# LEVEL

level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J Based on the electron conversion coefficient values for the 483.0 keV transition. This assignment is also supported by the angular correlation measurements of the 483.0-170.4 keV cascade (1999Da18) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J Based on the K electron conversion coefficient for the 711.5 keV transition which indicates an M1 or E0 component (1999Da18) 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
B(E1,636.3)/B(E2,241.5)=9.2 {i20} 10{+-7} b{+-1}, and B(E1,1047.9)/B(E2,241.5)=0.38 {i11} 10{+-7} b{+-1} (2000Ko16) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J Based on the electron conversion coefficient values for the 483.0 keV transition. This assignment is also supported by the angular correlation measurements of the 483.0-170.4 keV cascade 


level_energy_unit: KEV
level_spin_parity: (3)
level_comment:
J Assignment suggested by the angular correlation of the 830.9-170.4 keV cascade; however, an E0 component is also possible for the 830.9 keV transition, which would indicate a J|p=2+ for the 1001.3-keV level. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J Based on the K electron conversion coefficient for the 711.5 keV transition which indicates an M1 or E0 component 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T From adopted levels 
This level decays via two main |a transitions with an 7.5 {i3} % branching ratio (2000Ko16) to levels in {+174}Os: a) E(|a)=5447 {i4} keV, I{-|a}=96.5 {i29} %, to the 0+ g.s.; and, b) E(|a)=5289 {i8} keV, I{-|a}=3.5 {i4} %, to the 2+ level (2000Ko16). A reduced |a width |d{+2}=155 {I+17-20} keV for the 5447 keV |a transition was deduced by 2000Ko16. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from DDCM coincidence analysis gated on 427|g (2021He13). Other: 298 ps {I35} from two-state Bateman equation analysis (2021He13). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
MOMM1 From LASER resonance ionization spectroscopy; result also reported in 1999Sa40, 1999Ro28, 2000Le40, 2000Sa58 and 2001Sa44. 
|D<r{+2}>({+194}Pt,{+179}Pt)=-0.335 {I21} (1999Le52; also reported in 1999Ro28, 1999Sa40 and 2000Le40). 
<r{+2}>{+1/2}(charge)=5.392 {I6} (2004An14). 
T from 1993Me13. Others: 54 s {I4} (1982Bo04) and 33 s {I2} (1966Si08). See also the comment above on Q(|a). 
%|a: weighted average of 0.27 {I4} (1970Ha18) and 0.21 {I4} (1980Sc09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 60 s {I3} (1993Me13), 50 s {I5} (1966Si08), and 53 s {I4} (1968De01). 
%A$from 1966Si08. 
$|d<r{+2}>=-0.360 {I11} relative to {+194}Pt (2000Le40) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 153|g to 0+; band member 
MOMM1$from IPAC (1998Br33). Other: +0.70 {I16} from PDCO (extracted from Fig 19 of 2002Ro36 by evaluator). 


level_energy_unit: KEV
level_spin_parity: (5-,4+)
level_comment:
J$858|g to 6+, 1204|g to 4+; systematics of negative parity bands in neighboring Os isotopes favors the J|p=5- assignment 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Q(transition)=6.41 {I27} (2016Ch13) 
T$ (2016Ch13). This value can be compared with 22.9 ps {I28} in {+180}Pt Adopted Levels in the ENSDF database, where RDM value is taken from 2006Wi15 (Phys. Rev. C74, 024302). 1990De04 (Nucl. Phys. A507, 472) reported 52 ps {I10} from RDM. Compiler obtains an unweighted average of the three measured values as 37 ps {I8} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from convolution method (2018Mu02). Other: 291 ps {I21} from generalized centroid difference method (2018Mu02), but with large peak-to-background ratio in the analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from RDDM (2018Mu02). Other: 25.0 ps {I42} from generalized centroid difference method (2018Mu02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
%A$from a comparison of the number of {+180}Hg |a and {+180}Pt |a decays, neglecting the small %|a=0.6% branch for {+180}Au and taking %|a for {+180}Hg as 48 % {I2} (2020Cu02). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
%A 1966Si08 deduce %|a=0.06 from the measured relative I|a in {+181}Pt and {+182}Pt decays by assuming that the ratio of the maximum production cross section for ({+16}O,6n), ({+16}O,7n) and ({+16}O,8n) is the same for all Yb target isotopes used, and that %|a({+182}Pt)=0.023 {I+23-12}; value revised by evaluator to achieve consistency with %|a({+182}Pt)=0.031 {I8} adopted in 1998Ak04. 
|D<r{+2}>({+194}Pt,{+181}Pt)=-0.251 {I15} (laser spectroscopy, 1999Le52). 
MOMM1 From laser spectroscopy. 
T weighted average of 51.0 s {I25} (1966Si08) and 56 s {I5} (1993Me13). 
<r{+2}>{+1/2}=5.400 fm 4 for {+181}Pt 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: NS
level_lifetime_info: ;ERR=GT
level_comment:
J |D|p=yes 171|g from |p=+ 287; (M1) 23|g to 5/2- 94; band assignment. 
T from 1992Sa03; based on absence of coin between |g's feeding this level and the |g deexciting it. 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J 31|g from (7/2)+ 287, |g's to (7/2)- 117 and (5/2)- 167 imply J|p=(5/2,7/2,9/2-); |D|p=no 403|g from |p=- 659; band assignment. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
J 11|g from (7/2)+ 287; E1 41|g to (9/2)- 235; band assignment. 
T from |g-t in ({+40}Ar,3n|g) (1990De03). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$(<r{+2}>){+1/2}(rms charge radius)=5.3969 fm {I41} (2013An02,evaluation) 
$ |d<r>{+2}({+194}Pt-{+182}Pt)=-0.279 fm{+2} {I10} (1999Ro28) 
%A$from 1995Bi01. Others: 0.023 (1963Gr08,1966Si08) 
T$weighted average of 2.6 min {I1} (|g timing,1972Fi12), 3.0 min {I2} (|a timing,1966Si08) and 2.5 min {I5} (1963Gr08) 
T$ 2009Ni11: theory for half-life 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$perturbed |g|g(|q) from oriented nuclei (PDCO method) in high-spin reactions (2002Ro36,2002Ro12). 
J$E2 |g to 0+ 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$perturbed |g|g(|q) from oriented nuclei (PDCO method) in high-spin reactions (2002Ro36,2002Ro12). 
J$|DJ=2, E2 |g to 2+ 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$ |DJ=2 |g to 14+; band assignment 
T$effective half-life; side feeding correction could not be applied 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$1999Da18 suggest (0) from |g|g(|q), although other spins cannot be ruled out. Positive parity suggested by (E2) to 2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 409 ps {I71} (2012Gl01,RDM) and 491 ps {I30} (2012Wa16,RDM) 
$Q{-t}=5.77 eb {I17} (2012Wa16) for T{-1/2}=491 ps {I30} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$weighted average of 31 ps {I4} (2012Gl01,RDM) and 32.9 ps {I20} (2012Wa16,RDM) 
$Q{-t}=6.37 eb {I19} (2012Wa16) for T{-1/2}=32.9 ps {I20} 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$weighted average of 5.1 ps {I4} (2012Gl01,RDM) and 5.41 ps {I35} (2012Wa16,RDM) 
$Q{-t}=7.45 eb {I24} (2012Wa16) for T{-1/2}=5.41 ps {i35} 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.9 ps {I4} (2012Gl01,RDM) and 2.36 ps {I21} (2012Wa16,RDM) 
$Q{-t}=6.88 eb {I27} (2012Wa16) for T{-1/2}=2.36 ps {i21} 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.90 ps {I21} (2012Gl01,RDM) and 1.18 ps {I14} (2012Wa16,RDM) 
$Q{-t}=6.95 eb {I28} (2012Wa16) for T{-1/2}=1.18 ps {i14} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=563 ps {I12} (2021Ha23). Authors compared their result with their earlier measurement (2012Gl01) of |t=590 ps {I102}, and with |t=709 ps {I43} in 2012Wa16 from Notre Dame (Phys. Rev. C 85, 057302), using RDDS method with a plunger in both the studies. Note a large difference in the lifetimes from 2021Ha23 and 2012Wa16, the latter being higher by |?25%. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=41 ps {I5} (2021Ha23). Authors compared their result with their earlier measurement (2012Gl01) of |t=44 ps {I5}, and |t=47.5 ps {I29} in 2012Wa16 from Notre Dame (Phys. Rev. C 85, 057302), using RDDS method with a plunger in both the studies. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
MOMM1 From LASER resonance ionization mass spectroscopy; {+195}Pt reference standard. Others: +0.51 {I3} (1990Hi08), +0.52 {I3} (1992Hi07). 
<r{+2}>{+1/2}(charge)=5.403 fm {I4} (2004An14). 
|D<r{+2}>({+194}Pt,{+183}Pt)=-0.216 {I8} (1999Le52,1999Ro28,1999Sa40). Other: -0.17 {I5} (1992Hi07). 
%A From 1995Bi01; based on comparison of I|a with intensity of {+183}Pt |e+|b{++} decay, taking into account the 43 s component of that decay. Other %|a: 0.0013 (1963Gr08); expected to be correct within a factor of three, but authors may not have corrected for possible contribution to |e+|b{++} intensity from 43 s isomer (1995Bi01). 
MOMM1$from LASER spectroscopy (1999Le52,1999Ro28,1999Sa40), relative to |m({+195}Pt). Other: +0.521 {I27} from resonance ionization mass spectroscopy and pulsed-LASER induced desorption (1992Hi07). 
J J=1/2 from hfs spectrum (1992Hi07); |m consistent with that calculated for 1/2- 1/2[521] level (1999Le52,1999Ro28, 1999Sa40). Bandhead for band with decoupling parameter a=+0.85, typical of |n 1/2[521] configuration in this mass region; 
T from 1963Gr08. Other value: 7.0 min {I25} (1966Si08). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
MOMM1,MOME2$from LASER resonance ionization mass spectroscopy. Sternheimer correction applied to Q. 
MOMM1 {+195}Pt reference standard. Others: 0.96 {I8} (1992Ro21), 1.03 {I8} (1992St16); from static nuclear orientation with |g detection. 
Other Q: +3.7 {I3} (2000SaZZ) 
|D<r{+2}>({+194}Pt,{+183}Pt)=-0.106 {I8} (1999Le52,1999Ro28,1999Sa40). 
%A |a decay not observed. An |a branch to the 7/2- 7/2[514] {+179}Os level at 145.4 keV would have HF<1, unless %|a<3x10{+-4}. 
MOMM1,MOME2$from LASER spectroscopy (1999Le52,1999Ro28,1999Sa40); |m relative to |m({+195}Pt), sternheimer correction applied. 
T from 1979Vi02. 
J M3 35|g to 1/2- g.s.. 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2,11/2-)
level_comment:
J 165|g to (7/2)- 472; 393|g to (11/2)+ 244; weak branch from (5/2)- in |e decay (log| {Ift}|?7.2) makes J>7/2 unlikely. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_comment:
J E2+M1 597|g to 5/2-, uncertain 693|g to 1/2- g.s.; log| {Ift}=6.2 from (5/2)- in |e decay; 394|g to 7/2- 299. 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J E2+M1 607|g to 5/2-. Note that if the 702|g were to deexcite this level, as suggested by 1989Ro21, this band assignment would be incorrect. 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)-
level_comment:
J M1+E2 506|g to to 7/2- 299; M1+E2 521|g to 9/2- 314. log| {Ift}=6.7 from (5/2)- in |e decay for weak branch makes J=9/2 unlikely. 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)-
level_comment:
J M1+E2 526|g to 7/2- 299; 477|g to (5/2)- 348. log| {Ift}=6.8 from (5/2)- in |e decay for weak branch makes J=9/2 unlikely. 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J M1+E2 829|g to (9/2)- 150; 631|g to (5/2)- 348; M1 944|g to 7/2- 35; log| {Ift}=6.9 for weak branch from (5/2)- in |e decay. 


level_energy_unit: KEV
level_spin_parity: (+)
level_comment:
J (E2) 615|g to (7/2)+ 375 allows J=(3/2 to 11/2); log| {Ift}=7.2 for weak branch from (5/2)- in |e decay favors J|<(7/2). 


level_energy_unit: KEV
level_spin_parity: (GE7/2)
level_comment:
J 623|g to (7/2)+ 375; 755|g to (11/2)+ 244 suggests J|p=(7/2+,9/2, 11/2+). log| {Ift}=7.0 for weak branch from (5/2)- in |e decay favors J=(7/2). 


level_energy_unit: KEV
level_comment:
J 685|g to (7/2)- 373 implies J=(3/2 to 11/2); log| {Ift}=7.2 from (5/2)- inconsistent with J=9/2, 11/2, but branching may be too weak to be reliable. 


level_energy_unit: KEV
level_comment:
J 753|g to (7/2)- 373, 595|g to (9/2)+ 532 suggests J|p=(5/2+, 7/2,9/2,11/2-); log| {Ift}=6.9 from (5/2)- for weak branch in |e decay disfavors J=(9/2,11/2). 


level_energy_unit: KEV
level_comment:
J 1698|g to (9/2)- 150, possible 1813|g to 7/2- 35 imply J|p=(5/2-,7/2,9/2,11/2-). log| {Ift}=6.5 for weak branch from (5/2)- in decay renders J=9/2 or 11/2 very unlikely. 


level_energy_unit: KEV
level_comment:
J 1681|g to 7/2- 299 suggests J=(3/2 to 11/2). log| {Ift}=6.7 in |e decay for weak branch from (5/2)- favors J=(3/2,5/2,7/2). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
|D<r{+2}>({+194}Pt,{+184}Pt)=-0.221 {I7} (1999Le52,2000Le40), -0.232 {I26} (1992Hi07). 
<r{+2}>{+1/2}(charge)=5.403 {I4} (2004An14). 
T from 1972Fi12. Others: 1963Gr08 (20 min {I2}), 1966Si08 (16.5 min {I20}), and 1969Ha03 (18 min {I2}). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 From g=0.28 {I3} (1996St12; IPAC). 
T from |g|g(t) in |e decay (1972Fi12). Other T{-1/2}: 403 ps {I15} from RDM in {+154}Sm({+34}S,4n|g),{+172}Yb({+16}O,4n|g). 
J E2 163|g to 0+ g.s.. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J M1+E2(+E0) 1002|g to 6+ 798; 1364|g to 4+ 436; 569|g to 8+ 1231; J=6 member of established band built on 0+ 492 level. 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_comment:
I(|g+ce) imbalance at level: 2.6 {I6}. 
Level included in |g band in fig. 1 of 1992Xu02 but the J=4 and 5 |g band members are assigned as the 1028 and 1307 levels, respectively, in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
T$from multiscaling of delayed |g's (1970FiZZ). Other values: 72 min (1960Al20), 60 min (1965Qa01). 
J$observed |e decay to high-spin states in {+185}Ir suggests J|p=9/2+. Nilsson orbital assignment based on energy systematics of 9/2[924] in {+183}Os, {+181}W, {+179}Hf, and {+177}Yb (N=107 isotones). Measured |m=-0.83 {I1} (1989Du01, 1988Ro20) and -0.774 {I14} (2000Le40) agree with theory for 9/2+,9/2[624]. 
%|a=0.0050 {I20}, if 4444 keV {I10} |a particle originates from {+185}Pt |a decay (70.9 min) (1991Bi04). 
MOMM1 Nuclear magnetic resonance on oriented nuclei (1990Ed01). Other values: -0.723 {I11} from laser spectroscopy (2000Le40), -0.83 {I1} from resonance ionization mass spectroscopy (1989Du01, 1988Ro20); 0.772 {I15}, static (low temperature) nuclear orientation (1988Ed02, 1990Ed01). Isotope shift (1990Hi08, 1992Hi07). 
MOME2 Resonance ionization mass spectroscopy (not corrected for Sternheimer effect) (1989Du01, 1988Ro20). Other values: Q=+4.37 {I26} from Q({+185}Pt)/Q({+191}Pt)=-4.46 {I13} from nuclear magnetic resonance on oriented nuclei (1998Hi08); Q=+3.73 {I17} from laser spectroscopy (2000Le40), Q=+4.5 {I1} from nuclear magnetic resonance on oriented nuclei (1993HaZU); Q=+3.4 {I5} from static (low temperature) nuclear orientation (1988Ed02, 1990Ed01). 
<r{+2}>{+1/2}=5.4155 fm 29 for {+185}Pt 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: MIN
level_lifetime_info: ;ISO=M
level_comment:
T from multiscaling of delayed |g's (1970FiZZ). 
J Nilsson orbital assignment based on the similarity with energies observed for 1/2[521] in {+183}Pt and {+181}Pt. Observed |e decay to low-spin states in {+185}Ir supports J|p=1/2-. Measured |m=+0.540 {I9} (1992Hi07) and +0.503 {I5} (2000Le40) agree with theory for J|p=1/2- 
%IT<2 from B(M4)(W.u.)<10 (RUL) for a possible transition to g.s. 
%|a=0.0010 {I4}, if 4444 keV {I10} |a particle originates from {+185}Pt |a decay (33.0 min) (1991Bi04). 
MOMM1 Laser resonance ionization mass spectroscopy (1992Hi07). Other value: +0.503 {I5} from laser spectroscopy (2000Le40). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$77.7|g M1+E2 to 1/2-, see comment on 200.9 level. 
T$From time distribution of electron-|g coincidences (1996Om01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$310|g E1 to 9/2+ g.s., and M1-M1 cascade through 200.9 level to to the 3/2- 181.1 level uniquely establishes J|p=7/2- and 5/2- for the 310.6 and 200.9 levels, respectively. 
T$From time distribution of electron-|g coincidences (1996Om01). 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
J 207|g M1 to 3/2-; band head of 1/2[510] rotational band. J|p=3/2- for the 435.4 level and J|p=5/2- for the 488.4 level and the band structure support J|p=(1/2)- for this state. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J 389.8|g M1+E2 to 5/2-. |g|g(|q,H) (1985Va07). 7/2-,1/2[510] was assigned by 1988Ro13, based on the analogy with |g-ray decay pattern between the 1/2[510] and 1/2[521] rotational bands in {+183}Os. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
|D<r{+2}>({+194}Pt,{+186}Pt)=-0.200 fm{+2} {I6} (1999Le52). 
%A From 1963Gr08; observed |a peak tentatively assigned to the decay of {+186}Pt based on T{-1/2}. Authors state that {+187}Pt is another possibility for the origin of this peak. Intensity was estimated to be accurate within a factor of 2. 
T$From 1991Be25. Weighted average of data 2.10 h~{I5} (1991Be25), 2.0 h~{I1} (1972Fi12), 2.2 h~{I2} (1963Gr08), and 2.5 h~{I5} (1955Sm42 -labeled {+187}Pt) yields 2.09 h~{I4}. Other values: 2.9 h (1960Al20), 2.8 h (1965Qa01), 3.03 h (1963Gr22). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 From g-factor=0.27 {I3} (2020StZV, 1996St12, transient field), assuming g[{+192}Pt, 2+]=0.30 {I1} (1995An15). 
J E2 |g to 0+ 
T$Unweighted average of 220~ps~{I17} ({+36}S,4n|g) and 260~ps~{I10} ({+186}Au |e Decay). 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
J M1+E2 430|g to 3- 1408; 882|g(|q,H,t) allows J=2 or 4, and J=4 requires the smaller M2 admixture. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J 1092 keV |g transition to 6{++} level in ground state band, no decay to 4{++} and 3{+-} states, rules out 4, 5, 6{++}. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J |DJ=0,1 251|g to 10+; 766|g to 8+; based on similar DCO ratios for all transitions connecting this level's band to other bands, (|a,6n|g) favor J=10 over J=9. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
J M1+E2 |g to (7-) 1952; systematics of even-even Pt isotopes. 
T from 243|g-1074.8|g(t) in (|a,6n|g). Other: 4.6 ns in ({+16}O,4n|g). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J gammas to 10+ and 12+ but not to 8+; based on similar DCO ratios for all transitions connecting this level's band to other bands, 1987He29 favor J=12 over J=11. 
T from centroid shift in (|a,6n|g). 


level_energy_unit: KEV
level_spin_parity: (13-)
level_comment:
J$|DJ=0,1 856|g to 12+ 2336; 367|g to 14+ 2825; absence of |g to any 10+ levels; 1990He19 (|a,6n|g) favor |p=- due to D transitions from the next two members of this band (3531, 3984) to the g.s. band. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J 2+ from 192|g(|q,H,t) (1985Va07). 
T from 1972Fi12 
g-factor, relative to g[{+192}Pt, 2+]=0.30 {I1}, is from transient field IMPAC measurements of 1996St12. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
MOMM1$weighted average of -0.397 {I5} (1989Du01-resonance ion spectroscopy), 0.408 {I8} (1988Ed02, 1990Ed01-nuclear orientation NMR), -0.399 {I8} (2000Sa58-Laser spectroscopy), -0.43 {I2} (1992Hi07-Laser resonance ionization mass spectroscopy). 
MOME2$weighted average of -1.00 {I7} (1992Hi07-Laser spectroscopy- Sternheimer shielding corrected), and -0.98 {I5} (2000SaZQ-Laser spectroscopy-Sternheimer shielding corrected). Others: -1.13 {I5} (1989Du01-resonance ion spectroscopy), -1.3 {I3} (1990Ed01-nuclear orientation with |g-detection), and -1.08 {I6} (2000Sa58-Laser spectroscopy). 
J$spin from atomic beam (1975Ru06). Parity from Schmidt diagram. 
T$from 1973Se13. Other references: 2.2 h (1960Al20), 2.0 h {I4} (1960Ba43), 3 h {I1}, 2.5 h {I5} (1961Kr02), 2.6 h {I3}, 2.0 h {I3} (1962Gr27), 3.1 h {I5} (1963Gr22), and 2.1 h (1965Qa01). 
|D<r{+2}>({+187}Pt,{+194}Pt)=-0.175 {I20} (1992Hi07); <r{+2}>{+1/2}({+187}Pt)=5.407 {I4} fm (2004An14) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$From the analysis of experimental and theoretical A{-2} values for the 914.7|g-235.7|g and 235.7|g-181.1|g cascades. J|p=1/2- was ruled out from the cascade analysis in {+187}Au |e decay (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J From the cascade analysis of 706.1|g-609.4|g, 706.1|g-374.4|g, and 374.4|g-185.8|g including the experimental and theoretical A{-2} values The cascade analysis of 1189.4|g-213.6|g also leads to the same assignment ({+187}Au |e decay - 1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$115.9|g to 3/2- state. J|p=5/2- was ruled out from the analysis of 590.6|g-181.1|g correlation, constraining the range of measured mixing ratio and the experimental and theoretical A{-2} values in {+187}Au |e decay (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J From the cascade analysis of 706.1|g-609.4|g, 706.1|g-374.4|g, and 374.4|g-185.8|g including the experimental and theoretical A{-2} values ({+187}Au |e decay - 1992Ro15). 260.6|g E0+M1+E2 to 3/2-. 
T$from {+187}Au |e decay 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$From the cascade analysis of 1189.4|g-213.6|g including the experimental and theoretical A{-2} values ({+187}Au |e decay - 1992Ro15). 262.7|g E0+M1+E2 to (5/2-) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$247.4|g M1+E2 to 3/2- state. A possible 3/2- assignment is ruled out from the analysis of 833.0|g-247.4|g and 247.4|g-185.8|g cascade correlations including the experimental and theoretical A{-2} values ({+187}Au |e decay - 1992Ro15). 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
J$498.3|g (M1+E2) to (3/2-,5/2-). 1979Be51 and 1983Gn01 ({+187}Au |e decay) expected E0 component (%E0|?60 (1979Be51)) for the 498|g due to high |a(K)exp value (|a(K)exp>0.58-1979Be51, |a(K)exp=0.8 {I3}-1983Gn01). Either of the E0 component or abnormal M1 conversion in the mass region for this element is possible, however 1992Ro15 states it is difficult to determine unambiguously. Without a specific J|p assignment for this level, (M1+E2) is assigned by the evaluator. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J Cascade analysis of the 706.1|g-609.4|g, 706.1|g-374.4|g, and 374.4|g-185.8|g including the experimental and theoretical A{-2} values supports the J|p=1/2+ assignment ({+187}Au |e decay-1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$From the analysis of experimental and theoretical A2 values for the 914.7|g-235.7|g and 235.7|g-181.1|g cascades. J|p=1/2- was ruled out from the cascade analysis (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J From the cascade analysis of 706.1|g-609.4|g, 706.1|g-374.4|g, and 374.4|g-185.8|g including the experimental and theoretical A2 values. The cascade analysis of 1189.4|g-213.6|g also leads to the same assignment (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$115.9|g to 3/2- state. J|p=5/2- was ruled out from the analysis of 590.6|g-181.1|g correlation, constraining the range of measured mixing ratio and the experimental and theoretical A{-2} values (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J From the cascade analysis of 706.1|g-609.4|g, 706.1|g-374.4|g, and 374.4|g-185.8|g including the experimental and theoretical A2 values (1992Ro15). 
T$From 2004Om01 (148 ps 6{-syst} 3{-stat}): delayed |g|g coincidence - average of 142 ps 3 (direct deconvolution) and 154 ps {I4} (reconvolution). Other: 163 ps {I6} (1996Om01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J From the cascade analysis of 1189.4|g-213.6|g including the experimental and theoretical A2 values (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J The 369.2|g and 375.1|g with |a(K)exp values of 0.04 {I2} and 0.04 {I3}, respectively, from this level have dominant E2 contribution. The 369.2|g feeds 7/2- state and 375.1|g feeds (1/2,3/2)- state. Assuming a 914.6|g E1 feeding from the 1341-keV level J|p=1/2+ to this level, J|p=3/2- is assigned. 1983Gn01 assigned J|p=5/2- for this state. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$247.4|g M1+E2 to 3/2- state. A possible 3/2- assignment is ruled out from the analysis of 833.0|g-247.4|g and 247.4|g-185.8|g cascade correlations including the experimental and theoretical A2 values (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J Cascade analysis of the 706.1|g-609.4|g, 706.1|g-374.4|g, and 374.4|g-185.8|g including the experimental and theoretical A2 values supports the J|p=1/2+ assignment (1992Ro15). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J From a cascade analysis of the 1189.4|g-213.6|g including the experimental and theoretical A2 values (1992Ro15). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$not reported in {+173}Yb({+18}O,4n|g). 264.0|g placed from 3116 keV and 264.1|g placed from 3839 keV levels. Not adopted. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_uncertain: ?
level_comment:
E not reported in {+173}Yb({+18}O,4n|g). 379.0|g placed from 3992 keV (J=37/2) and 379.1|g from 2070 keV (J|p=25/2-). Not adopted. 
J From 1975De24. 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
J$Placement of the 597|g in the rotational band structure indicates J|p=29/2+ for this level, although no J|p is shown in the decay scheme (1975De39). J|p=(27/2+) is assigned by the evaluator comparing the placement of adopted 596.3(7) keV |g-ray from the 2091.6 keV (J|p=27/2+) adopted level. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
%A$Weighted average of 2.2|*10{+-5} {I5} (1979Ha10), 2.8|*10{+-5} {I5} (1978El11) and 3.0|*10{+-5} {I6} (1963Gr08). Other: 5.0|*10{+-5} {I+50-25} (1963Ka17) 
T$Weighted average of 10.5 d {I10} (1963Ka17), 10.2 d {I3} (1963Gr08), 10.0 d {I3} (1955Sm42), and 10.3 d {I4} (1954Na25) 
$E|a=3870 keV {I50} (1963Ka17), 3930 keV {I10} (1963Gr08), 3915 keV {I10} (1978El11) and 3905 keV {I15} (1979Ha10) 
$|D<r{+2}>({+190}Pt-{+188}Pt)=-0.040 fm{+2} {I8} (1988Le22). |D<r{+2}>({+194}Pt-{+188}Pt)=-0.188 fm{+2} {I7} (1992Hi07,1990Hi08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$265.63|g E2 to 0+ 
T$Weighted average of 65 ps {I5} (1995AnZQ) and 67 ps {I+4-3} (2017Ro07), both using the Dopler-shift recoil distance method. Other: 72 ps {I13} using 265.63|b|g(t) in 1972Fi12 
MOMM1$From g=+0.29 {I4} using the transient-field integral PAC technique (1996St12). |w|t(2{++})=160 mrad {I10} and |t(2{++})=93 ps {I7} were used 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$202.6|g E2 to 5-; 583.7|g (E1) to 6+; band assignment 
T$From 203ce(K)(t) in 1979Ri08. Other: 0.621 ns {I38} from 203ce(K)(t) in 1978Ti02, but the line is weak and contaminations cannot be excluded (see 1978Ti02 for details). A long-lived component of 14 ns {I2} was also reported to the 203ce(K) line in 1978Ti02, but not in 1979Ri08 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
J$689.3|g E2 to 7-; band assignment 
T$From 1979Ri08, where a delayed component is observed for the electron line associated with the 689-keV |g ray 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J$838.0|g (E2) to 8+. Assigned J|p=(9+) in 1988KaZW, but no value was given in 1979DaZN. The relatively lower population of this level, compared to the 10+ level at 2664 keV, would be consistent with J|p=8+. The alternative J|p=6+ assignment can be excluded since such a level won't be populated in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
J$108.1|g E2 to 10+ 
T$From 108-, 147- and 373ce(K)(t) in 1979Ri08. 
CONF$|n(i{-13/2}{+-2}) rotational-aligned state. The proposed shape isomer interpretation in 2014Mu12 seems to be incorrect. It is based on the observed reduced B(E2) values from 2002Si10 and comparison with Cranked-model calculations, but the values quoted in 2002Si10 are incorrect. See 2015Ko14 for detailed interpretation. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 65 ps {I5} (1995AnZQ) and 67 ps {I+4-3} (2017Ro07), both using the Dopler-shift recoil distance method 
G$from |g|g(|q,H,t) in 1996St12 using the transient-field integral PAC technique. |w|t(2{++})=160 mrad {I10} and T{-1/2}(2{++})=65 ps {I5} were used 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$From 203ce(K)(t) in 1979Ri08. Other: 0.621 ns {I38} from 203ce(K)(t) in 1978Ti02, but the line is weak and contaminations cannot be excluded (see 1978Ti02 for details). A long-lived compnent of 14 ns {I2} was also reported to the 203ce(K) line in 1978Ti02, but not in 1979Ri08, which may suggest that the line is contaminated 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
T$Observed longer-lived component in the electron line associated with the 689-keV |g ray in 1979Ri08 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J$Assigned (9+) in 1988KaZW, but no value given in 1979DaZN. The relatively lower population, compared to the 10+ level at 2664 keV, would suggest a lower spin 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
T$From 108-, 147- and 373ce(K)(t) in 1979Ri08. 
CONF$|n(i{-13/2}{+-2}) rotational-aligned state. The proposed shape isomer interpretation in 2014Mu12 seems to be incorrect. It is based on the observed reduced B(E2) values from 2002Si10 and comparison with Cranked-model calculations, but the values quoted in 2002Si10 are incorrect. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
$RMS charge radius <r{+2}>{+1/2}=5.4060 fm {I35} (2013An02 evaluation) 
J$spin from atomic beam (1975Ru06), parity from M1+E2 |g from 3/2- 
T$from 1964Le07. Other values: 12.1 h {I15} (2000Mo05,2000Zi04), 11 h (1975Ru06), 10.9 h (1967Na02), 10.9 h {I10} (1963Th07), 11.1 h {I4} (1961An02), 11.5 h (1960Po07), 10.5 h {I10} (1955Sm42) 
MOMM1$laser resonance ionization mass spectroscopy (1989Du01,2000SaZZ). Other values: -0.440 {I8} (1992Hi07, laser ionization mass spectroscopy), 0.439 {I9} (1985Ed05,1985Ed03,nuclear magnetic resonance on oriented nuclei), 0.433 {I9}, (1985Oh05, nuclear magnetic resonance on oriented nuclei), 0.42 {I3} (1980Be27, static nuclear orientation with gamma detection). 
MOME2$laser resonance ionization mass spectroscopy (1992Hi07,1989Du01). Others: -1.03 {I5} (1989Du01, laser spectroscopy), -1.21 {I6} from Q({+189}Pt)/Q({+191}Pt)=1.235 {I8} (1998Hi08) and Q({+191}Pt)=-0.89 {I5} (1988Ro20,1989Du01); -1.27 {I3} (1993HaZU, NMR-ON), -1.1 {I2} (1992Hi07), -0.7 {I3} (1985Ed05) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$L(d,p)=6,5 and systematics of odd-A Pt isotopes. 
T$from 1976Pi03 in {+188}Os(|a,3n|g),{+191}Ir(p,3n|g) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$in (|a,3n|g) this was assigned 11/2-. In ({+18}O,5n|g) this is tentatively assigned as (13/2-) based on a DCO measurement and expectation of yrast levels being more strongly populated in that reaction 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J$in (|a,3n|g) this was assigned 15/2-. In ({+18}O,5n|g) this is tentatively assigned as (17/2-) based on a DCO measurement and expectation of yrast levels being more strongly populated in that reaction 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
E$observed in {+188}Os(|a,3n|g) (1978DaZC), expected to be populated either directly by |e decay or indirectly by |g-ray deexcitation of higher levels. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
$%|e|b{++}=?. Double-beta decay mode is allowed, but only the lower limits of the half-life of this decay mode have been measured. 
$Evaluated rms charge radius=5.4108 fm {I30} (2013An02) 
$Evaluated |d<r{+2}>({+194}Pt,{+190}Pt)=-0.137 fm{+2} {I2} (2013An02) 
$|D<r{+2}>({+194}Pt-{+190}Pt)=-0.132 fm{+2} {I8} (1992Hi07). See also 1992Ki30 for |D<r{+2}> measurement 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$from B(E2)=1.82 {I9}, weighted average of 1.82 {I9} (1995An15, Coul. ex.); 2.5 {I+13-6} (1972Fi12, from (ce)|g(t) in |e decay); 1.75 {I22} (1966Gr20, Coul. ex., uncertainty from 2001Ra27 evaluation). 2016Pr01 evaluation gives B(E2)=1.854 {I90}, and corresponding T{-1/2}=61.1 ps {I+31-28} 
MOMM1,BE2$transient-field method in Coul. ex. (1995An15,1995AnZQ) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$E2, |DJ=2 |g to 5-; |DJ=1 |g to 6+ 
$Possible configuration=|n3/2[512]~#|n11/2[615] 
T$ce(t) for 167|g in (|a,4n|g). Weighted average of 0.77 ns {I14} (1979Ri08) and 0.80 ns {I5} (1978Ti02). Others: |g(t): <1 ns (1976Hj01), |?1.2 ns (1976Cu02) 
MOMM1$integral perturbed angular correlation (IPAC) method (2006Le06) 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: NS
level_comment:
J$(E2), |DJ=(2) |g to 8-; |g to 9- 
MOMM1$integral perturbed angular correlation (IPAC) method. Measured value is from 2006Le06. Other measurement: +0.09 {I8} in (|a,2n|g) (2001Ko41) 
$Configuration=|n9/2[505]|n11/2[615] (2001Ko41) from consistency measured and calculated g factor 
T$219|g(t) in (|a,2n|g) and (|a,4n|g). Weighted average of 48 ns {I5} (1976Hj01) and 47 ns {I6} (1976Cu02) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
J$E2, |DJ=2 |g to 10+ 
T$weighted average of 1.27 ns {I9} (1978Ti02, ce(t) for 191|g) and 1.52 ns {I9} (1979Ri08, ce(t) for 123|g and 191|g) in (|a,4n|g). Others: |g(t): <1 ns (1976Hj01), |?1.5 ns (1976Cu02) 
MOMM1$integral perturbed angular correlation (IPAC) method (2006Le06) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
J$(3-) from E1 |g to 2+ and |g to 4+, but (M1) |g to 0+ suggests (1+). Note that all the gamma-ray placements are questionable, thus no J|p is assigned for the 2797 level. 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: NS
level_comment:
T$from 219.2|g(t) (1976Hj01) 
G$from |g(|q,H) of 219|g, 447|g and 591|g 
$Configuration=|n9/2[505]|n11/2[615] (2001Ko41) from consistency measured and calculated g factor 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$from (ce for 167|g)(t). Weighted average of 0.77 ns {I14} (1979Ri08), 0.80 ns {I5} (1978Ti02). Other: |?1.2 ns from |g(t) (1976Cu02) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
T$weighted average of 1.27 ns {I9} (1978Ti02, ce(t) for 191|g) and 1.52 ns {I9} (1979Ri08, ce(t) for 123|g and 191|g). Other: |?1.5 ns from |g(t) (1976Cu02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$g({+190}Pt)/g({+194}Pt,first 2+)=0.96 {I3} (1995An15) 
BE2$other: 1.75 {I22} (1966Gr20 quoted 2.05 {I25}, relative to 1.94 for first 2+ state in {+194}Pt. This value has been adjusted using adopted B(E2)=1.642 {I22} for {+194}Pt (2001Ra27)) 
J$from the Adopted Levels 
T$from B(E2)|^ 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for 2|n2K decay to {+190}Os g.s. Others: |>5.2|*10{+14} y for 2|nKL decay to {+190}Os g.s., |>9.8|*10{+15} y for 2|n2|e decay for decay to the 2+, 186.7 of {+190}Os, |>2.3|*10{+16} y for 2|n2|e decay to the 2+, 558 of {+190}Os, |>5.2|*10{+16} y for 2|n2|e decay to the 0+, 911.8 of {+190}Os, |>1.9|*10{+16} y for 2|n2|e decay to the 2+, 1114.7 of {+190}Os, |>2.5|*10{+16} y for 2|nKN decay to the 1326.9 level of {+190}Os, |>4.7|*10{+16} y for 0|n2K decay to the g.s. of {+190}Os, |>4.6|*10{+16} y for 0|nKL decay to the g.s. of {+190}Os, |>3.2|*10{+16} y for 0|n2L decay to the g.s. of {+190}Os, |>7.6|*10{+15} y for 0|n2|e decay to the 2+, 186.7 of {+190}Os, |>1.9|*10{+16} y for 0|n2|e decay to the 2+, 558 of {+190}Os, |>4.8|*10{+16} y for 0|n2|e decay to the 0+, 911.8 of {+190}Os, |>1.6|*10{+16} y for 0|n2|e decay to the 2+, 1114.7 of {+190}Os, |>2.5|*10{+16} y for Res. 0|nKN decay to the 1326.9 level of {+190}Os, |>4.9|*10{+16} y for Res. 0|nLM decay to the 1382.4 level of {+190}Os, |>2.9|*10{+16} y for 2|n|e|b decay to the g.s. of {+190}Os, |>2.9|*10{+16} y for 0|n|e|b decay to the g.s. of {+190}Os, |>2.8|*10{+16} y for 2|n|e|b decay to the 2+, 186.7 of {+190}Os, |>2.8|*10{+16} y for 0|n|e|b decay to the g.s. of {+190}Os 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: D
level_comment:
$No |a (<5|*10{+-6}%) (1963Ka17). 
Nuclear charge radius: <r{+2}>{+1/2}=5.411 fm {I3} (2004An14). 
J atomic beam (1975Ru06). Parity from L=1 in (p,d). 
T Unweighted average of 2.861 d {I9} (unweighted average of discrepant raw data in 2000Mo05, nat Pt(|g,n), HPGe detector, dead-time correction - supersedes 2.862 d {I7} (2000Zi04)) and 2.802 d {I13} (1994Pa46, {+191}Ir(p,n), chemical separation, HPGe detector, pulser method, uncertainty transformed to 1 |s level). Others: 3.00 d {I2} (1949Wi08), 3.2 d {I2} (1953Sw20), 2.90 d {I5} (1954Co29), 3.0 d {I3} (1955Sm42), 2.8 d {I3} (1962Li12), 2.9 d {I2} (1963Gr22), 2.9 d {I2} (1970Ba56), 2.71 d {I6} (1970Sc20). 
MOMM1 From 2019StZV, 1988Ro20, 1989Du01 - Resonance ionization mass spectroscopy. Other values: -0.494 {I8} (1992Hi07) - resonance ionization mass spectroscopy; 0.500 {I10} (1985Ed05), 0.499 {I10} (1985Oh05), and 0.506 {I11} (1981La25) radiative detection of NMR; -0.46 {I+14-4} (1980Be27) static (low temperature) nuclear orientation and Mossbauer detection of oriented nuclei (1987Be36). 
MOME2 From 2016St14 (1992Hi07 - resonance ionization mass spectroscopy). Other values: -0.89 {I5} (1988Ro20 - Resonance ionization mass spectroscopy); -0.98 {I5} (1989Du01 - resonance ionization mass spectroscopy (no Sternheimer correction)); -0.64 {I26} (1985Ed05 - radiative detection of NMR). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J L=(3) in (p,d),(d,t), component of 1+(3) in the g.s.; 283.9|g M1+E2 from (5/2)- and 442.3|g M1 transition from 451.8 (L=1(+4) in (p,d)) can be used to exclude 7/2 for this level for J|p(451.8)=(3/2)-. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J 1/2,1/3 from L=1 in (p,d). 263.09|g E2 from J|p(293.45)=(5/2)- favors 1/2, while gamma transitions from J|p(253.9)=(7/2,5/2)- favors 3/2-. 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
J L=5,6 in (p,d); 48.37|g M2 from (13/2)+, 91.11|g E2 to (5/2,7/2)-. 
T from {+191}Pt IT decay (104 |ms) (1976Pi03). 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: US
level_comment:
J L=6 in (p,d) and 6,5 in ({+3}He,|a), 322.0|g E2 from (17/2)+ at 471. 
T from {+191}Pt IT decay (104 |ms). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J L=1,3 in (p,d) yields (1/2,3/2,5/2,7/2)- and 126.9|g M1+E2 from (5/2)- and 408.2|g M1+E2 from (1/2)- may be used to exclude 1/2,5/2,7/2. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J L=1+(4) in (p,d), corresponding to 453.8 keV and this level; 421.4|g M1 to (1/2)- and 442.3|g M1 to (5/2)-; for 453.8 keV level 147.5|g M1 to (9/2)+ and 280.4|g E2 to (11/2)+. Therefore, in (p,d), L=1 for 451.8 level, and L=(4) for 453.8. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J see comment for 451.8 keV level spin assignment. 7/2,9/3 from L=4 in (p,d) and 9/3 may be excluded for 280.4|g E2 to 173.4 keV level for J|p(173.4)=(11/2)+ 


level_energy_unit: KEV
level_spin_parity: (21/2)-
level_comment:
J$see comment on J|p for 2826.5 keV, (33/2)- level. A{-2}=+0.44 {I11} and A{-4}=-0.11 {I8} for 430.4|g in ({+11}B,p5n|g) is consistent for a |DJ=0 transition. 


level_energy_unit: KEV
level_spin_parity: (25/2)-
level_lifetime_unit: NS
level_comment:
J 164.3|g E2 to (21/2-). see comment on J|p for 2826.5 keV level. 
T from ce-|a(t) in (|a,3n|g) (1978Ti02). 


level_energy_unit: KEV
level_spin_parity: (33/2)-
level_comment:
J From 3317.3 keV (35/2)+ level to 989.5 keV (19/2)+, the sequence: 490.6|g D(+Q); 701.0|g (stretched E2); 579.6|g stretched (E2); 164.3|g E2, and 392.0|g (E1) to (19/2)+, defines that 490.6|g is E1 and all transitions are stretched and therefore the intermediate-level spins are (33/2)-, (29/2)-, (25/2)-, and (21/2)-. 


level_energy_unit: KEV
level_spin_parity: (35/2)+
level_comment:
$Configuration=Bef. 
J |p=+ (see 3452.0 keV level); 376.6|g D(+Q) to (33/2)+; yrast level from intensity of feeding. 


level_energy_unit: KEV
level_spin_parity: (39/2)+
level_comment:
J 151.0|g and 263.0|g D (E1 in ({+11}B,p5n|g)) to |p=- levels and 134.5|g (E2) to 3317 keV level gives |p=+ for this and 3317 levels; yrast level from intensity of feeding. 


level_energy_unit: KEV
level_spin_parity: (25/2)-
level_comment:
T{-1/2}=1.07 ns {I6}, from direct measurement of conversion electrons relative to cyclotron beam bursts (1978Ti02). 


level_energy_unit: KEV
level_spin_parity: 25/2(-)
level_lifetime_unit: NS
level_comment:
T from 1978Ti02 (direct measurement of conversion electrons relative to cyclotron beam bursts). Other value: 1.5 ns {I4} (1977Sa01). 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
S assuming J|p=3/2-. 
Doublet; for L=(4) component, C{+2}S=0 to 0.30 assuming J|p=7/2+ (1980Ka19). 1978Be09 assigned L=1+(3); L=(4) is compatible with level properties from {+191}Au |e decay. 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: US
level_comment:
T Weighted average of 95 |ms {I5} (1976Pi03 - 91|g(t)), 107 |ms {I3} (1967Co20 - X-ray(t), 90.8|g(t)), and 111 |ms {I22} (1968Io01). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T{-1/2}(|a)>6x10{+16} y (specific activity measurements, 1966Ka23). T{-1/2}(|a)>1.3x10{+17} to {+188}Os(2+, 155) and T{-1/2}(|a)>2.6x10{+17} to {+188}Os(4+, 478) (2011Be08). Others: 1956Po16, 1961Pe23, 1963Gr08. Calculated value: 9.05x10{+22} y (2011Qi12; density-dependent cluster model). 
<r{+2}>{+1/2}(charge)=5.418 {I9} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 Weighted average of following data after adjustment for consistency with adopted T{-1/2}: +0.559 {I45} if T{-1/2}=43.0 ps (IPAC; 1989Ra17, from 1975Ka42), +0.574 {I34} if T{-1/2}=44.4 ps (IPAC, 1992Al21 and 1992Bo20), +0.636 {I34} if T{-1/2}=43.0 ps (transient field IPAC, 1992Br03), +0.594 {I34} if T{-1/2}=43.0 ps (transient field IPAC, 1995An15). 
MOMM1 T CORRECTED VALUES: 0.550 44, 0.583 35, 0.626 33, 0.584 33. 
MOME2 Coulomb excitation reorientation (1989Ra17, from 1987Gy01). Other value: +0.62 {I6} (Coulomb excitation reorientation, 1989Ra17 from unpublished report referenced in 1987Gy01). 
J E2 |g to 0+. 
T deduced from B(E2) in Coulomb excitation and adopted |g-ray properties. Other value (Coulomb excitation): 48.5 ps {I5} (Doppler-shift recoil-distance measurements, 1977Jo05). Other values ({+192}Ir |b{+-} decay (73.829 d)): 27 ps {I4} (|g|g(t), 1962De14), 35 ps {I3} (|g|g(t), 1966Sc06), 34 ps {I5} (|gce(t), 1970Be08), 42.8 ps {I15} (|b|g|g(t), 1973Sm01), 33 ps {I4} (cece(t), 1976Bu20). Other: 1965Bu06 (<29 ps). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$weighted average of +0.72 {I14} (IPAC, 1989Ra17 from 1975Ka42) and +0.56 {I9} (transient field IPAC, 1992Br03). 
J E2 |g to 0+. 
T |b|g|g(t) in {+192}Ir |b{+-} decay (73.829 d) (1973Sm01). Other values ({+192}Ir |b{+-} decay (73.829 d)): 24 ps {I13} (cece(t), 1965Bu06), 20.1 ps {I21} (|gce(t), 1970Be08), 26.0 ps {I26} (cece(t), 1976Bu20). Other value (Coulomb excitation): 31 ps {I6} (deduced from B(E2)). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1 From transient field IPAC (1992Br03; relative to {+194}Pt(328) or {+196}Pt(356)). Other: +1.6 {I11} (IPAC, 1989Ra17; datum of 1969Ke11 recalculated for consistency with adopted T{-1/2}). 
B(E4)=0.041 from (|a,|a'). 
J E2 468|g to 2+; g.s. band member. 
T Doppler-shift recoil-distance measurements in Coulomb excitation (1977Jo05). Other values ({+192}Ir |b{+-} decay (73.829 d)): 11.8 ps {I21} (|b|g(t) and |b|g|g(t), 1966Sc06), 5 ps {I4} (cece(t), 1975Aw01), 13 ps {I10} (cece(t) and |bce(t), 1976Bu20), 6.0 ps {I17} (|bce(t), 1978Bu02). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J M1+E2 136|g to 4+ 785; M1+E2 208|g to 2+ 612. 
T |bce(t) in {+192}Ir |b{+-} decay (73.829 d) (1978Bu02) (if T{-1/2}(612.5 level)=26.5 ps {I15}). Other values ({+192}Ir |b{+-} decay (73.829 d)): 26 ps {I4} (cece(t) and |bce(t), 1976Bu20), <24 ps (cece(t), 1965Bu06). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J E2 581|g to 4+ 785; g.s. band member. 
T Doppler-shift recoil-distance measurements in Coulomb excitation (1977Jo05). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J E1+M2 593|g to 4+ 785; E1(+M2) 1062|g to 2+ 316. 
T deduced from B(E3) in Coulomb excitation and adopted |g-ray properties. 


level_energy_unit: KEV
level_spin_parity: (7)-
level_lifetime_unit: NS
level_comment:
J E2 134|g to (5)- 1384; band assignment. 
T |g|g(t) in {+190}Os(|a,2n|g), {+192}Os(|a,4n|g) (average value). 
MOMM1 Based on g-factor=+0.48 {I12} in (|a,2n|g) from IPAD. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J L(p,t)=0. Consistent with E2 1313|g to 2+ 317; however |a(K)exp for 1017|g to 2+ 612 exceeds |a(K)(M1). 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
J 1429|g to 2+ 612; 1257|g to 4+ 785; log| {Ift}=9.1 from 1-. M1 1114|g from |p=- 3155; M1 917|g from |p=- 2958. However, |a(K)exp favors E2 for 1257|g to |p=+ 612. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J E1 2130|g to 0+ g.s.; 752|g to 3- 1378. However, multipolarities of 1517|g and 1813|g may not be consistent with that of 2130|g. 


level_energy_unit: KEV
level_spin_parity: (10)-
level_lifetime_unit: NS
level_comment:
J M1 |g to (9)- 2103; bandhead assignment, with probable configuration |n 9/2[505]+|n 11/2[615], consistent with measured g-factor and analogous structure in {+190}Os (2006Le06). 
T weighted average of 250 ns {I30} (1976Cu02) and 310 ns {I30} (1976Hj01) from |g|g(t) in {+190}Os(|a,2n|g), {+192}Os(|a,4n|g) and 235 ns {I47} from fragment-|g|g(t) in {+198}Pt({+136}Xe,X|g) using 317|g-468|g pair as double |g-ray gate (2004Va03, 2004Re11). 
MOMM1 Based on g-factor=-0.0012 {I10} in (|a,2n|g) from IPAD. Other: 0.10 {I6} from g-factor=0.010 {I6} from 2001Ko41. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J E1 1941|g to 2+ 317; E1 1336|g to 3+ 921; log| {Ift}=7.4 from 1-. However, adopted J|p implies M2 multipolarity for 2257|g. 


level_energy_unit: KEV
level_spin_parity: (12)+
level_lifetime_unit: NS
level_comment:
J E2 105|g to (10)+ 2519; band structure. 
T in-beam direct timing of conversion electrons in {+190}Os(|a,2n|g), {+192}Os(|a,4n|g) (1978Ti02). Other values from (|a,xn|g): 3.5 ns {I5} (1976Cu02), 2.6 ns {I5} (1976Hj01). 
MOMM1 From g-factor=-0.18 {I9} (2006Le06) in (|a,2n|g) from IPAD. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T |g|g(t); weighted average of 2.1 ns {I4} (1976Cu02), 2.0 ns {I3} (1976Hj01), and 1.65 ns {I25} (1978Ti02, beam-ce(t)). 
g-factor=+0.48 {I12} (2006Le06, 2006Le44) from IPAD, using 134|g, 153|g, 183|g, 599|g (corrected for feeding from 10- isomer) and 581|g, 468|g, 317|g (corrected for feeding from 10- and 12+ isomers). 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: NS
level_comment:
T |g|g(t); average of 250 ns {I30} (1976Cu02) and 310 ns {I30} (1976Hj01). 
g-factor=-0.0012 {I10} (2006Le06, 2006Le44) from IPAD, using 208|g, 446|g, 585|g. Other: 0.010 {I6} (2001Ko41); discrepant but possibly superseded by datum from 2006Le06 (one author common to both 2006Le06 and 2001Ko41). 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
T in-beam direct timing of delayed conversion electrons (1978Ti02). Other values: 3.5 ns {I5} (1976Cu02), 2.6 ns {I5} (1976Hj01). 
g-factor=-0.18 {I9} (2006Le06, 2006Le44) from IPAD, using 105|g, 501|g, 653|g. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 2.00 {I4} (1970Br26), 2.10 {I12} (1971Mi08), 1.89 {I3} (1977Ro16), and 1.833 {I20} (1987Gy01). Others: 1966Gr20 (2.3 {I3}, relative to 1.94 {I20} for {+194}Pt(0+ to 2+)); 1984Mu19 (1.77 {I5}, relative to 1.620 {I15} for {+194}Pt(0+ to 2+)). 
T deduced from B(E2) and adopted |g-ray properties. Other value: 48.5 ps {I25} (Doppler-shift recoil-distance measurements, 1977Jo05). 
g-factor({+192}Pt)/g-factor({+194}Pt, 328)=1.00 {I4} (1995An15), 1.08 5 (1992Br03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 0.020 {I3} (1970Br26, relative to 1.65 {I2} for {+194}Pt(0+ to 2+)) and 0.013 {I2} (1977Ro16). 
T from B(E2) and adopted |g-ray properties. 
g-factor({+192}Pt)/g-factor({+194}Pt, 328)=0.95 {I10} (1992Br03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T Doppler-shift recoil-distance measurements (1977Jo05). 
g-factor({+192}Pt)/g-factor({+194}Pt, 328)=0.94 {I15} (1992Br03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
B(E3): from 1977Ro16; collective strength suggests octupole vibration character. 
E from 1977Ro16. 
T deduced from B(E3) and adopted |g-ray properties. 


level_energy_unit: KEV
level_comment:
$|s(5=1.0 
d|s/d|W (|mb/sr)=7.4 {I4} at 5|', 6.8 {I3} at 17.5|', 4.5 {I3} at 30|' (2010Il03). 
Other E: 2140 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=0.5 
d|s/d|W (|mb/sr)=1.9 {I2} at 5|', 3.4 {I2} at 17.5|', 1.0 {I2} at 30|' (2010Il03). 
Other E: 2153 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=1.0 
d|s/d|W (|mb/sr)=6.1 {I4} at 5|', 5.7 {I2} at 17.5|', 5.9 {I3} at 30|' (2010Il03). 
Other E: 2166 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=0.2 
d|s/d|W (|mb/sr)=0.8 {I1} at 5|', 2.7 {I2} at 17.5|', 0.9 {I1} at 30|' (2010Il03). 
Other E: 2188 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=1.1 
d|s/d|W (|mb/sr)=5.1 {I3} at 5|', 4.3 {I2} at 17.5|', 4.0 {I2} at 30|' (2010Il03). 
Other E: 2204 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=0.6 
d|s/d|W (|mb/sr)=2.5 {I2} at 5|', 3.7 {I2} at 17.5|', 4.6 {I2} at 30|' (2010Il03). 
Other E: 2271 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=0.8 
d|s/d|W (|mb/sr)=8.3 {I4} at 5|', 9.5 {I4} at 17.5|', 8.6 {I3} at 30|' (2010Il03). 
Other E: 2308 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=0.7 
d|s/d|W (|mb/sr)=0.7 {I2} at 5|', 0.9 {I2} at 17.5|', 0.6 {I1} at 30|' (2010Il03). 
E 2330 {I3} (1979De25) may be for 2321+2343 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=0.8 
d|s/d|W (|mb/sr)=2.1 {I2} at 5|', 2.4 {I2} at 17.5|', 3.1 {I3} at 30|' (2010Il03). 
E 2358 {I2} (1979De25) may be for 2350+2366 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=4.0 
d|s/d|W (|mb/sr)=1.2 {I2} at 5|', 0.3 {I1} at 17.5|', 0.5 {I2} at 30|' (2010Il03). 
E 2389 {I2} (1979De25) may be for 2386+2394 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=0.4 
d|s/d|W (|mb/sr)=0.5 {I1} at 5|', 1.1 {I1} at 17.5|', 1.2 {I2} at 30|' (2010Il03). 
E 2411 {I2} (1979De25) may be for 2403+2415 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=0.4 
d|s/d|W (|mb/sr)=1.8 {I3} at 5|', 3.9 {I4} at 17.5|', 1.9 {I3} at 30|' (2010Il03). 
E 2428 {I2} (1979De25) may be for 2420+2436 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=0.8 
d|s/d|W (|mb/sr)=3.0 {I3} at 5|', 3.7 {I2} at 17.5|', 2.2 {I2} at 30|' (2010Il03). 
Other E: 2450 {I2} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=1.3 
d|s/d|W (|mb/sr)=3.0 {I3} at 5|', 2.3 {I2} at 17.5|', 2.4 {I2} at 30|' (2010Il03). 
E 2486 {I2} (1979De25) may be for 2478+2491 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=2.2 
d|s/d|W (|mb/sr)=1.1 {I2} at 5|', 0.5 {I1} at 17.5|', 0.5 {I1} at 30|' (2010Il03). 
E 2506 {I3} (1979De25) may be for 2500+2512 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=0.6 
d|s/d|W (|mb/sr)=1.8 {I3} at 5|', 2.9 {I4} at 17.5|', 2.5 {I4} at 30|' (2010Il03). 
Other E: 2526 {I3} (1979De25). 


level_energy_unit: KEV
level_comment:
$|s(5=1.7 
d|s/d|W (|mb/sr)=1.6 {I2} at 5|', 0.9 {I2} at 17.5|', 0.9 {I2} at 30|' (2010Il03). 
E 2662 {I3} (1979De25) may be for 2653+2674 doublet. 


level_energy_unit: KEV
level_comment:
$|s(5=0.9 
d|s/d|W (|mb/sr)=1.9 {I2} at 5|', 2.1 {I2} at 17.5|', 1.8 {I2} at 30|' (2010Il03). 
E 2695 {I3} (1979De25) may be for 2684+2703 doublet. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
g-factor: from IMPAC measurement assuming T{-1/2}=44.3 ps. Others: 0.296 {I22} (1970Be08, |g(|q,H,t)). 
T{-1/2} data from {+192}Ir |b{+-} decay (73.829 d): 27 ps {I4} (|b|g|g(t), 1962De14), 35 ps {I3} (|g|g(t), 1966Sc06), 34 ps {I5} (|gce(t), 1970Be08), 42.8 ps {I15} (|b|g|g(t), 1973Sm01), 33 ps {I4} (ce-ce(t), 1976Bu20). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
g-factor: from |g(|q,H,t). 
T from |gce(t) (1973Sm01). Other values: 24 ps {I13} (cece(t), 1965Bu06), 20.1 ps {I21} (|gce(t), 1970Be08), 26.0 ps {I26} (cece(t), 1976Bu20). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T{-1/2} data from {+192}Ir |b{+-} decay (73.829 d): 11.8 ps {I21} (|b|g(t), 1966Sc06), 5 ps {I4} (cece(t), 1975Aw01), 13 ps {I10} (cece(t), 1976Bu20), 6.0 ps {I17} (|bce(t), 1978Bu02). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T from |bce(t) (1978Bu02), assuming T{-1/2}(612.5 level)=26.5 ps {I15}. Other values: 26 ps {I4} (cece(t), 1976Bu20), <24 ps (cece(t), 1965Bu06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (10)-
level_lifetime_unit: NS
level_comment:
T (target-like recoil fragments)-|g(t) (2004Va03,2004Re11); 317|g-468|g pair used as double |g-ray gate. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured isotope shift |d|n({+194}Pt,{+192}Pt)=-1.43 GHz {I27} (2017Hi05) 
$Measured |d<r{+2}>({+194}Pt,{+192}Pt)=-0.084 fm{+2} {I18} (2017Hi05) 
$Deduced <|b{-2}{+2}>{+1/2}=0.150 {I6} (2017Hi05) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: Y
level_comment:
J L=0 in {+195}Pt(p,t). 
T weighted average of 49 y {I6} (1971Ra18) and 64 y {I20} (1971Ho17) others: 1953Sw20 (no value reported), 1969Ho14 - partial half-life for L capture: 620 y {I250}, 
MOMM1 Resonance ionization mass spectroscopy (1992Hi07) 
Isotope shift: |D<r{+2}>=-0.047 fm{+2} 7 (relative to {+194}Pt) (1992Hi07) 
|% <r{+2}>=5.420 fm {I3} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
MOMM1 x-ray detection of nuclear magnetic resonance (1985Sc15,1986Sc04); negative sign suggested by systematics. 
J M4 |g to 5/2- 14.3 level 
T from IT decay (1949Wi08) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J L=1 in {+194}Pt(p,d), (d,t) 
Possibly same as the 522.5 level seen in {+193}Au |e decay (17.65 h) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E from {+195}Pt(p,t) 
J L=2 in {+195}Pt(p,t); the level at 1188 seen in {+194}Pt(p,d) is a doublet with L=1 for at least one member of doublet. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
T from 1949Wi08; however, they saw also a 170|g and an 1.5 MeV |g, obviously from some impurity. Other values: 4.5 d {I2} (1953Sw20), 3.35 d {I10} (1954Co29), 3.5 d {I4} (1955Br41), 4.4 d {I2} (1957Ew34). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T$(ce)(ce)(t) with metallic gold source; T{-1/2} is 4% longer when measured with a gold chloride source (1968Ma51). See 1977Do07 for a discussion of this and related phenomena. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
Part of a unresolved doublet with a stronger L=3, C{+2}S=0.11 level (probably the 728 level seen by 1978Be09) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Decay modes from {+193}Pt Adopted Levels in the ENSDF database (March 2017 update) 
E,T$from {+193}Pt Adopted Levels in the ENSDF database, according to which the isomer decays to the 1/2- g.s. through 135.50|g, M4 |) 12.63|g, M1+E2 |) 1.64|g, M1 |g cascade, forming a sequence of 149.78, 13/2+; 14.28, 5/2-; 1.64, 3/2-; 0.0, 1/2- levels. 


level_energy_unit: KEV
level_spin_parity: 25/2(-)
level_lifetime_unit: NS
level_comment:
T$measured by 2019Wa22 using centroid-shift method. Other: 3.2 ns {I3} in {+193}Pt Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$absence of hyperfine splitting (1935Fu06) consistent with J=0. 
$<r{+2}>{+1/2}=5.4236 fm {I25} (2013An02 evaluation). 
$|D<r{+2}>({+192}Pt,{+194}Pt)=0.052 fm{+2} {I5}, average of 0.051 fm{+2} {I5} (1988Le22) and 0.053 fm{+2} {I5} (1987Ne09). 
$|D<r{+2}>({+194}Pt,{+196}Pt)=0.054 fm{+2} {I5}, from 0.054 fm{+2} 5 (1988Le22) and 0.055 fm{+2} {I5} (1987Ne09). Others: 1992Hi07, 1988Bo31. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$328.5|g E2 to 0+. Also L(p,p')=L(p,t)=2 from 0+. 
T$from B(E2)=1.649 {I15} in Coulomb excitation. Uncertainty of 1% seems to be statistical only. Evaluators have assumed an uncertainty of 4% in deducing level half-life and B(E2)(W.u.). Others: 45.0 ps {I24} from recoil-distance method (RDM) in Coulomb excitation , 51 ps {I7} from |G{-|g} in (|g,|g') (1972Sh38), 35.0 ps {I35} from |g|g(t) in {+194}Ir |b{+-} decay (1972Be53); 50.5 ps {I22} from RDM in Coulomb excitation (1971NoZV) 
MOMM1$transient field integral perturbed angular correlations in Coulomb excitation (1992Br03). Others: +0.60 {I3} (1995An15), +0.592 {I44} (1991St04), 0.406 {I12} (1982Le02, 1987Be08), 0.600 {I23} (1975Ka42), +0.70 {I6} (1974Ga31), 0.64 {I6} (1972Do18), 0.49 {I3} (1970Ke14), +0.54 {I8} (1969Ku06), 0.64 {I8} (1967Ka16), 0.52 {I5} (1966Ag02), 0.45 {I4} (1965Ke11), 0.66 {I30} (1965Sp03), Values from 1975Ka42, 1970Ke14, 1966Ag02, 1965Ke11 are from IPAC technique in {+194}Ir |b{+-} decay and have been adjusted for adopted T{-1/2} of 328.5 level based on their measured precession angles (see {+194}Ir |b{+-} decay dataset for original values of g-factors). Other values are from different techniques in Coulomb excitation. 
$Measured precession angle |w|t(mrad): 106.7 {I35} (1975Ka42), 87 {I4} (1970Ke14), 99 {I9} (1966Ag02), 91.6 {I67} (1965Ke11), 97 {I4} (1964: A. Buyrn, L. Grodzins MIT Progress Report No. 2098, 251 (1964) 
MOME2$from Coulomb excitation reorientation (1986Gy04). Others: +0.63 {I6} (1978Ba38), 0.125 {I17} (1983Ch35), +0.77 {I50} (1973Gr06), 0.64 {I16} or 0.87 {I18} (1969Gl08, 1968Gl01), 0.25 {I17} (quoted by 1983Ch35 from muonic data of 1979HoZX). 1987Hi04 deduced Q=0.18 from a fit to (n,n') scattering data. 
$|b{-2}=-0.154 {I2} from 1981De12 in (p,p'), -0.170 {I5} from 1987Hi04 in (n,n'), -0.15 from 1980Se05 in (p,t). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$622.0|g E2 to 0+; E0 component in 293.5|g to 2+; L(p,t)=2 from 0+. 
T$from ce-|g(t) in {+194}Ir |b{+-} (1972Be53). Other: 42 ps {I3} from B(E2)(from g.s.)=0.0080 {I4} in Coulomb excitation and adopted %I(|g+ce)=11.15 {I15} for 622.0|g 
MOMM1$from g(622)/g(328)=0.95 {I18}, transient field integral perturbed angular correlations in Coulomb excitation (1992Br03), and |m(328)=+0.60 {I3}. Others: 0.69 {I9} (1975Ka42), 0.55 {I11} (1970Ke14), 0.53 {I14} (1966Ag02), 0.46 {I9} (1965Ke11), using IPAC method in {+194}Ir |b{+-} decay and adjusted for adopted T{-1/2}. 
$Measured precession angle |w|t(mrad): 102.7 {I61} (1975Ka42), 91 {I15} (1970Ke14), 83 {I20} (1966Ag02), 78 {I13} (1965Ke11) 
MOME2$from Coulomb excitation reorientation (1978Ba38). Not listed in 2020StZV evaluation 
$|b{-2}(Coulomb)=-0.154 {I2} ((p,p'), 1981De12). Other: (|a,|a') (1976Ba35). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$482.8|g E2 to 2+; L(p,p')=L(p,t)=4 from 0+. 
T$from Doppler-shift recoil-distance method in Coulomb excitation (1977Jo05). Others: 4.8 ps {I14} from DSAM in 1977St26 in Coulomb excitation; 4.7 ps {I2} from B(E2)(from 328.5, 2+)=0.78 {I3} in Coulomb excitation. 
MOMM1$from g(811)/g(328)=0.95 {I10}, transient field integral perturbed angular correlations in Coulomb excitation (1992Br03), and |m(328)=+0.60 {I3}. 
MOME2$from Coulomb excitation reorientation (1978Ba38). Value is not listed in 2020StZV evaluation 
$|b{-4}=-0.0455 {I10} ((p,p'), 1981De12), -0.040 {I5} ((n,n'), 1987Hi04). Others: ({+12}C,{+12}C') (1979Ba19); (|a,|a') (1976Ba35). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=L(p,t)=4 from 0+; 607.5|g E2 to 2+ 
T$from Doppler-shift attenuation method in Coulomb excitation (1977St26). Other: 1.53 ps {I+7-9} from B(E2)(from 622.0, 2+)=0.64 {I+3-2} in Coulomb excitation (1996Wu07) and adopted %I(|g+ce)=81.0 {I12} for 607.5|g 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$spin=0 from |g|g(|q) in {+194}Ir |b{+-}; 645.2|g and 938.7|g E2 to 2+. 
T$from B(E2)(from 622 level)=0.011 {I+3-2} (1996Wu07) in Coulomb excitation and adopted branching ratio %I(|g+ce)=66.9 {I4} for 645.2|g 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=6 from 0+; 600.5|g E2 to 4+. 
T$from Doppler-shift attenuation method in Coulomb excitation (1977St26). Other: 1.11 ps {I+3-8} from B(E2)(from 811.0, 4+)=0.93 {I+7-2} (1996Wu07) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(p,p')=L(p,t)=3 from 0+; 1104.0|g E1 to 2+, 621.3|g E1 to 4+ 
T$from B(E3)=0.120 {I8} in Coulomb excitation and adopted %I(|g+ce)=1.93 {I4} for 1432.5|g. Other: B(E3)=0.157 {I13} from (e,e') (1988Bo08) gives T{-1/2}=84 ps {I+10-8} 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
J$L(p,p')=(7) from 0+; 111.4|g (E2) to (5-) 
T$from |g|g(t) in {+194}Ir |b{+-} decay (171 d) (1970To14). 
MOMM1$from g=+0.26 {I8} (IPAD method in (|a,2n|g),2006Le06). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$576|g(|q) in (|a,2n|g) and (n,n'|g) consistent with stretched E2 to 3+. Also absence of transitions to levels with J|<2. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$spin=0 from |g|g(|q) in {+194}Ir |b{+-} (19.18 h); E0 transition to 0+. 
T$from B(E2)(from 328.5, 2+)=0.0191 {I+11-13} (1996Wu07) and adopted %I(|g+ce)=79.5 {I4} for 1218.8|g 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$|g|g(|q) in {+194}Au |e decay gives J=1 or 2; 855.8|g to 3+ is not E2 or M2 based on ce data in {+194}Au |e decay; 1156.5|g M1(+E2) to 2+. L({+3}He,d)=0+2 from 3/2+ also gives 1+ or 2+. A possible 345.98|g to 3- supports 2+ but not 1+ 


level_energy_unit: KEV
level_spin_parity: 2+,3+,4+
level_comment:
E$from (p,t). Others: 1870 {I1} in (p,p'), 1869 {I3} in (p,d), 1873 {I5} in (p,|a) 
J$L(p,d)=3 from 1/2-. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
J$696.4|g to 4+, 514.0|g to 6+; absence of |g rays to levels with J<4. 
T$from Doppler-shift attenuation method in Coulomb excitation (1977St26) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$L({+3}He,d)=0+2 for a group at 2000 {I20}; 1675.2|g (M1) to 2+, 1080.9|g (M1(+E2)) to 3+; 2003.65|g to 0+. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$weak |b{+-} feeding from 1- (log| {Ift}=9.0) and weak |e feeding from 1- (log| {Ift}=9.0); possible 1241.9|g to 4+, 162.6|g M1(+E2) from 1+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$the observed group at E=2090 {I5} in (p,d) with L=1+3 is either a doublet or a different level. 
J$E0 transition to 0+. 


level_energy_unit: KEV
level_spin_parity: (8)+
level_lifetime_unit: PS
level_comment:
J$687.7|g (E2), |DJ=(2) to 6+; absence of transitions to levels with J <6; E2 excitation in Coulomb excitation. 
T$from Doppler-shift attenuation method in Coulomb excitation (1977St26). Other: 0.65 ps {I+7-4} from B(E2)(from 1411.9, 6+)=0.73 {I+5-7} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$ce data from {+194}Au |e decay (38.02 h) give Mult=D+Q for 1186.37|g to 3+ and 1487.08|g to 2+; L(p,d)=1+3 from 1/2- for a group at E=2115 {I5}, a possible 2109+2114 doublet, favors 2+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$846.96|g and 2114.1|g M1 |g to 0+. Other: J=2 from (1786|g)(328|g)(|q) in {+194}Ir |b{+-} decay (19.18 h) (1965Ma10) is inconsistent 


level_energy_unit: KEV
level_spin_parity: (6-,7-)
level_comment:
E$from (p,t). Others: 2192 {I4} from (p,p') and 2191 {I10} from (p,d) 
J$L(p,d)=6 from 1/2- for an unresolved doublet at E=2191 {I20}, assuming i{-13/2} shell. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$1291.8|g (M1(+E2)) to 3+, 702.5|g (M1) to 2+, 2214.47|g to 0+; L(p,d)=1+3 from 1/2- suggesting 2+ for a group at 2214 {I5} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$the 2302 group in (p,d) with L(p,d)=1+3 (implying J|p=2+) may be a doublet or a different level. 
J$818.9|g, 1031.0|g, 2298.2|g M1 to 0+. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$strong E0 component in 1983.4|g to 2+, 1500.7|g (E2) to 4+, 2311.9|g (E2) to 0+; 197.8|g M1 to 1+ 


level_energy_unit: KEV
level_spin_parity: (6-,7-)
level_comment:
E$from (p,t). Others: 2323 {I4} from (p,p'), 2332 {I5} from (p,d) 
J$L(p,d)=6 from 1/2- assuming i{-13/2} orbit for a group at E=2332 {I5}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$E0 transition to 0+. 
E$2356.3 {I1} (2010Il03) and 2353 {I2} (1979De25) in (p,t) with L=(4) (1979De25) suggesting (4+) and non-zero L(p,t) in 2010Il03 has been listed as a separate level, assuming that angular distributions in (p,t) are correct 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$2356.3 {I1} from 2010Il03 and 2353 {I2} from 1979De25 in (p,t), with L(p,t)=(4) in 1979De25 and non-zero L(p,t) in 2010Il03 is probably a different level from 2356.059, 0+ level, assuming that angular distributions in (p,t) are correct 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$2365.9|g M1 to 0+. The group at 2363 {I5} in (p,d) with L=(1+3) suggesting (2+) could be a doublet; the |s(|q) data in (p,d) also consistent with L=(1+4) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$other: 2395.3 {I5} from (p,t) may be a different level 
J$L(p,d)=1+3 from 1/2- for a group at 2394 {I5}. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$2412.7|g M1 to 0+. L(p,d)=(0) from 1/2- suggesting (0-,1-) for a group at 2411 {I10} is inconsistent 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$338.8|g (E2), |DJ=2 to (8)+, 391.0|g (E1) to (9-); possible configuration=|ph{-11/2}{+-2} (2006Le06) from ({+82}Se,X|g) . 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
T$weighted average of 6.4 ns {I8} from {+194}Ir |b{+-} decay (171 d) and 5 ns {I1} from (|a,2n|g) 
J$possible band member of i{-13/2}{+-2} configuration from systematics and g factor measurements. 
T$|b|g(t) in {+194}Ir |b{+-} decay (1970To14). Other 5 ns {I1} in (|a,2n|g). Other: 6.6 ns {I6} only listed in Fig. 1 of 2015Ta25, with no data shown. 
MOMM1$from g=-0.17 {I7} (IPAD method in (|a,2n|g),2006Le06). Value is not listed in 2020StZV evaluation 


level_energy_unit: KEV
level_comment:
E$from (p,t). Other: 2500 {I10} from (p,d) for a triplet 
J$L(p,d)=(1+3) from 1/2- suggesting (2+) for a triplet of unresolved levels at 2500, 2515 and 2530; L({+3}He,d)=0+2 from 3/2+ suggesting 1+,2+ for a group at 2520 {I25} also for a composite peak 


level_energy_unit: KEV
level_spin_parity: (0+,1+,2+)
level_comment:
E$from (p,t). Other: 2677 {I3} from (p,p') 
J$L(p,d)=(1) giving (0+,1+,2+) for a group at 2667 {I10}, probably a doublet. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: PS
level_comment:
J$763.4|g to (6+); absence of transitions to levels with J<6. 
T$from B(E2)(from 1925.9, 6+)=0.46 {I+10-6} (1996Wu07) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
J$749|g to (8)+; band assignment 
T$from B(E2)(from 2099,8+)=0.28 {I+7-6} (1996Wu07) in Coulomb excitation 


level_energy_unit: KEV
level_comment:
J$L({+3},d)=0+2 suggesting 1+,2+ for a group at 2880 {I29}, probably a multiplet of 2856+2863+2879+2895+2908 levels 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
J$817|g to (8)+; no |g to levels with J<8. 
T$from B(E2)(from 2099,8+)=0.35 {I+9-11} (1996Wu07) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$from (p,d) 
J$L(p,d)=(1+3) from 1/2-. L({+3}He,d)=(0) suggesting (1+,2+) for a group at 3010 {I30}, probably a multiplet of 2980+3000+3015+3033 levels 


level_energy_unit: KEV
level_spin_parity: (18+)
level_comment:
E$3683 from reverse ordering of 183-255 cascade in ({+82}Se,X|g) 
J$255.0|g to (16+); possible band member. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
$On the basis of delayed coincidence data 1970To14 conclude that 562|g precedes 112|g, thus defining a level at 1486 rather than at 1936 (1968Su02) 
T$from |g|g(t) (1970To14) using two plastic scintillators 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
T$6.4 ns assigned to this level is now associated with a 12+ level lying 12.7 keV above this level as proposed by 2006Le06 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_uncertain: S
level_comment:
E$level proposed by 2006Le06 in (|a,2n|g) 
T$from |b(688|g)(t) (1970To14). 2006Le06 propose that 12+ state above the 10+ state at 2438 should be an isomeric state from systematics and comparison of measured g factor with calculated values. Proposed (2006Le06) configuration=|ni{-13/2}{+-2} 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$In order to balance the transition intensity at this level, 0.075 {I25} units of relative |g intensity should feed this level. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
$In order to balance the transition intensity at this level, 0.075 {I12} units of relative |g intensity should feed this level (2015Do06). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$spin=1 or 2 from |g|g(|q) of 1996TeZW; spin=1 is ruled out by Mult=D+Q from ce data for 855.8|g to 3+; 1156.6|g M1(+E2) to 2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: ?
level_comment:
E$2015Do06 cast doubt about the existence of this level for two reasons: 1. no other transition from this level reported. 2. coincidence with 328|g in 1996TeZW work suggests placement of all or part of the 1802.6|g from a new 2131 level, as proposed by 2015Do06. Also this level is not reported in any other study of decays and reactions. 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_uncertain: ?
level_comment:
E$level suggested by 2015Do06. 
J$2015Do06 analyze coincident summing and suggest that 0+ for this state is unlikely. The ground-state transition suggests J=1,2+. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
T$from the Adopted Levels 
G$from IPAD method (2006Le06) from analysis of 111.4, 482.8, 328.5 and 607.6 gamma rays 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
T$6.4 ns half-life assigned to this level (1976Hj01) is instead associated (by 2006Le06) with a 12+ level, 12.7 keV above the 2438 level. This interpretation is based on systematics and agreement of measured g factor with calculated values for 10+ and 12+ 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
E$level proposed by 2006Le06 from systematics of B(E2) values in the neighboring nuclides. 
T$from (338.8|g,391.0|g,687.7|g)(t) (1976Hj01). See also T{-1/2} comment for 2438.3 level. 
G$IPAD method (2006Le06) from analysis of 338.8, 600.5 and 687.7 gamma rays 
$Configuration=|ni{-13/2}{+-2} 


level_energy_unit: KEV
level_spin_parity: (14+)
level_comment:
E,J$energy revised upwards by 12.7 keV and spin higher by 2 units according to the proposed level scheme of 2006Le06 with the introduction of a new 12+ level at 2451 keV. 


level_energy_unit: KEV
level_spin_parity: (16+)
level_uncertain: ?
level_comment:
E$3742 from possible reverse ordering of the 255-183 cascade 
E,J$3754.7, (18+) in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$562.6|g(|q) consistent with J=5 and not with J=4 or 3. Excitation function (1981Fi01) consistent with J|>4 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$575.9|g(|q) consistent with stretched E2 to 3+. Excitation function (1981Fi01) consistent with J=4,5 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr)=5030 
$|b{-2}=-0.154 {I2} (1981De12), -0.145 (1980Ha47), -0.157 (1971Kr10) 
$|b{-2}(Coulomb)=-0.162, |b{-2}(nuclear)=-0.121 (1976Ba35) 
$d|s/d|W=0.92 mb/sr in (d,d') (1965Mu05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W (|mb/sr)=167 
$|b{-2}(Coulomb)=-0.152, |b{-2}(nuclear)=-0.124 (1976Ba35) 
$d|s/d|W=0.03 mb/sr in (d,d') (1965Mu05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W (|mb/sr)=328 
$|b{-4}=-0.0455 {I10} (1981De12) 
$|b{-4}(Coulomb)=-0.050, |b{-4}(nuclear)=-0.040 (1976Ba35) 
$d|s/d|W=0.02 mb/sr in (d,d') (1965Mu05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|b{-2}=-0.161 {I2}, B(E2)=1.84 {I5} from B(E2)=0.368 {I9} (1991Se04). |b{-2}=-0.110 {I7} (1990Se13). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$|b{-4}=-0.044 {I2}, B(E4)=0.037 {I4} from M(E4)=-1914 e fm{+4} {I92} (1991Se04). B(E4)=0.038 {I3} from M(E4)=-1953 e fm{+4} {I67} (1990Se13), recalculated by 1991Se04. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$|b{-4}=-0.030 {I1}, B(E4)=0.0171 {I14} from M(E4)=1307 e fm{+4} {I55} (1991Se04). B(E4)=0.0131 {I15} from M(E4)=1145 e fm{+4} {I67} (1990Se13), recalculated by 1991Se04. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$|b{-4}=-0.064 {I2}, B(E4)=0.078 {I6} from M(E4)=2799 e fm{+4} {I100} (1991Se04). B(E4)=0.052 {I3} from M(E4)=2290 e fm{+4} {I67} (1990Se13), recalculated by 1991Se04. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 1.46 {I+12-4} (1996Wu07), 1.661 {I11} (1986Gy04), 1.46 {I8} (1984WuZX), 1.620 {I15} (1978Ba38), 1.68 {I3} (1977Ro16), 1.87 {I9} (1971Mi08), 1.64 {I4} (1969Gl08), 1.9 {I2} (1961Mc01) 
T$from B(E2)=1.649 {I15}. From recoil distance method, T{-1/2}= 45.0 ps {I24} (1977Jo05, ({+40}Ar,{+40}Ar'|g)), 50.5 ps {I22} (1971NoZV). 
$g factor=+0.296 {I22} (transient field integral perturbed angular correlations, 1991St04), 0.203 {I6} (1982Le02, transient field technique), 0.349 {I31} (1974Ga31, IMPAC), 0.32 {I3} (1972Do18, recoil in vacuum), 0.32 {I4} (1967Ka16, IPAC), 0.33 {I15} (1965Sp03, IPAC). Value given by 1982Le02 (also 1987Be08) is much lower as compared to other values from Coulomb excitation and from IPAC technique in {+194}Ir |b{+-} decay (see Adopted Levels). See 1983St01 for a possible explanation of this low value. Others: 1979Ha06 (g-factor ratio of {+196}Pt/{+194}Pt); 1992Br03 report a value of +0.295 {I10} from weighted average of several literature values for the first 2+ levels in both {+194}Pt and {+196}Pt, which is used for normalization of other g-factors 
$Q=+0.48 {I14} (1986Gy04), 0.13 {I17} (1983Ch35), 0.63 {I6} (1978Ba38), +0.77 {I50} (1973Gr06), 0.64 {I16} or 0.87 {I18} (1969Gl08,1968Gl01). 1983Ch35 and 1978Ba38 are from the same group 
$E2 matrix element=(+)1.208 {I+49-17} (1996Wu07) 
$Static E2 matrix element=+0.54 {I+8-6} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from ce-|g(t) in {+194}Ir |b{+-} decay (1972Be53). Other: 42 ps {I3} from B(E2)(from g.s.)=0.0080 {I4} and adopted %I(|g+ce)=11.15 {I15} for 622.0|g 
$B(E2)(from g.s.)=0.0080 {I4}. Weighted average of 0.0079 {I2} (1996Wu07), 0.0079 {I4} (1984WuZX) and 0.0081 {I4} (1978Ba38). Others: 0.0070 {I10} (1977St26), 0.0094 {I15} (1977Ro16), 0.011 {I2} (1970Br26), 0.0087 {I20} (1961Mc01). 
$B(E2)(from 328.5, 2+)=0.437 {I16}. Weighted average of 0.460 {I+9-11} (1996Wu07), 0.423 {I15} (1978Ba38) and 0.456 {I17} (1984WuZX). Others: 0.58 {I7} (1977St26), 0.23 {I5} (1961Mc01). 
$g factor=+0.281 {I55}, from transient field integral perturbed angular correlations, normalized using g(622)/g(328)=0.952 {I183} and g(328)=0.295 {I10} (1992Br03). 
$E2 matrix element=+0.0888 {I12} (1996Wu07) 
$E2 matrix element (from 328,2+)=(+)1.517 {I+11-18} (1996Wu07) 
$E2 matrix element (from 811,4+)=+0.25 {I+14-6} (1996Wu07) 
$Static E2 matrix element=-0.40 {I+12-5} (1996Wu07) 
$M1 matrix element (622,2+ to 328,2+)=+0.028 {I+13-5} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from Doppler-shift recoil-distance method (1977Jo05). Others: 4.8 ps {I14} (Doppler-shift attenuation method, 1977St26); 4.7 ps {I2} from B(E2)(from 328.5) 
$B(E2)(from 328.5, 2+)=0.78 {I3} Weighted average of 0.749 {I+16-10} (1996Wu07), 0.92 {I9} (1988Fe08), 0.81 {I4} (1978Ba38), 0.75 {I2} (1984WuZX), 0.85 {I5} (1977St26), 0.86 {I13} (1971Mi08). 
$B(E2)(from 622,2+)=0.0069 {I+100-29} (1996Wu07) 
$B(E4)=0.05 {I4} (1988Fe08) 
$g factor=+0.279 {I31}, from transient field integral perturbed angular correlations, normalized using g(811)/g(328)=0.946 {I102} and g(328)=0.295 {I10} (1992Br03). 
$E2 matrix element=(+)1.935 {I+21-13} (1996Wu07) 
$Static E2 matrix element=+1.00 {I+12-24} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from Doppler-shift attenuation method (1977St26). Other: 1.53 ps {I+7-9} from B(E2)(from 622.0, 2+) (1996Wu07) and adopted %I(|g+ce)=81.0 {I12} for 607.5|g; this value disagrees with measured T{-1/2} from DSAM 
$B(E2)(from 328.5, 2+)=0.0097 {I10} (1996Wu07), 0.0097 {I15} (1984WuZX). Other: 0.018 {I9} (1978Ba38). 
$B(E2)(from 622.0, 2+)=0.64 {I+3-2} (1996Wu07), 0.63 {I5} (1984WuZX). Others: 1.2 {I5} (1978Ba38), 0.50 {I21} (1977St26). 
$B(E2)(from 811.4, 4+)=0.25 {I2} (1996Wu07), 0.25 {I6} (1984WuZX). Other: 0.87 {I31} (1978Ba38). 
$B(E4)(from g.s.)=0.017 {I6} (1978Ba38) 
$E2 matrix element (from 328,2+)=+0.220 {I9} (1996Wu07) 
$E2 matrix element (from 811,4+)=+1.51 {I+6-5} (1996Wu07) 
$E2 matrix element (from 1412,6+)=+0.16 {I+6-16} (1996Wu07) 
$E2 matrix element (from 622,2+)=(+)1.784 {I+45-29} (1996Wu07) 
$Static E2 matrix element=-0.07 {I14} (1996Wu07) 
$M1 matrix element (1229,4+ to 811,4+)=+0.19 {I+3-6} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 622.0, 2+)=0.011 {I+3-2} and adopted branching ratio %I(|g+ce)=66.9 {I4} for 645.2|g 
$B(E2)(from 328.5, 2+)=0.00098 {I+27-37} (1996Wu07), 0.0009 {I5} (1984WuZX) 
$B(E2)(from 622.0, 2+)=0.011 {I+3-2} (1996Wu07), 0.011 {I6} (1984WuZX) 
$E2 matrix element (from 328,2+)=0.070 {I+9-15} (1996Wu07) 
$E2 matrix element (from 611,2+)=(+)0.231 {I+30-21} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from Doppler-shift attenuation method (1977St26). Other: 1.11 ps {I+3-8} from B(E2)(from 811.0, 4+)=0.93 {I+7-2} (1996Wu07) 
$Other B(E2)(from 811.0, 4+)=0.93 {I9} (1984WuZX); 0.46 {I12} (1977St26) is discrepant 
$E2 matrix element=(+)2.90 {I+10-4} (1996Wu07) 
$Static E2 matrix element=+0.28 {I+12-27} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
T$from B(E3) and adopted %I(|g+ce)=1.93 {I4} for 1432|g from Adopted Gammas. 
$B(E3)=0.120 {I8}, weighted average of 0.125 {I8} (1989Li05), 0.111 {I9} (1978Ba38), 0.14 {I3} (1977Ro16) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 328.5, 2+)=0.0191 {I+11-13} and adopted %I(|g+ce)=79.5 {I4} for 1218.8|g in Adopted Gammas 
$B(E2)(from 328.5, 2+)=0.0191 {I+11-13} (1996Wu07), 0.019 {I7} (1984WuZX) 
$B(E2)(from 622.0, 2+)=0.0185 {I+13-11} (1996Wu07), 0.019 {I6} (1984WuZX) 
$E2 matrix element (from 328,2+)=+0.309 {I+9-10} (1996Wu07) 
$E2 matrix element (from 611,2+)=(+)0.304 {I+11-9} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_comment:
T$from Doppler-shift attenuation method (1977St26). 
$|g branchings deduced from T{-1/2} and B(E2) values. See Adopted Gammas for these values 
$B(E2)(from 811.0, 4+)=0.0056 {I+9-8} (1996Wu07), 0.0056 {I16} (1984WuZX) 
$B(E2)(from 1229.5, 4+)=0.48 {I+6-3} (1996Wu07), 0.48 {I9} (1984WuZX). T{-1/2}=1.3 ps {I2} gives B(E2)=0.40 {I9} (1977St26), assuming that 696|g is the main deexciting transition from the 1926 level 
$B(E2)(from 1411.9, 6+)=0.10 {I+2-4} (1996Wu07), 0.10 {I6} (1984WuZX) 
$E2 matrix element (from 811,4+)=0.224 {I+17-19} (1996Wu07) 
$E2 matrix element (from 1412,6+)=+1.14 {I+11-24} (1996Wu07) 
$E2 matrix element (from 1229,4+)=(+)2.09 {I+11-7} (1996Wu07) 
$Static E2 matrix element=+0.41 {I+26-22} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (8)+
level_lifetime_unit: PS
level_comment:
T$from Doppler-shift attenuation method (1977St26). Other: 0.65 ps {I+7-4} from B(E2)(from 1411.9, 6+)=0.73 {I+5-7} 
$B(E2)(from 1411.9, 6+)=0.73 {I+5-7} (1996Wu07), 0.79 {I15} (1984WuZX). T{-1/2}=1.1 ps {I3} gives B(E2)=0.47 {I14} (1977St26) 
$E2 matrix element=(+)3.08 {I+10-16} (1996Wu07) 
$Static E2 matrix element=[-0.10,0.43] (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.46 {I+10-6} 
$B(E2)(from 1925.9, 6+)=0.46 {I+10-6} (1996Wu07), 0.45 {I11} (1984WuZX) 
$E2 matrix element (from 1926,6+)=(+)2.44 {I+28-15} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
E$level seen in ({+136}Xe,{+136}Xe') only (1984WuZX,1996Wu07) 
T$from B(E2)(from 2099,8+)=0.28 {I+7-6} (1996Wu07) 
$E2 matrix element=2.20 {I+25-27} (1996Wu07) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 2099,8+)=0.35 {I+9-11} (1996Wu07) 
E$level seen in ({+136}Xe,{+136}Xe') only (1984WuZX,1996Wu07) 
$E2 matrix element=2.43 {I+32-41} (1996Wu07) 


level_energy_unit: KEV
level_comment:
E,L$probably an unresolved doublet with small mixture from L=6 
S$for L=1 and p{-1/2}. C{+2}S<0.15 for L=6 component 
$d|s/d|W=223 |mb/sr 


level_energy_unit: KEV
level_comment:
E$this level contaminated by a peak from {+195}Pt (g.s.). The authors have applied appropriate correction to cross sections 
$d|s/d|W=389 |mb/sr 


level_energy_unit: KEV
level_comment:
E,L$unresolved from a peak from {+193}Pt g.s. the L-transfer deduced by assuming L=1 for {+193}Pt peak 
$d|s/d|W=488 |mb/sr 


level_energy_unit: KEV
level_comment:
L,S$for triplet of unresolved levels at 2500, 2515 and 2530 
$d|s/d|W=1155 |mb/sr for 2500+2515+2530 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Enhancement=3.6 
$d|s/d|W(5|')=1761 |mb/sr {I10}, d|s/d|W(30|')=63 |mb/sr {I5}, d|s/d|W(17.5|')=112.1 |mb/sr {I12} 
$d|s/d|W(7|')=801 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=1.3 
$|b{-2}=-0.15 (1980Se05, coupled-channel calculations) 
$d|s/d|W(5|')=104 |mb/sr {I2}, d|s/d|W(30|')=69.9 |mb/sr {I10}, d|s/d|W(17.5|')=155.3 |mb/sr {I15} 
$E(level)=328, d|s/d|W(7|')=159 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.16 
$d|s/d|W(5|')=16.7 |mb/sr {I7}, d|s/d|W(30|')=9.2 |mb/sr {I4}, d|s/d|W(17.5|')=22.6 |mb/sr {I5} 
$E(level)=622, d|s/d|W(7|')=18 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.10 
$|b{-4}=-0.047 (1980Se05, coupled-channel calculations) 
$d|s/d|W(5|')=12.6 |mb/sr {I6}, d|s/d|W(30|')=4.0 |mb/sr {I2}, d|s/d|W(17.5|')=7.5 |mb/sr {I3} 
$E(level)=811, d|s/d|W(7|')=9 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.63 
$d|s/d|W(5|')=34.4 |mb/sr {I10}, d|s/d|W(30|')=21.4 |mb/sr {I5}, d|s/d|W(17.5|')=21.1 |mb/sr {I5} 
$E(level)=1229, d|s/d|W(7|')=30 |mb/sr (1979De25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Enhancement=0.08 
$d|s/d|W(5|')=25.2 |mb/sr {I9}, d|s/d|W(30|')=10.3 |mb/sr {I4}, d|s/d|W(17.5|')=4.9 |mb/sr {I2} 
$E(level)=1267, d|s/d|W(7|')=20 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.26 
$d|s/d|W(5|')=2.4 |mb/sr {I3}, d|s/d|W(30|')=5.0 |mb/sr {I3}, d|s/d|W(17.5|')=3.3 |mb/sr {I2} 
$E(level)=1374 {I1}, d|s/d|W(7|')=4 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.10 
$d|s/d|W(5|')=0.7 |mb/sr {I2}, d|s/d|W(30|')=1.3 |mb/sr {I1}, d|s/d|W(17.5|')=1.4 |mb/sr {I1} 
$E(level)=1414 {I1}, d|s/d|W(7|')=5 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=1.3 
$d|s/d|W(5|')=18.9 |mb/sr {I8}, d|s/d|W(30|')=9.8 |mb/sr {I4}, d|s/d|W(17.5|')=19.1 |mb/sr {I5} 
$E(level)=1433, d|s/d|W(7|')=12 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.03 
$Accurate |s(|q) in 2010Il03 could not be extracted for 1479.3 and 1485.5 peaks 
$d|s/d|W(5|')=0.7 |mb/sr {I2}, d|s/d|W(30|')=0.2 |mb/sr {I1}, d|s/d|W(17.5|')=1.6 |mb/sr {I1} 
$E(level)=1479 {I2}, d|s/d|W(7|')=3 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Accurate |s(|q) could not be extracted for 1479.3 and 1485.5 peaks 
$d|s/d|W(5|')=0.5 |mb/sr {I2}, d|s/d|W(30|')=1.5 |mb/sr {I2}, d|s/d|W(17.5|')=0.6 |mb/sr {I1} 
$E(level)=1486 {I2}, d|s/d|W(7|')=3 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=2.5 |mb/sr {I3}, d|s/d|W(30|')=0.8 |mb/sr {I1}, d|s/d|W(17.5|')=2.3 |mb/sr {I2} 
$E(level)=1512 {I3}, d|s/d|W(7|')=2 |mb/sr (1979De25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Enhancement=0.26 
$d|s/d|W(5|')=98.7 |mb/sr {I17}, d|s/d|W(30|')=36.5 |mb/sr {I7}, d|s/d|W(17.5|')=17.0 |mb/sr {I5} 
$E(level)=1547, d|s/d|W(7|')=46 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=2.2 |mb/sr {I2}, d|s/d|W(30|')=2.2 |mb/sr {I1}, d|s/d|W(17.5|')=5.7 |mb/sr {I3} 
$E(level)=1670 {I2}, d|s/d|W(7|')=5 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=1.9 |mb/sr {I2}, d|s/d|W(30|')=1.8 |mb/sr {I1}, d|s/d|W(17.5|')=4.8 |mb/sr {I3} 
$E(level)=1778 {I2}, d|s/d|W(7|')=6 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=7.2 |mb/sr {I3}, d|s/d|W(30|')=4.8 |mb/sr {I2}, d|s/d|W(17.5|')=5.7 |mb/sr {I3} 
$E(level)=1815 {I2}, d|s/d|W(7|')=14 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=4.4 |mb/sr {I3}, d|s/d|W(30|')=7.8 |mb/sr {I3}, d|s/d|W(17.5|')=16.2 |mb/sr {I5} 
$E(level)=1870 {I2} (1979De25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$L=(0) in 1977Se15 
$d|s/d|W(5|')=51.4 |mb/sr {I9}, d|s/d|W(30|')=11.6 |mb/sr {I3}, d|s/d|W(17.5|')=5.6 |mb/sr {I3} 
$E(level)=1892 {I2}, d|s/d|W(7|')=5 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=1.9 
$d|s/d|W(5|')=65.8 |mb/sr {I10}, d|s/d|W(30|')=47.0 |mb/sr {I7}, d|s/d|W(17.5|')=47.6 |mb/sr {I8} 
$E(level)=1911 {I2}, d|s/d|W(7|')=71 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=10.0 |mb/sr {I6}, d|s/d|W(30|')=8.4 |mb/sr {I6}, d|s/d|W(17.5|')=25.4 |mb/sr {I13} 
$E(level)=1931 {I2}, d|s/d|W(7|')=42 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=5.6 |mb/sr {I3}, d|s/d|W(30|')=5.5 |mb/sr {I2}, d|s/d|W(17.5|')=5.2 |mb/sr {I3} 
$E(level)=1947 {I2}, d|s/d|W(7|')=10 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=4.9 |mb/sr {I3}, d|s/d|W(30|')=2.7 |mb/sr {I2}, d|s/d|W(17.5|')=4.0 |mb/sr {I3} 
$E(level)=1980 {I2} (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.91,3.6 
$d|s/d|W(5|')=7.2 |mb/sr {I4}, d|s/d|W(30|')=10.6 |mb/sr {I3}, d|s/d|W(17.5|')=9.4 |mb/sr {I4} 
$E(level)=1990 {I2}, d|s/d|W(7|')=9 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.9 |mb/sr {I3}, d|s/d|W(30|')=5.4 |mb/sr {I2}, d|s/d|W(17.5|')=11.1 |mb/sr {I4} 
$E(level)=2001 {I2}, d|s/d|W(7|')=17 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=1.0 |mb/sr {I2}, d|s/d|W(30|')=2.5 |mb/sr {I2}, d|s/d|W(17.5|')=2.3 |mb/sr {I2} 
$E(level)=2031 {I2}, d|s/d|W(7|')=3 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.3 |mb/sr {I3}, d|s/d|W(30|')=2.2 |mb/sr {I2}, d|s/d|W(17.5|')=1.7 |mb/sr {I2} 
$E(level)=2062 {I2}, d|s/d|W(7|')=4 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=5.9 |mb/sr {I4}, d|s/d|W(30|')=5.1 |mb/sr {I3}, d|s/d|W(17.5|')=6.9 |mb/sr {I4} 
$E(level)=2105 {I2}, d|s/d|W(7|')=16 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.57 
$d|s/d|W(5|')=10.6 |mb/sr {I6}, d|s/d|W(30|')=13.1 |mb/sr {I6}, d|s/d|W(17.5|')=9.8 |mb/sr {I7} 
$E(level)=2125 {I2}, d|s/d|W(7|')=37 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=9.7 |mb/sr {I5}, d|s/d|W(30|')=13.4 |mb/sr {I5}, d|s/d|W(17.5|')=23.8 |mb/sr {I5} 
$E(level)=2137 {I2}, d|s/d|W(7|')=30 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.27 
$d|s/d|W(5|')=15.1 |mb/sr {I6}, d|s/d|W(30|')=11.6 |mb/sr {I4}, d|s/d|W(17.5|')=32.3 |mb/sr {I4} 
$E(level)=2155 {I2}, d|s/d|W(7|')=38 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.8 |mb/sr {I3}, d|s/d|W(30|')=7.1 |mb/sr {I3}, d|s/d|W(17.5|')=6.2 |mb/sr {I3} 
$E(level)=2189 {I2}, d|s/d|W(7|')=18 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=2.0 |mb/sr {I2}, d|s/d|W(30|')=1.9 |mb/sr {I2}, d|s/d|W(17.5|')=4.5 |mb/sr {I4} 
$E(level)=2210 {I2}, d|s/d|W(7|')=6 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=2.8 |mb/sr {I2}, d|s/d|W(30|')=2.4 |mb/sr {I2}, d|s/d|W(17.5|')=2.4 |mb/sr {I2} 
$E(level)=2224 {I2}, d|s/d|W(7|')=4 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.43 
$d|s/d|W(5|')=22.8 |mb/sr {I7}, d|s/d|W(30|')=13.4 |mb/sr {I4}, d|s/d|W(17.5|')=19.6 |mb/sr {I6} 
$E(level)=2246 {I2}, d|s/d|W(7|')=18 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.4 |mb/sr {I4}, d|s/d|W(30|')=1.2 |mb/sr {I1}, d|s/d|W(17.5|')=2.1 |mb/sr {I2} 
$E(level)=2277 {I2}, d|s/d|W(7|')=6 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=5.5 |mb/sr {I5}, d|s/d|W(30|')=2.4 |mb/sr {I2}, d|s/d|W(17.5|')=2.8 |mb/sr {I2} 
$E(level)=2284 {I2}, d|s/d|W(7|')=6 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.1 |mb/sr {I4}, d|s/d|W(30|')=2.5 |mb/sr {I2}, d|s/d|W(17.5|')=6.6 |mb/sr {I4} 
$E(level)=2296 {I2}, d|s/d|W(7|')=10 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.87 
$d|s/d|W(5|')=24.9 |mb/sr {I9}, d|s/d|W(30|')=22.1 |mb/sr {I7}, d|s/d|W(17.5|')=20.1 |mb/sr {I7} 
$E(level)=2353 {I2}, d|s/d|W(7|')=37 |mb/sr (1979De25) 
$A level at 2356.06 keV in the Adopted Levels is firmly assigned 0+. The level in (p,t) with L=(4) in 1979De25 and non-zero L value in 2010Il03 (see caption of Fig. 4 in this paper) suggest a separate level at this energy 


level_energy_unit: KEV
level_comment:
$Enhancement=0.33 
$d|s/d|W(5|')=6.9 |mb/sr {I5}, d|s/d|W(30|')=7.7 |mb/sr {I6}, d|s/d|W(17.5|')=18.4 |mb/sr {I7} 
$E(level)=2532 {I3}, d|s/d|W(7|')=28 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.56 
$d|s/d|W(5|')=6.7 |mb/sr {I5}, d|s/d|W(30|')=8.5 |mb/sr {I4}, d|s/d|W(17.5|')=8.8 |mb/sr {I6} 
$E(level)=2566 {I3}, d|s/d|W(10|')=11 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=4.4 |mb/sr {I4}, d|s/d|W(30|')=7.5 |mb/sr {I4}, d|s/d|W(17.5|')=8.2 |mb/sr {I6} 
$E(level)=2580 {I3}, d|s/d|W(7|')=27 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=2.0 |mb/sr {I3}, d|s/d|W(30|')=2.0 |mb/sr {I2}, d|s/d|W(17.5|')=3.6 |mb/sr {I3} 
$E(level)=2595 {I3}, d|s/d|W(7|')=16 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.61 
$d|s/d|W(5|')=3.9 |mb/sr {I4}, d|s/d|W(30|')=3.6 |mb/sr {I3}, d|s/d|W(17.5|')=3.4 |mb/sr {I4} 
$E(level)=2638 {I3}, d|s/d|W(7|')=29 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$Enhancement=0.61 
$d|s/d|W(5|')=1.3 |mb/sr {I3}, d|s/d|W(30|')=1.0 |mb/sr {I2}, d|s/d|W(17.5|')=1.1 |mb/sr {I3} 
$E(level)=2700 {I3}, d|s/d|W(7|')=18 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.1 |mb/sr {I4}, d|s/d|W(30|')=3.5 |mb/sr {I4}, d|s/d|W(17.5|')=3.1 |mb/sr {I6} 
$E(level)=2757 {I3}, d|s/d|W(7|')=30 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=1.2 |mb/sr {I2}, d|s/d|W(17.5|')=2.7 |mb/sr {I4} 
$E(level)=2815 {I3}, d|s/d|W(7|')=12 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=3.9 |mb/sr {I5}, d|s/d|W(30|')=2.9 |mb/sr {I4}, d|s/d|W(17.5|')=3.1 |mb/sr {I6} 
$E(level)=2840 {I3}, d|s/d|W(7|')=7 |mb/sr (1979De25) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(5|')=2.1 |mb/sr {I6}, d|s/d|W(17.5|')=2.0 |mb/sr {I7} 
$E(level)=2871 {I3}, d|s/d|W(7|')=13 |mb/sr (1979De25) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$other: |g|g(t) gives T{-1/2}=35.0 ps {I35} (1972Be53) 
$g-factor=+0.35 {I3} (1975Ka42, using T{-1/2}=35 ps {I3}), +0.28 {I3} (1970Ke14, using T{-1/2}=37 ps {I4}), +0.24 {I3} (1966Ag02, using T{-1/2}=45 ps {I5}), +0.21 {I3} (1965Ke11, using T{-1/2}=45 ps {I5}), with all measured using the integral perturbed angular correlation (IPAC). See Adopted Levels for |m values deduced from these g-factors with adjustments for adopted T{-1/2} 
$Measured precession angle |w|t(mrad): 106.7 {I35} (1975Ka42), 87 {I4} (1970Ke14), 99 {I9} (1966Ag02), 91.6 {I67} (1965Ke11), 97 {I4} (1964BuAA: A. Buyrn and L. Grodzins MIT Progress Report No. 2098 (1964) 251) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$adopted value from (ce)|g(t) (1972Be53) 
$g-factor from IPAC: 0.32 {I3} (1975Ka42, using T{-1/2}=38 ps {I4}), 0.22 {I4} (1970Ke14, using T{-1/2}=44 ps {I6}), 0.15 {I5} (1966Ag02, using T{-1/2}=62 ps {I14}), 0.13 {I3} (1965Ke11, using T{-1/2}=62 ps {I14}). See Adopted Levels for |m values deduced from these g-factors with adjustments for adopted T{-1/2} 
$Measured precession angle |w|t(mrad): 102.7 {I61} (1975Ka42), 91 {I15} (1970Ke14), 83 {I20} (1966Ag02), 78 {I13} (1965Ke11) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$Population of this level in {+194}Ir decay proposed by 2016Kr06, based on studies in {+194}Au |e decay to {+194}Pt 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J from nuclear magnetic resonance (1976Fu06) and L=1 in {+194}Pt(d,p). 
MOMM1 Nuclear magnetic resonance and {+23}Na standard (1951Pr02) 
Change of the mean-square charge radius (rel to {+198}Pt) |D<r{+2}>|?-0.1 (fm){+2} (1988Ro20) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J L=1 in {+194}Pt(d,p), |g to 1/2- is M1+E2. 
T from Mossbauer (1965Ha36). Others: 0.165 ns {I10} (1968GeZX), 0.152 ns {I14} (1966Bu04), 0.83 ns {I14} (1972Sh38), |>0.15 ns (1966At03), 0.163 ns {I2} (1974Ru03). 
MOMM1 Mossbauer effect and {+195}Pt standard (1967Ag01). Others: -0.60 {I15} (1967Bu20), -0.65 {I15} (1966At03). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J |g to 1/2- is E2 and L=3 in {+194}Pt(d,p). 
T weighted av of 0.62 ns {I7} (1966Bl08), 0.69 ns {I3} (1966Gr20,1966Gr20). Other: 0.61 ns {I7} (Coul. ex. B(E2)|^=0.19 {I2}). 
MOMM1 Mossbauer effect and {+195}Pt standard (1974Ru03). Others: 0.89 {I11} (1972Wo06), +0.81 {I+15-21} (1971Wa17) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J |g to 1/2- is M1+E2 
T from B(E2)|^=0.39 {I2} (Coul. ex.). Others: 53 ps {I9} (recoil-distance Doppler,1971NoZT), 67 ps {I8} (pulsed beam, 1965Bl10) 
MOMM1 From g=+0.104 {I21}, CEAD method (1972Va16). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J |g to 3/2- is M1+E2 and |g(|q) to 1/2- (Coul. ex. 1959Mc69,1970Br26). 
T from B(E2)|^=0.70 {I3} (Coul. ex.). Other: 80 ps {I4} in recoil-distance Doppler (1971NoZT). 
|m=+0.52 {I5} (1973Ga31,2011StZZ), +0.64 {I9} (1994La02,2011StZZ). 
MOMM1 Others: +0.56 {I7} (1972Va16), 0.74 {I13} (1972Sp03). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J L=6 in {+196}Pt(d,t),({+3}He,|a), |g(|q,H,t) analysis consistent only with J=13/2 ({+195}Pt IT decay,1972Ba22). 
T from |g(t) measurements ({+195}Pt IT decay,2000Mo05). Others: 4.02 d {I1} (|g(t) measurements in 1972PoZU), 4.1 d {I1} (1967Ab07), 4.5 d {I1} (1963Ka34), 3.5 d {I2} (1963Ve13), 4.08 d {I12} (1960Br11), 3.75 d {I25} (1978LeZA). 
|m=- from 1991Sc28. 
MOMM1 From NMR on oriented {+195}Pt (1972Ba22). 
MOME2 Static nuclear orientation with gamma detection (1985Ed05). 1Other: +1.4 {I7} (1985Ed03). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J |g(|q)'s to 5/2- and 3/2- ({+195}Pt(n,n'|g),1983Gh01), and level is Coulomb-excited. 
T from B(E2)|^=0.025 {I2} in Coul. ex. 
|m=+0.39 {I10} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J J from |g(|q) to 1/2- ({+195}Pt(n,n'|g),1983Gh01) and |p from M1(+E2) |g to 3/2- (Coul. ex.,1985Br31). 
T$from B(E2)|^=0.030 {I2} in Coul. ex. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2+)
level_comment:
J 1985Th02 suggest that the level is different from the 432.2 level with L(d,p)=4 and probably has J|p=17/2+ based on |s(|q). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J J=5/2 from |g(|q)'s to 5/2- and 3/2- ({+194}Pt(n,n'|g),1983Gh01) and |p from M1 |g to 3/2-. 
T from Doppler-broadened line-shape measurements (1994La02) 
|m=+1.6 {I6} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: PS
level_comment:
J L=3 in {+194}Pt(d,p) and {+196}Pt(d,t),({+3}He,|a). |g(|q) in (n,n'|g) (1983Gh01) favor 7/2. But J|p=5/2- from tentatively-assigned 3/2-[541] band member (1976Ya07). But J|p=7/2- from U(6/12) supersymmetry analysis with configuration=<6,1,0>-(2, 0) (1986Ma57). If their assignments are correct, this level could be a doublet. 
T from B(E2) in Coul. ex. if branching (409|g)=0.46 {I5} 
|m=+0.55 {I8} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J |g(|q) to 3/2- and |g to 1/2- in {+195}Pt(n,n'|g). 
T from Doppler-broadened line-shape measurements (1994La02) 
|m=+1.5 {I4} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J |g to 13/2+ is (M1+E2) and L=(6) in {+196}Pt(p,d), and |g from 9/2- is (E1). L({+3}He,|a)=5,6 for E=558 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T from B(E2) in Coul. ex. 
J L({+3}He,|a)=5,6 for E=558, E2 |g to 5/2- 
|m=+1.55 {I12} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: PS
level_comment:
T$from B(E2) in Coul. ex. 
J |g to 5/2- is M1(+E2), and L=3 in {+194}Pt(d,p) and {+196}Pt(p,d); no |g to 1/2- (g.s.). 
|m=+1.4 {I4} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
J |g to 5/2- is (E2) and U(6/12) multi-J supersymmetry scheme of interacting boson-fermion model (Coul. ex., 1986Ma57). 
T from 1994La02. 
|m=+1.52 {I16} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J L=3 in {+196}Pt(p,d). 
T from Doppler-broadened line-shape measurements (1994La02) 
|m=+1.23 {I28} (1994La02,2011StZZ). 
MOMM1 Transient field integral perturbed angular correlation (1994La02). 
E$from Coul. ex., uncertainty assigned by evaluator 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J L=3 in {+196}Pt(p,d) and {+196}Pt(d,t). May be be 3/2-[541] band member (7/2-) in {+194}Pt(d,p) (1976Ya07). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J |g to 1/2- is M1+E2 
T from B(E2)|^=0.0149 {I24} in Coul. ex. T{-1/2}: 12 ps {I+4-6} if |d=+1.0 {I4}, 22 ps {I4} if |d=3.6 {I14} 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J J|p=5/2+,(5/2-,1/2+,3/2+) from average resonance neutron capture measurements. J=3/2,5/2 from |g(|q) to 5/2+ in {+195}Pt(n,n'|g). |p=+ from E2(+M1) |g to 5/2+ in {+194}Pt(n,|g). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E thermal neutron binding energy deduced from thermal, 2- and 24-keV neutron capture measurements (1982Wa20), but no primary |g-rays from thermal neutron capture are given by 1982Wa20. 
J from s-wave thermal neutron capture 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T from Mossbauer measurement (1974Ru03). Others: 0.165 ns {I10} (1968GeZX), 0.83 ns {I14} (1972Sh38), 0.152 ns {I14} (1966Bu04), 0.17 ns {I2} (1965Ha36), |>0.15 ns (1966At03). 
G From average of -0.43 {I10} (1966At03), -0.41 {I3} (1967Ag01), -0.40 {I10} (1967Bu20), and -0.44 {I5} (1968GeZX). 
Isomer shifts: |D<r{+2}>/<r{+2}>=-(1.6 {I+44-9})E-4 (1971Wa17); |D<r{+2}>(130)/<r{+2}>(99)=1.3 {I2} (1971Ru13), 1.61 {I20} (1972Wo06); for the interpretation of isomer shifts see 1985De51. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T other: |<0.52 ns {I5} (1971Wa17 Moss). 
G From unweighted average of +0.36 {I3} (1971Ru13,1974Ru03), +0.35 {I4} (1972Wo06), and +0.324 {I+52-100} (1971Wa17). 
Branching ratio of I(|g+ce)(130|g)/I(|g+ce)(31|g): 0.049 {I5} (1972Wo06), 0.052 {I10} (1965Ha13). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T from 1974Ru03 (Moss). Other: 0.16 ns {I3} if av B(E2)=0.15 {I3} from 0.19 {I4} (1959Mc69), 0.11 {I4} (1966Gr20); T{-1/2}=0.34 ns {I6} from adopted B(E2). 
BE2 From B(E2)=0.076 {I12} (1985Br31) after correcting |a=7.6 to 7.1. Earlier values are incorrect since feeding from 199 level was not corrected for 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=3/2-<6,1,0>-(1,0) (1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T others: 0.61 ns {I7} if B(E2)|^=0.19 {I2} 
B(E2): 0.19 {I2} (1970Br26), 0.17 {I5} (1966Gr20), 0.39 {I13} (1959Mc69), 0.198 {I12} (1985Br31). 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=5/2-<6,1,0>-(1,0) (1986Ma57) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: NS
level_comment:
T from B(E2)|^. 
BE2 Weighted average of 0.098 {I14} (1970Br26), 0.076 {I12} (1971Mi08), 0.082 {I12} (1982Ku22), and 0.054 {I5} (1985Br31). These data have been corrected for adopted decay branching. 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=3/2-<6,1,0>-(1,1) (1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T from B(E2)|^. Others: 53 ps {I9} (1971NoZT) recoil distance, 67 ps {I5} (1965Bl10) pulsed beam, microwave. 
BE2 From weighted average of 0.43 {I5} (1959Mc69), 0.40 {I3} (1971Mi08) 0.35 {I4} (1966Gr20), 0.40 {I2} (1970Br26), 0.442 {I26} (1982Ku22), 0.38 {I2} (1985Br31). 
|g: +0.104 {I21} (1972Va16), +0.166 {I54} (1969Ku06) 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=3/2-<7,0,0>-(1,0)(1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T from B(E2)|^. Other: 80 ps {I4} (1971NoZT) recoil distance 
BE2 Weighted average of 0.66 {I5} (1970Br26), 0.71 {I9} (1959Mc69), 0.73 {I5} (1982Ku22). Values are all corrected for adopted decay branching. Other: 0.51 {I3} (1985Br31) but branching used by authors is not specified. 
g: 0.21 {I2} (1974Ga31), 0.22 {I3} (1972Va16) if T{-1/2}=80 ps. Other g: 1969Ku06, 1972Sp03 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=5/2-<7,0,0>-(1,0)(1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^ 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=5/2-<6,1,0>-(1,1)(1986Ma57) 
BE2$weighted average of 0.021 {I3} (1985Br31), 0.0264 {I19} (1982Ku22) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_uncertain: ?
level_comment:
E$evaluator considers authors' evidence for this level to be tentative 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=7/2-<6,1,0>-(1,1)(1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$excited via a two-step process (1986Ma57). 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=5/2-<6,1,0>-(2,0)(1986Ma57) 
E 449.6 (1982Ku22) may correspond to this level. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
B(E2)(99-508)=0.48 {I10} (1986Ma57) 
T{-1/2}: from B(E2) for branching (409|g)=0.46 {I5} 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=7/2-<6,1,0>-(2,0)(1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=3/2-<7,0,0>-(2,0)(1986Ma57) 
BE2$other: 0.030 (1986Ma57). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
B(E2)(130-563)=0.024 {I12} (1986Ma57) 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1}, |t{-2})=5/2-<7,0,0>-(2,0) (1986Ma57) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
B(E2)(211-613)=0.34 {I14} (1986Ma57) 
T$from B(E2) 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1},|t{-2})= 7/2-<7,0,0>-(2,0) (1986Ma57) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
B(E2)(239-667)=0.33 {I7} (1986Ma57) 
configuration=J|p<|s{-1},|s{-2},|s{-3}>-(|t{-1},|t{-2})= 9/2-<7,0,0>-(2,0)(1986Ma57) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2+
level_lifetime_unit: D
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$ from Adopted Levels 
$ This level decays by 129.5 - 129.8 |g cascade to g.s. of {+195}Pt 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Decay modes from {+195}Pt Adopted Levels in the ENSDF database (March 2014 update) 
E,T$from {+195}Pt Adopted Levels in the ENSDF database, according to which the isomer decays to the 1/2- g.s. through 129.5|g, M4 |) 129.73|g, E2 |) |g cascade, forming a sequence of 259.1, 13/2+; 129.77, 5/2-; 0.0, 1/2- levels. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J absence of hyperfine splitting (1935Fu06) consistent with J=0. |D<r{+2}>({+194}Pt,{+196}Pt)=0.926 fm{+2} {I4} (1987Ne09). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J from E2 |g to 0+ level. 
T from B(E2)=1.372 {I6}. Others: 35.4 ps {I35} (RDM,1971NoZT), 30.2 ps 21 (delayed coin, 1972Be53), and 32.2 ps {I15} (1981Bo32) (value recommended by 1981Bo32 based on their RDM, composite RDM, and DSA measurements). 
BE2 Weighted average of 1.368 {I4} (1992Li14) and 1.382 {I6} (1985Fe03, 1986Gy04). Others: see Coulomb excitation. 
|m: +0.588 {I46} (1991St04), +0.604 {I48} (1993Ta07). Compilation: 2005St24. 
MOMM1 Others: +0.534 {I14} from weighted average of g-factor measurements, see Coulomb excitation. 
Q: +0.62 {I8} (1992Li14). Compilation: 2005St24 
MOME2 Others: +0.63 {I7} (based on Coulomb excitation), 0.51 {I18} or 0.58 {I18} (1969Gl08) dependent upon the + or - sign of interference; +0.56 {I18} (1978LeZA); +0.84 {I6} (quoted by 1981Bo32); 0.82 {I6} (quoted by 1985Fe03 from 1978SpZW); +0.78 {I6} (1981Bo32); +0.79 {I12} (1985Fe03). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L=2 in {+198}Pt(p,t). 
T weighted average of 35.1 ps {I29} (value recommended by 1981Bo32 based on their RDM, composite RDM, and DSA measurements), 36 ps {I3} (ce-|g(t),1972Be53), and 33.6 ps {I8} from B(E2)=0.368 {I9} (see Coulomb excitation, assuming E0 fraction of 333|g is negligible) 
|m=+0.54 {I9} (1992Br03). Compilation: 2005St24 
MOMM1 Others: 0.49 {I10} from g/g(356 level)=0.92 {I19} (1981St24), see Coulomb excitation. 
$Q=-0.39 {I16} (1992Li14). Compilation: 2005St24 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L=4 in (p,t). 
T weighted average of 3.5 ps {I3} (value recommended by 1981Bo32 based on their RDM, composite RDM, and DSA measurements), and 3.55 ps {I5} from B(E2) (weighted average of 1971Mi08, 1990Ma37, and 1992Li14. See Coulomb excitation) 
BE4 From {+196}Pt(e,e'). Other: B(E4)=0.0308 {I23} from (pol p,p'). B(E4)=0.012 {I8} (1992Li14) from Coulomb excitation. 
|m=+1.38 {I16} (1992Br03). Compilation: 2005St24 
MOMM1 Others: 1.11 {I10} from g=0.277 {I26}, see Coulomb excitation. 
$Q=1.03 {I12} (1992Li14). Compilation: 2005St24 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J L=0 in (p,t). 
T from B(E2) and branching of 779|g. Others: 6 ps {I3} (composite RDM, 1981Bo32), >2.6 ps or >3.1 ps (depending on the extreme feeding assumptions) (1990Bo29). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J E1 |g to 4+, L=5 in (p,p'). 
T from delayed coincidence (1970To14) in {+196}Ir |b{+-} decay (1.40 h). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L=4 in (p,p'). 
T weighted average of 2.9 ps {I6} (RDM 1981Bo32) and 2.4 ps {I+11-3} from B(E2). See Coulomb excitation. 
BE4 Weighted average of 0.0201 {I28} from (e,e') and 0.025 {I3} from (pol p,p'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J E2 |g to 2+, |g's to 0+ and 4+. 
T T{-1/2}=50 ps {I+44-19} computed from B(E2)=0.0008 {I+7-3} in Coulomb excitation and adopted |g-ray properties. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J E2 |g to 5-, L=7 in (p,p'). 
T from |g(|q,H,t) (1983GoZP). Others: 4.01 ns {I16} from delayed coin (1970ToZZ), 4.0 ns (1984Sc19). 
MOMM1 From g=-0.03 {I2} (1983GoZP). Compilation: 2005St24 


level_energy_unit: KEV
level_spin_parity: (5-,6+)
level_uncertain: ?
level_comment:
J |g's from 2455 to 7- and 9-, from 1430 to 4+, and a connecting 2455 to 1430 |g give J|p(2455)=7- or 8, and J|p(1430)=5 or 6+. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
J E1 |g to 2+, L=3 in (p,t). 
T deduced from B(E3) and adopted |g-ray properties. See Coulomb excitation. 
BE3 See Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J g.s. band member. 
T weighted average of 1.0 ps {I3} (RDM, 1981Bo32) and 0.98 ps +12-5 from B(E2). See Coulomb excitation. 
$Q=-0.18 {I26} (1992Li14). Compilation: 2005St24 


level_energy_unit: KEV
level_spin_parity: 3-,4+
level_comment:
J |g's from 2469 to 0+ and 2+, from 1755 to 3- and 5-, and a connecting 2469 to 1755 |g give J|p(2469)=1- or 2+, and J|p(1755)=3- or 4+. 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J E2 |g to 7-, negative-parity band member. 
T from |g|g(t) (1968Ja06) in {+196}Ir |b{+-} decay (1.40 h). 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
J M1+E2 |g to 2+,4+, L=4 in {+196}Pt(p,p') 
BE4 Weighted average of 0.044 {I13} (1985Bo14), 0.0398 {I19} (1991Se04), and 0.044 {I13} (1992Po09). 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: PS
level_comment:
J |g's to 0+ and 2+, ARC gives 1+,(0+, 2+). 
T from Doppler broadening (1990Bo29) in {+195}Pt(n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J J|p=0+, 1+ and 2+ from E1 deexcitation from capture level 0-, and 1-, 0+ is ruled out from |g's to 3-. 


level_energy_unit: KEV
level_spin_parity: 3,4+
level_comment:
J$|g to 2+, ARC in 1979Ci04, large uncertainties of A{-2} and A{-4} in 2002Ta14. 3 in figure 2 of 2002Ta14 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J E2 |g to 4+, |g's to 6+, |g-band member. 
T deduced from B(E2) and adopted |g-ray properties, see Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J |g's to 3+, L=(2) natural parity in {+194}Pt(t,p). E1 |g from 0-, 1- capture level in (n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J |g's to 2+ and 3-, 4+, L=2 in {+197}Au(d,{+3}He). E1 |g from 0-, 1- capture level in (n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: PS
level_comment:
T from |G{-0}/|G=0.77 {I3}, |G{-0}=2.7 meV 9 in {+196}Pt(|g,|g') 
J |g's to 0+, E1 |g from 0-, 1- capture level in (n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J E2 |g to 6+, |g's to 7- and 9-, ground-state band member. 
T deduced from B(E2) and adopted |g-ray properties, see Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (2,3,4+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=?
level_comment:
J from data on |g(|q), excitation functions, decay patterns and T{-1/2}. See (n,n'|g). 
T from DSA in (n,n'|g), |DT{-1/2}=+400-37 (1993Di05). 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3)
level_lifetime_unit: FS
level_comment:
J from data on |g(|q), excitation functions, decay patterns and T{-1/2}. See (n,n'|g). 
T from DSA in (n,n'|g) (1993Di05). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
J L=3 in {+196}Pt(p,p'). 
T from DSA in (n,n'|g) (1993Di05). 
BE3 Weighted average of 0.070 {I14} (1988Co19) and 0.087 {I14} (1992Po09). 


level_energy_unit: KEV
level_spin_parity: 10-,11-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J E2 |g to 9-, no |g to J|p<9. 
T from |b|g(t) measurements (1968Ja06) in {+196}Ir |b{+-} decay (1.40 h). 


level_energy_unit: KEV
level_spin_parity: 0+,2+
level_comment:
J E1 |g from 0-, 1- capture level in (n,|g) E=thermal. 
J from the average capture results in {+195}Pt(n,|g) E=2 keV. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J from M1 excitation in {+196}Pt(|g,|g') 
T from |G{-0}/|G=0.63 {I6}, |G{-0}=13.6 meV 22 in {+196}Pt(|g,|g') 


level_energy_unit: KEV
level_spin_parity: (1,2,3)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=?
level_comment:
J from data on |g(|q), excitation functions, decay patterns and T{-1/2}. 
T from DSA, |DT{-1/2}=+527-42 (1993Di05). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J L=3 in {+196}Pt(p,p'). 
BE3 Weighted average of 0.070 {I14} (1988Co19) and 0.072 {I13} (1992Po09). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1+)
level_lifetime_unit: PS
level_comment:
J from M1 excitation in {+196}Pt(|g,|g') 
T from |G{-0}/|G=1, |G{-0}=3.6 meV 13 in {+196}Pt(|g,|g') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J from M1 excitation in {+196}Pt(|g,|g') 
T from |G{-0}/|G=0.41 {I4}, |G{-0}=27.5 meV 42 in {+196}Pt(|g,|g') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+,(2)+
level_lifetime_unit: PS
level_comment:
J J|p=1+ from M1 excitation in {+196}Pt(|g,|g'), L=(2) in {+194}Pt(t,p). 
T from |G{-0}/|G=1, |G{-0}=5.2 meV 9 in {+196}Pt(|g,|g') 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J supported by E1 deexcitation to 877 level. 
J also log| {Ift} from {+196}Au |e decay. 
T from delayed coin (1970To14); see also 1968Ja06. 


level_energy_unit: KEV
level_spin_parity: 10-,11-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J based upon E2 deexcitation to 9- level, and log| {Ift}=6.05, no |g's to J|p<9. 
T from |b|g(t) measurements (1968Ja06). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$from 1961Be14 
J$supported by E2 transition, Coul. ex. 
T$weighted av of 30.2 ps {I21}, delayed coin (1972Be53); 35.4 ps {I35}, recoil-distance Doppler shift (1971NoZT) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E from 1961Be14 
J supported by E0+M1+E2 transition to 356 level 
T from delayed coin, renormalized to T{-1/2}(356)=32 ps (1972Be53) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E from coin observation of 521.4 and 355.7 |g's (1962Wa16,1963Ik01) 
J supported by E2 character of 521.4|g, E1 character of 571|g, as well as log| {Ift}. See also {+196}Ir |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 1+,(0+,2+)
level_comment:
$I|g/E|g{+5}=2.10 
E av res capture feeds a possible doublet with another member having E=2529.3 {I3}. 


level_energy_unit: KEV
level_spin_parity: 1+,(0+,2+)
level_comment:
$I|g/E|g{+5}=2.10 
E av res capture feeds a possible doublet with another member having E=2527.831 {I34}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
E the observed peak is probably a 1270-1293 keV doublet. |s(|q) is not well fitted by an L=3 transfer. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
BE4 Weighted average of 0.0171 {I19} (1988Bo08), 0.024 {I5} (1985Bo14), and 0.0247 {I54} (1992Po09). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
BE3 Weighted average of 0.103 {I18} (1988Bo08) and 0.116 {I14} (1992Po09). 
The large error band of the 3- level is a consequence of inability to separate the 3- level from neighboring 6+ and 7- levels. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J this state can be understood in an octupole vibrational picture (1988Co16); the fragmentation of octupole strength is responsible for the apparent anomalous behavior of 3(1)- (1988Co19). 
BE3,B3 Also quoted in 1988Co16. Data of both are based on a reanalysis of data in 1981De12. 
BE3 From B(E3)(0+ to 3-)(W.u.)=6.2 {I6} (1988Co16). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3,B3 Data of 1988Co19 is based on a reanalysis of data in 1981De12. 
BE3 From B(E3)(0+ to 3-)(W.u.)=4.4 {I9} (1988Co19). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3,B3 Data of 1988Co19 is based on a reanalysis of data in 1981De12. 
BE3 From B(E3)(0+ to 3-)(W.u.)=2.1 {I4} (1988Co19). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3,B3 Data of 1988Co19 is based on a reanalysis of data in 1981De12. 
BE3 From B(E3)(0+ to 3-)(W.u.)=3.2 {I6} (1988Co19). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2). Others: 32.2 ps {I15} (RDM,1981Bo32), 35.4 ps {I35} (RDM,1971NoZT), 30.2 ps {I21} (delayed coin., 1972Be53). For comparison, the evaluation of 1987Ra01 gives 33.5 ps {I10} which is based on half-life as well as B(E2) measurements. 
BE2 Weighted average of 1.382 {I6} (1985Fe03,1986Gy04) and 1.368 {I4} (1992Li14). Others: 1.42 {I6} (1984Mu19), 1.36 {I7} (1971Mi08), 1.35 {I4} (1970Br26), 1.49 {I5} (1969Gl08), 1.39 {I15} (1967Ka16), 1.34 {I16} (1966Gr20). These B(E2) values have been renormalized to B(E2,328)=1.649 {I15} of {+194}Pt from 1989Si01. The evaluation of 1987Ra01 gives B(E2)=1.400 {I40} based on half-life and B(E2) data. Others: 1976Ba35, 1968Gl01, 1967Mi15, 1961Mc01, 1955St57. 
MOMM1 From weighted average of g factor. Other: 0.55 {I3} (1976Fu06). 
MOME2 Weighted average of +0.62 {I8} (1992Li14) and +0.66 {I12} based on Coulomb excitation reorientation (1986Gy04,1989Ra17). Others: 0.51 {I18} or 0.58 {I18} (1969Gl08) dependent upon the + or - sign of interference; +0.56 {I18} (1978LeZA); +0.84 {I6} (quoted by 1981Bo32); 0.82 {I6} (quoted by 1985Fe03 from 1978SpZW); +0.78 {I6} (1981Bo32); +0.79 {I12} (1985Fe03). 
G$weighted average of g=0.255 {I11} (from g({+196}Pt)/g({+194}Pt)=R=1.007 {I38}, 1992Br03, transient field), 0.266 {I12} (R=1.05 {I4}, 1986Ba19) , 0.266 {I21} (R=1.05 {I8}, 1979Ha06), 0.268 {I28} (R=1.06 {I11} 1972Sp03) [1992Br03, 1986Ba19, 1979Ha06 and 1972Sp03 scaled by evaluators to g({+194}Pt,328)=0.253 {I6}], 0.294 {I23} (1991St04, IMPAC), 0.296 {I46} (1974Ga31, IMPAC), 0.292 {I28} (1972Be53), and 0.284 {I47} (1968Be61). Lifetime-dependent results of 1974Ga31, 1972Be53 and 1968Be61 have been corrected for present adopted T{-1/2}. Others: g=0.213 {I21} (1982Le02); 0.346 {I13} (1981Ka23, IPAC); 0.265 {I35} (1968Mu02); 0.27 {I4} (1967Ka16). Value given by 1982Le02 is much lower as compared to other values from Coulomb excitation and from IPAC, see 1983St01 for a possible explanation of this low value. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T weighted average of 35.1 ps {I30} (RDM,1981Bo32), 36 ps {I3} (ce-|g(t),1972Be53), and 33.6 ps {I8} from B(E2)=0.368 {I9} (assuming E0 fraction of 333|g is negligible). 
BE2 Weighted average of B(E2)(2+(356) to 2+(689))=0.370 {I5} (1992Li14), 0.242 {I+52-50} (1990Ma37 scaled by evaluators to B(E2)(0+ to 2+)=1.382 {I6}), and 0.342 {I34} (1972Be53). 
G From IMPAC, g(2+,355)/g(2+,688)=1.09 {I22} (1981St24). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T weighted average of 3.5 ps {I3} (RDM,1981Bo32) and 3.55 ps {I5} from B(E2). 
BE2 Weighted average of B(E2)(2+ to 4+)=0.67 {I11} (1971Mi08), 0.734 {I+52-34} (1990Ma37 scaled by evaluators to B(E2)(0+ to 2+)=1.382 {I6}), and 0.73 {I1} (1992Li14). 
BE2 M(E2 to 355)=1.83 {I15} coul.ex (1971Mi08, quoted by 1988Fe08), 1.90 {I8} recoil distance (1981Bo32 quoted by 1988Fe08), 1.94 {I2} (quoted by 1986Gy04), 2.07 {I7} (1988Fe08). 
Others: B(E4)=0.0070 (1976Ba35), E4 matrix element M(E4)=-0.155 {I16} (e,e') (quoted by 1988Fe08 from 1985Bo14), -0.203 (quoted by 1988Fe08 from 1981De12), -0.084 (quoted by 1988Fe08 from 1976Ba35), M(E4 to 0)=0.18 {I7} (quoted by 1986Gy04), -0.11 {I11} (1988Fe08). 
-0.19 {I7} if M(E2 to 688)=0 or 0.5 (1988Fe08). 
G Weighted average of 0.296 {I33} (from g/g(2+,{+194}Pt)=1.169 {I129}, 1992Br03 scaled by evaluators to g({+194}Pt,328)=0.253 {I6}) and 0.245 {I43} from IMPAC, g(2+,356)/g(4+,876)=1.09 {I19} (1981St24). 
MOME2 Others: +2.5 {I11} if M(E2,4+,(877) to 2+,(356))=1.88 {I6} and M(E2,4+,(877) to 2+,(689))=0, (1988Fe08); or Q=2.3 {I11} (if M(E2,4+,(877) to 2+,(356)))=1.88 {I6} and M(E2)(4+,(877) to 2+,(689))=0.5 (1988Fe08) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T from B(E2) and branching of 779|g. Other: 6 ps {I3} (composite RDM, 1980Ke04). 
BE2 Weighted average of B(E2) 2+(356) to 0+(1135)=0.0056 {I10} (1992Li14) and 0.0061 {I+9-17} (1990Ma37 scaled by evaluators to B(E2)(0+ to 2+)=1.382 {I6}). 0.0044 {I20} (1979Bo31,1981Bo32) and 0.0045 {I9} (from M(E2 to 356)=0.15 {I3} (1986Gy04)). 
BE2 From 2+(689) to 0+(1135). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T weighted average of 2.9 ps {I6} (RDM 1981Bo32) and T{-1/2}=2.4 ps {I+11-3} from B(E2). 
BE2 From 2+(356) to 4+(1293). 1990Ma37 scaled by evaluators to B(E2)(0+ to 2+)=1.382 {I6}. Other: 0.002 {I4} (1992Li14). 
And 0.0054 {I18} (1979Bo31,1981Bo32). Others: M(E2,4+ to 2+(356))=0.164 {I27} (quoted by 1986Gy04). 
BE2 From 2+(689) to 4+(1293). 1990Ma37 scaled by evaluators to B(E2)(0+ to 2+)=1.382 {I6}. Other: 0.33 {I3} (1992Li14). Others: M(E2,4+ to 689)=1.26 {I13} (quoted by 1986Gy04). B(E2)=0.200 {I56} 
BE2 Weighted average of B(E2)(4+(1293) to 4+(877))=0.201 {I+73-26} (1990Ma37 scaled by evaluators to B(E2)(0+ to 2+)=1.382 {I6}), 0. 193 {I97} (1979Bo31,1981Bo32), and 0.084 {I14} (1992Li14 877 to 1293). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
T from B(E2) and adopted |g-ray properties. 
BE2 From 2+(356) to 2+(1362). 1990Ma37 scaled by evaluators to B(E2)(0+(0) to 2+(356))=1.382 {I6}. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
E from 1989Li05. 
T from B(E3) and adopted |g-ray properties. 
BE3 Weighted average of B(E3)(0+(0) to 3-(1447))=0.103 {I18} (1988Bo08), 0.116 {I14} (1992Po09) ({+196}Pt(e,e')), 0.099 {I10} ({+196}Pt(p,p'), 1988Co16), and 0.102 {I4} (1989Li05). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T weighted average of 1.0 ps {I3} (RDM,1981Bo32) and 0.98 ps {I+12-5} from B(E2). 
BE2 From 4+(877) to 6+(1526). 1990Ma37 scaled by evaluators to B(E2)(0+(0) to 2+(356))=1.382 {I6}. Other:0.64 {I4} (1992Li14). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T from weighted average of computed T{-1/2} from B(E2) and adopted |g-ray properties. 
BE2 From 4+(1293) to 6+(2007). 1990Ma37 scaled by evaluators to B(E2)(0+(0) to 2+(356))=1.382 {I6}. 
BE2 From 4+(877) to 6+(2007). 1990Ma37 scaled by evaluators to B(E2)(0+(0) to 2+(356))=1.382 {I6}. B(E2)=0.078 {I+151-72} (1990Ma37) 
BE2 From 6+(1526) to 6+(2007), calculated with the assumption |d(E2/M1)=-2.6. 1990Ma37 scaled by evaluator to B(E2)(0+(0) to 2+(356))=1.383 {I6}. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T computed from B(E2) and adopted |g-ray properties. 
BE2 From 6+(1526) to 8+(2253). 1990Ma37 scaled by evaluators to B(E2)(0+(0) to 2+(356))=1.382 {I6}. 


level_energy_unit: KEV
level_spin_parity: (7-,8+)
level_lifetime_unit: PS
level_comment:
T computed from B(E2) and adopted |g-ray properties. 
BE2 From 6+(2007) to 8+(2750). 1990Ma37 scaled by evaluators to B(E2)(0+(0) to 2+(356))=1.382 {I6}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E isomer shift in muonic atom: |DE(356)=0.39 keV {I+33-28} (1974Ba77) 
Isomer shift refers to the difference between the |g-transition energy in the muonic atom and that of the normal atom. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from gate on primary 5255|g in Clover detector together with 1978|g and 356|g gates on LaBr{-3}(Ce) detectors, effective |t(first 2+)+ |t(second 2+)=104 ps {I7}, from which |t(second 2+)=55 ps {I7} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from time spectra of 566|g-356|g cascade gated by 1046|g, effective |t(first 2+)+|t(third 0+)=54 ps {I7}, from which |t(third 0+)<12 ps using |t(first 2+)=49.2 ps {I2} from literature 
$No collective B(E2) values are found in this work for E2 transitions to the first 2+ and second 2+ states, the decay to the second 2+ state is forbidden by the So(6) selection rule. Half-life measurement in the present work provides a confirmation of this rule. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured isotope shift |d|n({+194}Pt,{+196}Pt)=+1.39 GHz {I27} (2017Hi05) 
$Measured |d<r{+2}>({+194}Pt,{+196}Pt)=+0.082 fm{+2} {I18} (2017Hi05) 
$Deduced <|b{-2}{+2}>{+1/2}=0.136 {I6} (2017Hi05) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
J J=1/2 from atomic beam (1976Fu06) and |p=- from L=1 in {+196}Pt(d,p) and {+198}Pt(p,d),(d,t). 
MOMM1 Other: +0.5 to +0.6 characterizes 1/2- g.s. of {+195}Pt, {+195}Hg, {+197}Hg 
T from 1992An13, |g(t) following |b-decay. Others: 19.96 h {I5} (2000Mo05), 18.3 h {I3} (1970Bo22), 18 h (1937Mc04), 20.00 h {I12} (1960Br11) scin |b{+-}, 17.5 h (1965Ha15) semi 77|g decay, 18 h (1965Ha15) semi 191|g decay. See also 1941Sh08, 1952Ch18, 1952Co12, 1952Ha16 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J E2 |g to 1/2-, L=3 in {+196}Pt(d,p) and {+198}Pt(p,d),(p,d). 
T from |g|g(t) measurements ({+197}Pt IT decay, 1982So05). Others: 18.5 ns {I15} (1967Ma46) and 16.5 ns {I15} (1970Ge01) 
MOMM1 Other: +0.851 {I25} (1989Ra17,1981Sa30,1982So05) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
From (I(|g+ce)(279|g)+I(|g+ce)(202|g))/I(|g+ce) (346|g). I|g(346|g):I|g(279|g):I|g(202|g)=100:0.21 {I2}:0.0031 {I12}$ 
J 13/2+ is also consistent with L=6 in {+196}Pt(d,p) and {+198}Pt(p,d),(d,t) and M4 |g to 5/2- 
T from |g(t) measurements in {+197}Pt IT decay (1982So05). Others: 94.4 min {I8} (1973Ur01, semi |g-decay curves), 95 min (1965Ha15), 83 min {I4} (1970Bo22), 96 min {I4} (1970Wi19). See also 1941Sh08, 1948Ho37, 1948Mo33, 1952Ch18, 1964Gr02, 1964Po05, 1964Pr06, 1970Wi19 
E 13/2+ isomerism in {+195}Pt and {+199}Pt occurs at 259 and 424 keV, respectively 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
May be doublet 
J J=7/2-,(3/2-); L=3,(1) in {+198}Pt(pol d,t). J=(1/2-,3/2-); L=1+3 in {+198}Pt(p,d). L(d,p)=(1). 


level_energy_unit: KEV
level_spin_parity: (5/2)-,(1/2-)
level_comment:
J J|p=(5/2)- from (pol d,t), J|p=(5/2-,1/2-) from (n,|g) E=thermal 
E unresolved doublet with L(d,t)=3, L(p,d)=3 for E=591 {I5}. L(t,p)=4 for E=590 {I4} is inconsistent with single-particle transfer values. Weakly populated in both reactions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J 1/2+,3/2+,5/2 from average resonance neutron capture in {+196}Pt(n,|g) E=2,24 keV; tentative (1/2)- from |s(|q) DWBA analysis (L=1) and vector analyzing power in {+198}Pt(pol d,t), too weakly populated in (pol t,d) and (d,t) reactions. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J L=1 in {+198}Pt(pol d,t) and primary |g-ray to this level in {+196}Pt(n,|g) E=2,24 keV. J|p=3/2- in (pol d,t), but too weakly populated. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2+)
level_comment:
J L=(4) in {+196}Pt(d,p), L=4 (1971WiYZ) IAR 
Configuration: (d,p) strength and L=4 suggest g9/2 neutron state 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T from |g|g(t) measurements (1982So05). Others: 18.5 ns {I15} (1967Ma46) (ce)(ce)(t), 16.5 ns {I15} (1970Ge01) |g|g(t) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T from |g(t) measurements (1982So05). Others: 94.4 min {I8} (1973Ur01) |g(t), 95 min (1965Ha15) semi 346|g, 83 min {I4} (1970Bo22) GM-counter |b{+-}, 96 min {I4} (1970Wi19) semi 346|g 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J from adopted levels for 854, 859 levels 
L L=3,4 in authors' table. L=3 in authors' figure 
S assumed J=5/2- 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (25/2-,27/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
T$ from decay curve of delayed |g rays (2011St21) 
$Experimental isomeric state population ratio |>5% {I2} 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$Decay modes from {+197}Pt Adopted Levels in the ENSDF database (Jan 2002 update) 
E,T$from {+197}Pt Adopted Levels in the ENSDF database, according to which the isomer decays to the 1/2- g.s. through 346.5|g, M4 |) 53.10|g, E2 |) |g cascade, forming a sequence of 399.50, 13/2+; 53.90, 5/2-; 0.0, 1/2- levels 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (25/2-)
level_lifetime_unit: NS
level_comment:
T$measured by 2019Wa22 using centroid-shift method. Other: 10.2 ns {I13} measured by 2011St21 (Phys. Rev. C 84, 044313) 
E$x is estimated as <100 keV by 2019Wa22. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T$Double |b{+-} decay to {+198}Hg. From measurements of double |b{+-} decay, half-life limits for decay to {+198}Hg g.s. have been determined: T{-1/2}(2|b{+-})|>3.5|*10{+18} y (2011Be32, value given for double |b{+-} decay to the 411.8 keV state of {+198}Hg including both two-neutrino and neutrinoless processes based on a fitted peak of 13 counts {I10}, which excludes 29 counts at 90% confidence level). 
|b{-2}, |b{-4}: From (|a,|a') and (p,p'), unweighted average. 
<r{+2}>{+1/2}=5.440 fm {I6} (2004An14). |D<r{+2}>=0.151 fm{+2} {I6} (1992Hi07), relative to {+194}Pt; other |D<r{+2}>=0.209 fm{+2} {I11}, |D<|b{+2}>=-0.0181 {I10} (1988Le22), relative to {+190}Pt; <|b{+2}>{+1/2}=0.11 (1981Mo24). 
J From L=0 in {+196}Pt(t,p) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T From B(E2)=1.090 {I7} (Coulomb excitation). Others: 24.0 ps {I8} (B(E2)=1.01 {I3}), 24.3 ps {I21} (1981Bo32), 23.3 ps {I11} (1980Ke04), 23.2 ps {I8} (1983St18) in Coulomb excitation. 
MOMM1 Transient field integral perturbed angular correlation (TF); and {+194}Pt standard (1995An15). Others: +0.70 {I6} (1993Ta07, TF; {+194}Pt standard), +0.59 {I7} (1991St04, TF), +0.69 {I6} (1981St13, TF; {+196}Pt standard), +0.62 {I10} (1979Ha06, TF; {+194}Pt standard) 
Q=+0.42 {I12} or +0.54 {I12} (1989Ra17,1986Gy04,2011StZZ) 
MOME2 Coulomb Excitation Reorientation(CER). Other: +1.2 {I5} (1969Gl08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 Re-evaluated data. Other: +0.72 {I13} (1981St13, TF; {+196}Pt standard) 
|b{-2}: From (p,p'), (p,p'|g). 
J From |g(|q) in {+198}Pt(n,n'),(n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
|m=+1.2 {I2} (1992Br03,2011StZZ, Re-evaluated). Other: +1.4 {I3} (1981St13. TF; {+196}Pt standard) 
|b{-4}: From (p,p'), (p,p'|g). 
J From |g(|q) in {+198}Pt(n,n'),(n,n'|g). 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
T From ce(t) in {+198}Pt(d,pn|g). 
$Configuration=(((|ph{-11/2}){+-1}d{-3/2})+((|ni{-13/2}){+-1}p{-1/2})) (1987CoZY). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J From interacting boson approximation calculations and systematics of even Pt isotopes (1981Bo32). 


level_energy_unit: KEV
level_comment:
L=3 suggested by 1976Ba35 in (|a,|a') for E=1722 probably corresponds to the 1680 level. L(1722)=3 is not confirmed by 1981De12. 


level_energy_unit: KEV
level_spin_parity: (12-)
level_lifetime_unit: NS
level_comment:
E$It is assumed that the isomer decays directly by 337|g, but possibility of a low-energy |g transition preceding 337|g is not ruled out 
T$(Target like recoil fragments)|g(t) (2004Va03,2004Re11); 407|g and 658|g double |g-ray gates. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
L=3 probably corresponds to the 1680 level. L(1722)=3 is not confirmed by 1981De12 in (p,p'),(p,p'|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T Deduced from B(E2)=1.090 {I7} 
B(E2): Adopted value=1.090 {I7} (1986Gy04). Others: 1.01 {I5} (1969Gl08), 1.02 {I15} (1966Gr20), 0.97 {I3} (1970Br26), 1.02 {I4} (1971Mi08), 1.06 {I3} (1984Mu19). 
G= 0.21 3 (1967Ka16), 0.324 26 (1981St13,1983St18), 0.225 32 (1983St01), +0.293 34 (1991St04). OTHER: 1979Ha06 
MOME2: 1.2 5 (1969Gl08), 0.42 12 OR 0.54 12 (1986Gy04). 
Q=+0.42 {I12} or +0.54 {I12} (1986Gy04) 
T Others: 24.3 ps {I21} (1981Bo32), 23.2 ps {I8} (1983St18). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured isotope shift |d|n({+194}Pt,{+198}Pt)=+2.43 GHz {I23} (2017Hi05) 
$Measured |d<r{+2}>({+194}Pt,{+198}Pt)=+0.143 fm{+2} {I20} (2017Hi05) 
$Deduced <|b{-2}{+2}>{+1/2}=0.122 {I8} (2017Hi05) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
T$weighted average of 30.8 min {I4} (1967Ba45), 30.6 min {I3} and 31.4 min {I5} (1965Bl18). Others: 30.79 min (1992An13), 30 min {I3} (1956Le44), 29 min {I1} (1941Sh08), 31 min (1937Mc04) 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
%B-$From log| {Ift}>5.1 to (11/2)- level in {+199}Au, %|b{+-}<0.06 
J$corresponds to i{-13/2} orbital; E3, M1 cascade to g.s.; systematics 
T$weighted average of 13.3 s {I2} (1973Ur01), 14.1 s {I3} (1959Wa15) 
$ 1993Ro22 ANALYZED ^Q{-0} FACTOR 


level_energy_unit: KEV
level_comment:
E$possibly the same as the 424 isomer; however, the discrepancy in measured energy suggests separate levels. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
J expect 3/2- or 5/2- in this region. Supported by M1 assignment to 32-keV |g. 
T from 'adopted levels' 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (25/2-,27/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
T$ from decay curve of delayed |g rays (2011St21). 
$Experimental isomeric state population ratio |>5% {I2} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+198}Pt,{+199g}Pt)=+2.13 GHz {I41} (2017Hi05) 
$Measured |d<r{+2}>({+194}Pt,{+199g}Pt)=+0.268 fm{+2} {I34} (2017Hi05) 
$Deduced <|b{-2}{+2}>{+1/2}=0.144 {I10} (2017Hi05) 
MOMM1,MOME2$from hyperfine structure in in-gas-cell laser ionization spectroscopy. The statistical and systematic uncertainties of 0.08 and 0.01 in |m respectively are combined. 
T$from |b-decay curve (2017Hi05). This value can be compared with 30.80 min {I21} in {+199}Pt Adopted Levels in the ENSDF database (Oct 2006 update) 
$543-keV |g ray from {+199}Pt to {+199}Au decay seen in the spectrum 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Measured isotope shift |d|n({+198}Pt,{+199m}Pt)=+0.39 GHz {I39} (2017Hi05) 
$Measured |d<r{+2}>({+194}Pt,{+199m}Pt)=+0.166 fm{+2} {I30} (2017Hi05) 
$Deduced <|b{-2}{+2}>{+1/2}=0.110 {I12} (2017Hi05) 
$Decay mode from {+199}Pt Adopted Levels in the ENSDF database 
MOMM1,MOME2$from hyperfine structure in in-gas-cell laser ionization spectroscopy. The statistical and systematic uncertainties of 0.05 and 0.02 in |m respectively are combined. 
T$from decay curve for 392|g (2017Hi05). This value can be compared with 13.6 s {I4} in {+199}Pt Adopted Levels in the ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (7-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x|<90 keV is suggested in {+9}Be({+208}Pb,X|g) (2005Ca02); x|<50 keV is suggested in {+9}Be({+208}Pb,X|g) (2011St21) 
J$From systematics of even-even Pt isotopes. 
T$Weighted average of 14.3 ns {I6} in {+198}Pt(t,p|g) (1988Ya03) and 14.0 ns 6 in {+9}Be({+208}Pb,X|g) (2005Ca02). Other: 17.0 ns {I5} from |g(t) in 2011St21. 
CONF$Possible |p (d{-3/2}{+-1},h{-11/2}{+-1}) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (12+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$y= x + |<90 keV is suggested in {+9}Be({+208}Pb,X|g) (2005Ca02) 
J$From syst of neighboring even-even Pt and Hg isotopes 
T$Weighted average of 10.3 ns {I24} (2005Ca02) and 13.9 ns {I10} (2011St21), both from |g(t) in {+9}Be({+208}Pb,X|g) 
CONF$Possible |n(i{-13/2}{+-2}) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (7-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x |<90 keV in 2005Ca02 and x |<50 keV in 2011St21 
T$From 464|g(t) and 470|g(t) in 2005Ca02. Other: 17.0 ns {I5} from |g(t) in 2011St21. The survival of this short-lived isomer through the Fragment Recoil Separator (time of flight |?300 ns) is explained by 2005Ca02 with the suppression of the electron conversion for highly-charged ions. 
$Experimental isomeric state population ratio |>25% (2005Ca02) and |>7% {I4} (2011St21) 
$Possible configuration=|p (d{-3/2}{+-1},h{-11/2}{+-1}) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=LT;ERR=?
level_spin_parity: (12+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From systematics of similar structures in neighboring nuclei, as suggested in 2005Ca02 
T$Weighted average of 10.3 ns {I24} (2005Ca02) and 13.9 ns {I10} (2011St21). The survival of this short-lived isomer through the Fragment Recoil Separator (time of flight |?300 ns) is explained by 2005Ca02 with the suppression of the electron conversion for highly-charged ions 
$Experimental isomeric state population ratio |>4% (2005Ca02) and |>2% {I1} (2011St21) 
$Possible configuration=|n (i{-13/2}{+-2}) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (7-)
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$From 299.0|g(t) and 463.4|g(t) in 1988Ya03 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured isotope shift |d|n({+198}Pt,{+200}Pt)=+2.69 GHz {I41} (2022Hi07) 
$Measured |d<r{+2}>({+194}Pt,{+200}Pt)=+0.295 fm{+2} {I30} (2022Hi07) 
$Deduced <|b{-2}{+2}>{+1/2}=0.107 {I11} (2022Hi07) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MIN
level_comment:
J$From systematics in neighboring N=123 nuclides and shell model predictions 
T$Weighted average of 2.5 m {I1} (1963Go06) and 2.3 m {I2} (1962Fa06) 
CONF$|n f{-5/2}{+-1}. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<90 keV in both 2005Ca02 and 2011St21. Direct |g-ray decay to the 1455.5 keV level was not observed 
T$from |g(t) in 2011St21. Other: 21 ns {I3} from |g(t) in 2005Ca02 
CONF$|n (f{-5/2}{+-1}) |p (d{-3/2}{+-1},h{-11/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<90 keV in both 2005Ca02 and 2011St21. Direct |g-ray decay to the 1455.5 keV level was not observed 
T$from |g(t) in 2011St21. Other: 21 ns {I3} from |g(t) in 2005Ca02 
CONF$|n (f{-5/2}{+-1}) |p (d{-3/2}{+-1},h{-11/2}{+-1}). The assignment is tentative 
$Experimental isomeric state population ratio |>32% (2005Ca02) and |>4% {I2} (2011St21) 


level_energy_unit: KEV
level_comment:
$Measured isotope shift |d|n({+198}Pt,{+201}Pt)=+2.31 GHz {I135} for J=1/2-, +0.35 GHz {I134} for J=3/2- and +4.20 GHz {I171} for J=5/2- (2022Hi07) 
MOMM1$0.044 {I7} for J=1/2-, -0.83 {I15} for 3/2- and +0.86 {I21} for 5/2- (2022Hi07) 
$Measured |d<r{+2}>({+194}Pt,{+201}Pt)=+0.287 fm{+2} {I81} for J=1/2, +0.172 fm{+2} {I79} for J=3/2- and +0.398 fm{+2} {I104} for J=5/2- (2022Hi07) 
MOME2$-2.7 {I45} for J=3/2- and +1.0 {I39} for J=5/2- (2022Hi07) 
$Deduced <|b{-2}{+2}>{+1/2}=0.073 {I45} for J=1/2- and 0.120 {I35} for 5/2- (2022Hi07) 
J$1/2- or 5/2- is preferred from <|b{-2}{+2}>{+1/2} systematics 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$Using 439.6|g(t) in {+202}Hg produced in {+202}Pt |b{+-} -> {+202}Au |b{+-} (T{-1/2}=28.4 s) -> {+202}Hg in 1992Sh12 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$From |g(t) in 2011St21. Other: 280 |ms {I+420-190} in 2005Ca02 
CONF$ |p(d{-3/2}{+-1},h{-11/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$From |g(t) in 2011St21. Other: 280 |ms {I+420-190} in 2005Ca02 
CONF$ |p(d{-3/2}{+-1},h{-11/2}{+-1}) 
$Experimental isomeric state population ratio=12% {I+1-2} (2011St21) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_comment:
T$From |b-|g(|Dt) analysis in 2014Mo15. Other: 10.1 s {I30} (2005KuZU) probably associated with the decay of the J|p=(13/2+) isomeric state (2013Mo20) 
$Configuration=|n(p{-1/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_uncertain: ?
level_comment:
T$From 2013Mo20, using 367|g(t) and 353|g(t). Other: 10.1 s {I30} (2005KuZU), associated with the ground state 
$Configuration=|n(i{-13/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (27/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Probably a long-lived isomeric state (2011St21) 
$Configuration=|n(i{-13/2}{+-1})|p[h{-11/2}{+-1},d{-3/2}{+-1}(7-)]. The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (33/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
T$From 1104|g(t) in 2011St21. 
$Experimental isomeric ratio=1.3% {I2} (2011St21) 
$Configuration=|n(i{-13/2}{+-1})|p[(h{-11/2}{+-2})(10+))]. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_comment:
J$Direct |b{+-} feeding to J=1/2 and 3/2 states in the daughter {+203}Au nucleus (2013Mo20); shell model predictions and similarity with the {+205}Hg and {+207}Pb (N=125) isotones 
T$From |b-|g(|Dt) analysis in 2014Mo15. Other: 10.1 s {I30} (2005KuZU) probably associated with the decay of the J|p=(13/2+) isomeric state (2013Mo20) 
$Configuration=|n(p{-1/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_uncertain: ?
level_comment:
%B-$ This branch was tentatively suggested in 2013Mo20, but the evaluator found no convincing evidences about its existence. See the comment with the 353|g in the {+9}Be({+208}Pb,X|g) data set 
T$From 2013Mo20, using 367|g(t) and 353|g(t). Other: 10.1 s {I30} (2005KuZU), associated with the ground state 
$Configuration=|n(i{-13/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (33/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
T$From 1104|g(t) in 2011St21. 
$Experimental isomeric ratio=1.3% {I2} (2011St21) 
$Configuration=|n(i{-13/2}{+-1})|p[(h{-11/2}{+-2})(10+)]. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$Weighted averages of 10.4 s {I18} (165|g(t)) and 10.1 s {I22} (305|g(t)) in 2009Mo17. The 165|g and 305|g were identified in 2009Mo17 as belonging to {+204}Au, produced following |b{+-} decay of {+204}Pt 


level_energy_unit: KEV
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$The energy of this level depends on the order of the 872|g and 1123|g, which could not be determined experimentally in {+9}Be({+208}Pb,X|g), but were placed based on comparison with the {+206}Hg level scheme and shell-model calculations. If the |g's are interchanged, this level energy is instead 1123 keV. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (7-)
level_lifetime_unit: US
level_comment:
E$|g decay to the 1995-keV level is expected, but not observed. 2008St20 suggest E|g is below the K x-ray threshold of 78.4 keV due to the absence of observed x rays associated with this decay. Such a low-energy transition would be dominated by internal conversion. 
$Proposed configuration: |p[(d{-3/2}){+-1}(h{-11/2}){+-1}]. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8+)
level_uncertain: ?
level_comment:
E$The energy of this level depends on the order of the 1061|g and 97|g, which could not be determined experimentally in {+9}Be({+208}Pb,X|g), but were placed based on comparison with the {+206}Hg level scheme and shell-model calculations. If the |g's are interchanged, this level energy is instead 2092+x keV. 
$Proposed configuration: |p[(h{-11/2}){+-2}]. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$The energy of this level depends on the order of the 872|g and 1123|g, which could not be determined experimentally in this study, but were placed based on comparison with the {+206}Hg level scheme and shell-model calculations. If the |g's are interchanged, this level energy is instead 1123 keV. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8+)
level_uncertain: ?
level_comment:
E$The energy of this level depends on the order of the 1061|g and 97|g, which could not be determined experimentally in this study, but were placed based on comparison with the {+206}Hg level scheme and shell-model calculations. If the |g's are interchanged, this level energy is instead 2092+x keV. 
$Proposed configuration: |p[(h{-11/2}){+-2}]. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
E$observed activity is assumed to correspond to decay of g.s. 
T$measured by 2014Mo15, from analysis of complex time-correlated structures by Monte Carlo simulations of experimental (ion)|b(|g) and |b(|g)(ion) correlations corresponding to time difference between implanted nuclei and subsequent |b-delayed |g transitions in the first case, and between implantations and preceding |g rays in the second. Ratio of the two correlations is an indicator of of half-life of the isotope being measured. Other: 10.3 s {I14} in {+204}Pt Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$From systematics of single-particle structures above N=126 
T$>300 ns from the time-of-flight in 2017Ca12, but the actual lifetime is expected to be much longer 
CONF$|n(g{-9/2}{++1}) and spherical shape 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
T$ >160 ns from tof in 2012Ku26. Others: 500 ms (2021Ko17,systematics), 20.7 s (2019Mo01,theory), 516 ms (2016Ma12,theory), 49 s (2020Ne08,theory), 600 ms (2011Bo26,theory) 
$ Production |s=0.033 nb {I11} (2012Ku26) 


level_energy_unit: KEV
level_comment:
$Only the |b{+-} decay is expected, followed possibly by |b{+-}n decay from theoretical T{-1/2}(|b)=9.2 s, T{-1/2}(|a)>10{+20} s (2019Mo01), thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=9.2 s, %|b{+-n}=1 (2019Mo01) 
$Theoretical T{-1/2}= 
E$observed {+207}Pt fragments are assumed to correspond to the g.s. 
J$|W{-n}=3/2+ (theory, 2019Mo01); 9/2+ (syst, 2021Ko07) 
T$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 9.2 s from theoretical calculations (2019Mo01), and 600 ms from systematics (2021Ko07). From a decreasing trend of half-lives with increasing neutron number in neutron-rich nuclei, expected T{-1/2}<10 s from known half-lives of 10.3 s for {+204}Pt, 22 s for {+203}Pt and 44 h for {+202}Pt. 
$Production |s=0.008 nb {I3} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ Predicted %|b{+-}n=5 (2019Mo01) 
E$the observed {+208}Pt fragments are assumed to correspond to the g.s. 
T$ > 160 ns from time-of-flight in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by T{-1/2}=9.2 s from theoretical calculations (2019Mo01) 
$ Production |s=0.0027 nb {I15} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
J unhindered |a decay to (2-) {+166}Ir. The likely g.s. orbital for {+171}Au and {+173}Au is (|p s{-1/2}), but in {+166}Ir the proton occupies the d{-3/2} orbital; analysis of {+170}Au p decay data indicates |Dl=2 transition to (7/2-) {+169}Pt (2004Ke06). 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E based on E|a=7107 {I6} from this level to E=172 {I6} level in {+166}Ir and E|a=7001 {I10} for {+170}Au(g.s.) to {+166}Ir(g.s.) transition (2004Ke06). E=282 {I13} based on E(p)=1743 {I6} and 1463 {I12}, respectively, for proton decay to {+169}Pt(g.s.) from this level and from {+170}Au(g.s.) (2004Ke06). 
J h{-11/2} proton emission observed from level (2004Ke06, 2002Ma61). Unhindered |a decay to (9+) {+166}Ir. Configuration probably includes (|p 11/2[505]) orbital (as in isomeric {+171}Au and {+173}Au), possibly coupled to f{-7/2} neutron (as in isomeric {+166}Ir). 
T other value: 0.57 ms {I+31-15} (2002Ma61). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_comment:
T$from 2004Ke06. Others: 17 |ms {I+9-5} (1999Po09), 37 |ms {I+7-5} (2003Bb21). 
%P$from 2004Ke06. Other: existence of a p decay branch is implied in 1997Da07 by observation of {+170}Pt |a decay following unobserved {+171}Au p decay. 
J$configuration=(|p s{-1/2}) (1999Po09, 2004Ke06) based on consistency between proton partial T{-1/2} calculated for s{-1/2} orbital (using WKB approximation) and observed partial T{-1/2}; analogous to low-lying structure of neighboring nuclides. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
%A$weighted average of 66 {I4} (2004Ke06) and 54 {I4} (1997Da07). 
T$weighted average of 1.09 ms {i3} (2004Ke06) and 1.014 ms {i19} (2003Bb21). The value from 2004Ke06 is an average of 1.13 ms {I5} from p(t) and 1.07 ms {I3} from |a(t) while the value from 2003Bb21 is combined from measured |a and p branches. Other: 1.02 ms {I10} (1997Da07). 
E$from E(p)=1694 {I6} to {+170}Pt g.s. from this level and E(p)=1437 {I12} from {+171}Au(g.s.) to {+170}Pt g.s. in 2004Ke06. Others: 250 {I16} (1999Po09), based on E(p)=1692 {I6} (1997Da07) and E(p)=1444 {I17} (1999Po09), respectively, for protons feeding the {+170}Pt g.s from this level and from the {+171}Au g.s. Also, based on observed E(p) from this level compared with E(p) limits calculated for the (1/2+) level using 1 |ms |< T{-1/2} |< 30 |ms and the WKB barrier transmission approximation, 1997Da07 estimate E |> 100 keV and E |< 260 keV for the (11/2-) level. 1997Da07 obtain an independent estimate of E=220 {I110} for this state, based on trends of the (1/2+) to (11/2-) level-energy differences from {+151}Tm to {+167}Ir. 
J configuration=(|p h{-11/2}) (1997Da07, 2004Ke06) based on comparison of proton partial T{-1/2} calculated for h{-11/2} orbital (using WKB approximation) with the observed value. An isomeric 11/2[505] level also occurs in {+173}Au at comparable energy (E=214 {I23}, 1999Po09). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%A |a decay only has been observed but proton and |e+|b{++} decay are possible. Calculated T{-1/2}(|e+|b{++})|?0.9 s (1973Ta30) from gross |b decay theory and 0.27 s (1997Mo25) imply %|e+%|b{++}|?2.4 and 8.1, respectively. 
T from 6762|a(t) (2009Ha42). 
J possible configurations: |p (s{-1/2},d{-3/2}) ~# |n (f{-7/2},h{-9/2}) or |p (s{-1/2},d{-3/2}) ~# |n i{-13/2} (2009Ha42). Possibly J|p=(3-), analogous to that suggested by 2004GoZZ for {+174}Au and {+176}Au. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J possibly (9+), analogous to that suggested by 2004GoZZ for {+174}Au and {+176}Au; very tentative value (2009Ha42). Possible configurations: |p h{-11/2} ~# |n i{-13/2} or |p h{-11/2} ~# |n (f{-7/2},h{-9/2}) (2009Ha42). 
T unweighted average of 9 ms {I+2-1} from 6870|a(t) (2009Ha42) and 6.3 ms {I15} from 6878|a(t) (1996Pa01). Others: 4 ms {I1} (1993Se09, from time difference of implanted fragments and decay events); 8 ms {I+5-2} from 6800|a(t) (2009Ha42). 
%A,%P |a decay only has been observed. Proton decay is possible, but 2009Ha42 and 1993Se09 set upper limits on %p of 0.02 (from correlation between 6453|a from {+171}Pt and any preceding {+172}Au decay) and 2, respectively. No experimental information about |e+|b{++} decay of {+172}Au is available, but gross |b decay theory (1973Ta30) predicts T{-1/2}(|e+|b{++})|?0.9 s which implies %(|e+|b{++})|?0.9. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E an alternative value of 896.2+x is possible because the order of 289|g and 437|g has not been established. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_uncertain: ?
level_comment:
E an alternative value of 1282.0+x is possible because the order of 460|g and 545|g has not been established. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: MS
level_comment:
T from 6762|a(t), as stated in table I from 2009Ha42; value in abstract is 22 ms {I+6-5} and that in fig. 3 is 22 ms {I6}. 
J possible |p (s{-1/2},d{-3/2}) ~# |n (f{-7/2},h{-9/2}) or |p (s{-1/2},d{-3/2}) ~# |n i{-13/2} state (2009Ha42). Possibly J|p=(3-) analogous to {+174}Au and {+176}Au (2009Ha42). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J Possible |p h{-11/2} ~# |n (f{-7/2},h{-9/2}) state. Possibly (9+), analogous to {+174}Au and {+176}Au; very tentative value (2009Ha42). 
T from 6870|a(t). Other: 8 ms {I+5-2} from 6800|a(t) (2009Ha42). Adopted value is 7.7 ms {I15}. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: MS
level_comment:
%EC+%B+ |?6 based on gross |b decay theory (1997Mo25); only |a decay observed, consistent with observed %|a. 
T$From a(t) (2012Th13) Other: 25 ms {I1} from 6890|a-|g(t) (2001Ko14). 
T from a-|g(t) in {+92}Mo({+84}Sr,p2n|g). Other: 20 ms {I+9-6} (1999Po09). 
J unhindered |a decay from (1/2+) {+177}Tl. Probable configuration=(|p 1/2[400]). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$From |a decay of {+173}Au isomer (2012Th13). Others: 14 ms {I1} from 6740|a-|g(t) in {+92}Mo({+84}Sr,p2n|g) (2001Ko44), 12 ms {I+3-2} (1999Po09), 15 ms {I2} (1996Pa01), 59 ms {I+45-18} (1983Sc24). 
E from {+177}Tl |a decay (0.23 ms). 
J unhindered |a decay from (11/2-) {+177}Tl. Probable configuration=(|p 11/2[505]). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E from E|a=6907 {I7} and 7487 {I13} for |a decay from g.s. and E=807 {I18} level of {+177}Tl, respectively (1999Po09). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: MS
level_comment:
T$Measured E|a=6688 keV {I14} from |a decay of {+173}Au g.s. (2012Th13) Other: 25 ms {I1} from 6890|a-|g(t) (2001Ko14). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$Measured E|a=6739 keV {I15} from |a decay of {+173}Au isomer (2012Th13) Other: 14 ms {I1} from 6740|a-|g(t) (2001Ko14) 
E$from adopted levels, x=214 {I23}. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from 1983Sc24. Other value: 171 ms {I29} (1996Pa01). 
{+174}Au was identified by 1983Sc24 from excitation-function measurements for |a emitters produced in {+92}Mo bombardments of Mo and Rb targets. Measured E|a, semi. 
{+174}Au was produced in heavy-ion fusion-evaporation reactions, and separated using a recoil mass separator. Measured E|a, semi (1996Pa01). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
%A From 1983Sc24. 
J$Favored alpha decay (HF|?2.1) to {+171}Ir (J|p=(11/2-)). 
T$Weighted average of 158 ms {I3} (2002Ro17) and 143 ms {I8} (2001Ko44). Others: 185 ms {I30} (1996Pa01), 200 ms {I22} (1983Sc24). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (13/2+)
level_comment:
(|p13/2(606)) oblate configuration based on similarity to analogous |p=+ sequences in heavier Tl nuclides (2001Ko44). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$From adopted levels. 
E$From a suspected doublet of 6438|a and 6412|a of {+175}Au |a decay (2002Ro17), it seems that 6568|a is a g.s. to g.s. transition from {+179}Tl (0.23 s) to {+175}Au, and the observed 7069|a and 7213|a 's are from 0.0+x to 0.0+x state transitions between {+179}Tl(1.5 ms) and {+175}Au (1998To14). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
J$From adopted levels. 
E$From a suspected doublet of 6438|a and 6412|a of {+175}Au |a decay (2002Ro17), it seems that 6568|a is a g.s. to g.s. transition from {+179}Tl (0.23 s) to {+175}Au, and the observed 7069|a and 7213|a 's are from 0.0+x to 0.0+x state transitions between {+179}Tl(1.5 ms) and {+175}Au (1998To14). The 1/2+ g.s. and 11/2- isomeric state, from systematics and experiment, for these isotopes also looks reasonable for these transitions with low HF values. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (13/2+)
level_comment:
(|p 13/2[606]) oblate configuration based on similarity to analogous |p=+ sequences in heavier Tl nuclides (2001Ko44). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_comment:
T$ measured in 2011Wa37 from time difference between recoil implantations and |a decays from {+175}Au 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J {+176}Au's 6282|a decays from this isomeric state to the 4.4 s state, which is assigned a spin of 3 based on beta decay feeding to the 2+ and 4+ states of the yrast band in {+172}Os (1992Sc16). Following 5520|a from the {+172}Ir to the excited state of {+168}Re and coincident 123|g E1 transition, a spin of (3-) is assigned for the 1.05 s isomeric state in 2004GoZZ. Possible configuration |p1/2[411]+|n7/2[503]. 
T From |a(t) in {+94}Mo({+84}Sr,pn|g) (2004GoZZ). Others: 0.83 s {I14} [from |t=1.2 s {I2} in 1999Da18], 1.00 s {I20} (1990SeZW), 0.84 s {I+17-14} (2002Ro17), 1.25 s {I30} (1975Ca06 - determined from 6260|a(t) - this E|a is not present in other reports). 
|a decay is reported in 2004GoZZ, 2002Ro17, 1975Ca06; and |b{++}/|e decay in 1999Da18. From feeding pattern into the {+176}Pt levels from {+176}Au |b{++}/|e decay, it is concluded that {+176}Au may have more than one |b-decaying states. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (9+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
J Assigned in {+94}Mo({+84}Sr,pn|g) (2004GoZZ) based on the strong beta decay feeding assumption from this state to the 8+ state in {+176}Pt (1999Da18). Possible configuration |p11/2[505]+|n7/2[503]. 
T From weighted average of 6080|a(t), 6117|a(t), and sum line of 6220 keV (t) [6080+212-K, 6117+175-K] in {+94}Mo({+84}Sr,pn|g) (2004GoZZ). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J {+176}Au's 6282|a decays from this isomeric state to the 4.4 s state, which is assigned a spin of 3 based on beta decay feeding to the 2+ and 4+ states of the yrast band in {+172}Os (1992Sc16). Following 5520|a from the {+172}Ir to the excited state of {+168}Re and coincident 123|g E1 transition, a spin of (3-) is assigned for the 1.05 s isomeric state in 2004GoZZ. Possible configuration |p1/2[411]+|n7/2[503]. 
T From 6282|a(t). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (9+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J Assigned in 2004GoZZ based on the strong beta decay feeding assumption from this state to the 8+ state in {+176}Pt (1999Da18). Possible configuration |p11/2[505]+|n7/2[503]. 
T From weighted average of 6080|a(t), 6117|a(t), and sum line of 6220 keV (t) [6080+212-K, 6117+175-K] in 2004GoZZ. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 4,5-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$configuration=[|pd{-3/2}~#|nf{-7/2}]{-4,5{+-}}, private communication by 2017An16 with the first author of 2017Ba04. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7+,8+,9+)
level_comment:
J$from fits to hyperfine spectrum and comparison of |m to theoretical predictions. 
%A$from comparison of number of decays of {+176}Au and the |b decay daughter {+176}Pt. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (2-,3-)
level_comment:
J$from fits to hyperfine spectrum and comparison of |m to theoretical predictions. 
MOMM1$ranges from 5.25 {I25} to 5.36 {I26} for J=7+ to 10+ and the Ekstrom approach and 5.09 {I19} to 5.20 {I20} for J=7+ to 10+ and applying a RHFA correction (2021Ha32) 
%A$from comparison of number of decays of {+176}Au and the |b decay daughter {+176}Pt. 
MOMM1$ranges from -0.767 {I43} to -0.873 {I55} for J=2- to 5- and different configurations, using the Ekstrom approach (2021Ha32) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3,4,5)
level_comment:
$|d|n{-176,197}=43340 MHz {I640} for J=3, 42860 MHz {I660} for J=4, and 45220 MHz {I700} for J=5 (2023Cu04). 
$|d<r{+2}>{+176,197}=-1.091 fm{+2} {I16} (stat) {I31} (syst) for J=3, -1.079 fm{+2} {I16} (stat) {I31} (syst) for J=4, and -1.071 fm{+2} {I16} (stat) {I31} (syst) for J=5 (2023Cu04) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (8,9)
level_comment:
$|d|n{-176,197}=42580 MHz {I310} for J=8 and 43070 MHz {I370} for J=9 
$|d<r{+2}>{+176,197}=-1.072 fm{+2} {I8} (stat) {I31} (syst) for J=8 and -1.085 fm{+2} {I9} (stat) {I31} (syst) for J=9 (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
%A$From 2009An14. %|e+|b{++} decay has not been directly measured. Other: %|a=35 (1975Ca06) 
J$J=1/2 from hyperfine splitting (2018Cu04); |p from |m; Favored alpha decay of {+181}Tl g.s. (J|p=1/2+); J|p systematics in neighboring odd-Z nuclei 
T$Unweighted average of 1.53 s {I7} (2009An14), 1.462 s {I32} (2001Ko44) and 1.511 s {I13} (2014AlZX). 
MOMM1$From hyperfine anomaly (2018Cu04) 
$E|a=6159 keV {I7} (2018Cu04), 6161 keV {I7} (2009An14), 6156 keV {I6} (2001Ko44), 6153 keV {I6} (2014AlZX), 6186 keV {I10} (1996To01), 6150 keV {I10} (1973Ga08), 6154 keV {I10} (1996Pa01) and 6180 keV {I20} (1993BoZK,1992BlZW,1992BoZO). 
CONF$|p(s{-1/2}{+-1}). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$From systematics of similar structures in neighboring nuclei and the proposed configuration. The assignment is tentative. Other: J|p=(5/2+) in 2009An14. 
CONF$|p(d{-3/2}{+-1}). The assignment is tentative. 


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 
%A$From 2009An14. %|e+|b{++} decay has not been directly measured. Other: %|a=65 (1975Ca06) 
J$Favored |a decay to the {+173}Ir isomeric state (J|p=11/2-); J|p systematics in neighboring odd-Z nuclei and proposed configuration 
T$Unweighted average of 1.180 s {I12} (2001Ko44) and 1.205 s {I3} (2014AlZX). Others: 1.0 s {I2} (2009An14), 1.3 s {I4} (1968Si01), 1.3 s {I2} (1996Pa01), 1.18 s {I7} (1991Se01) and 1.3 s {I1} (1975Ca06) 
$E|a=6124 keV {I7} (2009An14), 6122 keV {I6} (2001Ko44), 6118 {I6} (2014AlZX), 6118 keV {I9} (1996Pa01), 6110 keV {I10} (1975Ca06), 6110 keV {I10} (1973Ga08) and 6115 keV {I100} (1968Si01). 
CONF$Spherical (weakly-deformed) |p(h{-11/2}{+-1}) configuration. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (13/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$Systematics of similar structures in neighboring nuclei; proposed configuration 
CONF$Well-deformed |p1/2[660] (i{-13/2}) band member. 
$Coincidence relationship requires that this level decays to the 713.5-keV level. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J,T$From adopted levels. Values in (HI,xn|g): 1.462 s {I32} (2001Ko44) and 1.511 s {I13} (2014AlZX), using |a(t) 
CONF$|p(s{-1/2}{+-1}) orbital 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$From adopted levels. Values in (HI,xn|g): 1.180 s {I12} (2001Ko44) and 1.205 s {I11} (2014AlZX), using |a(t) 
CONF$|p(h{-11/2}{+-1}), spherical (weakly-deformed) shape 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (13/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Coincidence relationship requires that this level decays to the 713.5-keV level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_comment:
E,J$from the Adopted Levels of {+177}Au in the ENSDF database (2019 update) 
MOMM1$from hfs measurement using hyperfine anomaly of {+197}|D(6s)=0.1134 {I58} for l=11/2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: S
level_comment:
T$from |a(t) (2021Ha32) 
J$from the Adopted Levels of {+177}Au in the ENSDF database. 
E$from Venhart et al., PLB 806, 135488 (2020). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J,MOMM1$taken by 2020Ve03 from 2018Cu04 (Phys. Lett. B786, 355; hyperfine structure measurements) 
$T{-1/2} and decay modes from {+177}Au Adopted Levels in the ENSDF database (August 2019 update) 
$E|a=6161 {I7} from the decay of {+177}Au g.s. (2009An14: Phys. Rev. C 80, 024302) 
$Compiler's note: 2020Ve03, erroneously, quote in their Fig. 1, T{-1/2}=1.18 s, E|a=6.12 MeV, which correspond to the values for the isomer decay 
$Configuration=|p3s{-1/2}{+-1} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$J|p, T{-1/2} and decay modes from {+177}Au Adopted Levels in the ENSDF database (August 2019 update) 
$E|a=6124 {I7} from the decay of {+177}Au, (11/2-) isomer (2009An14: Phys. Rev. C 80, 024302) 
$Compiler's note: 2020Ve03, erroneously, quote in their Fig. 1, T{-1/2}=1.46 s, E|a=6.16 MeV, which correspond to the values for the g.s. decay 
$Configuration=|p1h{-11/2}{+-1} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2+)
level_comment:
$The (9/2+) state is interpreted (2020Ve03) as an anti-aligned coupled state: |p1i{-13/2}~#(2+ state of neighboring even-even core). This level is expected to be mixed with the (unknown) 9/2+ member of the g.s. band, expected at 700-760 keV 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (13/2+)
level_comment:
$In comparison with decay of the (13/2+) level in {+179}Au, this level is expected to decay to the (13/2-) level at 713.4 keV, and to the (11/2-) level at 713.9 keV through low-energy, highly converted E1 transitions 


level_energy_unit: KEV
level_spin_parity: 1/2
level_comment:
$|d|n{-177,197}=39290 MHz {I220} (2023Cu04). 
$|d<r{+2}>{+177,197}=-0.990 fm{+2} {I5} (stat) {I29} (syst) (2023Cu04) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2)
level_comment:
$|d|n{-177,197}=37860 MHz {I250} (2023Cu04). 
$|d<r{+2}>{+177,197}=-0.954 fm{+2} {I6} (stat) {I28} (syst) (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_comment:
MOMM1$from fit to hfs spectra using Voigt profiles taking into account hyperfine anomaly by application of the Moskowitz-Lombardi empirical rule (2018Cu04) 
J$from observed three components to the hfs spectrum (2018Cu04) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
Three |a transitions observed in the decay of {+178}Au: 5980 keV (I|a=23.5%), 5920 keV (I|a=65.9%), 5850 keV (I|a=10.6%) (1986Ke03). Other values: E|a=5920 {i10} keV (1968Si01), E|a=5920 {i20} keV (1978Fa16); E|a=5886 {i9} keV (1996Pa01). 
It is not clear which mother or daughter levels are involved in each case. 
%|a|>40 (1986Ke03,2003Au02). Other: %|a|<5 (1984ScZQ,1996Bu35). 
%|e+%|b{++}|<60, from limit for adopted |a branching. 
T from 1968Si01 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
T$from combined |g(t) statistics for 50.2|g and 113.4|g. Individual measurements yielded 285 ns {I18} for 50.2|g(t) and 319 ns {I20} for 113.4|g(t). 


level_energy_unit: KEV
level_spin_parity: (2,3)
level_comment:
$|d|n{-178,197}=24650 MHz {I260} for J=2 and 23800 MHz {I260} for J=3 
$|d<r{+2}>{+178,197}=-0.624 fm{+2} {I7} (stat) {I18} (syst) (2023Cu04) for J=2 and -0.603 fm{+2} {I7} (stat) {I18} (syst) for J=3 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7,8)
level_comment:
$|d|n{-178,197}=9790 MHz {I140} for J=7 and 10300 MHz {I140} for J=8 
$|d<r{+2}>{+178,197}=-0.254 fm{+2} {I3} (stat) {I8} (syst) (2023Cu04) for J=7 and -0.266 fm{+2} {I3} (stat) {I9} (syst) for J=9 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: S
level_comment:
J neighboring lower-mass Au isotopes probably have 1/2+ or 3/2+ ground states, but higher-mass isotopes probably have 3/2- or 5/2- ground states. |a decay to {+175}Ir (E|a=5848 {I5} (1968Si01), Q(|a)=5982 {I5} if g.s. to g.s. transition) is unhindered (HF<4), but Q(|a)=6052 {I18} from 2003Au03 suggests that an excited state in {+175}Ir is fed. Thus, the structure of {+179}Au(g.s.) appears to differ from that of the (5/2-) 1/2[541] {+175}Ir g.s. See 1999Mu05 for calculation of low-lying bandhead energies for odd-A Au isotopes with A=177 through 185. 
T weighted average of 7.2 s {I5} (1968Si01), 8.1 s {I7} (1968De01). 6.9 s {I3} (1980Da09). Other T{-1/2}: 3.3 s {I13} (1996Pa01). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2+,3/2+,5/2+)
level_comment:
E possibly, a low-energy transition connects this level to the g.s. but was missed in the |a-decay study reported in 2004Ra28. Alternatively, this level may itself Be the g.s. (i.e., x=0). 
J (E1) 62|g from (3/2-) 62+x level. If J=5/2, level may Be analogous to the low-lying 5/2[402] prolate bandhead in {+175}Ir. 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (5/2-)
level_comment:
J J=5/2 member of 1/2[541] band expected at lower energy than the J=9/2 member, but J=9/2 to 5/2 transition has not yet been observed. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (9/2-)
level_comment:
A (9/2-) 203.6+x level is observed in |a decay; its relationship (if any) with this level is not known. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3/2-)
level_comment:
J (E2) 89|g from (7/2-) 151+x. 
E an alternative value of 89.4+x is possible because order of 62|g-89|g cascade has not been firmly established. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT;ISO=M
level_comment:
E from difference in adopted values of E|a to this level and E|a to 203.6+x level in {+183}Tl |a decay (53.3 ms). 
T from {+183}Tl |a decay (53.3 ms); no |g observed in coincidence with |a feeding this level (2004Ra28). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2-)
level_comment:
J M1 52|g from (9/2-) 204+x. HF|?12 in |a-decay from the 9/2- isomer of {+183}Tl suggests a modest change of angular momentum in |a decay without underlying structural change (2004Ra28). This suggests similar structure for the (7/2-) 151+x and (9/2-) 204+x levels in {+179}Au. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_comment:
J |a decay from (9/2-) {+183}Tl(625 keV) is unhindered (HF=1.6 {I4}). 
The relationship (if any) between this level and the (9/2-) 0.0+y level observed in {+90}Zr({+90}Zr,p|g) is unclear. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3/2-)
level_comment:
E an alternative value of 89.4+x is possible because order of 62|g-89|g cascade has not been firmly established. 
J 2004Ra28 suggest (3/2-). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT;ISO=M
level_comment:
E from difference in adopted values of E|a to this level and E|a to 203.6+x level. 
T from 2004Ra28; no |g observed in coincidence with |a feeding this level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2-)
level_comment:
J 2004Ra28 suggest (7/2-). HF is consistent with a moderate angular momentum change in |a decay without underlying structural change; this suggests similar structure for the (7/2-) and (9/2-) levels in {+179}Au. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J,MOMM1$taken by 2020Ve03 from 2018Cu04 (Phys. Lett. B786, 355; hyperfine structure measurements) 
T$from {+179}Au Adopted Levels in the ENSDF database (Nov 2008 update) 
$E|a=5.85 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$from (evaporation residues)(62.4|g+89.5|g)(t) in {+107}Ag({+78}Kr,2p|a|g) (2011Ve01). Other: 316 ns {I43} (2011Ve01) from (evaporation residues)(62.4|g+89.5|g)|a(t) in the same reaction 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (9/2-)
level_comment:
E$y=44 {I15} (2011Ve01); absolute energy of this level is given as 134 {I15} in 2011Ve01 and 2020Ve03. This level is labeled with energy x in Fig. 1 of 2020Ve03 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (7/2-)
level_comment:
E$this level is labeled with energy x+20.6 in Fig. 1 of 2020Ve03 
$2020Ve03 show unobserved transitions to 89.5, (3/2-); 89.5+x, (5/2-); and 89.5+y, (9/2-) levels, and mention that there is some evidence for such transitions 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (9/2+)
level_comment:
E$this level is labeled with energy x+371.5 in Fig. 1 of 2020Ve03 
$The (9/2+) state is interpreted (2020Ve03) as an anti-aligned coupled state: |p1i{-13/2}~#(first-excited 2+ state of {+178}Pt core) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
T$from {+179}Au Adopted Levels in the ENSDF database (Nov 2008 update) 
J$(1/2+,3/2+) in 2011Ve01, 1/2+ in 2020Ve03 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$from (Er)|g(t) (2011Ve01) in {+107}Ag({+78}Kr,2p|a|g) reaction at Jyvaskyla (2011Ve01). Other: 316 ns {I43} from (Er)|a|g(t) (2011Ve01), also at Jyvaskyla, is consistent but less precise. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
T$from |a(t) using |a in energy range of 5500 to 5900 keV (2021Ha32) 
J$from the Adopted Levels of {+179}Au in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
T$from average of 13 measurements of individual transitions assigned the decay of the isomer. Half-lives were determined from recoil-|g(t) measurements. 
E$excitation energy of the isomer is 1615.9 keV {I4} relative to the 9/2-, 127-keV level. 


level_energy_unit: KEV
level_spin_parity: (1/2)
level_comment:
$|d|n{-179,197}=31570 MHz {I200} 
$|d<r{+2}>{+179,197}=-0.796 fm{+2} {I5} (stat) {I23} (syst) (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
T$from grow-in-decay-out method applied to alpha decays with E=5300-5700 keV (2020Ha24) 
J$1 is suggested from hfs measurements (2020Ha24), |p from configuration assignment 
MOMM1$from hfs measurement, includes correction for the relative hyperfine anomaly (2020Ha24) 
$configuration = (|p3/2[532])|~#(|n5/2[512]) 


level_energy_unit: KEV
level_spin_parity: (1)
level_comment:
$|d|n{-180,197}=10650 MHz {I200} 
$|d<r{+2}>{+180,197}=-0.274 fm{+2} {I5} (stat) {I9} (syst) (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: S
level_comment:
%A$from four measurements of %|e+%|b{++} based on absolute I|g or K| x ray data ({+181}Au |a-decay, 1995Bi01). Others: from comparison of parent and |e decay daughter |a intensities, 1970Ha18 report I|a({+181}Au)/I|a({+181}Hg)=0.030 {I5}, but they assign to {+181}Au only one |a (i.e., 43% of all {+181}Au |a decays, based on relative I|a in 1995Bi01). Thus, if %|a({+181}Hg)=31 {I5}, %|a({+181}Au)=3.1 {I9}, consistent with the adopted datum. However, 1979Ha10 report 1.04% {I14} for the sum of the three strongest lines (91% of all |a's, according to 1995Bi01), presumably assuming %|a({+181}Hg)=26 {I4} from their earlier work (viz., 1975Ho02). cf. 31% {I5} adopted here. 
T$weighted average, using limitation of statistical weights method, of data from {+181}Au |a-decay: 1995Bi01 (11 s {I3}, 14.2 s {I11}, 12.7 s {I24}, 15.1 s {I5}, 13.3 s {I17}, 14.1 s {I20}, 14.3 s {I5}), 1979Ha10 (13 s {I3}), 1968De01 (12.0 s {I12}, 11.0 s {I8}) and 1968Si01 (11.5 s {I10}). Others: |?10 s (1970Ha18). 
J unhindered |a decay to (3/2-) ({+177}Ir, 148) (1995Bi01); strongest |e decay branches feed |p=-, J|<5/2 levels in {+181}Pt. Note that {+183}Au and {+185}Au have 3/2- states at 12.8 and 35.8 keV, respectively, and 5/2- ground states, making a 3/2- g.s. for {+181}Au entirely plausible. Any apparent |e+|b{++} feeding to J>5/2 levels in {+181}Pt is presumed to result from an incomplete decay scheme. 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
$|d|n{-181,197}=7820 MHz {I230} 
$|d<r{+2}>{+181,197}=-0.203 fm{+2} {I6} (stat) {I7} (syst) (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: S
level_comment:
%A$from 1995Bi01. Others: 0.038 {I8} (1979Ha10), |?0.04 (1970Ha18) 
T$from weighted average of 15.6 s {I4} (1992Ro21), 15.3 s {I10} (1995Bi01, |g timing) and 14.5 s {I13} (1995Bi01,|a timing). Others: 20 s 2 (1979Ha10), 22.1 s {I13} (1972Fi12), 19 s {I2} (1970Ha18). 
T$ 1993BiZY is superseded by 1995Bi01 
J$M1 |g from (1+) gives (0+,1+,2+); 2,3,4 from g factor measurements of {+182}Au g.s. by nuclear orientation method (1992DeZO,1992Ro21, experiment using NICOLE system at ISOLDE-CERN) 
MOMM1$1992DeZO (also 1992Ro21) measured g factors by nuclear orientation technique and by spin-relaxation method. For spin of 1,2, 3,4 and 5 values are: 0.85 {I6}, 0.68 {I5}, 0.53 {I5}, 0.43 {I5}, 0.35 {I5}, respectively from nuclear orientation method and 0.73 {I5}, 0.62 {I5}, 0.55 {I5}, 0.51 {I6}, 0.46 {I3}, respectively, from spin-relaxation method. From comparison of results from the two methods, 1992DeZO conclude that for spin of 2,3 or 4 the values are in better agreement than with those from spin 1 and 5 choices. Value listed here is from average g factor=0.65 {I5}. 


level_energy_unit: KEV
level_spin_parity: (2)
level_comment:
$|d|n{-182,197}=7160 MHz {I200} 
$|d<r{+2}>{+182,197}=-0.186 fm{+2} {I5} (stat) {I6} (syst) (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: S
level_comment:
MOMM1 From resonance ionization mass spectroscopy. 
<r{+2}>{+1/2}(charge)=5.388 fm {I6} (2004An14). 
%A Unweighted average of 0.8 {I3} (1995Bi01), 0.30 {I5} (1970Ha18). 
|D<r{+2}>(183,197)=-0.130 {I9} fm{+2} (1988Kr18; see also 1990Hi08). 
T weighted average of 44.6 s {I19} (1995Bi01), 42 s {I4} (1970Ha18), 42.0 s {I12} (1970Ma24), 45 s {I4} (1968Si01). Other: 50 s {I2} (1968De01). 
J parity from log| {Ift}=5.4 to (7/2)- {+183}Pt(1957) level; J=5/2 expected based on energy systematics of 5/2- levels in neighboring odd-A Au isotopes. 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
J low energy 9/2- level expected based on energy systematics for 9/2- levels in neighboring odd-A Au isotopes; |D|p=no 284|g from |p=- 297 level. 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
J E1 61|g to (3/2)- 12.8; 1/2+ level energy systematics for neighboring odd-A Au isotopes; absence of |g to (5/2)- g.s.. Possibly an oblate nuclear state (1984Ma41). 
T based on absence of 60.5|g in coincidence spectra in |e decay (1984Ma41). 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: US
level_lifetime_info: ;ERR=LT
level_comment:
J M1 218|g to (9/2)- 12.4; hindrance of M1 deexcitation consistent with observations for h{-11/2} state in neighboring Au isotopes. 
T$5 ns|<T{-1/2}|<1 |ms proposed by 1984Ma41 on the basis of delayed coincidence intensity in |e decay. 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J Q 219|g to (9/2)-; band structure; 13/2- level energy systematics in neighboring odd-A Au isotopes. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
J$from log| {Ift}=4.9 {I+5-1}, based on I(|e+|b{++})=13% {I+15-5} for this level, as given by 2017Ve02 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_comment:
$|d|n{-183,197}=5620 MHz {I120} 
$|d<r{+2}>{+183,197}=-0.147 fm{+2} {I3} (stat) {I5} (syst) (2023Cu04) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: S
level_comment:
|D<r{+2}>(197,184)=-0.064 {I12} (1997Le22,1998Ro27), LASER spectroscopy. 
<r{+2}>{+1/2}(charge)=5.430 {I4} (2004An14). 
|m, Q: from LASER resonance ionization. Other |m: 2.0 to 4.0 from g=0.4-0.8 (1992Ro21), time-resolved on-line nuclear orientation. See also 1992St16. 
%|a=0.013 {I3} (1995Bi01). Other value: |<0.022 {I3} (1970Ha18). However, it is unclear whether the isomeric state or the g.s. (or both) contribute to the observed |a decay. 
|b=+0.264 {I14}, deduced by 1997Le22 from Q. 
J J=5 from hfs spectrum in resonance ionization spectroscopy; M3 68|g from |p=+ 68 level. Likely configuration=(|p 3/2[532])+(|n 7/2[514]), consistent with observed |m (1997Le22). 
T weighted average of 21 s {I1} (1997Za03; two-component fit to 222|g(t) and 362|g(t)) and 19 s {I2} (1992Ro21). Other: 12 s {I2} (1990Ed01); reason for discrepancy not known. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%|a=0.013 {I3} (1995Bi01). Other value: |<0.022 {I3} (1970Ha18). However, it is unclear whether the isomeric state or the g.s. (or both) contribute to the observed |a decay. 
|m, Q: from LASER resonance ionization spectroscopy. Other |m: +1.813 {I19} x (J/(J+1/2)), i.e., 1.450 {I15} (1988Kr18); 1.3 {I3} (1992Ro21) from g=0.65 {I14}, time-resolved on-line nuclear orientation. See also 1992St16. 
|b=+0.221 {I17}, deduced by 1997Le22 from Q. 
J J=2 from hfs spectrum in resonance ionization spectroscopy; |p=+ based on M1(159|g)-M1(263|g) cascade from |p=+ 491 level. Likely configuration=(|p 3/2[532])+(|n 1/2[521]), consistent with observed |m (1997Le22). 
T weighted average of 48 s {I1} (1997Za03; 68|g(t)), 45.8 s {I18} (1995Bi01; |a(t)), 45 s {I1} (1992Ro21; observed 363|g in Pt), 53.0 s {I14} (1972Fi12; 163, 273, 362, 487 |g and ce lines), 47 s {I3} (1970Ha18; |a(t)). The unweighted average is 47.8 s {I14}. Other: 60 s {I6} (1969Ha03; observed 163|g, 273|g, 362|g in {+184}Pt). See also the {+184}Au |e decay data set. 
|D<r{+2}>(197,184)=-0.100 {I12} (1997Le22,1998Ro27), resonance ionization spectroscopy. Others: -0.137 {I7} if J=3 (1988Kr18, resonance ionization mass spectrometry and pulsed LASER induced desorption); agrees well with datum from 1997Le22 after adjustment for adopted J=2; see also 1990Hi08. 
|D<r{+2}>({+184}Au{+g},{+184}Au{+m})=-0.036 {I3} (1997Le22,1998Ro27). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
Q|?0.75 from TDPAC but a J|p=1- state was assumed (1989Ra17). 
T from 157|g-237|g(t) (1994Ib01) in |e decay. Other T{-1/2}: 67 ns {I8} (H. Haas (1978), private communication to authors of 1994Ib01); 36 ns {I6} (1978Ne10). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J M1(+E2) 127|g from 1+ 491 level; M1 296|g to 2+ 68; log| {Ift}=5.6 from 0+ in |e decay rules out 2+. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J log| {Ift}=4.3 from 0+ in |e decay; allowed unhindered transition. 
T from |g delayed coin in |e decay (1978Ne10). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
T from 157|g-237|g(t) (1994Ib01). Other T{-1/2}: 67 ns {I8} (H. Haas (1978), private communication to authors of 1994Ib01); 36 ns {I6} (1978Ne10). 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
The intensity imbalance of 12% {I7} at this level may arise from an incomplete decay scheme and/or the acute dependence of I(|g+ce) from this level on |d(26|g). %|e+%|b{++}<0.25 is expected for the possible 1U branch to this level, based on log| {If{+1u}t}>8.5. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
T weighted average of 4.3 min {I2} (1953Ra02), 4.3 min {I2} (1968De01), 4.3 min {I1} (1968Si01), 4.2 min {I2} (1970FiZZ), 4.2 min {I3} (1970Ha18), and 4.2 min {I1} (1995Bi01,1991Bi04). 
J J from atomic beam (1980Ek04). Calculated |m|?2.3 (assuming a 5/2,1/2[541] Nilsson state mixed with the 5/2,3/2[532] by the Coriolis interaction) agrees with experimental |m. 
%A From 1995Bi01. %|a=0.10 {I3} was deduced from an |a-particle spectrum with {+185}Hg and {+185}Au (1970Ha18), and using evaluator's adopted %|a({+185}Hg)=6 {I1}. 1970Ha18 report %|a=0.093 {I20}, using %|a({+185}Hg)=5.5 {I7}. These values may have not been corrected for the |e decay of {+185}Au (6.8 min), and for the atomic vacancies created by internal conversion (1991Bi04). %|a=0.7 {I1} (1991Bi04). 
MOMM1 Resonance ionization mass spectroscopy (1989Wa11). Other values: +2.17 {I3}, resonance ionization mass spectroscopy (1987Wa06, 1987Wa23); 2.22 {I14}, static (low-temperature) nuclear orientation (1985Va07, 1989Ra17). Others: 1987WaZO, 1987VaZR, 1987Wo04. 
<r{+2}>{+1/2}=5.429 fm 4 for {+185}Au based on a global fit to charge radius data for all nuclides (2004An14). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T from multiscaling of delayed |g's (1970FiZZ). Other value: 7 min (1960Al20). 
|e decay was determined from observation of Pt K x-rays. A 145-keV |g ray (with |e or IT decay) was measured by 1970FiZZ. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
T$from ce ce(t). The large Weisskopf hindrance of 2.1|*10{+4} for the 211-keV M1 transition to the (9/2-) level may be explained by a change from an oblate to a prolate nuclear shape between the initial and final states. Similar hindrances for this transition have been observed in other odd-A Au isotopes (1983Be48). 
J 211.2|g M1 to (9/2-). K|p=1/2-, h{-11/2} rotational band. 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J$The 530.2 |g from the (27/2-) state of the K|p=5/2- band to the 1564.5 level and the 485.2 E2 |g from the 1994.6 level to the (23/2)- state of the K|p=5/2- band, and the 556.6 |g from the 1994.6 level to the (25/2)- state of the K|p=5/2- band establish the J|p's of the 1564.5 as (23/2-) and 1994.6 as (27/2-). From cascade information and band structure, plus 555.2 |g to (13/2-) of the K|p=5/2- band, the J|p of this level is determined. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$243.6 |g to (15/2)-, 558.9 |g to (11/2)-, 639.2 |g to (13/2)-, which are members of the K=5/2- g. s. band. Band head of K|p=13/2+ i{-13/2} rotational band. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$Based on energy systematics of the same J|p=3/2- state in {+187}Au (1056 keV) and {+189}Au (1059 keV) (1988Ko22). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_comment:
J$527.1 |g to (15/2-); possible (17/2-) member of K|p=1/2-, configuration=h11/2 (1986La08). (1988Ko22). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: MIN
level_comment:
MOMM1$weighted average of -1.263 {I29} and -1.284 {I33} from resonance ionization spectroscopy (2019StZV, from 1989Wa11 and 1990Sa21, respectively). Others: 1.07 {I13} from nuclear orientation (1989Ra17, from 1985Va07), 1.278 {I19} from NMR on oriented nuclei (preliminary result, 1988Sc19). 
MOME2 From laser spectroscopy (2016St14,1992Ki30); no Sternheimer correction applied. Sign from 1991Hi14. Others: +3.14 {I16} (1993Hi10 and 1996Ha09, revision of +3.12 {I20} (1991Hi14); NMR on oriented nuclei). Q/Q({+197}Au)=5.73 {I24} (1993Hi10,1996Ha09). 
|D<r{+2}>({+197}Au-{+186}Au)=-0.014 fm{+2} {I8} (1987Wa06, 1989Wa11), 0.021 fm{+2} {I15} (1990Sa21). 
T From 1970Jo02. Other values: 11.0 min {I10} (1972Fi12), 10 min {I2} (1995Bi01), 12 min (1960Al20). 
J J=3 from atomic beam (1976Ek01); E1-M1 cascade from |p=+ 364 level. Possible configuration=((|p 3/2[532])-(|n 9/2[624])). 
$%|a branching based on absolute |a and |g-ray ratio (1990Ak04) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$ cascade of M1+E2 |g's connecting the 189.7, 113.9, 36.1 levels with the 3- g.s. establish J|p(36)=2-, J|p(114)=1-, J|p(190)=1-. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J E1(112|g)-M1(252|g) cascade through 252 level to J=3 g.s. establish J|p(364)=1+, J|p(252)=2- and |p(g.s.)=-. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$M1+E2 gammas connecting the 464.2, and 349.1 keV levels and the 3- g.s., establish J|p(349.1)=2- and J|p(464.2)=1- 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (11-)
level_lifetime_unit: NS
level_comment:
E$Level energy held fixed In least-squares adjustment 
J by analogy with structure in higher mass odd-odd Au nuclei. 
T From ({+19}F,4n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (11+)
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$(11+) in ({+19}F,5n|g) and (10+) in ({+19}F,4n|g). ({+19}F,5n|g) reported better statistics. 
Considerable I|g imbalance at this level in ({+19}F,4n|g) suggests the existence of unobserved low-energy transition(s) deexciting it. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 11-
level_lifetime_unit: NS
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$by analogy with structure in higher mass odd-odd Au nuclei. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 10(+)
level_uncertain: ?
level_comment:
E$Order of 162.6|g and 384.3|g (based on I|g) is not certain, so alternative value of 391.2 is possible. Further, 1996Ib01 indicate that a later, unpublished study by M. G. Porquet failed to confirm either |g. In ({+19}F,5n|g) 2012Li08,2006Zh38 also do not report 384.3|g or 162.6|g. Evaluators mark this level and these two |g as questionable and not adopted. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (10+)
level_comment:
$Considerable I|g imbalance at this level suggests the existence of unobserved low-energy transition(s) deexciting it. 


level_energy_unit: KEV
level_spin_parity: 1/2(+)
level_lifetime_unit: MIN
level_comment:
J$spin from atomic beam (1976Ek01), parity from |m and configuration=|p 1/2+[431] - main component of the oblate orbital arising mainly from the d{-3/2} subshell (1990Sa21) 
T$weighted average of 8.4 min {I3} (1983Gn01), 8.0 min {I4} (1979Be51), and 8.5 min 7 (1973Se13); Other: 8 min (1960Al20) - measured in {+187}Au |e decay. 
MOMM1$from 1990Sa21 (Laser spectroscopy). Other values: +0.535 {I15} (1989Wa11-Laser spectroscopy), +0.54 {I3} (1987Wa06-Laser spectroscopy), and +0.72 {I7} (1980Ek04-Atomic beam magnetic resonance). 
|D<r{+2}>({+187}Au,{+197}Au)=-0.365 {I10} (1990Sa21); <r{+2}>{+1/2}({+187}Au)=5.400 {I6} fm (2004An14) 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: NS
level_comment:
J For prolate, configuration: 3/2+[402] (19.5 keV level) and configuration:1/2+[400] (g.s.) B(M1)=0.0018; and for oblate, configuration: 3/2+[431] (19.5 keV) and configuration:1/2+[431] (g.s.) B(M1)=0.59, calculated by 1978Bo05. 
T$weighted average of 6 ns {I1} (ce(19.5L)(t) - 1978Bo05) and 7 ns {I1} (ce(220K)-ce(19.5M)(t)-1986Be07). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
T$from |g-ce(103.3M)(t)-({+187}Hg |e decay-1983Be48). Other value: 50 ns {I5} from |g|g(t) ({+19}F,4n|g). 
J$103.4|g M1+E2 to 9/2(-), populated in {+172}Yb({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: NS
level_comment:
J 508.8|g (M1+E2) to (29/2-) 
MOMM1$deduced by the evaluator from g=0.25 {I3} (1997Pe26). The g factor is measured using time differential perturbed angular distribution. 
T$From ({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: NS
level_comment:
T$weighted average of 6 ns {I1} ce(19.5L)(t)-1978Bo05 and 7 ns {I1} (ce(220K)-ce(19.5M)(t)-1986Be07) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_comment:
J (11/2-) in the adopted levels. Placement of 525.5|g is from (13/2-) state at 749.9 keV in 1989Jo02 and from 17/2- state in 1989Bo10 


level_energy_unit: KEV
level_spin_parity: 31/2-
level_lifetime_unit: NS
level_comment:
T$Weighted average of 102 ns {I5} (1997Pe26) and 90 ns {I10} (1989Jo02); Other: 100 ns (1989Bo10) 
MOMM1$deduced by the evaluator from g=0.25 {I3} (1997Pe26). The g-factor is measured using time differential perturbed angular distribution. 1997Pe26 speculates that the g-factor might be for a (35/2-) state at 2669.8+|DE keV level feeding the 2669.8-keV level by a<40-keV |g-ray based on the hindrence factor calculation. 


level_energy_unit: KEV
level_spin_parity: (51/2+)
level_comment:
J from 1989Jo02. (53/2) in 1989Bo10. 617.6|g to 49/2+ state is consistent with the A{-2}=-0.15 {I9} (1989Jo02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
$|d<r{+2}>{+187m,187g}=0.243 fm{+2} {I7} (stat) {17} (syst) (2020Ba29) 
E$from the Adopted Levels of {+187}Au in the ENSDF database (2008 update) 
MOMM1$from hfs measurement (2020Ba29) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2)
level_comment:
$|d|n{-187,197}=5380 MHz {I160} 
$|d<r{+2}>{+187,197}=-0.139 fm{+2} {I4} (stat) {I4} (syst) (2023Cu04) 
E$from the Adopted Levels of {+187}Au in the ENSDF database (2008 update) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: MIN
level_comment:
MOMM1$LASER-resonance ionization mass spectroscopy (1989Wa11,1987Wa06, 1987Wa23). Other: 0.069 {I24} (atomic beam magnetic resonance,1980Ek04) 
$|D<r{+2}>({+197}Au,{+188}Au)=-0.347 fm{+2} {I9} (1989Wa11,1987Wa06,1987Wa23). Other: 1988LeZV 
J$J from atomic-beam magnetic resonance (1976Ek01,1978Ek05,1980Ek04) and resonance ionization mass spectroscopy (1989Wa11). |p is from |m and systematics 
T$From |b-265.6|g(t) and |b-339.9|g(t) in 1972Fi12,1970Fi16. Others: 8.8 min (1978CoYZ), 9.0 min {I4} (1970Jo02), 9 min {I1} (1969Na10), and 8 min (1960Po07) 
CONF$|p(s{-1/2}/d{-3/2}){+-1}~#|n(p{-1/2}){+-1} 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
J$ 16|g M1+E2 to 1-, no |e feeding from 0+ 
T$From (ce(M) 16|g)(ce(L) 66|g, ce(L) 98|g, ce(K) 190|g)(t) (1985Ab03) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J$82.7|g (E1) to 1-, 66.7|g (E1) to (2)-; strong direct feeding in {+188}Hg |e decay (J|p=0{++}) 
T$From (ce(L) 66|g)(KLL Auger)(t) (1985Ab03) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
J$114.8|g M1+E2 to 1-; weak population, if any, in {+188}Hg |e decay (J|p=0{++}) would argue against J=0,1 
T$From (ce(K) 115|g)(ce(K) 190|g, |g)(t) (1985Ab03) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$606.0|g E1 to 1-; weak population, if any, in {+188}Hg |e decay (J|p=0{++}) would argue against J=0,1 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$253.8|g M1+E2 to (2)+; weak population, if any, in {+188}Hg |e decay (J|p=0{++}) would argue against J=0,1 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$estimated by evaluators as 250 keV {I100}, based on known high-spin isomers in neighboring odd-odd Au nuclei. The excitation energy of the |p(h{-11/2}){+-1} orbital in neighboring odd-Z Au isotopes is 223.9 keV ({+187}Au) and 247.2 keV ({+189}Au), while that for the |n(i{-13/2}){+-1} one in {+189}Hg (N=109) is unknown, but it is located at 140.8 keV in {+193}Hg (N=113). 
J$Tentative assignment, based on proposed configuration 
T$ Lower experimental limit from the |g|gt measurement in 1992Ja01 
CONF$|p(h{-11/2}){+-1}~#|n(i{-13/2}){+-1}, based on similar signature splitting characteristics of bands in nearby odd-odd Au nuclei and B(M1)/B(E2) analysis 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (20+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ this level is assumed to decay via two low-energy transitions to two (18+) levels at 2217.99+x and 2258.1+x. The |g-rays are expected to be highly converted and lower than the energy threshold of the |g-detector array. This state could be an isomer. 
J$Based on similarity to structures observed in {+190,192}Au 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Excitation energy and bandhead spin of this band are unknown 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: (10-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Excitation energy of band is unknown 
J$(10-) suggested by 2010Fa19 based on proposed configuration. The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (20+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ this level is assumed to decay via two low-energy transitions to two (18+) levels at 2217.99+x and 2258.19+x. The |g-rays are expected to be highly converted and lower than the energy threshold of the |g-detector array 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MIN
level_comment:
$RMS charge radius <r{+2}>{+1/2}=5.4084 fm {I52} (2013An02 evaluation) 
MOMM1$laser resonance ionization mass spectroscopy (1989Wa11,1987Wa06). 
%A$ionization chamber measurement (1963Ka17). No |a decay observed. 
J$spin from atomic beam (1976Ek01). Systematics of {+191}Au-{+199}Au predict 1/2+, 3/2+ ground-state doublet. 
T$weighted average of 28.3 min {I5} (1970Fi16), 28.6 min {I10} (1970Jo02), 29.7 min {I8} (1967Na02), and 28.7 min {I4} (1966Fo13). Other values: 30 min (1960Po07,1960Al20), 42 min {I5} (1955Sm42). Activity identified by 1955Sm42 may have belonged to {+190}Au 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$M1+E2 from 5/2+ (248.6), |g to 1/2+. Systematics of {+191}Au-{+199}Au predict 1/2+, 3/2+ ground-state doublet. 
T$from 1975Be17 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1$laser resonance ionization mass spectroscopy (1989Wa11,1987Wa06). Other value: 6.17 {I15} (1986Va35,1985Va07, nuclear orientation, NMR) 
%IT$on the basis of decay curves, 1970Fi16 suggest a possible IT branch. RUL for a possible 237|g leads to %IT<5.5. 
J$spin from atomic beam (1976Ek01), parity from E2 |g from 7/2- 
T$weighted average of 4.55 min {I10} (1970Fi16), 4.7 min {I1} (1967He06,1967Al17) and 4.0 min {I3} (1966Fo13). 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_comment:
J$M1+E2 to 3/2+ (203.7); M1+E2 to 1/2+; |g to 5/2+ (248.6), strong |e feeding from {+189g}Hg (J|p=3/2-) 


level_energy_unit: KEV
level_spin_parity: 13/2-,15/2-
level_comment:
J$M1+E2 to 13/2- (646.2); strong |e feeding from {+189m}Hg, J|p=13/2+; 11/2 not likely from population in heavy-ion ({+19}F,4n|g) reaction 


level_energy_unit: KEV
level_comment:
J$in 1996Wo04, this level is shown in their Figure 15 with other low lying negative parity levels. However no spin parity was explicitly assigned to this level. 


level_energy_unit: KEV
level_spin_parity: (-)
level_comment:
J$in Figure 10 of 1996Wo04, the association of the decay of this level with the 11/2- isomeric level, indirectly fed via the 841 keV |g leads the authors to assign a negative parity. 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_comment:
J$|g to (21/2+); 1997Pe26 proposed 25/2+, based on assumed similarity of decay scheme from the (31/2+) isomers in {+189}Au and {+191}Au, which would require 188|g to be E2, rather than M1+E2, from other studies 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (31/2-)
level_lifetime_unit: NS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$The 9-ns isomer is populated in all the high-spin studies but its energy is differently interpreted 
T$|g(t) method (1975De20) in {+181}Ta({+12}C,4n|g). Others: 9 ns {I2} (1997Pe26) in {+181}Ta({+12}C,4n|g); 11 ns {I4} in {+191}Ir(|a,6n|g) (1979Go15) 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
E$2515.7+y, y=38.8 keV (2001MaZN, 39 in 1997Pe26). However, y=200 keV from 1975De20. 
J$(E2) |g to (27/2+) 
T$from |g(t) in {+181}Ta({+12}C,4n|g) (1997Pe26). Other: 440 ns {I50} from {+181}Ta({+12}C,4n|g) (1975De20) based on |g(t) for a 199.6-keV transition which is not confirmed in other studies 
MOMM1$time dependent perturbed angular distribution (1997Pe26); g factor=0.42 {I3} 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$level treated as questionable by the evaluators since 374|g is not reported in other high-spin studies 


level_energy_unit: KEV
level_comment:
J$in 1996Wo04, this level is shown in their Figure 15 with other low-lying negative parity levels. However no J|p was assigned to this level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$from Adopted Levels 
E$x=38.8 keV (2001MaZN, 39 in 1997Pe26). In Adopted Levels, this level is at 2555, (31/2+) 
$A 199.6-keV transition from this isomer proposed by 1975De20 was not confirmed by 1979Go15 from lack of coincidences between 200|g and 265.1|g or 188.0|g as required by level scheme in 1975De20 


level_energy_unit: KEV
level_spin_parity: 27/2-
level_lifetime_unit: NS
level_comment:
T$|g(t) (1979Go15). In Adopted Levels, this half-life is assigned to a 2554+x, (31/2-) level with no known transition from it. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Adopted Levels 
E$Level energy held fixed in the least-square fit 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 31/2-
level_lifetime_unit: NS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(27/2-) in 1992Bo23 
T$from |g(t) (1997Pe26) 


level_energy_unit: KEV
level_spin_parity: 57/2+
level_comment:
E,J$this level corresponds to 5634, (53/2+) in Adopted Levels; ordering of the 319-600 |g cascade is reversed in {+176}Yb({+19}F,6n|g) (1992Ve05) and in the Adopted dataset 


level_energy_unit: KEV
level_spin_parity: 31/2+
level_lifetime_unit: NS
level_comment:
E$2515.9+y, y=38.8 keV (2001MaZN), 39 keV (1997Pe26). See {+174}Yb({+19}F,4n|g) dataset for both references 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
E$in Adopted dataset, the 9-ns isomer lies above a 2554.7, (27/2-) level at an unspecified energy 
J$(27/2-) in Adopted Levels. 
T$|g(t) (1975De20) 


level_energy_unit: KEV
level_spin_parity: 29/2+
level_lifetime_unit: NS
level_comment:
T$|g(t) (1975De20). Note that the value is 242 ns {I10} in Adopted Levels, taken from 1997Pe26 
E,J$in Adopted dataset, this isomer with T{-1/2}=242 ns {I10} is at 2554.8 keV, J|p=31/2+ decaying by a 39-keV |g transition. 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_comment:
J$(35/2-) in Adopted Levels. 
$In the Adopted dataset, this level decays by 125.6 and 435.2 |g rays 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
E,J$from the Adopted Levels of {+189}Au in the ENSDF database (2017 update) 
MOMM1$from hfs measurement using hyperfine anomaly of {+197}|D(6s)=0.1134 {I58} for l=11/2 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius=5.4109 fm {I49} (2013An02) 
$Evaluated |d<r{+2}>({+197}Au,{+190}Au)=-0.284 fm{+2} {I5} (2013An02) 
$%|b{++}=2 (1961Ja17), <1 (1959Al94). From |e/|b{++}(theory), deduced %|b{++}<0.2 (Q(|b{+-})=-1600) 
MOMM1$laser-resonant ionization spectroscopy on mass-separated {+190}Au (1990Sa21). Others: -0.068 {I26} (1989Wa11); -0.063 (1985St10); 0.065 (1964Li06,1964Li11,1966Ch05) 
$|D<r{+2}>({+197}Au,{+190}Au)=-0.285 fm{+2} {I6} (1989Wa11,1987Wa06), -0.261 fm{+2} {I12} (1985St10), -0.282 fm{+2} {I8} (1990Sa21). Methods employed resonance ionization spectroscopy and fluorescence spectroscopy on mass-separated radioactive ion beams 
$|b{-2}=-0.139 (1989Wa11), -0.148 {I3} (1985St10), 0.139 (1990Sa21); deduced from |D<r{+2}> given above 
E$From least-squares fit to E|g data, assuming 0.3 keV uncertainty for E|g when not stated. 
J$spin from atomic beam (1964Li06,1966Ch05). |p from cascade of E1 and M1+E2 |g transitions from 171.6, 1+ level through the 29.1-keV level. Based on measured magnetic dipole moments for {+188}Au and {+190}Au ground states, 1985Ab03 and 1980Ek04 suggested oblate structure for {+190}Au ground state with possible configurations of |pd{-3/2}~#|n3p{-1/2} or |pd{-3/2}~#|n3p{-3/2}, both giving J|p=1-. 
T$from 1973Jo11. Others: 43 min {I1} (1969Na10), 38.8 min {I18} (1961An02); 1960Po07, 1960Al20, 1961Ja17. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$x=200 {I150} (2017Au03,syst); 260 {I100} (from energies of |g rays observed, but unplaced). 
J$from systematics, similar isomers in {+192}Au and {+194}Au with possible configuration=(|ph{-11/2}{+-1}~#|ni{-13/2}{+-1}){-11-} (1982Ne05) 
T$from |g(t) pulsed beam (1982Ne05) 
$Four |g rays observed (see {+190}Au IT decay) from this isomer but no level scheme is established 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (20+)
level_lifetime_unit: NS
level_comment:
T$from |g(t) pulsed beam (2001Gu29) 
$Configuration=|ph{-11/2}{+-1}~#|n(i{-13/2}{+-2},h{-9/2}{+-1}) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$x=200 {I150} (2017Au03,syst). Other: 260 {I100}, estimated from energies of all observed unplaced |g rays (41|g, 47|g, 115|g, 155|g), assuming the energy sum as the upper limit and the highest 155|g as the lower limit). 
T$from |g(t) pulsed beam (1982Ne05) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$x=200 {I150} (2017Au03,syst); 260 {I100} (from energies of |g rays observed, but unplaced). 
J$from systematics, similar isomers in {+192}Au and {+194}Au with possible configuration=|ph{-11/2}{+-1}~#|ni{-13/2}{+-1}(11-) (1982Ne05) 
T$from |g(t) with pulsed beam. The following |g rays were associated with the decay of the (11-) isomer: 41, 47, 115 and 155. The decay scheme of the isomer is not established 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
No |a (<5|*10{+-6}%) (1963Ka17). 
J atomic beam (1960Ew06). d{-3/2} from Schmidt diagram. 
T from 1967Jo06. Other values: 3.2 h {I1} (1961An03 - ce(t)), 3.0 h {I5} (1955Sm42), |?4 h (1954Gi04). 
Isotope shift: |D<r{+2}>({+191}Au, {+197}Au)=0.243 fm{+2} {I4} (1994Pa37), 0.242 fm{+2} {I5} (1989Wa11), 0.227 fm{+2} {I5} (1985St10); nuclear charge radius: <r{+2}>{+1/2}=5.415 fm {I5} (2013An02). 
MOMM1 From 2019StZV,1994Pa37 - Laser Resonance Ionization Mass Spectroscopy. Others: 0.137 {I1} (1980Ek04 - atomic beam on-line NMR), +0.137 {I3} (2000Sa58 - collinear laser spectroscopy - 1992Ki30 and 1992Le22 are earlier publication), |+0.137 {I7} (1964Ew02). 
MOME2 From 2016St14 (1994Pa37: +0.716 {I21} collinear laser spectroscopy). Others: +0.76 {I3} (2000Sa58 - collinear laser spectroscopy), -1.3 {I1} (1992Ki30 - resonance ionization mass spectroscopy). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_comment:
T 1986Be07, from ce-ce(t) in {+191}Hg |e decay (50.8 min). 
J s{-1/2} expected from shell model. Also discussed in 1983PaZR 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$|d<r{+2}>{+191,197}=-0.201 fm{+2} {I4} (stat) {I6} (syst) (2023Cu04) 
MOMM1 From 2020Ba17 - hfs measurement with respect to {+197}|D(6s)=0.1134 {I58} for J=11/2. Others: 6.6 {I6} (2019StZV, 1985Va07 - nuclear static (low-temperature) orientation). 4.96 {I35} (1982LiZV). 
Configuration: |p h{-11/2} 
T from 1971Be61 ({+191}Au IT decay (0.92 s)). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: ?
level_comment:
J Observed in the decay of {+191}Hg(49 min) (J|p=(3/2-)). d{-5/2} assignment expected from shell model. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
J 274.2|g M1+E2 to (11/2-); population in (|a,4n|g); fits h{-9/2} decoupled band systematics. 
T from |g(t) pulsed E|a=51 MeV in (|a,4n) (1979Go15). 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J 578.6|g M1+E2 to (11/2-); 578.6|g(|q) data in (|a,4n|g) is consistent for a |DJ=1 transition, the values A{-2}=-0.16 {I2} and A{-4}=-0.02 {I3} for a doublet 578.6|g+579.4|g. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J 357.0|g M1+E2 to (9/2-). |g(|q) data in (|a,4n|g) is consistent for a |DJ=1 transition, A{-2}=-0.48 {I13} and A{-4}=-0.04 {I19}. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J 579.5|g stretched E1 to (19/2-) 
T from 1985Ko13, ce-ce delayed coincidence; Other value: <2 ns (1979Go15) - both in (|a,4n|g). 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_uncertain: ?
level_comment:
E This is the intermediate level of the cascade 207.5|g-(88.9|g) to (21/2+), not connected to the scheme otherwise; hence E(level)=2198.5 is possible for opposite cascade. 
J 207.5|g M1+E2, |DJ=1 from (25/2+) (or to (21/2+) if 207.5|g proceeds from this level and the cascade is (88.9|g)-207.5|g) instead. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_comment:
J 775.4|g stretched E2 to (19/2-). States with similar transition pattern were observed in {+189}Au and {+193}Au (1976Go22). 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
J 269.9|g stretched (E2) to (23/2-). Possible configuration: |p (h{-11/2}{+-3}) (1997Pe26 - ({+11}B,6n|g)) 
T from 1985Ko13 (|a,4n|g), ce-ce delayed coincidence. 
MOMM1 integral perturbed angular distribution of |g rays following nuclear reaction (1985Ko13, not listed in 2020StZV). 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_lifetime_unit: NS
level_comment:
J 67.0|g (E2) to (27/2+); yrast |p=+ levels. Possible configuration: |n [(i{-13/2}{+-1}), (h{-9/2}{+-1})]{-10-} ~# |p [(h{-11/2}{+-1})] (1997Pe26 - ({+11}B,6n|g)). 
T from 1997Pe26 ({+11}B,6n|g), |g-|g delayed coincidence, BaF{-2}-HPGe. Other: >400 ns from ce-ce delayed coincidence 1985Ko13 (|a,4n|g). 
MOMM1 Based on g=0.42 {I3} from TDPAD (2020StZV, 1997Pe26). 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: NS
level_comment:
J 56.2|g (E2) to (27/2-); yrast |p=- levels. Possible configuration: |n (i{-13/2}{+-2}){-10+} ~# |p (h{-11/2}{+1}) (1997Pe26 - ({+11}B,6n|g)) 
T From 1985Ko13 (|a,4n|g), ce-ce delayed coincidence; Other values: 6 ns {I2} (1979Go15 - for 2447 level); 10 ns {I2} (1974Tj02 - for 1991 level) - latter two also in (|a,4n|g) are most likely for this level; 6 ns {I2} (1997Pe26 - ({+11}B,6n|g) |g-|g delayed coincidence). 


level_energy_unit: KEV
level_spin_parity: (33/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J 301.5|g (M1) to (31/2-) and 77.2|g M1 from (35/2-) 
T from 1985Ko13 (|a,4n|g), ce-ce delayed coincidence. 


level_energy_unit: KEV
level_spin_parity: (37/2+)
level_comment:
J 275.4|g from (41/2+); cascade 647.5|g (Q; |DJ=2) - 586.2|g (Q; |DJ=2) - 512.0|g - 168.0|g (E2) to (21/2+) rules out spins higher than 37/2 


level_energy_unit: KEV
level_spin_parity: (43/2-)
level_comment:
J 740.2|g stretched E2 to (39/2-). 
E This is the intermediate level of the cascade 828.3|g-740.2|g, not otherwise connected to the level scheme; hence E(level)=4202.1 is also possible, if opposite. 


level_energy_unit: KEV
level_spin_parity: (49/2+)
level_comment:
J 252.8|g from (53/2+) and 452.2 M1 to (47/2+) define level spin and establish Mult=(E2) for 252.8|g, |g(|q) data in ({+11}B,6n|g), A{-2}=-0.16 {I4} and A{-4}=-0.07 {I8}, implies Q(+D). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: JAP(19/2)
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$from 1993Vo04, based on the least-squares fit to formulas connecting E|g's and J|p's according to the formalism given by 1990Dr08 and 1992Be25 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J1AP(35/2)
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$From spin fits. Alignments indicated by the slopes of the theoretical Routhians require 39/2 (1997Sc22) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J2AP(33/2)
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$From spin fits. Alignments indicated by the slopes of the theoretical Routhians require 37/2 (1997Sc22) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T From 1971Be61: Weighted average of 0.95 s {I25} (241|g(t)) and 0.91 s {I12} (253|g(t)). The evaluator assumed 1971Be61 data superseded their earlier value 1.2 s {I3} (1970Be60). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: JAP(19/2)
level_comment:
J$from 1993Vo04, based on the least-squares fit to formulas connecting E|g's and J|p's according to the formalism given by 1990Dr08 and 1992Be25 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J1AP(35/2)
level_comment:
J$From spin fits. Alignments indicated by the slopes of the theoretical Routhians require 39/2 (1997Sc22) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J2AP(33/2)
level_comment:
J$From spin fits. Alignments indicated by the slopes of the theoretical Routhians require 37/2 (1997Sc22) 


level_energy_unit: KEV
level_spin_parity: 23/2+
level_comment:
E This is the intermediate level of the cascade 207.5|g-(88.9|g), not connected to the scheme otherwise; hence E(level)=2198.5 is also possible for opposite cascade. 


level_energy_unit: KEV
level_spin_parity: 43/2-
level_comment:
E This is the intermediate level of the cascade 828.3|g-740.2|g-, not connected to the level scheme otherwise; hence E(level)=4203.6 is also possible if opposite. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (31/2-)
level_lifetime_unit: NS
level_comment:
T Other values: 6 ns {I2} - most likely for this level (in 1979Go15 for 2447 level (259|g(t))); 10 ns {I2} - most likely for this level (in 1974Tj02 for 1991 level (579.3|g(t))). 
E from 1985Ko13. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
|D<r{+2}>({+192}Au-{+197}Au)=-0.208 {I5} (1985St10), -0.204 {I4} (1990Sa21), -0.2065 {I34} (1994Pa37). |D<r{+2}>({+192}Au-{+190}Au)=+0.045 {I8} (1988Le22). 
<r{+2}>{+1/2}(charge)=5.417 {I4} (2004An14). 
MOMM1 collinear laser spectroscopy. Other values: 0.009 {I24}, (atomic beam, 1989Ra17 from 1980Ek04); -0.0076 {I21} (resonance ionization mass spectroscopy, 1989Ra17 from data of 1990Sa21). 
MOME2 collinear laser spectroscopy. 
J J=1 atomic beam (1960Ew06); E1 307|g from |p=+ 306. g.s. configuration=((|p d{-3/2})(|n p{-1/2}))+((|p d{-3/2})(|n p{-3/2})) (1980Ek04), supported by |m (see also 1994Pa37). 
T weighted average of 4.85 h {I10} (1962Ma18) and 5.03 h {I10} (1966Ny01). Others: 1949Wi08, 1952Fi06, 1953En06. 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: MS
level_lifetime_info: ;ERR=?;ISO=M1
level_comment:
J spin: by analogy with similar isomers in {+194}Au, {+196}Au, {+198}Au; parity: E3 and M2 transitions to |p=- states. 
T ce(t) in Ir(|a,xn|g), {+193}Ir({+3}He,4n|g) (1976RoZE,1980RoZT). 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
J E3 60|g to (8)+ 372; analogy with similar isomers in {+190}Au, {+194}Au. 
T |g-ray timing spectra in Ir(|a,xn|g), {+193}Ir({+3}He,4n|g) (1982Ne05). Other value: 167 ms (ce(t), 1976RoZE,1980RoZT). 


level_energy_unit: KEV
level_spin_parity: (20+)
level_lifetime_unit: NS
level_comment:
Likely configuration: |p(h{-11/2}{+-1})|n(i{-13/2}{+-2})|n(h{-9/2}{+-1}). 
T from 341(ce(K))-|g (2001Gu29) in ({+11}B,5n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
Limit for possible |a decay: <1|*10{+-5}% (1963Ka17). Theory 1|*10{+-21}% (2001Mo07) 
J spin from atomic beam (1976Fu06); parity from Schmidt diagram, |m. 
T from 1968Sv01. Other values: 15.8 h {I3} (1948Wi01,1949Wi08), 17.5 h {I2} (1957Ew34), 15.3 h {I5} (1952Fi06) 
MOMM1 Collinear LASER spectroscopy (1994Pa37); others: 0.1396 {I6} NMR on oriented nuclei (1993Hi10), +0.140 {I1} atomic beam (2014StZZ,1980Ek04), 0.139 atomic beam (1976Fu06). 
MOME2 Collinear LASER spectroscopy (2014StZZ,1994Pa37) 
Isotope shift: |D<r{+2}>=-0.162 fm{+2} 2 (1994Pa37), relative to {+197}Au. Other: -0.157 fm{+2} 4 (1989Wa11,1985St10) 
|% <r{+2}>=5.421 fm {I4} (2004An14). 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: NS
level_comment:
J M1+E2 |g to 3/2+; 1/2+ suggested by shell model, systematics 
T from {+193}Hg |e decay (3.80 h) (1970Fo08) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 3/2+, E2 |g to (1/2)+; see J|p assignment for the 290.18 level. 
T from {+193}Au IT decay (3.9 s) (1970Fo08). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J E3 - M1+E2 cascade to 3/2+ g.s., direct transition to g.s. very weak and no transition to (1/2)+ 38.23 level. This indicates J|p=11/2- for the 290.18 level and J|p=5/2+ for the 257.97 level. Systematics of h11/2 levels in Au nuclei 
T from {+193}Au IT decay (1955Fi30) 
%|e+%|b{++}: deduced from I(|g+ce)(258.0|g in {+193}Au) relative to I(|g+ce)(135.5|g in {+193}Pt) (1955Br41). 
MOMM1 Radiative detection of NMR (2014StZZ,1983Ha10); other: 6.17 {I9} NMR (2014StZZ,1983Li21) 
MOME2$|g(|q,H,t) from {+193}Hg decay (11.8 h), NMR (2014StZZ,1996Se06) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J E2 |g to 11/2- level, (E1) - M1+E2 cascade to 3/2+ g.s.; this gives J|p=7/2- for this level and J|p=5/2+ for 382-keV level. 
T from {+193}Hg |e decay (11.8 h) (1970Ba56). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
J M1+E2 |g's to 7/2- and 11/2- levels; band structure 
T from {+193}Hg |e decay (11.8 h) (1975Be29). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J (M1) |g to (1/2)+, D+Q |g to 5/2+. 1/2+ discarded based on correlation analysis of 446|g and 381|g cascade. 


level_energy_unit: KEV
level_spin_parity: (9/2- : 13/2-)
level_comment:
J (E2) |g to 11/2- level; |g to 9/2- level; log| {Ift}=7.6, log| {If{+1u}t}=8.0 from 13/2+ {+193}Hg 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J E2 |g to (13/2)- level; |g to 7/2- level; log| {Ift}=7.8, log| {If{+1u}t}=7.0 from 13/2+ {+193}Hg. 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: NS
level_comment:
MOMM1 From differential perturbed angular distribution of |g rays following nuclear reactions. 
J E1 |g to (19/2)- level, (E3) |g to (15/2)- level. 
T from Ir(|a,xn|g) (1985Ko13) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J (E2) |g to (13/2)- level gives |p=(-) and 9/2|<J|<17/2; log| {If{+1u}t}=6.9 from 13/2+ {+193}Hg rules out J=9/2 and 17/2; 1196|g - 547 (E2) |g cascade to 5/2+ level rules out J=13/2 and 15/2 since 1196|g, competing with the 1262 (E2) |g, in unlikely to be an M2 transition. Therefore J(this level)=11/2 and J(929 level)=9/2 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T Ir(|a,xn|g) (1985Ko13). 
J 2007Ok05 ({+11}B,4n|g) assign 29/2+ based on 245.1|g E2 to 25/2+ and 161.8|g d from 31/2+. However, 1979Go15 (|a,xn|g) assign 27/2+ based on 244.9|g (M1) to 25/2+ and 161.8|g (E2) from 31.2+. Note that Multipolarity assignments in 2007Ok05 were from R(DCO) and polarization measurements, while for 161.8|g in 1979Go15 (M1) multipolarity from measured total conversion coefficient and |g-ray angular distribution measurements. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
MOMM1 From integral perturbed angular distribution. 
J (E2) |g to (23/2-) level; band structure 
T from Ir(|a,xn|g) (1985Ko13). 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: NS
level_comment:
J (E2) |g to (27/2-) level; band structure 
T from Ir(|a,xn|g) (1985Ko13). 
MOMM1 From integral perturbed angular distribution. 


level_energy_unit: KEV
level_spin_parity: (33/2-)
level_lifetime_unit: NS
level_comment:
J 2007Ok05 ({+11}B,4n|g) assign 33/2- based on 224.5|g M1+E2 to 31/2-. However, 1979Go15 (|a,xn|g) assign 35/2- based on 224.5|g as E2 to 31/2-. Note that Multipolarity assignments in 2007Ok05 were from R(DCO) and polarization measurements. In 1979Go15 Q multipolarity from |g-ray angular distribution measurements. 
T from Ir(|a,xn|g) (1985Ko13). 
MOMM1 From integral perturbed angular distribution. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T from (ce(L2) 133|g)(ce(K) 408|g)(t) (1985Ko13). Others: 15 ns {I2} (1979Go15), 12 ns {I2} (1974Tj02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 27/2-
level_lifetime_unit: NS
level_comment:
T (ce(L2) 99|g)(ce(K) 205K)(t) (1985Ko13). Other: <3 ns (1979Go15) 
g-factor|<0.7 (1985Ko13); from integral perturbed angular distribution measurements with external magnetic fields 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 31/2-
level_lifetime_unit: NS
level_comment:
g-factor=0.3 {I2} (1985Ko13) from integral perturbed angular distribution measurements with external magnetic fields 
T (ce(K) 225|g)(ce(L2) 99|g)(t) (1985Ko13). Other: 6 ns {I2} (1979Go15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 35/2-
level_lifetime_unit: NS
level_comment:
g-factor=0.13 {I11} (1985Ko13); from integral perturbed angular distribution measurements with external magnetic fields 
T (ce(K) 225|g)(t) (1985Ko13). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$7/2 with |d(861|g)=-2.28 {I+49-75} is also possible, but it is inconsistent with log {Ift} value in decay data 


level_energy_unit: KEV
level_spin_parity: (11/2:15/2-)
level_comment:
E,J$From Adopted Levels. Level not listed in Table 1 of 2014Th02, however needed for 274.95|g from 1630 keV level. 


level_energy_unit: KEV
level_spin_parity: 9/2+,11/2+,13/2+
level_comment:
J$Best fit to |g|g(|q) data is obtained for 13/2 -> 9/2 -> 5/2, yet 9/2 and 11/2 cannot be ruled out 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
E,J$from the Adopted Levels of {+193}Au in the ENSDF database (2017 update) 
MOMM1$from hfs measurement using hyperfine anomaly of {+197}|D(6s)=0.1134 {I58} for l=11/2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2
level_comment:
$|d|n{-193,197}=4780 MHz {I180} 
$|d<r{+2}>{+193,197}=-0.121 fm{+2} {I4} (stat) {I4} (syst) (2023CuAA) 
E$from the Adopted Levels of {+193}Au in the ENSDF database (2017 update) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: H
level_comment:
J$spin from atomic-beam method (1960Ew06); parity from systematics of neighboring nuclides ({+190}Au and {+192}Au both have g.s. J|p=1-). Small value of |m=0.076 is consistent with probable configuration=((|p d{-3/2})(|n p{-1/2})). 
T$from 1992Si02 (|g-decay curve, with reference to {+137}Cs half-life, which was counted at the same time). Others: 39.23 h {I51} (2019Ja03, from |g decay curve, average of 38.47 h {I+79-76} and 39.61 h {I39} from sources made in two different reactions, uncertainties are statistical only); 39.5 h {I5} (1949Wi08, |b decay curve), 39 h {I2} (1949St17). Unweighted average of all values is 38.9 h {I3} 
MOMM1$from resonance ionization mass spectroscopy with collinear fast-beam laser spectroscopy (1994Pa37). Other values: +0.079 {I3}, resonance ionization mass spectroscopy (1990Sa21); 0.080 {I24}, atomic beam magnetic resonance (1980Ek04); 0.074 {I4}, atomic beam magnetic resonance (1965Ch08, 1962Ch18). 2020Ba17 give 0.0754 {I25} from re-analysis of data in 1994Pa37 
MOME2$from collinear fast-beam laser spectroscopy (1994Pa37). 
$Evaluated <r{+2}>{+1/2}=5.4252 fm {I40} (2013An02). 
$Evaluated |D<r{+2}>({+194}Au,{+197}Au)=-0.131 fm{+2} {I1} (2013An02). Others: -0.1289 fm{+2} {I21} (1994Pa37), -0.130 fm{+2} {I4} (1990Sa21). 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$45.29|g(M1+E2)-35.22|g(M1+E2) cascade to 1- g.s., absence of direct transition to 1- g.s., and |g(|q) in (|a,3n|g) favor (3)- for this level and (2)- for 35.2 level. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
J$26.9|g (M2) transition to (3)- and syst (similar 5+ isomers are reported in {+192}Au and {+198}Au). Since (E3) assignment for 26.9|g is not ruled out, 6+ is also possible. In that case the spins of the levels based on this isomer will increase by one. 
T$from |g(t) and pulsed beam in {+194}Au IT decay (1975Ya14). Other: 600 ms {I50} (1982Ne05). 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: NS
level_comment:
J$137.08|g E2, |DJ=2 to (5+); band assignment 
T$from |g(t) in {+194}Au IT decay (420 ms) (1977Pa20) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_comment:
J$170.78|g M1+E2 |g to (5+); band assignment 
T$from |g(t) in {+194}Au IT decay (420 ms) (1977Pa20) 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
J$69.0|g (E3) transition to (8+). Similar 11- isomers with T{-1/2}=160 ms and 125 ms reported in {+192}Au and {+190}Au, respectively (1977Pa20). Also probable shell-model configuration. Since (M2) assignment to 69.0|g cannot be ruled out, 10- is also possible. In that case the spins of the levels based on this isomer will decrease by one. 
T$from |g(t) and pulsed beam (1975Ya14). Others: 420 ms {I20} (1982Ne05), 400 ms {I20} (1953He57). 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
E$from the Adopted Levels 
T$from |g(t) and pulsed beam (1975Ya14). Others: 420 ms {I20} (1982Ne05), 400 ms {I20} (1953He57) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
J J=3/2 from atomic beam (1976Fu06), |p=+ from L=2 in {+194}Pt(|a,t). 
T$From 2012Fi12, made a sample-height corrections based on 186.098 d {I47} measurement with reference ionization chambers (1991UnZZ,2002Un02). Others: 186.09 d {I4} (1982HoZJ, replaced by 2002Un02), 182.9 d {I5} (1963Ha17,1981KhZY), 185 d {I1} (1962Bo12), 199 d {I3} (1960Br11), 192 d {I5} (1959Bi07), 185 d {I3} (1949Wi08), 180 d {I15} (1949St17). 
|m=0.1487 {I6} (1993Hi10, 2011StZZ). 
MOMM1$Nuclear magnetic resonance on oriented nuclei(1993Hi10). Others: +0.149 {I1} (1980Ek04), +0.151 {I7} (1989Wa11), +0.145 {I5} (1990Sa21) 
Q=+0.607 {I18} (1993Hi10,2011StZZ) 
MOME2$Nuclear magnetic resonance on oriented nuclei ({+193}Au standard) (1993Hi10). 
Change of the mean-square charge radius |D<r{+2}>({+195}Au-{+197}Au): 0.063 (fm){+2} 9 (1983Kl02), -0.080 (fm){+2} 6 (1990Sa11). See also 1984Ro11. 
<|b{+2}>{+1/2}=0.120 (1990Sa21) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J L=0 in {+194}Pt(|a,t). Analogy with {+197}Au, probably s1/2. 
T from |g|g(t) measurement in {+195}Hg |e decay (10.53 h) (1970Fo08). Others: 3.2 ns {I5} (1962Ja04), 2.8 ns {I3} (1961Re08). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J |g to 3/2+ is M1+E2 and |g from 11/2- is E3 
T from |g|g(t) measurement in {+195}Hg |e decay (41.6 h) (1970Fo08). Other: <200 ps (1961Re08). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J log| {Ift}=7.39 (log| {If{+1u}t}=8.1) from 13/2+ and L=5 in {+194}Pt(|a,t). 
T weighted av of 30.6 s {I2} (1955Fi30), 30.2 s {I5} (1967Fr05). Other: 30 s (1952Hu54). 
|m=+6.17 {I9} (1983Li21,2011StZZ). 
MOMM1$Nuclear magnetic resonance on oriented nuclei(1983Li21). Other: 6.18 {I9} (1981Ha27) Q=+1.87 {I6} (1996Se06,2011StZZ). 
MOME2$MAPON method (1996Se06). Other: +1.41 {I10}, {+197}Au standard (1983Pe22) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J J=3/2 from (600|g)(180|g)(|q) in {+195}Hg |e decay (10.53 h) (1970Ca07) and |p=+ from |g of M1+E2 to 3/2+. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J |g to 11/2- is M1; L=5 allows J=9/2- and 11/2-; but |g to 549, with J|p|<7/2+, rules out J=11/2-. 


level_energy_unit: KEV
level_spin_parity: 13/2-,15/2-
level_comment:
J |g's to 13/2- and 15/2- are M1, and log| {Ift}=7.69 from 13/2+. J|p=15/2- favored by 1974Tj02 on the basis of corresponding J|p state in {+195}Au. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
J corresponding J|p state in {+193}Au in {+193}Ir(|a,2n|g). |p h11/2 coupled to 5- core state (1974Tj02). 
T From |g|g(t) (2013Dr01). Other: 8 ns {I2},from |g|g(t) measurement in {+193}Ir(|a,2n|g) (1974Tj02). 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
$Possible configuration=|ph{-11/2}{+-1}~#|n(i{-13/2}{+-1},h{-9/2}{+-1}) as proposed earlier for 31/2+ isomers in {+189}Au, {+191}Au and {+193}Au 
T From |g|g(t) (2013Dr01). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 31/2(-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T From |g|g(t) (2013Dr01). 
$ Possible configuration=|p11/2[505]{+-1}~#|n(9/2[624],11/2[615]){+-2} 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_comment:
$Possible configuration=|ph{-11/2}{+-1}~#|n(i{-13/2}{+-1},h{-9/2}{+-1}) as proposed earlier for 31/2+ isomers in {+189}Au, {+191}Au and {+193}Au 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
E,J$from the Adopted Levels of {+195}Au in the ENSDF database (2014 update) 
MOMM1$from hfs measurement using hyperfine anomaly of {+197}|D(6s)=0.1134 {I58} for l=11/2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2
level_comment:
$|d|n{-195,197}=1760 MHz {I220} 
$|d<r{+2}>{+195,197}=-0.045 fm{+2} {I5} (stat) {I1} (syst) (2023Cu04) 
E$from the Adopted Levels of {+195}Au in the ENSDF database (2014 update) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
%EC+%B+ Deduced by evaluator as follows: |b{+-}(%)=|b{+-}(g.s.,%)+ [100-|e(g.s.,%)-|b{+-}(g.s.,%)]|* I|g(426|g)(1+|a(426|g)/[I|g(426|g)(1+|a(426|g)+ I|g(356|g)(1+|a(356|g))]=7.0 {I3}; where |b{+-}(g.s.,%)|<0.3(from systematics),|e(g.s.,%)|<0.9(from systematics). Thus |e+|b{++}(%)=93.0 {I3} 
J J=1 from atomic beam method (1970Sc07) and L(p,d)=1 for |p. 
$|m=0.5906 {I5} (1987Oh11,1989Ra17). Compilation: 2005St24 
$Q=0.81 {I7} (1987Oh11,1989Ra17). Compilation: 2005St24 
MOMM1 From radiative detection of nuclear magnetic resonance on oriented nuclei (1987Oh11). Others: |m=+0.580 {I15} from resonance ionization mass spectroscopy (1987LeZV), |m=+0.5914 {I14} (1978LeZA). 
T from 2001Li17. Others: 6.183 d {I10} (1963Ik01),6.1 d {I1} (1976HeZF), 6.1 d {I1} (1963Ti02), 6.07 d {I11} (1962Li03), 6.15 d {I15} (1962Wa16), 6.17 d {I5} (1962Bo12), 5.3 d {I3} (1963Ka24), 5.6 d {I1} (1960Ba63) 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-
level_comment:
J$ L({+3}He,d)=0 from 1/2-,L(p,d)=1 from 3/2+. Supersymmetry scheme (1991Jo01) predicts a low-lying 1-, 2- doublet. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J 85 |g E3 to 2-,g.s. L(p,d)=6 from 3/2+ suggests 5+,6+,7+,8+ 
T weighted average of 8.2 s {I2} (1971Ro16) and 7.4 s {I6} (1972GlZX). 
B(E3)=1.4|*10{+-5}. 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_lifetime_unit: PS
level_comment:
T$From ce time spectra in (d,2n|g) 
J$ M1 |g to 0-,42. L({+3}He,d)=0+2 from 1/2-,L(p,d)=1+3 from 3/2+. 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
T$From ce time spectra in (d,2n|g) 
J$ L(pol d,|a)=3+5 from 0+. L(p,d)=3 from 3/2+ suggests 1-,2-,3-,4- 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
J 148|g E2 to 5+, 188|g M1+E2 from 8+. 
T from delayed coincidence (1967Wa02). 
B(E2)=0.23 from T{-1/2}. 


level_energy_unit: KEV
level_spin_parity: 10-,1-,2-,3-
level_uncertain: ?
level_comment:
J$ L(p,d)=1+3 from 3/2+. Weak population in (p,n|g) and its |g decay suggests (0-). 1999Me19 suggests 2-,3-. 


level_energy_unit: KEV
level_spin_parity: 6+,7+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$M1 |g to 7+, E2 |g to 5+. L(p,d)=6 from 3/2+ suggests 5+,6+,7+,8+. L({+3}He,d)=5 from 1/2- suggests 5+. 
T from ce|g(t) (1967Wa02). 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$L({+3}He,d)=3 from 1/2-. L(pol d, |a)=1,2+4 from 0+ suggests (2-,3+), L(p,d)=1 from 3/2+ suggests 0-,1-,2-,3-. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$ M1 |g to 7+, M1+E2 |g to 5+. L(p,d)=6 from 3/2+ suggests 5+,6+,7+,8+. 
T from ce|g(t) (1967Wa02). 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
J$ L(pol d, |a)=5 from 0+. L(pol d,t)=3 from 3/2+ suggests 2-,3-,4-, but 2- inconsistent with the excitation function in (p,n|g). 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
J$ L(p,d)=1+3 from 3/2+. Weak population in (p,n|g) and its |g decay suggests |<2-. L (pol d,t) suggests |<3-. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
J$M4 |g from 12-, E2 |g to 6+. L(p,d)=6 from 3/2+ suggests 5+,6+,7+,8+. 
T from delayed coincidence (1967Wa02). 


level_energy_unit: KEV
level_spin_parity: 12-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M2
level_comment:
$|m=+5.72 {I8} (1982Ha04,1989Ra17). Compilation: 2005St24 
MOMM1 From NMR on oriented nuclei (1982Ha04). |m=+5.35 {I20} static low temperature nuclear orientation (1971Ba94). 
J from atomic beam (1962Ch13,1976Fu06) and 175|g M4 to 8+. 
T weighted average of 9.7 h {I3} (1960Ba63), 9.5 h {I3} (1960Ka21), 9.7 h {I1} (1962Bo12), 10.4 h {I10} (1963Ka24), 9.5 h {I5} (1963Ti02), 9.5 h {I2}, 9.4 h {I2} (1982Ha04). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J$ L({+3}He,d)=0+2 from 1/2-. L(pol d, |a)=1 from 0+ suggests (0-,1-), L(p,d)=1+3 from 3/2+ suggests 1-,2-,3-. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E from E|g=84.660 keV {I20} in {+196}Au IT decay (9.6 h). 
T weighted average of 8.2 s {I2} (1971Ro16) and 7.4 s {I6} (1972GlZX). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
T from 2001Li17. Others: 6.183 d {I10} (1963Ik01),6.1 d {I1} (1976HeZF), 6.1 d {I1} (1963Ti02), 6.07 d {I11} (1962Li03), 6.15 d {I15} (1962Wa16), 6.17 d {I5} (1962Bo12), 5.3 d {I3} (1963Ka24), 5.6 d {I1} (1960Ba63) 


level_energy_unit: KEV
level_spin_parity: 12-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M2
level_comment:
MOMM1 From g=+0.476 {I7} (1982Ha04). Others: |m=+5.35 {I20} (1971Ba94). 
T weighted average of 9.7 h {I3} (1960Ba63), 9.5 h {I3} (1960Ka21), 9.7 h {I1} (1962Bo12), 10.4 h {I10} (1963Ka24), 9.5 h {I5} (1963Ti02), 9.5 h {I2} (1982Ho04) 


level_energy_unit: KEV
level_spin_parity: 1-&2-
level_comment:
S$0.13 {I3} for L=0, s{-1/2}; 1.14 {I9} for L=2, d{-3/2} 
$d|s/d|W=62 |mb/sr 
E$Attempt to separate this doublet showed that about 90% of the d{-3/2} strength is due to the 307-keV state. 
E$Doublet. 


level_energy_unit: KEV
level_spin_parity: 2-&3-
level_comment:
S$1.57 {I5} for L=2, d{-3/2}. Possible simultaneous d{-3/2} and d{-5/2} transfer cannot be seperated. S=1.19 {I4} for L=0, d{-5/2}. 
$d|s/d|W=74 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
S$for L=0, S=0.42 {I3} for s{-1/2} 
S$for L=0+2, S=0.37 {I4} for s{-1/2}; 0.15 {I9} for d{-3/2} 
$d|s/d|W=54 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 0-,1-
level_comment:
S$for L=0, J|p=0-,1-; S=1.40 {I3} for s{-1/2} 
S$for L=0+2; J|p=1-; S=1.10 {I5} for s{-1/2}; 0.76 {I12} for d{-3/2} 
$d|s/d|W=180 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 0-,1-
level_comment:
S$for L=0, J|p=0-,1-; S=1.09 {I3} for s{-1/2} 
S$for L=0+2, J|p=1-; S=0.96 {I4} for s{-1/2}; 0.40 {I9} for d{-3/2} 
$d|s/d|W=158 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
J$ |g to 2-,3-,4-. (pol d,t) suggests 2-,3-,4-, but 2- inconsistent with the excitation function in (p,n|g). 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.243 {I3} for L=1, p{-1/2}; 0.150 {I10} for L=3, f{-5/2}; 0.034 {I6} for L=3, f{-7/2}. The p{-1/2} component is dominant. 
L$p{-1/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.012 {I7} for L=1, p{-1/2}; 0.063 {I7} for L=1, p{-3/2}; 0.026 {I15} for L=3, f{-5/2}. The p{-3/2} component is dominant. 
L$p{-1/2}, p{-3/2}, f{-5/2}, (f{-7/2}) from a{-y}(|q) in (pol d,t) 
J$2004Wi08 favor the 1- spin-parity assignment to this level as a spin-parity of 2- would imply that the f{-7/2} transfer has a strength too weak to be identified. 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-,3-
level_comment:
S$0.0168 {I4} for L=1, p{-3/2}; (0.0072 {I8}) for L=3, f{-7/2} 
L$p{-3/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.052 {I9} for L=1, p{-3/2}; 0.593 {I21} for L=3, f{-5/2}; 0.130 {I22} for L=3, f{-7/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.238 {I13} for L=1, p{-1/2}; 0.270 {I9} for L=1, p{-3/2}; 0.16 {I3} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.028 {I3} for L=1, p{-1/2}; 0.0316 {I24} for L=1, p{-3/2}; 0.0498 {I6} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, (f{-7/2}) from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
S$(0.0012 {I12}) for L=1, p{-3/2}; 0.166 {I6} for L=3, f{-5/2}; 0.009 {I4} for L=3, f{-7/2}; 0.05 {I4} for L=5, h{-9/2} 
J$If L=1+3+5, then J{+|p}=3- (compilers' note) 
L$(p{-3/2}), f{-5/2}, f{-7/2}, (h{-9/2}) from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.031 {I7} for L=1, p{-1/2}; 0.036 {I5} for L=1, p{-3/2}; 0.0234 {I14} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0164 {I12} for L=1, p{-3/2}; 0.0084 {I3} for L=3, f{-5/2}; 0.042 {I4} for L=3, f{-7/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-
level_comment:
S$(0.004 {I3}) for L=1, p{-1/2}; 0.007 {I3} for L=1, p{-3/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t); no f{-5/2}, f{-7/2} strengths in table IV of 2004Wi08. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.017 {I6} for L=1, p{-1/2}; 0.031 {I6} for L=1, p{-3/2}; 0.116 {I12} for L=3, f{-5/2}; 0.059 {I9} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
S$0.0148 {I20} for L=1, p{-3/2}; 0.020 {I5} for L=3, f{-5/2} 
L$(p{-1/2}), p{-3/2}, f{-5/2}, (f{-7/2}) from a{-y}(|q) in (pol d,t); no p{-1/2}, f{-7/2} strengths in table IV of 2004Wi08. 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.0028 {I7} for L=1, p{-1/2}; 0.0030 {I5} for L=1, p{-3/2}; 0.0119 {I12} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, i{-13/2} from a{-y}(|q) in (pol d,t) for doublet. 


level_energy_unit: KEV
level_spin_parity: 5+,6+,7+,8+
level_comment:
S$0.187 {I1} for L=6, i{-13/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, i{-13/2} from a{-y}(|q) in (pol d,t) for doublet. 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-,3-
level_comment:
S$0.0140 {I12} for L=1, p{-3/2}; (0.0040 {I24}) for L=3, f{-7/2} 
L$(p{-1/2}), p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.192 {I3} for L=1, p{-3/2}; 0.127 {I7} for L=3, f{-5/2}; 0.112 {I7} for L=3, f{-7/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.073 {I5} for L=3, f{-5/2}; 0.015 {I3} for L=3, f{-7/2} 
L$f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0091 {I10} for L=1, p{-3/2}; 0.011 {I3} for L=3, f{-5/2}; 0.004 {I3} for L=3, f{-7/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0033 {I9} for L=1, p{-1/2}; 0.035 {I3} for L=3, f{-5/2}; 0.0033 {I19} for L=3, f{-7/2} 
L$p{-1/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0034 {I6} for L=1, p{-1/2}; 0.0076 {I8} for L=1, p{-3/2}; 0.0128 {I8} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0012 {I4} for L=1, p{-1/2}; 0.0008 {I4} for L=1, p{-3/2}; 0.0096 {I8} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0022 {I6} for L=1, p{-1/2}; 0.0008 {I4} for L=1, p{-3/2}; 0.0224 {I8} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0112 {I4} for L=1, p{-3/2}; 0.0240 {I12} for L=3, f{-5/2}; 0.170 {I14} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-,4-
level_comment:
S$(0.0008 {I4}) for L=1, p{-3/2}; 0.0678 {I12} for L=3, f{-5/2} 
L$(p{-3/2}), f{-5/2}, (f{-7/2}) from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.0012 {I8} for L=1, p{-1/2}; 0.0084 {I8} for L=1, p{-3/2}; 0.0066 {I24} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.018 {I3} for L=1, p{-1/2}; 0.0048 {I24} for L=1, p{-3/2}; 0.022 {I6} for L=3, f{-5/2}; 0.026 {I5} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
S$(0.0040 {I14}) for L=1, p{-3/2}; 0.013 {I4} for L=3, f{-5/2}; 0.030 {I4} for L=3, f{-7/2}; 0.12 {I3} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
S$0.0090 {I9} for L=4, g{-9/2}; 0.0067 {I10} for L=6, i{-13/2} 
L$i{-13/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$(0.0036 {I12}) for L=3, f{-5/2}; 0.0232 {I8} for L=3, f{-7/2}; 0.051 {I9} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0040 {I14} for L=1, p{-1/2}; 0.0084 {I12} for L=1, p{-3/2}; 0.029 {I4} for L=3, f{-5/2}; 0.029 {I4} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
S$0.0083 {I5} for L=4, g{-9/2}; 0.0108 {I17} for L=6, i{-13/2} 
L$g{-9/2}, i{-13/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0160 {I4} for L=1, p{-3/2}; 0.0144 {I24} for L=3, f{-5/2}; 0.0056 {I24} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0072 {I4} for L=1, p{-3/2}; 0.0060 {I18} for L=3, f{-5/2}; 0.0168 {I8} for L=3, f{-7/2}; 0.058 {I10} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.0144 {I18} for L=3, f{-5/2}; 0.0512 {I16} for L=3, f{-7/2} 
L$f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0026 {I6} for L=1, p{-1/2}; 0.0120 {I8} for L=3, f{-7/2} 
L$p{-1/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$(0.0012 {I4}) for L=1, p{-3/2}; 0.0144 {I18} for L=3, f{-5/2}; 0.0064 {I16} for L=3, f{-7/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0057 {I15} for L=1, p{-1/2}; 0.0027 {I14} for L=1, p{-3/2}; 0.010 {I4} for L=3, f{-5/2}; 0.017 {I3} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0056 {I16} for L=1, p{-3/2}; 0.008 {I5} for L=3, f{-5/2}; 0.005 {I4} for L=3, f{-7/2} 
L$(p{-1/2}), p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
S$0.0176 {I4} for L=1, p{-3/2}; 0.0072 {I12} for L=3, f{-5/2} 
L$p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$(0.0048 {I4}) for L=1, p{-3/2}; 0.0816 {I16} for L=3, f{-7/2}; 0.096 {I12} for L=5, h{-9/2} 
L$p{-3/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.0036 {I12} for L=3, f{-5/2}; 0.0024 {I8} for L=3, f{-7/2} 
L$f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0114 {I10} for L=1, p{-1/2}; 0.0024 {I8} for L=1, p{-3/2}; 0.0048 {I24} for L=3, f{-5/2}; 0.0160 {I16} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$0.0296 {I8} for L=3, f{-7/2}; 0.032 {I8} for L=5, h{-9/2} 
L$f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
S$0.0084 {I4} for L=1, p{-3/2}; 0.0084 {I12} for L=3, f{-5/2} 
L$p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
S$(0.0020 {I4}) for L=1, p{-3/2}; 0.0078 {I12} for L=3, f{-5/2}; 0.0160 {I8} for L=3, f{-7/2}; 0.052 {I9} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$(0.0012 {I4}) for L=1, p{-3/2}; 0.0704 {I24} for L=3, f{-7/2}; 0.104 {I20} for L=5, h{-9/2} 
L$p{-3/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.011 {I3} for L=3, f{-5/2}; 0.0200 {I24} for L=3, f{-7/2} 
L$f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0092 {I4} for L=1, p{-3/2}; 0.0240 {I16} for L=3, f{-7/2}; 0.133 {I14} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0196 {I4} for L=1, p{-3/2}; 0.0084 {I24} for L=3, f{-5/2}; 0.0080 {I16} for L=3, f{-7/2}; 0.085 {I15} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$(0.0032 {I8}) for L=1, p{-3/2}; 0.0248 {I16} for L=3, f{-7/2}; 0.039 {I15} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$(0.0006 {I4}) for (L=1, p{-1/2}); 0.0084 {I24} for L=3, f{-5/2}; 0.0064 {I16} for L=3, f{-7/2} 
L$(p{-1/2}), f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$(0.0004 {I1}) for L=1, p{-3/2}; 0.0120 {I8} for L=3, f{-7/2}; 0.04 {I1} for L=5, h{-9/2} 
L$(p{-3/2}), (f{-5/2}), f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$0.0064 {I4} for L=1, p{-3/2}; 0.0648 {I16} for L=3, f{-7/2}; 0.16 {I2} for L=5, h{-9/2} 
L$p{-3/2}, (f{-5/2}), f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.0096 {I18} for L=3, f{-5/2}; 0.0120 {I8} for L=3, f{-7/2}; (0.02 {I1}) for L=5, h{-9/2} 
L$f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-,3-
level_comment:
S$0.0096 {I4} for L=1, p{-3/2}; (0.0018 {I12}) for L=3, f{-5/2}; (0.02 {I1}) for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, (f{-7/2}), (h{-9/2}) from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-,5-
level_comment:
S$0.0072 {I8} for L=3, f{-7/2}; (0.01 {I1}) for L=5, h{-9/2} 
L$f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-,5-
level_comment:
S$(0.0020 {I12}) for L=1, p{-3/2}; (0.004 {I3}) for L=3, f{-5/2}; 0.0368 {I24} for L=3, f{-7/2} 
L$(p{-1/2}), p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-,5-
level_comment:
S$(0.0012 {I6}) for L=1, p{-1/2}; (0.004 {I3}) for L=3, f{-5/2}; 0.0104 {I24} for L=3, f{-7/2} 
L$p{-1/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0052 {I8} for L=1, p{-3/2}; 0.264 {I3} for L=3, f{-7/2}; 0.33 {I3} for L=5, h{-9/2} 
L$p{-3/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
S$(0.0010 {I8}) for L=1, p{-1/2}; 0.0116 {I8} for L=1, p{-3/2}; 0.0120 {I12} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-,5-
level_comment:
S$0.0432 {I8} for L=3, f{-7/2}; (0.03 {I2}) for L=5, h{-9/2} 
L$f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0046 {I10} for L=1, p{-1/2}; 0.0048 {I12} for L=1, p{-3/2}; 0.0042 {I24} for L=3, f{-5/2}; 0.0120 {I24} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.0204 {I18} for L=3, f{-5/2}; 0.0032 {I16} for L=3, f{-7/2} 
L$(p{-3/2}), f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0004 {I1} for L=1, p{-3/2}; 0.0016 {I8} for L=3, f{-7/2} 
L$p{-3/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-,5-
level_comment:
S$(0.0048 {I6}) for L=1, p{-1/2}; 0.2048 {I24} for L=3, f{-7/2} 
L$p{-1/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0108 {I4} for L=1, p{-3/2}; 0.0304 {I24} for L=3, f{-7/2} 
L$(p{-1/2}), (p{-3/2}), f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0088 {I16} for L=1, p{-3/2}; 0.002 {I4} for L=3, f{-5/2}; 0.006 {I3} for L=3, f{-7/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0220 {I8} L=1, p{-3/2}; 0.0176 {I24} for L=3, f{-7/2}; 0.21 {I3} for L=5, h{-9/2} 
L$p{-3/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.004 {I3} for L=1, p{-3/2}; 0.007 {I7} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0040 {I20} for L=1, p{-3/2}; 0.013 {I5} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, (f{-5/2}), f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
S$0.0025 {I3} for L=4, g{-9/2}; 0.018 {I4} for L=6, i{-13/2} 
L$g{-9/2}, i{-13/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
S$0.0108 {I16} for L=1, p{-3/2}; 0.015 {I3} for L=3, f{-5/2} 
L$(p{-1/2}), p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0036 {I4} for L=1, p{-3/2}; 0.0042 {I24} for L=3, f{-5/2}; 0.0072 {I16} for L=3, f{-7/2}; 0.03 {I2} for L=5, h{-9/2} 
L$(p{-1/2}), p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.0020 {I17} for L=3, f{-5/2}; 0.0060 {I16} for L=3, f{-7/2} 
L$f{-5/2}, f{-7/2}, i{-13/2} from a{-y}(|q) in (pol d,t) for doublet; f{-3/2} listed in figure 12 of accompanying appendix seems a misprint 


level_energy_unit: KEV
level_spin_parity: 5+,6+,7+,8+
level_comment:
S$0.0158 {I10} for L=6, i{-13/2} 
L$f{-5/2}, f{-7/2}, i{-13/2} from a{-y}(|q) in (pol d,t) for doublet; f{-3/2} listed in figure 12 of accompanying appendix seems a misprint 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.060 {I2} for L=1, p{-3/2}; 0.058 {I8} for L=3, f{-7/2}; 0.38 {I6} for L=5, h{-9/2} 
L$p{-3/2}, (f{-5/2}), f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_comment:
S$0.0092 {I12} for L=1, p{-3/2}; 0.007 {I5} for L=3, f{-5/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0200 {I4} for L=1, p{-3/2}; 0.012 {I4} for L=3, f{-5/2}; 0.0128 {I24} for L=3, f{-7/2}; 0.05 {I3} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0044 {I4} for L=1, p{-3/2}; 0.0072 {I16} for L=3, f{-7/2}; 0.05 {I2} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$(0.004 {I3}) for L=1, p{-1/2}; 0.0164 {I24} for L=1, p{-3/2}; 0.018 {I7} for L=3, f{-5/2}; 0.082 {I6} for L=3, f{-7/2} 
L$p{-1/2}, p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$0.0148 {I4} for L=1, p{-3/2}; 0.005 {I3} for L=3, f{-5/2}; 0.0056 {I24} for L=3, f{-7/2}; 0.07 {I2} for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0016 {I12} for L=1, p{-1/2}; 0.0048 {I24} for L=3, f{-7/2} 
L$p{-1/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$0.1160 {I24} for L=3, f{-7/2}; 
L$(p{-3/2}), f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 0.13 {I3} for L=5, h{-9/2} 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$0.0030 {I18} for L=3, f{-5/2}; 0.0192 {I16} for L=3, f{-7/2} 
L$(p{-3/2}), f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
S$0.0102 {I18} for L=3, f{-5/2}; 0.0024 {I16} for L=3, f{-7/2}; 0.06 {I2} for L=5, h{-9/2} 
L$f{-5/2}, f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 1-,2-
level_comment:
S$0.0014 {I10} for L=1, p{-1/2}; 0.0092 {I8} for L=1, p{-3/2}; 0.0066 {I18} for L=3, f{-5/2} 
L$p{-1/2}, p{-3/2}, f{-5/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
S$(0.0012 {I4}) for L=1, p{-3/2}; 0.0328 {I16} for L=3, f{-7/2}; 0.06 {I2} for L=5, h{-9/2} 
L$(p{-3/2}), f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-,5-
level_comment:
S$(0.0009 {I3}) for L=1, p{-3/2}; 0.009 {I3} for L=3, f{-7/2}; (0.02 {I1}) for L=5, h{-9/2} 
L$(p{-3/2}), f{-7/2}, h{-9/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_comment:
S$(0.0008 {I4}) for L=1, p{-3/2}; 0.009 {I3} for L=3, f{-5/2}; 0.0192 {I24} for L=3, f{-7/2}; (0.03 {I2}) for L=5, h{-9/2} 
L$p{-3/2}, f{-5/2}, f{-7/2} from a{-y}(|q) in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_comment:
S$0.0060 {I4} for L=1, p{-3/2}; 0.010 {I4} for L=3, f{-5/2}; 0.050 {I3} for L=3, f{-7/2} 
L$|s(|q), a{-y}(|q) not shown for this level in figure 14 of accompanying on-line appendix. 


level_energy_unit: KEV
level_spin_parity: (1)
level_comment:
S$0.0026 for L=1, J=1-; 0.0010 for L=0, J=1+; 0.0011 for L=2, J=1+ 
$d|s/d|W=0.4 |mb/sr 
J$1-,1+ in figure 15 of d|s/d|W(|q) within online appendix 


level_energy_unit: KEV
level_spin_parity: (3+,4-)
level_comment:
S$0.0021 for L=2, J=3+; 0.0081 for L=4, J=3+; 0.0012 for L=3, J=4-; 0.0109 for L=5, J=4- 
$d|s/d|W=2.1 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
S$0.0010 for L=1; 0.0003 for L=3 
$d|s/d|W=0.4 |mb/sr 
J$(2-) in figure 15 of d|s/d|W(|q) plot in online appendix 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
S$0.0124 for L=1 
$d|s/d|W=1.6 |mb/sr 
E$2004Wi08 assumed that this state was an unresolved doublet structure consisting of a 1- state in (pol d,|a) and an additional (3,4,5)- state, as in (pol d,t) data. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
T$ from ENSDF database for {+196}Au 
T$ measured change in half-life with temperature of 10K and 293K=+0.1% {I3} {I2}, the second uncertainty is systematic 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: H
level_comment:
E$from the Adopted Levels of {+196}Au in the ENSDF database 
T$average of 9.82 h {I+106-87} and 10.16 h {I+29-28} from 293.55|g(t) (2019Ja03). 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
E$level population in this decay proposed by 2020Mo24, based on a similar level from in-beam |g-ray study by 2000Gr32: Phys. Rev. C 62, 064304 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
J$ from ENSDF database for {+196}Au 
T$average of 6.1448 d {I24} and 6.1451 d {I12} for 333|g(t) and 356|g(t) (2011Hi19). Uncertainty is dominated by 0.23% systematic uncertainty 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J J=3/2 from optical spectroscopy (1939El03) and |p from L=2 in {+196}Pt({+3}He,t) 
|m=+0.145746 {I9} (2001StZZ,1989Ra17,1967Da04), +0.148158 {I8} ({+2}H standard, 2001StZZ,1989Ra17,1967Na13) 
Q=+0.594 {I10} (2001StZZ,1989Ra17,1967Bl16), +0.547 {I16} (2001StZZ,1989Ra17,1974Po12) 
<|b{-2}{+2}>{+1/2}=(-)0.11 (1989Wa11) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J L=0 in {+196}Pt({+3}He,t) 
|m=+0.420 {I3} ({+197}Au standard,2001StZZ,1989Ra17,1968Co17) 
T from (|g,|g) Mossbauer. Others: 1.93 ns {I3} (1973Ly01), from (191|g)(77|g)(t),1.95 ns {I5} (1967Ba27), 1.95 ns {I6} (1968Ra29), 1.84 ns {I2}(1972Gu03) from delayed coin 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
MOMM1$others: +0.74 {I5} (1989Ra17), +0.63 {I10} from g=+0.25 {I4} 
T recoil-distance Doppler shift in Coulomb excitation (1979Bo10) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
Others: +6.44 {I39} (1983Li21), +5.94 {I39} (1982LiZV) 
MOME2$Others: +1.35 {I22} ({+197}Au standard,1983Be68) 
J J=11/2 from |g|g(|q) measurements (1956Ka09, {+197}Au IT decay) and |p=- from L=5 in {+196}Pt({+3}He,d). 
See 1974Tj02 for |DJ=2 bands of {+191}Au, {+193}Au, {+195}Au up to J=23/2 based on decoupled h11/2 proton state 
T from |g(t) measurements(1986Ne05, {+197}Au IT decay).Others: 7.5 s {I2} (1966Sm01), 7.86 s {I4} (1972Jo05), 7.67 s {I7} (1967Yu01), 7.94 s {I17} (1967Bo26), 7.4 s {I3} (1947Fr04), 7.23 s {I28} (1955Fi30), 7.0 s {I2} (1963Ka34), 7.8 s {I1} (1981Ha52), 7.85 s {I4} (1970Jo16), 7.5 s {I4} (1973Fo15), 9 s {I2} (1963Va31), 7.2 s {I1} (1963Ve13), 7.5 s {I5} (1945Wi02). Other evaluation: 7.8 s {I1} (1981Ha52) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
|m=+0.84 {I8} (2001StZZ,1989Ra17,1988St16,1988St09) (from g=+0.241 {I21} in Coul. ex.), +0.52 {I7} (1989Ra17,1986Ba19) (from g=+0.15 {I2} in Coul. ex.), +0.53 {I7} (2001StZZ) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
Level polarization determined in Mossbauer study of oriented {+197}Pt |b{+-} decay (1970Eh01); deduced matrix element mixing for first-forbidden |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
Branching: I|g(269|g)/I|g(191|g)=0.049 {I10} (1974HeYW), 0.063 {I6} (1965He04), 0.07 {I1} (1965Ha15). See also {+197}Hg |e decay and Coul. ex. 
(77|g)(191|g)-coin: 1952Sc27, 1956Po05, 1965He04 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
(130|g)(279|g)(|q): A{-2}=-0.299 {I12}, A{-4}|?0 (1956Ka09) 
g=(+)1.087 {I16} (1984Ha12), 1.17 {I7} (1983Li21) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$others: 1.95 ns {I5} (1967Ba27), 1.95 ns {I6} (1968Ba29), 1.84 ns {I2} (1972Gu03) from delayed coin. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
Branching: I|g(269|g)/I|g(191|g)=0.062 {I4} (1979He12), 0.078 {I16} (1974HeYW), 0.07 {I2} (1967Bu22), 0.076 {I7} (1965Ha15), 0.067 {I10} (1965He04). See also {+197}Pt |b{+-} decay and Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
Branching: I|g(202|g)/I|g(279|g)=0.0146 {I21} (1965Ha15), 0.016 {I3} (1966Sm01), 0.0139 {I25} (1970Pl05); see also Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
Change of mean-square charge radius |D<r{+2}>=+8.6|*10{+-3} (fm){+2} (1985De51), 7.9|*10{+-3} (fm){+2} 17 (1982Ko30) 
<r{+2}>=29.485 (fm){+2} (1985Kl09) (using muonic x-ray data for calibration). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T av of 1.93 ns {I21} (1963Ro05), 1.892 ns {I14} (1969St04), 1.917 ns 12 (1971Er18), 1.90 ns {I5} (1973Po04) Mossbauer, gold metal absorber. 1973Pf01 observed no anomalously narrow line |G, as reported by 1973Po04 (T{-1/2}=2.31 ns {I8}) Mossbauer, gold alloy absorber 
|m: +0.419 {I5} (1968Co17), +0.413 {I5} (1971ThZU) relative to +0.14486 ({+197}Au g.s.). Other: 1976St23 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
Branching: I|g(432|g):I|g(657|g):I|g(667|g):I|g(858|g):I|g(93 6|g)=24 {I5}:20 {I4}:61 {I8}:25 {I6}:100 (1971Ba29), --:20:86:--:100 (1971Ne01) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
Branching: I|g(766|g):I|g(777|g):I|g(1044|g)=100:69 {I16}:48 {I16} (1971Ba29), 100:50:-- (1971Ne01) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
Branching: I|g(882|g):I|g(1073|g):I|g(1151|g)=100:93 {I29}: |?26 (1971Ba29), 100:89: <13 (1971Ne01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
T 1.91 ns {I2} (+0 Au), 1.97 ns {I8} (+10 Au) (1974Ul01). T{-1/2}(neutral atom Au)/T{-1/2}(10+ Au)=0.95 {I10} (1974Yo02) 
B(E2)=0.130 {I7} (1971FoZW), B(E2)/(1+|a)=0.0231 {I17} (1974Yo02) 
B(E2): for |a=4.23 {I7}, |d=-0.35 {I1} B(E2) values lead to T{-1/2}=1.63 ns 13 (1971FoZW), 1.75 ns {I16} (1974Yo02). The adopted value is 1.91 ns 1. 
Others: 1955Be19, 1958Mc02 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$recoil-distance method (1979Bo10). Others: 13.7 ps {I33} if B(E2)=0.083 {I6}, I(|g+ce 269|g)=3.3% {I3} and |a(269|g)=0.15; 13.9 ps {I35} (1986Ba19). Others: 1961Re02, 1969PrZV, 1970Sh12 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
g=+0.296 {I23} (1988St16,1988St09), +0.21 {I2} (1986Ba19) 
T recoil-distance method (1979Bo10). Others: 15.8 ps {I30} if B(E2)=0.314, I|g(279|g)-branching=98.5%, |d=-0.40; 20.4 ps {I+37-26} (1988St16) Doppler-broadened line shape technique; 16.0 ps {I28} (1986Ba19) Doppler-shift attenuation method. 
Other B(E2)'s: 1957El11, 1958Mc02, 1958Ma36, 1961Re02, 1970Sh12 
I|g(202|g)/I|g(279|g)=0.0150 {I12} (1971Mc14), 0.0142 (1970Sh12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T other: <2.8 ps (recoil-distance method,1979Bo10) 
Branching: I|g(426|g)/I|g(503|g)=3/97 (1988St16) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
B(E2)=0.457 {I12} (1971Fo12), 0.447 {I22} (1971Mc14) 
T others: 6.8 ps {I5} (1979Bo10) recoil-distance method; 4.65 ps 28 if B(E2)=0.447 {I22}, I|g(547|g)-branching=94.4%; |?5 ps (1974WaZA) Doppler-broadened lineshape; 4.57 ps {I28} (1981Ve12) RDM; 4.6 ps {I28} (1986Ba19) Doppler-shift attenuation method. 
Other B(E2)'s: 1957El11, 1961Co35, 1961Re02, 1970Sh12 
Branching: I|g(547|g):I|g(279|g):I|g(268.6|g)=100:0.7 {I2}:5.2 {I4} (1971Mc14), 100:--:7.3 (1970Sh12), 95:--:5 (1988St16) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T others: 5.1 ps {I22} (1979Bo10), 3.05 ps {I35} (1981Ve12), recoil-distance method. 
Branching: I|g(308|g)/I|g(577|g)=14/86 (1988St16), 8/92 (1981Ve12) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$ from {+197}Au in ENSDF. 
$ Configuration=h{-11/2} 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_comment:
E$ probably an admixture of multiple configurations: coupling of aligned h{-11/2} proton hole with 5- states observed in neighboring Pt, Hg, and Pb nuclei, which themselves are a mixture of configurations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (25/2,27/2,29/2)
level_lifetime_unit: NS
level_comment:
J$if no aditional low-energy transition exists 
T$from |g(t) (2006Wh02). The isomer may belong to the 2532 level a higher lying state at 2532+x deexciting by a low-energy transition 
$ Configuration for 27/2+: |ph{-11/2}~#(|ni{-13/2}~#|np{-3/2}){-8-} or |ph{-11/2}~#(|ni{-13/2}~#|nf{-5/2}){-8-} 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_uncertain: ?
level_comment:
$ Configuration: |ph{-11/2}~#(|ni{-13/2}~#|nf{-9/2}){-10-} for 31/2+; |ph{-11/2}~#(|ni{-13/2}~#|nh{-9/2}){-11-} for 33/2+ 
E$x<85 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
$ B(E2): first value from {+58}Cr beam, second value from {+60}Cr beam 
$ B(E2)=0.449 {I41} (ENSDF database for {+197}Au) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
No |e observed. For log| {If{+1u}t}>8.5, expected for the branch to g.s., %|e<0.04 
<r{+2}>{+1/2}=5.439 fm {I4} (2004An14). 
MOMM1 Atomic Beam Magnetic Resonance/Direct moment measurement (AB/D, 1967Va16). Other: +0.64 {I2} (1990Sa21, Laser Resonance Ionisation Mass Spectroscopy(LRIMS)) 
MOME2 Nuclear Magnetic Resonance on Oriented Nuclei(NMR/ON) and {+193}Au standard (1993Hi10). Others: +0.68 {I2} (1988Ed01, NMR/ON; {+197}Au standard), 0.76 {I4} (1984Ha03, NMR/ON, Nuclear Magnetic Resonance(NMR); {+197}Au standard), 0.88 {I8} (1985Ka16, NMR; {+197}Au standard), +0.69 {I4} (1983He26,1984Ha03, Static Nuclear Orientation with gamma detection(NO/S), NMR/ON; {+199}Au standard), +0.46 {I2} (1983He26,1983Pe22). Mossbauer Effect (ME), NO/S; {+197}Au standard) 
J J=2 from atomic beam (1976Fu06) and |p=- from L=3 in (d,p) and E1 primary |g from 1+ capture state in {+197}Au(n,|g) E=thermal. 
T$Weighted average of 2.697 d {I3} (1953Lo09), 2.699 d {I3} (1954Be61), 2.686 d {I5} (1955To07), 2.697 d {I5} (1956Jo24), 2.694 d {I6} (1956Sa75), 2.704 d {I4} (1958Ke26), 2.699 d {I4} (1960Ro22), 2.687 d {I5} (1964St20), 2.694 d {I4} (1965An07), 2.695 d {I7} (1968Go22), 2.697 d {I5} (1968La10), 2.693 d {I5} (1968Re04), 2.695 d {I2} (1969Vu04,1983LoZV), 2.6946 d {I10} (1970Ca09), 2.696 d {I4} (1970Co14), 2.693 d {I3} (1971De11), 2.6935 d {I4} (1980RuZV), 2.6966 d {I7} (1990Ab02), 2.6837 d {I50} (1994Mi03), 2.6924 d {I11} (2005Li66), 2.6948 d {I5} (2006No10), 2.6971 d {I20} (2008Ku09), 2.6939 d {I4} (2008Ru05), 2.6948 d {I9} (2010Go25), 2.684 d {I4} (from decay curve for 412|g at room temperature, another value: 2.687 d {I5} at 12 K temperature, 2010Fo13), 2.6899 d {I8} (2010Li48), 2.69445 d {I32} (2012Ha23) and 2.6934 d {I37} (2014Un01). Other measurements: 2.69 d {I1} (1949Si02), 2.66 d {I1} (1951Ca06), 2.73 d {I2} (1951Si25), 2.6937 d {I2} (1977MeZB,1977MeZN, superseded by 1980RuZV), 2.695 d {I2} (1982HoZJ, superseded by 2014Un01), 2.69517 d {I21} (1992Un01, superseded by 2014Un01), 2.69555 d {I30} (2004Un01, superseded by 2014Un01), 2.6949 d {I9} (2007Go39, superseded by 2010Go25), 2.706 d {I19} (2007Sp01, superseded by 2010Fo13), 2.6949 d {I8} (2010Ha12, superseded by 2012Ha23), 2.6782 d {I3} (2011Li52, Chauvenent outlier). Other evaluations: 2.6943 d {I3} (Decay Data Evaluation Project, DDEP), 2.6948 {I12} (2011Ch22), 2.6944 {I8} (2004BeZQ), 2.6945 d {I4} (1996ChZY), 2.6943 d {I8} (1991BaZS,1990Ni03), 2.696 d {I2} (1983Au08), 2.6935 d {I4} (1982RuZV). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: NS
level_comment:
|m from TDPAD 
J J=5 from |m analysis ((|g|g(|q,t), 1976Fu06) and |p=+ from E1 |g to 4- 
T From |g|g(t) in {+197}Au(n,|g) E=thermal (1975Mi05). Others: 118 ns 8 (|g|g(t)(1973Pa08)), 128 ns {I15} (p,|g(t)(1968Bo30)) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J M1 |g to 482, M1 |g from 482 to 5+ 312, and observed weak feeding of 636 level in 24-keV average resonance capture uniquely establishes J|p(637)=4+ and J|p(482)=4+ 


level_energy_unit: KEV
level_comment:
J 2-keV average resonance capture data give 0+, 24-keV average resonance capture data allow 0+ or 4+, but 0+ is in conflict with observed decay of level to 3-, and possible decay from 3+ 1095 


level_energy_unit: KEV
level_spin_parity: (12-)
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1 Nuclear Magnetic Resonance on Oriented Nuclei(NMR/ON) (1984Ha12). 
T From weighted average of 2.27 d {I2} (1972Cu06), 2.36 d {I7} (1973Pa08), and 2.26 d {I3} (1992ZhZG) 


level_energy_unit: KEV
level_uncertain: S
level_comment:
E Possible a proposed 646 level could resolve intensity imbalance at the 312 level. It could be fed directly from the isomer, or via a low-energy transition from 696-level. The latter is more likely, and would suggest I(|g+ce)(115.2|g)=100. Neither author would have seen a highly converted 50|g connecting the 696 and the possible 646 level. Unplaced 333.82|g could be placed between 646 and 312 levels. 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=172.5 {I82} 
J (1-,2-)+(1-,2) or (1-,2-)+(0-,3-) for 259.5+262.2 levels 
S Sum of 259.5+262.2 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=172.5 {I82} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 259.5+262.2 levels 
S Sum of 259.5+262.2 levels 


level_energy_unit: KEV
level_spin_parity: 0+,3+
level_comment:
$I|g/E|g{+5}=7.6 {I11} 
J Average resonance capture value is discrepant with |p=- required by mult(380|g)=E2 (taken from 1975Mi05) to 2-. 


level_energy_unit: KEV
level_spin_parity: 0-,3-
level_comment:
$I|g/E|g{+5}=48.9 {I18} 
E From authors' Table 2. Value of 511.6 in Table 1 is apparently a misprint. 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=138 {I20} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 528.88+530.27 levels known from (n,|g) E=thermal. 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=174 {I11} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 787.0+790.1 levels 
S Sum of 78.07+790.1 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=174 {I11} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 787.0+790.1 levels 
S Sum of 787.0+790.1 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=157.5 {I91} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 916.5+918.8 levels. 
S Sum of 916.5+918.8 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=154 {I12} 
E Multiplet structure consisting two (or more) unresolved primary transitions. 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=225.4 {I82} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 259.5+262.2 levels 
S Sum of 259.5+262.2 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=173.5 {I39} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 528.88+530.27 levels known from (n,|g) E=thermal. 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=190 {I11} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-3-) for 787.0+790.1 levels 
S Sum of 787.0+790.1 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=190 {I11} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 787.0+790.1 levels 
S Sum of 787.0+790.1 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=190 {I11} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 916.5+918.8 levels 
S Sum of 916.5+918.8 levels 


level_energy_unit: KEV
level_comment:
$I|g/E|g{+5}=190 {I11} 
J (1-,2-)+(1-,2-) or (1-,2-)+(0-,3-) for 916.6+918.8 levels 
S Sum of 916.5+918.8 levels 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
$ <r{+2}>{+1/2}=5.444 fm {I4} (2004An14, evaluation) 
J$spin from atomic beam (1956Ch08); parity from M1+E2 |g from 1/2+. Also L(t,p)=0 and L({+3}He,d)=2 
T$weighted av: 3.13 d {I9} (1972Em01), 3.129 d {I11} (1969La34), 3.14 d {I2} (1957Wr37), 3.148 d {I10} (1955Be42) 
MOMM1$from atomic-beam magnetic resonance (1967Va16). Other: +0.282 {I2}, +0.261 {I2} (laser-resonance ionization mass spectroscopy,1990Sa21). See also compilation by 2005St24 
MOME2$nuclear magnetic resonance on oriented nuclei (1993Hi10). Others: 0.64 {I6} (1985Ka16,1982Ha39); 0.55 {I3} (1984Ri15,1982Ha39); +0.37 {I1} (Mossbauer effect,1983Pe22,1983He26). Q({+198}Au)/Q({+199}Au)=1.24 {I2}(1988Ed01), 1.26 {I3} (1983He26), 1.37 {I3} (1983Ha48). See also compilation by 2005St24 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
J$L({+3}He,d)=5; syst of isomers in Au isotopes; E2 |g from 7/2- 
$Configuration=1/2[501] (1980AtZZ) 
T$from {+199}Pt |b{+-} decay (1968Bo22) 
%IT$From log| {Ift} systematics, %|b{+-} is negligible (%|b{+-}|?1|*10{+-6} for log| {Ift}|?6 for |b{+-} transition to the 13/2+ level in {+199}Hg) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+,7/2+
level_comment:
J$L(t,p)=2; not 1/2+ from log| {Ift}=8.2 (log| {If{+1u}t}<8.2) from 5/2-. L({+3}He,d)=(0) is inconsistent with adopted J|p 


level_energy_unit: KEV
level_comment:
J$L({+3}He,d)=6 for 1314 group (1980AtZZ) suggests 11/2+,13/2+; but L({+3}He,d)=3 for a 1335 group (1978Mu08) suggests 5/2-,7/2- 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)+
level_comment:
J$|g to 3/2+; L(t,p)=4. L({+3}He,d)=0 (1980AtZZ) for a 1563 group suggests 1/2+, but L({+3}He,d)=(2) for a 1580 group (1978Mu08) suggests (3/2+,5/2+) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$L({+3}He,d)=(6) for 1729 group (1980AtZZ) suggests (11/2+,13/2+); but L({+3}He,d)=3 for a 1770 group (1978Mu08) suggests 5/2-,7/2- 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$ C{+2}S=0.193 (1978Mu08) 
$ 3/2[402] (corresponding orbital is 3/2[431] in 1980AtZZ) assignment in 1978Mu08. The 319 level is associated with 3/2[431] orbital by 1980AtZZ 
$d|s/d|W=140 |mb/sr; |s(|a,t)/|s({+3}He,d)=0.91 (1978Mu08) 
$ |s(A,T)(45|')/|s(3HE,D)(30|')=10 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
E$ 76 3 (1978Mu08) 
$ C{+2}S=0.198 (1978Mu08) 
$d|s/d|W=76 |mb/sr; |s(|a,t)/|s({+3}He,d)=0.16 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+&5/2+
level_comment:
E$possibly a doublet: 317.0, 5/2+ and 323.6, 3/2+ in 'adopted levels' 
E$ 320 5 (1978Mu08) 
$3/2[431] assignment in 1980AtZZ, 1/2[400] (corresponding orbital is 1/2[431] in 1980AtZZ) in 1978Mu08 
$ C{+2}S=0.032 (1978Mu08) for 3/2+ 
$|s(|a,t)/|s({+3}He,d)=1.13 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+&11/2-
level_comment:
E$ 545 4 (1978Mu08) 
$ C{+2}S=0.070 for 5/2+, 0.098 for 11/2- (1978Mu08) 
E$543+549 unresolved doublet. 
$For 11/2- level: 1/2[501] in 1980AtZZ (corresponding orbital is 1/2[550] in 1978Mu08) 
$d|s/d|W=75 |mb/sr; |s(|a,t)/|s({+3}He,d)=2.0 for doublet (1978Mu08) 
$ |s(A,T)(45|')/|s(3HE,D)(30|')=10 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-,7/2-
level_comment:
J$7/2- in 'adopted levels' 
$If 7/2-, possible orbital is 1/2[501] (1980AtZZ) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=2.2 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$ C{+2}S=0.326 for L=0 (1978Mu08) 
S$2.6 for possible L=4, 7/2+ component (1980AtZZ) 
E$ 821 5 (1978Mu08) 
$1/2[440] orbital (1980AtZZ) (corresponding orbital is 1/2[411] in 1978Mu08) 
L$According to 1980AtZZ this peak possibly includes L=4 component, but the data seem to fit L=0 in both 1980AtZZ and 1978Mu08 
$d|s/d|W=180 |mb/sr; |s(|a,t)/|s({+3}He,d)=0.34 (1978Mu08) 
$ |s(A,T)(45|')/|s(3HE,D)(30|')=3.2 (1980AtZZ) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$3/2+,5/2+ in 'adopted levels' 
$Possible member of 1/2[440] (labeled as 1/2[411] by 1978Mu08) band (1978Mu08) 
$ C{+2}S=0.025 (1978Mu08) 
E,L$from 1978Mu08. A peak near this energy is present in the spectra shown by 1980AtZZ from both the ({+3}He,d) and (|a,t) reactions, but it is not listed as a level in {+199}Au in tabular data 
$d|s/d|W=27 |mb/sr (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$(3/2+,5/2+,7/2+) in 'adopted levels'; L=0 is inconsistent with 'adopted' J|p 
L$from 1978Mu08 
E$ 1159 5 (1978Mu08) 
$ C{+2}S=0.035 (1978Mu08) 
$d|s/d|W=40 |mb/sr (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$3/2+,5/2+,7/2+ in 'adopted levels'; L=(0) is inconsistent with 'adopted' J|p 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=6.2 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_comment:
J$no assignment in 'adopted levels' 
E$1335 {I5} group in 1978Mu08 is probably the same level as 1314 in 1980AtZZ 
L$3 (1978Mu08) for 1335 
$C{+2}S=0.034 for L=3, 7/2- (1978Mu08) 
$|s(|a,t)/|s({+3}He,d)=0.8 (1978Mu08) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=3.2 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_comment:
J$(11/2+,13/2+) in 'adopted levels' 
E,L$see comment for 1563 level 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=1.4 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$(5/2,7/2)+ in 'adopted levels'; L=0 is inconsistent with 'adopted' J|p 
E$1580 {I5} group in 1978Mu08 probably corresponds to 1542+1563 in 1980AtZZ 
L$(2) for 1580 (1978Mu08) (note that 7/2- listed by 1978Mu08 is inconsistent with their L=(2) assignment) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=1.7 (1980AtZZ) 
$d|s/d|W=28 |mb/sr; |s(|a,t)/|s({+3}He,d)=1.0 for 1580 (1978Mu08) 
$C{+2}S=0.019 for L=(2) (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2,9/2-
level_comment:
J$(5/2 to 11/2)+ in 'adopted levels' 
E,L,S$see comment for 1729 level 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=2.8 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2+)
level_comment:
J$no assignment in 'adopted levels' 
E$1770 {I5} group in 1978Mu08 probably corresponds to 1696+1729 in 1980AtZZ. 
L$3 for 1770 group (1978Mu08) 
$C{+2}S=0.032 for L=3, 7/2- (1978Mu08) 
$d|s/d|W=26 |mb/sr (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
J$9/2-,11/2- in 'adopted levels' 
$9/2[514] orbital (1980AtZZ) (corresponding label is 9/2[505] in 1978Mu08) 
E$1910 {I5} group in 1978Mu08 corresponds mainly to 1861 group in 1980AtZZ, but may contain contribution from 1890 group also 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=14 (1980AtZZ) 
$C{+2}S=0.374 for L=5, 9/2- (1978Mu08) 
$d|s/d|W=30 |mb/sr; |s(|a,t)/|s({+3}He,d)=4.97 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J$(5/2-,7/2-) in 'adopted levels' 
$Possible 7/2[514] orbital (1980AtZZ) 
E$2390 {I10} group in 1978Mu08 probably corresponds to 2374 in 1980AtZZ 
$C{+2}S=0.040 for L=3, 7/2- (1978Mu08) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=2.2 (1980AtZZ) 
$d|s/d|W=37 |mb/sr (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2
level_comment:
J$(3/2+,5/2,7/2-) in 'adopted levels' 
E$possibly the 2540 {I10} group in 1978Mu08 
L$3 in 1978Mu08 for 2540 group 
$C{+2}S=0.045 for L=3, 7/2- (1978Mu08) 
$d|s/d|W=61 |mb/sr; |s(|a,t)/|s({+3}He,d)=1.19 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2-
level_comment:
J$(3/2+,5/2,7/2-) in 'adopted levels' 
E$possibly the 2650 {I10} group in 1978Mu08 
L$(3) in 1978Mu08 for 2650 group 
$C{+2}S=0.037 for L=(3), 7/2- (1978Mu08) 
$d|s/d|W=37 |mb/sr (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2-
level_comment:
J$(3/2+,5/2,7/2-) in 'adopted levels' 
E$possibly the 2950 {I10} group in 1978Mu08 
L$3 in 1978Mu08 for 2950 group 
$C{+2}S=0.035 for L=3, 7/2- (1978Mu08) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=2.9 (1980AtZZ) 
$d|s/d|W=82 |mb/sr (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-,13/2+
level_comment:
J$(9/2-,11/2,13/2+) in 'adopted levels' 
$If 13/2+, possible 13/2[606] orbital (1980AtZZ), 1978Mu08 associated 3400 level with this orbital 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=2.6 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J$(5/2-,7/2-) in 'adopted levels' 
$Possible 7/2[523] orbital (1980AtZZ) 
E$3130 {I10} group in 1978Mu08 probably corresponds to 3044+3083, since the 3044 group in 1980AtZZ and 3130 group in 1978Mu08 is the second most intense peak in the spectra shown, the most intense being 1861 group in 1980AtZZ and 1910 group in 1978Mu08 
$C{+2}S=0.084 for L=3, 7/2- (1978Mu08) 
$d|s/d|W=300 |mb/sr; |s(|a,t)/|s({+3}He,d)=0.64 (1978Mu08) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
J$(11/2+,13/2+) in 'adopted levels' 
$ C{+2}S=0.45 (1978Mu08) 
$possible i{-13/2} orbital (1978Mu08) 
$d|s/d|W=31 |mb/sr; |s(|a,t)/|s({+3}He,d)=5.6 (1978Mu08) 


level_energy_unit: KEV
level_comment:
$|s(|a,t)/|s({+3}He,d)=0.91 
$d|s/d|W(20|')=73 |mb/sr 9 (1977MuZD) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=10 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(|a,t)/|s({+3}He,d)=2.0 
E$ 545 (1978Mu08) 
E$doublet: 5/2[543] and 11/2[549] states 
$d|s/d|W(20|')=210 |mb/sr 15 (1977MuZD) 
$|s(|a,t)(60|')/|s({+3}He,d)(30|')=10 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(|a,t)/|s({+3}He,d)=0.34 
E$ 821 (1978Mu08) 
$d|s/d|W(20|')=73 |mb/sr 15 (1977MuZD) 
$|s(|a,t)(45|')/|s({+3}He,d)(30|')=3.2 (1980AtZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(|a,t)/|s({+3}He,d)=3.2 
E$1335 in 1978Mu08 probably the same level as 1314 in 1980AtZZ 
$|s(|a,t)(20|')/|s({+3}He,d)(20|')=0.8 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(|a,t)/|s({+3}He,d)=1.7 
E$1580 in 1978Mu08 probably the same level as 1542+1563 in 1980AtZZ 
$|s(|a,t)(20|')/|s({+3}He,d)(20|')=0.8 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(|a,t)/|s({+3}He,d)=14 
E$1910 in 1978Mu08 corresponds to 1861 (and possibly 1890 also) in 1980AtZZ 
$d|s/d|W(20|')=581 |mb/sr 24 (1977MuZD) 
$|s(|a,t)/|s({+3}He,d)=5.0 (1978Mu08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(|a,t)/|s({+3}He,d)=1.19 
E$2540 in 1978Mu08 probably the same level as 2512 in 1980AtZZ 
L$for 2540+2650 (1977MuZD) 
$d|s/d|W(20|')=157 |mb/sr 44 (1977MuZD) for 2540+2650 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: MIN
level_comment:
J$Strong population of the J|p=0+ and 2+ (1593.4 keV) levels in {+200}Hg following {+200}Au |b{+-} decay; |p from systematics of single-particle structures in neighboring odd-mass nuclei 
T$From |b(t) in 1959Ro53. Others: 48 min {I1} (1960Gi01) and 48 min {I2} (1941Sh08) 
CONF$Dominant |p(d{-3/2}{+-1})~#|n(f{-5/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: 12-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
$%IT is from 1972Cu07; Others: %IT=14.8 {I26} by the evaluator using I(|g+ce)(497.7|g,{+200}Hg) and I(|g+ce)(332.8|g) (assumed E2) from 1972Cu07, the later being the strongest |g ray assigned to follow the decay of the isomer (1972Cu07) and %IT=3 (1968Sa08) 
E$From 2021Ko07, based on AME mass adjustment - see 2021Hu06 for details. 
J$Directly measured in 1973Ba11 using the nuclear magnetic resonance of oriented nuclei technique; measured |m; strong |b{+-} feeding of the J|p=11- state at 2641.57 keV in {+200}Hg following {+200m}Au |b{+-} decay 
T$From 580|g(t) in 1968Sa08 
MOMM1$From |m=5.80 {I9} in 1984Ha45 determined using the NMR on oriented nuclei technique. Other: 6.10 {I20} (1973Ba11) 
CONF$|p(h{-11/2}{+-1})~#|n(i{-13/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: 12-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
$%IT is from 1972Cu07; Others: %IT=14.8 {I26} by the evaluator using I(|g+ce)(497.7|g,{+200}Hg) and I(|g+ce)(332.8|g) (assumed E2) from 1972Cu07, the later being the strongest |g ray assigned to follow the decay of the isomer (1972Cu07) and %IT=3 (1968Sa08) 
T$From 580|g(t) in 1968Sa08 
MOMM1$5.80 {I9} in 1984Ha45 determined using the NMR on oriented nuclei technique. Other: 6.10 {I20} (1973Ba11) 
CONF$|p(h{-11/2}{+-1})~#|n(i{-13/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
T$Weighted average of 26 min {I1} (1957Er24), 27 min {I2} (1962Fa06), 22 min {I3} (1962Eu01) and 26.4 min {I16} (1972Pa24). Other: 26 min (1952Bu80) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
E$Introduced by the evaluator by assuming that 638|g directly feeds the J|p=11/2- isomer. The existence is tentative 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
E$Introduced by the evaluator by assuming that 378.2|g precedes 638.0|g. The assignment is tentative 
J$From 378.2|g (M2) to (15/2-). The assignment is tentative. 
T$From 378.2,638.0|g(t) in {+9}Be({+208}Pb,X|g) (2011St21) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$ From adopted levels 
T$ From 553|g(t) in 2011St21 
$Experimental isomeric state population ratio=13% {I+36-11} 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
E$Introduced by the evaluator by assuming that 378.2|g precedes the 638.0|g. The assignment is tentative 
T$From 378.2,638.0|g(t) in 2011St21 
$Experimental isomeric state population ratio=5% {I3} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
J$Predominant |b{+-} decay branches to 0+ states in {+202}Hg (1984Cr01, 1972Pa06); d|s/d|W(|q) DWBA analysis in 2003WiZW suggests J|p=(1-), but A{-y}(|q) in the same work is consistent with J|p=0-; systematics of structures in neighboring odd-odd Au nuclei suggest J|p=1- or 2- 
T$Weighted average of 28.8 s {I19} (440|g(t),1984Cr01), 30 s {I3} (440|g(t),1967Wa23), 27 s {I2} (|b(t),1972Bu05) and 29 s {I3} (440|g(t),1972Pa06,1972Pa38). Others: |?25 s (1952Bu80) 
CONF$|p(d{-3/2}{+-1})~#|n(f{-5/2}{+-1}). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
T$From |b|g(|Dt) in 1994We02. Others: 53 s {I2} from 690|g(t) in 1972Bu42. However, no such gamma ray has been identified in |b{+-} decay of {+203}Au and, hence, this value has been excluded; |?55 s (1952Bu80); 7 h {I2} from 830|g(t) and 1041|g(t) in 1979Na08. However, no such gamma rays were identified in |b{+-} decay of {+203}Au and, hence, this value has been excluded. 
$Dominant configuration=|p(d{-3/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$From 563.3|g(t) in 2011St21. Other: 0.04 ms {I+700-2} from 563.3|g(t) in 2005Ca02. 
$Dominant configuration=|p(h{-11/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$Also: 976.8|g to 3/2+; direct feeding in {+203}Pt |b{+-} decay (J|p=1/2-); shell model predictions 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$Also: 943.6|g to 1/2+; direct feeding in {+203}Pt |b{+-} decay (J|p=1/2-); shell model predictions 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$From adopted levels 
T$From 563|g(t) in 2011St21. Other: 0.04 ms {I+700-2} from 563.3|g(t) in 2005Ca02. 
$Experimental isomeric ratio=2.5% {I+8-10} (2011St21) 
$Configuration=|p(h{-11/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
J${+204}Au |b{+-} decay feedings to the 1947.7-keV (J|p=2+) and 2812.8-keV (J|p=3-) levels in {+204}Hg favor J=2,3. The negligible |b{+-} decay branch to the 1128.2-keV (J|p=4+) level suggest J=2. Ground-state J|p of neighboring {+203}Au (3/2+) and {+203}Pt (tentative 1/2-) nuclei support J|p=2-. 
$Configuration=((|p d{-3/2}){+-1}(|n p{-1/2}){+-1}), based on shell model predictions in 1984Cr01 and 1972Pa06. The Nordheim rule (1950No10) favors J|p=2- assignment 
T$From 436.6|g(t), 691.7|g(t), and 723.0|g(t) in 1984Cr01. This value agrees with earlier result of 40 s {I3} from measurement of several intense |g's by 1972Pa06. A value of T{-1/2}=4.0 s 10 and |b{+-} branch with endpoint energy of E(|b{+-})=4500 keV {I300} was reported in 1967Wa23, but this T{-1/2} was not corroborated by 1972Pa06 or 1984Cr01. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_lifetime_unit: US
level_comment:
E$839.0|g and 976.6|g were assigned firmly to {+204}Au in 2008StZY. They follow decay of an isomer with the same lifetime. Thus, the excitation energy of this state is larger than 976.6 keV 
T$From 839|g(t) and 977|g(t) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_lifetime_unit: US
level_comment:
E$Since both the 839.0|g and 976.6|g show the same lifetime, the excitation energy of the isomer is larger than 976.6 keV 
T$From 839|g(t) and 977|g(t) in 2008StZY 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
E$observed activity is assumed to correspond to decay of g.s. 
T$measured by 2014Mo15, from analysis of complex time-correlated structures by Monte Carlo simulations of experimental (ion)|b(|g) and |b(|g)(ion) correlations corresponding to time difference between implanted nuclei and subsequent |b-delayed |g transitions in the first case, and between implantations and preceding |g rays in the second. Ratio of the two correlations is an indicator of of half-life of the isotope being measured. Other: 39.8 s {I9} in {+204}Au Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
J$from {+204}Au Adopted Levels in the ENSDF database (Oct 2009 update) 
T$measured by 2017Ca12 and 2016Ca25 (rounded to 34 s {I15} in latter). paper). Method: (ion)|b correlated decay curve and analyzed by maximum-likelihood method. This value agrees with previous more precise measurements of 37.2 s {I8} (2014Mo15: Phys. Rev. Lett. 113, 022702); and 39.8 s {I9} in {+204}Au Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (16+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$ from decay curve of delayed |g rays (2011St21). 
$Experimental isomeric state population ratio=0.6% {I2} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
J$Systematics in neighboring Au nuclei; shell model predictions 
T$Weighted average of 31 s {I2}, using |b-gated 379|g, 467|g and 946|g(t) spectra, (1994We02) and 32.5 s {I14}, using implant-|b(t) (2014Mo15), and the smallest experimental uncertainty. Other: 34 s {I2} (2009Po01) superseded by 2014Mo15, and 34 s {I15} using implant-|b(t) in 2017Ca12 and 2016Ca25 
CONF$|p(d{-3/2}{+-1}) and spherical shape. 


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$From 2009Po01, based on the observed K- and L-conversion electron lines of 825 keV and 896 keV, respectively. 
%B-$The |b{+-} decay branch is postulated from the observed in 2009Po01 966- and 1015-keV |g rays of the {+205}Hg daughter, depopulating the known 1346-keV (J|p=7/2-) and 1395-keV (J|p=9/2-) levels, that are not directly fed in the |b{+-} decay of the {+205}Au ground state (J|p=(3/2+)) 
J$907|g (M4) to (3/2+); systematics in neighboring Au isotopes; shell model 
T$From 825ce(t) and 896ce(t) in 2009Po01 
CONF$ |p(h{-11/2}{+-1}) and spherical shape. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
J$962.5|g to (13/2-); shell model 
T$From |g(t) in 2009Po14 using all |g rays below the isomer (except the 243.4 keV one) 
CONF$ |p((h{-11/2}{+-2}){-10{++}}(s{-1/2}{+-1})) 


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$From 2009Po01, based on the observed K- and L-conversion electron lines of 825 keV and 896 keV, respectively. 
%B-$The |b{+-} decay branch is postulated from the observed in 2009Po01 967- and 1016-keV |g rays of the {+205}Hg daughter, depopulating the known 1346-keV (J|p=7/2-) and 1395-keV (J|p=9/2-) levels, that are not directly fed in the |b{+-} decay of the {+205}Au ground state (J|p=(3/2+)) 
T$From 825ce(t) and 896ce(t) in 2009Po01 
CONF$ |p(h{-11/2}{+-1}) and spherical shape. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
T$From |g(t) in 2009Po14 using all |g rays below the isomer (except the 243.4 keV one) 
CONF$ |p((h{-11/2}{+-2}){-10{++}}(s{-1/2}{+-1})) 


level_energy_unit: KEV
level_spin_parity: (5+,6+)
level_lifetime_unit: S
level_comment:
E$Early identification in 2009St16, 2008StZY, but no level properties were measured 
%B-$Neutron-rich nuclide with |b{+-} decay being the only expected decay mode 
J$Possible direct |b{+-}-decay feeding to the J|p=5- level in {+206}Hg (2015Mo20). Particle-hole character of the proposed configuration (repulsive for mutual alignment) would be consistent with J|p=5+,6+. The authors of 2015Mo20 proposed a tentative J|p=(4+,5+) assignment. 
T$From sum of |b{+-}-gated 1068|g(t) and 1034|g(t) spectra in 2015Mo20 and the maximum likelihood method. The uncertainty includes both statistical and systematics components, but the individual contributions were not given by the authors. Other: 56 s {I17} from |b{+-}(t) in 2017Ca12. 
CONF$|p(d{-3/2}){+-1}~#|n(g{-9/2}){++1}. The |p(d{-3/2}){+-1} orbital is associated with the ground state of the even-N Au nuclei, while the |n(g{-9/2}){++1} orbital is associated with the ground state of the {+209}Pb and {+211}Po (N=127) isotopes. If J|p=5+, admixtures with the |p(s{-1/2}){+-1}~#|n(g{-9/2}){++1} configuration are possible. The authors of 2015Mo20 proposed a tentative configuration=|p(s{-1/2}){+-1}~#|n(g{-9/2}){++1} 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Only the |b{+-} decay is expected, followed possibly by |b{+-}n decay from theoretical T{-1/2}(|b)=23.4 s, T{-1/2}(|a)>10{+20} s (2019Mo01), thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=23.4 s, %|b{+-n}=3 (2019Mo01) 
$Theoretical T{-1/2}= 
$From A/Z plot (Fig. 1 in 2010Al24), eight events are assigned to {+207}Au 
E$it is assumed that the observed fragments correspond to nuclei in their ground state 
J$|W{-p}=3/2+ (2019Mo01, theory); 3/2+ from systematics (2021Ko07) 
T$lower limit of 300 ns from time-of-flight as given in 2006Ca30 for a similar setup. Actual half-life is expected to be much larger as suggested by the theoretical value of 23.4 s ((2019Mo01) for |b decay; and systematic value of 3 s (2021Ko07). From a decreasing trend of half-lives with increasing neutron number in neutron-rich nuclei, expected T{-1/2}<40 s from known half-lives of 40 s for {+206}Au, 32 s for {+205}Au and 40 s for {+204}Au. 
$Production cross section measured in 2010Al24, values are given in Fig. 2, plot of |s versus mass number for Au isotopes, with statistical uncertainty=10%, and systematic uncertainty=20% 
$Production |s=1.65 nb (from e-mail reply of Oct 29, 2010 from H. Alvarez-Pol) 


level_energy_unit: KEV
level_comment:
$ Production |s=0.748 nb (from e-mail reply of Oct 29, 2010 from H. Alvarez-Pol, which also stated that further analysis was in progress) 
$The |b{+-} and delayed neutron decay are the only decay modes expected 
$Calculated %|b{+-}n=4 (2019Mo01) 
E$ it is assumed that the observed fragments correspond to nuclei in their ground state 
$From A/Z plot (figure 1 in 2010Al24), 15 or 18 events are assigned to {+208}Au 
T$ >300 ns from time-of-flight as given in 2006Ca30 for a similar setup. Actual half-life is expected to be much larger as suggested by the calculated value of 9.5 s (2019Mo01) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$%|b{+-}n=90.8 predicted in 1997Mo25 
J$from systematics in neighboring odd mass Au isotopes (J|p=3/2+ in {+205}Au, {+203}Au, {+201}Au, and {+199}Au); J|p=1/2+ is predicted in 1997Mo25 
T$lower limit estimated from the time-of-flight between the production target and the focal plane in 2006Ca30. The actual lifetime is expected to be much longer. For example, T{-1/2}|?1 s is estimated from systematics of log(T{-1/2}) versus log(Q{-|b}{+5}) data from neighboring {+199}Au, {+201}Au, {+203}Au and {+205}Au isotopes. T{-1/2}|?88 s is predicted in 1997Mo25 
$configuration=|p(d{-3/2}){+-1}. The assignment is tentative 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Production |s=0.131 nb (from e-mail reply of Oct 29, 2010 from H. Alvarez-Pol to B. Singh at McMaster). Also in figure 2 (2010Al24). Statistical uncertainty=10%, systematic uncertainty=20%. 
$The |b{+-} and delayed neutron decay are the only decay modes expected 
$Calculated %|b{+-}n=13 (1997Mo25) 
E$it is assumed that the observed fragments correspond to nuclei in their ground state 
$From A/Z plot (figure 1 in 2010Al24), 3 or 4 events are assigned to {+210}Au 
T$lower limit from time-of-flight as given in 2006Ca30 for a similar setup. Actual half-life is expected to be much larger as suggested by the calculated value of 0.35 s for |b decay and >10{+20} s for |a decay (1997Mo25), and systematic value of 1 s for |b decay (2012Au07) 
J$1/2+ for proton and 11/2+ for neutron configuration predicted (1997Mo25). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$2019Hi06 assigned %|a |? 100, as only the |a decay was observed in this work, as |b decay half-life is expected to be much longer. Theory T{-1/2}(|b decay)=0.118 s, T{-1/2}(|a)=8.9 |ms (2019Mo01). With S(2p)=-1850 {I340} (2021Wa16), 2p-decay mode is likely, but from a search for this decay mode, no evidence was found for this decay mode by 2019Hi06 
$Measured E|a=7590 {I30} from the decay of the g.s. of {+170}Hg (2019Hi06) 
T$measured by 2019Hi06 from observation of one (recoils)|a-|a-|a-|a correlated decay chain ({+170}Hg|){+166}Pt|){+162}Os|){+158}W) and analysis by maximum likelihood method. 


level_energy_unit: KEV
level_lifetime_unit: US
level_comment:
%A |a decay only has been observed (2004Ke06). Gross |b-decay theory (1973Ta30) predicts a partial |b half-life of |? 0.6 s which implies %|e+|b{++}|?0.01%. 
T from 2004Ke06. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: US
level_comment:
%A |a decay only has been observed (2009Sa27,2004Ke06,1999Se14). Gross |b decay theory predicts a partial |b-decay halflife of |?0.7 s (1973Ta30) and microscopic calculations |?0.20 s (1993Hi08), implying %|e+%|b{++}|?0.04% and |?0.13%, respectively. 
J g.s. of even-even nucleus. 
T from recoil-|a(t) (2009Sa27). Others: 0.25 ms {I+35-9} from a(t) (1999Se14) and 0.32 ms {I+32-11} (2004Ke06). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$measured in 2012Od01 from 7208|a(t). Others: 0.59 ms {I+47-18} (2004Ke06), 0.93 ms {I+57-26} (1999Se14) 
$Measured E|a=7208 {i5} (2012Od01), 7192 {I13} (2004Ke06), 7211 {I11} (1999Se14). Other: 2009Sa27 
%A$|a decay only has been observed (1999Se14). Gross |b decay theory predicts partial |b-decay halflife |?0.9 s (1973Ta30), implying %|e+%|b{++}|?0.1%. 
J$Unhindered a decay to (7/2-) {+169}Pt 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$ measured in 2012Od01 from time decay of 7208|a peak and using method maximum likelihood. Others: 0.59 ms {I+47-18} (2004Ke06) 
$ Measured E|a=7208 {I5} (2012Od01) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
J$ favored |a decay to {+171}Pt g.s. with J|p=7/2- (J|p quoted by 2009Od01 in their reference 25: to be published) From proton decay of {+176}Tl, 2004Ke06 proposed 7/2-,9/2- in their study of {+176}Tl proton decay 
T$ weighted average of 10 ms {I1} (2009Od01) and 10.8 ms {I4} (2002Ro17). Others: 7 ms {I+4-2} (2004Ke06), 13 ms {I+6-4} (1997Uu01), 8 ms {I8} (1996Pa01), 20 ms {I+40-13} (1983Sc24). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$ from (recoil)(6913|a)(t) where measured E|a=6913 {I5} from {+175}Hg |a decay (2009Od01) 
J$ from favored |a decay to {+171}Pt g.s. with J|p=7/2- (J|p quoted by 2009Od01 in their reference 25: to be published) 
$ Most likely f{-7/2} state 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T Weighted average of 18 ms {I10} (1996Pa01), 20 ms {I3} (1999To11), 21 ms {I4} (1999Po09), 21 ms {I3} (2001Ju09,1998Mu25) 20 ms {I2} (2002Ro17). Other value: 34 ms {I+18-9} (1983Sc24). 
%|a from 1999Po09. Other value: %|a=96 {I25} (1999To11). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MS
level_comment:
%A$100 {I5} in 2009An20 from comparison of the number of |a{-1}(6990-7100 keV,{+181}Pb) decays and the number of |a{-1}(6990-7100 keV,{+181}Pb)-|a{-2}(6582 keV,{+177}Hg) correlated decays. Other: %|a=85, an estimate from 1979Ha10, but the %|e+|b{++} decay has not been observed 
$E|a=6582 keV {I15} (2009An20), 6580 keV {I5} (2004GoZZ), 6580 keV {I8} (1979Ha10), 6577 keV {I9} (1996Pa01) and 6580 keV (1991Se01). 
J$From hyperfine splitting measurements in 2019Se04; favored |a decay to the J|p=(7/2-) state in {+173}Pt; similarity with the neighboring {+179}Hg isotope. 
T$ Weighted average of 114 ms {I15} (1996Pa01) and 118 ms {I8} (2009An20). Others: 127 ms {I2} (2002Ro17), 170 ms {I50} (1979Ha10), and 130 ms {I5} (1991Se01) 
MOMM1,MOME2$From the laser-induced, resonance-ionization spectroscopy technique in 2019Se04 
$|d<r{+2}>{+198,177}=1.067 {I8} (statistical) {I78} (systematics) in 2019Se04 
CONF$Weakly-deformed |nf{-7/2}/h{-9/2} orbital or spherical |n(f{-7/2}{+-1}) assignment (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J$77.2|g M1 to 7/2- 
CONF$Weakly-deformed state associated with the |nf{-7/2}/h{-9/2} orbital or spherical |n(h{-9/2}{+-1}) assignment (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
J$246|g M2 to 9/2-; systematics of similar isomers in neighboring odd-mass nuclei. 
T$From recoil-246|g(t) in 2003Me20 ({+144}Sm({+36}Ar,3n|g )) 
CONF$Weakly-deformed |ni{-13/2} orbital. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MS
level_comment:
%A$100 {I5} in 2009An20 from comparison of the number of |a{-1}(6990-7100 keV, {+181}Pb) decays and the number of |a{-1}(6990-7100 keV, {+181}Pb)-|a{-2}(6582 keV,{+177}Hg) correlated decays 
$E|a=6582 keV {I15} (2009An20), 6580 keV {I5} (2004GoZZ), 6580 keV {I8} (1979Ha10), 6577 keV {I9} (1996Pa01) and 6580 keV (1991Se01). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
This level decays to the {+174}Pt g.s. by an unhindered |a transition, with E|a=6429 {i3} keV, weighted average of 6425 {i15} keV (1971Ha03), 6425 {i15} keV (1976HoZD), 6430 {i6} keV (1979Ha10), 6428 {i9} keV (1996Pa01), 6429 {i4} keV (2000Ko01), 6429 {i5} keV (2004GoZZ). 
T Average from 0.283 {i23} (2004GoZZ), 0.269 {i3} (2002Ro17), 0.262 {i4} (2000Ko01), 0.287 {i23} (1996Pa01), 0.250 {i25} (1991Se01), 0.26 {i3} (1979Ha10), 0.26 {i3} (1976HoZD). 
J g.s. of even-even nucleus 
%A |?60 to |?80 from systematics, based on b{-|a}|?84% (1971Ha03), and b{-|a}|?50% (1979Ha10). The quoted value is consistent with calculations in 1998Ak04, which yield 70<%|a|<100. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%A$ measured by 2012Ve04 
$ Reduced |a-decay width |d{+2}{-|a}=86 keV {I7} (2012Ve04) 
T$ from Adopted Levels of {+178}Hg in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+178}Hg)=-0.968 fm{+2} {I6}(stat) {I71}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+178}Hg)=49500 MHz {I290} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
%|a: from 1982HeZM. 1971Ha03 estimate %|a|?53, based on extrapolation of |b strength function systematics (which predicts a partial |b half-life of 2.3 s). 
%|ep: 0.15 {I7} from Ip/I|a exp=0.0028 {I4} (1971Ho07) and I|a=55 {I25} (1982HeZM). 
T weighted average of 1.09 s {I4} (1971Ha03), 0.93 s {I11} (1996Pa01), 1.00 s {I5} (2002Ko09) and 1.08 s {I9} (2002Ro17) from 6285|a(t). Other: 1.3 s {I+5-8} (1982HeZM). 
J unhindered |a decay (HF<4) to (7/2-) {+175}Pt g.s. which, in turn, exhibits unhindered |a decay to 77-keV (7/2-) 5/2[523] level in {+171}Os. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: US
level_comment:
J M2 111|g to (9/2-) 61; Q 480|g from (17/2+) 651. Oblate 13/2[606] level (2001Ko13), analogous to 13/2+ states known in heavier odd-A Hg isotopes. 
T from {+183}Pb |a decay (415 ms). 


level_energy_unit: KEV
level_spin_parity: (9/2,11/2-)
level_comment:
J 150|g from (11/2-) 476; possible |g's to (7/2-) g.s. and (9/2-) 61; deexciting gammas expected to feed levels with equal or lower J. J|p=(9/2-) is proposed by 2002Ko09. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5/2-)
level_comment:
E the |g's from this level appear to be associated with decay to (7/2-) g.s., but specific placements have not been established. 
J band assignment. 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J |g from (17/2-) 995 level and (stretched Q)-M1 cascade via 61 level to (7/2-) g.s. imply J|p=(13/2-) and (9/2-), respectively, for 603 and 61 levels. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (13/2+)
level_lifetime_unit: US
level_comment:
E x=171.4 {I4} from Adopted Levels. 
T from Adopted Levels. 
Oblate-deformed 13/2[606] level (2001Ko13). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
%A$ measured by 2012Ve04 from (evaporation residues)-|a-|a correlated events 
$ Reduced |a-decay width |d{+2}{-|a}=62 keV {I5} (2012Ve04) 
$ Hindrance factor for {+179}Hg g.s. to {+175}Pt g.s. decay=1.4 {I2} (2012Ve04) relative 1.0 for {+178}Hg g.s. to {+174}Pt g.s. 
J,T$ from Adopted Levels of {+179}Hg in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$the hyperfine structure spectra in 2019Se04 were consistent with spins of 7/2 or 9/2, but the measured magnetic moment agreed with theoretical value for only the |nf{-7/2} configuration, not with |nh{-9/2}. For |nh{-9/2}, theoretical magnetic moment is positive. 
$Measured |m=-0.948 {I24}, Q=+0.76 {I28} (2019Se04) for ground-state spin of 7/2; magnetic moment corrected for estimated hyperfine anomaly. 
$Measured |m=-0.947 {I27}, Q=+1.45 {I31} (2019Se04) for ground-state spin of 9/2; magnetic moment corrected for estimated hyperfine anomaly. 
$Measured |d<r{+2}>({+198}Hg,{+179}Hg)=-0.905 fm{+2} {I5}(stat) {I70}(syst) (2019Se04) for ground-state spin of 7/2 
$Measured |d<r{+2}>({+198}Hg,{+179}Hg)=-0.915 fm{+2} {I5}(stat) {I70}(syst) (2019Se04) for ground-state spin of 9/2 
$Measured isotope shift |d|n({+198}Hg,{+179}Hg)=46310 MHz {I240} (2019Se04) for ground-state spin of 7/2 
$Measured isotope shift |d|n({+198}Hg,{+179}Hg)=46820 MHz {I230} (2019Se04) for ground-state spin of 9/2 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 2.60 s {I1} (2013KoZR), 2.59 s {I2} (2000Ko48), 2.6 s {I8} (1996Pa01), 2.56 s {I2} (1993Wa03), 2.6 s {I3} (1986Si19), 3.0 s {I3} (1977Hu05), and 2.9 s {I3} (1970Hu18). Other: 5.9 s {I8} (1968De01). 
$%|a: weighted average of 48 {I2} (1999To11), 47 {I5} (1986Si19), and 49 {I5} (1982HeZM). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$large E0 component in 167|g to 2+. 
E$The relative order of the 602|g-797|g cascade is reversed in {+92}Zr({+90}Zr,2n|g) giving a level at 797.2 rather than at 601.6. The evaluator adopts the |e decay ordering since I|g(602|g)>I|g(797|g) in that decay. The I|g data from {+92}Zr({+90}Zr,2n|g) are consistent with this order. 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_comment:
J$|DJ=1, D 765|g to 6+, |DJ=1, D 1091|g to 4+; |p=- is suggested by 2000Ko48 based on decay pattern and theoretical comparisons 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$the relative order of the 602|g-797|g cascade is reversed in {+180}Tl |e decay (1.09 s), giving a level at 602. The evaluator adopts the |e decay ordering since I|g(602|g)>I|g(797|g) in that decay. The {+92}Zr({+90}Zr,2n|g) I|g data are consistent with this order. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$authors give 10 ps<T{-1/2}<14 ps from assumption that unobserved feeding time varies from prompt to that of the 4+ state lifetime 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+180}Hg)=-0.808 fm{+2} {I5}(stat) {I60}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+180}Hg)=41330 MHz {I240} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
MOMM1$NMR of nuclei polarized by optical pumping with beta asymmetry detection (2001StZZ, from 1976Bo09); diamagnetic correction included. 
%A$weighted average of 24 {I3} (2004An07), 36 {I4} (1982HeZM), 23 {I4} (1979Ha10) and 26 {I4} (1975Ho02). Other value: 27 (1971Ho07). 
%ECP from I(p)/I|a=5.0x10{+-4} 8 (1971Ho07), assuming %|a=27 {I2}. 
%ECA based on %|e|a=9x10{+-6} 3 if %|a=26 {I4} (1975Ho02) 
J J from nuclear radiation detected optical pumping (1976Bo09); |p based on systematics of the neighboring odd-A Hg and Pb isotopes. 
$|D<r{+2}>(198-181)=-0.095 {I3} (1986Ul02). 
<r{+2}>{+1/2}=5.437 fm 3 for {+181}Hg based on a global fit to charge radius data for all nuclides (2004An14). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: 13/2+
level_comment:
J$Populated by |a-decay from the 13/2+ state of {+185}Pb with HF=1.7 {I9} 
$Probably the oblate deformed i{-13/2} isomeric state known in A|>185 odd-A Hg isotopes. 
J$populated by |a-decay from the 13/2+ state of {+185}Pb with HF=1.7 {I9} 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (13/2+)
level_lifetime_unit: MS
level_comment:
T$ measured by 2009An17 
$ From a comparison of the total number of {+181}Hg implants and absolute intensity of 90.3|g, 2009An17 conclude that 51% {I9} of the deexcitation path proceeds via 0.48-ms isomer. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+181}Hg)=-0.111 fm{+2} {I6}(stat) {I11}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+181}Hg)=5390 MHz {I280} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$(<r{+2}>){+1/2}(rms charge radius)=5.3833 fm {I52} (2013An02,evaluation) 
$|d<r{+2}>({+198}Hg-{+182}Hg)=-0.6384 fm{+2} 20 (1986Ul02) 
$Based on deduced quadrupole invariants <Q{+2}> and <cos(3|d)>, ground state is weakly deformed with |b|?0.15; consistent with oblate-like deformation (2014Br05, Coulomb excitation) 
T$from 1993Wa03. Others: 11.3 s {I2} (1992Ro21), 11.2 s {I10} (1972Fi12,1971JoZK,1972HuZL), 11.3 s {I5} (1970Ha18,1969Ha03), 9.6 s {I2} (1968De01). Weighted average of all the values is 10.78 s {I18} 
%A$weighted average of 13.3 {I5} (1997Ba21, from correlating |a particles from {+186}Pb decay with subsequent {+182}Hg decays) and 15.2 {I8} (1980Sc09, from a comparison of |a-particle intensities of {+182}Hg and its daughter nucleus {+178}Pt in the same spectrum. Other: %|a=9 {I2} was determined from a comparison of K| x ray and |a-particle intensities (1970Ha18). This method is less precise because the decay scheme of {+182}Hg is not well known, and therefore the contribution of x rays due to internal conversion cannot be accurately calculated. 
T$ 2009Ni11, 2009Wa01: theory for |a decay, half-life 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
$Based on deduced quadrupole invariants <Q{+2}> and <cos(3|d)>, first excited state is prolate deformed (2014Br05, Coulomb excitation) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$others: 28.4 ps {I21} (2009Gr09), 29.7 ps {I18} (deduced from B(E2) values in Coulomb excitation) 
$ Q(transition)=4.1 {I2}, |b{-2}=0.15 {I1} (2010Sc03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluator from B(E2)=0.37 {I+4-3} from g.s. and branching ratios supplied by authors in May 16, 2014 e-mail reply. Using B(E2)=2.9 {I7} for 335,0+ to 548,2+ level gives T{-1/2}=9.0 ps {I+60-37}, consistent with that obtained from B(E2) value for g.s. to 548 level 
$B(E2)(from 0,0+)=0.37 {I+4-3} (2014Br05) 
$B(E2)(from 335,0+)=2.9 {I7} (2014Br05) 
$B(E2)(from 352,2+)=0.97 {I+38-32} (2014Br05) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$others: 24.7 ps {I10} (2009Gr09), 26.1 ps {+9-8} (2014Br05, deduced from B(E2) values in Coul. ex.) 
$Q(transition)=7.4 {I2}, |b{-2}=0.26 {I1} (2010Sc03) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Based on deduced quadrupole invariants <Q{+2}> and <cos(3|d)>, ground state is weakly deformed with |b|?0.15; consistent with oblate-like deformation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
$Based on deduced quadrupole invariants <Q{+2}> and <cos(3|d)>, first excited state is prolate deformed 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluator from E2 matrix element from g.s., assuming 100% branch for 352|g 
$E2 matrix element (0,0+ to 352,2+)=+1.29 {I+4-3} (2014Br05) 
$B(E2)(from 0,0+)=1.66 {I+11-7} 
$E2 matrix element (335,0+ to 352,2+)=-2.68 {I+15-13} (2014Br05) 
$B(E2)(from 335,0+)=7.2 {I+7-8} 
$Diagonal E2 matrix element (352,2+ to 352,2+)=-0.04 {I+130-140} (2014Br05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluator from B(E2)=0.37 {I+4-3} from g.s. and branching ratios supplied by authors in May 16, 2014 e-mail reply. Using B(E2)=2.9 {I7} for 335,0+ to 548,2+ level gives T{-1/2}=9.0 ps {I+60-37}, consistent with that obtained from B(E2) value for g.s. to 548 level 
$E2 matrix element (0,0+ to 548,2+)=-0.61 {I3} (2014Br05) 
$B(E2)(from 0,0+)=0.37 {I+4-3} 
$E2 matrix element (335,0+ to 548,2+)=-1.7 {I2} (2014Br05) 
$B(E2)(from 335,0+)=2.9 {I7} 
$E2 matrix element (352,2+ to 548,2+)=-2.2 {I4} (2014Br05) 
$B(E2)(from 352,2+)=0.97 {I+38-32} 
$Diagonal E2 matrix element (548,2+ to 548,2+)=+0.8 {I+10-6} (2014Br05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluator from E2 matrix element from 352,2+, assuming 100% branch for 261|g 
$E2 matrix element (352,2+ to 613,4+)=+3.71 {I6} (2014Br05) 
$B(E2)(from 352,2+)=2.75 {I9} 
$E2 matrix element (548,2+ to 613,4+)=+3.1 {I3} (2014Br05) 
$B(E2)(from 548,2+)=1.9 {I+4-3} 


level_energy_unit: KEV
level_comment:
E$A 1547.6 level is given in Table 1 but treated as the same level as the 1548.6 level in the decay scheme in Figure 4. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+182}Hg)=-0.653 fm{+2} {I5}(stat) {I48}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+182}Hg)=33350 MHz {I260} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
<r{+2}>{+1/2}(charge)=5.442 fm {I3} (2004An14). 
%A From %I(5904|a)=10.6 {I20} (1970Ha18) and %|a=1.07 {I14} for all other |a branches (1979Ha10); from I|a/I(K| x ray). Evaluator adopts this value in preference to %I(5904|a)=23.2 {I14} (1980Sc09, from parent-daughter I|a comparison) because it leads to a more reasonable hindrance factor for the 5904|a transition (note that 1980Sc09 had to apply a significant correction to the daughter I|a data because the range of the recoils exceeded their implantation depth). 
%ECP From I(p)/I(|a)=2.2x10{+-5} 3 (1971Ho07), assuming %|a=11.7 {I20}. %|ep would rise to 0.00056 {I8} were the %|a=25.5 {I15} datum of 1980Sc09 correct. 
%EC+%B+ 100 - (adopted %|a=11.7 {I20}). 
MOMM1 NMR of nuclei polarized by optical pumping with |b-asymmetry detection. 
T weighted average of 8.8 s {I5} (1970Ha18), 12 s {I2} (1984Ma41) and 10.7 s {I8} (1992BoZO) (the unweighted average is 10.5 s {I9}). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J 3/2-, 5/2- from E2 67|g to 1/2- g.s.; member of g.s. band; it is (assumed that the 67|g seen in {+187}Pb |a decay is the same as that seen in ({+32}S,4n|g) E=159 MeV). 
T based on observation of prompt |a|g coin in {+187}Pb |a decay (15.2 s). 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J suggested configuration=(|n i{-13/2})~#(slightly oblate 0p-2h Hg core) (1999An10). Unhindered |a decay from (13/2+) {+187}Pb. 
T possibly exceeds 8 |ms, based on absence of |a|g coin in {+187}Pb |a decay (18.3 s). 
E from |a decay (18.3 s). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J possible configuration=(|n 2p{-3/2})~#(slightly oblate 0p-2h Hg core) (1999An10); (M1) 276|g to 1/2- g.s.. Consistent with apparently unhindered |a decay from (3/2-) {+187}Pb. 
T based on observation of prompt |a|g coin in {+187}Pb |a decay (15.2 s). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
No |a branch observed to this level. 1981Mi12 estimate an upper limit of 1.5% of all parent |a decays for such a branch; the implied lower limit for its hindrance factor (790 {I240}) is surprisingly high compared with that for the branch to the 67-keV level (13 {I4}) which has been postulated to be a member of the same rotational band. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
Other E: 44 {I19} from Q(|a) and E|a if parent level energy is 33 {I13} and 65 {I19} if E(parent)=2 {I15}. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
T absence of 6077|a-|g coin may indicate that T{-1/2}(266 level) exceeds the 8 |ms coincidence time employed in the experiment of 1981Mi12. 
E from Q(|a)=6393 {I6} (2012Wa38) and E|a=6077 {I7} from {+187}Pb(g.s.). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+183}Hg)=-0.065 fm{+2} {I5}(stat) {I7}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+183}Hg)=3100 MHz {I260} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
%A$From comparison of 6080|a events to 5905|a events (2022Hu09). 
T$From recoil-5905|a(t) (2022Hu09) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 7/2-
level_comment:
E$x |> 16 keV based on the established upper energy limit of 83 keV between 13/2{++} and 9/2{+-} states (2022Hu09) 
E$decay path is either to the ground state or the 3/2{+-}, 67-keV level. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
%A from 1980Sc09 by comparing parent and daughter activities. Other %|a: 1.25 {I20} from 1970Ha18. 
<r{+2}>{+1/2}(charge)=5.395 {I5} (2004An14). 
|D<r{+2}>({+198}Hg,{+184}Hg)=-0.5337 {I13} (1986Ul02). 
J g.s. of even-even nucleus. 
T weighted average of 30.9 s {I3} (1994Wa23), 30.6 s {I3} (1972Fi12), 32.5 s {I10} (1970Ha18) from 5535|a(t), 32.0 s {I10} (1969Ha03). 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J D 213|g to 4+ 1087, so J=3,4,5; both ({+32}S,4n|g) studies propose J=5. However, 765|g to 2+ 534 is the strongest deexcitation branch so evaluator considers J|p=(3,4+) to Be most likely. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J 757|g to 6+ 994; 256|g from J=(8) 2007; 452|g to (3,4+) 1300. Not a member of J=(7) band based on its inconsistent intraband B(M1)/B(E2) ratio. 


level_energy_unit: KEV
level_spin_parity: 18+
level_lifetime_unit: PS
level_comment:
T from DSAM in ({+32}S,4n|g): E=163 MeV (1995Sf01). Other: 0.21 ps {I+6-11} from DSAM in ({+32}S,4n|g): E=156,160 MeV. 


level_energy_unit: KEV
level_spin_parity: 5
level_comment:
J=5 seems unlikely considering that strongest |g branch feeds the 2+ 534 level; adopted J|p=(3,4+). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9
level_lifetime_unit: PS
level_comment:
T$from 329.1|g 
$Q(transition)=5.62 {I19}; revised uncertainty from e-mail reply of Feb 12, 2014 from L. Gaffney based on correct uncertainty of 1.7% in branching ratio of 329.1|g; see also Erratum 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from E2 matrix element from g.s. 
$E2 matrix element (0,0+ to 367,2+)=+1.27 {I3} (2014Br05) 
$B(E2)(from 0,0+)=1.61 {I+8-7} 
$E2 matrix element between 375,0+ and 367,2+=+3.3 {I8} (2014Br05) 
$Diagonal E2 matrix element (367,2+ to 367,2+)=+1.5 {I+18-12} (2014Br05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from B(E2)=0.044 {I+9-8} from g.s. and branching ratios supplied by authors in May 16,2014 e-mail reply. Using B(E2)=1.6 {I7} for 375,0+ to 534,2+ level gives T{-1/2}=43 ps {I+69-27}, consistent with that obtained from B(E2) value for g.s. to 534 level 
$E2 matrix element (0,0+ to 534,2+)=+0.21 {I2} (2014Br05) 
$B(E2)(from 0,0+)=0.044 {I+9-8} 
$E2 matrix element (375,0+ to 534,2+)=+1.25 {I28} (2014Br05) 
$B(E2)(from 375,0+)=1.6 {I7} 
$E2 matrix element (367,2+ to 534,2+)=+0.91 {I14} (2014Br05) 
$B(E2)(from 367,2+)=0.17 {I5} 
$Diagonal E2 matrix element (534,2+ to 534,2+)=-2.6 {I20} (2014Br05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from E2 matrix element from 367,2+, and |g- branching ratios listed here from Author e-mail reply of May 16, 2014 
$E2 matrix element (367,2+ to 653,4+)=+3.15 {I6} (2014Br05) 
$B(E2)(from 367,2+)=1.98 {I+8-7} 
$E2 matrix element (534,2+ to 653,4+)=+5.8 {I5} (2014Br05) 
$B(E2)(from 534,2+)=6.7 {I+12-11} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+184}Hg)=-0.542 fm{+2} {I6}(stat) {I40}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+184}Hg)=27680 MHz {I270} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
T weighted average of 50 s {I2} (1980ToZZ), 48.0 s {I15} (1970Ha18), 50 s {I2} (1970FiZZ), 43 s {I5} (1968De01), and 53 s {I4} (1963Ka17). Other: 1982Bo27, 1960Al20, 1953Ra02. 
J$J from optical pumping with radiation detection (1976Bo09). Experimental |m=+0.508 {I3} suggests a 1/2,1/2[521] Nilsson state assignment. 
%|a=6 {I1} adopted by evaluator from data of 1970Ha18. See {+185}Hg(49 s) |a decay. %|a=5.5 {I7} was given by 1970Ha18. 
MOMM1 Weighted average of +0.509 {I4} (1986Ul02) and +0.507 {I4} (1976Bo09), optical pumping/radiation detection. 
<r{+2}>{+1/2}=5.4406 fm 31 for {+185}Pt based on a global fit to charge radius data for all nuclides (2004An14). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E 1976GrZC looked for Hg K- and L-x rays expected from possible isomeric transitions, but did not observe any. They concluded that the energy of this isomeric level is <15 keV. This upper limit disagrees with 99 keV {I8} (1982Bo27). 
T$weighted average of 28 s {I5}, 30 s {I4} (1982Bo27), 17 s {I5} (1970Ha18), and 21 s {I1} (1970FiZZ). 
J$J from optical quantum-beat spectroscopy (1979Kr11) and agreement between experimental and theoretical |m. 
%IT from 1982Bo27; %|a from 1976GrZC, renormalized to %IT=54. 
MOMM1 Optical pumping with radiation detection (1986Ul02). Other value: -1.07 {I7} optical spectroscopy, LASER fluorescence (1979Da06). 
MOMM1 Isotope shift: 1986Ul02, 1985Kl09, 1979Da06. The large isotope shift measured for {+185}Hg (J|p=13/2+) suggests the Nilsson state 13/2+,13/2[606] with a slightly deformed oblate shape, and the Nilsson state 1/2-,1/2[521] for {+185}Hg (J|p=1/2-) with a strongly deformed prolate shape. 
MOME2 Optical pumping with radiation detection (includes Sternheimer correction) (1986Ul02). Other value: 0.9 {I17} optical spectroscopy laser fluorescence (includes Sternheimer correction) (1979Da06). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Measured |d<r{+2}>({+198}Hg,{+185}Hg)=-0.069 fm{+2} {I6}(stat) {I7}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+185}Hg)=3350 MHz {I300} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$from 2013Sa43 (Eur. Phys. J. A49, 109). Other: 99.3 keV {I5} in {+185}Hg Adopted Levels in the ENSDF database (Nov. 2005 update) 
$J|p, T{-1/2} and decay modes from {+185}Hg Adopted Levels in the ENSDF database 
$Measured |d<r{+2}>({+198}Hg,{+185m}Hg)=-0.543 fm{+2} {I4}(stat) {I40}(syst) (2019Se04) 
$Measured isotope shift |d|n({+198}Hg,{+185m}Hg)=27780 MHz {I190} (2019Se04) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
|D<r{+2}>({+186}Hg-{+198}Hg)=-0.4643 fm{+2} {I10} (1986Ul02). 
T Weighted average of 1.38 min {I13} (1969Ha03), 1.33 min {I10} (1970Fi16), 1.42 min {I10} (1970Ha18). Other: 1.5 min (1960Al20). 
%A From I(K| x ray)/I|a (1970Ha18). Other: 0.018 (1993ToZY, from I|g/I|a). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Others 16~ps {I2} ({+40}Ar,4n|g) (2014Br05), 18~ps {I3} ({+34}S,4n|g) (1974Pr02), 20~ps {I25} {+186}Tl |e decay (1994Jo13). 
J E2 405|g to 0+. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E0+M1+E2 216|g to 2+; Band assignment. 
T$From {+186}Tl |e decay. Other: |J38~ps (Coulomb excitation). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J Stretched E2 403|g to 2+ 405; Band assignment. 
T$From Coulomb excitation. Others: 3.9~ps~{I14} ({+40}Ar,4n|g) and 9~ps~{I3} ({+34}S,4n|g),({+20}Ne,4n|g). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J Stretched E2 357|g to 4+; Band assignment. 
T$Other: 5~ps {I2} ({+34}S,4n|g),({+20}Ne,4n|g) (1974Pr02). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$From {+154}Gd({+36}S,4n), positive parity assigned for the band from several Q crossing transitions (1993Ma02) to the K=0 prolate |b band. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J Stretched E2 424|g to 6+; Band assignment. 
T$Other: |J3~ps ({+34}S,4n|g),({+20}Ne,4n|g) (1974Pr02). 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: US
level_comment:
J$|g to 8+ and (8+) levels, systematics of K isomers in N=106 isotones. 
T$From ({+34}S,4n|g). Other value: 100~|ms~{I10} in ({+28}Si,4n|g). 


level_energy_unit: KEV
level_spin_parity: (23-)
level_comment:
E this band member appears at E=6071.7 in ({+36}S,4n|g) because the 609|g, thought to deexcite it in ({+28}Si,4n|g), is absent in ({+36}S,4n|g), and the 642.6-keV cascade |g above the 609|g was placed from this band member instead. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
J Assumes mult(607)=E1 determined in Tl |e decay; however 607|g is a doublet in (HI,xn|g). (4+) in Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6-)
level_comment:
J $ 7(-) in Adopted Levels. The 607 keV |g-ray de-exciting this state was shown to be D based on DCO ratios (1992Ra34, 2017MaZZ) De-excites to 1578 keV Level. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Based on deduced quadrupole invariant <Q{+2}>, ground state is weakly deformed with |b|?0.15 and consistent with oblate-like deformation. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
$E2 matrix element (0,0+ to 621,2+)=+/-0.05 {I1} (2014Br05), 
$B(E2)(from 0,0+)=0.0025 {I+11-9} 
$E2 matrix element (523,0+ to 621,2+)|>+3.7 {I8} (2014Br05) 
$B(E2)(from 523,0+)|>14 {I6} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$B(E2)|^=2.3~{I3} (From 405,2+) 
T $B(E2), lifetime taken from 402.7 keV transition. 
$E2 matrix element (405,2+ to 809,4+)=+3.4 {I2}. 
$E2 matrix element (621,2+ to 809,4+)=-5.3 {I+13-5}, corresponding B(E2)= 5.6 {I+1.2-2.4}, lifetime=2.7 ps {I+21-5}. 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: MIN
level_comment:
J$spin measured by optical pumping (1971Bo31), parity from comparison of experimental |m with Schmidt limit for configuration |n p{-3/2}. 
MOMM1,MOME2$from 1986Ul02 (radiative detection of optical pumping), Q(|b{+-})Sternheimer shielding corrected. Same values in 1989Ra17 and 2005St24. 
T$from 1970Ha18. In 1970Ha18, half-lives 1.9 min 3 and 2.4 min 3 are measured for 5035|a 20 and 4870|a 20, respectively, in the {+187}Hg |a decay. 5035|a 20 feeding the 3/2- state in {+183}Pt at 84.62 keV from this level. 
%A$Estimated by the evaluator using |a T{-1/2} (calculated) from 1997m025. 1970Ha18 reports %|a>1.2|*10{+-4}, expecting the K X-rays contribution both from the {+187}Hg g.s. and Isomeric state |e decays. 
<r{+2}>{+1/2}({+187}Hg)=5.405 {I4} fm (2004An14) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 13/2(+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$a level energy of 59 keV 16 deduced from mass doublet method in 2003Au02 
MOMM1,MOME2$|m from 1979Da06 (LASER spectroscopy), Q from 1986Ul02 (radiative detection of optical pumping)-Sternheimer shielding corrected. In 1989Ra17 Q=+0.45 {I33}. 
J$spin measured by pulsed laser beam (1979Kr11). Parity from comparison of experimental |m with Schmidt limit for configuration |n i{-13/2}) 
T$from 1970Ha18. Evaluator assumed 4870|a 20 from this level. Please see the T{-1/2} comments at the g.s. level. Other: 3 min (1960Al20) 
%A$Estimated by the evaluator using |a T{-1/2} (calculated) from 1997m025. 1970Ha18 reports %|a>2.5|*10{+-4}, expecting the K X-rays contribution both from the {+187}Hg g.s. and Isomeric state |e decays. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
T$from {+187}Tl |e decay (1983CoZP) 
J$This level gets more low-spin feeding compared to the 167.7 keV level and so J|p=11/2+ for the 167.7 keV level suggests 9/2+ for this level. A B(E2) of ~1.3 W.u. which is very slow for an E2 transition suggests a 9/2+[624] configuration for this level, consistent with the ground-state Nilsson assignments for all the N=107 isotones (2008WoZY). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2+)
level_comment:
J$This level gets less low-spin feeding compared to the 161.5 keV level and so J|p=11/2+ for this level suggests 9/2+ for the 161.5 keV level ({+187}Tl |e decay - 2008WoZY). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J$This level gets more low-spin feeding compared to the 167.7 keV level and so J|p=11/2+ for the 167.7 keV level suggests 9/2+ for this level. A B(E2) of ~1.3 W.u. which is very slow for an E2 transition suggests a 9/2+[624] configuration for this level, consistent with the ground-state Nilsson assignments for all the N=107 isotones (2008WoZY). 
T From 1983CoZP. 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J$This level gets less low-spin feeding compared to the 161.5 keV level and so J|p=11/2+ for this level suggests 9/2+ for the 161.5 keV level (2008WoZY). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
%A$ from 1979Ha10. Other: 4.2|*10{+-5}, preliminary value from 1993ToZY 
T$from 190.2|b|g(t) in 1972Fi12. Others: 3.7 min (1960Po07) and 3.17 min (1978CoYZ) 
$|D<r{+2}>({+188}Hg,{+198}Hg)=-0.3944 fm{+2} {I10} (1986Ul02) and |D<r{+2}>({+188}Hg,{+204}Hg)=-0.80 fm{+2} {I9} (1977Ku11) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$412.9|g E2 to 0+ 
$B(E2,0+ to 2+)|^=1.72 {I26} from E2 matrix element (0,0+ to 413,2+)=+1.31 {I10} (2014Br05). 
T$From B(E2,0+ to 2+)|^ 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$B(E2,2+ to 4+)|^=0.86 {I7} from E2 matrix element (413,2+ to 1005,4+)=+2.07 {I8} (2014Br05) 
T$From B(E2,2+ to 4+)|^ 
J$592.0|g E2 to 2+ 


level_energy_unit: KEV
level_spin_parity: (6+)
level_uncertain: ?
level_comment:
J$280.0|g to 8+ consistent with J from 6 to 10. Non-observation in HI,xn|g data sets would be consistent with non-yrast status and hence lowest spin 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
J$61.6|g to 10+; |m; systematics of similar isomers in the region 
T$Unweighted average of 134 ns {I15} (1983Ha15) and 173 ns {I35} (2004Gl04) 
MOMM1,MOME2$|m is from g=-0.168 {I10} in 1983Se20. Both |m and Q were deduced using the TDPAD technique 
CONF$|n(i{-13/2}){+-2} 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
J$1984Co17 suggest J|p=(4-6)+, based on E1 assignment to 292|g. But the ce data of 1976Bo04 and |g(|q), |g(lin pol) data in (HI,xn|g) support mult=E2 for 292|g, thus giving J|p=7- 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2,0+ to 2+)|^=1.72 {I26} from E2 matrix element (0,0+ to 413,2+)=+1.31 {I10} (2014Br05). Diagonal E2 matrix element (413,2+ to 413,2+)=+1.0 {I+6-4} (2014Br05) 
T$From B(E2,0+ to 2+)|^ 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$B(E2,2+ to 4+)|^=0.86 {I7} from E2 matrix element (413,2+ to 1005,4+)=+2.07 {I8} (2014Br05) 
T$From B(E2,2+ to 4+)|^ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
$RMS charge radius <r{+2}>{+1/2}=5.4100 fm {I40} (2013An02 evaluation) 
%A$from 1963Ka17, determined for both parent and isomer assuming T{-1/2}=9.5 min. E(|a)|?4850 from systematics. Not seen by 1963Ka17. 
MOMM1$optical pumping/rad detection and NMR/rad detection (1986Ul02). 
MOME2$NMR optical pumping/rad detection (1986Ul02). Other values: 1.1 {I4} (1985Kl09, optical pumping/rad detection), 1.15 {I25} (1976Bo09) 
J$spin from optical pumping/rad detection (1976Bo09), parity from comparison of |m with Schmidt limit for configuration=|np{-3/2} 
T$weighted average of 8.0 min {I7} (1976KeZO), 7.5 min {I2} (1975Be17) and 7.7 min {I2} (1970ErZX). Others: 8.5 min {I2} (1966Na01), 9.5 min (1963Ka17), 9.6 min (1961An02), 9 min (1960Po07), 23 min {I2} (1957Ch34), 20 min {I10} (1955Sm42) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 13/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
%A$see comment on ground state 
MOMM1$collinear laser spectroscopy (1979Da06). 
MOME2$NMR/optical pumping/rad detection (1986Ul02) 
E$x=80 {I30} (2001Sc41,2017Au03, mass doublet) 
J$spin from optical quantum beat spectroscopy (1979Da06), parity from comparison of |m with Schmidt limit for configuration=|ni{-13/2}. 
T$weighted average of 8.7 min {I2} (1975Be17), 8.7 min {I2} (1970ErZX), 8.5 min {I3} (1967Na02) and 8.4 min {I5} (1966Fo13). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J AP (29/2,31/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from fitting by 1992Be18 and 1992Be25. The procedure, as described in 1992Be18, involves fitting of the experimental dynamic moments of inertia with rotational frequencies ~h|w. Other: J=31/2 from fitting by 1994Zh40 and 1998Li54. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$%|b{++}<1 (1959Al94) 
$Evaluated rms charge radius=5.4158 fm {I37} (2013An02) 
$Evaluated |d<r{+2}>({+198}Hg,{+190}Hg)=-0.326 fm{+2} {I1} (2013An02) 
$%|a from detection limit of expected peak at 4043 from {+190}Hg |a decay (1993ToZY). Other: <5|*10{+-5} (1963Ka17) 
$|D<r{+2}>({+198}Hg,{+190}Hg)=-0.3188 fm{+2} {I8} (1986Ul02), from collinear LASER spectroscopy 
$|b{-2}=0.142 {I8} (1986Ul02, deduced from |D<r{+2}>) 
$Isotope shift ({+190}Hg,{+204}Hg)=31.8 GHz {I3} (1977Du03), from LASER spectroscopy 
T$from 1964Ja05. Others: 19.8 min {I6} (1961An02), 21 min {I2} (1969Na10), 21 min {I2} (1959Al94), 1960Al20, 1960Po07, 1954Gi04 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$other: 14.6 ps {I62} from |g|g(t) fast-timing technique combined with GCD method, with 625.4|g as the feeder and 416.3|g as the decay transition (2018Es04); a systematic uncertainty of 3 ps is included to account for contamination from the 419.9-keV transition from the yrast 14+ level; reaction used was {+178}Hf({+16}O,4n|g),E({+16}O)=87 MeV. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 2+ 
T$other: <8.3 ps, from |g|g(t) fast-timing technique combined with GCD method, with 731.1|g as the feeder transition and 625.4|g as the decaying transition (2018Es04). Reaction used was {+178}Hf({+16}O,4n|g), E({+16}O)=87 MeV. 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
J$probable member of a band from configuration=(|n i{-13/2}){++2}. The g-factor deduced from this configuration agrees well with the experimental value (see 1980Hj01) 
T$|g(t). Weighted average of 21 ns {I2} (1980Hj01), 24 ns {I3} (1975Li16); 24.5 ns {I15} (1972In02) 
$g=-0.21 {I2} (1980Hj01) 
MOMM1$time differential perturbed angular distribution (1980Hj01) 
MOME2$time differential perturbed angular distribution (1984Dr09) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_comment:
J$|g to (14+). The spin of the lowest level in SD-1 may be 12 or 13, assuming that the linking transitions carry no more than two units of angular momentum, the former is preferred since it is consistent with the feeding of normal-deformed levels. Also the band may be considered as a quasivacuum band in an even-even nucleus, which makes odd spins for inband levels unlikely (2010Wi02) 


level_energy_unit: KEV
level_spin_parity: (28+)
level_comment:
J$|DJ=2 |g to (26+) 
$Possible terminating state with configuration= |ni{-13/2}{+10}~#|nh{-9/2}{+-2}~#|nf{-7/2}{+-2} (1994Be27) 


level_energy_unit: KEV
level_spin_parity: (28+)
level_comment:
$Possible terminating state with configuration= |ni{-13/2}{+10}~#|nh{-9/2}{+-2}~#|nf{-7/2}{+-2} (1994Be27) 
J$|DJ=2 |g to (26+) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_comment:
J$the spin of the lowest known SD band level may be 12 or 13, assuming that the linking transitions carry no more than 2 units of angular momentum, the former is preferred since it is consistent with the feeding of normal-deformed levels. Also the band may be considered as a quasivacuum band in an even-even nucleus, which makes odd spins for inband levels unlikely 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$|g|g(t) fast-timing technique combined with GCD method, with 625.4|g as the feeder and 416.3|g as the decay transition (2018Es04). A systematic uncertainty of 3 ps is included to account for contamination from the 419.9-keV transition from the yrast 14+ level 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$|g|g(t) fast-timing technique combined with GCD method, with 731.1|g as the feeder transition and 625.4|g as the decaying transition (2018Es04). 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: NS
level_comment:
T$|g(t) (1980Hj01). Other: 24.5 ns {I15} (1972In02) 
$g factor=-0.21 {I2} (1980Hj01) (differential perturbed |g(|q)) 


level_energy_unit: KEV
level_spin_parity: (8)-
level_comment:
E$level proposed (evaluators) on the basis of a similar level in in-beam |g ray work, deexciting through only one transition 240.3|g, mult=M1+E2 


level_energy_unit: KEV
level_spin_parity: (4-,5,6+)
level_comment:
$See comment for 2318.4 level. The 240.1|g proposed by 1976Bi09 from this level is assigned to the 2318.4 level, instead. This is because 437.6|g and 1276.7|g are not reported in any of the in-beam |g ray-studies 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: MIN
level_comment:
No |a decay: <5|*10{+-6}% (1963Ka17). 
RMS charge radius: 5.417 fm {i4} (2004An14) 
Isotope shift: |D<r{+2}> =-0.3041 fm{+2} {i15} (1986Ul02, relative to {+198}Hg) 
J J=3/2, from |b-radiation detected optical pumping (1976Bo09). Systematics of g.s. J|p in {+187}Hg, {+189}Hg, and {+193}Hg. Parity from systematics and magnetic moment (Schmidt plot). 
T From 1974Va19 (196.2|g(t), 224.7|g(t) in {+191}Hg |e decay). 
MOMM1$ From 2019StZV,1986Ul02 - Nuclear Magnetic Resonance/Optical pumping. 
MOME2$ From 2016St14,1986Ul02/1979Da06 - |b radiative detection of optical pumping. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: NS
level_comment:
T From 1985Ab03 in {+191}Tl |e decay (conversion-electron (ce)-|g and ce-ce delayed coincidence measurements). 


level_energy_unit: KEV
level_spin_parity: 13/2(+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
Isotope shift: |D<r{+2}> =-0.3037 fm{+2} {i13} (1986Ul02, relative to {+198}Hg) 
No IT decay. |a decay limit: <5|*10{+-6}% (1963Ka17). 
E From precision atomic mass measurements in 2001Sc41. Others: 128 keV {i22} (2021Ko07 - NUBASE). x|?130 keV was expected from extrapolation of estimates for similar states in {+193}Hg and {+195}Hg. Labeled as 0.0+x in the previous evaluation (2007Va21). 
J optical quantum-beat spectroscopy (1979Kr11). Systematics of 13/2+ state in neighboring odd-A mercury isotopes. 
T From 241, 253, 371, 521, 536, 579, and 718|g(t) (1971Be61 - {+191}Hg |e decay (50.8 m)). Others: 57 m {I5} (1954Gi04), 55 m {I10} (1955Sm42). 
MOMM1$ From 2019StZV,1979Da06 - Collinear Laser Spectroscopy 
MOME2$ From 2016St14,1979Da06 - |b-radiative detection of optical pumping. 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: NS
level_comment:
J 166.6|g E2 to (21/2-). 
T From ce(L2)(167|g), ce(K)(535|g), and ce(K)(781|g)(t) measurements (1978Me11 - (|a,7n|g)). 


level_energy_unit: KEV
level_spin_parity: (33/2-)
level_comment:
E$This level was proposed to be populated from 6128 keV level in (HI,xn|g):SD 
J 566.8|g Q to (29/2-). 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_comment:
E$This level was proposed to be populated from 6128 keV level in (HI,xn|g):SD 
J 677.2|g Q to (31/2-). 


level_energy_unit: KEV
level_spin_parity: JAP(31/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$31/2 from linking transitions reported in 2004Si19,1998ReZV,1999SiZZ 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: NS
level_comment:
T from conversion-electron (ce)-|g and ce-ce delayed coincidence measurements in 1985Ab03. Also in 1976BoYC. 


level_energy_unit: KEV
level_spin_parity: 13/2(+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$Level energy held fixed In least-squares adjustment 
E$from Adopted Levels. Labeled as 0.0+x in the previous evaluation (2007Va21) 
T,J from Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J 1988WoZZ suggest (7/2-). This would be inconsistent with the M1+E2 multipolarity for the 430 keV |g to the 3/2(-) g.s. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E from weak coincidences of the deexciting 828.66 keV |g to the 51.58 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 575.7 keV |g to the 377.9 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 687.3 keV |g to the 336.32 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 1147.7 keV |g to the 51.58 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 859.9 keV |g to the 377.9 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 800.1 keV |g to the 563.5 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 1339.2 keV |g to the 51.58 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 1092.9 keV |g to the 377.9 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
from weak coincidences of the deexciting 1160.6 keV |g to the 377.9 keV level (1988WoZZ). Not adopted. 


level_energy_unit: KEV
level_spin_parity: 13/2(+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Adopted Levels. Labeled as 0.0+x in the previous evaluation (2007Va21). 
T from adopted levels. 


level_energy_unit: KEV
level_spin_parity: 25/2(-)
level_lifetime_unit: NS
level_comment:
T from ce(L2)(167|g), ce(K)(535|g), and ce(K)(781|g)(t) measurements populated in the {+192}Pt({+3}He,4n) reaction at 35 MeV (1978Me11). The population of the J|p=33/2+ state in this reaction was negligible. 


level_energy_unit: KEV
level_spin_parity: 33/2+
level_lifetime_unit: NS
level_comment:
T from ce(K)(662|g)(t) measurements populated in the {+192}Pt(|a,5n) reaction at 56 MeV (1978Me11). The J|p=33/2+ state was strongly populated in this reaction. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Adopted Levels. Labeled as 0.0+x in the previous evaluation (2007Va21). 


level_energy_unit: KEV
level_spin_parity: JAP(31/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E from y=5689+x (2004Si19,1999SiZZ), where "x" is the energy of the isomeric 13/2(+) level (see comments in the adopted dataset). Also see comments for 6128 level. 
J 31/2 from linking transitions (2004Si19,1998ReZV,1999SiZZ) to Nd states and supported by particle-number conserving (PNC) method calculations (2005He21). 


level_energy_unit: KEV
level_spin_parity: J+2
level_comment:
E$6000+x from observation (2004Si19,1998ReZV,1999SiZZ) of two linking transitions to normal bands: 2778|g to 3222+x (35/2-), 3350 in the adopted dataset, and 3310|g to 2690.6+x (33/2-), 2818.5 in the adopted dataset. See also comments for the 2778 and 3310 keV |g rays. 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J1AP(21/2)
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$ Band head spin assignment was supported by nuclear softness (NS) analysis in combination of the ratio-R method (2017Da18). 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: J2AP(23/2)
level_comment:
E$Level energy held fixed In least-squares adjustment 
J$ Band head spin 23/2 was supported by nuclear softness (NS) analysis in combination of the ratio-R method (2017Da18), although it was termed and ambiguous in 2017Da18. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
|D<r{+2}>({+192}Hg-{+198}Hg)=-0.2405 {I14} (1986Ul02) 
<r{+2}>{+1/2}(charge)=5.423 {I4} (2004An14). 
%|a<4|*10{+-6} (1963Ka17). Other: 1961Fo06. 
T from 1961Ja10. Other value: 5.7 h {I5} (1952Fi06). 


level_energy_unit: KEV
level_spin_parity: (3,4)
level_comment:
J 1422|g to 2+ 423; J=3,4 favored by I(1421|g, low-J decay):I(1421|g, high-J decay) in {+192}Tl |e decay (1981So09). 


level_energy_unit: KEV
level_spin_parity: (7)-
level_lifetime_unit: NS
level_comment:
J E1 174|g to 6+ 1803; stretched Q 133|g to (5)- 1844. 
T (|a)(ce)(t) in (|a,4n|g), (|a,6n|g) (1978Me11). Other value: 2.5 ns {I10} (1975Li16) in (|a,xn|g). 


level_energy_unit: KEV
level_spin_parity: (10)+
level_lifetime_unit: NS
level_comment:
J E2 60|g to 8+ 2447; D 283|g to (9)- 2224. 
T ce(t), |g|g(t) in (|a,4n|g), (|a,6n|g) (1983Gu05). Other values: 16 ns {I3} (1975Li16), 15.9 ns {I10} (1978Me11) in (|a,xn|g) (superposition of T{-1/2} for 2507 and 2535 levels). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
T ce(t), |g|g(t) in {+192}Pt(|a,4n|g), {+194}Pt(|a,6n|g) (1983Gu05). See also comment on T{-1/2} for 2507 level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+2
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E,J$From the study of quasi-continuum |g-ray spectra, 2000La31 estimate level energy as 5800 {I500} and J=9.7 {I10} using data for {+194}Hg SD-1 band as a reference 
T from RDDS (1994Wi06) in (HI,xn|g):SD. 
Q(transition)>6 (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+4
level_lifetime_unit: PS
level_comment:
T RDDS (1994Wi06). Others: 3.1 ps {I+10-6} (RDDS, 1994Le24); 3.1 ps {I10} (RDDS, 1993De35). From (HI,xn|g):SD. 
Q(transition)=18.3 {I16} (1994Wi06), 19.3 {I+50-25} (1993De35) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+6
level_lifetime_unit: PS
level_comment:
T RDDS (1994Wi06). Others: 2.0 ps {I+8-6} (RDDS, 1994Le24); 2.1 ps {I12} (RDDS, 1993De35). From (HI,xn|g):SD. 
Q(transition)=18.5 {I10} (1994Wi06), 17.5 {I+35-25} (1994Le24), 17 {I+11-3} (1993De35) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+14
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: 0.16 ps {I5} (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=20.7 {I+31-25} (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+16
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Others: 0.13 ps {I3} (1990Mo16), 0.19 {I3} (1998Bu03). From (HI,xn|g):SD. 
Q(transition)=19.3 {I+17-11} (1994Wi06), 19.9 {I+31-25} (1998Bu03). From (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+18
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Others: 0.089 ps {I31} (1990Mo16); 0.13 {I+2-3} (1998Bu03). From (HI,xn|g):SD. 
Q(transition)=19.6 {I+17-11} (1994Wi06), 20.3 {I+31-21} (1998Bu03). From (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+20
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: 0.058 ps {I17} (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=19.6 {I+19-13} (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+22
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: 0.055 ps {I14} (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=17.7 {I12} (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+24
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: 0.042 ps {I17} (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=17.4 {I+24-15} (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+26
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: 0.034 ps {I9} (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=19.3 {I+29-23} (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+28
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: 0.032 ps {I14} (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=16.9 {I+15-20} (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+32
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Other: <0.03 ps (1990Mo16). From (HI,xn|g):SD. 
Q(transition)=18 +|@-6 (1994Wi06) in (HI,xn|g):SD. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T from ce(t), |g|g(t) (unpublished data quoted in 1983Gu05). Other values: 16 ns {I3} (1975Li16), 15.9 ns {I10} (1978Me11) (superposition of T{-1/2} for 2507 and 2535 levels). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+2
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T RDDS (1994Wi06) 
Q(transition)>6 (1994Wi06) 
E,J$From the study of quasi-continuum |g-ray spectra, 2000La31 estimate level energy as 5800 {I500} and J=9.7 {I10} using data for {+194}Hg SD-1 band as a reference 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+4
level_lifetime_unit: PS
level_comment:
T RDDS (1994Wi06). Others: 3.1 ps {I+10-6} (RDDS, 1994Le24); 3.1 ps {I10} (RDDS, 1993De35). 
Q(transition)=18.3 {I16} (1994Wi06), 19.3 {I+50-25} (1993De35). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+6
level_lifetime_unit: PS
level_comment:
T RDDS (1994Wi06). Others: 2.0 ps {I+8-6} (RDDS, 1994Le24); 2.1 ps {I12} (RDDS, 1993De35). 
Q(transition)=18.5 {I10} (1994Wi06), 17.5 {I+35-25} (1994Le24), 17 {I+11-3} (1993De35). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+16
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Others: 0.13 ps {I3} (1990Mo16), 0.132 ps {I21} (1998Bu03). 
Q(transition)=19.3 {I+17-11} (1994Wi06), 19.9 {I+31-25} (1998Bu03). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+18
level_lifetime_unit: PS
level_comment:
T DSAM (1994Wi06). Others: 0.089 ps 31 (1990Mo16); 0.090 ps +14-21 (1998Bu03). 
Q(transition)=19.6 {I+17-11} (1994Wi06), 20.3 {I+31-21} (1998Bu03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$using GCD method applied to 634.8|g as feeder and 422.8|g as decay transition (2018Es04). A systematic uncertainty of 3 ps is included to account for contamination from the 416.2 keV transition which depopulates the yrast 14+ level. 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: H
level_comment:
MOMM1 From optical pumping (1971Mo24,2014StZZ), with diamagnetic correction applied. 
MOME2 From collinear fast-beam laser spectroscopy, corrected for polarization effects (Sternheimer corrections) (1986Ul02,2014StZZ), 
Limit for possible |a decay: <10{+-5}% (1963Ka17), 10{+-17}% (2001Mo07); other estimated value: <1|*10{+-14}% (1997Mo25). 
J spin from optical spectroscopy, optical level crossing (1976Fu06); parity from Schmidt diagram, |m. 
T from 1974ViZS. Other values: 4 h (1958Ma50), 3.5 h {i5} (1965KaZZ), 3 h (1966Ha47). 
RMS charge radius: 5.4239 fm {i35}(2004An14) 
Isotope shift: |D<r{+2}> =-0.234 fm{+2} {i8} (1986Ul02, relative to {+198}Hg) 


level_energy_unit: KEV
level_spin_parity: 13/2(+)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
MOMM1 From 1973Re04, optical pumping, with diamagnetic correction applied. 2014StZZ list as -1.058430 {i3}. Other: -1.0416 {I3} (1971Mo24, optical pumping, no diamagnetic correction). 
MOME2 Re-evaluated value listed in 2014StZZ from 2013StZZ. 1986Ul02 report +0.916 {I97}, collinear fast-beam laser spectroscopy, corrected for polarization effects (Sternheimer corrections). 
J spin from optical spectroscopy (1976Fu06); parity from Schmidt diagram, |m. 
T from {+193}Hg IT decay (11.8 h) (1974ViZS). Other values: 11.1 h {I5} (1970Pl01), 10.0 h {i5} (1952Fi06), 11 h {i1} (1958Br88). 
%IT From {+193}Hg IT decay (11.8 h) 
Isotope shift: |D<r{+2}> =-0.2160 fm{+2} {i24} (1986Ul02, relative to {+198}Hg) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J J|?(19/2-) 
1993Fa07 suggested that the lowest transition in this band is 192 keV, but 1993Jo09 do not seem to confirm this 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J J{-2}|?(27/2-) 
1998Li54 suggest J=25/2 for this level on the basis of the systematics for the bandhead moments of inertia 


level_energy_unit: KEV
level_spin_parity: 13/2(+)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T from resolution of complex decay curves for ce(K) peaks in combined {+193}Hg (3.80 h) and {+193}Hg (11.8 h) sources (1974ViZS). Other values: 10.0 h {i5} (1952Fi06), 11 h {i1} (1958Br88), 11.1 h {i5} (1970Pl01). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$weighted average of 477 y {I32} (1981Ho18, specific activity) and 358 y {I55} (1979Pr15, {+197}Au(p,xn) yields). Original values of 520 y {I32} in 1981Ho18 (using %I(328.5|g)=67) and 367 y {I55} in 1979Pr15 (using %I(328.5|g)=63) were adjusted (by 2015Do01) using adopted %I(328.5|g)=61.4% {I7} in {+194}Pt from {+194}Au |e decay. Note that 2015Do01 list a weighted averaged value of 447 y {I28}. Evaluators cannot reproduce a low uncertainty of 28 y. Others: >15 y and <540 y (1973Or02); 260 y {I40} (1977PrZX), 1.17 y {I14} (1967Cr09), 1.9 y {I3} (1964Be14), |?1.6 y (1958Br88), and 0.4 y (1961Me12, 1958Ma50, 1955Br12) are discrepant. 
$Evaluated rms charge radius <r{+2}>{+1/2}=5.4309 fm {I33} (2013An02) 
$Evaluated |d<r{+2}>({+198}Hg,{+194}Hg)=-0.164 fm{+2} {I1} (2013An02). -0.1607 fm{+2} {I7} from 1986Ul02. Others: 1987WaZO, 1975Hu05, 1966Da07, 1964To05, 1963Kl03, 1963To07. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$427.9|g E2 to 0+. 
T$weighted average of 19 ps {I1} from {+194}Tl |e decay (32.8 min) and 14.6 ps {I28} from ({+12}C,4n|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$636.4|g E2 to 2+; member of g.s. band. 
T$using GCD method applied to 748.9|g and 734.8|g as feeder transitions in ({+12}C,4n|g) (2018Es04). Other: <3 ps from |g|g(t) in {+194}Tl |e decay (32.8 min) (2019Ol05) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$748.8|g |DJ=1, E1 to 4+; spin=5 from |g(|q) in ({+13}C,5n|g) and (|a,xn|g). 
T$from ce-|g(t) in {+194}Tl |e decay (32.8 min) (1970To14). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$96.92|g E2 to 5-; band assignment 
T$weighted average of 3.46 ns {I3} (2019Ol05, |g|g(t) in |e decay (32.8 min)), 4.0 ns {I6} (2001Gu31, recoil-shadow asymmetry method listed in ({+13}C,5n|g)), and 3.75 ns {I11} (1970To14, ce-|g(t) in |e decay (32.8 min)). Other: 4.46 ns {I11} (1974Ca30, ce(K)(t) in {+197}Au(p,4n ce), not corrected for partial feeding from 8.1 ns, 12+ isomer at 2475). Note that reduced |h{+2}=3.6 is somewhat higher than the critical |h{+2}=3.0 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: NS
level_comment:
J$227.88|g E2+M1 to 7-; spin=8 from |g(|q) in ({+13}C,5n|g) and (|a,xn|g); band assignment. 
T$from |g(t) (1977Gu05) in (|a,xn|g). Other: 1.1 ns {I5} (2001Gu31, recoil-shadow method) in ({+13}C,5n|g) 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
J$232.9|g E2 to 7- and spin=9 from |g(|q) in ({+13}C,5n|g) and (|a,xn|g); band assignment 
T$weighted average of 302 ps {I9} (2018Es04, |g|g(t) in ({+13}C,5n|g)) and 291 ps {I50} (1977Gu05, ce(t) in (|a,xn|g)) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: NS
level_comment:
T$weighted average of 2.9 ns {I5} from |g(t) in 1981Kr04 and 4.0 ns {I10} from ce(L2)(52) ce(M)(59.5)(t) in 1985Ko13 in (|a,xn|g). In 1981Kr04, fitting of 233|g(t), 280|g(t), and 565|g(t) in terms of a two half-life pattern gives 2.9 ns for 10+ isomer and 8.1 ns for 12+ isomer. 
$g(average)=-0.24 {I4} (1980Kr21,2014StZZ) in (|a,xn|g), from integral PAD method, using T{-1/2}=12 ns {I1}. The g factor corresponds to both or either of the 12+ and 10+ isomers at 2475 and 2423, respectively. 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
T$from |g(t) in 1981Kr04 in (|a,xn|g). See T{-1/2} comment for 2423.6 level. This value consistent with 7.5 ns {I20} from (ce(L3) of 52|g)(t) (1983Gu05). Others from |g(t): 11.6 ns {I10} (1977Gu05), 10 ns {I2} (1974Pr13), and 11 ns {I2} (1975Li16) in (|a,xn|g), corresponding to both of the 12+ and 10+ levels 
$g(average)=-0.24 {I4} (1980Kr21,2014StZZ) from integral PAD method in (|a,xn|g), using T{-1/2}=12 ns {I1}. The g factor corresponds to both or either of the 12+ and 10+ isomers at 2475 and 2423, respectively. A correction for revised T{-1/2} needs to be considered. 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_comment:
T$from 2001De42 in ({+48}Ca,4n|g). Others: 1.9 ps 7 RDDS for 254.3|g (1997Ku03), deduced Q(intrinsic)=20 {I+5-3} (1997Ku03), 18.1 {I+25-19} (2001De42). 
$|?42% of the decay is through unresolved multi-step statistical decays. 


level_energy_unit: KEV
level_spin_parity: (14+)
level_lifetime_unit: PS
level_comment:
T$from 2001De42. Other: 2.3 ps {I4} from RDDS for 254.3|g (1997Ku03), deduced Q(intrinsic)=20 {I+5-3} (1997Ku03), 17.6 {I+20-15} (2001De42). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: PS
level_comment:
T$from 2001De42. Other: 1.0 ps {I3} from RDDS for 254.3|g (1997Ku03), deduced Q(intrinsic)=20 {I+5-3} (1997Ku03), 15.9 {I+12-10} (2001De42). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
T$from (650|g)(749|g)(t) with 428|g also in gate (2019Ol05). Other: |<0.15 ns (1970To14, (ce)|g(t)) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$unweighted average of 3.46 ns {I3} (2019Ol05) and 3.75 ns {I11} (1970To14). Value of 2019Ol05 is from (255|g)(735|g)(t) with 428|g also in gate; (209|g)(749|g)(t) and (209|g)(111|g)(t) (2019Ol05). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_comment:
T$from 2001De42. Other: 1.9 ps {I7} (RDDS,1997Ku03). Deduced Q(intrinsic)=18.1 {I+25-19} (2001De42), 20 {I+5-3} (1997Ku03). 1997Ku03 quote T{-1/2}=0.77 ps {I26} from another study (reference 15 in 1997Ku03). 
$|?42% of the decay is through unresolved multi-step statistical decays (1997Ha49). 


level_energy_unit: KEV
level_spin_parity: (14+)
level_lifetime_unit: PS
level_comment:
T$from 2001De42. Other: 2.3 ps {I4} (RDDS,1997Ku03). Deduced Q(intrinsic)=17.6 {I+20-15} (2001De42), 16.8 {I+17-13} (1997Ku03). 1997Ku03 quote T{-1/2}=1.46 ps {I30} from another study (reference 15 in 1997Ku03). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: PS
level_comment:
T$from 2001De42. Other: 1.0 ps {I3} (RDDS,1997Ku03). Deduced Q(intrinsic)=15.9 {I+12-10} (2001De42), 18.3 {I+34-22} (1997Ku03). 1997Ku03 quote T{-1/2}=0.78 ps {I14} from another study (reference 15 in 1997Ku03). 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
T$from (280.2|g)(232.9|g)(t) and GCD method (2018Es04). Other measured values in 2018Es04: 284 ps {I28} from slope method, and 270 ps {I14} from convolution method; none of these adopted by the authors as time-correlated background contributions were not taken into account. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$from ce(K)(t) for 749|g in {+197}Au(p,4n ce) (1974Ca30). The authors did not correct for partial feeding from 12+ isomer. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T$from fitting of 233|g(t), 280|g(t), and 565|g(t) in terms of a two half-life pattern giving 2.9 ns for 10+ isomer and 8.1 ns for 12+ isomer (1981Kr04). Others: 4.0 ns {I10} (1985Ko13, ce(L2)(52)(t) and ce(M)(59.5)(t)); 1977Gu05 assign 11.6 ns {I10} half-life from ce(t), and also 1975Li16 assign 11 ns {I2} from |g(t) to this level, which actually belongs to the half-life of the 2476, 12+ level from studies by 1981Kr04 1985Ko13. 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
E,J$from the Adopted Levels. 1975Li16 and 1974Pr13 assign this isomeric state to the 2424, 10+ level, thus missing the 12+ level at 2476 keV 
T$from 1981Kr04. See T{-1/2} comment for 2423.6 level. This value is consistent with 7.5 ns {I20} from ce(L3)(52)(t) (1983Gu05). Others: 11.6 ns {I10} (1977Gu05, ce(t)), 11 ns {I2} (1975Li16, 280|g(t)), 10 ns {I2} (1974Pr13, |g(t)) 
$g factor=-0.24 {I4} (1980Kr21) 
G$integral PAD method. 1980Kr21 used T{-1/2}=12 ns {I1}. The g factor corresponds to both or either of the 12+ and 10+ isomers at 2476 and 2423, respectively. 


level_energy_unit: KEV
level_spin_parity: (17-)
level_comment:
E$this level corresponds to 4498, (19-) in the Adopted Levels. 1975Li16 missed the intermediate (17-) level at 4115 keV 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
J optical double resonance and |m analysis (1978LeZA,1976Fu06) 
T$From 2001Li17 (weighted average of six |g(t) measurements). Others: 9.5 h {I5} (1952Hu54), 11.5 h {I10} (1973Vi09) 
MOMM1 From optical pumping, nuclear magnetic resonance (1973Re04); {+199}Hg standard. Others: +0.541475 {I1} (1978LeZA), +0.542272 {I34} (1978LeZA, calculated with the use of hyperfine-structure ratio relative to {+199}Hg), +0.538 (1976Fu06). For the |m calculation see 1985Kr14. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J |g to 1/2- is E2 and |g from 13/2+ is M4 
T from |g|g(t) measurement in {+195}Hg IT decay (1969Ba42). Other: 0.79 ns {I7} (1961Re12) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
MOMM1 From optical pumping, nuclear magnetic resonance (1973Re04), {+199}Hg standard. Others: -1.044647 {I3} (1978LeZA), -1.05565 {I13} (1978LeZA, calculated with the hyperfine-structure ratio relative to {+199}Hg standard), -1.038 (1976Fu06). 
MOME2 {+201}Hg standard. Other: +1.27 {I11} (1978LeZA), +1.2 (1976Fu06). For the Q calculation see 1985Kr14. 
J optical double resonance and |m analysis (1978LeZA,1976Fu06) 
T from |g(t) measurement (1973Vi09). Others: 43 h {I5} (1961Ju06), 42 h {I3} (1954Br56), 40.0 h {I5} (1953Hu44), and 38.0 h (1951Mo55). 
For the suggested configuration, see 1986AgZZ. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J 373-, 844-, 847- and 1304-keV levels are low-spin members of the i13/2+ band; (3/2+) to 5/2+ to 9/2+ to 13/2+ and (3/2+) to 7/2+ to 9/2+ to 13/2+ are |g-ray cascades of the 456-471-197 and 426-501-197 keV; the energies of the transitions in these levels are close to the analogous cascades in {+197}Hg (1977Ke18,1977ZgZZ); E2 of the 197 and 471-keV |g's are consistent (1978Go15). 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_comment:
J bandhead of the coupled i13/2 band with signature |a=-1/2 in (HI,xn|g). 
For the suggested possible configuration, see 1986AgZZ. 


level_energy_unit: KEV
level_spin_parity: 25/2-
level_lifetime_unit: NS
level_comment:
J |g to 21/2- is E2 and member of the coupled i13/2 band with signature |a=-1/2. 
T from ce(t) measurement in (HI,xn|g) (1978Me11). 


level_energy_unit: KEV
level_spin_parity: 33/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J |g to 29/2+ is stretched E2 and decoupled i13/2+ band member 
T from ce(t) measurement in (HI,xn|g) (1978Me11). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+4
level_comment:
J$ 333.9|g assigned as 33/2 to 29/2 transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J+2
level_comment:
J$ 273.9|g assigned as 27/2 to 23/2 transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J+4
level_comment:
J$ 284.5|g assigned as 29/2 to 25/2 transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: J+2
level_comment:
J$ 341.9|g assigned as 35/2 to 31/2 transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T 0.72 ns {I3} (1969Ba42) (ce(L3) 123|g)(ce(M) 16.2|g)(t) and 0.73 ns {I3} (1969Ba42) (ce(L3) 123|g)(ce(L) 37|g)(t). Other: 0.79 ns {I7} (1961Re12) (ce(L) 123|g)(ce(L) 37|g)(t) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T$from |g(t) measurement (1973Vi09). Others: 43 h {I5} (1961Ju06), 42 h {I3} (1954Br56), 40.0 h {I5} (1953Hu44), and 38.0 h (1951Mo55). 


level_energy_unit: KEV
level_energy_info: ;OFF=V
level_spin_parity: J
level_comment:
It is a complicated decay path, the main intensity flows going into the positive-parity levels (about 70%). Because the decay is highly fragmented it is not possible to link the dipole sequence to the lower-lying states. 
J can not be determined 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J+4
level_comment:
J$ 333.9|g assigned as 33/2 to 29/2 (J+4 to J+2) transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J+2
level_comment:
J$ 273.9|g assigned as 27/2 to 23/2 (J+2 to J) transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J+4
level_comment:
J$ 284.5|g assigned as 29/2 to 25/2 (J+4 to J+2) transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: J+2
level_comment:
J$ 341.9|g assigned as 35/2 to 31/2 (J+2 to J) transition based on Harris expansion of moment of inertia versus angular frequency (1997Ha01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 From g=-0.005 {I40} (DPAD, IPAD. 1984Go06). 
J 426|g E2 to 0+ g.s. 
T weighted average of 13.6 ps {I20} from |b|g(t) (1963De21) and 17.3 ps {I3} deduced from B(E2)=1.12 {I2} (1979Bo02). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J 1451|g E0 to 0+ g.s. 
E identified new level (1986VeZU), also seen in (p,t). |DE from 1985VeZZ. Intruder proton configuration. X(i11)=0.059 {I11}, 5 times larger than the vibrator value (0.017) (1985VeZZ). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J 1644|g E0 to 0+ g.s. 
E identified new level (1986VeZU), also seen in (p,t). |DE from 1985VeZZ. Intruder proton configuration. X(i11)=0.076 {I15}, X(i12)=0.006 {I2} (1985VeZZ). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J 696|g E1 to 4+, no |g to J|p<4, fed by {+196}Tl |e decay from (7+) 
MOMM1 From g=-0.048 {I50} (1984Go06). 
T from ce-|g(t) in 1.41 h {+196}Tl |e decay (1970To14). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J 84|g E2 to 5-, rotational band member. 
T from ce-|g(t) in 1.41 h {+196}Tl |e decay (1970To14). Other: 5.6 ns {I6} from |g|g(t) in (p,2n|g) (1974Ca30). 
B(E2)(|_)=0.2041 {I87} (1970To14). 
MOMM1 From g=-0.030 {I17} (2006Le06). 
MOMM1 Other: -0.28 {I13} (1984Go06),From g=-0.040 {I19} (1984Go06). |g from -0.031 {I28} for DPAD; -0.048 {I23} for IPAD (1984Go06) g factor indicate that the quasiparticle structure of these states is determined mainly by the rotationally aligned i13/2 neutron and a neutron with low J. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J based on directional correlation ratios and proposed band structure (see (|a,6n|g)). 
J rotational band member, 302|g to 5-, 273|g to (6+). 
This level is confirmed by a definite 273|g deexcitation branch to the (6+) level (1983He14). 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: NS
level_comment:
J 80|g E2 to (8+), rotational band member. 
T weighted average of 4.75 ns {I22} from ce time spectra (1985Ko13), and 5.1 ns {I4} from ce time spectra (1981Kr04). 
T average |w|t=0.14 {I6} (1980Kr21). B(E2)=0.236 {I13} (1985Ko13), 0.218 {I20} (1983Gu05), 0.220 {I17}, neglecting 10+ to 9- branch |<15% (1981Kr04). 
MOMM1 From g=-0.19 {I6} (IPAD, 2006Le06). 
MOMM1 Other: -2.6 {I13}, From g=-0.26 {I13} (IPAD, 1980Kr21), recalculated for adopted T{-1/2}. Note: the 2439 {I12}+ level, with T{-1/2}=3.5 ns could be contributing to the precession, the authors' g factor measurement is probably a composite of values of the 10+ 2342 and 12+ 2439 levels. 
CONF As |n(i13/2)-2 aligned quasiparticle state (1981Kr04). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
J 97|g E2 to (10+), rotational band member. 
T weighted average of 3.5 ns {I1} from time spectra (1983Gu05), 3.52 ns {I32} from ce-T{-1/2} (1985Ko13) and 3.49 ns {I30} (1981Kr04). 
T B(E2)=0.254 {I23} (1985Ko13), 0.254 {I15} (1983Gu05), and 0.256 {I22}, neglecting 10+ to 9- branch |<15% (1981Kr04). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
G g=-0.040 {I19} (1984Go06), From -0.031 {I28} for DPAD; -0.048 {I23} for IPAD (1984Go06). Other: -0.030 {I17} for IPAD (2006Le06) 
G g factor indicate that the quasiparticle structure of these states is determined mainly by the rotationally aligned i13/2 neutron and a neutron with low J. 
T from |g(|q,H,t) (1984Go06). 
B(E2)(|_)=0.2041 {I87} (1970To14). 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: NS
level_comment:
G Recalculated for T{-1/2}=4.83 ns {I19} from g=-0.18 {I9} if |t=10.1 ns {I14} (1980Kr21). 
G Other: -0.19 {I6} for IPAD (2006Le06) 
G The authors' g factor measurement is probably a composite of values for the 10+ 2342 and 12+ 2439 levels (evaluators). 
Average |w|t=0.14 {I6} (1980Kr21). 
As |n(i13/2)-2 aligned quasi-particle state (1981Kr04) 
T weighted average of 4.75 ns {I22} from ce time spectra (1985Ko13), and 5.1 ns {I4} from ce time spectra (1981Kr04). Others: 7 ns {I1} from |a|g(t) (1974Pr13). 
T average |w|t=0.14 {I6} (1980Kr21). B(E2)=0.236 {I13} (1985Ko13), 0.218 {I20} (1983Gu05), 0.220 {I17}, neglecting 10+ to 9- branch |<15% (1981Kr04). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
T from ce time spectra (1981Kr04). 
T B(E2)=0.254 {I23} (1985Ko13), 0.254 {I15} (1983Gu05), and 0.256 {I22}, neglecting 10+ to 9- branch |<15% (1981Kr04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E identified new level (1986VeZU), also seen in (p,t). Intruder proton configuration. X(i11)=0.059 {I11}, 5 times larger than the vibrator value (0.017) (1985VeZZ). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E identified new level (1986VeZU), also seen in (p,t). Intruder proton configuration. X(i11)=0.076 {I15}, X(i12)=0.006 {I2} (1985VeZZ). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
T$using GCD method applied to 301.5|g as feeder and 695.5|g as decay transition (2018Es04). Others: 548 ps {I35} using slope method and 540 ps {I21} using convolution method. 


level_energy_unit: KEV
level_spin_parity: 18+
level_comment:
$2019La20 estimate that 1147-keV transition accounts for |?50% of the intensity from the decay of the band below 5351 keV, thus there are likely to be additional decay paths that have not been observed as yet. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
|m=+0.5273744 {I9}({+199}Hg standard,2001StZZ,1989Ra17, \1973Re04) 
MOMM1 Optical pumping, NMR (1973Re04) 
J from optical spectroscopy and |m analysis (1973Re04,1976Fu06,1978LeZA). 
T from 1966El09. Others: 1943Fr01, 1948Hu24, 1952Co01, 1963Ti02, 1967Bu22, 1967Ki11 
Change of mean-square charge radius |D<r{+2}>=-0.0532 (fm){+2} 20 (1986Ul02). 
<|b{-2}{+2}>{+1/2}=+0.106 {I2} (1986Ul02). See also 1986He27. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
|m=+0.855 {I15}({+199}Hg 158 standard,2001StZZ, 1989Ra17,1977Kr11) 
Q=-0.081 {I6} ({+199}Hg 158 standard,2001StZZ, 1989Ra17,1981Kr16,1980Kr12,1980He05), 0.080 {I10} ({+197}Hg 299 standard, 2001StZZ,1989Ra17,1980He05; {+199}Hg standard, 1989Ra17,1973Re04) 
J E2 |g to 1/2-, M4 |g from 13/2+ 
T from 1977Kr11 ((ce)|g(t) in {+197}Hg IT decay (23.8 h)). Others: 8 ns {I1} (1950De06), 7 ns {I1} (1950Mc12), 7.0 ns {I2} (1961Su11), 7.3 ns 2 (1970Ge01). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
|m=-1.0276844 {I26} ({+199}Hg standard,2001StZZ, 1989Ra17,1978LeZA,1973Re04) 
Q=+1.24 {I14} ({+201}Hg standard, 2001StZZ, 1989Ra17,1986Ul02,1978LeZA) 
Change of mean-square charge radius |D<r{+2}>=-0.0427 (fm){+2} 16 (1986Ul02). 
<|b{-2}{+2}>{+1/2}=+0.110 {I2} (1986Ul02). 
J from optical spectroscopy and |m analysis (1973Re04,1976Fu06,1978LeZA). 
T from 1966El09. Other: 23.5 h {I3} (1971KhZV). See also 1943Fr01, 1951Hu17, 1954Br56, 1963Ti02, 1967Bu22, 1967Ki11. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J M1 |g to 5/2-, (E2) |g to 1/2-; relative excitation function in (|a,xn|g) indicates J(307.8)>J(308.5). J=3/2 is not favored. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T 8.07 ns {I16} (1977Kr11) (ce)(|g)(t). Others: 8 ns {I1} (1950De06), 7 ns {I1} (1950Mc12), 7.0 ns {I2} (1961Su11), 7.3 ns {I2} (1970Ge01), 7.0 ns {I2} (1971Ba71), 8.2 ns {I3} (1972Ko25) 
g-factor: +0.342 {I6} (1970Ge01,1977Kr11) recalculated for T{-1/2} dependence. Other: 0.45 {I13} (1972Ko25) 
Q=-0.081 {I6} (1980He05,1980Kr12,1981Kr16) from time-dependent perturbed angular correlation. Other: 0.47 {I6} (1977Vi01). 1980He05, 1980Kr12, and 1981Kr16 discuss discrepancy in Q(5/2-,{+197}Hg) measurements, in addition to deviation from Q(5/2-,{+199}Hg)=+0.95 {I7} 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
|g|g(|q),ce|g(|q),(ce)(ce)(|q): 1950Wa75, 1956Br65, 1956Gi33, 1957Co49, 1961Pe06, 1962Ge10, 1970Ch24, 1972Ba39; A{-2} coef determined 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
Branching: I|g(270|g):I|g(426|g):I|g(444|g):I|g(578|g)=4.0 {I4}:100:4.4 {I4}:34 {I3} (1979Br12), 4.8 {I5}:100:3.8 {I4}:28 {I2} (1973Va26) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
Branching: I|g(278|g):I|g(433|g):I|g(451|g):I|g(585|g)=10.5 {I10}:100:42 {I4}:20 {I2} (1979Br12), 14 {I2}:100:43 {I6}: <35 (1973Va26) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
Branching: I|g(484|g):I|g(640|g):I|g(658|g):I|g(792|g)=14 {I1}:49 {I6}:5.9 {I8}:100 (1979Br12), 17 {I2}:59 {I8}:6.8 {I11}:100 (1973Va26) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
Branching: I|g(397|g):I|g(405|g):I|g(674|g):I|g(831|g):(983|g )=6.8 {I9}:14.4 {I15}:100:3.5 5l86 9 (1979Br12), 11 {I3}:21 {I4}:100:--:82 {I11} (1973Va26) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
Branching: I|g(701|g):I|g(857|g):I|g(1009|g)=50 {I6}:100:19 {I2} (1979Br12), 56 {I7}:100:19 {I3} (1973Va26) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
Branching: I|g(545|g):I|g(645|g):I|g(852|g):I|g(1130|g):I|g(1 285|g):I|g(1438|g)= 16 {I2}:18 {I3}:3.4 {I12}:7.5 {I11}:100:72 {I8} (1979Br12), 18 {I4}:20 {I6}: <14:--:100:71 {I11} (1973Va26) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
Branching: I|g(771|g):I|g(1254|g):I|g(1256|g):I|g(1411|g):I|g (1429|g)= 1.9 {I3}:10 {I2}:7 {I2}:100:19 {I2} (1979Br12), 1.8 {I4}: <18: <18:100:18 {I2} (1973Va26) 


level_energy_unit: KEV
level_spin_parity: 1/2(-),3/2(-)
level_comment:
Branching: I|g(902|g):I|g(1108|g):I|g(1385|g):I|g(1542|g):I|g (1694|g)=30 {I3}:7.3 {I15}:100:17 {I2}:55 {I6} (1979Br12), 20 {I6}:11 {I3}:100:17 {I3}:53 {I8} (1973Va26) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_comment:
T$from 191.2|g(t) (2020Le04); determined from two exponential fit and fixing the T{-1/2} of the isomer to 23.82 h {I4}. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T$from 133.79|g(t) (2020Le04). Other 23.81 h {I6} from 278.65|g(t) (2020Le04). 
%EC$from ratio of total intensities of 130|g and 409|g from |e decay to 164.8|g and 133.8|g from IT decay (2020Le04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+ 
T From B(E2)=0.990 {I12} (adopted in 2001Ra27). 
MOMM1 Transient Field integral perturbed angular correlation(TF) and {+199}Hg standard (1995Br34). Others: +1.0 {I2} (1986Ko02, Perturbed Angular Correlation after Ion Implantation(IMPAC); {+199}Hg standard), +0.70 {I14} (1977Kr11, Recoil Into Gas or Vacuum(RIGV)) 
Q=+0.68 {I12} or +0.84 {I12} (1984Fe08,2011StZZ). 
MOME2 Coulomb Excitation Reorientation(CER). Others: +0.7 {I2} or +0.8 {I2} (1979Bo16, CER), +0.5 {I2} (1979Ha08, Muonic x-ray Hyperfine Structure, Mu-X) 
<r{+2}>{+1/2}=5.447 fm {I3} (2004An14). 
<(|b{-2}){+2}>{+1/2}=0.106 {I2} (1986Ul02). 
|D<r{+2}>=-0.0968 fm{+2} {I3} (1987Za02), relative to {+206}Hg 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
|m=+1.6 {I2} (1995Br34,2011StZZ) 
MOMM1 TF; {+199}Hg standard. 
J J=4 from |g|g(|q) in {+198}Tl |e decay (5.3 h) and |p=+ from E2 |g to 2+ 
T From B(E2)(412-1048)=0.537 {I20} in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J J=5 from |g(|q) in {+198}Pt(|a,4n|g) and {+196}Pt(|a,2n|g); |p=- from E1 |g to 4+. 
T From |gce(t) in {+198}Tl |e decay (1.87 h) (1971Be09). Other: |<100 ps (1970Du10,1970To14). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T From |gce(t) in {+198}Tl |e decay (1.87h) (1970Du10, 1970To14). Others: 7.4 ns {I4} (1971Be09), 6.6 ns {I5} (1971Pa06), and 7.1 ns {I1} (1984Go06). 
MOMM1 IPAD. Other: -0.22 {I11} (TDPAD, IPAD, 1984Go06) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E E(level)=1900 with L=0 could correspond to 1899 and/or 1901 levels 
J J=(2) from |g|g(|q) in {+198}Tl |e decay (5.3 h) and |p=(+) from (M1+E2) |g to 2+. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
MOMM1 IPAD. 
T Weighted average of 1.85 ns {I16} (|a|g(t),1977Gu05) and 1.94 ns {I10} (cece(t),1985Ko13). 


level_energy_unit: KEV
level_spin_parity: 5-
level_uncertain: ?
level_comment:
E Determined by 587.2|g (1971Pa06,1971Be09). Since feeding to 5- is impossible this level is doubt; 587.2|g may be unplaced here (may be from {+198}Tl |e decay (1.87 h)). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T From |gce(t) measurements (1970Du10,1970To14). Others: 7.4 ns {I4} (1971Be09), 6.6 ns {I5} (1971Pa06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T From 1974Bu13 (self-comparison method, sources: {+198}Au). Others: 22 ps {I5} (1953Da23), 22 ps {I2} (1954Me55), and 34 ps {I2} (1963Fr05). 
J |g|g(|q): A{-2}=+0.37 {I6}, A{-4}=+1.07 {I8} (1955Me41) fits 0(E2)2(E2)0 sequence. Cross-section ratio (120|'/160|')=0.37 {I5} (1963Fr05) is compatible with |g|g(|q) (1955Me41) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)=0.990 {I12} (adopted in 2001Ra27) 
g=0.52 {I10} (1986Ko02), 0.368 {I34} (1990Ba40) 
Q: 0.82 {I12} or 0.66 {I12} (1977Es02); 0.80 {I18} or 0.66 {I18} (1979Bo16); 1.13 {I34} (1956Ba45); 0.84 {I12} or 0.68 {I12} (1984Fe08) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B(E2)(412-1048)=0.537 {I20} 
B(E2): From weighted average of 0.533 {I23} (1979Bo16), and 0.553 {I43} (1981Gu07). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)(412-1087)=0.070 {I5} 
B(E2): From average of 0.065 {I7}, 0.079 {I8} (1979Bo16), and 0.062 {I12} (1981Gu07). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$g=0.487 {I7} (1984Ha12). Other g: +0.55 {I11} (1964Ko15,1973Di15,1974Ka18) |g|g(|q,H) external H=57.15 kG; +0.36 to +0.40 (1964Ke02,1973Ra35,1974Do01). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|s(5|')=0.7956 {I798}, |s(17|')=0.0597 {I62}, |s(30|')=0.4052 {I409} 
$|s(5|')/|s(17.5|')=13.32 {I38} 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$from (556|g)(587|g)-coin, centroid-shift method (2021Su02). Authors also obtain 7.2 ns {I7} from (227|g)(587|g)-coin. These values can be compared with 6.9 ns {I2} in {+198}Hg Adopted Levels in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T$2021Su02 measured cumulative half-life of 3.1 ns {I3} for the 2435, 10+ and 2578, 12+ levels from (348|g)(524|g) and (560|g)(767|g), centroid-shift method 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Electric dipole moment (d)<2.1|*10{+-28} e cm (2001Ro05). 
$ <r{+2}>{+1/2}=5.448 fm {I3} (2004An14, evaluation) Others: 1995Ja22, 1993Ja13, 0.7|*10{+-26} {I15} e cm (1987La22,1989La24) 
T$measured (1990Bu28) lower limits for cluster decay: >2.2|*10{+21} y (for {+24}Ne decay mode), >2.5|*10{+21} y (for {+28}Mg decay mode) 
$ Analysis of electric dipole moment: 2004En01, 2004Hi02 
$ Electric Dipole moment (theory): 2002Dz01, 1996Kh08, 1986Fl01 
J$spin from optical spectroscopy (1931Sc03) and NMR (1951Pr02); parity from L(d,t)=1 
Isotope shifts from K| x ray energies (1978Le09); charge parameters (1985Kl09,1983Gu02); charge radius, deformation deduced from isotope shifts (1986Ul02). 
MOMM1$NMR using optically pumped ions (1961Ca21). Others: optical spectroscopy: 0.547 {I2} (1940Mr10), +0.532 (1957Bl10), +0.51 (1961Ag03), +0.454 (1963Sc34), 0.506 {I3} (1967Dr09). Others: 1959Pe33, 1960Mc11, 1961Hi16, 1963St15, 1977Ei02. NMR studies: 1996Su17, 1996Ju04, 1994Su30. Compilation: 2005St24 
$ Analysis of magnetic dipole moment: 1998Gu22, 1994Ga46, 1987Za02 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$E2 |g to 1/2-, L(d,t)=L(p,d)=3 
T$weighted average of 2.47 ns {I5} (1975Ed01), 2.49 ns {I3} (1971Si20), 2.38 ns {I7} (1967Ba27), 2.37 ns {I7} (1966Ra28), 2.42 ns {I15} (1963Li08), 2.32 ns {I8} (1961Gr29,1962Ba37), 2.53 ns {I15} (1961Re12), 2.35 ns {I20} (1952Be26). See datasets: {+199}Au |b{+-} decay, {+199}Hg IT decay and {+199}Tl |e decay 
MOMM1$TDPAC (1977Kr11). Others: +0.91 {I9} (IPAC,1977Kr11), +0.60 {I15} (transient-field technique,1986Ko02), 1961Gr29, 1956Po14. Compilation: 2005St24 
MOME2$Muonic x rays (1979Ha08). Others: 0.70 {I9} (TDPAC, 1973Ha61), +0.85 {I12} (muonic x rays,1983Gu02), +0.8 {I4} (Mossbauer effect,1985La21,1979Wu12). Compilation: 2005St24 
Isomer shift (1985La21,1983Gu02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$M1+E2 |g to 1/2-; L(d,t)=1 
T$from {+199}Au |b{+-} decay. Other: 70 ps {I5} from Coul ex, 60 ps 9 from (|g,|g) 
MOMM1$transient-field technique (1990Ba40). Others: -0.29 {I15} (transient-field,1986Ko02,1989Ra17), -0.47 {I8} (IMPAC,1986Ko02), 1974Do01, 1973Ka17. Compilation: 2005St24 
MOME2$muonic x rays (1983Gu02). other: +0.62 {I15} (1979Ha08). Compilation: 2005St24 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$E2 |g to 1/2-; L(p,d)=(3); |g|g(|q) in Coul ex 
T$from B(E2)|^=0.097 {I16} in Coul ex 
MOMM1$transient-field technique. Other: -0.70 {I25} (1986Ko02,1989Ra17). Compilation: 2005St24 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$M4+E5 |g to 5/2-; L(d,t)=6; |m consistent with configuration=|ni{-13/2} 
T$timing of 374|g and 158|g from isomer produced in (|g,|g') (2001Li17). Others: 42.6 min {I2} (1969Kl06), 39.7 min {I6} (1968Bo28), 43.0 min {I5} (1965Sm02), 42 min {I1} (1955Bo29), 44.4 min {I5} (1948Mo33). Weighted average of all the values is: 42.66 min {I22} 
%IT$%|e<0.1% from log| {Ift} syst 
Isomer shift (1979St04,1985Kl09) 
MOMM1,MOME2$NMR of nuclei polarized by optical pumping with |b asymmetry detection. Other: 1972Co10. Compilation: 2005St24 


