# LEVEL

level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Decay mode and J|p from {+70}Br Adopted Levels in ENSDF database (June 2016 update) 
$T{-z}=0 
T$from ion-|b(t) (2017Mo18). In fitting the X and Y strips separately 2017Mo18 also obtain T{-1/2}=77.2 ms {I30} and 76.8 ms {I29}, respectively. 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: MS
level_comment:
$Decay mode, E(level) and J|p from {+70}Br Adopted Levels in ENSDF database 
T$from ion-|b|g(t) in 2017Mo18 using the 945|g, 964|g, 1034|g, and 1094|g. Value is reported as 2157 ms {I30} stat {I+44-38} syst with uncertainties added in quadrature by the compiler. 
$T{-z}=0 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from 2019Si33, using |X{+2} fit to implant-|b(t) exponential decay included contributions from the parent, daughter and grand-daughter decays (if appropriate), as well as a constant background. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Measured |s=201 mb {I11}(stat) {I20}(syst) for {+197}Au target (2021Wi01) at E({+70}Br)=152 MeV/nucleon 
$Measured |s=14.6 mb {I5}(stat) {I8}(syst) for {+9}Be target (2021Wi01) at E({+70}Br)=140 MeV/nucleon 
$Deduced nuclear deformation length |d{-N}=1.09 fm {I3} (2021Wi01), where uncertainty includes 0.02 fm statistical and 0.03 systematic. 
$Deduced E2 matrix element=0.381 eb {I31} (2021Wi01), where uncertainty includes 0.012 eb statistical, 0.022 eb systematic, and 0.018 eb theoretical 
$Deduced B(E2)=0.1454 e{+2}b{+2} {I233} (2021Wi01), where uncertainty includes 0.0091 e{+2}b{+2} statistical, 0.0165 e{+2}b{+2} systematic, and 0.0137 e{+2}b{+2} theoretical 
T$deduced by compiler from B(E2) value. This value can be compared T{-1/2}=2.74 ps {I40} measured using RDDS method (2014Ni09: Phys. Lett. B733, 52) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Observed by 2001De46. All other levels are reconstructed by |g-|g coincidence technique and observing ground state transition. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from 2022Wa34. Half-life measured in (implants)(decay events)-correlated decay curve, with a constant background. This value is compared with 79.1 ms {I8} in {+70}Br Adopted Levels in the ENSDF database; and with 78.42 ms {I51} (2017Mo18: Phys. Rev. C 95, 064327). Also, 79.7 ms {I24} measured by 2019Si33: Phys. Rev. C 100, 044311. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from 2022Wa34. Half-life measured in (implants)(decay events)-correlated decay curve, with a constant background. This value is compared with 2.2 s {I2} in {+70}Br Adopted Levels in the ENSDF database, and with 2157 ms {I53} (2017Mo18: Phys. Rev. C 95, 064327) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: S
level_comment:
J$log| {Ift}=5.1 to 5/2- state in {+71}Se; systematics 
T$from 1982Ha32, time decay of 4 strongest |g rays and Se x-rays. Others: 21.5 s {I5} (1981Vo04, multiscaling of |b activity), <1 min (1976Ro01). The evaluators recommend T{-1/2} from 1982Ha32 because of better isotopic selectivity through |g-ray detection, even though this value has somewhat larger uncertainty than in 1981Vo04 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J$5/2- in 2022Wa34 
$Level proposed by 2005Fi10 from spectral data of 1997Oi01, and confirmed by 2022Wa34 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(p)({+71}Br)+x, where x<8319 keV, from Q(e)({+71}Kr)-S(p)({+71}Br) 
E$wide group from E(p)=1.5 to 5.5 MeV, this proton group feeding the g.s. and the first excited state of {+70}Se (2022Wa34). Other: |?4250 (1997Oi01) from wide group from E(p)|?2.3 MeV, a broad bump at this energy, assuming that this proton group feeds the g.s. of {+70}Se 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J$from {+72}Kr |e decay, where the g.s. to g.s. transition has an intensity of 34%, which gives log| {Ift}=4.7 
T$from 1974Co14. Others: |?100 s (1970No03), 78 s {i30} (1971Do01) 
$|m=0.55 {i21}, from low temperature nuclear orientation (1992Gr20,2005St24). 
$<r{+2}>{+1/2} (mass)=4.22 fm {i25} (2005Le43) 
$|m: Static nuclear orientation with |g detection (1992Ba68) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$unweighted average of 10.3 s {i6} (1982Ga06) and 10.9 s {i1} (1980DaZO) 
J$(M2) |g to 1+ g.s 
$|m>0.7 (1992Gr20) 
$1980DaZO report a weak |e+|b{++} branch, but no intensity is given 
$|m: Static nuclear orientation with |g detection (1992Gr20,2005St24) 


level_energy_unit: KEV
level_spin_parity: (1)
level_comment:
J$log| {Ift}=6.2 from 0+ parent, the intensity from which this is based has a 60% uncertainty, and J=2 could also be a possibility. 


level_energy_unit: KEV
level_spin_parity: (1,3)
level_comment:
J$the (1) value is from log| {Ift}=6.4 {I2}, deduced from a total intensity with 40% uncertainty. In Heavy ion studies, this level is assigned a J|p=(3-), and several higher lying levels J|p's are based on this assignment. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$DSA analysis combined with RDM give 0.4<T{-1/2}|<2.1 ps (1988Ul01). Other: T{-1/2}<5 ps (1982Ga22). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
J$spin from absence of anisotropy measured for 16 |g rays in {+73}Se from {+73}Br decay in low-temperature nuclear orientation measurements of 1992Gr20 (also 1988Gr26). Parity from allowed |b decay (log| {Ift}=5.7) to 3/2- 
T$weighted average of 3.4 min {I2} (1987He21), 3.6 min {I4} (1974Ro11) and 3.3 min {I3} (1970Mu02) 
$Strong absorption radius r{-0}=1.036 fm {I18}; rms matter radius <r{+2}>{+1/2}=4.04 fm {I14}, deduced from measured reaction |s{-R} in Si({+73}Br,X),E|?50-60 MeV/nucleon and Glauber model analysis (2004Li29,2005Le43) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_lifetime_unit: NS
level_comment:
MOMM1$from g factor=1.3 by TDPAD (1987He27), assuming J=3/2. 
J$62.4|g M1 to 3/2-; 45.6|g D from (5/2)+ 
T$|g(t) with respect to the beam in {+40}Ca({+36}Ar,3p|g) (1987He27) 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_lifetime_unit: PS
level_comment:
J$804.4|g E2 to (13/2)+; band assignment 
T$average of 1.5 {I4} (RDM), 0.97 {I21} (DSAM), and 0.9 {I2} (DSAM) (1987He27) 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: PS
level_comment:
J$850.2|g to (13/2-); band assignment 
T$average of 0.67 {I17} (RDM) and 0.73 {I17} (DSAM) (1987He27) 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: PS
level_comment:
J$995.2|g E2 to (17/2)+; band assignment 
T$average of 0.41 {I6} (DSAM) and 0.45 {I6} (DSAM) (1987He27) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_lifetime_unit: NS
level_comment:
T$|g(t) in ({+36}Ar,3p|g) (1987He27, earlier value was 37 ns {I6} in 1985Wo12) 
G$from Larmor precession 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$average of 1.5 {I4} (RDM), 0.97 {I21} (DSAM), and 0.9 {I2} (DSAM) (1987He27). Other: <1.2 ps (1985Wo12, same group as 1987He27) 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: MIN
level_comment:
T$ from {+74}Br |e decay. Weighted average of 1974Co38, 1974Sc28, 1960Bu22 
J$ log| {Ift}=8.0 to 0+ and 7.6 to 2+ levels in {+74}Se. Probable configuration=|p3/2[431]|n3/2[301] (1983Wi01) favors 0- 


level_energy_unit: KEV
level_spin_parity: 4(+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
No isomeric transitions observed 
MOMM1$ NMR on oriented nuclei. Other: 1.68 {I18} (1992Pr06,static nuclear orientation with gamma detection). See also 2005St24 compilation 
J$ from atomic-beam magnetic resonance measurements in (1980Ek02). Parity from systematics. 
T$ from {+74}Br |e decay. Weighted average of values from 1984Ma35 and 1981Ga11 for |g-rays emitted by longer lived activity only. Other values in literature (from 1984Ma35,1981Ga11,1974Ro11,1972Co32,1971RoZV,1969La15,1966Be17, 1957Be46,1953Ho53) give a slightly lower average value (41 min {I2}) probably due to small contribution from 25-min activity 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$ band assignment, from T{-1/2} in the ns range (1983Wi01) and corresponding B(E1)(W.u.) and B(M1)(W.u.) values, negative parity is favored. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
Not reported in this experiment. Included here by evaluators on the basis of {+74}Kr |e decay and (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
1974LuZM suggest level at 72.3 but in the in-beam |g-ray study the level is proposed above the 46-min isomer 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4-)
level_comment:
E$ 1974LuZM suggest level at 187.9 but in the in-beam study the level is based on the 46-min isomer at 13.8 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$ 1974LuZM propose level at 203.0. But from {+74}Kr |e decay and in-beam |g study the level is at 212.8 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
E$1983Wi01 proposed two separate levels near this energy with J|p=(4-) and (3-), respectively. From (HI,xn|g), only one level is adopted 


level_energy_unit: KEV
level_spin_parity: 7(+)
level_lifetime_unit: PS
level_comment:
T$recoil-distance method. Weighted average of 9.0 ps {I14} (1991Ho01) and 9.7 ps {I21} (1999Ga21). Other: 10.4 ps {I7} (1982NeZP) 


level_energy_unit: KEV
level_spin_parity: 11(+)
level_lifetime_unit: PS
level_comment:
T$from 1999Lo17. Other: 0.31 ps {I10} (1991Ho01). Value of 51 ps {i3} quoted by 1991Ho01 from 1982NeZP seems in error 


level_energy_unit: KEV
level_spin_parity: (12-)
level_lifetime_unit: PS
level_comment:
T$from 1999Lo17 (uncertainty from table 4a of 1999Lo17). Other: <0.35 ps (1991Ho01). UNCERTAINTY is quoted as 0.035 PS IN TABLE 4b OF 1999Lo17 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
MOMM1$nuclear orientation (1992Gr20). Others: 0.73 {I9} (1988Gr26), positive (1992Ba68) 
Configuration=((|p 3/2[312])) (1992Ba68) 
J$atomic-beam method (1980Ek02). log| {Ift}=5.4 to 3/2- 286 level in {+75}Se 
T$weighted average of 95 min {I3} (1953Ho53), 95 min {I5} (1957Be46), 100 min {I5} (1961Ba43), 95.5 min {I15} (1969La07), 106 min {I5} (1969Ra24), 101 min {I4} (1972Co06). Others: 91.8 min {I12} (1974Ro11), 1.7 h (1948Wo08) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$|DJ=1, M1+E2 |g to 3/2-; 1/2 not allowed by |g(|q) 
T$from pulsed beam |g-ray timing method (1981Wi05) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: NS
level_comment:
J$E1 |g to 3/2-; |g(|q) in ({+3}He,pn|g) 
T$weighted average 5.6 ns {I4} (1974Ro12,1981Wi05) and 6.4 ns {I3} (1995Ma97) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: NS
level_comment:
J$E1 |g to 3/2-; (M1) |g to (5/2)+; |g(|q) in ({+3}He,pn|g) 
T$from pulsed beam |g-ray timing method (1981Wi05) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$dipole |g to 3/2-; isotropic |g(|q) in (p,|g) favors 1/2; log| {Ift}=7.8 from 5/2+ parent favors negative parity 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
J$E2 |g to (5/2)+, |g(|q) in ({+3}He,pn|g). 
T$from 1995Ma97. Others: 26 ns {I2} (1981Wi05), 39 ns {I4} (1981Kr10) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
J$|g rays to 3/2- and (9/2)+ suggest (5/2+,7/2-), |g(|q) in ({+3}He,pn|g) and band structure support J|p=7/2- 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
J$|g's to (9/2)+ and (5/2-) suggest (5/2+,7/2,9/2-), |g(|q) in ({+3}He,pn|g) and band structure support J|p=9/2- 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Level is doubtful since it is not confirmed in ({+30}Si,p2n|g). A 1332|g is reported in ({+16}O,p2n|g), but it is assigned elsewhere. In ({+30}Si,p2n|g), gammas reported near this energy are 1327.4 and 1336.3 placed from different levels 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Level in doubt since it is not confirmed in ({+30}Si,p2n|g). No 1152.8|g reported in ({+30}Si,p2n|g) 


level_energy_unit: KEV
level_spin_parity: (45/2+)
level_uncertain: ?
level_comment:
Level considered suspect since it is not confirmed in ({+30}Si,p2n|g) (1999So10), where 45/2+ member of this band is reported at 12106 decaying through 1956|g 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1974Ro12) with a NaI(Tl)-NaI(Tl) combination. Other: 6.5 ns {I8} (1974Ro12) with Ge(Li)-NaI(Tl) combination 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
T$ from Adopted Levels 
$ No transition to the g.s. was observed by 1995BeZS. The 221 keV gamma is a sum peak from 132.5 and 88.5 keV lines. 1974Ro12 listed the energy as 220.9 {I3} with I|g=0.18 {I8} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
T$ 2009Mu16 quote 26.3 ns {I14} with an incorrect source reference 
$Q{-t} and BE2 recalculated by evaluator using the ^Adopted T. 
$ Q{-t}=3.5 {I9} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
$Configuration=|p3/2[312]~#|n5/2[422] favors |m in 1980Ek02. 
J$spin from atomic-beam method (1960Li11); parity from E1 |g from 1+ 
T$weighted average of 16.1 h {I2} (1971La01), 16.3 h {I3} (1960Bu22) and 16.1 h {I2} (1959Gi46). Others: 17.5 h (1955Th01), 17.2 h (1952Fu04, earlier abstract in Phys. Rev. 83, 875 (1951)); 16.5 h {I5} (1951Ho42); 15.7 h (quoted by 1948Se40 compilation from a priv. comm., with formation of {+76}Br in As(|a,3n) reaction at Berkeley cyclotron facility). 
MOMM1,MOME2$other: |g(|q,H,Temp) (1992Gr20,1988Gr26,1988Wh03). Q=0.270 {I3} in 1960Li11 is reanalyzed to +0.251 {I4} in 2016St14, based on electric field gradients in {+79}Br analyzed in 1966Br03 and 2000Ha64. Hyperfine structure study by NMR technique on oriented has been studied by 1993Oh09 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
J$cascade of M2-M1 transitions from 103 level to 1- g.s. limits J|p(103 level) to 0+,2+,3+,4+ and J|p(45 level) to 0-,1-, 2-. Very weak (or absence of) crossover transition from 103 level favors 4+ for 103 level, thus 2- for 45 level. A band based on the 103 level has been identified in (HI,xn|g) which is consistent with a 4+ choice for the 103 level. First excited state in {+78}Br, {+80}Br, {+82}Br has J|p=2- which supports the given assignment for 45 level, however, a solid argument for unique assignments for 45.5- and 102.6- level still seems lacking 
T$from (ce)(ce)(t) in {+76}Kr |e decay (1973Lo07) 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Possible configuration=|p3/2[431]~#|n5/2[422] (1982Do11) 
J$see comment for 45 level 
T$from 1980Ha23. Others: 1.35 s {I5} (1981Vo04), 1.3 s (1979Kr04), 1.49 s {I2} (1978Sc30) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: NS
level_comment:
J$E1 |g to 1-; 199.8|g M1+E2 from 1+; possible |g to (4)+ 
T$|g|g(t) in {+76}Kr |e decay (1973Lo07) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
J$89.5|g D, |DJ=1 to (3-); 199.3|g D, |DJ=0 to (4)+. Possible configuration=|pg{-9/2}~#|n(p{-3/2} or f{-5/2}) (1982Do11) 
T$RDDS in (HI,xn|g) (1986KuZW). Other: |g|g(t) (1982Do11) 


level_energy_unit: KEV
level_spin_parity: (5)
level_lifetime_unit: PS
level_comment:
J$124.0|g to (4-) can only be E1 or M1 from RUL; 262.2|g D, |DJ=1 from (6-) 
T$from RDDS in (HI,xn|g) (1986KuZW) 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: PS
level_comment:
J$M1+E2, |DJ=1 |g to (6)+ and band assignment. 350|g(|q) (|g to (5)+) (1981We07), however, disagrees with that expected for |DJ=2 transition 
T$RDDS in (HI,xn|g) (1986KuZW) 


level_energy_unit: KEV
level_spin_parity: (9)+
level_lifetime_unit: PS
level_comment:
J$E2, |DJ=2 |g to (7)+; |DJ=1, M1+E2 |g to (8)+. 526|g(|q) (|g to (7)+) (1981We07), however, disagrees with that expected for |DJ=2 transition 
T$weighted average of 0.59 ps {I6} from DSA method (1990Bu07) and 0.83 ps {I14} (RDDS,1986KuZW) in (HI,xn|g); 0.707 ps {I+35-28} from DSAM (2022Xu06) in ({+12}C,p3n|g). 


level_energy_unit: KEV
level_spin_parity: (10)+
level_lifetime_unit: PS
level_comment:
J$E2, |DJ=2 |g to (8)+; band assignment 
T$unweighted average of 0.49 ps {I6} from DSA method (1990Bu07) and 0.90 ps {I14} (RDDS,1986KuZW) in (HI,xn|g), and 0.652 ps {I35} from DSAM (2022Xu06) in ({+12}C,p3n|g) 


level_energy_unit: KEV
level_spin_parity: (11)+
level_lifetime_unit: PS
level_comment:
J$E2 |DJ=2 |g to (9)+; band assignment 
T$weighted average of 0.284 ps {I14} from ({+12}C,p3n|g) and 0.21 ps {I4} from (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (13+)
level_lifetime_unit: PS
level_comment:
J$E2 |DJ=2 |g to (11+); band assignment 
T$weighted average of 0.208 ps {I28} from ({+12}C,p3n|g) and 0.20 ps {I2} from (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (15+)
level_lifetime_unit: PS
level_comment:
J$E2, |DJ=2 |g to (13+); band assignment 
T$weighted average of 0.097 ps {I14} from ({+12}C,p3n|g) and 0.11 ps {I3} from (HI,xn|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+,2+,4+)
level_comment:
E,J$triplet. Analogs of 1122, 0+; 1216, 2+; 1330, 4+ levels in {+76}Se; estimated uncertainty=100 keV 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$This level is assigned 12+ by 1990Bu07 but a 1067.2|g is placed from a 3286 level in 1997Wi01 and 1997Pa35 


level_energy_unit: KEV
level_spin_parity: (12+)
level_comment:
$The 12+ level is suggested at 2578 by 1990Bu07 on the basis of 1066|g in coin with 823|g. But 1066|g is not confirmed in later studies of 1997Pa35 and 1997Wi01 


level_energy_unit: KEV
level_spin_parity: (14+)
level_comment:
$The 14+ band member is suggested at 3836 by 1990Bu07 on the basis of a 1258|g in coin with other |g rays in the band, but 1258|g is placed from a 4365 level in 1997Pa35 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=1.02 ps {I+5-4}. T{-1/2}=0.71 ps {I11} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.94 ps {I5}. T{-1/2}=0.65 ps {I10} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.57 ps {I+7-6}. T{-1/2}=0.40 ps {I8} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=1.17 ps {I+13-7}. T{-1/2}=0.81 ps {I+15-13} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 11+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.41 ps {I2}. T{-1/2}=0.284 ps {I44} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.46 ps {I+7-6}. T{-1/2}=0.32 ps {I7} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.78 ps {I+6-5}. T{-1/2}=0.54 ps {I9} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 11+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.28 ps {I+9-7}. T{-1/2}=0.19 ps {I+7-6} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.53 ps {I4}. T{-1/2}=0.37 ps {I6} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 13+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.30 ps {I4}. T{-1/2}=0.208 ps {I43} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 12-
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.37 ps {I+7-6}. T{-1/2}=0.256 ps {I60} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.15 ps {I2}. T{-1/2}=0.104 ps {I21} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 15+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=0.14 ps {I2}. T{-1/2}=0.097 ps {I20} with a systemmatic uncertainty of 15% added in quadrature by the evaluators 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
MOMM1$from NMR-nuclear orientation (1993Oh09); measured |m=0.9730 {I6} by 1993Oh09 is re-evaluated to 0.9731 {I6} by 2019StZV. Others: 0.9738 {I5} (1992Pr06, NMR nuclear orientation); 0.92 {I5} (1992Gr20,1988Gr26). 
MOME2$multiple adiabatic passage NMR on oriented nuclei (1998Se09). Value of 0.530 {I22} is re-evaluated to 0.50 {I2} in 2016St14 
$Configuration=|p3/2[312] (1992Gr20) 
J$atomic-beam method (1959Gr92); parity from L({+3}He,d)=1 
T$from integral counting with an ionization chamber (1975Wa28); uncertainty quoted here is dominated by 0.2% systematic uncertainty specified in 1975Wa28, statistical uncertainty is negligible. Others: 53.76 h {i96} (2012Ba12), 54.6 h {i2} (1963Ku06), 58.0 h {i5} (1959Gi62), 57 h {i1} (1951Ho42), 58 h {i2} (1948Wo08) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$atomic-beam magnetic resonance method (1980Ek02); parity from L({+3}He,d)=4 
T$from |g-decay curve (1961Go39). Others: 4.2 min {I2} (1972De54), 4.2 min {I2} (1959Go67), 1971Do01, 1955Th01 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
MOMM1$time dependent perturbed angular correlation technique (1991Gr15) 
$Static Q|?0.4 (1978HaXP, differential PAC method (1978HaXP). Note that this measurement is listed only in 1989Ra17 compilation, not in 2016St14 evaluation or 2014StZZ compilation, thus should be viewed caution 
J$L({+3}He,d)=2; (E2) |g to 9/2+ 
T$|g|g(t) in {+77}Kr |e decay (1967Ho16) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
$In ({+3}He,d), 162 and 167 levels are unresolved 
J$L({+3}He,d)=3; M1+E2 |g to 3/2-; |g(|q) and excitation function in (p,n|g) rule out 1/2 and 3/2- 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: PS
level_comment:
J$M1+E2 |g to 5/2+. Excitation function in (p,n|g) gives J=3/2 (1988Fe07); however, 1977Fe13, also from excitation in (p,n|g), assign J=5/2 
T$(ce)|g(t) in {+77}Kr |e decay 


level_energy_unit: KEV
level_spin_parity: 7/2(+)
level_comment:
J$log| {Ift}=6.4 from 5/2+; |DJ=1, (M1) |g to 9/2+. Excitation function and |g(|q) in (p,n|g) favor 7/2 over 5/2 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$L({+3}He,d)=(0); isotropic |g(|q) in (p,n|g). Note that L({+3}He,d)=3 was also suggested by 1978Kll0, which could relate this level to 781.1 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$log| {Ift}=6.7 from 5/2+; gammas to 3/2- and (3/2)+. Excitation function in (p,n|g) suggests 1/2+ or 3/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2)
level_comment:
J$gammas to 5/2+ and 9/2+; log| {Ift}=7.5 from 5/2+. Excitation function in (p,n|g) supports 7/2 but the analysis is complicated by the presence of impurity lines (1988Fe07) 


level_energy_unit: KEV
level_comment:
$E(p)(c.m.)=3336 keV {I10} 
$Level-energy difference=207 keV {I11}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 239 and/or 250 levels in {+77}Se 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(p)(c.m.)=3650 keV {I10}, |G=10 keV {I2} 
$Level-energy difference=521 keV {I11}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 521, 3/2- level in {+77}Se 
S$0.34 in (d,p) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E(p)(c.m.)=3820 keV {I10}, |G=15 keV {I2} 
$Level-energy difference=691 keV {I11}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 680, 5/2+ level in {+77}Se 
S$1.23 in (d,p) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(p)(c.m.)=4092 keV {I10}, |G=23 keV {I2} 
$Level-energy difference=963 keV {I11}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 956, 1/2+ level in {+77}Se 
S$0.25 in (d,p) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(p)(c.m.)=4158 keV {I10}, |G=18 keV {I2} 
$Level-energy difference=1029 keV {I11}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 1005, 3/2- level in {+77}Se 
S$0.17 in (d,p) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(p)(c.m.)=4216 keV {I10}, |G=31 keV {I2} 
$Level-energy difference=1087 keV {I11}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 1126, 1/2+ level in {+77}Se 
S$0.76 in (d,p) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E(p)(c.m.)=4360 keV {I10}, |G=24 keV {I2} 
$Level-energy difference=1231 keV {I12}, relative to the 8401 energy normalized to g.s. in {+77}Se; identified as analog of 1252, 5/2+ level in {+77}Se 
S$1.11 in (d,p) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=1.93 (4.5|'), 0.68 (8|'), 0.38 (12|') 
S$for p{-3/2} from |s at 4.5|'. Others: 0.35 (1983Zu01), 0.146 (1978Kl10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=4.23 (4.5|'), 4.05 (8|'), 2.93 (12|') 
S$for g{-9/2} from |s at 12|'. Others: 2.1 (1983Zu01). 1978Kl10 give L=3, S=1.22, 2.14 for a level at 114 that may be a composite of 106 and 130 levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W (mb/sr)=2.82 (4.5|'), 2.84 {I34} (8|'), 1.45 (12|') 
S$from |s at 8|' 
L,S$others: 0.52, 0.44 for L=1 and 2.06 for L=3, f{-5/2} (1983Zu01); 0.107, 0.18 for L=1 and 0.84, 1.46 for L=3 (1978Kl10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W (mb/sr)=3.17 {I38} (4.5|'), 0.83 (8|'), 0.63 (12|') 
L,S$see comment for 162 level. Spectroscopic factor from |s at 4.5|' 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.82 (4.5|'), 0.25 (8|'), 0.18 (12|') 
L$1 in 1983Zu01, confirmed in 2008KaZT. 1978Kl10 give L=1+3 with corresponding S factors 
S$for 3/2- from |s at 4.5|'. Others: 0.119, 0.102 (1983Zu01), 1978Kl10 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=2.80 (4.5|'), 0.90 (8|'), 0.62 (12|') 
S$from |s at 4.5|'. Others: 0.70, 0.60 (1983Zu01); 0.17, 0.29 (1978Kl10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.56 (4.5|'), 0.59 (8|'), 0.36 (12|') 
S$for f{-5/2} from |s at 8|'. Others: 0.44 (1983Zu01); 0.18, 0.31 (1978Kl10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.12 (4.5|'), 0.039 (8|'), 0.036 (12|') 
S$for 3/2- from |s at 4.5|'. Other: 0.020, 0.018 (1983Zu01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.092 (4.5|'), 0.093 (8|'), 0.072 (12|') 
L$ (3) in 1978Kl10, L=3 confirmed in 2008KaZT 
S$for 5/2- from |s at 8|'. Others: 0.035, 0.061 (1978Kl10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.67 (4.5|'), 0.23 (8|'), 0.14 (12|') 
S$from |s at 4.5|' 
S$others: 0.116, 0.101 (1983Zu01); 0.037, 0.066 (1978Kl10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.51 (4.5|'), 0.21 (8|'), 0.14 (12|') 
S$from |s at 4.5|' 
S$others: 0.105, 0.091 (1983Zu01); 0.032, 0.057 (1978Kl10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.24 (4.5|'), 0.17 (8|'), 0.10 (12|') 
E$ most likely a doublet. see Adopted Levels for details 
L$(2+4) in 1983Zu01, L=2 in 2008KaZT but no other data details 
S$for L=2; 0.079, 0.042 for L=4 (1983Zu01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.29 (4.5|'), 0.25 (8|'), 0.17 (12|') 
S$from |s at 12|'. Other: 0.20, 0.105 (1983Zu01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=1.35 (4.5|'), 1.17 (8|'), 0.89 (12|') 
L$4 in 1983Zu01; L=4 confirmed in 2008KaZT. L=(3) in 1978Kl10 is discrepant 
S$from |s at 12|'. Others: 1.24, 0.66 (1983Zu01); 0.64, 1.12 for L=(3) (1978Kl10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$Level not reported by 1983Zu01, unless this level is the same as the L=4, 1908 level reported by 1983Zu01 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.162 (4.5|'), 0.104 (8|'), 0.082 (12|') 
S$from |s at 12|'. Other: 0.15, 0.082 (1983Zu01). See also comment for 1879 level 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.30 (4.5|'), 0.21 (8|'), 0.15 (12|') 
L$(1) in 1983Zu01, L=1 confirmed in 2008KaZT. 
S$from |s at 4.5|'. Other: 0.014, 0.012 (1983Zu01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.11 (4.5|'), 0.040 (8|'), 0.030 (12|') 
S$from |s at 4.5|' 
L$(1) in 1983Zu01, L=1 confirmed in 2008KaZT. 1978Kl10 report a level at 2142 with L=3, which is probably a composite of 2132 and 2150 levels reported by 1983Zu01 
S$other: 0.020,0.017 (1983Zu01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (mb/sr)=0.23 (4.5|'), 0.065 (8|'), 0.042 (12|') 
L$(1) in 1983Zu01, L=1 confirmed in 2008KaZT. 
S$from |s at 4.5|'. Other: 0.033, 0.029 (1983Zu01) 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2)
level_comment:
J$excitation function data supports 7/2, but the analysis is complicated by the presence of impurity lines 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J$spin from atomic-beam method (1980Ek02); parity from L(p,d)=1+3 and L({+3}He,d)=1 
T$weighted average of 6.46 min {I4} (1973Hi01), 6.4 min {I3} (1973ArZI), 6.4 min {I4} (1962Va27), 6.47 min {I10} (1961Sc11), 6.5 min {I1} (1961Ri02), 6.25 min {I20} (1960Pi06), 6.5 min {I5} (1951Ho42), 6.3 min {I2} (1938Bu04), 6.4 min {I1} (1937Sn02) 
MOMM1$static nuclear orientation with measurement of |g rays (1992Pr06). See also 2005St24 compilation 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
MOMM1$TDPAD method (1973Pl07). See also 2005St24 compilation 
T$unweighted average of 8.3 ns {I9} from |g(t) in (|a,n|g) (1979Kl05) and 14.2 ns {I3} from pulsed-beam method in {+78}Ge IT decay (1972Ch34) 
J$sign of g-factor suggests |p=-. The ratio I|g(148|g)/I|g(32|g) suggests (E1,M1) for 32|g and (E2,M2) for 148|g. |g(|q) of 32|g rules out J=0 for 32|g. Thus J|p=(1-,2-) for 32 level and J|p=(1-, 2-, 3-, 4) for 181 level. Long T{-1/2} of 181 level suggests M2 rather than E2. |g to 32 level and no |g decay to g.s. from 181 level supports J|p=(4+) for 181 level. Similarly J|p=(2-) for 32 level, assuming 32|g is E1. L(p,d)=1 gives positive parity 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1$g=+1.028 {I3} (1974FoYO,NMR). Others: g=+1.02 {I2} (1972Ch34, differential-perturbed angular distribution method); g=+1.025 {I3} (1971Br31,NMR). See also 2005St24 compilation 
J$see comments for 32 level 
T$from |g(t). Weighted average of 120 |ms {I1} (1982Be03), 119.2 |ms {I10} (1970De46), 111 |ms {I10} (1969Ru10), 123 |ms {I25} (1968Io01), 124 |ms {I25} (1967Iv03,1967Iv04), 118.0 |ms {I15} (1961Sc11), 127 |ms {I5} (1958Du80). Others: 80 |ms {I2} (1971In04) is discrepant, 127 |ms (1965Mc03) 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_lifetime_unit: NS
level_comment:
J$L(p,d)=2+4; |g to 1+ 
T$from |g(t) in {+77}Se(|a,2np|g),{+75}Ge({+7}Li,5n|g) (1982Be03). Other: |g(t) measurement in 1979Kl05 gives 13.8 ns {I11} from the unresolved |g-ray doublet at 46.3 keV 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_comment:
J$|DJ=1 |g's to (5-) and (5+) 
T$from |g(t). Weighted average of 6.5 ns {I7} (1979Kl05) and 9.0 ns {I10} (1982Be03) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=(1) |g's to (5+) 
T$from 196|g(t) in {+77}Se(|a,2np|g),{+75}Ge({+7}Li,5n|g) (1982Be03), assuming 196.0|g seen in that work mainly deexcites the 423 level 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
E$573 in ({+3}He,d) and 579 in (p,d) are assumed (by evaluators) to correspond to the same level. 
J$L(p,d)=1; L({+3}He,d)=3 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
E$1254 in ({+3}He,d) and 1261 in (p,d) are assumed (by evaluators) to correspond to the same level. 
J$L(p,d)=1; L({+3}He,d)=3 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
T$pulsed beam technique (1972Ch34). 
g-factor=-0.56 {I2} (1973Pl07). This has been deduced with reference to g-factor for 198 keV level in {+19}F=+1.442 {I3} (by differential perturbed angular distribution method). 1973BaYF get -0.56 {I2} 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$from 'adopted levels'. In {+78}Br it decay measured values from |g(t) are: 119.2 |ms {I10} (1970De46,pulsed beam), 80 |ms {I2} (1971In04), 111 |ms {I10} (1969Ru10), 123 |ms {I25} (1968Io01), 124 |ms {I25} (1967Iv03), 127 |ms (1965Mc03), 118 |ms (1961Sc11), 127 |ms {I5} (1958Du80) 
g-factor=+1.028 {I3} (1974FoYO), NMR-PAC method in {+78}Se(p,n). Others: +1.02 {I2} (1972Ch34) by differential perturbed angular distribution and stroboscopic observation of perturbed angular distribution of |g-rays; 1.025 {I3} (1971Br31) by NMR-PAC 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
$Level proposed by the evaluators based on ({+11}B,3n|g) results, reassigning 196.0|g 
T$from 196|g(t) (1982Be03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius=4.1629 fm {I21} (2013An02) 
J$atomic-beam method (1932To02,1930Br01,1976Fu06); L({+3}He,d)=1 
$Probable |pp{-3/2} orbital 
MOMM1$NMR method (1972Bl07). Others: 1954Wa37, 1951Sh33, 1949Zi02, 1947Br24, 1947Po16 
MOME2$atomic-beam magnetic resonance method (1954Ki11), reanalyzed by 2001Bi17. Recalculations: +0.318 {I5} (2004Al08), +0.305 {I5} (2000Ha64), +0.331 {I4} (1978Ta24), +0.293 (1962Ko22), +0.367 or +0.445 (1971Am02). Others: 1954Sc10, 1954Ro43, 1953Ko22, 1953Fa33, 1951De16, 1951Go37, 1950Sm56, 1948To10, 1948Po09. Q({+79}Br)/Q({+81}Br) (1969He04) 
Magnetic octupole moment=+0.116 (1966Br03,1989Ra17) (hyperfine structure measurement using atomic-beam magnetic resonance method). Recalculated as +0.123 or +0.093 by 1971Am02 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$E3 |g to 3/2- 
$Probable |pg{-9/2} orbital 
T$weighted average of 4.86 s 10 (1986Al11), 4.97 s 10 (1972Jo05), 4.86 s 4 (1967Bo26,1968Bo52), 4.88 s {I7} (1967Yu01), 4.87 s {I15} (1967Sc14), 4.80 s {I5} (1963Ka34), 4.78 s {I15} (1961Go39). Others: 5.1 s 4 (2009Mu15), 5.08 s {I7} (1962An13), 1974Co11, 1970Ru08, 1967Ab08, 1954Sc37 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$M1+E2 |g to 3/2-; L({+3}He,d)=3+4 for a doublet 207+217 where L=4 corresponds to 207 level and L=3 to 217 level 
T$from DSAM in Coul. ex. (1994Sp05). Others: 51 ps {I12} (RDDS in (|a,pn|g) (1988Sc13)), 34 ps {I23} or 52 ps {I35} (from B(E2) in Coul. ex.); |<0.14 ns (1970Be79,1969Sh12) 
MOMM1$from |g(|q,H) in Coul. ex. (1994Sp05) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$M1 |g to 5/2-; M1+E2 |g to 3/2-; log| {Ift}=6.15 from 1/2- 
T$from |gce(t) (1972OhZX). Others: 0.91 ns {I8} |g|g(t) (1970Be79), >125 ps ((|g,|g') 1970We01). Value from 1970Be79 is inconsistent with B(E2) (from Coul. ex.) and |d(261|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=1. 1970We01 suggest that J=1/2 is favored from a comparison of measured A{-2} for 306|g(|q) in Coul. ex. (1967Ro03) and that expected from |d=0.13 (deduced from B(E2)(|^) and T{-1/2}) 
T$from DSAM in Coul. ex. (1994Sp05). Other: 8.3 ps {I17} for J=1/2, 17 ps {I3} for J=5/2 in (|g,|g') (1970We01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
J$L({+3}He,d)=2; |g to 9/2+ 
T$from T{-1/2}(173.7|g)(partial)=6 ns {I2} (1995Kh02) in (|g,|g') and adopted branching ratio 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=1; excitation function in (d,n|g) supports 3/2 
T$from (|g,|g') (1970We01) for 1/2. T{-1/2}=26 ps {I8} for J=3/2 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=3; |DJ=0,1 |g to 3/2- and Coul. ex. 
T$from DSAM in Coul. ex. (1994Sp05). Other: 1.3 ps {I4} (from (|g,|g') (1970We01)) 
MOMM1$|g(|q,H) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=1; M1+E2 |g to 5/2- 
T$from DSAM in Coul. ex. (1994Sp05). Other: 2.0 ps {I3} in (|g,|g') (1970We01) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to 5/2-; |DJ=2, E2 |g to 3/2- 
T$from DSAM in Coul. ex. (1994Sp05). Other: 1.2 ps {I2} in (|g,|g') (1970We01) 
MOMM1$|g(|q,H) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_lifetime_unit: PS
level_comment:
J$|DJ=0,1 |g to 3/2-; excitation function in (d,n|g) supports 5/2; not 1/2 from |g(|q) 
T$DSAM in Coul. ex. (1994Sp05) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$L({+3}He,d)=2 
E$from energy matching this level seems to correspond to 954.08 but L({+3}He,d)=2 is inconsistent with J|p deduced |g(|q) and excitation data for 954.08 level 


level_energy_unit: KEV
level_spin_parity: (7/2)
level_comment:
J$|DJ=1 |g to 5/2-; possible |g to 3/2-; L({+3}He,d)=4 implies 7/2+ or 9/2+, but L({+3}He,d)=3 implying 5/2-,7/2- is also suggested 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J$L({+3}He,d)=3; excitation function in (d,n|g) supports 7/2 whereas |g(|q) in ({+6}Li,3n|g) favors 9/2 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2-)
level_comment:
J$|gs to 3/2- and (7/2)-. Excitation function in (d,n|g) suggests 3/2 whereas 9/2 is suggested by |g(|q) in ({+6}Li,3n|g). There may be two separate levels near this energy 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$L({+3}He,d)=2; |g to (7/2)- 
Uncertain in {+79}Kr |e decay. There may be two separate levels near this energy. One deexcited by 666|g (in ({+6}Li,3n|g) and (d,n|g)) and the other by 1358|g, 1575|g (in (n,n'|g)) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 7/2-; |DJ=1, (M1+E2) |g to 9/2- 
T$from DSAM in ({+7}Li,4n|g) E=32 MeV (1999Ra02). Other: 0.42 ps {I+35-14} (DSA in (|a,p2n|g),1988Sc13) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$|DJ=1, dipole |g from 15/2-; |gs to (9/2-) and 11/2-. In {+76}Ge({+6}Li,3n|g), (9/2-) suggested by 1988NaZP from |g(|q) and excitation function is inconsistent 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 9/2-; |g to 13/2+ 
T$effective T{-1/2} (not corrected for feeding time) from DSA in (|a,p2n|g) (1988Sc13) 


level_energy_unit: KEV
level_spin_parity: (21/2)-
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to (19/2)-; |DJ=(2), (E2) |g to 17/2- 
T$others: 0.76 ps {I14} (1988Sc13), 0.69 ps {I21} (1999Ra02) 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 21/2+; band member 
T$others: 0.28 ps {I14} (1988Sc13), 0.25 ps {I+17-10} (1999Ra02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T$from |g(ce)|g(t) (1972OhZX). Others: 0.91 ns {I8} (|g|g(t),1970Be79). Value from 1970Be79 is inconsistent with B(E2) (from Coul. ex.) and |d(261|g) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E$1988NaZP propose two levels near this energy but all three |g-rays can be fitted assuming only one level 


level_energy_unit: KEV
level_comment:
E$IAR of 1156, 1/2+ in {+79}Se. 1968Zi03 report a doublet near this energy with values of 10945 and 10976 
S$in {+78}Se(d,p) S=0.47 (1978Mo12), 0.66 (1965Li08) 
E(p)(lab)=4694 ({+78}Se(p,p)); 4697 ({+78}Se(p,n), 1968Ba23); 4676, 4707 (1968Zi03) 
|G(total)=43 keV {I5} ({+78}Se(p,p)); 46 keV {I10} ({+78}Se(p,n),1968Ba23) 


level_energy_unit: KEV
level_comment:
E$IAR of 1253, 5/2+ in {+79}Se 
S$for J=5/2. In {+78}Se(d,p) S=0.24 (1978Mo12), 0.34 (1965Li08) 
E(p)(lab)=4808 ({+78}Se(p,p)); 4810 ({+78}Se(p,n), 1968Ba23); 4807 (1968Zi03) 
|G(total)=24 keV {I9} ({+78}Se(p,p)); 38 keV {I10} ({+78}Se(p,n), 1968Ba23); 35 keV {I7} (1968Zi03) 


level_energy_unit: KEV
level_comment:
E$IAR of 1491, 1/2+ in {+79}Se 
S$in {+78}Se(d,p) S=0.04 (1978Mo12), 0.066 (1965Li08) 
E(p)(lab)=5089 ({+78}Se(p,p)); 5088 ({+78}Se(p,n), 1968Ba23); 5086 (1968Zi03) 
|G(total)=16 keV {I5} ({+78}Se(p,p)); 35 keV {I10} ({+78}Se(p,n), 1968Ba23); 30 keV {I6} (1968Zi03) 


level_energy_unit: KEV
level_comment:
E$IAR of 1597, 3/2+ in {+79}Se 
E(p)(lab)=5168 (1968Ba23), 5143 (1968Zi03) 
|G(total)=35 keV {I10} (1968Ba23), 45 keV {I8} (1968Zi03) 


level_energy_unit: KEV
level_comment:
E$there are probably two levels near this energy: 1332 level defined by 809.9|g, 1115.9|g and 1333 level defined by 571.6|g and possibly 809|g. J|p(1332)=3/2- and J|p(1333)=(5/2,7/2,9/2) (see Adopted Levels and gammas). 1989DjZW propose only one level with J|p=3/2- 


level_energy_unit: KEV
level_comment:
S$doublet. First value for J|p=9/2+ and second for J|p=5/2-. Other: (2J+1)S=2.85 for L=4, 9/2+ and 1.43 for L=3, 5/2- 


level_energy_unit: KEV
level_comment:
L$from 1978Kl10. Authors also give L=3+4 as a possible choice 
S$for J|p=7/2- (1978Kl10). 1983Zu01 do not give C{+2}S' 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$this group reported only by 1978Kl10 may correspond to 1039+1080 groups seen by 1983Zu01, thus the 1053 level is not listed in the Adopted Levels 


level_energy_unit: KEV
level_comment:
L,S$from 1978Kl10 
E$doublet at 2516 (1978Kl10) corresponds to 2512, 2529 levels 
S$for L=1. For L=3, C{+2}S'=0.16, 0.27 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
Population of this level here is uncertain since 397|g (about 10 times as intense as 136|g (see Adopted Gammas)) has not been reported by 1988Sc13. However, in a spectrum shown by 1988Sc13 there is some evidence of a 397 |g-ray line which has been assigned to an impurity by 1988Sc13 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_uncertain: ?
level_comment:
$Population of this level in this reaction is uncertain since 1115|g or 1333|g (intense |g rays from this level in Adopted Gammas) is not seen 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$DSA in (|a,pn|g) and (|a,p2n|g); weighted average of four separate values from singles |g and p|g coin data 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
T$DSA in (|a,pn|g) and (|a,p2n|g); weighted average of values from singles |g and p|g coin data. Feeding correction is not applied 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
T$for J=1/2. T{-1/2}=16.6 ps {I34} for J=3/2 
J$1970We01 suggest that 1/2 is favored from 306|g(|q) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0395 {I33} (1967Ro03), 0.0260 {I22} (1985Si08), <0.02 (1968An12), 0.023 {I5} (1957Wo32). Weighted average=0.029 {I5} 
T$B(E2)=0.0395 {I33} (1967Ro03) and |d(217|g) from |g(|q) imply T{-1/2}=34 ps {I23} (52 ps if B(E2)=0.0260 {I22} (1985Si08)) for |d=0.088 {I30} and 4.3 ns for |d=4.9. The former T{-1/2} is in agreement with adopted T{-1/2}=51 ps {I12} (1988Sc13) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
B(E2)=0.0070 {I6} (1967Ro03), 0.0046 {I15} (1968An12), 0.0040 {I4} (1985Si08). Weighted average=0.0049 {I10} 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0211 {I18} (1967Ro03), 0.011 {I2} (1968An12), 0.0115 {I20} (1985Si08). Weighted average=0.015 {I3} 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
B(E2)=0.0033 {I5} (1967Ro03), 0.0032 {I3} (1985Si08), <0.002 (1968An12). Weighted average=0.0032 {I4} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.095 {I9} (1967Ro03), 0.096 {I19} (1968An12), 0.088 {I8} (1985Si08). Weighted average=0.092 {I8} 
T$0.9 ps {I4} deduced from B(E2) and |d(523|g)=0.21 {I5}. This agrees with 1.3 ps {I3} from (|g,|g'). Other possible |d(423)=-12 {I+5-23} gives T{-1/2}=20 ps {I2} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0152 {I23} (1967Ro03), 0.018 {I5} (1968An12), 0.017 {I5} (1985Si08). Weighted average=0.0159 {I23} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.128 {I22} (1967Ro03), 0.12 {I3} (1968An12), 0.114 {I10} (1985Si08). Weighted average=0.117 {I10} 
T$1.2 ps {I2} (from B(E2) value and J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
MOMM1$atomic-beam (1964Wh05) 
MOME2$atomic-beam (1964Wh05). Value recalculated by 1978Ta24 as 0.196 {I3}, 0.181 {I4} by 2000Ha64 and 0.185 {I2} by 2001Bi17. 1989Ra17 quoted value from 1978Ta24 
J$atomic-beam (1959Li21) and L(p,d)=L(d,p)=1 from 3/2- 
T$from 1972Co26 
$ Configuration=(|p2p{-3/2}{+-1})(|n2p{-1/2}{+-1}) (1978Do06) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
MOMM1$differential PAD in (p,n|g) (1973Pl07) 
MOME2$ 0.173 {I6} from differential PAC in {+80}Br IT decay (1978Ta24); recalculated as 0.159 {I7} by 2000Ha64 and 0.163 by 2001Bi17. 1989Ra17 quoted value from 1978Ta24 
J$M3 |g from 5-, and E1 |g to 1+ 
T$from |g|g(t) in {+80}Br IT decay (1978Ta24). Other: 7.8 ns {I5} from |g|g(t) in (p,n|g) (1977Do08) 
$Configuration=(|p(2p{-3/2}){+-1})((|n(1g{-9/2}){+3}){-7/2}) (1978Do06) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$atomic-beam (1964Wh05) 
MOME2$atomic-beam (1964Wh05). Value recalculated as +0.751 {I10} by 1978Ta24, +0.69 {I2} by 2000Ha64 and +0.709 by 2001Bi17. 1989Ra17 quoted value from 1978Ta24 
J$from atomic-beam (1959Li21) and L(d,p)=L(p,d)=4 from 3/2- 
T$from 1990Ab06. Others: 4.754 h {I32} at room temperature and 4.791 h {I34} at 77|'K (2003Al36); 4.42 {I1} (1969Ka06), 4.42 {I1} (1968Re04), 4.37 {I4} (1961Ha32), 4.40 {I5} (1960Sc04), 4.38 {I2} (1957Ki21), 1958Gu09, 1951Mi16, 1938Bu04, 1937Sn02, 1937Bo10. It should be noted that the value obtained by 2003Al36 is quoted with 0.7% uncertainty but is about 7.5% too high as compared to the other values in the literature; thus not used in deducing the adopted value. Weighted average of all the values quoted above but with uncertainty increased to 0.01 for the value from 1990Ab06, is 4.43 h {I3} 
$ Configuration=|p2p{-3/2}{+-1}|n1g{-9/2}{++1} (1978Do06) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J$from |g(|q) in (d,2n|g); D(+Q) |g's to 5- and (3)-. Positive parity less likely since it would give large M2 admixture 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$from |g(|q) in (d,2n|g), |DJ=0,1 |g's to (4)- and (6-). Negative parity suggested by L(p,d)=4 from 3/2- for 512 group 
J$ 4(-) IN 1994HoZU 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$ M1 |g to (2)+; |DJ=2 |g to 1+; (E1) |g to (4)-. Positive parity also suggested by L(p,d)=(3) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$|g to 1+. 661|g(|q) in (d,2n|g) and L(p,d)=1+3 from 3/2- give 1+, 2+. But |g to 586 level would rule out 1+ for 661 and 5- for 586 level 


level_energy_unit: KEV
level_spin_parity: (3,4-,5-)
level_comment:
J$|g to (3)- and |g(|q) in (d,2n|g) for |g to (4)-. L(p,d)=2+4 from 3/2- gives negative parity for 683 and/or 685 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$|g to (4)-; average resonance capture in (n,|g); L(p,d)=2+4 and L(d,p)=(2) give negative parity for 683 and/or 685. 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_comment:
J$|g's to 1+, 2- and (2)+. L(p,d)=1+3 and from 3/2- supports positive parity for 718 and/or 724. Excitation function in (p,n|g) disfavors J=3. Average resonance capture gives 0-,3- for 724+727 doublet 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$L(d,p)=1 from 3/2-. |g(|q) in (p,n|g) for |g to 1+ gives |DJ=0,1. Excitation function in (p,n|g) disfavors J=1 
J$ 3+ IN 1994HoZU is in disagreement with |g(|q) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$L(p,d)=1 from 3/2- and |g's to 2- and (2)+. |g(|q) in (p,n|g) for |g to 2- disfavors J|p=2+. Excitation function in (p,n|g) disfavors J=1 


level_energy_unit: KEV
level_spin_parity: (1-,2,3)
level_comment:
J$|g's to (2)+ and (3)-. Primary |g (in (n,|g)) from 1-,2-. L(p,d)=2+4 from 3/2- gives negative parity for 908 and/or 915 


level_energy_unit: KEV
level_spin_parity: (0+,1,2)
level_comment:
J$|g's to 1+ and (2)+. |g(|q) in (p,n|g) for |g to 1+ gives |DJ=0,1. L(p,d)=2+4 from 3/2- gives negative parity for 908 and/or 915 


level_energy_unit: KEV
level_spin_parity: (1-,2,3+)
level_comment:
J$|g's to 1+ and (3)-. L(p,d)=1+3 from 3/2- and L(d,p)=(1) give positive parity for 1143, 1146, and/or 1148 levels 


level_energy_unit: KEV
level_spin_parity: (LE 4)
level_comment:
J$primary |g from 1-,2-. L(p,d)=1+3 from 3/2- gives (1,2,3)+ whereas L(d,p)=2 from 3/2- gives (1 to 4)- for 1191, 1198 and/or 1203. J|p=4+ is unlikely 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1978Ta24). Other values from ce|g(t): 7.43 ns {I25} (1966Tu02), 7.4 ns {I3} (1965Hu02), 7.37 ns {I21} (1964Fl01), |<4 ns (1951Wr13) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T$from 1990Ab06. Others: 4.754 h {I32} at room temperature and 4.791 h {I34} at 77|'K (2003Al36); 4.42 {I1} (1969Ka06), 4.42 {I1} (1968Re04), 4.37 {I4} (1961Ha32), 4.40 {I5} (1960Sc04), 4.38 {I2} (1957Ki21), 1958Gu09, 1951Mi16, 1938Bu04, 1937Sn02, 1937Bo10. It should be noted that the value obtained by 2003Al36 is quoted with 0.7% uncertainty but is about 7.5% too high as compared to the other values in the literature; thus not used in deducing the adopted value. Weighted average of all the values quoted above but with uncertainty increased to 0.01 for the value from 1990Ab06, is 4.43 h {I3} 


level_energy_unit: KEV
level_spin_parity: (2)+&(3)-
level_comment:
E,J$doublet; J|p from 'adopted levels' 
$ I|g/E|g{+5}=4.06 {I5} (E(n)=2.8 keV), 6.4 {I3} (E(n)=58 keV) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0-,3-
level_comment:
E,J$723+727 doublet with J|p=(1,2) for one and (1-,2,3) for the other 
$ I|g/E|g{+5}=4.9 {I4} (E(n)=2.8 keV), 3.3 {I4} (E(n)=58 keV) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: H
level_comment:
T$ 0.7 ns shown for this level in Fig. 1 of 2011Wa21 is a typo, as communicated by the authors to the compilers. 0.7 ns is the half-life listed for 331, 5+ level in Adopted Levels of {+80}Br in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
<r{+2}>{+1/2}(charge)=4.1599 fm {I21} (2013An02). 
J 3/2 from hyperfine splitting (1930Br01,1954Ki11); L({+3}He,d)=1. (|p p{-3/2}) configuration dominant (1996Ja09). 
MOMM1 from NMR (2019StZV, from 1972Bl07). Their earlier value |m=2.262612 {I4} (1970Bl08). g({+81}Br)/g({+79}Br)=1.0779355 {I3} (1970Lu02). 
MOME2 from 2021StZZ, 2018Py01, 2013Ch52 (Atomic Beam). Others: +0.2615 {I25} (2001Bi17 - (reassessment of atomic beam data from 1954Ki11)), +0.266 {I4} (2004Al08, erratum) and +0.254 {I6} (2000Ha64), +0.276 {I4} (1989Ra17 from 1978Ta24; 1998Se09); all reassessments of atomic beam data of 1954Ki11. Sternheimer correction included. Q({+79}Br)/Q({+81}Br)=1.1970568 {I15} (1969He04). 
MOMM3 atomic beam magnetic resonance (1966Br03). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J L({+3}He,d)=3, M1+E2 275|g to 3/2-. (|p f{-5/2}) dominates configuration (1996Ja09). 
T from DSAM in Coulomb excitation (1996Ja09). Others: 235 ps {I15} from 290|g-276|g(t) in {+81}Se |b{+-} decay (18.5 min) (1974SaYH, 1974LiZL), 10 ps {I6} from B(E2)|^=0.0508 {I25} in Coulomb excitation and adopted transition properties. 
MOMM1 from (2020StZV, 1996Ja09) transient field integral perturbed angular correlation in Coulomb excitation and adopted J. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J M2 |g to 5/2-. L({+3}He,d)=4+1 for (536+538) doublet; this level is presumed to be the L=4 component since |p=+ based on |g-decay mode. (|p g{-9/2}) configuration dominant (1996Ja09). 
T weighted average of 35 |ms {I9} and 40 |ms {I10} from 1967Iv03 (different reactions), 46 |ms {I7} (1968Iv02), 32 |ms {I3} (1971Ch28), 37 |ms {I3} (1958Du80 - |g(t) - authors speculated T{-1/2} could be either of {+79}Br or {+81}Br - the evaluator considers it is for the latter isotope - produced by (|g,|g')). 
MOMM1 stroboscopic perturbed angular distribution [2020StZV, from 1972Ch34 (does not include Knight-shift corrections) - authors other article report g-factor=1.261 {I10} (1971Ch28) yields |m=5.675 {I45}]. Absolute |m=5.84 {I7} from measured g-factor=1.297 {I15} (1971Br31). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 3/2-. L({+3}He,d)=4+1 for (536+538) doublet; this level presumed to be the L=1 component since |p=- from |g-decay mode. J=1/2 favored by excit in (d,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J E2+M1 |g to 5/2- and 3/2-; log| {Ift}=6.4 from 1/2- in {+81}Se |b{+-} decay (18.5 min). 
T 68 ps {I+32-18} if |d(566|g)=-3.0 {I5}; 0.5 ps {I13-5} if |d(566|g)=-0.08 {I5} (however, see comment on |d from (p,|g) for 566|g). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 3/2- and 5/2-; absence of |b{+-} branch from 1/2- {+81}Se. 
MOMM1 from transient field integral perturbed angular correlation (2020StZV, 1996Ja09) in Coulomb excitation and adopted J. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J direct excitation in Coulomb excitation of 3/2- {+81}Br; |g(|q) in (p,|g); E2, |DJ=2, |g to 3/2-. 
T from Coulomb excitation (DSAM and B(E2)). 
MOMM1 from transient field integral perturbed angular correlation (2020StZV, 1996Ja09) in Coulomb excitation and adopted J. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E level shown as tentative because the transitions involved are weak and/or might also be placed elsewhere in {+79}Br or {+81}Br level schemes. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J L({+3}He,d)=1; J=1/2 favored by |g(|q) and excit in (d,n|g). 
E from E|g in (d,n|g). E=1105 {I2} in (n,n'|g) for tentative level. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J L({+3}He,d)=3 for level at 1325.7 {I19} which evaluator presumes to be this level since energy scale in ({+3}He,d) is typically several keV high; 1323|g to 3/2- g.s.; 486|g to 7/2- 837; J=5/2 from excit in (d,n|g), consistent with |g(|q). 
T from measured B(E2) in Coulomb excitation and adopted branching, assuming J=5/2. 


level_energy_unit: KEV
level_comment:
J |g to 3/2- and 5/2-, so J|<(7/2). 
Level assumed to differ from 1535.9 level in (d,n|g) because |g branching differs significantly. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J D 977.0|g to 3/2- 566 and D 1267.2|g to 5/2- 276; 706.6|g to 7/2- 837; excit in (d,n|g). L({+3}He,d)=1 for a 1545-keV level. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Probably differs from 2221 level in (d,n|g) because E from ({+3}He,d) is typically too high by several keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$ g-factor=1.261 {I10} (1971Ch28 - no Knight-shift corrections); g-factor=1.297 {I15} (1971Br31). 
T From 1971Ch28. 


level_energy_unit: KEV
level_comment:
E,S unresolved doublet. For L=4, C{+2}S'=8.5 {I9} if J=7/2, 4.4 {I4} if J=9/2; for L=1 component, C{+2}S'=1.17 {I12} if J=1/2, 1.01 {I10} if J=3/2. 


level_energy_unit: KEV
level_comment:
S,E unresolved doublet. For L=1 component, C{+2}S'=0.026 {I3} if J=1/2, 0.022 {I2} if J=3/2. For L=4 component, C{+2}S'=0.191 {I19} if J=7/2, 0.101 {I10} if J=9/2. 


level_energy_unit: KEV
level_comment:
S,E unresolved doublet. C{+2}S'=0.019 {I2} for J=1/2 component. For L=1 component, C{+2}S'=0.049 {I5} if J=1/2, 0.044 {I4} if J=3/2. 


level_energy_unit: KEV
level_comment:
S,E unresolved doublet. For L=2 component, C{+2}S'=0.024 {I2} if J=3/2, 0.019 {I2} if J=5/2. For L=4 component, C{+2}S'=0.167 {I17} if J=7/2, 0.089 {I9} if J=9/2. 


level_energy_unit: KEV
level_comment:
S,E unresolved doublet. If L=1 component: C{+2}S'=0.010 {I1} if J=1/2- or 0.009 {I1} if J=3/2-, and 0.330 {I33} if J=7/2+ or 0.176 {I18} if J=9/2+. If L=2 component: C{+2}S'=0.015 {I2} if J=3/2- or 0.012 {I1} if J=5/2- and 0.29 {I3} J=7/2+ and 0.157 {I16} if J=9/2+. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J 5/2 from 276|g(|q) (1972Ro27), M1+E2 |g to 3/2-. 
g-factor: from |g(|q,H,t), corrected for feeding from the 837 level (1996Ja09). 
T from |t=14 ps {I2} (1996Ja09 (DSAM)), applying a small correction for feeding from the 837 level. However, most of the 276|g intensity (|?84%) results from direct excitation of the 275 level. T{-1/2}=10 ps {+7-5} from adopted 276|g properties and B(E2)|^. 
B(E2): weighted average of 0.0514 {I27} (1972Ro27) and 0.0503 {I25} (1985Si08). Others: 0.041 {I4} (1969Sa23, relative to B(E2)[{+79}Br, 217 level]=0.040 {I3}), 0.049 {I10} (1968An12), 0.029 {I5} (1957Wo32). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
J 538|g(|q) also allows J=5/2, but implied |d=-0.19 {I4} or +10 (1972Ro27) is inconsistent with |d=0.059 {I1} deduced from B(E2) and T{-1/2} assuming J=5/2. 
T$from |t=1.09 ps {I4} (1996Ja09 (DSAM)). Other: 0.60 ps {I13} (1972Ro27 - from |t=0.87 ps {I19}). 
B(E2): Same value in 1972Ro27 and 1985Si08. 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-,7/2-
level_comment:
B(E2): unweighted average of 0.0025 {I2} (1972Ro27) and 0.0044 {I3} (1985Si08). Other: 0.031 {I7} (1968An12) (possibly based on combined yields of 561|g and 566|g (1972Ro27)). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-,5/2
level_lifetime_unit: PS
level_comment:
T from |t=3.8 ps {I4} (1996Ja09). Others: 3.6 ps {I+10-19} (1972Ro27 - from |t=5.2 ps {I14-27}), 2.6 ps {I4} from B(E2)|^ and adopted |g-ray properties. 
B(E2): weighted average of 0.00224 {I13} (1972Ro27) and 0.0023 {I2} (1985Si08). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: PS
level_comment:
g-factor: from |g(|q,H,t) (1996Ja09). 
B(E2): weighted average of 0.0301 {I16} (1972Ro27) and 0.0340 {I23} (1985Si08), and 0.04 {I1} (1968An12). 
T weighted average of 0.55 ps {I3} (1996Ja09 - authors' recommended value based on T{-1/2}=0.53 ps {I3} (491|g) and 0.561 ps {I14} (767|g)) and 0.42 ps {I9} (1972Ro27). Other: 0.57 ps {I6} from B(E2)|^ and adopted 767.2|g-ray properties. 
J not 7/2 from 767|g(|q); probably not 3/2 based on apparently non-zero A{-2} for 767|g(|q) (1972Ro27). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J from Adopted Levels. 
T weighted average of 0.49 ps {I7} (1996Ja09 - from |t=0.7 ps {I1}) and 0.36 ps {I12} (1972Ro27 - from |t=0.52 ps {I17}). 
B(E2): weighted average of 0.0087 {I10} (1972Ro27) and 0.0103 {I12} (1985Si08). 1972Ro27 datum derived from 552|g yield assuming I(828|g)/I(552|g)=3.0 {I2} (cf. adopted value of 3.1 {I3}) because 828|g was believed to include a contaminant. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J also from beam-561|g-276|g(|q) and 561|g(|q) (1972Ro27). 
T weighted average of 1.04 {I7} (1996Ja09, DSAM, based on 1.05 ps {I4} from 561|g and 1.04 ps {I7} from 837|g) and 1.29 ps {I+34-28} from B(E2) and adopted 837|g branching. Other: 0.64 ps {I15} from Doppler broadening of 561|g (1972Ro27); inconsistent with aforementioned values. 
B(E2): from 1985Si08. Others: 0.050 {I17} (1968An12); 0.067 {I10} (1972Ro27 datum, as recalculated by the evaluator from authors' data using adopted branching of 27% {I8} for the 836|g; 1972Ro27 report 0.055 {I4} based on yield of the 561|g and T{-1/2} from their DSAM measurements). 
g-factor: from |g(|q,H,t) (1996Ja09). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J from Adopted Levels. 
T |<0.20 ps, |<0.31 ps, 0.33 ps {I8} for J=3/2, 5/2, 7/2, respectively, from B(E2) and adopted branching; listed value is for the adopted J=5/2. 
B(E2) from 1972Ro27. Level not reported in 1985Si08. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T 235 ps {I15} from 290|g-276|g(t) (1974SaYH). Inconsistent with adopted value (9.7 ps {I14}) for reasons which are unknown. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$In 2010Mi21, total intensity of K component of the radiative electron capture (REC) was measured to be 1.2|*10{+-4} {I1} and 1.64|*10{+-4} {I8} from two measurements, with an average value of 1.42|*10{+-4} {I22} per K capture. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
Analog of {+81}Se g.s. 
E from E{-lab}=3827 keV {I10} (1967Co04) 
T$weighted average of 16 keV {I5} (p,n) (1967Co04), 15 keV {I5} (p,p) (1968Ba23), and 21 keV {I3} (1968Zi03). |G{-p}=2.3 keV {I1} (1978KaZW). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
Analog of {+81}Se 468 level. 
E from E{-lab}=4302 keV {I10} (1967Co04) 
$ |G{-p}=0.80 keV {I13} (1978KaZW). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
Analog of {+81}Se 1053 level. 
E from E{-lab}=4851 keV {I10} (1968Ba23) 
T$weighted average of 14 keV {I5} (p,n) and 14 keV {I5} (p,p) (1968Ba23), and 21 keV {I3} (1968Zi03). |G{-p}=1.3 keV {I1} (1978KaZW). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
Analog of {+81}Se 1233 level. 
E from E{-lab}=4984 keV {I10} (1968Ba23) 
J from L(p,p)=0. 
T$Weighted average of 63 keV {I20} (p,n) and 44 keV {I5} (p,p) (1968Ba23), and 54 keV {I7} (1968Zi03). |G{-p}=8.1 keV {I9} (1978KaZW). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
Analog of {+81}Se 1304 level. 
E from E{-lab}=5066 keV {I10} (1968Ba23) 
T$Weighted average of 34 keV {I10} (p,n) and 35 keV {I5} (p,p) (1968Ba23), and 30 keV {I4} (1968Zi03). |G{-p}=3.8 keV {I3} (1978KaZW). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
Analog of {+81}Se 1406 level. 
E from E{-lab}=5227 keV (1968Zi03) 
$ |G{-p}=2.7 keV {I10} (1978KaZW). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: H
level_comment:
J$atomic beam (1959Ga12,2013Ma15). L(d,p)=4 on 3/2- target. 
MOMM1 from atomic-beam magnetic resonance and low-temperature nuclear orientation (2014StZZ). 
MOME2$From 2016St14, Aomic beam; recalculated , Sternheimer correction included. Others: +0.69 {I2} (2000Ha64); +0.748 {I10} (1998Se09) 
T weighted average of 35.281 h {I6} (1989Ab22), 35.28 h {I1} (1973Co11), 35.34 h {I3} (1968Re04), and 35.39 h {I5} (1985An25). Other: 36.0 h {I17} (2012Ba12) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J M3 |g to 5-. High spin excluded by primary |g in (n,|g). 
T weighted average of 6.05 min {I3} (1965An01), 6.20 min {I3} (1965Em02), both from x-ray activity, and 6.15 min {I9} (1965Em02) from |b activity. 


level_energy_unit: KEV
level_spin_parity: (1)+
level_lifetime_unit: NS
level_comment:
J E1 |g to 2-. Hauser-Feshbach calculation in (p,n|g) determines J=1 (1980Fe09). 
T from from p,|g(t) in (p,n|g) (1977Do08). 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J L(d,p)=4 on 3/2- target. 2,3 from p,|g(|q) in (p,n|g). Hauser-Feshbach calculation in (p,n|g) determines J=3 (1980Fe09). 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J 1,2 from p,|g(|q) in (p,n|g). (M1) |g to (1)+. |g to (3)-. L(d,p)(362+376)=1+4. Also supported by Hauser-Feshbach calculation in (p,n|g) (1980Fe09). 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
J |g's to 2-, (1)+, (2+). L(d,p)=1 if level is identical to that observed at 771 keV {I6}. J=1 from Hauser-Feshbach calculation in (p,n|g) (1980Fe09). However, 1980Fe09 did not resolve the 760-762-763 triplet, so the assignment is not quite conclusive. J|p=2- from ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$2017Fr02: L=1+3; d|s/d|W(q{-max})=0.30 mb/sr; relative spin-dipole transition strength K{-|s}(M2) in units of fm{+2}=1.54 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$2017Fr02: d|s/d|W(q{-max})=0.16 mb/sr; relative spin-dipole transition strength K{-|s}(M2) in units of fm{+2}=0.84 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$2017Fr02: d|s/d|W(q{-max})=0.041 mb/sr; relative spin-dipole transition strength K{-|s}(M2) in units of fm{+2}=0.21 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$d|s/d|W=0.106 {I2} 
$2016Fr06: J=1+,2-; G-T = 75%; B(G-t) = 0.011 {I1} 
$2017Fr02: J=2-; d|s/d|W(q{-max})=0.05 mb/sr; relative spin-dipole transition strength K{-|s}(M2) in units of fm{+2}=0.26 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J$L=1 and analyzing power in (pol d,{+3}He). 
T$weighted average of 2.373 h {I3} (2015Kr02), 2.41 h {I2} (1961Bo22), 2.48 h {I5} (1962Cr08), 2.39 h {I3} (1963Pa09), and 2.35 h {I4} (1969Ph03). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L(|a,p)=1, L(pol d,{+3}He)=(1). 
E$given the poor resolution in (|a,p) and (pol d,{+3}He), could correspond to the 1660-keV level. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$E2 609|g to 9/2+; excitation function in ({+7}Li,|a2n|g) 
E$see {+83}Se |b{+-} decay (22.25 min) dataset for discussion on possible doublet of levels at this energy 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
E$the 1809.3 level seen in ({+3}He,d) is probably identical to the 1810 level or a doublet containing the 1810 level. 
J$L({+3}He,d)=2+4, 372|g to 9/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$the 2050.1-keV level seen in ({+3}He,d) with L=(1+2) is assumed to be a doublet including the 2051-keV and 2058-keV levels. 
J$log {Ift}=4.8 from 1/2- parent 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: US
level_comment:
T$from |g(t) in {+198}Pt({+76}Ge,X|g) (1997Is13). Other: 0.6 |ms {I2} from |a|g(t) in ({+7}Li,|a2n|g). 
J$D(+Q) 303|g to 17/2+, excitation function in ({+7}Li,|a2n|g), systematics of neighboring Rb isotopes. 


level_energy_unit: KEV
level_comment:
E$Doublet. 
L$one of the transitions contributing to this doublet has L=1. The other has L=4, or possibly, 3. A somewhat better fit is obtained with L=1+4 versus L=1+3. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
E$energy sums involving this level group into two values which differ by 0.4 keV suggesting this level is possibly a closely spaced doublet (2015Kr02). Further support for a doublet comes from the negative |b{+-} feeding intensity derived for this level and the fact that the 671- and 1702-keV transitions would correspond to E5 or M6 multipolarities given the adopted J|p's of the levels. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
J$shape of |b spectrum of transition to 0+ is that expected for a first-forbidden unique transition (1970Ha21); possible configuration=|p1f{-5/2}{+3}~#|n1g{-9/2}{+-1} (1970Ha21) 
T$from weighted average of 31.7 min {I2} (1960Sa05), 31.80 min {I8} (1957Jo21) and 31.6 min {I2} (1956Fi36). Others: 32 min (1951Du03), 33 min (1950Ka02), 30 min (1943Bo02,1943Bo01), 30 min (1940St03), 40 min (1939Do02), 30 min (1939Ha14). 
MOMM1$from |g(|q,H,t) (1992Pr06). See also 2005St24 compilation 


level_energy_unit: KEV
level_spin_parity: (6)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$%IT: no IT decay from this level has been observed, probably <0.1% 
E$from difference in Q(|b{+-}) values for the two activities (1970Ha21). 
E$ other: 340 100 (2003Au02) 
J$log| {Ift}=5.1 to 5-. J|p=4- is not likely as E2 transition to 2- g.s. would be expected to be fast and 5- is less likely as B(M3)(W.u.) for %IT<0.1 would be smaller than for any other M3 transition in this region. Possible configuration=|p1p{-3/2}{+-1}~#|n1g{-9/2}{+-1} configuration (1970Ha21) 
T$from 1960Sa05. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
T$weighted average of 3.00 min {I5} (1949Su14) and 2.87 min {I3} (1974Gr29, earlier value=2.87 min {I1} in 1970OsZZ). Others: 3.0 min {I3} (1975Hu02), 3.0 min {I5} (1940St03,1943Se01,1943Bo01) 
J$L=1 and vector analyzing power in (d,{+3}He) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$|DJ=1 |g to (7/2-); possible configuration=|pg{-9/2}{+-1} from systematics (2006As07,2015Ba14). Negative parity is expected if 1514.8|g to 5/2- level exists, unless the level has long half-life 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
E$level is shown populated in ({+82}Se,X|g), but 864.5|g is seen in this reaction and placed from a level not adopted here 
J$gammas to (13/2+) and (11/2+) 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
E$this level is not included in Adopted Levels since 864.5|g is relocated based on results from 2005Fo05 and 2006As07 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
E$due to the reordering of 594-1161 |g cascade and non-confirmation of 296.9|g in other studies, this level is located at 2165 keV in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (9/2,11/2)
level_comment:
J$(9/2+) in Adopted Levels. If 1514.8|g to 5/2- level exists, then 9/2+ and 11/2 are less likely, unless the level is long-lived. A 9/2+ level is expected in this energy region from systematics, with possible configuration=|pg{-9/2}{+-1}. 
E$2005Fo05 suggested that intensity imbalance at this state may be due to the presence of a short-lived isomer at this energy. But this conclusion is not supported in the high-spin study of 2006As07 who did not find this imbalance and ascribe the one deduced by 2005Fo05 to possible problems with the splitting the intensities of the doublet at 432.5+434.6 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
J$log| {If{+1u}t}|?9.6 to 0+. Possible configuration=|pp{-3/2}~#|nd{-5/2} (2009Po10). 
T$weighted average of 55.2 s {I5} (1976LuZV), 55.7 s {I5} (1974Gr29), and 54.1 s {I6} (1972KrYX). Others: 55 s {I2} (1975Hu02), 1972Nu03, 59 s {I4} (1972Ac01), 54 s {I2} (1962St13), 1.0 min (1960Sa05, authors assigned {+87}Se to {+87}Br activity incorrectly, half-life of 16 s for parent activity suggests correct assignment as {+86}Se to {+86}Br), 50-70 s (1959Ye08) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
E$from the differences of the 430.5|g-435.5|g and 1042.0|g-1047.1|g doublets. Another evidence for the existence of this level is the depopulation of the 207.5 level by the 154.2|g-48.3|g cascade. 
J$|g from 1+. Possible 2- state of configuration=|pf{-5/2}~#|nd{-5/2} (2009Po10). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$M1 to (2-). Possible 3- state of configuration=|pf{-5/2}~#|nd{-5/2}. J|p=3- is in conflict with log| {Ift}=6.2 (log| {If{+1u}t}=8.1) from 0+ in |b{+-} decay, but the |b feeding in this decay to the 53-keV level is only an apparent value due to possible unobserved |g transitions feeding this level from higher-energy levels 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
E$deduced from the differences of the 430.5|g-435.5|g and 1042.0|g-1047.1|g doublets. Another evidence for the existence of this level is from the depopulation of the 207.5 level by the 154.2|g-48.3|g cascade. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$Theoretical calculations give 8% contribution from g{-7/2} neutron, 2016Ur03 proposed that this level is populated by a Gamow-Teller transition 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) distribution method as described in authors' paper 2015Cz01 (Phys. Rev. C 92, 014328) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
J$The shell model indicates that |pf{-5/2} or |pp{3/2} leads to (3/2-,5/2-). Two levels in {+87}Kr populated in |b{+-} decay are 4710 and 4961. These both have |g transitions to a 9/2+ level at 1578 keV. So the J|p values for both levels are likely 5/2+ or 7/2-. The logft values for the 4710 and 4961, 5.5 and 5.7 respectively, are both allowed, implying |DJ=0,1 and |D|p=no. For the {+87}Br ground state, this leads to 3/2+,5/2+,7/2+ or 5/2-,7/2-,9/2-. Combining with the shell model argument leads to (5/2-). This is the argument presented in 2006Po09. 
T weighted average of 56.1 s {I7} (1949Su14 by the extraction and measurement of {+87}Kr activity), 55.8 s {I3} (1966Si09 by neutron counting), 55.4 s {I7} (1966Wi03), 55.60 55.60 s 15 (1971De35 by neutron counting), 56.3 s {I5} (1974Gr29 from milking and 4|p|b counting), 55.9 s {I16} (1974Kr21 by neutron counting), and 55.6 s {I3} (1993Ru01 by neutron counting); the associated reduced-|h{+2} is 0.43. Other measurements: 54.5 s (1957Ke67 by neutron counting, though will include {+86}Br as well), 55.4 s {I7} (1962Wi20 and 1963Wi02, superseded by 1966Wi03) 55.6 s {I3} (1970DeZQ or 1970MaZT, superseded by 1971De35), 56.0 s {I3} (1970OsZZ, superseded by 1974Gr29). 
%B-N weighted average of 3.1 {I6} (1964Ar24), 3 {I1} (1967Ga19), 2.63 {I5} (1967Pa26), 2.3 {I3} (1971De35), 2.3 {I4} (1972Sc48), 2.35 {I40} (1975Iz03), 2.6 {I4} (1978Kr15), 2.57 {I15} (1980Lu04), 2.1 {I4} (1980ReZQ, with 10% systematic uncertainties added in quadrature to the reported statistical uncertainty of {I3}), and 2.56 {I10} (1993Ru01). Others: 2.1 {I3} (1970DeZQ, superseded by 1971De35), 2.3 {I5} (1974Kr21, superseded by 1978Kr15), 2.16 {I33} (1976ReZN, superseded by 1977Re05, 1980Lu04, and 1980ReZQ), 2.56 {I38} (1976ShZL), 2.55 {I49} (1976NiZZ), 2.5 {I3} (1977Re05, superseded by 1980Lu04 and 1980ReZQ). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
T$from 1993Ru01. Other values: 16.20 s {I10} (1987PfZX), 16.7 s {I2} (1976Ru01), 16.2 s {I4} (1975Kr17), 16.5 s {I2} (1974Gr29), 16.5 s {I3} (1974NoZR), 16.5 s (1975Al11), 16.4 s {I6} (1974Kr21), 16.3 s {I8} (1971BrYH), 15.9 s {I2} (1966Si09), 15.5 s {I3} (1949Su14). 
%B-N$from 1993Ru01 compilation. Measured values are 6.0 {I16} (1964Ar24), 6.2 {I9} (1971De35), 6.4 {I7} (1972Sc48), 6.6 {I4} (1980Lu04), 6.1 {I4} (1980ReZQ), 7.3 {I6} (1987PfZX), 6.72 {I27} (1993Ru01). 2002Pf04 compilation lists 6.55 {I18}. 
J$log| {If{+1u}t}=9.9 to 2276-keV, J|p=0+ level and log| {If{+1u}t}=10.3 to 1643-keV, J|p=4+ level in the decay to {+88}Kr determine J|p=(2-); see general comment in {+88}Se |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_comment:
J$E2 - M1+E2 cascade from the 270.1-keV isomeric level to J|p=(2-) ground state suggests tentative J|ps of (1-), (2-), or (3-) for the 159.2-keV level and corresponding J|ps of (3-), (4-), or (5-), respectively, for the 270.1-keV level. 


level_energy_unit: KEV
level_spin_parity: (3-,4-,5-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 5.1 |ms {I4} (1999Ge01), 4.9 |ms {I4} (1976SeZN) and 6.3 |ms {I5} (1970Gr38,1972GrYM). Other 4 |ms {I1} (2009Fo05). 
J$see J|p comment for 159.2-keV level. 
E$decay pattern distinguishes this level from one at 272.7 observed in {+88}Se |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: (3-,4-,5-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 5.1 |ms {I4} (1999Ge01), 4.9 |ms {I4} (1976SeZN) and 6.3 |ms {I5} (1970Gr38,1972GrYM). Other 4 |ms {I1} (extracted from Fig. 2 of 2009Fo05 by evaluator). 
$Configuration of (|nd{-5/2}|pp{-3/2}){-4-} is favored by 1999Ge01 based on comparison with {+88}Rb. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: US
level_comment:
T$from 111|g(t) (2017Cz01). This value can be compared with 5.3 |ms {I4} in {+88}Br Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$A strong 273|g from this level proposed earlier by 1980Ze04 (J. Inorg. Nucl. Chem. 42, 1387) was not confirmed by 2015Cz01 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
$It is possible there is a weak 286-keV transition from this level to the 159-keV level, although, the main placement of this |g ray is from 286 level 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
%B-N$from 2020Li32 evaluation based on weighted average of 13.4 {I6} (1993Ru01); 14.6 {I13} (1987PfZX); 13.6 {I8} (1984Ew01); 13.9 {I14} (1981Ho07); 13.9 {I14} (1980ReZQ). Others: 2004PiZZ, 14.2 {I9} (1980Al15); 13.9 {I8} (1980Lu04); 12.5 {I20} (1978Kr15); 16.9 {I17} (1977Re06,1977Re05); 16.6 {I25} (1976ReZN); 13.2 {I21} (1974Kr21); 13.5 {I25} (1972Sc48), 7 {I2} (1964Ar24); 2004PiZZ, 1981Ho17, 1976Ru01, 1975Al11, 1974Ru07, 1974NoZR, 1971Ch38, 1966Si09, 1965Sh07, 1964Ar24, 1959Pe28, 1949Su14, 1948Hu33, 1947Re02 
J$from shell-model predictions (2021Ny02) and analogy with experimental level structure of {+87}Br and ground states of other Br isotopes. 1/2+ proposed in theoretical calculations (2019Mo01). 
T$from decay curves for neutrons, weighted average of 4.348 s {i22} (1993Ru01) 4.37 s {i3} (1976Ru01), 4.55 s {i10} (1974Gr29,1970OsZZ), 4.30 s {i14} (1984Ew01), 4.44 s {i20} (1974Kr21,1975Kr17,1971Kr22) and 4.32 s {i5} (1974NoZR). Others: 4.5 s (1971Ch38), 1971BrYH, 4.5 s {i8} (1966Si09, also 1971To13), 4.4 s {i5} (1959Pe28), 4.51 s {i10} (1948Hu33), 4.45 s {i15} (1947Re02), 4.4 s (Snell et al., Phys Rev 72, 541 (1947)). 
$Compilations of T{-1/2} and %|b{+-}n: 2020Li32, 2002Pf04, 1993Ru01 (also 1982Ru01, 1979RuZQ, 1977Ru10); 1989BrZI 
$Theoretical calculations of T{-1/2} and %|b{+-}n): 2019Mo01, 2016Ma12, 1984Ta06, 1981Al25, 1978Gj02, 1978Gj01, 1977Sh10, 1972Pa11 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<3652 {I7} from Q(|b{+-})({+89}Se)-S(n)({+89}Br), where Q(|b{+-})=9282 {I5} and S(n)=5630 {I5} from 2021Wa16. This represents a range of unobserved levels that subsequently decay to {+88}Br via one-neutron emission. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$weighted average of 1.910 s {I10} (1993Ru01), 1.93 s {I3} (1987PfZX), 1.92 s {I6} (1984Ew01), 1.92 s {I2} (1980Al15), and 1.80 s {I15} (1975As04). Others: 2.09 s {I23} (2012Qu01 from maximum-likelihood fit), 1.85 s {I18} (2012Qu01 from least-squares fit), 1.96 s {I5} (1976Ru01), 1.71 s {I14} (1975Kr17), 1.3 s {I2} (1972Sc48) and 1.4 s {I8} (1971Ch38) 
%B-N$weighted average of 29.0% {I21} (1993Ru01), 24.3% {I30} (1987PfZX), 24.8% {I15} (1984Ew01), 24.6% {I17} (1980Al15), 22.6% {I31} (1975As04). Others: 18.9% {I39} (1978Kr15), 20% {I5} (1974Kr21) and 30% {I7} (1972Sc48). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
%B-N Unweighted average of 22 {I10} (1993Ru01), 25.5 {I35} (1988Kr10), 30.1 {I21} (relative to %|b{+-}n({+89}Br)=13.6 {I8}) (1984Ew01), 19.2 {I13} (1980Al15), 14.1 {I36} (1978Kr15), 9.9 {I20} (1975As04), 16 {I5} (8.3 {I25} from 1974Kr21, after revision by 1993Ru01). The weighted average of all data is 19.3 s {I27}. 
T weighted average of 0.549 s {I9} (1993Ru01) and 0.541 s {I5} (1976Ru01). Other data: 495 ms {I50} and 615 ms {I+61-51} (2012Qu01; from ({+136}Xe,X|g)), 0.510 s {I20} (1988Kr10), 0.53 s {I3} (1984Ew01), 0.63 s {I7} (1976Ah01), 0.60 s {I5} (1975As04), 0.64 s {I7} (1975Kr17), 0.63 s {I7} (1974Kr21). The weighted average of all data is 0.543 s {I5} and the unweighted average is 0.574 s {I17}. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T from 2012Qu01 (based on least-squares fit); 30 ms systematic uncertainty, 40 ms statistical uncertainty. Other: 615 ms from maximum likelihood analysis; 35 ms systematic uncertainty, {I+60-50} ms statistical uncertainty. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T unweighted average of 0.29 s {I+7-6} (2012Qu01), 0.31 s {I1} (1988Kr10), 0.365 s {I7} (1976Ru01), 0.31 s {I2} (1984Ew01), 0.35 s {I4} (1978Cr03) and 0.26 s {I4} (1974Kr21); the weighted average of these data is 0.342 s {I13}. 
%|b{+-}n is weighted average of 32.0 {I45} (1988Kr10), 34.6 {I25} (1984Ew01) and 21 {I8} (1978Cr03), consistent with value recommended in 1993Ru01. Others: 1974Kr21, 1978Kr15. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J from shell-model systematics. 
T from 1988Kr10; multiscaling of delayed n and |b{+-}. 
%|b{+-}n: from 2001Lh01; supported by %|b{+-}n=77 in 1989PfZZ. %|b{+-}n=10 {I+5-3} from 1988Kr10 (as recommended in 1993Ru01) is incorrect due to diffusion of the Kr daughter out of transport tape backing (2000PfZZ). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$ Total of 45 implantations observed, and 20 correlated decay sequences. 
T$ value listed in table I is: 69 ms {I1} (syst) {I+40-25} (stat); maximum-likelihood method for T{-1/2} analysis. Value in Adopted dataset for {+93}Br in ENSDF database is 102 ms {I10}. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T$assumed to be approximately equal to or larger than the flight time through the separator, which for this experiment was 150 ns. 
%B-N$calculated using the Kratz-Herrmann formula (2002Pf04) 


level_energy_unit: KEV
level_spin_parity: (3/2-,1/2)
level_lifetime_unit: US
level_comment:
$ Number of implanted fragments=5.0|*10{+4} 
T$ from |g(t) method (2012Ka36); constant background component was separately deduced. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T$assumed to be approximately equal to or larger than the flight time through the separator. 
$%|b{+-}n calculated using the Kratz-Herrmann formula (2002Pf04) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_comment:
$ Number of implanted fragments=4.1|*10{+3} 
T$ from |g(t) method (2012Ka36); constant background component was separately deduced. 


level_energy_unit: KEV
level_comment:
$Only the |b{+-} decay mode is expected, accompanied by delayed neutron decays 
$Theoretical T{-1/2}=26.0 ms, %|b{+-}n=74, %|b{+-}2n=17, %|b{+-}3n=0.0 (2019Mo01). 
$Theoretical T{-1/2}=17 ms, %|b{+-}n=64.6, %|b{+-}2n=1.5, %|b{+-}3n=0.1 (2016Ma12). 
$Theoretical %|b{+-}n=48.3, %|b{+-}2n=25.0 (2014Mi23). 
T$half-life of the {+98}Br activity has not been measured. It is expected to be greater than the time-of-flight of 634 ns (value from priv. comm. with T. Kubo, July 14, 2010) through the beam transport system. From systematics of half-lives of neighboring Br isotopes, the half-life is expected to be <70 ms (70 ms for {+94}Br, 102 ms for {+93}Br and 314 ms for {+92}Br), assuming a decreasing trend of half-life as neutron number increases in neutron-rich nuclei. 2017Au03 give 5 ms from some other systematics 
$Measured |s=10 pb (2010Oh02), systematic uncertainty|?50% 
$Probability of misidentification of {+98}Br isotope<0.001% and <0.094% in two different settings (2010Oh02) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$A total of 82 events were assigned in 2016Go26 to {+67}Kr. 
$Production |s=3.0 fb {I8} (2016Bl05) in {+9}Be({+78}Kr,X), E=345 MeV/nucleon 
$Proton peak observed at 1690 keV {I17} (2016Go26,2020Gi02) 
E$It is assumed that the observed events correspond to the ground-state 
J$5/2- proposed from theory in 2019Mo01; and 3/2- from systematics in 2021Ko07. 
T$measured by 2016Go26 (same T{-1/2} given in 2020Gi02 and 2017GoZT thesis) from correlated decay curve for {+67}Kr implants and subsequent decays 
$Several theoretical calculations as cited in Fig. 1 of 2016Go26 predict negative S(2p) value for {+67}Kr, making this nucleus a possible 2p-emitter 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$A total of 479 events were assigned in 2016Bl05 (also 2020Gi02) to {+68}Kr. 
$Production |s=33 fb {I21} (2016Bl05) in {+9}Be({+78}Kr,X), E=345 MeV/nucleon 
T$measured by 2020Gi02 (also 2017GoZT thesis) from correlated decay curve for {+68}Kr implants and subsequent decays 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
T$from weighted average of 27 ms {I3} (2011Ro47) and 28 ms {I1} (2014De41). Other: 32 ms {I10} (1997Xu01) 
J$Member of {+69}As T{-z}=3/2 analog nuclei. From the |b delayed proton spectrum for {+69}Kr in 2014De41, an upperlimit of 6.7% proton decay from the IAS {+69}Br to the g.s of {+68}Se (J|p=0+) was estimated. A lower branching ratio suggests {+69}Kr g.s with Jp=5/2- for an increased angular momentum barrier for the g.s state decay. Consistent with this, is the weakly populated proton group at 3.81 MeV {I20} observed by 2011Ro47 (see also 2014Ro14) suggesting a J|p=(5/2-) for g.s {+69}Kr 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) in 2014Ro14. Others: 42 ms {I31} (2002Bl17) and 57 ms {I21} (2000Oi02) 
$T{-1/2} is consistent with superallowed |e decay to {+70}Br g.s. (2000Oi02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2016De29. This value can be compared with 40 ms {I6} in {+70}Kr Adopted Levels in the ENSDF database (July 2016 update). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Measured |s=349 mb {I36}(stat) {I27}(syst) for {+197}Au target (2021Wi01) at E({+70}Kr)=150 MeV/nucleon 
$Measured |s=14.5 mb {I46}(stat) {I10}(syst) for {+9}Be target (2021Wi01) at E({+70}Kr)=140 MeV/nucleon 
$Deduced nuclear deformation length |d{-N}=1.10 fm {I19} (2021Wi01), where uncertainty includes 0.19 fm statistical and 0.04 systematic. 
$Deduced E2 matrix element=0.522 eb {I43} (2021Wi01), where uncertainty includes 0.028 eb statistical, 0.021 eb systematic, and 0.025 eb theoretical 
$Deduced B(E2)=0.2726 e{+2}b{+2} {I451} (2021Wi01), where uncertainty includes 0.0294 e{+2}b{+2} statistical, 0.0224 e{+2}b{+2} systematic, and 0.0258 e{+2}b{+2} theoretical 
T$deduced by compiler from B(E2) value, using unweighted averaged E|g=881 {I4} from measured values of 885 {I8}, 882 {I7} and 886 {I12} in 2018Wi08 and tentative 870 {I1} in 2016De29 (Phys. Rev. C 94, 054311) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: MS
level_comment:
$%|ep=3.06 {I27} (2022Wa34, measurement of |b-delayed proton spectrum correlated with implants, Monte-Carlo analysis used for separation of charged particles into positron and protons). Others: %|ep=2.1 {I7} (1997Oi01), 5.2 {I6} (1995Bl23). Due to much higher statistics and a refined analysis in 2022Wa34, value from this work is preferred over those from 1997Oi01 and 1995Bl23. 
J$log| {Ift}=3.64 to (5/2)- g.s. of {+71}Br; mirror partner of {+71}Br, g.s. J|p=(5/2)- (see 2022Wa34 and 2005Fi10 for discussion). Possible |nf{-5/2} configuration 
T$94.9 ms {I4} (2022Wa34, (implants)(decay events)-correlated decay curve, with a constant background; authors also measured T{-1/2}=95.3 ms {I22} from (implants)|b|g-correlated decay curve; the uncertainty includes statistical as well as systematic). Others: 98.8 ms {I3} (2019Si33, (implanted ions)(|b{++})-decay curve, with exponential fit to the decay curve, including contributions from the decays of parent, daughter and grand-daughter activities and a constant background, however no decay curve is in the paper); 92 ms {I9} (2014Ro14, |b{++} decay correlation spectrum); 83 ms {I48} (2002Lo13); 100 ms {I3} (1997Oi01); 64 ms {I+8-5} (1995Bl23); 97 ms {I9} (1981Ew01). Weighted average of all the measured values listed above, except that from 1995Bl23, is 97.4 ms {I8}, but with reduced |h{+2}=10.5 as compared to 2.1 at 95% confidence level; unweighted average is 94.4 ms {I22}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from |g(t) in 2003Pi03. Others: 17.4 s {I4} (1973Da22) and 16.7 s {I6} (1973Sc17). 
$<r{+2}>{+1/2} (mass)=4.43 fm {i27} (2008Ya08) 


level_energy_unit: KEV
level_comment:
E$Assuming that this level de-excites with the 1444 |g and is fed by the 1432 |g. The order of the 1444 and 1432 |g rays is reversed in {+40}Ca({+40}Ca,2|a|g) 


level_energy_unit: KEV
level_comment:
E$In the adopted values, following the later work of 2007An12 in (HI,xn|g), the order of the 1444-1432 cascade is reversed. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$2005Ga22 suggest soft oblate deformation for the g.s. based upon agreement between theoretical values of |b{-2} and that determined by the authors from B(E2) strength and |>1|s discrepancy between experimental and theoretical |b{-2} for multiple models used in 2005Ga22. 
$The oblate g.s. can be due to the occupation of the 9/2[404] orbit by two protons and neutrons 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2) 
BE2$deduced from angle-integrated cross section at |q{-lab}|<3.0|'. Other: 0.52 {i8} at |q{-lab}|<2.5|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_uncertain: ?
level_comment:
$This level is shown in the level-scheme Fig. 3 of 2020Ho06, but its population in {+73}Sr |b{++}p decay is not discussed. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$reported as 0.4023 {I81} (stat) {I290} (syst) {I380} (theory) (2020Wi05); uncertainties added in quadrature by the compiler. 
$|s=27.2 mb {I4} (syst) {I15} (syst) for scattering off Be and 468 mb {I9} (syst) {I29} (syst), for scattering off Au. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
BE2$reported as 0.0665 {I39} (stat) {I58} (syst) {I63} (theory) (2020Wi05); uncertainties added in quadrature by the compiler. 
$|s=4.5 mb {I3} (syst) {I2} (syst) for scattering off Be and 79 mb {I4} (syst) {I5} (syst), for scattering off Au. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: S
level_comment:
$Others for |ep studies: %|ep=0.68 {I12} (1972Ho20), 2003Pi03 (authors state that their measured value is in agreement with 0.24 {I3} from 1999Mi17, but do not provide their own value). 1981Ha44 measured 82% proton decay branch to the g.s. and 18% to the first 2+ state in {+72}Se. See also 1976HaWO from the same group as 1981Ha44 
J$log| {Ift}=5.7 {I1} to 1/2-; log| {Ift}=6.4 to (5/2)+ 
T$weighted average of 25.9 s {I6} (1973Da22), 28.4 s {I7} (1981Ha44) and 29.0 s {I10} (1999Mi17) 


level_energy_unit: KEV
level_spin_parity: (61/2+)
level_comment:
$Maximum configuration spin state of |a=+1/2 signature, this band does not show a strong decrease in quadrupole collective behavior (2010St05) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$Note large intensity imbalance at 144 level: I(|g+ce)(224|g)+I(|g+ce)(249|g)=173 {I6}, whereas I(|g+ce)(144|g)=100 {I6} 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
E$this level is not included in Adopted Levels, Gammas dataset, as the tentative 1354|g is not confirmed in {+40}Ca({+40}Ca,|a2pn|g) (2010St05) 


level_energy_unit: KEV
level_spin_parity: (61/2+)
level_comment:
$Maximum configuration spin state of |a=+1/2 signature, this band does not show a strong decrease in quadrupole collective behavior 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$|D<r{+2}>({+86}Kr-{+74}Kr)=+0.03 fm{+2} 11 (1995Ke04) 
$<r{+2}>{+1/2}=4.187 fm {I4} (2004An14) 
T$ from time decay of |g rays (1975Sc07). Others: 1974Co38, 1974Ro11, 1973HoYM, 1973DaYM, 1960Bu22, 1960Gr19 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$ from recoil-distance (RDDS,2005Go43). Others: 16.3 ps {I14} (RDDS,1990Ta12), 20 ps {I4} (RDDS,1984Ro01), 9.7 ps {I30} (1976AlYY). 2001Ra27 evaluation adopted 17.3 ps {I21} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$E0 transition to 0+ 
T$from delayed ce spectra in {+9}Be({+78}Kr,X) (2003Bo05). Others: 23 ns {I5} (2000Ch07, reanalyzed result of 29 ns {I6} (1997Ch46) using least-squares method and taking into account prompt component), 14 ns {I7} (1999Be11,2000Be43,2001Ko15) 
$Interpreted as a state with oblate-prolate shape coexistence, dominated by oblate shape 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$ from recoil-distance (RDDS) method (2005Go43). Other: 9.1 ps {I5} (1984Ro01). Note large discrepancy in the two measurements. The value from 2005Go43 is preferred due to better reaction channel selection through the use of large gamma-ray detector array. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.76 ps 16 (2005Go43), 0.75 ps 10 (2000Al02), 0.63 ps 7 (1991He02), 0.62 ps 10 (1990Ta12) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.069 ps 21 (2000Al02) and 0.125 ps 35 (1990Ta12). Other: |<0.08 ps (1991He02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
$Interpreted as a state with oblate-prolate shape coexistence, dominated by oblate shape 
T$ from 2003Bo05. Others: 23 ns {I5} (2000Ch07,reanalyzed result of 29 ns {I6} (1997Ch46) using least-squares method and taking into account prompt component), 14 ns {I7} (1999Be11,2000Be43,2001Ko15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ other: 29.6 ps {I21} for free fit 
$E2 diagonal matrix element=-0.70 {I+33-30} 
$Q{+s}{-0}=+1.9 {I+9-8} 
$Q{+t}{-0}=+2.48 {I2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$ other: 4.09 ps {I35} for free fit 
$E2 diagonal matrix element=-1.0 {I+6-2} 
$Q{+s}{-0}=+2.1 {I+12-4} 
$Q{+t}{-0}=+3.16 {I5} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 diagonal matrix element=+0.33 {I+28-23} 
$Q{+s}{-0}=0.9 {I+7-6}, sign is negative for K=0 and positive for K=2 
$Q{+t}{-0}=-1.51 {I+10-11} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$E2 diagonal matrix element=+0.4 {I+11-4} 
$Q{+s}{-0}=1.1 {I+31-10}, sign is negative for K=0 and positive for K=2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$ other: 0.97 ps {I35} for free fit 
$E2 diagonal matrix element=-1.8 {I+5-7} 
$Q{+s}{-0}=+3.1 {I+8-13} 
$Q{+t}{-0}=+3.10 {I+15-13} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime=31 ps {I3} from differential recoil-distance Doppler shift (DRDDS) method (2018Mo30). Uncertainty includes statistical and systematic, the latter due to feedings from higher levels. Other: mean lifetime=33 ps {I3} from analysis which does not include feeding from higher lying levels. Earlier measured value from traditional RDDS method, from the same group, was 22.3 ps {I15} (2014Iw01). Other: 23.43 ps {I42} from differential-decay curve and recoil-distance Doppler-shift method by 2005Go43: Eur. Phys. J. A26, 153. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$Measured scattering |s=6.1 mb {I11} (2023Sp02) for one step process. Estimated |?0.5 mb for the two-step process. 
$Deduced |b{-4}=+0.23 {I2}(stat) {I2}(syst) (2023Sp02) for constructive interference, and |b{-4}=-0.17 {I2}(stat) {I2}(syst) for destructive interference between the one-step and the two-step processes. Authors preferred positive deformation parameter, based on a geometric idea of the polar-gap model of |b{-4} deformations, where positive deformations are expected at the beginning of a shell and negative hexadecapole deformations are expected at the end of a shell 
$B(E4)(W.u.)(4+ to 0+)=29 {I2}(stat) {I2}(syst) (2023Sp02) for positive |b{-4}; 16 {I2} for negative |b{-4}, the latter numerical value from e-mail reply of May 05, 2023 from M. Spieker. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
J$spin from hyperfine structure (1995Ke04). Parity from log| {Ift}=5.6 to positive parity states (132 and 154) in {+75}Br. 
Probable |n5/2[422] orbital with |b{-2}=0.4 (1995Ke04) 
$ RMS charge radius <r{+2}>{+1/2}=4.2097 fm {I41} (2004An14 evaluation; and 2008 update available at http://cdfe.sinp.msu.ru) 
|D<r{+2}>({+86}Kr-{+75}Kr)=0.22 fm{+2} {I8} (1995Ke04) 
MOMM1,MOME2$from hyperfine-structure measurement using collinear fast-beam LASER spectroscopy (1995Ke04) 
T$from 1995BeZS. Others: 4.5 min {I3} (1974Ro12), 4.2 min {I2} (1974Ho35), 5.5 min {I4} (1960Bu22). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.2020 fm {I36} (2013An02 evaluation) 
T$weighted average of 14.82 h {I5} (1963Do04, from parent-daughter separations); 14.7 h {I1} (1963Do04, growth-decay curve for annihilation radiation, using 16.2 h half-life for {+76}Br decay); 14.6 h {I2} (1973Pa02, |g-decay curves). 1963Do04 measured decay curves for three prominent |g rays and reported T{-1/2}=14.1 h, 14.2 h, and 14.3 h, with a counting uncertainty of 0.1 h but an overall uncertainty of 0.5 h in each value. Others: 10.5 h (1955Th01), 9.7 h {I5} (1954Ca03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
MOMM1$transient-field technique in Coul. ex. (2004Ku11,2005Be61) 
MOME2$from Coulomb excitation (2007Cl02). No value is given in 2021StZZ compilation 
T$from recommended B(E2)|^=0.758 {I26} (2016Pr01 evaluation), based on the following measurements: RDDS measurements, mean lifetime |t=41.5 ps {I8} (2005Go43), 37.7 ps {I30} (1990He04), 36 ps {I1} (1984Wo10) and 35 ps {I3} (1982Ke01). B(E2)|^=0.721 {I10} (2007Cl02, Coul. ex. with incident energy above Coulomb barrier). Other: |t=53 ps {I7} (1974No08) from RDDS seems discrepant. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$(346|g)(424|g)(|q) in {+76}Br |e decay (1978LiZU). Also L=0 in (p,t) 
T$from |b|g(t) in {+76}Rb |e decay. Other: 47.3 ps {I17} (2007Cl02, Coulomb excitation using GOSIA analysis) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$B(E2)(from 424,2+)=0.444 {I6} (2007Cl02 from Coulomb excitation) 
J$|DJ=2, E2 |g to 2+; rotational band member 
T$weighted average of 3.05 ps {I14} (2007Cl02,Coulomb excitation, free fit analysis by GOSIA code), 2.54 ps {I6} (RDDS,2005Go43), 2.08 ps {I21} (RDDS,1998Sk01), 3.4 ps {I3} (RDDS,1984Wo10); 3.5 ps {I14} (DSA,1982Pi01); 2.9 ps {I7} (RDDS,1982WiZS), uncertainty in 2005Go43 was increased to 5%. Others: 5.7 ps {I16} (RDDS,1974No08) seems discrepant; and 4.30 ps {I14} (RDDS,1982Ke01) is effective half-life 
MOME2$from Coulomb excitation (2007Cl02). No value is given in 2021StZZ compilation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=2 from 0+ 
T$from Coulomb excitation using GOSIA analysis (2007Cl02). Other: |?1 ps (RDDS,1982Ke01) 
MOME2$from Coulomb excitation (2007Cl02). No value is given in 2021StZZ compilation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=2 from 0+ 
T$from Coulomb excitation using GOSIA analysis (2007Cl02). 
MOME2$from Coulomb excitation (2007Cl02). Other: <4.8 ps from |b|g(t) in |e decay. No value is given in 2021StZZ compilation 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 4+; member of rotational band 
T$weighted average (NRM) of 0.67 ps {I20} (RDDS,2005Go43); 0.55 ps {I21} (RDDS,1998Sk01); 0.82 ps {I9} (DSA,1989Gr21); 1.04 ps {I14} (RDDS,1984Wo10); 0.87 ps {I8} (DSA,1982Pi01); 0.55 ps {I14} (RDDS,1982WiZS); and 0.568 ps {I35} (2007Cl02, Coulomb excitation, free fit analysis by GOSIA code). 
MOME2$from Coulomb excitation (2007Cl02) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 2+; |DJ=1, M1+E2 |g to 4+ 
T$from Coul. ex. (2007Cl02) using GOSIA analysis. Other: <0.90 ps {I28} (effective half-life from DSAM in ({+12}C,2n|g), 1982Pi01) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$effective half-life=0.76 ps {I28} from DSAM in ({+12}C,2n|g) (1982Pi01) 
J$|DJ=1, M1+E2 |g to 4+; |DJ=2, E2 |g to 3+ 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 6+; member of rotaional band 
T$weighted average of 0.23 ps {I2} (DSA,1989Gr21); 0.208 ps {I21} (DSA,1982Pi01); 0.22 ps {I3} (RDDS,1982WiZS); 0.173 ps {I21} (from Coul. ex. using GOSIA analysis, 2007Cl02). Other: 0.31 ps {I5} (DSA,1984Wo10, effective half-life) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (5-) and |DJ=1 |g to 6+; 
T$from DSAM in ({+28}Si,p2n|g) (1999Mu21) (See ({+12}C,2n|g) dataset). Other: 0.256 ps {I42} (DSAM,1982Pi01) 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$879.9|g E2, |DJ=2 to 5+; 1474|g D+Q to 6+ 
T$effective half-life=0.71 ps {I21} from DSAM in ({+12}C,2n|g) (1982Pi01) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 8+; member of rotational band 
T$from DSA method. Weighted average of 0.097 ps {I14} (1982Pi01); 0.12 ps {I3} (1982WiZS); 0.104 ps {I21} (Coul. ex. using GOSIA analysis, 2007Cl02). Others (effective half-lives): 0.56 ps {I11} (1989Gr21), 0.14 ps {I4} (1984Wo10) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in ({+28}Si,p2n|g) (1999Mu21) (See ({+12}C,2n|g) dataset). Other: 0.35 ps {I8} (effective half-life, and 0.111 ps {I42} from gating above, both from DSAM in ({+12}C,2n|g),1982Pi01) 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E$this level is only from ({+12}C,2n|g),({+24}Mg,|a2p|g) (1982Pi01, 1989Gr21). It is not reported in more recent studies with high statistics: {+54}Fe({+28}Si,|a2p|g) (1996Do07) and {+40}Ca({+40}Ca,4p|g) (2005Va09) 
T$effective half-life=0.29 ps {I7} from DSAM in ({+12}C,2n|g) (1982Pi01) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in ({+12}C,2n|g); weighted average of 0.180 ps {I+35-28} (1999Mu21) and 0.12 ps {I5} (1982Pi01) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$member of rotational band 
T$effective half-life=0.166 ps {I35} from DSAM in ({+12}C,2n|g) (1982Pi01) 


level_energy_unit: KEV
level_spin_parity: (13-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in ({+28}Si,p2n|g) (1999Mu21) (See ({+12}C,2n|g) dataset). Other: 0.24 ps {I6} (effective half-life from DSAM in ({+12}C,2n|g),1982Pi01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$The g factor measured by transient-field technique in Coul. ex. 
T$from free fit. Other: 28.6 ps {I4} from constrained fit 
$E2 matrix element (0,0+ to 424,2+)=+0.849 {I6} 
$B(E2)=0.721 {I10}, deduced from E2 matrix element 
$E2 diagonal matrix element=-0.9 {I3} 
$Q{+s}{-0}=+2.5 {I8} 
$Q{+t}{-0}=2.69 {I2} 
$|s(19|' to 51|')=2.7 b {I3} (1992Os02) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from free fit. Other: 2.70 ps {I7} for constrained fit 
$E2 matrix element (424,2+ to 1035,4+)=+1.49 {i1} 
$E2 diagonal matrix element=-2.3 {I4} 
$Q{+s}{-0}=+4.7 {I8} 
$Q{+t}{-0}=2.94 {I3} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (from 0,0+ to 1222,2+)=+0.183 {I+8-6} 
$E2 matrix element (from 1222,2+ to 1957,4+)=+0.89 {I+10-13} 
$E2 matrix element (from 424,2+ to 1222,2+)=-0.09 {i4} 
$E2 matrix element (from 1035,4+ to 1222,2+)=-0.62 {I+4-5} 
$E2 matrix element (from 770,0+ to 1222,2+)=+1.22 {I+8-4} 
$E2 diagonal matrix element=-1.0 {I5} 
$Q{+s}{-0}=2.6 {I13}, positive sign for K=2, negative sign for K=0 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (from 0,0+ to 1688,2+)=+0.121 {I+4-5} 
$E2 matrix element (from 424,2+ to 1688,2+)=-0.200 {I+9-8} 
$E2 matrix element (from 770,0+ to 1688,2+)=+0.87 {I+4-2} 
$E2 matrix element (from 1035,4+ to 1688,2+)=+0.52 {I5} 
$E2 matrix element (from 1222,2+ to 1688,2+)=+0.81 {I+10-24} 
$E2 diagonal matrix element=+1.3 {I5} 
$Q{+s}{-0}=-3.4 {I13} 
$Q{+t}{-0}=2.77 {I+12-7} 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from free fit. Other: 0.53 ps {I4} for constrained fit 
$E2 matrix element (1035,4+ to 1859,6+)=+1.90 {I+11-3} 
$E2 diagonal matrix element=-2.9 {I4} 
$Q{+s}{-0}=+5.1 {I7} 
$Q{+t}{-0}=2.98 {I+17-6} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (from 424,2+ to 1957,4+)=0.09 {I+1-19} 
$E2 matrix element (from 1035,4+ to 1957,4+)=+0.43 {I3} 
$Q{+t}{-0}=1.77 {I+20-26} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
$This level is included here for completeness, but does not appear to be populated in Coulomb excitation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$Measured scattering |s=5.1 mb {I5} (2023Sp02) for one step process. Estimated |?0.8 mb for the two-step process. 
$Deduced |b{-4}=+0.201 {I9}(stat) {I16}(syst) (2023Sp02) for constructive interference, and |b{-4}=-0.127 {I9}(stat) {I22}(syst) for destructive interference between the one-step and the two-step processes. Authors preferred positive deformation parameter, based on a geometric idea of the polar-gap model of |b{-4} deformations, where positive deformations are expected at the beginning of a shell and negative hexadecapole deformations are expected at the end of a shell 
$B(E4)(W.u.)(4+ to 0+)=22.7 {I10}(stat) {I18}(syst) (2023Sp02) for positive |b{-4}; 9.1 {I6} for negative |b{-4}, the latter numerical value from e-mail reply of May 05, 2023 from M. Spieker. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$Deduced |b{-4}=+0.151 {I11}(stat) {I12}(syst) (2023Sp02) for assumed single-step mechanism. 
$B(E4)(4+ to 0+)=12.9 {I9}(stat) {I20}(syst) (2023Sp02) 
$B(E4)(W.u.)(4+ to 0+)=36 {I2}(stat) {I4}(syst) (2023Sp02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from RDDS. Weighted average of 28.8 ps {I6} (2005Go43), 21.5 ps {I21} (1998Sk01), 26.1 ps {I21} (1990He04), 24.9 ps {I7} (1984Wo10), 24.3 ps {I21} (1982Ke01), 23.6 ps {I14} (priv comm quoted by 1984Wo10), assuming a minimum uncertainty of 5% to account for systematic uncertainties. Other: 37 ps {I5} (1974No08) is in disagreement with more recent measurements 
$Q(transition)=2.90 {I4}, 2.60 {I11}, 2.39 {I10}, 2.66 {I13}, 2.53 {I17} (1989Gr21, deduced from transitions up to 10+). This leads to |b{-2}=0.33 {I1} for the yrast band 
$Q(transition)=3.1 {I3} (1998Sk01) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$weighted average (NRM) of 2.54 ps {I6} (RDDS,2005Go43), 2.08 ps {I21} (RDDS,1998Sk01), 3.4 ps {I3} (RDDS,1984Wo10); 3.5 ps {I14} (DSA,1982Pi01); 2.9 ps {I7} (RDDS,1982WiZS), assuming a minimum uncertainty of 5% to account for systematic uncertainties. Others: 5.7 ps {I16} (RDDS,1974No08), 4.30 ps {I14} (RDDS,effective half-life, 1982Ke01) 
$Q(transition)=3.3 {I3} (1998Sk01) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.67 ps {I20} (RDDS,2005Go43); 0.55 ps {I21} (RDDS, 1998Sk01); 0.82 ps {I9} (DSA,1989Gr21); 1.04 ps {I14} (RDDS,1984Wo10); 0.87 ps {I8} (DSA,1982Pi01); 0.55 ps {I14} (RDDS,1982WiZS) 
$Q(transition)=2.9 {I11} (1998Sk01) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.23 ps {I2} (DSA,1989Gr21); 0.208 ps {I21} (DSA,1982Pi01); 0.22 ps {I3} (RDDS,1982WiZS). Other: 0.31 ps {I5} (DSA,1984Wo10,effective half-life) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$from DSA method. Weighted average of 0.097 ps {I14} (1982Pi01) and 0.12 ps {I3} (1982WiZS). Others (effective half-lives): 0.56 ps {I11} (1989Gr21), 0.14 ps {I4} (1984Wo10) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: PS
level_comment:
T$other from 1982Pi01: 0.35 ps {I8} (effective half-life from DSAM), 0.111 ps {I42} (from DSAM by gating from above) 
$Q(transition)=3.66 {I27} (1999Mu21) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: PS
level_comment:
T$from DSAM. Weighted average of 0.12 ps {I5} (1982Pi01) and 0.180 ps {I+35-28} (1999Mu21) 
$Q(transition)=3.80 {I+41-37} from averaged T{-1/2}=0.15 ps (1999Mu21) 


level_energy_unit: KEV
level_spin_parity: (13-)
level_lifetime_unit: PS
level_comment:
T$Other: 0.24 ps {I6} (effective half-life from DSAM,1982Pi01) 
$Q(transition)=3.06 {I+62-38} (1999Mu21) 


level_energy_unit: KEV
level_spin_parity: (19-)
level_comment:
E$1988Ka28 show a 1521|g deexciting a 17- level, and a 1532|g deexciting a 19- level of the same band, but no 1521|g is observed by 1989Gr21; instead, a 1533.5|g (probably the same as 1532|g from 1988Ka28) is suggested (1989Gr21) to deexcite 17- level and a 1615|g a 19- level. Ordering of the 1615-1521-1536 cascade is based on results in 2005Va09 in {+40}Ca({+40}Ca,4p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
$Evaluated charge radius <r{+2}>{+1/2}=4.2082 fm {I37} (2013An02) 
$Evaluated |d<r{+2}>({+86}Kr,{+77}Kr)=0.209 fm{+2} {I5} (2013An02) 
J$hyperfine structure (1995Ke04); L+1/2 and L=2 in (pol d,t) 
MOMM1,MOME2$from hyperfine-structure measurement using collinear fast-beam LASER spectroscopy (1995Ke04). 
$|D<r{+2}>({+86}Kr-{+77}Kr)=0.209 fm{+2} {I5} (1995Ke04). The uncertainty is statistical. Total uncertainty including systematic errors is 0.060 fm{+2} (1995Ke04); rms charge radius=4.2082 fm {i16} (1995Ke04) 
T$from 2019Ze02 (decay curves for the two strong |g rays from the decay of {+77}Kr, and weighted average of six measurements). Value from 2019Ze02 is adopted here as this work gives full details of the measurements and uncertainty assignments, while little details are provided in the older references. Others: 73.5 min {I11} (1974Ho37), 75 min {I3} (1973Ba22), 74.7 min {I7} (1971Bo30), 71.1 min {I5} (1960Bu22), 69 min {I6} (1957Be46), 73 min (1955Th01), 66 min (1948Wo07). Weighted average of values from 2019Ze02, 1974Ho37, 1973Ba22, 1971Bo30, 1960Bu22 and 1957Be46 is 71.9 min {I6}, but with normalized |h{+2}=4.9. The NRM weighted average, where the uncertainty in the value from 1971Bo30 gets doubled, is 71.57 min {I45}, with acceptable normalized |h{+2}=2.3 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$L(d,t)=1 and L+1/2 from analyzing powers in (pol d,t) 
T$from |g|g(t) (1975No11, {+63}Cu({+16}O,pn|g) E=42 MeV) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$analyzing power in (pol d,t) gives J|p=5/2- and 9/2+ for the 245 and 279 unresolved doublet; |DJ=1 |g to 3/2-. L(p,d)=(1) for a 230 level implying (1/2-,3/2-) is in disagreement 
T$from RDDS in ({+16}O,pn|g) E=49-58 MeV (1984Wo10); others: 33 ps {I9} (from Doppler-shift method, ({+16}O,pn|g) E=42 MeV, 1975No11), 32 ps 8 (1982ZoZY) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 5/2+. J=1/2 ruled out by asymmetric |g(|q). 
T$RDDS (1984Wo10). Other: 114 ps {I14} (1982ZoZY) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 3/2-; 1/2 not allowed by |g(|q). L(p,d)=(4) for a 430 level implying (7/2+,9/2+) is in disagreement 
T$ from RDDS (1984Wo10). Other: 13 ps {I2} (RDDS,1982ZoZY) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 7/2+; |DJ=1, M1+E2 |g to 9/2+ 
T$weighted average of 1.19 {I24} (DSAM,1990Jo07) and 2.1 ps {I3} (RDDS,1984Wo10) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 9/2+; |DJ=1, dipole |g to 11/2+ 
T$RDDS (1984Wo10). Other: 1.8 {I5} (DSAM,1990Jo07) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 7/2-; |DJ=1, M1+E2 |g to 9/2- 
T$weighted average of 1.07 {I21} (DSAM,1990Jo07) and 1.25 ps {I14} (RDDS,1984Wo10) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 9/2-; |DJ=1, M1+E2 |g to 11/2- 
T$weighted average of 0.60 {I12} (DSAM,1990Jo07) and 0.69 ps {I14} (RDDS, 1984Wo10). Other: 0.9 ps {I2} (1982ZoZY) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 11/2+; |DJ=1, M1+E2 |g to 13/2+ 
T$weighted average of 0.51 {I10} (DSAM,1990Jo07) and 0.83 ps {I14} (DSAM, 1984Wo10). 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 13/2+; |DJ=1, dipole |g to 15/2+ 
T$weighted average of 0.39 {I8} (DSAM,1990Jo07) and 0.62 ps {I10} (DSAM, 1984Wo10). Other: 0.5 ps {I2} (1982ZoZY) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 11/2-; |DJ=1, (M1+E2) |g to 13/2- 
T$DSAM (1990Jo07). Other: 0.90 ps {I21} (DSAM,1984Wo10,not corrected for side feeding) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 13/2-; |DJ=1, (M1+E2) |g to 15/2- 
T$DSAM (1990Jo07). Other: 0.7 ps {I3} (DSAM,1984Wo10,not corrected for side feeding) 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 15/2+; |DJ=1, M1+E2 |g to 17/2+ 
T$DSAM (1990Jo07). Other: 0.28 ps {I14} (DSAM,1984Wo10,not corrected for side feeding) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 17/2+; |DJ=1 d |g to 19/2+ 
T$DSAM. Weighted average of 0.16 {I4} (1990Jo07) and 0.18 ps {I6} (1984Wo10) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=2, E2 |g to 17/2-; |DJ=1, (M1+E2) |g to 19/2- 
T$0.33 ps {I6} from DSAM (1990Jo07), not corrected for side feeding 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 21/2+; |DJ=1, (M1) |g to 23/2+ 
T$DSAM (1990Jo07). Other: 0.30 ps {I10} (1984Wo10, not corrected for side feeding 


level_energy_unit: KEV
level_spin_parity: 31/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=2, E2 |g to 27/2+; |DJ=1, dipole |g to 29/2+ 
T$0.090 ps {I21} from DSAM (1990Jo07), not corrected for side feeding 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=2, (E2) |g to (27/2-); band member 
T$0.14 ps {I3} from DSAM for 1317|g which was placed from a 5620 level in ({+32}S,2pn|g) (1990Jo07). Adopted placement of 1317|g is from {+58}Ni({+29}Si,2p2|a|g). Lifetime is not corrected for side feeding 


level_energy_unit: KEV
level_spin_parity: 37/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=2, E2 |g to 33/2+; |g to 35/2+ 
T$0.062 ps 14 from DSAM (1990Jo07), not corrected for feeding 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
E$level is not included in Adopted Levels since 1317|g has a revised placement based on the work of 1997Sy01 in ({+29}Si,2|a2p|g). 
T$assigned to 6670 level in Adopted Levels based on reassignment of 1317|g in 1997Sy01 


level_energy_unit: KEV
level_lifetime_unit: MIN
level_comment:
T$from weighted average of 71.34 m {I25}, 71.21 m {I37}, 71.24 m {I20} from 129.7|g(t) and 71.26 m {I29}, 71.21 m {I42}, and 71.18 m {I28} from 146.5|g(t) (2019Ze02). Value is relative to that of {+241}Am using reference method. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$ <r{+2}>{+1/2}=4.2032 fm {I16} (2004An14 evaluation) 
T$|>1.5|*10{+21} y (2006Ga43, 90% confidence limit) for double |b decay (2|e(K),2|n+0|n mode). Others: 2000Ga54, 1998Ga27, 1995Sa58, 1994Sa31. See also 2002Tr04 evaluation. 
T$ theory, analysis and compilation of double |b decay: 2008Mi17, 2005Do07, 2000Ki24, 2000Se12, 1998Ru08, 1998Su19, 1997To05, 1996Au07, 1996Ru21, 1994Hi03, 1994Hi06, 1992Do12, 1991St08, 1989Ba85, 1984Ab02 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ |b{-2}(p,p')=0.351 (DWBA analysis), 0.317 (coupled-channel) 
MOMM1$ transient magnetic field technique following Coulomb excitation (2004Ku11). Other: +0.86 {I6} (2001Me20). See also 2005St24 compilation 
J$L(p,p')=2 and also from |g(|q) and |g(linear pol) 
T$weighted average of values from recoil-distance Doppler-shift method in in-beam |g-ray studies, DSA and B(E2) in Coul. ex. Values in ps are: 21.7 {I+7-8} (B(E2) in Coul. ex.,2006Be18), 22.2 {I14} (RDDS,2002Jo07), 19.1 {I17} (DSAM in Coul. ex.,2001Me20), 21.1 {I9} (RDDS,1990Ga22), 22.9 {I21} (RDDS,1985Wi01,1982An06), >3.5 (DSA,1980Ro02), 22.2 {I14} (RDDS,1979He18), 25 {I3} (RDDS,1974No08). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$E0 transition to 0+ (1995Gi13); L(p,t)=0 
T$weighted average of 11.1 ps 6 (B(E2) in Coul. ex.,2006Be18) and 7.6 ps 21 (DSA in (p,p'|g,1995Gi13) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$ transient magnetic field technique following Coulomb excitation (2001Me20). See also 2005St24 compilation 
|b{-2}(DWBA)=0.101, B(E4)(W.u.)=5.5 {I11} in (p,p') 
J$L(p,p')=4 and from |g(|q) and |g(linear pol) 
T$weighted average of values from recoil-distance Doppler-shift method in in-beam |g-ray studies, DSA and B(E2) in Coul. ex. Values in ps are: 2.42 {I+8-17} (B(E2) in Coul. ex.,2006Be18), 2.36 {I21} (RDDS,2002Jo07), 2.09 {I18} (DSAM in Coul. ex.,2001Me20), 2.70 {I35} (DSA,1993Bi04), 2.91 {I14} (RDDS,1990Ga22), 2.56 {I35} (RDDS,1985Wi01,1982An06), 6.2 {I28} (DSA,1980Ro02), 2.50 {I21} (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$ transient magnetic field technique following Coulomb excitation (2001Me20). See also 2005St24 compilation 
|b{-2}(DWBA)=0.065, B(E2)(W.u.)=1.8 {I4} from (p,p') 
J$L(p,p')=2 and from |g(|q) and |g(linear pol) 
T$weighted average of 2.2 ps +5-4 (B(E2) in Coul. ex.,2006Be18), 3.1 ps 6 (RDDS,1982An06) and 4.02 ps 35 (RDDS,1979He18). Other: >0.6 ps (DSA,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J$|g(|q); |g(linear pol) of 735|g from 5+ (2299) level 
T$weighted average of 5.1 ps 4 (RDDS,1982An06) and 4.44 ps 35 (RDDS,1979He18). Other: >1.0 ps (DSA,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g's to 0+ and 4+ 
T$from B(E2) for 739|g in Coul. ex. (2006Be18). Other: 0.074 ps {I12} from B(E2) for 1756|g in Coul. ex. (2006Be18) is discrepant 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(linear pol) 
T$weighted average of 1.72 ps +14-20 (B(E2) in Coul. ex.,2006Be18), 2.1 ps 7 (RDDS,1982An06) and 1.32 ps 21 (RDDS,1979He18). Other: >2.1 ps (DSA,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(linear pol) 
T$weighted average of values from Doppler-shift (DSA) method in in-beam |g-ray studies and B(E2) in Coul. ex. Values in ps are: 0.61 {I7} (B(E2) in Coul. ex.,2006Be18), 0.82 {I19} (DSA,2006Dh01), 0.57 {I21} (DSA,2002Jo07), 0.83 {I14} (DSA,1993Bi04), 0.49 {I14} (DSA) and 0.69 {I14} (RDDS) (1985Wi01,1982An06), 1.25 {I28} (DSA,1980Ro02), 0.62 {I10} (RDDS and DSA,1979He18), <2 (RDDS,1974No08) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(linear pol) 
T$weighted average of 0.44 ps 9 (DSA,2002Jo07), 1.10 ps 28 (RDDS,1982An06), 1.0 {I+10-3} (DSA,1980Ro02) and 1.25 ps 28 (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
J$E1 |g to 2+. Small |e feedings from 4(-) and 0(+) giving inconsistent assignments are probably not reliable 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
J$band assignment; |g's to 4+ and 6+ 
T$weighted average of 1.4 ps 7 (RDDS,1982An06), 1.7 ps 9 (DSA,1980Ro02) and 1.4 ps 7 (DSA,1979He18) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(linear pol) 
T$weighted average of 0.76 ps +62-28 (DSA,1985Wi01,1982An06), 0.9 {I+14-5} (DSA,1980Ro02) and 1.52 ps 21 (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: PS
level_comment:
J$E1 |g's to 3+ and 4+; log| {Ift}=6.2 from 4(-) 
T$from <2.08 ps {I35} (effective half-life,RDDS,1985Wi01,1982An06) and >1.4 ps (DSA,1985Wi01) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(pol) 
T$weighted average of values from Doppler-shift (DSA) method in in-beam |g-ray studies and B(E2) in Coul. ex. Values in ps are: 0.28 {I3} (B(E2) in Coul. ex.,2006Be18), 0.28 {I7} (DSA,2006Dh01), 0.44 {I9} (DSA,2002Jo07), 0.37 {I5} (DSA,1993Bi04), 0.25 {I4} (DSA,1985Wi01), 0.30 {I+10-7}, 0.26 {I6}, 0.22 {I4} (DSA,1982An06), 0.49 {I14} (DSA,1980Ro02), 0.31 {I4} (DSA,1979He18) 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 5+; band assignment 
T$weighted average of 0.62 ps 21, 0.38 ps 14, 0.49 ps {I14} (DSA,1982An06), 0.69 ps 28 (DSA,1980Ro02) and 0.62 ps +42-21 (DSA,1979He18) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: PS
level_comment:
J$|g(|q); |g's to 5+ and 6+; band assignment 
T$weighted average of 4.9 ps 14 (RDDS,1985Wi01) and 5.1 ps +21-14 (RDDS,1982An06) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$|g(|q), |g(linear pol); band assignment 
T$weighted average of 1.94 ps 21 (RDDS,1985Wi01,1982An06), 1.3 ps 8 (DSA,1980Ro02) and 2.01 ps 21 (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(linear pol) 
T$weighted average of 1.9 ps 5 (DSA,line shape), 2.6 ps {I+10-8} (RDDS)(1982An06) and 1.0 ps +14-4 (DSA,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 6+; band assignment 
T$weighted average of 0.16 ps 4 (DSA,line shape), 0.208 ps 35 (DSA), 0.187 ps 35 (DSA) (1982An06) and 0.24 ps 7 (DSA,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(linear pol) 
T$weighted average of 0.83 ps 35 (RDDS,1985Wi01,1982An06), 1.39 ps 35 (DSA,1980Ro02) and 0.83 ps 21 (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: PS
level_comment:
J$|g(|q), |g(linear pol) 
T$weighted average of 0.94 ps 14 (DSA,2006Dh01), 0.97 ps 28 (DSA) and 1.2 ps 5 (RDDS)(1985Wi01,1982An06), 1.5 ps 6 (DSA,1980Ro02) and 0.76 ps 7 (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 8+ 
T$weighted average of values from Doppler-shift (DSA) method in in-beam |g-ray studies and B(E2) in Coul. ex. Values in ps are: 0.24 {I+2-3} (B(E2) in Coul. ex.,2006Be18), 0.152 {I35} (DSA,2006Dh01), 0.20 {I4} (DSA,2002Jo07, also 0.19 {I8} and <0.35 listed), 0.42 {I14} (DSA,1993Bi04,effective value), 0.21 {I4} (DSA,1985Wi01, 1982An06), 0.208 {I35} (DSA,line shape) and 0.097 {I28} (DSA) (1982An06), 0.33 {I7} (DSA,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: PS
level_comment:
J$|DJ=(2), (E2) |g to 7+ 
T$unweighted average of 0.083 ps 28 (DSA,line shape), 0.125 ps {I35} (DSA), 0.21 ps 8 (DSA) (1982An06), 0.35 ps 7 (DSAM,1980Ro02) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
J$|DJ=(0), (M1) |g to 10+; |g to 8+ 
T$from DSA (1985Wi01,1982An06). Other: 0.10 ps 4, 0.08 ps +5-4(DSA) (1982An06) 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=2, E2 |g to 8- 
T$weighted average of 1.25 {I35} (DSA,1985Wi01,1982An06) and 1.11 ps 35 (RDDS,1985Wi01,1982An06) is 1.18 ps 35. As stated by 1985Wi01 this value is effective half-life, thus given as an upper limit here. Other: |<1.0 ps (RDDS,1979He18) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
J$|g to (8+) 
T$from DSA (line-shape) (1982An06). Other: 0.24 ps 9 and 0.12 ps 6 from DSA (1982An06) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 9- 
T$from DSA. Weighted average of 0.24 ps 6 (2006Dh01), 0.38 ps 7 (1985Wi01,1982An06), 0.49 ps +35-21 and 0.44 ps +23-15 (1982An06), 0.49 ps 7 (1980Ro02), 0.25 {I8} (1979He18) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 10+ 
T$from DSA. Weighted average of 0.15 ps 4 (2006Dh01), 0.18 ps 3 and 0.21 ps 4 (2002Jo07), 0.17 ps 10 (1985Wi01) 


level_energy_unit: KEV
level_spin_parity: (13-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (11-) 
T$from DSA. Weighted average of 0.132 ps 28 (2006Dh01), 0.22 ps 10 (1979He18) 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 12+ 
T$from DSA. Weighted average of 0.118 ps 35 (2006Dh01), 0.09 ps 4 and 0.076 ps 21 (2002Jo07), 0.15 ps 6 (1979He18) 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_comment:
J$|DJ=(2), (E2) |g to 14+ 
T$from DSA. Weighted average of 0.20 ps 5 (2006Dh01), 0.10 ps 6 and 0.146 ps 35 (2002Jo07). Other: |<0.14 ps (1979He18) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$average of 0.48 ps {I14} (DSAM) and 0.69 ps {I14} (RDDS) (1985Wi01) 
T$ 0.69 PS 10 (^RDDS,1982An06) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.16 ps {I5} (line shape), 0.208 ps {I35} (DSAM in (|a,2n|g)) and 0.187 ps {I35} (DSAM in ({+12}C,2n|g)) (1982An06) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: PS
level_comment:
T$average of 0.97 ps {I35} (DSAM) and 1.2 ps {I5} (RDDS) (1985Wi01) 
T$ 1.2 PS +5-7 (^RDDS,1982An06) 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: PS
level_comment:
T$1.11 ps 35 (RDDS, effective half-life,1985Wi01) 
T$ 1.25 PS 28 (DSAM), 1.11 PS 35 (^RDDS IN (12C,2NG)) (1982An06) 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: PS
level_comment:
T$1.11 ps 35 (RDDS, effective half-life,1985Wi01) 
T$ 1.25 PS 28 (LINE SHAPE), 1.11 PS 35 (^RDDS IN (12C,2NG)) (1982An06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)=0.67 {I3} (2006Be18). Others: 0.62 {I7} (2005Ga22), 0.55 {I3} (1981Ca01), 0.54 {I13} (1957He48). See also analysis by 2006Co03 
G$ from transient field technique (2004Ku11), earlier value from the same group: +0.43 {I3} (2001Me20) 
T$ from B(E2)(|_)=0.134 {I+5-4} (2006Be18) who used 22.8 ps {I11} (from 1991Ra06) as starting point in GOSIA analysis. 2001Me20 measured 19.1 ps {I17} from DSAM following Coulomb excitation 
$Diagonal E2 matrix element=-0.80 {I4} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$ from B(E2)(|_)=0.091 {I5} (2006Be18) who used 7.6 ps {I21} (from 1995Gi13) as starting point in GOSIA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
G$ from transient field technique (2001Me20) 
$Diagonal E2 matrix element=-0.73 {I+15-14} 
T$ from B(E2)(|_)=0.180 {I+14-6} (2006Be18). 2006Be18 used 2.5 ps {I2} (from 1991Ra06) as starting point in GOSIA analysis. 2001Me20 measured 2.09 ps {I18} from DSAM following Coulomb excitation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ from transient field technique (2001Me20) 
$Diagonal E2 matrix element=+0.58 {I+4-8} 
T$ from B(E2)(|_)(1148|g)=0.005 {I+1} and branching(1148|g)=0.386 {I4}. 2006Be18 used 3.7 ps {I4} (from 1991Ra06) as starting point in GOSIA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Diagonal E2 matrix element=(-0.22 {I+9-14}) 
T$5.3 ps {I4} from B(E2)(|_)(739|g)=0.013 {I1} and Branching(739|g)=0.267 {I6}; but 0.074 ps {I12} from B(E2)(|_)(1756|g)=0.006 {I1} and Branching(1756|g)=0.131 {I5}. Note large discrepancy in the two half-life values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$ from B(E2)(|_)(725|g)=0.093 {I+12-7} and branching(725|g)= 0.565 {I20}; 1.41 ps {I+28-21} from B(E2)(|_)(1418|g)=0.0006 {I1} and Branching(1418|g)=0.085 {I6}. 2006Be18 used 1.4 ps {I2} (from 1991Ra06) as starting point in GOSIA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
$Diagonal E2 matrix element=-0.87 {I+16-12} 
T$ from B(E2)(|_)=0.20 {I2}. 2006Be18 used 0.6 ps {I1} (from 1995Gi13) as starting point in GOSIA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$ from B(E2)(|_)=0.19 {I+3-2}. 2006Be18 used 0.27 ps {I4} (from 1991Ra06) as starting point in GOSIA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$ from B(E2)(|_)=0.14 {I+2-1}. 2006Be18 used 0.24 ps {I5} (from 1991Ra06) as starting point in GOSIA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Diagonal E2 matrix element=-0.96 {I+11-7} (2018Lu02) 
$Compiler deduces T{-1/2}=22.2 ps {I5} from E2 matrix element for 455|g in 2018Lu02 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Diagonal E2 matrix element=+1.0 {I+3-7} (2018Lu02) 
$Compiler deduces T{-1/2}=2.16 ps {I+15-13} from E2 matrix element for 1148|g in 2018Lu02 and adopted |g-ray branching ratios. From E2 matrix element for 693|g, compiler obtains T{-1/2}=1.0 ps {I4} using Adopted gamma-branching ratio and |d(E2/M1) for 693|g 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Diagonal E2 matrix element=1.6 {I+18-5} (2018Lu02) 
$Compiler deduces T{-1/2}=3.6 ps {I+8-5} from E2 matrix element for 1301|g in 2018Lu02, Adopted branching ratios and |d(E2/M1) for 1301|g 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
$Evaluated rms charge radius=4.2034 fm {I32} (2013An02) 
$Evaluated |d<r{+2}>({+79}Kr,{+86}Kr)=0.168 fm{+2} {I4} (2013An02) 
J$L(pol d,p)=1. Probable p{-1/2} orbital 
T$from 1974Co05. Others: 34.92 h {I5} (1964Bo25), 34.5 h {I2} (1952Ra13), 36 h {I1} (1952Be55), 34.5 h {I10} (1940Cr06). The uncertainty given by 1964Bo25 is small but it may be an underestimate whereas that given by 1974Co05 includes an estimate of systematic error also 
MOMM1$collinear fast beam LASER spectroscopy (1995Ke04) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
MOMM1,MOME2$collinear fast beam LASER spectroscopy (1995Ke04). Note that 1995Ke04 give Q=+0.40 {i4} with a comment that conventional estimated uncertainty of 10% from calibration and the expected small Sternheimer shielding correction is included. It seems 2013StZZ evaluation removes this uncertainty 
J$E3 |g to 1/2- 
T$from 1969Ha03 (from a single |g-ray in a mass-separated source). 1940Cr06 give 55 s {I2} using a source containing mixed activities 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$E2 |g to 1/2- 
T$weighted average of 77.7 ns {I15} (|g(t) in (p,n|g),1968Bl04); 78 ns {I6} (1978Li28), 81.2 ns {I32} (1975Bu10), 79.1 ns {I15} (1972Br31). The last three values are from |g|g(t) in {+79}Rb |e decay 
MOMM1$|g(|q,H,t) in (p,n|g) (1968Bl04) 
MOME2$differential PAD method (1978HaXP) 
Quadrupole coupling constants measured using |g|g PAC method with {+79}Rb source (1981Ha37) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$L(pol d,p)=4. In (pol d,p) |s(|q) and Ay(|q) data for a composite group (130,147,149 levels) are fitted well with L=4, 7/2+ for 130, L=3, 5/2- for 147 and L=4, 9/2+ for 149 level 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$M1 |g to 1/2- and M1+E2 |g from 5/2- 
T$from |g(t) pulsed beam (1990Sc07). Others: 0.52 ns {I10} (1986ZhZW), |<0.6 ns (|g|g(t) in {+79}Rb |e decay,1972Br31) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$M1+E2 |g to 7/2+ and D+Q |g to 3/2- 
T$143|g(t) pulsed beam (1990Sc07). Other: 0.21 ns {I7} (1986ZhZW). It should be noted that value of 0.21 ns (1986ZhZW) for 290 level agrees with 0.21 ns (1990Sc07) for 183 level and 0.52 ns (1986ZhZW) for 183 level agrees with 0.62 ns (1990Sc07) for 290 level 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(pol d,p)=3. Also E2 |g to 1/2- 
T$RDDS for 219|g and 402|g (1990Sc07). Other: 17 ps {I5} (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 3/2- and E1 |g to 7/2+ 
T$RDDS for 302|g and 320|g (1990Sc07). Other: 35 ps {I10} (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: PS
level_comment:
J$|DJ=0 or 1 M1+E2 |g to 5/2- and band assignment 
T$RDDS for 293|g (1990Sc07). Other: 7 ps {I+7-4} (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 5/2- and |DJ=1 M1+E2 |g to 7/2- 
T$RDDS for 667|g (1990Sc07). Other: 4.2 ps {I14} (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 7/2+ and |DJ=1 M1+E2 |g to 9/2+ 
T$DSA for 748|g and 767|g. Weighted average of 1.39 ps {I28}, 1.59 ps {I21}, (1988Wi01) and 1.25 ps {I63} (1985ZhZX). Other: 1.2 ps {I6} (RDDS for 748|g, 1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: PS
level_comment:
J$|DJ=0 or 2 |g to 9/2+ and |DJ=1 M1+E2 |g to 7/2(+). Excitation function supports 9/2+ 
T$RDDS for 285|g (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: PS
level_comment:
J$|DJ=(2) E2 |g to 9/2+; |DJ=0 or 1 |g to 11/2+ and band assignment 
T$DSA for 827|g. Weighted average of 1.87 ps {I21}, 2.22 ps {I21} (1988Wi01), 1.94 ps {I35} (1985ZhZX) and 1.87 ps {I21} (RDDS,1982Pa20) 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_comment:
J$|DJ=1 |g to 9/2+ and band assignment 
E$transitions of 378, 654 and 747 keV as given in {+79}Br(p,n|g) cannot be placed with this level due to large J|p change. It is possible that these transitions define another low-spin level near 1038 keV 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 5/2- and |DJ=0 or 1 |g to 7/2- 
T$RDDS for 661|g (1986ZhZW). Others: <3 ps (1990Sc07), >0.7 ps (DSA,1990Sc07), >1.4 ps (DSA,1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_comment:
J$|g to 1/2- and log| {Ift}=7.31 from 5/2+. J|p=1/2- is possible from log| {If{+1u}t}=8.4 but would be difficult to populate in (|a,xn|g) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 7/2- and |g to 9/2+ 
T$RDDS for 721|g (1990Sc07). Other: 1.7 ps {I+7-4} (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
J$|gs to 3/2- and 7/2+. Possible |g to 9/2+ and |g from 3/2+. log| {Ift}=6.56 from 5/2+ 
T$DSA for 792|g (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2 (E2) |g to (7/2)- and |DJ=1 |g to 9/2- 
T$DSA for 756|g (1990Sc07). Other: 1.3 ps {I4} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (13/2)-
level_lifetime_unit: PS
level_comment:
J$|DJ=(2) E2 |g to 9/2- and |DJ=1 |g to 11/2+ 
T$DSA for 848|g. Weighted average of 2.8 ps {I14}, 0.84 ps {I28} (1990Sc07) and 0.69 ps {I21} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 11/2+ and |DJ=1 |g to (13/2)+ 
T$DSA for 909|g and 988|g. Weighted average of 0.32 ps {I4}, 0.35 ps {I4} (1988Wi01); 0.35 ps {I14}, 0.49 ps {I14} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 9/2- and |DJ=0 or 1 |g to 11/2- 
T$DSA for 852|g. Weighted average of 1.4 ps {I6}, 0.77 ps {I35} (1990Sc07) and 0.76 ps {I21} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to (13/2)+ and |DJ=1 |g to 15/2+ 
T$DSA for 1026|g. Weighted average of 0.65 ps {I6}, 0.51 ps {I5}, 0.52 ps {I5} (1988Wi01); 0.49 ps {I14}, 0.76 ps {I28} (1985ZhZX) and 0.62 ps {I21} (RDDS,1982Pa20) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to 11/2- and |DJ=0 or 1 |g to (13/2)+ 
T$DSA for 885|g. Weighted average of 0.77 ps {I7}, 0.56 ps7, 0.56 ps 14 (1990Sc07) and 0.55 ps {I18} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (19/2)+
level_lifetime_unit: PS
level_comment:
J$|DJ=(2) (E2) |g to 15/2+ and |DJ=1 M1 |g to (17/2)+ 
T$DSA for 977|g and 1094|g. Weighted average of 0.31 ps {I5}, 0.15 ps {I4} and 0.21 ps {I3} (1988Wi01) 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: PS
level_comment:
J$|DJ=2 E2 |g to (17/2)+ and band assignment 
T$DSA for 1144|g. Weighted average of 0.36 ps {I4}, 0.21 ps {I4}, 0.22 ps {I4} (1988Wi01); 0.55 ps {I14} (1985ZhZX) and 0.32 ps {I11} (RDDS,1982Pa20) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$from 1969Ha03 (mass separated source). Other: 55 s {I2} (1940Cr06) (source contained mixed activities) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$from 143|g(t) (pulsed beam) (1990Sc07). Other: 0.21 ns {I7} (1986ZhZW). It should be noted that value of 0.21 ns (1986ZhZW) for 290 level agrees with 0.21 ns (1990Sc07) for 183 level and 0.52 ns (1986ZhZW) for 183 level agrees with 0.62 ns (1990Sc07) for 290 level 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$DSA for 748|g and 767|g. Weighted average of 1.39 ps {I28}, 1.59 ps {I21} (1988Wi01) and 1.25 ps {I63} (1985ZhZX). Other: 1.2 ps {I6} (RDDS for 748|g, 1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: PS
level_comment:
T$DSA for 827|g. Weighted average of 1.87 ps {I21}, 2.22 ps {I21} (1988Wi01); 1.94 ps {I35} (1985ZhZX) and 1.87 ps {I21} (RDDS,1982Pa20). Other: 1.7 ps {I6} (1986ZhZW) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T$RDDS for 661|g (1986ZhZW). Others: <3 ps (1990Sc07). DSA results give >0.7 ps (1990Sc07) and >1.4 ps (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (13/2)-
level_lifetime_unit: PS
level_comment:
T$DSA for 848|g. Weighted average of 2.8 ps {I14}, 0.83 ps {I28} (1990Sc07) and 0.69 ps {I21} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
T$DSA for 909|g and 988|g. Weighted average of 0.32 ps {I4}, 0.35 ps {I4} (1988Wi01); 0.35 ps {I14}, 0.49 ps {I14} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
T$DSA for 852|g. Weighted average of 1.4 ps {I6}, 0.76 ps {I35} (1990Sc07) and 0.76 ps {I21} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_lifetime_unit: PS
level_comment:
T$DSA for 1026|g. Weighted average of 0.65 ps {I6}, 0.51 ps {I5}, 0.52 ps {I5} (1988Wi01); 0.49 ps {I14}, 0.76 ps {I28} (1985ZhZX) and 0.62 ps {I21} (RDDS,1982Pa20) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T$DSA for 885|g. Weighted average of 0.69 ps {I7}, 0.55 ps {I7}, 0.55 ps {I14} (1990Sc07) and 0.55 ps {I+21-14} (1985ZhZX) 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: PS
level_comment:
T$DSA for 1144|g. Weighted average of 0.36 ps {I4}, 0.21 ps {I4}, 0.22 ps {I4} (1988Wi01); 0.55 ps {I14} (1985ZhZX) and 0.32 ps {I11} (RDDS,1982Pa20) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$weighted average of 8.3 ps {I7}(DSAM,2001Mu25); 7.8 ps {I5} (DSAM in Coul. ex.); 8.3 ps {I7} (DSAM and RDM,1981Fu03); 8.8 ps {I5} (RDM,1975Fr04). Evaluation by 2001Ra27 adopted 8.6 ps {I5} from 1981Fu03 and 1975Fr04 
MOMM1$transient-field technique in Coul. ex. (2001Me20) 
|b{-2}(p,p')=0.28 (1979Sa14) 
T$others: 9.4 ps (from B(E2)(Coul. ex.)=0.34) 
|D<r{+2}>({+80}Kr-{+86}Kr)=0.088 fm{+2} {I7} (1990Sc30), 0.0866 fm{+2} {I9} (1981Ge06,1979Ge06), 0.144 fm{+2} {I7} (1995Ke04). Uncertainties quoted are statistical only. The total uncertainties including the systematic errors are: 0.068 fm{+2} (1990Sc30), 0.044 fm{+2} (1995Ke04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 2+ 
MOMM1$transient-field technique in Coul. ex. (2001Me20) 
|b{-2}(p,p')=0.059 (1979Sa14) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|g(|q,pol); E2 |g to 2+ 
T$DSAM in Coul. ex. (2001Me20). Others: 1.7 ps {I2} (1975Fr04), 1.6 ps {I4} (1981Fu03) 
MOMM1$transient-field technique in Coul. ex. (2001Me20) 
|b{-4}(p,p')=0.061 (1979Sa14) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J$|g's to 5- and 4-. Greater |s(|g) of 628|g and 695|g in (|a,4n|g) as compared to those in (|a,2n|g) favors J=6 (1981Fu03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$B(EL)(W.u.)=37 {I6} 
E$617 {I15} (1979Sa14) 
|b{-2}(DWBA)=0.284, |b{-2}(coupled-channel)=0.268 (1979Sa14). Deduced B(E2)=0.38 {I6} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(EL)(W.u.)=1.5 {I3} 
E$1250 {I15} (1979Sa14) 
|b{-2}(DWBA)=0.059, |b{-2}(coupled-channel)=0.054 (1979Sa14). Deduced B(E2)=0.015 {I3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$B(EL)(W.u.)=2.3 {I5} 
E$1417 {I15} (1979Sa14) 
|b{-4}(DWBA)=0.061, |b{-4}(coupled-channel)=0.064 (1979Sa14). Deduced B(E4)=0.0015 {I3} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (g.s., 0+ to 617, 2+)=+0.645 {I7} (2021Gi14) 
$B(E2)(g.s., 0+ to 617, 2+)=0.4159 {I84} (2021Gi14) 
$Diagonal E2 matrix element (617, 2+ to 617, 2+)=-0.43 {I7} (2021Gi14) 
$T{-1/2}=7.63 ps {I16}, deduced by compiler from B(E2)(up)=0.4159 {I84} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (g.s. 0+ to 1256, 2+)=+0.078 {I15} (2021Gi14) 
$B(E2)(g.s. 0+ to 1256, 2+)=0.0061 {I23} (2021Gi14) 
$E2 matrix element (617, 2+ to 1256, 2+)=+0.73 {I14} (2021Gi14) 
$B(E2)(617, 2+ to 1256, 2+)=0.1074 {I406} (2021Gi14) 
$Diagonal E2 matrix element (1256, 2+ to 1256, 2+)=+0.4 {I17} (2021Gi14) 
$M1 matrix element (617, 2+ to 1256, 2+)=+0.065 {I16} (2021Gi14) 
$B(M1)(617, 2+ to 1256, 2+)=0.00085 {I39} (2021Gi14) 
$T{-1/2}=3.7 ps {I+22-10}, deduced by compiler from B(E2)(up)=0.1074 {I406} for 639.6|g. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (617, 2+ to 1320, 0+)=+0.33 {I12} (2021Gi14) 
$B(E2)(617, 2+ to 1320, 0+)=0.0223 {I155} (2021Gi14) 
$E2 matrix element (1256, 2+ to 1320, 0+)=-0.08 {I63} (2021Gi14); 64.3 keV transition is not observed 
$B(E2)(1256, 2+ to 1320, 0+)=0.0014 {I180} (2021Gi14) 
$T{-1/2}=2.9 ps {I+10-12}, deduced by compiler from B(E2)(up)=0.0223 {I155} for 703.9|g, assuming 100% branching for this transition. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (617, 2+ to 1436, 4+)=+1.069 {I30} (2021Gi14) 
$B(E2)(617, 2+ to 1436, 4+)=0.2287 {I130} (2021Gi14) 
$Diagonal E2 matrix element (1436, 4+ to 1436, 4+)=-0.77 {I22} (2021Gi14) 
$T{-1/2}=1.20 ps {I7}, deduced by compiler from B(E2)(up)=0.2287 {I130} 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (1436, 4+ to 2392, 6+)=+1.68 {I12} (2021Gi14) 
$B(E2)(1436, 4+ to 2392, 6+)=0.3140 {I430} (2021Gi14) 
$T{-1/2}=0.33 ps {I5}, deduced by compiler from B(E2)(up)=0.3140 {I430} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: Y
level_comment:
MOMM1$from collinear laser fast-beam spectroscopy (1995Ke04,2019StZV); relative to {+83}Kr standard, diamagnetic correction included. Other: -0.909 {I4} (1993Ca41; laser resonance fluorescence spectroscopy, {+83}Kr standard). 
MOME2$ From 2021StZZ - based on +0.629 {I13} (1993Ca41; laser resonance fluorescence spectroscopy, if Q({+83}Kr)=0.253 {I5} (1989Ra17)), adjusted by 2001Ke15 to +0.644 {I4} assuming their value of 0.259 {I1} for Q({+83}Kr). Other: +0.64 {I7} (1995Ke04, collinear laser fast-beam spectroscopy); uncertainty includes uncertainty in electric-field gradient and the Sternheimer correction. 
|D<r{+2}>({+86}Kr,{+81}Kr)=+0.099 fm{+2} (1995Ke04); uncertainty is 0.004 (statistical only), 0.018 (including systematic uncertainties), 0.034 (total uncertainty). 
|D<r{+2}>({+80}Kr,{+81}Kr)=-0.015 fm{+2} {I8} (1996Li25; statistical uncertainty only). 
J E3 |g from 1/2-; 49.57|g M1(+E2) from 9/2+. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$Weighted average of 3.9 ns {I4} from (|a,n|g) and 4.0 ns {I4} from (p,n|g) 
J from (pol d,p)=4 and vector analyzing power. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%|e from {+81}Kr |e decay (13.10 s). 
MOMM1$ From collinear laser fast-beam spectroscopy (1995Ke04,2019StZV); relative to {+83}Kr standard, diamagnetic correction included. 
|D<r{+2}>({+86}Kr,{+81}Kr)=+0.080 fm{+2} (1995Ke04); uncertainty is 0.008 (statistical only), 0.022 (including systematic uncertainties), 0.041 (total uncertainty). 
|D<r{+2}>({+80}Kr,{+81}Kr)=-0.034 fm{+2} {I11} (1996Li25; statistical uncertainty only). 
<r{+2}>{+1/2}(charge)=4.1952 fm {I26} (2013An02). 
J from (pol d,p)=1 and vector analyzing power. 
T from 1987Lo06. Others: 13.32 s {I15} from 1987Da06, 13 s {I2} (1940Cr06), 13 s {I1} (1969Ha03), 12.8 s {I3} (1986Al11), 13.4 s {I7} (2005Ka39). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$5/2+ from (pol d,p)=2 and vector analyzing power; J=5/2 favored by excitation function data in (|a,n|g), however, 682|g(|q) in (|a,n|g) supports |DJ=1 instead as a |DJ=2 transition to 9/2+. Also 682|g to 9/2+ is M1,E2 from |a(K)exp in (p,n|g). Uncertain placement of the 682|g in |e decay (30 min). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J log {Ift}=6.7 from 9/2+ in |e decay; 932.0|g(|q) data consistent with |DJ=1 or 0 to 9/2+ and 981.6|g(|q) data consistent with |DJ=1 to 7/2+ (both in (|a,3n|g)); J=11/2 favored by 932|g and 982|g excit in (p,n|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-,5/2-
level_comment:
J log| {Ift}=5.7 from 3/2-. 537.61|g E2(+M1) to 5/2-; J|p=5/2- if the placement of weak 994|g to 7/2+ g.s. is correct. 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_comment:
J E1 |g to 5/2+, log {Ift}=5.9 from 3/2-. J|p=(5/2)- if weak 1025|g to 7/2+ g.s. is correctly placed. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-,5/2-
level_comment:
J log| {Ift}=5.5 from 3/2-. If the placement of 701.47|g to 1/2+ 976 is correct, 5/2- can be ruled out. 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J M1+E2 368|g to 13/2- 2166; D intraband 113|g to (13/2-) 2420; 166|g M1(+E2) from 17/2- at 2699; band assignment. 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J E2, |DJ=2, |g to 13/2-; |gs to 15/2+ and 17/2+; band assignment. 
T From centroid shift in (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
J (15/2,17/2)- from M1 |g to 15/2- and D 128.6|g to 17/2-; 834.5|g stretched E1 to 15/2+ (|a,5n|g); bandhead of level sequence similar to one in {+83}Kr. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$from ({+3}He,t). Other: 9700 {I10} from (p,n) 
Isobaric analog of {+81}Br g.s. 
J L=0 in ({+3}He,t) and (p,n). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+,3/2)
level_comment:
J excitation function favors 3/2, decay mode favors 5/2. 549|g(|q) does not distinguish between |DJ=1 and |DJ=2, and 499.8|g(|q) is isotropic. Adopted value is 5/2+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
J$3/2 from isotropic 608.4|g angular distribution measurements and excitation function data (1983Ka03). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
L based on sharp forward peak |s(|q). 
J analog of 3/2- {+81}Br g.s.; based on L, |G and excitation strength in high energy (p,n) reaction. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_uncertain: ?
level_comment:
E this level is placed in this decay scheme by 1981FrZY only. 1977Li14 placed it in (30.5 min) |b{++} decay scheme. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E,J isobaric analog of {+81}Br g.s., based on E, |G and L=0. Level energy from 1982Ko06, based on {+51}V-{+51}Cr mass difference (cf. 9675 {I32} based on {+87}Rb-{+87}Sr mass difference, 1981Ko24). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
|D<r{+2}>({+82}Kr-{+86}Kr)=0.071 fm{+2} {I3} (1995Ke04, total uncertainty including systematic uncertainty is 0.028), 0.053 fm{+2} {I7} (1990Sc30, the uncertainty is 0.044 fm{+2} including systematic errors). 
|D<r{+2}>({+82}Kr-{+81}Kr)=-0.028 fm{+2} {I5} (1996Li25) (uncertainty only statistical) 
|D<r{+2}>({+83}Kr-{+82}Kr)=-0.040 fm{+2} {I4} (1996Li25) (uncertainty only statistical) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L(p,p')=2. First excited state in Coulomb excitation. 
T$from measured B(E2) in Coul. Ex. Others: 4.7 ps {I7} from recoil-distance Doppler shift in (|a,2n|g) (1984Ke10), 4.8 ps {I8} from resonance fluorescence (1966Be16). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from B(E2) measured in Coulomb excitation. Others: 1.0 ps {I+10-6} from recoil distance, 0.8 ps {I+10-4} from Doppler shift attenuation, both observed in (|a,2n|g) (1984Ke10). 
J L(p,p')=4 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J$|g(|q) in (|a,2n|g) indicates J=4 (1984Ke10,1983Me08) with quadrupole |g to 2+ probably being E2. |g|g(|q) results in |b{+-} decay are in strong conflict (1980So06 and 1968Gu08 concluded J=3, while 1977CoZO deduced J=4). 
T from B(E2) measured in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J log| {Ift}=7.6, (log| {If{+1u}t}=7.8) from 2-, |g from 5(-). Also supported by |g(|q) in (|a,2n|g). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J stretched (E2) to 2+ indicated by |g(|q) in (|a,2n|g) (1984Ke10). 1983Me08 deduced J=3 from their |g(|q) data. 
T from B(E2) measured in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_lifetime_unit: PS
level_comment:
J J=3,5 from (1007|g)(1044|g)(|q) (1969Li14). log| {Ift}=6.1, (log| {If{+1u}t}=5.9) from 5-, Polarization of 1007|g in (|a,2n|g) indicates |p=- (1984Ke10). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
J stretched (E2) cascade indicated by |g(|q) in (|a,2n|g). 
T average of 2 ps {I1} from Doppler-shift attenuation, 3 ps {I+2-1} from recoil distance, both observed in (|a,2n|g), and 4 ps {I2} from recoil distance observed in (HI,xn|g). Other: 0.8 ps {I4} from B(E2) measured in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: NS
level_comment:
J from |g(|q) in (|a,n|g). 
T from recoil-distance Doppler shift in (|a,2n|g). Others: 0.55 ns {I14} from |g(t), 0.26 ns {I7} from recoil distance in (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (g.s., 0+ to 776, 2+)=+0.504 {I8}(stat) {I3}(syst) (2021Gi14) 
$B(E2)=0.2537 {I80}(stat) {I31}(syst) (2021Gi14) 
$Diagonal E2 matrix element (776, 2+ to 776, 2+)=-0.33 {I8}(stat) {I6}(syst) (2021Gi14) 
$Spectroscopic quadrupole moments (in eb units) deduced by 2021Gi14 from diagonal E2 matrix element. Authors list this value as -0.25 eb {I6}(stat) {I4}(syst). Compiler has combined the two uncertainties in quadrature 
T$3.96 ps {I14} deduced by compiler from B(E2)=0.2537 {I86}, combining the two uncertainties in quadrature 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
$E2 matrix element (g.s., 0+ to 1475, 2+)=+0.0330 {I12}(stat) {I1}(syst) (2021Gi14) 
$B(E2)=0.00109 {I8}(stat) {I1}(syst) (2021Gi14) 
$E2 matrix element (776.5, 2+ to 1475, 2+)=+0.252 {I9}(stat) {I1}(syst) (2021Gi14) 
$B(E2)=0.0127 {I9}(stat) {I1}(syst) (2021Gi14) 
$M1 matrix element (776, 2+ to 1475, 2+)=+0.073 {I9}(stat) {I1}(syst) (2021Gi14) 
$B(M1)=0.0011 {I2}(stat) {I3}(syst) (2021Gi14) 
T$13.6 ps {I10} deduced by compiler from B(E2)=0.00109 {I8} for 1474.89|g 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (776, 2+ to 1820, 4+)=+0.74 {I7}(stat) {I1}(syst) (2021Gi14) 
$Diagonal E2 matrix element (1820.5, 4+ to 1820.5, 4+)=+0.04 {I75} (2021Gi14) 
$B(E2)=0.1092 {I211}(stat) {I31}(syst) (2021Gi14) 
T$0.75 ps {I15} deduced by compiler from B(E2)=0.1092 {I213}, combining the two uncertainties in quadrature 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
$Lifetime |t=1.67 ps {I21} 
$Sidefeeding lifetime |t{-s}=0.30 ps {I3} 
$Dynamic moment of inertia I{+(2)}=10.4 ~h{+2}MeV{+-1}, I{+(2)}/B(E2)=74 ~h{+2}MeV{+-1}/e{+2}b{+2} {I9} 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
$Lifetime |t=0.39 ps {I5} 
$Sidefeeding lifetime |t{-s}=0.26 ps {I3} 
$Dynamic moment of inertia I{+(2)}=19.6 ~h{+2}MeV{+-1}, I{+(2)}/B(E2)=218 ~h{+2}MeV{+-1}/e{+2}b{+2} {I28} 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
$Lifetime |t=0.34 ps {I5} 
$Sidefeeding lifetime |t{-s}=0.22 ps {I2} 
$Dynamic moment of inertia I{+(2)}=14.9 ~h{+2}MeV{+-1}, I{+(2)}/B(E2)=298 ~h{+2}MeV{+-1}/e{+2}b{+2} {I60} 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Lifetime |t<0.52 ps 
$Dynamic moment of inertia I{+(2)}=21.0 ~h{+2}MeV{+-1}, I{+(2)}/B(E2)<2100 ~h{+2}MeV{+-1}/e{+2}b{+2} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$from optical spectroscopy (1955Ra46) and atomic beam (1961Ku07). |p=+ from comparison of experimental |m with Schmidt limits. 
MOMM1$from atomic beam (1968Br16, 2011StZZ) 
MOME2$from collinear fast beam laser spectroscopy (1995Ke04, 2011StZZ). Others: 0.253 {I5} atomic beam (1963Fa01), 0.259 {I1} recalculation (2001Ke15). 
$MOME2=+0.253 5 from 1989Ra17 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$M1+E2 9.4|g to 9/2+, log {Ift}=7.9 from {+83}Rb |e decay with J|p=5/2-. 
T$weighted average of 156.94 ns {I34} from {+83}Kr IT decay (1.83 h) and 155.1 ns {I12} from {+83}Rb |e decay. 
MOMM1$from Mossbauer (1969Ca06, 2011StZZ). Other: -1.82 {I25} DPAC (1978LeZA). 
MOME2$from Mossbauer (does not include polarization correction) (1977Ho33, 2011StZZ). Other: -0.507 {I3} recalculation (2001Ke15). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1$from collinear fast beam laser spectroscopy (1995Ke04, 2011StZZ) 
J$E3 32|g to 7/2+, log| {Ift}=5.0 from {+83}Br |b{+-} decay with J|p=3/2- 
T$from {+83}Kr IT decay (1.83 h) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$stretched E2 1003|g to 7/2+, (M1+E2) 1012|g to 9/2+ 
T$other: 1.20 ps {I14} from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$stretched E2 619|g from 13/2+, (M1+E2) 1093|g to 7/2+, (M1+E2) 1103|g to 9/2+. 
T$other: 0.21 ps {I6} from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+76}Ge({+11}B,p3n|g). Other: 4.9 ps {I14} from RDDS in {+80}Se(|a,n|g). 
J$(M1+E2) 200.6|g to (15/2-); band assignment 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
J$M1(+E2) 316|g to (17/2-); band assignment 
T$from DSAM in {+76}Ge({+11}B,p3n|g). Others: 1.2 ps {I+6-3} from RDDS in {+80}Se(|a,n|g), 2.8 ps {I+14-7} from DSAM in {+82}Se(|a,3n|g). 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+76}Ge({+11}B,p3n|g). Other: 1.0 ps {I+4-3} from DSAM in {+82}Se(|a,3n|g) 
J$761|g to (17/2-), (M1+E2) 446|g to (19/2-); band assignment 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+76}Ge({+11}B,p3n|g). Other: 0.55 ps {I+35-21} from DSAM in {+82}Se(|a,3n|g). 
J$(M1+E2) 615|g to (21/2-), 1061|g to (19/2-); band assignment 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: PS
level_comment:
T$other: < 0.7 ps from DSAM in {+76}Ge({+11}B,p3n|g). 
J$stretched (E2) 1267|g to (21/2-); band assignment 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_lifetime_unit: PS
level_comment:
J$assigned as J|p=11/2+ in 1981Ca01. Analysis of 1144|g in excitation function data in 1986Pi05 suggests J|p=15/2+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L$from shell model arguments, if the 569-keV level is the L=1, 3/2- state, then the 35-keV level is likely the L=1, 1/2- level. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
T$weighted average of 1.856 h {I36} from ce(t) of 32.1|g (2009Ka30), 1.846 h {I49} from ce(t) of 9.4|g (2009Ka30), 1.82 h {I2} (2010Li13), 1.83 h {I2} (1971Ru17). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$<r{+2}>{+1/2}=4.1882 fm {I14} (2004An14 evaluation). 
J$ hyperfine structure measurement (1933Ko02) consistent with J=0 
$|D<r{+2}>({+86}Kr-{+84}Kr)=+0.042 {i12} fm{+2} from isotope shift (1995Ke04). Others: +0.033 {i22} (1990Sc30, 1979Ge06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L(p,p')=2 
MOMM1$ from g=+0.267 {I13} (2001Me20, transient-field technique). 
T$From 2001Me20, DSA in Coul ex. Other: 4.35 ps {I18} from B(E2)=0.122 {i5} measured in Coulomb excitation (1982Ke01); 3.2 ps {i14} from recoil-distance in (|a,2n|g). 2001Ra27 evaluation gives adopted half-life=4.26 ps 20 and B(E2)(|^)=0.125 {I6}. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L(p,p')=4 
1987Ha21, from their (n,|g) study, propose that the 446.9|g and 1463.8|g deexcite two levels at 2344.3 keV and 2345.6 keV. The 2344.3 is assigned 3+ on the basis of systematics. These conclusions are not adopted by the evaluators since (1) the intensity ratios I|g(446.9)/I|g(1463.8) are nearly the same in (n,|g), |b{+-} decay (31.76 min), and |b{+-} decay (6.0 min), and (2) log| {Ift}=7.0, log| {If{+1u}t}=8.3 for |b{+-} decay from (5-,6-) would limit J=4 to 7. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J L(p,p')=3 
$B(E3)(|^)=0.042 {I15} (2002Ki06 evaluation, data from 1978Ma11, 1974Ar29). Deduced B(E3)(W.u.)=14 {I5} 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
J E2 |g to 6+ in (|a,2n|g). Configuration=(|n g{-9/2}){+-2} 
MOMM1$TDPAD method in (|a,2n|g) (1982Za04). See also 2005St24 compilation 
MOME2$from level-mixing spectroscopy (LEMS) technique (2006Sc22) using Q({+79}Kr, 5/2-)=0.456 {i26} as reference value 
T$from 2006Sc22. Others: 1.89 |ms {I4} from time-differential perturbed angular distribution observed in (|a,2n|g); 1.4 |ms {I4} (1997Is13) based on particle-|g-|g measurement in {+76}Ge+{+198}Pt reaction. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$J=3 preferred from |g|g(|q) in (n,|g), but other J values are not definitely excluded. M1+E2 |g to 3-. 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
MOMM1$from TDPAD method in (|a,2n|g) (1990Ro10,1985Ro22). See also 2005St24 and 1989Ra17 compilations 
J stretched E2 cascade indicated by |g(|q) and linear polarization in (|a,2n|g). 
T$ from |a,|g(t) in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$possible configuration=((|p f{-5/2}){+-1}(|p g{-9/2})) or configuration=((|p p{-3/2}){+-1}(|p g{-9/2})) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_comment:
MOME2$From level-mixing spectroscopy (lems) technique (2006Sc22) using Q({+79}Kr, 5/2-)=0.456 {i26} as reference value 
J$configuration=(|n g{-9/2}){+-2} 
T$Authors give av of their value 1.93 |ms {I4} and 1.84 |ms {I4} (1982Za04) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
J$configuration=((|p f{-5/2}){+-1}(|p p{-3/2}){+-1}(|n g{-9/2}){+-2}) 
G$average value given by 1990Ro10 from their measurement of +0.175 {i15} and their earlier (1985Ro22) measurement of +0.14 {i3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L$J|p(3219 level)=5- in (|a,2n|g). |s(|q) shape for 3225 is not too different from L=5 {i3650} level. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 From 1982Ke01 with a negative sign for the interference term. Other: 0.13 {i1} (1981Ca01). 
$ g factor: from |g(|q,H,t), transient-field technique (2001Me20) 
T$other: 4.35 ps {I18} from B(E2) (1982Ke01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from measured mean lifetime |t=5.541 ps {I13}(stat) {I63}(syst). This value is weighted average of three mean lifetimes |t=5.50 ps {I2}, 5.50 ps {I3} and 5.591 ps {I19}. Other two values, not included in the averaging procedure, were |t=2.53 ps {I8} and 6.39 ps {I4}, both with larger |h{+2} than the first three values. See data in Table 3 of 2018Ch01 for details. Comparison with mean lifetime |t=5.84 ps {I18} from DSAM in Coulomb excitation (2001Me20: Phys. Rev. C 64, 024314). Note that there are four B(E2) measurements from Coulomb excitation, and one RDM measurement in the literature for this state. Based on six measurements (from 1957 to 2002) in the literature, 2016Pr01 (At. Data Nucl. Data Tables 107, 1) evaluation adopted mean lifetime |t=6.04 ps {I+13-22} or T{-1/2}=4.19 ps {I+9-15}, while in {+84}Kr Adopted Levels in the ENSDF database, value was adopted from 2001Me20. The value from 2018Ch01 is the most precise (|?1% uncertainty) and also lower by |?5% as compared to the next precise (|?3% uncertainty) value from 2001Me20. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: Y
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.1846 fm {I22} (2013An02 evaluation) 
J$spin from optical spectroscopy (1955Ra13); L=4 and analyzing power in (pol d,p) 
$Configuration=|ng{-9/2}{+-1} (1989Wi01) 
T$weighted average (NRM method) of 3916.8 d {I25} (2004Sc04 from PTB; this measurement is considered to supersede earlier PTB measurements: 3915 d {I3} in 1992ScZZ and 3909 d {I11} in 1983Wa26), 3905 d {I19} (2012Fi12, corrected value from original 3935.7 d {I12} in 2002Un02, re-evaluated from 3934.4 d {I14} in 1992Un01 and 1982HoZJ, NIST measurement; also 10.75 y {I3} in 1965An07 at NBS, predecessor of NIST), and 3930.2 d {I37} (from 10.76 y {I1} measured in 1963Le07 with assigned 0.02 uncertainty at 95% confidence level). Reduced |h{+2}=2.5 is below the critical |h{+2} value of 3.0 at 95% confidence level. The NRM weighted average is 3922.6 d {I51} or 10.739 y {I14} using 1 sidereal year=365.25636 d. Note that in NRM method, uncertainties were adjusted upwards to 4.6 d from 2.5 d in 2004Sc04 and 4.8 d from 3.7 d in 1973Le07. Others: 10.714 y {I57} (quoted in DDEP evaluation from J.W. Johnston, Battelle Pacific North-Western Lab report B-369 (1974)), 10.27 y {I18} (1953Wa17), 10.57 y {I14} (1953Tu22), 9.4 y {I4} (1947Th06, also Nucleonics 3, 14 (1948)). 2004Wo02 evaluation gives 3927 d {I8} or 10.751 y {I22}, and 2004BeZR evaluation gives 10.752 y {I23}, both heavily influenced by the incorrect and very precise value in 2002Un02. 
T$In DDEP evaluation (2004BeZR) of decay of {+85}Kr isotope, half-life of 10.775 y {I49} or 3929 d {I18} is quoted from 1996Er06. But perusal of 1996Er06 paper does not seem to show any half-life measurement, authors seem to have taken the value quoted above from some other reference 
MOMM1$collinear fast beam laser spectroscopy (1995Ke04). Others: -1.0055 {I4} (1993Ca41,laser resonance fluorescence spectroscopy); 1.000 {I2} (1981Ge06,hyperfine structure); 1.005 (1961Ku07); 1.005 {I2} (1955Ra13,optical spectroscopy). 
MOME2$collinear fast beam laser spectroscopy (1995Ke04), recalculated by 2001Ke15. Others: +0.433 {I8} (1993Ca41,laser resonance fluorescence spectroscopy), +0.433 {I9} (1981Ge06,hyperfine structure); +0.43 {I3} (1955Ra13). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T$from decay curve for 151|g and 305|g (1970Wo08). Others: 4.5 h (1950Ho02), 4.36 h {I9} (1949Ko13), 1949Su14, 4.6 h {I2} (1948Wo07), 4.6 h (1943Bo01,1943Se01,1946Ri07), 4.5 h {I1} (1937Sn02) 
MOMM1$collinear fast beam laser spectroscopy (1995Ke04). 
J$L=1 and analyzing power in (pol d,p); M4 |g to 9/2+ 
T$from IT decay. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: US
level_comment:
T$quoted by 2012Au07 from M. Rudigier et al., Proc. Conf. Leuven, p367 (2011). Other: 1.2 |ms {I+10-4} from p|g(t) in {+82}Se({+7}Li,p3n|g) (1989Wi01) 
J$E2 |g to (13/2+); >13/2 from excitation functions of 60|g and 1931|g in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: US
level_comment:
T$from p|g(t) (1989Wi01) 
$From systematics and shell-model predictions, proposed configuration= |ng{-9/2}{+-1}~#|p(f{-5/2}{+-1},p{-3/2}{+-1}) (1989Wi01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.1301 {I2} 
$E(n)(lab)=1.404 {I2}. |G{-|g}=0.1401 eV {I2}, g|G{-n}=1.812 eV {I4} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$g|G{-n}|G{-|g}/|G=0.074 {I6} 
$E(n)(lab)=65.191 
$This entry is repeated in 2006MuZX, with g|G{-n}|G{-|g}/|G=0.213 eV {I11} in other place 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Spin: optical spectroscopy measurement (1933Ko02) 
$RMS charge radius <r{+2}>{+1/2}=4.1835 fm {I21} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$from g factor=+1.10 {I5} (2014Ku10) measured using transient-field technique in Coulomb excitation. Other: +2.24 {I28} (2001Me20,2014StZZ) 
J$L(t,p)=2 
T$weighted average of 0.308 ps {I17} (DSA, 2001Me20) and B(E2)=0.128 {I10} (1981Ji03), both in Coulomb excitation. Other: B(E2)=0.11 {I3} (1981Ca01) in Coulomb excitation. 
MOMM1$(2001Me20) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
MOMM1$from g=+1.03 {I14} (2014Ku10) measured using transient-field technique in Coulomb excitation. 
J$L(p,p')=4 
T$from |g(t) in {+82}Se({+7}Li,p2n|g). 
$Configuration=|pf{-5/2}{+-1}~#|pp{-3/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(p,p')=3 
$B(E3)=0.036 {I12} (2002Ki06 evaluation based on |b{-3} from data in 1974Ar29 and 1978Ma11) 


level_energy_unit: KEV
level_spin_parity: (5)
level_comment:
J$L(p,p')=(5) suggests 5-. J|p=5+ is also proposed in (p,p') from |s(|q) data and |n(d{-5/2}(g{-9/2}){+-1}) excitation 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
J$L(t,p)=3,4; L(t,|a)=(3) from 3/2- suggests (1 to 5)(+) 
E$this level is most likely different from 3935 due to different spin assignments implied from L-transfers 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
$Configuration=(|pf{-5/2}){+-3}~#(|pp{-3/2}){+-1}~# (|pp{-1/2}){+2}(0+)~#(|ng{-9/2}){+-1}~#(|nd{-5/2}){+1} 
J$|DJ=2, E2 |g to 4+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$this level is most likely different from 4175 due to different spin assignments implied from L-transfers 
J$L(t,p)=2 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$|g rays to 2+ and 3-; no |g rays to 0+ and 4+; level not populated in (|g,|g'); possible allowed |b transition (log| {Ift}=5.4) from (1-) parent. L(t,p)=3,4 is inconsistent, unless S=1 is involved with L=3 in the transfer of two neutrons 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J$|DJ=1, D+Q |g to (5-) and probable configuration= |pg{-9/2}{++1}~#|pf{-5/2}{+-1}~#|pg{-9/2}{++1}~#|pp{-3/2}{+-1}. 


level_energy_unit: KEV
level_comment:
J$this level may have high spin since |s(|q) pattern is not characteristic of any other observed L-transfer. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$The g factor is weighted average of g=+1.03 {I6}, +1.11 {I10}, and +1.19 {I8} measured at E({+86}Kr)=3.2, 3.1 and 3.0 MeV/nucleon, respectively (2014Ku10). Other: +1.12 {I14} (2001Me20) 
BE2$from 1981Ji03, value is not corrected for reorientation. The authors also give B(E2)=0.136 {I11} assuming Q=-0.33. Other: B(E2)=0.11 {I3} (1981Ca01). 
T$from DSA (2001Me20) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
$The g factor is weighted average of g=+0.91 {I22}, +1.24 {I27}, and +1.00 {I27} measured at E({+86}Kr)=3.2, 3.1 and 3.0 MeV/nucleon, respectively (2014Ku10) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$Proposed as member of configuration=|nf{-5/2}{+-1}~#|pg{-9/2}. Strong population in the decay of 1- g.s. of {+86}Br suggests an admixture of |ng{-7/2} -> |pg{-9/2} Gamow-Teller transition 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$mean lifetime |t=336 fs {I4}(stat) {I20}(syst). Authors compare their value with the following from literature: 444 fs {I25} (2001Me20: Phys. Rev. C64, 024314); 341 fs {I27} (1981Ji03: Phys. Rev. C24, 1350); 396 fs {I108} (1981Ca01: J. Phys. G7, 65). Excluding discrepant value from 2001Me20, 2018He09 obtain a weighted averaged value of |t=339 fs {I16} or T{-1/2}=235 fs {I11} by combining their result with values from 1981Ji03 and 1981Ca01, although, compiler notes that value from 1981Ca01 with a large uncertainty of 108 fs does not contribute much to the weighted average. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
From laser spectroscopy (1995Ke04), |d<r{+2}>{-86,87} = 0.125 fm{+2}; authors give three associated uncertainty components 
J from laser spectroscopy (1995Ke04), L=2 in (d,p) and analyzing power in (pol d,p). 
T weighted average of 76.3 m 6 (1972Eh02, |b decay measurements), 76.4 m 10 (1964Cl01, mass spectrometer measurements), 78 m 2 (1949Ko13), and 74 m 2 (1937Sn02). This average has a reduced-|h{+2} of 0.68. The weighted average is the same if the two older values are omitted; then the reduced-|h{+2} is 0.01. 
MOMM1 from 2011StZZ evaluation, based on laser spectroscopy data of 1995Ke04; other: see 1989Ra17 evaluation 
MOME2 from 2011StZZ evaluation, based on laser spectroscopy data of 1995Ke04 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J from L=(2) in (d,p) and isobaric analog of the 15854 level in {+87}Rb J{+|p}=(3/2+,5/2+), confirmed by agreement of spectroscopic factors in {+86}Kr(d,p) and {+86}Kr(p,p') IAR. and L=2 in {+2}H({+86}Kr,p) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$L=2 in (d,p) and L=2 in {+2}H({+86}Kr,p). The direct feed from 1/2+ in (n,|g) makes the 5/2+ alternative less likely 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J from L=5 in {+2}H({+86}Kr,p) and isobaric analog of the 16240 level in {+87}Rb (J{+|p}=9/2-,11/2-), confirmed by agreement of spectroscopic factors in {+86}Kr(d,p) and {+86}Kr(p,p') IAR. Confirmed 11/2- with in-beam spectroscopy (2006Po09) from the expected yrast nature 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J from |g's to 1/2+ and 5/2+ levels. the 952.66 |g to a (7/2+) weakly rules out 1/2+ and suggests |p=+ for 3/2 


level_energy_unit: KEV
level_comment:
J$L=2 in (d,p) and {+2}H({+86}Kr,p) implies 3/2+ or 5/2+ for the 2832 or 2836 level, or both levels. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)
level_comment:
J log {Ift}=6.7, log {If{+1u}t}=8.3 from 5/2-, |g to 5/2+. L=2 in (d,p) and {+2}H({+86}Kr,p) implies 3/2+ or 5/2+ for the 2832 or 2836 level, or both levels. 


level_energy_unit: KEV
level_comment:
J$L=2 in (d,p) and {+2}H({+86}Kr,p) implies 3/2+ or 5/2+ for the 3020 or 3026 level, or both levels. 


level_energy_unit: KEV
level_comment:
J$L=(0+2) in {+2}H({+86}Kr,p) implies 1/2+ and 3/2+,5/2+ for the 3217 or 3226 level, or both levels. 


level_energy_unit: KEV
level_spin_parity: 3/2(-),5/2,7/2
level_comment:
J log {Ift}=6.0, log {If{+1u}t}=7.2 from 5/2-, |g to 5/2+. The 2754 |g to (9/2+) makes 3/2+ unlikely 


level_energy_unit: KEV
level_spin_parity: 3/2(-),5/2,7/2
level_comment:
J log {Ift}=5.9, log {If{+1u}t}=7.0 from 5/2-, |g to 5/2+. The 2943|g to (9/2+) makes 3/2+ unlikely 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2,7/2(-)
level_comment:
J log {Ift}=5.8, log {If{+1u}t}=6.8 from 5/2-, |g's to 5/2+ and 1/2+, although an E3 seems unlikely. 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2,7/2(-)
level_comment:
J log {Ift}=5.9, log {If{+1u}t}=6.8 from 5/2-, |g's to 5/2+ and 1/2+ although an E3 seems unlikely. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J log {Ift}=6.9, log {If{+1u}t}=7.6 from 5/2-, |g to 5/2+, not observed as resonance in (n,X) (see 1983Ra21). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J log {Ift}=7.0, log {If{+1u}t}=7.8 from 5/2-, |g to 5/2+, not observed as resonance in (n,X) (see1983Ra21). 


level_energy_unit: KEV
level_spin_parity: 3/2-,(3/2+)
level_comment:
E,J,L,WIDTHN$1988Ca17 report an unresolved doublet in (n,x) with l=1 and l=(2). For the l=1 component, |G{-n}=780 kev {I 25} and for the l=(2) component, |G{-n}=83 eV {I 13}, both for J=3/2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2+)
level_comment:
J$ Adopted: (11/2-) L=(5) in the (d,p) dataset suggests |p=- for this level. It seems unlikely that a 13/2+ level could be populated in (d,p) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_comment:
T$consistent with a core-coupled 2+~#|n2d{-5/2} configuration. Other: 2.4 ps {I+11-10} (short-lived side feeding) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$S=0.44 {I+9-13} deduced with ANC value {Ib{-d5/2}}=6.46 fm{+-1/2} {I+112-57} using Koning-Delaroche global optical model (2003Ko01). 
L$from 1970Ha16. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$weighted average of 2.804 h {I15} (2012Wa21), 2.860 h {I17} (1972Eh02) and 2.805 h {I25} (1964Cl01). Others: 2.78 h {I6} (1949Ko13), 2.92 h {I17} (1940Gl05). 
$|d<r{+2}>=0.282 fm{+2} {I4} relative to {+86}Kr (2013An02 evaluation). Measured values: 0.282 fm{+2} {I53} (1995Ke04) and 0.304 fm{+2} {I37} (1990Sc30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2 
T$deduced from measured B(E2) and adopted |g-ray properties 
BE2$preliminary result given in 2007Mu07, 2009MuZW 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$stretched Q or |DJ=0, D 460|g gives J=4 or 6. 1328|g to 2+ prefers J=4 and non-zero mixing ratio suggests positive parity. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
BE2$from measured yields of 775|g and 1440.5|g, taking a branching ratio of 85.4% for the 1440.5|g and normalizing to B(E2; 0+ to 775)=0.093 {I9} from 2009MuZW. 
T$deduced by evaluator from B(E2)=0.04 {I2} (2016Mo34) and branching ratio for 2216|g decay from Adopted Levels of {+88}Kr in the ENSDF database (November 2013 update). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$(3-) in {+88}Kr Adopted Levels in ENSDF database (Nov 2013 update). 2017El04, tentatively, assign 2+ on the basis that 3- would give unreasonably high B(E3)(W.u.)>63 for 2420-keV transition 
$Measured |s=11 mb {I3} (2017El04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=10.6 {I+48-50} (2018De35). Others: T{-1/2}=7.7 ps {I11} (from B(E2)=0.131 {I19} in 2017El04: Phys. Rev. C 96, 044332); 11.1 ps {I12} (from B(E2) value, 2007Mu07: Prog. Part. Nucl. Phys. 59, 361, and 2009MuZW: AIP Conf. Proc. 1090, p587) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$from |g(t) (2021Ch46). Measurements were performed using the 196|g and 2392|g at two source to detector distances. Result is a weighted average of 2.802 h {I9}, 2.803 h {I8}, 2.803 h {I4} for 196|g(t) for 50 cm, 15 cm, and combined 50 cm+ 15 cm data, respectively and 2.798 h {I12}, 2.807 h {I12}, 2.802 h {I5} for 2392|g(t) at 50 cm, 15 cm, and combined 50 cm+ 15 cm data, respectively. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$measured by 2012Wa21. Two irradiations were done for {+88}Kr and the final half-life is the mean value of these two experiments, which have half-lives of 2.804 h {I11}, 2.804 h {I10}. The uncertainty budget is discussed. The 2392.1 keV |g-ray from the 2392.1 keV level was used for the half-life measurement. The values of E|g and level energy are taken from the Adopted Levels, Gammas dataset for {+88}Kr in the ENSDF database. Other: half-life=2.825 h {I19} in {+88}Kr Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: MIN
level_comment:
$RMS charge radius: (<r{+2}>){+1/2}=4.2289 fm {I54} (2004An14 evaluation; and 2008 update available at http://cdfe.sinp.msu.ru) 
$|D<r{+2}>({+86}Kr-{+89}Kr)=0.379 fm{+2} {i71} (1995Ke04) 
J$collinear fast LASER beam spectroscopy (1995Ke04). Parity from systematics 
MOMM1,MOME2$collinear fast LASER spectroscopy (1995Ke04). Note that original value of Q=+0.16 {I2} has been re-evaluated to +0.166 {I2} in 2016St14 and 2021StZZ evaluations with reference to re-evaluated Q=+0.259 {I3} for {+83}Kr g.s. by 2018Py01 
T$weighted average of 2.97 min {I7} (1972Eh02), 3.07 min {I8} (1970Fi04), 3.178 min {I23} (1969Ca03), and 3.11 min {I6} (1965Pa14). Others: 3.18 min (1951Ko10,1951Ko50), 2.6 min {I1} (1950Di01), 2.5 min (1943Ha09) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
J$from systematics of nuclides in this mass region, 3/2+ and 5/2+ are expected at low excitations 
T$weighted average of 22.0 ns {I13} (SF decay) and 21 ns {I2} ({+89}Br |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J$spin from |DJ=1, dipole |g from |g|g(|q) in {+252}Cf SF decay, parity from similarity of level structure with {+91}Sr (2008Hw03). Evaluator notes a level at 2077.5, (11/2-) in {+91}Sr Adopted Levels in the ENSDF database (Sept 2013 update), decaying by |DJ=1, dipole |g to (9/2+) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$level introduced by evaluator to account for population of neutron-unbound levels to account for %|b{+-}n decay of {+89}Br x<3346 {I5} (from Q(|b{+-})-S(n)({+89}Kr), where Q(|b{+-})=8262 {I4} and S(n)=4916 {I3} (2021Wa16) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$From |g(t) with mass separation and Ge(Li) (1969Ca03). 
$|D<r{+2}> ({+89}Kr, {+90}Kr)=0.116 fm{+2} {I11} (1996Li25); |D<r{+2}> ({+86}Kr, {+90}Kr)=0.5 fm{+2} {I1} (1995Ke04). Others: 1992Li24, 1992Ne09. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 707|g to 0+ 
T$deduced from B(E2) in Coulomb Excitation. Other: 10.4 ps {I69} from centroid difference between 707|g and 1123|g in LaBr{-3} coincidence spectra in {+235}U(n,F|g). 


level_energy_unit: KEV
level_spin_parity: (3,4,2)+
level_comment:
J$|g|g(|q) data limit J to 2,3,4 in {+235}U(n,F|g). J|p=2+ is less likely due to absence of a ground state transition. Q (assumed E2) transitions to 2+ levels give positive parity. 


level_energy_unit: KEV
level_spin_parity: (5+,6+)
level_comment:
J$|g|g(|q) data in {+235}U(n,F|g) are consistent with J=4,5,6; 4+ is less likely due to the absence of transitions to any of the 2+ states 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<4464 keV from Q(|b{+-})({+90}Br)-S(n)({+90}Kr), where Q(|b{+-})= 10959 {I4} and S(n)=6495 {I3} (2017Wa10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
E$the 799.3|g from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 467.9|g from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$either E(level)=2599.7, as quoted by 2000Rz02 seems to be in error or E|g=832.5 needs adjustment. Evaluator opts for the adjustment of E(level) to be consistent with {+252}Cf SF decay (2011Li34) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 1171.5|g from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 771.4|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 1255.5|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$The |g rays from this level have been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 1258.1|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 916.6|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
J$confirmed from angular correlation of 707.6-799.1 keV cascade; consistent with 2000Rz02 
E$the 799.1|g from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 468.3|g from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 1172.1|g from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from Adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 771.5|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from the Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 1255.6|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from the Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the |g rays from this level have been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from the Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 1259.0|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from the Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$the 916.8|g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from the Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$The 1075.8 |g ray from this level has been assigned to {+91}Kr by 2017Rz01 in {+235}U(n,F|g). Hence, this level is excluded from the Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from centroid difference between 707|g and 1123|g in LaBr{-3} coincidence spectra (2014Re15). Spectra obtained by summing gates on the 199 keV and 331 keV transitions (from the complementary partner {+144}Ba) in the EXILL array (2014Re15). |DT{-1/2} includes uncertainty from large Compton background and prompt response difference uncertaint of 10 ps (2014Re15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+,4+
level_comment:
J$|g|g(|q) data are consistent with J=2,3,4; 2+ is rejected by 2017Rz01 due to the absence of transition to the g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+,6+
level_comment:
J$|g|g(|q) data are consistent with J=4,5,6; 4+ is rejected by 2017Rz01 due to the absence of transition to any of the 2+ states 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: S
level_comment:
|D<r{+2}>({+91}Kr-{+86}Kr)=0.597, uncertainty 0.006 (statistical only), 0.020 (systematic included), 0.114 (including uncertainties arising from evaluation of isotope shifts) (1995Ke04). 
<r{+2}>{+1/2}(charge)=4.255 fm {I8} (2004An14). 
|m, Q: from collinear fast beam laser spectroscopy (2005St24 from 1995Ke04). |m is relative to {+83}Kr, diamagnetic correction included; uncertainty includes estimate of effect of hfs anomaly. 
J J=5/2 from hfs (1995Ke04); |p from assignment of state to 2d{-5/2} shell (1995Ke04) based on hfs data, |m and Q (|m suggests configuration=(|n d{-5/2}){+-1} mixed with 1+ states arising from excitations from d{-5/2} shell to d{-3/2} shell). 
T from 1969Ca03. Other measurements: 8.6 s {I1} (1974Ac01), 9.16 s {I9} (1974Gr29), 8.36 s {I15} (1965Pa14). The weighted average of all data is 8.64 s {I12}. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J E2 144|g to 5/2(+) g.s.; analogy with {+89}Kr and {+93}Sr; probable configuration=(|n d{-5/2}{+3})3/2 (1995Ke04,1990WoZZ). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$This level is not ascribed by 2017Rz01 to g{-7/2} neutron orbital, in contrast to the 7/2+ levels in {+93}Kr and {+95}Kr 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
|D<r{+2}>({+92}Kr-{+86}Kr)=0.751; uncertainty is 0.005 (statistical only), 0.022 (systematic included), 0.139 (including uncertainties arising from evaluation of isotope shifts) (1995Ke04). For discussion of differential changes in |D<r{+2}>, see 1996Li25. 
J g.s. of even-even nucleus. 
T from 1969Ca03. Other data: 1.92 s {I7} (1965Pa14), 1.70 s {I25} (1967Am04), 2.2 s {I3} (1970Lu05). 
%B-N value recommended in evaluation by 1993Ru01; weighted average of 0.040 {I7} (1969Ta04) and 0.0323 {I26} (1975As05). 
<r{+2}>{+1/2}(charge)=4.273 fm {I10} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
J E2 769|g to 0+. E consistent with that for first 2+ state of even-even N=56 isotones in Sr, Mo and Ru (540, 787 and 837 keV, respectively). 
T from preliminary B(E2)|^=0.21 (10%-15% uncertainty) from Coulomb excitation; see comment on 769|g.. 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J 1447|g to 0+ g.s.; D 678|g to 2+ 769. 1989PfZZ suggest J|p=2+ based on energy systematics. If 358|g from 4+ 1804 exists, J|p=(2+) would Be favored. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J stretched E2 1035|g to 2+ 769 level. 1989PfZZ suggest this level may be the expected 3- state; however, that J|p is ruled out by E2 1035|g to 2+, 769 level. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
|D<r{+2}>(relative to {+86}Kr) is 0.811 from collinear fast beam laser spectroscopy (1995Ke04); uncertainties are 0.004 (statistical), 0.023 (with systematic error in voltage calibration), 0.151 (total error, including uncertainty in evaluation from isotope shifts). 
<r{+2}>{+1/2}(charge)=4.280 {I11} (2004An14). 
%B-N Value recommended by 1993Ru01; weighted average of data from 1975As04 (1.9% {I2}), 1975As03 (1.92% {I14}), 1969Ta04 (2.6% {I5}). Other: 3.9% {I6} (1968AmZZ). 
|m: from collinear fast beam laser spectroscopy (1995Ke04); {+83}Kr standard, diamagnetic correction included. 
T weighted average of 1.33 s {I5} (1976Ru01), 1.27 s {I2} (1975As04), 1.289 s {I12} (1969Ca03). Others: 1.17 s {I4} (1965Pa14), 1.19 s {I5} (1968AmZZ) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_comment:
T from {+252}Cf SF decay. Other: 22 ns {I12} from |g|g(t) in {+93}Br |b{+-} decay. 
J |D|p=no 237|g to (3/2+) 117; absence of |g to 1/2+ g.s.; analogy to N=57 isotone {+97}Zr and N=59 nuclides {+99}Zr and {+97}Sr. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J 359|g to 1/2+ g.s.; (M1) 242|g to (3/2+) 117; probably not 1/2+, by analogy to {+97}Zr, {+99}Zr and {+97}Sr. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
$ Total of 1661 implantations observed, and 831 correlated decay sequences. 
T$ values listed in table I: 1040 ms {I65} (syst) {I+80-75} (stat), from maximum likelihood method (MLH); 1243 ms {I30} (syst) {I70} (stat), least-squares fit method. Value in Adopted dataset for {+93}Kr in ENSDF database is 1.286 s {I10}. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
T$ measured by 2013Mi13 from fitting of growth and decay curve for 253-keV |g ray from the decay of {+93}Kr. Diffusion of krypton atoms from implantation tape was accounted for in the reported value of half-life. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n from 2003Be05. Other: 5.7% {I22} (1975As04), measured |b and n activities, deduced %|b{+-}n 
T$from 2003Be05. Others: 0.20 s {I1} (1972Am01), 0.22 s {I2} (1975As04), 0.33 s {I10} (1996Me09) 
$|D<r{+2}>(94,86)=0.99 fm{+2} {I18} (1995Ke04). <r{+2}>{+1/2}=4.301 fm {I13} (2004An14) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ from B(E2) deduced from cross section measurements in projectile Coulomb excitation (2012Al03) 
MOME2$ from E2 diagonal matrix element=-0.34 eb {I+5-22} (2012Al03) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$ Total of 881 implantations observed, and 480 correlated decay sequences. 
T$ values listed in table I: 282 ms {I10} (syst) {I+28-25} (stat), from maximum likelihood method (MLH); 275 ms {I1} (syst) {I27} (stat), least-squares fit method. Value in Adopted dataset for {+94}Kr in ENSDF database is 212 ms {I5}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$ from Adopted Levels of {+94}Kr. 
T$ from B(E2) deduced from cross section measurements in projectile Coulomb excitation (2012Al03,2013Al05) 
MOME2$ from E2 diagonal matrix element=-0.34 eb {I+5-22} (2012Al03, 2013Al05); value is from erratum to 2012Al03, same value in 2013Al05 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$ measured by 2013Mi13 from fitting of growth and decay curve for 187-, 220-, and 629-keV |g rays from the decay of {+94}Kr. Diffusion of krypton atoms from implantation tape was accounted for in the reported value of half-life. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2016Mi18 from decay curves for 187-, 220- and 629-keV |g rays. This value is compared with 212 ms {I5} measured by 2003Be05 (Nucl. Phys. A714, 21) and adopted in the ENSDF database for {+94}Kr Adopted Levels (March 2011 update) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: NS
level_comment:
T$weighted average of 30 ns {I5} from delayed curve spectrum and 33 ns {I3} from prompt-delayed |DT spectrum (2020Ge11) 


level_energy_unit: KEV
level_spin_parity: 1/2(+)
level_lifetime_unit: S
level_comment:
J$from experimental hyperfine spectra (1995Ke04); parity from systematics 
T$from |b(t) and n(t) (2003Be05). Others: 0.78(3) 1976Ah01 (gas-flow method). 
MOMM1$from 1995Ke04 using CFBLS (colinear fast beam laser spectroscopy) 
$|D<r{+2}>(95,86)=1.05 {I19} fm{+2} (1995Ke04) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: S
level_comment:
$|D<r{+2}>(95,86)=1.05 {I19} fm{+2} (1995Ke04) 
MOMM1$from 1995Ke04 using CFBLS (colinear fast beam laser spectroscopy) 
T$from |b(t) and n(t) (2003Be05). Others: 0.78(3) 1976Ah01 (gas-flow method). 


level_energy_unit: KEV
level_spin_parity: 1/2(+)
level_lifetime_unit: MS
level_comment:
$ Total of 152 implantations observed, and 68 correlated decay sequences. 
T$ values listed in table I: 250 ms {I10} (syst) {I+75-55} (stat), from maximum likelihood method (MLH). Value in Adopted dataset for {+95}Kr in ENSDF database is 0.114 s {I3}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from average of 80 ms {I8} and 80 ms {I10} measured by 2003Be05 from fits to neutron and |b decay curves, respectively 
$%|b{+-}n: average of 3.5 {I8} and 3.8 {I4} (2003Be05) 
$The rms charge radius <r{+2}>{+1/2}=4.327 fm {I16} (2008 update of 2004An14 evaluation, available on webpage: http://cdfe.sinp.msu.ru) 
$|Dr{+2}({+96}Kr-{+86}Kr)=1.22 fm{+2} {i23} (1995Ke04). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
J$ Coulomb excitation from 0+; systematics of even-even nuclides. 
T$from E2 matrix element obtained from cross section measurements in projectile Coulomb excitation (2012Al03) 
MOME2$ from E2 diagonal matrix element=+0.2 eb {I7} (2012Al03) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
T$from E2 matrix element obtained from cross section measurements in projectile Coulomb excitation (2012Al03) 
MOME2$ from E2 diagonal matrix element=+0.2 eb {I7} (2012Al03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$ this level is questionable in view of results of Coulomb excitation experiment (2012Al03); thus not given in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$from Adopted Levels of {+96}Kr. 
T$ from B(E2) deduced from cross section measurements in projectile Coulomb excitation (2012Al03,2013Al05) 
MOME2$ from E2 diagonal matrix element=+0.2 eb {I7} (2012Al03, 2013Al05); ; value is from erratum to 2012Al03, same value in 2013Al05 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$ measured by 2011Ni01 from the analysis of the (ion)|b-correlated decay curve. Earlier value: 63 ms {I4} (2003Be05: Nucl Phys A 714, 21 (2003) 
E$ it is assumed that the observed activity corresponds to the g.s. of {+97}Kr 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=83.8 ms, %|b{+-}n=12, %|b{+-}2n=0.0 (2019Mo01). 
$Theoretical T{-1/2}=34.6 ms, %|b{+-}n=0.9, %|b{+-}2n=0.1 (2016Ma12). 
T$weighted average of 42 ms {I4} (2011Ni01, analysis of the (ion)|b-correlated decay curve) and 46 ms {I8} (2003Be05, from decay of |b-delayed neutrons) 
$%|b{+-}n from |bn-coin (2003Be05) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$Value measured in 2011Ni01. Other value: 40 ms {i11} (2003Be05). 
Activity assumed to be from the ground state of {+99}Kr 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is possible, and has been observed (2011Ni01). The |b{+-} decay is expected to be followed by delayed-neutron emissions. 
T$measured by 2011Ni01 from the analysis of the (ion)|b-correlated decay curve, and compared with FRDM+QRPA and KTUY+GT2 calculations. 
$Theoretical T{-1/2}=37.9 ms, %|b{+-}n=30, %|b{+-}2n=0.0 (2019Mo01). 
$Theoretical T{-1/2}=21.1 ms, %|b{+-}n=1.9, %|b{+-}2n=0.1 (2016Ma12). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Measured |s=10 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 15.7 ms (1997Mo25) 
$Probability of misidentification of {+101}Kr isotope<0.001% (2010Oh02) 
J$ 5/2+ predicted in calculations (1997Mo25) 
$Calculated %|b{+-}n=22.8, %|b{+-}2n=1.9 (1997Mo25). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
$Proton decay mode of {+72}Rb is expected to be dominant, as S(p) value is negative from a systematic trend (2021Wa16), and theoretical T{-1/2}(|b decay)=28.4 ms (2019Mo01). 
E$observed events assumed to correspond to the g.s. of {+72}Rb. 
T$estimated by 2017Su31, based on time-of-flight of 769.0 ns through the BigRIPS and the ZeroDegree spectrometers, and comparison of expected activity with the measured yield for {+72}Rb, where the expected activity was determined from quadratic interpolation of the measured yields for neighboring rubidium nuclides, giving expected 10020 {I230} events versus 14 observed events, resulting in estimated half-life of 81-124 ns. 
J$from S(p) and finite-range droplet model and shell model calculations, 2017Su31 suggested the proton transition is either 5+ to 5/2- state in {+71}Kr, or 9+ to 9/2+ state in {+71}Kr, with preference for the former assignment. From density functional theory calculations using Skyrme functional UNEDF0, and comparison with the structure and decay of {+76}Y g.s., 2019Si33 proposed oblate ground state for {+72}Rb, with deformation |b=-0.14, and the most likely configuration=|p3/2[321]~#|n1/2[321], J|p=1+ for the g.s. from G-M rule, in agreement with established 1+ g.s. of mirror nucleus {+72}Br. However, 2019Si33 did not rule out the possibility that the observed decays in both the nuclides may be due to excited states, with a possible 5+ state in both the nuclei. Other: 1+ or 8+ from |W{-p}=7/2+ and |W{-n}=9/2+ (2019Mo01, theory). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
$Evidence for proton decay and unbound character of {+73}Rb g.s. found by 1996Jo17, but percent decay mode was not deduced 
T$from 2017Su31. No events, associated with {+73}Rb decay, were seen by 1996Pf01, 2005Ro39 or 2017Su31. 1996Pf01 estimated T{-1/2}<30 ns from EPAX parametrization and expected |?75 events for {+73}Rb (based on number of events observed for {+74}Rb). 2005Ro39 estimated T{-1/2}<24 ns. 2017Su31 estimated T{-1/2}<81 ns from non-observation of any events associated with {+73}Rb g.s. decay and comparison with EPAX cross sections, whereas 7730 {I130} events were expected. Evaluators prefer a conservative limit of half-life from 2017Su31, as the authors seemed to have better statistics than in 1996Pf01 
J$3/2- from systematics (1996Pf01). |W{-proton}=7/2+ (theory,2019Mo01) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E$deduced from E(p)(lab)=3750 {I40} (1993Ba61) in {+73}Sr |ep decay and S(p)({+73}Rb)=-570 {I200} (syst,2017Wa10) 
J$from 1993Ba61 
$This level decays by protons to {+72}Kr g.s. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$The g.s. (expected E(p)|?570 keV) is not seen in the proton spectrum of {+73}Sr |ep decay due to low-energy cut-off at E>1 MeV (1993Ba61). 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E$deduced from E(p)(lab)=3750 {I40} (1993Ba61) in {+73}Sr |ep decay and S(p)({+73}Rb)=-570 {I200} (syst,2017Wa10) 
$This level decays by protons to {+72}Kr g.s. 


level_energy_unit: KEV
level_comment:
$Population of g.s. in this decay is assumed. If only the g.s. and the IAS at 3.28 MeV are populated in |e decay, then %|b{++}+%|e=37 {I3} for the ground state of {+73}Rb, with log| {Ift}=4.16 {I9} 
$With S(p)=-570 {I200} (syst, 2017Wa10: AME-2016) and T{-1/2}<81 ns (estimated by 2017Su31: Phys. Rev. Lett. 119, 192503, from observation of no events which could be assigned to {+73}Rb), the ground state is expected to decay 100% by proton emission 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E$deduced from E(p)=3.80 MeV {I2} (2020Ho06) in {+73}Sr |ep decay and S(p)({+73}Rb)=-570 {I200} (syst,2017Wa10). E(p) given in 2020Ho06 is assumed by compiler as the lab energy. 
J$assigned by 2020Ho06, based on comparison of measured proton branching ratios from {+73}Rb IAS to the g.s. and the first 2+ state of {+72}Kr, and the predicted values from the GCC calculations, with oblate deformation for the {+72}Kr core. 
$Two strong proton peaks are observed from beta-delayed proton decay: {+73}Sr |) {+73}Rb |) {+72}Kr. The most intense peak at 3.80 MeV {I2} with 62% {I3} branching was assigned to feed the ground state of {+72}Kr, while from the observation of ten (709.7|g)p-coin events, the second peak with 38% {I3} was assigned to feed the first 2+ state in {+72}Kr. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
J$Superallowed |b transition (log| {Ift}=3.5) to 0+. Identified as isospin=1, J|p=0+ state. {+74}Rb is expected to have two low-lying levels, one with isospin=1,J|p=0 and the other with isospin=0. From systematics (1973Ta30), T{-1/2}=2 s is estimated (1977Da04) for the isospin=0 level. A search of isomers for A=74 in this half-life range proved negative (1977Da04,1975Ra03,1978Al23). From |b{+-} syst, 1975Ra03 estimated T{-1/2}=6 s for isospin=0 level. 
T$ from weighted average of 64.761 ms {I31} (2001Ba12,includes systematic uncertainty of 0.015 ms added in quadrature), 64.90 ms {I9} (2002Oi02,2001Oi04), 64.77 ms {I17} (2001Oi04, with gating at E{-|b}>5.2 MeV), 72 ms {I18} (2001Ga24), 60 ms {I10} (1999Lo07), 64 ms {I10} (1998Lo17), 64.9 ms {I5} (1977Da04). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$ since ordering of the 248-443 cascade is not established, the energy of the intermediate level may be 921 or 726 


level_energy_unit: KEV
level_spin_parity: 0
level_comment:
$ The rms charge radius <r{+2}>{+1/2}=4.19 fm {I1} with known radius of {+87}Rb g.s. as reference. |d<r{+2}>({+74}Rb,{+87}Rb)=-0.04 fm{+2} {I5} with <r{+2}>{+1/2}=4.1985 fm {I18} for {+87}Rb from 2004An14. 
$ Measured isotope shift |d|n({+74}Rb-{+78}Rb)=+99 {I10} (2011Ma66) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime=27 ps {I6}, determined from differential recoil-distance Doppler shift (DRDDS) method (2018Mo30). Uncertainty includes statistical and systematic, the latter due to feedings from higher levels, and background contributions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
T$determination of the lifetime of this level by the same method as for the first 2+ was not successful as the statistics were too low to obtain a reliable result (2018Mo30) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$weighted average of 65.5 ms {I8} from |h{+2} fit to implant-|b(t) exponential decay included contributions from the parent, daughter and grand-daughter decays (if appropriate), as well as a constant background and 65.0 ms {I5} from logarithmic binning method (2019Si33) 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: S
level_comment:
$ Measured isotope shift |d|n({+75}Rb-{+78}Rb)=-41.1 MHz {I17} (2011Ma66, collinear laser spectroscopy) 
J$spin from hyperfine structure using collinear-laser spectroscopy at TRIUMF facility. Probable 3/2[312] proton orbital (1997Gr07) 
T$weighted average of 21.4 s {I10} (1983Ke08), 17.0 s {I10} (1977Da04), 17.6 s {I16} (1975Bo52), 21 s {I3} (1975Ra03) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: S
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.2273 fm {I70} (2013An02 evaluation) 
$<r{+2}>(relative to {+87}Rb)=0.220 {I27} (1981Th04) 
J$spin from |b(|q) measurement from oriented ensemble of nuclei (1978Fi01,1978Bo38) and hyperfine structure studies (1981Th04). Parity is from allowed |b feedings to |p=- states in {+76}Kr; agreement of |m and Nilsson configurations suggested by 1984Mo22 
T$weighted average of 36.2 s {I2} (1993Al03), 39.1 s {I6} (1975Bo52), 36.8 s {I15} (1975Ra03). A 1.5-min activity reported by 1972Ve02 has not been confirmed by 1975Bo52 
MOMM1$hyperfine structure studies (1981Th04). Other: -0.372 {I4} (deduced by 2015Pr03 from hyperfine coupling constants measured by 2011Ma66) 
MOME2$value deduced by 2015Pr03 from hyperfine coupling constants measured by 2011Ma66. Measured value of +0.340 {I74} is re-evaluated to +0.41 {I9} in 2021StZZ. Other: +0.46 {I20} (1981Th04,2016St14) from hyperfine structure studies 
$Possible configuration=|p3/2[431]~#|n5/2[303] (1984Mo22) 
$Isotope shift=-494 MHz {I17} (1981Th04). Isotope shift |d|n({+76}Rb,{+78}Rb)=-24.3 MHz {I12} (2011Ma66, hyperfine structure measurements) 
$See 1980Ca23 for theory about isotope shifts 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: US
level_comment:
T$from |g(t) (2000Ch07). Other: 3.20 |ms {I10} (1986Ho22). Weighted average of the two results is 3.051 |ms {I10} 
J$syst of Rb-Kr-Br isotones with N=41, 39 (1988Ga13). Similar 4+ bands in {+76}Br, {+78}Rb and {+74}Br 
$Proposed configuration=|pg{-9/2}~#|ng{-9/2} (1986Ho22) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$316.96 {I8} in the Adopted Levels 
T$from |g(t) (2000Ch07). Other: 3.20 |ms {I10} (1986Ho22). Weighted average of the two results is 3.051 |ms {I10} 
$Proposed configuration=|pg{-9/2}~#|ng{-9/2} (1986Ho22) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius <r{+2}>{+1/2}=2.2356 fm {I80} (2013An02) 
$Evaluated |d<r{+2}>({+87}Rb,{+77}Rb)=0.2884 fm{+2} {I69} (2013An02) 
MOMM1,MOME2$from hyperfine-structure measurement using laser technique on a mass-separated atomic beam of {+77}Rb produced by the fission of uranium or by spallation reaction on niobium (1986Du16,1981Th04). Measured |m=+0.6568 {I41} (1981Th04), +0.6544680 {I16} (1986Du16) is re-evaluated to +0.65434 {I2} by 2019StZV. Other: +0.652 {I7} (1978Ek04). Q=+0.70 {I4} in 1981Th04 is re-evaluated to +0.84 {I17} in 2016St14 
$|D<r{+2}>({+77}Rb-{+87}Rb)=0.283 fm{+2} {I7}; rms charge radius=4.2335 fm {i26} (1981Th04). 
J$from atomic-beam method (1978Ek04). Parity from agreement of measured magnetic dipole moment with shell-model calculations 
T$weighted average of 3.78 min {I4} (1993Al03), 3.62 min {I10} (1975BaWR), 3.8 min {I3} (1975Ra03), 3.9 min {I1} (1975Li13), 3.9 min {I1} (1972Ar02) and 3.6 min {I2} (1972De40). Others: 6.1 min in 1972Ve02 probably belongs to {+78}Rb, 2.8 min {I10} (1971Do01, assignment to {+77}Rb or isomer in {+77}Kr) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.89 ps {I6} (DSA, 1997Ha08), 1.41 ps {I17} (DSA) 1.09 ps {I26} (RDDS). The last two values are quoted by 1997Ha08 from thesis by Luhmann. 1986Lu08 give 1.28 ps {I21} from DSA 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.64 ps {I3} (DSA, 1997Ha08), 0.78 ps {I15} (DSA), 0.88 ps {I18} (RDDS). The last two values are quoted by 1997Ha08 from thesis by Luhmann. 1986Lu08 give 0.83 ps {I10} from DSA 


level_energy_unit: KEV
level_spin_parity: 0(+)
level_lifetime_unit: MIN
level_comment:
$|D<r{+2}> (relative to {+87}Rb)=0.3060 {I23} (1981Th04); isotope shift (relative to {+87}Rb)=-478.4 {I15} (1981Th04) 
$ <r{+2}>{+1/2}=4.241 fm {I8} (2004An14 evaluation) 
J$spin from atomic-beam method (1978Ek04,1978Ek05). |b|g coin measurement (1981Ba40) gives negligible feeding of 2+, suggesting |p=+; however, |p=- is not completely ruled out. Proposed (1978Ek04) configuration= |p5/2[422]|n5/2[422] consistent with 0+ 
T$from weighted average of timing of 455|g, 511-keV annihilation radiation, 562|g, 2982|g, 3437|g and 3893|g (1981Ba40,also 1975BaWR thesis). Others: 16.5 min {I12} (1979He18), 10.6 min {I30} (1974Sa32), 17.5 min {I30} (1973Br32), 19 min (1972ArZS), 17.5 min {I20} (1972No14) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: US
level_comment:
J$(E1) |g to 0(+) 
T$|g|g(t) (1997Mu02) in {+78}Sr decay. Other: 0.42 |ms {I7} from |g|g(t) in {+58}Ni({+23}Na,2pn|g) (1996Ka24). Unweighted average of the two values is 0.67 |ms {I24} 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1,MOME2$atomic-beam laser spectroscopy (1981Th04). Other: |m=+2.56 {I3} (atomic beam method,1978Ek04). See also 2005St24 compilation. 
$%IT decay revised from 10% {I2} in 1975BaWR to 9% {I2} by the evaluators. See it decay dataset for details 
$|D<r{+2}> (relative to {+87}Rb)=0.1912 {I26}; isotope shift (relative to {+87}Rb)=-403.8 {I17} (1981Th04) 
T$from weighted average of timing of Rb x ray, 46.8|g, 103|g, 455|g, 511-keV annihilation radiation and 664|g (1981Ba40,also 1975BaWR thesis). Others: 5.8 min {I2} (1979He18), 4.4 min {I8} (1974Sa32), 6.5 min {I5} (1973Ba03), 6.0 min {I5} (1972No14), 6 min {I2} (1972ArZS), 6.0 min {I2} (1972De54), 6.55 min {I18} (1969Ch18), 6.0 min {I10} (1968To05), (1972Bo31) 
J$spin from atomic-beam method (1978Ek04). (M3) |g to (1-). The measured magnetic moment agrees with proposed (1978Ek04) configuration=|p5/2[422]~#|n3/2[301] of negative parity 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$ possible bandhead of |pg{-9/2}~#|ng{-9/2} configuration expected from systematics of odd-odd nuclides in this region. A well-developed band is observed up to 19+ with interlocking dipole and quadrupole transitions. 


level_energy_unit: KEV
level_spin_parity: (0-,1,2+)
level_comment:
J$ |g's to 1(+), (1-) and (2-); possible |e+|b{++} feeding from 0+; (2+) proposed in in-beam |g-ray studies 


level_energy_unit: KEV
level_spin_parity: (0-,1)
level_comment:
J$ |g's to 1(+), (1-) and (2-); possible |e+|b{++} feeding from 0+. No J|p proposed in in-beam |g-ray studies 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$from multispectrum studies 
E$from 1991McZZ. Earlier estimate (103+x, x<15 keV) was quite close to this energy 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4(-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$ Configuration=|p5/2[422]~#|n3/2[301],K|p=4- 
E,J,T$ from Adopted Levels of {+78}Rb in ENSDF database; isomer not not populated in {+78}Sr decay 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
$ Configuration=|p3/2[312]~#|n3/2[301],K|p=3+ 
$ No |g from this level is reported. The feeding 112.6|g has 1.49 {I9} units of relative intensity or 0.47 {I3} units of absolute intensity 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius=4.2284 fm {I65} (2013An02) 
$Evaluated |d<r{+2}>({+79}Rb,{+87}Rb)=0.2291 fm{+2} {I23} (2013An02) 
MOMM1,MOME2$from hyperfine structure in LASER-spectroscopy (1981Th04). Other: |m=3.37 {I7} (1978Ek05,1978Ek04). Q=-0.098 {I22} in 1981Th04 re-evaluated in 2013StZZ 
J$spin from atomic-beam method (1978Ek04,1981Th04); parity from L({+3}He,d)=2 
T$average of 22.8 min {I5} (1972Br31) and 23.0 min {I5} (1971Li02). Others: 23.0 min {I5} (1973BoXS), 24 min {I2} (1968To05), 20.9 min {I8} (1961Ch16), 24 min {I1} (1957Ch31) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_comment:
T$average of 18 ns {I1} (1982De36) and 23 ns {I1} (1981Li12) 
J$dipole |g to 5/2+ and evidence of |e feeding from 3/2(-). Linkages of transitions from the negative parity band to positive band and measured lifetimes favor 3/2- over 5/2- 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=4; |DJ=2 |g to 5/2+ 
T$from |g(t) (1994Io02). Other: 18 ns {I4} (1982Pa20) 
MOMM1$TDPAD in {+79}Br({+3}He,3n|g) (1994Io02) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=1 |g to 3/2- (1/2 not allowed by |g(|q)); probable band assignment. L({+3}He,d)=3 for a 366 group gives 5/2- or 7/2- for 363 or 357 level 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.83 ps {I14} (1982Pa20), 0.69 ps {I21} (1993Ho15), 0.769 ps {I30} (2006Si26) 


level_energy_unit: KEV
level_comment:
J$(17/2+) suggested by 1996Sm07 from |DJ=2 |g to 13/2+; 1993Ho15 suggest (15/2+) from |DJ=1 |g to 13/2+ 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.042 ps {I14} (1993Ho15), 0.069 ps {I28} (2006Si26). Other: <0.21 ps (1982Pa20) 


level_energy_unit: KEV
level_comment:
J$2006Si26 assign 27/2+ (37/2 seems a misprint in paper), but implied M3 for 1897.3 transition to 21/2+ is unlikely 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
$<r{+2}>{+1/2}=4.229 fm {I7} (2004An14) 
$ Isotope-shift ({+80}Rb-{+87}Rb)=-352.8 MHZ 44 (1981Th04) 
$ |D<r{+2}>({+80}Rb-{+87}Rb)=0.2166 fm{+2} {I18} (1981Th04) 
T$ from 1993Al03. Other: 34 s {I4} (1961Ho13) 
J$log| {Ift}=4.79 from 0+. In-beam optical pumping methodS (1974NeZI,1977CoZP) 
MOMM1$value quoted by 1978Ek04 from measurement (atomic beam method using lasers) by 1974NeZI. Other: -0.0833 {I17} (1981Th04,hyperfine structure study using lasers) 
MOME2$hyperfine structure measurement using LASER spectroscopy 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: US
level_comment:
E$ microsecond isomer first reported by 1980RaZL in {+66}Zn({+16}O,pn|g) reaction. From its possible deexcitation through a transition of high internal conversion, the estimated value was |<50 keV above the 486 level. The current level energy is based on 494.4 from 1992Do10 
T$|g(t) (1996Io01). Others: 1.60 |ms {I2} (1980RaZL,1979RaZS), 2.4 |ms {I2} (quoted by 1992Do10 from HMI-318 report, p80 (1979)) 
J$ agreement of experimental g=+0.563 {I4} (1996Io01) with calculated value of +0.543 for 2-quasiparticle configuration: |pg{-9/2}|ng{-9/2} 
MOMM1$ Time-differential PAD method. Others: +3.36 {I6} (1980RaZL, 1979RaZS,1989Ra17), +3.342 {I30} (quoted by 1989Ra17 from HMI-318 report, p80 (1979)) 
MOME2$differential PAD in (HI,xn|g). Value quoted by 1989Ra17 is from measurement by Stenzel (thesis,1986, HMI) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: US
level_comment:
E$ microsecond isomer first reported by 1980RaZL in {+66}Zn({+16}O,pn|g) reaction. From its possible deexcitation through a transition of high internal conversion, the estimated value was |<50 keV above the 486 level. The current level energy is from 1992Do10 
T$|g(t) (1996Io01). Others: 1.60 |ms {I2} (1980RaZL,1979RaZS), 2.4 |ms {I2} (quoted by 1992Do10 from HMI-318 report, p80 (1979)) 
G$ others: =0.56 {I1} (1980RaZL),1979RaZS), +0.557 {I5} (quoted by 1989Ra17 from HMI-318 report, p80 (1979)). Differential PAD method 
MOME2$ 1989Ra17 quote from work by Stenzel,thesis, 1986,HMI). Differential PAD method 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ |g rays feeding this state have no coincidences with |g rays below it, since it is |ms isomer 
E,T$ from {+80}Rb Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
MOMM1 from 2019StZV (in 1981Th04 +2.0595 {I14}, atomic beam laser spectroscopy). 
MOME2 from 2021StZZ (in 1981Th04 Q{-s}=+0.398 {I23} - laser induced optical pumping; includes anti-shielding correction). 
<r{+2}>{+1/2}(charge)=4.221 fm {I5} (2013An02). 
J atomic beam (1956Ho52); L({+3}He,d)=1. 
T weighted average of 4.570 h {I4} (2004Sc04; decay followed for ~15 half-lives), 4.580 h {I9} (1970Wa38; authors' value based on independently determined values of 4.582 h {I9}, 4.581 h 9 and 4.575 h {I35}) and 4.565 h {I9} (1982Gr07; followed for 6-10 half-lives). Other: 4.6 h {I5} (1972Va41). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$%|e+%|b{++} deduced by the evaluator using data in 1977Li14. See {+81}Rb |e decay (30.5 m) dataset. %IT=100 - (2.1 {I4}). 
MOMM1$from 2019StZV (in 1981Th04, +5.5980 {I17} - atomic beam laser spectroscopy, 1981Th04). Q includes Sternheimer correction. 
MOME2$From 2020StZV (in 1981Th04 -0.74 {I6} - atomic beam laser spectroscopy, includes Sternheimer correction). 
J atomic beam (1956Hu69); E3 |g to 3/2- 
T weighted average of 31.5 min {I20} (1956Do52), 30.25 min {I25} (1977Li14), 30.59 min {I28} (1980Ho28), and 33.2 min {I11} (1981FrZY). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J L({+3}He,d)=3+1 for E=184 keV doublet; this level must correspond to the L=3 component since J(188 level)<5/2; D(+Q) |g to 3/2-. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J L({+3}He,d)=3+1 for E=184 keV doublet, presumably L=1 is the dominant component for this level (see comments for 153.484 keV level.). I(|e+|b{++}) from 1/2-. 


level_energy_unit: KEV
level_spin_parity: 1/2(-),3/2(-)
level_comment:
J stronger I(|e+|b{++}) feeding from 1/2-; |g to 5/2-. 3/2-,5/2- doublet at 461 keV in (|a,p); however, the 463 level is also a possible candidate for the 3/2- member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)-
level_comment:
E average of 461 (|a,p) and 454 ({+3}He,d). 
J L({+3}He,d)=3+1; 3/2- + 5/2- doublet in (|a,p). Levels energetically not resolved from neighboring levels, but none of those is a candidate for J|p=5/2-. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2)
level_comment:
J I(|e+|b{++}) feeding from 1/2-; 549|g to 5/2-. L({+3}He,d)=1 at 701 keV; J=(3/2) from J dependence in (|a,p) for 705-keV state. |p=- for the 702 and/or the 712 level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_comment:
J L({+3}He,d)=2+1 for E(level)=920; J|p=(5/2+) from J dependence in (|a,p) for E(level)=913. Evaluator assumes the latter corresponds to L=2 component of the ({+3}He,d) doublet; the L=1 component in ({+3}He,d) could correspond to the 909 and/or the 923 level(s). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J presence of (|e+|b{++}) feeding from 1/2- in |e decay; presumed to be the L=1 component of 1559-keV doublet in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_lifetime_unit: PS
level_comment:
J E2, |DJ=2, |g to (13/2)+; band structure. 
T weighted average of 0.73 ps {I14} from DSA in {+55}Mn({+29}Si,2pn|g) and 0.87 ps {I7} from RDM and DSA in {+65}Cu({+19}F,p2n|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
E from (|a,p) 
J 5/2 from J dependence of |s(|q) in (|a,p); |p=+ from L({+3}He,d)=0+2 for 1726-keV doublet. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J |g to (5/2+); presence of (|e+|b{++}) feeding from 1/2- in |e decay; probably L=0 component of L=0+2, E=2195 doublet in ({+3}He,d). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
E from (|a,p); E=2195 for doublet in ({+3}He,d). 
J J dependence in (|a,p); probably the L=2 component of the L({+3}He,d)=0+2 doublet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
E from (|a,p); 2406 keV doublet in ({+3}He,d). 
J J dependence of (|a,p) measurement. Probable L=2 component L({+3}He,d)=0+2 doublet. 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J tentative candidate in {+68}Zn({+19}F,|a2n|g) for 13/2 member of a band which includes the (17/2-) 2697 level; in that reaction, the 210.5|g (not the unconfirmed 155|g of {+53}Cr({+31}P,2pn|g)) was assigned to the |g cascade following the 61|g which deexcites the J=17/2 band member. 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: PS
level_comment:
J E2 |g to (17/2)+; band assignment. 
T weighted average of 0.42 ps {I14} from {+65}Cu({+19}F,p2n|g) and 0.33 ps {I6} {+55}Mn({+29}Si,2pn|g), both from DSA; not corrected for feeding. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
E from (|a,p). Other: 2812 ({+3}He,d). 
J J dependence in (|a,p); L=0 component of L({+3}He,d)=0+2 doublet. 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J D 1472|g to (17/2)+; 761|g to (15/2-) 2294; band assignment. Other: (19/2+) in {+68}Zn({+19}F,|a2n|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
E average of 3257 (|a,p) and 3227 ({+3}He,d). 
J J=5/2 from spin dependence of |s(DWBA) in (|a,p); L({+3}He,d)=2. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
J D |g to (21/2)+; (Q) intraband |g to (19/2-). Other: 23/2+ in ({+31}P,2pn|g). 
T From Doppler-shifted lineshape in {+68}Zn({+19}F,|a2n|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_comment:
E$level energy held fixed in the least-squares adjustment 
E rounded-off value from Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (19/2+)
level_comment:
J probable 19/2+ member of band built on 7/2+ 434-keV level (1989Ta09). Note, however, that adopted band assignment differs from this. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2)+
level_lifetime_unit: PS
level_comment:
T from |t=8.7 ps {I4} (1982Pa06 - RDM). Other: 6.0 ps {I4} (from |t=8.7 ps {I5} 1975Fr04, RDDS, cascade feeding taken into account - level energy listed as 623 in Table I). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2)+
level_lifetime_unit: PS
level_comment:
T From |t=1.25 ps {I10} (1982Pa06 - RDM). Other measurement: T{-1/2}=0.215 ps {I28} (from |t=0.31 ps {I4} 1975Fr04, DSA - level energy listed as 876 in Table I); source of discrepancy unclear. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2)+
level_lifetime_unit: PS
level_comment:
T from |t=0.6 ps {I2} (1982Pa06 - DSA). Other: 0.111 ps {I21} from |t=0.16 ps {I3} table I of 1975Fr04 (DSA) level energy listed as 1024, but another uncertainty of 0.040 given in text. Reason for discrepant lifetime is unclear. 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$GDR strength=0.90 {I5} 
$Mean angular momentum <J>=17 ~h {I4} 
$IVGDR intrinsic width remains constant with the excitation. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J J=1 from atomic beam (1981Th04). log| {Ift}=4.8 from 0+. 
T$from 1987Wo01. Others: 1.273 min {I2} (1978Gr17), 1.25 min {I3} (1953Li27), 1.27 min {I8} (1953Kr10) 
MOMM1 LASER induced optical pumping of thermal atomic beam with and without rf resonance (1986Du16); value relative to |m=2.751816 {I2} for {+87}Rb(g.s.) and subject to hyperfine anomaly correction, high-resolution LASER spectroscopy on atomic beam (1981Th04). Other value: +0.554 {I6} (1978Ek04), radiative detection of optical pumping, recalculated (1989Ra17) 
MOME2$Revised from +0.19 {I7} (1981Th04), laser induced optical pumping of thermal atomic beam, polarization correction included. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
J J=5 from atomic beam (1981Th04). log| {Ift}=4.9 to 4-. 
T from 1982Gr07. Other: 6.2 h {I5} (1967Vr07). 
MOMM1 Atomic beam (1957Hu75,1976Fu04); value relative to |m=2.751816 {I2} for {+87}Rb(g.s.) and subject to hyperfine anomaly correction. Other values: +1.5133 {I24} from high-resolution LASER spectroscopy on atomic beam (1981Th04); +1.51 {I2} from recalculation of atomic beam data (1978Ek04) 
MOME2$Revised from +1.01 {I12} (1981Th04), LASER induced optical pumping of thermal atomic beam, Sternheimer correction included 
%IT If B(M4)(W.u.)<30 (RUL). 
See 1991Ko24 for production of {+82}Rb via the {+82}Kr(p,n) process at a low energy cyclotron. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
$|m,T{-1/2} from |g(|q,H,t) (1996Io01). Isomer produced in {+79}Br({+4}He,n), {+81}Br({+3}He,2n). Other T{-1/2}=13.9 ns {I21} (1991Do05) in (|a,n|g) 
J$on the basis of g measurement configuration=((|p g{-9/2})(|n g{-9/2}){+3}) is suggested (1999Io01) 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J$from |g(|q) and linear polarization of the decay |g, and systematics consideration. Configuration=((|p p{-3/2})(|n g{-9/2})) (1999Do02) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_comment:
J$suggested as a 4-quasiparticle state with configuration=((|p g{-9/2}){+2}(|p p{-3/2})(|p f{-5/2})(|n g{-9/2})) (1999Do02) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J$adopted value. Assignment of 5+ by 1991Do05 is disputed by later work using (HI,xn|g) by 1999Do02 (some of the same authors as 1991Do05). This assignment, however, is not in agreement with linear polaization measurement. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J$from 2000Sc17. J|p=(6-,7-) in 1999Do02. Assignment of 5+ by 1991Do05 is disputed by later work by 1999Do02 (some of the same authors as 1991Do05). This assignment, however, is not in agreement with lin pol measurement for 325|g by 1991Do05 


level_energy_unit: KEV
level_spin_parity: (11-)
level_comment:
J$suggested as a 4-quasiparticle state with configuration=((|p g{-9/2}){+2}(|p p{-3/2})(|p f{-5/2})(|n g{-9/2})) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: D
level_comment:
MOMM1$from Atomic Beam Laser Spectroscopy (1981Th04,2011StZZ), value relative to |m=+2.751818 {I2} for {+87}Rb. 
MOME2$from Atomic Beam Laser Spectroscopy (1981Th04); value includes polarization correction. Other: +0.27 {I5} in optical double resonance (1973Ac02). 
J$J=5/2 from atomic beam (1976Fu06). |p=- from comparison of experimental |m with Schmidt values. 
T$86.2 d {I1} is reported by 1972Br37 and 2000Hu20. Others: 86.0 d {I4} (1976Gi14), 85.7 d {I13} (1973Ll02). 
$|d<r{+2}>{+83,87}Rb=0.0512 fm{+2} {I15} (1981Th04). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$M1 5.2|g to 5/2-, L=1 component of L({+3}He,d)=3+1 doublet (g.s. + 5.24) 
T$from ce|g(t) in {+83}Sr |e decay. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MS
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
J$M2 42|g to 5/2-, L({+3}He,d)=4. 
T$from RUL of B(M2)(W.u.)|<1. 1968Et01 report an unpublished value of T{-1/2}=7.8 ms {I7} for this level. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L({+3}He,d)=1 limits J|p to 1/2-,3/2-; 1649.5|g from 1748 level, which decays also to 9/2+ and 9/2-, excludes 1/2-. 
T$T{-1/2}<150 ps from delayed coincidence (1973Br32) in {+83}Sr |e decay is inconsistent with |d for the 94.11|g since B(E2)(W.u.) would be >300. 1968Et01 report an unpublished value of T{-1/2}=1.2 ns for the 94.11|g, which is in agreement with M1+E2 multipolarity. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$3/2 from excitation function in {+80}Se({+6}Li,3n|g), |p=- from E2(+M1) 389|g to 5/2- 
T$from DSAM in {+82}Kr(p,|g),{+83}Kr(p,n|g). Other: <130 ps from delayed coincidence in {+83}Sr |e decay 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$E2 381.5|g to 9/2+, E1 418|g to 3/2- 
T$from DSAM in {+82}Kr(p,|g),{+83}Kr(p,n|g). Other: <150 ps from delayed coincidence in {+83}Sr |e decay. 
E$the 439 level seen in ({+3}He,d) with L=1+2 is likely a doublet of the 423 level and 440 level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
E$from (|a,p). The 439 level seen in ({+3}He,d) with L=1+2 is likely a doublet of the 423 level and the 440 level. 
J$J-dependence of (|a,p), L({+3}He,d)=1 component of the L=1+2 doublet. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
J$E2(+M1) 382|g to 5/2+, E2(+M1) 763|g to 9/2+, 805|g to 5/2- gives J|p=5/2+,7/2+; excitation function in {+80}Se({+6}Li,3n|g) is consistent with J=7/2. 
T$others: <60 ps from delay coincidence in {+83}Sr |e decay, <1.0 ps from DSAM in {+82}Kr(p,|g),{+83}Kr(p,n|g). 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2)
level_comment:
J$log| {Ift}=6.6 from 7/2+ parent, 1019|g to 11/2+. J|p=7/2+,9/2+ from ({+3}He,d) if the L=4 component of the L({+3}He,d)=1+4 doublet at 2062 keV is the same as the 2057-keV level. 


level_energy_unit: KEV
level_spin_parity: (13/2)
level_comment:
J$(11/2,13/2) from excitation function in {+80}Se({+6}Li,3n|g), D 208|g from 15/2-, D 1168.5|g to 11/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
E$average of 2904 keV ({+3}He,d) and 2907 keV (|a,p). 
J$L({+3}He,d)=0+2 (doublet), J dependence of (|a,p). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$considered questionable, see the Adopted Levels. 
T$other: 1.2 ns, unpublished value reported by 1968Et01, considered questionable. 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.07 ps {I12} (2009Sc22) and 0.97 ps {I21} (1985Zh09), both from DSAM. Other: 0.40 ps {I+14-10} (2006Ga10) also from DSAM. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
T$other: <3.5 ps (2009Sc22) from DSAM, deduced from the effective lifetime without feeding corrections. 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
T$other: 1.5 ps {I+6-4} from DSAM in 2006Ga10; value not adopted as it leads to a rather large B(M1)=1.9 W.u. for the 182 |g-ray transition. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.41 ps {I13} (2009Sc22) and 2.0 ps {I5} (1985Zh09), both from DSAM. Other: 0.64 ps {I+26-12} (2006Ga10), also from DSAM. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$other: 0.69 ps {I21} from DSAM in 2006Ga10; value is not adopted as it leads to a rather large B(E2)=310 W.u. for the 362 |g-ray transition. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from singles DSAM. Other: <0.6 ps from coincidence DSAM, however, this analysis contains a contribution of up to 80% from the 763|g in {+85}Rb 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
$<r{+2}>{+1/2}=4.1992 fm {I22} (2004An14 evaluation). 
$ Measured |D<r{+2}>({+84}Rb-{+87}Rb)=0.0078 fm{+2} {I32} (1981Th04). 
%B-$deduced by the evaluator from I|b{+-}(g.s.)/I|b{++}(g.s.)=0.29 {I15} (an estimate by 1958Be81 with a 50% uncertainty assumed by the evaluator) and I|b{++}(g.s.)=13.6% {I9}, calculated by the evaluator using the following information: I|b{++}(882)/I|b{++}(g.s.)=0.97 {I5} (average of 0.92 and 1.008 {I12} as deduced from |b{++} spectra (1971Bo01) and |g{+|+}|g{+|+} and |g{+|+}|g{+|+}882|g triple coincidences (1971Ge10), respectively), |e(g.s.)/I|b{++}(g.s.)=1.026 {I12} (from theory, deduced using Q(|e)=2686 keV {I3} (2009AuZZ)), and |e(882)/I|b{++}(882)=4.43 {I18} (1970Go44). %|e+%|b{++}=100 - %|b{+-} 
J$from atomic beam (1956Ho52); L(p,d)=4 (J|p=5/2- for the target); |g|g(|q) in {+84}Rb IT decay (1958Co67) 
T$weighted average of 32.77 d {I14} (1976Gi14) and 32.84 d {I8} (2000Hu20). Both work used Ge detectors to detect 881.6|g as a function of time and followed the decay for a time period of approximately three half-lives. Other: 33.2 d {I4} (1976Bo19), 34.5 d {I2} (1971Ge10), 33.0 d {I2} (1955We40). 
MOMM1$from atomic beam (1962Kh03). Others: -1.3246 {I16} using the high-resolution LASER spectroscopy on atomic beam technique (1981Th04), -1.296 {I11} using the optical double resonance technique (1973Ac02), -1.33 {I2} (atomic beam,1957Hu75). See also 2005St24 compilation 
MOME2$using the high-resolution LASER spectroscopy on atomic beam technique (1981Th04). Other: +0.005 {I1} using the optical double resonance technique (1973Ac02). See also 2005St24 and 1989Ra17 compilations 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
J$248.02|g E2(+M1) to 2-; 215.61|g M3+E4 from 6-; |g|g(|q) in {+84}Rb IT decay (1958Co67) 
T$From 216ce-248|g(t) centroid shift in {+84}Rb IT decay (1968Se02) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$ Measured |D<r{+2}>({+84}Rb-{+87m}Rb)=0.004 fm{+2} {I16} (1981Th04). 
$A small |e+|b{++} branch (%|e+%|b{++}|<0.0012) seems possible, but not definitely established (1979Er03, see {+84}Rb IT decay). 
J$From atomic beam (1978Ek04); L(p,d)=4 (J|p=5/2- for the target); |g|g(|q) in {+84}Rb IT decay (1958Co67) 
T$From 1982Gr07; the uncertainty is statistical only. Others: 20.6 min {I8} (1976Sl07), 21.2 min {I5} (1976Bo19), 20.0 min {I5} (1970Pa09), 20.5 min {I2} (1969Kn05), and 19.8 min {I7} (1958Co67). 
MOMM1,MOME2$Using the high-resolution LASER spectroscopy on atomic beam technique (1981Th04). See also 2005St24 and 1989Ra17 compilations 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
$218.3|g E2 to 3-; (3.4|g) to 6- 
T$From |g(t) in {+81}Br(|a,n|g), but the gating transitions were not provided by the authors (1991Do04) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: NS
level_comment:
J$70.7|g to (4-); 76.4|g to 5-; 79.8|g to 6-; comparison with |p=+ sequence in several odd-odd Br nuclides. 
T$From |g(t) in {+81}Br(|a,n|g) (1991Do04) 
$Possible configuration=((|p g{-9/2})(|n g{-9/2})) 


level_energy_unit: KEV
level_spin_parity: 4-,5,6
level_comment:
J$135.5|g to 5-; 139.0|g to 6-; the weak population of this state in {+81}Br(|a,n|g) and the non-observation in {+76}Ge({+11}B,3n|g) would argue against J|p=7- 


level_energy_unit: KEV
level_spin_parity: (4,5)-
level_comment:
J$L(p,d)=4 (J|p=5/2- for the target); 141.3|g to (4-); 146.9|g to (5-); 150.4|g to 6-; the weak population of this state in {+81}Br(|a,n|g) and the non-observation in {+76}Ge({+11}B,3n|g) would argue against J|p=6- 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
J$L(p,d)=0+2 (J|p=5/2- for the target) and the assumption that the (p,d) peak corresponds to a single level. 


level_energy_unit: KEV
level_spin_parity: (17-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$766.4|g to (16-); 1489.3|g to (15-); band assignment 
T$Effective value, not corrected for side-feeding 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$From adopted levels 
T$From 1982Gr07, but the uncertainty is statistical only. Others: 20.6 min {I8} (1976Sl07), 21.2 min {I5} (1976Bo19), 20.0 min {I5} (1970Pa09), 20.5 min {I2} (1969Kn05), and 19.8 min {I7} (1958Co67). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: NS
level_comment:
T$from |g(t), but the gating transitions were not provided by the authors 
CONF$1991Do04 state that the assigned configuration=((|p p{-1/2})(|n g{-9/2})) to this state explains the high M1 strength of the 3.4|g. However, see evaluator's note on the authors' B(M1)(W.u.) value. 


level_energy_unit: KEV
level_spin_parity: 5(+)
level_lifetime_unit: NS
level_comment:
T$from 80.6|g(t) 
$Configuration=((|p g{-9/2})(|n g{-9/2})) from comparison with |p=+ sequence in several neighboring odd-odd Br nuclides. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.2036 fm {I24} (2013An02 evaluation) 
J$spin from optical spectroscopy (1933Ko01) and atomic beam (1936Mi01); parity from L({+3}He,d)=L(d,{+3}He)=3 
$1936Ko05: Zeit Physik 103, 485 (1936): see 1933Ko01 
MOMM1$atomic-beam laser spectroscopy (1993Du08). Others: +1.353028 {I3} (1968Eh01,atomic beam magnetic resonance); +1.35302 {I2} (1968Wh01,optical pumping with radiative detection); +1.357 {I1} (1981Th04,atomic beam laser spectroscopy); +1.3533515 {I8} (NMR, weighted average in 1976Fu06 evaluation recalculated in 1989Ra17 evaluation); 1969DeZY; 1967Gr08; 1967Ba47; 1954Wa37 and 1952Wa08; 1951Ya03; 1939Ku07. 
$1968ZuZZ superseded by 1968Zu01, 1972GuZA superseded by 1972Gu08 
MOME2$optical-double resonance (1973Fe05), recalculated by 1999Ke12. Others: +0.23 {I4} (1981Th04,atomic-beam laser spectroscopy), +0.273 {I2} (molecular beam,recalculated by 1971St12), 1972Gu08 and 1971Ch61, 1970Fi17, 1968Zu01, 1968Bu06, 1967Bo40, 1966Bu17, 1965Sc08, 1962Pe14, 1961Bu02, 1956Se59, 1955Me07, 1954Tr35. 2011StZZ compilation quoted an alternative recalculated value of +0.286 {I1} from 1999Ke12. It does not appear that 1999Ke12 support this higher value. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=L(d,{+3}He)=1; M1+E2 |g to 5/2-. 
T$weighted average of 0.65 ns {I14} from (p,|g), 0.67 ns {I7} from Coulomb excitation, 0.79 ns {I8} from |b{+-} decay (4,480 h), 0.6 ns {I1} in (|a,|a') (1988Ko08) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=L(d,{+3}He)=1; 451|g(|q) from 732 level allows only 1/2. 
T$weighted average of 40 ps {I4} from Coulomb excitation, 39 ps {I7} from (p,|g), and 39 ps {I6} calculated from B(E2)|^ from Coulomb excitation if J=1/2 and I|g=0.58 {I6} from (p,|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$L({+3}He,d)=L(d,{+3}He)=4; comparison of |m with Schmidt values. 
T$|g(t), from |e decay (64.84 d). Other measurement: 985 ns {I20} from (n,n'|g) 
MOMM1,MOME2$optical pumping with radiative detection. Others: |m=+6.046 {I10} (1984Sh24), +6.16 {I5} (1974He22, time-differential PAD and stroboscopic observation of PAD). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_lifetime_unit: PS
level_comment:
J,E$5/2-,7/2- from L(d,{+3}He)=3; 1/2-,3/2- from L(t,|a)=1 and log| {Ift}=8.1 {I4} for weak population from 1/2- parent in {+85}Sr |e decay (67.63 min); Hauser-Feshbach analysis of |s in (n,n'|g) suggests 5/2-. 7/2- is ruled out by |g to 1/2-, but 1/2- is not completely ruled out. Other possibility is that there are two closely spaced levels near this energy, one with J|p=5/2- and the other with 1/2-,3/2- 
T$may be overestimated by about 0.15 ps due to sizeable feeding from levels with comparable half-lives 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=L(t,|a)=(3); gammas to 1/2- and 5/2-. L({+3}He,d)=4 is inconsistent with |g transition to 1/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=L(t,|a)=1; gammas to 1/2- and 5/2-. L(d,{+3}He)=3 is inconsistent with L=1 in ({+3}He,d) and (t,|a) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$(7/2-) from shell model calculations in (n,n'|g), (9/2-) from DCO in ({+7}Li,4n|g); gammas to 5/2-, 7/2- and 9/2+; |g from (13/2-) 


level_energy_unit: KEV
level_spin_parity: (19/2)-
level_lifetime_unit: NS
level_comment:
MOMM1$time differential PAD method (1990Ka26). Other: |<1.6 (1989Wi01) from g factor |<0.17. 
J$|DJ=1, E1 |g to (17/2)+ 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
E,J this level may be a doublet of a level with J|p=(5/2-) and another one with J|p=(7/2)+, but the agreement in branching of 1175|g and 1024|g between this reaction and (p,|g) suggest that both reactions populate the same single level which then cannot have J|p=7/2+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
BE2$weighted average of 0.0037 {I4} (1973Bo24), 0.0033 {I4} (1959Al04), and 0.0034 {I6} (1956Fa29). 1956Fa29 quote B(E2)/(1+|a). 
T$weighted average of 0.70 ns {I7} from 1969Sh12 (delayed coincidences) and 0.6 ns {I1} from 1988Ko08 (generalized centroid-shift method). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$|g(|q) rules out 1/2 and 9/2. B(E2) and T{-1/2} allow 5/2 and 7/2. 
T$weighted average of 2.9 ps {I4} (1973Bo24) and 2.1 ps {I5} (1974Le34). Other: 1.6 ps {I2} (1973ErZS). 
BE2$weighted average of 0.036 {I4} (1973Bo24) and 0.033 {I7} (1968An12). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T$the value measured by 1989Wi22 might be too small since only <3% of the total intensity of the 779|g in the spectrum is shifted by the Doppler effect. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: NS
level_comment:
$ g factor |< 0.17 (1989Wi01) 
T,G$from 1989Wi01, (beam)|g(t) and TDPAD method 
J$(15/2+) in 1982Ze02 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
$RMS charge radius <r{+2}>{+1/2}=4.2025 fm {I23} (2013An02) 
J$spin from atomic beam (1953Be19); parity from L(d,p)=4 from 5/2-. Dominant configuration=|p1f{-5/2}{+-1}~#|n1g{-9/2}{+-1} 
T$weighted average of 18.631 d {I18} (1981Mi10), 18.82 d {I11} (1972Em01), 18.61 d {I4} (1971Ba28), 18.82 d {I11} (1967Gl05), 18.68 d {I7} (1957Wr37), 18.64 d {I4} (1955Ni09), 18.66 d {I3} (1955Em20). Others: 18.7 d 5 (1958Ro62), 19.5 d (1948Za02), 19.5 d (1941He02), 18 d (1937Sn02) 
MOMM1$atomic-beam LASER spectroscopy (1981Th04). Others: -1.6920 {I14} (atomic beam magnetic resonance, 1961Br16), 1.70 {I1} (atomic beam magnetic resonance, 1953Be19) 
MOME2$atomic beam LASER spectroscopy (1981Th04, measured value of +0.193 {i32} reevaluated by 2013StZZ). Other: +0.20 {I3} (Optical double resonance and Optical level crossing methods (1973Ac02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$L(d,|a)=0+2. Probable 1+ member of configuration=|p2p{-3/2}{+-1}~#|n2p{-1/2}{+-1} doublet. 
T$from DSAM in (p,n|g) (1982Fa12). 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$spin from atomic beam (1981Th04); parity from L(d,|a)=3+5 for 556+557 doublet. Probable 6- member of configuration=|p2p{-3/2}{+-1}~#|n1g{-9/2}{+-1} multiplet. 
T$from 1967Yu01. Others: 1.020 min {I17} (1969Sc10), 1.02 min {I3} (1953Sc39), 1.06 min {I2} (1951Fl17) 
MOMM1$atomic beam LASER spectroscopy (1981Th04). 
MOME2$atomic beam LASER spectroscopy (1981Th04, measured value of +0.369 {i95} reevaluated by 2013StZZ) 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$primary |g from 2-,3-. |g to 2-. L(d,|a)=3+5 for the unresolved doublet. Probable 3- member of configuration=|p2p{-3/2}{+-1}~#|n1g{-9/2}{+-1} multiplet. Assignment supported by shell-model calculations (1969Da15). 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
J$L(d,{+3}He)=1 from 9/2+; L(d,|a)=3. Probable mixture of two configurations=|p2p{-3/2}{+-1}~#|n1g{-9/2}{+-1} and |p1f{-5/2}{+-1}~#|n1g{-9/2}{+-1} (1972Ko37,1975Du02). 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_comment:
J$L(d,p)=1 from 5/2-; L(d,t)=1 from 3/2-. Possible 2+ member of configuration=|p2p{-3/2}{+-1}~#|n2p{-1/2}{+-1} doublet. 


level_energy_unit: KEV
level_spin_parity: (5)-
level_comment:
J$L(d,p)=(4+2) from 5/2-; L(d,t)=4 from 3/2-; |g to 6-. From (|g,n) J|>5. Probable configuration=|p2p{-3/2}{+-1}~#|n1g{-9/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
J$L(d,t)=3+1 from 3/2-; |g to 2-; 89.6|g between 1196 level (J|p=3- to 6- from L(d,{+3}He)=1+3 from 9/2+) further limits J|p(1105.6) to 2+,3+ and J|p(1196) to 3-,4- 


level_energy_unit: KEV
level_spin_parity: (0)+
level_comment:
J$strongly excited in (d,t) with L(d,t)=1 from 3/2-. Possible 0+ member of configuration=|p2p{-3/2}{+-1}~#|n2p{-3/2}{+-1} multiplet. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$primary |g from 2-,3-; L(d,t)=1 from 3/2-; L(d,|a)=4. The 1390 group reported in ({+3}He,p) with L=0 may be a different level 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
J$primary |g from 2-,3-; L(d,t)=1 from 3/2-; |g to (3-). Possible 2+ member of configuration=|p2p{-3/2}{+-1}~#|n2p{-3/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=175.6 {I1} eV. 2g|G{-n}=1.17 {I11} meV, 2g|G{+1}{-n}=296 meV, g|G{-n}|G{-|g}/|G=0.5 {I1} meV 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=223.2 {I1} eV. 2g|G{-n}=1.05 {I12} meV, 2g|G{+1}{-n}=185 meV, g|G{-n}|G{-|g}/|G=0.7 {I1} meV. 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=235.0 {I1} eV. 2g|G{-n}=15.6 {I15} meV, 2g|G{+0}{-n}=1.02 {I10} meV g|G{-n}|G{-|g}/|G=5.8 {I1} meV 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=427.1 {I2} eV. 2g|G{-n}=3.40 {I33} meV, 2g|G{+1}{-n}=220 meV, g|G{-n}|G{-|g}/|G=1.7 {I1} meV 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=461.0 {I2} eV. 2g|G{-n}=3.4 {I3} meV, 2g|G{+1}{-n}=202 meV, g|G{-n}|G{-|g}/|G=1.8 {I1} meV 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=474.0 {I2} eV. 2g|G{-n}=48 {I3} meV, 2g|G{+0}{-n}=2.20 {I12} meV, g|G{-n}|G{-|g}/|G=19.6 {I1} meV 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=526.7 {I2} eV. 2g|G{-n}=1.63 {I3} eV, |G{-|g}=239 {I3} meV, 2g|G{+0}{-n}=71.2 {I12} meV, g|G{-n}|G{-|g}/|G=119.0 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=542.7 {I2} eV. 2g|G{-n}=13.0 {I14} meV, 2g|G{+1}{-n}=610 meV, g|G{-n}|G{-|g}/|G=4.2 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=593.2 {I2} eV. 2g|G{-n}=7.3 {I10} meV, 2g|G{+1}{-n}=297 meV, g|G{-n}|G{-|g}/|G=3.6 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=654.9 {I2} eV. 2g|G{-n}=292 {I15} meV, |G{-|g}=258 {I11} meV, 2g|G{+0}{-n}=11.4 {I6} meV, g|G{-n}|G{-|g}/|G=61.9 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=781.2 {I2} eV. 2g|G{-n}=1.6 {I2} meV, 2g|G{+1}{-n}=43 meV, g|G{-n}|G{-|g}/|G=0.8 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=799.1 {I2} eV. 2g|G{-n}=20.4 {I17} meV, 2g|G{+1}{-n}=532 meV, g|G{-n}|G{-|g}/|G=9.0 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=1007.0 {I3} eV. 2g|G{-n}=133 {I13} meV, 2g|G{+0}{-n}=4.2 {I4} meV, g|G{-n}|G{-|g}/|G=42.3 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1010.0 {I3} eV. 2g|G{-n}=11.7 {I21} meV, 2g|G{+1}{-n}=215 meV, g|G{-n}|G{-|g}/|G=5.6 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1030.0 {I3} eV. 2g|G{-n}=2.8 {I2} meV, 2g|G{+1}{-n}=50 meV, g|G{-n}|G{-|g}/|G=1.4 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=1042.0 {I3} eV. 2g|G{-n}=0.89 {I7} eV, |G{-|g}=215 {I4} meV, 2g|G{+0}{-n}=27.6 {I22} meV, g|G{-n}|G{-|g}/|G=97.8{I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1181.0 {I3} eV. 2g|G{-n}=3.04 {I20} meV, 2g|G{+1}{-n}=44 meV, g|G{-n}|G{-|g}/|G=1.5 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=1203.0 {I4} eV. 2g|G{-n}=1.46 {I3} eV, |G{-|g}=220 {I3} meV, 2g|G{+0}{-n}=42.1 {I9} meV, g|G{-n}|G{-|g}/|G=109.3 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1241.0 {I4} eV. 2g|G{-n}=3.0 {I2} meV, 2g|G{+1}{-n}=40 meV, g|G{-n}|G{-|g}/|G=1.5 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1250.0 {I4} eV. 2g|G{-n}=2.8 {I2} meV, 2g|G{+1}{-n}=37 meV, g|G{-n}|G{-|g}/|G=1.4 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=1408.0 {I4} eV. 2g|G{-n}=6.07 {I15} eV, |G{-|g}=212 {I2} meV, 2g|G{+0}{-n}=162 {I4} meV, g|G{-n}|G{-|g}/|G=119.0 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1456.0 {I4} eV. 2g|G{-n}=1.8 {I2} meV, 2g|G{+1}{-n}=19 meV, g|G{-n}|G{-|g}/|G=0.9 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=1506.0 {I4} eV. 2g|G{-n}=132 {I16} meV, 2g|G{+0}{-n}=3.4 {I4} meV, g|G{-n}|G{-|g}/|G=51.2 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=1670.0 {I5} eV. 2g|G{-n}=0.51 {I5} eV, |G{-|g}=232 {I16} meV, 2g|G{+0}{-n}=12.5 {I12} meV, g|G{-n}|G{-|g}/|G=87.3 {I14} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1677.0 {I5} eV. 2g|G{-n}=10.8 {I17} meV, 2g|G{+1}{-n}=93 meV, g|G{-n}|G{-|g}/|G=5.2 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1915.0 {I6} eV. 2g|G{-n}=35 {I4} meV, 2g|G{+1}{-n}=246 meV, g|G{-n}|G{-|g}/|G=11.4 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=1964.0 {I6} eV. 2g|G{-n}=5.3 {I3} meV, 2g|G{+1}{-n}=360 meV, g|G{-n}|G{-|g}/|G=2.6 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=1984.0 {I6} eV. 2g|G{-n}=1.38 {I9} eV, |G{-|g}=184 {I4} meV, 2g|G{+0}{-n}=31 {I2} meV, g|G{-n}|G{-|g}/|G=92.9 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2041.0 {I6} eV. 2g|G{-n}=7.0 {I5} meV, 2g|G{+1}{-n}=45 meV, g|G{-n}|G{-|g}/|G=3.4 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=2082.0 {I6} eV. 2g|G{-n}=0.42 {I4} eV, |G{-|g}=241 {I19} meV, 2g|G{+0}{-n}=9.3 {I8} meV, g|G{-n}|G{-|g}/|G=84.6 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2161.0 {I7} eV. 2g|G{-n}=37 {I4} meV, 2g|G{+1}{-n}=217 meV, g|G{-n}|G{-|g}/|G=12.7 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2213.0 {I7} eV. 2g|G{-n}=37 {I4} meV, 2g|G{+1}{-n}=209 meV, g|G{-n}|G{-|g}/|G=16.5 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2241.0 {I7} eV. 2g|G{-n}=4.3 {I2} meV, 2g|G{+1}{-n}=24 meV, g|G{-n}|G{-|g}/|G=2.1 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2282.0 {I7} eV. 2g|G{-n}=25 {I1} meV, 2g|G{+1}{-n}=135 meV, g|G{-n}|G{-|g}/|G=11.3 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2293.0 {I7} eV. 2g|G{-n}=63 {I6} meV, 2g|G{+1}{-n}=339 meV, g|G{-n}|G{-|g}/|G=31.9 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=2398.0 {I7} eV. 2g|G{-n}=7.71 {I15} eV, |G{-|g}= 231 {I2} meV, 2g|G{+0}{-n}=158 {I3} meV, g|G{-n}|G{-|g}/|G=128.0 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=2503.0 {I7} eV. 2g|G{-n}=0.44 {I3} eV, |G{-|g}=251 {I9} meV, 2g|G{+0}{-n}=8.7 {I6} meV, g|G{-n}|G{-|g}/|G=70.4 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=2583.0 {I8} eV. 2g|G{-n}=1.84 {I10} eV, |G{-|g}=190 {I2} meV, 2g|G{+0}{-n}=36.2 {I20} meV, g|G{-n}|G{-|g}/|G=98.8 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2640.0 {I8} eV. 2g|G{-n}=12.2 {I24} meV, 2g|G{+1}{-n}=53 meV, g|G{-n}|G{-|g}/|G=5.8 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2653.0 {I8} eV. 2g|G{-n}=69 {I3} meV, 2g|G{+1}{-n}=298 meV, g|G{-n}|G{-|g}/|G=34.5 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2663.0 {I8} eV. 2g|G{-n}=6.4 {I4} meV, 2g|G{+1}{-n}=28 meV, g|G{-n}|G{-|g}/|G=3.1 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2776.0 {I8} eV. 2g|G{-n}=0.9 {I8} eV, 2g|G{+1}{-n}=364 meV, g|G{-n}|G{-|g}/|G=35.0 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2916.0 {I8} eV. 2g|G{-n}=81 {I8} meV, 2g|G{+1}{-n}=304 meV, g|G{-n}|G{-|g}/|G=27.9 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=2985.0 {I9} eV. 2g|G{-n}=40 {I9} meV, 2g|G{+1}{-n}=145 meV, g|G{-n}|G{-|g}/|G=17.2 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=2994.0 {I9} eV. 2g|G{-n}=3.31 {I20} eV, |G{-|g}=232 {I2} meV, 2g|G{+0}{-n}=61 {I4} meV, g|G{-n}|G{-|g}/|G=123.2 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E{-n}(lab)=3008.0 {I9} eV. 2g|G{-n}=2.18 {I10} eV, |G{-|g}=151 {I3} meV, 2g|G{+0}{-n}=39.8 {I18} meV, g|G{-n}|G{-|g}/|G=81.4 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3020.0 {I9} eV. 2g|G{-n}=72 {I5} meV, 2g|G{+1}{-n}=260 meV, g|G{-n}|G{-|g}/|G=28.5 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3161.0 {I9} eV. 2g|G{-n}=11.9 {I22} meV, 2g|G{+1}{-n}=40 meV, g|G{-n}|G{-|g}/|G=5.7 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=3210.0 {I10} eV. 2g|G{-n}=2.38 {I23} eV, |G{-|g}=226 {I4} meV, 2g|G{+0}{-n}=42 {I4} meV, g|G{-n}|G{-|g}/|G=93.3 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3246.0 {I10} eV. 2g|G{-n}=29 {I3} meV, 2g|G{+1}{-n}=93 meV, g|G{-n}|G{-|g}/|G=13.1 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=3335.0 {I10} eV. 2g|G{-n}=0.67 {I7} eV, |G{-|g}=277 {I17} meV, 2g|G{+0}{-n}=11.6 {I12} meV, g|G{-n}|G{-|g}/|G=130.2 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3426.0 {I11} eV. 2g|G{-n}=145 {I12} meV, 2g|G{+1}{-n}=428 meV, g|G{-n}|G{-|g}/|G=48.2 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3549.0 {I11} eV. 2g|G{-n}=95 {I12} meV, 2g|G{+1}{-n}=265 meV, g|G{-n}|G{-|g}/|G=46.2 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3577.0 {I11} eV. 2g|G{-n}=120 {I12} meV, 2g|G{+1}{-n}=332 meV, g|G{-n}|G{-|g}/|G=42.1 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3633.0 {I12} eV. 2g|G{-n}=84 {I12} meV, 2g|G{+1}{-n}=227 meV, g|G{-n}|G{-|g}/|G=31.0 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3675.0 {I12} eV. 2g|G{-n}=34 {I2} meV, 2g|G{+1}{-n}=90 meV, g|G{-n}|G{-|g}/|G=15.1 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3704.0 {I12} eV. 2g|G{-n}=8.0 {I11} meV, 2g|G{+1}{-n}=21 meV, g|G{-n}|G{-|g}/|G=3.9 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3712.0 {I12} eV. 2g|G{-n}=8.3 {I10} meV, 2g|G{+1}{-n}=22 meV, g|G{-n}|G{-|g}/|G=4.0 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=3854.0 {I12} eV. 2g|G{-n}=82 {I4} meV, 2g|G{+1}{-n}=203 meV, g|G{-n}|G{-|g}/|G=31.3 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4015.0 {I13} eV. 2g|G{-n}=74 {I4} meV, 2g|G{+1}{-n}=172 meV, g|G{-n}|G{-|g}/|G=28.8 {I18} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=4021.0 {I13} eV. 2g|G{-n}=4.2 {I4} eV, |G{-|g}=198 {I4} meV, 2g|G{+0}{-n}=66 {I6} meV, g|G{-n}|G{-|g}/|G=79.2 {I17} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4030.0 {I13} eV. 2g|G{-n}=46 {I3} meV, 2g|G{+1}{-n}=106 meV, g|G{-n}|G{-|g}/|G=19.6 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4124.0 {I14} eV. 2g|G{-n}=23.7 {I12} meV, 2g|G{+1}{-n}=53 meV, g|G{-n}|G{-|g}/|G=10.9 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=4211.0 {I14} eV. 2g|G{-n}=6.7 {I5} eV, |G{-|g}=246 {I10} meV, 2g|G{+0}{-n}=103 {I8} meV, g|G{-n}|G{-|g}/|G=99.5 {I15} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4267.0 {I14} eV. 2g|G{-n}=69 {I4} meV, 2g|G{+1}{-n}=147 meV, g|G{-n}|G{-|g}/|G=27.5 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4295.0 {I14} eV. 2g|G{-n}=3.7 {I6} meV, 2g|G{+1}{-n}=7.8 meV, g|G{-n}|G{-|g}/|G=1.8 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4323.0 {I14} eV. 2g|G{-n}=95 {I6} meV, 2g|G{+1}{-n}=198 meV, g|G{-n}|G{-|g}/|G=35.0 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4367.0 {I14} eV. 2g|G{-n}=117 {I10} meV, 2g|G{+1}{-n}=2.4 meV, g|G{-n}|G{-|g}/|G=40.7 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4347.0 {I14} eV. 2g|G{-n}=87 {I5} meV, 2g|G{+1}{-n}=178 meV, g|G{-n}|G{-|g}/|G=32.7 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4496.0 {I15} eV. 2g|G{-n}=67 {I13} meV, 2g|G{+1}{-n}=132 meV, g|G{-n}|G{-|g}/|G=36.5 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4508.0 {I15} eV. 2g|G{-n}=47.0 {I24} meV, 2g|G{+1}{-n}=92 meV, g|G{-n}|G{-|g}/|G=20.1 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4562.0 {I15} eV. 2g|G{-n}=23 {I3} meV, 2g|G{+1}{-n}=44 meV, g|G{-n}|G{-|g}/|G=10.5 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4671.0 {I15} eV. 2g|G{-n}=34.5 {I15} meV, 2g|G{+1}{-n}=64 meV, g|G{-n}|G{-|g}/|G=15.2 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4694.0 {I16} eV. 2g|G{-n}=144 {I14} meV, 2g|G{+1}{-n}=266 meV, g|G{-n}|G{-|g}/|G=48.3 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4723.0 {I16} eV. 2g|G{-n}=13 {I3} meV, 2g|G{+1}{-n}=23 meV, g|G{-n}|G{-|g}/|G=6.1 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4731.0 {I16} eV. 2g|G{-n}=47 {I3} meV, 2g|G{+1}{-n}=86 meV, g|G{-n}|G{-|g}/|G=19.8 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4745.0 {I16} eV. 2g|G{-n}=23.5 {I11} meV, 2g|G{+1}{-n}=43 meV, g|G{-n}|G{-|g}/|G=10.8 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4836.0 {I17} eV. 2g|G{-n}=112 {I11} meV, 2g|G{+1}{-n}=119.7 meV, g|G{-n}|G{-|g}/|G=42.8 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=4877.0 {I17} eV. 2g|G{-n}=10.1 {I6} eV, |G{-|g}=267 {I13} meV, 2g|G{+0}{-n}=145 {I8} meV, g|G{-n}|G{-|g}/|G=151.2 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4885.0 {I17} eV. 2g|G{-n}=66 {I3} meV, 2g|G{+1}{-n}=115 meV, g|G{-n}|G{-|g}/|G=26.3 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=4903.0 {I17} eV. 2g|G{-n}=150 {I20} meV, 2g|G{+1}{-n}=259 meV, g|G{-n}|G{-|g}/|G=47.5 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=5001.0 {I17} eV. 2g|G{-n}=0.85 {I10} eV, |G{-|g}=0.25 {I12} meV, 2g|G{+0}{-n}=12.0 {I14} meV, g|G{-n}|G{-|g}/|G=90.1 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5084.0 {I17} eV. 2g|G{-n}=62 {I3} meV, 2g|G{+1}{-n}=102 meV, g|G{-n}|G{-|g}/|G=25.2 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5106.0 {I17} eV. 2g|G{-n}=8 {I8} meV, 2g|G{+1}{-n}=13 meV, g|G{-n}|G{-|g}/|G=3.9 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5131.0 {I17} eV. 2g|G{-n}=143 {I10} meV, 2g|G{+1}{-n}=231 meV, g|G{-n}|G{-|g}/|G=45.6 {I13} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=5149.0 {I18} eV. 2g|G{-n}=2.38 {I10} eV, |G{-|g}=222 {I11} meV, 2g|G{+0}{-n}=33.2 {I14} meV, g|G{-n}|G{-|g}/|G=117 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=5172.0 {I18} eV. 2g|G{-n}=0.99 {I10} eV, |G{-|g}=241 {I12} meV, 2g|G{+0}{-n}=13.8 {I14} meV, g|G{-n}|G{-|g}/|G=83.4 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5287.0 {I18} eV. 2g|G{-n}=54 {I4} meV, 2g|G{+1}{-n}=83 meV, g|G{-n}|G{-|g}/|G=22.5 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: [1]+
level_comment:
$E{-n}(lab)=5319.0 {I18} eV. 2g|G{-n}=0.22 {I3} eV, 2g|G{+1}{-n}=335 meV, g|G{-n}|G{-|g}/|G=31.7 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5364.0 {I18} eV. 2g|G{-n}=75 {I4} meV, 2g|G{+1}{-n}=114 meV, g|G{-n}|G{-|g}/|G=29.3 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5387.0 {I18} eV. 2g|G{-n}=51 {I2} meV, 2g|G{+1}{-n}=77 meV, g|G{-n}|G{-|g}/|G=21.1 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5407.0 {I18} eV. 2g|G{-n}=32 {I2} meV, 2g|G{+1}{-n}=48 meV, g|G{-n}|G{-|g}/|G=14.2 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5497.0 {I19} eV. 2g|G{-n}=56 {I3} meV, 2g|G{+1}{-n}=82 meV, g|G{-n}|G{-|g}/|G=23 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5509.0 {I19} eV. 2g|G{-n}=8.1 {I14} meV, 2g|G{+1}{-n}=12 meV, g|G{-n}|G{-|g}/|G=3.9 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5546.0 {I19} eV. 2g|G{-n}=128 {I15} meV, 2g|G{+1}{-n}=184 meV, g|G{-n}|G{-|g}/|G=38.0 {I13} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=5599.0 {I20} eV. 2g|G{-n}=3.25 {I20} eV, |G{-|g}=190 {I10} meV, 2g|G{+0}{-n}=43 {I3} meV, g|G{-n}|G{-|g}/|G=104 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5709.0 {I20} eV. 2g|G{-n}=166 {I15} meV, 2g|G{+1}{-n}=229 meV, g|G{-n}|G{-|g}/|G=65.8 {I18} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=5734.0 {I20} eV. 2g|G{-n}=0.94 {I9} eV, |G{-|g}=383 {I20} meV, 2g|G{+0}{-n}=12.4 {I12} meV, g|G{-n}|G{-|g}/|G=151.6 {I25} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5822.0 {I20} eV. 2g|G{-n}=55 {I5} meV, 2g|G{+1}{-n}=74 meV, g|G{-n}|G{-|g}/|G=22.9 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=5869.0 {I21} eV. 2g|G{-n}=5.1 {I5} eV, |G{-|g}=0.28 {I4} eV, 2g|G{+0}{-n}=67 {I6} meV, g|G{-n}|G{-|g}/|G=110.0 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5923.0 {I21} eV. 2g|G{-n}=0.33 {I9} eV, 2g|G{+1}{-n}=430 meV, g|G{-n}|G{-|g}/|G=73.5 {I18} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=5949.0 {I21} eV. 2g|G{-n}=41 {I6} meV, 2g|G{+1}{-n}=53 meV, g|G{-n}|G{-|g}/|G=17.9 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6123.0 {I21} eV. 2g|G{-n}=44 {I6} meV, 2g|G{+1}{-n}=55 meV, g|G{-n}|G{-|g}/|G=18.8 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6176.0 {I22} eV. 2g|G{-n}=136 {I16} meV, 2g|G{+1}{-n}=166 meV, g|G{-n}|G{-|g}/|G=50.3 {I17} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6200.0 {I22} eV. 2g|G{-n}=23 {I3} meV, 2g|G{+1}{-n}=28 meV, g|G{-n}|G{-|g}/|G=10.7 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=6277.0 {I23} eV. 2g|G{-n}=1.09 {I11} eV, |G{-|g}=186 {I9} meV, 2g|G{+0}{-n}=13.8 {I14} meV, g|G{-n}|G{-|g}/|G=67.8 {I17} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6314.0 {I23} eV. 2g|G{-n}=112 {I20} meV, 2g|G{+1}{-n}=133 meV, g|G{-n}|G{-|g}/|G=39.4 {I17} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6326.0 {I23} eV. 2g|G{-n}=47 {I10} meV, 2g|G{+1}{-n}=56 meV, g|G{-n}|G{-|g}/|G=20.0 {I15} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6426.0 {I23} eV. 2g|G{-n}=53 {I10} meV, 2g|G{+1}{-n}=61 meV, g|G{-n}|G{-|g}/|G=22.1 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=6599.0 {I23} eV. 2g|G{-n}=1.58 {I16} eV, |G{-|g}=259 {I13} meV, 2g|G{+0}{-n}=19.5 {I20} meV, g|G{-n}|G{-|g}/|G=127.2 {I24} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6623.0 {I24} eV. 2g|G{-n}=17 {I2} meV, 2g|G{+1}{-n}=188 meV, g|G{-n}|G{-|g}/|G=8.0 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=6694.0 {I25} eV. 2g|G{-n}=1.15 {I16} eV, |G{-|g}=213 {I11} meV, 2g|G{+0}{-n}=14.1 {I20} meV, g|G{-n}|G{-|g}/|G=76.8 {I19} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6840.0 {I25} eV. 2g|G{-n}=182 {I17} meV, 2g|G{+1}{-n}=191 meV, g|G{-n}|G{-|g}/|G=65.4 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6863.0 {I25} eV. 2g|G{-n}=132 {I20} meV, 2g|G{+1}{-n}=138 meV, g|G{-n}|G{-|g}/|G=44.2 {I16} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6924.0 {I25} eV. 2g|G{-n}=29 {I2} meV, 2g|G{+1}{-n}=30 meV, g|G{-n}|G{-|g}/|G=13.2 {I10} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=6954.0 {I25} eV. 2g|G{-n}=85 {I6} meV, 2g|G{+1}{-n}=87 meV, g|G{-n}|G{-|g}/|G=32.3 {I14} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=7052.0 {I26} eV. 2g|G{-n}=2.18 {I25} eV, |G{-|g}=234 {I12} meV, 2g|G{+0}{-n}=26 {I3} meV, g|G{-n}|G{-|g}/|G=122 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=7167.0 {I27} eV. 2g|G{-n}=6.8 {I5} eV, |G{-|g}=343 {I17} meV, 2g|G{+0}{-n}=80 {I6} meV, g|G{-n}|G{-|g}/|G=189.3 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7215.0 {I27} eV. 2g|G{-n}=93 {I6} meV, 2g|G{+1}{-n}=90 meV, g|G{-n}|G{-|g}/|G=34.5 {I15} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7277.0 {I27} eV. 2g|G{-n}=0.36 {I11} eV, 2g|G{+1}{-n}=345 meV, g|G{-n}|G{-|g}/|G=76.6 {I22} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7335.0 {I27} eV. 2g|G{-n}=16 {I3} meV, 2g|G{+1}{-n}=15 meV, g|G{-n}|G{-|g}/|G=7.6 {I16} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=7430.0 {I28} eV. 2g|G{-n}=1.72 {I17} eV, |G{-|g}=243 {I12} meV, 2g|G{+0}{-n}=20 {I2} meV, g|G{-n}|G{-|g}/|G=122 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7537.0 {I29} eV. 2g|G{-n}=44 {I4} meV, 2g|G{+1}{-n}=40 meV, g|G{-n}|G{-|g}/|G=18.9 {I19} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7547.0 {I29} eV. 2g|G{-n}=75 {I5} meV, 2g|G{+1}{-n}=68 meV, g|G{-n}|G{-|g}/|G=29 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
$E{-n}(lab)=7556.0 {I29} eV. 2g|G{-n}=0.52 {I7} eV, |G{-|g}=247 {I13} meV, 2g|G{+1}{-n}=472 meV, g|G{-n}|G{-|g}/|G=50 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7586.0 {I29} eV. 2g|G{-n}=104 {I8} meV, 2g|G{+1}{-n}=94 meV, g|G{-n}|G{-|g}/|G=36.9 {I18} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7652.0 {I30} eV. 2g|G{-n}=0.35 {I9} eV, 2g|G{+1}{-n}=312 meV, g|G{-n}|G{-|g}/|G=94 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7668.0 {I30} eV. 2g|G{-n}=0.17 {I5} eV, 2g|G{+1}{-n}=154 meV, g|G{-n}|G{-|g}/|G=45.3 {I25} meV. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
$E{-n}(lab)=7684.0 {I30} eV. 2g|G{-n}=0.53 {I7} eV, |G{-|g}=289 {I14} meV, 2g|G{+0}{-n}=6.1 {I8} meV, g|G{-n}|G{-|g}/|G=83 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7719.0 {I30} eV. 2g|G{-n}=28 {I3} meV, 2g|G{+1}{-n}=24 meV, g|G{-n}|G{-|g}/|G=12.5 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
$E{-n}(lab)=7784.0 {I30} eV. 2g|G{-n}=0.35 {I7} eV, |G{-|g}=225 {I25} meV, 2g|G{+1}{-n}=4.0 {I8} meV, g|G{-n}|G{-|g}/|G=74.9 {I25} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7825.0 {I30} eV. 2g|G{-n}=3.7 {I18} meV, 2g|G{+1}{-n}=3.1 meV, g|G{-n}|G{-|g}/|G=1.8 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
$E{-n}(lab)=7886.0 {I30} eV. 2g|G{-n}=0.78 {I9} eV, |G{-|g}=0.26 {I3} eV, 2g|G{+0}{-n}=8.8 {I10} meV, g|G{-n}|G{-|g}/|G=108.9 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=7920.0 {I31} eV. 2g|G{-n}=0.27 {I7} eV, 2g|G{+1}{-n}=226 meV, g|G{-n}|G{-|g}/|G=28.8 {I16} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=7964.0 {I31} eV. 2g|G{-n}=3.0 {I3} eV, |G{-|g}=0.27 {I3} eV, 2g|G{+0}{-n}=34 {I3} meV, g|G{-n}|G{-|g}/|G=105 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8163.0 {I32} eV. 2g|G{-n}=56 {I3} meV, 2g|G{+1}{-n}=45 meV, g|G{-n}|G{-|g}/|G=23.3 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=8181.0 {I32} eV. 2g|G{-n}=0.72 {I9} eV, 2g|G{+0}{-n}=8.0 {I10} meV, g|G{-n}|G{-|g}/|G=149 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8262.0 {I32} eV. 2g|G{-n}=56 {I3} meV, 2g|G{+1}{-n}=44 meV, g|G{-n}|G{-|g}/|G=23.3 {I16} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=8327.0 {I33} eV. 2g|G{-n}=0.55 {I9} eV, 2g|G{+0}{-n}=6 {I1} meV, g|G{-n}|G{-|g}/|G=97 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=8390.0 {I33} eV. 2g|G{-n}=3.3 {I4} eV, |G{-|g}=304 {I15} meV, 2g|G{+0}{-n}=36 {I4} meV, g|G{-n}|G{-|g}/|G=160 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8471.0 {I34} eV. 2g|G{-n}=0.37 {I6} eV, 2g|G{+1}{-n}=283 meV, g|G{-n}|G{-|g}/|G=90 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8521.0 {I34} eV. 2g|G{-n}=0.37 {I6} eV, 2g|G{+1}{-n}=281 meV, g|G{-n}|G{-|g}/|G=80 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8579.0 {I34} eV. 2g|G{-n}=0.26 {I6} eV, 2g|G{+1}{-n}=195 meV, g|G{-n}|G{-|g}/|G=66 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8639.0 {I35} eV. 2g|G{-n}=162 {I40} meV, 2g|G{+1}{-n}=121 meV, g|G{-n}|G{-|g}/|G=50.4 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8669.0 {I35} eV. 2g|G{-n}=7.2 {I22} meV, 2g|G{+1}{-n}=5.3 meV, g|G{-n}|G{-|g}/|G=3.5 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8722.0 {I35} eV. 2g|G{-n}=270 {I6} meV, 2g|G{+1}{-n}=198 meV, g|G{-n}|G{-|g}/|G=66.7 {I25} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8761.0 {I35} eV. 2g|G{-n}=13.9 {I30} meV, 2g|G{+1}{-n}=10 meV, g|G{-n}|G{-|g}/|G=6.6 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8825.0 {I35} eV. 2g|G{-n}=52 {I4} meV, 2g|G{+1}{-n}=38 meV, g|G{-n}|G{-|g}/|G=21.7 {I17} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8912.0 {I36} eV. 2g|G{-n}=0.28 {I6} eV, 2g|G{+1}{-n}=201 meV, g|G{-n}|G{-|g}/|G=56.3 {I25} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=8989.0 {I36} eV. 2g|G{-n}=0.29 {I8} eV, 2g|G{+1}{-n}=200 meV, g|G{-n}|G{-|g}/|G=114.0 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9077.0 {I37} eV. 2g|G{-n}=154 {I17} meV, 2g|G{+1}{-n}=110 meV, g|G{-n}|G{-|g}/|G=48.9 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=9142.0 {I37} eV. 2g|G{-n}=19.1 {I13} eV, |G{-|g}=251 {I25} meV, 2g|G{+0}{-n}=200 {I14} meV, g|G{-n}|G{-|g}/|G=144.1 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9182.0 {I37} eV. 2g|G{-n}=150 {I16} meV, 2g|G{+1}{-n}=105 meV, g|G{-n}|G{-|g}/|G=48 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=9303.0 {I38} eV. 2g|G{-n}=1.60 {I20} eV, 2g|G{+0}{-n}=16.6 {I21} meV, g|G{-n}|G{-|g}/|G=168 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=9352.0 {I39} eV. Possible doublet. 2g|G{-n}=6.4 {I5} eV, 2g|G{+0}{-n}=66 {I5} meV, g|G{-n}|G{-|g}/|G=277 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9476.0 {I39} eV. 2g|G{-n}=138 {I14} meV, 2g|G{+1}{-n}=92 meV, g|G{-n}|G{-|g}/|G=45.6 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: [2]+
level_comment:
$E{-n}(lab)=9502.0 {I39} eV. 2g|G{-n}=0.43 {I10} eV, |G{-|g}=214 {I31} meV, 2g|G{+1}{-n}=277 meV, g|G{-n}|G{-|g}/|G=63 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9559.0 {I39} eV. 2g|G{-n}=140 {I14} meV, 2g|G{+1}{-n}=90 meV, g|G{-n}|G{-|g}/|G=45.9 {I24} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9697.0 {I40} eV. 2g|G{-n}=8.0 {I24} meV, 2g|G{+1}{-n}=5 meV, g|G{-n}|G{-|g}/|G=3.9 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9746.0 {I41} eV. 2g|G{-n}=150 {I16} meV, 2g|G{+1}{-n}=94 meV, g|G{-n}|G{-|g}/|G=48 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=9775.0 {I41} eV. 2g|G{-n}=5.9 {I6} eV, |G{-|g}=256 {I26} meV, 2g|G{+0}{-n}=60 {I6} meV, g|G{-n}|G{-|g}/|G=142.1 {I2} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9898.0 {I41} eV. 2g|G{-n}=174 {I22} meV, 2g|G{+1}{-n}=106 meV, g|G{-n}|G{-|g}/|G=52.7 {I26} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=9950.0 {I41} eV. 2g|G{-n}=41.1 {I32} meV, 2g|G{+1}{-n}=25 meV, g|G{-n}|G{-|g}/|G=17.8 {I16} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10010.0 {I42} eV. 2g|G{-n}=9.3 {I22} meV, 2g|G{+1}{-n}=6 meV, g|G{-n}|G{-|g}/|G=4.5 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10090.0 {I42} eV. 2g|G{-n}=130 {I11} meV, 2g|G{+1}{-n}=77 meV, g|G{-n}|G{-|g}/|G=43.0 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=10130.0 {I43} eV. Possible doublet. 2g|G{-n}=11.7 {I12} eV, 2g|G{+0}{-n}=116.0 {I12} meV, g|G{-n}|G{-|g}/|G=226 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10230.0 {I43} eV. 2g|G{-n}=19.8 {I26} meV, 2g|G{+1}{-n}=12 meV, g|G{-n}|G{-|g}/|G=9.2 {I13} meV. 


level_energy_unit: KEV
level_spin_parity: [2]+
level_comment:
$E{-n}(lab)=10280.0 {I44} eV. 2g|G{-n}=0.61 {I20} eV, |G{-|g}=0.27 {I3} eV, 2g|G{+1}{-n}=350 meV, g|G{-n}|G{-|g}/|G=82 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10450.0 {I44} eV. 2g|G{-n}=0.33 {I10} meV, 2g|G{+1}{-n}=185 meV, g|G{-n}|G{-|g}/|G=90 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10650.0 {I45} eV. 2g|G{-n}=183 {I6} meV, 2g|G{+1}{-n}=100 meV, g|G{-n}|G{-|g}/|G=54.4 {I25} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=10820.0 {I47} eV. 2g|G{-n}=3.1 {I4} eV, |G{-|g}=216 {I15} meV, 2g|G{+0}{-n}=30 {I4} meV, g|G{-n}|G{-|g}/|G=85 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=10900.0 {I47} eV. 2g|G{-n}=3.6 {I4} eV, |G{-|g}=243 {I24} meV, 2g|G{+0}{-n}=35 {I4} meV, g|G{-n}|G{-|g}/|G=96 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10920.0 {I47} eV. 2g|G{-n}=0.20 {I3} eV, 2g|G{+1}{-n}=106 meV, g|G{-n}|G{-|g}/|G=58 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=10950.0 {I48} eV. 2g|G{-n}=79 {I5} meV, 2g|G{+1}{-n}=41 meV, g|G{-n}|G{-|g}/|G=31 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=10960.0 {I48} eV. 2g|G{-n}=9.2 {I8} eV, 2g|G{+0}{-n}=88 {I8} meV, g|G{-n}|G{-|g}/|G=47.5 {I1} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11130.0 {I48} eV. 2g|G{-n}=0.19 {I3} meV, 2g|G{+1}{-n}=98 meV, g|G{-n}|G{-|g}/|G=55 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11120 {I5} eV. 2g|G{-n}=24.4 {I24} meV, 2g|G{+1}{-n}=13 meV, g|G{-n}|G{-|g}/|G=11.2 {I14} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11160 {I5} eV. 2g|G{-n}=16.6 {I26} meV, 2g|G{+1}{-n}=8.4 meV, g|G{-n}|G{-|g}/|G=7.8 {I13} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11220 {I5} eV. 2g|G{-n}=107 {I9} meV, 2g|G{+1}{-n}=54 meV, g|G{-n}|G{-|g}/|G=38.0 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=11300 {I5} eV. 2g|G{-n}=1.11 {I21} eV, |G{-|g}=0.34 {I4} eV, 2g|G{+0}{-n}=1044 meV, g|G{-n}|G{-|g}/|G=146 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11490 {I5} eV. 2g|G{-n}=0.20 {I3} eV, 2g|G{+1}{-n}=99 meV, g|G{-n}|G{-|g}/|G=58 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=11630 {I5} eV. 2g|G{-n}=3.2 {I4} eV, |G{-|g}=221 {I15} meV, 2g|G{+0}{-n}=30 {I4} meV, g|G{-n}|G{-|g}/|G=87 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [3]+
level_comment:
$E{-n}(lab)=11660 {I5} eV. 2g|G{-n}=0.50 {I11} eV, |G{-|g}=207 {I25} meV, 2g|G{+1}{-n}=238 meV, g|G{-n}|G{-|g}/|G=82 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=11700 {I5} eV. 2g|G{-n}=1.28 {I22} eV, |G{-|g}=0.30 {I3} eV, 2g|G{+0}{-n}=11.8 {I20} meV, g|G{-n}|G{-|g}/|G=138 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11770 {I5} eV. 2g|G{-n}=126 {I12} meV, 2g|G{+1}{-n}=59 meV, g|G{-n}|G{-|g}/|G=42.8 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11820 {I5} eV. 2g|G{-n}=700 {I22} meV, 2g|G{+1}{-n}=328 meV, g|G{-n}|G{-|g}/|G=80 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11860 {I5} eV. 2g|G{-n}=0.39 {I11} eV, 2g|G{+1}{-n}=181 meV, g|G{-n}|G{-|g}/|G=69 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11900 {I5} eV. 2g|G{-n}=47 {I6} meV, 2g|G{+1}{-n}=22 meV, g|G{-n}|G{-|g}/|G=20 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11920 {I5} eV. 2g|G{-n}=190 {I26} meV, 2g|G{+1}{-n}=88 meV, g|G{-n}|G{-|g}/|G=55 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=11970 {I5} eV. 2g|G{-n}=0.28 {I11} eV, 2g|G{+1}{-n}=130 meV, g|G{-n}|G{-|g}/|G=95 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=12130 {I6} eV. 2g|G{-n}=5.5 {I7} eV, |G{-|g}=0.29 {I3} eV, 2g|G{+0}{-n}=50 {I6} meV, g|G{-n}|G{-|g}/|G=160 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=12260 {I6} eV. 2g|G{-n}=1.11 {I22} eV, 2g|G{+0}{-n}=10 {I2} meV, g|G{-n}|G{-|g}/|G=148 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=12360 {I6} eV. 2g|G{-n}=1.89 {I22} eV, 2g|G{+0}{-n}=17 {I2} meV, g|G{-n}|G{-|g}/|G=110 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=12470 {I6} eV. 2g|G{-n}=10.1 {I9} eV, 2g|G{+0}{-n}=80 meV, g|G{-n}|G{-|g}/|G=222.9 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=12680 {I6} eV. 2g|G{-n}=0.68 {I23} eV, 2g|G{+1}{-n}=290 meV, g|G{-n}|G{-|g}/|G=150 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=12760 {I6} eV. 2g|G{-n}=53 {I7} meV, 2g|G{+1}{-n}=22 meV, g|G{-n}|G{-|g}/|G=22 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=12790 {I6} eV. 2g|G{-n}=16.5 {I23} eV, 2g|G{+0}{-n}=146 {I20} meV, g|G{-n}|G{-|g}/|G=81 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=12950 {I6} eV. 2g|G{-n}=3.4 {I5} eV, |G{-|g}=244 {I20} meV, 2g|G{+0}{-n}=30 {I4} meV, g|G{-n}|G{-|g}/|G=131.2 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=13360 {I6} eV. Possible doublet. 2g|G{-n}=2.5 {I4} eV, 2g|G{+0}{-n}=22 {I3} meV, g|G{-n}|G{-|g}/|G=213 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=13400 {I6} eV. 2g|G{-n}=2.1 {I4} eV, |G{-|g}=244 {I25} meV, 2g|G{+0}{-n}=18 {I3} meV, g|G{-n}|G{-|g}/|G=125.0 {I8} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=13540 {I6} eV. Possible doublet. 2g|G{-n}=10.9 {I12} eV, 2g|G{+0}{-n}=94 {I10} meV, g|G{-n}|G{-|g}/|G=213.6 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=13650 {I6} eV. 2g|G{-n}=144 {I15} meV, 2g|G{+1}{-n}=54 meV, g|G{-n}|G{-|g}/|G=47 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=13740 {I6} eV. 2g|G{-n}=166 {I20} meV, 2g|G{+1}{-n}=62 meV, g|G{-n}|G{-|g}/|G=51 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=13880 {I6} eV. 2g|G{-n}=21 {I5} meV, 2g|G{+1}{-n}=78 meV, g|G{-n}|G{-|g}/|G=9.8 {I24} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=13990 {I6} eV. 2g|G{-n}=0.40 {I16} eV, 2g|G{+1}{-n}=150 meV, g|G{-n}|G{-|g}/|G=59 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: [3]+
level_comment:
$E{-n}(lab)=14150 {I7} eV. 2g|G{-n}=0.67 {I24} eV, |G{-|g}=261 {I25} meV, 2g|G{+1}{-n}=240 meV, g|G{-n}|G{-|g}/|G=105 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=14210 {I7} eV. 2g|G{-n}=0.46 {I19} eV, 2g|G{+1}{-n}=160 meV, g|G{-n}|G{-|g}/|G=55 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=14300 {I7} eV. 2g|G{-n}=3.6 {I4} eV, |G{-|g}=262 {I26} meV, 2g|G{+0}{-n}=30 {I3} meV, g|G{-n}|G{-|g}/|G=103 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=14330 {I7} eV. 2g|G{-n}=121 {I10} meV, 2g|G{+1}{-n}=43 meV, g|G{-n}|G{-|g}/|G=42 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=14540 {I7} eV. 2g|G{-n}=4.8 {I5} meV, |G{-|g}=282 {I20} meV, 2g|G{+0}{-n}=40 {I4} meV, g|G{-n}|G{-|g}/|G=154 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=14700 {I7} eV. 2g|G{-n}=5.1 {I7} eV, |G{-|g}=226 {I22} meV, 2g|G{+0}{-n}=42 {I6} meV, g|G{-n}|G{-|g}/|G=91 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=14730 {I7} eV. 2g|G{-n}=58 {I4} meV, 2g|G{+1}{-n}=20 meV, g|G{-n}|G{-|g}/|G=24 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=14770 {I7} eV. 2g|G{-n}=0.34 {I10} eV, 2g|G{+1}{-n}=110 meV, g|G{-n}|G{-|g}/|G=75 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=14860 {I7} eV. 2g|G{-n}=78 {I6} meV, 2g|G{+1}{-n}=26 meV, g|G{-n}|G{-|g}/|G=30 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=14950 {I7} eV. 2g|G{-n}=0.31 {I8} eV, 2g|G{+1}{-n}=102 meV, g|G{-n}|G{-|g}/|G=72 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=15030 {I7} eV. 2g|G{-n}=1.5 {I4} eV, |G{-|g}=0.29 {I3} eV, 2g|G{+0}{-n}=12 {I3} meV, g|G{-n}|G{-|g}/|G=102 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=15090 {I7} eV. 2g|G{-n}=103 {I9} meV, 2g|G{+1}{-n}=34 meV, g|G{-n}|G{-|g}/|G=37 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=15140 {I7} eV. 2g|G{-n}=1.23 {I25} eV, |G{-|g}=0.31 {I3} eV, 2g|G{+0}{-n}=10 {I2} meV, g|G{-n}|G{-|g}/|G=106 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=15420 {I8} eV. 2g|G{-n}=60 {I7} meV, 2g|G{+1}{-n}=19 meV, g|G{-n}|G{-|g}/|G=24 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$E{-n}(lab)=15480 {I8} eV. Possible doublet. 2g|G{-n}=1.24 {I25} eV, 2g|G{+0}{-n}=10 {I2} meV, g|G{-n}|G{-|g}/|G=263 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=15620 {I8} eV. 2g|G{-n}=87 {I7} meV, 2g|G{+1}{-n}=27 meV, g|G{-n}|G{-|g}/|G=33 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=15680 {I8} eV. 2g|G{-n}=150 {I16} meV, 2g|G{+1}{-n}=46 meV, g|G{-n}|G{-|g}/|G=48 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=15830 {I8} eV. 2g|G{-n}=55 {I6} meV, 2g|G{+1}{-n}=17 meV, g|G{-n}|G{-|g}/|G=23 {I3} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=15910 {I8} eV. 2g|G{-n}=1.51 {I25} eV, 2g|G{+0}{-n}=12 {I2} meV, g|G{-n}|G{-|g}/|G=249 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=16040 {I8} eV. 2g|G{-n}=113 {I9} meV, 2g|G{+1}{-n}=34 meV, g|G{-n}|G{-|g}/|G=40 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=16200 {I8} eV. Possible doublet. 2g|G{-n}=1.66 {I25} eV, 2g|G{+0}{-n}=13 {I2} meV, g|G{-n}|G{-|g}/|G=243 {I11} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=16320 {I8} eV. 2g|G{-n}=0.22 {I4} eV, 2g|G{+1}{-n}=64 meV, g|G{-n}|G{-|g}/|G=61 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=16400 {I8} eV. 2g|G{-n}=110 {I9} meV, 2g|G{+1}{-n}=32 meV, g|G{-n}|G{-|g}/|G=39 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=16470 {I8} eV. 2g|G{-n}=3.90 {I77} eV, 2g|G{+0}{-n}=30 {I6} meV, g|G{-n}|G{-|g}/|G=151 {I7} meV. 


level_energy_unit: KEV
level_spin_parity: [2]-
level_comment:
$E{-n}(lab)=16640 {I9} eV. 2g|G{-n}=18.10 {I26} eV, |G{-|g}=207 {I21} meV, 2g|G{+0}{-n}=140 {I2} meV, g|G{-n}|G{-|g}/|G=85 {I6} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=16850 {I9} eV. 2g|G{-n}=5.2 {I8} eV, 2g|G{+0}{-n}=40 {I6} meV, g|G{-n}|G{-|g}/|G=97 {I12} meV. 


level_energy_unit: KEV
level_spin_parity: [3]-
level_comment:
$E{-n}(lab)=16940 {I9} eV. 2g|G{-n}=5.2 {I10} eV, |G{-|g}=262 {I26} meV, 2g|G{+0}{-n}=40 {I8} meV, g|G{-n}|G{-|g}/|G=144 {I20} meV. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$E{-n}(lab)=16970 {I9} eV. 2g|G{-n}=14.0 {I13} eV, 2g|G{+0}{-n}=108 {I10} meV, g|G{-n}|G{-|g}/|G=278 {I17} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=17030 {I9} eV. 2g|G{-n}=122 {I15} meV, 2g|G{+1}{-n}=33 meV, g|G{-n}|G{-|g}/|G=42 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18020 {I10} eV. 2g|G{-n}=164 {I22} meV, 2g|G{+1}{-n}=41 meV, g|G{-n}|G{-|g}/|G=51 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18510 {I10} eV. 2g|G{-n}=88 {I9} meV, 2g|G{+1}{-n}=21 meV, g|G{-n}|G{-|g}/|G=33 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18530 {I10} eV. 2g|G{-n}=94 {I9} meV, 2g|G{+1}{-n}=23 meV, g|G{-n}|G{-|g}/|G=35 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18560 {I10} eV. 2g|G{-n}=180 {I26} meV, 2g|G{+1}{-n}=43 meV, g|G{-n}|G{-|g}/|G=54 {I4} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18610 {I10} eV. 2g|G{-n}=41 {I9} meV, 2g|G{+1}{-n}=10 meV, g|G{-n}|G{-|g}/|G=18 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18640 {I10} eV. 2g|G{-n}=99 {I13} meV, 2g|G{+1}{-n}=24 meV, g|G{-n}|G{-|g}/|G=36 {I5} meV. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$E{-n}(lab)=18850 {I10} eV. 2g|G{-n}=43 {I5} meV, 2g|G{+1}{-n}=10 meV, g|G{-n}|G{-|g}/|G=18.4 {I23} meV. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
$E{-n}(lab)=19080 {I10} eV. 2g|G{-n}=13.0 {I5} eV, 2g|G{+0}{-n}=94 {I4} meV, g|G{-n}|G{-|g}/|G=329 {I9} meV. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
T$from |g(t) in 2016Ma49, measured 61 times over a period of 38 days. 
J$from Adopted Levels of {+86}Rb in the ENSDF database (December 2014 update). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: Y
level_comment:
J$from atomic beam magnetic resonance (1962Pe14), optical spectroscopy (1976Fu06), confirmed by hyperfine-structure measurement (1981Th04). |p from L=1 in ({+3}He,d). 
T$Taken from most recent measurement using 4|p|b liquid scintillation counting in a photomultiplier-tube spectrometer (2003Ko66). Full precision is 4.967|*10{+10} y {i32} 
Others: 4.72 {I4} (1966Mc12), 4.88 {I8} (1974Ne14,1972Ne19), and 4.89 {I4} (1977De22), 5.560 {I25} [E. Akatsu, Radioisotopes 30 (1981) 647], 5.21 {I15} (1965Br25), 4.60 {I6} (1965ThZY, as cited in 1990Ho28), 4.77 {I10} (1964Ko11), 5.80 {I12} (1962Le08), 5.25 {I10} (1961Mc07), 5.82 {I10} (1961Eg01), 5.53 {I10} (1961Be41), 4.72 {I8} (1960Ra01), 5.02 {I20} [G. V. Ovchinnikova, Geochemica 5 (1959) 393, as cited in 1990Ho28], 4.7 {I1} (1959Fl40), 5.07 {I20} (1957Li42), 4.6 {I5} (1956Fr12), 5.0 {I2} (1956Al31), 6.2 {I3} (1954Ma31), 4.3 {I3} (1954Ge60), 6.2 {I2} (1954Fl18), 5.9 {I3} (1952Le24), and 6.15 {I30} (1951Cu30) where all numbers are in units of 1x10{+10} y. There are several other measurements reported before 1950. Many of these values have been taken from citations in 1961Be41 or 1990Ho28. In the previous evaluation, the evaluator averaged only the three recent measurements of 1966Mc12 and 1977De22, who determined the amount of {+87}Sr produced in the {+87}Rb |b{+-} decay, and of 1974Ne14 (absolute counting in proportional counter), where systematic errors which were shown to be inherent in the older measurements (see 1976Ne10) were avoided to a large extent. This weighted average has an internal uncertainty of 0.027, a reduced-|h{+2} of 4.9, and an external uncertainty of 0.06. This uncertainty was increased to 0.09 to include the two most precise values. It is clear that the adopted half-life depends greatly on which values are included in the average. For example, note that the four values from 1961 and 1962 range from 5.25 {I10} to 5.82 {I10}. Others: in the process of analyzing some meteorite data, 1982Mi14 state that, if their {+87}Rb-{+87}Sr data are to agree with their U-Th-Pb data, the {+87}Rb decay constant would need to be 1.402 {I8} x10{+-11} y{+-1}, which corresponds to a half-life of 4.94 {I3} x10{+10} years. Determination of the half-life is, for some techniques, dependent on the |b spectrum shape factor function, discussion of which may be found in 2007Gr05 and 2007Gr06 
MOMM1 from 2011StZZ evaluation and based on data of 1993Du08; others: +2.751818 {I2}, and +2.751235 {I3} cited in 1989Ra17 evaluation. 
MOME2 from 2011StZZ evaluation, where the measured values are given as +0.132 {I 1} (1973Fe05), +0.127 {I 1} (1971St12) +0.134 {I1}, +0.128 {I1} (1999Ke12). Other: +0.13 {I2} (1981Th04) 
|d<r{+2}>({+85,87}Rb)=0.03 {I6} fm{+2} and |d<r{+2}>({+87,89}Rb)=0.28 {I6} fm{+2} (1999GaZU). Plot in 1981Jo01 gives similar values. 
MOMM3$-0.58 b |u{-n} {I39} from combining measured hyperfine intervals with atomic structure calculations, 2009Ge02 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
J$a comparison of T{-1/2} measured by DSAM in {+12}C(86Kr,x|g) with g|G{+2}{-|g0}/|G measured in (n,n'|g) gives J=1/2 
T$DSAM (2013St05). Other: 95 fs {I +14-11} from |G in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L=2 in (p,p') from 3/2-, comparison of |g excitation functions in (n,n'|g) with Hauser-Feshbach calculations gives 3/2-. 
T$Calculated from (|g,|g') level width 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$L=4 in ({+3}He,d), comparison with model calculation supports an assignment of g{-9/2} (1975Me02). 
T$from (|a,|a') using a pulsed beam technique (1995Ka18) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L=2 in (p,p') from 3/2-, comparison of |g excitation functions in (n,n'|g) with Hauser-Feshbach calculations gives 3/2- 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2)
level_comment:
J$From (|g|g'). The 1/2+ can be ruled out since the the 1975 |g transtion to the 403 keV 5/2- level would then have mult=M2 with the g|G{+2}{-|g0}/|G value leading to B(M2)(W.u.)=830 exceeding RUL 


level_energy_unit: KEV
level_spin_parity: (+)
level_comment:
J$L=(5) in (p,p') from 3/2-, this level is probably not identical with the 2379 level observed in |b{+-} decay because of |g to 3/2- from the latter level. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E$only from ({+3}He,d) and (g,g'). 
J$L=0 in ({+3}He,d). 
T$Calculated by evaluator from (|g,|g') level width 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J$The authors state that the 845 keV |g excitation function leads to a better fit for 1/2- than for 3/2-. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J$L(p,p')=2 allows 1/2- to 7/2-. L({+3}He,d)=1 limits to 1/2-, 3/2- and the Hauser-Feshbach fit in 1980Ba29 narrows this to 1/2-. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$J{+|p} is fit best by J{+|p}=11/2+ in the Hauser-Feshbach analysis, but J{+|p}=9/2+ is also allowed. Note also that the deexciting 1578 |g may be from the 1/2-,3/2- level at 1578 keV, and the 1175|g is the one measured, not the 1578|g 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$A{-2}=-0.148 {i27} consistent only with J=5/2 (1964Al28). 
T$from B(E2)=0.0056 {i5} and |d(402)=-0.24 {I +9-12}, the level half-life is 0.080 ns {I+11-60}; 
BE2$weighted average of 0.0054 {I6} (1973Bo24), 0.0058 {I12} (1956Fa29), and 0.0073 {I25} (1959Al04, with |DE{-|g} from a general comment). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L$1972Ha24 give L=1 with a good fit to angular distribution, 1973Co28 give L=1+3 with a poor fit, although their datapoints are still consistent with L=1, although the situation there is ambiguous. 1972NeZR give L=4, and 1987Li12 give L=(4). But the level is a doublet in {+87}Rb Adopted Levels with J{+|p}=1/2-,3/2- at 1578.01 and J{+|p}=(9/2)+ at 1578.10. 
S$C{+2}S=0.15 for L=1 from 1971NeZN should be considered approximate since other values in 1971NeZN were revised in 1971NeZR. Also, C{+2}S=0.22 for L=1 (1972Ha24) and C{+2}S|<0.35 for L=1 (1973Co28). 
E$Uncertainty from 1972Ha24 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2)-
level_lifetime_unit: EV
level_comment:
$g|G{-0}{+2}/|G=0.00157 eV 33 
T$For |G{-0}/|G=0.81 using branching from the Adopted Levels. No uncertainty is available for this branching, so the uncertainty quoted for |G is a lower limit. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2)-
level_lifetime_unit: EV
level_comment:
$g|G{-0}{+2}/|G=0.00084 eV 31 
T$For |G{-0}/|G=0.87 using branching from the Adopted Levels. No uncertainty is available for this branching, so the uncertainty quoted for |G is a lower limit. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$From Adopted levels. 
$Earlier Configuration, in the literature, was proposed as: 85%[(g{-9/2}~#0+)]+14%[(g{-9/2}~#2+)]; 2005Fo05 suggest a small admixture of p{-3/2}~#3- based upon observation of proposed E3 transition from isomer. 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_comment:
J$based on systematics of surrounding levels in {+87}Rb. (11/2)+ is also listed in table I with final level for 408.0|g. |p from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$Inferred from R(ADO) of 1831|g assuming (Q) to be E2. It is suggested that the somewhat smaller than expected value may be due to a loss of alignment due to higher lying isomeric states. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
J$from atomic beam (1968Va03). L(d,p)=0+2 on 3/2- target. 
T$from 1989Ab22. Evaluators have increased the uncertainty to 0.1%. Value reported by 1989Ab22 is 17.773 min {I11}. Others: 17.78 min {I11} (1969Ra05), 17.7 min {I1} (1969He16). 
$|m,Q: from high-resolution LASER spectroscopy (1981Th04). Others: 0.508 {I5} (1968Va03) and 0.50761 {I1} (1979Ek02) both from atomic beam. 
$|d<r{+2}>{+88,87}=0.139 fm{+2} {I8} (2013An02). 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: NS
level_comment:
J$(M2) 647|g to (5-). 
T$from |g|g(t) in {+208}Pb({+18}O,F). Other: |?100 ns (2000PoZZ). 
$Configuration: |pg{-9/2}|nd{-5/2} (2009Po10). 


level_energy_unit: KEV
level_spin_parity: 3+,4+,5+
level_comment:
J$L({+3}He,p)=4. Level is distinct from a tentatively observed 2089 level in {+88}Kr |b{+-} decay (not adopted) as the 1892|g decay to (1)- is inconsistent with the spin of this level. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$From the coincidence relation and the difference between 340 keV and 313 keV transitions; the 27.5 keV transition was not observed in the experiment. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (2009Po10). Other: |?100 ns (2000PoZZ). 
$Configuration: |pg{-9/2}|nd{-5/2} (2009Po10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
E$in particle spectrum gated on 2231 keV {I422}, a single event at 2231 keV was observed in |g ray spectrum (2019Za07) 
$B(>)=0.006 {I+20-6} for excitation energy bin of 2231 keV {I422} 
E$rounded value from Adopted Levels of {+88}Rb in the ENSDF database 


level_energy_unit: KEV
level_comment:
E$only energy bin below the neutron separation energy with non-zero B(>). Corresponds to several excited 1+ observed previously in the |b{+-} decay of {+88}Kr. 


level_energy_unit: KEV
level_lifetime_unit: MIN
level_comment:
T$from weighted average of 17.784 m {I47} using 4|p|b method and 17.778 m {I41} using 4|p|b|g method (2020Ch42). Final value quoted by 2020Ch42 is weighted average, with uncertainty taken to cover maximum boundry range of the uncertainties from each method. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
$RMS charge radius: (<r{+2}>){+1/2}=4.2420 fm {I79} (2004An14 evaluation; and 2008 update available at http://cdfe.sinp.msu.ru) 
J$spin from 1978Ek05 (hyperfine structure measurement by atomic-beam resonance method), parity from log| {If{+1u}t}=10.2 to 7/2+. |s(|q) in (|a,p) is consistent with 3/2- 
T$from weighted average (using normalized-residuals method) of 15.60 min {I9} (1972Eh02), 15.15 min {I12} (1969Ca03), 14.9 min {I3} (1956Ok06) and 15.4 min {I2} (1940Gl05); reduced |h{+2}=2.6 with adjusted uncertainty of 0.16 min for value from 1972Eh02. Other averaging methods give: 15.39 min {I13} (LWM method, |h{+2}=3.8) and 15.22 min {I9} (Rajeval technique, |h{+2}=1.2 with adjusted uncertainty of 0.4 min for value from 1972Eh02). Other: 15.5 min (1940Ha10) 
MOMM1$from hyperfine structure measurement of Rb by LASER spectroscopy (1981Th04). Others: 2.378 {I4} (1979Ek02), 2.377 {I5} (1979Kl03). 
MOME2$from hyperfine structure (1981Th04). Other: +0.16 {I3} (1979Kl03) 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_comment:
J$ |DJ=1, dipole |g to 3/2- from |g|g(|q) in ({+48}Ca,X|g); 1/2 not allowed by anisotropic |g distribution; |s(|q) distribution in (|a,p). Probable shell-model configuration= |p(p{-3/2}{+4},f{-5/2}{+5})~#|nd{-5/2}{+2} (1973He01). 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$probable shell-model state with configuration= |p(p{-3/2}{+2},f{-5/2}{+6},p{-1/2}{+1})~#|nd{-5/2}{+2} (1973He01). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2-)
level_comment:
J$gammas to 3/2- and 5/2(-); |g from (5/2+,7/2-); log| {Ift}=7.6 from 3/2(+) disfavors 7/2+. Possible weak 79.4|g to (1/2-) disfavors 5/2+,7/2- 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_comment:
J$|DJ=(2) |g to (5/2-); |DJ=1 |g to (7/2-); nanosecond isomer from heavy-ion studies. log| {Ift}=7.9 from 3/2(+) would be inconsistent 
T$from analysis of the timing parameter in delayed coincidences between |g rays above and below the 1195.4,9/2+ state in ({+48}Ca,X|g) (2009Pa20). Others: 15.2 ns {I28} (2010ToZY), few nanosecond in {+238}U,{+192}Os({+82}Se,X|g) (2007Bu35). Note that value in 2010ToZY is almost twice as large as from 2009Pa20. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_comment:
J$|DJ=2 |g to (17/2+). Shell-model calculations predict two states of 19/2+ and 21/2+ close in energy 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2-)
level_comment:
E$ordering of 1534-867 cascade was reversed in 1972Po13 defining a level at 1534 instead of that at 867. (|a,p) data support a level near 867 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2-)
level_comment:
E$doublet proposed by 1972Po13 (from 710-711 and 931-932 |g-ray doublets) at 930.7 and 931.5 is not confirmed by 1973He01 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$estimated (evaluator) for a weak unlabelled group in figure VIII-5 (1983StZQ). This may correspond to 497 known from {+89}Kr |b{+-} decay 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$|s(EXP)/|s(DWBA)=1.15 
E$peak labeled as 497 in figure VIII-5 (1983StZQ) is incorrect in energy. The evaluator estimates the energy of this peak at |?600. This group may correspond to 577, 586 doublet known from {+89}Kr |b{+-} decay 
S$for L=1, J|p=1/2- 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_comment:
T$ measured by 2010ToZY using |g(t) method. Other: 8 ns 2 (2009Pa20). Note a large difference in the two measurements 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$from analysis of the timing parameter in delayed coincidences between |g rays above and below the 1195.4, 9/2+ state. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
T$ this level is proposed to have lifetime of few nanosecond based on weaker observed intensities of transitions below this level 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: S
level_comment:
J$J=0 from atomic-beam measurement (1979Ek02). |p from {+90}Rb(g.s.) |b{+-} decay with log| {If{+1u}t}=8.42 {I6} to {+90}Sr(832) 2+ state. 
T$weighted average of 153 s {I3} (1969Ca03) and 162 s {I3} (1977Hu03), both from |g(t) with mass separated sources and Ge(Li). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: S
level_comment:
%IT$from measured I|g, |a and normalization (1981Ta05), see {+90}Rb |b{+-} decay (258 s). 
J$J=3 from atomic-beam measurement (1979Ek02); M3 106.9|g to 0-. 
T$weighted average of 258 s {I5} (1967Am01) and 258 s {I4} (1977Hu03), both from |g(t) with mass separated sources and Ge(Li). 
MOMM1$from atomic-beam laser spectroscopy (1981Th04). Other: 1.612 {I5} (atomic-beam magnetic resonance, 1979Ek02) 
MOME2$from atomic-beam laser spectroscopy (1981Th04,2016St14). Measured value given in 1981Th04 is 0.20 {I5}, evaluated to +0.25 {I7} by 2016St14. 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$M1+E2 55.8|g to 3- 
$Configuration=|pp{-3/2}{+-1}~#|n(d{-5/2}{+3}) or less likely |pf{-5/2}{+-1}~#|n(d{-5/2}{+3}) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g|g(|q) for 965-56 cascade in {+235}U(n,F|g) gives 5 or 6; (M1+E2) 365.1|g from 6(+) favors (5+) 


level_energy_unit: KEV
level_spin_parity: 5
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g|g(|q) for the 1042-55.8 cascade in {+235}U(n,F|g); J=4 and 6 are excluded by the |g|g(|q) analysis. 
$Proposed configuration=|pf{-5/2}{+-1}~#|n(d{-5/2}{+3}) (2016Cz01) which would result in J|p=5- 


level_energy_unit: KEV
level_spin_parity: 6(+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g|g(|q) data for 365-965 cascade in {+235}U(n,F|g) are consistent with 6->5->4 or 6->6->4 sequences and large |d(Q/D) value for the 365|g in both spin sequences. This implies mult=M1+E2, and thus the same parity for 1493 and 1128 levels. The |g|g(|q) data for the 288-1042 cascade is consistent with J=5 or 6 for 1493 level. Absence of transition to 163, 4- level suggests positive parity for J=6 for the 1493 level 


level_energy_unit: KEV
level_spin_parity: (7,6)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g|g(|q) in {+235}U(n,F|g) is consistent with J=6 or 7, but absence of transitions to 1128, (5+) and 1204, 5 makes J=6 less likely 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$from the Adopted Levels, held fixed in least-squares adjustment. 
$Configuration=|pp{-3/2}{+-1}~#|n(d{-5/2}{+3}) or |pf{-5/2}{+-1}~#|n(d{-5/2}{+3}) 


level_energy_unit: KEV
level_spin_parity: 5
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$J=4 and 6 are not consistent with |g|g(|q) result for the 1042-55.8 cascade, with |d(55.8)=0.302 (2016Cz01) 
$Proposed configuration=|pf{-5/2}{+-1}~#|n(d{-5/2}{+3}) would give J|p=5- 


level_energy_unit: KEV
level_spin_parity: 6(+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g|g(|q) data for 365-965 cascade are consistent with 6 ->5 ->4 or 6 -> 6 ->4 sequences and large |d(Q/D) value for the 365|g in both spin sequences. This implies mult=M1+E2, and thus the same parity for 1493 and 1128 levels. The |g|g(|q) data for the 288-1042 cascade is consistent with J=5 or 6 for 1493 level. Absence of transition to 163, 4- level suggests positive parity for J=6 for the 1493 level 


level_energy_unit: KEV
level_spin_parity: (7)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g|g(|q) consistent with J=6 or 7, but absence of transitions to 1128, (5+) and 1204, 5 makes J=6 less likely 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: S
level_comment:
|D<r{+2}>({+81}Rb-{+87}Rb)=-0.532 {I12} (1979Kl03), 0.558 {I4} (1981Th04). 
<r{+2}>{+1/2}(charge)=4.278 fm {I13} (2004An14). 
J J from nuclear radiation detected optical pumping (1978Bo38). Parity from shell-model systematics. Possible configuration: 1/2[321] (2010Ro31). 
T unweighted average of 59.2 s {I2} (1970OsZZ), 57.8 s {I5} (1970ChYZ), 58.2 s {I2} (1969Ca03), and 57.4 s {I3} (1967Am01). Other measurements: 1971Kr22, 1972Eh02 (66.6 s {I12}), 1974Ac01 (62 s {I4}), 1974Gr29 (58.2 s {I10}). 
MOMM1 from high-resolution laser spectroscopy on atomic beams (1989Ra17 and 2011StZZ; from 1981Th04). No hfs anomaly allowed for in |m({+87}Rb) standard. Other |m from hfs measurements: 2.177 {I5} (1987Ra17 and 2011StZZ, from 1979Kl03), 2.177 {I3} (if no hfs anomaly) (1989Ra17 and 2011StZZ, from 1979Ek02) or 2.18 {I3} allowing 1% additional uncertainty from unknown hfs anomaly (1979Ek02)). 
MOME2 from high-resolution laser spectroscopy on atomic beams (2011StZZ from +0.154 {I26} with Sternheimer correction, from 1981Th04 and 1989Ra17). Other Q: 0.14 {I3} after Sternheimer correction; from continuous beam LASER spectroscopy (1989Ra17 and 2011StZZ, from 1979Kl03). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: NS
level_comment:
J M1(+E2) transition to 3/2(-) g.s.; log| {Ift}=6.4, log| {If{+1u}t}=8.4 from 5/2(+); systematics favor J=5/2. 
T from centroid shift of |b|g(t) in |b{+-} decay (1976Gl02). 


level_energy_unit: KEV
level_spin_parity: (LE7/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J (M1,E2) 613|g to (5/2-) 109; 722|g to 3/2(-) g.s.; log| {Ift}=7.2, log| {If{+1u}t}>9.6 from 5/2(+). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_comment:
J by analogy with similar structures built on isomers in lower-mass odd-a Rb isotopes (2009Hw03,2009Pa20); supported by shell-model calculations (2010Si17). However, log| {Ift}=7.1, log| {If{+1u}t}=9.0 from 5/2(+) in |b{+-} decay seems unreasonably low. 
T weighted average of 16 ns {I1} from |g|g(t) in {+252}Cf SF decay and 17.0 ns {I8} from |b|g(t) (1986Si20) in |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
%IT: only IT decay has been observed. 
T from |g|g(t) (2010Si17); summed time spectrum double-gated on prompt 707|g, 1138|g, 1119|g and delayed 412|g, 613|g, 1025|g fitted by exponential decay plus constant background. From {+252}Cf SF decay. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_comment:
J 27/2- state with dominant configuration of |pg{-9/2}~#|n(g{-7/2}h{-11/2}) is predicted from calculations by 2010Si17. 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: S
level_comment:
%B-N value recommended in evaluation by 1993Ru01; weighted average of 0.012 {I4} (1969Ta04), 0.0125 {I15} (1975As05), 0.0109 {I12} (1980Lu04), 0.0091 {I15} (1980ReZQ), 0.0098 {I10} (1980ReZQ), 0.0109 {I7} (1993Ru01). Other: 0.012 {I2} (1977Re05). 
J J=0 from atomic beam (1979Ek02); log| {Ift}=7.5 to 2+ {+92}Sr(815 level) rules out |p=+ and log| {Ift}<6.4 to {+92}Sr(0+ g.s.) rules out 0+. The likely configuration=((|p 1f{-5/2}){+-1}(|n d{-5/2}){+-1}) (1979Ek02). 
T unweighted average of 4.43 s {I5} (1967Am01), 4.50 s {I3} (1969Ca03), 4.50 s {I4} (1974Gr29), 4.54 s {I2} (1975Re10), 4.34 s {I6} (1976Ru01), 4.57 s {I7} (1979En02), 4.46 s {I2} (1993Ru01); weighted average of these data is 4.492 {I20}. Other measurements: 1960Fr05, 1966Wa22. 
<r{+2}>{+1/2}(charge)=4.298 fm {I16} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
J stretched E2 142|g to 1- 143. 
T from {+248}Cm SF decay. 1974ClZX report a T{-1/2}=57 ns 142|g from {+92}Rb which is strongly coincident with itself and with K| x ray(Rb) in {+252}Cf SF decay; this implies the existence of an isomeric level in {+92}Rb with E|>284 keV which is not populated in {+92}Kr |b{+-} decay (1974ClZX). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
T from (1363|g)(142.2|g)(t) (2012Ur01), time spectrum fitted with exponential decay and a constant background. The presence of this isomer was also confirmed in an independent measurement using cold neutron beam facility at Grenoble by measuring delayed |g rays following fission of {+235}U by thermal neutrons using an array of 15 Ge detectors. 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: NS
level_comment:
T from (734.5|g)(276|g)(t) and (734.5|g)(1363|g)(t) (2012Ur01); time spectra of 276|g and 1363|g fitted with exponential decay and a constant background. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
T 1974ClZX report a T{-1/2}=57 ns 142|g from {+92}Rb which is strongly coincident with itself and with K| x ray(Rb); this implies the existence of an isomeric level in {+92}Rb with E|>284 keV which is not populated in {+92}Kr |b{+-} decay (1974ClZX). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
J from hyperfine structure (1981Th04). |p from comparison of |m with Schmidt values. 
%B-N Weighted average of: 1.43% {I18} (1969Am01), 1.65% {I30} (1969Ta04), 1.24% {I14} (1974Ro15), 1.16% {I8} (1975As03), 1.2% {I1} (1975As04), 1.86% {I13} (1977Re05), 1.40% {I8} (1980Lu04), 1.36% {I14} and 1.37% {I10} (1980ReZQ), 1.97% {I22} (1981En05), 1.53% {I9} (1993Ru01). Others: 2.6% {I4} (1968AmZZ), 2.1% {I6} (1972Sc48; revised to 1.9 {I5} in 1993Ru01). 1993Ru01 recommend %|b{+-}n=1.35 {I5}, but omit the 1977Re05 datum from the average. 
%B-N: 1.39% 7 (W.A. OF 11 DATA); 1.40% 7 (W.A. OF 13 DATA); 1.59% 43 (LIMITATION OF RELATIVE STATISTICAL WEIGHTS, 13 DATA). 
|m, Q: from LASER induced optical pumping of thermal atomic beam with magnetic state selection (1989Ra17, based on 1981Th04). |m relative to {+87}Rb. Others: |m=+1.400 {I6}, Q=0.27 {I6} from collinear fast-beam LASER spectroscopy (1979Kl03). 
|D<r{+2}>({+93}Rb,{+87}Rb)=0.813 {I3} (1981Th04), 0.797 {I12} (1979Kl03, recalculated by 1981Th04). 
<r{+2}>{+1/2}(charge)=4.314 {I19} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_comment:
J M1 |g to J|p=5/2-; log| {Ift}|?6.5 from 1/2+. 
$T{-1/2} 57 |ms {I15} from (fission fragment)-(257|g or x-ray) delayed coin (1970Gr38). Isomer not confirmed in recent work (2014Mi12) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J D, |DJ=1 552|g from (9/2+) 1285 in 248Sm SF decay. 2009Hw03 suggest configuration of |pf{-5/2}~#({+92}Kr g.s. band) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J Q, |DJ=2 1285|g to (5/2-) g.s.; likely configuration of |p g{-9/2}~#({+92}Kr g.s.) (2009Hw03); M2 transitions are observed to deexcite the low-lying 9/2+ states in {+91}Rb and {+95}Rb also. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
J level T{-1/2} is consistent with Weisskopf estimate for an E2 100-keV transition to the (23/2-) 4322 level; similarity of this isomer to the K|p=27/2- |p g{-9/2}~#|n (g{-7/2}h{-11/2}) isomer in the {+95}Y isotone suggests the same dominant configuration for this level also. Supported by shell model calculations (2010Si17). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
J level T{-1/2} is consistent with Weisskopf estimate for an E2 100-keV transition to the (23/2) 4322 level; similarity of this isomer to the K|p=27/2- |p g{-9/2}~#|n (g{-7/2}h{-11/2}) isomer in the {+95}Y isotone suggests the same dominant configuration for this level; supported by shell model calculations (2010Si17). 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: S
level_comment:
$%|b{+-}n: from weighted average of 10.9 {I7} (1993Ru01), 9.7 {i6} (1983Ok07), 11.1 {i9} (1981En05), 10.1 {i6} (1980Lu04), 9.7 {i5} (1979Ri09), 11.6 {i7} (1979WaZU), 13.7 {i10} (1977Re05), 9.6 {i8} (1975As04), 9.3 {i18} (1975Iz03), 12.1 {i13} (1974Ro15 recalibrated by 1981Bj01). 
$J: from optical pumping detected by |b{+-} asymmetry (1978Bo38). Parity deduced from shell model. 
T$from |b{+-} multiscaling (1984Ka24). Other measurements: 2.76 s 6 (1981En05), 2.73 s 2 (1979Ri09), 2.73 s 1 (1977Re05), 2.69 s 2 (1976Ru01), 2.67 s 6 (1975As04), 2.76 s 8 (1974Ro15), 2.67 s 4 (1974WoZJ), 2.67 s 4 (1971ShZD), 2.74 s 6 (1967Am01) from n multiscaling. 2.80 s 4 (1979En02), 2.83 s 3 (1975Re10), 2.8 s 1 (1972Am01), 2.63 s 4 (1967Am01) from |b{+-} multiscaling, 2.711 s 14 (1993Ru01), from n and |b{+-} multiscaling. 
MOMM1,MOME2$from 1989Ra17 
$<r{+2}>{+1/2}=4.329 fm {I21} (2004An14) 


level_energy_unit: KEV
level_spin_parity: (8)
level_comment:
E$1750 given in figure 4 of 2008Ts03 seems a misprint. The E|g=345 seems correct in view of a 345.0 gamma ray shown in figure 3 of 2008Ts03 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: S
level_comment:
T,J$from {+94}Rb Adopted Levels in the ENSDF database (March 2011 update). The ground state is interpreted as part of |pf{-5/2}{+-1}~#|ns{-1/2} multiplet 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$low-lying 2- is expected from |pf{-5/2}{+-1}~#|ns{-1/2} multiplet (2016Mi18) 
$Transition from this level to the g.s. is expected to be M1 and highly converted with theoretical conversion coefficient |a=180 (from BrIcc code), and has not been seen (2016Mi18) 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: NS
level_comment:
J$possible E2 transition to (2-); 4- is rejected by 2016Mi18 as this level is not populated as the yrast 4- state in {+252}Cf SF decay (2008Ts03: Phys. Rev. C78, 011301(R)). This state is interpreted as built on |pf{-5/2}{+-1}~#|nd{-5/2} configuration 
T$measured by 2016Mi18 from |b(99.2|g)(t) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$strong (allowed) |b transition from 0+ parent state. 2016Mi18 propose that this state is built on |pg{-9/2}~#|ng{-7/2} multiplet 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
%B-N$from 2002Pf04 
J$J=5/2 from atomic beam experiment (1979Ek02); |p=- from J and |m 
T$weighted av of 384 ms {i4} (2003Be05), 379 ms {i2} (1993Ru01), 378 ms {i2} (1987GaZF), 377 ms {i1} (1986ReZU), { 377 ms} {i6} (1979Ri09), and 377 ms {i4} (1975Re10). 
MOMM1,MOME2$from 1981Th04 using atomic beam laser spectroscopy (ABLS); Others: 1989Ra17, 2005St24 
$|D<r{+2}>(95,87)=1.0781(56) fm{+2}, deduced from isotope shift (1981Th04) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
$ Total of 7587 implantations observed, and 3253 correlated decay sequences. 
T$ values listed in table I: 410 ms {I20} (syst) {I25} (stat), from maximum likelihood method (MLH); 412 ms {I1} (syst) {I13} (stat), least-squares fit method. Value in Adopted dataset for {+95}Rb in ENSDF database is 377.7 ms {I8}. 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_lifetime_unit: MS
level_comment:
J$J=2 from atomic beams (1981Th04). 
T$weighted av of 0.22 s {i1} (1981En05), 197 ms {i5} (1979Ri09), 188 ms {i2} (1979Pe01), 203 ms {i4} (1978Wo09), 205 ms {i4} (1977Re05), 203 ms {i3} (1976Ru01), 199.0 ms {i35} (1974Ro15), and 207 ms {i3} (1971Tr02) 
MOMM1,MOME2$abls. |m calculated by 1989Ra17 using hyperfine-structure ratio and |m({+87}Rb). "Sternheimer" or other polarization correction applied to Q. 
$Configuration=|pf{-5/2}|ns{-1/2} (1999Ge01). 
$<r{+2}>{+1/2}(charge)=4.36 {I3} (2004An14) 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: US
level_comment:
T$From timing of 300 keV transition in {+96}Rb IT decay (2005Pi13). Other: 1.65 |ms {i15} (1999Ge01) 
$Configuration=[|pg{-9/2}|nh{-11/2}]{-10-} (1999Ge01). 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: US
level_comment:
T$From timing of 300 keV transition (2005Pi13). Other: 1.65 |ms {i15} (1999Ge01) 
$Configuration=[|pg{-9/2}|nh{-11/2}]{-10-} (1999Ge01). 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_lifetime_unit: MS
level_comment:
$ Total of 1972 implantations observed, and 1904 correlated decay sequences. 
T$ values listed in table I: 220 ms {I8} (syst) {I17} (stat), from maximum likelihood method (MLH); 212 ms {I6} (syst) {I16} (stat), least-squares fit method. Value in Adopted dataset for {+96}Rb in ENSDF database is 203 ms {I3}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
MOMM1,MOME2$atomic beam laser spectroscopy (1981Th04). Original measured value of Q=+0.581 {I44} in 1981Th04 is re-evaluated to +0.70 {I15} by 2013StZZ 
$Total of 291 implantations observed, and 164 correlated decay sequences (2012Qu01). 
J$spin from atomic beam (1981Th04). Measured magnetic moment is consistent with |p3/2[431] or |p3/2[301], but in the Coulomb excitation experiment, 3/2[301] is ruled out from trend of observed M1 transition rates and B(M1)/B(E2) ratios. See also theoretical calculations by 2010Ro31 which predicts prolate ground state with |p3/2[431] Nilsson configuration 
T$half-life determined by delayed neutron counting by 1993Ru01, 1983Re10, 1981En05, 1979Ri09, 1977Re05, 1976Ru01, 1974Ro15; |b{+-} counting by 1979En02, 1978Wo09, 1977Re05; |g counting by 1979Pe01; ion-|b correlated decay curves by 2011Ni01 and 2012Qu01. 
T$weighted average of 168 ms {I1} (1993Ru01, earlier value of 172 ms {I3} in 1976Ru01); 169 ms {I2} (1987PfZX); 169 ms {I1} (1986Wa17, earlier values of 169 ms {I2} in 1983Re10, 167 ms {I2} from neutron counting and 182 ms {I7} from |b{+-} counting in 1977Re05); 200 ms {I20} (1981En05, earlier value of 187 ms {I19} in 1979En02); 173 ms {I3} (1979Pe01); 171 ms {I4} (1979Ri09); 170 ms {I2} (1978Wo09); 172.2 ms {I50} (1974Ro15); 176 ms {I5} (1971Tr02). Other recent but much less precise measurements: 208 ms {I+42-36} (2012Qu06); 0.17 s {+14-5} (2011Ni01). Value of 135 ms {I10} in 1969Am01 seems discrepant 
%B-N$weighted average of 30.9 {I31} (1993Ru01), 24.5 {I15} (1987PfZX), 26.1 {I13} (1986Wa17, earlier values of 26.9 {I19} in 1983Re10 and 35.9 {I26} in 1977Re05), 21.5 {I25} (1981En05), 25.2 {I18} (1979Ri09), 27.2 {I30} (1974Ro15). 
$Theoretical T{-1/2}=43.6 ms, %|b{+-}n=13.1, %|b{+-}2n=0 (2003Mo09) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$unweighted average of 5.1 |ms {i4} (2013Ruo7,from ion-|g time correlation of 76.5|g) and 6.33 |ms {I+37-34} (2012Ka36, |g(t) method; with constant background component separately deduced). Weighted average of the two values is 5.8 |ms {I6} but reduced |h{+2} is 5.3 
J$E1 |g to 3/2+. Comparison with HFB and QPRM calculations suggests |p3/2[312] prolate or (|p1/2[321],|p3/2[321]) oblate quasiparticle state (2013Ru07), thus favoring 1/2 or 3/2. 2012Ka36, however, propose (5/2), but do not discuss orbital configuration 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$unweighted average of 5.1 |ms {i4} (2013Ruo7,from ion-|g time correlation of 76.5|g) and 6.33 |ms {I+37-34} (2012Ka36, |g(t) method; with constant background component separately deduced). Weighted average of the two values is 5.8 |ms {I6} but reduced |h{+2} is 5.3 
J$E1 |g to 3/2+. Comparison with HFB and QPRM calculations suggests |p3/2[312] prolate or (|p1/2[321],|p3/2[321]) oblate deformed quasiparticle state (2013Ru07); thus favoring 1/2 or 3/2. 2012Ka36, however, propose (5/2), but do not discuss orbital configuration 


level_energy_unit: KEV
level_spin_parity: 0(-)
level_lifetime_unit: MS
level_comment:
$Evaluated rms charge radius=4.434 fm {I42} (2013An02). 
$Evaluated |d<r{+2}>({+87}Rb,{+98}Rb)=1.855 fm{+2} {I15} (2013An02) 
J$spin based on a fit with a Voigt profile to the optical spectrum of this state from collinear fast beam laser spectroscopy, which is in agreement to that expected for a single transition typical of J=0 (2015Pr03); parity from systematics of odd-odd Rb nuclei. Atomic-beam measurement by 1981Th04 also suggested J=0 
T$weighted average of 145 ms {I25} (2015Pr03, ion-|b correlated decay curve) and 114 ms {I5} (1980Sc13, decay curve for 167|g in {+97}Sr). These values are preferred over many other measurements where the measured half-lives may have corresponded to combined activities of 115 ms and 96 ms. Other measurements from timing of neutrons, |b or |g: 102 ms {I4} (2011Ni01, (ion)|b-correlated decay curve); 127 ms {I1} (2003Be05, |bn coin); 109 ms {I1} (1993Ru01, n-decay); 106 ms {I2} (1987PfZX, |bn-decay); 106 ms {I1} (1986ReZU,1986Wa17, |bn-decay); 108 ms {I1} (1983Re10, |bn-decay, same group as 1986ReZU); 110 ms {I20} (1981En05, |bn-decay); 100 ms {I20} (1979En02, |b-decay); 112 ms {I4} and 109 ms {I12} (1979Pe01, |bn-decay); 114 ms {I13} (1979Ri09, |bn-decay); 108 ms {I5} (1978Wo09, |b|g-decay); 98 ms {I18} (1976AmZW, |b-decay); 140 ms {I10} (1976Ru01, |bn-decay); 106 ms {I6} (1974Ro15, |bn-decay); 140 ms {I8} (1971Tr02, |b-decay); 131 ms {I31} (1970KlZZ, |b-decay). 
%B-N$weighted average of 13.0 {I10} (1987PfZX), 13.6 {I9} (1986ReZU, 1986Wa17, earlier values 13.4 {I19} in 1983Re10 and 12.8 {I20} in 1980ReZQ), 16.7 {I16} (1981En05), 15.8 {I26} (1979Pe01), 18.4 {I29} (1979Ri09), 19 {I3} (1974Ro15, original value of 13.3 {I21} in 1974Ro15 renormalized by 1981Jo01), 
%B-2N$from |b{+-}n/|b{+-}2n=267 {I33} (1981Re05) and %|b{+-}n=14.3 {I9}. 1981Re05 give %|b{+-}2n=0.060 {I9} based on %|b{+-}n=16.1 {I13}. Other: <0.1 (1974Ro15) 
$%|b{+-}n and %|b{+-}2n are combined for the decays of g.s. and isomer 
$|b{+-}n compilations: 1993Ru01, 1984Ma39, 1983En03, 1982Ru01, 1981Jo01, 1979RuZQ, 1975Iz03, 1989BrZI 
$|D<r{+2}>({+98}Rb,{+87}Rb)=1.821 fm{+2} {I15} (1981Th04) 
$|d<r{+2}>({+87}Rb,{+98}Rb)=+2.063 fm{+2} {I9}(stat) {I93}(syst); |d<|b{+2}{-2}>=+0.174 for |d|n({+87}Rb,{+98}Rb)=-910.5 MHz {I53} (2015Pr03, hyperfine structure measurements) 
$The sources of {+98}Rb used for many of the studies cited above for half-life and decay modes most likely contained small admixture of 96 ms isomer also. On the basis of T{-1/2} of 167|g (in {+97}Sr from {+98}Rb |b{+-}n decay), it is assumed here that predominant |b{+-}n decay is from the 115-ms activity. It is possible that the 141|g (in {+97}Sr) is from |b{+-}n decay of the 96-ms isomer, but T{-1/2} of 141|g is not known 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
J$Coulomb excitation from J=0(-) g.s. 2016Cl03 propose same parity for g.s., 114 and 432 levels 
T$from RDDS analysis, and scaled upwards by a factor of 1.4, as estimated from a comparison of lifetime determined by 2016Cl03 in Coulomb excitation using a similar analysis for the first 2+ state in {+98}Sr and the corresponding value in literature 


level_energy_unit: KEV
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$from (implant)|g(t) in {+98} IT decay (2012Ka36). Other: : 0.70 |ms {I+6-5} (2009Fo05, implant-|g(t)) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (3+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
E$from |b|g data and Q(|b{+-}) measurement (1982Pa24,1988GrZX). 2017Au03 suggest E(level)=73 {I26} 
J$spin tentatively assigned by 2015Pr03 from hyperfine structure measurements, where J=4 was not ruled out; 2002Lh01 also tentatively proposed 3+ with possible configuration=|p3/2[431]~#|n3/2[411] 
T$weighted average of 90 ms {I10} (2015Pr03, ion-|b correlated decay curve) and 96 ms {I3} (1980Sc13, decay curve for 289|g and 433|g in {+98}Sr). See numerous other half-life measurements in comments for the g.s., where these values may be for combined activity of g.s. and the isomer. 
$<|b{-2}>{+2}=+0.126, extracted from the quadrupole moment (2015Pr03) 
$|d<r{+2}>({+87}Rb,{+98}Rb)=+2.084 fm{+2} {I9}(stat) {I93}(syst); |d<|b{+2}{-2}>=+0.177 for |d|n({+87}Rb,{+98}Rb)=-922.5 MHz {I53} (2015Pr03) 
MOMM1,MOME2$deduced from measured hyperfine parameters relative to known values of {+87}Rb (2015Pr03). Uncertainties are statistical only. 
$%|b{+-}n and %|b{+-}2n are combined for the decays of g.s. and isomer. See the details of the measurements in comments for the g.s. 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
J$2016Cl03 in Coulomb excitation propose 1 or 2, based on 432|g to the g.s. The authors also propose same parity for g.s., 114 and 432 levels 


level_energy_unit: KEV
level_lifetime_unit: US
level_comment:
$Number of implanted fragments=1.7|*10{+6} 
T$from implant-|g(t) in 2012Ka36. Other: 0.70 |ms {I+6-5} from implant-|g(t) in 2009Fo05 


level_energy_unit: KEV
level_spin_parity: 0
level_lifetime_unit: MS
level_comment:
J$based on a fit with a Voigt profile to the optical spectrum of this state, which is in agreement to that expected for a single transition typical of J=0 (2015Pr03). 
$|d<r{+2}>({+87}Rb,{+98}Rb)=+2.063 fm{+2} {I9}(stat) {I93}(syst); |d<|b{+2}{-2}>=+0.174 for |d|n({+87}Rb,{+98}Rb)=-910.5 MHz {I53} (2015Pr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (3)
level_lifetime_unit: MS
level_comment:
J$tentatively assigned by 2015Pr03. J=4 was not ruled out. 
MOMM1,MOME2$deduced from measured hyperfine parameters relative to known values of {+87}Rb (2015Pr03). Uncertainties are statistical only 
$<|b{-2}>{+2}=+0.126, extracted from the quadrupole moment (2015Pr03) 
$|d<r{+2}>({+87}Rb,{+98}Rb)=+2.084 fm{+2} {I9}(stat) {I93}(syst); |d<|b{+2}{-2}>=+0.177 for |d|n({+87}Rb,{+98}Rb)=-922.5 MHz {I53} (2015Pr03) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
J$Coulomb excitation from J|p=0(-) g.s. 2016Cl03 propose same parity for the 114 and 432 levels 
T$from RDDS analysis, and scaled upwards by a factor of 1.4, as estimated from a comparison of lifetime determined using a similar analysis for the first 2+ state in {+98}Sr and the corresponding value in literature 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
J$2016Cl03 propose 1 or 2, based on 432|g to the g.s. The authors also propose same parity for g.s., 114, and 432 levels 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
%B-N$Recommended value from 1993Ru01. Others: 20.5% {i30}, 13.0% {i15} (both from 1987PfZX), 20.7% {i13} (1986ReZU), 13.1% {i18} (1984Ma39), 15% {i3} (1979Pe01) 
J$Tentative assignment based on syst for deformed odd-A Rb. 
T$LWM (Limitation of relative statisical weight method (1994Ka08)) average of 54.2 ms {i13} (2011Ni01), 50.3 ms {i7} (1993Ru01), 58 ms {i2} (1986ReZS, 1986ReZU, earlier value of 55 ms {i2} in 1983Re10), 59 ms {i1} (1984Pf01), 52 ms {i5} (1983Wo10), 59 ms {i4} (1979Pe01), 59 ms {i4} (1978Ko29). Others: 76 ms {i5} (1971Tr02); 55 ms {i2} (1983Re10), superseded by 1986ReZS, 1986ReZU. 
$Theoretical T{-1/2}=40.4 ms, %|b{+-}n=27.5, %|b{+-}2n=0.03 (2003Mo09) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: MS
level_comment:
J$from configuration=|p3/2[431]~#|n5/2[532] and proposed by 2001Lh02, based on ground-state configurations of neighboring nuclides. For this configuration, Gallagher-Moszkowski favors 4- g.s. and 1- at higher energy. J|p=(3+) was also suggested earlier in 1995Pf04 by the same authors as 2001Lh02, on the basis that there seemed to be a strong |b{+-} feeding to a 2+ level in {+100}Sr and that the possible configuration could be |p3/2[431]~#|n3/2[411]. 
T$weighted average of 48 ms {I3} (2011Ni01, (ion)|b-correlated decay curve); 53 ms {I2} (1987PfZX, |b and n decay); 59 ms {I10} (1986ReZU, |b and n decay, |bn-coin, 55 ms {I18} in 1986Wa17 is superseded by 1986ReZU); 51 ms {I17} (1979Pe01, n decay); 50 ms {I10} (1978Ko29, |b and |g decay) 
$%|b{+-}n: weighted average of 8 {I2} (1987PfZX) and 5.0 {I10} (1986ReZU). others: |?35 (2010MaZS), 26 {I8} (2001Lh02, from gamma-ray intensities and assuming no |b feeding to {+100}Sr g.s.). 
$%|b{+-}2n: from measured %|b{+-}2n/%|b{+-}n=0.027 {I7} (1981JoZV), and adopted %|b{+-}n=5.6 {I12}. 
$Theoretical T{-1/2}=35.3 ms, %|b{+-}n=29, %|b{+-}2n=0.0 (2019Mo01). 
$Theoretical T{-1/2}=44.0 ms, %|b{+-}n=6.9, %|b{+-}2n=0.3 (2016Ma12). 
$1999PfZZ superseded by 2001Lh02 
$Calculations of probability for %|b{+-}n decay and %|b{+-}2n decay have been carried out in a series of papers by the same group (1983Ly06,1983Ly03,1983Ly01,1984LyZW). %|b{+-}n(theory)=26, %|b{+-}2n(theory)=1.2 (1983Ly06). Other: 1986RaZG 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
J,%B-N$from Adopted Levels for {+101}Rb in ENSDF database 
T$ measured by 2011Ni01 from the analysis of the (ion)|b-correlated decay curve. Earlier value: 32 ms {I5} (Adopted Levels for {+101}Rb in ENSDF database) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from Adopted Levels for {+102}Rb in ENSDF database 
T$ measured by 2011Ni01 from the analysis of the (ion)|b-correlated decay curve. Earlier value: 37 ms {I3} (Adopted Levels for {+102}Rb in ENSDF database) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from Adopted Levels for {+102}Rb in ENSDF database 
$Theoretical %|b{+-}n=20.1, %|b{+-}2n=2.0 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+102}Rb 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier values: 37 ms {I3} (Adopted Levels for {+102}Rb in ENSDF database, taken from 1987PfZX conference proceedings article), 35 ms {I+15-8} (2011Ni01: Phys. Rev. Lett. 106, 052502; from the same group as 2015Lo04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=48.4, %|b{+-}2n=1.9 (1997Mo25). 
E$measured half-life is assumed to correspond to the ground state of {+103}Rb 
J$3/2+ from systematics (2012Au07) and from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
$Measured |s=110 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+103}Rb is <0.001% (2010Oh02) 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical T{-1/2}=12.1 ms, %|b{+-}n=53, %|b{+-}2n=8 (2019Mo01) 
$Theoretical T{-1/2}=17.2 ms, %|b{+-}n=67.2, %|b{+-}2n=2.3 (2016Ma12) 
$A total of two counts were assigned to {+104}Rb, with the spectrometer setting on Nb. Misidentification of this isotope is not likely since no events were observed for neighboring hydrogen-like peaks (2018Sh11) 
E$it is assumed that the observed events correspond to ground-state activity. 
J$1+ or 2+ from |W{-|p}=3/2+ and |W{-|n}=1/2+ orbitals proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 12.1 ms (2019Mo01) and 17.2 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+104}Rb is expected to be <25 ms, based on measured half-lives of 32 ms for {+101}Rb, 37 ms for {+102}Rb, and 26 ms for {+103}Rb, available in literature. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_lifetime_info: ;ERR=AP
level_comment:
$Delayed proton group reported by 1993Ba61 at E(p)(lab)=3750 {I40}, but percent decay mode was not deduced 
J$|W{-neutron}=3/2- (theory,2019Mo01). 1/2- from systematics (2017Au03) 
T$estimated from total transit time of |?25 ms (1993Ba61). From systematics and decreasing trend of half-lives of Sr isotopes as the neutron number decreases, value is expected to be <30 ms. T{-1/2} values are: 27 ms for {+74}Sr, 88 ms for {+75}Sr, 7.89 s for {+76}Sr, 9.0 s for {+77}Sr and 160 s for {+78}Sr. Theoretical value for |b decay=42.8 ms (2019Mo01) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$weighted average of 24.3 ms {I53} from |h{+2} fit to implant-|b(t) exponential decay included contributions from the parent, daughter and grand-daughter decays (if appropriate), as well as a constant background and 28 ms {I+5-4} from logarithmic binning method (2019Si33) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$%|e+|b{++} decay of {+73}Sr assumed as 100%, although, with S(2p)({+73}Sr)=200 {I420} (syst, 2017Wa10), two-proton decay mode to {+71}Kr cannot be ruled out. Note that S(p)({+73}Sr)=910 {I640} (syst, 2017Wa10), which makes one-proton decay mode almost forbidden. 
E$2020Ho06 mention that the observation of ions decaying only with one half-life suggests that these events correspond to the ground-state of {+73}Sr. 
J$assigned by 2020Ho06, based on (5/2-) for {+73}Rb IAS, deduced from comparison of measured proton branching ratios from {+73}Rb IAS to the g.s. and the first 2+ state of {+72}Kr, and the predicted values from the GCC calculations, with oblate deformation for the {+72}Kr core. With the g.s. J|p=1/2- for the g.s. of {+73}Br, mirror nucleus of {+73}Sr, 2020Ho06 discussed the violation of mirror-symmetry breaking in the case of the two mirror nuclides. Note that 26.9-keV, (5/2-) level in {+73}Br is the likely the analog of {+73}Sr g.s., thus reversing the order of the ground and the first excited states in the two mirror nuclei. 
T$from 2020Ho06, decay curve for correlated implants of {+73}Sr ions and their subsequent decays, by rejected the latter if another implantation event occurred within 10 half-lives of {+73}Sr. The analysis was done using logarithmic-binning method for low statistics. Other: 23.5 ms {I18} from direct fitting of the data (2020Ho06). The half-life from 2020Ho06 can be compared with 24.3 ms {I53} and 28 ms {I+5-4} measured by 2019Si33 (Phys. Rev. C 100, 044311), the first value from least-squares fit to ({+73}Sr implants)|b decay curve, and the second value from logarithmic binning method for 42 observed (implants)|b events. Weighted average of all the four values, deduced by compiler, is 23.6 ms {I14}, whereas weighted average of the two values obtained from the logarithmic binning method is 23.6 ms {I15}. 
$Two strong proton peaks are observed from beta-delayed proton decay: {+73}Sr |) {+73}Rb |) {+72}Kr. The most intense peak was E(p)=3.80 MeV {I2}, identified as emanating from {+73}Rb isobaric-analog state (IAS) to feed the ground state of {+72}Kr. From observation of ten (709.7|g)p-coin events, the second strong peak was attributed to the branching of {+73}Rb, IAS decays to the first 2+ state in {+72}Kr. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2014He29 from events in the whole DSSD and a |b-energy threshold of 3 MeV. Low statistics prevented use of decay curve method, instead method proposed by 1984Sc13 was used. Authors mention (ref. 18 in paper) that this value is in agreement with a recent (unpublished) measurement at RIKEN 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
%ECP$other: 6.5 {I33} (1995Bl23). 
T$from decay curves of |b|g and p|g spectra (2003Hu01), weighted average of 87 ms 3 and 89 ms 5. Others: 80 ms {I+400-40} (2001Ki13,2002Fa13,2007WeZX), 71 ms {I+71-24} (1995Bl23). 
J$from mirror analogy between T=1/2 ground states of {+75}Sr and {+75}Rb, the latter assigned (3/2-) in high-spin measurements. See also review article by 2008Se10 about Ft values of the T=1/2 mirror |b transitions 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$multiscaling of |b particles (2004De24). Other: 8.9 s {I3} (1992Gr09). Weighted average of the two values is 7.94 s {I22} with reduced |h{+2}=11; unweighted average is 8.4 s {I5} 
$The shape of g.s. of {+76}Sr nuclide was investigated through TAGS measurement of {+76}Sr decay and derived |b-strength function, the latter compared to the calculated shapes for oblate and prolate deformation of the g.s. of {+76}Sr. The agreement was obtained only for the prolate shape (2004Na16 and 2013Pe13, also 2005Ru07, 2004De24, 2004Na17 and 2003Ma69). From this study estimated |b{-2}=0.4 (2004Na16), with a definite prolate shape. This result is in agreement with |b{-2}=0.45 {I3} in 2012Le05, deduced from lifetime measurement of the first 2+ state in {+76}Sr 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Deformation parameter |b{-2}=0.45 {I3} (2012Le05) 
J$262.3|g E2, |DJ=2 to 0+ 
T$mean lifetime |t=278 ps {I36} from weighted average of |t=250 ps {I44} (2020Ll01) and |t=296 ps {I36} (2012Le05, T{-1/2} of 205 ps {I25} from T{-1/2}=207 ps {I+16-14} at forward angles and 203 ps {I+18-16} at backward angles). The values are from {+9}Be({+76}Rb,{+76}Sr|g),({+80}Y,{+76}Sr|g) using Doppler-shift attenuation method (DSAM). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted averaged mean lifetime |t=278 ps {I36} from |t=250 ps {I44} (2020Ll01) and |t=296 ps {I36} (2012Le05, T{-1/2} of 205 ps {I25} from T{-1/2}=207 ps {I+16-14} at forward angles and T{-1/2}=203 ps {I+18-16} at backward angles); from DSAM in both the studies 
$Deduced |b{-2}=0.45 {I3} from T{-1/2} (2012Le05) 
$Inclusive population=51% {I12} (2012Le05) 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: S
level_comment:
%ECP$other: <0.25 (1976Ha29) 
$Evaluated rms charge radius <r{+2}>{+1/2}=2.2569 fm {I44} (2013An02) 
$Evaluated |d<r{+2}>({+88}Sr,{+77}Sr)=0.253 fm{+2} {I12} (2013An02) 
T$from 1983Li11, |g decay curve. Other: 9.0 s {I10} (1976Ha29) 
J$measured hyperfine splitting using laser spectroscopy (1992Li11). Parity from possible |n5/2[422] configuration 
MOMM1,MOME2$fast ion-beam collinear LASER spectroscopy (1992Li11,1992Li29). Q=+1.40 {I11} in 1992Li11 is re-evaluated to +1.27 {I5} in 2016St14 
$|D<r{+2}>({+88}Sr-{+77}Sr)=0.248 fm{+2} {I12}, charge radius=4.2544 fm {i22} (1992Li11) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$ <r{+2}>{+1/2}=4.255 fm {I4} (2004An14 evaluation) 
T$ weighted average of 168 s {I12} (1997Mu02, timing of 46.8|g), 159 s {I8} (1992Gr09, timing of 103.5|g) and 150 s {I18} (1982Li17, timing of x-rays and |g-rays). Other: 170 s {I30} (quoted by 1992Gr09 from H. Grawe et al., 1981 Ann Rep HMI B373, 89 (1982)). Note that 1982Li17 quote an uncertainty of 18 s in the abstract but 12 s in the text with no decay plot shown. 
$ CALCULATION OF T1/2: 2008Mi17 
Isotope shift and mean-square radius determined (1990Bu12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ average of 188 ps {I+17-15} at forward angles and 195 ps {I+21-19} at backward angles. Statistical and systematic uncertainties are included 
$ Deduced |b{-2}=0.40 {I3} from T{-1/2} (2012Le03) 
$ Inclusive population=51% {I12} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from mean lifetime |t=286 ps {I20} (2020Ll01) for fully stripped ion, determined using a 2D |h{+2}-minimization procedure, as described in 2016Mi04 (Phys. Rev. C 93, 024318). Systematic uncertainties are included. Previous measured values were |t=276 ps {I39} by 2012Le05 (Phys. Rev. C 85, 0041303(R)) from another experiment at NSCL, and 224 ps {I27} by 1982Li08 (Phys. Rev. Lett. 49, 308). 2020Ll01 give a weighted average of the three results as |t=266 ps {I15} or T{-1/2}=184 ps {I10}. Compiler's note: in the weighted averaging of the three results, uncertainty of 15 ps in |t given by 2020Ll01 is the internal uncertainty, whereas external uncertainty is 20 ps, which should preferably be used. 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius=4.2586 fm {I39} (2013An02) 
$Evaluated |d<r{+2}>({+79}Sr,{+88}Sr)=0.266 fm{+2} {I6} (2013An02) 
T$weighted av of 1.97 min {I12} (1982De36), 2.30 min {I10} (1981Li12), 2.31 min {I6} (1981FrZY). Others: 1.90 min {I15} (1980De13); 2.5 min {I2} (1973BoXS); 4.4 min {I2} (1972La32); 8.1 min {I3} (1971Bi10); 1.9 min {I5} (1971Do01) 
J$from hyperfine structure study (1987Bu11,1990Bu12). Negative parity is supported by agreement of measured |m with that calculated for 3/2[301] neutron state 
MOMM1,MOME2$collinear fast-beam LASER spectroscopy (1990Bu12, 1990Li28,1987Bu11); 2002Ma09 reanalyzed data and Q=+0.73 {I6} of 1990Bu12 and obtained 0.708 {I6} (4% theoretical uncertainty not included). This result further re-evaluated by 2013StZZ 
|D<r{+2}>({+88}Sr-{+79}Sr)=0.261 fm{+2} {I6} (1990Bu12) 
|D<r{+2}>({+79}Sr-{+84}Sr)=0.144 fm{+2} {I6} (1987Ea01) 
Evaluation of charge radii data: 1992Ne09, 1992Li24 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
T$weighted average of 20 ns {I1} (n|g(t),1990Ch07); 23 ns {I2} (|b|g(t),1992Mu12); 23 ns {I2} (|g|g(t) in in-beam,1992Mu12). Other: 23 ns {I4} (n|g(t),1973BoXS) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: PS
level_comment:
T$from RDDS and DSAM. Weighted average of 1.04 ps {I14} (1990He04), and 0.87 ps {I+40-21} (DSAM,2007Ka13) and 2.8 ps {I14} (RDDS,1990Ca16) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: PS
level_comment:
T$from DSAM and RDDS. Weighted average of 0.83 ps {I21} (DSAM,1990He04), 0.91 ps {I21} (RDDS,1990He04), 0.69 ps {I+17-12} (DSAM), and 2.1 ps {I7} (RDDS,1990Ca16) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: PS
level_comment:
T$other: 0.97 ps {I14} (RDDS), 0.97 ps {I7} (DSAM) (1990He04); effective half-lives, not corrected for feedings 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$<r{+2}>{+1/2}=4.255 fm {I5} (2004An14) 
T$from 1973Br32 
|D<r{+2}>({+88}Sr-{+80}Sr)=0.243 fm{+2} {I33} (1990Bu12,1988Si06); 0.249 fm{+2} {I6} (deduced by 1988Si06 from data of 1987Ea01,1986Ea01); 0.294 fm{+2} {I21} or 0.227 fm{+2} {I20} (1987An02,1986An39) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from RDM (1990He04). Others: 37 ps {I3} (1982Li08), 40 ps {I7} (1982HiZT), 44 ps {I6} (1974No08), 30 ps {I10} (1982De36,|g|g(t) in {+80}Y |e decay). 2001Ra27 evaluation also adopts 34.2 ps {I12} 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 4+ 
T$from RDM and DSA method (1990He04). Other: 1.2 ps {I4} or 1.3 ps +22-13 (DSA,1987Da05) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: PS
level_comment:
T$ from average of 0.28 ps {I3} (DSAM,2000Wi01), 0.22 ps {I3} (DSA,1987Da05) and 0.33 ps {I4} (RDM and DSA method,1990He04) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
T$ from DSAM in {+28}Si,|a2p|g) (2000Wi01). Others: {0.24 ps} {I3} (DSA,1987Da05), (0.17 ps {I6} (1987Da05), <0.340 ps {I14} (DSAM,1990He04,uncorrected for side-feeding) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: 0.079 ps {I17} (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: 0.35 ps {I6} (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (14+)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: 0.037 ps {I11} (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (13-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: 0.16 ps {I+3-6} (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: <0.27 ps (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: 0.013 ps {I13} (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (17-)
level_lifetime_unit: PS
level_comment:
T$from DSAM in {+28}Si,|a2p|g) (2000Wi01). Other: <0.31 ps (DSA,1987Da05) in {+54}Fe({+29}Si,n2p|g),{+58}Ni({+24}Mg,2p|g) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
T$others: 0.17 ps {I6} (1987Da05, with full feeding correction); 0.340 ps {I14} (1990He04, DSA method with no correction for feeding cascades) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
J J=1/2 from hyperfine structure (1987Bu11). |p=- from comparison of |m with Schmidt diagram. 
T weighted average of 24.5 min {I20} (1971Do01), 26.0 min {I15} (1973Br32), 22.15 min {I22} (1980Ho28), and 25 min {I2} (1982De36). 
MOMM1 from 2019StZV, 1990Bu12 (collinear fast-beam laser spectroscopy); uncertainty arising from hfs anomaly included; {+87}Sr standard. Others: +0.542 {I4} (1987An02, atomic beam with laser fluorescence spectroscopy), +0.5434 {I8} (1990Li28 - fast ion-beam collinear laser spectroscopy). 
<r{+2}>{+1/2}(charge)=4.255 fm {I3} (2013An02). 
|D<r{+2}>({+80}Sr,{+81}Sr)=-0.011 fm{+2} {I9} (1996Li25; statistical uncertainty only). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: US
level_comment:
J E2, |D|p=no 79|g to 1/2- g.s.; 3/2,5/2 from excit in (|a,xn|g). 
T weighted average of 0.326 |ms {I55} and 0.370 |ms {I85} from {+81}Y |e decay, 0.55 |ms {I10} from {+78}Kr(|a,n|g) (1983Ar16) and 0.44 |ms {I10} (1989Wu01 - {+58}Ni({+28}Si,4pn|g)). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: US
level_comment:
J absence of |g to 1/2- g.s.; level energy systematics for N=43 nuclei favor (7/2+). 
T from |g(t) (1989Wu01 - produced from {+58}Ni({+28}Si,4pn|g)). Other: >1.5 |ms from (|a,xn|g). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_comment:
J 217|g from (5/2+) has mult. (E2) and linear polarization which excludes a J to J-1 transition; 5/2 unlikely from 119|g excit. |p: B(E1)(W.u.) more typical in this mass region than B(M1)(W.u.) for 119|g to 1/2-. 
T from pulsed beam measurements in (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J M1+E2, |DJ=1, 43|g to (7/2+) 89; J(132 level)>J(79 level) from 43|g excit. 
T from pulsed beam measurements in (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J excit 155|g requires this level to have one of the lowest spins occurring in {+81}Sr; not J=1/2 or 5/2 from 155|g(|q) in (|a,n|g); M1+E2 |g from 5/2-; D(+Q) 155|g to 1/2- g.s.. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
J D, |DJ=0, 124|g to (5/2)- 79; |g to (7/2+); allowed |e decay (log| {Ift}|?5.6) from (5/2+) {+81}Y. 
T from (|a,n|g). Other: <3.5 ns ({+81}Y |e decay). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
J from (|a,xn|g). (M1+E2) |g to (3/2+); anisotropy 115|g too large for a 3/2 to 3/2 transition; excit 115|g favors J=5/2. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J D |g to (5/2+); band assignment. 
T from observation of prompt 408|g-511|g coin and time resolution in {+81}Y |e decay. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J E2 961|g to (13/2+) 905; band assignment. 
T from (|a,n|g). Other: |>0.55 ps from ({+29}Si,p2n|g). 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: PS
level_comment:
J D intraband 306|g to (21/2+) 3407; likely J=23/2 member of (|n 5/2[422])(|p g{-9/2}){+2} band (1996Sm07). 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_uncertain: ?
level_comment:
E differs from that in ({+31}P,p2n|g) because, in that reaction, a 1016.0|g placed in the |g cascade, and here instead a 1060|g adopted from ({+30}Si,|a2pn|g) to deexcite this level. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J stretched E2 1074|g to (19/2-) 2904; from (HI,xn|g) systematics, deexciting |g probably feeds a level with lesser or equal spin. 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_uncertain: ?
level_comment:
E differs from that in ({+31}P,p2n|g) because, in that reaction, instead of 1016.0|g from 21/2- and 1058.0 from 25/2- in the |g cascade 1060|g and 1134.8|g (instead of from 29/2- for the latter) are adopted here, respectively, from ({+30}Si,|a2pn|g) 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
XREF: the |g which deexcites this level was seen in ({+29}Si,p2n|g), but was placed differently there. 
Sharp cut off of cascade I|g above this level in ({+30}Si,|a2pn|g) suggests that this level may be isomeric (1996Sm07). 


level_energy_unit: KEV
level_spin_parity: (29/2-)
level_uncertain: ?
level_comment:
E differs from that in ({+31}P,p2n|g) because |g cascade from 33/2- to 29/2- to 25/2- to 21/2- of that reaction assigned from (29/2-) to (25/2-) to (21/2-) to (17/2-) in the adopted dataset. 


level_energy_unit: KEV
level_comment:
J$31/2+ proposed by authors in 1996Sm07. 1181.2|g to (27/2+), DCO ratio: 0.76 {I14} (1996Sm07) - possibly contaminated by nearby transition. 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_comment:
XREF: deexcitation |g also present in ({+29}Si, p2n|g) but level energy differs due to wrongly placed |g lower in cascade. 


level_energy_unit: KEV
level_spin_parity: (39/2-)
level_comment:
E=9333 in ({+31}P,p2n|g) for J=39/2 band member because, in that reaction, the 1488|g (which separates the 1581|g and the 1402|g) was not included in the relevant |g cascade. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (27/2+)
level_lifetime_unit: PS
level_comment:
T from |t=0.31 ps {I5}: unweighted average of |t=0.35 ps {I10} and |t=0.26 ps {I7} (from 646|g and 1039|g, respectively). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T weighted average of 0.326 |ms {I55} (1982De36 - from |t=470 ns {I80}) and 0.370 |ms {I85} (1985Li12,1981Li12). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T from 1981Li12. Based on electronic time resolution (408|g and 511|g observed to be in prompt coincidence). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
T$from T{-1/2}=25.36 d {I3} (HPGe, 2009Pi02; Ge(Li) 1987Ho06), 25.34 d {I2} (ic, 2009Pi02), 25.34 d {I5} (1987Ju02). Others: 25.55 d {I15} (1978Gr17) 25.0 d {i4} (1958Sa20), 25.5 d {I5} (1953Kr10). 
|D<r{+2}>({+88}Sr-{+82}Sr)=0.179 fm{+2} {I24} (1990Bu12,1988Si06); 0.182 fm{+2} {I6} (1988Si06, deduced from data of 1987Ea01,1986Ea01); 0.169 fm{+2} {I13} or 0.220 fm{+2} {I15} (1987An02,1986An39). 
|D<r{+2}>({+83}Sr-{+82}Sr)=-0.017 fm{+2} {i7} (1996Li25) 
|D<r{+2}>({+82}Sr-{+81}Sr)=-0.053 fm{+2} {i8} (1996Li25) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$g=+0.44 {I19} (2014Ku10) measured using the transient-field (tf) technique in inverse kinematics with perturbed angular correlation method in {+12}C({+78}Kr,2|a|g). Other g=0.47 {I7} (2008Yu04,2010Fa08); values of g factors were read from figure 1 of 2008Yu04 
J L(p,t)=2 
T$other: 10.7 ps {I21} from 1996Jo05 in {+58}Ni({+27}Al,3p), while studying {+82}Y 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$g=+0.53 {I39} (2014Ku10) measured using the transient-field (tf) technique in inverse kinematics with perturbed angular correlation method in {+12}C({+78}Kr,2|a|g). Other g=0.46 {I8} (2008Yu04,2010Fa08); values of g factors were read from figure 1 of 2008Yu04 
J stretched E2 cascade indicated by angular distribution and polarization in ({+16}O,2n2p|g). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
MOMM1$From g=0.58 {I8} (2008Yu04,2010Fa08) measured by transient-magnetic field ion-implantation perturbed angular distribution method in {+58}Ni({+28}Si,4p|g); values of g factors were read from figure 1 of 2008Yu04 
J stretched E2 cascade indicated by angular distribution and polarization in ({+16}O,2n2p|g). 
T other value: 0.9 ps {I1} from RDM, {+70}Ge({+16}O,2n2p|g). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J from |g(|q) and polarization in ({+16}O,2n2p|g) indicating E1 transition to 4+. 
MOMM1$From g-factor=+0.3 {i4} (1989Ku11), transient-field method. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J tentative assignment from the seven linking gammas which connect this state to 4+, 6+, 5-, 6-, and 7- states. The four DCO ratios measured in ({+29}Si,2pn|g) are consistent with this assignment. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J |g to (5)- shows |DJ=1 angular distribution, ({+16}O,2p2n|g); |g to 4- is consistent with stretched E2. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
MOMM1$From g=0.82 {I12} (2008Yu04,2010Fa08) measured by transient-magnetic field ion-implantation perturbed angular distribution method in {+58}Ni({+28}Si,4p|g); values of g factors were read from figure 1 of 2008Yu04 
J stretched E2 |g to 6+ state. 
g-factor=+0.7 {I1} (1989Ku11) transient-field method. T{-1/2}=0.76 ps {I14} (1989Ku11). 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
J from |g(|q) in ({+16}O,2n2p|g), consistent with DCO ratios of decay |g's obtained in ({+29}Si,2pn|g). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J stretched E2 cascade indicated by angular distribution and polarization in ({+16}O,2n2p|g). 
MOMM1$From g-factor=+0.7 {i1} (1989Ku11), transient-field method. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J stretched E2 cascade indicated by angular distribution and polarization in ({+16}O,2n2p|g). 
MOMM1$From g-factor=+1.1 {i5} (1989Ku11), transient-field method. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$|?18 from 2003Le08. Others: J|?(19) from 1995Sm08. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
J$J=7/2 from collinear fast-beam spectroscopy (1987Bu11,1990Li28). |p from E3 259|g from 1/2-. 
T$from 1982Gr07. Others: 32.4 h {I2} (1964Do02), 31.4 h (1972Ch13), 32.9 h (1961Ku08). 
MOMM1$from collinear fast-beam LASER spectroscopy (1990Bu12, 2011StZZ), relative to |m=-1.092828 {I65} for {+87}Sr, Others: |m=-0.8286 {I12}, (CFBLS, 1990Li28); |m=-0.8298 {I3} (LASER induced fluorescence spectroscopy in thermal atomic beam, 1987An02). 
MOME2$from collinear fast-beam LASER spectroscopy (1990Bu12, 2011StZZ), relative to Q=0.335 {I20} for {+87}Sr. Others: Q=0.823 {I50} (LASER induced fluorescence spectroscopy in thermal atomic beam, 1987An02); Q=+0.761 {I12} (re-evaluation of 1990Bu12 result with theoretical calculations by 2002Ma09). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$from pulsed beam measurement reported as a private communication in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g). 
J$M1 35.5|g to 7/2+, L({+3}He,|a)=L(d,t)=4, DWBA analysis of |s(|q) in (d,t). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$J=1/2 from collinear fast-beam laser spectroscopy (1987Bu11,1990Li28), |p from L({+3}He,|a)=1. 
T$from 1972Tu07. 
MOMM1$from collinear fast-beam LASER spectroscopy (1990Bh03, 2011StZZ), relative to |m=-1.09282 {I65} for {+87}Sr. Other: |m=0.5809 {I12} (CFBLS, 1990Li28). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$log| {Ift}=5.7 from 3/2- parent; log| {Ift}=5.2 from 9/2+ to 1371-keV level and 618|g between these levels suggests J|p(754)=(5/2-) and J|p(1371)=(7/2+). 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$M1+E2 859|g to 9/2+; |g(|q) and excitation function in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g). 
T$given as a range with 1.0 ps < T{-1/2} < 2.1 ps 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$E2 875|g to 9/2+, excitation function in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g), band assignment 
T$other: 2.6 ps {I10} from DSAM in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g). 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J$M1+E2 680|g to 11/2+, excitation function in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g). However, (13/2-) is assigned in {+68}Zn({+19}F,p3n|g). 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.7 ps {I2} from RDDM in {+74}Ge({+12}C,3n|g) and 1.0 ps {I3} from DSAM in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g). 
J$E2 1077|g to 13/2+, band assignment 


level_energy_unit: KEV
level_spin_parity: 23/2+
level_lifetime_unit: PS
level_comment:
J$M1+E2 528|g to 21/2+, excitation function in {+80}Kr(|a,n|g),{+82}Kr(|a,3n|g). 
T$from RDDM in {+74}Ge({+12}C,3n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (41/2)
level_comment:
J$|?(41/2) estimated (1995Ba26,1995La21,2003Le08) (within one unit of spin) from depopulation into the highest spin states (45/2+,39/2-) of normal-deformed bands in {+83}Sr (see 1995La21 and 1992WiZU for normal high-spin states above 23/2). 
E$13.0 MeV {I15} (1995La21) 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


level_energy_unit: KEV
level_energy_info: ;OFF=X+928
level_comment:
E$doublet; one component corresponds the E=952- or 963-keV levels in the Adopted Levels. No corresponding level for the L=1 component in any data set. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (41/2)
level_comment:
J$|?(41/2) estimated (1995Ba26,1995La21,2003Le08) (within one unit of spin) from depopulation into the highest spin states (45/2+,39/2-) of normal-deformed bands in {+83}Sr (1995La21,1992WiZU) 
E$x=13.0 MeV {I15} (1995La21) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$given as a range with 1.0 ps < T{-1/2} < 2.1 ps 
J$|g(|q) gives 7/2+ or 11/2+, |g(|q) for 858.5|g in 1980Ar02 favors J to J-1 transition and excitation function in 1980Ek03 favors the higher spin. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
T$reported as 31.87 h {I116} (stat) {I42} (syst); compiler combines uncertainties in quadrature. Value is weighted average of 30.94 h {I140} (stat) {I29} (syst) and 33.88 h {I206} (stat) {I54} (syst), both from 762.7|g(t) (2021Ha10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$<r{+2}>{+1/2}=4.2364 fm {I17} (2004An14 evaluation). 
T$>7.3|*10{+13} y (1952Fr23, double |b decay). Other:>10{+17} y probably for neutrino-less double |b/|e decay, preliminary result from H.J. Kim, presented at 16th Int. Conf. on Supersymmetry and the Unification of Fundamental Interactions, Seoul, June 2008 Communication with the author on April 16, 2009 revealed that the analysis of this experiment is still in progress. 
J$ L(p,t)=0 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$from g-factor=+0.419 {i47} measured in Coulomb ex. (1988Ku01). See also 2005St24 compilation 
T$weighted average of 3.19 ps 35 (1982De05) and 4.2 ps +28-14 (1980Ek03). Other: 6.2 ps 21 (1982De05 value reanalyzed by 1994Ch28) 2001Ra27 evaluation gives adopted T{-1/2}=3.2 ps 5 and B(E2)(|^)=0.289 {I44}. 
J$E2 |g to 0+; L(p,t)=2 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 to 2+. L(p,t)=(4) is consistent 
T$unweighted average of 1.73 ps 21 (1982De05) and 0.97 ps 28 (1980Ek03). Other: 4.16 ps 14 (1982De05 value reanalyzed by 1994Ch28) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(p,t)=L(d,d')=3. Configuration=(g{-9/2},f{-5/2}{+-1}) or (g{-9/2},p{-3/2}{+-1}) (1982De05). 
$B(E3)(|^)=0.043 {I18} (2002Ki06 evaluation, data from 1973Re01). Deduced B(E3)(W.u.)=15 {I6} 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$2+ or 4+ from 1145|g(|q) indicating |DJ=0 or 2; J=4 favored by excitation function and band assignment 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: PS
level_comment:
MOMM1$ transient-field integral perturbed-angular correlation in {+74}Ge({+12}C,2n|g) (1989Ku11) 
J$ |DJ=1, DIPOLE G TO 4+; L(p,t)=(5) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 4+ 
T$weighted average of 1.04 ps 21 (1982De05), 0.97 ps 28 (1994Ch28). Other: 2.6 ps 4 from (1982BrZO). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 6+ 
MOMM1$ from g factor=-0.15 {I7} from spin precession in polarized hyperfine fields of a tilted multi-foil target (1981Br20). Other: -0.8 {I16} from g=-0.1 {I2} (1989Ku11, transient-field integral perturbed-angular correlation in {+74}Ge({+12}C,2n|g)) See also 2005St24 compilation 
J$Configuration=(|ng{-9/2 }){+-2} {-8+}~#(g.s. of {+86}Sr core) (1982De05). 
T$from 1982De05. Others: 163 ps 3 (1982De05 value reanalyzed by 1994Ch28), 170 ps 7 (1982BrZO) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: PS
level_comment:
MOMM1$ transient-field integral perturbed-angular correlation in {+74}Ge({+12}C,2n|g) (1989Ku11) 
J$|DJ=2, E2 |g to (5-); |DJ=1 |g to 6+ 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$configuration=|pg{-9/2}{=2}{-8+} ~# {+82}Kr core (1982De05). 
MOMM1$ transient-field integral perturbed-angular correlation in {+74}Ge({+12}C,2n|g) (1989Ku11) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 8+. configuration=(|ng{-9/2}){+-2}{-8+}~#(2+ of {+86}Sr core) (1982De05) 
MOMM1$ transient-field integral perturbed-angular correlation in {+74}Ge({+12}C,2n|g) (1989Ku11) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (7-). Configuration=|ng{-9/2}{+-2} ~# (3-) (1982De05) 
MOMM1$ transient-field integral perturbed-angular correlation in {+74}Ge({+12}C,2n|g) (1989Ku11) 


level_energy_unit: KEV
level_spin_parity: 20+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g to 18+; band member 
T$0.14 ps 4, effective half-life from 1994Ch28, not corrected for side feeding 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
$g-factor is an average for the feeding states, except for the 3488, 7- state 
J$spin from |g(|q) and excitation function 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
G$ from spin precession in polarized hyperfine fields of a tilted multi-foil target (1981Br20). Other: -0.1 {I2} (1989Ku11) 
T$ other: 170 ps {I7} (1982BrZO), 162.9 ps 35 (1982De05 value reanalyzed by 1994Ch28) 
$Configuration: |n(g{-9/2}{+-2})(8+) ~# (g.s. of {+86}Sr core) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$a Comparison of measured B(E2) values for {+84}Sr, {+86}Sr and {+88}Sr in 1963Al31 and those deduced from adopted lifetimes shows (see table below) that values in 1963Al31 are consistently too high 
$ ------------------------------------------------- 
$ Nuclide B(E2) (1963Al31) B(E2) (from adopted T{-1/2}) 
$ {+84}Sr 0.34 {I10} 0.17 {I+6-5} 
$ {+86}Sr 0.19 {I6} 0.12 
$ {+88}Sr 0.20 {I7} 0.09 
$ ------------------------------------------------- 


level_energy_unit: KEV
level_comment:
$Enhancement=1.3 
$ d|s/d|W=2.27 at 10|' 
L$(4) is supported by 1973Ba56 and (5) by 1973Mo11 Adopted value requires L=5. !!! check the adopted 


level_energy_unit: KEV
level_comment:
J$2017Du08 point out that (7+) proposed in literature is inconsistent with transition to J=3,4 level at 2735 keV 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: D
level_comment:
$RMS charge radius (<r{+2}>){+1/2}=4.2304 fm {I21} (2013An02 evaluation) 
J$spin from hyperfine structure using collinear laser spectroscopy (1990Bu12,1987Bu11); parity from L({+3}He,|a)=L(d,p)=4; L({+3}He,n)=0 from 9/2+ target. 
MOMM1,MOME2$collinear fast beam laser spectroscopy (1990Bu12, also 1987Bu11). Q value=+0.29 {I3} (1990Bu12) recalculated by 2002Ma09. Other: |m=-1.0005 {I3}, Q=+0.323 {I20} (1987An02,atomic beam with laser fluorescence spectroscopy). 
T$note that in DDEP evaluation (2004BeZR), uncertainty in the value from 1962Sa12 is quoted incorrectly as 2.7 d, instead of 0.27 d 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J$spin from hyperfine structure using collinear laser spectroscopy (1990Bu12,1987Bu11); parity from L({+3}He,|a)=L(d,p)=1 
MOMM1$collinear fast beam laser spectroscopy (1990Bu12). Other: +0.599 {I2} (1987An02,atomic beam with laser fluorescence spectroscopy) 
E$240 {I3} in (d,t) and 234 {I8} in ({+3}He,|a) are associated with 238.66 level on the basis of L=1 transfer in both the reactions. It is possible, however, that these groups also contain small contribution of known 231.6, (7/2+) level. 
T$weighted average of 67.55 min {I7} (1982Gr07), 67.66 min {I7} (1970LyZZ), 67.66 min {I7} (1972Em01: 4|p ionization chambers), 67.92 min {I25} (1972Em01: solid well-type scintillation counters), and 67.3 min {I3} (1971Bu08). Others: 69.5 min {I5} (1966Ka24,1964Gu08), 70 min (1940Du05) 
%IT,%EC$from normalization of decay schemes of {+85}Sr IT decay (67.63 min) and {+85}Sr |e decay (67.63 min); see these datasets for details 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,t)=L(d,p)=L({+3}He,|a)=1; 1/2- not allowed by RUL(E2) for 215.9|g to 5/2- 
T$weighted average of 0.14 ps {I+6-3} from (p,n|g) and 0.11 ps {I5} from ({+3}He,|a|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to 7/2+; M1+E2 |g to 9/2+ and (7/2)+; L({+3}He,|a)=4,(3) for a 1230 {I15} group 
E$1110 in ({+3}He,n) with L=0 probably corresponds to this level. Uncertainty in ({+3}He,n) is |?100 keV 
T other: 0.18 ps {I+9-5} from (p,n|g). 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
J$|g to 9/2+, (5/2)+ and (5/2-). L(d,p)=2 gives 5/2+ if the level seen in (d,p) corresponds to 1555.3 level 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
J$log| {Ift}=6.9 (log| {If{+1u}t}=7.6) from (1/2)-. L(d,p)=2 gives (3/2)+ if the level seen in (d,p) corresponds to 1559.3 level 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2,11/2+)
level_comment:
J$log| {Ift}=7.0 (log| {If{+1u}t}=7.8) from (9/2)+; |g to 7/2+; L(p,t)=(2) for 1919.68 and/or 1928 levels 


level_energy_unit: KEV
level_spin_parity: (17/2)-
level_lifetime_unit: NS
level_comment:
J$|DJ=2, E2 |g to 13/2-; band member 
T$Doppler shift method, weighted average of 1.1 ns {I4} in (|a,n|g) and 2.4 ns {I12} in ({+12}C,3n|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 67.55 min {I7} (1982Gr07), 67.66 min {I7} (1970LyZZ), 67.66 min {I7} (1972Em01: 4|p ionization chambers), 67.92 min {I25} (1972Em01: solid well-type scintillation counters), and 67.3 min {I3} (1971Bu08). Others: 69.5 min {I5} (1966Ka24,1964Gu08), 70 min (1940Du05) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: NS
level_comment:
T$from 1981Bu02. Other: >0.76 ns (1983Lu05, seems incorrectly assigned to 2102, 17/2- level and 991|g) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.15 ps {I21} (1981Bu02) and 2.56 ps {I28} (1983Lu05). Other: 0.62 ps {I21} (1988ZhZV) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
T$from weighted average of 2.22 ps {I28} (1981Bu02) and 2.36 ps {I21} (1983Lu05), 1.7 ps {I6} (1988ZhZV. Lifetime not corrected for possible side feedings. 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
J$proposed J=25/2 (1988ZhZW) is inconsistent with mult=M1+E2 for 312|g to 21/2+ 
T$from 1983Lu05, not corrected for possible side feedings. 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
J$13/2-,17/2- from |g(|q,pol) (1980Ek03) if J(2102)=13/2-; excitation function favors 17/2 (1977Ar04). 
T$Doppler-shift analysis (1977Ar04) 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_lifetime_unit: PS
level_comment:
J$13/2+,17/2+ from |g(|q,pol) (1980Ek03); excitation function favors 17/2 (1977Ar04). 
T$at 18 MeV. Other: <0.1 ns (1977Ar04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=0.3646 keV {I8}. g|G{-n}=1.3 eV {I2}, |G{-|g}=235 meV {I20}, g|G{-n}|G{-|g}/|G=199 meV {I20} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T$reported as 68.24 m {I84} (stat) {I11} (syst); compiler combines uncertainties in quadrature. Value is weighted average of 68.69 m {I160} (stat) {I11} (syst), 67.83 m {I148} (stat) {I11} (syst), and 68.26 m {I132} (stat) {I12} (syst), all from combined 151.2|g(t) (2021Ha10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$optical spectroscopy (1931Fr01) 
$RMS charge radius <r{+2}>{+1/2}=4.2307 fm {I20} (2013An02) 
|D<r{+2}>({+86}Sr-{+88}Sr)=+0.050 fm{+2} {I8} (1990Bu12) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|b{-2}(p,p')=0.158 {I16} 
J$L(p,t)=2; E2 |g to 0+ 
$T{-1/2}: weighted average of values from Coulomb excitation; 1.39 ps {I7} (DSAM, 2012Ku14), 1.46 ps {I15} (DSAM, 1988Ku01), B(E2)=0.118 {I16} (1964Sy01), 0.087 {I26} (1963Al31). Other: B(E2)=1.121 {I5} in (e,e') (1992Ki20) 
MOMM1$transient field integral perturbed angular correlations. Other: +0.55 {I10} (transient field, 1998Ku01). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=2 
$T{-1/2}: from B(E2) and adopted branching ratio 
MOMM1$transient field integral perturbed angular correlations 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$T{-1/2}: from DSAM in Coul. ex. (2012Ku14) 
J$L(p,t)=L(e,e')=4; |DJ=2, E2 |g to 2+ 
MOMM1$transient field integral perturbed angular correlations 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2 
$T{-1/2}: from B(E2) and branching ratio as quoted here. T{-1/2}=182 fs {I20} if the level decays by g.s. transition only 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$Differential perturbed angular distribution of |g rays (1978Ha52). Others: -1.944 {I32} ( Stroboscopic method, 1975Ma02), 1.93 {I12} (|g(|q,H,t), 1973Ha36) 
J$L(e,e')=8; L(p,t)=(8). L(p,d)=4 from 9/2+ 
$T{-1/2}: from |g(t). Weighted average of 0.40 |ms {I4} (1997Is13), 0.457 |ms {I7} (1978Ha52), 0.41 |ms {I5} (1975Ma02) and 0.46 |ms {I3} (1971Is04). Unweighted average is 0.432 |ms {I16} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(e,e')=L(p,t)=3. L(p,|a)=4 from 1/2-. L(p,d)=4+1 from 9/2+ 
E$doublet in (p,d) from L=4+1; other component with J=0 to 9, |p=+ 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(e,e')=L(p,t)=5. Also L=4+1 in (p,d) from 9/2+. In {+82}Se({+9}Be,5n|g) J|p is assigned (6-) based on an unlikely [M2+E3] multipolarity assigned for 826.02|g (2014Li25). 
E$doublet in (p,d) from L=4+1; other component with J=0 to 9, |p=+ 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E$doublet indicated by L(d,t)=3+4 from 9/2+; other component with negative parity and J=1 to 8 
J$L(e,e')=6 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$log| {Ift}=6.1 (log| {If{+1u}t}=7.0) from 4-. M1,E2 |g to 5-. |p=- from the L(p,d)=1 component from 9/2+ 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_comment:
J$log| {Ift}=7.4 (log| {If{+1u}t}=8.3) from 4-. |g to 5-. |p=+ from the L(p,d)=4 component from 9/2+ 


level_energy_unit: KEV
level_comment:
E,J$doublet from L(p,d)=(4+1) from 9/2+; one with J=0 to 9 with positive parity, other with J=3 to 6 with negative parity 


level_energy_unit: KEV
level_spin_parity: 3,4(+)
level_comment:
J$log| {Ift}=6.9 (log| {If{+1u}t}=6.3) from 4-. |g to 2+. 
E$doublet in (p,d) from L=4+1 from 9/2+; one with J=0 to 9 with positive parity, other with J=3 to 6 with negative parity 


level_energy_unit: KEV
level_comment:
E,J$doublet from L(p,d)=4+1 from 9/2+; one with J=0 to 9 with positive parity, other with J=3 to 6 with negative parity 


level_energy_unit: KEV
level_comment:
E,J$doublet from L(p,d)=(4+3) from 9/2+; one with J=0 to 9 with positive parity, other with J=1 to 8 with negative parity 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: FS
level_comment:
J$from systematics of g.s. widths (see (|g,|g')) 
$T{-1/2}: from |G=0.10 eV {I5} measured in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$This level was treated as tentative in 1970Ra06, but several other reactions confirm its existence 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from |g(t). Weighted average of 0.40 |ms {I4} (1997Is13), 0.457 |ms {I7} (1978Ha52), 0.41 |ms {I5} (1975Ma02) and 0.46 |ms {I3} (1971Is04). 
G$from transient field technique in heavy-ion induced reactions (1978Ha52). Others: -0.243 {I4} from |g(|q,H,t) in (|a,2n|g) (1975Ma02); -0.241 {I15} from |g(|q,H,t) in (p,p2n|g) (1973Ha36). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$Others: 0.118 {I16} (1964Sy01), 0.087 {I26} (1963Al31). 
$g factor=+0.323 from Target III: with iron as ferromagnetic material (243 MeV) (2012Ku14). 
G$Others: +0.273 {I50} (1988Ku01). 
T$1.46 ps {i15} (1988Ku01). 


level_energy_unit: KEV
level_comment:
L$1974Ve08 assign p1/2 transfer on the basis of a dip in the incomplete |s(|q) distribution (not shown in the paper) at 65|' 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Half-life and decay mode of the isomer are from Adopted Levels of {+86}Sr in the ENSDF database (Nov 2014 update) 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
$Proposed configuration=|p(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+1}g{-9/2}{+0} )~#|n(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+2}g{-9/2}{+9}) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_comment:
$Proposed configuration=|p(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+1} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
$Proposed configuration=|p(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+1} )~#|n(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+2}g{-9/2}{+9}) (35.8% with JUN45 interaction), and |p(p{-3/2}{+4}f{-5/2}{+4}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (10.2% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 13+
level_comment:
$Proposed configuration=|p(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+1} )~#|n(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+2}g{-9/2}{+9}) (43.6% with JUN45 interaction), and |p(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+1})~# |n(p{-3/2}{+4}f{-5/2}{+5}p{-1/2}{+2}g{-9/2}{+9}) (40.0% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 14+
level_comment:
$Proposed configuration=|p(p{-3/2}{+4}f{-5/2}{+4}p{-1/2}{+0}g{-9/2}{+2} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (30.8% with JUN45 interaction), and |p(p{-3/2}{+4}f{-5/2}{+4}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (45.8% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 15+
level_comment:
$Proposed configuration=|p(p{-3/2}{+4}f{-5/2}{+4}p{-1/2}{+0}g{-9/2}{+2} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (26.5% with JUN45 interaction), and |p(p{-3/2}{+4}f{-5/2}{+4}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (45.5% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 16+
level_comment:
$Proposed configuration=|p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (48.8% with JUN45 interaction), and |p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (36.1% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 17+
level_comment:
$Proposed configuration=|p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (48.7% with JUN45 interaction), and |p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (37.2% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 18+
level_comment:
$Proposed configuration=|p(p{-3/2}{+2}f{-5/2}{+5}p{-1/2}{+1}g{-9/2}{+2} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (30.2% with JUN45 interaction), and |p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (39.0% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 19+
level_comment:
$Proposed configuration=|p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2} )~#|n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (45.4% with JUN45 interaction), and |p(p{-3/2}{+3}f{-5/2}{+5}p{-1/2}{+0}g{-9/2}{+2})~# |n(p{-3/2}{+4}f{-5/2}{+6}p{-1/2}{+2}g{-9/2}{+8}) (30.7% with jj44b interaction) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from DSAM (2017Du08). Other values: <146 fs (SDM), 87 fs {I19} (DSAM), 189 fs {I+35-32} (effective half-life, DSAM) (2017Du08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
T$from DSAM (2017Du08). Other value: 130 fs {I+24-25} (DSAM,effective half-life) (2017Du08). Literature value=25 fs {I12} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$assignment of (4) in literature is in disagreement 
T$from DSAM (2017Du08). Other (effective) half-life from DSAM: 261 fs {I+32-31} as averaged of 270 fs {I+42-40} and 248 fs {I+53-46}, (2017Du08) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: FS
level_comment:
T$average of 200 fs {I+44-42}, 119 fs {I+80-69} and 132 fs {I+46-44} (2017Du08), all the three values are effective half-lives 


level_energy_unit: KEV
level_spin_parity: 7-,6,5
level_comment:
J$assignment of (4+) in literature is in disagreement. 370.4|g from 3925, (4)+ level makes 7- and 6- less likely (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 4+,3,2+
level_lifetime_unit: FS
level_comment:
E$only one level at 3645.0 was assigned in literature with 144.5, 1163.0, 1415.2, 1790.9, and 2567.97 |g rays from this level. 2017Du08 propose two separate levels near this energy 
J$assignment of (3-) in literature 
T$average of 148 fs {I+80-67} and 152 fs {I+45-41} (2017Du08), both are effective half-lives 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$from paramagnetic resonance (1976Fu06) and laser spectroscopy (1987An02,1987Bu11,1990Li28). |p from L(d,p)=4. Configuration is g{-9/2} 
MOMM1 from 2011StZZ evaluation as quoted in 1990Bu12 and based on data of 1972Ol01; other: -1.0936030 {I13} cited in 2011StZZ, -1.089274 {I7} from 1974Sa25, -1.0924 {I7} (1987An02) 
MOME2 from 2006Sa21; calculated by combining the B/Q value from RCC theory and the measured B value from the 4D{+2}{-5/2} state of singly ionized {+87}Sr from Barwood, et al., Phys. Rev. A 67, 013402 (2003). other: +0.323b {I20} (2004Yu05), +0.327b {I24} (2002Ma09), +0.335 {I20} (1977He21), +0.36 (1962Bu14) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
J$from laser spectrometry (1987An02,1987Bu11,1990Li28) and |p from L(d,p)=1. 
T from IT decay. 
%EC,%IT from {+87m}Sr |e+|b+ decay. 
MOMM1 from 2011StZZ evaluation and based on data of 1990Bu12; other: +0.787 {I9} (1987An02). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J L=1 in (pol d,p) (1986Bu14) and |g(|q) and linear polarization measurements in (|a,n|g) (1981Ek01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J L=3 in ({+3}He,|a), E2 |g to J{+|p}=1/2- level. 
T other: 0.25 ps {I+23-9} from (p,n|g), but this value is considered by evaluator as not probable because of a large B(E2)(W.u.) for 865 |g. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J E2 |g to J{+|p}=9/2+; from |g yield function in (|a,n|g) it follows that 1740 |g is part of the yrast cascade. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J Coupled-channel analysis in ({+3}He,|a) and |g linear polarization and angular distribution in (|a,n|g) give 7/2+. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
J$L(d,p)=0, but a |g to 5/2- level suggests an interesting configuration allowing a competitive M2 transtion. 
T$from (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
J M1 |g to 5/2+; |g(|q), linear polarization, and excitation function in (|a,n|g) favor J{+|p}=(7/2)+. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E weighted average of 2631 {I15} from (p,n), 2633 {I20} from (p,d), 2630 {I15} from (d,|a), and 2634 {I 8} from (p,p') 
J L=1 in (p,d). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: PS
level_comment:
J M1 |g to 5/2+; |g(|q), linear polarization, and excitation function in (|a,n|g) favor J{+|p}=(3/2)+. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E weighted average of 3133 {I8} from (p,p') and 3140 {I10} from ({+3}He,|a). 
J L=3 in ({+3}He,|a). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J L=2 in (d,p); isobaric analog to one of the members of the unresolved 11960 doublet in {+87}Y with J{+|p}=(3/2)+ and (5/2)+ while the other part of this doublet is assigned to the 3166 level [J{+|p}=(5/2)+]. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J L=0 from 9/2+ in (p,p'). 
E weighted average of 3278 {I8} from (p,p') and 3260 {I10} from ({+3}He,|a). 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J L=(5) from 9/2+ in (p,p'), (D) |g to 17/2. From |g yield functions in (|a,n|g), it follows that 142 |g is part of the yrast cascade. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J L=3 in ({+3}He,|a) and |g to 1/2-. Fed by a primary from 1/2+ in (n,|g), so there is a conflict as the 5/2- assignment would require the primary to have mult=M2 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J L=3 from 1/2- in (d,|a) and the 3118|g branching to 1/2- is too strong to be M2 so 5/2+ can be ruled out. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E weighted average of 3528 {I8} from (p,p') and 3510 {I10} from ({+3}He,|a). 
J L=3 in ({+3}He,|a). 


level_energy_unit: KEV
level_spin_parity: (21/2)
level_comment:
J (D) |g to 19/2, from |g yield functions in (|a,n|g) it follows that 220 |g is part of the yrast cascade. 


level_energy_unit: KEV
level_spin_parity: (23/2)
level_comment:
J presumably dipole |g to 21/2+; from |g yield functions in (|a,n|g) it follows that 829 |g is part of the yrast cascade. 


level_energy_unit: KEV
level_comment:
J$Both 4462.6 and 4485.0 levels possibly correspond to the 4470 level in XREF=|g and therefore no J assignment is adopted 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_comment:
E$The high spin of this level makes it unlikely to be the 6074.44 level populated in (n,|g) 
J$From DCO ratio and cascade placement 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E isobaric analog to {+87}Rb gs (J{+|p}=3/2-). 
J L=1 in ({+3}He,|a), isobaric analog to {+87}Rb gs (J{+|p}=3/2-). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E isobaric analog to the 403 level in {+87}Rb. 
J L=3 in ({+3}He,|a); isobaric analog to the 403 level in {+87}Rb (J{+|p}=5/2-). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E isobaric analog to the 845 level in {+87}Rb. 
J L=1 in ({+3}He,|a); isobaric analog to the 845 level in {+87}Rb (J{+|p}=1/2-). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T weighted average of 2.80 h {I3} (1951Hy24), 2.83 h {I2} (1965Bo42), 2.805 h {I1} (1968Go30, with reported uncertainty divided by 3 to give 1|s value), 2.83 h {I5} (1969Zo04), 2.793 h {I9} (1970Le07), 2.81 h {I2} (1970LyZZ), 2.97 h {I10} (1971Bu08), 2.83 h {I1} (1971Ja24 and 1971Oo01), 2.81 h {I2} (1972Em01), 2.795 h {I13} (1982Gr07), 2.827 h {I1} (1992An19), and 2.811 h {I27} (1997We13). The two most precise values, 2.805 {I1} and 2.827 {I1}, differ by about 20 |s and the reduced-|h{+2} value for the average is 28. Although the 2.805 value is somewhat old, it is from a reliable lab and measured by T{-1/2} experts, who have provided metrology standards for several nuclei. The next most precise value is 2.793 {I9}, which supports this lower value. With the two uncertainties of 0.001 increased to 0.003, the reduced-|h{++2} is 3.7 and the Limitation of Relative Statistical Weight method (1985ZiZY,1992Ra09) expands the final uncertainty to include the most precise value; and this uncertainty of 0.012 is adopted. 
T a change in this half-life has been measured to be 0.8% {I5} for a change in temperature from 293 K to 77 K (2001Al23). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: PS
level_comment:
J |g excitation function suggests J=(5/2) (1981Ek01). 
T from measurement at E{-|a}=11 Mev; at E{-|a}=14 MeV 1981Ek01 measure 0.19 ps 4. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
J |g(|q) and polarization for 1050|g give 5/2+,7/2+, 9/2+ and J |g excitation function suggests J |> 9/2 (1981Ek01). 


level_energy_unit: KEV
level_spin_parity: (23/2)
level_comment:
J presumably dipole |g to 21/2+; from |g yield functions in it follows that 829 |g is part of the yrast cascade. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E neutron-capture state. E is from adopted S(n). The authors give E=8428.16 {I 17} 
J from s-wave capture on a 0+ target 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$This may correspond to the 2676 level with 3/2+, the 2679 level with 1/2-,3/2-, or the 2682 level with (3/2)+ in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
L weak assignment only by 1989Fo01; however, confirmed by 1977Bl08. 
J Definitive assignment in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 17/2(+)
level_comment:
J$Assigned as (17/2) in Adopted Levels. Although the authors take the 1946|g as a stretched quadrupole, the large uncertainty for the DCO ratio does not exclude dipole character 


level_energy_unit: KEV
level_spin_parity: 23/2(-)
level_comment:
$Configuration=|p(f{-5/2}{+-1}g{-9/2})~#|ng{-9/2}{+-1} 
J$As the dipole character of the 830|g only establishes |DJ, this is assigned as (23/2) in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 1826|g to 0+, L(p,t)=2 
T$weighted average of 0.155 ps {I8} from (|g,|g') and 0.152 ps {I12} from DSAM in Coul. Ex. Others: 0.159 ps {I13} from B(E2) in (e,e') and 0.185 ps {I14} from DSAM in (n,n'|g) 
MOMM1$from transient field technique in Coul. Ex. (2012Ku14) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=3 
T$weighted average of 0.78 ps {I5} from B(E3) in (e,e') and 0.67 ps {I3} from DSAM in Coul. Ex. Other: 0.67 ps {I+19-13} from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(t,p)=2 
T$weighted average of 21 fs {I7} from DSAM in (n,n'|g), 13 fs {I3} from (|g,|g'), and 20 fs {I11} from B(E2)=0.013 {I7} in (e,e') 


level_energy_unit: KEV
level_comment:
T$170 ps {I60} based on DSAM in (n,n'|g) of 1006|g which has only a tentative assignment to this level 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: FS
level_comment:
J$L(d,p)=2(+0) on 9/2+ target. 1970Ra10 deduced L(t,p)=2+6 for an unresolved doublet. Also 1987Li02 concluded this level to be a doublet from the large L(d,p)=2 strength. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 0+ g.s. 
E$Candidate for 2+ x 3- two-phonon state (2002Pi08) 
T$Other: <6 fs from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6-)
level_uncertain: ?
level_comment:
J$from (e,e'). Form factor is significantly different from that expected for a 1- level, suggesting this level is distinct from the 4742.5 level. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
J$(E2) 5170|g to 0+ 
E$measured F(|t) of 5169.9 depopulating transition is sufficiently different from F(|t)'s of |g's depopulating the 5168.8 level to suggest that the 5170.1 level is distinct. 


level_energy_unit: KEV
level_spin_parity: (2,3)
level_lifetime_unit: FS
level_comment:
J$1095|g to 1, 1687|g to (3+), 2588|g to 3- 
$Possibly identical to the 5321.36 level, however, depopulating transitions observed by (n,|g), E=thermal and (n,n'|g) are different. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: FS
level_uncertain: ?
level_comment:
E$possibly identical to 6011.15 level, however, depopulating transitions observed in (n,n'|g) are different. 
J$2058|g to 5-, 2856|g to 0+. 


level_energy_unit: KEV
level_comment:
J$L(t,p)=(3) 
E$depopulating transitions observed in (n,n'|g) and (n,|g), E=thermal for levels at |?6125 keV are different, suggesting two closely spaced levels. 


level_energy_unit: KEV
level_spin_parity: (12)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$(D) 320|g to (11) 
T$effective half-life from DSAM in {+80}Se({+11}B,p2n|g); feeding corrections have not been incorporated. 


level_energy_unit: KEV
level_spin_parity: (12)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$effective half-life from DSAM in {+80}Se({+11}B,p2n|g); feeding corrections have not been incorporated. 
J$(D) 561|g to (11) 


level_energy_unit: KEV
level_spin_parity: (16)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$effective half-life from DSAM in {+80}Se({+11}B,p2n|g); feeding corrections have not been incorporated. 
J$D 762|g to (15) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|b-transition to g.s. has first-unique forbidden shape (1969Ly01,1955Th01,1951Bu02). 
$I|b=65.5% (1969Ly01), 76% {I4} from I|g(1836|g)/|SI|b=0.231 {I11} (1969Ra05). 


level_energy_unit: KEV
level_comment:
L$2 from 1974Se10 and 1968Co20. 
$d|s/d|W{-max}=432 |mb/sr for L=(0) component and 1283 for L=2 component (1987Li02). 


level_energy_unit: KEV
level_comment:
L$2 from 1974Se10 and 1968Co20. 
$d|s/d|W{-max}=2030 |mb/sr for L=(0) component and 2790 for L=2 component (1987Li02). 


