# LEVEL

level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
E,J$1999Po09 suggest s{-1/2} orbital to lie below h{-11/2} orbital. J|p is from favored |a decay from (1/2+) g.s. of {+169}Ir 
T$from a fit to |a-decay time distribution using the Maximum-Likelihood method (2012Th13). Other: 2.61 s {I+14-13} reported in 2005Sc22, from the same laboratory and with mostly the same authors as 2012Th13 
T$2.61 s {I+14-13} from 2005Sc22 is not confirmed by a subsequent study (d. O'Donnell et al., (to be published); D.T. Joss, R.D. Page and D. O'Donnell, (private communication to C. Reich, June, 2011)) by some of the same authors as 2005Sc22 did not confirm this result. 
$E|a=5556 keV {I6} from {+165}Re g.s. decay correlated with 6019|a and 6688|a from decays of {+169}Ir g.s. and {+173}Au g.s., respectively (2012Th13) 
$%|a from 2012Th13; %|e+%|b{++} is assumed to be 100-%|a, but no information on level structure is avaiable from this decay mode 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$%|a from 2012Th13; %|e+%|b{++} is assumed to be 100-%|a, but no information on level structure is avaiable from this decay mode. Other %|a: 13 {I3} (1981Ho10) 
E$from 1999Po09, deduced from |a-decay energies in the |a-decay chain of the ground and isomeric states of {+177}Tl|){+173}Au|){+169}Ir|){+165}Re. 2021Ko07 give 28 keV {I22} 
J$from favored |a decay from (11/2-) isomer of {+169}Ir, and systematics (1999Po09). 
T$from a least-squares fit to |a-decay time distribution in 2012Th13. Others: 2.37 s {I+10-9} (2005Sc22), 1.9 s {I3} (1996Pa01), 2.2 s {I4} (1984Sc06,1978Sc26), and 2.4 s {I6} (1981Ho10). Weighted average of all the values, except the one from 2005Sc22, is 1.76 s {I6} 
$E|a=5520 keV {I6} (2012Th13) correlated with |a peaks from parent and grandparent decays; 5518 {I5} (1996Pa01); 5506 {I10} (1981Ho10) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
%A Both |a decay and |e decay have been observed, but the branching has not been measured. Based on a comparison of excitation function data for the various nuclides they studied, 1978Sc26 estimate 30|<%|a({+166}Re)|<100. However, based on T{-1/2} and assuming r{-0}({+162}Ta)=1.562 {I3} (unweighted average of r{-0}=1.567 {I24} ({+160}Hf), 1.556 {I16} ({+162}W), 1.563 {I11} ({+164}W) from 1998Ak04), %|a<24 for HF>1 if a g.s. to g.s. transition is assumed and %|a<6 if Q(|a)=5510 {I70} from 2003Au03; further, if this is an unhindered decay, HF<4 would imply %|a>6 or >1.35 respectively, for these two Q(|a) possibilities. The evaluator adopts an upper limit of 24 for %|a, implying %|e+%|b{++}>76 since p decay is not expected (S(p)>0 from 2003Au03). The much higher estimate of %|a in 1978Sc26 might Be unreliable due to the similarity of both E|a and T{-1/2} for the {+166}Re and {+165}Re decays. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (3-)
level_comment:
E this may or may not Be the g.s.; if it is, y=0. However, a comparison of E|a from low-spin {+170}Ir |a decay with Q(|a) from systematics (2003Au03) suggests that it is not. 
J |a decay is possibly unhindered (HF=4.4 {I18}) from (3-) low-spin isomer in {+170}Ir. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E an alternative value of 69+x is possible because the order of the 53|g and the 69|g has not been established. 
|p probably opposite to |p(0+x) level based on (E1) 53|g to 0.0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E 70+x 14 from energy difference between possible |a group feeding this level and the 6121|a feeding the 0+x level. 
|p probably same as |p(0+x) level based on (M1) 75|g to 0.0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E 117+x 12 from energy difference between possible |a group feeding this level and the 6121|a feeding the 0+x level. 
|p probably opposite to |p(0+x) level based on (E1) 122|g to 0.0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E 174+x 14 from energy difference between possible |a group feeding this level and the 6121|a feeding the 0+x level. 
|p probably opposite to |p(0+x) level based on (E1) 175|g to 0.0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3-)
level_comment:
E this may or may not be the g.s.; comparison of E|a with Q(|a) from systematics (2003Au03) suggests that it is not. 
J |a decay possibly unhindered from low-spin (3-) {+170}Ir. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E an alternative value of 69+x is possible because the order of the 53|g and the 69|g could not be established (2007Ha45). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
Other E: 70+x 14 from energy difference between |a group feeding this level and the possible 6121|a feeding the 0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
Other E: 119+x 12 from energy difference between |a group feeding this level and the possible 6121|a feeding the 0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
Other E: 174+x 14 from energy difference between |a group feeding this level and the possible 6121|a feeding the 0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_lifetime_unit: PS
level_comment:
T$weighted averaged mean lifetime |t=480 ps {I80} (2016Li13) deduced from |t=440 ps {I90} from RDDS for 331|g and 590 ps {I150} from RDDS for 398|g 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9-)
level_lifetime_unit: PS
level_comment:
T$from RDDS for 121|g 
E$compiler notes feeding transition intensity exceeds depopulating transition intensity 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
$%|a: |a decay observed, but no gammas associated with |e+|b{++} decay could be identified (1992Me10). 
J$tentative configuration=|p1/2[411], analogous to {+161},{+163},{+165}Re. 
T$from 5015|a decay curve (1992Me10). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$%|a: from 1992Me10, assuming the 137|g and 221|g observed following |e decay of this level represent total |e decay intensity. Supported by T{-1/2}=5.7 s {I14} (1992Me10) from |g({+167}W)(t), which suggests that {+167}Re |e decay occurs predominantly from the 5.9-s activity 
E,J$from systematics, and possible configuration=|p9/2[514], analogous to g.s. of {+169}Re 
T$weighted average of 6.2 s {I5} (from 5263|a(t), 1992Me10), 6.6 s {I15} (1984Sc06, originally assigned to isomeric {+168}Re) and 5.5 s {I5} (1978Ca11, originally assigned to {+168}Re). Others: 5.6 s {I19} from 137|g(t) and 5.8 s {I22} following |e decay of {+167}Re (1992Me10) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
J$tentative configuration=|p11/2[505], analogous to {+169}Re (1992Sc16). Unhindered |a decay from (11/2-) {+171}Ir. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_lifetime_unit: S
level_comment:
E,J,T$from the Adopted Levels 
J$tentative configuration=|p9/2[514], analogous to {+169}Re (1992Sc16) 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: S
level_comment:
%|a: deduced from I|a/I|g(199.3|g in {+168}W) and |e decay scheme for {+168}Re (1992Me10). 
E the observed |e decay (4.4 s) branch to 6+ 1042 level in {+168}W suggests that the high-spin isomer of {+168}Re is the ground state. 
J M1+E2 162|g from (8+) 162; strongest |e branches feed 6+ and 8+ states in {+168}W, but decay scheme may be incomplete. 2004GoZZ suggest a K|p=7+ configuration of (|p 9/2[514])+(|n 5/2[523]) but 1992Me10 suggest (|p 9/2[514])+(|n 3/2[521]), giving K|p=6+; the neighboring {+167}Hf, {+169}W and {+171}Os isotones are believed to have |n 5/2[523] ground states, compatible with the former configuration. 
T from 1992Me10 (363|g(t), 480|g(t) in |e decay to {+168}W daughter). Others: 1984Sc06, 1992Me10 (7.1 s {I25} from 4830|a(t)). 


level_energy_unit: KEV
level_comment:
J (2,3,4) if the (E1) 123|g deexcites J=(3) 349 level; highly tentative because order of the 123|g-136|g-90|g cascade is unestablished. 2004GoZZ suggest the K|p=2+ configuration (|p 9/2[514])-(|n 5/2[523]), but J|p=2+ is not compatible with a low-multipolarity two-step deexcitation to a (7+) g.s.. 


level_energy_unit: KEV
level_comment:
J (2,3,4) if 123|g is correctly placed. 2004GoZZ suggest a K|p=2+ configuration of (|p 9/2[514])-(|n 5/2[523]); however, higher than E2 multipolarity would then be required for one of the 2 cascade gammas to a (7+) g.s., inconsistent with measured I(K| x ray). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$from 2014An10. Other: (7+) in {+168}Re Adopted Levels in ENSDF database 
$Possible configuration=|p9/2-(h{-11/2} orbital)~#|n3/2-(f{-7/2} or h{-9/2} orbital) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7+)
level_comment:
J$from 2014An10. Other: (8+) in {+168}Re Adopted Levels in ENSDF database 
$Possible configuration=|p11/2-(h{-11/2} orbital)~#|n3/2-(f{-7/2} or h{-9/2} orbital) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: S
level_comment:
%A |?0.01 to |?0.001 (1992Me10). Both |a and |e+|b{++} decays were observed by 1992Me10. 
J possible 9/2[514] bandhead, analogous to {+171}Re; M1+E2 intraband 136|g from possible 11/2- 136 level. 
T weighted average of 6.6 s {I9} from 4700|a(t) (1992Me10) and 8.3 s {I3} from 101|g(t) (1992Me10). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E level energy held fixed in least-squares adjustment; x=175 {I13} (2012Au07). 
Identification: three-particle channels for {+27}Al and {+28}Si bombardment of {+144}Sm show activity in second reaction only (1984Sc06); observation of same activity with Re compound nucleus (1978Ca11) confirms formation from {+144}Sm({+28}Si,p2n). Assignment to isomer based on systematics (1984Sc06). 
%|a: estimated from extrapolation of log T{-1/2}(|a) versus log Q(|a). Only |a decay observed, but other decay modes apparently dominate. 
J fed in |a decay (HF=6 {I4}) from a possible 3/2[402] or 5/2[402] bandhead state (1992Sc16); parent state assigned (1/2+,3/2+) in 2001Ko44 based on favored |a decay from (1/2+,3/2+) {+177}Au g.s.. 
T weighted average of 12.9 s {I11} from 5050|a(t) in 1984Sc06 and 16.3 s {I8} from 5061|a(t) in 1992Me10 (the unweighted average is 14.6 s {I17}). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J |a decay from (11/2-) {+173}Ir state probably has HF=1.3 {I3}. However, |a decay parent state is suggested to be the 11/2[505] bandhead by 1992Sc16 (not the 11/2- 9/2[514] state assigned here). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J (D), |DJ=(1) 497|g to (11/2-) 136; intraband 98|g to (5/2-) 536. 
Only the 98-keV branch was reported in ({+28}Si,p2n|g). 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_comment:
J stretched D 281|g to (15/2+) 1343; intraband stretched D 405|g to (19/2-) 1218. Differs from (19/2) proposed in ({+28}Si,p2n|g). 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_comment:
J intraband stretched D 176|g to (17/2+) 1623; 215|g to (21/2-) 1584; D 859|g to (17/2-) 940. Differs from (21/2+) proposed in ({+28}Si,p2n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E x=175 {I13} (2012Au07). If Q(|a)=5716 {I10} (2012Wa38) is correct, E|a to this level implies x=170 {I11}; not consistent with the known E=215.9 {I4} J=(3/2) level. 


level_energy_unit: KEV
level_spin_parity: (35/2)
level_comment:
E adopted value differs because adopted order of 622|g-642|g cascade is the reverse of that shown here. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: S
level_comment:
J (E2) 210|g from (7+); (E2) 225|g from (3+). Possible configuration=(|p 1/2[541])+(|n 5/2[523]) (1992Me10). 
T from 1992Me10. Others: 8.0 s {I5} (1975St02), 9 s {I2} (1974Be59). 
%EC+%B+$%|a<0.01 from systematics of partial T{-1/2}(|a) vs Q(|a). 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
E$order of 20.2|g and 190.2|g not established; reverse ordering would result in a level at 190.2 keV. 
J (E1) |g from (7+); (E1) |g to (5+). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$order of 31.4|g and 193.5|g not established, reverse ordering would result in a level at 193.5 keV. 
J (M1) 31|g to (5+); absence of |a feeding from (7+) parent. 


level_energy_unit: KEV
level_spin_parity: (7+)
level_comment:
J |a from (7+) {+174}Ir to this level probably is a favored transition (hindrance factor=1.9 {I3}). Possible parent configuration=(|p 11/2[505])+(|n 3/2[521]) (1992Sc16). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J |a from (3+) {+174}Ir to this level probably is a favored transition (hindrance factor=1.7 {I11}). Possible parent configuration=(|p 11/2[505])-(|n 5/2[523]) (1992Sc16). 


level_energy_unit: KEV
level_spin_parity: (7+)
level_comment:
I(|g+ce) imbalance at the 210 level in 5316|a-|g coin implies that additional transition(s) feed the 210 level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9-)
level_comment:
E connection with known 210.5 level could not be established, but coincidences between transitions in band based on this level and the 210.5|g from the known 210.5 level imply x>210.5. 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES FIT. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (22-)
level_uncertain: ?
level_comment:
E$level not adopted; more extensive data from a subsequent ({+55}Mn,3n|g) study fail to confirm its existence. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: S
level_comment:
$|a decay not observed; HF|?4 if %|a|?3x10{+-5} and r{-0}({+167}Ta)=1.56 (based on r{-0} for {+166}W, {+168}W, {+166}Os, {+168}Os in 1998Ak04). 
J$see 0.0 level in {+171}W Adopted Levels. 
T$from 1987Ru05. Other value: <20 s (1987Sz03). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5+)
level_lifetime_unit: S
level_comment:
$%|a|<0.0003 (from |a syst) 
E$from theoretical calculations by 2005Wa25, (5+) is likely the ground state of {+172}Re. This level may correspond to 0+z or 0+u in high-spin structures 
J$favored |a transition from (5+) {+176}Ir parent; probable |e feeding of 4+ and 6+ levels in {+172}W 
T$from 1977Be66. Others (probably mixture of two activities): 23 s (1975St02), 30 s {I5} (1974Be59), 36 s {I12} (1973Be67), 48 s {I12} (1972Be89) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (2)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$%|a|<0.001 (from |a syst) 
E$0 {I100} (from systematics, 2012Au07) 
J$probable |e feeding of 2+ and 4+ levels in {+172}W, no |e feeding of levels in {+172}W with J>4 
T$from 1977Be66 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
%|a|?2.5|*10{+-5} from extrapolation of Q(|a) vs. T{-1/2}(|a) for {+163,165}Re. 
J$favored |a decay from {+177}Ir (J|p=(5/2-)). 5/2- 1/2[541] Nilsson state assigned, as for {+175}Re and {+177}Re. 
T$from 1986Sz05. Other value: 2 min (1973BeWB). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$fixed by |g-ray connections to g.s. band; deexcitation not observed, indicating level possibly isomeric. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (8-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
T$crude estimate (2012Gu14) from comparison of experimental |a(exp)=0.62 {I10}, theory |a=0.27 for 115.5|g, mult=E1, and the time window of 200 ns 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
T from 1984Sz07. Other values: 5.7 min, private communication from G.F. Blower, quoted by 1984Sz07; 4.6 min {I4} (1977Ha24); 4.4 min {I10} (1972Be89); and 5 min {I1} (1967Na17). 
J,CONF Systematics of the 1/2[541] Nilsson state in other odd-A rhenium isotopes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2-)
level_uncertain: S
level_comment:
E$Estimated value. State's excitation energy was unknown, but based on the basis of population intensity in {+161}Dy({+19}F,5n|g) (1992Ki06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 29/2+
level_comment:
Level not adopted, because both 272.1|g and 534.5|g depopulating this level are lower by about 20 keV than as observed in {+161}Dy({+19}F,5n|g) and resulted different level energy for the 29/2+ state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 31/2+
level_comment:
Level not adopted, because depopulating 280|g feeding to the 29/2+ state, whose energy level disagrees by about 20 keV with the {+161}Dy({+19}F,5n|g) dataset not adopted. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_uncertain: S
level_comment:
E$Estimated value. State's excitation energy was unknown, but based on the basis of population intensity in 1992Ki06. 


level_energy_unit: KEV
level_spin_parity: 29/2+
level_comment:
Level not adopted, because both 292.1|g and 554.8|g depopulating this level are higher by about 20 keV than as observed in {+156}Gd({+23}Na,4n|g) and resulted different level energy for the 29/2+ state. 


level_energy_unit: KEV
level_spin_parity: 33/2+
level_comment:
Level not adopted, because depopulating 592|g feeding to the 29/2+ state, whose energy level disagrees by about 20 keV with the {+156}Gd({+23}Na,4n|g) dataset not adopted. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: MIN
level_comment:
J log| {Ift}=6.7 to 109.1 (J|p=2+) level, log| {Ift}=6.2 to 349.3 (J|p=4+) level in {+176}Re |e decay. configuration: |p(1/2[541])~#|n1/2[521] with a band head at (3+). 
T weighted average of 5 min {I1} (1967Na17), 5.7 min {I8} (1970Go20), 5.6 min {I10} (1972Be89), and 5.2 min {I4} (1977Ha24). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5-)
level_comment:
J configuration: |p(1/2[541])~#|n(7/2[633]). Measured B(M1)/B(E2) value and calculation result are consistent with the configuration ({+16}O,5n|g). 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J configuration: |p(1/2[541])~#|n1/2[521] with a band head at 3+. Deduced experimental alignment is in good agreement with theory. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5-)
level_comment:
J configuration: |p(1/2[541])~#|n(7/2[633]). Measured B(M1)/B(E2) value and calculation result are consistent with the configuration. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
J 99.5|g E1 to (7+) state at 14.8+x. 
T From time spectrum, setting a gate on the 99.5|g in 1999Ca08. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
J$Preferred strong |e+|b{++} feeding to the 3/2-, 5/2- and 7/2- levels of the |n1/2[521] (p{-3/2}) band in the daughter nucleus {+177}W; J|p systematics; band assignment. 
T$From 196.9|g(t) following {+177}Re |e decay (1970Go20). Others: 16 min (1968Be43) and 17 min (1957Ha04). 
CONF$|p1/2[541] (h{-9/2}) Nilsson orbital (|a=+1/2). The band is strongly Coriolis mixed. Based on the observed decoupled character of the band, alignment properties and configuration systematics. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$An upper energy limit of about 40 keV is suggested (1986Wa32, 1983Ya08), since no transitions (photon and conversion electron) depopulating this level were observed in either in-beam or out-of-beam time region. 
J$J|p systematics; band assignment. 
T$No direct |g-ray decay from the bandhead has been observed. The value is a lower limit based on the applied |g|g coincidence window in 1995Ba67. 
CONF$|p9/2[514] (h{-11/2}) Nilsson orbital. The assignment is supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$84.7|g to 5/2-; J|p systematics; band assignment. 
T$From 1972Le04 in (HI,xn|g) 
CONF$|p5/2[402] (d{-5/2}) Nilsson orbital. The assignment is supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. The decrease of g{-K}-g{-R} values as the spin increases implies a significant mixing with the 7/2[404] (g{-7/2}) band. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$276.18|g M1(+E2) to the 5/2+ level; configuration assignment; J|p systematics. 
CONF$|p7/2[404] (g{-7/2}) Nilsson orbital. The assignment is supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. The increase of g{-K}-g{-R} values as the spin increases implies a significant mixing with the 5/2[402] (d{-5/2}) band. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$411.0|g to 5/2+, 457.0|g to (1/2-); J|p systematics; proposed configuration 
CONF$|p1/2[411] Nilsson configuration. Systematics in the region. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 15/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$872.37|g E1 to the 15/2- level, 1086.4|g E1 to the (13/2-) level. 
CONF$K|p=15/2+: probable |p{+3}(1/2[541],5/2[402],9/2[514]) or |p9/2[514]~#3- (octupole phonon) configuration. 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_comment:
J$1246.42|g to 13/2-; band assignment. 
CONF$At low spin it is associated with the |p1/2[541]~#|n(i{-13/2}){+2} configuration; at high spin (after band mixing) it evolves to |p1/2[541] (|a=+1/2) configuration. The assignment is supported by the observed in-band properties. See 1995Ba67 for details. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 17/2+
level_comment:
J$124.9|g M1+E2 to the 15/2+ level, 997.0|g E1 to the 15/2- level; band assignment. 
CONF$K|p=17/2+: probable |p{+3}(1/2[541],7/2[404],9/2[514]) or |p9/2[514]~#|n{+2}(1/2[521],7/2[633]) configuration. The assignment is supported by the observed in-band properties, such as alignment, g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (17/2-)
level_comment:
J$389.35|g to (15/2-), 623.69|g to (13/2-); band assignment. 
CONF$K|p=15/2-: probable |p9/2[514]~#|n{+2}(1/2[521],5/2[512]) configuration. 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_comment:
J$1128.09|g (E1) to 17/2-; band assignment. 
CONF$Probable |p1/2[660]~#|n(i{-13/2}){+2} configuration. The assignment is supported by the observed in-band properties. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_comment:
J$328.35|g from 25/2+; band assignment. 
CONF$Probable |p1/2[660]~#|n(i{-13/2}){+2} configuration. The assignment is supported by the observed in-band properties. See 1995Ba67 for details. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$149.05|g M1 to the 19/2+ level; band assignment. 
CONF$K|p=21/2+: configuration=|p9/2[514]~#|n{+2}(5/2[512],7/2[633]). The assignment is supported by the observed in-band properties, such as alignment, g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 23/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$134.7|g (M1) to the 21/2+ level; band assignment. 
CONF$K|p=23/2+: configuration=|p9/2[514]~#|n{+2}(7/2[514],7/2[633]). The assignment is supported by the observed in-band properties, such as alignment, g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (29/2+)
level_comment:
J$770.97|g (E2) to 25/2+, 589.18|g to 27/2+; configuration assignment 
CONF$K|p=(29/2+): probable configuration= |p{+3}(5/2[402],7/2[404],9/2[514])~#|n{+2}(1/2[521],7/2[633]). The assignment is supported by the observed in-band properties, such as alignment, g{-K}-g{-R} values, and systematics of similar structures in neighboring nuclei. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 33/2-
level_comment:
J$629.09|g E2 to the 29/2- level; band assignment. 
CONF$|p9/2[514]~#0+, where a pair of protons occupies the |p1/2[541] (h{-9/2}) orbital. See 1995Ba67 for details. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (37/2)
level_comment:
J$331.5|g to (35/2+); J|p systematics. The proposed in 1995Ba67 configuration implies K|p=37/2-, thus 587.3|g to (33/2+) requires Mult=M2 and, hence, a longer lifetime associated with this level 
CONF$K|p=(37/2-): |p{+3}(1/2[541],7/2[404],9/2[514])~#|n{+4}(1/2[521],5/2[512],7/2[514], 7/2[633]). The assignment is tentative. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (41/2)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$294.79|g to (39/2); band assignment. 
CONF$K|p=(41/2+): |p{+3}(5/2[402],7/2[404],9/2[514])~#|n{+4}(1/2[521],5/2[512],7/2[514], 7/2[633]). The assignment is tentative. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$An upper energy limit of about 40 keV is suggested (1986Wa32, 1983Ya08), since no transitions (photon and conversion electron) depopulating this level were observed in either in-beam or out-of-beam time region. 
T$No direct |g-ray decay from the bandhead has been observed. The value is a lower limit based on the applied coincidence window in 1995Ba67. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: MIN
level_comment:
This level not seen in (HI,xn) reactions. While an attempt was made in 1986Da13 to justify that this might be the band head for Band 1, this suggestion has not been adopted in later work. 
T from 1970Go20. Other values: 15 min (1957Ha04). Other: 1969Hu03. 
J log| {Ift}=6.4 to 106 (J|p=2+) level, log| {Ift}=6.2 to 343 (J|p=4+) level. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
|m: from on-line nuclear orientation (1992Bo39). 
J log| {Ift}=5.3 to 3/2+ 720; log| {If{+1u}t}<8.5 to 7/2+ 531 in {+179}Re |e decay. 
T from 1975Me20. Other values: 20 min {I4} (1971NaZV), 19.7 min {I5} (1966Ho16), 20 min {I5} (1960Ha18). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J (1/2-,3/2,5/2-) from 166|g to (1/2-) 118, 219|g to (5/2-) 65; proposed as J=3/2 member of 1/2[541] band by 1976Be62 in |e decay. 


level_energy_unit: KEV
level_spin_parity: (21/2)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
J stretched Q 296|g to (17/2-) 906. 
T from |g(t) (1976RoYE) in {+181}Ta(|a,6n|g). However, this isomer could not Be identified in ({+18}O,4n|g) study by 1989Ve08. 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J 727|g to (17/2-) 570; (Q) 1045|g to (11/2-) 253; suggested configuration=((|p 9/2[514])+(|n 7/2[514])-(|n 1/2[521])) (2002Th12). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J stretched (Q) 1098|g to (13/2-) 447; 640|g to (17/2-) 906. 
Possible J=17/2 member of band built on 1298 level; supported by implied moment of inertia for band. However, 1618 level could alternatively Be that member (2002Th12). 


level_energy_unit: KEV
level_comment:
J 1279|g to (3/2-) 284; fed in |e decay from 1/2-. Possible J|p=(3/2-), three-quasiparticle state, based on |g-ray decay pattern and |e population from 1/2- parent (1976Be62) in |e decay. 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J (Q) 1107|g to (15/2-) 665; D 608|g to (19/2-) 1164; D 866|g to (17/2-) 906. 
Suggested configuration=((|p 5/2[402])+(|n 7/2[514])+(|n 7/2[633])) (2002Th12), analogous to 1603 level in {+177}Ta; calculated E(level)=1753. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT. 
J band assignment. 
T from time spectrum measured with gates on 866|g and 1107|g below level, using pulsed beam (0.54 |ms on, 19.8 |ms off) in ({+11}B,5n|g). Other: >0.4 |ms in ({+18}O,4n|g). 
E x|<140 (estimate from ({+18}O,4n|g) based on absence of deexciting transition in prompt-delayed and delayed-delayed spectra (1989Ve08)). However, B(M2)(W.u.) exceeds RUL, unless x>240 keV. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_comment:
J based on absence of |g rays to levels below J|p=19/2- 1771 level in ({+18}O,4n|g). 
T level found to Be isomeric but T{-1/2} could not Be determined in ({+18}O,4n|g) (1989Ve08). 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J,CONF possible K|p=29/2+ five-quasiparticle state with configuration ((|p 5/2[402])+(|n 9/2[624])+(|n 7/2[514])+(|n 7/2[633])+(|n 1/2[521])) (2002Th12); deexcites to (27/2+) states. 
T from ({+11}B,5n|g). 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J,CONF possible K|p=31/2+ five-quasiparticle state with configuration ((|p 9/2[514])+(|n 9/2[624])+(|n 7/2[514])+(|n 5/2[512])+(|n 1/2[521])) (2002Th12); M1 117|g to (29/2+) 3160; 653|g to (33/2-) 2624. 
T from analysis of time-difference spectra in ({+11}B,5n|g). 


level_energy_unit: KEV
level_spin_parity: (47/2,49/2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J |g to (45/2+); a seven-quasiparticle state with configuration ((|p 11/2[505])+(|p 9/2[514])+(|p 7/2[404])+(|p 5/2[402])+(|p 1/2[541]) +(|n 7/2[514])+(|n 7/2[633]))47/2+ is expected near this energy (2002Th12). 
T from ({+18}O,4n|g) data, using pulsed and chopped beam, 0.11 ms on and 6.4 ms off (2002Th12) (see ({+11}B,5n|g) source data set). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (21/2,23/2)
level_comment:
J based on absence of |g rays feeding levels below the J|p=19/2- 1684+x level 
T level is isomeric, but T{-1/2} could not be determined. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
Level not adopted; deexcitation transitions not confirmed in later (HI,xn|g) study (viz., by 2002Th12). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
Possible J=17/2 member of band built on 1298 level; supported by implied moment of inertia for band. However, 1618 level could, alternatively, be that member. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (23/2+)
level_lifetime_unit: NS
level_comment:
T from time spectrum measured with gates on 866|g and 1107|g below level, using pulsed beam (0.54 |ms on, 19.8 |ms off) and the ({+11}B,5n|g) reaction. 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_comment:
Possible collective state in a band which accommodates the 565|g and the unplaced 502|g, 441|g and 377|g. 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
Possible five quasiparticle state with configuration ((|p 5/2[402])+(|n 9/2[624])+(|n 7/2[514])+(|n 7/2[633])+(|n 1/2[521])) 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
Possible five quasiparticle state with configuration ((|p 9/2[514])+(|n 9/2[624])+(|n 7/2[514])+(|n 5/2[512])+(|n 1/2[521])) 
T from analysis of time-difference spectra (2002Th12). 
An intensity imbalance of 65 {I23} exists for this level, but 2002Th12 indicate that an additional, unidentified branch exists to the K|p=(23/2+) band based on the 1772+x level. 


level_energy_unit: KEV
level_spin_parity: (45/2+)
level_comment:
Drawn as member of K|p=33/2- band in table II but neither parity nor energy nor discussion in text is consistent with that assignment. 


level_energy_unit: KEV
level_spin_parity: (47/2,49/2+)
level_lifetime_unit: MS
level_comment:
J |g to (45/2+); seven-quasiparticle state with configuration ((|p 11/2[505])+(|p 9/2[514])+(|p 7/2[404])+(|p 5/2[402])+(|p 1/2[541]) +(|n 7/2[514])+(|n 7/2[633]))47/2+ expected near this energy. However, J|p=47/2- or 49/2+ cannot be ruled out. 
T from ({+18}O,4n|g) data, using pulsed and chopped beam, 0.11 ms on and 6.4 ms off (2002Th12). 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: MIN
level_comment:
J$20.1|g E1 from 1+; direct feeding to J|p=2-, 1006 level in {+180}W. 
MOMM1$Static Nuclear Orientation with gamma detection (1992Bo39) 
T$weighted average of 2.42 min {I7} (1955Fi30), 2.45 min {I10} (1966Ho16), 2.6 min {I2} (1977Ha24), and 2.47 min {I3} (2009Fa01). 
$Configuration: |p5/2[402]|n7/2[514] 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J$directly fed in {+180}Os |e decay (J|p=0+). 
T$from |g|g(t) in {+180}Os |e decay. 
$Configuration: |p9/2[514]|n7/2[514] 


level_energy_unit: KEV
level_energy_info: ;OFF=X+284.2
level_spin_parity: 9-
level_lifetime_unit: NS
level_comment:
T$weighted average of 75.6 ns {I14} from |g|g(t) in {+176}Yb({+11}B,5n|g) and 73 ns {I3} from |g|g(t) in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). Other: 78 ns {I9} from |g(t) in {+176}Yb({+10}B,6n|g). 
J$assigned as (7+) in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). 
$Configuration: |p9/2[514]|n9/2[624] 


level_energy_unit: KEV
level_energy_info: ;OFF=X+1566.8
level_spin_parity: 13+
level_lifetime_unit: NS
level_comment:
T$weighted average of 74.2 ns {I14} from |g|g(t) in {+174}Yb({+11}B,5n|g) and 70 ns {I3} from |g|g(t) in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). Other: 67 ns {I9} from |g(t) in {+176}Yb({+10}B,6n|g). 
J$assigned as (11-) in {+170}Er({+14}N,4n|g),{+181}Ta(|a,5n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 21-
level_lifetime_unit: US
level_comment:
T$from beam pulse-|g(t) in {+174}Yb({+11}B,5n|g) using sum of 261|g, 264|g, 286|g, 457|g, and 678|g (2005El10). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
MOMM1$measured by radiative detection of NMR (1981Ha22). 
J$atomic beam, log| {Ift}=5.7 to 3/2+, rotational band member. 
T$from 1968Sc27. Other measurements: 18 h {I1} (1963Gr22) and 20.9 h {I19} (1969Hu03). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
J$9/2-[514] band head. log| {Ift}|?4.7 from 7/2- of {+181}Os. 
T$weighted average of 157 ns {I2} from {+176}Yb({+11}B,6n|g), 158 ns {I10} from {+181}Os |e decay (2.7 min) and 140 ns {I14} from (|a,4n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
MOMM1$differential perturbed angular correlations (1978Be67). 
J$599.6 keV level is directly fed by |e from 1/2- with log| {Ift}=7.02. It M1+E2 decays to the 356.7 keV state, which then E1 decays to the 118.0 keV state of J|p=7/2+. The cascade uniquely determines the J|p of 356.7 keV as 5/2- and J|p of 599.6 keV as 3/2- 
T$From {+176}Yb({+11}B,6n|g). Others: 96 {I4} ns from {+181}Os |e decay (105 min); 98 ns from p|g(t) (1971IsZQ) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: NS
level_comment:
T$From {+176}Yb({+11}B,6n|g). Others: 7 |ms {I1} from 2002Pf01; >2 |ms from (a,4n|g) (1974Si14). 1976Ne03 (a,4n|g) conclude that 45 ns < T{-1/2} < 11.4 |ms 
J$|g to 17/2- and 19/2- members of 9/2-[514] band 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_comment:
J$(D) to 15/2- and 17/2- states of 9/2-[514] band; K|p=17/2+ band head. Probable configuration=|p1/2[541]|n(9/2[624]7/2[514]). 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: US
level_comment:
T$weighted average of 12 |ms {I2} from {+176}Yb({+11}B,6n|g) and 11.4 |ms {I10} from (a,4n|g) 
J$M2 to 21/2- state. Band head of configuration |p9/2[514]|n(9/2[624]7/2[514]). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$M1 |g to 3/2-, fed by |e from 1/2- with log| {Ift}=3.7 
E$very low log| {Ift} value seems to indicate the configuration of the final level as 3 quasiparticle state with |n1/2[521]~#|n7/2[514]~#|p9/2[514]. 


level_energy_unit: KEV
level_spin_parity: (33/2)
level_comment:
J$from level diagram of 2000Pe18 and further clarification from the first author (C. J. Pearson). J|p=35/2+ is quoted in the |g-table of 2000Pe18. 


level_energy_unit: KEV
level_lifetime_unit: H
level_comment:
T$weighted average of 19.4 h {I23} (360|g(t)), 18.5 h {I21} (365|g(t)), 18.5 h {I24} (639|g(t)), and 20.2 h {I30} (953|g(t)) (2020Al21). 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: H
level_comment:
J$spin from nuclear orientation measurement (1983Sp05). Parity from log| {If{+1u}t}=8.3 to 5- 
T$weighted average of 64.3 {I5} (2011Bo01,from 1427.4|g-decay curve, source produced in W(p,xn) reaction), 64.3 h {I32} (2014Ma43, same group as 2011Bo11 but source produced in W(d,xn) reaction) and 64.0 h {I5} (1950Wi14). Other: 60 h (1958Ga24) 
MOMM1$from 1983Sp05, 1980Sp01 (NMR/rad. detection). Other: 2.84 {I6} from 1981Ha22 (NMR/rad. detection). 
MOME2$from 1983Ha49 (NMR-ON) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E$2012Au07 give x=60 {I100}, 1984Sl01 estimate it as |?50 keV based on singlet and triplet coupling of |p5/2[402] and |n9/2[624] 
T$from 470.3|g-decay curve, weighted average of 14.50 h {I45} (2014Ma43, source produced in W(d,xn) reaction) and 13.74 h {I48} (2011Bo01, source produced in W(p,xn) reaction). Others: 12.7 h {I2} (1950Wi14), 14 h (1950Dy61), 13 h (1959Ga15), 12.5 h {I5} (1963Ba37). Value of 12.7 h {I2} from 1950Wi14 has been adopted for the last 75 years or so, but recent measurements (2014Ma43 and 2011Bo01 report a higher value near 14 h). The value measured by 1963Ba37 from positron spectra recorded with a magnetic spectrometer agreed with that from 1950Wi14. However, the evaluator prefers to adopt a weighted average of the recent values from 2014Ma43 and 2011Bo01, since in 1950Wi14 and also perhaps in 1963Ba37, the value was deduced from a composite exponential decay curve of both the activities of {+182}Re, whereas in 2011Bo01 and 2014Ma43, T{-1/2} is deduced from decay curve for a 470.3|g ray which is emitted by the decay of the isomeric activity only, thus providing a better selectivity 
J$spin from atomic-beam magnetic resonance (1975Ru06,1978Ru04); parity from M1 |g from 1+ 
MOMM1$from 1987Oh10 (nuclear orientation). Other: 3.15 {I33} (1980Sp01) 
MOME2$from 1981Er01 (nuclear orientation), also 1985Ha41 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
J$E1 |g to (3)+; E1 |g from 1+; (E1+M2) |g to 2+ 
T$average of 570 ns {I30} (1973Bu08) and 600 ns {I30}(1969An13) 
MOMM1$from 1978Be67 (TDPAC) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (4-)
level_lifetime_unit: US
level_comment:
J$|g to 2+; long level half-life suggests mult(461|g) is M2 or higher 
T$from |g|g(t) in {+181}Ta(|a,3n|g),{+182}W(p,n|g) 1984Sl01 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1)-
level_comment:
J$M1 |g to 1-; log| {Ift}=7.1 from 0+. J|p=0- is considered as less likely for possible E2 admixture in 111.39|g to 1- 


level_energy_unit: KEV
level_spin_parity: (16-)
level_lifetime_unit: NS
level_comment:
$g factor measured by in-beam |g(|q,H,t) (TDPAD) technique 
J$(E2) |g to (14-); (M1) |g to (15-). Proposed (1988Ja02) as K|p=(16-) 4-quasiparticle state with configuration=|p9/2[514]~#|n[(9/2[624])(7/2[514])(7/2[503])] 
T$from |g|g(t) in (|a,3n|g) (1988Ja02). Other: 88 ns {I8} (1984Sl01) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$2012Au07 give 60 {I100} from |b decay data, 1984Sl01 estimate it as |?50 keV based on singlet and triplet coupling of |p5/2[402] and |n9/2[624] 


level_energy_unit: KEV
level_spin_parity: (16-)
level_lifetime_unit: NS
level_comment:
J$from 1988Ja02, based on proposed K|p=(16-) configuration=((|p 9/2[514])(|n 9/2[624])(|n 7/2[514])(|n 7/2[503])) (1988Ja02) which gives g factor=+0.29. 1984Sl01 suggest 15+ on the assumption of mult(345|g)=E1 and mult(647|g)=M2. But 15+ with a possible configuration given by 1988Ja02 gives g factor=+0.92 
T$from 1988Ja02. Other: 88 ns {I8} (1984Sl01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
MOMM1 From NMR on oriented nuclei; relative to {+186}Re. 
MOME2 Presumed to supersede 2.3 {I2} (1983Ha49). From static orientation with |g detection, relative to {+187}Re. 
J L({+3}He,d)=2; log| {Ift}=6.8 (log| {If{+1u}t}<8.5) to 7/2- 453 in {+183}W. 
T weighted average of 67.6 d {I25} (1958Fo47), 71 d {I3} (1958Ga17), and 71 d {I2} (1965Bl06). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
|m: from TDPAD; relative to {+19}F(197). 
Q: from TDPAC; relative to {+187}Re. 
J M2 496|g to 5/2+ g.s.; E1 236|g to 9/2+ 260. 
T weighted average of 7.7 ns {I5} (1960Ne03 in |e decay (13.0 h)) and 7.9 ns {I5} (1988BeYU). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J log| {Ift}=7.9 (log| {If{+1u}t}<8.5) from 1/2-; 1354|g to 5/2+ g.s.; (M1) 252|g to (1/2)+ 1102; band assignment. 


level_energy_unit: KEV
level_spin_parity: LE(1/2-,3/2,5/2+)
level_comment:
J 965|g to (5/2)- 599, 734|g to (3/2)- 829 imply J|p=(1/2-,3/2,5/2,7/2-); log| {Ift}=8.3 from 1/2-. 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J 1288|g to 13/2+ 639; 1492|g to 11/2+ 435; dominant configuration: |p(5/2[402]+9/2[514]+1/2[541])? from ({+11}B,4n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (21/2)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M4
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E x <75 keV to account for non-observance of transition feeding the 1937 level. The 1937 level has a 10 ns {I4} isomeric feeding component attributed to a low energy transition for which low detection efficiency or strong electron conversion could render it unobservable in ({+11}B,4n|g). 
T from ({+11}B,4n|g). 
J (D) transition to 19/2- 1937. 


level_energy_unit: KEV
level_spin_parity: (25/2)+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E consistent with adopted E(level)=1907.21 {I15} 
T weighted average of 1.02 {I6} ms (1966Em02) and 1.05 {I6} ms (1981Av04). Other value: 0.90 {I18} ms (1968Io01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T from 1988BeYU (stated E(level)=899 presumed to be in error). Other values: 2.0 ns {I1} (1974Ma26) and 2.1 ns {I2} (1974Si14) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
This level was identified as the 7/2+ member of the 7/2[404] rotational band observed in decay. The |g ray branching ratios disagree substantially with those observed in decay. 


level_energy_unit: KEV
level_spin_parity: (25/2)+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T weighted average of 1.02 ms {I6} (1966Em02) and 1.05 ms {I6} (1981Av04). Other value 0.90 ms {I18} (1968Io01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (49/2-)
level_comment:
Proposed by authors to be J=49/2 member of K|p=29/2- band built on 2737 level, but 6178 level, instead, has been adopted here as that member (as proposed by 2000Pu01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T$from weighted average of 5.59 ns {I4} from (168|g)(382|g)(t), 5.74 ns {I5} from (224|g)(382|g)(t), and 5.70 ns {I12} from (197|g)(382|g)(t) (2017Gu23) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T$from weighted average of 2.09 ns {I3} from (142|g)(114|g)(t), and 2.06 ns {I3} from (380|g)(114|g)(t) (2017Gu23) 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: D
level_comment:
MOMM1 from 1981Ha22, NMR on oriented nuclei. Others: 2.53 {I9} (1973Hu06), 2.48 {I12} (1973Kr01) from static nuclear orientation. 
MOME2 from 1983Ha52, static nuclear orientation. Other: 1981Er01 +3.3 {I3} (1981Er01; nuclear orientation). 
J |m consistent with J=3 only; parity from Nilsson assignment. 
T from 2006Ha51; source produced by {+185}Re(|g,n) reaction which should not excite the 169 d isomer. Others: 1960Bo07 (38 d {I1}), 1962Dz04 (38.0 d {I5}), 1963Jo03 (33 d {I3}), 1965Bl06 (34 d {I5}); some or all of these measurements may have been perturbed by presence of the then-unknown 169 d isomer. 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_comment:
J M4-M1+E2 cascade from the 188 level to the 104 level to the 3(-) g.s., and crossover from 188 to g.s. with mult=E3 or E4 or E5. 


level_energy_unit: KEV
level_spin_parity: 8(+)
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
MOMM1 from nuclear orientation; weighted average of 2.86 {I13} (1973Hu06) and 2.90 {I15} (1973Kr01). 
T from 1963Jo03. Others: 1965Bl06 (166 d {I12}), 1964Ha06 (160 d). 
J see comment on 104.7 level. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J possible bandhead for (|n 1/2[510] + |p 9/2[514]) configuration; 314|g from (5-,6-) 703. 
No deexciting transition observed in ({+7}Li,3n|g); may be an isomeric state with T{-1/2}>>1 |ms or, alternatively, a level whose decay is fragmented over many states. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J possible bandhead for |n 1/2[510] + |p 9/2[514] configuration 
No deexciting transition observed; either an isomeric state with T{-1/2}>>1 |ms or, alternatively, a state whose decay is fragmented over many levels. 


level_energy_unit: KEV
level_comment:
$d|s/d|W(d,t)=7 
d|s/d|W(d,t)=5 at 30|'; d|s/d|W({+3}He,|a)=39 at 40|' for E=704 through 793 multiplet. 


level_energy_unit: KEV
level_comment:
$d|s/d|W(d,t)=6 
d|s/d|W(d,t)=4 at 30|'; d|s/d|W({+3}He,|a)=39 at 40|' for E=704 through 793 multiplet. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
$d|s/d|W(d,t)=31 
d|s/d|W(d,t)=23 at 30|' for 741+751 doublet; d|s/d|W({+3}He,|a)=39 at 40|' for E=704 through 793 multiplet. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
$d|s/d|W(d,t)=22 
d|s/d|W(d,t)=23 at 30|' for 741+751 doublet; d|s/d|W({+3}He,|a)=39 at 40|' for E=704 through 793 multiplet. 


level_energy_unit: KEV
level_comment:
$d|s/d|W(d,t)=12 
d|s/d|W(d,t)=8 at 30|'; d|s/d|W({+3}He,|a)=39 at 40|' for E=704 through 793 multiplet. 


level_energy_unit: KEV
level_comment:
$d|s/d|W(d,t)=9 
d|s/d|W(d,t)=10 at 30|'; d|s/d|W({+3}He,|a)=39 at 40|' for E=704 through 793 multiplet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8(+)
level_lifetime_unit: D
level_comment:
E,J$from Adopted Levels of {+184}Re in ENSDF database. Energy is rounded value. 
T$weighted average of 208 independent measurements of decay curves of different |g transitions from the |e decay of this isomer using reference transitions from decays of {+186}Re, {+134}Cs, and {+60}Co. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: D
level_comment:
T$35.43 d weighted average of 35.12 d, 36.16 d and 35.00 d measured using 792.067|g(t), 894.760|g(t) and 903.282|g(t), respectively after correcting contributions from the decays of the isomeric state (104.739|g, 161.269|g, 216.547|g, 318.008|g, 920.933|g and 1173.770|g) in 2022La12. Authors state that the final standard uncertainty is determined using Pomm~e's technique. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1 NMR (2001StZZ). 
MOME2 Hyperfine structure of pionic x rays (1981Ko11, 1989Ra17). Other value: Q=+2.21 {I4} (hyperfine structure of muonic x rays (1981Ko11)). 
Q({+185}Re)/Q({+187}Re)= 1.0565 {I3} (1968Se09), 1.059 {I14} (1970Bu09), 1.056709 {I17} (1978Se09). Others: 1990Su20. 
J$J from optical spectroscopy, microwave absorption (1976Fu06). L=2 in (|a,t). |m(exp) agrees with value calculated for the 5/2+,5/2[402] Nilsson state. See 1970Va02, 1973Ra06, 1974Ba18, 1974El08, 1976Ga35 for calculated |m values, and see 1977Ra15 for calculated Q. 
<r{+2}>{+1/2}=5.329 fm 13 based on a global fit to charge radius data for all nuclides (2004An14). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
MOMM1 |g|g(H,|q) in {+185}Os |e decay (2001StZZ). 
J$125.3|g M1+E2 to 5/2+; band structure. 
T from Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T from {+186}W(d,3n|g). 
J J|p and Nilsson orbital assignment are based on the energy and half-life systematics of the 9/2[514] orbital in odd-A rhenium isotopes. |g to 7/2+ state of the 5/2[402] band; but not to the 5/2+ state. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J level is Coulomb excited, 646.1|g E2 to 5/2+, L=0,1 in ({+3}He,d). 
T$from {+185}Re(|g,|g'). Other: 4.5 ps {I9} from Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J 71.3|g M1+E2 to 1/2+; 592|g E2 to 7/2+. 
T$from {+185}Re(|g,|g'). Other: 2.6 ps {I8} from Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$874.8|g M1 to 5/2+, 749.46|g to 7/2+; log| {Ift}=7.2 (log| {If{+1}t}=6.1) from {+185}Os (J|p=1/2-) |e decay. 
T from {+185}Re(|g,|g'). 


level_energy_unit: KEV
level_comment:
J possible doublet comprising the J|p=5/2- and 9/2- members of the band. Transition intensity in ({+3}He,d) is consistent with this interpretation. L=4 in ({+3}He,d) is not consistent with |p=-. 


level_energy_unit: KEV
level_spin_parity: 15/2
level_lifetime_unit: NS
level_comment:
$Possibly 3-quasiparticle configuration, or vibrational configuration 9/2-[514]~#3- octupole 
J$DCO ratio for the 449 keV transition to the 13/2- state is consistent with a |DJ=1 assignment; |g to 15/2- state. 
T$From (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J L=5 in ({+3}He,d), presented in 1971Lu01; L=4, possibly a misprint, shown in tables (1971Lu01). Probable Nilsson orbital=11/2[505]. 


level_energy_unit: KEV
level_spin_parity: 17/2
level_comment:
J$DCO ratio for the 204 keV transition to the 1206 (J=15/2) state is consistent with a |DJ=1 assignment; band structure 


level_energy_unit: KEV
level_spin_parity: 19/2
level_comment:
J$DCO ratio for the 281 keV transition to the 1410 (J=17/2) state is consistent with a |DJ=1 assignment; band structure 


level_energy_unit: KEV
level_spin_parity: (21/2)
level_lifetime_unit: NS
level_comment:
J$115|g E1(+M2) to (19/2) 
T$Weighted average of 123 ns {I23} from (HI,xn|g) (1997Sh37) and 120 ns {I15} from (HI,xn|g) 2002Pf01. Other: 164 ns {I10} from (HI,xn|g) 2004Va03. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
$B(E2)=1.96 {I19} from |e(|g)B(E2)=0.52 {I5} (1958Mc02). 
Measured B(E2)'s (|a(125|g)=2.76 {I2} is used): B(E2)=1.2 {I3} from |e(|g)B(E2)=0.33 {I7} (1957Wo32), B(E2)=2.9 {I6} from |e(|g)B(E2)=0.76 {I16} (1959De29), B(E2)=1.37 {I7} from |a' spectrum at |q=90|' (1967Bi10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
$B(E2)=0.67 {I7} (1958Mc02). 
Deduced B(E2) values (corrected for adopted |a's): B(E2)=0.52 {I10} (1957Wo32), B(E2)=0.76 {I35} (1959De29), B(E2)=0.52 {I7} (1967Bi10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_comment:
$B(E2)=0.030 {I10} (1967Bi10). 
|e(750|g)B(E2)=0.03 was measured by 1960Na13; B(E2)=0.11 {I2} was obtained by 1967Bi10 for the 646, 717, and 769 levels with relative probabilities 1:1.0 {I8}:0.8 {I2} from a spectrum at |q=90|'. This gives B(E2)(768)=0.030 {I10}, B(E2)(717)=0.039 {I10}, and B(E2)(646)=0.037 {I7}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 15/2
level_lifetime_unit: NS
level_comment:
$Possibly 3-quasiparticle configuration, or vibrational configuration 9/2-[514]~# 3- octupole vibration. 
T$From centroid shift analysis of the |g|g time-difference spectrum between the transitions above and below the state. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
MOME2$from hyperfine splitting of 5g to 4f transition (2020An04). Value is reported as 2.07 b {I2} (stat) {I5} (syst), uncertainty combined in quadrature. Other: 2.07 b {I5} (stat) {I8} (syst) from data with other HPGe detector. 
J$from the Adopted Levels of {+185}Re in the ENSDF database (November 2005 update) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$from the Adopted Levels of {+185}Re in ENSDF database. 
MOMM1$3.1567 {I3} {I12} from the uncorrected experimental NMR value combined with the shielding constant obtained in 2022Sk02. The first |D|m is experimental and the second one is due to the present theory. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: D
level_comment:
MOMM1$from atomic-beam triple resonance method (2019StZV, based on 1965Ar01). Other: 1980Za10. 
MOME2$from atomic beam method (2016St14, 1981Bu13) using {+185}Re and {+187}Re (2016St14, 1981Ko11) as reference standards. Other values: +0.54 {I9} from static nuclear orientation using {+187}Re standard (2014StZZ, based on 1983Oe01 and 1985Ha41); +0.60 {I6} from static nuclear orientation using {+187}Re standard (2014StZZ, from 1983Ha49); +0.88 {I12} nuclear orientation relative to {+187}Re reference standard (1981Er01). 
%|e, %|b{+-}: from {+186}Re |e decay (3.7186 d). 
J$J=1 from atomic-beam spectroscopy (1963Do13); |p=- from log {Ift}=8.0 for 2{++} state feeding in {+186}Re |b{+-} Decay (3.7185 d). 
CONF$|p5/2[402]~#|n3/2[512], K{+|p}=1{+-} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J M1+E2 to 1- g.s. (1969La11); J|p=1- ruled out at 99.9% confidence level from (n,|g) E=2-110 eV (1983Be27, 1980BeYB); band member (1973Gl06,2009Wh01). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
J M1+E2 40|g to 2- 59-keV level and E2 99|g to g.s.; |p=- from L=1 in {+185}Re(p,d) because J|p(target)=5/2+ (1969La11); configuration assignment. 
CONF$|p5/2[402]~#|n1/2[510], K{+|p}=3{+-} 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: Y
level_lifetime_info: ;ERR=?;ISO=M1
level_comment:
%IT %|b{+-}<10 from {+186}Re IT decay; no |b{+-} decay has been observed (1972Se06). 
T from {+186}Re IT decay (1972Se06). 
J (E5) 49|g to 3-. Possible configuration built on K|p=8+ (1972Se06). Energy is comparable with systematics of possible 8+ state in {+182}Re (154 keV) and in {+184}Re (188 keV). 
CONF$|p5/2[402]~#|n11/2[615], K{+|p}=(8{++}) 
E$based on placement of 267|g as depopulating the 415-keV level from {+187}Re(n,2n|g) in 2015Ma60. 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J M1+E2 75|g to 3- 99-keV level; configuration assignment. 
CONF$|p5/2[402]~#|n3/2[512], K{+|p}=4{+-} 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J Level not populated by primary |g in (n,|g) E=thermal which favors J|>5 since capture state J|p=2{++},3{++} (1969La11,2016Ma35); L=3 in {+185}Re(d,p) (1969La11) for doublet whose other component is expected to have L=1; systematics of heavier odd-odd Re isotopes. Possible configuration built on K{+|p}=6{+-} (1969La11,2009Wh01). Level is expected to deexcite via M2 and E2 transitions to the (8{++}) 148 and 4{+-} 174-keV levels, respectively (1973Gl06). No deexciting transitions have been reported, however, transitions to these levels proposed at approx. 12 and 38 keV also favor a J|p=6{++} according to statistical-model predictions in (n,|g) E=thermal (2016Ma35). 
CONF$|p5/2[402]~#|n 7/2[503], K{+|p}=(6{+-}) 
T$Probably a long-lived isomeric state, associated in 1969La11 with T{-1/2}=70 |ms {I1} that was measured by 1964Br27. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J M1 211|g to 1- g.s.; M1(+E2) 111|g to 3- 99-keV level; M1+E2 152|g to 2- 59-keV level; configuration assignment. 
CONF$|p5/2[402]~#|n1/2[510], K{+|p}=2{+-} 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J M1+E2 169|g to 3- 99-keV level; 4- from (n,|g) E=2-110 eV while 2-,3- ruled out at 99.9% confidence level (1983Be27,1980BeYB); band member. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: NS
level_comment:
MOMM1$From time-dependent perturbed angular distribution using {+19}F(197) standard (2020StZV, based on 1980Za10). 
J E1 255|g to 2- 59-keV level; E1 215|g to 3- 99-keV level; E=thermal (n,|g) statistical-model analysis favors 3+; configuration assignment. 
CONF$|p5/2[402]~#|n11/2[615], K{+|p}=3{++} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: NS
level_comment:
J M1 316|g to 1- g.s.; M1+E2 257|g to 2- 59-keV level; 1- from (n,|g) E=2-110 eV (1983Be27,1980BeYB); statistical-model analysis from (n,|g) E=thermal favors 1- (2016Ma35); configuration assignment. 
CONF$|p5/2[402]~#|n7/2[503], K{+|p}=1{+-} 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J M1+E2 144|g to 4- 174; 2-,3-, and 4- ruled out from (n,|g) E=2-110 eV (1983Be27,1980BeYB); band member. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: NS
level_comment:
MOMM1$from time-dependent perturbed angular distribution using {+19}F(197) standard (2020StZV, based on 1980Za10). 
J E1 144|g to 6- 180-keV level; E1+M2 150|g to 4- 174-keV level; configuration assignment (1973Gl06). 
CONF$|p 9/2[514]~#|n 1/2[510], K{+|p}=5{++} 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J E1 252|g to 3- 99-keV level; 4+ favored in E=thermal (n,|g) statistical-model analysis (2016Ma35); configuration assignment. Other value 3+ from possible coupling |p9/2[514]-|n3/2[512] (1973Gl06). 
CONF$|p9/2[514]~#|n1/2[510], K{+|p}=(4){++} 


level_energy_unit: KEV
level_spin_parity: (9+)
level_comment:
J$Supported by similarity with 446 level in {+184}Re and from the shape of the experimental and modeled excitation functions (TALYS and CoH codes) for the 266.7 |g transition (2015Ma60); band member. 7- assignment suggested in E=thermal (n,|g) from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J M1+E2 149|g to 4-; no primary transitions to this level in (n,|g) E=2-110 eV (1983Be27,1980BeYB) or (n,|g) E=thermal (1969La11, 2016Ma35) implying J|>5; band member. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J M1+E2 112|g to (3+) 314-keV level; E=thermal (n,|g) statistical-model analysis (2016Ma35). Other value 3+ from possible coupling |p9/2[514]-|n3/2[512] (2020Kr05). See (n,|g) E=thermal data set. 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J M1+E2 189|g to 4- 274-keV level; 2-,3-,4- ruled out from (n,|g) E=2-110 eV (1983Be27,1980BeYB); band member. 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J M1 296|g to 4- 174-keV level; M1+E2 147|g to 3- 322-keV level; band member; member of possible 3- & 4- doublet in (n,|g) E=2-110 eV (1983Be27), the 3- member of which is assigned as the 470.5 level. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J M1+E2 92|g to 2- 378-keV level; band member; member of possible 3- & 4- doublet in (n,|g) E=2-110 eV (1983Be27); statistical-model analysis from (n,|g) E=thermal favors 3- (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J Intraband 179 |g to 5- 318-keV level; band member; statistical-model analysis from (n,|g) E=thermal favors 6- (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J M1+E2 150|g to (4)+ 351-keV 5+; E=thermal (n,|g) statistical-model analysis (2016Ma35). Other value 4+ if built on K|p=3+ configuration (|p 9/2[514])-(|n 3/2[512]) (1973Gl06). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J M1 360|g to 4- 174-keV level; 4- favored in (n,|g) E=2-110 eV (1983Be27,1980BeYB) and E=thermal (n,|g) statistical-model analysis (2016Ma35); configuration assignment. 
CONF$|p1/2[411]~#|n7/2[503], K{+|p}=(4{+-}) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J M1+E2 123|g to 4+ 426-keV level; E=thermal (n,|g) statistical-model analysis (2016Ma35). Other value 4+ if band member built on K|p=3{++} configuration (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J Configuration assignment (2017Ma39); M1+E2 232|g to 5+ 324-keV level; E=thermal (n,|g) statistical-model analysis (2016Ma35). 
CONF$|p9/2[514]~#|n3/2[512], K{+|p}=(6{++}) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J M1+E2 intraband 139|g to (4+) 421-keV level; band member; E=thermal (n,|g) statistical-model analysis (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J (M1) 261|g to (1-) 316-keV level; configuration assignment (1973Gl06,2009Wh01); E=thermal (n,|g) statistical-model analysis (2016Ma35); 2- or 3- in (n,|g) E=2-110 eV (1983Be27,1980BeYB). 
CONF$|p5/2[402]~#|n9/2[505], K{+|p}=2{+-} 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J Intraband 118|g to 3- 471-keV level; band member; E=thermal (n,|g) statistical-model analysis (2016Ma35); E=2-110 eV (n,|g) (1983Be27,1980BeYB). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J E1+M2 391|g to 2- 211-keV level; E1+M2 285|g to 1- 316-keV level; configuration assignment (1973Gl06); J|>2 ruled out in statistical-model analysis from (n,|g) E=thermal (2016Ma35). 
CONF$|p9/2[514]~#|n7/2[503], K{+|p}=(1{++}) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J from (n,|g) E=2-110 eV (1983Be27,1980BeYB); 413|g to 2- 211-keV and 301|g 3- 322-keV level; preferred assignment from statistical-model analysis from (n,|g) E=thermal (2016Ma35). Favored 2- assignment from depopulation-data analysis in 2020Kr05. 


level_energy_unit: KEV
level_spin_parity: (6)+
level_comment:
J M1+E2 164|g to (5)+ 501-keV; band member; 6+ assignment favored in E=thermal (n,|g) statistical-model analysis (2016Ma35). Other value 5+ if built on K{+|p}=3{++} configuration (|p 9/2[514])-(|n 3/2[512]) (1973Gl06). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J 680|g to 1- g.s. and 357|g to 3- 322-keV level; E=thermal (n,|g) statistical-model analysis (2016Ma35); E=2-110 eV (n,|g) supports 2- or 3- (1983Be27,1980BeYB); 2- favored from depopulation- data analysis in E=thermal (n,|g) (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J M1+E2 308|g to (2-) 378-keV level; intraband 108|g to (2-) 577-keV level; band member; E=thermal (n,|g) statistical-model analysis (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J Intraband 228|g to 5- 463-keV level; band member; E=thermal (n,|g) statistical-model analysis (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$Assignment deduced by evaluator according to rotational band structure. Other value 5+ if band member built on K|p=3{++} configuration (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J Intraband (M1+E2) 147|g to (4-) 589-keV level; band member; no primary |g feeding in (n,|g) E=2-110 eV (1983Be27,1980BeYB) or (n,|g) E=thermal (2016Ma35) favoring J|>5; statistical-model analysis from (n,|g) E=thermal favors 5- (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J M1 intraband 87|g to (2+) 658-keV level; band member; E=thermal (n,|g) statistical-model analysis (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
J E=2-110 eV (n,|g) (1983Be27,1980BeYB). 
(d,p) presumed to excite this, but not the 745-keV, level because the latter's configuration should not be excited in (d,p); (2)- in (n,|g) E=thermal (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_comment:
J 439|g to (3)- 322 keV, possible 762|g to 1- g.s.; member of |p=- doublet (other member not listed here) in (n,|g) E=2-110 eV (1983Be27, 1980BeYB). 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_comment:
J 407|g to (2-) 378-keV level, possible 469|g to (1-) 316-keV level; 2- assignment favored in depopulation analysis (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_comment:
J E=2-110 eV (n,|g) (1983Be27,1980BeYB) 2- and 3- ruled out at 99% confidence level; suggested (2,3)- assignment in (n,|g) E=thermal with preferred 3- from depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J 381|g to (9+) 415-keV, 648|g to (8+) 148-keV level. 
CONF$Possible K|p=10+, |p5/2[402]~#|n{+3}(1/2[510],3/2[512],11/2[615]) or |p5/2[402]~#|n11/2[615]~#2{++}{-|g} configuration (2017Ma39). 


level_energy_unit: KEV
level_spin_parity: (LE 3-)
level_comment:
J 797|g to 1- g.s.; |p=- for doublet (other member not listed here) in E=2-110 eV (n,|g) (1983Be27,1980BeYB); 2- preferred assignment in (n,|g) E=thermal from depopulation analysis (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
J$(1-) from E=2-110 eV (n,|g) (1983Be27,1980BeYB); (1,2)- from (n,|g) E=thermal with 1- favored assignment from depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
J 645|g to 4- 174-keV, 607|g to 2- 211-keV level; E=2-110 eV (n,|g) (1983Be27,1980BeYB); 3- favored assignment from analysis of depopulation data in (n,|g) E=thermal (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J 220|g to (1+) 602-keV, 163|g to (2+) 658 allow J|p=(0+,1,2,3+); deduced configuration assignment (2020Kr05). 
CONF$|p9/2[514]~#|n9/2[505], K{+|p}=(0{++}) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J M1+E2 140|g to (3-) 686-keV level; band member; E=2-110 eV (n,|g) (1983Be27,1980BeYB); E=thermal (n,|g) statistical-model analysis (2016Ma35); (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
J Intraband 197|g to (2+) 658-keV and 110|g (3+) 745-keV levels; band member; E=thermal (n,|g) statistical-model analysis (2016Ma35); (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
Complex level in (d,p) which presumably includes this level but not the 855 level because the latter's configuration should not be excited in (d,p). 
J$Other: (1,2)- with preferred 2- assignment in (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (2-,3-,4-)
level_comment:
J |p=- doublet in E=2-110 eV (n,|g) (1983Be27,1980BeYB); 3- favored in (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
J$Other: (2,3,4)- with preferred 3- assignment in (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J$Other: (3,4)- with preferred 3- assignment in (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$Reported energy below (1+) band member at 965.4 due to Newby energy shift (2020Kr05). 
J$Band member. 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
J$Other: (3-,4-) with preferred 3- assignment in (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E$Reported energy above (2+) band member at 910.5 due to Newby energy shift (2020Kr05). 
J$Band member. 


level_energy_unit: KEV
level_spin_parity: (2-,3-,4-)
level_comment:
J$3- assignment favored in (n,|g) E=thermal from analysis of depopulation data (2020Kr05); |p=- doublet in E=2-110 eV (n,|g) (1983Be27,1980BeYB). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_uncertain: ?
level_comment:
J Intraband 142|g to (4+) 855-keV level; band member; (n,|g) E=thermal from analysis of depopulation data (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: Y
level_lifetime_info: ;ERR=?;ISO=M1
level_comment:
E Other: 149 keV {I7} deduced from E|g (1972Se06). 
J Deduced configuration K|p=8+, |p5/2[402]~#|n11/2[615] (1972Se06). 
T From mass spectrometry and average absolute photon intensity measurements in 1972Se06; uncertainty not stated. Secondary datum: 1.7|*10{+5} y from consistency check that measured equilibrium |b{+-} activity using a proportional counter, corrected for |b{+-} self-absorption and photon background (1972Se06). 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
E$May deexcite to 99, 148 (8+), 146 and/or 174 levels; however, no deexciting transitions were identified in 1969La11, 1973Gl06. Transitions proposed to 148- (2016Ma35) and 174-keV (2016Ma35, 2020Kr05) levels; intensity estimated based on statistical-model analysis (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$Assignment based on statistical-model analysis in 2016Ma35 together with measured E1 252|g to 3{+-} and [E1] 205|g to 3{+-}. Earlier (3)+ value (1969La11) based on measured E1 252|g alone in 1969La11. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$(2+,3+,4+) in earlier evaluation (2003Ba44) based on (n,|g) E=2-110 eV (1983Be27,1980BeYB) and observed 112|g to 3+ 314; 3+ in 2020Kr05 from analysis of depopulation data and reported configuration. 4+ assignment from statistical-model analysis in 2016Ma35 adopted due to reproduction of experimental data up to critical energy of 746 keV. Other value 3+ from possible coupling |p9/2[514]-|n3/2[512] (2020Kr05). 
CONF$K|p=3+, (|p9/2[514])-(|n3/2[512]) proposed in 2020Kr05 implies alternative J|p=3+ assignment. 


level_energy_unit: KEV
level_spin_parity: 6+
level_uncertain: ?
level_comment:
J$(4)+ in earlier evaluation (2003Ba44) based on (|p 9/2[514])-(|n 1/2[510]) configuration (1973Gl06) and M1+E2 141|g to 5{++} 324. Current assignment supports M1+E2 (2016Ma35) but implies different configuration. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$(4)+ in earlier evaluation (2003Ba44) based on M1+E2 150|g to previously assigned (3)+ 351 (see level at 351 keV) 1969La11. New 4+ assignment for 351 is consistent with M1+E2 150|g (2016Ma35). 401|g to 3- 99 is consistent with [M2] assuming current J|p assignments rather than [E1]. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$|p=(+) in earlier evaluation (2003Ba44) based on M1+E2 124|g to previously tentative (2+,3+,4+) 426 (see 426 level) 1969La11; Current assignment adopted based on reproduction of experimental data up to critical energy of 746 keV from statistical model (2016Ma35). Other value 4+ if band member built on K|p=3{++} configuration (2020Kr05). Both 4+ and 5+ assignments support M1+E2 to 4+ 426. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J$(5)+ in earlier evaluation (2003Ba44) based on M1+E2 164|g to previously assigned (4)+ 501 (see level at 501 keV) 1969La11. New assignment consistent with M1+E2 164|g to 5+ 501 (2016Ma35). 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$(2-,3-) in earlier evaluation (2003Ba44) from (n,|g) E=2-110 eV (1983Be27,1980BeYB) and observed gammas to 1{+-} g.s. and 3{+-} 322; (2,3)- from analysis of depopulation data with favored 2- assignment (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$Assignment deduced by evaluator based on suggested band member above 549 level (2020Kr05). Other value 5+ if band member built on K|p=3{++} configuration (2020Kr05). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E,J$Reported in Fig. 4 of 2020Kr05 as member of band built on K|p=0{++} configuration, but no transitions connecting this level to other band members were identified because only |g rays above 120 keV were measured. Level energy is lower than 1+ 965-keV band member due to Newby energy shift (2020Kr05). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from adopted levels. 
J$data are compatible with a doublet with J|p=3- and 4- near 470 keV (1983Be27); 4- from adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from adopted levels. 
J$data are compatible with a doublet with J|p=3- and 4- near 470 keV (1983Be27); (3-) from adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_lifetime_unit: Y
level_lifetime_info: ;ERR=?;ISO=M1
level_comment:
E$Level energy held fixed In least-squares adjustment 
E$From 2015Ma60. The level energy was held fixed during the least-squares fit adjustment. 


level_energy_unit: KEV
level_spin_parity: (6)-
level_comment:
E,T$Probably a long-lived isomeric state, associated in 1969La11 with T{-1/2}=70 |ms {I1} that was measured by 1964Br27. 
CONF$K|p=6-, |p5/2[402]~#|n7/2[503] 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
CONF$Possible K|p=10+, |p5/2[402]~#|n{+3}(1/2[510],3/2[512],11/2[615]) or [|p5/2[402]~#|n11/2[615]]~#2{++}{-|g} configuration 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
E$Level energy held fixed In least-squares adjustment 
E$Based on placement of 266.7|g as depopulating the 415-keV level. 


level_energy_unit: KEV
level_spin_parity: (9+)
level_comment:
J$From analogue state at 446 keV in {+184}Re and the shape of the experimental and modeled excitation functions (TALYS and COH codes) for the 266.7 |g transition 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$Supported by similarity with 728 level in {+184}Re and from the shape of the experimental and modeled excitation functions (TALYS and COH codes) for the 381.2 and 647.7 |g transitions 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: Y
level_comment:
MOMM1$from 1951Al11 (NMR). Same value by 1989Ra17 and 2005St24. 
MOME2$from 1981Ko11 (from pionic and muonic x rays). Same value by 1989Ra17 and 2005St24. 
<r{+2}>{+1/2}({+187}Re)=7.69 {I32} fm (magnetic) (1998Lo04); <r{+2}>{+1/2}({+187}Re)=5.339 {I13} fm (charge) (2004An14). 
%A$no |a's observed for 1.5<E|a<3.7 MeV, emulsion (1954Po24). 
J$spin from optical and microwave spectroscopy (1976Fu06). Parity from L=2 ({+3}He,d) and angular distribution and analyzing power in (Pol t,|a). 
T$weighted average of 4.12|*10{+10} y {I11} (2001Ga01), 4.35|*10{+10} y {I13} (1986Li11) and 4.56|*10{+10} y {I12} (1983Lu09, 1980Lu10) - measured growth of {+187}Os daughter. Other values: 4.3|*10{+10} y {I4}{-stat} 3{-syst} (1999Al20), 4.3|*10{+10} y {I5} (1963Hi08), 6.2|*10{+10} y {I7} (1958He06) from measurements of daughter growth; 3.5|*10{+10} y {I4} (1984Na04), 6.6|*10{+10} y {I13} (1965Br12), 3.|*10{+10} y (1962Wa15) from specific activity measurements. T{-1/2}=4.5|*10{+10} y {I3}, from neutral {+187}Re decay to singly ionized {+187}Os (1993As02). Fully ionized {+187}Re half-life T{-1/2}=32.9 y {I20} (1996Bo37); Others: 33 y {I2} (1997No07), 31.2 y {I+30-25} (1997We08), and 33 y {I6} (1996Ki23). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
MOMM1$from 1989Ra17 and 2005St24 (perturbed angular correlations) 
J 134.2|g M1+E2 to 5/2+. 
T$Weighted average of 11.1 ps {I10} (Coulomb excitation), 10.4 ps {I14} (1960Mo08,Mossbauer), and 10.0 ps {I+10-14} (1963Bl12, (p,|g); in the weighted average 10.0 ps {I12} was used). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$from 1989Ra17 and 2005St24 (differential perturbed angular correlations) 
J$206.2|g M2+E3 to 5/2+ state and 72.0|g E1(+M2) to 7/2+ state. 
T$from {+187}W |b{+-} decay ((479|g)(72|g)t) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$168.5|g M1+E2 to 7/2+ and 303 E2 to 5/2+. 
T$from Coulomb excitation (using B(E2)|^=0.57 {I3} and adopted 303|g properties). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J L=0 in (|a,t),({+3}He,d). 
T$Weighted average of 17 ps {I6} (|g,|g') and 13 ps {I3} (Coulomb excitation). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$77.4|g M1 to 1/2+ state, 454.9|g E2 to 7/2+ state, and 589|g M1(+E2) to 5/2+ state. 
T from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: PS
level_comment:
T$from (|g,|g'). Other: <50 ps ({+187}W |b{+-} decay-1974Da31 |b(ce(K) 107|g)t) 
J$106.6|g M1+E2 to 1/2+ state and 36.4|g M1+E2 to (5/2+) state. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_comment:
J$113.7|g M1 to 1/2+ state. If 491.2|g to 7/2+ state is correct, J|p=3/2+; however, band assignment is consistent with 1/2+. 
T from {+187}W |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$479.5|g E2 to 9/2- state, 551.5|g E1(+M2) to 7/2+ state, and 685.8|g E1(+M2) to 5/2+ g.s.. 
T$from (|g,|g'). Other values: 11.5 ps {I21} ({+187}W |b{+-} decay), weighted average of 10 ps {I3} from 1974Da31 |b(ce(K) 686|g) and 13 ps {I3} (1967Be62); 5.9 ps (1973SaZD). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: PS
level_comment:
J$772.9|g M1+E2 to 5/2+ g.s., 261|g to 1/2+ state. 
T$from (|g,|g'). Other value: 0.18 ps {I3} (1964La02,Mossbauer). 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_comment:
J$708|g to 7/2+ state and 842|g to 5/2+ state, both states are member of 5/2+[402] band; 453|g to 11/2- state. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: FS
level_comment:
J$from Coulomb excitation. A large B(E2)(W.u.)=1.3|*10{+5} value weakens the tentative assignment of this level or the (5/2+) of 582 keV level. 
T$from Coulomb excitation. Note that adopted branching yields a large B(E2)(W.u.)=1.3|*10{+5}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$239|g M1+E2 to (1/2+) state, 246|g M1(+E2) to 5/2+ g.s., 246.2|g M1+E2 to 3/2+ state. 
T from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
J$745|g M1(+E2) to 7/2+ state, log| {Ift}=7.89 from 3/2-, band assignment. 
T$from {+187}Re(|g,|g') (1967La15), 0.17 ps {I5} in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$from comparison with the calculated level energy assuming a g.s. band member - proposed in {+187}W |b{+-} decay (1976Br09). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E Weighted average of 1208 {I3} (t,|a),(pol t,|a) and 1211 {I3} (|a,t),({+3}He,d). 
J L=(5) in (|a,t),({+3}He,d), band assignment. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E Weighted average of 1232 {I3} (t,|a),(pol t,|a) and 1233 {I3} (|a,t),({+3}He,d). 
J$L=(3) in (|a,t),({+3}He,d) and band assignment. 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$367.6|g and 634.8|g feeding (17/2-) and (15/2-) states, respectively, members of 9/2-[514] band; and (M1,E1) and from multipolarity assumptions for 155|g and 207|g using intensity balance at this level. A possible configuration for the K|p=19/2- state: |p{5/2+[402]}~#|n7-{3/2-[512] 11/2+[615]} 
T From ({+82}Se,{+81}Se|g) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E Weighted average of 1484 {I6} (t,|a),(pol t,|a) and 1488 {I3} (|a,t),({+3}He,d). 
J$L=(2) in (|a,t),({+3}He,d). Assignment from (t,|a). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$(3/2+) is the most likely from (t,|a), (pol t,a) (1977Hi06) - (1/2,5/2)- are less likely assignments. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_comment:
J 207|g (E1) to (19/2-) state. Possible K|p=19/2+ configuration: |p(9/2-[514])~#|n5-(-1/2-[510] 11/2+[615]). 
T Determined from a time difference spectrum between the 329|g and the 215|g, 207|g, and 329|g ({+82}Se,{+81}Se|g). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T$from 1972Gu03 (479|g)(72|g)t. Other values: 526 ns {I12} (1949Bu09), 550 ns {I50} (1949Mc29), 568 ns {I12} (1964Ha51), 557 ns {I12} (1963Ko19), 570 ns {I5} (1963Wa16), 505 ns {I13} (1965Br26), and 550 ns {I20} (1971Ni01). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_comment:
T$Weighted average of 534 ps {I20} (1973SaZD |b(618|g)T{-1/2} ), 530 ps {I50} (1966Pe03), 520 ps {I30} (1969An17), 550 ps {I20} (1971Be82), and 548 ps {I20} (1974Da31). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 10 ps {I3} from 1974Da31 |b(ce(K) 686|g) and 13 ps {I3} (1967Be62). Other value: 5.9 ps (1973SaZD). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$for 686|g. Other values: 6.0 ps {I8} (480|g), 6.0 ps {I9} (552|g), 6.0 ps {I5} (1964La02) and 4.3 ps {I7} (1973KaYR). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
$d|s/d|W=1.0E3 
E from {+187}W |b{+-} decay 
1.5|*10{+3} (90|') and 9.7|*10{+3} (150|') d|s/d|W (|mb/sr) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$d|s/d|W=82 
E doublet (J|p=11/2+) 
BE2$for the 511+589+647 composite level (1967Bi10) 
87 (90|') and 102 (150|') d|s/d|W (|mb/sr) 


level_energy_unit: KEV
level_spin_parity: (17/2)
level_comment:
J Assigned to leading the K=(13/2) for the Band II, requiring at least 3~h spin transfer for the 586|g. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$367.6|g and 634.8|g feeding 17/2- and 15/2- states, respectively, members of 9/2-[514] band; and from (M1,E1) multipolarity assumptions for the 155|g and 207|g using intensity balance at this level. A possible configuration for the K|p=19/2- state: |p(5/2+[402]) ~# |n(3/2-[512]11/2+[615]){-7-} 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_comment:
J or (21/2+). 207|g (E1) to 19/2- state. K|p=19/2+ is favored from systematics by authors, a possible configuration: |p(9/2-[514]) ~# |n(-1/2-[510]11/2+[615]){-5-}. K|p=(21/2+) configuration: |p(9/2-[514]) ~# |n(1/2-[510]11/2+[615]){-6-} 
T Determined from a time difference spectrum between the 329|g and the 215|g, 207|g, and 329|g. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 1.14 {I23} (1957Wo32), 1.47 {I15} (1958Mc02), 2.0 {I4} (1959De29), and 1.47 {I10} (1967Bi10). Other values: 0.6 {I3} (1955Mc44), 1.3 (1956Da40), and 1.8 (1956Hu49). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.63 {I4} (1957Wo32), 0.56 {I8} (1958Mc02), 0.56 {I25} (1959De29), 0.52 {I4} (1967Bi10), and 0.6 {I2} (1959De29). Other values: 0.45 (1956Da40), 0.4 (1956Go47). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: FS
level_comment:
BE2$from 1967Bi10 
T$Using B(E2)=0.080 {I12} and adopted 845|g ray properties, and assumed 639|g has negligible intensity. B(E2)(W.u.)|?1.3|*10{+5} for the 263|g indicates either substantial unobserved feeding from this level or incorrect branching intensities. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2+,5/2-)
level_comment:
J$3/2+ assignment is regarded by 1977Hi06 as the most likely J|p value from analyzing power, angular distributions, and the moderate cross section. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
E,T$from {+187}Re Adopted Levels in the ENSDF database 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T$from |g(t) (2016ReAA). Note that the previous value is 114 ns {I23} in {+187}Re Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
MOME2$from hyperfine splitting of 5g to 4f transition (2020An04). Value is reported as 1.94 b {I2} (stat) {I5} (syst), uncertainty combined in quadrature. Other: 1.94 b {I5} (stat) {I8} (syst) from data with other HPGe detector. 
J$from the Adopted Levels of {+187}Re in the ENSDF database (November 2008 update) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$from the Adopted Levels of {+187}Re in ENSDF database. 
MOMM1$3.1891 {I3} {I12} from the uncorrected expermental NMR value combined with the shielding constant obtained in 2022Sk02. The first |D|m is experimental and the second one is due to the present theory. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
J$from atomic-beam method (1963Do13); |p from |m 
T$weighted average of 17.001 h {I23} (2014Un01), 17.003 h {I3} (2004Sc04), 17.007 h {I15} (2002Po17) and 17.006 h {I4} (1989Ab18). Others: 17.0035 h {I22} (2001Sc23 - superseded by 2004Sc04), 17.001 h {I22} (2002Un02, updated from 17.021 h {I25} in 1994Co02 and 1992Un01 - superseded by 2014Un01), 16.93 h {I17} (1984Zh08), 16.98 h {I2} (1971Mi16), 16.74 h {I6} (1958Gu09), 16.7 h {I5} (1954Dz19), 16.9 h {I3} (1951Li07). 
MOMM1$atomic-beam magnetic resonance (1965Ar01). others: 1965Sc13, 1964Wi09 
MOME2$from atomic-beam method (1981Bu13). Others: +0.36 {I16} (1983Oe01,nuclear orientation), +0.88 {I14} (1981Er01,nuclear orientation). 1981Er01 assumed |b mixing ratio for 1- to 2+ |b{+-} transition as 0.424 {I25}. Other values for this ratio are 0.387 {I23} (1981Oe01) from |g(|q,t) of 155|g; |?0.4 (1965Ar01,1966Ku07) 
CONF$|p5/2[402]~#|n3/2[512], K{+|p}=1{+-} 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$63.583|g M1+E2 to 1-; band member. 
T$from 63|g-105|g(|Dt) (1968Ma14). Others: |<1.2 ns (1965Hu02) and |<20 ns (1964Ta07) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$105.8530|g M1+E2 to 2-, 169.441|g to 1-; assigned configuration 
CONF$|p5/2[402]~#|n1/2[510], K{+|p}=3{+-} 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$15.93|g M3 to 3-. 
T$from 1989Ab18. Others: 18.5 min {I3} (1965Na01), 18.7 min {I2} (1964Ta07), and 18.7 min {I3} (1953Fl07) 
CONF$|p5/2[402]~#|n7/2[503], K{+|p}=6{+-} 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
J$13.3|g and 26.7|g to 3-; absence of transitions to J|p=1-; assignment in (d,p) 
T$From |g|g(t) in 1978Sc10. Other: 17.6 ns {I30} (1972Sh13) 
CONF$|p5/2[402]~#|n3/2[512], K{+|p}=4{+-} 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$141.7588|g M1+E2 to 2-, 35.9|g to 3- 
T$Weighted average of 3.7 ns {I3} (1978Sc10) and 3.2 ns {I6} (1972Sh13) 
CONF$|p5/2[402]~#|n9/2[505], K{+|p}=2{+-} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$207.8477|g E1 to 1-; Absence of transitions to J|p=2- and 3- 
T$Weighted average of 3.8 ns {I2} (1978Sc10) and 3.2 ns {I4} (1972Sh13) 
CONF$|p9/2[514]~#|n9/2[505], K{+|p}=0{++} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
J$167.327|g E1 to 2-, 74.864|g (E1) to 3-; assigned configuration 
T$Weighted average of 21.4 ns {I15} (1978Sc10) and 20.9 ns {I20} (1972Sh13) 
CONF$|p9/2[514]~#|n3/2[512], K{+|p}=3{++} 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$256.92|g M1+E2 to 1-, 193.35|g M1+E2 to 3- 
T$From 1978Sc10. 
CONF$|p5/2[402]~#|n1/2[510], K{+|p}=2{+-} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$290.6828|g M1+E2 to 1-, 227.0731|g M1+E2 to 2-; configuration assignment 
T$From 1978Sc10. 
CONF$|p5/2[402]~#|n7/2[503], K{+|p}=1{+-} 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: NS
level_comment:
J$188.8109 E1 to 6-, 129.9797|g to 3+ 
T$Weighted average of 5.5 ns 6 (1978Sc10) and 6.0 ns {I25} and 5.2 ns {I10} (1972Sh13) 
CONF$|p9/2[514]~#|n1/2[510], K{+|p}=5{++} 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$132.8210|g to 5+, 262.796|g to 3+; assigned configuration 
CONF$|p9/2[514]~#|n1/2[510], K{+|p}=4{++}. Assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$219.430|g M1+E2 to 2-, 374.51|g to 0+ 
T$From 1978Sc10. 
CONF$|p1/2[400]~#|n3/2[512], K{+|p}=1{+-} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$609.2|g to 1-, 352.13|g to 2-. 
CONF$|p9/2[514]~#|n11/2[615], K{+|p}=1{+-}. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$65.137|g to 1-, 177.153|g to 3-; band member 
CONF$|p5/2[402]~#|n3/2[501] mixed with |g band is suggested in 1972Sh13 


level_energy_unit: KEV
level_spin_parity: 2,3,4
level_comment:
J$575.57|g to 3-; direct feeding by primary |g ray from the J|p=2+,3+ neutron capture state; the absence of |g ray to the g.s. would argue against J=1 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_uncertain: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From 2017Wa10 
J$s-wave capture on {+187}Re g.s. (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from 1989Ab18. Others: 18.5 min {I3} (1965Na01), 18.7 min {I2} (1964Ta07), and 18.7 min {I3} (1953Fl07) 


level_energy_unit: KEV
level_spin_parity: (5/2&7/2)+
level_comment:
E$doublet containing 5/2+ and 7/2+ members of the 1/2[411] rotational band. 
$In the previous evaluation, based on energy summation, a 222 |g line was shown depopulating this level. The |b{+-} measurement by 2009Yu11 could not confirm this |g transition with more reliable coincidence measurements. In {+190}Os(t,|a) it is stated that this is level is an unresolved doublet, so this may be a combination of the 471- and 490-keV levels established in |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
$d|s/d|W=4.7 {I7} 
J$(7/2+,9/2-) from |s(|q) and A{-y}(|q) data, 9/2- supported by model interpretation 
$Experimental NSF=0.05; theoretical value=0.005 for 9/2, 9/2[514] 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
$d|s/d|W=5.9 {I9} 
J$L-1/2 from |s(|q) and A{-y}(|q) data, 7/2+ supported by model interpretation 
$Experimental NSF=0.07; theoretical value=0.03 for 7/2, 5/2[402] 


level_energy_unit: KEV
level_spin_parity: (5/2&7/2)+
level_comment:
E,J$unresolved doublet with positive analyzing power. Broad peak with angular distribution consistent with states of different spin 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$d|s/d|W=62 {I6} 
J$(7/2-,9/2+,11/2-) from A{-y}(|q) data, however, a tentative (11/2-) could be explained by hexadecapole deformation effects (1977Hi06) 
$Experimental NSF=0.82 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (t,|a),(pol t,|a) (1976Hi08,1977Hi06) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: MIN
level_comment:
J$allowed |b feeding (log{Ift}=5.1) to 3-; absence of |b{+-} feeding to 4- 
$Configuration=|n9/2[505]~#|p5/2[402], K|p=2- (1976Ha39, 1974Ya02) 
T$weighted average of 3.1 m {I3} (1969Ha44), 2.8 m {I5} (1955At21), and 2.92 m {I20} (1973DeWI). The original uncertainty of 0.10 in 1973DeWI seems too small (probably statistical only) and has been increased by a factor of 2 in the average by the evaluators. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$119.1|g M1(+E2) to (2)-; probable band member 
$3- member of configuration=|n9/2[505]~#|p5/2[402], K|p=2- (1976Ha39, 1974Ya02) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$157.6|g (M1) from 1+; 162.1|g (M2) to (2)- 
$Configuration=|n9/2[505]~#|p9/2[514], K|p=0+ (1976Ha39, 1974Ya02) 
T$>0.94 |ms (from RUL(M2)<1) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E$from measured mass difference between the isomer and the g.s. (2012Re19). Other: 227 {I40} from an earlier ESR measurement at the same lab as 2012Re19 
J$log{Ift}=7.9 to 5-; weak |b{+-} feeding of (8)+; a (6)- isomer is known in {+188}Re at 169 keV. Also proposed configuration=|n7/2[503]~#|p5/2[402], K|p=6- (1976Ha39, 1974Ya02). J|p can also be 7- from configuration=|n9/2[505]~#|p5/2[402], same as for the g.s., but with K|p=7-, according to GM rule. 
T$weighted average of 3.3 h {I2} (1974Ya02), 3.0 h {I5} (1972Ru06), and 2.96 h {I20} (1973DeWI)in {+190}Re IT decay. The original uncertainty of 0.10 in 1973DeWI seems too small (probably statistical only) and has been increased by a factor of 2 in the average by the evaluators. Other: 2.8 h (1962Ba60) 
$%IT: deduced by the evaluators from |g+ce intensity balances of |g transitions in {+190}Os from |b{+-} decays of the 3.0-min g.s. and the 3.1-h isomer of {+190}Re in equilibrium (which means the total number of {+190}Re g.s. decays is equal to the total number of {+190}Re IT decays that feeds the g.s.) measured by 1974Ya02. Note that the relative |g intensities given as for {+190}Re isomer |b{+-} decay in 1974Ya02 are actually for the combination of {+190}Re isomer and g.s. |b{+-} decays, with the latter fed by the IT decays of {+190}Re isomer in equilibrium. See those decay datasets of {+190}Os for more details. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: MIN
level_comment:
$Number of ions detected>40 (2012Re19) 
$Configuration=|p5/2[402]~#|n9/2[505], K{+|p}=2- (1974Ya02) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E$from measured mass difference between the isomer and the g.s. (2012Re19), with number of ions detected>60 
T$the adopted value is from weighted average of 3.3 h {I2} (1974Ya02), 3.0 h {I5} (1972Ru06), and 2.96 h {I20} (1973DeWI). The original uncertainty of 0.10 in 1973DeWI seems too small (probably statistical only) and has been increased by a factor of 2 in the average by the evaluators. Other: 2.8 h (1962Ba60) 
$Configuration=|p5/2[402]~#|n7/2[503], K{+|p}=6- (1974Ya02). Also possible configuration=|n9/2[505]~#|p5/2[402], same as for the g.s., but with K|p=7-, according to GM rule. 


level_energy_unit: KEV
level_spin_parity: (3/2+,1/2+)
level_lifetime_unit: MIN
level_comment:
Probable doublet comprised of J=1/2 and J=3/2 members of the 1/2[411] rotational band. 
T From Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_comment:
Doublet comprised of the J=5/2 and 7/2 members of the 1/2[411] band. Transition strength relative to g.s. doublet agrees well with experimental values in {+187}Re and {+189}Re, but it disagrees with the theoretical value. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
Possible vibrational state analogous to the 512-keV state in {+187}Re, although the transition strength is twice that of {+191}Re. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J by analogy with the second J=11/2 {+187}Re and {+189}Re, where state with a larger transition strength (charge exchange) was observed. 


level_energy_unit: KEV
level_spin_parity: (3/2+,1/2+)
level_lifetime_unit: MIN
level_comment:
E|b{+-}=1800 keV {I200} (1953At24 - absorption measurement). 
Probable doublet comprised of J=1/2 and J=3/2 members of the 1/2[411] rotational band. 
T$from 1953At24. Assignment to {+191}Re was based on chemical separation and production of the isotope by (n,p). Measured |b{+-} (1953At24). Other value: 9.70 min (1970HaZI). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E$From (t,|a),(pol t,|a). Least squares fit of E|g yields 285.1, |DE|g(140.0) not available. 
J$M1+E2 140.0|g to (9/2-), band member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2-)
level_comment:
J |g to (11/2-) and (9/2-). Assigned as a bandhead in comparison with that in {+187}Re and {+189}Re ({+136}Xe,x|g - 2016Re02). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J by analogy with the second J=11/2 in {+187}Re and {+189}Re, where state with a larger transition strength (charge exchange) was observed. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (25/2-)
level_lifetime_unit: US
level_comment:
E 0+x level in ({+208}Pb,x|g) probably is the same level in consideration of the level lifetime. 
J 93.8|g (M2) (21/2+), 115.9|g (E2) to (21/2-), band member. 
T$From |t=73 |ms {I5} ({+136}Xe,X|g) - |g(t). Other: 77 |ms {I33} ({+208}Pb,x|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_comment:
E$May be the same level at 1601.6 in adopted dataset, based on comparable lifetime of the level. In 2011St21 and 2005Ca02, isomer level energy was not determined. 
T$From |g(t) of the delayed |g rays (2011St21). Other: 1-75 |ms (2005Ca02 - lower counting statistics did not permit the quantitative determination of decay half-lives. However, the recording time ranges provide constraint on the isomer half-life). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2-)
level_comment:
J$|g to (11/2-) and (9/2-). Bandhead assignment in comparison with that in {+187}Re and {+189}Re (2016Re02) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_uncertain: ?
level_comment:
E x |<50 keV; upper limit based on energy threshold for experimental arrangement used by 2005Ca02 in IT decay. 
T from K| x ray(t) and 160|g(t) (2008StZY) in IT decay (85 |ms). Others: 120 |ms {I+210-50} (2005Ca02) and 93 |ms {I15} (2009Al30) from decay-time spectra of delayed (3-350 |ms) events in {+192}Re IT decay (85 |ms). The weighted average of data from 2008StZY and 2009Al30 is 87 |ms {I8}. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_uncertain: ?
level_comment:
T from K| x ray-160|g(t) (2008StZY,2011St21). Others: 93 |ms {I15} from 2009Al30 based on time spectrum of delayed events associated with the isomer in a 3 |ms to 350 |ms time window; 120 |ms {I+210-50}, measured by 2005Ca02 at the final focus of the FRS for ions at rest. 
E x |<50 keV. This upper limit is based on energy threshold for the experimental arrangement used by 2005Ca02 and it is lower than K-shell binding energy for Re. 
Isomeric state population ratio: 3% {I1} (2011St21). 


level_energy_unit: KEV
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
E from time-resolved Schottky mass spectrometry (2012ReZZ). 
T Lorentz-corrected value from 2012ReZZ. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
E$ from measured mass difference between the isomer and g.s. (2012Re19) 
T$ measured in 2012Re19 for bare {+186}W ion. 
$ Number of ions detected>27 
$ Isomer to g.s. transitions were observed from the isomer, implying |g-ray emission 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_lifetime_unit: US
level_comment:
T$Weighted average of 65 |ms {I9} (2011St21) and 72 |ms {I8} (2009Al30, 2009Al16). Uncertainty lower input value. Other: 75 |ms {I+450-40}, upper-limit corresponds to 100% isomeric formation ratio (2005Ca02). 
$Experimental isomeric state population ratio=16% {I+4-5} (2011St21) 


level_energy_unit: KEV
level_spin_parity: (0+,1)
level_lifetime_unit: S
level_comment:
$The |b{+-} decay is the only decay mode observed 
T$from decay curve for 478|g (2012Al05, previous value of 7.6 s {I23} in 2009ReZW); 6 s {I1} is also mentioned in authors' text, as also referred in 2014Mo15. Other: 1.0 s {I5}, deduced from position-time correlations between the implanted fragments and the subsequent |b-decay in 2009Ku28, but half-life retracted by authors in their later analysis in 2014Ku23 
$Approximate number of nuclei implanted in the plastic stopper reported to be 101200 {I300} (2009St16,2008StZY) 
J$from Nilsson multi-quasiparticle (MQP) calculations, 2012Al05 proposed low-lying oblate state of 0+, 1- and 1+ with configurations: |n1/2[660]|^~#|p1/2[411]|_ at 64 keV, |n1/2[660]|^~#|p1/2[550]|^ at 0, and |n1/2[660]|^~#|p3/2[402]|_ at 174 keV, respectively, which by |b{+-} decay possibly populates 0+ g.s. and excited 0+ at 696.5 keV in {+194}Os. 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$from Nilsson multi-quasiparticle (MQP) calculations, 2012Al05 proposed this level as a low-lying prolate state with configuration of |n13/2[606]|^~#|p9/2[514]|^, which by |b{+-} decay populates possible high-spin (|?10-11) cascade 554|g |) 349|g |)194|g in {+194}Os. Note that theoretical energy for this prolate state is calculated at 46 keV, in disagreement with the measured energy of 285 keV in 2012Re19 
T$decay spectra for 194|g, 349|g, 554|g give T{-1/2}=32 s {I8}, 25 s {I8}, 25 s {I8}, respectively 


level_energy_unit: KEV
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$This isomer possibly feeds the 6+ state in {+194}Os. Decay spectra for 218|g, 383|g, 530|g give T{-1/2}=40 s {I8}, 46 s {I8}, 100 s {I10}, respectively 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
E,T$isomer identified by 2005Ca02 and 2011St21 in {+9}Be({+208}Pb,X|g) E=1 GeV/nucleon. Half-life is from 2011St21. Other: 1-75 |ms (2005Ca02). It is possible that there are two different isomers, the one reported by 2005Ca02 with T{-1/2}=1-75 |ms decaying by |g rays of 128, 148 and 464 keV in a delayed |g-ray spectrum; and the second by 2011St21 decaying by only the 86.3-keV |g ray. As the two half-lives overlap within the uncertainties, evaluators assume only one isomer. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$it is possible there are two different isomers, the one reported by 2005Ca02 decaying by |g rays of 128, 148 and 464 keV in the delayed |g-ray spectrum; and the other by 2011St21 decaying by only the 86.3-keV |g ray 
T$from decay curve of delayed Re x rays and |g ray (2011St21). Other: 1 to 75 |ms (2005Ca02), counting statistics did not permit the quantitative determination of decay half-lives. However, the recording time ranges provide constraints on the isomer half-life. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_lifetime_unit: S
level_comment:
$Approximate number of nuclei implanted in the plastic stopper reported to be 60800 {I200} (2009St16,2008StZY) 
E$ the observed fragments are assumed to be in the ground state of {+195}Re nuclei 
$The |b{+-} decay is the only decay mode expected 
T$ deduced from position-time correlations between the implanted fragments and the subsequent |b-decay (2009Ku28). Others: T{-1/2}=3.29 s is predicted by 1997Mo25, 30 s from systematics (2011AuZY) 
J$ 3/2- predicted in 1997Mo25 calculations 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$3/2- is predicted in 1997Mo25 calculations 
T$the half-life was deduced from position-time correlations between the implanted fragments and the subsequent |b decay (2009Ku28). Other: T{-1/2}=3.29 s is predicted in 1997Mo25 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$ measured by 2009Ku28, time correlations between implanted fragments and |b decay. Comparison of measured half-life with model calculations (2012Be38) 
$ Only |b{+-} decay mode is expected. Predicted %|b{+-}n=0 (1997Mo25) 
J$ 1/2- for valence proton and 1/2- for valence neutron predicted (1997Mo25) 
$ For production |s, see figure 3 in 2012Ku26 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Only |b{+-} decay mode is expected. 
E$ the observed {+197}Re fragments assumed to correspond to the g.s. 
J$5/2+ suggested from systematics (2012Au07); 1/2- predicted (1997Mo25) 
T$ limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by 300 ms from systematics (2012Au07); 4.9 s from theoretical calculations (1997Mo25) 
$ For production |s, see figure 3 in 2012Ku26 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Only |b{+-} decay mode is expected. Predicted %|b{+-}n=0 (1997Mo25) 
E$The observed {+198}Re fragments assumed to correspond to the g.s. 
J$1/2- for valence proton and 3/2- for valence neutron predicted (1997Mo25) 
T$Limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by 300 ms from systematics (2012Au07), and 2.3 s from theoretical calculations (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E$The observed {+198}Re fragments assumed to correspond to the g.s. 
T$Limiting value from time-of-flight of 160 ns. 
$Production |s=0.028 nb {I7}. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Only |b{+-} decay mode is expected. Predicted %|b{+-}n=0 (1997Mo25) 
E$ the observed {+199}Re fragments assumed to correspond to the g.s. 
J$ 1/2- predicted (1997Mo25) 
T$ limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by 2.38 s from theoretical calculations (1997Mo25) 
$ Production |s=0.0076 nb {I27} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
E assumes that the observed activity represents the {+161}Os g.s. 
%A The theoretical calculations of 1997Mo25 give a value of 167 ms for the |b decay halflife of {+161}Os, suggesting that |a decay is the dominant decay mode for this nuclide. 
J proposed configuration is |nf{-7/2}, proposed by 2010Bi03 based on an analysis of the |a branching to the {+157}W levels, assumed to Be (7/2-) and (9/2-) for the g.s. and 318-keV, respectively. The {+157}W g.s. assignment was proposed by 2008PaZV based on the observation that, among the expected available orbitals, only |nf{-7/2} accounts for the |e feeding with comparable intensities to the 11/2- and 1/2+ levels in the daughter nucleus, {+161}Ta. 
T from analysis of the decay of the |a peaks using the method of maximum likelihood, 2010Bi03 deduce T{-1/2}=640 |ms {i60}. 2008PaZV report T{-1/2}=590 |ms. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T weighted average of 1.9 ms {I2} (2000Ma95, |a(t)) and 2.1 ms {I1} (2004Jo12, |a(t)). Others: 1.5 ms {I+7-5}, (1996Bi07, |a(t)); and 1.9 ms {I7}, (1989Ho12, |a(t)). 
%A From measured T{-1/2} value and T{-1/2} value for |e+|b{++} decay computed by 1997Mo25 (0.153 s), one estimates %|e+%|b{++}=1.4. From intensities observed in the parent-daughter correlated |a-decay data (1996Bi07), %|a|?100. From theoretical estimate by 1973Ta30 of T{-1/2} for |e+|b{++} decay, %|e+%|b{++}|?0.2. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
E regardless of the ordering of the |g's deexciting this level and those lying below it, this energy may be independent of that ordering. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$from 1996Bi07. Others: 12 ms {I+11-7} (1996Pa01); 7.5 ms {I+42-20} (2001Ke05). 
%A$from parent-daughter intensity correlations (1996Bi07) 
$%|e+%|b{++}<2% from theoretical (1997Mo25) |b-decay T{-1/2}=0.226 s and |a-decay T{-1/2}=4.79 ms 
J$l=5 proton decay (involving the |ph{-11/2} orbital) from a high-spin (probably 9+) state in {+164}Ir. Probable configuration=|nf{-7/2}. Systematics (2012Au07) also support 7/2- 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%A$96 {I5} from measurement by 2008Bi15, based on the observation of fraction of {+168}Pt |a-parent nuclei correlated with |a-decay of {+164}Os, |g-ray tagging method was used by placing gate on 575-587-keV |g. Others: %|a=98 {I2}, deduced from the measured T{-1/2}=21 ms {I1} and from partial theoretical |b half-lives from 1973Ta30 and 1997Mo25; 100% {I70} (1981Ho10), |?95% (1996Bi07, from parent-daughter activities). 
T$from |a decay (1996Pa01). Others: 27 ms {I4} (1996Bi07), 41 ms {I20} (1981Ho10) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$%|a is measured by 2008Bi15 from correlated |a events in {+169}Pt -> {+165}Os -> {+161}W |a decay chain. Other: 100 {I40} (1981Ho10). 
$%|e+%|b{++} is assumed to be 100-%|a; this decay branch has not been observed 
J$from 1997Da07, based on proton decay from {+166}Ir. Possible configuration=|nf{-7/2} from systematics 
T$from timing of |a decay of {+165}Os (1996Pa01). Others: 72 ms {I8} (1991Se01), 65 ms {I+70-30} (1981Ho10) 
$E(|a)=6188 {I7} (1996Pa01), 6164 {I10} (1981Ho10), 6200 {I20} (1978Ca11,1977Ca23) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
J even-even nucleus ground state. 
T$weighted average of 210 ms {I6} (2015Li24), 220 ms {I7} (1996Pa01; 6000|a(t)), 194 ms {I17} (1991Se01) and 181 ms {I38} (1981Ho10). Other: 0.3 s {I1} (1978Ca11). 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
E an alternative value (E=1647.3) is possible because the order of the 626|g-704|g cascade is not established. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2015Li24 from recoil-|a-|a-|a correlations. Authors note that this half-life is in agreement with 220 ms {I7} from 1996Pa01: Phys. Rev. C53, 660. 
$Measured E|a by 2015Li24 is in agreement with literature value of 6000 keV {I6} (1996Pa01: Phys. Rev. C53, 660); value not listed by 2015Li24, only labeled as 6000 keV in their figure 1b. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
%A$others: 58% {I12} (1981Ho10, from positions and intensities of correlated parent/daughter events); 76% {I10} (1982En03, from matching of {+171}Pt-{+167}Os velocity distributions following recoil-mass selection of the evaporation residues formed by 5-neutron emission from {+176}Pt); and 49% {I7} (1996Pa01). 
$%|e+%|b{++} from 100-%|a 
T$from 2010Sc02, measured from |a-decay correlated with 3-s recoils. Others: 0.65 s {I15} (1977Ca23,1978Ca11), 1.05 s {I35} (1981Ho10), 0.8 s {I2} (1982En03), 0.84 s {I7} (1996Pa01). 
T$value of 835 ms {I9} in Fig. 8 is a misprint as confirmed in an e-mail reply from C. Scholey on Feb 4, 2010. 
$Unweighted averages: %|a=61 {I8}, T{-1/2}=0.84 s {I8}. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$from 2010Sc02, measured from time differences between recoil implantations and delayed |g rays detected in the GREAT focal plane spectrometer. Delayed |g rays were observed at 86.7 and 347.6 keV. Note that T{-1/2}=672 ns {I7} stated in level-scheme Fig. 11 of 2010Sc02 is a misprint, as communicated in an e-mail reply from C. Scholey on Feb 5, 2010 


level_energy_unit: KEV
level_comment:
J$(23/2-) assigned by 2001Jo11 in {+112}Sn({+58}Ni,2pn|g), but none assigned in 2009Od02 since mult(990.8|g) could not be established 


level_energy_unit: KEV
level_comment:
J$(27/2-) assigned by 2001Jo11 in {+112}Sn({+58}Ni,2pn|g), but none assigned in 2009Od02 since mult(488.4|g) could not be established 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J,T$from Adopted Levels, with data adopted from 2010Sc02 in {+167}Os IT decay. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$from 2010Sc02, measured from |a-decay correlated with 3-s recoils. 
T$value of 835 ms {I9} in Fig. 8 is a misprint as confirmed in an e-mail reply from C. Scholey on Feb 4, 2010 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$from 2010Sc02, measured from time differences between recoil implantations and delayed |g rays detected in the GREAT focal plane spectrometer. Delayed |g rays were observed at 86.7 and 347.6 keV. Note that T{-1/2}=672 ns {I7} stated in level-scheme Fig. 11 of 2010Sc02 is a misprint, as communicated in an e-mail reply from C. Scholey to Balraj Singh on Feb 5, 2010 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
J even-even nucleus ground state. 
T from |a decay. Weighted average of 1.9 s {I1} (1978Ca11), 2.0 s and 2.4 s {I2} (1978Sc26), 2.2 s {I1} (1982En03), 2.0 s {I2} (1984Sc06), 2.1 s {I6} (1995Hi02), 2.1 s {I1} (1996Pa01), 2.6 s {I2} (2004GoZZ). 
%|a: weighted average of 49 {I3} from matching of {+172}Pt-{+168}Os velocity distributions following recoil-mass selection of the evaporation residues formed by neutron emission from {+176}Pt (4n) (1982En03), 40 {I3} from (1996Pa01) and 36 {I4} (2004GoZZ). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
%A Weighted average of 15 {I4} (2004GoZZ; 12% {I3} for 5581|a), 13.8 {I13} (1996Pa01; 11% {I1} for 5576|a), 13 {I2} (1995Hi02), 13.8 {I13} (1982En03; 11% {I1} for 5572|a) assuming 5580|a constitutes 80% of {+169}Os |a decay (1984Sc06). 
J unhindered |a decay to (5/2-) {+165}W g.s.. Configuration proposed by 1995Hi02 is 5/2[523]. 
T unweighted average of 3.0 s {I5} (1972To19, 5560|a), 3.2 s {I2} (1978Sc26, 5570|a), 3.4 s {I2} (1982En03, 5572|a), 3.5 s {I2} (1984Sc06, 5564|a), 3.2 s {I3} (1995Hi02, 5578|a), 3.6 s {I2} (1996Pa01, 5576|a), 4.1 s {I4} (2004GoZZ, 5581|a). The weighted average of these data is 3.43 s {I9}. Others: 1978ReZZ, 3.5 s {I2} (1984Sc06, 5470|a-5540|a), 3.4 s {I8} (1995Hi02, 5536|a), 6 s {I3} (1995Hi02, 5508|a). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
%A$weighted average of 12 {I1} (1982En03), 8.6 {I6} (1996Pa01), and 10 {I3} (2004GoZZ). The unweighted average of these data is 10.2 {I10}. Others: %|a=3 estimated by 1978Sc26 based on comparison of measured |a intensities and calculated excitation function for reaction producing {+170}Os; 5 {I1} (1995Hi02, assuming 162|g and 216|g in {+170}Re are M1) or 9 {I2} (1995Hi02, neglecting internal conversion of 162|g and 216|g). Calculated values: 2017Ph01, 2017Zh03, 2016Sa16, 2016Su09, 2015Ab11, 2014Gi01. 
T 7.37 s {I18} from weighted average of 7.2 s {I2} (2004GoZZ, 5410|a(t); units misprinted as ms instead of s), 9 s {I1} (1996Pa01), 7.9 s {I3} (1995Hi02, 5403|a(t)), 9.3 s {I16} (1995Hi02, 162|g(t)), 8.5 s {I5} (1995Hi02, 216|g(t)), 6.9 s {I8} (1984Sc06), 7.1 s {I2} (1982En03), 7.1 s {I5} (1972To06); the unweighted average of these data is 7.9 s {I3}. Other: 4.0 s {I2} (1978Sc26). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
$%|a: weighted average of 1.7 {I3} (1979Ha10) (deduced from intensity ratio of {+171}Os daughter |a's and {+175}Pt parent |a's in same spectrum) and 1.9 {I3} (1995Hi02) (assuming mult=E2 for the 190|g({+171}Re) produced in {+171}Os |e decay). 
T$from 5241|a(t) (1995Hi02). Others: 7.8 s {I10} (1978Sc26), 8.2 s {I8} (1972To06), 10.0 s {I10} (1995Hi02, 190|g(t)), 8.0 s {I24} (1995Hi02, 705|g(t)) and 8 s {I2} (1995Hi02, 5166|a(t)). Weighted average of all data is also 8.3 s {I2}. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=4.7 eb {I4} (2021Zh52) 
T$using recoil-gated |g|g-coin spectra at 253.8 keV (17/2+ |) 13/2+) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=4.4 eb {I6} (2021Zh52) 
T$using recoil-gated |g|g-coin spectra at 447.7 keV (21/2+ |) 17/2+) on (feeding) 627.7 keV (29/2+ -> 25/2+) 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=4.6 eb {I16} (2021Zh52) 
T$using recoil-gated |g|g-coin spectra at 566.8 keV (25/2+ |) 21/2+) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=4.3 eb {I11} (2021Zh52) 
T$using singles spectra at 627.7 keV (29/2+ |) 25/2+). Authors assume unobserved side-feeding does not significantly affect the lifetime. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
Level based on the ordering of 221-354 cascade given by 1990Ba29. 1989We06 suggested the opposite order implying a level at 2282 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
$%|a from 1995Hi02. %|a=0.021 {I9} (1971Bo06) 
J$Favored |a decay from 5/2- {+177}Pt. 5/2- 5/2[523] Nilsson state assigned, as for the neighboring N=97 isotones {+171}W, {+169}Hf, and {+167}Yb. 
T$from |a(t), |g-K| x ray(t) (1995Hi02). Other: 22.4 s |a(t) (2002Du22); 16 s {I5} (1971Bo06). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (13/2+)
level_comment:
J$13/2+ 5/2[642] Nilsson state assignment from systematics for N=97 isotones and features of band structure. x<60 keV, estimated by 1990Ba29. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
T$estimate from prompt |g|g-timing width (1992Bo21); 1990Ba29 estimate several microseconds in (HI,xn|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 11/2+
level_comment:
J$1990Ba29 proposed (13/2) from mult=dipole for 218.6|g, in disagreement with results from 1991Ka05. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
T$from Adopted Levels in ENSDF (2015 update) 
$Compilers' note: it is not clear whether 141.3, (9/2+) level is a member of the band with configuration=|n5/2[642], i{-13/2}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 45 s {I5} (1973Be67) and 42 s {I6} (1972Be89). 
%|e=99.98 {I1}; %|a=0.02 {I1} 
%A From 1971Bo06 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_lifetime_unit: PS
level_comment:
J$may not be a band head (1990Fa02). It has been assigned as the J=5 member of a K|p=3- band in {+174}Ir |e decay. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
J$the assignment of the ground-state configuration to 5/2[512] is based on the values of g{-K}-g{-R} determined from crossover-cascade branching ratios in ({+29}Si,4n|g). 
T$from 1972Be89. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) in ({+29}Si,4n|g). 
J$105.7|g (E1) and assigned from 7/2[633] Nilsson configuration as such bands present throughout the odd Os isotopes at low spin levels in ({+29}Si,4n|g). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
J$The assignment of the ground-state configuration to 5/2[512] is based on the values of g{-K}-g{-R} determined from crossover-cascade branching ratios. 
T$From 1972Be89. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_comment:
T$from |g|g(t). 
J$105.7|g (E1) and assigned from 7/2[633] Nilsson configuration as such bands present throughout the odd Os isotopes at low spin levels. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
J$Favored |a-decay from the {+181}Pt g.s. (J|p=1/2-); strong |e+|b{++} feeding to the 1/2- and 3/2- levels in {+177}Re; J|p systematics; configuration assignment. 
T$Weighted average of 2.8 min {I3} (1976Be62), 3.1 min {I2} (weighted average of 3.0 min {I5} (157|g), 3.1 min {I2} (196|g), 3.5 min {I5} (300|g) and 3.0 min {I7} (457|g) from 1972Be89) and 3.5 min {I8} (1970Ar15). Other: 3.8 min {I5} (84|g) in 1972Be89, but this value was excluded since E|g overlaps with 81.5|g following decay of {+176}Os (T{-1/2}=3.6 min {I5}). 
CONF$|n1/2[521] (p{-3/2}) Nilsson configuration. Based on the measured J|p, the favored |a-decay from the J|p=1/2- g.s. (|n1/2[521]) of {+181}Pt, the observed in band properties, such as large signature splitting and rotational alignment, and configuration systematics. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
J$152.3|g to 1/2-; J|p systematics; band assignment. 
T$From |g|g(t) by gating on |g rays below and above the isomer in {+164}Er({+17}O,4n|g), {+166}Er({+16}O,5n|g) (1983Dr05). 
CONF$|n5/2[512] (h{-9/2}) Nilsson configuration. Supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
J$60.2|g to 7/2-, 148.3|g (E1) to 5/2-; band assignment. 
T$From n|g(t) by gating on the 148.3|g in {+164}Er({+17}O,4n|g), {+166}Er({+16}O,5n|g) (1983Dr05). 
CONF$|n7/2[633] Coriolis-mixed (i{-13/2}) Nilsson configuration. Supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values. The assignment is consistent with the measured E1 transition strength for 60.2|g and 148.3|g, and systematics of similar transitions in neighboring nuclei. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T from 1972Be89. 
%|e+%|b adopted from 2003Au02 
Quadrupole deformation |b{-2}=0.209 {i7} (2005Mo33). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J E2 132.2 keV |g ray to the 0{++} g.s., and E0 component in the 732.2 keV transition from the 2{++} 864 keV level. 
T Average from two methods: a) electronic timing using a pulsed {+16}O beam on {+166}Er at 80 MeV, with an 2.6 ns FWHM pulse; b) recoil distance Doppler shift (2005Mo33,2005De48). 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J E2 266.6-keV |g ray to the 2{++} 132 keV level, and E2 372.1 keV |g ray from the 2{++} 772 keV level. Rotational g.s. band level sequence indicates J|p=4{++}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
This level proposed as bandhead for a K|p=0{++} |b rotational band from {+178}Ir |e decay studies (1994Ki01) (see dataset). 
J E2 518.0-keV |g ray to the 2{++} 132 keV level. Band-head of the |b band suggests J|p=0{++}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J E2 864.4 keV |g ray to the 0{++} g.s., and E0 component in the 732.2 keV transition to the 2{++} 132 keV level. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J E0 component in the 624.4 keV transition to the 4{++} 399 keV level. Agreement with level sequence in |b band. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J M1+E2 multipolarities of the 633.0 keV transition to the 4{++} 399 keV level, and of the 899.7 keV transition to the 2{++} 132 keV level, establish the J|p=3{++} value uniquely. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J M1+E2 814.2-keV transition to the 4{++} 399 keV level, E2 1080.7 keV transition to the 2{++} 132 keV level. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J E0 component in 634.4 keV transition to the 6{++} 762 keV level, E2 372.6 keV transition to the 4{++} 1023 keV level. 


level_energy_unit: KEV
level_spin_parity: (5+,6+)
level_comment:
J M1+E2 654.8-keV transition to the 6{++} 762 keV level, and E2 1017.7 keV transition to the 4{++} 399 keV level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (4+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
See Comment for this level and band in the (HI,xn|g) dataset 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J E2 132.2 keV |g ray to the 0{++} g.s., and E0 component in the 732.2 keV transition from the 2{++} 864 keV level. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J E2 266.6-keV |g ray to the 2{++} 132 keV level, and E2 372.1 keV |g ray from the 2{++} 772 keV level, which allows the range (0+ to 4+). Rotational g.s. band level sequence indicates J|p=4{++}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J E2 518.0 keV |g ray to the 2{++} 132 keV level, which allows the range (0+ to 4+). Band-head of the |b band suggests J|p=0{++}. If that is correct, the 650 keV |g ray deexciting to the 0{++} g.s. would have to have pure E0 character. The available spectra in 1994Ki01 do not allow to decide this issue unambiguously (see also Comment for the 650.4 keV transition). 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J M1+E2 654.8-keV transition to the 6{++} 762 keV level, and E2 1017.7 keV transition to the 4{++} 399 keV level. Those acutally allow (5+,6+) as possible J|p values. A value of 6+ would imply an M3 multipolarity for the 384.5 keV |g ray to the 3{++} 1032 keV level. If this possibility can not be excluded, a J|p=(5+,6+) should probably be quoted instead of the 5+ assignment in 1994Ki01. 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
B(E1,587)/B(E2,242)=7.5|*10{+-7} {i11} b{+-1}, B(E1,1020)/B(E2,242)=0.35|*10{+-7} {i5} b{+-1} (1982Dr03) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (4+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
This is the lowest identified level for a proposed |b band in 1982Dr03. These authors propose, on the basis of unassigned strong lines in the electron spectra at 689 and 692 keV, that these might represent E0 transitions linking to the g.s. band levels. They thus suggest for the energy of this level x|?1167 keV, assuming a 689 keV transition connecting from the second level of this new band to the 6{++} state in the g.s. band. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T weighted average of 6.3 min {I3} (1976Be62), 6.5 min {I5} (1973GoYJ), 9 min {I2} (1971NaZV), and 8 min {I1} (1968Be43). Others: 1972Be89, 1970Ar15. 
J unhindered |a decay (HF=1.2) from 1/2- {+183}Pt g.s. 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: US
level_lifetime_info: ;ERR=?
level_comment:
J M1 45|g to 5/2- 100; band assignment. 7/2[514] Nilsson orbital assigned by analogy with {+181}Os. T{-1/2} of this level is consistent with the degree of K-forbiddenness of the transition to the J|p=(5/2-) member of the 1/2[521] g.s. rotational band. 
T from |g|g(t), gating on transitions above and below the 146 level, and from two-component fits to 86.3|g and 100.3|g time spectra in n-|g(t) in ({+16}O,4n|g) (1983Dr05). 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_comment:
J if band assignment is correct, the 327 keV cascade |g feeding from the (29/2-) band member would be expected to be E2. The DCO ratio of 1.3 {I3} for the 245|g deexciting to a (25/2-) level cannot differentiate between pure Q and pure D multipolarity; the level scheme requires D, |DJ=0. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: US
level_lifetime_info: ;ERR=?
level_comment:
T from |g|g(t), gating on transitions above and below the 146 level, and from two-component fits to 86|g and 100|g time spectra in n-|g(t) (1983Dr05). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 23 min {I3} (1965Be32), 21 min {I2} (1966Be41), 21.7 min {I6} (1966Ho16), 23 min {I2} (1968Ko10) following the decay of 20|g, 19.8 min {I10} (1969Hu03), and 22.0 min {I8} (1970Ar15). T{-1/2}=25.5 min {I4} also obtained by 1968Ko10 from a |g|g-coin measurement disagrees with all the other values and may be affected by a systematic uncertainty. The 0.4-min uncertainty reported by 1968Ko10 may represent only the deviation of the experimental points in the decay curve. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J$E2 132|g to 0+. 
T$from centroid shift method in {+168}Er({+16}O,4n|g). Other: 0.80 ns {I+21-14} from RDM in {+150}Nd({+34}S,4n|g) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J$E1+M2 492|g to 3+, E1+M2 1106|g to 4+; band member 
E$there are discrepancies in some depopulating transitions from the closely spaced 1514.6-keV and 1515.56-keV levels. {+150}Nd({+36}S,6n|g):Delayed reports only the 1515.6-keV, 4+ level and places all transitions from this level, whereas, other studies resolve the two levels and their depopulating transitions. See Adopted Gammas for further information. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$E2 258|g to 5-, E1(+M2) 605|g to 8+. 
T$from centroid shift in {+168}Er({+16}O,4n|g). Other: 17 ns {I3} from |g(t) in {+150}Nd({+36}S,6n|g):Delayed 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$E1 52|g to 6+, (E1) 671|g to 8+, 
T$from |g(t) in {+168}Er({+16}O,4n|g). Others: 15.9 ns {I21} from |g|g(t) in {+168}Er({+16}O,4n|g), 17 ns {I3} from {+150}Nd({+36}S,6n|g),{+150}Nd({+34}S,4n|g), and 26 ns {I3} from |g(t) in {+150}Nd({+36}S,6n|g):Delayed. 
$configuration=|n7/2[514]|n7/2[633] 


level_energy_unit: KEV
level_spin_parity: 8-
level_comment:
E,J$observation of a 184|g populating the 7-, 1929-keV level in {+150}Nd({+36}S,6n|g),{+150}Nd({+34}S,4n|g) results in an energy shift and change of J|p to the band members observed in {+166}Er({+18}O,4n|g),{+168}Er({+16}O,4n|g). See the latter dataset for additional comments. 


level_energy_unit: KEV
level_spin_parity: (11,12)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T$from |g|g(t) in {+150}Nd({+36}S,6n|g),{+150}Nd({+34}S,4n|g) 
J$D(+Q) 1020|g to 12-, D(+Q) 1237|g to 11- 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$from beam-|g(t) using 1134|g in 2005Mo33. Authors state a similar result is obtained by analysis of the long-lived components of the time distributions of the ground state band transitions. Other: 15.9 ns {I21} from |g|g(t) (1982Dr03). 
$configuration: |n7/2[633]|n7/2[514] 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
E$level and its isomeric character not observed in either {+150}Nd({+36}S,6n|g),{+150}Nd({+34}S,4n|g) or {+166}Er({+18}O,4n|g),{+168}Er({+16}O,4n|g) reactions and thus not included in the Adopted Levels. 
J$|>20 from the assumption that the 286.8|g and 1427|g are both |DJ=1 character 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T$from 1966Ho16. Others: 1966Be47, 1968Be43, 1969Hu03. 
J$Coriolis coupled bandhead. Shell model calculations predict the low-lying states of |n1/2[521], (g.s.) |n7/2[514] (49.22) and |n9/2[624] (156.93) configurations. The ground state is assigned as |n1/2[521], and it |e decays to 1/2-,3/2- members of 1/2[541] band in {+181}Re. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from 1967Go25. Other value: 2.8 min {I1} (1966At06). 
J$log| {Ift}|?4.7 to 9/2-[514] of {+181}Re and no population to higher band members. Band head of |n7/2[514] configuration. See comments in the J|p argument of the ground state. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (HI,xn|g) (2003Cu03). Other: 316 ns {I18} from (p,5n|g) (1974Ka19). 
J$E1 to 7/2-. See comments in the J|p argument of the ground state. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T$Other: 13 ns {I2}. quoted by 1995Ku14 in (HI,xn|g) from a priv comm. with Ts. Venkova (1990) 
$Configuration=|n7/2[514](|n9/2[624]|n5/2[512]) 
J$|DJ=0 to 21/2+, and D from 23/2- member of the K|p=23/2- t-band. 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_comment:
J$810|g to the 19/2- state of the |n7/2[514] band and 1035|g to the 17/2- state of the |n7/2[514] band 


level_energy_unit: KEV
level_spin_parity: 25/2-
level_comment:
J$189|g (M1) to the 25/2- state of the |n1/2[521] band and 622|g to the 21/2- state of the |n1/2[521] band 


level_energy_unit: KEV
level_spin_parity: 33/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
$Configuration: 5 quasiparticle state |n(7/2[514],9/2[624],1/2[521])|p(5/2[402],11/2[505]) 
J$D (|DJ=0) to 33/2- state at 2824.3; Q to 29/2- state at 2384.4 


level_energy_unit: KEV
level_spin_parity: 35/2-
level_lifetime_unit: NS
level_comment:
$Configuration: 5 quasiparticle state |n(7/2[514],9/2[624],1/2[521])|p(7/2[404],11/2[505]) 
T$from |g|g(t) (HI,xn|g) (2003Cu03). Other: 34 ns {I6} from 1991VeZV 
J$M1 to K=33/2- state 


level_energy_unit: KEV
level_spin_parity: (41/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$from the minimum lifetime obtainable from the E|g-time lifetime analysis with the large-volume GAMMASPHERE detectors in (HI,xn|g) (2003Cu03) 
J$D to (39/2+) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T$Other: 13 ns {I2} quoted by 1995Ku14 from a priv comm from Ts. Venkova (1990) 
$Configuration=|n7/2[514](|n9/2[624]|n5/2[512]) 


level_energy_unit: KEV
level_spin_parity: 35/2-
level_lifetime_unit: NS
level_comment:
$Configuration: 5 quasiparticle state n(7/2[514],9/2[624],1/2[521]) |p(7/2[404], 11/2[505]) 
T$Other: 34 ns {I6} from |g|g time spectra (1991VeZV) 


level_energy_unit: KEV
level_spin_parity: (41/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$from the minimum lifetime obtainable from the E|g-time lifetime analysis with the large-volume GAMMASPHERE detectors (2003Cu03) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
J$ABMR measurement of spin (1978Ru04,1975Ru06) 
T$weighted average of 22.0 h {I2} (1976Ka22), 22.10 h {I25} (1973Sv01), 22.6 h {I24} (1969Hu03), 21.1 h {I3} (1960Ne03) and 21.9 h {I1} (1958Fo47); reduced |h{+2}=2. Values of 20.0 h {I2} (1963Gr22) and 24 h {I1} (1950St89) seem discrepant, thus not included in the averaging procedure. Weighted average of all the measurements is: 21.6 h {I3}, but with reduced |h{+2}=17. Other: 1966Be47 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$from |g|g(t) in {+182}Ir |e decay (1970BrZP). Other: 0.95 ns {I10} (1972HuZL,1970ErZY). 2001Ra27 evaluation of these two measurements lists 832 ps {I69} 


level_energy_unit: KEV
level_spin_parity: (13-)
level_comment:
J$|g to 11(-); possible K|p=13- with a 4-quasiparticle configuration=|n[(7/2[514])(9/2[624])]~#|p[(9/2[514])(1/2[541])] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: (20+)
level_comment:
J$|gs to (20+) and (19); possible K|p=20+, 6-quasiparticle state with, configuration=|n[(7/2[503])(9/2[624])(7/2[514])(7/2[633])]~# |p[(9/2[514])(1/2[541])] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: (21+)
level_comment:
J$|DJ=1, (M1+E2) |g to (20+); |DJ=2 |g to (19+); possible K|p=21+, 6-quasiparticle state with configuration= |n[(9/2[505])(9/2[624])(7/2[514])(7/2[633])]~#|p[(9/2[514])(1/2[541])] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: (22+)
level_comment:
J$|DJ=1, (M1+E2) |g to (21+); possible K|p=21+, 6-quasiparticle state with configuration=|n[(9/2[505])(11/2[615])(7/2[514])(7/2[633])]~# |p[(9/2[514])(1/2[541])] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: (23+)
level_comment:
J$|DJ=1, (M1+E2) |g to (22+); |DJ=2 |g to (21+); possible K|p=23+, 6-quasiparticle state with configuration= |n[(9/2[505])(11/2[615])(7/2[514])(7/2[633])]~#|p[(9/2[514])(3/2[532])] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: (25+)
level_lifetime_unit: NS
level_comment:
MOMM1$from g factor=+0.425 {I8} (|g(|q,H,t) 1989Al19) 
MOME2$observation of time dependent quadrupole interaction pattern of |g radiation (TDPAD) (1991Br25) 
J$|DJ=1, (M1+E2) |g to 24+; |DJ=2 |g to (23+); possible K|p=25+, 6-quasiparticle state with configuration= |n[(9/2[624])(7/2[633])(7/2[503])(7/2[514])]~#|p[(9/2[514])(11/2[505])] (1989Al19,1988Ch27). This gives g factor=0.38, in agreement with the measured value 
T$from |g|g(t) in ({+36}S,4n|g) (1989Al19). Other: 130 ns {I20} (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: 20(+)
level_comment:
$K|p=20+, configuration= |n7/2[503]~#|n9/2[624]~#|n7/2[514]~#|n7/2[633]~#|p9/2[514]~#|p 1/2[541] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: 21(+)
level_comment:
$K|p=21+, configuration= |n9/2[505]~#|n9/2[624]~#|n7/2[514]~#|n7/2[633]~#|p9/2[514]~#|p1/2[541] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: 22(+)
level_comment:
$K|p=22+, configuration= |n9/2[505]~#|n11/2[615]~#|n7/2[514]~#|n7/2[633]~#|p9/2[514]~#|p1/2[541] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: 23(+)
level_comment:
$K|p=23+, configuration= |n9/2[505]~#|n11/2[615]~#|n7/2[514]~#|n7/2[633]~#|p9/2[514]~#|p3/2[532] (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: 25(+)
level_lifetime_unit: NS
level_comment:
MOME2$observation of time dependent quadrupole interaction pattern of |g radiation 
$g factor from |g(|q,H,t) 
$K|p=25+, configuration= |n9/2[624]~#|n7/2[633]~#|n7/2[503]~#|n7/2[514]~#|p9/2[514]~#|p11/2[505] (1989Al19,1988Ch27). This gives g factor=0.38 
T$|g|g(t) (1989Al19). Other: 130 ns {I20} (1988Ch27) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
MOMM1 NMR on oriented nuclei; from g=(-)0.176 {I3}. 
MOME2 From static nuclear orientation with |g detection; relative to {+186}Os(137). 
J J=9/2 from atomic beam (1975Ru06). |p from comparison of |m with Nilsson prediction (-0.77) for 9/2[624] orbital. 
T from 1960Ne03, corrected for feeding by 9.9-h isomer (1975Ar33). Other values: 13.5 h {I10} (1966Be47), 14 h (1976Ka22), 15.4 h {I3} (1958Fo47). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
%IT from IT decay (9.9 h). 
J M4 171|g to 9/2+ g.s.. 
T from 1960Ne03 in IT decay (9.9 h). Other values: 10 h {I1} (1958Fo47), 9.1 h (1976Ka22). 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J (D) 1185|g to 15/2+ 375 interpreted as D |DJ=0 in ({+18}O,5n|g); 602|g to (13/2)- 958; 1341|g to 13/2+ 219; band assignment. 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_comment:
J intraband D+Q 114|g to (19/2-) 1665; intraband stretched Q 196|g to (17/2-) 1584; 523|g to 23/2+ 1256. 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2)
level_comment:
J 1710|g to 9/2- 510 and 1455|g to (7/2)- 764; log| {Ift}=7.7 (log| {If{+1u}t}<8.5) from 5/2- in |e decay. 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2)
level_comment:
J 2250|g to 9/2+ g.s.; 1857|g to (7/2)- 992; log| {Ift}=7.3 (log| {If{+1u}t}<8.5) from 5/2- in |e decay. 


level_energy_unit: KEV
level_spin_parity: (7/2)
level_comment:
J 1544|g to 9/2+ 714; 1494|g to (7/2)- 764; log| {Ift}=6.8 from 5/2- in |e decay; 1748|g to 9/2- 510. 


level_energy_unit: KEV
level_spin_parity: (33/2+)
level_comment:
J 689|g to 33/2+ 2674; 1346|g to 29/2+ 2017; intraband 617|g to 29/2(+) 2746; 841|g to (31/2+) 2522. 


level_energy_unit: KEV
level_spin_parity: (43/2-)
level_lifetime_unit: NS
level_comment:
J D, |DJ=1 351|g to (41/2+) 4716; (E1) 133|g to J|<(43/2) 4935. 
Other T{-1/2}: |?30 ns for this and/or 5167 level from (|a,7n|g). 


level_energy_unit: KEV
level_spin_parity: (43/2+)
level_lifetime_unit: NS
level_comment:
Other T{-1/2}: |?30 ns for this and/or 5067 level from (|a,7n|g). 
J D+Q 451|g to (41/2+) 4716; 1079|g to 39/2+ 4088. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
<r{+2}>{+1/2}(charge)=5.3820 {I23} (2004An14). 
T $from 1976Sp04, proportional counter measurement, 95% confidence level. Other: 1956Po16, T{-1/2}>2|*10{+13} y, nuclear emulsion, corrected by evaluator assuming natural abundance in the source. Note that, using the equation of 1961Ta22, the predicted half-life is 2|*10{+13} y; a similar prediction of T{-1/2}=1.3|*10{+15} y for {+186}Os agrees within the experimental uncertainty. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
Q: from Coulomb excitation reorientation (1972La16). 
J E2 120|g to 0+ g.s.. 
T from {+184}Ir |e decay. Other data: <2.2 ns from (|a,6n|g). 


level_energy_unit: KEV
level_spin_parity: (3+,4+)
level_comment:
J M1+E2(+E0) 1314|g to 4+ 384, E1,E2 1579|g to 2+ 120. However, 1698|g to 0+ g.s. is inconsistent with this J|p. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
J M1(+E2) 496|g to 10+ 1871; stretched E2 1092|g to 8+ 1275. 
T from ({+13}C,5n|g). Other: 20 ns {I5} from |g|g(t) in IT decay (1988Ch27). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_comment:
Band assignment from ({+18}O,4n|g) considered uncertain because J=16 to 14 transition was not verified in the ({+13}C,5n|g) study. 


level_energy_unit: KEV
level_spin_parity: (18-)
level_lifetime_unit: NS
level_comment:
T from |g|g(t) in ({+18}O,4n|g). 
Configuration=|n(9/2[624]+11/2[615])+|p(5/2[402]+11/2[505]), K|p=18-. 


level_energy_unit: KEV
level_spin_parity: (20+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
Possible configuration: (|n 11/2[615])+(|n 9/2[624])+(|p 11/2[505])+(|p 9/2[514])), K|p=20+ (2002Wh01). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T from ce-|g(t) (1971Bb09). Others: 1.18 ns {I5} (1970Be18), 1.36 ns {I3} (1970BrZP), 1.10 ns {I5} (1970ErZY). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T from Adopted Levels. 
1988Ch27 deduce g{-K}=0.21 {I5} or 0.43 {I5} based on their analysis of transitions feeding this state (253|g, 267|g, 496|g, 520|g); the uncertainty arises primarily from assumed value for g{-R} and does not include statistical uncertainty. Authors assume g{-R}=+0.32 {I5}. 


level_energy_unit: KEV
level_spin_parity: (15)
level_comment:
Not adopted. In ({+18}O,4n|g), more extensive band structure is established and the 647.5|g is placed higher in the intraband cascade than suggested in this ({+13}C,5n|g) study. 


level_energy_unit: KEV
level_spin_parity: 15-
level_comment:
Level not adopted; the 648|g deexciting it in 2002Wh01 is placed in ({+18}O,4n|g) as the J=16 to 14 transition instead of the J=15 to 13 transition of the band. 


level_energy_unit: KEV
level_spin_parity: 20+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
Possible configuration: K|p=20+, |n(11/2[615]+9/2[624])+|p(11/2[505]+9/2[514]). 
From level scheme in figure 2 of 2002Wh01, an additional unidentified |g deexcites this level, presumably the 1216|g and/or 602|g known from Adopted Levels, Gammas. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 2+, 103.6-keV level in {+180}W. Other: |> 4.6 |* 10{+16} y for decay to the 4+, 337.6-keV level in {+180}W. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for 2|n2K decay to the ground state of {+184}W. Other: > 2.0 |* 10{+16} y for 2|nKL decay to the ground state of {+184}W. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 2+, 103.6-keV level in {+180}W. Other: |> 4.8 |* 10{+16} y for decay to the 4+, 337.6-keV level in {+180}W. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
J L=0 in (p,t), J|p({+187}Os)=1/2-. 
T from 1957Jo09. Other values: 94.7 d {I28} (1947Go01), 93.4 d {I18} (1958Fo47). Others: 1948Ka08, 1951Tu09, 1960Su13, 1963Gr22. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: US
level_comment:
J energy systematics of 7/2[503] Nilsson orbital in other odd-A Os isotopes. See comments on 666 level for J|p assignment. 
T from {+185}Ir |e decay (1970FiZZ). Other: |? 3 |ms from {+183}W(|a,2n|g) (1975So01). 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: US
level_comment:
J$126.9|g M1+E2 from 9/2+, band head of |n11/2[615] rotational band. The |g transitions from the 1176.7 state of the band based on the 402.4 level to the 414.2, 590.3, 776.3 and 1025.0 states of this band and the band structures establish the the 275.5 state and 402.4 state as the band heads of the 11/2+[615] and 9/2+[624], respectively. 
T from {+185}Ir |e decay (1970FiZZ). Other: T{-1/2}|?0.7 |ms from {+183}W(|a,2n|g) (1975So01). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J 300.1|g E1 to 7/2- state of 7/2-[503] band, energy systematics of 9/2[624] Nilsson orbital in other odd-A Os isotopes. See also, the comment for J|p argument of the 275.5 state. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2)
level_comment:
J populated by primary |g ray in (n,|g); |g to 1/2- and 5/2- states. 1/2-,1/2[521] assignment has been suggested in (n,|g) by 1974Pr15. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2)
level_comment:
J populated by primary |g ray in (n,|g); |g to 1/2- and 5/2- states. 3/2-,1/2[521] assignment has been suggested in (n,|g) by 1974Pr15. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J$|g to 5/2- and 7/2- states of 1/2-[510] band; band structure. However, J=5/2-,1/2[521] assignment was suggested in (n,|g) by 1974Pr15. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E$K=3/2 band. Possible K-2 |g-vibrational state based on 1/2[510]. 
J$Large (p,t) cross section expected for coupling the 2+, |g-vibration, of even core to form the K=3/2 and 5/2 |g band. 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
J 211.4|g M1+E2 to 11/2-, Q to 9/2-; band structure. I|g(399.6|g)/I|g(342.4|g)exp=0.32 {I3} agrees with a value of 0.3, calculated with Coriolis-mixed Nilsson wave functions (1975So01) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
J$The transition of 451|g Q from 1117 level of 1/2-[510]band, and the 348.3|g to the 318 level of of 1/2-[510]band, establishes the J|p of this state as 13/2-. D to 11/2-, Q to 9/2- and band structure consequently establishes J|p=7/2- of the bandhead at 102 level. I|g(348.3|g)/I|g(405.5|g)exp=0.26 {I6} is in fair agreement with a value of 0.44, calculated with Coriolis-mixed Nilsson wave functions (1975So01) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E$K=5/2 band head. Possible K+2 |g-vibrational state coupled to 1/2[510]. 
J$See J|p comment for the 599 state. 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2,5/2+
level_comment:
J$populated by primary |g ray in (n,|g). May be the same as the 1/2- level observed at 1070 keV in (p,t). 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_comment:
J$|g to 13/2+ and 15/2+ states; band structure. 
J$|g to 13/2+ and 15/2+, 17/2+, 19/2+ states of 11/2+[615] band. 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_comment:
J$742.9|g D to 17/2+, 929.1|g Q to 15/2+, 494.9 |g to 19/2+ states, which are members of 11/2+[615] band. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_comment:
J$|g to 17/2+ state; |g to the 17/2+, 19/2+ and 21/2+ states of the 11/2+[615] band; band structure. 


level_energy_unit: KEV
level_spin_parity: (41/2)
level_lifetime_unit: NS
level_comment:
J$|g to (39/2) 
T$from (HI,xn|g) (2004Sh08) 
$K=41/2 isomer. Possible configurations with 7 quasiparticles: |n(1/2[510]1/2[521]7/2[503]9/2[624]11/2[615])~#|p(5/2[402]7/2[404]); or |n(1/2[510]1/2[521]3/2[512]9/2[624]11/2[615])~#|p(7/2[404]9/2[514]); or |n(1/2[521]3/2[512]7/2[503]9/2[624]11/2[615])~#|p(1/2[541]9/2[514]) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2- & 7/2-
level_comment:
$|S|ssin|q=110.5 
E$Doublet, possibly 5/2- state of 1/2[510] band, and 7/2- state of 7/2[503] band. 


level_energy_unit: KEV
level_spin_parity: (41/2)
level_lifetime_unit: NS
level_comment:
T$from decay curve of the time difference spectra between transitions above and below the isomer (2004Sh08) 
$K=41/2 isomer. Possible configurations with 7 quasiparticles: |n(1/2[510]1/2[521]7/2[503]9/2[624]11/2[615])~#|p(5/2[402]7/2[404]); or |n(1/2[510]1/2[521]3/2[512]9/2[624]11/2[615])~#|p(7/2[404]9/2[514]); or |n(1/2[521]3/2[512]7/2[503]9/2[624]11/2[615])~#|p(1/2[541]9/2[514]) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
J$ from Adopted dataset for {+185}Os in ENSDF database 
T$ from time variation of 646-keV |g from {+185}Os decay (2012Kr05). Value in the ENSDF database is 93.6 d {I5} 
$ Measured capture |s=3480 b {I+3480-1160} and resonance integral=330 b {I+330-110} (2012Kr05). Large uncertainties are due to 50% uncertainty in natural abundance of {+184}Os adopted as 0.02% {I1}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T From 1975Vi01. Others: |> 3.3 |* 10{+17} y for decay to the 2+, 100.1-keV level in {+182}W and |> 6.0 |* 10{+18} y for decay to the 4+, 329.4-keV level in {+182}W (2020Be23 - from a 15,851 h measurement). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 From 2020StZV (based on 1976St23 - Mossbauer). Additional value: +0.524 {I30} (2016St14, from 1982Le02), transient integral PAC assuming T{-1/2}=0.83 ns. 
MOME2 From muonic x ray hyperfine structure (2021StZZ, from 1981Ho22). Others: -1.61 {I5} (2014StZZ, from 1972Wa24), -1.18 {I16} (1989Ra17). 
J E2 137|g to 0+ g.s. 
T$weighted average of 842 ps {I12} from {+186}Re |b decay, 923 ps {I18} and 840 ps {I50} from {+186}Ir |e decay (16.64 h). Uncertainty the lowest input value. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J E2 365|g to 3+ 910; E2 407|g to 6+ 869; E consistent with that expected for J=5 member of |g band. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
MOMM1 -0.22 {I14} from DPAD (2020StZV, from 1984Go06) if T{-1/2}=10.4 ns; adjusted by evaluators to be consistent with adopted half-life. 
J possible stretched (E2) 146|g to 5- 1629. 
T weighted average of 8.5 ns {I3} from ({+14}C,4n|g) and 8.1 ns {I4} from (|a,4n|g). Other values: 10-15 ns (1973Ya05) from (p,2n|g); 10.5 ns {I10} and 10.4 ns {I8} from (|a,2n|g). The latter data from (|a,2n|g) were not adopted because probable feeding from the 2165 level (5.7 ns {I4}) would result in an apparently longer half-life. 


level_energy_unit: KEV
level_spin_parity: 4+,5+
level_comment:
J E2(+M1) 705|g to 4+ 1070; 907|g to 6+; anisotropy 705|g in {+186}Ir |e decay (16.64 h) inconsistent with J=6. However, suggested as J=6 member of K=4 band in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J |g to 6+ 1491; |g-band member excited in multiple Coulomb excitation. 
T from Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: NS
level_comment:
J M1 |g to (8-). 
T Unweighted average of 5.3 ns {I2} from (|a,4n|g) and 6.1 ns {I2} from ({+14}C,4n|g). 


level_energy_unit: KEV
level_spin_parity: (6)+
level_comment:
J E2 1107|g to (5)+; |g to 4+; log| {Ift}|?8.0 from 5+; anisotropy of 1107|g excludes J=4 and 5 in {+186}Ir |e decay (16.40 h). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
J possible E0+M1+E2 2399|g to 6+; however, possible 3132|g to 2+. One of these gammas may be misplaced. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From Adopted Levels. Other: 0.91 ns {I3} - weighted average of 0.84 ns {I5} (1970Be18) and 0.923 ns {I18} (1971Bb09). 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$Since |e feeding to this level would be second-forbidden, essentially none is expected. The intensity imbalance of 3.5% {I7} at this level must presumably be balanced by unidentified transition(s) from higher energy levels. 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
J$anisotropies of 565|g and 1188|g rule out J=4; that of 1622|g favors J=6, but J=5 cannot be ruled out (1978Sp05). 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
g-factor=-0.032 {I20} from DPAD (1984Go06). 
J possible configuration=((|n i{-13/2})(|n p{-3/2} or p{-1/2} or f{-5/2}))7- (1984Go06) (consistent with g-factor). 
T from 1984Go06. Other value: 10.5 ns {I10} (1978Sh21) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
g-factor: 0.262 {I15} (1982Le02) from the unperturbed particle-gamma angular distribution, if T{-1/2}=0.830 ns, 0.274 {I19} (1967Gi02). Others: 1972Si43. 
BE2 Other values: 3.1 {I4} (1967Ca08), 3.0 {I4} (1967Gi02), 3.21 {I28} (1971Mi08), 2.9 {I4} (1972La16), 3.10 {I25} (1976Ba06), 3.15 {I3} (muonic atom, 1977Ho23). 
Static matrix element, <2+ M(E2) 2+> =-1.75 {I+22-13} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2 For 2+ to 4+ excitation. Others: 1.51 {I21} (1971Mi08), 1.69 {I12} (1969Ca19). 
Static matrix element, <4+ M(E2) 4+>=-2.02 {I+39-18} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 For excitation from g.s. Others: 0.188 {I25} (1971Mi08), 0.244 {I24} (1969Ca19). 
B(E2)(from 2+ 137 keV level)=0.163 {I+23-8} (1996Wu07). Others: 0.107 {I11} (1969Ca19), 0.082 {I12} (1971Mi08). 
Static matrix element, <2+ M(E2) 2+> =+2.12 {I+6-22} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
BE2$for excitation from 4+ 434 level. Other: 1.64 {I25} (1969Ca19). 
Static matrix element, <6+ M(E2) 6+> =-1.7 {I3} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
1996Wu07 report B(E2)(from 2+ 767)=0.032 {I+20-12} assuming B(E2)(from first 2+)/B(E2)(from second 2+)=0.25 (estimated from systematics for second 0+ levels in {+188}Os, {+190}Os and {+192}Os); this implies B(E2)(from 2+ 137)=0.13 {I+8-5}, but 1996Wu07 do not specifically report this datum, even though this corresponds to the only |g they actually observed deexciting the 1061 level. If present, a 294-keV transition to the 767 level would presumably be masked by the strong 297|g connecting the 2+ and 4+ members of the g.s. band. 
T$0.13~ps {I+5-8} if branching to 137~keV level is 100%. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2 For excitation from 2+ 137 keV level. Other: 0.026 {I6} (1969Ca19). 
B(E2)(from 4+ 434 level)=0.165 {I+17-15} (1996Wu07). Other: 0.18 {I5} (1969Ca19). 
B(E2)(from 2+ 768 level)=0.77 {I+7-5} (1996Wu07). Other: 0.99 {I35} (1969Ca19) is derived from authors' B(E2)(from 4+ 434) and an obsolete I|g(303)/I|g(933) value. 
B(E2)(from 6+ 869 level)=0.035 {I+5-2} (1996Wu07). 
Static matrix element, <4+ M(E2) 4+> =-1.12 {I+25-23} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2 For excitation from 2+ 768 level. 
B(E2)(from 2+ 137 keV level)=0.0013 {I+21-13} (1996Wu07). 
B(E2)(from 3+ 910 level)=0.33 {I+14-4} (1996Wu07) assuming |d, branching from elsewhere. 
B(E2)(from 4+ 1071 level)=0.37 {I+14-12} if pure E2 (1996Wu07). 
Static matrix element, <4+ M(E2) 4+> =+2.4 {I+9-7} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
BE2 For excitation from 6+ 867 level. 
Static matrix element, <8+ M(E2) 8+> =-2.26 {I+24-108} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
BE2 For excitation from 4+ 1070 level. 
B(E2)(from 6+ 869 level)=0.144 {I+20-22} (1996Wu07). 
B(E2)(from 4+ 434 level)=0.0117 {I+15-18} (1996Wu07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 14+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
BE2 For excitation from 12+ 2782 level. 
Probable member of a rotation-aligned band which becomes yrast for J|>14. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From Adopted Levels. Other: 0.842 ns {I12} - from |b-ce or |b|g delayed coincidence; weighted average of 0.81 ns {I3} (1968Ma14), 0.845 ns {I20} (1964Ro19), 0.82 ns {I3} (1963Fo02), 0.87 ns {I4} (centroid shift) and 0.890 {I35} (1962Ba14), 0.84 ns {I3} (1961Bo08). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Admixtures of the two-quasiparticle components of configuration |p5/2[402]-|p5/2[402] is 1.5 {I4} (expt) compared with the predicted value of 0.16 {I1} for single j and l. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Admixtures of the two-quasiparticle components of configuration |p5/2[402]-|p1/2[400] is 0.33 {I10} (expt) compared with the predicted value of 0.16 from Quasiparticle phonon model calculations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$Admixtures of the two-quasiparticle components of configuration |p5/2[402]+|p3/2[402] is 0.34 {I10} (expt) compared with the predicted value of 0.41 from Quasiparticle phonon model calculations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E existence of level unconfirmed in subsequent, more extensive (HI,xn|g) studies (e.g., 1999Wh02); not included in adopted levels. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$a 10-15~ns half-life was assigned to the 1629 level by 1973Ya05. The evaluators reassign this value to the 1775 level because the 146-keV transition connecting the 1775 and 1629 levels was shown in (|a,2n|g) (1974Ya03) to be delayed and to possess a similar half-life. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 2+, 100.1-keV level in {+182}W. Other: |> 6.0 |* 10{+18} y for decay to the 4+, 329.4-keV level in {+182}W. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$spin from optical spectroscopy (1976Fu06), parity from magnetic moment. 
MOMM1$from 1974Sa25 (NMR). Same value in 1989Ra17 and 2005St24. 
<r{+2}>{+1/2}({+187}Os)=5.3934 {I17} fm (2004An14) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$9.7|g M1(+E2) to 1/2- state, L=0(+2) from {+189}Os(p,t), target({+189}Os) J|p=3/2- 
T$from {+187}Ir |e decay (|g-ce coincidence measurement-1971Ma24) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L=0 in {+189}Os(p,t), target({+189}Os) J|p=3/2-; 74.3|g M1+E2 to 1/2- state, 64.6|g M1+E2 to 3/2- state. 
T$Using B(E2)|^=0.68 (1963Mc18), 74.3|g and adopted properties (Coulomb excitation) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J 75|g E2 to 1/2- state, band assignment. 
T$from {+187}Ir |e decay (|g-ce coincidence measurement-1971Ma24). Other: 1.7 ns {I5} from B(E2)|^=0.90 (Coulomb Excitation - assuming 20% uncertainty) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J$90.4|g E2 to 3/2- state, 25.6|g M1 to 5/2- state, band assignment. 
T$from {+187}Ir |e decay (|g-ce coincidence measurement-1971Ma24); other value: 120 ns {I20} (1964Kr02) from {+188}Os(|g,n) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$187.4|g E2 to 1/2- state, band assignment. 
T$Using the reported B(E2)|_=0.446 {I33} of 187|g (1997Br18) and the adopted |g-ray properties (Coulomb excitation) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: US
level_comment:
J$156.6|g M2+E3 to 7/2- state. 
T$from 156.6|g-t and the |g-ray associated x-ray-t (1967Co20)- (d,2n|g),(p,n|g); other value: 225 |ms {I10} (1964Br27) from {+188}Os(|g,n). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L=0 in {+189}Os(p,t), target({+189}Os) J|p=3/2-; 725.7|g M1+E2 to 1/2- state, 651.4|g to 3/2- state. 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: US
level_comment:
T$from 1967Co20. Other values: 225 |ms {I10} (1964Br27), 216 |ms (1965Mc03), 240 |ms (1967Iv03), 239 |ms {I50} and 221 |ms {I50} (1968Io01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
B(E2)|^=1.69 (1963Mc18) 
T Using the 187|g and it's corresponding B(E2)|_ (1997Br18). Contamination of 187|g from {+189}Os and {+190}Os, stated by 1997Br18, seems insignificant. Since 112.3|g, 113.2|g, and 177.7|g and their corresponding B(E2)|_ values yield statistically consistent T{-1/2} of 108 ps {I17}, 111 ps {I19}, and 110 ps {I27}, respectively. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 3/2-, 46.5-keV level in {+183}W. Other: |> 1.9 |* 10{+17} y for decay to the 5/2-, 99.1-keV level in {+183}W. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$|D<r{+2}>({+188}Os,{+186}Os)=0.104 fm{+2} {I4} (1981Ho22) 
$|D<r{+2}>({+190}Os,{+188}Os)=0.090 fm{+2} {I4} (1981Ho22) 
$isotope shifts, |d|n=|n({+188}Os) - |n({+192}Os))= +4227 {I2} (MHz) (atom) and 4261.9 {I34} (MHz) (ion) (2006Av09) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
BE2$Others: 2.635 {I30} (1988Bo08), 2.82 {I3} (1981Ho22), 2.52 {I13} (1976Ba06), 2.69 {I27} (1972Ca16), 2.78 {I15} (1971Mi08), 2.90 {I8} (1970Pr09), 2.7 {I4} (1967Ca08), 3.7 {I5} (1961Re02), 3.17 {I33} (1961Mc18), 2.80 {I31} (1961Mc01,1958Mc02), and 3.5 {I10} (1957Ba11). 
MOMM1$From IMPAC (weighted average adopted by 1992St06). Others: +0.584 {I20} (1985St05,adopted weighted average), +0.51 {I5} (1984St11), +0.60 {I3} (1982Le02), +0.58 {I6} (1972Si03,1972Si43,1972SiYG), 0.51 {I5} (1971SiYO), 1970Be36, 0.61 {I3} (1970Wa06), 1967Gi02, 1966Go06, 0.62 {I5} (1965Ch14), 1964Sp02, 1963Go05 
MOME2$From muonic-x ray. Others: Q=-1.15 {I25} (1980Ba42,Coul. ex.), -1.33 {I10} (Coul. ex. quoted by 1989Ra17 from Annual Report Rochester (1978),p.9), -1.36 {I9} (1972Wa24,Mossbauer), -1.81 {I24} (1970Wa06,Mossbauer), 1972La16, 1970Pr09 
J$155.044|g E2 to 0+; band member 
T$Weighted average of 0.711 ns {I9}, weighted average of values directly measured in Coul. ex., |b{+-} and |e decay of 0.645 ns {I97} (2001Wu03), 0.714 ns {I35} (1997Bb08), 0.718 ns {I17} (1971Bb09), 0.714 ns {I21} (1971Bo13), 0.710 ns {I30} (1970Be18), 0.680 ns {I30} (1968Ma14), 0.707 ns {I35} (1966As03), 0.710 ns {I20} (1963Fo02), 0.728 ns {I69} (1963Go05) and 0.730 ns {I60} (1962Ba14) and 0.695 ns {I10} from B(E2)=2.512 {I32} (1996Wu07) in Coul. ex. Others (directly measured): 0.65 ns {I15} (1955Su64) and 1.7 ns {I4} (1953Mc39)) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$322.92|g E2 to 2+; band member 
T$From 2001Wu03 using the recoil-distance method in Coulomb excitation. Other: 19.3 ps {I+3-4} from B(E2)(from 155, 2+) (1996Wu07) 
BE2$Others: 1.47 {I15} (1971Mi08), 1.41 {I11} (1969Ca19), and 1.36 {I20} (1967Ca08) 
BE4$From {+188}Os(e,e') 
MOMM1$from g=+0.358 {I35}, using transient-field integral PAC in Coulomb excitation (1985St05). Other: g(478)/g(155)=1.32 {I17} (1984St11) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$633.03|g E2 to 0+ 
T$From 2001Wu03 using the recoil-distance method in Coulomb excitation. Other: 6.46 ps {I+26-9} from B(E2)(from 0, 0+) (1996Wu07) 
MOMM1$from g=+0.392 {I35}, using transient-field integral PAC in Coulomb excitation (1985St05). Other: +0.86 {I16} (1967Mu05) 
MOME2$from reorientation method in Coulomb excitation (1980Ba42,1978BaYK). Note, that Q=+1.0 {I3} is recommended in 2016St14 
BE2$from the ground state (0.0,0+). Others: 0.247 {I15} (1971Mi08), 0.250 {I22} (1969Ca19), 0.211 {I30} (1967Ca08), 0.20 {I6} (1961Mc01); 0.241 {I9} from {+188}Os(e,e') 
$B(E2)(from 155,2+)=0.150 {I4} (1996Wu07), 0.156 {I11} (1971Mi08), 0.146 {I13} (1969Ca19), 0.164 {I24} (1967Ca08). 
$B(E2)(from 478,4+)=0.016 {I+4-5} (1996Wu07). B(E2)(633,2+ to 155,2+)/B(E2)(633,2+ to g.s.)=3.5 {I2} (1980Ba42) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$462.38|g E2 to 4+; band assignment 
T$From 2001Wu03 using the recoil-distance method in Coulomb excitation. Other: 3.09 ps {I5} from B(E2)(from 633, 4+) (1996Wu07) 
MOMM1$from g=+0.41 {I6}, using the transient-fields in integral PAC in Coulomb excitation (1985St05) 
BE2$from 633,4+. Other: 1.68 {I26} (1969Ca19) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$332.62|g E2 to 2+, 810.60|g E2 to 4+; band assignment 
T$From 2001Wu03 using the recoil-distance method in Coulomb excitation. Other: 5.7 ps {I6} from B(E2)(from 155, 2+) (1996Wu07) 
BE2$from 155,2+; Other: 0.020 {I4} (1969Ca19). B(E2)(from 478,4+)=0.135 {I7} (1996Wu07); Other: 0.159 {I32} (1969Ca19). B(E2)(from 633,2+)=0.63 {I+5-4} (1996Wu07); Other: 1.05 {I35} (1969Ca19). B(E2)(from 940,6+)=0.025 {I+6-11} (1996Wu07) 
MOMM1$from g=+0.40 {I12}, using the transient-fields in integral PAC in Coulomb excitation (1985St05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
BE2$from 155, 2+. Other: 0.0061 {I15} (1969Ca19). B(E2)(from 633,2+)=0.0055 {I+4-3} (1996Wu07) 
J$L(p,t)=0; 931.34|g E2 from |g|g(|q) to 2+ 
T$From B(E2)|^ and the corresponding branching ratios 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$from 633, 2+. Others: B(E2)(from 155,2+)=0.0030 {I11} (1996Wu07) and B(E2)(from 965,4+)=0.299 {I26} (1996Wu07), assuming pure E2 
J$L({+3}He,d)=2. {I645}.9|g (E2) to 2+. 
T$From 2001Wu03 using the recoil-distance method in Coulomb excitation. 
CONF$dominant |p(3/2[402],5/2[402]) assignment (see 2010Ph01 and references therein). However, 2001Wu03, 1974Ya03, 1973Ya05 interpret this state as a dominant two-phonon |g-vibrational configuration 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$L(p,t)=(3); 448.1|g to 2+, 780.8|g to 4+. Absence of a transition to g.s. (J|p=0+), would argue against J=1 and 2+ 
$B(E3)=0.147 {I8} (1988Bo08) from (e,e') 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$459.4|g to 4+,484.7|g to 6+; excitation in Coul. excit. from 4+; band assignment 
T$from B(E2)(from 965,4+) 
$B(E2)(from 940,6+)=0.164 {I+21-40} (1996Wu07) 
$B(E2)(from 478,4+)=0.00179 {I+24-12} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$672.5|g E1 to 3+; direct feeding in {+188}Re |b{+-} decay (J|p=1-) and {+188}Ir |e decay (J|p=1-) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$574.4|g E2 to 6+; band assignment 
T$From 2001Wu03 using the recoil-distance method in Coulomb excitation. Other: 0.96 ps {I6} from B(E2)(940, 6+) (1996Wu07) 
BE2$From 940,6+ (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$719.55|g to 4+, 1530.06|g to 2+ would be consistent with J|p=2+,3,4+. However, a possible direct population of this level in {+188}Ir |e decay (41.5 h) and {+188}Re |b{+-} decay (17.005 h) would be consistent with J|p=2+ or 3+. The absence of |g to 0+ would argue against 2+ 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
MOMM1$from g=-0.025 {I15} using differential PAD method in 1984Go06 
J$102.3|g E2 to (5-); proposed configuration based on |m 
T$From 390|g(t)+729|g(t) in 2009Mo05, by taking into account the decay of the 10- isomer. Others (from |g(t)): 13.9 ns {I8} (1984Go06), 14.0 ns {I10} using 155|g(t) and 102.2 |g(t) in 1978Sh21 and 14 ns in 1979WiZS 
CONF$ K|p=7-,|n(3/2-[512],11/2+[615]) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$1209.80|g M1(+E2) to 2+, 1843.0|g to 0+. Since I|g(1843|g)< I|g(1688|g), J|p=2+ is more likely than 1+ 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$1957.10|g to 0+. |a(pair) for 1802|g and 1957|g support positive parity, but |a(K)exp for 1802|g gives negative parity 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
BE2$from 1424, 6+ in Coul. ex. 
J$excitation through E2 transition from (6+) in Coul. ex. 
T$from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$1435.42|g M1+E2 to 2+, 2068.9|g to 0+. Since I|g(2068.9|g) < I|g(1435.42|g), one may expect J|p=2+ to be favored compared to 1+ 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
MOME2$from muon-x ray method (1979Ho23) 
E$from (|m{+-},|g). Uncorrected for isomer shift 
J$1643.1|g to 4+, 1966.2|g to 2+. Parity from requirement that product of this state and muonic 2p{-3/2} state mix with product of 0+ and muonic 2d{-3/2} state 
$B(E3)=0.005 {I5} in 1979Ho23 (|m{+-},|g) 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: NS
level_comment:
J$89.2|g (M1) to 9-; systematics of similar structures in neighboring nuclei 
T$From 284|g(t) (2009Mo05) in (HI,xn|g) 
CONF$|n(9/2-[505],11/2+[615]) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$2011.39|g (E2) to 2+, 703.38|g to 2-, 1688.04|g to 4+; direct feeding in {+188}Ir |e decay (J|p=1-) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$2049.78|g M1+E2 to 2+, 1726.9|g to 4+; |g(|q,t) in {+188}Ir |e decay; direct feeding in {+188}Ir |e decay (J|p=1-) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$2252.09|g to 0+, 1286.35|g to 4+; 1618.8|g M1(+E2) to 2+; direct feeding in {+188}Ir |e decay (J|p=1-) 


level_energy_unit: KEV
level_spin_parity: (13-)
level_comment:
J$359.5|g M1 to (12-), 634.6|g E2 to (11-) 
CONF$possible |n(1/2-[510],7/2-[503],9/2-[505],11/2+[615]) 


level_energy_unit: KEV
level_spin_parity: (15-)
level_comment:
J$353.8|g E2 to (13-) 
CONF$possible |n(3/2-[512],7/2-[503],9/2-[505],11/2+[615]) or |n(1/2-[510],11/2+[615])~#|p(9/2-[514],11/2-[505]) 


level_energy_unit: KEV
level_spin_parity: (14+)
level_comment:
J$378.6|g E1 to (13-), 615.5|g E2 to 12+ 
CONF$possible |n(1/2-[510],9/2-[505],9/2+[624],11/2+[615]) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|D<r{+2}>({+188}Os,{+186}Os)=0.104 fm{+2} {I4} (1981Ho22) 
$|D<r{+2}>({+190}Os,{+188}Os)=0.090 fm{+2} {I4} (1981Ho22) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$From adopted levels. Values measured in {+188}Ie |e decay: 0.714 ns {I21} (|e|g(t),1971Bo13) and 0.710 ns {I30} (|ece(t),1970Be18). 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
T$from |g(t) in 1984Go06. Others: 14.0 ns {I10} using 155|g(t) and 102.2 |g(t) in 1978Sh21 and 14 ns in 1979WiZS 
$g factor: differential PAD method in 1984Go06 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ From Quasiparticle phonon model calculations. Dominant configuration (|p5/2[402],|p5/2[402])=1.3 {I4} (expt), compared with the predicted value of 1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$ From Quasiparticle phonon model calculations, squared amplitude of two quasiparticle configuration |p{+2}(5/2[402],1/2[400])=0.28 {I8} (expt) compared to the predicted value of 0.10 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$ From Quasiparticle phonon model calculations, squared amplitude of two quasiparticle configuration |p{+2}(5/2[402],3/2[402])=0.27 {I9} (expt) compared to the predicted value of 0.32. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$g=0.305 {I15} (1970Wa06) and 0.310 {I27} (1965Ch14). Q=-1.36 {I9} (1972Wa24) and -1.81 {I24} (1970Wa06). Q({+188}Os,2+)/Q({+186}Os,2+)=0.91 {I2} (1972Wa24). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|b{-2}(Coulomb)=0.191, |b{-2}(nuclear)= 0.132, 0.149, 0.145 (1976Ba06) from interference data. |b{-2}(Coulomb)=0.22 (1971Kr10) from |s(|q) data. |b{-2}=0.218 (1976Ba06) from E(|a)=13 MeV data 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$|b{-4}(Coulomb)=-0.031, |b{-4}(nuclear)=-0.080, -0.028 (1976Ba06) from interference data. |b{-4}=-0.237 (1976Ba06) from E(|a)=13 MeV, sub-Coulomb data 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$1978Bu21 analyze |s(|q) and absolute cross section data by assuming the population of this level through successive E2 excitations, direct E4 excitation and coherent mixture of both mechanisms. Agreement was obtained by considering a significant contribution from direct E4 excitation 
$|b{-4}=0.027 (1978Bu21) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$From adopted levels. Directly measured values in Coulomb excitation: 0.645 ns {I97} (RDM,2001Wu03), 0.714 ns {I35} (1997Bb08), 0.707 ns {I35} (RDM,1966As03), and 0.728 ns {I69} (RDM,1963Go05). Other: 0.695 ns {I10} from B(E2) in 1996Wu07 
BE2$ Others: 2.52 {I13} (1976Ba06), 2.69 {I27} (1972La16), 2.78 {I15} (1971Mi08), 2.90 {I8} (1970Pr09), 2.7 {I4} (1967Ca08), 3.7 {I5} (1961Re02), 3.17 {I33} (1961Mc18), 2.80 {I31} (1961Mc01,1958Mc02) and 3.5 {I10} (1957Ba11) 
G$From |g(|q,H) in Coulomb excitation. Others: 0.259 {I25} (1984St11), 0.29 {I3} (1972Si03,1972Si43,1972SiYG), 0.256 {I26} (1971SiYO), 0.300 {I15} (1982Le02), 0.285 {I12} (1970Be36), 0.284 {I21} (1967Gi02), 0.270 {I18} (1966Go06), 0.23 {I3} (1964Sp02), 0.20 {I2} (1963Go05). 1992St06 quote a weighted average value of +0.298 {I11}, which includes values obtained from studies other than Coulomb excitation. 
MOME2$earlier values from the same group: -1.32 {I23} (1972La16), -1.31 {I34} (1970Pr09). Others: 1975Ro24 and 1964Sp09 give ratios of Q's for first 2+ levels in {+188}Os, {+190}Os, {+192}Os 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$Other: 19.3 ps {I+3-4} from B(E2)(from 155, 2+) 
BE2$Others: 1.47 {I15} (1971Mi08), 1.41 {I11} (1969Ca19), 1.36 {I20} (1967Ca08) 
G$From |g(|q,H) (1985St05). Other: g(478)/g(155)=1.32 {I17} (1984St11) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$from g.s. Others: 0.247 {I15} (1971Mi08) 0.250 {I22} (1969Ca19), 0.211 {I30} (1967Ca08), 0.20 {I6} (1961Mc01). 
$B(E2)(from 155,2+)=0.150 {I4} (1996Wu07). Others: 0.156 {I11} (1971Mi08), 0.146 {I13} (1969Ca19), 0.164 {I24} (1967Ca08). 
$B(E2)(from 478,4+)=0.016 {I+4-5} (1996Wu07) 
$B(E2)(633,2+ to 155,2+)/B(E2)(633,2+ to g.s.)=3.5 {I2} (1980Ba42) 
G$From |g(|q,H) in Coulomb excitation. Other: g(633)/g(155)=1.45 {I18} (1984St11) 
T$Other: 6.46 ps {I+26-9} from B(E2)(from 0, 0+) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
BE2$from 633,4+. Other: 1.68 {I26} (1969Ca19) 
T$Other: 3.09 ps {I5} from B(E2)(from 633, 4+) 
G$From |g(|q,H) in Coulomb excitation. 
$ E2 matrix element (from 478,4+)=(+)3.31 4 (1996Wu07) 
$Static E2 matrix element (940 to 940)=-1.60 {I+18-33} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$from 155,2+. Other: 0.020 {I4} (1969Ca19) 
$B(E2)(from 478,4+)=0.135 {I7} (1996Wu07). Other: 0.159 {I32} (1969Ca19) 
$B(E2)(from 633,2+)=0.63 {I+5-4} (1996Wu07). Other: 1.05 {I35} (1969Ca19) 
$B(E2)(from 940,6+)=0.025 {I+6-11} (1996Wu07) 
G$From |g(|q,H) in Coulomb excitation. 
T$Other: 5.7 ps {I6} from B(E2)(from 155, 2+) 
$Static E2 matrix element (965 to 965)=-1.22 {I+16-10} (1996Wu07) 
$ E2 matrix element (from 155,2+)=+0.283 +8-7 (1996Wu07) 
$ E2 matrix element (from 478,4+)=+1.10 3 (1996Wu07) 
$ E2 matrix element (from 633,2+)=(+)1.78 +7-5 (1996Wu07) 
$ E2 matrix element (from 940,6+)=+0.57 +7-12 (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
BE2$from 155, 2+. Other: 0.0061 {I15} (1969Ca19). 
$B(E2)(from 633,2+)=0.0055 {I+4-3} (1996Wu07) 
$ E2 matrix element (from 155,2+)=0.078 2 (1996Wu07) 
$ E2 matrix element (from 633,2+)=(+)0.165 +6-4 (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$from 633, 2+ 
$B(E2)(from 155,2+)=0.0030 {I11} (1996Wu07) 
$B(E2)(from 965,4+)=0.299 {I26} (1996Wu07), assuming pure E2 
T$Other: 3.3 ps {I+3-4} from B(E2)(from 633, 2+) 
$ E2 matrix element (from 155,2+)=+0.123 23 (1996Wu07) 
$ E2 matrix element (from 633,2+)=(+)0.83 +4-3 (1996Wu07) 
$ E2 matrix element (from 790,3+)=-1.17 +17-5 (1996Wu07) 
$ E2 matrix element (from 965,4+)=+1.64 7 (1996Wu07) 
$Static E2 matrix element (1279 to 1279)=+2.68 {I+22-19} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
BE2$from 965, 4+ 
$B(E2)(from 940,6+)=0.164 {I+21-40} (1996Wu07) 
$B(E2)(from 478,4+)=0.00179 {I+24-12} (1996Wu07) 
T$from B(E2)(from 965,4+) 
$ E2 matrix element (from 478,4+)=0.127 +6-12 (1996Wu07) 
$ E2 matrix element (from 940,6+)=+1.46 +13-25 (1996Wu07) 
$ E2 matrix element (from 965,4+)=(+)2.46 10 (1996Wu07) 
$Static E2 matrix element (1424 to 1424)=-1.33 {I+23-56} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
BE2$from 940, 6+ 
T$Other: 0.96 ps {I6} from B(E2)(940, 6+) 
$ E2 matrix element (from 940,6+)=(+)3.97 11 (1996Wu07) 
$Static E2 matrix element (1515 to 1515)=-1.38 {I+44-26} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
BE2$from 1424,6+ 
$ E2 matrix element (from 1424,6+)=(+)2.55 +22-69 (1996Wu07) 
$Static E2 matrix element (1979 to 1979)=-2.4,-0.8 (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
BE2$from 1515, 8+ 
$ E2 matrix element (from 1515,8+)=(+)5.00 +34-21 (1996Wu07) 
$Static E2 matrix element (2170 to 2170)=-1.73,-0.8 (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$From adopted levels. Values measured in {+188}Re |b{+-} decay: 0.718 ns {I17} (1971Bb09), 0.680 ns {I30} (|b(t),1968Ma14), 0.71 ns {I2} (|b-ce(k)(155|g)(t), 1963Fo02), 0.73 ns {I6} (|b-ce(k)(155|g)(t), 1962Ba14), 0.652 {I153} (1955Su64) and 1.698 {I194} (1953Mc39) 
G$from (931|g)(155|g)(|q,H): 0.36 {I4} (1962Le17) and 0.30 {I3} with H=29.2 kG and |w|t=0.0423 {I34} (1961Ka09) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
G$from (1133|g)(633|g)(|q,H(Fe)): 0.66 {I20} (1967Ke01) and 0.38 {I8} (1967Mu05), both used T{-1/2}=6.3 ps and H(Fe)=-1.11 mg 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$proposed from |g|g coin. in 1984Zh08, but the assignmnet is questionable, since no such level has been reported in any other studies of {+188}Os levels. It is possible that 810.5|g deexcites the 965-keV level 


level_energy_unit: KEV
level_spin_parity: 15-
level_comment:
CONF$possible |n(3/2-[512],7/2-[503],9/2-[505],11/2+[615]) or |n(1/2-[510],11/2+[615])~#|p(9/2-[514],11/2-[505]) 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 2+, 111.2-keV level in {+184}W. Other: |> 5.0 |* 10{+19} y for decay to the 4+, 364.1-keV level in {+184}W. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 2+, 111.2-keV level in {+184}W. Other: |> 8.1 |* 10{+19} y for decay to the 4+, 364.1-keV level in {+184}W. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$RMS charge radius <r{+2}>{+1/2}=5.4016 fm {I12} (2013An02 evaluation) 
MOMM1$NMR (1954Lo36, subject to correction for chemical effects). Other: +0.6565 {I3} (1968Sc03) 
MOME2$Mossbauer effect (1972Wa24). Other: +0.98 {I6} (2002Kr01) for 5d{+6}6s{+2}, and 0.97 {I9} for 5d{+7}6s from laser induced fluorescence spectroscopy, +0.8 {I2} from optical spectroscopy includes polarization correction (1962Mu04), +0.91 {I10} from optical spectroscopy (1968Hi04). 
J$spin from optical spectroscopy (1954Lo36) and NMR (1952Mu40); parity from L(d,p)=1 from 0+ target 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
J$M3+E4 |g to 3/2-; L=5 in (d,p), (d,t). 
T$weighted average of 5.65 h {I15} (2000Ah03), 6.0 h {I1} (1963Pr12) and 5.7 h {I1} (1958Sc30). Others: 5.7 h (1973Ot01), 6 h (1950Ch11) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
MOMM1$Mossbauer effect (1969Wa02) 
J$M1+E2 to 3/2-, |g|g(|q) isotropic. 
T$weighted average of 0.53 ns {I3} from delayed coincidence in {+189}Ir |e decay (1970Ma37) and 0.50 ns {I3} from Mossbauer (1969Wa02). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$E2 to 1/2-, L=3 in (d,p), (d,t). 
T$weighted average of delayed coincidence measurements 1.59 ns {I8} (1970Ma37), 1.63 ns {I4} (1969Gr10), and 1.7 ns {I1} (1969An17) in {+189}Ir |e decay. Others: Mossbauer 1.8 ns {I2} (1968Pe09); Coulomb excitation 1.5 ns {I3}; delayed coincidence 2.12 ns {I10} (1971Be71). 
MOMM1$Mossbauer effect (1972Wa24, does not include polarization correction). Others: +0.82 {I23} from IPAC (1968Pe09), 1971Be23 
MOME2$Mossbauer effect (1972Wa24), deduced from the Q{-5/2-}/Q{-3/2-} ratio of -0.735 {I12}. Other value: -0.67 {I7} (1972Wa24, if the value for Q{-3/2-} of +0.91 {I10} used in this reference is taken). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 to 1/2- and 5/2- 
T$from delayed coincidence in {+189}Ir |e decay (1970Ma37). Other: 0.10 ns {I2} from Coulomb excitation. 
MOMM1$IPAC (1971Be71) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 to 9/2-, E2 to 3/2- 
T$from B(E2) in Coulomb excitation. Others: 77 ps {I10} from (|g,|g') Res. Fluorescence (1995La15); <0.3 ns from delayed coincidence in{+189}Ir |e decay (1970Ma37). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 to 9/2-, E2 to 3/2- 
T$from B(E2) in Coulomb excitation. Other: 0.19 ns {I3} from Coulomb excitation (1967Hr01); < 0.3 ns from (d,d') (1975Mo29) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 to 3/2- and 5/2-, band assignment 
T$from B(E2) in Coulomb excitation. Others: 0.28 ns {I13} from Coulomb excitation; |?0.1 ns from (d,d') (1975Mo29) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 to 3/2-, M1 to 7/2- 
T$weighted average of 0.16 ns {I4} from B(E2) in Coulomb excitation and 0.17 ns {I3} from delayed coincidence in {+189}Ir |e decay (1970Ma37) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$E2 |g to 11/2+, |gs to 5/2- and 7/2-. A 446 {I4} level in (d,p) with L=1 (implying J|p=1/2-,3/2-) is given by 1975Mo29 but not confirmed by 1976Be50 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$M1 to 5/2-, fed by primary |g in (n,|g) (1976Be50) 
T$from (|g,|g'): Res. Fluorescence (1995La16) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$L=2 in (d,d'); primary |g from {+188}Os(n,|g) E=2,24 keV res: av. 
RI from 557.7 of Coulomb Ex. (1983Jh01) ignored 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J$|g rays to 1/2-, 5/2- and 7/2-. However, L>3 in (d,p),(d,t) indicating J=(7/2+,9/2-); possibly doublet, 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$|g to 7/2-, primary |g from (n,|g) E=2,24 keV res: av. However, L>3 in (d,p),(d,t) J|p assignments conflict 


level_energy_unit: KEV
level_spin_parity: 3/2,1/2(-)
level_comment:
J$assigned as 3/2+ in 1992Br17, but not reported in ARC measurements, and with |g transitions to 1/2-,3/2- and 5/2-, but no multipolarity is available, thus a more definite assignment can not be made 


level_energy_unit: KEV
level_comment:
$d|s/d|W=9 {I1} 
$Configuration=9/2[505] 
E$from 1975Mo29. 1976Be50 list 30.81 from compilations 
$L=high (1975Mo29) 
$d|s/d|W(90|')(d,t)=19 mb/sr {I2} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=147 {I12} 
E$70 {I2} (1975Mo29) 
$L=3 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=245 mb/sr {I7} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=233 {I16} 
E$95 {I1} (1975Mo29) 
$L=1 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=451 mb/sr {I10} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=84 {I6} 
E$from 1975Mo29. 1976Be50 list 216.8 from compilations 
$L=3 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=252 mb/sr {I7} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W=48 {IAP} 
E$from 1975Mo29. 1976Be50 list 275.8 from compilations 
$L=3 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=24 mb/sr {I2} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=64 {I5} 
E$365 {I3} (1975Mo29) 
$L=3 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=82 mb/sr {I4} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=100 {IAP} 
E$doublet at 436 {I2} and 446 {I4}, each with L=1, reported by 1975Mo29 but not confirmed by 1976Be50. 
$L=1 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=147 mb/sr {I5} for 439 level 


level_energy_unit: KEV
level_comment:
$d|s/d|W=60 {I5} 
E,L$from (d,p) only in 1975Mo29. Level population is treated as uncertain by the evaluators 


level_energy_unit: KEV
level_comment:
$d|s/d|W=5 {ILT} 
$Level either not populated in (d,p) or obscured by an impurity 
E$526 {I1} (1975Mo29) 
$L<5 in 1976Be50 
$d|s/d|W(90|')(d,t)=20 mb/sr {I3} 


level_energy_unit: KEV
level_comment:
$Level either not populated in (d,p) or obscured by an impurity 
E$554 {I1} (1975Mo29) 
$L=3 in 1975Mo29 is inconsistent with tentative (3/2-) assignment in authors' Fig. 4 
$d|s/d|W(90|')(d,t)=20 mb/sr {I3} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=193 {I14} 
E$597 {I3} (1975Mo29) 
$L=1 (1975Mo29,1976Be50) 
$d|s/d|W(90|')(d,t)=100 mb/sr {I4} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=8 {I2} 
$|s at 125|' in (d,p) (1975Mo29); <11 at 90|' 
E$620 {I1} (1975Mo29) 
$L=(high) in 1975Bo29 
$d|s/d|W(90|')(d,t)<5 mb/sr 


level_energy_unit: KEV
level_comment:
$Level either not populated in (d,p) or obscured by an impurity 
E$684 {I2} (1975Mo29) 
$L=1 in 1976Be50. L=3 in 1975Mo29 
$d|s/d|W(90|')(d,t)=149 mb/sr {I5} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=11 {I2} 
$|s at 125|' in (d,p) (1975Mo29) 
E$793 {I3} (1975Mo29) 
$L=(high) in 1975Bo29 
$d|s/d|W(90|')(d,t)<5 mb/sr 


level_energy_unit: KEV
level_comment:
$d|s/d|W=43 {I4} 
E$weighted average of (d,p),(d,t), and (n,|g) (1976Be50) 
E$997 {I1} (1975Mo29); (d,p) only 
$L=1 (1975Mo29,1976Be50) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=11 {I2} 
$Level from (d,p) in 1975Mo29, not populated in (d,t). Not reported in 1976Be50 
$L=high (1975Bo29) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
BE2$From 1961Re02. Other: 0.63 (1963Mc18) 
E$No |g transitions measured from this level. Only conversion electrons measured. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
BE2$others: 0.67 {I10} (1967Hr01) assuming B(E2,0+ to 2+)=2.30 for {+190}Os (1989Ra16 evaluation); 1.10 (1963Mc18) including contribution from 216 level 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T$weighted average of delayed coincidence measurements 1.59 ns {I8} (1970Ma37), 1.63 ns {I4} (1969Gr10), and 1.7 ns {I1} (1969An17) in {+189}Ir |e decay. 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 3/2-, g.s and 1/2-, 23.5-keV levels in {+185}W. Other: |> 7.6 |* 10{+17} y for decay to the 5/2- 65.9-keV level in {+185}W. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$186.7|g E2 to 0+ 
T$from B(E2)=2.364 {I50}, weighted average of the following values: B(E2)=2.34 {I13} (2012MaZP, from T{-1/2}=375 ps {I20}, |g|g(t) in ({+7}Li,2np|g); 2.35 {I16} (2001Wu03, from mean lifetime |t=540 ps {I36}, RDDS in Coul. ex.); 2.341 {I+62-34} (1996Wu07, Coul. ex.); 2.315 {I60} (1988Bo08, from (e,e'), uncertainty of 0.027 in 1988Bo08 increased to 0.060 by evaluators); 2.46 {I8} (1981Ho22, from muonic x-ray, uncertainty of 0.02 in 1981Ho22 increased to 0.06 by evaluators); 2.14 {I11} (1976Ba06, Coul. ex., uncertainty of 5% assigned by evaluators); 2.48 {I25} (1972La16, Coul. ex.); 2.37 {I13} (1971Mi08, Coul. ex.); 2.39 {I6} (1970Pr09, Coul. ex.); 2.55 {I25} (1969Ca19, Coul. ex., earlier value was 2.50 {I37} in 1967Ca08); 2.15 {I23} (1966Go06, from mean lifetime |t=0.58 ns {I6}, RDDS in Coul. ex.); 2.70 {I27} (1961Mc18, Coul. ex., previous values were 2.53 {I25} in 1961Mc01 and 2.55 {I26} in 1958Mc02); 2.51 {I36} (1958Su54, from T{-1/2}=0.35 ns {I5} from |g|g(t) in IT decay). Others: 1.86 {I8} (1967As03, from mean lifetime |t=680 ps {I30}, RDDS in Coul. ex.); 3.38 {I40} (1961Re02, Coul. ex.); 1.8 {I+12-5} (1958Be72, from T{-1/2}=0.5 ns {I2} in |e decay); 2.5 {I7} (1957Ba11, Coul. ex.). 2016Pr01 evaluation gives B(E2)=2.354 {I90} and corresponding T{-1/2}=373 ps {I15} 
$1958Su57 is same as 1958Su54. 
MOMM1$transient fields in Coulomb excitation (1992St06). Others: |m=+0.700 {I22} (1985St05) is reevaluated by 1987St14; 0.662 {I32} (1973BaUA; meson hyperfine structure), +0.66 {I6} (1972Si43,1972Si03; Coul. ex.), +0.62 {I3} (1970Be36,1967Gi02,1966Go06; Coul. ex.), 0.54 {I6} (1970Le04; IPAC in {+190}Ir |e decay using T{-1/2}=240 ps for 187 level). 
MOME2$muonic x-ray method (1981Ho22). Others: in Coulomb excitation, -0.99 {I13} (1970Pr03), -0.99 {I19} (1977RuZY), -0.95 {I21} (1972La16), -0.95 {I30} (1980Ba42, relative to Q=-1.47 for first 2+ state in {+188}Os), -0.8 {I3} (1980Ba42, relative to Q=-1.33 for first 2+ state in {+188}Os), 1.08 {I10} (1975Ro24, relative to 1.0 for first 2+ state in {+188}Os), 1.03 {I30} (1964Sp09, relative to 1.0 for the first 2+ state in {+192}Os); in {+190}Os(|g,|g):Mossbauer, 0.86 {I5} (1972Wa24, relative to 1.0 for 155, 2+ state in {+188}Os). 
$|b{-2}=0.225 from (p,p'), 0.181 from (|a,|a'), 0.168 from (n,n') 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$361.1|g E2, |DJ=2 to 2+ gives 0+ or 4+; spin=4 from |g(|q) in {+190}Ir |e decay (11.78 d); 447.8|g(E2)-207.9|g(E2(+M1)) cascade and 656.0|g(E2+M1) both from 1204 level to 548 level require J(548)|>2 
T$weighted average of 12.8 ps {I7} by recoil distance and 14.2 ps {I+4-10} from B(E2)(from 187,2+)=1.11 {I+8-3} in Coulomb excitation. Others: 40 ps {I20} from |g|g(t) in {+190}Os IT decay (1958Su57) 
BE2$from Coul. ex for transition from 187,2+ 
MOMM1$transient fields in Coul. ex. (1985St05). Value of 1.58 given by 1985St05 relative to |m(187)=+0.700 {I22} is adjusted (by evaluators) for adopted |m(187)=0.692 (1992St06,2014StZZ). Other: 0.88 {I48} (1970Le04, IPAC in {+190}Ir |e decay) 
$|b{-4}=-0.03 {I1} from (n,n') 
$B(E4)=0.045 {I5} from (e,e') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$from recoil distance in Coul. ex. Others: 14.8 ps {I+7-8} from B(E2)(from g.s.)=0.205 {I+8-6} in Coul. ex. (weighted average is 14.9 ps {I+7-8} if averaged with the RDM result); 7.9 ps {I+15-11} from B(E2)(from 187,2+)=0.42 {I6} in muonic atom with adopted branching ratios seems discrepant. 
MOMM1$transient fields in Coul. ex. (1985St05). Value of 0.69 given by 1985St05 adjusted (evaluators) for adopted |m(187)=0.692 (1992St06,2014StZZ) 
$Q=+0.9 {I4} or 0.55 {I30} from 1980Ba42 in Coul. ex., using Q=-0.8 for 187 level 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,t)=0; spin=0 from |g|g(|q) in (n,|g) E=th 
T$B(E2)(from 558,2+)=0.030 {I5} in Coul. ex. and adopted branching 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$768.6|g and 397.4|g E2 to 2+; 407.5|g E2+M1 to 4+; spin=4 from |g|g(|q) in {+190}Ir |e decay (11.78 d) 
T$others: 6.7 ps {I4} from B(E2)(from 558,2+)=0.70 {I3} and 7.5 ps {I6} from B(E2)(from 187,2+)=0.0082 {I+6-5} in Coul. ex. together with adopted branching 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$502.6|g E2 to 4+; spin=(6) from |g|g(|q) in {+190}Ir |e decay (11.78 d); band member; possible 631|g from 5- 
T$other: 2.60 ps {I11} from B(E2)(from 548,4+)=0.98 {I+4-3} in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$605.2|g E2 to 2+; 207.9|g to 4+; 407.2|g E2+M1 to 3+; E4 excitation in (|a,|a') 
T$other: 6.2 ps {I+11-8} from B(E2)(from 558,2+)=0.119 {I15} and adopted branching 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$447.8|g E2 to 3+; 656.0|g E2+M1 to 4+; spin=5 from |g(|q) in (n,n'|g) and {+190}Ir |e decay (11.78 d) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$828.96|g E1 to 2+, 223.8|g E1 to 4+; spin=3 from |g(|q) and |g|g(|q) in {+190}Ir |e decay (11.78 d) 
T$from B(E3)(from g.s.)=0.154 {I13} in (e,e') and adopted branchings 
$|b{-3}=0.06 (from (n,n')) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$877.7|g E2(+M1) to 2+; 481.0|g and 887.9|g to 4+, 524.0|g to 0+; spin=2 from 680|g(|q) in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J$690.0|g (E2) to 3+, 490.7|g (E2) to 4+, 282.9|g E2(+M1) to 4+; spin=(5) from 690|g(|q) and excitation function in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
J$518.8|g to 4+, 423.8|g to 6+; probable band member 
T$other: 2.3 ps {I+6-4} from B(E2)(from 955,4+)=0.75 {I+7-10} and adopted branching 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
E$in (d,p) and (t,|a) the groups correspond to 1569 and/or 1570 
J$1011.0|g E2(+M1) to 2+, 1021.9|g to 4+; spin=(3) from 1011|g(|q) and excitation function in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J$196.9|g E2+M1 to 3-, 380.0|g E1 to 5+, 1036.1|g E1 to 4+ 
$Excitation considered uncertain in {+190}Re |b{+-} decay (3.1 h) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$1117.7|g M1(+E2) to 2+, 919.6|g E2(+M1) to 3+; spin=(2) from excitation function and 920|g(|q) in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$|gs to 4+ and 0+; |g(|q) of |g to 2+ in (n,n'|g) 
$On the basis of excitation function data in (n,n'|g), two separate levels are reported, at 1688.9 (deexcited by 1131|g and 1142|g) and 1689.2 (deexcited by 933|g and 1502|g); however, the relative intensities of all the four |g rays agree well in both reactions: (n,|g) (E=th and E=res) and (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$38.9|g M2+E3 to 8+ 
T$from |g(t) in 2012Kr05. Others: 9.9 min {I1} (1958Sc30), 9.85 min {I14} (1964Ti01), 11 min (1962Ma24), 1961Ma31, 10 min {I2} (1955At32), 9.5 min (1950Ch11) 
MOMM1$from |g(|q,t,H) (1987Be54) 
$Configuration=|n9/2[505]+|n11/2[615] 


level_energy_unit: KEV
level_spin_parity: (2+,3,4+)
level_comment:
J$753.2|g to 4+, 1150.7|g to 2+. 952|g(|q) in (n,n'|g) disfavors 3-. Possible population in (d,d') (priv. comm., cited by 1984KlZY) makes 3+ unlikely 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J$excitation function and 1616|g(|q). J|p=1+ less likely if possible population in (d,d') (priv. comm., cited by 1984KlZY) 


level_energy_unit: KEV
level_spin_parity: (1+,2,3+)
level_comment:
J$1255|g(|q) (to 2+) implying D+Q suggests J|=0,1-,3- and excitation function favors low spin (|<3) 
$Uncertain in (n,|g) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$log {Ift}=7.4 from (6-); 673.1|g to 4+. Because of direct multi-step excitation in Coul. ex., J=5+ less likely. 


level_energy_unit: KEV
level_spin_parity: (3+,4-)
level_comment:
E$in (n,n'|g), on the basis of excitation functions, two levels are suggested: at 1902.9 (decaying through 1147|g) and 1903.3 (decaying through 740|g). However, branching ratios of both transitions agree well in {+190}Ir |e, (n,|g) and (n,n'|g) 
J$log {Ift}=6.2 from 4-; 1147|g(|q) (to 3+) in (n,n'|g) implying D+Q suggests J|=5, 3- 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$1154.4|g E2(+M1) to 3+, 955.7|g to 4+; primary 5881.2|g from 1- and 2- resonances in (n,|g) E=res. Possible population in (d,d') (priv. comm., cited by 1984KlZY) makes 3+ unlikely 


level_energy_unit: KEV
level_spin_parity: (2+,3+,4)
level_comment:
J$from |g(|q) in (n,n'|g). Possible population in (d,d') (priv. comm., cited by 1984KlZY) makes 3+ unlikely 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_comment:
E$from (n,|g). This level is uncertain in (n,|g) 
J$possible primary 5749.7|g from 1- and 2- in (n,|g) E=res 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E$weighted average of 2451 {I10} from (t,p), 2450 {I5} from (d,p), 2437 {I8} from (t,|a), and 2440 {I10} from (p,t) 
J$L(t,p)=(0) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$populated in Coul. ex.; 654|g to (10+) 
T$0.7 ps to 1.9 ps from B(E2)(from 2357,10+)=0.32 to 0.76 in Coul. ex. 
$Either of the 3011 or 3126 levels may be member of g.s. band 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$populated in Coul. ex.; 769|g to (10+) 
T$0.4 ps to 4.8 ps from B(E2)(from 10+ level)=0.048 to 0.55 in Coul. ex. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Magnetic splitting=0.66 keV {I+8-4} (1972Li33) 
$Muonic isomer shift (from |g-ray data)=-0.145 keV {I+65-45} (1974Ba77). Other: -0.01 keV {I7} (from x-ray data, 1981Ho22) 
$|m=0.662 {I32} (1973BaUA) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2)(from 2+,187)=0.42 {I6} (1981Ho22) 
$Muonic isomer shift (from |g-ray data)=+1.44 keV {I12} (1974Ba77) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$A detailed analysis of |s(|q) data with coupled-channel calculations by 1978Bu21 gives a strong evidence for E4 excitation, thus identifying this state as due to hexadecapole vibrations 
$|b{-4}=0.019 (1978Bu21) (for pure E4 excitation). The authors also give |b{-4}=0.0163 (for constructive interference) and 0.0230 (for destructive interference) when both modes of excitation (E4 and 2-step E2) are considered 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 2.341 {I+62-34} (1996Wu07), 2.48 {I25} (1972La16), 2.37 {I13} (1971Mi08), 2.39 {I6} (1970Pr09), 2.50 {I37} (1967Ca08), 2.53 {I25} (1961Mc01), 2.72 {I27} (1961Mc18), 2.55 {I26} (1958Mc02), 2.5 {I7} (1957Ba11). Other: 3.4 {I4} (1961Re02) 
J$|g(|q) indicates spin=2 (1957Mc43,1961Mc18) 
T$weighted average of 374 ps {I25} from 2001Wu03 and 369 ps {I+5-9} from B(E2)=2.37 {I+6-3}. Other: 0.47 ns {I2} from 1967As03 by recoil distance seems discrepant 
G$from transient-field technique (1992St06). Others: +0.338 {I10} (reevaluated by 1987St14 from 0.350 {I11} given in their earlier work (1985St05)) (transient-field technique); 0.33 {I3} (1970Be36,1967Gi02, 1966Go06), +0.39 {I3} (1972Si43,1972Si03). 
MOME2$others: -0.99 {I19} (1977RuZY), -0.95 {I21} (1972La16), -0.95 {I30} (1980Ba42, relative to Q=-1.47 for first 2+ state in {+188}Os), -0.8 {I3} (1980Ba42, relative to Q=-1.33 for first 2+ state in {+188}Os), 1.08 {I10} (1975Ro24, relative to 1.0 for first 2+ state in {+188}Os), 1.03 {I30} (1964Sp09, relative to 1.0 for the first 2+ state in {+192}Os) 
$Static E2 matrix element (187 to 187)=-1.25 {I+22-13} (1996Wu07) 
$E2 matrix element (from g.s.,0+)=(+)1.530 {I+20-11} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$from 187,2+, weighted average of 1.12 {I+8-3} (1996Wu07), 1.19 {I12} (1971Mi08), and 1.07 {i10} (1969Ca19) 
T$weighted average of 12.8 ps {I7} from 2001Wu03 by recoil distance, and 14.2 ps {I+4-10} from B(E2)=1.11 {I+8-3} 
G$from (|g(|q,H), transient fields) in 1985St05. Since the measurement was relative to g factor (187 level), value of 0.396 {I47} given by 1985St05 has been adjusted (evaluators) for revised g factor(187 level)=0.346 (1992St06) 
$Static E2 matrix element (548 to 548)=-1.28 {I+27-19} (1996Wu07) 
$E2 matrix element (from 187,2+)=(+)2.37 {I+8-3} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 15.2 ps {I14} from 2001Wu03 by recoil distance, and 14.8 ps {I+7-8} from B(E2)(from g.s.)=0.205 {I+8-6} and branching ratio %I(|g+ce)=57.9 {I20} for 558|g deduced from the Adopted I|g values 
BE2$from g.s.,0+, weighted average of 0.197 {I+8-6}, 0.234 {i14} (1971Mi08), 0.220 {i20} (1969Ca19), 
$B(E2)(from 187,2+)=0.227 {I+8-16} (1996Wu07), 0.270 {i20} (1971Mi08), 0.245 {i22} (1969Ca19) 
$B(E2)(from 548,4+)=0.004 {I+7-3} (1996Wu07) 
$E2 matrix element (from g.s.,0+)=+0.444 {I+9-7} (1996Wu07) 
$E2 matrix element (from 187,2+)=(+)1.065 {I+20-37} (1996Wu07) 
$E2 matrix element (from 548,4+)=+0.19 {I+12-9} (1996Wu07) 
$Static E2 matrix element (558 to 558)=+1.53 {I+6-31} (1996Wu07), +1.2 {I5} (1980Ba42) 
G$from (|g(|q,H), transient fields) in 1985St05. Since the measurement was relative to g factor (187 level), value of 0.344 {I43} given by 1985St05 has been adjusted (evaluator) for revised g factor(187 level)=0.346 (1992St06) 
$Q=0.9 {I4} or 0.55 {I30} from 1980Ba42, using Q(187 level)=-0.8. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$B(E2)(from 558,2+)=0.030 {I5} (1996Wu07) 
$E2 matrix element (from 558,2+)=(+)0.384 {I+37-32} (1996Wu07) 
$E2 matrix element (from 187,2+)=0.119 {I10} (1996Wu07) obtained by using branching ratios from literature 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$others: 6.7 ps {I4} from B(E2)(from 558,2+)=0.70 {I3} and 7.5 ps {I6} from B(E2)(from 187,2+)=0.0082 {I+6-5}, with %I(|g+ce) branching ratios for 397|g and 769|g deduced from the Adopted I|g values 
$B(E2)(from 187,2+)=0.0082 {I+6-5} (1996Wu07), 0.0187 {I37} (1969Ca19) 
$B(E2)(from 558,2+)=0.70 {I3} (1996Wu07), 0.88 {I18} (1969Ca19) 
$B(E2)(from 548,4+)=0.229 {I14} (1996Wu07), 0.36 {I7} (1969Ca19) 
$E2 matrix element (from 187,2+)=+0.230 {I7} (1996Wu07) 
$E2 matrix element (from 548,4+)=+1.44 {I4} (1996Wu07) 
$E2 matrix element (from 558,2+)=(+)1.87 {I4} (1996Wu07) 
$Static E2 matrix element (955 to 955)=-1.29 {I+20-25} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$other: 2.60 ps {I11} from B(E2)=0.98 {I+4-3} from 1996Wu07 
$B(E2)(from 548,4+)=0.98 {I+4-3} (1996Wu07). Other: 1.50 {i23} (1969Ca19) 
$B(E2)(from 955,4+)=0.048 {I+46-11} (1996Wu07) 
$Static E2 matrix element (1050 to 1050)=-0.91 {I+24-15} (1996Wu07) 
$E2 matrix element (from 548,4+)=(+)2.97 {I+6-4} (1996Wu07) 
$E2 matrix element (from 955,4+)=+0.66 {I+26-8} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$other: 6.2 ps {I+11-8} from B(E2)(from 558,2+)=0.119 {I15} and adopted branching ratios 
$B(E2)(from 187,2+)=0.00054 {I+11-13} (1996Wu07) 
$B(E2)(from 548,4+)=0.0044 (1996Wu07) 
$B(E2)(from 558,2+)=0.119 {I15} (1996Wu07) 
$B(E2)(from 955,4+)=0.28 {I+4-6} (1996Wu07) 
$E2 matrix element (from 187,2+)=+0.052 {I+5-7} (1996Wu07) 
$E2 matrix element (from 548,4+)=[-0.2,0.2] (1996Wu07) 
$E2 matrix element (from 558,2+)=(+)0.77 {I5} (1996Wu07) 
$E2 matrix element (from 756,3+)=(-)1.55 {I+7-40} (1996Wu07) obtained by using branching ratio in literature 
$E2 matrix element (from 955,4+)=+1.59 {I+11-17} (1996Wu07) 
$Static E2 matrix element (1163 to 1163)=+1.02 {I+18-4} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
T$other: 2.3 ps {I+6-4} from B(E2)(from 955,4+)=0.75 {I+7-10} and adopted branching ratios 
$B(E2)(from 548,4+)=0.0042 {I40} (1996Wu07) 
$B(E2)(from 955,4+)=0.75 {I+7-10} (1996Wu07) 
$B(E2)(from 1050,6+)=0.24 {I+6-4} (1996Wu07) 
$E2 matrix element (from 548,4+)=+0.20 {I7} (1996Wu07) 
$E2 matrix element (from 955,4+)=(+)2.60 {I+12-16} (1996Wu07) 
$E2 matrix element (from 1050,6+)=+1.76 {I+20-15} (1996Wu07) 
$Static E2 matrix element (1474 to 1474)=-0.80 {I+47-27} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$0.78 ps {I4} from B(E2) 
$B(E2)(from 1050,6+)=1.06 {I+6-5} (1996Wu07) 
$Static E2 matrix element (1667 to 1667)=-0.94 {I+49-41} (1996Wu07) 
$E2 matrix element (from 1050,6+)=(+)3.72 {I10} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_lifetime_unit: PS
level_comment:
$B(E2)(from 1474,6+)=0.52 {I+15-7} (1996Wu07) 
$E2 matrix element (from 1474,6+)=(+)2.60 {I+39-19} (1996Wu07) 
$Static E2 matrix element (2090 to 2090)=-1.05 {I+62-38} (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
$B(E2)(from 1667,8+)=0.93 {I+22-17} (1996Wu07) 
$E2 matrix element (from 1667,8+)=(+)3.98 {I4} (1996Wu07) 
$Static E2 matrix element (2357 to 2357)=[-1.9,-0.7] (1996Wu07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (12+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$B(E2)(from 2357,10+)=0.32 to 0.76 (1996Wu07) 
$E2 matrix element (from 2357,10+)=[2.6,4.0] (1996Wu07) 
T$0.7 ps to 1.9 ps from B(E2) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (12+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$B(E2)(from 2357,10+)=0.048 to 0.55 (1996Wu07) 
$E2 matrix element (from 2357,10+)=[1.0,3.4] (1996Wu07) 
T$0.4 ps to 4.8 ps from B(E2) 


level_energy_unit: KEV
level_spin_parity: 4-
level_uncertain: ?
level_comment:
$Population in {+190}Re decay is suspect since the only |g ray reported is 1036.0, other |g rays of comparable intensity such as 196.8|g, 380.0|g, 420.6|g are not reported 


level_energy_unit: KEV
level_spin_parity: (10)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from time variation of 4 |g lines (186.7, 361.1, 502.5, 616.3 keV) from {+190m}Os decay, weighted average of 28 values (2012Kr05). Other: 9.1 m {I1} (1958Sc30) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured by 2012MaZP (also reported in 2013Ma74) from time difference between 187 depopulating |g and 361-371 doublet feeding transitions 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$Excitation function data do not support a 1383|g from this level as suggested by 1979Ca02 in (n,|g) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=9.2 {I7} 
$Doublet (548+558). Estimated |s=1.2 for 548 and 8.0 for 558 (1979Ba25). Ay(doublet)=-0.02 {I14} (1987Ci06) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=27.8 {I12} 
$A{-y}=+0.27 {I7} (1987Ci06) 
$Interpreted as an hexadecapole vibration with main component (|?54% in the analysis by 1997Bu10) from configuration=|p3/2[402]+|p5/2+[402], K|p=4+ (1987Ci06,1997Bu10). Also interpreted as a mixture of phonon components such as g-boson and s-d boson states in the interacting boson model (1985Ba64) 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 2+, 122.6-keV level in {+186}W. Other: |> 8.6 |* 10{+19} y for decay to the 4+, 396.5-keV level in {+186}W. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: D
level_comment:
J$L(d,p),(d,t)=5; spectroscopic factors in (d,p) and (d,t) are consistent with 9/2, 9/2[505]. Nilsson orbital assignment based also on energy systematics of this orbital in other odd-mass Os isotopes. 
T$From 2012Kr05 (129|g(t)). Other values: 15.4 d {I1} (1967Ag07), 14.60 d {I43} (1980Da24), 14.4 d {I11} (1969Bi01), 14.6 d {I3} (1958Na15, 1958Na45), 16.0 d {I3} (1950Ch11), 16.1 d {I2} (1948Sa18), 15.0 d (1948Ka08). Unweighted average of all value: 15.2 d {I3}; Weighted average without 16.0 d {I3} (1950Ch11) and 16.1 d {I2} (1948Sa18) is 15.00 d {I4} - |h{+2}=4.8 cf. |h{+2}{-crit}=2.4. 
MOMM1 From 2019StZV,1996Oh03 - NMR-oriented nuc in {+191}Os |b-decay in Fe matrix. 
MOME2$From 2016St14,1979Er09 - static (low-temperature) nuclear orientation. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
No |b{+-} decay observed (<5%) (1952Sw57). Other study: 1963Pl01. 
J M3+E4 |g to 9/2- g.s., primary |g in (n,|g) from 1/2+. In {+189}Os, 3/2[512] orbital is the ground state. Spectroscopic factors in (d,p) and (d,t) are smaller than those predicted by the Nilsson model, but they follow the trend observed for this orbital in {+189}Os. 
T from 1975Ca03. Other values: 13.03 h {I21} (1966Pl02), 13.0 h {I5} (1963Pl01), 14 h {I2} (1952Sw57). 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J 57.5|g M1+E2 from (3/2)-; populated by a primary transition from 1/2+ in (n,|g); Nilsson orbital assignment based on energy systematics of this orbital in other odd-mass Os isotopes and on band structure. Level not populated in (d,p) nor (d,t), consistent with 1/2, 1/2[510]. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$ L=3 in (d,p) and (d,t), 47.5|g E2 to (1/2)-. Spectroscopic factors in (d,p) and (d,t) follow the trend observed for the 3/2[512] orbital in {+189}Os. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$L=1 in (d,p) and (d,t), 67.5|g M1+E2 to 3/2-. Nilsson orbital assignment based on band structure. Spectroscopic factors in (d,p) and (d,t) follow the trend observed for this orbital in {+189}Os. This state is expected to be mixed with the 3/2, 3/2[512] state by a Coriolis interaction. 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_comment:
J 176|g E1 to 9/2-; 177|g from (13/2)+ 352.9; 349|g (E2) cross-over from 524.7 yrast state, which also feeds (13/2)+ at 352.9. 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_comment:
J L=6 in (d,p) and (d,t). Nilsson orbital assignment based on energy systematics of this orbital in other odd-mass Os isotopes. Spectroscopic factors in (d,p) and (d,t) are consistent with 13/2, 11/2[615]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)-
level_comment:
J L=3 for 442 + 447 in (d,p) and (d,t). Energy consistent with that of 446.9 level. However, observed as a doublet in (d,p) and (d,t), with spectroscopic factors consistent with 5/2, 1/2[510]. The same state has been observed in {+193}Os by 1979Wa04 and a spin of 5/2 was assigned on the basis of its decay to a J=1/2 level. Nilsson orbital assignment based also on band structure. This state is mixed by the Coriolis interaction with other N=5 orbitals. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$189.7|g M1+E2 to 5/2-, 462.5|g M1+E2 to 9/2-. Spectroscopic factors in (d,p) and (d,t) are consistent with 7/2, 7/2[503]. The predominant hole character indicated by the transfer cross sections further supports this assignment. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
J$553|g M1(+E2) to (1/2)-, 365|g E2(+M1) to 5/2-; populated by (E1) primary |g ray from 1/2+ capture state in {+190}Os(n,|g) E=2 keV. 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J L=1 in (d,t),(d,p), (3/2+,5/2+,7/2+) in (n,|g) E=thermal. 414|g M1+E2 from 1176.6 {I3}/2+,(5/2+) is inconsistent with parity for L=1. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
J 347.5|g E1 to 1/2-,3/2-, 353.8|g E2 to 7/2+. 
Level observed in {+192}Os(p,pn|g) and deep inelastic may be different; insufficient information on decay properties 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$378.4|g M1+E2 to (3/2)-; populated by (E1) primary |g from 1/2+ capture state in (n,|g) E=2 keV; 302.6|g M1 from (5/2)-. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
J$590|g M1+E2 to (3/2)-; populated by (E1) primary |g ray from 1/2+ capture state in (n,|g) E=2 keV. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
J$950|g M1(+E2) to (3/2)-; populated by (E1) primary |g ray from 1/2+ capture state in (n,|g) E=2 keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (29/2,31/2)
level_lifetime_unit: NS
level_comment:
J 453|g to (27/2)+ yrast level in {+192}Os({+82}Se,{+83}Se|g) and {+198}Pt({+136}Xe,{+143}Ba). 
T$From 2004Va03, time-delayed |g|g coincidence in {+198}Pt({+136}Xe,{+143}Ba){+191}Os E=850 MeV (see {+192}Os({+82}Se,{+83}Se|g) dataset) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E$5758.73 keV {I16}, deduced value in 1991Bo35. Sn=5758.73 {I11} in 2021Wa16 - AME. 
J$for s-wave capture. 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_uncertain: ?
level_comment:
J 326|g (Q) to g.s. and more intense than 349|g in |p=+ band indicates stretched E2 yrast band transition 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E,J From 1985Ni12, level not reported in other studies and not adopted. See general comments on this dataset. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
E$Comparable to 1118.001 excited level in the adopted dataset - however depopulating |g rays of this level are different compared to that of the adopted level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2)+
level_comment:
2005Jo19 deduce (g{-K}-g{-R})/Q{-0}=0.022 {I3} from experimental |g-intensity values, assumed spins, and K=11/2. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (19/2+)
level_comment:
2005Jo19 deduces (g{-K}-g{-R})/Q{-0}=0.024 {I7} from experimental |g-intensity values, assumed spins, and K=11/2. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (29/2,31/2)
level_lifetime_unit: NS
level_comment:
E$ It is assumed that the isomer decays directly by 453|g, but possibility of a low-energy |g transition preceding 453|g is not ruled out. Suggested configuration (2005Jo19): |n11/2[615]+|p11/2[505]+|p9/2[514], J|p=31/2+, giving an hindrance factor for the 453|g, deduced to be E2, in agreement with the systematics in the mass region. 
T$ (target like recoil fragments)|g(t) (2004Va03,2004Re11); 349|g-453|g pair; 176|g-453|g-457|g-459|g-657|g cascade used as |g-ray gates. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T{-1/2}(2|b{+-})>9.8|*10{+12} y (specific activity measurements, 1952Fr23, as reassessed by 1995Tr07 assuming Q(2|b{+-})=413 {I3}). 
<r{+2}>{+1/2}(charge)=5.4127 {I11} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 IMPAC (1989Ra17; from 1985St05, 1973BaUA, 1972Si43, 1971Ki13, if T{-1/2}=289 ps {I7}). See 1987St14, 1992St06, 2011StZZ for further evaluation/compilation of |m data. 
MOME2 Hyperfine structure of muonic x rays (1989Ra17 from 1981Ho22). Other values: -0.80 {I18} and -0.86 {I20} (Coulomb excitation reorientation; 1989Ra17, from 1983Ch35 and 1988Li22, respectively). 
|b{-2}(nuclear)=0.14, |b{-2}(Coulomb)=0.164 from (|a,|a'). 
J E2 206|g to 0+ g.s. 
T other value: 300 ps {I20} (X|g(t) in {+192}Ir |e decay (73.829 d), 1973Ch26). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 Transient field IPAC (1989Ra17, from 1985St05 and 1983Bo13); value relative to +0.792 {I20} for {+192}Os(205.8 level). 
MOME2 Coulomb excitation reorientation (1989Ra17, from 1980Ba42); value relative to -1.46 {I4} for {+188}Os(155 level). 
J E2 489|g to 0+ g.s. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$transient field IPAC (1989Ra17, from 1985St05 and 1983Bo13); value relative to +0.792 {I20} for {+192}Os(205.8 level). 
B(E4): weighted average of 0.037 {I4} and 0.048 {I4} from (e,e'). 
|b{-4}(nuclear)=-0.026 from (|a,|a'); E4 matrix element is -1960 e|*fm{+4} {i110} from (pol p,p'). 
J E4 excitation in (e,e'); E2 374|g to 2+ 206. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1 Transient field IPAC (1989Ra17, from 1985St05); value relative to +0.792 {I20} for {+192}Os(205.8 level). 
|b{-4}(nuclear)=+0.005 from (|a,|a'); E4 matrix element is 1160 e|*fm{+4} {i290} from (pol p,p'). 
J analyzing powers in {+193}Ir(t,|a), (pol t,|a); evidence for 4+ excitation in {+192}Os(p,p'), (pol p,p') and {+192}Os(|a,|a'). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
|b{-4}(nuclear)=-0.010 from (|a,|a'); E4 matrix element is 1080 e|*fm{+4} {i270} from (pol p,p'). 
J M1+E2 379|g to 3+ 690; E4 excitation in {+192}Os(p,p'), (pol p,p') and {+192}Os(|a,|a'). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J E3 excitation in (e,e') and Coulomb excitation. |g-ray branchings to 2+, 3+, and 4+ levels in {+192}Os(p,p'|g), (d,d'|g) fit Alaga rule for E1. 
T from measured B(E3)|^=0.131 {I9} from (e,e') assuming 1341.4|g in (n,n'|g) deexcites this level. Note, however, that T{-1/2}=28 ps {I4} if B(E3)|^=0.37 {I4} (from Coulomb excitation) is assumed. 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
Identification: excitation functions for neutrons on {+192}Os and absence of |b{+-} activity (1973Pa21, 1979KaYT); decay to known levels in {+192}Os (1965Bl12, 1973Pa21, 1979KaYT). 
%IT: only IT decay observed. %|b{+-}<13 was deduced from I|b/I|g(205.8|g)<0.2 (1973Pa21). 1965Bl12 reported |b{+-} activity with E|b|?2.5 MeV, but results were never confirmed and are not consistent with Q(|b{+-}). 
J (M2) 307|g to 8+ 1708; level is most likely a 2-quasiparticle state with neutron configuration (9/2[505]+11/2[615]) (analogous to {+190}Os (9.9 min) which has a similarly-hindered M2 transition to the J=8 member of the g.s. band). 
T from IT decay (5.9 s) (1979KaYT). Other values: 6.2 s {I8} (1965Bl12), 6.1 s {I2} (1973Pa21). 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J from excit in (n,n'|g); consistent with 1585|g to 3+ 690 and 2069|g to 2+ 206 which limit J|p to (1+,2,3,4+). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
E assuming that the isomer decays directly by 446|g, but the possibility of a low-energy transition preceding the 446|g cannot be ruled out. 
J tentative value suggested in {+198}Pt({+136}Xe,X|g); 446|g feeds (14+) 2987. 
T (target-like recoil fragments)-|g(t) (2004Va03,2004Re11); 446|g-375|g pair and 681|g-568|g pair used as double |g gates. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
B(E2)=2.009 {I32} (1984Re10; analysis combined authors' (e,e') data with earlier muonic-atom data); B(E2)=1.999 {I23} (1988Bo08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
Other B(E3)|^:0.130 {I34} (1984Re10). 
E average of 1341 (1984Re02,1984Re10) and 1362 (1988Bo08). Level is equated with 1341.1, 3- adopted level (B(E3) very close to calculated (random phase approximation) strength for 3- bandhead and to B(E3) for neighboring Os isotopes (1984Re10)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
J from behavior of form factor at low momentum transfer (1988Bo08). 
B(E4)=1.60|*10{+-3} {I13} (1988Bo08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E4=1080 {I27} 
1985Ba64, 1989Ba54 suggest that level is lowest g-boson intruder state (single g-boson coupled to a 0+ system of s and d bosons). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4-)
level_uncertain: ?
level_comment:
E,J 1976Ja18 establish level from a surprisingly strong 220|g-852|g coin and assign J|p=(4-) based on transitions to (3-) and (5+) levels and on level systematics in neighboring even-A Os isotopes. 1983Kl06 (in {+192}Os(n,n'|g)) observe both the gammas placed from this level by 1976Ja18; however, in (n,n'|g), the 220|g is placed from the 910 level, and excit for the unplaced 417|g is inconsistent with J=4. A 219.7|g (in {+192}Ir) is expected from competing reactions, but should not appear in a spectrum gated by the 852|g. Nevertheless, the evaluator considers the existence of this level to be questionable. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)(g.s. to 206(2+))=2.043 {I22}. 
BE2 Unweighted average of 2.04 {I21} (1958Mc02), 1.92 {I25} (1967Gi02), 2.21 {I22} (1969Ca19), 2.04 {I6} (1970Pr09), 1.99 {I11} (1971Mi08), 2.09 {I21} (1972La16), 2.10 {I2} (muonic atom; 1981Ho22), 2.01 {I3} ({+192}Os(e,e'); 1984Re10), 1.999 {I23} ({+192}Os(e,e'); 1988Bo08), 2.030 {I13} (1988Li22), 2.120 {I+23-26} (1996Wu07), 1.97 {I16} (1997Bb08). The weighted average of these data is 2.047 {I13}. 
Static matrix element, <2+ M(E2) 2+> =-1.21 {I+6-17} (1996Wu07). 
g-factor=0.30 {I4} (1967Gi02), 0.39 {I3} (1972Si43), 0.383 {I9} (1987St14, reevaluation of 0.393 {I18} in 1985St05); g/g({+188}Os 2{++})=1.31 {I5} (1992St06). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)(g.s. to 489(2+))=0.185 {I+7-4} (1996Wu07). 
BE2 Other B(E2): 0.215 {I19} (1969Ca19), 0.196 {I12} (1971Mi08), 0.19 {I3} ((e,e'), 1984Re10), 0.187 {I6} ((e,e'), 1988Bo08). The unweighted average of all data is 0.195 {I5} 
B(E2)(206(2+) to 489(2+))=0.303 {I+17-8} (1996Wu07). Others: 0.36 {I3} (1969Ca19), 0.33 {I4} (1971Mi08), 0.37 {I5} (muonic atom, 1981Ho22). 
Static matrix element, <2+ M(E2) 2+> =+0.99 {I+5-9} (1996Wu07). 
g-factor=0.32 {I3} (1985St05). 
T weighted average of 34.1 ps {I+14-19} from B(E2)(283|g) and 32.1 ps {I+8-13} from B(E2)(489|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B(E2)(206(2+) to 580(4+))=0.895 {I24} (1996Wu07). Other values: 0.98 {I9} (1969Ca19); 0.97 {I12} (1971Mi08). 
B(E2)(489(2+) to 580(4+))=0.024 {I+28-5} (1996Wu07). 
Static matrix element, <4+ M(E2) 4+> =-0.73 {I+26-6} (1996Wu07). 
g-factor=0.39 {I4} (1985St05). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B(E2)(489(2+) to 910(4+))=0.536 {I+16-21} (1996Wu07). Other: 0.31 {I6} (1969Ca19). 
B(E2)(580(4+) to 910(4+))=0.203 {I+24-12} (1996Wu07). Other: 0.37 {I18} (1969Ca19). 
B(E2)(206(2+) to 910(4+))=0.0034 {I+3-4} (1996Wu07). 
Static matrix element, <4+ M(E2) 4+> =-0.83 {I+9-8} (1996Wu07). 
T from B(E2)(421|g); 9.7 ps {I+12-15} from B(E2)(329|g), 9.0 ps {I+13-8} from B(E2)(704|g). 
g-factor=0.43 {I9} (1985St05). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
B(E2)(489(2+) to 956(0+))=0.040 {I+4-3} (1996Wu07). Other: 0.0154 {I16} (1993Os05), inconsistent with datum from 1996Wu07. 
B(E2)(206(2+) to 956(0+))=0.00079 {I+22-23}, assuming adopted branching (1996Wu07). 
T from B(E2)(467|g); 10 ps {I3} from B(E2)(751|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B(E2)(489(2+) to 1069(4+))=0.124 {I+11-18} (1996Wu07). Other: 0.103 {I11} (1993Os05). 
B(E2)(206(2+) to 1069(4+))=0.0026 {I+25-12} (1996Wu07). Other: 0.021 {I15} (1993Os05); inconsistent with datum from 1996Wu07 and with branching from other reactions. 
B(E2)(690(3+) to 1069(4+))=0.38 {I+5-10}, assuming transition is E2 (1996Wu07). 
B(E2)(910(4+) to 1069(4+))=0.157 {I+22-27}, assuming transition is E2 (1996Wu07). 
Static matrix element, <4+ M(E2) 4+> =+1.28 {I+15-41} (1996Wu07). 
T from B(E2)(580|g). 
State contains a significant two-phonon |g vibrational component (based on systematics of E, branching, E2 strengths, static Q), but must also contain a hexadecapole component (based on E4 strength and transfer reaction cross sections) (2001Wu03 and subsequent discussion of that paper). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
B(E2)(580(4+) to 1089(6+))=0.95 {I+5-3} (1996Wu07). Other: 1.26 {I25} (1969Ca19). 
B(E2)(910(4+) to 1089(6+))=0.017 {I+9-10} (1996Wu07). 
Static matrix element, <6+ M(E2) 6+> =-1.16 {I+11-26} (1996Wu07). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
B(E2)(690(3+) to 1128(2+))=0.0101 {I10} (1993Os05). 
B(E2)(489(2+) to 1128(2+))=0.00247 {I25} (1993Os05). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
B(E2)(910(4+) to 1465(6+))=0.49 {I+3-6} (1996Wu07). 
B(E2)(580(4+) to 1465(6+))=0.0005 {I+52-5} (1996Wu07); |g not observed. 
B(E2)(1089(6+) to 1465(6+))=0.171 {I+36-14} (1996Wu07). 
Static matrix element, <6+ M(E2) 6+> =-1.35 {I+11-37} (1996Wu07). 
T from B(E2)(556|g). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
B(E2)(1089(6+) to 1708(8+))=0.99 {I5} (1996Wu07). 
Static matrix element, <8+ M(E2) 8+> =-1.31 {I+18-36} (1996Wu07). 


level_energy_unit: KEV
level_spin_parity: (7+)
level_uncertain: ?
level_comment:
1993Os05 report a 323|g deexciting this level, but not the much stronger 606-keV branch which is expected; therefore, the evaluator considers excitation of this level to be uncertain. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
B(E2)(1465(6+) to 2134(8+))=0.41 {I+6-5} (1996Wu07). 
Static matrix element, <8+ M(E2) 8+> =-0.9 {I+5-3} (1996Wu07). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
B(E2)(2419(10+) to 3104(12+))|<0.21 (1996Wu07). 
Member of |p=+ band whose states are yrast for J|>12. 


level_energy_unit: KEV
level_comment:
$A{-y}=+0.22 {I12} 
d|s/d|W(50|')=12.1 |mb/sr (1979Ba25). 
Transition not dominated by single-step d{-3/2} p transfer, but includes either some d{-5/2} transfer strength or reflects presence of some higher-order mechanism (1987Ci06). 


level_energy_unit: KEV
level_comment:
$A{-y}=+0.33 {I8} 
d|s/d|W(50|')=29.3 |mb/sr (1979Ba25). 
Level contains large amplitudes of both two-phonon |g-vibration and one-phonon hexadecapole vibration (1979Ba25). Analyzing power from 1987Ci06 supports this interpretation. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (16+)
level_lifetime_unit: NS
level_comment:
E it is assumed that the isomer decays directly by 446|g, but the possibility of a low-energy transition preceding the 446|g cannot be ruled out. 
T (target-like recoil fragments)-|g(t) (2004Va03,2004Re11); 446|g-375|g pair and 681|g-568|g pair used as double |g-ray gates. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (10-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$half-life of highly-ionized (H-like) {+192m}Os deduced by 2015Ak02 from a least-squares fit to the decay curve obtained using the Schottky mass spectroscopy (2015Ak02). In comparison half-life of neutral atom is 5.9 s {I1} as in Adopted Levels of {+192}Os in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Only the IT decay mode has been observed. In the Adopted Levels for {+192}Os in ENSDF database, %|b{+-} is listed as <13% based on estimate by 1973Pa21: Physica Fennica 8, 345 
CONF$|n9/2[505]~#|n11/2[615] 
T$from {+192}Os Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from (206|g in LaBr{-3})(374|g in LaBr{-3})(t) (2017Da06). This value can be compared with 288 ps {I4} in {+192}Os Adopted Levels in the ENSDF database (June 2012 update) 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for decay to the 0+, g.s. level in {+188}W. Other: |> 2.7 |* 10{+19} y for decay to the 2+, 143.2-keV level in {+188}W. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J$primary |g from 1/2+ in average neutron resonance capture; log| {Ift}=7.52 and 7.70 for |b decay to 139-keV (J|p=5/2+) and 740-keV (J|p=5/2-) levels in {+193}Ir, respectively. 
T From 2012Kr05. Other values: 30.11 h {I1} (1992An13), 30.0 h {I3} (1969Co08), 31.5 h {I5} (1958Na15), 30.6 h {I4} (1950Ch11), 31.9 h {I10} (1947Go01), and 2010ZaZX report 30.05 h {I14}, 29.952 h {I17}, 29.953 h {I8} averaging 75 data points (25 {I5}-mg enriched {+192}Os target for 3 |g rays) using averaging methods of Limitation of Relative Statistical Weight, the Rajeval Technique, and the Normalized Residuals, respectively. Evaluator recommends 2012Kr05 value over the other precise measurement of 1992An13 due to possible influence of higher {+193}Os irradiation-end activity, as noted in 2012Kr05 and comparing values in 2010ZaZX. Evaluator's note: Irradiation end {+193}Os activity was six times higher in 1992An13 compared to 150 kBq of 2012Kr05. Note 1969Co08 value is statistically in agreement with the recomended value, which was measured using enriched (98.7%) target and 280- and 460-keV K lines. 
MOMM1$NMR-ON (1989Ed01), sign from |g-ray circular polarization from oriented nuclei decay (1991Sc28). Other: +0.75 {I3} (2014StZZ) recalculated value, from low temperature I(|q) and Mossbauer effect (1985Be03); 0.78 {I7} (2014StZZ) recalculated value, from static low-temperature nuclear orientation (1984Gh01). 
MOME2$2014StZZ evaluation of 1979Er09 low temperature dependence of |g-anisotropy data reanalyzed by 1985Be03. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$primary |g from 1/2+ in (n,|g); absence of (d,p) strength and position of level, relative to that for 3/2[512] orbital, consistent with 1/2[510] Nilsson assignment. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
$Configuration=9/2-[505] 
J$from configuration assignment in 2014Ga14. 
T$Weighted average of 110 ns {I28} (2014Ga14 - ({+7}Li,{+6}Li|g)) and 132 ns {I29} (2011St21 - ({+208}Pb,X|g)). Uncertainty - lower input value. 


level_energy_unit: KEV
level_comment:
J$1/2-,3/2- can be assigned to at least one member of the 888.6-889.5 doublet on the basis of population in average resonance capture. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
J$L=1 in {+192}Os(d,p); assignment uncertain (level should be, but is not, populated in average resonance capture). 


level_energy_unit: KEV
level_comment:
E$Level established based on 3334.7 primary and 1540.0|g coincidence by 2002Ba66. The other closeby level established based on |g|g coin of almost comparable energy of 3334.80 primary with five other secondary transitions. Considering the possibility of random coincidences - not adopted by evaluator. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E$From least squares fit to primary |g's. S(n)=5583.42 {I20} (AME 2017Wa10) 
J$s-wave capture by even-even nucleus. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E$approximate energy of 2-keV resonance capture states (E(level)=S(n) + 2 keV). 
J$s-wave capture dominant; target J|p=0+. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_comment:
E$315.9 keV in Adopted Levels 
$Experimental isomeric state population ratio |>7% {I4} 
T$ from decay curve of 242-keV transition (2011St21) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
$Configuration=9/2-[505] 
$Configuration: from a comparison of the hindrance factor per degree of K forbiddenness in the neighboring {+187}W and {+191}Os nuclei, configurations of 9/2-[505] and 9/2+[624] are suggested. Systematics of these configurations in lighter odd-A Os isotopes suggest the 9/2-[505] configuration is most likely. 
T$from |g(t) of 242.7|g (2014Ga14) 
J$from configuration assignment in 2014Ga14. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
J$L(t,p)=0 from 0+ 
T$from 1965Jo10 (decay curve of {+194}Os and {+194}Ir equilibrium mixture using an end-window proportional counter, followed for six years). Others: 5.8 y {I4} (1964Wi07, preliminary value, measured over only 10 months), 700 d (1951Li19) 
$Quadrupole deformation parameter <|b{+2}{-2}>{+1/2}=0.147 {I10} from isotope-shift measurement in 2020Ch33. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
J$L(t,p)=(2) from 0+ 
T$from (218|g in LaBr{-3})(150-382 |g region in LaBr{-3})(531|g in HPGe)(t) (2017Da06) in {+192}Os({+18}O,{+16}O|g). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$L(t,p)=(4) from 0+ 
T$(218|g in HPGe)(382|g in LaBr{-3})(150-1000 |g region in LaBr{-3})(t) gives FWHM=888 ps for the prompt response fit for the time-difference spectra (Fig. 7d 2017Da06) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_comment:
$A high-spin isomer at high excitation is implied from out-of-beam |g-ray data in {+186}W,{+187}Re,{+192}Os({+136}Xe,X|g),E=6 MeV/nucleon reaction studied by 2014DrZZ. The details of this work are not yet available 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (10+)
level_uncertain: ?
level_comment:
$This level is treated as questionable by the evaluators due to the reassignment of 749|g by 2017Da06 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from (218|g in LaBr{-3})(150-382 |g region in LaBr{-3})(531|g in HPGe)(t) (2017Da06). Other: 385 ps {I26} (Fig. 7c in 2017Da06) from (218|g in LaBr{-3})(250-1300 |g region in LaBr{-3})(382|g in HPGe)(t). The first value is adopted by 2017Da06 
$Deduced effective |b{-2}=0.140 {I10} (2017Da06) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
T$(218|g in HPGe)(382|g in LaBr{-3})(150-1000 |g region in LaBr{-3})(t) gives FWHM=888 ps for the prompt response fit for the time-difference spectra (2017Da06) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E,J$from Fig. 2 of 2017Da06; not listed in authors' Table I. This level is not discussed in authors' text. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MIN
level_comment:
T$from 2013Bi14, which believe 1957Re01 indeed observed the decay of {+195}Os, and refitted the data as presented in Fig.2 of 1957Re01. The fit contained 3 components: the decay of {+195}Os, the growth and decay of {+195}Ir(T{-1/2}=2.29 h {I17} of 2013Bi14), and the decay of {+193}Os (T{-1/2}=29.830 h {I18} of 2012Kr05). 
J$from systematics in neighbour nuclide 


level_energy_unit: KEV
level_lifetime_unit: MIN
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
E$ from measured mass difference between the isomer and g.s. (2012Re19) 
T$ measured in 2012Re19 for bare {+195}Os ions. 
$ Isomeric transition was observed, implying |g-ray emission 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_uncertain: ?
level_comment:
T$The value given for the half-life of this isomer is for ions of {+195}Os at rest, measured at the final focus of the FRS. The half-life was determined by fitting the time dependence of the |g-ray intensity with a convolution of Gaussian and exponential functions. 


level_energy_unit: KEV
level_lifetime_unit: MIN
level_lifetime_info: ;ERR=GT
level_comment:
E$ from measured mass difference between the isomer and g.s. (2012Re19) 
T$ measured in 2012Re19 for bare {+195}Os ions, one ion was lost from the ring. Assuming the ion loss was due to atomic electron capture, the measured T{-1/2}=32 min {I+154-16}; and |b decay, the measured T{-1/2}=16 min {I+29-7}. 
$ Number of ions detected=73 
$ Isomeric transition was observed, implying |g-ray emission 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: S
level_comment:
T$from fit to summed decay curve involving 6 |g-ray transitions (2020Wa12) 
E$from the Adopted Levels of {+195}Os in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$measured by 2018Hi07 from growth and decay curve of |b radiation from the decay of {+196}Os. This value agrees with 34.9 min {I2} in {+196}Os Adopted Levels in the ENSDF database (Feb 2017 update), taken from 1977Ha32: Phys. Rev. C16, 1559. 


level_energy_unit: KEV
level_lifetime_unit: MIN
level_comment:
$ Only |b{+-} decay mode is possible and has possibly been observed by 2003Xu08. 
$ The fragments assigned by 2008St04 are assumed to correspond to the ground state of {+197}Os. 
T$ from timing of |g rays (2003Xu08). In the opinion of the evaluator this half-life should be considered as tentative since the activity formed in Pt(n,2p) reaction and assigned to {+197}Os was not separated by mass or chemistry. Calculated value: >100 s (1997Mo25). 
J$ 1/2- neutron orbital predicted by 1997Mo25 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$ from (particle)|g(t) (2008StZY). 
$ Four |g rays with almost equal intensities were reported by 2008StZY at 204, 416, 487 and 629 keV, but the level scheme was not established 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (25/2-,27/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$ from decay curve of delayed |g rays (2011St21) 
$Experimental isomeric state population ratio=4% {I2} 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$measured by 2018Hi07 from decay curve for |b{+-} radiation. Measured half-lives from decay curve 478.7- and 495.1-keV |g rays was 101 s {I18} (2018Hi07). Table I in 2018Hi07 lists measured half-lives from decay curves for |g rays in {+197}Ir emitted by the decay of {+197}Os: 166 s {I61} for 51.4|g, 112 s {I52} for 58.9|g, 131 s {I31} for 222.3|g, 121 s {I54} for 333.2|g, 58 s {I37} for 365.6|g, 68 s {I44} for 441.5|g, 167 s {I2098} for 449.3|g, 116 s {I23} for 478.7|g, 109 s {I26} for 495.1|g, 27 s {I21} for 599.7|g, 68 s {I44} for 879.8|g, and 70 s {I59} for 896.1|g; with a weighted average of these values as 87 s {I12}. Note that value of 2.8 min {I6} (or 168 s {I36} in {+197}Os Adopted Levels in the ENSDF database (May 2009 update) is in disagreement with value from 2018Hi07. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Only |b{+-} decay mode is possible. 
T$There is no measurement of half-life of g.s. It is expected to several seconds as suggested by the calculated value of >100 s (1997Mo25). In the neighboring Os isotopes the half-lives are: 39 min for {+196}Os, |?5-6 s for {+199}Os and {+200}Os. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$measured for the first time by 2018Hi07 from decay curve for |b{+-} radiation. Half-lives measured from decay curves for Ir x-rays and |g rays from the decay of {+198}Os and {+198}Ir were: 66 s {I68} for 64.9-keV x rays, 336 s {I163} for 73.6-keV x rays, 108 s {I36} for 230.6|g in {+198}Ir, 106 s {I60} for 407.22|g in {+198}Pt, and 72 s {I42} for 507.3|g in {+198}Pt. Weighted average of values from x rays and |g rays is 97 s {I23}. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$3/2- from predictions in 1997Mo25 
T$From implant-|b time differences (2007KuZW). T{-1/2}=15.2 s {I32} in 2005KuZU. Other: >100 s value predicted in 1997Mo25 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$3/2- is predicted by 1997Mo25 
T$the half-life was deduced from position-time correlations between the implanted fragments and the subsequent |b decay (2007KuZW). Other: T{-1/2}>100 s is predicted by 1997Mo25 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$ from decay curve of 379-, 402-, 425-, 737-, and 971-keV transitions (2011St21) 
$Experimental isomeric state population ratio |>1.4% {I7} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$From implant-|b{+-}(|Dt) in 2014Ku23,2014Mo15,2009Ku28. Other: 4.6 s {I13} in 2005KuZU (early result from the same group) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$assuming spherical shape and systematics of N=125 isotones in the region; shell model predictions 
T$ >160 ns from from the time-of-flight in 2012Ku26. |? 3 s estimated in 2021Ko07. Predicted T{-1/2}(|b): 56 s (2019Mo01, FRDM16), 2.1 s (2016Ma12, CDFT) and 87 s (2020Ne08, QRPA with Skyrme EDF) 
CONF$|n p{-1/2}{+-1} from systematics of N=125 isotones in the region; shell model predictions 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
T$ >160 ns from from time-of-flight in 2009St16, 2012Ku26. |?2 s estimated in 2021Ko07. Predicted T{-1/2}(|b): 51 s (2019Mo01, FRDM16), 1.1 s (2016Ma12, CDFT) and 39 s (2020Ne08, QRPA with Skyrme EDF) 
$ Production |s[{+9}Be({+238}U,x)]=0.0044 nb {I20} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$ Assuming spherical shape and systematics of N=127 isotones in the region; shell-model predictions. 
T$ >300 ns from time-of-flight in 2012Ku26, but the actual half-life is expected to be much longer. T{-1/2} |J 300 ms estimated in 2021Ko07. Predicted T{-1/2}(|b{+-}): 6.62 s (2019Mo01, FRDM16), 0.506 s (2016Ma12, CDFT) and 11.1 s (2020Ne08, QRPA with Skyrme EDF) 
CONF$|n(g{-9/2}{++1}) from systematics of N=127 isotones in the region; shell model predictions 
$ Production |s=0.0025 nb {I18} (2012Ku26) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$Ground state of {+164}Ir is not yet identified. From systematics, 2017Au03 give half-life=1 ms and J|p=2-. Theoretical half-life=0.14 s (1997Mo25) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Alpha decay is reported by 2014Dr02 and proton decay by 2001Ke05, 2002Ma61 and 2014Dr02 
E,J$ the observed proton activity is assigned to a possible high-spin isomer in {+164}Ir (2002Ma61) in comparison with similar assignment for {+166}Ir. Possible configuration=|ph{-11/2}~#|nf{-7/2}, the proton emitting orbital is most likely |ph{-11/2}. From systematics x=260 {I100} (syst, 2017Au03) 
T$measured by 2014Dr02 from proton decay curve using method of maximum likelihood. Others: 69 ms {I+41-29} from |a-decay events (2014Dr02), 58 |ms {I+46-18} (2002Ma61) and 113 |ms {I+62-30} (2001Ke05) 
$E(p)=1814 {I6} (2014Dr02), 1807 {I14} (2002Ma61) and 1817 {I9} (2001Ke05) from decay of {+164}Ir. 
$E|a=6880 {I10} from decay of {+164}Ir, observed by 2014Dr02. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
E,J$the ground state of {+165}Ir has not yet been identified; from systematics, s{-1/2} orbital is expected to lie below h{-11/2} orbital (2021Ko07) 
T$<1 |ms from calculations for Q(p)=1503 and J|p=1/2+, in agreement with lower value from time-of-flight measurement in FMA (1997Da07); 50 ns from systematics (2021Ko07) 
$No evidence was found by 2014Dr02 for the ground state decay of {+165}Ir 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$%p and %|a in 2014Dr02 were based on observed {+165}Ir |a-decay yield with 35 events, and proton-decay yield with 270 events. Values of %p=87 {I4}, %|a=13 {I4} measured by 1997Da07 are nearly the same, but somewhat less precise. 
$Deduced reduced proton width=0.30 {I5} (2014Dr02) 
E$x=230 {I110} (1997Da07) from systematics of energy differences between the s{-1/2} and h{-11/2} orbitals in {+153}Lu, {+157}Ta and {+161}Re. Other: 180 {I50} proposed from systematics (2021Ko07) 
T$weighted average of 340 |ms {I40} (2014Dr02, maximum likelihood method applied for decay events), 0.39 ms {I16} (1997Da07, |a decay curve) and 0.29 ms {I6} (1997Da07, protons decay curve) 
J$E(p)=1707 {I7} (1997Da07), Q(p)=1733 {I7}, %p=87 {I4}, J|p=11/2- give calculated T{-1/2}(p)=0.34 ms {I7}, in agreement with the experimental value 
$Configuration=|ph{-11/2} 
$E(|a)=6715 {I7} (1997Da07) from the decay of {+165}Ir isomer 
$Production |s|?0.2 |mb (1997Da07) in {+92}Mo({+78}Kr,p4n),E=384 MeV. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
%A From 1997Da07. 99% calculated by 1981HoZM. Only |a decay was investigated by 1981Ho10. 
J d{-3/2} proton emission observed from level (1997Da07). Probable configuration=(|p d{-3/2})~#(|n f{-7/2}); the Nordheim strong rule predicts that the lowest energy state for this configuration will have J|p=2- (1997Da07) (possibly (|p 3/2[402]-|n 7/2[514]) at small prolate deformation). 
T 10.5 ms {I22} from 1997Da07 (6565|a(t)). Others: 17 ms {I+12-5} (2004Ke06), 12 ms {I1} (1996Pa01, 6556|a(t)), >5 ms (1981Ho10). 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: MS
level_comment:
E from 1997Da07, based on measured E(p)=1316 {I8} and 1145 {I8}, respectively, to {+165}Os g.s. from this level and from {+166}Ir g.s. (uncertainty takes into account the cancellation of systematic uncertainty included in quoted E(p)). 
T from 6561|a(t) (1997Da07). Other: 14.3 ms {I+19-15} (2004Ke06) from 6545|a(t). 
J h{-11/2} proton emission observed from level (1997Da07). Probable configuration=(|p h{-11/2})~#(|n f{-7/2}); the Nordheim weak rule favors J|p=9+ or possibly 2+ (which should not Be isomeric) for the lowest energy state for this configuration (1997Da07) (possibly |p 11/2[505]+|n 7/2[514] at small prolate deformation). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
$%|a=43.5 {I20} from weighted average of %|a=43 {I2} (2005Sc22) and 48 {I6} (1997Da07). 
$%p=39.0 {I15} from weighted average of %p=39.3 {I13} (2005Sc22) and 32 {I6} (1997Da07). 
$%|e+%|b{++}=17.5 {I25} from 100-(summed %|a and %p) 
J$from considerations of s{-1/2} proton-decay mode of {+167}Ir, and comparison of experimental half-life with theoretical half-lives calculated for s{-1/2}, d{-3/2} and h{-11/2} proton emission for {+167}Ir (odd-Z, even-N nucleus) using Wentzel-Kramers-Brillouin (WKB) barrier penetration approximation (1997Da07, 2001Da31, 2005Sc22) 
T$weighted average of 30.9 ms {I13} (2005Sc22, |a decay); 29.3 ms {I6} (2005Sc22, proton decay); 39.7 ms {I49} (1997Da07, |a decay); and 34.3 ms {I22} (1997Da07, proton decay). Reduced |h{+2} of 4.1 is somewhat higher than critical |h{+2}=2.6. Unweighted average is 32.4 ms {I14}. Other: >5 ms (1981Ho10). 
$E(p)=1062 {I6} (2005Sc22), 1064 keV {I6} (1997Da07) from the decay {+167}Ir g.s. Weighted average E(p)=1063 {I6} 
$E|a=6348 {I3} (2005Sc22), 6351 {I4} (2001Da31, earlier value of 6351 {I5} in 1997Da07) from the decay {+167}Ir g.s. Weighted average E|a=6349 {I3} 
$Production |s|?10 |mb (1997Da07) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$%|a=90 {I3} from weighted average of %|a=90 {I3} (2005Sc22) and 80 {I10} (1997Da07). 
$%p=0.42 {I8} from weighted average of %p=0.42 {I8} (2005Sc22) and 0.4 {I1} (1997Da07). 
$%|e+%|b{++}=9.6 {I30} from 100-(summed %|a and %p) 
E$from energy differences of proton peaks from the two activities of {+167}Ir (2001Da31). 
J$from considerations of h{-11/2} proton-decay mode of {+167}Ir, and comparison of experimental half-life with theoretical half-lives calculated for s{-1/2}, d{-3/2} and h{-11/2} proton emission for {+167}Ir (odd-Z, even-N nucleus) using Wentzel-Kramers-Brillouin (WKB) barrier penetration approximation (1997Da07, 2001Da31, 2005Sc22) 
T$weighted average of the following values: 28.8 ms {I13} (2005Sc22, proton decay); 28.7 ms {I33} (2005Sc22, |a decay); 25.7 ms {I8} (2004Ke06, |a decay); 30.0 {I6} ms (1997Da07, |a decay); 34 ms {I9} (1997Da07, proton decay); and 34 ms {I4} (1996Pa01, |a decay). Reduced |h{+2} of 4.2 is somewhat higher than critical |h{+2}=2.2. Unweighted average is 30.2 ms {I13} 
$E(p)=1248 {I7} (2005Sc22), 1238 keV {I7} (1997Da07) from the decay of {+167}Ir isomer. Weighted average E(p)=1243 {I7} 
$E(|a)=6404 {I6} (2005Sc22), 6394 {I2} (2004Ke06), 6410 {I5} (1997Da07), 6410 {I11} (1996Pa01), 6386 {I10} (1981Ho10) from the decay of {+167}Ir isomer. Weighted average E|a=6397 {I3} 
$Production |s|?100 |mb (1997Da07) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%|a: only |a decay has been observed, but |e+|b{++} and p decay are possible. Gross |b decay theory (1973Ta30) predicts T{-1/2}(|e+|b{++})|?1 s implying %|e+%|b{++}|?22% and 1997Mo25 predict T{-1/2}(|e+|b{++})=359 ms implying %|e+%|b{++}=62%, so |e+|b{++} branching is expected to Be appreciable. 
T from 6230|a(t) (2009Ha42). Other T{-1/2}: 125 ms {I40} from 6227|a(t) (1996Pa01); not unambiguously differentiated from A=169, but E|a favors A=168 assignment although it is unclear whether it corresponds to g.s. or isomeric state decay. 
J HF|<4 for |a decay from low-spin {+172}Au if %|a({+172}Au)=100, so low J is expected for this level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
%|a: weighted average of 82 {I14} (1996Pa01) and 75 {I11} (2009Ha42); only |a decay has been observed, but a significant |e+|b{++} branch is expected and p decay is probably possible also. 
T weighted average of 161 ms {I21} from 6323|a(t) (1996Pa01), 160 ms {I+30-20} from 6320|a(t) and 153 ms {I+40-30} from 6260|a(t) (2009Ha42). See also the comment on T{-1/2}(g.s.). 
J high-spin state; fed strongly in |a decay from high-spin {+172}Au. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E from difference between E|a feeding this level and that feeding the 0.0+x level in {+172}Au |a decay (7.7 ms) (2009Ha42). 
J probably a high-spin state; fed in |a decay from high-J {+172}Au. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E from energy difference between |a feeding this level and that feeding the 0+x level (2009Ha42). Consistent with E=65.0 {I4} and 73.0 {I6} for photons observed to be correlated with 6800|a from {+172}Au, but those energies (and their relative I|g) are also close to expectation for K|a| x ray and K|b| x ray for Ir so they probably result, instead, from a highly-converted transition at somewhat higher energy. If so, the presence of K| x ray implies E|g>76 keV, the K shell binding energy for Ir. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
%|a: weighted average of 42 {I15} (2005Sc22) and 50 {I18} (1999Po09) 
%p: see 1983Al09 and 1984Gr14 for discussions of expected proton decay; S(p) (=-621 {I24} (2003Au03)) consistent with predictions. 
J unhindered |a decay from (1/2+) {+173}Au. 
T from 5993|a(t) (2005Sc22). Other: 0.64 s {I+46-24} (1999Po09). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%A Unweighted average of 59 {I4} (2005Sc22), 84 {I8} (1999Po09) and 72 {I13} (1996Pa01). Other: 83 {I+17-42} (1984ScZQ). 
E from {+173}Au |a decay (14.0 ms). 
J unhindered |a decay from (11/2-) {+173}Au. 
T weighted average of 0.308 s {I22} from 6119|a(t) (1996Pa01) and 0.280 s {I3} from 6117|a(t) (2005Sc22). Others: 0.32 s {I+9-7} (1999Po09), 0.4 s {I1} (1978Ca11), 0.4 s {I2} (1978Sc26). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J,T from Adopted Levels. 
E based on E|a=6732 {I4} from 214 {I23} parent level and Q(|a)=6836 {I5}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J from Adopted Levels. |DE=24 keV for this level. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: MS
level_comment:
J$from Adopted Levels of {+169}Ir in ENSDF database 
T$from a least-squares fit to |a-decay time distribution in 2012Th13 
$E|a=6019 keV {I14} from the decay of {+169}Ir g.s. correlated with 6688|a from {+173}Au g.s. decay 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_comment:
E,J$from Adopted Levels of {+169}Ir in ENSDF database 
T$from a least-squares fit to |a-decay time distribution in 2012Th13 
$E|a=6120 keV {I14} from the decay of {+169}Ir isomer correlated with 6739|a from {+173}Au isomer decay 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: S
level_comment:
%A From measurement of 5815|a (2002Ro17). 
T from 5815|a(t) (2002Ro17). See also comment on T{-1/2} for 0+x level. 
E the identification of this level as the {+170}Ir g.s. (2002Ro17) is based on the consistency of E|a=5815 from this level with E|a systematics for neighboring Ir isotopes ({+167}Ir to {+174}Ir). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
%A Weighted average of 36 {I10} (1996Pa01) and 39 {I6} (2004GoZZ). Note, however, that E|a reported by 1996Pa01 and 2004GoZZ for decay from this level differ from values from 2007Ha45. 1978Sc26 suggested %|a|?100 based only on |a-decay systematics. 
T authors' recommended value from 2007Ha45, based on the following |a(t) data: 802 ms {I+30-28} (6007|a), 826 ms {I+30-28} (6053|a), 830 ms {I+58-53} (5951|a), 801 ms {I+63-57} (6121|a). Others: 0.43 s {I5} (2002Ro17, 6082|a), 0.83 s {I30} (1996Pa01, 6083|a), 1.05 s {I15} (1978Sc26, 6030|a), 1.1 s {I2} (1977Ca23 and 1978Ca11, 6010|a), 0.8 s {I2} (1977ScYH, 6045|a); it is unclear whether these all belong to the {+170}Ir high-spin isomer. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9+)
level_comment:
J suggested by 2004GoZZ; this state is populated in |a decay from (9+) {+174}Au by the strongest, least hindered branch and that branch is possibly unhindered. Consistent with (M1) 153|g to tentative (8+) 0+x level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9-)
level_comment:
J based on plot of aligned angular momentum for band containing this level compared with that for 11/2[505] band in {+171}Ir and on the apparent blocking of the (|n i{-13/2}{+2}) band crossing seen in {+171}Ir, 2007Ha45 suggest a configuration with a deformation-aligned (|p 11/2[505]) coupled to a rotationally-aligned (|n 1/2[660]). J=9 is the closest integer to their predicted spin for such a coupling. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T authors' recommended value based on the following |a(t) data: 802 ms {I+30-28} (6007|a), 826 ms {I+30-28} (6053|a), 830 ms {I+58-53} (5951|a), 801 ms {I+63-57} (6121|a). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9-)
level_comment:
J based on plot of aligned angular momentum for band containing this level compared with that for 11/2[505] band in {+171}Ir and the apparent blocking of the i{-13/2}{+2} band crossing seen for the {+171}Ir 11/2[505] band, 2007Ha45 suggest a configuration with a deformation-aligned (|p 11/2[505]) coupled to a rotationally-aligned (|n 1/2[660]). J=9 is the closest integer to their predicted spin for such a coupling. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J from Adopted Levels. 
E the possibility that this is not the {+170}Ir g.s. but, instead, a low-spin excited state, cannot be entirely ruled out. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_uncertain: ?
level_comment:
E from difference in E|a to g.s. and possible E|a to this level. Level not adopted because 2004GoZZ identify their 6548|a as a sum peak. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
%A$from 2013An10, from comparison of |a decays of {+175}Au(g.s.) and {+171}Ir(g.s.). |a decay was also observed by 2002Ro17. 
T$from 6412|a({+175}Au)-5717|a({+171}Ir) correlation data (2002Ro17). 
J$by analogy with {+167}Ir and {+169}Ir. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$%|a: weighted average of 58 {I11} (1996Pa01) and 53 {I5} (2010An01). Other %|a: |?100 (1978Sc26). 
$%|e+%|b{++}: 1992Sc16 searched for evidence for |e decay, but observed no gammas in coincidence with Os K| x ray. 
J$by analogy with nearby odd-A Ir nuclides. 
E$energy of analogous state is 153 {I24} in {+169}Ir (1999Po09) and 175.3 {I22} in {+167}Ir (1997Da07). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (23/2)
level_comment:
E$y>1116; level decays to 1353 (19/2-) and 1116 (17/2-) levels via unidentified linking transitions. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (23/2)
level_comment:
E$level decays to 1353+x (19/2-) and 1116+x (17/2-) levels via unidentified linking transitions; so y>1353 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3-,4-)
level_lifetime_unit: S
level_comment:
$Other %|a<2 (2004GoZZ), also a low value is consistent with the measurements in 2014An10, but a precise branching ratio could not be extracted by 2014An10 due to detection sensitivity limit 
J$from 2014An10 based on favored |a decay from (3-,4-) parent state of {+176}Au. Possible configuration=|p1/2+,(s{-1/2} orbital)~# |n7/2-,(f{-7/2} or h{-9/2} orbital). From |a and |b-decay studies of {+172}Ir decay, (3+) proposed by 1992Sc16 and (2,3) by 1992Bo21 
T$from |a decay (1992Sc16) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (7+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$138 keV {I3} (based on data in 1992Sc16) and 139 keV {I10} listed in 2012Au07 are no longer supported by the measurements in 2014An10 who propose two activities in {+168}Re, a low-spin and a high-spin. Some of the |g rays reported by 1992Sc16 and which implied the energy of this level were not confirmed by 2004GoZZ 
$%|a measured by 2014An10 by two methods: |a|g-coin and |a|a-correlations, first giving a value of 10% {I2} and the other 9% {I1}. Other measured values of %|a: 23 {I3} (1992Sc16), 22 {I6} (2004GoZZ), <32 (1984ScZQ) 
J$from 2014An10 with possible configuration= |p11/2-,(h{-11/2} orbital)~#|n3/2-,(f{-7/2} or h{-9/2} orbital). From |b and |a-decay studies of {+172}Ir, (7+) proposed by 1992Sc16 and (5+,6+) by 1992Bo21 
T$from |a decay, weighted average of 2.26 s {I5} (2004GoZZ), 2.0 s {I1} (1992Sc16) and 2.1 s {I1} (1978Sc26). Others: 1.7 s {I5} (1967Si02), 2.1 s {I5} (1984ScZQ). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (8+,9+)
level_comment:
J$2014An10 assign (8+,9+) based on favored |a decay from (8+,9+) parent state. But (9+) is not likely if 175.2|g to (7+) is (M1) 
$Possible configuration=|p11/2-,(h{-11/2} orbital)~#|n7/2-,(f{-7/2} or h{-9/2} orbital) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (8+,9+)
level_comment:
J$2014An10 assign (8+,9+) based on favored |a decay from (8+,9+) parent state. But (9+) is not likely if 211.6|g to (7+) is (M1) 
$Possible configuration=|p11/2-,(h{-11/2} orbital)~#|n7/2-,(f{-7/2} or h{-9/2} orbital) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3-,4-)
level_comment:
J$from 2014An10 based on favored |a decay from (3-,4-) parent state of {+176}Au 
$Possible configuration=|p1/2+,(s{-1/2} orbital)~#|n7/2-,(f{-7/2} or h{-9/2} orbital) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (7+)
level_comment:
J$from 2014An10 with possible configuration= |p11/2-,(h{-11/2} orbital)~#|n3/2-,(f{-7/2} or h{-9/2} orbital) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
%|a: from I|a(5416|a) relative to I|g(49.6|g) in {+173}Ir |e decay (9.0 s) (1992Sc16). 
J$3/2+ 3/2[402] or 5/2+ 5/2[402] orbital assigned, consistent with systematics and daughter J|p in both {+169}Re and {+173}Os. (HI,xn|g) data consistent with placement several hundred keV below 9/2- 1/2[541] state. 
T$average of 8.1 s {I3} (1992Bo21) and 9.8 s {I14} (1992Sc16). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
%|a: from I|a(5674|a) relative to I|g(49.6|g) in {+173}Ir |e decay (2.20 s) (1992Sc16). Other value: %|a=2.02 {I8} (1986Ke03). 
J$configuration=11/2-[505] from systematics and favored |a decay to 11/2- level in {+169}Re. 
T$from 1992Sc16. Other value: 3.0 s {I10} (1967Si02). 
E,J$ from 2009An14 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E$from |a decay energies measured by 2021Ha32, ground state {+177}Au mass and {+177m}Au isomer excitation energy (2021Ha32) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: S
level_comment:
J$favored |a decay to 224.7-keV level (J|p=(3+)) in {+170}Re. |e decay to J|p=2+,4+ levels in {+174}Os (1992Sc16). 
T$weighted average of 9 s {I2} (1992Sc16) and 7.8 s {I6} (1992Bo21). 
%A From 1992Sc16 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$favored |a decay to 210.3-keV level (J|p=(7+)) in {+170}Re. |e decay to J|p=6+,8+ levels in {+174}Os (1992Sc16). 
T$weighted average of 4.9 s {I3} (1992Sc16) and 5.0 s {I4} (1992Bo21). 
%A From 1992Sc16 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
%A From 1986Ke03. Other value: %|a|<5 (1992Sc16). 
J$Assignments are based on the systematic properties of odd-proton nuclei in this mass region, on measured angular anisotropies for the strongest |g-rays and on total-Routhian-surface (TRS) calculations (1991Ce02). 
T$weighted average of 7.2 s {I13}, |a counting (1992Sc16); 11 s {I3}, |g-ray counting (1992Sc16); and 13 s {I2}, |g-ray counting (1992Bo21). Other value: 4.5 s {I10} (1967Si02). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_comment:
J$From systematics of neighboring odd Ir nuclei and population intensity arguments and BCS calculation (1991Dr06). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$ measured in 2010Wa02. From timing of 105.6|g from the decay of {+175}Ir, T{-1/2} was obtained as 13.7 s {I8}, but after fitting the decay curve with a double exponential, half-life of 8.8 s was obtained for the shorter-lived component. This activity is known from earlier studies with a half-life of 9 s {I2} (Adopted dataset for {+175}Ir in ENSDF database) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: S
level_comment:
T$ measured in 2010Wa02. From timing of 399.0|g from the decay of {+175}Ir. New activity proposed in 2010Wa02. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$weighted average of 9.2 s {I7} (2005Wa25), 8 s {I1} (1967Si02), 8 s {I1} and 9 s {I1} (1990Bo19). In 2005Wa25, T{-1/2}=17.6 s {I17} (607.2|g-t), 10.9 s {I4} (135.0|g-t), 10.1 s {I3} (260.3|g-t), 9.6 s {I6} (346.9|g-t), 9.9 s {I11} (1361.5|g-t), and 9.8 s {I8} (1360|g-t) probably indicate the presence of a long lived isomer in {+176}Ir with two component |b-feeding to some levels in {+176}Os. 
%|a from 1990Bo19. Uncertainty has a 3 |s confidence level. Other value: %|a=2.1 {I4} (1986Ke03). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
J 97.3|g E1 to (7+) state. 
T From centroid shift technique ({+31}P,4n|g) (2003Ba07). Time difference spectrum constructed with gates on transitions of band 1, detected in the Ge detectors as "start", and 97 keV |g ray detected in the LEPS detectors as "stop". In ({+31}P,4n|g) the half life is attributed to the head of band 1, however it is possible that the bandhead actually decays by unobserved transitions to another level that emits 97|g according to authors. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
J 97.3|g E1 to (7+) state. 
T From centroid shift technique (2003Ba07). Time difference spectrum constructed with gates on transitions of band 1, detected in the Ge detectors as "start", and 97 keV |g ray detected in the LEPS detectors as "stop". In 2003Ba07 the half life is attributed to the head of band 1, however it is possible that the bandhead actually decays by unobserved transitions to another level that emits 97|g according to authors. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
%A$From the comparison of |a- and |g-ray intensities in singles spectra in 1990Bo19. Other: 0.13 {I7} (1986Ke03). 
%EC+%B+$Not measured directly, but estimated from %|a. 
T$Weighted average of 31 s {I2} ({+177}Ir |a-decay) and 27 s {I3} ({+177}Ir |e+|b{++} decay) in 1990Bo19. Other: 21 s 2 (1967Si02). 
J$Favored |a-decay to the {+173}Re g.s. (J|p=5/2-); J|p systematics; band assignment. 
CONF$|p 1/2[541] Nilsson configuration. The band is strongly Coriolis mixed. The assignment is supported by the observed in-band properties, such as large signature splitting and rotational alignment. It is consistent with systematics of similar structures known in neighboring odd-Z nuclei. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$Band assignment; J|p systematics 
T$A lower limit based on the non-observation of a direct decay from this state to the J|p=5/2- ground state and/or the J|p=9/2- band member and the applied coincidence window. The value depends on the excitation energy of this state and the decay pattern. 
CONF$|p 9/2[514] Nilsson configuration. The assignment is supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values. It is consistent with systematics of similar structures known in neighboring odd-Z nuclei. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
E$Other: 46 keV {I7} from |a-decay energy differences in {+181}Au |a decay. 
J$J|p systematics; band assignment. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$71.8|g to (1/2-), 157.2|g to 5/2-; J|p systematics. 
CONF$|p 3/2[402] Nilsson configuration (1993Me13). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT;ISO=M2
level_comment:
J$100.8|g M1(+E2) from 7/2+; band assignment; J|p systematics 
T$Lower limit based on the non-observation of a direct decay from this state via the 180.6|g to the J|p=5/2- ground state and the applied coincidence window. Using B(E1)=2.8|*10{+-8} {I3} (W.u.) from equivalent decay to the J|p=5/2-, |p1/2-[541] ground state of {+181}Ir (1993Dr02), one may expect T{-1/2} |? 1.2 |ms 
CONF$|p 5/2[402] Nilsson configuration. The assignment is supported by the observed in-band properties, such as alignment and g{-K}-g{-R} values, and configuration systematics. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
E$From E|g=94.3 keV {I5} 
J$94.3|g from the 13/2+ level; band assignment. 
CONF$|p 1/2[660] Nilsson configuration. The assignment is supported by the observed in-band properties, such as the decoupled character of the band and rotational alignment, and configuration systematics. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From Adopted Levels. 46 keV {I7} from |a-decay energy differences 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$A lower limit based on the non-observation of a direct decay from this state to the J|p=5/2- ground state and/or the J|p=9/2- band member and the applied coincidence window. The value depends on the excitation energy of this state and the decay pattern. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT;ISO=M2
level_comment:
T$Lower limit based on the non-observation of a direct decay from this state via the 180.6|g to the J|p=5/2- ground state and the applied coincidence window. Using B(E1)=2.8|*10{+-8} {I3} (W.u.) from equivalent decay to the J|p=5/2-, |p1/2-[541] ground state of {+181}Ir (1993Dr02), one may expect T{-1/2} |? 1.2 |ms 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T from 1973HaVR. Other values: 30 s {i18} (1970AcZX,1972BaWW). 
%|e+%|b{++}=100 (adopted value in 2003Au02). 


level_energy_unit: KEV
level_comment:
E from |a-particle energy differences in {+182}Au decay (1995Bi01). 1993Me13 see a 127-keV |g in coincidence spectra gated by the 54.4 keV |g ray. Because of the energy uncertainty this |g-ray may deexcite the same level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: [5+,6+,7+]
level_comment:
J Suggested by evaluators based on (M1,E2) multipolarity of the 101-keV |g ray feeding this level, and the proposed J|p=(6+) of the originating level at 140.1+y (2003Ho03). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (11+)
level_comment:
Bandhead for band G 
E Level energies in this band are tentative, and based only on the suggested placement of the 187.5-keV transition connecting this bandhead to the (10-) level in band I (2003Ho03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
This level suggested in 1993Me13 on the basis of the observed coincidences of the 36.9 and 55.0 keV |g rays, and the agreement of the energy sum with the energy of the probable cross-over 91.7 keV |g ray. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
A similar level is suggested from |a decay studies in 1995Bi01, who quote an E(lev)=123 {i7} keV, deduced from their |a-ray energy differences. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J from the hindrance factor of the |a transition feeding this level, which indicates that it has the same J|p and structure as the {+182}Au g.s., for which a J|p=(2+) has been established (2001Ib02). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_comment:
E This level is proposed as the initial level for the 81.8 keV |g ray in 2003Ho03. This indicates an E(lev)=-42.7+y keV for the final level for that transition, below the 0.0+y keV band A bandhead, which is the lowest among all such states in the level scheme. If the energy for the final level of the 81.8-kev transition is taken as the reference energy for the level scheme all energies listed in the level table have to be shifted upwards by a common offset of 42.7 keV. Notice that neither the 0.0+x nor the 0.0+y states can be considered the actual ground state of the {+178}Ir nucleus. See also the |e and |a decay datasets. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (11+)
level_comment:
Bandhead for band G 
E The energy for the levels in this band is tentative, and based only on the suggested placement of the 187.5-keV transition connecting this bandhead to the (10-) level in band I (2003Ho03). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: S
level_comment:
J HF<4 from (5/2)- in {+183}Au |a decay; consistent with J|p(g.s.) for neighboring Ir isotopes. Note, however, that apparent |e+|b{++} feeding to (7/2-) and (9/2-) and (9/2+) states in {+179}Os suggests J=7/2 instead. 
T from |b-delayed |g rays (1992Bo19). Other: 4 min {I1} (1971Na27). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_comment:
E x=35 keV {I10} estimated by evaluator based on energy systematics; see comment on E(level) values in (HI,xn|g) data set. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2,3/2)+
level_comment:
J E1 172|g to (1/2)- 100. However, log| {Ift} in |e decay from 1/2- is far too low for the implied first-forbidden decay. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 45/2+
level_lifetime_unit: PS
level_comment:
T from DSAM (1994Mu18). Other: 0.18 ps {I+10-7} (1996Ji04). 
Q(transition)=8.2 {I+22-15} (1996Ji04). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 49/2+
level_lifetime_unit: PS
level_comment:
T from DSAM (1994Mu18). Other: 0.14 ps {I+5-4} (1996Ji04). 
Q(transition)=7.8 {I+14-11} (1996Ji04). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: MIN
level_comment:
J$direct feeding to 4+, 5, and 6+ states in {+180}Os. 
T$weighted average of 1.5 min {I1} (1972Ak03) and 1.5 min {I2} (1973LaZC). Others: 1971Na27, 1992Bo19. 
E$doubly-decoupled band observed in {+154}Sm({+31}P,5n|g) assigned to the ground state by evaluator 
$configuration=|p1/2[541]|n1/2[521]; doubly-decoupled band. 


level_energy_unit: KEV
level_comment:
$E|g=80.4 observed in {+184}Au |a-decay. E|g=80.6 from {+180}Pt |e-decay is probably the same transition. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E|g=113.5 observed in {+184}Au |a-decay. E|g=113.0 from {+180}Pt |e-decay is probably the same transition. 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (9-)
level_comment:
J$from comparison of the (9-) to (7-) transition energies in similar bands in neighboring Ir and Re nuclei 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5+)
level_comment:
E$this state may correspond to the ground state of {+180}Ir 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
T$from 1978La04. Other values: 5.0 min {I3} (1972Ak03), 10 min {I2} (1971Na27) 
J$populated by |a-decay from {+185}Au (J|p=5/2-) HF=0.7. Configuration=1/2[541] 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J$Directly populated by {+181}Pt (J|p=1/2-) |e-decay, log| {Ift}|?5.5; E2 to 5/2-. Possibly the 1/2- member of the 1/2[541] band (1992Sa03) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_comment:
J$populated by |a-decay from {+185}Au (J|p=5/2-); M1+E2 to 5/2-, |g to (1/2)- Possibly the 3/2- member of the 1/2[541] band (1992Sa03) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
T$from (HI,xn|g) (|g|g(t) spectrum (1993Dr02)). Other: 0.33 |ms {I+10-6} from 1992Ka01. 
J$Directly fed by {+181}Pt (J|p=1/2-) |e-decay, log| {Ift}|?7.4; E1 to 5/2- of 1/2[541] band. Configuration: 5/2[402] 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 10.3 ps {I8} from (HI,xn|g) 1995Wa18 and 9.7 ps {I21} from (HI,xn|g) 1990Ka11. 
J$E2 to 13/2- 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.15 ps {I21} from (HI,xn|g) 1995Wa18 and 2.4 ps {I8} from (HI,xn|g) 1990Ka11. 
J$E2 to 17/2- 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 8.2 ps {I6} from (HI,xn|g) 1995Wa18 and 6.9 ps {I14} from (HI,xn|g) 1990Ka11. 
J$E2 to 17/2+; |g to 19/2- and 21/2- states of 1/2[541] band 


level_energy_unit: KEV
level_spin_parity: 23/2+
level_lifetime_unit: NS
level_comment:
T$from 1992Ka01. Other: 29 ns from (HI,xn|g) 1993Dr02. 
J$|g to 21/2- of 9/2[514] band; |g to 21/2+ 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 146 ps {I12} from 1995Wa18 and 149 ps {I10} from recoil distance method (1990Ka11) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T$from |g|g-t coincidence (1992Ka01). Others: 134 ns from |g|g(t) spectrum (1993Dr02); 190 ns {I60} from 1990Kr06 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 10.3 ps {I8} from 1995Wa18 and 9.7 ps {I21} from recoil distance method (1990Ka11). 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.15 ps {I21} from 1995Wa18 and 2.4 ps {I8} from recoil distance method (1990Ka11). 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 8.2 ps {I6} from 1995Wa18 and 6.9 ps {I14} from recoil distance method (1990Ka11). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_comment:
$(<r{+2}>){+1/2}(rms charge radius)=5.37 fm {I11} (2013An02,evaluation) 
J,MOMM1,MOME2$from LASER spectroscopy COMPLIS experiment at ISOLDE facility at CERN (2006Ve10, also 2000Ve10,2000Sa58). Other: |m=2.28 {I8} (1992Bo39), on-line nuclear orientation. 
$2006Ve10 provide detailed comparison of experimental quadrupole moment with that from model calculations. The results agree with mixed K|p=0+ and 1+ prolate (|b{-2}=+0.20) configuration= |n1/2[521]~#|p1/2[541] 
E$it is assumed that the lowest state populated in the ({+14}N,4n|g) reaction is the ground state. In a recent study of {+182}Ir |e decay, the 15-min activity of {+182}Ir was produced by a similar heavy-ion reaction: {+168}Er({+19}F,5n) at 106 MeV. Thus it is likely that the g.s. is the bandhead of the decoupled band 
T$From weighted average of 15 min {I1} (1972Ak03), 15.0 min {I15} (1971Na27), 15 min {I1} (1961Di04). Others: 16.7 min {I19} (1972HuZL), 15.5 min {I25} (1971Na27) 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
J$E1 |gs to (5)+ and (4)+, |g to 3+. Possible configuration=K|p=4-, |p1/2[541]~#|n9/2[624] + |p1/2[541]~#|n7/2[633] 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$E1 |g from 1+; M1+E2 |g to (2)-; |g to (3)-. Possible configuration=K|p=2-, |p3/2[532]~#|n7/2[633] 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$M1 |g to (3)+, E1 |g to (3)-; M1(+E2) |g from 1+. Possible configuration=K|p=2+, |p1/2[541]~#|n5/2[512] 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 5+
level_comment:
E$x=25.6 keV based on data from {+182}Pt |e decay (1995Sa42,1999Sa40, 2007Ho20) and Adopted Levels 
J$from systematics of doubly decoupled bands (1990Kr06) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
%EC+%B+$%|a<0.1 from systematics of lighter Ir isotopes. 
|m: from static nuclear orientation with |g detection. Other: 1992Ro21. 
<r{+2}>{+1/2}(charge)=5.39 fm {I11} (2004An14). 
T unweighted average of 55 min {I7} (1961Di04) and 60 min {I6} (1961La05). 
J log| {Ift}=6.1 to 2274 level in {+183}Os which must have J|p|>7/2-, log| {Ift}=7.2 to 453 level in {+183}Os which must have J|p|<3/2-. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J log| {Ift}|<4.7 from 7/2- typical of unhindered allowed decay in this mass region between |n 7/2[514] and |p 9/2[514] states. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J low log| {Ift} (|<4.6) typical of unhindered allowed decay in this mass region (between |n 7/2[514] and |p 9/2[514] states). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: H
level_comment:
MOMM1 Value from NMR (19880h02); sign from 2000Ve10 (LASER spectroscopy). Other values: 0.8 {I2} from nuclear orientation (1981Sp06), +0.69 {I3} (2000Ve10, LASER spectroscopy); +0.72 {I3} (2006Ve10, LASER spectroscopy). 
MOME2 From Q/Q({+189}Ir)=+2.742 {I11} (1996Se15, NMR on oriented nuclei), assuming Q({+189}Ir)=+0.878 {I10}. Others: +2.1 {I4} (revision by 2005St24 of +2.2 {I4} (1981Ha33); nuclear orientation); +2.0 {I3} (1982Al34, nuclear orientation); +2.6 {I4} (2000Ve10, LASER spectroscopy); +2.5 {I4} (2006Ve10, LASER spectroscopy). 
|D<r{+2}>({+191}Ir,{+184}Ir)|?-0.176 {I3} from 2006Ve10. 
<r{+2}>{+1/2}(charge)=5.39 {I11} (2004An14). 
J |<5- from E1-M1-M1-M1 |g cascade from 1+ level; log| {Ift}=7.8 for |e decay to 6+ 774 level so J|>4; log| {Ift}=7.7 to 6- 1833 level rules out J|p=4-. Note, however, that based on systematics, 2004Ve10 propose J one unit lower than adopted here. 
T weighted average of 3.14 h {I2} (1982Al34), 3.08 h {I3}, 3.01 h {I3} (1981Ha33), and 3.02 h {I6} (1972Fi12). Others: 1960Ba43 (3.1 h {I3}), 1960Ma28 (2.6 h {I6}), and 1961Di04 (3.2 h {I2}). 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J E1+M2 155|g from 3+ 226; M1 71|g to 5- g.s.. 
T from ce-ce coin in |e decay (1996Om01). Other: <300 ps (1987BrZR). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J M2 226|g to 5- g.s.; M1-M1 cascade from 1+ 
T from 155|g(t) in {+176}Lu({+12}C,4n|g), E=68 MeV, pulsed beam (1988Kr17). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J M1+E2 68|g to 3+ 226; M1+E2 611|g from 1+ 904. 
T from ce-ce coin and ce-|g coin in |e decay (1996Om01). Other: |?1 ns (1987BrZR). 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: NS
level_comment:
J M2 329|g to 5- g.s.; properties of band built on this level. Supported by |g population pattern in (HI,xn|g) (1988Kr17); 287|g to (6)- 42. 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
J M1(+E2) 183|g to (2,3,4)+ 296; 277|g from (2)+ 856; log| {Ift}=6.8 from 0+ for weak |e branch favors J=1. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J E1 499|g to 5- g.s.; M1(+E2) 140|g from (3)+ 639. 1988Be16 very tentatively suggest a configuration of (|p h{-9/2})~#(|n 7/2[503]) for this state. If correct, the J=5 level with this configuration may lie at slightly lower energy. 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
J M1(+E2) 149|g to 2- 355; E1 399|g from 1+ 904. log| {Ift}=6.8, log| {If{+1u}t}<8.5 from 0+ for possible weak |e branch favors 1-. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J M1(+E2) 216|g to 2+ 293; M1 394|g from 1+ 904. log| {Ift}=6.7 from 0+ for weak |e branch favors J=1. 


level_energy_unit: KEV
level_spin_parity: (0,1)+
level_comment:
J M1,E2 581|g to 2+ 293; 531|g to 1+ 343; log| {Ift}=6.4 from 0+ for weak |e branch makes J=2 and 3 very unlikely. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: H
level_comment:
T$from 1982Al34. Other values: 14.0 h {I9} (1963Em02), 15 h {I3} (1958Di44). 
J$J from atomic beam (1975Ru06). K=1/2 assignment from experimental Q. Nilsson orbital assignment 1/2[541] based on the agreement between experimental and calculated |m (1985Va07) (including the Coriolis interaction between the 1/2[541] and 3/2[532] orbitals). 
MOMM1$radiative detection of nuclear magnetic resonance (1988Oh02,1989Ra17). Other values: 2.601 {I14}, radiative detection of nuclear magnetic resonance (1986Ed02). Other values: 2.6 {I2} (1981Sp06), 2.49 {I20} (1985Va07) static (low-temperature) nuclear orientation. 
MOME2$radiative detection of nuclear magnetic resonance (1988Oh02,1989Ra17). Other values: -1.9 {I5} radiative detection of nuclear magnetic resonance (1986Ed02); -2.5 {I3} (1982Al34), -1.9 {I3} recalculated for consistency with standards (1981Ha33,1989Ra17) static (low temperature) nuclear orientation. Other: 1988Oh08. 
<r{+2}>{+1/2}=5.39 fm 11 for {+185}Ir based on a global fit to charge radius data for all nuclides (2004An14). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
T from {+185}Pt |e decay (1979Sc20). 
J 135.3|g E2 to 5/2-; 94.3 E1 from 229.6 state, which is the band head of 3/2[402] rotational band; level not populated in {+185}Re(|a,4n), {+187}Re(|a,6n) makes high J unlikely. 135.3 |g is noted as mostly from the 33.0 min {+185}Pt decay (1979Sc20). The 1/2-[541] state. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T from {+185}Pt |e decay (1979Sc20). 
J$94.3|g E1 to 1/2-, 229.6|g E1 to 5/2-; 3/2[402] rotational band head. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
J 640.8|g (M1) to 9/2-, 488.0|g to (13/2)-. 
T from {+185}Re(|a,4n|g) (1979An20). Other value: 19 ns {I3}, from {+185}Pt |e decay (1970FiZZ). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$weighted average of 2.1 ns {I3} from |g|g(t), ce |g(t) (1979Sc20), and 2.1 ns {I2} from delayed |g|g coincidences (1970FiZZ). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: H
level_comment:
MOMM1$From (2019StZV, 1980Ha49 - NMR). Other values: 3.88 {I5} (1982Al11 - static nuclear orientation); +3.8 {I2} (2006Ve10 - laser spectroscopy); +3.69 {I15} (2000Ve10 - resonance ionization LASER spectroscopy); and 3.78 {I5} (1981Sp06 - NMR). 
MOME2$From 2021StZZ, 1996Se15 (NMR on oriented nuclei). Other values: -2.6 {I9} (2006Ve10 - laser spectroscopy); -2.89 {I10} (1980Ha49 - nuclear orientation); -2.5 {I2} (1980Mu07); -2.3 {I2} (1979Er06 and 1970Wa18 - nuclear orientation); -2.65 {I18} (preliminary result using NMR on oriented nuclei (1996Ha09)); -2.6 {I9} (2000Ve10, resonance ionization LASER spectroscopy). 
|d<r{+2}>({+191}Ir,{+186}Ir) =-0.073 fm{+2} {I4} (2006Ve10). 
J J=5 from atomic beam magnetic resonance (1975Ru06,1978Ru04). |p from decay to (3)- 1481 with log| {If{+1u}t}=10.1 and decay to 6+ 868 keV level with log ft = 7.8. 
T from 1982Al34. Others: 14 h {I2} (1955Sm42), 16 h {I3} (1958Di44), 15 h {I2} (1959Sc23), 14.5 h {I10} (1960Ma28), 14 h {I1} (1961Kr02), 15 h {I1} (1962Bo22), 15.8 h {I3} (1963Em02), 17 h {I1} (1963Ma47), and 16.3 h {I9} (1972Fi12). 


level_energy_unit: KEV
level_energy_info: ;OFF=X+0.0
level_spin_parity: 2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
MOMM1$g-factor=0.319 {I4} (1990Ed01, NMR on oriented nuclei); Sign from 2000Ve10. Others: -0.66~{I3} (2014StZZ, 2006Ve10 - laser spectroscopy); -0.63 {I3} (2000Ve10, resonance ionization LASER spectroscopy). 
MOME2$From 1996Se15 - NMR on oriented nuclei. Others:+1.5 {I2} (2006Ve10), +1.5 {I1} (2000Ve10); +1.53 {I10} from 1996Ha09, NMR on oriented nuclei (preliminary result). 
|d<r{+2}>({+191}Ir,{+186}Ir)=-0.221 fm{+2} {I2} (2006Ve10). 
J E1 689|g from 1+ x+689; |e decay to 3+ 910 with log| {Ift}=7.3 and to 4+ 434 with log| {If{+1u}t}=9.2; J=2 from NMR and temperature dependence of 767|g anisotropy following |e decay from Ir in Fe host (1990Ed01). Probable configuration=((|p 3/2[402])-(|n 7/2[503])) (1975Ya10,1991Be25); based on systematics and on hindrance of unobserved E|<1.5 keV IT. 
T from 1991Be25. Other values: 1.75 h {I15} (1972Fi12), 1.7 h {I2} (1963Ma47), 2.0 h {I5} (1963Gr22), 1.7 h {I2} (1962Bo22). 
%IT 20-30% estimated from 1991Be25, based on their {+186}Pt |e decay scheme and observation of time variation of intensities of 434|g({+186}Os) and 987|g({+186}Os) produced exclusively in {+186}Ir |e decay (16.64 h) and {+186}Ir |e decay (1.90 h), respectively. 
E 0<x|<1.5 (1991Be25), based on absence in {+186}Pt |e decay of any conversion electron line from an E>2.6 transition having adequate intensity to be the expected (x+1.1 to g.s.) transition. 


level_energy_unit: KEV
level_energy_info: ;OFF=X+1.10
level_spin_parity: (3)+
level_comment:
J 1991Be25 expect low-lying 3+ and 5+ states arising from configuration=((|n 1/2[510])(|p h{-9/2})) at approximately the same energy (in {+184}Ir and {+184}Au, the 3+ state lies at the lower energy; here, the 5+ may be the g.s.). M1-M1 612|g-77|g cascade from 1+ x+689 establishes |p=+ and eliminates the J=5 option. 


level_energy_unit: KEV
level_energy_info: ;OFF=X+252.57
level_spin_parity: (1,2,3,4)
level_comment:
J$Doubly placed |g's to (2,3,4)+ x+72 level (181|g) and from 1+,2+ x+447 level (194|g). Possible configuration=(|n 7/2[503]) (|p h{-9/2}) (1991Be25) allows J{+|p}=3+ and 4+, but the |g to 5+ g.s. expected for that state has not been reported. 


level_energy_unit: KEV
level_energy_info: ;OFF=X+331.20
level_spin_parity: (0,1)
level_comment:
J 94|g to (0,1)+ x+237 level, 253|g to (2)+ x+78 keV level, no observed |g to (3)+ x+1.1 keV level. 


level_energy_unit: KEV
level_spin_parity: (10-)
level_comment:
J D 236|g to 520 keV level. band configuration (|p h{-11/2})(|n i{-13/2}), similar to (|p h{-11/2}) band in {+185}Ir (1997Ca01). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
MOMM1 Laser spectroscopy (2000Ve10). Other: +0.17 {I1} (2006Ve10) 
MOME2 by quadrupole-interaction-resolved NMR on oriented nuclei (1996Se15); Same in 2005St24. Others: +0.88 {I10} (2000Ve10), +0.9 {I1} (2006Ve10) - both from Laser spectroscopy. 
T$From 1963Em02. Other values: 11 h {I1} (1961Kr02), 11.8 h {I3} (1950Ch11), and 13 h {I3} (1958Di44). 
|D<r{+2}>({+187}Ir,{+191}Ir)=-0.168 {I3} (2006Ve10); <r{+2}>{+1/2}({+187}Ir)=5.39 {I11} fm (2004An14) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
J 247.6|g M1 to 9/2- state, band structure. 
MOMM1,MOME2$from 1989Ra17 (differential perturbed angular distribution). Same values in 2005St24. 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_comment:
E$ existence of this level seems questionable since it is not shown in level scheme figures of 2010Mo09, it is only from placement of 392.7|g from a 2413 level shown in table I of 2010Mo09 (Compiler's note) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_comment:
$Mixed configurations=|p11/2[505]~#|n(7/2[503],1/2[510])+ |p1/2[541]~#|n(11/2[615],9/2[624])+|p1/2[400]~#|n(9/2[505],9/2[624])+ |p3/2[402]~#|n(7/2[503],9/2[624]) 


level_energy_unit: KEV
level_comment:
J$ (21/2)- listed as initial J|p with 166.2|g in table I of 2010Mo09, no J|p given in level scheme figures or with 746.7|g in table I 


level_energy_unit: KEV
level_comment:
J$ 23/2- listed as initial J|p with 466.3|g in table I of 2010Mo09, no J|p given in level scheme figures or with 991.5|g in table I 


level_energy_unit: KEV
level_comment:
J$ 23/2- listed as initial J|p with 535.2|g in table I of 2010Mo09, no J|p given in level scheme figures or with 882.7|g in table I 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_comment:
$Mixed configurations=|p11/2[505]~#|n(9/2[505],1/2[510])+ |p9/2[514]~#|n(9/2[505],3/2[512])+|p3/2[402]~#|n(9/2[505],9/2[624])+ |p1/2[400]~#|n(9/2[505],11/2[615]) 


level_energy_unit: KEV
level_comment:
J$ 25/2- listed as initial J|p with 497.3|g in table I of 2010Mo09, no J|p given in level scheme figures 


level_energy_unit: KEV
level_spin_parity: 29/2-
level_lifetime_unit: US
level_comment:
T$ measured in 2010Mo09 from difference in multiplicity distributions for transitions above and below the isomer 
$ Configuration=|p9/2[514]~#|n(11/2[615],9/2[624]) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
J$J was directly measured using the NMR (1985Ed02) and resonance ionization spectroscopy (2006Ve10) techniques; |p from |m and 478.3|g E1 from 1+ 
MOMM1$using resonance ionization spectroscopy technique. Others: 0.302 {I10} (NMR-nuclear orientation,1985Ed02) 0.385 {I20} (1980Be27), 1974EkZW 
MOME2$using the NMR on oriented nuclei method. Others: +0.46 {I5} (2006Ve10), +0.507 {I34} (1996Ha09), +0.543 {I18} (1985Ed02), +0.492 {I26} (1988Oh05,1988Oh08), 1.26 (1980Mu07) (for J=2). 
$|D<r{+2}>({+191}Ir,{+188}Ir)=-0.140 {I4} (2006Ve10) 
T$from 1950Ch11. Others: 41 h {I1} (1963Gr22), 41 h {I4} (1955Sm42), and 40 h {I3} (1954Na25) 
CONF$Dominant K|p=1-, |p3/2{++}[402]~#|n1/2{+-}[510] with possible |p1/2{++}[400]~#|n3/2{+-}[512] admixtures 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$54.85|g M1+E2 to 1-; 97.2|g M1 from (3)-; absence of a direct |b{+-} feeding to this level in {+188}Pt |e decay (10.2 d) (J|p=0+) 
T$From 54.8e(L{-ii}+L{-iii})-140.3e(K)(t) in 1969Ma37. Others: 2.3 ns {I2} (1965Ja06) and 2.7 ns {I8} (1965Kr03,1970Ba53), but the accuracy of those values is disputed in 1969Ma37 
CONF$Most likely a member of the K|p=1- g.s. band, given the large B(E2) strength 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$96.70|g E2+M1 to 1-; 114.6|g M1(+E2) from (3)-; absence of a direct |b{+-} feeding to this level in {+188}Pt |e decay (10.2 d) (J|p=0+) 
T$From 41.9e(L)-381.6|g(t) in 1969Ma37. 
CONF$K|p=2-, |p3/2{++}[402]~#|n1/2{+-}[510] with possible |p1/2{++}[400]~#|n3/2{+-}[512] admixtures 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$97.2|g M1 to 2-; the absence of direct population in {+188}Pt |e decay (10.2 d) (J|p=0+) would argue against J|p=1- 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: PS
level_comment:
J$187.59|g E2(+M1) to 1-; direct population of this level in {+188}Pt |e decay (10.2 d) (J|p=0+) 
T$From KLL-187.59(L{-I})(t) in 1969Ma37 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
J$140.35|g M1(+E2) to 2-; 195.05|g M1(+E2) to 1-; direct population of this level in {+188}Pt |e decay (10.2 d) (J|p=0+) would argue against J|p=2- 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$114.6|g M1(+E2) to 2-; the absence of direct population in {+188}Pt |e decay (10.2 d) (J|p=0+) would argue against J|p=1- 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_comment:
J$280.30|g E2+M1 to 1-; direct population in {+188}Pt |e decay (10.2 d) (J|p=0+) would argue against J|p=3-, but first forbidden unique |b{+-} transition cannot be excluded (log| {Ift}=7.3) 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J$56.2|g M1 to (4)+; assigned by the evaluators as a member of the K|p=(4)+ band, by reordering the 56.2|g and 81.6|g. This assignment is consistent with the expected smooth behavior as a function of spin of a K=4 rotational band 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$478.3|g E1 to 1-; 381.43|g E1 to 2-; direct population of this level in {+188}Pt |e decay (10.2 d) (J|p=0+) would argue against J|p=2+ 
T$From LMM - 300 (and higher)|g(t) in 1969Ma37 


level_energy_unit: KEV
level_spin_parity: (7)+
level_comment:
J$149.9|g M1,E2 to (6)+; band member. J|p=(8+) in {+186}W({+7}Li,5n|g) (2008Ju02), see the comment to the 815-keV level 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J$172.8|g to (7)+, 322.5|g to (6)+; J|p=(9+) in {+186}W({+7}Li,5n|g) (2008Ju02), but the assignment is incorrect since 322.5|g would be Mult.=M3 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11-)
level_lifetime_unit: MS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Presumably decays via a low-energy transition (E|g<80 keV), so x <80 keV 
J$From systematics of similar high-spin isomers in neighboring {+190}Ir and {+192}Ir nuclei. The assignment is consistent with the expected configuration at ~880 keV. The proposed J|p=(9-) assignment in 2004Ba91 and 2008Ju02 is unlikely, since the band-head spin is inconsistent with the proposed |ph{-9/2}~#|ni{-13/2} configuration, where the low-K, (|p1/2{+-}[541] (h{-9/2}) and high-K (|n11/2{++}[615] (i{-13/2}) orbitals are near the Fermi surfaces, thus leading to J|p=6- 
T$Weighted average of 4.1 ms {I3} (1984Kr18), 4.1 ms {I4} (1975An08), and 4.2 ms {I2} (1971Go21). Other: 3.8 ms {I2} (1973RoYQ) 
CONF$Likely |p11/2{+-}[505]~#|n11/2{++}[615] configuration, expected at ~880 keV from energies of known proton and neutron orbitals in neighboring Ir and Os nuclei. This configuration was assigned to the known isomers in {+190}Ir and {+192}Ir 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (11-)
level_lifetime_unit: MS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Transitions directly depopulating this level have not been observed. The authors stated that the isomer may decay via low-energy, highly converted gamma rays. The value of x is probably less than |? 100 keV. 
J$From adopted levels 
T$Weighted average of 4.1 ms {I3} (1984Kr18), 4.1 ms {I4} (1975An08), and 4.2 ms {I2} (1971Go21). Other: 3.8 ms {I2} (1973RoYQ) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
T$From 54.8e(L{-ii}+L{-iii})-140.3e(K)(t) in 1969Ma37. Others: 2.3 ns {I2} (1965Ja06) and 2.7 ns {I8} (1965Kr03,1970Ba53), but the accuracy of those values is disputed in 1969Ma37 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (9-)
level_lifetime_unit: MS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from the Adopted Levels. The excitation energy of the isomer in 2008Ju02 is given as >642 keV 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
$RMS charge radius <r{+2}>{+1/2}=5.390 fm {I106} (2013An02 evaluation) 
J$spin from atomic beam (1975Ru06,1978Ru04); parity from L(p,t)=0 from 3/2+ target 
T$weighted average of 13.1 d {I1} (1975Ba35), 13.3 d {I1} (1964Le07), 13.3 d {I2} (1963Gr22), and 13.8 d {I7} (1959Ka09). Other values: 10.5 d (1965Qa01), 12.5 d (1960Po07) and 11 d (1955Sm42) 
MOMM1$laser spectroscopy measurements (2006Ve10, also 2000Ve10, 2000Sa58). Other: 0.13 {I+3-4} (1980Be27, low-temperature nuclear orientation) 
MOME2$from 2016St14 evaluation. Measured values: +0.85 {I7} (2006Ve10, resonant ionization mass spectrometry/laser spectroscopy, also earlier reports 2000Ve10 and 2000Sa58), +0.878 {I10} (1996Se15, NMR on oriented nuclei), +0.79 {I6} (1992Ka49,1992Ka48), +1.0 {I2} (1985Ha41, nuclear orientation), 1.0 {I1} (1980Mu07, quadrupole interaction nuclear orientation). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J$M1+E2 |g to 3/2+; E2 |g from 5/2+; band assignment 
T$weighted average of delayed coincidence measurements 11.3 ns {I3} (1969Ha03), and 11.6 ns {I6} (1972Ba21) from {+189}Pt |e decay. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
J$E3 to 5/2+, M2(+E3) to 7/2+, RUL. 
T$weighted average of 13.4 ms {I2} (1973RoYQ), 12.3 ms {I5} (1967Co20) and 14 ms {I1} (1963Re13). Other values: 10.0 ms {I6} (1960Mo19), 14 ms {I3} (1968Io01) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_lifetime_unit: NS
level_comment:
J$E1 to 7/2+, |g to 9/2+, and 7/2 excluded by being fed by (13/2)- level at 742 keV in rotational band 
T$measured by 2012MaZP from time difference between 178 feeding |g 263 depopulating transition. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 from 1184 level, and E2 to 11/2- uniquely establish J|p(615)=7/2- and J|p(1184)=5/2- 
T$delayed coincidence from 1970Ba56 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
J$E1+M2 to (23/2-,25/2-), (D) to 23/2-, no |gs to levels of J|p|<21/2- with the possible exception of the 2109.5 level. The transition to the 2109.5 level is weak and the 223.8|g is consistent with M2 leading to a tentative assignment of J|p(2109.5)=(21/2-) 
T$weighted average of 3.8 ms {I2} (1975Ke06) and 3.2 ms {I4} (1975An08); from |g(t) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 13.4 ms {I2} (1973RoYQ), 12.3 ms {I5} (1967Co20), and 14 ms {I1} (1963Re13). Other values: 10.0 ms {I6} (1960Mo19), 14 ms {I3} (1968Io01) 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_comment:
$841|g and a tentative 972|g placed by 1975An08 deexciting this level, but the intensity balance arguments for levels fed by these two transitions do not support these placements. 


level_energy_unit: KEV
level_comment:
$d|s/d|W=6 
$E=173, |s=1.4 mb (1978St09) 
L$|s(|q) for 173 level in 1978St09 is given under L=0 cases in their Fig. 3, but |s(|q) distribution for this level in 1978St09 as well as in 1978Lo07 differs significantly from those for other L=0 transitions 
$3/2+ member of |p1/2[400] band 


level_energy_unit: KEV
level_comment:
$Tentatively interpreted as |p5/2[402] state (1978St09) 
$|s=0.2 mb (1978St09) 
$Possible |ph{-11/2}, J|p=11/2- state 


level_energy_unit: KEV
level_comment:
$d|s/d|W=11 
$E=748, |s=3.4 mb (1978St09) 
$Interpreted as 7/2+, |g-vibrational state based on the g.s. (1978Lo07) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=3 
$E=1184, |s=3.4 mb (1978St09) The 1184 keV value is used in the Adopted Levels supported by |g transitions 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$weighted average of 11.3 ns {I3} (1969Ha03) and 11.6 ns {I6} (1972Ba21). Other values: 12 ns {I1} (1965Ja12), 11 ns {I1} (1966Kr08) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T$measured by 2012MaZP from time difference between the 178|g feeding this level, and the deexciting 263|g. 


level_energy_unit: KEV
level_comment:
$841|g and a tentative 972|g placed by 1975An08 deexciting this level, but the intensity balance arguments for levels fed by these two transitions in the 3.7-ms IT decay dataset do not support these placements. The 841|g is tentatively placed from a 1548 level, and the 972|g is unplaced here. 


level_energy_unit: KEV
level_spin_parity: (23/2)-
level_comment:
E,J$this level is defined at 2212 keV with J|p=(25/2,27/2)+ in 1975An08 due to reversed ordering of the 121|g-85|g cascade 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
J$(27/2)- in 1975An08 
T$weighted average of 3.8 ms {I2} (1975Ke06) and 3.2 ms {I4} (1975An08); from |g(t) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: D
level_comment:
J$spin from direct |e feeding to 3-, 4+, 4-, and 5- levels in {+190}Os, respectively; parity based on 22.5|g E2 from 6- and L(d,t)=3 from 3/2+ to the lowest energy state which is most probably the ground state 
T$from 1975Ba35. Others: 12.1 d {I2} (1969Sa18), 11 d {I1} (1963Gr22), 12.3 d {I4} (1960Ka14), 11 d (1955At32), 12.6 d {I3} (1950Ch11), 10.7 d {I3} (1947Go01) 
MOMM1$nuclear orientation with |g detection (1983Al15) 
MOME2$nuclear orientation with |g detection (1980Mu07) (relative to 1.0 for {+189}Ir). Other: +2.71 {I19} (quoted in 1985Ha41, also 2014StZZ from a thesis by Schneider (1980)) 
$1996Ga30 propose that this state is a mixture of two configurations: |n9/2[505]-|p1/2[400] (dominant), with 18% admixture of |p3/2[402]+|n5/2[503], to explain spectroscopic strength in (d,t) as as well as the measured magnetic moment 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J$22.5|g E2 to J|p=4- ground state; 205.2|g E1 from 7+ 
$Possible configuration=|n9/2[505]+|p3/2[402] (1995Ga04), same as for the 38.1 level, but with K|p=6-, consistent with GM rule 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
$%IT=100 is assigned as only the isomeric decay of this activity has been reported by 1996Ga30, with a reasonable B(M3)(W.u.) value for the 26.1-keV transition, although, some branching by |e decay is possible. 
J$26.1|g M3 to 4-; L(d,t)=1 from 3/2+ and L(p)=(2) for a group at 26 keV. This level was assigned to have J|p=7+ by 1964Ha06 based on a 148.7, M4 transition to this level from the (11)- 3.1-h isomer at an energy of 175 keV as proposed by 1964Ha06, and later based on the newly-identified |g transitions from the |g decay of the 3.1-h isomer and the ce data of the 26.1-keV transition, 1996Ga30 claimed that the 3.1-h isomer is at E=374.6 keV and that the 26.1-keV transition does not belong to the decay path of the 3.1-h isomer, and assigned J|p=1- to the 1.1-h isomer. 
T$from 1996Ga30. Other: 1.2 h (1964Ha06) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT;ISO=M2
level_comment:
J$36.2|g E1 to 4-. See comments for 171.5 level. 
T$estimated by 1996Ga30 from absence of 36.1-keV transition in (ce)|g-coin spectrum in IT decay, shown in their Fig. 5. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$L(d,t)=5 from 3/2+ 
$Configuration=|n9/2[505]-|p3/2[402], K|p=(3)- (1995Ga04). See also possible configuration for the 22.46, (6)- level 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: NS
level_comment:
J$L(d,t)=1+3 from 3/2+ for a doublet; 82.6|g D, |DJ=(1) to 4- 
T$centroid-shift method in (p,3n|g),(d,4n|g) (2000Ga03) 
$Configuration=|p3/2[402]-|n1/2[510], K|p=1- and configuration=|p3/2[402]+|n3/2[512] for a doublet (1995Ga04) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
T$(beam pulse)(149|g)(t) in (p,3n|g),(d,4n|g) (2000Ga03) 
$A 90 ns {I3} isomer is indicated in (149|g)(beam pulse)(t) decay curve in Fig. 4 of 2000Ga03. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$56.1|g M1 from 7+, and 135.4|g E2 to 36.2 level which has 36.2|g E1 to 4-, determine J|p(36.2)=4+ and J|p(171.5)=6+ 
T$from ce-ce(t) (p,3n|g),(d,4n|g). Other: 3.7 ns {I1} from ce-ce(t) in IT decay 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
E$unresolved doublet 
J$L(d,t)=(1,3) from 3/2+. L(p)=(0+2) from 3/2- suggests 1-,2- 
$Configuration=|p1/2[400]+|n3/2[512] and configuration=|p3/2[402]+|n1/2[510] for two components 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
J$148.7|g M4 from 11- 
T$ce-ce(t) (1996Ga30) in IT decay 
$Configuration=|p3/2[402]~#|n11/2[615], K|p=7+ bandhead 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
$In delayed |g|g-coin spectrum of Fig. 6 in 2000Ga03 showed a cascade of 82.6|g and 148.7|g, with the latter lying below the 82.6-keV transition. This isomer and decay scheme connected with it are not shown by 2000Ga03. Also note that 82.6-keV transition is assigned as a g.s. transition by 2000Ga03 with a statement that a major fraction of its intensity remains unplaced. 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E$weighted average of 270.3 {I14} from ({+3}He,d) and 268.8 {I11} from (|a,t) 
J$L(p)=(0+2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
E$weighted average of 284.8 {I19} from ({+3}He,d), 282.9 {I16} from (|a,t), and 284.9 {I3} from (d,t) 
J$L(d,t)=1+3 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
E$weighted average of 311.1 {I11} from ({+3}He,d), 313.3 {I8} from (|a,t), and 313.4 {I4} from (d,t) 
J$L(d,t)=1+3 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M4
level_comment:
E$this isomer was proposed by 1964Ha06 to be at an energy of 175 keV and to feed the 1.12-h isomer at E=26.1 keV by the 148.7|g transition, and later based on their newly-identified |g transitions from the |g decay of the 3.1-h isomer and the ce data of the 26.1-keV transition, 1996Ga30 claimed that the 3.1-h isomer is at E=374.6 keV and that the 26.1-keV transition does not belong to the decay path of the 3.1-h 
J$11- is proposed by 1964Ha06 from their observation of a strong allowed |e feeding (log{Ift}=4.8) to the (10)- isomer in {+190}Os and possible configuration=|p11/2[505]+|n11/2[615], based on the configuration of 10- isomer in {+190}Os. 
T$from 1996Ga30. Others: 3.25 h {20} (1970Bo22), 3.0 h {I2} (1963Gr22), 3.2 h {I2} (1950Ch11) 
$%|e from 1996Ga30. Other: 94.4 {I8} (1964Ha06) 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E$weighted average of 379.0 {I9} from ({+3}He,d) and 380.6 {I8} from (|a,t) 
J$L(p)=(0+2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E$weighted average of 431.4 {I13} from ({+3}He,d) and 429.0 {I21} from (|a,t) 
J$L(p)=(0+2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$weighted average of 465.9 {I21} from ({+3}He,d) and 465.1 {I16} from (|a,t) 
J$L(p)=(4,5) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E$weighted average of 499.3 {I16} from ({+3}He,d) and 497.8 {I9} from (|a,t) 
J$L(p)=(0+2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (0:3)-
level_comment:
E$weighted average of 511.1 {I16} from ({+3}He,d), 511.1 {I13} from (|a,t), and 510.9 {I5} from (d,t) 
J$L(d,t)=1 from 3/2+. L(p)=(0+2) from 3/2- suggests 1-,2- 


level_energy_unit: KEV
level_spin_parity: (0:3)-
level_comment:
E$weighted average of 589.6 {I16} from ({+3}He,d), 589.9 {I13} from (|a,t), and 589.3 {I6} from (d,t) 
J$L(d,t)=1 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (0:4)(-)
level_comment:
E$weighted average of 620.7 {I13} from ({+3}He,d) and 622.2 {I13} from (|a,t) 
J$L(p)=(2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (0:4)(-)
level_comment:
E$weighted average of 670.0 {I14} from ({+3}He,d) and 671.5 {I13} from (|a,t) 
J$L(p)=(2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_comment:
E$weighted average of 694.5 {I14} from ({+3}He,d) and 694.0 {I9} from (|a,t) 
J$L(p)=(0+2) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E$weighted average of 714.9 {I22} from ({+3}He,d) and 717.0 {I17} from (|a,t) 
J$L(p)=(4,5) from 3/2- 


level_energy_unit: KEV
level_spin_parity: (0:4)(-)
level_comment:
E$weighted average of 741.3 {I13} from ({+3}He,d) and 741.9 {I13} from (|a,t) 
J$L(p)=(2) from 3/2- 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_uncertain: ?
level_comment:
$y |>3100, T{-1/2}=60-130 d (2001Ma73). From |a, |g, |a-|g and |a-|g-x coin studies (by 2001Ma73) of reaction products from {+181}Ta({+28}Si,4a3n){+190}Au reaction followed by |e decay chain {+190}Au-{+190}Pt-{+190}Ir, two |a groups at 5290 and 5430, and 144.0|g-141.0|g cascade in {+186}Re (possibly populating 471-330-186 levels in {+186}Re) were tentatively assigned to the decay of this isomer. This isomer was interpreted as a possible (SD) state in the second-potential well 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
J$this level was assigned to have J|p=7+ by 1964Ha06 based on a 148.7, M4 transition to this level from the (11)- 3.1-h isomer at an energy of 175 keV as proposed by 1964Ha06, and later based on the newly-identified |g transitions from the |g decay of the 3.1-h isomer and the ce data of the 26.1-keV transition, 1996Ga30 claimed that the 3.1-h isomer is at E=374.6 keV and that the 26.1-keV transition does not belong to the decay path of the 3.1-h isomer, and assigned J|p=1- to the 1.1-h isomer. 
T$from ce(t) in 1996Ga30. Other: 1.2 h (1964Ha06) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J$spin=4 from observation of |e feeding to J=3, 4 and 5 levels in {+190}Os by 1974Ya02; negative parity is assigned by 1996Ga30 based on their measured ce data of 36.2|g, 56.1|g, 135.4|g and 205.2|g, that are identified and assigned by 1996Ga30 as from the negative-parity 3.087-h isomer. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT;ISO=M1
level_comment:
T$estimated by 1996Ga30 from absence of 36.1-keV transition in ce-|g-coin spectrum shown in their Fig. 5. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M2
level_comment:
E$this isomer was proposed by 1964Ha06 to be at an energy of 175 keV and to feed the 1.12-h isomer at E=26.1 keV by the 148.7|g transition 
J$11- is proposed by 1964Ha06 from their observation of a strong allowed |e feeding (log{Ift}=4.8) to the (10)- isomer in {+190}Os and possible configuration=|p11/2[505]+|n11/2[615], based on the configuration of 10- isomer in {+190}Os. 
T$from ce(t) (1996Ga30). Others: 3.35 h {I20} (1970Bo22), 1963Gr22, 1950Ch11 


level_energy_unit: KEV
level_spin_parity: (2-)&(3-)
level_comment:
$|s(|mb/sr)=35 {I4} 
E$proposed to be a doublet 
$Configuration=|p3/2[402]-|n1/2[510]; K|p=1- and configuration=|p3/2[402]+|n3/2[512] for a proposed doublet 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$|s(|mb/sr)=13.4 {I17} 
E$unresolved doublet 
$Configuration=|p1/2[400]+|n3/2[512] and configuration=|p3/2[402]+|n1/2[510] for the two components 


level_energy_unit: KEV
level_spin_parity: (2-)&(3-)
level_comment:
$|s(|mb/sr)=57 {I6} 
E$proposed to be a doublet 
$Configuration=|p3/2[402]-|n1/2[510], K|p=1- and configuration=|p3/2[402]+|n3/2[512] for a proposed doublet 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$|s(|mb/sr)=8.5 {I10} 
E$unresolved doublet 
$Configuration=|p1/2[400]+|n3/2[512] and configuration=|p3/2[402]+|n1/2[510] for two components 


level_energy_unit: KEV
level_spin_parity: (2)-&(3)-
level_comment:
S$0.22 {I6} for L=3 
E$proposed to be a doublet 
$Configuration=|p3/2[402]-|n1/2[510], K|p=1- and configuration=|p3/2[402]+|n3/2[512] for a proposed doublet 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
S$0.31 {I5} for L=3 
E$unresolved doublet 
$Configuration=|p1/2[400]+|n3/2[512] and configuration=|p3/2[402]+|n1/2[510] for two components 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
T$centroid-shift method 
$Configuration=|p3/2[402]-|n1/2[510], K|p=1- and configuration=|p3/2[402]+|n3/2[512] for a doublet (1995Ga04) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: D
level_comment:
J$from the Adopted Levels of {+190}Ir in the ENSDF database. 
T$from 186.7|g(t), 518.6|g(t), 569.3|g(t), and 557.9|g(t) (2024Ja07). Measurements were made relative reference lines {+192}Ir (308.5|g and 316.5|g) and {+133}Ba (276.4|g and 302.9|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J optical spectroscopy (1950Br75,1952Mu40,1953Si61). Parity from L=2 in ({+3}He,d) and (|a,t). Nilsson assignment 3/2[402] based on energy systematics of this orbital in other odd-mass Ir isotopes. Spectroscopic factors in ({+3}He,d) and (|a,t), and L=0 population in (p,t) are consistent with 3/2, 3/2[402]. 
MOMM1 Atomic beam (direct); independent of the Knight shift (1984Bu15,2000Ve10,2019StZV). Other values: +0.1461 {I6}, NMR, includes +1.3% {I4} Knight-shift correction (1968Na01); +0.152 {I4} hfs in resonant laser spectroscopy (2006Ve10), 0.146 {I8} (1969Da11). 
MOME2 Meson hfs (1983Ta14,1984Ta04,1985St28,2016St14). Other values: +0.81 {I21}, atomic beam, optical spectroscopy, including Sternheimer correction (1978Bu17); +0.774 {I24}, hfs in Mossbauer (1967Wa12); +0.82 {I8}, hfs in resonant laser spectroscopy (2006Ve10), 0.78 {I20} (1973Bu15 - atomic-beam magnetic-resonance), 0.86 (1974ScYF preliminary). 
Nuclear charge radius: <r{+2}>{+1/2}=5.40 fm {I11} (2004An14) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J L=0 in ({+3}He,d) and (|a,t). Relative values of spectroscopic factors in ({+3}He,d) and (|a,t) agree with theory for 1/2[400] Nilsson orbital assignment. Absolute values are about one-half of the theoretical predictions for 1/2[400]. This is probably due to a mixture of a (K-2) |g-vibration coupled to the 3/2[402] ground-state orbital. The Nilsson orbital 1/2[400] has been observed in other odd-mass Ir isotopes at about the same energy. 
T Weighted average of 4.02 ns {I12} (from |t=5.18 ns {I17} - 82|g(t) (1971Bo13)), 4.17 ns {I10} (1969Ha03 - 82|g(t)); in {+191}Pt |e decay: 3.85 ns {I35} (1955Su64 - (|b)(ce)(t)); 3.8 ns {I4} (K| x-ray)(|g)(t), 4.1 ns {I3} (K| x-ray)(ce)(t), and 3.7 ns {I6} Mossbauer (all three values in 1969Ow02); 4.21 ns {I16} (Coulomb excitation). 
MOMM1 From 1983Wa31, 2020StZV - Mossbauer Effect. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in ({+3}He,d); ce-|g(|q) (1964De06) using ce(41.9L,E3) from level seen with L=5+2 in ({+3}He,d),(|a,t) and 129.4|g (M1+E2) to 3/2+ within possible spin choices determine this and 171.2-keV-level spins. G.s. band assignment from 129.4|g to ground state with enhanced B(E2). Spectroscopic factors in ({+3}He,d) and (|a,t) are consistent with 5/2,3/2[402]. 
T$weighted average of 90.5 ps {I11} from (|g,|g): Mossbauer, and 87.9 ps {I16} from Coulomb excitation. Others: 122 ps {I6} from {+191}Os |b{+-} decay (15.4 d); 120.4 ps {I34} (1986Ko20 - in Coul. Ex.). 
MOMM1 transient field IMPAC in Coulomb excitation (2000Be07, 2020StZV; supersedes 1996St22). Other value: +0.450 {I23} (1986Ko20), transient field IMPAC in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J See comment on 129.4 keV level J|p. Nilsson orbital assignment 11/2[505] based on energy systematics of this orbital in other odd-mass Ir isotopes. This assignment is consistent with experimental |m (theoretical |m=+6.9). 
T from {+191}Ir IT decay (4.9 s). 
MOMM1 NMR, radiative detection; no hfs-anomaly correction (1974Kr06,1971Es03,2019StZV). Sign=+, nuclear orientation/NMR (1988Sc20, 1996Oh03, 1991Sc28 (Compton Polarimeter)). Other: 3.27 {I12} (1973Kr05). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J 96.5|g M1+E2 to 1/2+. 
T from B(E2)|^=0.102 {I6} (Coulomb excitation) and adopted |g properties. Other: 40 ps {I12} (1970Ma10 - {+191}Pt |e decay). 
MOMM1 IPAC (1973Il02,2020StZV). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J |p=+ from Coulomb excitation; 343.3|g E2 to 3/2+ and component L=(4) from the 343-351 doublet in ({+3}He,d) and (|a,t) (see comment on 351 keV level J|p); |g(|q) in low-energy Coulomb excitation. 
T From Coulomb excitation. 
MOMM1 From g-factor=+0.401 {I18}, transient field IMPAC measurement in Coulomb excitation (2000Be07, supersedes 1996St22, 2020StZV). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J 268.7|g E2 to 1/2+ excludes component L=(4) from L=(4+2) for 343-351 doublet in ({+3}He,d) and (|a,t) and limits choices to 3/2+ and 5/2+; band member. 
T From Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J L=3 in ({+3}He,d) and (|a,t); 219.7|g E2 to 11/2- is E2(+M1) in {+191}Pt |e decay (adopted E2). 
T from 1970Ba56, (ce)(ce)(t) - {+191}Pt |e decay. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
J 373.1|g E2 to 5/2+, with enhanced B(E2) (g.s. band member). 
T from 2000Be07, recoil-distance method listed in Coulomb excitation. 
MOMM1 From g-factor=+0.53 {I5}, transient field IMPAC measurement in Coulomb excitation (2000Be07, supersedes 1996St22, 2020StZV). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J 325.2|g to 3/2+; 161.2|g to (7/2)+; 152.9|g (D(+Q); |DJ=1) to (5/2)+; populated in {+191}Ir(n,n'|g) with the expected intensity for the 7/2 member of band. 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J 385.3|g (|DJ=1) to 11/2-; 385.3|g excitation function discussed in 591.32 keV level J|p comment. Feeding pattern in {+192}Ir(p,2n),(d,3n|g) suggests yrast level. 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
J L=2 in ({+3}He,d) and (|a,t). 
T from {+191}Ir(|g,|g') res fluorescence; T{-1/2}=0.27 ps {I4} if J|p=3/2+, T{-1/2}=0.40 ps {I6} if J|p=5/2+. 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J 419.9|g (Q) to 11/2-; 419.9|g excitation function in {+192}Ir(p,2n),(d,3n|g), relative to 385.3|g from 556.82 keV level, increases with projectile energy; hence |DJ(419.9|g)>|DJ(385.3|g)=(1). Feeding pattern in {+192}Ir(p,2n),(d,3n|g) suggests yrast level. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J 541.6|g (M1) to 1/2+; populated in {+191}Ir(n,n'|g) with the expected intensity for the 1/2 member of band. The 1/2[411] Nilsson orbital has been observed at about 560 keV in {+193}Ir. 
T from {+191}Ir(|g,|g'). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J 267.9|g E2 to 7/2- from {+191}Pt |e decay; 576.5|g to 1/2+ 
T From 1970Ba56, Auger-ce(t) - {+191}Pt |e decay. Others: >0.05 fs and 0.78 ps {I+1590-38} in (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J L=4 in ({+3}He,d) and (|a,t), 557.0|g M1+E2 to 5/2+, 686.4|g E2 to 3/2+. 
T from Coulomb excitation. 
MOMM1 From 2020StZV, 2000Be07 - transient field IMPAC measurement in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J 209.0|g M1(+E2) to 3/2+; 404.1|g to (7/2)+; populated in {+191}Ir(n,n'|g) with the expected intensity for the 5/2 member of band. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J 140.9|g M1 to (3/2)-; 409|g to 7/2-; populated in {+191}Ir(n,n'|g) with the expected intensity for the 5/2 member of band. 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_lifetime_unit: PS
level_comment:
J 329.4|g D(+Q) (|DJ=1) to (9/2)+ 
T from Coulomb excitation. 
MOMM1 From 1996St22, 2020StZV - Transient Field method. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J 389.1|g to 3/2+; 425.5|g to (9/2+); populated in {+191}Ir(n,n'|g) with the expected intensity for the 7/2 member of band. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
J 853.5|g to 1/2+ and 806.4|g to 5/2+; log ft=7.4 in {+191}Pt |e decay from 3/2-. 1987Pr10 suggests 7/2+ from population in {+191}Ir(n,n'|g), but then log| {If{+1u}t} in {+191}Pt |e decay would be 6.4 implying |DJ=0,1. The band member was reassigned to 928 keV level. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J 568.5|g to 7/2-, 318.4|g to (3/2)-; |g-decay pattern and population in {+191}Ir(n,n'|g) agrees with expectation of the 7/2 member of band. If the assignment is confirmed, the level seen with L=2 in ({+3}He,d) and (|a,t) must be a different level. 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J 487.1|g to (7/2+), 489.0|g to (9/2)+; populated in {+191}Ir(n,n'|g) with the expected intensity for the 11/2 band member. 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J 445.5|g (|DJ=1) to (15/2-); populated in {+191}Ir(n,n'|g) with the expected intensity for the 17/2 band member. 


level_energy_unit: KEV
level_comment:
1987Pr10 from {+191}Ir(n,n'|g) and 1979Lu01 from {+192}Ir(p,2n|g) suggest J|p=(9/2+); |g-branching ratios in (n,n'|g) and (p,2n|g) do not match. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J 229.9|g to (7/2-); populated in {+191}Ir(n,n'|g) with the expected intensity for the 9/2 member of band 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J 414.3|g to (13/2+) and 586|g to (11/2+) in (d,3n|g) and Coulomb excitation suggest 15/2 member of the g.s. band. 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
J 308.5|g M3 to (25/2+) 
CONF$possible |n(9/2{+-}[505],11/2{++}[615])~#|p(11/2{+-}[505]) 
T$From |t=8.3 s {I8} (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T Weighted average from: 4.90 s {I5} (1963Ka34), 4.95 s {I5} (1967Ab09), 4.88 s {I3} (1970Jo16,1972Jo05). Other values: 4.96 s {I20} (1968Lu01), 4.91 s {I14} (1955Fi30), 4.9 s {I1} (1956Ca50), 4.53 s {I18} (1958Cl42). Others: 1954Bu02, 1954Mi93, 1954Na34, 1963Ve13, 1968Bo28. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T From Adopted Levels. Data of this dataset would yield 3.92 ns {I30} from weighted average of 3.85 ns {I35} (1955Su64 - (|b)(ce)(t)), 3.8 ns {I3} (K x-ray)(|g)(t) from |t=5.5 ns {I5}, 4.1 ns {I3} (K x-ray)(ce)(t) from |t=5.9 ns {I4} both in 1969Ow02 (also 3.7 ns {I6} reported in 1969Ow02 - see (|g,|g'): Mossbauer). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
g-factor=+0.244 {I22} (recalculated by evaluator for adopted T{-1/2}=89.7 ps {I12}), perturbed angular correlation (in 1969Ow02 +0.22 {I2} for their T{-1/2}=99.8 ps {I69} from |t=144 ps {I10}). 
T From adopted levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
Unresolved doublet. Dividing the intensity in the same proportion of the similar states in {+193}Ir, 1971Pr13 obtained: L=5 and C{+2}{-jl}U{+2}=0.87 (0.71 in (|a,t)) for 171 level; L=2 and C{+2}{-jl}U{+2}=0.06 (0.06 in (|a,t)) for 178 level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S for L=2; 0.79 for L=4. C{+2}{-jl}U{+2}=0.13 for L=2 and 0.21 for L=4 in (|a,t). 
Doublet. 7/2, 3/2[402] + 5/2, 1/2[400] 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S for L=5; 1.66 for L=6. Spectroscopic factors in (|a,t) are 2.08 for L=5, 1.65 for L=6. 
Probable doublet, 9/2, 1/2[541] + 13/2, 1/2[660]. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOME2 from Q({+191}Ir)/Q({+193}Ir)=1.03 {I3} from isomer shifts (1967Wa12) using Q({+193}Ir)=+0.751 {I9} from hyperfine structure of muonic x rays (2016St14,1984Ta04). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T From |t=5.3 ns {I8} (1969Ow02). Other: T{-1/2}=2.3 ns (discrepant datum probably due to broadening of Mossbauer line - noted in 1967Jh02). 
g-factor=+1.200 {I6}, recalculated for consistency with standard (1983Wa31,1989Ra17); sign=- (1987Be36) Mossbauer detection of oriented nuc disagrees with adopted sign. Other: +1.083 {I9} (1967Wa20), +1.03 {I5} (1969Ow02) Mossbauer. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T Weighted average of: 97 ps {I+14-7} (1959Mo05 - from |t=140 ns {I+20-10}), 89.4 ps {I14} (1969St04 - from |t=129 ps {I2}), 100 ps {I7} (1969Ow02 - from |t=144 ps {I10}), 91.2 ps {I16} (1993Wa05 - from 5.00 eV {I9}) |* 10{+-6} obtained from |G{-v}=1.16 cm/s {I2} given in Table II. 
g-factor=+1.7 {I3} (recalculated by evaluator for adopted T{-1/2}=89.7 ps {I12} in adopted levels) (1968Da19). This value disagrees with the adopted value, +0.322 {I22}, from transient field IMPAC measurements in Coulomb excitation (2000Be07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
T |J 0.25 ps if J|p=3/2+, or |J 0.37 ps {I6} assuming J|p=5/2+, deduced from (1.76 ps {I20})|*(g2/g1)(|G{-0}/|G){+2}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
T Other: <0.12 ns from null observation of isomer formation by 1995Kh02. Other: 0.78 ps {I+1590-38} (1995La25). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J This level fits better the |g-decay pattern expected from the band member in {+192}Ir(p,2n|g),(d,3n|g) reaction, and has population rate in (n,n'|g) similar to 935.7 level, assigned by 1987Pr10 as the 7/2+ member of 1/2[411] band. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J Adopted: (1/2+,3/2,5/2+). 1987Pr10 suggests this level as the (7/2+) member of 1/2[411] band, but it was not seen in {+192}Ir(p,2n|g),(d,3n|g). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
BE2$from 1984Mu19. Other values: 0.068 {I8} (quoted by 1986Mc01 from 1981HuZU); 0.083 {I11} (1971No01); 0.055 {I7} (1969Av03). Other: 1971Pr12. 
T From B(E2)=0.0662 {I15} and adopted |g-ray properties. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
g-factor=+0.322 {I22} transient field IMPAC measurements (2000Be07). Other: 0.34 {I6} (1970Av02), perturbed angular correlation, recalculated by evaluator with adopted T{-1/2}=89.9 ps {I9}. 
BE2 Weighted average of 0.897 {I25} (quoted by 1986Mc01 from 1981HuZU), 0.98 {I5} (1984Mu19), 0.89 {I7} (1971No01), and 0.82 {I8} (1969Av03). Other: 0.97 (1957Be56). 
T Weighted average of 87.9 ps {I16} (2000Be07 - |t=126.8 ps {I23} - recoil-distance method) and 94 ps {I4} (from B(E2)=0.905 {I20} and adopted |g properties). Other: 120.4 ps {I34} (1986Ko20 - |t=173.7 ps {I72}- recoil-distance method). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 0.108 {I9} (quoted by 1986Mc01 from 1981HuZU), 0.074 {I13} (1984Mu19), 0.11 {I10} (1971No01). Other: 0.18 {I11} (1969Av03); 1971Pr12. 
T Calculated using B(E2)=0.102 {I6} and adopted |g properties. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
g-factor=+0.401 {I18} transient field IMPAC measurements (2000Be07). 
BE2 Unweighted average of 0.556 {I12} (quoted by 1986Mc01 from 1981HuZU), 0.60 {I1} (1984Mu19), 0.50 {I7} (1971No01), and 0.54 {I6} (1969Av03). Other: 1971Pr12. 
T Weighted average of 20.4 ps {I15} (2000Be07, 2004StZZ - |t=29.4 ps {I22} - recoil-distance method), 20.3 ps {I8}, B(E2)=0.549 {I21} and adopted |g-ray properties, and 21.3 ps {I30} (1986Ko20 - |t=30.8 ps {I44} - recoil-distance measurement). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
BE2 (1984Mu19). Other: 0.030 {I8} (quoted by 1986Mc01 from 1981HuZU); 1971Pr12. 
T From B(E2)|^=0.0170 {I6}, adopted 351|g and other |g-ray properties. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
B(E2)|^=1.11 {I3} (based on B(E2)|_=102 {I3}*0.00652=0.665 {I20} - quoted in 1986Mc01 (Table III) from 1981HuZU). 
g-factor=+0.53 {I5} transient field IMPAC measurements (2000Be07). 
T Weighted average of 13.4 ps {I19} (2000Be07 - |t=19.3 ps {I27} - recoil-distance method), 9.6 ps {I4}, calculated by evaluator from B(E2)(129 to 502)=1.11 {I3} and adopted |g properties, 13.1 ps {I32} (1986Ko20 - |t=18.9 ps {I46} - recoil-distance measurement). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
g-factor=+0.23 {I9} transient field IMPAC measurements (2000Be07). 
BE2 Unweighted average of 0.126 {I4} (quoted by 1986Mc01 from 1981HuZU), 0.13 {I1} (1984Mu19), and 0.094 {I11} (1971No01). 
T Calculated by evaluator from B(E2)|^=0.117 {I11} and adopted |g ray properties. Other: T{-1/2}<2.8 ps (from |t=1.6 ps {I25} - 1986Ko20). 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_lifetime_unit: PS
level_comment:
g-factor=+0.61 {I17} transient field IMPAC measurements (2000Be07). 
B(E2)|^=0.70 {I4} (based on B(E2)|_=72 {I4}*0.00652=0.469 {I26} - quoted by 1986Mc01 in Table III from 1981HuZU). 
T Calculated by evaluator from B(E2)(343 to 832)=0.70 {I4}, adopted 489|g and other |g-ray properties. 


level_energy_unit: KEV
level_comment:
E$Level not reported in other studies. 1979Lu01 proposed based on the multiple placement of 360.4|g. Level not adopted by the evaluator. 


level_energy_unit: KEV
level_comment:
E$Level not reported in other studies. 1979Lu01 proposed based on the multiple placement of 420.1|g. Level not adopted by the evaluator. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J %|b{+-} feeding of 0.09 {I7} from transition intensity balance is consistent with J|p=1/2+. %|b{+-} feeding estimated based ce(L)(47.0):ce(L)(82.4) exp=96 {I20}:32 {I3} (1969Ma07 with uncertainty in ce(L)(47.0) including 20% for E(ce) energy range). 
T From Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T coincidence peak centroid shift method, weighted average of: 126 ps {I11} (1969Ma07), 125 ps {I12}(1966Ra01), 80 ps {I16} (1962Be46) ce-|b; 131 ps {I10} (1962Li12) ce-ce in {+191}Pt |e decay. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$Level energy held fixed In least-squares adjustment 
E,J,T$from Adopted Levels 
CONF$|p(11/2{+-}[505]) 


level_energy_unit: KEV
level_spin_parity: 25/2-
level_comment:
E$observed to be fed in both in-beam and out-of-beam time periods, consistent with the non-isomeric nature 


level_energy_unit: KEV
level_spin_parity: 31/2(+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
T$From |t=8.3 s {I8}: weighted average of mean lifetimes 8.4 s {I9} (using 395|g(t), when gating on 420|g-536|g pair) and 7.9 s {I21} (using 308|g(t), when gating on 420|g-519|g pair) (2012Dr02). In text 2012Dr02 also mention T{-1/2}=5.5 s {I7} and corresponding |t=7.9 s {I10}. Also |t=8.2 s {I7} in Table I. 
CONF$possible |n(9/2{+-}[505],11/2{++}[615])~#|p(11/2{+-}[505]) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: D
level_comment:
%|b{+-}, %|e: from |S(I(|g+ce) to {+192}Pt g.s.), representing all decays by |b{+-}, and |S(I(|g+ce) to {+192}Os g.s.), representing all decays by |e. 
MOMM1 Magnitude from radiative detection of NMR (1989Ra17); value relative to |m=+0.1637 {I6} for {+193}Ir(g.s.). Sign from nuclear orientation, |g-ray circular polarization (1988Sc20). 
MOME2 Average of +2.15 {I6} (from Q/Q({+189}Ir)=+1.658 {I5} and Q({+189}Ir)=+0.878 {I10}; 1996Se15, NMR on oriented nuclei) and +2.28 {I6} (value relative to Q=+0.751 {I9} for {+193}Ir(g.s.); radiative detection of NMR, 1989Ra17 from 1985Ed02). Other values: +2.03 {I23} and +2.36 {I11} (1989Ra17 from 1986Gr26 and 1985Ha41); +2.28 {I6} (preliminary result, 1996Ha09). 
J spin from atomic beam (1963Do13); E3 |g from |p=- 57 level establishes |p=+. The probable configuration for {+192}Ir g.s. is configuration=((|p 3/2[402])-(|n 11/2[615]))+((|p 11/2[505])-(|n 3/2[512])) (1991Ke10), as for {+190}Ir; supported by measured |m. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_uncertain: ?
level_comment:
J possible mixed configuration=((|p 1/2[400])+(|n 11/2[615]))+((|p 11/2[505])+(|n 1/2[512])) (1997BaZV). 


level_energy_unit: KEV
level_spin_parity: (6-)
level_uncertain: ?
level_comment:
J possible E2 50.8|g from (4)- 67 level; tentative bandhead for configuration=((|p 3/2[402])+(|n 9/2[505])) (1997BaZV) which is expected to lie below the 3- 84 level (based on Gallagher-Moszkowski rule); absence in (n,|g) E=2, 24 keV favors J>3. However, the expected strong L=5 excitation of this configuration in (d,t) is unobserved up to E=200 keV (1994Ga05). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
%|b{+-}: from |SI|b{+-} (three groups) relative to total number of disintegrations (1959Sc41; uncertainty unstated). 
J L(d,p)=1; E3 57|g to J=4 g.s. 
T from 1953We02, 1954We10. Other value: 1.42 min {I10} (1961Sc07). Others: 1937Mc04, 1948Ho37, 1954Mi85. 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: NS
level_comment:
J L(d,p)=3 for 3/2+ target; 67|g to 4+ is not M2 or higher; absence of primary |g in (n,|g) (average resonance capture) favors J>3; tentative configuration=((|p 3/2[402])+(|n 5/2[503])) (1994Ga05) or configuration=((|p 1/2[400])-(|n 9/2[505])) (1997BaZV) (or mixture of the two) implies J=4. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
J E1 119|g to 4+; fed by primary |g from 1+,2+ in (n,|g) E=thermal. Possible bandhead for configuration=((|p 3/2[402])+(|n 3/2[512])) (1991Ke10). 


level_energy_unit: KEV
level_spin_parity: (0)-
level_comment:
J M1 72|g to 1- 57; L(d,t)=1 for 3/2+ target; band assignment. 
E|g=128.736 {I25} for a transition in (n,|g) E=thermal suggests a placement from this level, but the implied M4 multipolarity (|a=1082) rules this out because that |g was absent from the ce spectrum. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_uncertain: ?
level_comment:
J population ratio for 127|g in (n,|g) (E=resonance) favors J=4 (1991Ke10) or J=5 (1997BaZV); possible M1 127|g to (6+) 13; proposed (1997BaZV) bandhead for possible mixed configuration=((|p 1/2[400])-(|n 11/2[615]))+((|p 11/2[505])-(|n 1/2[512])). 


level_energy_unit: KEV
level_spin_parity: (1)-
level_comment:
J 1-,2- based on M1 86|g to 1- and L(d,t)=1,3; band assignments from 1997BaZV and 1994Ga05 differ, but both require J=1. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_uncertain: ?
level_comment:
J possible (M1) 145|g to 4+ g.s.; possible g.s. band member (1997BaZV), consistent with observed excitation strength in ({+3}He,|a) and absence in (d,t) (1994Ga05). However, implied rotational band parameter (A|?14 keV) is lower than anticipated (1997BaZV, 1994Ga05). 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M2
level_comment:
%IT: only IT decay has been observed (|g-ray spectrum from very old source almost identical to spectrum from {+192}Ir g.s. decay (1959Sc41)). The |b{+-} and |e+|b{++} decay energies are such that the highest spin state available for population would be the (7-) 1518 level in {+192}Pt. 
IF JPI=9+, LOGF1UT>8.5 IMPLIES %IB<27 TO 7- 1518 LEVEL. 
E assuming IT decay feeds the tentative 12.98 level as suggested in 1997BaZV. 
J (E5) 155|g to highly tentative (6+) 13 level. See also comment on J|p for this level in {+192}Ir (241 y) IT decay data set. 
T from 1970Ha32. Others: 1959Sc41, 1963Ha17. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J M1 109|g to 3- 84 level; M1 49|g to (1)- 144. Possible configuration=((|p 3/2[402])+(|n 1/2[510])) (1994Ga05). 


level_energy_unit: KEV
level_spin_parity: LE 3
level_comment:
E 202.9 11 (C), 198 2 (EF), 202.8 11 (I) 
J fed by primary |g in (n,|g) E=thermal; 1+,2+ suggested by (n,|g) E=2,24 keV. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
J 217|g population ratio in (n,|g) (E=resonance) favors J=3 (1991Ke10) or J=4 (1997BaZV); possible M1 217|g to 4+ g.s.; proposed as bandhead (1997BaZV) for mixed configuration=((|p 3/2[402])-(|n 11/2[615]))+((|p 11/2[505])-(|n 3/2[512])) (amplitudes orthogonal to those for g.s. configuration). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_uncertain: ?
level_comment:
J possible E1 207|g to (6-) 16; multiply-placed 210|g to (6+) 13; proposed as bandhead (1997BaZV) for possible mixed configuration=((|p 1/2[400])+(|n 11/2[615]))+((|p 11/2[505])+(|n 1/2[512])) (amplitudes orthogonal to those for 13-keV level configuration). 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J E2 169|g to 1- 57; M1 107|g to 3- 119 level; M1 121|g to (1)- 105. Possible configuration=((|p 1/2[400])+(|n 3/2[512])) (1994Ga05). 


level_energy_unit: KEV
level_spin_parity: (LE2-)
level_uncertain: ?
level_comment:
J possible M1 166.1|g from (1,2,3)- 392 level; doubly-placed M1 170|g to 1- 57; nominated as bandhead for a second expected K|p=0- configuration (1997BaZV). 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J possible M1+E2 179|g to 1- 57; possible M1 107|g to (0)- 129. Tentative configuration=((|p 1/2[400])+(|n 1/2[510])) (1994Ga05). Not excited in transfer reactions. 


level_energy_unit: KEV
level_spin_parity: (4,5)-
level_comment:
E 257.2 5 (E), 256.8 2 (F) 
J L(d,p)=3, so J=1 to 5; absence in (n,|g) studies favors J>3. Tentative configuration=((|p 3/2[402])+(|n 7/2[503])) (1994Ga05) favors J=5; however, configuration=((|p 3/2[402])+(|n 5/2[503])), J=4 is also possible. 


level_energy_unit: KEV
level_spin_parity: (0-)
level_uncertain: ?
level_comment:
J possible M1 208|g to 1- 57; postulated as a third K|p=0- bandhead (1997BaZV); (n,|g) E=2, 24 keV is consistent with the excitation of a 0- and 3- doublet comprising this level and the (3)- 267 level. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J L(d,t)=1,3; M1 152|g to (2)- 116 level; J=3 from population ratio for 152|g in (n,|g) (E=resonance). 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
J 3-,4- from M1 194|g to 3- 84 level and L(d,t)=5; absence of primary |g in (n,|g) E=thermal favors J>3; should be (but is not) strongly excited in (n,|g) E=2, 24 keV if J|p=3-. J=4 required by band assignment. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J M1 232|g to 1- 57 level; M1 95|g to (2)- 192.9; J=2 or possibly 3 from population ratio for 184|g in (n,|g) (E=resonance). 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J M1 66|g to (2)- 226 level; 1-,2- from (n,|g) E=2, 24 keV; band assignment. 292|g to 4+ g.s. may be wrongly placed (1991Ke10). 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J M1 226|g to (1)- 105 level; M1 216|g to (2)- 116 level; J=2 from population ratios for 188|g and 226|g in (n,|g) (E=resonance). 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J E2 352|g to 4+ g.s.; 158|g to (1)+ 193.5 level; J=2 or possibly 1 from population ratio for 267|g in (n,|g) (E=resonance); 232|g to 3- 119. Possible K=2 bandhead (1997BaZV). 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_uncertain: ?
level_comment:
J possible M1 99|g to (3)- 267; possible M1 140|g to (2)- 225.9. However, proposed as a J=4 band member (1997BaZV). 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J M1+E2 285|g to (1)- 105 level; M1 123|g to (3)- 267; J=1,2 from population ratio for 149|g in (n,|g) (E=resonance). However, preferred (based on |g decay pattern) over the 392 level for J=3 member of band which includes the 105 level (1994Ga05). 


level_energy_unit: KEV
level_spin_parity: (1,2,3)-
level_comment:
J M1 199|g to (2)- 192.9 level; 274|g to 3- 119 level. J=3 if tentative band assignment is correct. 


level_energy_unit: KEV
level_spin_parity: (3+,4+)
level_uncertain: ?
level_comment:
J possible E1 334|g to 3- 84 level; possible 278|g to (5+) 140. J=3 if tentative band assignment is correct. 


level_energy_unit: KEV
level_comment:
J possible J=8 member of configuration=((|p 3/2[402])+(|n 11/2[615])) based on excitation strength in ({+3}He,|a) (1994Ga05). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
J possible M1 72|g to (3+) 441; possible M1 95|g to (3+,4+) 418; tentative band structure (1997BaZV). 


level_energy_unit: KEV
level_spin_parity: 0- : 3-
level_comment:
E 543.63 21 (C), 542.7 8 (E), 543.4 10 (F), 543.3 4 (I) 
E from (n,|g) E=thermal: primary. 
J L(d,p)=1. 


level_energy_unit: KEV
level_spin_parity: 0- : 3-
level_comment:
E from (n,|g) E=thermal: primary. Others: 603.2 {I4} from {+191}Ir(n,|g) E=2, 24 keV, 604 {I4} from (p,t), 603.7 {I7} from (d,t). 
J L(d,t)=1. 


level_energy_unit: KEV
level_spin_parity: 0- : 3-
level_comment:
E average of 614.4 {I7} in (d,p) and 615.5 {I7} in (d,t); however, E=612.9 {I8} in (n,|g) E=thermal: primary. 
J L(d,p)=1. 


level_energy_unit: KEV
level_comment:
E 663.30 20 (C), 660.7 8 (E), 662.0 7 (F) 
J L(d,p)=1, L(d,t)=1,3 for E(level)=660.7 {I8}, 662.0 {I7}, respectively. 


level_energy_unit: KEV
level_spin_parity: 0- : 3-
level_comment:
E 702.8 3 (C), 700.7 9 (E), 702.3 9 (F); 697 4 (H). 
E 697 {I4} from (p,|a) excluded from average. 
J L(d,p)=1. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: S
level_comment:
E neutron separation energy from 2011AuZZ. Not a discrete state. 
J s-wave neutron capture by 3/2+ target. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T from 1953We02, 1954We10. Other value: 1.42 min 10 (1961Sc07). Others: 1937Mc04, 1948Ho37, 1954Mi85. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Not observed by 1994Ga05; authors estimate S<0.03 if L=1. Not resolved from tentative 131 level seen in (d,t) by 1991Ke10. 


level_energy_unit: KEV
level_comment:
E,L,S for doublet composed of the adopted levels at 366.7 and 368.4 (1994Ga05). E=366.4 {I4} for this doublet in 1991Ke10. 


level_energy_unit: KEV
level_comment:
E=288.5 {I3} for unresolved 288+294 doublet in 1994Ga05; evaluator assigns L and S deduced for doublet to the 288 component because, in 1991Ke10, the 294 level contributes only 8% and 14%, respectively, to doublet's d|s/d|W(15 MeV, 45|') and d|s/d|W(22 MeV, 120|'). 


level_energy_unit: KEV
level_comment:
E resolved only at E(d)=14 MeV (1991Ke10). 
L=1,3 and S=0.046 {I4}, 0.096 {I19} for 390+391 doublet (1994Ga05). 


level_energy_unit: KEV
level_comment:
E,L E=540.4 {I7} in 1994Ga05, suggesting that the 537 and 543 levels are unresolved in 1994Ga05; if so, L and S may be unreliable. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J optical spectroscopy (1976Fu06), L({+3}He,d)=2, L(d,{+3}He)=2 
MOMM1 Atomic beam (direct) (2014StZZ,1984Bu15). Other: +0.1591 {I6} (NMR 2014StZZ,1968Na01) 
MOME2 Hyperfine structure of muonic x rays (2014StZZ,1984Ta04); Others: +0.7 {I2} Atomic beam (1978Bu17), +0.73 {I7} Laser spectroscopy (2006Ve10). 
Isotope shift: |D<r{+2}>({+191}Ir,{+193}Ir)=0.044 fm{+2} {I4} (1989Sa31); <r{+2}>{+1/2}=5.40 fm {I11} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J J=1/2 from {+193}Ir(|g,|g): Mossbauer; |p from M1+E2 |g to 3/2+ level. 
T from {+193}Os |b{+-} decay; other: 4.1 ns {I3} (B(E2) in Coulomb excitation) 
MOMM1 Mossbauer (2014StZZ,1969Pe05) 
2005Ki01 observed nuclear excitation by electron transitions (NEET) of 2.8|*10{+-9} {I4} times the K-shell photoelectric cross section at energy: Ir K-edge + 128 eV (76.229 keV); synchrotron radiation, internal conversion electron time spectroscopy using Si avalanche photodiode. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 3/2+ level, M1+E2 |g from 7/2+ level; 
T from recoil-distance method in Coulomb excitation (2000Be07). Other: 80 ps {I5} ({+193}Os |b{+-} decay); 80 ps {I2} ({+193}Ir(|g,|g):Mossbauer) 
MOMM1 From transient field IMPAC measurement (({+58}Ni,{+58}Ni') and ({+65}Cu,{+65}Cu') - 2000Be07). Others: +0.53 {I3} transient field IMPAC measurement (({+32}S,{+32}S') (Coulomb excitation) 2014StZZ,1986Ko20); +0.93 {I5} (1996St22) (transient field IMPAC measurement) (1996St22) (the reason for discrepancy with the datum from 1986Ko20 is not clear (1996St22)). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 1/2+ level 
T unweighted average of 59 ps {I7} ({+193}Os |b{+-} decay) and 28 ps {I4} (B(E2) in Coulomb excitation) 
MOMM1 from integral perturbed angular correlation. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J L=3 in {+194}Pt(d,{+3}He); J=L+1/2 {+194}Pt(pol t,|a); E2 |g to 11/2- level. 
T from |g|g(t) in {+193}Os |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J |g|g(|q) in Coulomb excitation (1958Mc02) is consistent only with J=7/2; M1+E2 |g to |p=+ level; L=2 in inelastic scattering. 
T from recoil-distance method in Coulomb excitation (2000Be07,1986Ko20). 
MOMM1 From transient field IMPAC measurement (({+58}Ni,{+58}Ni') and ({+65}Cu,{+65}Cu') - 2014StZZ, 2000Be07, 1996St22). Others: +1.7 {I3} (transient field IMPAC measurement in Coulomb Excitation - relative to |m (138.9 level)=+0.528 {I30} - 2014StZZ,1986Ko20). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in {+194}Pt(d,{+3}He), (E2) to 1/2+ 
T weighted average of 36 ps {I7} ({+193}Os |b{+-} decay) and 25 ps {I3} (B(E2) in Coulomb excitation) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 1/2+ level, band structure. 
T Weighted average of 17 ps {I4} ({+193}Os |b{+-} decay), 13.8 ps {I10} (B(E2) in Coulomb excitation), 11 ps {I2} ({+193}Ir(|g,|g'):res fluorescence) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
J (M1) |g to 7/2+ level, (E2) |g to 5/2+ level; band structure 
T From recoil-distance method in Coulomb excitation 
MOMM1 From transient field IMPAC measurement (({+58}Ni,{+58}Ni') - 2014StZZ, 1996St22). Other: +3.8 {I11} (relative to |m(138.9 level)=+0.528 {I30}, transient field IMPAC in Coulomb excitation (1986Ko20)). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in {+194}Pt(d,{+3}He); M1 |g to 5/2+ level 
T from {+193}Ir(|g,|g') res fluorescence 
configuration: assigned as 5/2+ 5/2[402] state by 1971Pr13 ({+193}Os({+3}He,d), (|a,t)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J M1 |g from 5/2- level; |g to 1/2+ level. Band structure. 
T from {+194}Ir(|g,|g'): res fluorescence 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J L=4 in {+194}Pt(d,{+3}He) and {+192}Os({+3}He,d), (|a,t); J=L-1/2 in {+194}Pt(pol t,|a); |g to 3/2+. 
T from recoil distance method and B(E2) in Coulomb excitation 
MOMM1 From transient field IMPAC measurement (({+58}Ni,{+58}Ni') - 2014StZZ, 1996St22). Other: +0.5 {I4} (relative to |m(138.9 level)=+0.528 {I30} transient field IMPAC measurement in Coulomb excitation 2014StZZ, 1986Ko20) 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_lifetime_unit: PS
level_comment:
J (E2) |g to 7/2+ level, (M1) |g to (9/2)+ level; band structure 
T From B(E2) to 357.8 level in Coulomb excitation 
MOMM1 From transient field IMPAC measurement (({+58}Ni,{+58}Ni') - 2014StZZ, 1996St22). 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J |g's to 1/2+ and 7/2+. Assigned 7/2+ member of the second K|p=1/2 band in (n,n'|g); however, this assignment is inconsistent with observed transitions to 1/2+ levels. 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2(+),5/2+
level_comment:
J |g's to 1/2+ and 5/2+ levels; 3/2- not consistent with {+193}Ir(n,n'|g) data; multiply placed |g to 7/2+ level would rule out 1/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J L=3 in {+192}Os({+3}He,d), (|a,t); |g to 3/2+ level. Assigned as 5/2- 1/2[541] state by 1971Pr13 ({+192}Os({+3}He,d), (|a,t)) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
J L=5 in {+192}Os({+3}He,d), (|a,t); 9/2- consistent with band assignment. Alternatively assigned as 9/2- 1/2[541] state by 1971Pr13 ({+192}Os({+3}He,d), (|a,t)) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T weighted average of 6.3 ns {I2} |b(ce)(t) (1969Li13), 6.34 ns {I16} |g|g(t) (1969Ba28), 5.90 ns {I11} |g|g(t) (1972Be85,1973Il02), with increased uncertainty (discrepant data set) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T Weighted average of 75 ps {I10} (ce)(ce)(t) (1970Be06), 77 ps {I17} |g|g(t) (1969Ba28), 74 ps {I11} |b(ce)(t) (1969Li13), 88 ps {I9} |b(ce)(t) (1968Av02). Other: 1960Fe03. Adopted value 69.7 ps {I10} from recoil-distance method in Coulomb excitation (2000Be07). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T weighted average of 55 ps {I+8-15} (ce)(ce)(t) (1970Be06), 46 ps {I15} |g|g(t) (1969Ba28), 66 ps {I10} |b(ce)(t) (1969Li13); other: <35 ps (1968Av02). Adopted value 43 ps {I16}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T weighted average of 19 ps {I5} (1968Av02), 15 ps {I6} (1969Va36,1969Li13) |b(ce)(t); other: 1973Il02. Adopted value 13.2 ps {I10}. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
T$Absolute electron counting in 4|p|b proportional counter (1987Li16). Other values: 11.9 d {I5} (1957Bo12), 10.8 d {I5} (1969Bi01), 12 d {I2} (1970Ba56), 10.60 d {I11} (1975Ba35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
B(E2)|^|<0.13 ((p,p') 1980Ha47) 
Level composed of 73.0 level (J|p=1/2+), plus possible minor component from 80.2 level (J|p=11/2-) ((p,p') 1980Ha47) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
|b{-2}=0.145; B(E2)|^=0.66 ((p,p') 1980Ha47) 
Level composed of 357.7 (J|p=7/2+) and possibly also 361.9 (J|p=5/2+) levels ((p,p') 1980Ha47) 


level_energy_unit: KEV
level_spin_parity: 1/2+ & 11/2-
level_comment:
Unresolved doublet, with division of intensity assumed to be the same as that for the analogous states in {+191}Ir. L=0 and C{+2}{-jl}U{+2}=0.25 (0.24 in (|a,t)) for 73.0 level; L=5 and C{+2}{-jl}U{+2}=0.77 (0.89 in (|a,t)) for 80.2 level. 


level_energy_unit: KEV
level_spin_parity: 7/2+ & 5/2+
level_comment:
Unresolved doublet. If the entire cross section is assumed to be of the assigned L, C{+2}{-jl}U{+2}=1.28 (0.50 in (|a,t)) for L=4 and C{+2}{-jl}U{+2}=0.30 (0.26 in (|a,t)) for L=2. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
g(73 level)/g(g.s.)=9.1 {I3} (1967At03), +8.875 {I18} (1967Wa20) 
J from shape of absorption spectrum (magnetic splitting of 73.0 level) (1967At03); |p from adopted levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T from [(2J+1)/(2J(g.s.)+1)] x [|G{+2}{-|g0}/|G] =7.6|*10{+-6} eV {I12} (1967Me12); adopted value T{-1/2}=14.9 ps {I18} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T the value given in 1970Me16, mean life =1.65 {I24}, had been corrected to reflect the adopted branching ratios and |g properties (see adopted gammas). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
J alternate 7/2+ assignment by 1987Pr10 not consistent with observation of 733.9|g to 1/2+ (evaluator) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
1987Pr10 suggest that this is the 7/2+ member of the second K|p=1/2+ band. However, a weak |g to 1/2+ level, seen in {+193}Os |b{+-} decay contradicts this assignment. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
BE2 Weighted average of 0.11 {I1} (1971No01), 0.111 {I12} (1969Av03) 
T In Adopted Levels: 6.09 ns {I15} (from {+193}Os |b{+-} decay) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
BE2 Limited weight method average of 0.81 {I3} (2000Be07), 0.71 {I7} (1971No01), 0.64 {I6} (1969Av03), 0.74 {I7} (1958Mc02) 
g-factor=+0.356 {I16} transient field IMPAC measurements (2000Be07). Other: 0.211 {I12} (static field), +0.215 {I13} (transient field) IMPAC measurements (1986Ko20); 1970Av02. 
T 2000Be07 (recoil-distance method). Others: 92 {I4} ps (recoil-distance method, 1986Ko20); 78 {I4} ps (from B(E2)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 0.095 {I14} (1972Pr04), 0.085 {I10} (1971No01). Other: 0.25 {I15} (1969Av01) 
T Adopted value: 43 ps {I16}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 0.50 {I2} (2000Be07), 0.525 {I10} (1984Mu19), 0.54 {I8} (1972Pr04), 0.49 {I7} (1971No01), 0.47 {I5} (1969Av03), 0.61 {I7} (1958Mc02) 
g-factor=+0.441 {I16} transient field IMPAC measurements (2000Be07). Other: +0.41 {I8} (static field), +0.62 {I13} (transient field) IMPAC measurements, (1986Ko20) 
T weighted average of 18.6 ps {I7} (2000Be07) and 20.4 ps {I24} (1986Ko20) (recoil-distance). Other: 14.9 ps {I7} from B(E2), not included in the average because depends on I|g(219) from 357.8 level seen as an unresolved doublet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
B(E2)=0.827 {I30} (138.9 level to 521.9 level) (1987Mc01) 
g-factor=+0.54 {I15} (transient field IMPAC measurement), 2000Be07 - unweighted average of {+58}Ni runs at 155 and 180 MeV. Other: +0.84 {I25} (transient field IMPAC measurement, 1986Ko20) 
T weighted average of 13.9 ps {I22} (2000Be07) and 11 ps {I4} (1986Ko20) (recoil-distance); 10.4 ps {I6} from B(E2) was not included because J is uncertain 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2)+
level_lifetime_unit: PS
level_comment:
1984Mu19 report B(E2)=0.046 {I15}; however, assuming 557|g pure E2 to determine an upper limit, this B(E2) gives T{-1/2}=6 {I2} ps, much smaller than the measured T{-1/2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 0.110 {I6} (1984Mu19), 0.121 {I18} (1972Pr04), 0.090 {I11} (1971No01) 
g-factor=+0.33 {I4} (transient field IMPAC measurement, 2000Be07). Other:+0.15 {I11} (transient field IMPAC measurement, 1986Ko20) 
T weighted average of 4.4 ps {I5} (2000Be07) and 6.1 ps {I17} (1986Ko20) (recoil-distance method), and 4.2 ps {I4} (from adopted B(E2)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_comment:
B(E2)=0.013 {I4} (1987Mc01) 
J (7/2+) assignment from 1987Mc01 not consistent with observation of 733.9|g (to 1/2+) in {+193}Ir(n,n'|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2)+
level_lifetime_unit: PS
level_comment:
B(E2)=0.50 {I3} (357.7 level to 857 level) (1987Mc01) 
g-factor=+0.49 {I13} (transient field IMPAC measurement, 2000Be07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
695 and 712 levels not resolved. 
L$for 695 and 712 levels combined. 
C{+2}S=0.52 if entire cross section is assumed to be for 695 level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
695 and 712 levels not resolved. 
L$for 695 and 712 levels combined. 
C{+2}S=0.73 if entire cross section is assumed to be for 712 level. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from Adopted Levels 
CONF$|p(11/2{+-}[505]) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d<r{+2}>{+191,193}=+0.065 fm{+2} {I+7-6} (2020Mu16) 
J$from the Adopted Levels of {+193}Ir in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
T$weighted average (NRM) of 19.20 h {I2} (2016Kr06, decay curve for 328|g recorded for 2.5 half-lives, uncertainty was increased to 0.03 to bring down the relative weight to 50%); 19.15 h {I3} (1972Ge10); 19.41 h {I1} (1972Em01, uncertainty got increased to 0.10 in the NRM procedure); 19.0 h {I2} (1947Go01). Other measurements: 17.4 h {I1} (1964Pe18), 19.7 h {I7} (1958Gu09), 20.7 h {I5} (1947Se33), 19.5 h (1941Wi07), 19.5 h (1938Ja01), 1935Am01. Weighted average of the four values is 19.37 h {I5}, but with reduced |h{+2}=35. The unweighted average of these values is 19.19 h {I9}. 
J$spin from atomic-beam method (1963Do13). Parity from L(d,p)=1 from 3/2+ target. 
MOMM1$Radiation detection of nuclear magnetic resonance (1982Ha28). Other value: 0.37 {I4}, low temperature nuclear orientation (1969Re06); sign of |m=+, low temperature nuclear orientation (1988Sc20,1991Sc28). 
MOME2$Radiation detection of nuclear magnetic resonance (1985Ed02,1982Ha28). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
J$M2 |g to 2-; absence of |g to 1- suggests J>3. 
T$from 1972Br53. Others: 30 ms {I2} (1968Lu01), 50 ms (1962Fe02), 32 ms {I2} (1961Al21), 1959Ca13. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (10,11)
level_lifetime_unit: D
level_lifetime_info: ;ISO=M2
level_comment:
T$from 1968Su02. 
J$|b{+-} decay is mainly to the 2438 level with J|p=(8+,9+,10+), with no significant feeding to levels with J|p|<(9-). 1968Su02 pointed out that J|p=11- would result from configuration=|n11/2[605]~#|p11/2[505]. 
E$x=50 keV to 250 keV. From an estimate of |b- end-point energy x|<250 keV (1968Su02). Log| {Ift}|>5.0 for feeding to 2438 level gives x|>50. 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
J$E1 |g to (3)-; doubly-placed |g to 2-. (2-) in (pol d,|a) for a 590.7 level is in disagreement if the levels are the same. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$M1 |g to 1-; |g to (3)-; doubly-placed (E2) |g to 0-. 5+,(4-) from |s(|q) and A{-y}(|q) in (pol d,|a) for a 639.6 level is in disagreement if the levels are the same. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$M1 |gs to 3- and 4-; |g to (2)+. J|p=4-,(3+) from |s(|q) and A{-y}(|q) for 669.2 level in (pol d, |a) is in disagreement if the level is the same as in (n,|g). 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_uncertain: S
level_comment:
E$S(n)+E(n), S(n)=6066.79 {I11} (2021Wa16), E(n)=2 keV. 
J$probable s-wave capture in {+193}Ir g.s., J|p=3/2+. 


level_energy_unit: KEV
level_spin_parity: (0-,1,2,3-)
level_uncertain: S
level_comment:
E$S(n)+E(n), S(n)=6066.79 {I11} (2021Wa16), E(n)=24 keV. 
J$p-wave and s-wave capture in {+193}Ir g.s., J|p=3/2+. 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_uncertain: S
level_comment:
E$S(n)+E(n), S(n)=6066.79 {I11} (2021Wa16), E(n)=2 keV. 
J$probable s-wave capture in {+193}Ir g.s., J|p=3/2+ 


level_energy_unit: KEV
level_spin_parity: (0-,1,2,3-)
level_uncertain: S
level_comment:
E$S(n)+E(n), S(n)=6066.79 {I11} (2021Wa16), E(n)=24 keV 
J$p-wave and s-wave capture in {+193}Ir g.s., J|p=3/2+ 


level_energy_unit: KEV
level_comment:
E$-0.3 {I4} relative to E=112.2 (1994Ga30); 0.10 {I16} (1998Ba42) 
$d|s/d|W=26 |mb/sr {I6} (1994Ga30) 
$d|s/d|W=30 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=168 {I13} (20|'), 133 {I13} (30|'), 98 {I13} (40|'), 55 {I5} (50|') (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=43.3 {I3}, d|s/d|W=32 |mb/sr {I5} (1994Ga30) 
$d|s/d|W=24 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=138 {I11} (20|'), 118 {I14} (30|'), 89 {I12} (40|'), 50 {I5} (50|'); E(level)=43.06 {I16} (1998Ba42) 


level_energy_unit: KEV
level_comment:
L,S$ for complex of 82.3+84.3 states 
$E(level)=83.8 {I1}, d|s/d|W=192 |mb/sr {I23} for doublet (1994Ga30) 
$d|s/d|W=162 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=975 {I70} (20|'), 850 {I70} (30|'), 560 {I60} (40|'), 343 {I24} (50|'); E(level)=83.88 {I8} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=112.2, d|s/d|W=185 |mb/sr {I23} (1994Ga30) 
$d|s/d|W=173 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=955 {I60} (20|'), 685 {I60} (30|'), 555 {I60} (40|'), 333 {I23} (50|'); E(level)=112.22 {I8} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=138.3 {I4}, d|s/d|W=37 |mb/sr {I6} (1994Ga30) 
$d|s/d|W=37 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=203 {I20} (20|'), 137 {I18} (30|'), 62 {I12} (40|'), 5 (50|'); E(level)=138.4 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=148.7 {I2}, d|s/d|W=97 |mb/sr {I13} (1994Ga30) 
$d|s/d|W=115 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=610 {I40} (20|'), 430 {I40} (30|'), 340 {I40} (40|'), 193 {I17} (50|'); E(level)=148.75 {I13} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=161.0 {I1}, d|s/d|W=102 |mb/sr {I29} (1994Ga30) 
$d|s/d|W=92 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=490 {I40} (20|'), 448 {I40} (30|'), 314 {I37} (40|'), 179 {I17} (50|'); E(level)=161.14 {I13} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$189.7 {I12} (1994Ga30) 
$d|s/d|W=9 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=20 (20|'), 18 {I5} (30|'), 10 (40|'), 10 {I3} (50|'); E(level)=192.70 {I12} (1998Ba42) 


level_energy_unit: KEV
level_comment:
L,S$for the complex of 245.1+245.5 states 
$E(level)=244.1 {I4}, d|s/d|W=24 |mb/sr {I4} for doublet (1994Ga30) 
$d|s/d|W=15 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=89 {I15} (20|'), 63 {I9} (30|'), 47 {I10} (40|'), 30 {I5} (50|'); E(level)=244.4 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=254.6 {I4}, d|s/d|W=29 |mb/sr {I5} (1994Ga30) 
$d|s/d|W=22 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=106 {I16} (20|'), 77 {I11} (30|'), 54 {I11} (40|'), 37 {I6} (50|'); E(level)=255.1 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=278.9 {I3}, d|s/d|W=98 |mb/sr {I13} (1994Ga30) 
$d|s/d|W=107 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=475 {I40} (20|'), 303 {I28} (30|'), 345 {I40} (40|'), 208 {I16} (50|'); E(level)=278.74 {I12} (1998Ba42) 


level_energy_unit: KEV
level_comment:
S$for L=3 
$E(level)=296.7 {I4}, d|s/d|W=109 |mb/sr {I5} (1994Ga30) 
$d|s/d|W=181 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=1030 {I70} (20|'), 570 {I50} (30|'), 565 {I60} (40|'), 287 {I21} (50|'); E(level)=296.34 {I10} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$312.1 {I14} (1994Ga30), complex of 308.9+314.0 states 
$d|s/d|W=14 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=103 {I16} (20|'), 70 {I10} (30|'), 58 {I11} (40|'), 37 {I7} (50|'); E(level)=311.6 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
L,S$ for the complex of 337.5+337.6 states 
$E(level)=337.0 {I4}, d|s/d|W=47 |mb/sr {I9} for doublet (1994Ga30) 
$d|s/d|W=36 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=195 {I30} (20|'), 118 {I19} (30|'), 114 {I19} (40|'), 62 {I11} (50|'); E(level)=337.4 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=347.2 {I3}, d|s/d|W=89 |mb/sr {I13} (1994Ga30) 
$d|s/d|W=78 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=455 {I50} (20|'), 370 {I40} (30|'), 240 {I31} (40|'), 156 {I16} (50|'); E(level)=346.76 {I19} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=377.7 {I4}, d|s/d|W=196 |mb/sr {I26} (1994Ga30) 
$d|s/d|W=179 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=1010 {I70} (20|'), 740 {I60} (30|'), 645 {I70} (40|'), 359 {I26} (50|'); E(level)=376.76 {I11} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=7 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=20 (20|'), 18 {I8} (30|'), 16 {I7} (40|'), 11 {I5} (50|'); E(level)=393.00 {I12} (1998Ba42) 


level_energy_unit: KEV
level_comment:
L,S$ for the complex of 419.9+424.8 states 
$E(level)=422.6 {I6}, d|s/d|W=24 |mb/sr {I12} for doublet (1994Ga30) 
$d|s/d|W=30 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=306 {I23} (20|'), 204 {I19} (30|'), 145 {I24} (40|'), 87 {I8} (50|'); E(level)=422.15 {I16} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=433.6 {I15}, d|s/d|W=9 |mb/sr {I4} (1994Ga30) 
$d|s/d|W=8 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=66 {I9} (20|'), 31 {I7} (30|'), 33 {I6} (40|'), 27 {I21} (50|'); E(level)=433.9 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=467.5 {I11}, d|s/d|W=8 |mb/sr {I2} (1994Ga30) 
$d|s/d|W=5 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=33 {I5} (20|'), 28 {I5} (30|'), 23 {I7} (40|'), 17 {I4} (50|'); E(level)=467.7 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=490.1 {I12}, d|s/d|W=28 |mb/sr {I7} (1994Ga30) 
$d|s/d|W=21 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=195 {I12} (20|'), 114 {I9} (30|'), 90 {I11} (40|'), 64 {I6} (50|'); E(level)=489.55 {I18} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$from 1998Ba42. Level is not reported in 2008Ba25, although, a level at 500.3 keV, apparently different from 501.9, is reported by these authors. 
$E(level)=500.2 {I11} (1994Ga30); this could correspond to 500.3 and/or 501.9 levels in 2008Ba25 and 1998Ba42. 
$Relative d|s/d|W=75 {I8} (20|'), 41 {I6} (30|'), 34 {I6} (40|'), 22 {I7} (50|') (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=3 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=68 {I7} (20|'), 17 {I3} (30|'), 10 {I3} (40|'), 9 {I2} (50|'); E(level)=522.5 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=545.7 {I12}, d|s/d|W=20 |mb/sr {I4} (1994Ga30) 
$d|s/d|W=35 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=217 {I13} (20|'), 119 {I9} (30|'), 105 {I11} (40|'), 62 {I5} (50|'); E(level)=545.37 {I16} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=555.8 {I14}, d|s/d|W=5 |mb/sr {I2} (1994Ga30) 
$d|s/d|W=4 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=39 {I7} (20|'), 19 {I4} (30|'), 20 {I5} (40|'), 11 {I4} (50|'); E(level)=557.8 {I5} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=2 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=15 (20|'), 23 {I7} (30|'), 33 {I10} (40|'), 5 (50|'); E(level)=572.4 {I7} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=579.6 {I8}, d|s/d|W=23 |mb/sr {I5} (1994Ga30) 
$d|s/d|W=19 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=94 {I15} (20|'), 94 {I8} (30|'), 61 {I14} (40|'), 46 {I8} (50|'); E(level)=578.97 {I23} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$591.9 {I14} (1994Ga30) 
$d|s/d|W=5 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=15 (20|'), 39 {I5} (30|'), 27 {I5} (40|'), 12 {I3} (50|'); E(level)=591.9 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=11 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=48 {I10} (20|'), 64 {I6} (30|'), 44 {I7} (40|'), 25 {I3} (50|'); E(level)=605.73 {I17} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=6 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=14 {I5} (20|'), 63 {I6} (30|'), 38 {I5} (40|'), 22 {I4} (50|'); E(level)=619.9 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=640.7 {I13}, d|s/d|W=13 |mb/sr {I3} (1994Ga30) 
$d|s/d|W=8 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=38 {I5} (20|'), 74 {I7} (30|'), 54 {I6} (40|'), 28 {I10} (50|'); E(level)=639.55 {I21} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=14 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=78 {I10} (20|'), 77 {I8} (30|'), 49 {I6} (40|'), 29 {I4} (50|'); E(level)=656.42 {I22} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$668.1 {I12} (1994Ga30) 
$d|s/d|W=11 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=51 {I7} (20|'), 66 {I7} (30|'), 46 {I6} (40|'), 23 {I7} (50|'); E(level)=667.5 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=677.1 {I15}, d|s/d|W=21 |mb/sr {I4} (1994Ga30) 
$d|s/d|W=19 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=80 {I8} (20|'), 94 {I9} (30|'), 56 {I7} (40|'), 49 {I4} (50|'); E(level)=677.49 {I23} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=3 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=11 {I4} (20|'), 31 {I4} (30|'), 29 {I6} (40|'), 18 {I2} (50|'); E(level)=694.5 {I5} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=7 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=36 {I5} (20|'), 40 {I5} (30|'), 29 {I7} (40|'), 17 {I6} (50|'); E(level)=707.7 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=8 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=31 {I4} (20|'), 26 {I4} (30|'), 25 {I6} (40|'), 18 {I2} (50|'); E(level)=719.1 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=11 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=50 {I6} (30|'), 58 {I12} (40|'), 40 {I5} (50|'); E(level)=746.3 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=760.7 {I15}, d|s/d|W=17 |mb/sr {I7} (1994Ga30) 
$d|s/d|W=20 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=56 {I7} (30|'), 80 {I15} (40|'), 54 {I6} (50|'); E(level)=759.0 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$773.4 {I14} (1994Ga30) 
$d|s/d|W=8 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=41 {I6} (30|'), 23 {I6} (40|'), 32 {I4} (50|'); E(level)=772.6 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=3 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=11 {I3} (30|'), 35 {I12} (40|'), 10 (50|'); E(level)=799.7 {I8}(1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=27 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=188 {I19} (20|'), 88 {I10} (30|'), 70 {I15} (40|'), 83 {I15} (50|'); E(level)=808.7 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$E(level)=819.3 {I14}, d|s/d|W=23 |mb/sr {I7} (1994Ga30) 
$d|s/d|W=13 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=68 {I9} (30|'), 74 {I14} (40|'), 85 {I16} (50|'); E(level)=819.2 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=4 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=15 {I4} (30|'), 11 {I4} (40|'), 10 (50|'); E(level)=834.2 {I9} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=4 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=27 {I5} (30|'), 28 {I8} (40|'), 41 {I9} (50|'); E(level)=853.8 {I4} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=18 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=63 {I13} (30|'), 72 {I14} (40|'), 36 {I10} (50|'); E(level)=872.4 {I3} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=12 |mb/sr (20|') (2008Ba25) 
$E(level)=879.0 {I15}, d|s/d|W=16 |mb/sr {I4} (1994Ga30) 
$Relative d|s/d|W=45 {I12} (30|'), 38 {I11} (40|'), 52 {I12} (50|'); E(level)=879.4 {I6} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=5 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=10 {I4} (30|'), 10 (40|'), 13 {I4} (50|'); E(level)=888.00 {I14} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=6 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=34 {I5} (30|'), 28 {I8} (40|'), 21 {I6} (50|'); E(level)=897.4 {I5} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=4 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=10 (20|'), 17 {I4} (30|'), 18 {I6} (40|'), 17 {I4} (50|'); E(level)=908.2 {I6} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=2 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=10 (20|'), 17 {I3} (30|'), 10 (40|'), 19 {I4} (50|'); E(level)=921.2 {I5} (1998Ba42) 


level_energy_unit: KEV
level_comment:
E$level not reported by 2008Ba25 
$Relative d|s/d|W=10 (20|'), 20 {I6} (30|'), 12 {I4} (40|'), 7 {I3} (50|') (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=61 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=283 {I21} (20|'), 283 {I23} (30|'), 141 {I20} (40|'), 149 {I14} (50|'); E(level)=948.11 {I18} (1998Ba42) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=20 |mb/sr (20|') (2008Ba25) 
$Relative d|s/d|W=10 (20|'), 20 {I6} (30|'), 12 {I4} (40|'), 7 {I3} (50|'); E(level)=965.9 {I7} (1998Ba42), although 2008Ba25 do not compare the energies in the two studies in their Table I 


level_energy_unit: KEV
level_spin_parity: 5+,(4-)
level_comment:
L$Other possibilities: (3,5) 
$Other G{-LJ}=0.0070 for L=3, 0.0121 for L=5, 0.0096 for L=6 
$d|s/d|W=6.0 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 5+,(4-)
level_comment:
L$other possible: (3,5) 
$Other G{-LJ}=0.0032 for L=3, 0.0091 for L=5 , 0.0088 for L=6 
$d|s/d|W=3.1 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 4-,(3+)
level_comment:
L$other possible: (2,4) 
$Other G{-LJ}=0.0031 for L=2, 0.0143 for L=5, 0.0116 for L=4 
$d|s/d|W=3.1 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
T$From 2013Bi14, which digitized the data of Fig.2 of 1957Re01 displaying the decay curve of {+195}Ir and then a least-squares fit. Others: 2.8 h {I1} (1968Ho01) from an analysis of the 99keV |g ray from the decay of the first excited state in the {+195}Pt daughter, in which this |g ray was assigned only to the ground state activity in {+195}Ir; but 1968Ja06 demonstrated that this state is also populated by 11/2{+-} isomeric state in {+195}Ir, thus this value is likely too high. 2.3 h {I2} (1968Ja06) from an analysis of the 99keV, 129keV |g-decay curve measurements with semi detector (the contributions from ground state and 11/2{+-} isomeric state in {+195}Ir are considered). 2.2 h (1957Re01) from chemically extracting iridium fractions following the decay of its parent {+195}Os. 2.3 h (1952Ch18,1954Bu02). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
%B-,%IT$see {+195}Ir |b{+-} decay (3.67 h) and {+195}Ir IT decay (3.67 h). 
T$ from an analysis of the 173keV, 365keV, 433keV |g decay-curve measurements (1968Ja06,1973Ja10) .Other:4.00 h {I15} (1968Ho01) 
configuration=11/2-[505] (1978Ya03) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E from (t,|a). Other: 120 {I40} derived from Q(|b{+-},{+195}Ir g.s.)=1110 {I30} and Q(|b{+-},3.67-h {+195}Ir)=1230 {I20} 
IT decay unobserved; %IT<10 deduced from ce spectrum (1973Ja10). This branching yields B(M4)(W.u.)|<8.8 compared to 2.05 {I7}, 2.2 {I8}, and 2.35 {I19} for analogous transitions in {+193}Ir, {+195}Au, and {+197}Au, respectively 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: S
level_comment:
J supported by the |b decay to {+196}Pt 0+ g.s. ( 0+ to 0+ isospin forbidden ). 
T weighted average of 54.5 s {I20} (1968Ja06), 52 s {I2} (1967Mo10), and 50 s {I2} (1966Vo05). 


level_energy_unit: KEV
level_spin_parity: (1-)
level_uncertain: ?
level_comment:
J log| {Ift}|<6.6 from 0+. 
E there is no other |g-ray transition connecting this level. Its placement is speculative. 


level_energy_unit: KEV
level_spin_parity: (10,11-)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E from |b energies measured in 52 s and 1.40-h {+196}Ir decay. 
J supported by log| {Ift}=6.03 for |b decay to 2468-keV level in {+196}Pt. J=9,12 less likely from log| {Ift} values or from limits found for |b decay branches to levels in {+196}Pt (1968Ja06). 
T from {+196}Ir |b{+-} decay (1968Ja06). Others: 1965Bi04, 1959Ga11. 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: S
level_comment:
J From {+196}Ir adopted levels. Proposed configuration |p(1/2+(400)) + |n(1/2-(510)), Nilsson orbitals (1977Ha32). 


level_energy_unit: KEV
level_spin_parity: 1,2-
level_lifetime_unit: S
level_comment:
MOMM1$from fit to hfs with J=1 (2020Mu16). Other: +0.34 {I+5-14} for J=2. Fits with J=0 and J=3 give a larger chi squared. 
T$from fit to growth and decay curves (2020Mu16) 
$|d<r{+2}>{+191,196}=+0.16 fm{+2} {I+3-2} (2020Mu16) 
J$from fit to hfs measurement and comparison to shell model calculations (2020Mu16). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
T from |g-decay curves (1978PeZJ). Others: 1952Ch18, 1954Bu02, 1961Ho10 
Ay(|q=30|')=-0.52 {I2}; d|s/d|W(|q=30|')=340 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
%B-,%IT For B(M4)(W.u.)=3.2 {I13}. From syst of M4 transitions (h11/2 to d3/2) for 5 cases B(M4)(W.u.) ranges from 1.9 to 4.5 (1980Sc26). 
T from |g-decay curves (1978PeZJ). Others: 9.8 min {I4} (1976PeZW), 10 min {I1} (1976HiZF). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d<r{+2}>{+191,197}=+0.23 fm{+2} {I2} (2020Mu16) 
J$from the Adopted Levels of {+197}Ir in the ENSDF database. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T From 1972ScYY. Others: 8 s {I3} (1973Sz03). 8 s {I2} from time correlations between implantations and |b decay events (2014Ku23). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
E$The observed fragments are assumed to be in the ground state of {+198}Ir nuclei (2014Ku23) 
T$From time correlations between implantations and |b decay events (2014Ku23). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_uncertain: ?
level_comment:
T$The value given for the half-life of this isomer is for ions of {+198}Ir at rest, measured at the final focus of the FRS (2005Ca02). Other: 73 ns {I11} from decay curve of 116-keV transition (2011St21) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$2018Hi07 erroneously quote J|p=(0,1)- from NNDC databases. No spin-parity is assigned in the ENSDF database. 
T$measured by 2018Hi07 from decay curves of |b{+-} radiation. Half-lives measured from decay curves of |g rays were: 7.5 s {I26} for 407.2|g and 17 s {I11} for 507.3|g, which gives weighted average of 8.0 s {I25}. value is 8 s {I2} measured by 2014Ku23 (Eur. Phys. Jour. A50, 135); and 8 s {I1} in {+198}Ir Adopted Levels in the ENSDF database (Dec 2015 update). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: S
level_comment:
MOMM1$from fit to hfs with J=1 (2020Mu16). Others: fits with J=0, J=2, and J=3 give a larger chi squared. 
T$from fit to growth and decay curves (2020Mu16) 
$|d<r{+2}>{+191,198}=+0.16 fm{+2} {I+3-2} (2020Mu16) 
J$from fit to hfs measurement and comparison to shell model calculations (2020Mu16). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$3/2+ (syst,2003Au02,1997Mo25) 
T$From 2007KuZW. Others: 20 s (syst,2003Au02), >100 s (calculated,1997Mo25) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_uncertain: ?
level_comment:
T$80-390 ns quoted by 2005Ca02. The counting statistics did not permit the quantitative determination of decay half-lives. However, the recording time ranges provide constraints on the isomer half-life. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$3/2+ is predicted by 1997Mo25 
T$the half-life was deduced from position-time correlations between the implanted fragments and the subsequent |b decay (2007KuZW). Other: T{-1/2}>100 s is predicted by 1997Mo25 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_lifetime_unit: S
level_comment:
J$Tentative assignment based on the probable |b{+-} feedings to 2+ levels and the absense of any |b{+-} feeding to the 0+, 1583.1-keV level in the daughter nucleus {+200}Pt (2013Mo20); J|p=3- predicted in 2011Ji02 
T$From implant-|b{+-}(|Dt) in 2014Mo15 
CONF$Probable |p(d{-3/2}{+-1})~#|n(f{-5/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
J$ assuming spherical shape and systematics of neighboring Z=77 nuclei; shell model predictions 
T$from 2014Mo15, using Monte Carlo analysis of ion-|b|g(time) data 
CONF$|p d{-3/2}{+-1} from systematics of known Z=77 isotopes; shell model predictions 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
E$ 439.6 keV, 452.0 keV and 680.9 keV |g rays observed below the isomer (2011St21), but the ordering is unknown. Given the reported |g-ray intensities in 2011St21, 439.6|g and 452.0|g are most-likely in paralel in the decay scheme. Thus, E(level)=1132.9 keV can be expected 
T$ from sum of 439.6,452.0,680.9|g(t) in 2011St21 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$From sum of 440,452,681|g(t) in 2011St21 
$Experimental isomeric state population ratio |>3% {I2} (2011St21) 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_lifetime_unit: S
level_comment:
J$From {+202}Ir |b{+-} decay to levels with J=1 to 4 in the daughter nucleus {+202}Pt (2013Mo20); systematics of known structures in neighboring nuclei and the proposed configuration 
T$Weighted average of 11 s {I3} from implant-|b(t) in 2014Ku23 (also 2007KuZZ and 2009Ku28) and 15 s {I3} from implant-|b|g(|Dt) in 2014Mo15 
$Possible configuration=|p(d{-3/2}{+-1})~#|n(p{-1/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_lifetime_unit: US
level_comment:
E$From 311.5|g, 737.2|g, and 889.2|g assigned in 2011St21 to follow the decay of the isomer and by assuming (by the evaluator) that they are in a cascade; the evaluator associates the 655.9|g and 967.6|g (also obsrved in 2011St21) to directly depopulate the isomer. 
T$From 655.9|g(t)+737.2|g(t)+889.2|g(t) in 2011St21. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_lifetime_unit: US
level_comment:
E$From adopted levels 
T$From 655.9|g(t)+737.2|g(t)+889.2|g(t) in 2011St21 
$Experimental isomeric state population ratio=0.7% {I+2-3} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$ Assuming spherical shape and systematics in the region; shell-model predictions. The assignment is tentative. 
T$ >160 ns from time-of-flight in 2012Ku26, but the actual half-life is expected to be much longer. T{-1/2} |J 7 s estimated in 2021Ko07. Predicted T{-1/2}(|b): 43.4 s (2019Mo01, FRDM16) and 1.82 s (2016Ma12, CDFT) 
CONF$|p(d{-3/2}{+-1}) from systematics in the region; shell model predictions. The assignment is tentative. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x=200 keV {I50} estimated in 2021Ko07 
T$possibly a long-lived isomeric state; T{-1/2}>100 ns was estimated in 2021Ko07 
J$Assuming spherical shape and systematics of Z=77 (even-N) isotopes; shell-model predictions 
CONF$|p(h{-11/2}{+-1}) and spherical shape. The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$From 841|g(t) and 895|g(t) in 2011St21 
CONF$|p[(h{-11/2}{+-2}){-10{++}}(d{-3/2}{+-1})]. The assignment is tentative 
$Experimental isomeric ratio=4.7% {I+31-34} (2011St21) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$possibly a long-lived isomeric state 
CONF$ |p(h{-11/2}{+-1}) and spherical shape. The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$From 841|g(t) and 895|g(t) in 2011St21 
CONF$ |p[(h{-11/2}{+-2}){-10{++}}(d{-3/2}{+-1})]. The assignment is tentative 
$Experimental isomeric state population ratio=4.7% {I+31-34} (2011St21) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Only |b{+-} decay mode is expected. Predicted %|b{+-}n=0.01 (1997Mo25) 
E$ the observed {+204}Ir fragments assumed to correspond to the g.s. 
J$3/2+ for neutron orbital and 9/2+ for proton orbital predicted (1997Mo25) 
T$ limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by systematics value of 200 ms (2012Au07), and >100 s from theoretical calculations (1997Mo25) 
$ For production |s see figure 3 in 2012Ku26 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
E$ The observed {+205}Ir fragments in 2012Ku26 are assumed to correspond to the g.s. 
J$From systematics of single-particle structures near Z=82 
T$ >160 ns from the time-of-flight in 2012Ku26, but the actual lifetime is expected to be much longer 
CONF$|p(d{-3/2}{+-1}) and spherical shape 
$ Production |s=0.003 nb {I2} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$2019Hi06 assigned %|a|?100, as only the |a decay was observed in this work and |b decay half-life is expected to be much longer. Theory T{-1/2}(|b decay)=0.277 s (2019Mo01), T{-1/2}(|a)=0.18 ms (2019Mo01) and 0.12 ms (2022Xu04). With S(2p)=-1440 {I500} (2021Wa16), 2p-decay mode is likely, but no evidence was found for this decay mode in 2019Hi06 
J$probable unhindered |a decay with HF|?2.9 (2019Hi06) to {+161}Os, g.s. J|p=(7/2-) as in {+161}Os Adopted Levels in the ENSDF database (June 2011 update) 
T$measured by 2019Hi06 from observation of four recoil-|a-|a correlated decay chains ({+165}Pt|){+161}Os|){+157}W|){+157}Ta|){+153}Lu) and analysis by maximum likelihood method. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$Only the |a decay has been detected by 1996Bi07, 2004Ke06 and 2019Hi06. From theoretical calculations in 2019Mo01, T{-1/2}(|b)=0.2167 s implying %|e+%|b{++}|?0.4. From Gross theory of |b decay, T{-1/2}(|b)|?0.9 s (1973Ta30) implying %|e+%|b{++}=0.1 
T$from |a decay, weighted average of 1.1 ms {I2} (2019Hi06), 0.9 ms {I+3-2} (2004Ke06) and 0.7 ms {I2} (1996Bi07) 
J$probable favored |a decay to (7/2-) g.s. in {+163}Os. Possible |nf{-7/2} orbital. Additionally, (7/2-) g.s. of {+169}Pt and {+171}Pt, and 7/2- g.s. for {+175}Pt. 7/2- proposed by 2021Ko07 from systematic trend. In theoretical calculations, 2019Mo01 give 3/2- 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%|a: only |a decay observed. Gross |b decay theory (1973Ta30) predicts a partial |b decay T{-1/2}|?1 s implying %|e+%|b{++}|?0.2. 
J g.s. of even-even nucleus. 
T weighted average of 1.98 ms {I16} (2009Go16), 2.1 ms {I2} (2004Ke06), 2.0 ms {I2} (1998Ki20) and 2.0 ms {I4} (1996Bi07) from a(t). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
%A 1999Se14 report that number of {+169}Pt daughter |a's correlated with {+173}Hg decays is consistent with %|a=100 for {+169}Pt. This is consistent with gross |b decay theory prediction of a partial |b half-life of |?1 s (1973Ta30) and microscopic theory prediction of 0.26 s (1997Mo25), implying %|e+%|b{++}|?0.7 and 2.7, respectively. Only |a decay has been observed for {+169}Pt. 
J unhindered |a decay to (7/2-) {+165}Os. Supported by p emission data from {+170}Au isomers whose configurations probably include (|n f{-7/2}) orbital. 
T from 2004Ke06. Others: 13 ms {I+11-4} (2004Ke06, 6693|a), 5 ms {I3} (1996Pa01), 2.5 ms {I+25-10} (1981Ho10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T weighted average of 14.7 ms {I5} (1996Bi07) and 13.5 ms {I3} (1998Ki20). Other T{-1/2}: 6 ms {I+5-2} from |a(t) measurement (1981Ho10); 15 ms {I+16-6} (1997Uu01). 
%A Gross |b decay theory calculations predict partial |b half-life to be |?2 s (1973Ta30) and 1997Mo25 predict 0.38 s, implying %|e+%|b{++}|?0.7 or 3.6, respectively; based on this, the evaluator adopts %|a=98 {I2}. |a decay of {+170}Pt has been observed (1981Ho10,1982En03,1996Bi07), but %|a has not been measured. |e+|b{++} decay has not been observed. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J The 10+ member of the g.s. band is either the 3025 or the 3038 level; 2006Jo04 assign 10+ to 3025 in level scheme in figure 1 and in the text, but assign 10+ to 3038 in table I. 2005Jo18 assigned the 3038 level as the J=10 band member. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J The 10+ member of the g.s. band is either the 3025 or the 3038 level; 2006Jo04 assign 10+ to 3025 in level scheme figure 1 and in the text, but assign 10+ to 3038 in table I. 2005Jo18 assigned 10+ to 3038 level. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
%A Unweighted average of 83 {I3} (2010Sc02) and 96 {I5} (2004GoZZ). Only |a decay of {+171}Pt has been observed (1981De22,1981Ho10,1982En03,1997Uu01,2004GoZZ,2010Sc02). Gross |b decay theory predicts a partial |b halflife |?2 s (1973Ta30), implying %|e+%|b{++}|?2.  
%EC+%B+ From 100-%|a. 
J M1 90|g from (9/2-) 90 level; unhindered |a decay to (7/2-) {+167}Os g.s.. Same as g.s. J|p for {+169}Pt but not {+173}Pt. 
T unweighted average of 40 ms {I10} (1981De22), 43 ms {I3} (1996Pa01), 51 ms {I2} (2002Ro17), 48 ms {I1} (2010Sc02); the weighted average is 48.1 ms {I12}. Other values: >20 ms (1981Ho10), 20 ms {I6} (1982En03), 25 ms {I+11-6} (1997Uu01). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T from 2010Sc02 based on time differences between a recoil implant and {+171}Pt |a decay, correlated within 960 ms of a recoil and also within 2.73 s and 8 s, respectively, of |a decay from {+167}Os and {+163}W. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: NS
level_comment:
T from text and fig. 16 of 2010Sc02, based on time difference between recoil implantation in double-sided Si detector and detection of 90|g and 323|g in the clover and planar detectors and ce in PIN diodes. The 4 ns uncertainty shown in fig. 14c of 2010Sc02 is presumed to be a misprint; this presumption was confirmed in an e-mail communication from C. Scholey to B. Singh on Feb 5, 2010. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%A From 2004GoZZ. Other: 94 {I+6-32} (1984ScZQ). 
%EC+%B+ From 100-%|a. 
J g.s. of even-even nucleus. 
T 97.6 ms {I13} (2003Da06) from 6316|a(t). Other data: 104 ms {I7} (2002Ro17), 96 ms {I3} (1996Pa01), 0.110 s {I20} (1993ToZY), 0.09 s {I1} (1982En03), 0.12 s {I1} (1981De22), 0.10 s {I1} (1975Ga25), 0.12 s {I5} (1984ScZQ). The weighted average of all data is 97.8 ms {I12}. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
T from 6232|a(t) (2004GoZZ). The weighted average of all data (325 ms {I20} (1981De22), 360 ms {I20} (1982En03), 290 ms {I60} (1992ToZX), 376 ms {I11} (1996Pa01), 370 ms {I13} (2002Ro17), 382 ms {I2}, 400 ms {I11}, 392 ms {I15}, 411 ms {I19} (2004GoZZ), 430 ms {I40} (2009An20)) is 386 ms {I3}. 
%|a: weighted average of 84 {I6} from ratio of intensities of |a group for {+173}Pt daughter and for {+177}Hg parent in the same spectrum (1979Ha10) 83 {I14} (1996Pa01) and 82 {I6} (2004GoZZ) yields %|a=83 {I4} for |a which constitutes 96% {I1} of total {+173}Pt |a decay (2004GoZZ). 
J |a decay to (5/2-) {+169}Os is probably unhindered. Based on systematics, 2003Au02 suggest J|p=5/2-. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T weighted average (|h{+2} /|n=1.8) of 0.80 s {I5} (1981De22), 0.90 s {I1} (1982En03), and 0.890 s {I20} (1996Pa01). 
%A Weighted average (|h{+2} /|n=4.2) of 67% {I6} (1996Pa01) and 83% {I5} (1979Ha10). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
$2004Go38 indicates that this level might belong to another structure, due to the nonrotational behaviour of the 463 transition, which feeds this level. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_comment:
J$Based on unhindered (HF=1.31 {I7}) 6286 {I4} keV |a transition from {+179}Hg to the g.s. of {+175}Pt, deduced |a-decay reduced widths, information of the daughter {+175}Pt and grand-daughter {+175}Os nuclei (2002Ko09). 
%A$From 1979Ha10 (a%=4.8 {I8}, 55 {I5}, and 4.7 {I1}.0 of 6038|a, 5964|a, and 5831|a respectively). Other: 56 {I5} (1996Pa01 5960|a), consistent with measured value of 57.3 {I11} for I|a(6038 keV) + I|a(5964 keV) (1986Ke03). 
T$Weighted average of 2.4 s {I3}(1996Pa01), 2.56 s {I10}(1979Ha10), 2.54 s {I15}(1979Ha10), and 2.52 s {I8}(1973Ga08). 
 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
T$from |a|g correlated decay curves (2014Pe02). As per e-mail reply of Feb 25, 2014 from P. Peura, value of 2.43 s quoted on page 5 and elsewhere in paper is incorrect. See also Erratum: Phys Rev C 89, 049902 (2014) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1973Ga08. Other values: 6.7 s {I7} (1996Pa01), 6.0 s {I5} (1966Si08), 11.0 s {I2} (1982Bo04). 
%|a from weighted average of 42 {I4} (1996Pa01), 42 {I4} (1970Ha18), and 38 {I3} (1979Ha10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T From {+180}Hg |a decay [1993Wa03]. 
E Reported in {+180}Hg |a decay, but an expected 179|g from this level was not observed in {+176}Au |b{++}/|e decay (1999Da18). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
%A$From singles spectra in 1979Ha10. Others: 5.2 {I18} (1982HeZM), 9.0 {I8} (1970Ha18). %|e+%|b{++} was not measured directly, but it was deduced from %|a 
J$Favored |a decay to the J|p=5/2- ground state of {+173}Os. J|p systematics. Properties of the rotational band supports J|p=5/2- 
T$Weighted average of 11 s {I2} (1970Ha18), 11 s {I1} (1982Bo04) and 9.8 s {I4} (1993Me13). Others: 6.6 s {I10} (1966Si08) and 7.0 s {I6} (1968De01). 
CONF$ |n5/2[512] Nilsson configuration. Based on the established J|p, the observed in-band properties, such as alignment and g{-K}-g{-R} values. 
$E|a=5527 {I6}, I|a=88 {I7}, E|a=5435 {I10}, I|a=12 {I1} (1979Ha10), E|a=5535 {I20} (1982HeZM); E|a=5525 {I20}, I|a=66 {I6} and 5485 {I20}, I|a=34 {I3} (1970Ha18); E|a=5510 {I10} (1966Si08); E|a=5530 {I25} (1968De01); E|a=5510 {I3} (1982Bo04). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
J$94.8|g E1 to 5/2-. 
T$From |g|g(t) spectrum produced by gating on the 94.8 keV transition (below the isomer) and several in-band transitions (above the isomer) in {+149}Sm({+32}S,4n|g) (1990Dr03). 
CONF$ |n 7/2[633] (i{-13/2}) Nilsson configuration. Based on the established J|p, the observed in-band properties, such as large alignment, delayed first band crossing, g{-K}-g{-R} values and configuration systematics. The assignment is consistent with the measured transition strength for the E1 94.8 keV |g ray and systematics of similar transitions in the N=99 {+175}Os and {+173}W isotones. See also 1990Dr03. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$147.5|g to 5/2-; favored |a decay from the {+181}Hg g.s. (J|p=1/2-); J|p systematics; band properties. 
T$From |a|g(t) time-difference spectrum produced by gating on E|a=6006 keV and E|g=147.7 keV in {+181}Hg |a-decay (1979Ha10). 
CONF$|n1/2[521] Nilsson configuration. Based on the established J|p, the observed in-band properties, such as large signature splitting (decoupled band) and rotational alignment 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
$E|a=5527 keV {I6}, I|a=88 {I7}, E|a=5435 keV {I10}, I|a=12 {I1} (1979Ha10). Others: E|a=5535 keV {I20} (1982HeZM); E|a=5525 keV {I20}, I|a=66 {I6} and 5485 keV {I20}, I|a=34 {I3} (1970Ha18); E|a=5510 keV {I10} (1966Si08); E|a=5530 keV {I25} (1968De01); E|a=5510 keV {I3} (1982Bo04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T Weighted average of 20 s {i1} (2000Ko16), 22 s {i2} (1993Me13), and 21 s {i1} (1982Bo04). 
%A From I|a(5440|a)=7.5% {i3} (1980Sc09) and I|a(5284|a)/I|a(5440|a)=0.028 {i10} (1970Ha18). 
Isotope shift: |D<r{+2}> =-0.529 {i16} fm{+2} relative to {+194}Pt (2000Le40,1999Sa40,1999Ro28). 
Deformation variation: |D<|b{+2}> =0.0261 {i14} relative to {+194}Pt (2000Le40,1999Ro28); deformation parameter (<|b{+2}>){+1/2}=0.216 {i5} (1999Sa40,1999Ro28). 
RMS charge radius, <r{-0}{+2}>{+1/2}=5.372 {i7} fm (2004An14) 


