 
J$from comparison of excitation function data with statistical model calculations using CINDY code. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
$Mean lifetime |t=1180 fs {I+320-210} 
J$from |g(|q) data 
$Previous 484.8 and 1324 |g rays from this level in 1995Si03 were not observed by 2019Mu04 
$1977SiZT proposed two levels at 2654.0 and 2657.0 but only one level confirmed by 2019Mu04 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: PS
level_comment:
$Mean lifetime |t=560 fs {I+150-101} 
$A |g transition with E|g=1588.0 {I5}, I|g=40 in 1977SiZT is placed by 2019Mu04 as 1586.41|g from 2917 level 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
$|g-branching ratios are not given by 2019Mu04 from this level as 562.3|g is a doublet, and a 335|g from this level in 1995Si03 evaluation is not observed by 2019Mu04 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_comment:
$Mean lifetime |t=141 fs {I11} 
J$from isotropic |g(|q) for 1815 and 2472 |g rays and comparison of excitation function data with statistical model calculations using CINDY code. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$Mean lifetime |t=660 fs {I+120-90} 
J$from 1853|g(|q) 
$Previous 399.5, 897.0 and 3072.0 |g rays from this level were not observed by 2019Mu04 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)|^=0.422 {I5} (1977Le11,1974Ba80). Others: 0.419 {I+6-7} (2019He07), 0.42 {I4} (from E2 matrix element in 1995Ka29), 0.45 {I4} (1970AgZV), 0.48 {I5} (1962St02), 0.45 {I4} (1962Ga13), 0.43 (1956Te26), 0.41 {I4} (1975NeZR). 
MOME2$others: -0.35 {I4} (2019He07), -0.30 {I8} (1976VoZY) 
$|b{-2}=0.309 (1974Ba80), 0.319 (1970AgZV) 
$E2 matrix element (0,0+ to 559,2+)=+0.647 {I33} (1995Ka29) 
$Diagonal E2 matrix element (559,2+ to 559,2+)=-0.45 {I7} (1995Ka29) 
$E2 matrix element (0,0+ to 559,2+)=+0.647 {I5} (2019He07) 
$Diagonal E2 matrix element (559,2+ to 559,2+)=-0.463 {I+52-53} (2019He07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 559,2+)=0.017 {I4}, weighted average of 0.044 {I+23-17} from E2 matrix element in 1995Ka29, 0.0163 {I+30-29} in 2019He07 
$E2 matrix element (559,2+ to 1119,0+)=+0.47 {I+11-10} (1995Ka29) 
$E2 matrix element (from 1216,2+ to 1119,0+)=+0.15 {I+8-18} 
$E2 matrix element (559,2+ to 1119,0+)=+0.285 {I+26-27} (2019He07) 
$Level given by 1964By02, 1995Ka29 and 2019He07 
T$Other: from unresolved (560|g)(559|g) cascade, 1964By02 deduced B(E2)(559,2+ to 1109,0+)/B(E2)(g.s. to 559,2+)=0.042 {I15} from which T{-1/2} is deduced as 11 ps {I5}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 0,0+)=0.0120 {I5}, weighted average of 0.0125 {I14} (1995Ka29) and 0.0119 {I5} (2019He07) 
$B(E2)(from 0,0+)=0.0125 {I14} from E2 matrix element in 1995Ka29 
$B(E2)(from 559,2+)=0.089 {I10} from E2 matrix element in 1995Ka29 
$E2 matrix element (0,0+ to 1216,2+)=+0.112 {I6} (1995Ka29) 
$E2 matrix element (559,2+ to 1216,2+)=+0.667 {I36} (1995Ka29) 
$E2 matrix element (1331,4+ to 1216,2+)=+0.09 {I+12-9} (1995Ka29) 
$Diagonal E2 matrix element (1216,2+ to 1216,2+)=+0.24 {I+6-8} (1995Ka29) 
$B(E2)(from 0,0+)=0.0119 {I5} (2019He07) 
$B(E2)(from 559,2+)=0.0820 {I30} (2019He07) 
$B(E2)(from 1122,0+)=0.033 {I+13-15} (2019He07) 
$B(M1)(from 559,2+)=0.00091 {I+8-7} (2019He07) 
$E2 matrix element (0,0+ to 1216,2+)=+0.110 {I2} (2019He07) 
$E2 matrix element (559,2+ to 1216,2+)=+0.640 {I11} (2019He07) 
$E2 matrix element (1122,0+ to 1216,2+)=+0.182 {I+33-47} (2019He07) 
$Diagonal E2 matrix element (1216,2+ to 1216,2+)=+0.245 {I+57-60} (2019He07) 
$M1 matrix element (from 559,2+ to 1216,2+)=+0.067 {I3} (2019He07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 559,2+)=0.2450 {I50} (2019He07) 
$B(E2)(from 559,2+)=0.26 {I3} from E2 matrix element in 1995Ka29 
$E2 matrix element (559,2+ to 1331,4+)=+1.14 {I6} (1995Ka29) 
$Diagonal E2 matrix element (1331,4+ to 1331,4+)=-0.36 {I+24-14} (1995Ka29) 
$B(E2)(from 1216,2+)=0.00045 {I+122-38} (2019He07) 
$E2 matrix element (559,2+ to 1331,4+)=+1.108 {I+12-11} (2019He07) 
$E2 matrix element (1216,2+ to 1331,4+)=+0.047 {I+44-29} (2019He07) 
$Diagonal E2 matrix element (1331,4+ to 1331,4+)=-0.387 {I+55-53} (2019He07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 559,2+)=0.0017 {I2} in 2019He07 and adopted |g branching ratios and mixing rtios in Adopted Gammas. 
$B(E2)(from 0,0+)=0.0004 {I+12-4} from E2 matrix element in 1995Ka29 
$B(E2)(from 559,2+)=0.00098 {I+30-26} from E2 matrix element (1995Ka29) 
$B(E2)(from 1119,0+)=0.35 {I+44-33} from E2 matrix element in 1995Ka29 
$B(E2)(from 1216,0+)=0.087 {I+64-33} from E2 matrix element in 1995Ka29 
$E2 matrix element (0,0+ to 1788,2+)=+0.02 {I+2-4} (1995Ka29) 
$E2 matrix element (559,2+ to 1788,2+)=+0.07 {I1} (1995Ka29) 
$E2 matrix element (1119,0+ to 1788,2+)=+0.59 {I+30-74} (1995Ka29) 
$E2 matrix element (1216,2+ to 1788,2+)=0.66 {I+21-14} (1995Ka29) 
$E2 matrix element (2026,4+ to 1788,2+)=+0.79 {I+27-13} (1995Ka29) 
$B(E2)(from 0,0+)=0.0016 {I1} (2019He07) 
$B(E2)(from 559,2+)=0.0017 {I2} (2019He07) 
$B(E2)(from 1119,0+)=0.283 {I+22-19} (2019He07) 
$B(E2)(from 1216,2+)=0.014 {I+8-4} (2019He07) 
$B(E2)(from 1331,4+)=0.0190 {I+20-10} (2019He07) 
$B(M1)(from 559,2+)=0.0070 {I3} (2019He07) 
$B(M1)(from 1216,2+)=0.006 {I+3-1} (2019He07) 
$E2 matrix element (0,0+ to 1788,2+)=+0.040 {I1} (2019He07) 
$E2 matrix element (559,2+ to 1788,2+)=-0.093 {I+7-6} (2019He07) 
$E2 matrix element (1119,0+ to 1788,2+)=+0.532 {I+21-18} (2019He07) 
$E2 matrix element (1216,2+ to 1788,2+)=+0.26 {I+7-4} (2019He07) 
$E2 matrix element (1331,4+ to 1788,2+)=+0.418 {I+18-15} (2019He07) 
$M1 matrix element (from 559,2+ to 1788,2+)=+0.186 {I+4-5} (2019He07) 
$M1 matrix element (from 1216,2+ to 1788,2+)=+0.168 {I+4-2} (2019He07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 1216,2+)=0.120 {I11}, weighted average of 0.118 {I11} (2019He07) and 0.169 {I+52-68} (1995Ka29) 
$B(E2)(from 559,2+)=0.0029 {I+43-27} from E2 matrix element in 1995Ka29 
$B(E2)(from 1216,2+)=0.169 {I+52-68} from E2 matrix element in 1995Ka29 
$B(E2)(from 1331,4+)=0.0011 {I+14-7} from E2 matrix element in 1995Ka29 
$E2 matrix element (559,2+ to 2026,4+)=+0.12 {I+7-9} (1995Ka29) 
$E2 matrix element (1216,2+ to 2026,4+)=+0.92 {I+13-21} (1995Ka29) 
$E2 matrix element (1331,4+ to 2026,4+)=+0.10 {I+5-4} (1995Ka29) 
$B(E2)(from 559,2+)=0.0003 {I+8-1} (2019He07) 
$B(E2)(from 1216,2+)=0.118 {I11} (2019He07) 
$B(E2)(from 1331,4+)=0.060 {I+9-6} (2019He07) 
$B(M1)(from 1331,4+)=0.003 {I+2-1} (2019He07) 
$E2 matrix element (559,2+ to 2026,4+)=+0.039 {I+35-7} (2019He07) 
$E2 matrix element (1216,2+ to 2026,4+)=+0.768 {I+36-37} (2019He07) 
$E2 matrix element (1331,4+ to 2026,4+)=+0.73 {I+51-38} (2019He07) 
$M1 matrix element (1331,4+ to 2026,4+)=+0.158 {I+5-3} (2019He07) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 1331,4+)=0.210 {I+20-18}, weighted avearge of 0.261 {I+56-61} from E2 matrix element in 1995Ka29, and 0.2050 {I+200-180} (2019He07). 
$E2 matrix element (1331,4+ to 2262,6+)=+1.53 {I+16-19} (1995Ka29) 
$E2 matrix element (1331,4+ to 2262,6+)=+1.390 {I+64-58} (2019He07) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$B(E2)=0.092 {I+65-26} from E2 matrix element in 1995Ka29 
$E2 matrix element (2026,4+ to 2976,6+)=+0.91 {I+28-14} (1995Ka29) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$B(E2)=0.207 {I+59-36} from E2 matrix element in 1995Ka29 
$E2 matrix element (2262,6+ to 3270,8+)=+1.64 {I+22-15} (1995Ka29) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W (|mb/sr)=0.49 
$At 6|' (lab) this group is the most intense below 3 MeV excitation (Fig. 1 in 1987OgZY) 


level_energy_unit: KEV
level_comment:
L$from 2007Fr10 and other authors 
$|s=7.1 mb/sr (2007Fr10) at 3|' 
$Relative |s=100 at 3|', |s(3|')/|s(22|')=150 (2007Fr10) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$the ground-state pairing in {+76}Se and {+76}Ge appears quite similar with no evidence of pairing vibration, thus no breaking of the BCS approximation for paired protons with an upper limit of 5-7% 
$Measured d|s/d|W (in mb/sr) for g.s.+559,2+ state: 259 {I13} at 6.2|', 242 {I13} at 7.0|', 239 {I15} at 7.8|', 185 {I16} at 8.6|', 139 {I14} at 10.8|', 127 {I13} at 11.5|', 112 {I15} at 12.2|', 72 {I11} at 12.9|', 39 {I14} at 16.4|', 32 {I13} at 21.0|'. 


level_energy_unit: KEV
level_comment:
E$this level can correspond to any of the known 12 or so levels between 4.0 and 4.2 MeV, thus not shown populated explicitly in Adopted dataset 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G (meV)=71 {I11} 
J$ 1+ in Table I of 2013Go19 is a misprint; should be 1- according to e-mail reply of Dec 9, 2013 from P.M. Goddard. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G (meV)=57E1 {I15} 
T$mean lifetime |t=2.9 fs {I2} listed in Table I of 2013Go19 should be 1.15 fs {I30} 


level_energy_unit: KEV
level_comment:
$|b{-2}=0.28 {I1}, |b{-2}R=1.41 (HVM), 1.39 (SRM) (1993Mo05,1986MoZR). |b{-2}=0.310 {I10} (1984De01, asymmetric rotor model); 0.301 {I15} (1984De01, rotational-vibrational model); 0.267 {I40} (1983Ma59, rotor model); 0.281 {I42} (1983Ma59, vibrational model); 0.278 {I7} (1979Ma28, coupled-channel); 0.293 {I7} (1979Ma28,1979Ma41, DWBA). Other: 0.323 (1970He10) 


level_energy_unit: KEV
level_comment:
$|b{-4}=0.049 {I10} (HVM), 0.012 (SRM) (1986MoZR). |b{-4}R=0.069 (SRM) (1986MoZR,1993Mo05). |b{-4}=0.014 {I5} (1983Ma59, rotor model); 0.012 {i4} (1983Ma59, vibrational model); 0.040 (srm,1984De01) 


level_energy_unit: KEV
level_comment:
$|b{-3}=0.17 {I1}, |b{-3}R=0.86 (1986MoZR,1993Mo05); |b{-3}=0.15, |b{-3}R=0.78 (1984De01); |b{-3}=0.16, |b{-3}R=0.86 (1979Ma28,1979Ma41) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated charge radius <r{+2}>{+1/2}=4.1395 fm {I18} (2013An02) 
J$spin from NMR and microwave technique (1949St07,1950Ge05,1953We51, 1954Wa37,1954Da05). Spin and parity from L=1 and Ay(|q) in (pol d,p) 
MOMM1$measured |m=+0.5350422 {I6}, NMR method relative to {+23}Na (1978Ko39,1953We51). Other: |m=0.53507424 {I28} (1978Ko39, relative to {+1}H). 2019StZV re-evaluated |m=+0.53356 {I5} using NMR shielding constants in SeH{-2} from 2013Ja18. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$weighted average of 17.31 s {I8} (1986Ne05), 17.38 s {I8} (1980Jo11), 17.38 s {I9} (1967Yu01). Others: 17.4 s 8 (2009Mu15), 17.58 s 12 (1972Jo05), 17.5 s 2 (1968Ma12), 1967Ab08, 17.70 s 3 (1963Al32), 17.5 s 2 (1963Ka34), 1963Ve13, 18.83 s 4 (1962Ma38), 17.5 s 5 (1952Ru10), 17.5 s 18 (1951Ca23), 17.4 s 2 (1950Fl62), 17.5 s 10 (1949Gi04), 17.5 s 3 (1947Ar01). Values from 1972Jo05, 1963Al32 and 1962Ma38 are precise but systematically higher than a group of values centered around 17.4 s from many other measurements, thus not included in the averaging procedure. Weighted average of values from 1986Ne05, 1980Jo11, 1972Jo05, 1967Yu01 and 1963Al32 (uncertainty increased to 0.09) is 17.45 s 7 with reduced |h{+2}=3.3. High value from 1962Ma38 is an outlier. 
J$E3 |g to 1/2- (see {+77}Se IT decay and {+76}Se(n,|g)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to 1/2- 
T$from (|a,n|g)(1990KuZS; RDDS method). Other: 25 ps {I9} from B(E2) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$E1 |g to 7/2+, |DJ=2, E2 |g to 1/2- 
T$from |g|g(t) in {+77}Br |e decay (1988Mo16; time-differential perturbed angular correlation technique). Others: 1984Za08 (9.56 ns 10), 1964En01, 1963Ly01 
MOMM1$DPAC method (1984Za08). Other: +1.20 {I15} (1964En01). 
MOME2$DPAC method (1983Un02). Value of 1.1 {I5} is re-evaluated to +0.76 {I5} in 2008Py02 and 2016St14. Other: 1996Lo11, measured |g|g(|q,H), deduced quadrupole interaction and electric field gradient. 
$g-factor (1984Za08) and quadrupole coupling constants (1983Un02) measured by time differential perturbed angular correlation method. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
T$1990KuZS reported T{-1/2}=7 ps to 35 ps from (|a,n|g). This value is inconsistent with T{-1/2}>212 ps from B(E2)(W.u.)<300 (RUL) for 125.8|g, thus T{-1/2} value is considered suspect. 
J$L=2 and Ay(|q) in (pol d,p) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L=1 and Ay(|q) in (pol d,p); L(p,d)=1; excited in (|g,|g') from 1/2- {+77}Se g.s. In ({+3}He,|a) (2007ScZX), cross section for a 522 level does not allow L=1, instead L=3 is favored implying 5/2-,7/2-, which is in disagreement with results form (pol d,p) and with L(d,p)=1 in 2007ScZX. Perhaps there is a different level populated in ({+3}He,|a), although, the evaluator considers this as a less likely possibility at low-energy excitations, where the level density is not high 
T$from (|g,|g') (1995Kh02). Other; 7 ps {I+7-5} from B(E2) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$L=1 and Ay(|q) in (pol d,p). The circular polarization measurement in {+76}Se(n,|g) also supports 1/2- 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$log| {Ift}=7.56 from 3/2- and gammas to 1/2+, 1/2-, 5/2+, and 5/2-. L(d,p)=1,2 for an 1187 group may correspond to a doublet 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$from (n,n'|g) (1991Ko45,DSAM) 
J$primary |g from 1/2+ and |g to 7/2-. L(p,d)=(1) favors 3/2-; L(d,p)=1,2 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
J$strong primary transition from 1/2+ capture state. Circular polarization in {+76}Se(n,|g) (1971Kn06) favors 1/2- 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_comment:
E$ this level is associated with either or both of the two 3-qp bands, one based on 2818, (15/2-) and the other on 3015, (17/2-) 
J$|DJ=1 |g to (19/2-) 


level_energy_unit: KEV
level_comment:
J$L=(d,p)=(2) and |g to 1/2- give 3/2+ but a transition to 7/2- favors 3/2- instead. It is possible that the levels populated in the two reactions are different 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E$from least-squares fit, in agreement with S(n)=7418.86 {I6} (2017Wa10) 
J$s-wave capture in {+76}Se g.s. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from weighted average of 17.31 s {I8} (1986Ne05), 17.38 s {I8}(1980Jo11), 17.38 s {I9} (1967Yu01). Others: 2009Mu15, 1972Jo05, 1968Ma12, 1967Ab08, 1963Al32, 1963Ka34, 1962Ma38, 1952Ru10, 1951Ca23, 1950Fl62, 1947Ar01. See details in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$1990KuZS quote T{-1/2}=7 ps to 35 ps. This value is inconsistent with T{-1/2}|?250 ps deduced from RUL(E2)=300 for 125.5|g 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$from 1995Kh02. Other: 90 ps {I+3-4} (1969Bo29). 1995Kh02 pointed out an error in the integrated |s given by 1969Bo29, and T{-1/2} should be 9 ps instead of 90 ps. The value of (2J+1)|G|g{-0}|G|g/2|G: 4.1|*10{+-8} {I+35-10} quoted by 1969Bo29 is probably low by an order of magnitude 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from the Adopted Levels 
E$not directly excited in Coulomb excitation. Populated indirectly through 87|g from 250 level (1962Ro03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.186 {I20} (1970AgZV), 0.13 {I3} (1968An12), 0.177 {I16} (1965Ro09). 
T$from B(E2) in Coulomb excitation. 1963Ly01 give 48 ps {I35} (pulsed beam method) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
BE2$weighted average of 0.0106 {I20} (1970AgZV), 0.0094 {I26} (1965Ro09), 0.0125 {I20} (1963Ly01). Other: 0.0043 {I15} (1968An12) 
T$from |g|g(t) in {+77}Br |e decay. From B(E2)=0.0111 {I12} and branching=0.653 {I7} one gets T{-1/2}=10.3 ns {I11}. From pulsed beam technique, 1963Ly01 obtained 9.1 ns {I8} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 from 440|g(|q) 
BE2$weighted average of 0.228 {I20} (1970AgZV), 0.21 {I4} (1968An12), 0.259 {I17} (1962Ro03) 
T$from B(E2). 
$g-factor=0.41 {I11} (1970RoZS) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
BE2$from 1962Ro03. 1968An12 give 0.027 {I7} 
T$from B(E2), T{-1/2}=7 ps {I+7-5}. This is quite discrepant from the value obtained in (|g,|g'). The discrepancy could be due to error in B(E2) or in the |G factor in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1988Mo16). Other: 9.3 ns {I4} (1964En01), 9.56 ns {I10} (1984Za08). 
$g-factor=+0.447 {I10} (1984Za08). Other: +0.48 {I6} (1964En01). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=2.569 keV {I2}, g|G{-n}=14.240 eV {I85}, |G{-|g}=0.230 eV {I46}, g|G{-n}|G{-|g}/|G=0.230 eV {I46} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=3.381 keV {I3}, g|G{-n}=14.0 eV {I9}, |G{-|g}=0.25 eV {I5}, g|G{-n}|G{-|g}/|G=0.25 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=4.313 keV {I31}, g|G{-n}=4 eV {I2}, |G{-|g}=0.21 eV {I5}, g|G{-n}|G{-|g}/|G=0.20 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 3/2-&5/2-
level_comment:
E$unresolved doublet (239 and 250 levels in Adopted Levels) 
S$other: 0.180 for L=1 component (2007ScZX) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W=0.75 mb/sr 
L$assignment from 2007ScZX, cross section value does not allow L=1. But this result is in disagreement with L(d,p)=1 in 2007ScZX and in other studies. It is possible that the level populated in ({+3}He,|a) is different from that in the other studies, although, the evaluator considers this as a less likely possibility 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ <r{+2}>{+1/2}=4.1407 fm {I18} (2004An14 evaluation) 
BE2$weighted average of 0.325 {I45} (2003Ha15), 0.392 {I66} (deduced from T{-1/2}=8.3 ps {I14} (1987Sc07),RDM measurement in (|a,2n|g)), 0.327 {I7} (1977Le11), 0.385 {I35} (1962St02), 0.35 {I3} (1962Ga13), 0.36 {I7} (1960Le07) and 0.36 {I5} (1956Te26). All values, except for 1987Sc07, are from cross sections and yields in Coulomb excitation. Other: 0.335 {I9} (2001Ra27 evaluation) 
T$from B(E2)=0.332 {I7}. Other: 9.69 ps {I26} (2001Ra27 evaluation) 
J$from L(t,p)=2. Also, L=2 and vector analyzing power in (p,p') 
MOMM1$from transient-field technique in Coul. ex. (1998Sp03), sign from 1969He11. Other: +0.78 {I22} (1969He11,IMPAC technique). See also 1989Ra17 evaluation and 2005St24 compilation 
MOME2$from Coulomb excitation (2003Ha15). Others:-0.26 {I9} (1977Le11), -0.30 {I11} (1976VoZY). See also 1989Ra17 evaluation and 2005St24 compilation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$from transient-field technique in Coul. ex. (1998Sp03). See also 2005St24 compilation 
MOME2$from Coulomb excitation (2003Ha15) 
T$from B(E2) in Coulomb excitation. Other: 3.8 ps {I10} from recoil-distance method in (|a,2n|g) (1987Sc07). Weighted average of the two values is also 4.2 ps {I3} 
J$from L(t,p)=2. Also, L=2 and vector analyzing power in (p,p') and J=2 from circular polarization in (n,|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$from transient-field technique in Coul. ex. (1998Sp03). See also 2005St24 compilation 
J$|g(|q) and linear polarization in (|a,2n|g) 
T$weighted average of 1.05 ps {I5} from B(E2) in Coul. ex. and 0.9 ps {I2} from DSA in (|a,2n|g) (1987Sc07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2; L(p,p')=2; J=2 from circular polarization in (n,|g) 
T$from B(E2)(|^) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$L(t,p)=0. But L(d,p)=1 for E=2360. It is possible that the (t,p) and (d,p) reactions correspond to the 2335 level 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
BE3$from Coul. ex. 
J$L(p,p') and vector analyzing power in (p,p') 
T$recoil-distance method in (|a,2n|g) (1987Sc07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$L(t,p)=4, L(p,p')=4. J|p inconsistent with possible primary transition in (n,|g) and log| {If{+1u}t} from 2- small, but decay mode of 2682 level is consistent in (n,|g), |b{+-}, and (p,p'|g); so only one level appears to Be involved 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
J$|g(|q) and polarization in (|a,2n|g) (1987Sc07). E2 |g from 6- and E1 |g to 4+ 
T$recoil-distance method in (|a,2n|g) (1987Sc07). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$|g(circ pol) in (n,|g); |g to 0+ 
E$from primary transition in (n,|g). The 757 and 2140 |g's are not seen in (n,|g), and the 2156|g is not seen in (n,n'|g) or (p,p'|g). It is possible that the |g transitions define more than one level, in particular, the 2753 {I10}+ level reported in (t,p) is perhaps being excited. Transitions from the 2754.46 level are both included in the least-squares fit for determining the energies of other levels 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
T$recoil-distance method in (|a,2n|g) (1987Sc07) 
J$L(t,p)=5; |g(|q) and polarization measurements in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L(p,p')=2 
E$from primary transition in (n,|g). Deexciting transitions 3241.8 and 2627.87 (doubly placed) are placed by 1979BrZE, with additional transitions reported and placed by 1987Su05 (all from (n,|g)), and give excitation energies of 3242.8 {I3}, 3242.8 {I2}, 3241.5 {I2}, 3243.3 {I3} and 3243.4 {I1}. The spread in excitation energies suggests that either one or more transitions are misplaced, or that there is more than one level at this energy. Transitions of energy 2629 and 3243 are reported also in (n,n'|g) and placed from a 3242 level. The 1484|g is not reported in (n,n'|g). Transitions from this level are not used in the least-squares fit for determining the energies of the other levels. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$|g(|q) and polarization measurements in (|a,2n|g) 
E$the 8+ member of |b band is either 3831 or 4121 level 
T$DSA in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|g(|q) and polarization data in (|a,2n|g) 
E$this level may Be the 8+ member of |b band, although, 3831 level is presently assigned as the 8+ member 
T$DSA in (|a,2n|g). Upper limit is <0.35 ns from pulsed-beam |g-timing in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$an unplaced 6274.40 {I16} transition in (n,|g), if a primary, would define a level at 4222.75 {I17}, but the transition would Be 1- to 3- 
J$L(t,p)=3 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$an unplaced 6091.81 {I18} transition in (n,|g), if a primary, would define a level at 4405.65 {I19} 
J$L(t,p)=2 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$an unplaced 6077.24 {I18} transition in (n,|g), if a primary, would define a level at 4420.22 {I19} 
J$L(p,p')=(2) 


level_energy_unit: KEV
level_spin_parity: (0+&4+)
level_comment:
E$an unplaced 5932.03 {I21} transition in (n,|g), if a primary, would define a level at 4565.45 {I22} 
J$L(t,p)=0+4 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$0.87 ps {I21} from DSA and 0.97 ps {I28} recoil-distance method (1987Sc07) with adopted value of 0.9 ps {I2} 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: NS
level_comment:
T$adopted by 1987Sc07. Recoil-distance method gives 3.8 ns {I7}, pulsed beam |g-timing method gives 2.7 ns {I3} 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$this level may be the 8+ member of |b band, although, 3831 level is presently assigned as the 8+ member 
T$upper limit is <0.35 ns from pulsed-beam |g-timing method (1987Sc07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$|g|g(|q) is consistent only with J=2. |g(circ pol) is consistent with J=2 or, less likely, with J=1 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$|g|g(|q) is consistent only with J=2 or 4. J=4 is inconsistent with possible primary transition. See comment in adopted levels 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$from primary transition. The deexciting transitions placed by 1987Su05 give excitation energies of 2754.6 {I3} and 2755.2 {I4}, and label the level with E=2754.6. One or more of these transitions may be misplaced, or there may be more than one level involved. The transitions from this level are not included in the least-squares fit for determining the energies of the other levels 
J$|g(circ pol) is consistent only with J=2 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$from primary transition. Deexciting transitions with energies 3241.8 {I4} and 2627.87 (doubly placed) are placed by 1979BrZE. The additional transitions are reported and placed by 1987Su05 and lead to excitation energies of 3242.8 {I3}, 3242.8 {I2}, 3241.5 {I2}, 3243.3 {I3}, and 3243.4 {I1}. The spread in excitation energies suggests either that one or more transitions are misplaced, or that there is more than level at this energy. Transitions of energy 2629 and 3243 are reported also in (n,n'|g) and placed from a 3242 level. The 1484|g is not reported in (n,n'|g). Transitions from this level are not used in the least-squares fit for determining the energies of the other levels 


level_energy_unit: KEV
level_comment:
$|b{-4}R=0.005 (symmetric rotor model) (1993Mo05) 
E,L$1503 with adopted J|p=4+ and 1498 with adopted J|p=0+ are not resolved. 1986Og01 report L=4, suggesting that, at 65 MeV, the 1503 level is populated more strongly than the 1498 level. L=0+4 is reported by 1984De01 at E=16 MeV 


level_energy_unit: KEV
level_comment:
E,L$could include the adopted 2327 level with J|p=1+,2+ as determined from |g decay, and the adopted 2335 level with J|p=0+. L=2 reported by 1986Og01 suggests that, at 65 MeV, the 2327 level is more strongly populated than the 2335, and that J|p(2327)=2+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|b{-3}R=0.821 (harmonic vibrator model) (1993Mo05) 
J$from L transfer and vector-analyzing power (1984De10) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$others: -0.26 {I9} (1977Le11), -0.30 {I11} (1976VoZY) 
$ <Q{+2}>=0.26 {I14}, |b{-rms}=0.24 {I6} (2003Ha15) 
G$other: +0.35 {I9} (1969He11 using T{-1/2}=10.1 ps {I3}) 
BE2$weighted average of 0.325 {I45} (2003Ha15), 0.327 {I7} (1977Le11), 0.385 {I35} (1962St02), 0.35 {I3} (1962Ga13), 0.36 {I7} (1960Le07) and 0.36 {I5} (1956Te26) 
$E2 matrix element=+0.57 {I4} (2003Ha15) 
$E2 diagonal matrix element=-0.27 {I9} (2003Ha15). Other: -0.34 {I12} (1977Le11) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ <Q{+2}>=0.09 {I7}, |b{-rms}=0.14 {I5} (2003Ha15) 
BE2$from g.s. 
BE2$others: 0.0065 {I15} (2003Ha15), 0.0105 {I35} (1962Mc03), 0.0140 (1962Ga13) 
$B(E2)(from 613.8,2+)=0.205 {I36} 
$From 613.8,2+: E2 matrix element=+0.45 {I4}; M1 matrix element=+0.07 {I1} (2003Ha15) 
$From g.s.: E2 matrix element=+0.08 {I1} (2003Ha15) 
$E2 diagonal matrix element=+0.23 {I12} (2003Ha15) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$From 613.8,2+: E2 matrix element=+0.18 {I6} (2003Ha15) 
$B(E2): from 613.8,2+. Other: B(E2)(from 613.8,2+)=0.0065 {I+50-36} (2003Ha15) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$B(E2): from 613.8,2+. Other: B(E2)(from 613.8,2+)=0.131 {I+20-18} (2003Ha15) 
$From 613.8,2+: E2 matrix element=+0.81 {I6} (2003Ha15) 
$E2 diagonal matrix element-0.90 {I20} (2003Ha15) 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
$B(E1, 699.7|g)/B(E2, 382.6|g)=0.0040|*10{+-6} fm{+-2} {I9}. Compiler obtains 0.0039|*10{-4} b{-1} {I5} 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
$B(E1, 571.5|g)/B(E2, 564.4|g)=0.089|*10{+-6} fm{+-2} {I22}. Compiler obtains 0.090|*10{+-4} b{-1} {I14} 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
$B(E1, 383.0|g)/B(E2, 633.1|g)=0.163|*10{+-6} fm{+-2} {I40}. Compiler obtains 0.163|*10{-4} b{-1} {I15} 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
$B(E1, 581.1|g)/B(E2, 888.9|g)=0.181|*10{+-6} fm{+-2} {I44}. Compiler's note: 581.1|g feeds 8+ level in Band #1 in Fig. 5. There is no E1 |g to band #3. Compiler obtains 0.30|*10{-4} b{-1} {I5} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: Y
level_comment:
J$microwave absorption (1953Ha50). L(p,d)=4 and E3 |g from 1/2-. Probable configuration=(|ng{-9/2}{+-3}){-7/2+} (1953Ha50) 
MOMM1,MOME2$from microwave absorption (1953Ha50,1954Bi40), recalculated by 1962Ko22 
T$unweighted average of 2.78|*10{+5} y {I18} (2014Do20) (AMS and liquid scintillation counting), 3.27|*10{+5} y {I8} (2010Jo09, inductively coupled plasma optical emission spectrometry (ICP-OES) and liquid scintillation counting); 3.77|*10{+5} y {I19} (2007Bi01, inductively coupled plasma mass spectrometry (ICP-ms) and liquid scintillation counting (LSC)). In 2014Do20, source was obtained from 57% enriched {+78}Se irradiated with neutrons. In 2010Jo09 and 2007Bi01, source was obtained from chemical separation of {+79}Se fission fragment from reactor fuel. 2010Jo09 accounted for contaminants present in the sample by |g counting whereas 2007Bi01 and 2014Do20 did not seem to correct for the presence of contaminants. The weighted average is 3.26|*10{+5} y {I18}, but the reduced |h{+2}=7.2 as compared to the critical |h{+2}=3.0 at 95% confidence level. 
T$others: earlier values from the same research group as 2014Do20 using different methods: 9.15|*10{+4} y {I45} (2010JiZZ, AMS spectrometry), 2.95|*10{+5} y {I38} (2002Ji07,2001Ji04,AMS (accelerator mass spectrometry); 2.80|*10{+5} y {I36} (2002He19, AMS and x-ray detection method), 2.9|*10{+5} y {I5} (revised by 2001Ji04 from 1.24|*10{+5} y {I19} in 2000He19); 11|*10{+5} y {I2} (1997Ji07,1996Ji06); 11.3|*10{+5} y {I17} (1997Li44,chemical method); 4.8|*10{+5} y {I4} (1995Yu08,chemical method). Earliest measurement: |<6.5|*10{+5} y (T{-1/2}|<6.5|*10{+4} y reported by 1949PaZZ corrected by 1993HeZW) for a possible arithmetic error by a factor of 10). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$L(pol d,p)=L(p,d)=1 and L(t,p)=0 from 1/2-. Probable p{-1/2} orbital 
T$from 1990Ab02. Others: 3.9 min {I2} (1969Mu03), 3.91 min {I5} (1954Yt03), 3.88 min {I6} (1953Cu33), 3.5 min {I2} (1952Ru10), 3.9 min {I1} (1950Fl62) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_uncertain: ?
level_comment:
Level interpreted from L(d,p)=1+4 for E=128 {I5} group corresponding to 137, 9/2+ level. No other reaction supports existence of this level 
J$L(pol d,p)=1+4 for E=128 {I5} group 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_comment:
J$L(t,p)=(1) from 1/2- 
From energy values, it is possible that 750 is the same as the 729 level, but J|p values deduced from L-transfers indicate two separate levels 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
T$1988KuZP give 1.18 ps {I+35-21} from DSA method in (|a,n|g) 
J$RUL and |g(|q) of |gs to 5/2-, 7/2+ and 9/2+ give 7/2-. Excitation function consistent with 7/2 or 9/2 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
E$uncertain in {+79}As |b{+-} decay and (p,d) 
J$primary |g from 1/2+ in (n,|g) and |DJ=0,1 |g to 5/2- (from |g(|q) in (|a,n|g)); L=(1) in (d,p) for 1080 and/or 1089 levels 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
J$L(p,d)=4 and excitation function in (|a,n|g). |g(|q) of |gs to 7/2+ and 9/2+ consistent with 9/2+ 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
J$|DJ=0,1 |g to 7/2+ and excitation function. |g(|q) of |gs to 5/2- and 9/2+ are consistent with 9/2- 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$doublet in (p,d) and uncertain in (d,p) 
J$|DJ=0,1 |g to 5/2- (from |g(|q) in (|a,n|g)). Excitation function in (|a,n|g) consistent with 7/2. Also possible |gs to 3/2- and 9/2+ 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$primary |g from 1/2+ in (n,|g). |DJ=0,1 |g (from |g(|q) in (|a,n|g)) to 5/2-. Excitation function in (|a,n|g) consistent with 3/2, 5/2 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J$L(p,d)=3 
E$from energy matching, 2092 in (p,d) and 2110 in (d,p) may correspond to the same level but L values indicate two separate levels. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2,5/2+
level_comment:
J$primary |g from 1/2+ and |g to 5/2-. L(t,p)=2 from 1/2- for for a 3176 group and L(d,p)=(2) for a 3182 group would limit J|p=3/2- for one of the two levels (3171 and 3177) and J|p=(3/2+,5/2+) for the other 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E$S(n)+E(n), where S(n)=6962.83 {I13}, E(n)(lab)=0.3830 {I1} 
J$s-wave capture in 0+ g.s. of {+78}Se 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
T$13 ps {I+6-4} (from RDDS method for 790|g,1991KuZY). But from DSA method for 653|g, 1988KuZP give 1.18 ps {I+35-21} 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: PS
level_comment:
Two separate levels near 2182 are suggested by 1987FuZO and 1991KuZY. T{-1/2} from DSAM for 925|g (1991KuZY) 


level_energy_unit: KEV
level_comment:
E$doublet with 30% L=2 and 70% L=4 
S$for L=2, S=0.018 for 3/2+ and 0.015 for 5/2+. For L=4, S=0.143 for 7/2+ and 0.083 for 9/2+ 


level_energy_unit: KEV
level_comment:
E$reported by 1978Kl12 only. Doublet with 10% L=2 and 90% L=4. 
S$for L=2, S=0.020 for 3/2+ and 0.017 for 5/2+. For L=4, S=0.279 for 7/2+ and 0.160 for 9/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=1.2 ps {I2}. This value is compared with |t=1.7 ps {I+5-3} in 1988KuZP (Program and Theses, Proc. 38th Ann. Conf. Nucl. Spectrosc. Struct. At. Nuclei, Baku, p.65 (1988), previous report by the same group as 1991KuZY). Note that 1991KuZY report |t=19 ps {I+8-6} from Recoil-distance Doppler-shift (RDDS) method 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.5 ps {I1}. This value can be compared with |t=1.2 ps {I+6-4} in 1991KuZY 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$<r{+2}>{+1/2}=4.1399 fm {I19} (2004An14) 
$ 2|b decay: theoretical calculations: 2005Do07, 2001Ka15, 2000Bo05. No experimental information is available. 
$ Others for 2|b decay (theory): 1988Si03, 1985Gr11 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,p')=2 
T$from B(E2) taken from evaluation of 2001Ra27. Other: 8.3 ps {I8} (from (|g,|g'),1976KaYY) 
MOMM1$ transient-field technique in Coul. Ex. (1998Sp03). Other: 0.84 {I24} (IMPAC in Coul. ex.,1969He11,1989Ra17) 
MOME2$reorientation effect in Coul. ex. (1977Le11). Other: -0.35 {I12} (1976VoZY) 
$ |b{-2}(p,p')=0.21 (1993Mo05), 0.193 (1988Ba35,1986Og01), 0.22 {I1} (1986MoZR), 0.229 {I15} (1984De01), 0.195 {I30} (1983Ma59), 0.210 {I15} (1979Ma28), 0.234 (1970He10). 
$ |b{-2}(n,n')=0.225 (1990Go13), 0.244 {I10} (1988Ba35,1984Ku09), 0.265 {I20} or 0.293 {I25} (1984De01), 0.25 (1979Ef01,1976La12) 
$ |b{-2}(|a,|a')=0.255 or 0.190 (1988Ba35) 
$ |b{-2}(Coul. ex.)=0.232 {I2} (1977Le11), 0.224 {I2} (1974Ba80), 0.245 (1962St02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$ transient-field technique in Coul. Ex. (1998Sp03). 
1449 and 1479 are unresolved in (|a,|a') 
J$L(p,p')=2 and |g|g(|q) in (|g,|g') 
|b{-2}(p,p')=0.047 (from |b{-2}R=0.25 (1986Og01)), 0.082 {I20} or 0.065 {I5} (1986MoZR) 
|b{-2}(|a,|a')=0.05 (1988Ba35). |b{-2}(Coul. ex.)=0.054 (1974Ba80) 
T$other: 0.2 ps {I+24-3} (DSAM in (n,n'|g)) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$ transient-field technique in Coul. Ex. (1998Sp03). 
J$L(p,p')=4 
|b{-4}(p,p')=-0.033 (from |b{-4}R=-0.18 (1986Og01)), -0.026 {I8} or -0.034 {I10} (1983Ma59). Others: 1984De01, 1986MoZR 
|b{-4}(|a,|a')=0.07 or -0.02 (1988Ba35) 
T$other: 0.7 ps {I+10-4} (DSAM in (n,n'|g)) 


level_energy_unit: KEV
level_spin_parity: (0)+
level_comment:
J$L(t,p)=0 but L(p,p')=2. |g|g(|q) in (|g,|g') gives J=0 or 2; 0+ supported by comparison of experimental and theoretical yields in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|g|g(|q) in (|g,|g') and L(p,p')=2 
T$from DSAM in (n,n'|g). Other: 2.8 ps {I+14-7} or 7 ps {I+9-3} (from B(E2) in Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
J$L(t,p)=1, but |g|g(|q) in (|g,|g') suggests J=2; 2+ also supported from comparison of experimental and theoretical yields in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$primary transition in (|g,|g') from 1(-); 0+ from comparison of experimental and theoretical yields in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(p,p')=L(t,p)=3 
$B(E3) adopted in evaluation by 2002Ki06 from (p,p') (1993Mo05, 1986Og01,1979Ma28). Other: B(E3)=0.0084 {I14} from Coul. ex. (1974Ba80) 
$Average |b{-3}(from inelastic scattering)=0.154 from |b{-3}(|a,|a')=0.161 (1988Ba35); |b{-3}(n,n')=0.151 {I10} (from b3r=0.78 {I5},1984Ku09); |b{-3}(p,p')=0.163 (1993Mo05), 0.124 (deduced by 1988Ba35 from 1986Og01), 0.144 (deduced by 1988Ba35 from 1984De01), 0.17 {I1} (1986MoZR), 0.167 (1979Ma28). |b{-3}(from B(E3) in Coul. ex.)=0.083 


level_energy_unit: KEV
level_spin_parity: (2+,1+)
level_comment:
J$ 2+ from |g|g(|q) in (|g,|g') and L(p,p')=(2); 1+ from comparison of experimental and theoretical yields in (n,n'|g) 


level_energy_unit: KEV
level_comment:
$|e=0.48 
$ d|s/d|W=6.0 mb/sr {I15} for a possible doublet 
$ |e: 0.14 for L=2 component and 0.34 for L=6 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: PS
level_comment:
J$from HFM analysis (1999Ko46); (1+,2+) in 'adopted levels' 
T$other: 0.19 ps {I+9-4} (1989Do14,1987KaZR) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
T$other: 0.8 ps {I+10-4} (1989Do14). It should be noted that (T{-1/2}=0.035 ps {I+35-21}) was reported (1987KaZR) in an earlier communication by the authors of 1989Do14 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: PS
level_comment:
J$from HFM analysis (1999Ko46); (1+,2+) in 'adopted levels' 
T$other: 0.021 ps {I14} (1989Do14,1987KaZR) 
T$ ?? CHECK: 1999Ko46 QUOTE 0.042 21 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
J$from HFM analysis (1999Ko46); (2+) in 'adopted levels' 
T$from 1989Do14; not measured by 1999Ko46 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
|b{-2}=0.242 {I10} or 0.247 {I10} (deduced by 1988Ba35 from |b{-2}R=1.25 {I5} (1984Ku09)), 0.25 (1976La12). Data from 1976La12 reanalyzed by 1984De01 and 1981Br23 giving |b{-2}R=1.34 {I4} (1981Br23); |b{-2}=0.265 {I20} or 0.293 {I25} (1984De01). Others: 0.225 (1990Go13), 0.25 (1979Ef01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$ |b{-2}=0.193 (deduced by 1988Ba35 from |b{-2}R=1.03 (1986Og01)), 0.21 (1993Mo05) from |b{-2}R=1.041 or 1.062, 0.21 {I1} or 0.22 {I1} (1986MoZR), 0.228 {I15} or 0.230 {I15} (1984De01), 0.196 {I30} or 0.194 {I30} (1983Ma59), 0.210 {I5} (1979Ma28), 0.234 (1970He10). Two values correspond to vibrational and rotational model calculations, respectively 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
|b{-2}=0.047 (deduced by 1988Ba35 from |b{-2}R=0.25 (1986Og01)), 0.087 {I20} or 0.065 {I5} (1986MoZR) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$ |b{-4}=-0.033 (deduced by 1988Ba35 from |b{-4}R=-0.18 (1986Og01)), |b{-4}R=-0.121 (1993Mo05), -0.025 {I10} or -0.051 {I9} (1986MoZR), 0.013 (1984De01), -0.026 {I8} or -0.034 {I10} (1983Ma59). Two values correspond to rotational and vibrational model calculations, respectively 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$ |b{-3}=0.163 (deduced by 2002Ki06 from |b{-3}R=0.842 (1993Mo05)), |b{-3}=0.124 (deduced by 1988Ba35 from |b{-3}R=0.66 (1986Og01)), 0.17 {I1} (1986MoZR), 0.144 (deduced by 1988Ba35 from |b{-3}R=0.742 (1984De01)) 0.167 (1979Ma28) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ g factor from transient-field technique in Coul. ex. (1998Sp03); Others: 0.39 {I12} (1969He11, IMPAC in Coul. ex. ). Value given by 1969He11 has been adjusted for T{-1/2}(666 level)=8.56 ps 
$Q=-0.31 {I7} (1977Le11). Other: -0.35 {I12} (1976VoZY). Q measured by reorientation method in Coul. ex. 
$ B(E2)=0.252 {I4} (1977Le11). Others: 0.236 {I+28-24} (1995Ka29), 0.248 {I5} (1974Ba80), 0.24 {I3} (1970AgZV), 0.283 {I25} (1962St02), 0.26 {I2} (1962Ga13), 0.23 {I5} (1960An07), 0.23 {I3} (1956Te26) 
|b{-2}=0.229 {I2} (1974Ba80), 0.232 {I2} (1977Le11), 0.245 (1962St02) 
$E2 matrix element (666,2+ to 0,0+)=+0.486 {I+28-25} (1995Ka29) 
$Static E2 matrix element (666,2+ to 666,2+)=-0.26 {I+4-3} (1995Ka29) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ g factor from transient-field technique in Coul. ex. (1998Sp03); 
|b{-2}=0.054 
$ B(E2)(from g.s.)=0.0134 {I4} (1974Ba80), 0.0112 {I13} (1995Ka29) 
$ B(E2)(from 666,2+)=0.038 {I3} (1974Ba80), 0.029 {I3} (1995Ka29). Others: 1962Ga13, 1962Mc03 
$E2 matrix element (1449,2+ to 0,0+)=+0.106 {I6} (1995Ka29) 
$E2 matrix element (1449,2+ to 666,2+)=+0.379 {I+22-20} (1995Ka29) 
$E2 matrix element (1449,2+ to 1701,4+)=0.09 {I+4-5} (1995Ka29) 
$Static E2 matrix element (1449,2+ to 1449,2+)=+0.53 {I3} (1995Ka29) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$ B(E2)(from 666,2+)=0.0028 {I4} (1974Ba80), 0.0029 {I5} (1995Ka29) 
$B(E2) (from 1449,2+)=0.0005 {I+15-2} (1995Ka29) 
$E2 matrix element (1478,0+ to 666,2+)=+0.12 {I1} (1995Ka29) 
$E2 matrix element (1478,0+ to 1449,2+)=-0.05 {I+1-5} (1995Ka29) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$ g factor from transient-field technique in Coul. ex. (1998Sp03); 
$ B(E2)(from 666,2+)=0.130 {I4} (1974Ba80), 0.134 {I13} (1995Ka29) 
$ B(E2)(from 1449,2+)=0.0009 {I+10-7} (1995Ka29) 
$E2 matrix element (1701,4+ to 666,2+)=+0.82 {I4} (1995Ka29) 
$Static E2 matrix element (1701,4+ to 1701,4+)=-0.85 {I+11-6} (1995Ka29) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ B(E2)(from g.s.)=0.00045 {I25} (estimated,1974Ba80), 0.0012 {I+3-4} (1995Ka29) 
$ B(E2)(from 666,2+)=0.0020 {I15} (1974Ba80), 0.0020 {I+9-10} (1995Ka29) 
$ B(E2)(from 1479,0+)=0.053 {I+25-48} (1995Ka29) 
$ B(E2)(from 1449,2+)=0.0010 {I+40-8} (1995Ka29) 
|b{-2}=0.010 
$E2 matrix element (1960,2+ to 0,0+)=+0.034 {I+4-6} (1995Ka29) 
$E2 matrix element (1960,2+ to 1478,0+)=+0.23 {I+5-16} (1995Ka29) 
$E2 matrix element (1960,2+ to 666,2+)=+0.10 {I+2-3} (1995Ka29) 
$E2 matrix element (1960,2+ to 1449,2+)=0.07 {I+9-10} (1995Ka29) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
J$(3+) in adopted levels 
$ B(E2)(from 666,2+)=0.00002 to 0.004 (1995Ka29) 
$ B(E2)(from 1449,2+)=0.09 {I+2-4} (1995Ka29) 
$E2 matrix element (2121,4+ to 666,2+)=0.01 {I+13-6} (1995Ka29) 
$E2 matrix element (2121,4+ to 1449,2+)=+0.67 {I+8-18} (1995Ka29) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
J$(1+,2+) in adopted levels 
$ B(E2)(from g.s.)=0.0009 {I+7-5} (1995Ka29) 
$ B(E2)(from 666,2+)=0.0016 {I+13-6} (1995Ka29) 
$ B(E2)(from 1479,0+)=0.18 {I+3-10} (1995Ka29) 
$ B(E2)(from 1449,2+)=0.026 {I+13-15} (1995Ka29) 
$ B(E2)(from 1701,4+)=0.010 {I+13-9} (1995Ka29) 
$ B(E2)(from third 4+)=0.18 {I+5-3} (1995Ka29) 
$E2 matrix element (2344,2+ to 0,0+)=+0.486 {I+28-25} (1995Ka29) 
$E2 matrix element (2344,2+ to 666,2+)=+0.486 {I+28-25} (1995Ka29) 
$E2 matrix element (2344,2+ to 1479,0+)=+0.486 {I+28-25} (1995Ka29) 
$E2 matrix element (2344,2+ to 1449,2+)=+0.486 {I+28-25} (1995Ka29) 
$E2 matrix element (2344,2+ to 1701,4+)=+0.486 {I+28-25} (1995Ka29) 
$E2 matrix element (2344,2+ to third 4+)=+1.28 {I+17-12} (1995Ka29). 
$Static E2 matrix element (2344,2+ to 2344,2+)=-0.76 {I+24-22} (1995Ka29) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T weighted average of 18.2 min {I2} (1954Yt03), 18.6 min {I1} (1957Ap46), 17.9 min {I5} (1971Do09), and 18.2 min {I2} (1975Fe07). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J L(d,p)=4, E3(+M4) |g to 1/2-. 
T from 1989Ab18. Others: 57.28 min {I5} (1971Do09), 56.6 min {I6} (1967Ra08). All measurements from 103|g(t). 
$%|e+%|b{++} deduced by the evaluator using data of {+81}Se IT decay and |b{+-} decay (57.28 m). See {+81}Se |b{+-} decay (57.28 m) dataset. 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J primary |g from 1/2+; 1725|g to 1/2- g.s.; L(p,d)=2 for level at 1753 {I25}, assumed by evaluator to be the same as this 1725 level. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J 1785|g to 3/2- 468; 1960|g to 9/2+ 294; primary |g from 1/2+. Assignment implies [E2] for primary |g from 1/2+. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J 5/2+ from (pol d,p), consistent with primary |g from 1/2+ but 2332|g to 1/2- g.s. implies level half-life > 1.7 ps for B(M2) W.u. |< 1 (RUL). L(p,d)=(2+4) for E=2325, so another |p=+ level may exist at approximately this energy. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
J J|p=5/2+ from (pol d,p) is in conflict with L(p,d)=4. The evaluator adopts (5/2)+ because the DWBA fit is better and |s(|q) spans a greater angular range in the (d,p) measurement. Alternatively, a different level with J|p=7/2+,9/2+ and similar energy may be excited in (p,d). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J negative parity assigned ({+18}O,x|g) based on non-observation of a transition to (13/2+) state at 1372. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J log {Ift}=4.9 from 3/2-; 2832|g to 7/2+ 103. Consistent with L=(3) component of 2893 doublet in (p,d). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_uncertain: ?
level_comment:
E from |b{+-} decay; see comment in source data set. 
J |g to (5/2-) and 7/2+, log| {Ift}>4.9 from 3/2- (if deexcitation |g rays placed correctly). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J negative parity assigned by the authors based on non-observation of a transition to (13/2+) state at 1372. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$From 2012Si23 for T{-1/2}(2|n2|b-)({+82}Se 0+ to 0+) other values: 0.83|*10{+20} y {I+9-7} (1999Pi08,1999Sa02), 10.8|*10{+20} y {I+26-6} from 1992El07 (see also 1987El11, 1987El10, 1986El01), 1.2|*10{+20} y {I1} from geochemical measurements (1988Li11); 1.0|*10{+20} y {I4} (1985Ma57), 2.8|*10{+20} y {I9} (1973Sr05), 1.4|*10{+20} y {I3} (1970Ki21), all from isotopic anomaly of {+82}Kr in geological samples, 0.9|*10{+20} y {I1} (2002Ba52) 
T$T{-1/2}(0|n2|b-)({+82}Se 0+ to 0+)>3.2|*10{+23} y (90% confidence level); (2012Si23); >2.4|*10{+21} y (1999Sa02,2000Ar16, 2001Va34) other: >2.7|*10{+22} y (1993Mo36). Calculated T{-1/2} (2002Su13,2002Si12) 
T$>2.4E24 y lower limit for 0|n|b|b decay mode (2018Az05); measured at 90% credible interval, from a maximum likelihood analysis of events in the 2800-3200 keV region. This half-life can be compared with T{-1/2}>3.6|*10{+23} y, obtained using NEMO detector with a larger {+82}Se exposure of |?3.5 kg y (2011Ba55) 
$From the half-life limit, deduced effective Majorana neutrino mass of <(376-770) meV, depending on the nuclear matrix element calculations (2018Az05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J from angular distribution and vector-analyzing power in (pol p,p') (1984De01). 
T$from 2016Pr01,deduced from B(E2) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L(t,p)=2+4, L(p,p')=2+4 for the unresolved 1731+1735 doublet. log| {Ift}=7.0 from (1+) and |g to 0+ indicate that this is the 2+ member of 1731+1735 doublet. 
T$from B(E2) deduced from Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J log| {Ift}=5.5 from (5-). |g to (3,4+). L(t,p)=0+(5) at 3449 keV. Note, however, that the angular momentum of the L=5 admixture is more speculated than established. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$From (HI,xn|g) assumed stretched E2 cascade. Expected configuration=(|n g{-9/2}){+-2}. Systematics of 8+ isomers in N=48 nuclides (1999Ma21,2002Is03). 
T$from IT decay (1999Ma21) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2) from 2016Pr01,Q from 1977Le11. Constructive interference of the second excited state has been assumed (Q=-0.11 {I7} for destructive interference). B(E2)=0.180 {I3} (1977Le11),0.175 {I9} (1974Ba80), 0.17 {I3} (2005Iw03), 0.179 {I19} (1995Ka29); others: 1970AgZV, 1962Ga13, 1962St02, 1960An07,1956Te26. 
G$from 1998Sp03, based on 1978Br38. Other: +0.43 {I12} from |g(|q,H) (1969He11). 
T$From 2016Pr01, deduced from B(E2) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
B(E2)(2+ to 0+)=0.0015. B(E2)(|_)(1409 level)/B(E2)(|_)(655 level)=0.22 from reinspection of the 1974Ba80 |g spectrum (see 1977Le11). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)(2+ to 2+')=0.0106 {I15}; B(E2)(0+ to 2+')=0.0145 {I15} (1974Ba80). Pure E2 was assumed for B(E2)(2+ to 2+'). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3,4+)
level_comment:
J$J|p adopted as (3,4+). Level feeding in (n,n'|g) supports J=3. 1995Ka29 assumed it to be 4+ for their calculations. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$measured lower limit for 0|n|b|b decay mode of {+82}Se, at 90% credible interval, corresponding to m{-|b|b}<(311-638) meV depending on the nuclear matrix element calculations (2019Az02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$from 2020Ar02 for the 2|n|b|b decay mode for the decay branch of g.s. to g.s. at 90% confidence level. Other: |>2.3|*10{+22} year at 90% confidence level for 0|n|b|b decay from g.s. to g.s. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$for 2|n|b|b decay mode of {+82}Se, reported as 8.60|*10{+19} y {I3} (stat) {I+19-13} (stat) (2019Az04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for 0|n|b|b decay mode of {+82}Se to the ground state of {+82}Kr. Others: >3.0 |* 10{+23} y for decay to the first excited 2+ in {+82}Kr and >3.2 |* 10{+23} y for decay to the second excited 2+ state in {+82}Kr. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$for 2|n|b|b decay mode of {+82}Se to the ground state of {+82}Kr. Reported as 8.69|*10{+19} y {I5} (stat) {I+9-6} (syst) (2023Az05); uncertainty added in quadrature. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for 0|n|b|b|h{-0} decay mode for n=1. Others: >3.8 |* 10{+22} y for 0|n|b|b|h{-0} decay mode for n=2, >1.4 |* 10{+22} y for 0|n|b|b|h{-0} decay mode for n=3, and >2.2 |* 10{+21} y for 0|n|b|b|h{-0} decay mode for n=7. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 22.6 min {I2} (1967Ma35), 22.4 min {I2} (1969To11), 22.1 min {I1} (1974Kr27), and 22.4 min {I2} (1974KrZG). 
J$L(pol d,p)=4, vector-analyzing power. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 70.4 s {I3} (1969Ph03), 69.2 s {I6} (1974Kr27), and 69 s {I2} (1974KrZG). 
J$L(pol d,p)=1, vector-analyzing power. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$weighted average of 3770 keV {I15} (1978Mo12) and 3790 keV {I20} (1965Li08). 
$d|s/d|W{-max}=1.79 mb/sr (1965Li08). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$weighted average of 3830 keV {I15} (1978Mo12) and 3860 keV {I20} (1965Li08). 
$d|s/d|W{-max}=3.03 mb/sr (1965Li08). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 3.1 min {I1} (1974KrZG), 3.1 min {I2} (1975Hu02), 3.5 min {I1} (1970Ei02), 3.1 min {I2} (1968Re12), and 3.3 min {I3} (1960Sa05). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$assumed that 3934 {I8} in (t,p) is the same as 3916 {I11} in ({+84}Se,{+84}Se'|g); listed level energy is the weighted average of the two 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$This level is uncertain in view of a 1361.5|g feeding 3537 level from a 4898 level in 2013DrZY and 2004Pr10 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_comment:
J$level originally thought to be a 1- by 2002AoZY. The level was later identified as (4+) in |g spectroscopy studies. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^=0.105 {I15} in 2010Ga14. The experiment in 2015Li42 is less sensitive to mean lifetimes of less than 1 ps. Upper limit of 0.7 ps half-life is suggested by 2015Li42 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from method 2, as described for {+86}Se in 2015Li42; the lower uncertainties of 1.8 (stat) and 3.4 (syst) are combined in quadrature by compiler. Other T{-1/2}=8.7 ps {I+31-44} from authors' method 1, same as used for half-life of the 4+ state in {+86}Se 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
$A 164.18 keV {I21} |g with a branching of 29% from this level and known from previous experimental work is not discussed by 2015Li42 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: S
level_comment:
J$L=2 in {+2}H({+84}Se,p) reaction; systematics of N=51 nuclei. 
T$from |g timing. Weighted average of 33.0 s {I2} (1978Ze08) and 31.4 s {I10} (1975Hu02). Others: 19 s (1975Al11,1970OsZZ), 33 s {I2} (1974KrZG, from the same group as 1978Ze08), 39 s {I4} (1960Sa05). 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$|s(|q) distribution in {+2}H({+84}Se,p) gives L=2+4, with slight preference for the latter. J|p=3/2+ is not completely ruled out 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$group of neutron-decaying levels above S(n)({+85}Se)=4537 keV, including 6055, 6931, 7160, 7187, 7377 and 8090 listed above 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L$following tentative spin assignment of (3/2+,7/2+) by 1991Om02, angular distribution data were fitted by 2007Th15 with L=2 and L=4. There is slight preference for L=4, but no certain assignment can be made 
S$for 0.06 {I2} for L=2; S{-lj}=0.77 {I27} for L=4 
$C{+2}{-lj}=0.42 fm{+-1} {I11} for L=2, 0.049 fm{+-1} {I12} for L=4 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$1438+1444 doublet. 
L$angular distribution data were compared with representative distributions for L=2, d{-3/2} and L=2, d{-5/2}. No assignment could be made from these data. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 14.1 s {I2} (1978Ze02, from decay curve for 154|g), 14.4 s {I10} (1975Hu02), 16.1 s {I6} (1974KrZG), 14.3 {I5} (1973Ta19 for 154|g, other values reported are 14.4 s {I20} for 49|g and 15.9 s {I12} for 207|g), and 16 s {I3} (1960Sa05, authors assigned) activity to {+87}Se, but the measured half-life is much closer to that of {+86}Se than the recommended 5.5 s half-life for {+87}Se). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$E2 |g to 2+; yrast band member 
T$effective half-life=6.9 ps {I+23-15}, upper limit is given by 2015Li42 since no information is available about feeding of this state from higher levels 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
T$effective half-life=6.9 ps {I+23-15}, upper limit is given by 2015Li42 since no information is available about feeding of this state from higher levels 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$(4) in 2013Cz02. 2006Jo01 assigned (6+) but (3-) in their later paper 2011Li34 changed to (3-). 2013Cz02 do not support (3-) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4,5,6+)
level_comment:
E,J$level with J|p=(6+) from 2011Li34. This level is included here since a similar level reported by 2013DrZY in {+238}U(p,F) work 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$From log| {Ift} value, observation of this level in {+87}As |b{+-}n decay and lack of observation in prompt fission data. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Measured |s=230 mb {I30} (2017El04) 
$|s=227 mb {I34} if 613 peak is not included in the analysis, and 233 mb {I35} if this peak is included 
$B(E2)|^ value is in e{+2}b{+2} units. 
$B(E2)|^=0.2170 {I330} if 613 peak included in the analysis. Systematic uncertainty is included by the authors 
T$deduced by compiler from B(E2)|^ value in 2017El04 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=10.3 {I+12-22} (2018De35). Others: T{-1/2}=7.8 ps {I12} (from B(E2)=0.211 {I32} in 2017El04: Phys. Rev. C 96, 044332); 7.5 ps {I+48-26} (from RDDS method, 2015Li42: Phys. Rev. C 92, 064322) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
J$Systematics of the N=53 isotones suggest either 5/2+ or 3//2+. Based on shell model calculations of for the E(5/2+) and E(3/2+) for the N=53 isotones. The calculations indicate large and nearly constant B(E2) values with a significant deformation. Calculations assuming a K=3/2 band were consistent with the excitation levels and B(E2) values, thus placing the 3/2+ spin level below that for 5/2+. See 2013Rz02 for details. with shell model calculations (2013Rz02) 
T$from unweighted average of 5.9 s {I2} (1970De08), 5.85 s {I15} (1970Kr05), 5.41 s {I10} (1971To13, supersedes 1968To06), 5.8 s {I3} (1978Ze08) and 5.29 s {I11} (1993Ru01) all determined from neutron counting. Other values are: 16 s {I3} (1960Sa05) from {+87}Br grow-in, 5.5 s {I2} (1970ToZT, superseded by value from 1971To13), and 5.60 s {I16} (1982Ru01, superseded by value from 1993Ru01). 
%B-N from unweighted average of 0.26 {I7} (1970De08, Adjusted by 1993Ru01; original was 0.23 {I7}), 0.51 {I17} and 0.24 {I8} (1970Kr05), 0.17 {I3} (1971To13, Adjusted by 1993Ru01; original 0.16 {I3}), and 0.60 {I12} (1993Ru01). The reduced-|h{+2} value for this average is 4.02, higher than the critical value 2.37, due to discrepant values. Therefore, an unweighted average is adopted. Other values are: |< 0.8 (1968To06); 0.44 {I20} (1969WaZS); 0.18 {I4} (1970ToZT; see 1971To13 value by same authors); and 0.19 {I3} (1982Ru01). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$Systematics of the N=53 isotones suggest either 5/2+ or 3//2+. Based on shell model calculations of for the E(5/2+) and E(3/2+) for the N=53 isotones. The calculations indicate large and nearly constant B(E2) values with a significant deformation. Calculations assuming a K=3/2 band were consistent with the excitation levels and B(E2) values, thus placing the 3/2+ spin level below that for 5/2+. See 2013Rz02 for details. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1971To13 (from neutron counting, included both statistical and systematic errors). Others: 0.65 s {I+18-14} (2012Qu01), 1.51 s {I4} from |g counting (1982Re08, systematic errors not included); 1.6 s {I5} (1978Ze08 ); 1.4 s {I3} (1970Kr05), 1.3 s {I3} (1970De08) 
%B-N$1993Ru01 and 1984Ma39 evaluations recommended 0.99 {I10} and 0.94 {I16}, respectively, based on 1971To13 result. Measurements: %|b{+-}n=0.75 {I6} (1971To13), 0.15 {I9} (1970Kr05), |<1 (1970De08). The values from 1971To13 and 1970Kr05 were adjusted in 1993Ru01 evaluation to 0.99 {I10} and 0.23 {I15}, respectively, using improved values of %|b{+-}n for {+87}Br and {+88}Br decays. Other: 0.67 {I30} from 2002Pf04 compilation (source references not cited). 
%B-N$ 1982Ru01 compilation quotes %|b{+-}-n=0.6 {I3} from a 1980 conference (Nuclear Data evaluation methods, Upton, New York, Sept 1980) report by P.L. Reeder. It is not clear whether this was an evaluation or an independent measurement 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$886|g reported from a first 2+ level in 2006Jo01 (Phys. Rev. C 73, 017301) was not seen by 2017Ch18. 2017Gr07 also reported the first 2+ level at 589 keV 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
%B-N$original value of 5.0 {I15} from 1971To13 (based on %|b{+-}n({+89}Br)=8.8 {I9}) revised by 1993Ru01 to 7.8 {I25} using %|b{+-}n({+89}Br)=13.8 {I4}. The same value is obtained using %|b{+-}n({+89}Br)=13.7 {I6} in {+89}Br Adopted Levels 
J$from shell-model predictions; also systematics (2021Ko07). Other: 3/2+ in theoretical calculations (2019Mo01) 
T$weighted average of 0.41 s {i4} (1971To13,(|b)(fission neutrons)(t)); 0.56 s {I8} (1982Re08), 0.345 s {i20}(syst) {I+95-75}(stat) (2012Qu01; maximum-likelihood method for 90 correlated events). Reduced |h{+2}=1.9. 
$Compilations of T{-1/2} and %|b{+-}n: 2020Li32, 2002Pf04, 1993Ru01 (also 1982Ru01, 1979RuZQ, 1977Ru10), 1989BrZI, 1984Ta06, 1981Al25 
$Theoretical calculations of T{-1/2} and %|b{+-}n): 2019Mo01, 2016Ma12, 2007Na28. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from |b-decays correlated with implants (2012Qu01). Value given in 2012Qu01 is 195 ms {I7} (syst) {I+95-65} (stat) using maximum likelihood method for analysis of T{-1/2} data from 70 implants and 30 correlated decay sequences. 
$Calculated %|b{+-}n=1 (2019Mo01), 2.6 (2012Mc04) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_comment:
$ Number of implanted fragments=6.4|*10{+4} 
T$ from |g(t) method (2012Ka36); constant background component was separately deduced. 
$ 503.4-, 538.8- and 897.8-keV |g rays deexcite this isomer but the level scheme is not known 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
T 1995CzZZ report that a detectable number of nuclei survived the 150 ns flight path through the fragment mass separator. 
J from systematics. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_comment:
$ Number of implanted fragments=3.7|*10{+3} 
T$ from |g(t) method (2012Ka36) 
$ 208.3- and 469.9-keV |g rays deexcite this isomer but the level scheme is not known 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Measured |s=20 pb (2010Oh02), systematic uncertainty |?50% 
T$ lower limit from time-of-flight in 2010Oh02, as communicated to the evaluator by T. Kubo in an e-mail reply of July 14, 2010. Actual half-life is expected to be much longer as suggested by the calculated value of 31 ms (1997Mo25). 
$ Probability of misidentification of {+95}Se isotope<0.001% 
$Calculated %|b{+-}n=13.9, %|b{+-}2n=3.1 (1997Mo25) 
J$ 3/2+ in theoretical predictions of 1997Mo25 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$Assuming that decay of {+67}Kr probably populates the g.s. of {+67}Br 
$Theoretical T{-1/2}(|e)=46.9 ms (2019Mo01) 
J$9/2+ from theory (2019Mo01), 1/2- from systematics (2021Ko07) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
E$assuming the observed events correspond to the ground state 
$Corrected yield of {+68}Br was 14.7 {I50} (stat) {I18} (syst) for {+70}Br beam, 33 {I16} (stat) {I4} (syst) for {+70}Kr beam, 13.7 {I60} (stat) {I12} (syst) for {+71}Kr beam and 10 {I4} (stat) {I2} (syst) for {+72}Kr beam. 
T$estimated by 2019Wi08 based on measured versus expected yield, length of flight path to focal plane of the ZeroDegree Spectrometer and time dilation. Value is given here as average of |t=51 ns {I6}, 57 ns {I7}, 46 ns {I6}, and 51 ns {I6} determined for the {+70}Br, {+70}Kr, {+71}Kr, and {+72}Kr beams, respectively. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$from 2014De41. Others: J|p=(3/2-) in 2011Ro18 based on mirror symmetry with {+69}Se, and (1/2-) in 2011Ro47 (also in 2012Au07) 
T$from 1996Pf01. Others: <100 ns (1995Bl06), |?30 ns (1995MoZV). 
%P${+69}Br g.s. is unbound towards proton emission from observation of E(p)=641 keV {I42} (2014De41) proton group from the decay of {+69}Br g.s. to {+68}Se g.s. Also 2011Ro47, in their experiment to observe beta-delayed proton emission from {+69}Br g.s. did not find any evidence of delayed proton emission activity with an upper limit of 5%. 1996Pf01 had also found unbound nature of {+69}Br g.s. based on upper limit of half-life deduced from expected cross section 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3/2-)
level_comment:
E$from analysis of |b delayed proton spectrum of {+69}Kr in 2014De41 with two closely spaced states decaying by protons. The analysis of the doublet peak was supported by shell model calculations. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E$from proton decay with energy of 2939 keV {I22} observed in correlation with 854|g from the first 2+ state of {+68}Se. Isobaric analog state (IAS) of {+69}Kr in {+69}Br. 
J$IAS of {+69}Kr g.s. of proposed J|p=(5/2-) based on log {Ift}=3.43 {I11}, typical of that for superallowed |b transitions. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3/2-)
level_comment:
$E(p)=751 keV {I+132-42} from analysis of proton spectrum in 2014De41 is in good agreement with value of 785 keV reported by 2011Ro18 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$This level decays by protons since S(p)({+69}Br)=-641 {I42} (2014De41). 
E$from 2014De41. Others: 3039 keV {I64} (2011Ro47) and 3.85 MeV {I53} (1997Xu01). Proton group 2.939 MeV {I22} (2014De41) is consistent with 2.97 MeV {I5} (2011Ro47) that depopulates this isobaric analog state (IAS) in {+69} in correlation with the 854|g from the first 2+ state in {+68}Se. However, E(p)=4.07 MeV {I5} in 1997Xu01, implying proton decay to the g.s. of {+68}Se, is in disagreement with results from 2014De41 and 2011Ro47 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 80.2 ms {I8} (1978Al23, from |b(t)) and 78.5 ms {I6} (1988Bu12, from |b(t)). Other: 79 ms {I36} (2002Lo13) and 70 ms {I19} (2014Ro14). 
J$super allowed |e to 0+ {+70}Se 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$2.23 MeV {I9} deduced from decay energy of isomer and estimated Q value of {+70}Br (2004Ka38) 
T$from |b(t) in 1981Vo04. Other: 2.2 s {I3} preliminary value given in 2002Ro25. 
%EC+%B+$IT decay has not been observed 
J$Allowed |e decay to 8+, systematics 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$From the Adopted Levels 
E$a tentative (9+) isomer proposed by 2001De46 at 1214 is assigned at 2293 by 2002Je07 


