# LEVEL

level_energy_unit: KEV
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$from 1987Gr18, derived from |b|g coin. 
J$high (1982Ke05) 
T$average of: 0.85 s {I2} (1976Ah06), 0.91 s {I2} (1980BaZL), 0.99 s {I7} (1982Ke05), 1.0 s {I1} (1996Me09) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$based on the systematics of rotational {+101,103,105}Nb bands (1991Ho16); band-head of the 5/2+[422] rotational band 
T$weighted average of 2.99~s~{I8} from 94|g(t) in 1984Sh03, 2.9~s~{I1} from 247|g(t) in 1984Sh03 and 2.8~s~{I1} in 1996Me09 
CONF$5/2+[422] 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$from the adopted levels 
T$weighted average of 2.99~s~{I8} from 94|g(t) in 1984Sh03, 2.9~s~{I1} from 247|g(t) in 1984Sh03 and 2.8~s~{I1} in 1996Me09 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
%B-N$from weighted average of 5 {I1} (2009Pe06) and 4.5 {I3} (1996Me09) 
J$proposed configuration=|p3/2[301]~#|n5/2[413] (2014Lu07). Other: 2+ from syst (2012Au07) 
T$from 1983Sh06, from decay curves for 171.6 and 350.7 |g rays emitted by {+106}Nb. Others: 1.240 s {I21} and 1.030 s {I72} (2009Pe06, from ion-|b correlated events, first value from least-squares fit analysis with 0.015 s systematic and 0.015 s statistical uncertainties; second value from maximum likelihood method (MLH) analysis with 0.065 s systematic and 0.030 s statistical uncertainties); 0.90 s {I2} (1996Me09, |b-gated and neutron singles multiscaling curves by fitting the total growth-in and decay periods of the time spectra); |?1 s (1976Ah06, from decay curve for 172|g), 1.08 s {I7} (1969WiZX, from decay curve for 172|g). The value from 1983Sh06 is preferred by the evaluator since the selectivity by characteristic |g rays is better than in other methods where presence of impurities can affect the value. The result in 1996Me09 is the most precisely quoted, but it is in disagreement with values from 2009Pe06. The values obtained by 2009Pe06 by two different analyses are in mutual disagreement, but their value from MLH analysis agrees well with that from 1983Sh06. Weighted average of all the values (using 1.030 s {I72} from 2009Pe06, and increasing the uncertainty to 0.05 s in 1996Me09) is 0.99 s {I4}. If 1.240 s {I21} is used from 2009Pe06, 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Decay mode: only the isomeric transitions have been seen 
T$from |g(t) method. Weighted average of 0.66 |ms {+11-10} (2012Ka36) and 0.84 |ms {I4} (1999Ge01) 
J$proposed configuration=|p1/2[431]~#|n5/2[413] (2014Lu07). But note B(M2)(W.u.) or B(E3)(W.u.) values are much higher than RUL for M2 and E3 transitions 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E,J$it is assumed that the ground state of {+106}Nb is populated in this decay; J|p from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$value of 416 keV {I100} is given in 2012Au07, which seems to assume that the 63.5 and 147.5 |g rays (unplaced here) are in cascade with 204.9 gamma ray, but neither 1999Ge01 nor 2012Ka36 provide information about the placement of the 63.5 and 147.5 gamma rays 
$Number of implanted fragments=1.3|*10{+4} 
T$from |g(t) method. Weighted average of 0.66 |ms {+11-10} (2012Ka36) and 0.84 |ms {I4} (1999Ge01) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (4-)
level_lifetime_unit: S
level_comment:
J,T$From 2020Ha14. Half-life from decay curve for 171.4|g 
$Proposed configuration=|p3/2[301]~#|n5/2[413], with antiparallel-spin coupling (2020Ha14) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$2021Mi07 propose a J|p of greater than or equal to 3 based on |b decay feeding pattern and theoretical considerations. 
T$from |g(t) in 2021Mi07. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$Av: 300 ms {I30} (1996Me09), 300 ms {I10} (1991Hi02). Others: 330 ms {I50} (1991AyZY), 440 ms {I60} (1986ReZS) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n=6 {I2} (1996Me09) 
T$ from 2009Pe06; systematic uncertainty=15 and statistical uncertainty=10 combined in quadrature by compilers 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from 2009Pe06 (Phys. Rev. C79, 035806) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Others: 280 ms {I18} (2009Pe06: Phys. Rev. C79, 035806); 300 ms {I9} in {+107}Nb Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from 2019Ku16, based on weighted average of several |g(t) measurements of transitions following the decay of {+107}Nb. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: MS
level_comment:
%B-N$weighted average of 6.2 {I5} (1996Me09) and 8 {I2} (2009Pe06) 
$Theoretical T{-1/2}=307 ms, %|b{+-}n=16.6, %|b{+-}2n=0.0 (2003Mo09) 
J$from log| {Ift}=5.0 to 3+ and 5.4 to 2+. Possible configuration= |p5/2[422]~#|n1/2[411] (1996Pe25) 
T$weighted average of 195 ms {I6} (2015Lo04, correlated ion-|b decay curves and maximum likelihood analysis technique), 220 ms {I18} (2009Pe06, least-squares fit and maximum likelihood method of time differences of implantations and correlated |b decay events, with systematic uncertainty=10 ms and statistical uncertainty=15 ms), 0.20 s {I3} (1996Pe25, 0.19 s {I2} in 1996Me09 from the same group as 1996Pe25, from |b-gated and neutron singles multiscaling curves by fitting the total growth-in and decay periods of the time spectra). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E,J$it is assumed that the ground state of {+108}Nb is populated in this decay; J|p from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (4-,5)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Number of implanted fragments=2.7|*10{+6} 
J$assigned by 2012Au07 based on decay pattern 
T$from |g(t) method (2012Ka36) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
J,T$From 2020Ha14. Half-life from decay curve for 192.8|g 
$Proposed configuration=|p5/2[422]~#|n1/2[541], with parallel-spin coupling (2020Ha14) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
$Others: %|b{+-}n=31 {I5} (1996Me09) 
T$weighted average of 110 ms 6 from ion-|b|g(t) in 2015Lo04, 100 ms +9-8 from ion-|b(t) in 2011Ni01 and 130 ms 21, from 130 ms {I5}(syst) {I20}(stat) in 2009Pe06 using ion-|b(t). Others: 190 ms 30 in 1996Me09. 
J$from systematics in lighter, odd-A Nb isotopes and the expected configuration. The assignment is tentative 
CONF$likely |p5/2+[422] orbital, as in the lighter, odd-A Nb isotopes. The assignment is tentative. PES calculations in 20111Wa03 predicted J{+|p}=3/2-, |p3/2-[301] with |b{-2}=0.324, |b{-4}=-0.030 and |g=0{+o}. Calculations of 1997Mo25 predicted J{+|p}=5/2-, |p5/2-[303] with |b{-2}=0.355, |b{-4}=-0.067 and |b{-6}=0.007 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$systematics of the lighter, odd-A Nb isotopes indicate that this is most likely the first member of the ground state band. However, the alternative, J{+|p}=5/2-, |p5/2-[303] assignment cannot unambiguously be excluded 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
T$unweighted average of 114 ns +8-7 using 117, 213|g(t) in 2012Ka36 and 150 ns 30 using 117, 196, 213|g(t) in 2011Wa03 in {+9}Be({+238}U,F|g) 
CONF$interpreted as an oblate-shape isomer and associated with the |p7/2[413] orbital in 2011Wa03. The assignment is tentative. |p5/2[303] assignment cannot unambiguously be excluded 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
T$From adopted levels. 110 ms 6 using ion-|b|g(t) in 2015Lo04 and 100 ms +9-8 using ion-|b(t) in 2011Ni01 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
$The number of implanted {+109}Nb ions in the isomeric state was 1.6|*10{+6} (2012Ka36) and 2.3|*10{+5} (2011Wa03) 
T$unweighted average of 114 ns +8-7, using 117, 213|g(t) in 2012Ka36, and 150 ns 30, using 117, 196, 213|g(t) in 2011Wa03. 
CONF$interpreted as an oblate-shape isomer and associated with the |p7/2+[413] Nilsson orbital in 2011Wa03 


level_energy_unit: KEV
level_spin_parity: (5)
level_lifetime_unit: MS
level_comment:
%B-N$ from intensities of neutrons, |b particles and |bn coincidences in 1996Me09 
J$Direct feeding of J|p=4+, 5+ and 6+ levels in {+110}Mo following {+110}Nb |b{+-} decay. Since the decay scheme is incomplete (pandemonium), the proposed assignment is tentative 
T$Weighted average of 86 ms {I6} (from 2011Ni01 using the analysis of the (ion)|b-correlated decay curve) and 79 ms {I5} (from 2011Wa26, weighted average of 81 ms {I6} (214|g(t)) and 75 ms {I9} (a sum of 281, 421, 463, 487 and 494|g(t)). Other: 170 ms {I2}, from both |b-gated and neutron-singles multiscaling curves by fitting the total growth-in and decay periods of time spectra (1996Me09) 
J$Direct feeding of J|p=4+, 5+ and 6+ levels in {+110}Mo following {+110}Nb |b{+-} decay. Since the decay scheme is incomplete (pandemonium), the proposed assignment is tentative 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$ from intensities of neutrons, |b particles and |bn coincidences in 1996Me09 
T$from both |b-gated and neutron-singles multiscaling curves by fitting the total growth-in and decay periods of time spectra (1996Me09) 


level_energy_unit: KEV
level_spin_parity: (5)
level_lifetime_unit: MS
level_comment:
J,%B-N$from Adopted Levels for {+110}Nb in ENSDF database 
$Theoretical T{-1/2}{-1/2}=206.5 ms, %|b{+-}n=19.57, %|b{+-}2n=0.04 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+110}Nb 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 82 ms {I4} (Adopted Levels of {+110}Nb in ENSDF database, value taken from 2011Ni01: Phys. Rev. Lett. 106, 052502; and 2011Wa26: Phys. Lett. B 704, 270). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (6-)
level_lifetime_unit: MS
level_comment:
J,T$From 2020Ha14, half-life from decay curve for 462.6|g+531.5|g+563.3|g+563.4|g 
$Proposed configuration=|p5/2[422]~#|n7/2[523], with parallel-spin coupling (2020Ha14) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
J,T$From 2020Ha14, half-life from decay curve for 213.4|g 
$Proposed configuration=|p5/2[422]~#|n1/2[541], with parallel-spin coupling (2020Ha14) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=151 ms, %|b{+-}n=55.6, %|b{+-}2n=0.0 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+111}Nb 
J$5/2+ from syst (2012Au07); 5/2- from theoretical predictions (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 51 ms {I+6-5} from ion-|b correlations (2011Ni01). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$using maximum-likelihood analysis of HI-|b(t) data in {+238}U({+9}Be,X|g) (2011Ni01). A value of |?75 ms is predicted in 2003Mo09 
%B-N,%B-2N$Calculated %|b{+-}n=61.2 and %|b{+-}2n=1.7 in 2003Mo09 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=74.7 ms, %|b{+-}n=61.2, %|b{+-}2n=1.7 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+112}Nb 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 33 ms {I+9-6} (Adopted Levels of {+112}Nb in ENSDF database; value from 2011Ni01: Phys. Rev. Lett. 106, 052502; same lab as 2015Lo04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=50.5 ms, %|b{+-}n=86.5, %|b{+-}2n=2.1 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+113}Nb 
J$5/2+ from syst (2012Au07); 1/2+ from theoretical predictions (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: US
level_comment:
J$the authors state that the measured small isomeric ratio of 0.17 {I2} indicates a higher spin for this isomer than that of ground state according to the in-flight fission and fragmentation mechanism. 
T$from 135|g(t) 
$Isomeric ratio=0.09 {I2} (2022Wu18) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=21.0 ms, %|b{+-}n=38.3, %|b{+-}2n=12.5 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+114}Nb 
J$0+ in 2012Au07 seems a misprint 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
$Measured |s=11 pb (2010Oh02), systematic uncertainty|?40% 
$Probability of misidentification of {+114}Nb isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=63.3, %|b{+-}2n=0.88 (1997Mo25) 
E$measured half-life is assumed to correspond to the ground state of {+115}Nb 
J$5/2+ from systematics (2012Au07), 7/2+ from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
$Measured |s=3 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+115}Nb isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=12.9 ms, %|b{+-}n=54, %|b{+-}2n=5 (2019Mo01) 
$Theoretical T{-1/2}=21.5 ms, %|b{+-}n=79.6, %|b{+-}2n=2.0 (2016Ma12) 
$A total of two counts were assigned to {+116}Nb, one event with the spectrometer setting on Nb, and one event for setting on Pd. Misidentification of this isotope is not likely since no events were observed for neighboring hydrogen-like peaks (2018Sh11) 
$Production |s=0.05 pb, 30% systematic uncertainty for one event with setting on Nb. 
E$it is assumed that the observed event corresponds to ground-state activity. 
J$1- or 6- from |W{-|p}=7/2+ and |W{-|n}=5/2- orbitals proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 12.9 ms (2019Mo01) and 21.5 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+116}Nb is expected to be <25 ms, based on measured half-lives of 32 ms for {+113}Nb, 17 ms for {+114}Nb, and 23 ms for {+115}Nb, available in literature. 


level_energy_unit: KEV
level_comment:
E$the observed activity is assumed to be in its ground state 
T$>450 ns lower limit for assumed time-of-flight. Actual half-life is expected to be much longer as suggested by theoretical T{-1/2} of 31.7 ms for |b decay (2019Mo01) 
J$5/2+ in theoretical calculations (2019Mo01) 
$Measured production |s=(2 mb {I+5-2})|*10{+-11} (2017Su26), their earlier value 2|*10{+-11} mb (2013Su23 - figure 6) - both from one count assigned to {+81}Mo isotope. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$the observed activity is assumed to be in its ground state 
T$>437 ns from tof (2013Su23). Actual half-life is expected to be much longer as suggested by theoretical T{-1/2} of 66.5 ms for |b decay (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) correlations (2001Ki13). Data analyzed with the maximum likelihood method taking into account three decay generations and applying background subtraction. Only one decay event of {+83}Mo was observed. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$ from |b-correlated {+84}Mo fragments; weighted average of 2.2 s {I2} (2009St04) and 3.7 s {I+10-8} (2007WeZX,2002Fa13,2001Ki13) 
$ Delayed proton decay is possible but none has been studied 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_comment:
$%|ep estimated from measured half-life and predicted half-life for delayed proton decay. 
T$from timing of 540|g in {+84}Zr populated in |ep decay of {+85}Mo (1999Hu05, also 1997Hu15,2005Xu04). Others: 5.6 s (1976HaXI) in delayed proton study, 6.3 s {I+13-10} from |b events correlated with {+85}Mo fragments (2000WeZZ) 
$Note: T1/2: 1976HaXI and 2000WeZZ match; both about double that of 1999Hu05. 
J$1/2- suggested by 1999Hu05 from comparison of measured delayed proton spectrum and statistical calculations, but 1/2+ is also shown in authors' later paper: 2005Xu04. Others: 1/2- (systematics, 2002Ma11), 3/2+ (predicted,1997Mo25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from weighted average of values obtained from decay curves for |g rays, x rays and conversion electrons (2005Ka39). Other: 19.6 s {I11} (1994Sh07) is in good agreement but less precise 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
$From 1997Hu07: Branching ratio percentages for |b-delayed proton decay populating the first 2+, 4+, and 6+ states in {+86}Zr are 11 {i6}, 2 {i1}, and 2 {i1}. 
J from systematics of N=45 isotones. 
T weighted average of 14.6 {I15} (1977Ko05), 15 {I2} (1982De43), 13.3 {I4} (1983Ha06), and 14.5 {I3} and 14.2 {I10} (1991Mi15) all from |g(t) measurements in {+87}Mo decay. 


level_energy_unit: KEV
level_spin_parity: (15/2)
level_comment:
J$proposed as (13/2-) in 1993IdZY The evaluator notes that the presence of the 1123 transition does appear to make this proposal somewhat more likely assuming the proposed (9/2-) assignment for the 847 keV level. Based as that is on preliminary report data, the older adopted J|p is kept 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$from the analysis of the shape of the overlapping peaks in the revolution time spectrum using exponentially modified Gaussian (EMG) function in 2023Xi01. 
J$based on the systematics of the J|p of the observed isomers in the neighboring nuclei in 2023Xi01. The authors of 2023Xi01 states that the isomeric state is a neutron-hole state. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$E2 972|g to 4+, band member 
G$from IMPAD technique (1995We03). Mean g-factor for the 6+ and 8+ yrast states, dominated by the 8+ g-factor. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$E2 586|g to 6+, band member 
G$from IMPAD technique (1995We03). Mean g-factor for the 6+ and 8+ yrast states, dominated by the 8+ g-factor. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
G$from IMPAD technique (1995We03). Mean g-factor for the 6+ and 8+ yrast states, dominated by the 8+ g-factor. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MIN
level_comment:
T$weighted average of 1.98 min {I14} (1985Be12: |g{+|+} timing in coin with {+89}Nb |g transitions), 2.15 min {I20} (1981Ga05: beam chopper system) and 2.2 min {I1} (1983OxZZ: |g timing). Other: a 7.1-min activity assigned to {+89}Mo by 1964Bu12 was not confirmed by 1975Ha11 and gave upper limits of <2 min for decay of 9/2+ isomer and <1 m for decay of 1/2- isomer 
$Configuration=|ng{-9/2}{+-1} + seniority=3 states (1993We04) 
J$3/2+ in 2019Mo01 (theory) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$Configuration=|np{-1/2}{+-1} + seniority=3 states (1993We04) 
T$from 1980Ga16 
%IT$from log| {Ift}>3.6 for the transition to the J|p=(1/2)- state in {+89}Nb %|e+%|b{++} is estimated to be <10. From log| {Ift}>5, based on systematics of values for similar transitions in this mass region %|e+%|b{++}<0.4. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: NS
level_comment:
T$from |g(t) of 168|g, 487|g, 320|g, 1016|g, 1080|g, 1399|g (1995Ka06). Other: |?21 ns (1993We04) 
MOMM1$from g=+0.79 {I4} (TDPAD method, 1995We12). 
$Configuration=40% |pg{-9/2}{+2}(8+)~#|ng{-9/2}{+-1} + 21% |pg{-9/2}{+2}(6+)~#|ng{-9/2}{+-1} + 15% |pg{-9/2}{+2}(8+)~#|ng{-9/2}{+-3}(7/2+) + 1% |ng{-9/2}{+-3} gives theoretical g=+0.79 (1995We12). 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: NS
level_comment:
T$from |g(t) of 168|g, 487|g, 320|g, 1016|g, 1080|g, 1399|g (1995Ka06). Other: |?21 ns (1993We04) 
$Configuration=40%((|pg{-9/2}{+2}){-8+}|ng{-9/2}{+-1})+ 21%((|pg{-9/2}{+2}){-6+}|ng{-9/2}{+-1})+ 15%((|pg{-9/2}{+2}){-8+}(|ng{-9/2}{+-3}){-7/2+})+1%(|ng{-9/2}{+-3}) gives calculated g=+0.79 (1995We12). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$weighted average of 5.67 h {I5} (1966Pe10), 5.60 h {I15} (1965Gr29), 5.32 h {I7} (1969Ol01), and 5.7 h {I2} (1953Di08). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$from L(p,t)=5 
MOMM1$From IMPAD (ion-implantation perturbed angular distribution) (1994We09,2014StZZ). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_comment:
J$systematics of half-lives for J|p=8+ member of g.s. rotational band in {+88}Zr and {+86}Sr. L(p,t)=(6) is in disagreement. 63|g to 6+. 
T$weighted average of 1.14 |ms {I5} (1978Ha52), 1.05 |ms {I10} (1971Is04) and 1.15 |ms {I5} (2017Pa35), 1.14 |ms {I5} (2019Ha26), and 1.17 |ms {I+11-7} (2004Ch35). 
MOMM1$from TDPAD (time-differential perturbed angular distribution) (1978Ha52, 2014StZZ). 
MOME2$from TDPAD (time-differential perturbed angular distribution) (1985Ra09, 2016St14). 


level_energy_unit: KEV
level_comment:
E$possible |e+|b{++} feeding from J|p=8+ suggests that this level is different from the 3148 level. 


level_energy_unit: KEV
level_comment:
J$feeding from 8+ parent in {+90}Tc |e decay would suggest J=7,8,9. However, 1291.4|g to 4+ and 482.3|g to 6+ suggests J=4+,5,6+. 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
MOMM1$from g-factor=0.50 {I6}, by IMPAD (ion-implantation perturbed angular distribution) (1994We09,2014StZZ). 
J$E2 476.95|g to 10+ 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
MOMM1$from g-factor=0.42 {I13}, by IMPAD (ion-implantation perturbed angular distribution) (1994We09,2014StZZ). 
T$other: < 0.7 ps from ({+28}Si,2p2n|g) 
J$E2 544.2|g to 9- 


level_energy_unit: KEV
level_spin_parity: (13+)
level_lifetime_unit: PS
level_comment:
J$D+Q 821.4|g to 12+ 
T$weighted average of 1.0 ps {I3} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 1.94 ps {I13} from {+59}Co({+35}Cl,2p2n|g) 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T$from {+59}Co({+35}Cl,2p2n|g), uncertainty increased by evaluators. Others: 2.7 ps {I1} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 4.8 ps {I14} from ({+28}Si,2p2n|g) 
J$E2 1069.1|g to 12+ 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
J$M1+E2 526.5|g to 13+ 
T$weighted average of 1.7 ps {I4} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 1.39 ps {I28} from {+59}Co({+35}Cl,2p2n|g) 


level_energy_unit: KEV
level_spin_parity: 15+
level_lifetime_unit: PS
level_comment:
T$from {+59}Co({+35}Cl,2p2n|g). Others: <0.3 ps from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and <1.4 ps in ({+28}Si,2p2n|g) 
J$M1+E2 244.5|g to 14+ 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_comment:
J$M1+E2 598.0|g to 15+ 
T$weighted average of 3.6 ps {I7} from {+58}Ni({+36}Ar,4p|g),({+35}Cl,3p|g) and 1.91 ps {I14} from {+59}Co({+35}Cl,2p2n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: US
level_comment:
E$isomeric ratio R=61% {I3} (2017Pa35) 
T$from implant-|g(t) in 2017Pa35, but the gating |g-ray transitions were not specified by the authors. Also 1.14 |ms {I5} from implant-|g(t) in 2019Ha26. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
MOMM1 from hyperfine structure in laser spectroscopy (2011StZZ from 2009Ch09). 
|D<r{+2}>({+91}Mo,{+92}Mo)=+0.021 fm{+2} 1 (2009Ch09); uncertainty is statistical only. 
Isotope shift({+91}Mo,{+92}Mo)=-171 MHz 5 (2009Ch09); total uncertainty is given; statistical uncertainty is 2. 
J J(pol p,d)=9/2; L(pol p,d)=4 
T from 1965Eb01. Other measurements: 16.6 min {I8} (1976De37), 15.6 min {I4} (1976Bo19), 15.7 min {I2} (1965Cr10), 15.2 min {I3} (1961Ra06), 15.7 min {I3} (1955Ax02), 15.5 min {I2} (1953Ka11), 15.5 min {I5} (1949Du10). 
WEIGHTED AVERAGE OF ALL "other" T DATA: 15.57 M 11. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%|e+%|b{++}, %IT: from {+91}Mo |e decay (64.6 s). 
J J(pol p,d)=1/2; L(pol p,d)=1 
T weighted average of 63.5 s {I10} (1990KaZW), 65.1 s {I12} (1976De37), 68 s {I2} (1965Cr10), 64 s {I1} (1957Pr44), 66 s {I3} (1955Ax02), 65.5 s {I20} (1953Ka11). 


level_energy_unit: KEV
level_spin_parity: 21/2(+)
level_lifetime_unit: NS
level_comment:
MOMM1 From time-differential perturbed angular distribution. Unweighted average of +8.81 {I8} (1983Ra08) and +8.97 {I9} (1978Ha52) (the data listed in 2011StZZ and 1989Ra17). 
J stretched E2 200|g to 17/2(+) 2068; measured g factor consistent (via additivity rule) with the configuration (|n g{-9/2}){+-1}~#((|p g{-9/2}){+2}(6+ or 8+)) coupled to give a J|p=21/2+ state (1983Ra08). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
MOMM1 From time-differential perturbed angular distribution (2011StZZ and 1989Ra17, from 1983Ra08). Relative to {+90}Mo 2875 level. 
J 212|g to 17/2(+) 2068 in (|a,3n|g); measured g factor supports (via additivity rule) the configuration ((|n g{-9/2}){+-1}~#({+92}Mo, 5- level))17/2- (1983Ra08). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J L(pol p,d)=(3), J=(7/2) for 3591 level; supported by L({+3}He,d). L(p,d)=(4) is probably erroneous due to incomplete |s(|q). 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
J D(+Q) 870|g to (23/2+) 2940, (M1) 264|g to (25/2+) 3545 in; ({+31}P,n2p|g); absence of |g to J<23/2. 
T from RDM in ({+28}Si,2pn|g). Other: >20 ps from (|a,3n|g). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$L=(3 and 4), J=(7/2 and 9/2) in (pol p,d) for 4151-keV doublet which may include L=3 {I4133} level. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J L(n)=4, J=9/2 for 4283 level in (pol p,d). L(p,d)=3 assigned by 1976Ka08, but |s(|q) does not appear to rule out L=4. 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
J |DJ=1 d+Q 532|g to (25/2+) 3811 in ({+28}Si,2pn|g). 
Other T{-1/2}: <1.4 ps from RDM in ({+28}Si,2pn|g). 


level_energy_unit: KEV
level_spin_parity: (5/2-&7/2-)
level_comment:
J L(n)=(3&3), J=(5/2&7/2) for 4383 doublet in (pol p,d). It is unclear whether this doublet is comprised of two levels near 4385 or of the 4408+4385 levels. 


level_energy_unit: KEV
level_comment:
J L({+3}He,|a)=3 for a 4500 {I20} level; this may correspond to the 4481 and/or 4522 levels adopted here. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_uncertain: ?
level_comment:
J,E J(pol p,d)=7/2, L(n)=3. However, it is possible that the 4796 peak in (pol p,d) corresponds to the 4780 or 4780+4815 levels in (p,d). 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
J |DJ=1 d(+Q) 617|g to (27/2+) 4342 in ({+28}Si,2pn|g) 
Other T{-1/2}: <1.4 ps from RDM in ({+28}Si,2pn|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J J=7/2, L(n)=3 from (pol p,d). 
E may be the same level as that seen in ({+3}He,|a) at 5230 {I20}. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
J L(n)=1 for 5900 {I20} doublet in ({+3}He,|a), but L(n)=3, J=7/2 in (pol p,d) for 5930 line which presumably may also be a doublet. 


level_energy_unit: KEV
level_spin_parity: (37/2+)
level_comment:
J (E2) 1810|g to (37/2+) 6469 in ({+31}P,n2p|g); J=37/2 supported by shell-model calculations (2004Ra12). 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
G Weighted average of +0.839 {I8} (1983Ra08) and +0.854 {I9} (1978Ha52), both from time-differential perturbed angular distribution. 
T from time-differential perturbed angular distribution (1978Ha52). Other: 40 ns {I4} from |a-|g(t) (1973Ni04). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
G From time-differential perturbed angular distribution in {+77}Se({+16}O,3n|g) (1983Ra08). 
T from |a-|g(t) (1973Ni04). 


level_energy_unit: KEV
level_comment:
L differs from adopted value (L=4). L({+3}He,|a)=1 for 3330 {I20} level, but it is unclear to which level(s) in (p,d) this corresponds. 


level_energy_unit: KEV
level_comment:
L differs from adopted value and from ({+3}He,|a) (viz., L=3, 1982Ma07) and (p,d) (viz., L=1, 1973Ko03). 


level_energy_unit: KEV
level_comment:
L shown as tentative because L=3 not conclusively ruled out for 4790 {I20} level in ({+3}He,|a); also, that peak is close to a contaminant peak. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
MOMM1 from hyperfine structure in laser spectroscopy. 
$|D<r{+2}>({+91}Mo,{+92}Mo)=+0.021 fm{+2} {i1} (2009Ch09); uncertainty is statistical only. 
Isotope shift({+91}Mo,{+92}Mo)=-171 MHz {i5} (2009Ch09). Total uncertainty is given here; statistical uncertainty is 2. 
J,T from Adopted Levels, Gammas. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T For (0|n+2|n) double |b decay, 1997Ba35 report (at 90% confidence level) lower limits of 1.9|*10{+20} y, 8.9|*10{+20} y and 8.1|*10{+20} y, respectively, for |b{++}|e(to Zr g.s.), |e|e(to Zr 449 level) and |e|e(Zr 935 level); these data supersede earlier data from the same research group (1995Au09). For neutrinoless double |b decay of {+92}Mo, 2011Le23 report a lower limit of 2.3|*10{+20} y at 90% confidence level. Other lower limits on T{-1/2}: 3|*10{+17} y, from nonobservation of |b{++},|e(2|n) double |b decay (1985No03); 2.7|*10{+18} y for |b{++},|e(0|n) (1987El13); 3|*10{+18} y for double-|e decay (1982Be20). 
<r{+2}>{+1/2}(charge)=4.3156 fm {I11} (2004An14). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 From g=+1.15 {I14}, weighted average of +1.3 {I5} (2001Ma17, transient field) from Coulomb excitation and +1.14 {I14} from reevaluation by 2001Ma17 of g=1.07 {I19} (TDPAD) from 1978HaYJ. The g-factor is consistent with that expected for a g{-9/2}{+2} configuration. 
J E2 1509|g to 0+ g.s. 
T weighted average of 0.344 ps {I20} from Coulomb excitation, 0.331 ps {I15} from (e,e') and 0.404 ps {I25} (1977Me01) in (|g,|g') is 0.348 ps {I19}. Others: 0.36 ps {I+8-5} (p,p'|g), 0.30 ps {I+15-10} (|a,|a'|g). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
MOME2 differential perturbed angular distribution (1989Ra17 from 1985Ra09). Sign of Q from 1991Ha04 (TDPAD) in {+59}Co({+37}Cl,2p2n|g)). 
MOMM1 from (|a,2n|g); TDPAD (1977Ha49). Other: +11.35 {I8} (1989Ra17, recalculation of datum from 1977Ku22, TDPAD). |m calculation: 1998Jo17. 
J E8 excitation in (e,e'). 
T weighted average of 192 ns {I7} ({+92}Tc decay), 206 ns {I11} and 191 ns {I7} and 219 ns {I22} in (|a,2n|g), and 184 ns {I5} and 195 ns {I13} from (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J L=3 in (p,p'), (|a,|a'), (p,t), ({+14}C,{+14}C'). 
T weighted average from (|a,|a'|g), (p,p'|g). 
For summary of B(E3)|^ data, see 1989Sp01; recommended value is 0.070 {I24} based on b{-3} from angular distribution in (p,p'). This corresponds to 5.3% {I18} of energy-weighted E3 sum rule. 


level_energy_unit: KEV
level_spin_parity: (4,5)-
level_comment:
J D+Q 480|g to 5- 2527; weak 157|g to 3- 2850; level population in (n,n'|g) rules out J=6 and favors J=4 (2010Go15). L=5 in (p,p') but level only weakly excited. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J D+Q 537|g to 5- 2527; 214|g to 3- 2850; |d(537|g)=14 {I3} makes |p=+ unlikely; 1123|g from (6+) 4187. However, B(M2)(W.u.) for 306|g from 4+ 3369 exceeds RUL, unless T{-1/2}(3369) exceeds ~80 ns (which seems far too large to have remained unobserved); alternatively, the 305|g may be complex in (n,n'|g) making |d unreliable (see comment on 305|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T unweighted average of 22 fs {I12} (1971Yo02), 35 fs {I3} (1973DoZB in (p,p'|g)), 30.3 fs {I21} from B(E2) (1987MiZL in (e,e')), 27 fs {I3} (1977Me01 in (|g,|g')), and 21 fs {I6} (1975Pa19 in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J E4 excitation of 3369 level in (e,e'). Also: Q 1859|g to 2+ 1510, D+Q 362|g to (4,5)- 3007 and D+Q 1086|g to 4+ 2283. However, |d(362|g) and |d(305|g) are too large for |D|p=yes transitions, unless the 3369 level has a significantly long half-life. 
T from (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J L=2 in (p,t), (p,p'); E2 3542|g to 0+ g.s. 
T from B(E2)=0.0020 {I6} in (e,e') and adopted branching. Others: 90 fs {I+40-30} (1973DoZB), 61 fs {I+24-17} (1975Pa19) in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T weighted average of 10.7 fs {I22} from (|g,|g') and 10.5 fs {I13} from B(E2)=0.0188 {I20} in (e,e'), with uncertainty (1.1 fs) increased to that for most precise measurement. Others: 17 fs {I+17-10} (1973DoZB), 20 fs {I+20-12} (1975Pa19). 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
T from (|g,|g'); value rises to 9.7 fs {I14} if only the 3945|g deexcites this level. Others: 10 fs {I+10-3} (1973DoZB), 21 fs {I+20-12} (1975Pa19) in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 4(+),5(-)
level_comment:
J D+Q 1623|g to 5- 2527; D(+Q) 1868|g to 4+ 2283; 1301|g to 3- 2850. L(p,p')=4+5 for E=4159 {I7}; probably this is L=4 component. 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
J D+Q 2147|g to 4+ 2283; D(+Q) 1579|g to 3- 2850; 2920|g to 2+ 1510; |g(|q) in (n,n'|g) rules out J=4 (2010Go15). 


level_energy_unit: KEV
level_spin_parity: 3(-),4(+),5
level_comment:
J D+Q 2195|g to 4+ 2283 allows J=3,5, but makes J|p=4- unlikely; 1951|g to 5- 2527; absence of level in (e,e') possibly suggests an unnatural parity state, thereby favoring J|p=5+. 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: NS
level_comment:
J E2 235|g to 9- 4251. 
T weighted average of 8.7 ns {I2} (1971Le19), 9.2 ns {I5} (1977Ha49), 8.2 ns {I8} (from (|a,2n|g), ({+32}S,2n2p|g) and ({+16}O,6n|g), respectively). 
MOMM1$differential perturbed angular distribution (1989Ra17 from 1977Ha49), if J=11, from ({+32}S,2n2p|g). Other: +14.17 {I13} (1989Ra17, revision of datum from 1977Ku22), TDPAD. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: FS
level_comment:
T from (|g,|g'), assuming only 2 gammas deexcite level. However, see comment on 3125|g from this level. 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J 3440|g to 2+ 1510; 2666|g to 4+ 2283; 1941|g to (4,5)- 3007; level population is not consistent with 2+. 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: MEV
level_comment:
J D 7950|g to 0+ g.s.; M1 resonance from (p,p'); possible conf=(|n g{-7/2})(|n g{-9/2}){+-1} (1982Dj04). 
T |G from (p,p'). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: MEV
level_comment:
J M1 resonance in (p,p'); possible conf=(|n g{-7/2})(|n g{-9/2}){+-1} (1982Dj04). 
T |G from (p,p'). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
MOMM1 g-factor=1.413 {I6} (1977Ha49,1978Ha52) from TDPAD. Others: +1.419 {I10} (1977Ku22, TDPAD), 1.409 {I16} (1971Na16), 1.40 {I7} (1971Co08). 
MOME2 Q({+94}Mo, 8+)/Q({+92}Mo, 8+)=1.48 {I12} (1974Ba11, TDPAD). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{+2}\{-|g0}/|G (eV)=0.0114 {I21} 
|G{+2}{-|g0}/|G: unweighted average of 0.0093 {I6} (1977Me01) and 0.0134 {I15} from I{-s}=27 eVb 3 (2006Ru06). Other: 0.017 {I6} (2000DeZY, if J=2). 
T assuming |G{-|g0}/|G=0.822 {I14} from Adopted Gammas. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{+2}\{-|g0}/|G (eV)=0.018 {I3} 
|G{+2}{-|g0}/|G: weighted average of 0.018 {I3} (1977Me01), 0.019 {I6} (2000DeZY, if J=2) and 0.0176 {I32} from I{-s}=22 eVb 4 (2006Ru06). |G{-|g0}=0.028 {I10} eV (2000DeZY). 
T assuming |G{-|g0}/|G=0.65 {I4} from Adopted Gammas. 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{+2}\{-|g0}/|G (eV)=0.043 {I6} 
|G{+2}{-|g0}/|G: unweighted average of 0.040 {I6} (1977Me01), 0.054 {I6} (2000DeZY) and 0.036 {I4} from I{-s}=27 eVb 3 (2006Ru06). 
|G{-|g0}=0.060 {I20} from self absorption (1977Me01). 
T if %I|g(3944)=78 {I28}; T{-1/2}=9.7 fs {I14} if only the 3944|g deexcites this level. 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
$|G{+2}\{-|g0}/|G (eV)=0.0086 {I15} 
J Q transition to 0+ g.s. 
|G{+2}{-|g0}/|G: from I{-s}=8.2 eVb 14 (2006Ru06). 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: FS
level_comment:
$|G{+2}\{-|g0}/|G (eV)=0.086 {I8} 
|G{+2}{-|g0}/|G: unweighted average of 0.086 {I13} (1977Me01), 0.101 {I5} (2000DeZY), and 0.080 {I6} (from I{s}=43 eVb 3, 2006Ru06). 
|G{-|g0}=0.112 {I8} eV (2000DeZY). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
E from Adopted Levels. Adopted J|p=8+. 
T from time distribution of 1509|g measured using a pulsed-beam technique. Weighted average of 184 ns {I5} (1972Ad01) and 195 ns {I13} (1979Ha60). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J J=3,4,5 from 537|g(|q), but |d unreasonably large if J|p=5+ or 3. Absence of level in (|a,|a') may suggest unnatural |p, favoring a 4- assignment. Adopted J|p=(5-). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T 1975Pa19 obtain 0.061 ps {I+24-17}. 
J 2033|g(|q) allows J=2,3, not 1. Mult(3541|g)=E1,M1,E2, from T{-1/2}. |g rays to 2+, 0+ levels. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2) is weighted average of data from 1971WaZP (after revision by 1987Ra01) and 1964St04. 
E from E|g. 
T from B(E2)=0.105 {I6} and adopted E|g. 
g-factor=+1.3 {I5} (2001Ma17). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
E$Isomeric ratio R=48 % {I10} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$T{-1/2}: From measured mean lifetime {|t}=0.59 ps 15 (2022Pe15) by fitting the Decay Curve. Systematic uncertainty was taken into account when having contaminated transitions and for short lifetimes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$$ T{-1/2}: From measured mean lifetime {|t}=35.5 ps 6 (2022Pe15) by fitting the Decay Curve and performing the Differential Decay Curve Method (DDCM), using a Total Kinetic Energy Loss (TKEL) condition and a subtraction of the contribution of long-lived feeding from higher-lying states [{|t}{-5{+-}}=1.55 ns 4 and {|t}{-6{++}}=1.53 ns 4 from ENSDF Adopted dataset for {+92}Mo]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
T$from |t=31 ps {I6}, weighted average of 37 ps {I11} from EXP1 and 29 ps {I7} from EXP2 (2023Le18) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: Y
level_comment:
J L(d,p)=2; E2 1477|g from J|p=9/2+ 1477. 
CONF |n d{-5/2}. 
<r{+2}>{+1/2}=4.92 fm for |n 2d{-5/2} orbital from (t,d). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J L(d,p)=2; log| {Ift}=6.5, log| {If{+1u}t}=7.6 from J|p=1/2-. 
T from (p,n|g). Other: 0.04 ps {I3} ({+13}C,{+12}C|g). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J primary |g from 1/2+ in (n,|g) E=res; D+Q 779|g to 7/2+ 1363. 5/2+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
XREF: may also be present in (d,p). 
J E4 263|g from J=21/2, 2425; E2 685|g to J|p|<9/2+. 
T from IT decay. Other: >1.6 ps in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
J D+Q 836|g to J|p=7/2+ 1520; 864|g to 3/2+ 1492; 5/2- from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J L(p,d)=4; D 162|g to (11/2+) 2247; Q 2409|g to 5/2+ g.s. 9/2+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
J from |m=9.49 {I22} from low temperature nuclear orientation in iron (1973Ka21) and g=0.936 {I25} from NMR with oriented nuclei (weighted average of 0.877 {I19} (1973Ka21) and 0.946 {I8} (1981Ha12)); E4 263|g to |p=+ 2162. 
Configuration: (|n (d{-5/2})~#(|p (g{+2}{-9/2})){+21/2+}; analogous to 21/2+ isomers in N=51 isotones {+91}Zr and {+95}Ru. 
T from IT decay. 
%IT, %|e+%|b{++}: from 1977Me03. 
|m: from radiative detection of NMR (1989Ra17), based on g=0.946 {I8} (1981Ha12); value relative to {+95}Mo. Others: 9.49 {I22} (1973Ka21), 10.0 {I7} (1977Be19). Sign probably +. 
Configuration=((|n d{-5/2})(|p 1g{-9/2}){++2}) (1985Su04). 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_lifetime_unit: NS
level_comment:
J E2 268|g to J|p=13/2+ 2162; |g(|q) in (p,n|g) is consistent with stretched Q transition. 17/2+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
J M1+E2 2431|g to 5/2+ g.s.; D(+Q) 1068|g to 7/2+ 1363; 403|g from (9/2)- 2834. However, |p=- from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: PS
level_comment:
J 279|g to 13/2+ 2162, 963|g to 9/2+ 1477, 136|g to 11/2- 2304 imply J|p=(9/2+,11/2,13/2+); (11/2-) from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: NS
level_comment:
J E1 |g from J|p=(11/2+,13/2+); E1 203|g to J|<11/2 {I2247}; (13/2-) from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: FS
level_comment:
J log| {Ift}=7.18, log| {If{+1u}t}=7.46 from 9/2+; 2479|g to 5/2+ g.s.; 7/2+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: FS
level_comment:
J L=4 in ({+3}He,|a); 2535|g to 5/2+ g.s.; 9/2+ from statistical analysis of (p,n|g) via IAS. Probable L=4 component of L=1+4 doublets in (p,d) and (d,t) at E=2523 {I12}. 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_lifetime_unit: FS
level_comment:
J D+Q 1047|g to 3/2+ 1492; J=3/2 from statistical analysis of (p,n|g) via IAS. Information on parity is contradictory: |p=- from log| {Ift}=5.5 from 1/2- and |p=- is favored in (p,n|g), but |p=+ based on large |d(1047|g) to |p=+ 1492 level. 
T from DSAM in (p,n|g) (1999Ka60). 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J 143|g to J|p=(17/2)+ 2430, D 411|g to 13/2+ 2162 imply J|p=(13/2+,15/2); 15/2- from statistical analysis of (p,n|g) via IAS. 
T >0.18 ps from (p,n|g). 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J D 480|g to 13/2+ 2162; D 212|g to (17/2+) 2430; |p=+ from statistical analysis of (p,n|g) via IAS. 
T >0.18 ps from (p,n|g). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: FS
level_comment:
J log| {Ift}=5.6 from 1/2-; 2698|g to J|p=5/2+ g.s. However, |p=+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: FS
level_comment:
J log| {Ift}=5.9, log| {If{+1u}t}=5.8 from J|p=9/2+; 2731|g to J|p=5/2+ g.s.; 9/2+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J 369|g to (11/2-) 2440; M1 237|g to (15/2-) 2573; 13/2- from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J log| {Ift}=5.7 from J|p=1/2-; 2862|g to J|p=5/2+ g.s.; 1/2-,3/2- from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: FS
level_comment:
J log| {Ift}=4.8 from J|p=9/2+; 2902|g to J|p=5/2+ g.s.; 9/2+ from statistical analysis of (p,n|g) via IAS. 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2,11/2+)
level_comment:
J 378|g to (7/2+) 2833; 455|g to (11/2-) 2755. The 11/2- assignment by 1983Mi13 in (p,n|g) would imply M2 multipolarity for the 378|g which seems untenable for the strongest deexcitation branch. 


level_energy_unit: KEV
level_spin_parity: (LE5/2)
level_comment:
J 2463|g to 1/2+ 943. In (p,n|g), 1983Mi13 suggest J|p=(5/2-) based on excit, but this implies that 4653|g is M2 which seems unlikely. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
J L(p,t)=0 on 5/2+ target; from the large cross section measured by 1972OhZT, it follows that this reaction proceeds via a large |DS=0 component. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
J stretched E2 279|g to J=(23/2-) 4159. Interpreted in ({+16}O,5n|g) (2005Fu01) as arising from weak coupling of (|n d{-3/2}) to 11- isomer in {+92}Mo, based on energy of this level and nearby lower-energy states; however, other configurations may contribute. 
T from centroid-shift method (2005Fu01), based on 278|g and 1735|g time distribution spectra in ({+16}O,5n|g). 


level_energy_unit: KEV
level_spin_parity: (35/2,37/2)
level_comment:
J D or Q transition from (39/2-) 9669+x level assumed by 2005Fu01 in ({+16}O,5n|g). 669|g to (33/2,35/2) 9001 level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (39/2-)
level_lifetime_unit: US
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E x is expected to be small. The existence of this isomer is deduced by 2005Fu01 from the observation of many delayed gamma rays belonging to {+93}Mo. The location of the isomer in the level scheme was deduced from intensities of each cascade in the nuclide. Probably not an yrast state (2005Fu01). 
J possible 5-quasiparticle configuration: |n ((d{-5/2}g{-7/2}h{-11/2})~#(|p (g{+2}{-9/2})){+39/2-} (2005Fu01). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E from (d,t). Isobaric analog of {+93}Nb(g.s.). Other E: 10740 {I60} from ({+3}He,t). 
J L(p,d)=4; isobaric analog of 9/2+ state. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=0.3470 {I2} 
|G{-|g}=0.178 eV; g|*' |G{-n}=0.0079 eV {I6}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=7.7 meV 5. 
WIDTHG Assumed by 1973Wa17. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=1.8688 {I11} 
|G{-|g}=0.240 eV; g|*' |G{-n}=0.047 eV {I10}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=45 meV 3. 
WIDTHG Assumed by 1973Wa17. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=2.3226 {I16} 
|G{-|g}=0.240 eV; g|*' |G{-n}=0.050 eV {I6}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=55 meV 4. 
WIDTHG Assumed by 1973Wa17. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=3.1690 {I25} 
|G{-|g}=0.216 eV {I20}; g|*' |G{-n}=7.8 eV {I6}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=210 meV 20. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=4.292 {I4} 
|G{-|g}=0.230 eV {I24}; g|*' |G{-n}=1.05 eV {I20}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=320 meV 35. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=5.577 {I5} 
|G{-|g}=0.34 eV {I5}; g|*' |G{-n}=0.50 eV {I5}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=288 meV 27. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=6.031 {I5} 
|G{-|g}=0.340 eV; g|*' |G{-n}=0.58 eV {I15}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=314 meV 30. 
WIDTHG Assumed by 1973Wa17. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(n)(lab)=6.482 {I6} 
|G{-|g}=0.110 eV {I10}; g|*' |G{-n}=1.1 eV {I1}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=100 meV 10. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=6.812 {I7} 
|G{-|g}=0.17 eV {I3}; g|*' |G{-n}=0.58 eV {I5}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=133 meV 11. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=7.132 {I7} 
|G{-|g}=0.17 eV {I5}; g|*' |G{-n}=0.52 eV {I10}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=128 meV 11. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 3/2-&1/2-
level_comment:
$E(n)(lab)=8.9 {IAP} 
|G{-|g}=0.210 eV {I20} and 0.24 eV {I3}, g|*' |G{-n}=2.5 eV {I5} and 3.5 eV {I3} and g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=360 meV 30 and 220 meV 20 for E(n)=8.802 {I9} and 8.918 {I9} resonances (E(level)=8078.53 {I9} and 8078.63 {I9}), respectively. 1973Wa17 assume |G{-|g}=0.240 eV for E(n)|?8.9 doublet. 


level_energy_unit: KEV
level_spin_parity: [1/2-]
level_comment:
$E(n)(lab)=9.135 {I5} 
|G{-|g}=0.24 eV {I4}; g|*' |G{-n}=1.6 eV {I3}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=202 meV 18. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=10.590 {I11} 
|G{-|g}=0.37 eV {I10}; g|*' |G{-n}=0.46 eV {I7}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=284 meV 30. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=11.112 {I11} 
|G{-|g}=0.20 eV {I6}; g|*' |G{-n}=0.36 eV {I6}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=191 meV 19. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=11.520 {I12} 
|G{-|g}=0.160 eV {I15}; g|*' |G{-n}=11.0 eV {I15}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=158 meV 16. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=12.850 {I13} 
g|*' |G{-n}=0.22 eV {I3}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=193 meV 20. 
1973Wa17 assume |G{-|g}=0.240 eV. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=13.760 {I14} 
|G{-|g}=0.119 eV {I11}; g|*' |G{-n}=32 eV {I3}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=119 meV 13. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(n)(lab)=14.140 {I14} 
|G{-|g}=0.172 eV {I16}; g|*' |G{-n}=5.2 eV {I4}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=166 meV 15. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=14.460 {I15} 
|G{-|g}=0.24 eV {I8}; g|*' |G{-n}=0.22 eV {I4}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=150 meV 16. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 1/2-&3/2-
level_comment:
$E(n)(lab)=15.7 {IAP} 
|G{-|g}=0.192 eV {I20} and 0.170 eV {I20}, g|*' |G{-n}=6.0 eV {I14} and 1.9 eV {I7}, and g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=186 meV 20 and 289 meV 25 for E(n)=15.670 {I16} and 15.720 {I16} resonances (E(level)=8085.31 {I9} and 8085.36 {I9}), respectively. 1973Wa17 assume |G{-|g}=0.240 eV for E(n)|?15.7 doublet. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=16.550 {I17} 
|G{-|g}=0.151 eV {I15}; g|*' |G{-n}=63 eV {I6}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=151 meV 15. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=17.300 {I17} 
|G{-|g}=0.21 eV {I10}; g|*' |G{-n}=0.25 eV {I7}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=157 meV 15. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 3/2-&(1/2)-
level_comment:
$E(n)(lab)=18.1 {IAP} 
|G{-|g}=0.169 eV {I20} and 0.218 eV {I20}, g|*' |G{-n}=0.8 eV {I3} and 4.00 eV {I15}, and g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=238 meV 20 and 207 meV 20 for E(n)=18.020 {I18} and 18.145 {I18} resonances (E(level)=8087.64 {I9} and 8087.76 {I9}), respectively. 1973Wa17 assume |G{-|g}=0.240 eV for E(n)|?18.1 doublet. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=19.200 {I19} 
|G{-|g}=0.206 eV {I20}; g|*' |G{-n}=6.0 eV {I15}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=385 meV 34. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=20.335 {I20} 
|G{-|g}=0.19 eV {I3}; g|*' |G{-n}=0.49 eV {I20}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=136 meV 15. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 1/2-&3/2-
level_comment:
$E(n)(lab)=20.60 {IAP} 
|G{-|g}=0.153 eV {I26} for 20.600 {I21} resonance; g|*' |G{-n}=0.50 eV 22 and 0.14 eV {I6}, and g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=117 meV 15 and 125 meV 15 for E(n)=20.600 {I21} and 20.680 {I21} resonances (E(level)=8089.93 {I9} and 8090.19 {I9}), respectively. 1973Wa17 assume |G{-|g}=0.150 eV for E(n)|?20.6 doublet. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=21.100 {I21} 
|G{-|g}=0.166 eV {I14}; g|*' |G{-n}=31 eV {I3}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=165 meV 20. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$E(n)(lab)=21.740 {I22} 
g|*' |G{-n}=0.27 eV {I5}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=260 meV 25. 1973Wa17 assume |G{-|g}=0.177. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=23.950 {I24} 
|G{-|g}=0.42 eV {I4}; g|*' |G{-n}=15.2 eV {I15}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=800 meV 90. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=25.480 {I25} 
|G{-|g}=0.177 eV {I15}; g|*' |G{-n}=8.4 eV {I8}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=340 meV 30. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=25.830 {I26} 
|G{-|g}=0.175 eV {I17}; g|*' |G{-n}=37 eV {I4}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=174 meV 17. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(n)(lab)=26.220 {I26} 
|G{-|g}=1.58 eV {I20}; g|*' |G{-n}=73 eV {I5}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=1.55 eV 20. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=28.040 {I28} 
|G{-|g}=0.39 eV {I5}; g|*' |G{-n}=13.0 eV {I6}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=0.73 eV 80. 


level_energy_unit: KEV
level_spin_parity: [1/2+]
level_comment:
$E(n)(lab)=28.55 {I3} 
|G{-|g}=0.054 eV {I20}; g|*' |G{-n}=0.5 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=49 meV 8. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(n)(lab)=28.71 {I3} 
|G{-|g}=0.26 eV {I3}; g|*' |G{-n}=26.0 eV {I19}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=260 meV 30. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(n)(lab)=29.82 {I3} 
|G{-|g}=0.175 eV {I20}; g|*' |G{-n}=37.0 eV {I4}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=174 meV 20. 


level_energy_unit: KEV
level_spin_parity: [1/2-]
level_comment:
$E(n)(lab)=30.32 {I3} 
|G{-|g}=0.137 eV {I14}; g|*' |G{-n}=5.6 eV {I8}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=134 meV 15. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=31.13 {I3} 
|G{-|g}=0.14 eV {I4}; g|*' |G{-n}=20 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=270 meV 30. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E(n)(lab)=31.22 {I3} 
|G{-|g}=0.103 eV {I20}; g|*' |G{-n}=57 eV {I3}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=103 meV 20. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=32.59 {I3} 
|G{-|g}=0.56 eV {I8}; g|*' |G{-n}=40 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=1.08 eV 15. 


level_energy_unit: KEV
level_spin_parity: [1/2+]
level_comment:
$E(n)(lab)=33.49 {I3} 
|G{-|g}=0.089 eV {I15}; g|*' |G{-n}=0.5 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=75 meV 10. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=34.46 {I3} 
|G{-|g}=0.15 eV {I3}; g|*' |G{-n}=10 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=283 meV 40. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$E(n)(lab)=34.67 {I4} 
|G{-|g}=0.16 eV {I3}; g|*' |G{-n}=5 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=150 meV 30. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E(n)(lab)=34.83 {I4} 
|G{-|g}=0.26 eV {I5}; g|*' |G{-n}=10 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=500 meV 65. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$E(n)(lab)=35.60 {I4} 
|G{-|g}=0.21 eV {I4}; g|*' |G{-n}=1 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=171 meV 30. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$E(n)(lab)=35.74 {I4} 
|G{-|g}=0.20 eV {I4}; g|*' |G{-n}=3 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=182 meV 30. 


level_energy_unit: KEV
level_spin_parity: [1/2-]
level_comment:
$E(n)(lab)=36.00 {I4} 
|G{-|g}=0.23 eV {I4}; g|*' |G{-n}=10 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=226 meV 35. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_comment:
$E(n)(lab)=36.48 {I4} 
|G{-|g}=0.52 eV {I8}; g|*' |G{-n}=40 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=1.05 eV 15. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_comment:
$E(n)(lab)=37.06 {I4} 
|G{-|g}=0.23 eV {I4}; g|*' |G{-n}=2 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=380 meV 60. 


level_energy_unit: KEV
level_spin_parity: [1/2+]
level_comment:
$E(n)(lab)=37.71 {I4} 
|G{-|g}=0.146 eV {I25}; g|*' |G{-n}=30 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=146 meV 25. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$E(n)(lab)=37.97 {I4} 
|G{-|g}=0.138 eV {I18}; g|*' |G{-n}=1 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=216 meV 35. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_comment:
$E(n)(lab)=38.47 {I4} 
|G{-|g}=0.73 eV {I10}; g|*' |G{-n}=4 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=1.05 eV 15. 


level_energy_unit: KEV
level_spin_parity: [1/2-]
level_comment:
$E(n)(lab)=39.12 {I4} 
|G{-|g}=0.22 eV {I5}; g|*' |G{-n}=3 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=204 meV 30. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_comment:
$E(n)(lab)=40.22 {I4} 
|G{-|g}=0.41 eV {I7}; g|*' |G{-n}=15 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=786 meV 125. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_comment:
$E(n)(lab)=40.36 {I4} 
|G{-|g}=0.27 eV {I5}; g|*' |G{-n}=60 eV; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=533 meV 65. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(n)(lab)=47.93 {I5} 
|G{-|g}=0.110 eV {I20}; g|*' |G{-n}=50 eV {I25}; g|G{-|g}|G{-n}/(|G{-|g}+|G{-n})=111 meV 20. 


level_energy_unit: KEV
level_comment:
In fig. 5 of 1972Ma16, a 2437|g also deexcites this level; however, it is absent in the relevant p'-|g spectrum and in the level scheme of fig. 6, so it is not included here. 


level_energy_unit: KEV
level_comment:
E from 1972Du13. Possibly the same level as the 2842 {I1} level in 1972Ma16; not included in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T weighted average of 0.32 ps {I+19-9} (1976Du01, Doppler effect) and 0.24 ps {I+13-9} (1975Ch05). Others: 0.8 ps {I+6-3} (1976Ru03), 0.66 ps {I+10-14} (1999Ka60). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T weighted average of 1.0 ps {I+6-3} (1976Ru03) and 0.62 ps {I+55-17} (1976Du01). Other: >0.83 ps (1999Ka60), >0.19 ps (1975Ch05). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J adopted value is (3/2); |p could not be assigned there because of contradictory data. 
T from 1999Ka60. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T,%IT from Adopted Levels. 
Configuration: (|n (d{-5/2})~#(|p (g{+2}{-9/2})). Analogous to 21/2+ isomers in N=51 isotones {+91}Zr and {+95}Ru. 


level_energy_unit: KEV
level_spin_parity: 27/2-
level_lifetime_unit: NS
level_comment:
T from centroid-shift method (2005Fu01), based on 278|g and 1735|g time distribution spectra. 
Possible configuration=(|n d{-5/2}) ~# (11- isomer in {+92}Mo) (weak coupling), but additional configurations are also possible as suggested by transition rates (2005Fu01) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (39/2-)
level_lifetime_unit: US
level_comment:
E x is expected to be small. The existence of this isomer was deduced by 2005Fu01 from the observation of many delayed gamma rays belonging to {+93}Mo. The location of the isomer in the level scheme was deduced from intensities of each cascade in the nuclide. 
Percent population=1.8 {I+10-15} (2005Fu01); probably not an yrast state. 
Possible 5-quasiparticle configuration: (|n (d{-5/2}g{-7/2}h{-11/2})~#(|p (g{+2}{-9/2})){+39/2-}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2)+
level_lifetime_unit: NS
level_comment:
$Probability of excitation of 2430-keV isomer, P{-exc}=0.010 {I3}, deduced by 2018Ch13 from the ratio of intensities of the 268-keV and 2475-keV peaks in double-gated |g|g-coin spectra, corrected for detector efficiency, background contributions and internal conversion of 268|g. Area of the 2475-keV Doppler-corrected peak=1.54|*10{+4} {I3} counts, from coincidence spectrum in Fig. 3a of 2018Ch13. Area of the 268-keV peak=510 {I160} in Fig. 3b of 2018Ch13. The detector efficiency ratio R=|e(2475|g)/|e(268|g)=0.28, and |a(268|g,E2)=0.0356. Then P{-exc}=Area(268|g)(1+|a)R/Area(2475|g) 
$Cross section averaged over the entire target thickness>40 b, deduced by 2018Ch13 from the excitation probability, and target composition, including carbon layers. See details of calculation in the Online contents of the paper by 2018Ch13 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2)+
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
$probability of excitation of 2430-keV isomer, P{-exc} < 2 |* 10{+-5}, deduced by 2022Gu07 from the ratio of maximum number of 268|g events over the number of implanted {+93m}Mo ions. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: Y
level_comment:
T$from determination of Mo concentration through mass spectrometry and activity through liquid scintillation counting (2021Ka50) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2. Vector analyzing power (pol p,p') (1981Pl07). 
T$from B(E2)=0.203 {I4} (see Coulomb Excitation). 
MOME2$-0.13 {i8} or +0.01 {i8} (1989Ra17). Q=-0.13 {i8} from Coulomb excitation if the excitation to higher excited states interferes constructively, as is usual in this mass region. Q=+0.01 {i8} for destructive interference. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$a clear L=0 distribution was seen in (p,t), while in (t,p) an unresolved group was observed at this energy with no indication for an L=0 contribution. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$weighted average of 3375 {i5} from (p,t), 3376 {i5} from (p,p') and (d,d'), and 3378 {i10} from (d,t) 
J$L(p,t)=(5); J|p=(4+) from analysis in (p,p') and (d,d'); L(d,t)=4 gives J|p=1+ to 7+ 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E$level not shown (in Table I of 2003Fr02) as populated in {+94}Tc |e decay, but required by 358|g from 3163 level 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
$Q(8+,{+94}Mo)/Q(8+,{+92}Mo)=1.48 {i12} from time-differential perturbed angular distribution of the stretched-downward cascade (1974Ba11). 
G$From time-differential perturbed angular distribution of the 848, 702, and 870 |g's (1975Fa04). Other: g=1.308 {i10} (1979LeZL). 
T$from time-differential perturbed angular distribution (1975Fa04). Other: 109 ns {i10} from |g(t) (1971Le19). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$J=0 from the strong anisotropy of |s(|q) (1974Mc02). Excitation functions and |g-ray angular distribution restrict J|p to 0+ or negative parity (1976Su04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$B(E2)(2+ to 2+')=0.116 {i26}, B(M1)=0.020 {i7} if |d=2.0 {i3}; B(E2)(0+ to 2+')=0.0032 {i7} (1972Ba90) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$|D<r{+2}>({+94}Mo,{+92}Mo)=+0.322 fm{+2} {I3} (2009Ch09); uncertainty is systematic 
$ Isotope shift({+94}Mo,{+92}Mo)=-762 MHz {I9} (2009Ch09); total uncertainty is given; statistical uncertainty is 1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_uncertain: ?
level_comment:
E$level listed only in the data received by email of Nov 7, 2013 from C. Romig; 5916.25 at 7.65 MeV, 5918.28 at 8.7 MeV data 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_uncertain: ?
level_comment:
E$level listed only in the data received by email of Nov 7, 2013 from C. Romig 
J$from |g(pol) data 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$5/2 from paramagnetic resonance (1956Ow04) and optical spectroscopy (1951Ar29, 1976Fu06). |p=+ from L(d,p)=2 
MOMM1$NMR (Nuclear Magnetic Resonance)(2005St24) 
MOME2$AB (Atomic beam magnetic resonance,thermal beam) calculated from ratio and Q({+97}Mo); no polarization correction included(1989Ra17). Other: -0.015 {i4} ABLDF (Atomic beam with laser double resonance detection) (1978Du24) 
$|D<r{+2}>({+95}Mo,{+92}Mo)=+0.410 fm{+2} {i26} (2009Ch09); uncertainty is systematic 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$3/2+,5/2+ from L(p,d),(d,t)=2; |=5/2 from linear pol in Coulomb ex. 
T$from |g|g(t) in 61-d |e decay. Others: see Coulomb excitation 
MOMM1$IPAC (Integral perturbed angular); Other: -0.378 {i15} (1976Jo03) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$7/2+,9/2+ from L(d,p)=4; 7/2 from |g(|q) in (|g,|g); 7/2+ from L({+3}He,|a)=4 
T$from |s(res) in (|g,|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$3/2+,5/2+ from L(d,p)=2; |=5/2 from |g|g(|q) and linear pol in 61-d |e decay. (5/2) from s(d,t)/s(d,p) discrepant 
T$from |s(res) in (|g,|g) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$7/2+,9/2+ from L(d,p)=4; |=7/2 from |g(|q) in Coul. ex. 
T$weighted av of 2.66 ps {i29} (DSAM) and 2.57 {I12} (B(E2)|^) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$3/2+,5/2+ from L(d,p)=2; 5/2 from primary I|g(135|')/I|g(90|') in (n,|g) E=24.3 keV 
T$from B(E2)|^ in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$7/2+,9/2+ from L(p,d),(d,t)=4; M1+E2 |g to 5/2+ 
T$from B(E2)|^ in Coul. ex. and adopted level and |g properties 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$L(d,p)=2; 3/2+ from s(d,t)/s(d,p) for 1364 doublet. L(p,d),(d,t)=(1) for 1367 doublet; consistent with (|a,n|g),(|a,3n|g) reaction 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_uncertain: ?
level_comment:
$May correspond to preceding level but energies disagree 
J$L(d,p)=2; 3/2+ from s(d,t)/s(d,p) for 1364 doublet. L(p,d),(d,t)=(1) for 1367 doublet. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$3/2+,5/2+ from L(d,p)=2. |=3/2+ from possible d,E2 |g from (9/2)+. 3/2 from s(d,t)/s(d,p) discrepant 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$7/2+,9/2+ from L(p,d),(d,t)=4. |=7/2+ from possible (E1) |g from 11/2- 
T$upper limit from |g(t) in (|a,3n|g); lower limit from B(E2)|^<0.0042 in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (9/2)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_uncertain: ?
level_comment:
J$(1/2 to 9/2) from possible D,Q |g to (3/2+,5/2+), (7/2+ to 15/2+) from possible D,E2 |g to 11/2+, and (7/2- to 15/2-) from D,E2 |g from 11/2- 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_uncertain: ?
level_comment:
J$(7/2+ to 15/2+) from possible D,E2 |g to to 11/2+, |<7/2 from possible D,Q |g to 3/2+, and (7/2- to 15/2-) from possible D,E2 |g from 11/2- discrepant 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$J|p(1879)=7/2+,9/2+ from L(p,d),(d,t)=4; J(2059)=13/2 from |g(|q) in (|a,n|g),(|a,3n|g). J|p(1879)=9/2+, J|p(2059)=13/2+ from a possible connecting D,E2 |g 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J$L+1 transfer from Ay(|q); 1g{-9/2} for L=4; uncertain assignment either the |s(|q) or the Ay(|q) discrepant DWBA calculations 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$11/2- from L({+3}He,|a)=5; supported by 9/2-,11/2- from L(d,p)=5; 11/2(-) from |g(|q) and |g-pol in (|a,n|g),(|a,3n|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$from {+94}Mo(n,|g) E=thermal 
J$from (d,t) data of 1970Di06; Unresolved doublet with E{-x}=2240 {i15}, L=1+2 in 1977Bi02 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$weighted av of 2319 {i12} from (p,d),(d,t) and 2312 {i10} from from ({+3}He,|a) 
J$From angular momentum transfer in (d,p) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E,J$Energy from 2003Au03, and spin and parity is from the assumption of s-wave capture on an even-even target 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$weighted av of 742 ps {i14} (1958Qu01. |g|g(t); NaI), 755 ps {i15} (1965Me08. |g|g(t); scin) and 756 ps {i14} (1970Bo28) 
G$Niobium-foil source; -0.30 {i4} for liquid source 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$1/2+ from |g|g(|q) and linear polarization (1973Be34) assuming J(786)=1/2,3/2, J(821)=1/2,3/2,5/2, and J(1039)=1/2,3/2 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$3/2+ from |g|g(|q) and linear polarization (1973Be34) assuming J(786)=1/2,3/2, J(821)=1/2,3/2,5/2, and J(1039)=1/2,3/2 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_comment:
$Level not adopted on the basis of relative intensity values of 770.7 keV and 666.0 keV |g rays; placed in reverse order by {+16}O({+82}Se,3n|g) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_comment:
$Level adopted following {+16}O(82Se,3n|g); however, it decays by 770.7 keV |g ray instead of 666.0 kev |g ray 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_uncertain: ?
level_comment:
J$(23/2+) from |g(|q) and |g-polarization 
$Not included in Adopted Levels, following placement of 902.7 keV from 3672.4 keV level in {+16}O(82Se,3n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
$|s(RES)(mb)=34.9 {I17} 
J$7/2 from |g(|q) (1967La14) 
T,S$other: 2.0 ps {I+11-7} and 80 mb {i20} (1967La14) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$3/2,5/2 from |g(|q) and |=5/2 from linear pol (1958Mc02) 
BE2$Weighted av of 0.035 {i3} (1958Mc02) and 0.0380 {i24} (1975Ba02). Others: 0.043 {i5} (1972BoZV) and 0.029 {i3} (1975An17). See 1975Ba02 for other references 
G$IMPAC, assuming T{-1/2}=756 ps {i7} (weighted av of 811 ps {i42} (1966An02), 756 ps {i14} (1970Bo28), 742 ps {i14} (1958Qu01), 769 ps {i28} (1958Mc02), 762 ps {i63} (1961Ho05), and 755 ps {i15} (1965Me08)) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
BE2$B(E2)=0.0004 {i1} (1975An17) reduced by 20% to account for feeding from 1551 state. Others: |<0.0005 (1972BoZV) and <0.00013 (1975Ba02) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$|=7/2 from |g(|q) (1975Ba02); 3/2 or 9/2 from |g(|q) (1972BoZV) 
T$from B(E2) 
BE2$Weighted av of 0.048 {i5} (1972BoZV), 0.0506 {i31} (1975Ba02), and 0.044 {i4} (1975An17). 0.050 {i5} (1972BoZV) and 0.0525 {i25} (1975Ba02) reduced by 3.6% {i36} to account for feeding from 1551 state which was not observed by them. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$|=9/2 from |g(|q) (1975Ba02); |<7/2 from |g(|q) (1972BoZV) 
BE2$Unweighted av of 0.040 {i5} (1972BoZV), 0.0386 {i21} (1975Ba02), and 0.032 {i3} (1975An17) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$|D<r{+2}>({+95}Mo,{+92}Mo)=+0.410 fm{+2} {i26} (2009Ch09); uncertainty is systematic 
$Isotope shift({+95}Mo,{+92}Mo)=-925 MHz {i13} (2009Ch09); total uncertainty is given; statistical uncertainty is 1 
J,T$from adopted levels 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
E$1056 keV level was directly populated in the (d,p) reaction in 2016Wi01 but was not included in the ENSDF (d,p) source data set. J|p=5/2+ was inferred from a combination of ENSDF assignment and the results from 2016Wi01. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
E$: 1073 keV level was directly populated in the (d,p) reaction in this paper and also observed in the particle spectra from 1969Mo24, even though this level has never been reported in a (d,p) measurement. However, the 253-keV |g-ray with an intensity of 32 % {I32} was not observed in this measurement. 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
J$Although the ENSDF assignment is J=5/2, it was reported as J|p = 3/2+ in 1969Mo24, 1977Bi02, 2004Su22, which corresponded to the results obtained in 2016Wi01. 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
E$A level is reported in ENSDF at a slightly lower energy of 1660 keV. A E{-|g}=1457 keV transition to the first excited at 204 keV was clearly observed, but no transition to the ground state was seen. The energy dependence of the proton spectrum above S{-n} exhibited J=3/2 characteristics, which is consistent with the ENSDF assignment of J|<5/2. 


level_energy_unit: KEV
level_spin_parity: 9/2
level_comment:
E$The ENSDF assignment for the level at 1667 keV {I8} is J|p=7/2+, 9/2+. This spin assignment using the method described in this paper is J=9/2, is also consistent with the observation of a 262 keV transition to J|p=11/2- state at 1937 keV. 


level_energy_unit: KEV
level_spin_parity: 9/2
level_comment:
E$A level at 1879 keV {I12} with J|p=9/2+ was reported in 1977Bi02. The tentative assignment of J=9/2 and its transition were confirmed. ENSDF reported an assignment of 337.3 keV transition to 1888.5 keV {I2} level, but observation from 2016Wi01 and 1972Me03 confirmed that the 1888.5 keV level was either misplaced or mislabeled. The correct level energy is approximately 1879 keV. 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
E$1968 keV level with J=5/2 was observed, and was in agreement with previous results from a (d,p) reaction in 1969Mo24. 


level_energy_unit: KEV
level_comment:
E$1984 keV {I15} level with J|p=3/2+,5/2+ were observed using (p,t) and (d,t) reactions listed in ENSDF. 2016Wi01 was unable to determine the spin, but the observed |g decay to a J=9/2+ 947-keV level strongly favors the J|p=5/2+ assignment to the 1978 keV level. 


level_energy_unit: KEV
level_comment:
E$If this state is the 2383-keV level previously observed in several (d,p) reactions stated in ENSDF, then the tentative J=3/2 assignment is not consistent with the observed E{-|g}=1438-keV transition to J|p=9/2+ 947-keV level. 


level_energy_unit: KEV
level_comment:
E$A J|p=9/2+ level at 2531 keV {I12} is reported in the ENSDF database. This is in keeping with several other measurements including 1977Bi02, 2004Su22, 1970Di05. However, the observed |g decay to a 3/2+ level does not support this spin assignment. The authors of 2016Wi01 state that this constitutes strong evidence for the existence of a new level at 2528 keV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|g to 0+ is E2 
T$from B(E2)=0.270 {i4} (Coul. ex) 
$Q=-0.20 {I8} or +0.04 {I8} (1976Pa13) 
$|m measured using transient field method following Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=2 
T$From B(E2)(0+ to 2+)=0.0156 {i13} (Coul. ex), other 0.74 ps {I+63-25} from DSAM in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|g's to 6+ and 4+. A questionable gamma feeds a 2+ level. The {+82}Se({+18}O,4n|g) dataset assigns J=5+, while the remaining datasets assign j=4+. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$this level is interpreted by 2007Le05 as a mixed-symmetry, one- phonon 2+ state based on high value of B(M1)=0.17 {i2} for transition to the first 2+ state 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$this level is interpreted by 2007Le05 as a mixed-symmetry, two- phonon 2+ state based on high value of B(M1)=0.10 {i2} for transition to the second 2+ state 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E$this level is interpreted by 2007Le05 as a mixed-symmetry, two- phonon 3+ state based on B(M1)=0.06 {i1} for transition to the second 2+ state 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$this level is interpreted by 2007Le05 as a mixed-symmetry, two- phonon 1+ state based on high value of B(M1)=0.11 {i2} for transition to the second 2+ state 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$this level is interpreted by 2007Le05 as a possible mixed-symmetry, two-phonon 2+ state based on strong decay to the main mixed-symmetry 2+ state at 2096 and a weak E2 transition to the g.s. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$this level is interpreted by 2007Le05 as a mixed-symmetry, two- phonon 1+ state based on high value of B(M1)=0.11 {i4} for transition to the g.s. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$it was assigned by 2004Fr30 as a mixed-symmetry 1+ state, but 2007Le05 reject this assignment based on their lifetime measurements and deduced transition probabilities 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
BE2$From 1976Pa13; interference with higher 2+ states may change B(E2) to 0.269 or 0.271. B(E2)=0.284 {i14} from 1971Ba59. Other measurements: B(E2)=0.284 {i14} (1971Ba59), 0.302 {i33} (1958St32) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$B(E2)(|g to g.s.)=0.0156 {i19}; B(E2)(|g to 778.2)=0.045 {i7}, |b(M1)=0.09 {i1} 
$|b(EL): if |d(719.5)=0.18 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$B(E2)(to g.s.)=0.0015 {i4}; B(E2)(|g to 778.2)=0.045 {i15}, |b(M1)=0.020 {i6} 
$|b(EL): if |d(847.6)=1.08 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$|D<r{+2}>({+96}Mo,{+92}Mo)=+0.597 fm{+2} {I11} (2009Ch09); uncertainty is systematic 
$ Isotope shift({+96}Mo,{+92}Mo)=-1390 MHz {I16} (2009Ch09); total uncertainty is given; statistical uncertainty is 1 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$ 2+ assigned for a 3024.58 level in ENSDF database for {+96}Mo 
$ d|s/d|W=0.022 mb/sr {I1} at 6|', 0.0048 mb/sr {I4} at 15|'. |s(6|')/|s(15|')>2 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$ 3- assigned for a 3178.69 level in ENSDF database for {+96}Mo 
$ d|s/d|W=0.023 mb/sr {I1} at 6|', 0.0042 mb/sr {I4} at 15|'. |s(6|')/|s(15|')>2 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$ 4+ assigned for a 3186.81 level in ENSDF database for {+96}Mo 
$ d|s/d|W=0.0109 mb/sr {I9} at 6|', 0.0043 mb/sr {I4} at 15|'. |s(6|')/|s(15|')>2 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Candidate for one-phonon mixed symmetry state 
T$effective T{-1/2}=0.201 ps {I35} of 1317.63|g. For B(E2) and B(M1) values listed with |g rays, T{-1/2}=97 fs {I11} is used by 2016Th01 taken from {+96}Mo Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$(1190.45|g)(849.99|g)(|q) gives J=4,5,6; but |g to 2+ rules out J=5,6 
T$effective T{-1/2}=0.152 ps {I21} of 1190.45|g 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E$based on different decay characteristics observed, this level is considered as different by 2016Th01 from the previously known 3416.82, 4+ level 
T$effective T{-1/2}=0.215 ps {I42} of 975.52|g 


level_energy_unit: KEV
level_comment:
E$this level may be different from the previously known level at 3597, 2+, since 862.4|g from this level is shown to feed a 2735,5+ level in Table 1 of 2016Th01. If the 862.4|g feeds the 2736, 3+ level, then this level can be the same as the previous one 


level_energy_unit: KEV
level_spin_parity: (9+)
level_comment:
J$2016Th01 assign 7+,9; but 879|g between 3916,(11)+ level makes J=7 unlikely, thus compiler assigns (9+) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$uncertainty is purely statistical. Systematic uncertainty from GOSIA code is approximately 3% (2023Ru06). 
BE2$obtained for 3 of the 4 possible combinations of interference terms from the 2{-2}{++} and 2{-3}{++} levels. Other: 0.269 {I10} from fourth possibility of interference term. 
MOME2$values are -0.53 {I9}, -0.45 {I9}, -0.35 {I9}, and -0.28 {I9} for the 4 possible combinations of interference terms from the 2{-2}{++} and 2{-3}{++} levels. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$from L=2 in {+95}Mo(t,p) (2008Ra13); also J=5/2 (1976Fu06); |p=+ from L=2 in ((d,p), (t,d), (p,d) and (d,t) reactions. 
MOMM1$measured by nuclear magnetic resonance (1951Pr02) 
MOME2$measured by atomic beam magnetic resonance - thermal beam (reevaluated by 1989Ra17); Q({+97}Mo)/Q({+95}Mo)=-11.48 {I1} (1984Ol02), 11.4 {I3} (1975Ka23). 
$|D<r{+2}>({+97}Mo,{+92}Mo)=+0.630 fm{+2} {I12} (2009Ch09); uncertainty is systematic 
$ Isotope shift({+97}Mo,{+92}Mo)=-1391 MHz {I21} (2009Ch09); total uncertainty is given; statistical uncertainty is 1 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$L=4 in (d,p), (t,d), (p,d); 7/2 from 1024.49|g excit, |g(|q) (|a,n|g). If same level as 1025 then J|p=5/2+ 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$9/2, 11/2 from 751.41|g excit (|a,n|g), ({+3}He,2n|g); stretched E2 to 7/2+ level, no |g to g.s. 
T$deduced from prompt coin (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$J|>9/2 from |g excit, |g to 9/2+ level with |DJ=1 |g(|q) ({+3}He,2n|g); |p from strong |g to 7/2+ level 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$3/2,5/2 from 823.20|g excit (|a,n|g), 1281.78|g excit (n,n'|g); |g's to 7/2+ and 9/2+ levels. Tentative contradictory assignment (7/2+,11/2+) in ({+3}He,2n|g) based on |g(|q) result obtained with contaminated |g 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$L=4 member of the doublet at 1961 keV in (p,d); 1481.0|g, 1959.3|g excit in (n,n'|g); decay to 5/2+ and 3/2+ levels 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$3/2-,5/2-,7/2- from L=1 in (t,p); (7/2-) from |g to 9/2+, 1117 (also |DJ Ne 2 for |g to 9/2+ level in ({+3}He,2n|g)) ({+3}He,2n|g) 


level_energy_unit: KEV
level_comment:
L$a good fit to the measured angular distribution for this state was obtained only with the sum of L=0+2 distributions. 
S$for the L=0 state C{+2}S'=0.08 {I1}, L=2 state C{+2}S'=0.13 {I1}. 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
J$from 237.93 excit: 5/2 preferred but 3/2, 7/2 not ruled out; from 718.8|g excit: 5/2 preferred but 7/2 not ruled out. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$from (480.9|g)(|q) 
T$other: 8.5 ps {I4} (1975BoYF, unpublished measurement, quoted in 1975Ba02), >2.4 ps (1974Er01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$(238.3|g)(|q) rules out 1/2 and 7/2 
T$other: >0.7 ps (1974Er01). Alternate value of |d(719.3|g) gives T{-1/2}=57 ps {I7} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$from (721.1|g)(|q) fits J=3/2, 5/2 or 7/2 
T$other: >0.7 ps (1974Er01). Alternate value of |d(721.1|g) gives T{-1/2}=98 ps {I15} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$only 7/2, 9/2 considered in fitting (1024.6|g)(|q) 
T$from 1974Er01. Other: 0.37 {I26} ps (from B(E2)|^) 


level_energy_unit: KEV
level_spin_parity: 7/2+,(1/2+)
level_comment:
J$from 1975Bi10; may include the 2040.9-keV (9/2,11/2), 2049.9-keV (7/2,9/2), and 2033.7-keV 1/2+ levels. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0128 {I11} (at 6|'), 0.037 {I3} (at 18|'), 0.0099 {I10} (at 31|'), 0.0122 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=2.99 {I15} (at 6|'), 0.299 {I16} (at 18|'), 0.447 {I23} (at 31|'), 0.202 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.429 {I22} (at 6|'), 0.036 {I3} (at 18|'), 0.055 {I4} (at 31|'), 0.0250 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0150 {I11} (at 6|'), 0.0190 {I22} (at 18|'), 0.0227 {I15} (at 31|'), 0.0118 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0073 {I7} (at 6|'), 0.0240 {I23} (at 18|'), 0.0046 {I5} (at 31|'), 0.0060 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.0101 {I10} (at 6|'), 0.0220 {I15} (at 18|'), 0.0380 {I22} (at 31|'), 0.044 {I3} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0160 {I13} (at 18|'), 0.0300 {I18} (at 31|'), 0.0320 {I19} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.183 {I10} (at 6|'), 0.0210 {I15} (at 18|'), 0.0310 {I19} (at 31|'), 0.0100 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0230 {I23} (at 6|'), 0.031 {I3} (at 18|'), 0.0090 {I11} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0068 {I9} (at 6|'), 0.0050 {I7} (at 18|'), 0.0098 {I9} (at 31|'), 0.0103 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0035 {I6} (at 6|'), 0.0160 {I13} (at 18|'), 0.0038 {I6} (at 31|'), 0.0053 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0110 {I12} (at 6|'), 0.0070 {I11} (at 18|'), 0.0040 {I6} (at 31|'), 0.0016 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0080 {I11} (at 6|'), 0.00100 {I11} (at 18|'), 0.0100 {I11} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0092 {I10} (at 6|'), 0.0071 {I8} (at 18|'), 0.0032 {I5} (at 31|'), 0.0007 {I4} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0027 {I6} (at 6|'), 0.0064 {I8} (at 18|'), 0.0128 {I11} (at 31|'), 0.0140 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.081 {I5} (at 6|'), 0.070 {I5} (at 18|'), 0.0160 {I13} (at 31|'), 0.0210 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 6|'), 0.0300 {I25} (at 18|'), 0.035 {I3} (at 31|'), 0.047 {I3} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.051 {I3} (at 6|'), 0.071 {I7} (at 18|'), 0.0171 {I11} (at 31|'), 0.0250 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0058 {I6} (at 6|'), 0.0049 {I8} (at 18|'), 0.010 {I5} (at 31|'), 0.0080 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.081 {I5} (at 6|'), 0.071 {I4} (at 18|'), 0.0214 {I13} (at 31|'), 0.0195 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.010 {I8} (at 6|'), 0.0102 {I10} (at 18|'), 0.0210 {I15} (at 31|'), 0.0260 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.037 {I3} (at 6|'), 0.045 {I3} (at 18|'), 0.0084 {I9} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0018 {I6} (at 6|'), 0.0093 {I10} (at 18|'), 0.0080 {I11} (at 31|'), 0.0022 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0170 {I13} (at 6|'), 0.0210 {I15} (at 18|'), 0.0210 {I15} (at 31|'), 0.028 {I3} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0220 {I15} (at 6|'), 0.0280 {I17} (at 18|'), 0.0036 {I7} (at 31|'), 0.0150 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 6|'), 0.0110 {I12} (at 18|'), 0.0130 {I12} (at 31|'), 0.013 {I3} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0049 {I7} (at 6|'), 0.0070 {I8} (at 18|'), 0.0043 {I5} (at 31|'), 0.0037 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0070 {I8} (at 6|'), 0.0053 {I7} (at 18|'), 0.0045 {I5} (at 31|'), 0.0053 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0140 {I12} (at 6|'), 0.0160 {I13} (at 18|'), 0.0042 {I5} (at 31|'), 0.0055 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0013 {I5} (at 6|'), 0.0035 {I6} (at 18|'), 0.0070 {I7} (at 31|'), 0.0061 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0050 {I8} (at 6|'), 0.0040 {I7} (at 18|'), 0.0041 {I6} (at 31|'), 0.0038 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0113 {I11} (at 6|'), 0.0100 {I11} (at 18|'), 0.0042 {I6} (at 31|'), 0.0044 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0240 {I16} (at 6|'), 0.0290 {I25} (at 18|'), 0.0051 {I7} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.004 {I1} (at 6|'), 0.0070 {I11} (at 18|'), 0.0080 {I11} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 6|'), 0.0090 {I11} (at 18|'), 0.0200 {I14} (at 31|'), 0.0170 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0270 {I24} (at 6|'), 0.0260 {I17} (at 18|'), 0.0090 {I9} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 6|'), 0.0150 {I13} (at 18|'), 0.0330 {I19} (at 31|'), 0.038 {I3} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0150 {I13} (at 6|'), 0.0190 {I14} (at 18|'), 0.0062 {I9} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.005 {I1} (at 6|'), 0.004 {I1} (at 18|'), 0.0110 {I12} (at 31|'), 0.0100 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.756 {I38} (at 6|'), 0.709 {I36} (at 18|'), 0.557 {I28} (at 31|'), 0.335 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.463 {I24} (at 6|'), 0.251 {I13} (at 18|'), 0.155 {I8} (at 31|'), 0.1010 {I54} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0610 {I37} (at 6|'), 0.0230 {I15} (at 18|'), 0.0180 {I14} (at 31|'), 0.0150 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0620 {I37} (at 6|'), 0.0500 {I27} (at 18|'), 0.035 {I2} (at 31|'), 0.0250 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.1070 {I57} (at 6|'), 0.0610 {I32} (at 18|'), 0.0365 {I20} (at 31|'), 0.0220 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.216 {I11} (at 6|'), 0.1310 {I69} (at 18|'), 0.0720 {I37} (at 31|'), 0.0570 {I35} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.1520 {I82} (at 6|'), 0.1410 {I77} (at 18|'), 0.0870 {I45} (at 31|'), 0.0580 {I35} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.401 {I21} (at 6|'), 0.262 {I13} (at 18|'), 0.1320 {I69} (at 31|'), 0.0800 {I45} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0750 {I48} (at 6|'), 0.0480 {I31} (at 18|'), 0.0280 {I17} (at 31|'), 0.0170 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0180 {I14} (at 6|'), 0.01040 {I72} (at 18|'), 0.00650 {I52} (at 31|'), 0.00410 {I45} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0430 {I24} (at 6|'), 0.0242 {I14} (at 18|'), 0.01380 {I85} (at 31|'), 0.00990 {I78} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0172 {I11} (at 18|'), 0.01030 {I65} (at 31|'), 0.00700 {I61} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0200 {I14} (at 6|'), 0.0170 {I11} (at 18|'), 0.00870 {I66} (at 31|'), 0.00680 {I61} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.1010 {I54} (at 6|'), 0.0710 {I37} (at 18|'), 0.0388 {I21} (at 31|'), 0.0257 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.666 {I34} (at 6|'), 0.456 {I23} (at 18|'), 0.242 {I12} (at 31|'), 0.1370 {I71} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0790 {I44} (at 6|'), 0.0470 {I26} (at 18|'), 0.0260 {I17} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0220 {I23} (at 6|'), 0.0230 {I15} (at 18|'), 0.01300 {I96} (at 31|'), 0.00690 {I69} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0340 {I26} (at 6|'), 0.0220 {I15} (at 18|'), 0.01180 {I92} (at 31|'), 0.00760 {I98} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0650 {I38} (at 6|'), 0.0390 {I22} (at 18|'), 0.0217 {I14} (at 31|'), 0.0133 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0570 {I35} (at 6|'), 0.0530 {I28} (at 18|'), 0.0370 {I21} (at 31|'), 0.0260 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0100 {I21} (at 6|'), 0.0095 {I10} (at 18|'), 0.00540 {I75} (at 31|'), 0.005 {I2} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+&9/2+
level_comment:
$|s(mb/sr)=1.269 {I64} (at 6|'), 0.784 {I40} (at 18|'), 0.412 {I21} (at 31|'), 0.266 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0230 {I23} (at 6|'), 0.0160 {I11} (at 18|'), 0.012 {I1} (at 31|'), 0.0083 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0370 {I27} (at 6|'), 0.0210 {I15} (at 18|'), 0.0104 {I11} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_comment:
E$not seen in (p,d) in 2017Fr08 
$|s(mb/sr)=0.0200 {I32} (at 6|'), 0.0130 {I12} (at 18|'), 0.0100 {I11} (at 31|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0140 {I21} (at 18|'), 0.0110 {I12} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0610 {I37} (at 6|'), 0.0490 {I27} (at 18|'), 0.0250 {I16} (at 31|'), 0.0200 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0380 {I28} (at 6|'), 0.0380 {I22} (at 18|'), 0.0200 {I14} (at 31|'), 0.0190 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0300 {I25} (at 6|'), 0.0240 {I23} (at 18|'), 0.0140 {I12} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0730 {I88} (at 6|'), 0.0490 {I39} (at 18|'), 0.0180 {I71} (at 31|'), 0.0200 {I41} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.200 {I91} (at 6|'), 0.1230 {I73} (at 18|'), 0.0650 {I86} (at 31|'), 0.0410 {I45} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0400 {I28} (at 6|'), 0.0180 {I14} (at 18|'), 0.0150 {I21} (at 31|'), 0.0110 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_comment:
$|s(mb/sr)=0.501 {I26} (at 6|'), 0.300 {I34} (at 18|'), 0.1600 {I83} (at 31|'), 0.1040 {I56} (at 40|') 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_comment:
$|s(mb/sr)=0.114 {I7} (at 6|'), 0.0760 {I43} (at 18|'), 0.0390 {I28} (at 31|'), 0.0220 {I32} (at 40|') 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_comment:
$|s(mb/sr)=0.183 {I10} (at 6|'), 0.127 {I7} (at 18|'), 0.0640 {I38} (at 31|'), 0.0390 {I28} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius=4.3847 fm {I15} (2013An02) 
$Evaluated |d<r{+2}>({+92}Mo,{+98}Mo)=+0.834 fm{+2} {I1} (2013An02) 
J$no hyperfine structure observed in optical spectroscopy (quoted by 1969Fu11 as priv comm from Arroe (1951)) 
T$>1.0|*10{+14} y (1952Fr23) from neutrino-less |b|b decay 
$|b|b decay (theory): 2000Bo05, 1985Gr11 
$|D<r{+2}>({+98}Mo,{+92}Mo)=+0.811 fm{+2} {I20} (2009Ch09), laser spectroscopic technique at ISOLDE-CERN facility 
$Isotope shift({+98}Mo,{+92}Mo)=-1842 MHz {I20} (2009Ch09) 
$|D<r{+2}>({+96}Mo,{+98}Mo)=-0.210 fm{+2} {I5} (1985Go10); 0.150 fm{+2} {I12} (1978Au05); |D<r{+2}>({+98}Mo,{+100}Mo)=0.227 fm{+2} {I19} (1978Au05). Others: 1980Sc01, 1965Ch05 (muonic data); 1975Dr06 ((e,e') data) 
$Neutron occupancies deduced from neutron-removal reactions {+98}Mo(d,p),(p,d),({+3}He,|a) (2017Fr08): 0.17 {I1} for |n2s{-1/2} orbital, 3.34 {I17} for |n1d orbital, 1.13 {I6} for |n0g{-7/2} orbital, and 1.25 {I9} for |n0h{-11/2} orbital, to add to a total of 5.88 {I20}, compared to expected value of 6. 
$Proton vacancies from proton-removal reaction {+98}Mo({+3}He,d) (2017Fr08): 0.91 {I5} for |p1p orbital, 6.78 {I34} for |n0g{-9/2} orbital, to add to a total of 7.69 {I34}, compared to expected value of 8. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$L(pol t,p)=L(p,t)=0. Also E0 to 0+ seen in (t,p ce) 
T$from ce(t) in (p,p'|g) (1972Bu18). Others: 22 ns {I2} (1971AnZV), 1970Co01 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 787.4|g to 0+ 
MOMM1$from Coulomb excitation. Others: +0.97 {I7} (2001Ma17), +0.7 {I4} (1969He11) 
MOME2$from Coul. ex., value applies to constructive interference of the higher excited 2+ states as for other nuclides in this mass region. Q=+0.09 {I9} for destructive interference 
$|b{-2}(p,p')=0.180 {I14} (1992Ke07). Others: 1990Pi14, 1975Bu04, 1972Aw03, 1971Lu07 
$|b{-2}(d,d')=0.167 {I4} (2001Uk01), 0.153 (1978Wa11), 0.155 (1977Pe18) 
$|b{-2}(|a,|a')=0.142 or 0.150 (1990Bu25). Others: 1975Bu04, 1972Ma56 
$|b{-2}(Coul. ex.)=0.174 {I5} (1972Ba90) 
T$from B(E2)(from g.s.)=0.2692 {I54}, weighted average of 0.277 {I8} (2002Zi06); 0.267 {I4} (1979Pa11, 0.266 {I5} in 1976Pa13); 0.286 {I14} (1972Ba90); 0.275 {I15} (1971WaZP); 0.270 {I32} (1962Ga13); 0.26 {I4} (1962Er05); 0.270 {I32} (1958St32); 0.27 {I4} (1956Te26); and B(E2)|^=0.260 {I10} deduced from T{-1/2}=3.60 ps {I14} (Doppler broadening,1972SiZP). Final uncertainty was adjusted to 2%. Value of B(E2) is 0.2695 {I57} in 2016Pr01 evaluation, without the inclusion of 2002Zi06 value. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 1432.2|g to 0+ 
T$from B(E2) in Coul. ex. 
$|b{-2}=0.052 (1975Bu04,(p,p')); 0.046 (1977Pe18,(d,d')); 0.033 (1975Bu04,(|a,|a')); 0.037 {I2} (1972Ba90,Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
E$possibly a doublet at 1460 in (d,{+6}Li) 
J$stretched E2 722.6|g to 2+; L(p,p')=L(d,d')=4 from 0+ 
$|b{-4}=0.023 (1992Pi08,(p,p')); 0.021 (1992Pi08,(d,d')); 0.034 (1975Bu04,(|a,|a')) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 1023.7|g to 0+; L(pol t,p)=L(p,t)=2 
$|b{-2}=0.03 (1972Aw03,(p,p')); 0.029 (1977Pe18,(d,d')); 0.11 {I5} (1972Ba90,Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(pol t,p)=L(p,t)=3 
$|b{-3}(p,p')=0.210 {I16} (1992Ke07). Others: 1990Pi14, 1975Bu04, 1972Aw03, 1971Lu07 
$|b{-3}(d,d')=0.191 {I4} (2001Uk01), 0.180 (1990Pi14). Others: 1978Wa11, 1977Pe18, 1966Ki04 
$|b{-3}(|a,|a')=0.155 (1975Bu04), 0.160 {I12} (1972Ma56) 
$|b{-3}(Coul. ex.)=0.220 {I11} (1972Ba90) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$spin=3 from |g(|q) in (n,n'|g) and |g|g(|q) in (|a,2n|g); 672.5|g and 1317.4|g M1+E2 to 2+. log| {Ift}=9.0 from (5)+ is in conflict with this assignment, but I|b to this level may be overestimated (see {+98}Nb |b{+-} decay). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol t,p)=L(p,t)=2 
T$upper limit from effective half-life=0.208 ps {I49} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E$This level is defined separately from the 2333.4 level based on |g|g-coin evidence in (|a,2n|g) for the 900.85-keV transition, and Doppler shift shown by this |g ray, and not by the other |g rays from 2333.4,4+ level. Another evidence is provided by |b{+-} (51.1 min), where 900.97|g in 1984Me04 is very weak as compared to the 1546|g, and there it is placed from a 3737 level. A 900.9|g in (n,|g) E=th and a 900.96|g in (n,n'|g), where this |g is placed from the 2333.4, 4+ level, is now placed here from the 2333.2, 2+ level by evaluators. 
J$L(pol t,p)=L(p,t)=L(p,p')=2 
T$upper limit from effective half-life=0.35 ps {I12} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|g(|q) in (|a,2n|g) suggested stretched Q (E2) to 4+, also L(d,{+6}Li)=6; L(pol t,p)=2(+6) 
T$from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol t,p)=2. L(p,p')=(1) is in disagreement 
T$upper limit from effective half-life=0.326 ps {I41} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$2- suggested from cross section data in (p,p'), described as a 2-step process. In (n,|g) E=thermal, J=1 is suggested from |g|g(|q) data 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(t,p)=L(p,t)=2; |g|g(|q) in (|a,2n|g). L(p,p')=(4) is in disagreement 
T$upper limit from effective half-life=0.173 ps {I35} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L(p,p') or L(d,d')=L(t,p)=L(p,t)=2. L(d,{+6}Li)=(2+0) indicates a doublet. |g|g(|q) in (|a,2n|g) gives J=2,3 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J$|g|g(|q) in (|a,2n|g); L(t,p)=6 for a 2826 {I10} group and L(p,p') or L(d,d')=6. L(p,t)=L(|a,|a')=4 is in disagreement 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,p')=L(d,d')=4 
T$upper limit from effective half-life=0.152 ps {I14} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(t,p)=2, L(p,p') or L(d,d')=2 
T$upper limit from effective half-life=0.076 ps {I+62-42} from DSAM in (|a,2n|g) (2016Th01) 
E$doublet in (t,p) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(t,p)=L(p,t)=4; |g|g(|q) in (|a,2n|g) 
T$upper limit from effective half-life=0.44 ps {I23} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(t,p)=4 for 3044 group ; 1618.8|g to 2+ and 544.5|g to 5+ 
T$upper limit from effective half-life=0.125 ps {I21} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$L(p,t)=3; log| {Ift}=8.8 from (5)+. L(p,p')=5 for a 3060 level (1972Aw03) and J=2 for a 3067 level (1990Pi14) are in conflict 


level_energy_unit: KEV
level_spin_parity: (7-)
level_comment:
J$from |g(|q) in (|a,2n|g), |g to (5-) consistent with stretched E2, but L(p,p') or L(d,d')=(6) suggests 6+ 


level_energy_unit: KEV
level_spin_parity: (2+,3,4)
level_comment:
J$primary |g from (2+,3+) and |g to (4+). L(p,p') or L(d,d')=2 for a 3106 group suggests 2+ for 3103 and/or 3109. L(p,t)=2 for 3105.3 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$590.9|g to 5-, 705.5|g to 5+, possible 2424.1|g to 2+; log| {Ift}=6.4 from (5)+; L(p,t)=4 for 3211.6 group 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$415.5|g to 2+, 885.6|g to 6+, 1718.8|g to 4+ 
T$upper limit from effective half-life=0.152 ps {I21} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
E$this state decays to g.s. and the first excited 0+ state, indicative of two coexisting configurations are mixed in the 0+ states (2006Ru06) 
$B(M1)(2817|g, to excited 0+)/B(M1)(3551|g, to g.s.)=0.28 {I5} (2006Ru06), if J|p=1+ 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,p')=L(d,d')=4 for a 3560 {I5} group 
T$effective half-life=0.166 ps {I49} from DSAM in (|a,2n|g) (2016Th01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
E level energy held fixed in least-squares adjustment 
T$units quoted in Table 1 of 2016Th01 are erroneous, should be in ns. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$This level is defined separately from the 2333.41 level based on |g|g-coin evidence for the 900.85-keV transition, and Doppler shift shown by this |g ray, and not by the other |g rays from 2333.41,4+ level 
J$from (901|g)(1432|g)(|q) as shown in Fig. A.7 of 2016Th01; J=3 and 4 are not supported by these data 
T$effective T{-1/2}=0.35 ps {I12} from 900.85|g 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$from (1546|g)(787|g)(|q) as shown in Fig. A.8 of 2016Th01; J=2 and 3 are not supported by these data 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$from (661|g)(1023|g)(|q) (Fig. A.5 in 2016Th01); J|p=3- from a previous (p,t) experiment disagrees with the present results 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$from (996|g)(722|g)(|q) (Fig. A.6 in 2016Th01); rejecting the previously proposed assignments of (3) or (3-,4+) 


level_energy_unit: KEV
level_spin_parity: 2(+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$2016Th01 assign J=2, referring to 2003Si07 evaluation, but there this level is assigned (1-,2+). Parity is from Table 6 in 2016Th01 
T$effective T{-1/2}=0.326 ps {I41} from 1093.32|g 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Candidate for mixed symmetry state 
J$|g|g(|q) (2016Th01) favors J=2, but J=1 and 3 are not completely ruled out 
T$effective T{-1/2}=0.173 ps {I35} from 1913.60|g 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$2016Th01 assigned J|p=(5-), referring to 2003Si07 evaluation, but there this level is assigned (4+). Also (5-) requires unlikely mult=E3 for four transitions from this level to 2+ levels, thus evaluators assign (4+) 


level_energy_unit: KEV
level_spin_parity: 5+,6(+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$2016Th01 assign 5+,6,7+,8+, however, 1718.80|g to 4+ seems to exist from previous |b decay results, which makes J|p=6-,7+ and 8+ unlikely, thus the evaluators assign 5+,6(+) 
T$effective T{-1/2}=0.152 ps {I21} from 885.5|g 


level_energy_unit: KEV
level_comment:
E$ce line reported by 1984De17 
$d|s/d|W=0.055 mb/sr at 27.5|' (1988Ch29), 0.0038 mb/sr at 35|' (1980Fl03) 


level_energy_unit: KEV
level_comment:
L$from 1964Hj02 
$d|s/d|W (max)=0.71 mb/sr (1964Hj02), 0.55 mb/sr (1960Co10). d|s/d|W (at 20|', 10.1 MeV)=0.47 {I12} mb/sr (1968Ev01) 
S$2.5 (1964Hj02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
E$from 1971Lu07, 740 in 1975Bu04 
L$from 1975Bu04 
T$from ce(t) data (1972Bu18). Others: 22 ns {I2} (1971AnZV), 1970Co01 
$Strength parameter for 735 E0=0.0273 {I25} (1971AnZV) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
S$from reanalysis (by 1992Ke07) of data from 1972Aw03 or 0.175 {I13} of data from 1971Lu07. Others: 0.172 (1990Pi14), 0.154 (1975Bu04), 0.16 (1972Aw03), 0.17 (1971Lu07) 
$B(E2)(W.u.)=21.5 {I32} or 22.7 {I34} (reanalysis by 1992Ke07 of data from 1971Lu07 and 1972Aw03), 21 {I6} (1975Bu04) 


level_energy_unit: KEV
level_comment:
S$from reanalysis (by 1992Ke07) of data from 1972Aw03 or 0.205 {I26} of data from 1971Lu07. Others: 0.197 (1990Pi14), 0.20 (1972Aw03,1971Lu07), 0.19 (1975Bu04) 
$B(E3)(W.u.)=30 {I5} or 32 {I5} (reanalysis by 1992Ke07 of data from 1971Lu07 and 1972Aw03), 27 {I8} (1975Bu04) 
$|g-ray branching ratios given by 1973InZY from (p,p'|g) are: 2018|g/1230|g/259|g=20/70/10 


level_energy_unit: KEV
level_comment:
S$other: 0.07 (1972Aw03) 
$1971Lu07 give |b{-2}=|b{-4}=0.06 for a 2208 group (J|p=2+,4+) 
$B(E4)(W.u.)=3.44 {I24} (1992Pi08), 1.6 {I5} (1975Bu04); %EWSR=0.144 


level_energy_unit: KEV
level_comment:
$The analysis assumes overlapping 2333 and 2334 levels (1992Pi08) 
L,S$1971Lu07 give L=6, |b{-6}=0.11 for a 2343 group. 1972Aw03 give |b{-4}=0.09 
$B(E4)(W.u.)=8.1 {I18} (1992Pi08), 7.1 {I20} (1975Bu04); %EWSR=0.037 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E,L,S$from 1971Lu07 only. B(E4)(W.u.)=1.6. It is possible that 2450 is the composite of 2419 and 2484 levels from 1992Pi08 


level_energy_unit: KEV
level_comment:
S$1972Aw03 and 1971Lu07 give L=3 for a 2530 group. |b{-3}=0.06 (1971Lu07), 0.05 (1972Aw03). B(E3)(W.u.)=3.2 (1971Lu07), but 1992Pi08 suggest a doublet near this energy (2525 and 2537) 


level_energy_unit: KEV
level_comment:
$J|p=2- is suggested (1990Pi14) from cross section data. The population of this unnatural parity state is probably through a two-step process 


level_energy_unit: KEV
level_comment:
E$1975Bu04 report a 4+ level at 3020 with B(E4)(W.u.)=6.4 {I19} 
$B(E4)(W.u.)=1.50 {I17}, %EWSR=0.086 


level_energy_unit: KEV
level_comment:
E,L$from 1977Pe18. 
E$1978Wa11 state that the 735 level could not be observed due to the strong peak of the 787 level 


level_energy_unit: KEV
level_comment:
S$from 2001Uk01. Others: 0.153 (1978Wa11), 0.155 (1977Pe18). 1990Pi14 used |b{-2}=0.163 in analysis of data for other levels 
$B(E2)=0.56 (1977Pe18), B(E2)/|b(ISL)=1.46 {I16} (2001Uk01) 


level_energy_unit: KEV
level_comment:
S$from 2001Uk01. Others: 0.180 (1990Pi14), 0.176 (1978Wa11), 0.152 (1977Pe18), 0.24 (at 60|') or 0.15 (at 45|') (1966Ki04) 
$B(E3)/|b(ISL)=1.2 {I3} (2001Uk01) 


level_energy_unit: KEV
level_comment:
E,S$from 1999Ho27. Other: E=2574 {I5}, |b{-L}=-0.039 (1992Pi08) 
$B(E4)(W.u.)=8.3 {I10}, %EWSR=0.404 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S$0.145 {I7} (1972Ma56). 1990Bu25 deduce |b{-2}=0.142 (coupled-channel) and 0.150 from DWBA calculations 
$B(E2)(W.u.)=21 {I6} (1975Bu04), 20.7 {I20} (1972Ma56) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L$the shape of |s(|q) is consistent with L=4 but the phase is in disagreement (1975Bu04) 
$B(E4)(W.u.)=1.6 {I5} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$others: +0.478 {I42} (2001Ma17), and 0.495 {I67} (reanalysis by 2001Ma17 of 0.49 {I8} in 1978HaYJ), +0.34 {I18} (1969He11) 
T$from B(E2)(from g.s.)=0.2692 {I54} (weighted average in 2016Pr01 evaluation from 0.277 {I8} (2002Zi06); 0.267 {I4} (1979Pa11, 0.266 {I5} in 1976Pa13); 0.286 {I14} (1972Ba90); 0.275 {I15} (1971WaZP); 0.270 {I32} (1962Ga13); 0.26 {I4} (1962Er05); 0.270 {I32} (1958St32); 0.27 {I4} (1956Te26); and B(E2)|^=0.260 {I10} deduced from T{-1/2}=3.60 ps {I14} (Doppler broadening,1972SiZP). Final uncertainty was adjusted to 2%. Value of B(E2) is 0.2695 {I57} in 2016Pr01 evaluation, without the inclusion of 2002Zi06 value. 
$B(E2)(from 735,0+)=0.130 {I+14-34} (2002Zi06). Other: 0.293 {I14} (1978La17). Value from 2002Zi06 is preferred as the analysis considers a large dataset of Coulomb excitation yields, with a least-squares fit of these yields, and using some well-known spectroscopic parameters for {+98}Mo. 
$E2 matrix element (from g.s.)=+0.526 {I+8-6} (2002Zi06) 
$E2 matrix element (from 735,0+)=+0.36 {I+2-5} (2002Zi06) 
$Diagonal E2 matrix element=-0.06 {I3} (2002Zi06) 
MOME2$for constructive interference from higher states (as is the general trend for nuclides in this mass region,1976Pa13). For destructive interference Q=+0.09 {I9} (1979Pa11). Other: -0.20 {I9} or +0.16 {I9} for constructive interference and -0.18 {I9} or +0.14 {I9} for destructive interference (1976Pa13). 1978La17 do not quote measured Q but indicate that the value is |?70% of that predicted by the rotational model 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from g.s.)=0.0139 {I15} (weighted average of 0.0151 {I9} (2002Zi06), 0.0120 {I11} (1972Ba90)) and adopted branching. Other B(E2): 1962Ga13 
$B(E2)(from 735,0+)=0.063 {I7} (2002Zi06), 0.032 {I11} (1972Ba90) 
$B(E2)(from 787,2+)=0.124 {I11} (2002Zi06), 0.134 {I24} (1972Ba90) 
$E2 matrix element (from g.s.)=+0.123 {I+3-4} (2002Zi06) 
$E2 matrix element (from 735,0+)=+0.251 {I9} (2002Zi06) 
$E2 matrix element (from 787,2+)=+0.25 {I1} (2002Zi06) 
$M1 matrix element (from 787,2+)=+0.49 {I1} (2002Zi06) 
$Diagonal E2 matrix element=-0.025 {I+50-48} (2002Zi06) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 787,2+)=0.204 {I4} (2002Zi06). Other B(E2)=0.220 {I23} (1972Ba90) 
$B(E2)(from 1432,2+)=0.0180 {I25} (2002Zi06) 
$E2 matrix element (from 787,2+)=+1.01 {I1} (2002Zi06) 
$E2 matrix element (from 1432,2+)=-0.30 {I2} (2002Zi06) 
$Diagonal E2 matrix element=-43 {I+6-4} (2002Zi06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)(from 735,0+)=0.097 {I3} (2002Zi06) and adopted branching. Other B(E2)=0.10 {I9} (1972Ba90) 
$B(E2)(from g.s.)=0.00044 {I4} (2002Zi06), <0.0005 (1972Ba90) 
$B(E2)(from 787,2+)=0.0029 {I+10-5} (2002Zi06), 0.015 {I12} (1972Ba90) 
$B(E2)(from 1432,2+)=0.46 {I6} (2002Zi06) 
$B(E2)(from 1510,4+)=0.021 {I+4-3} (2002Zi06) 
$E2 matrix element (from g.s.)=-0.021 {I1} (2002Zi06) 
$E2 matrix element (from 735,0+)=+0.311 {I6} (2002Zi06) 
$E2 matrix element (from 787,2+)=+0.12 {I+2-1} (2002Zi06) 
$E2 matrix element (from 1432,2+)=-1.51 {I+8-9} (2002Zi06) 
$E2 matrix element (from 1510,4+)=-0.44 {I+5-3} (2002Zi06) 
$Diagonal E2 matrix element=-0.3 {I1} (2002Zi06) 
$M1 matrix element (from 787,2+)=+0.234 {I8} (2002Zi06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
E$level from 2002Zi06 
T$from B(E2)(from 1510,4+)=0.0391 {I12} (2002Zi06) 
$E2 matrix element (from 1510,4+)=+0.593 {I9} (2002Zi06) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=1296 {I31} 
$d|s/d|W=3.44 mb/sr {I1} at 6|', 0.885 mb/sr {I4} at 15|'. |s(6|')/|s(15|')>2 (2012ThZZ) 
$Relative strength=79.4 (2012Th07) at 6|' 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=219 {I13} 
E$others: 734.6 {I9} in 2012Th07, 737 {I10} in 1973Sh09 
$d|s/d|W=0.643 mb/sr {I5} at 6|', 0.150 mb/sr {I2} at 15|'. |s(6|')/|s(15|')>2 (2012ThZZ) 
$Relative strength=13.5 (2012Th07) at 6|' 


level_energy_unit: KEV
level_comment:
$d|s/d|W=74 {I8} 
E$other: 790 {I10} (1973Sh09) 
$d|s/d|W=0.070 mb/sr {I1} at 6|', 0.094 mb/sr {I1} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=2.4 {I4} 
E$other: 1431 {I10} (1973Sh09) 
$d|s/d|W=0.0021 mb/sr {I2} at 6|', 0.0047 mb/sr {I2} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=7.6 {I9} 
E$other: 1515 {I10} (1973Sh09) 
$d|s/d|W=0.0056 mb/sr {I3} at 6|', 0.0076 mb/sr {I4} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=6.9 {I12} 
E$other: 1768 {I10} (1973Sh09) 
$d|s/d|W=0.0039 mb/sr {I3} at 6|', 0.0140 mb/sr {I5} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=13.7 {I12} 
E$other: 1964 {I10} (1973Sh09) 
$d|s/d|W=0.0457 mb/sr {I9} at 6|', 0.0083 mb/sr {I4} at 15|' (2012ThZZ) |s(6|')/|s(15|')>2 
$Relative strength=0.883 (2012Th07) at 6|' 


level_energy_unit: KEV
level_comment:
$d|s/d|W=40.1 {I20} 
E$other: 2021 {I10} (1973Sh09) 
$d|s/d|W=0.0052 mb/sr {I4} at 6|', 0.0228 mb/sr {I7} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=0.0137 mb/sr {I5} at 6|', 0.0038 mb/sr {I4} at 15|' (2012ThZZ) |s(6|')/|s(15|')>2 
$Relative strength=0.264 (2012Th07) at 6|' 


level_energy_unit: KEV
level_comment:
$d|s/d|W=46 {I3} 
E$other: 2211 {I10} (1973Sh09) 
$d|s/d|W=0.062 mb/sr {I1} at 6|', 0.128 mb/sr {I2} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
E$other: 2227 {I10} (1973Sh09) 
$d|s/d|W=0.0136 mb/sr {I6} at 6|', 0.0207 mb/sr {I6} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=35.6 {I16} 
E$other: 2336 {I10} (1973Sh09) 
$d|s/d|W=0.033 mb/sr {I1} at 6|', 0.0682 mb/sr {I8} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=3.1 {I5} 
E$other: 2423 {I10} (1973Sh09) 
$d|s/d|W=0.0048 mb/sr {I4} at 6|', 0.0052 mb/sr {I2} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
E$other: 2504 {I10} (1973Sh09); probably corresponds to 2489+2502 in 2012Th07 
$d|s/d|W=0.0007 mb/sr {I1} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=45 {I3} 
E$other: 2579 {I10} (1973Sh09) 
$d|s/d|W=0.0486 mb/sr {I10} at 6|', 0.0508 mb/sr {I7} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=56 {I4} 
E$other: 2617 {I10} (1973Sh09) 
$d|s/d|W=0.165 mb/sr {I3} at 6|', 0.0298 mb/sr {I8} at 15|' (2012ThZZ) |s(6|')/|s(15|')>2 
$Relative strength=3.17 (2012Th07) at 6|' 


level_energy_unit: KEV
level_comment:
$d|s/d|W=16.8 {I19} 
E$other: 2708 {I10} (1973Sh09) 
$d|s/d|W=0.032 mb/sr {I1} at 6|', 0.060 mb/sr {I1} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
E$other: 2740 {I10} (1973Sh09) 
$d|s/d|W=0.0150 mb/sr {I8} at 6|', 0.0367 mb/sr {I8} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$other: 2803 {I10} (1973Sh09) 
$d|s/d|W=0.025 mb/sr {I1} at 6|', 0.0046 mb/sr {I10} at 15|' (2012ThZZ) |s(6|')/|s(15|')>2 
$Relative strength=0.49 (2012Th07) at 6|' 


level_energy_unit: KEV
level_comment:
E$other: 2840 {I10} (1973Sh09) 
$d|s/d|W=0.0022 mb/sr {I3} at 6|', 0.0058 mb/sr {I3} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
E$other: 2920 {I10} (1973Sh09) 
$d|s/d|W=0.0217 mb/sr {I9} at 6|', 0.0476 mb/sr {I10} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=17.2 {I19} 
E$other: 2978 {I10} (1973Sh09) 
$d|s/d|W=0.020 mb/sr {I2} at 6|', 0.0191 mb/sr {I6} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=7.9 {I13} 
E$other: 3025 {I10} (1973Sh09) 
$d|s/d|W=0.0032 mb/sr {I4} at 6|', 0.0029 mb/sr {I2} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=5.1 {I11} 
E$other: 3073 {I10} (1973Sh09) 
$d|s/d|W=0.0031 mb/sr {I3} at 6|', 0.0052 mb/sr {I3} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=4.3 {I5} 
E$other: 3110 {I10} (1973Sh09) 
$d|s/d|W=0.0086 mb/sr {I6} at 6|', 0.0201 mb/sr {I6} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=7.3 {I9} 
E$other: 3215 {I10} (1973Sh09) 
$d|s/d|W=0.0045 mb/sr {I6} at 6|', 0.0077 mb/sr {I4} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=19.9 {I14} 
E$other: 3270 {I10} (1973Sh09) 
$d|s/d|W=0.048 mb/sr {I1} at 6|', 0.0045 mb/sr {I3} at 15|' (2012ThZZ) |s(6|')/|s(15|')>2 
$Relative strength=0.94 (2012Th07) at 6|' 


level_energy_unit: KEV
level_comment:
E$other: 3302 {I10} (1973Sh09) 
$d|s/d|W=0.0046 mb/sr {I4} at 6|', 0.0117 mb/sr {I5} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_comment:
E$other: 3487 {I10} (1973Sh09) 
$d|s/d|W=0.0018 mb/sr {I3} at 6|', 0.0037 mb/sr {I3} at 15|' (2012ThZZ) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$wide structure at 8.8 MeV with |G=4.5 MeV reported by 1982Na06. This is interpreted as due to 2-hole states from pick up of two neutrons from 1g{-9/2}, 2p{-1/2}, 2p{-1/2} and 1f{-5/2} orbits, with d|s/d|W (12.5|')=230 |mb/sr 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
J$1+ in 2005Ru14 
$|G=0.035 eV {I3}, I{-s}=28 eVb {I2} 
E$this state decays to g.s. and the first excited 0+ state, indicative of two coexisting configurations are mixed in the 0+ states (2006Ru06) 
$B(M1)(2817|g, to excited 0+)/B(M1)(3551|g, to g.s.)=0.28 {I5} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: H
level_comment:
J atomic-beam magnetic resonance (1974Ru05); L(d,t)=0 
T$Value corrected for ionization chamber source-holder instability (2014Un01). 
T$Other values: 65.976 h {I24} (2004Wo02), 65.974 h {I14} (2004Sc04), 65.924 h {I5} (2002Un02), 65.945 h {I3} (1980Ho17), 65.924 h {I6} (1982HoZJ), 65.942 h {I12} (1983Wa26), 66.02 h {I1} (1972Em01), 66.16 h {I30} (1979Di07), 66.5 h {I2} (1971Ba28), 66.69 h {I6} (1968Re04), 65.98 h {I10} (1967Ba37), 66.7 h {I1} (1965Cr03), 67.2 h {I2} (1958Pr71), 66.96 h {I9} (1957Wr37), 66.00 h {I15} (1957Gu62). Other: 2011Ch51, 2000Ch01. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: US
level_comment:
J L(t,p)=0 on 5/2+ target. 
T from (|g,|g') (1978Ba18). Other: 16.9 |ms {I14} from pulsed particle beam experiment (1978Ho06), 13 |ms {I2} from |b|g(t) in {+99}Nb |b{+-} decay (2.56 min) (1971Ca18), 16.3 |ms {I10} from {+100}Mo(|g,n|g') (1958Du80). 
MOMM1 From g=-0.310 {I2} (average of g=-0.3110 {I14} from (|a,n|g) (liquid target) and g=-0.3092 {I10} from (d,p|g) (heated solid target)) (1978Ra21) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J L(p,d)=4; 138|g (M1) to 5/2+. 
T from centroid shift of |b|g(t) in |b{+-} decay (15 s) (1982Ba36). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$From 1997Lh01. 
J L(d,t)=2; vector analyzing power in (pol d,p) determines J=3/2. 549|g M1+E2 to 1/2+. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
J L(p,d)=5; excit; |g(|q) for 449|g is isotropic 
T from (1978Ba18). Other: 0.75 |ms {I30} in (d,p|g) (1975Di15) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J from |g(|q) for |g's to 7/2+, 5/2+ and |g from 9/2+; note, however, that L(d,t)=3 and vector-analyzing power in (pol d,p) suggest J|p=5/2- 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J 656|g E1 to 5/2+ note, also, that L(d,t)=3 and vector analyzing power in (pol d,t) suggest J|p=7/2-. See 1988Du02 for discussion of J|p 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J 433|g M1+E2 to 5/2+, 697|g E2 to 3/2+; note, however, that L(d,t)=3 and vector analyzing power in (pol d,p) suggest J|p=5/2- 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$From logft=5.9 in |b{+-} feeding in {+99}Nb (15.0 s) |b{+-} decay. 
J |g to 7/2(+) is |DJ=0, D+Q; excit 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J log| {Ift}=6.6, log| {If{+1u}t}=7.7 from 1/2-. L(p,d)=1. L(d,t)=3 is probably in error. |g ray to (5/2+) states. 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_comment:
J log| {Ift}=6.3, log| {If{+1u}t}=7.2 from 1/2-. J|p=3/2+ if level is identical to L(p,d)=2 level observed at 2330 keV {I10}. 


level_energy_unit: KEV
level_comment:
J doublet. The lower energy peak has L=5, higher L=3 and J=5/2 from vector analyzing power measurements. No spin assignment is given for the L=5 state. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=2.98 {I15} (at 6|'), 0.307 {I16} (at 18|'), 0.406 {I21} (at 31|'), 0.248 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.133 {I7} (at 6|'), 0.1560 {I84} (at 18|'), 0.321 {I16} (at 31|'), 0.1500 {I78} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.1200 {I63} (at 6|'), 0.350 {I18} (at 18|'), 0.0760 {I43} (at 31|'), 0.0740 {I38} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=3.46 {I17} (at 6|'), 0.327 {I17} (at 18|'), 0.474 {I24} (at 31|'), 0.248 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.486 {I25} (at 6|'), 1.177 {I60} (at 18|'), 0.210 {I11} (at 31|'), 0.287 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.259 {I13} (at 6|'), 0.962 {I49} (at 18|'), 0.1830 {I94} (at 31|'), 0.215 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.0450 {I25} (at 6|'), 0.0640 {I38} (at 18|'), 0.1200 {I63} (at 31|'), 0.134 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0227 {I15} (at 6|'), 0.0230 {I15} (at 18|'), 0.0420 {I23} (at 31|'), 0.0245 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0460 {I25} (at 6|'), 0.0890 {I49} (at 18|'), 0.0590 {I31} (at 31|'), 0.0375 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0600 {I32} (at 6|'), 0.226 {I12} (at 18|'), 0.0480 {I26} (at 31|'), 0.0490 {I27} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0159 {I11} (at 6|'), 0.0188 {I13} (at 18|'), 0.0380 {I22} (at 31|'), 0.0205 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.070 {I4} (at 6|'), 0.1570 {I84} (at 18|'), 0.0320 {I19} (at 31|'), 0.0430 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+&9/2+
level_comment:
$|s(mb/sr)=0.943 {I47} (at 6|'), 0.1580 {I82} (at 18|'), 0.266 {I14} (at 31|'), 0.220 {I11} (at 40|') 
S$for L=0 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.1360 {I71} (at 6|'), 0.476 {I24} (at 18|'), 0.1030 {I53} (at 31|'), 0.1170 {I59} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.00220 {I23} (at 6|'), 0.00210 {I23} (at 18|'), 0.00490 {I39} (at 31|'), 0.00300 {I25} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.1500 {I78} (at 6|'), 0.0460 {I25} (at 18|'), 0.0360 {I19} (at 31|'), 0.01550 {I92} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0205 {I13} (at 6|'), 0.0168 {I10} (at 18|'), 0.0306 {I17} (at 31|'), 0.01260 {I81} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.00670 {I52} (at 6|'), 0.01410 {I93} (at 18|'), 0.00320 {I34} (at 31|'), 0.00380 {I36} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0089 {I6} (at 6|'), 0.0090 {I6} (at 18|'), 0.0188 {I11} (at 31|'), 0.01360 {I79} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0880 {I45} (at 6|'), 0.236 {I12} (at 18|'), 0.0497 {I27} (at 31|'), 0.0670 {I35} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0400 {I22} (at 6|'), 0.0820 {I42} (at 18|'), 0.0206 {I12} (at 31|'), 0.0232 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.01090 {I68} (at 6|'), 0.00100 {I21} (at 18|'), 0.00160 {I22} (at 31|'), 0.00060 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0590 {I31} (at 6|'), 0.00640 {I51} (at 18|'), 0.0089 {I6} (at 31|'), 0.00310 {I25} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.01110 {I82} (at 6|'), 0.0080 {I11} (at 18|'), 0.0226 {I13} (at 31|'), 0.0210 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.00810 {I72} (at 6|'), 0.01220 {I86} (at 18|'), 0.00400 {I36} (at 31|'), 0.00460 {I46} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0219 {I14} (at 6|'), 0.0199 {I13} (at 18|'), 0.0400 {I22} (at 31|'), 0.0400 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0510 {I28} (at 6|'), 0.1800 {I92} (at 18|'), 0.0360 {I21} (at 31|'), 0.0510 {I28} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0750 {I43} (at 6|'), 0.331 {I17} (at 18|'), 0.0700 {I37} (at 31|'), 0.0940 {I51} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0290 {I18} (at 6|'), 0.0710 {I41} (at 18|'), 0.01040 {I72} (at 31|'), 0.0210 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.00460 {I74} (at 6|'), 0.0212 {I13} (at 18|'), 0.00560 {I57} (at 31|'), 0.00940 {I76} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0065 {I6} (at 6|'), 0.0154 {I11} (at 18|'), 0.0222 {I14} (at 31|'), 0.0320 {I19} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_comment:
$|s(mb/sr)=0.00490 {I56} (at 6|'), 0.00740 {I62} (at 18|'), 0.00820 {I73} (at 31|'), 0.00500 {I56} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0209 {I14} (at 6|'), 0.0820 {I46} (at 18|'), 0.0166 {I12} (at 31|'), 0.0220 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0204 {I14} (at 6|'), 0.0840 {I47} (at 18|'), 0.01370 {I98} (at 31|'), 0.0230 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.00390 {I45} (at 6|'), 0.0145 {I10} (at 18|'), 0.0080 {I11} (at 31|'), 0.0060 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.00230 {I42} (at 6|'), 0.0280 {I17} (at 18|'), 0.00410 {I45} (at 31|'), 0.00620 {I68} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_comment:
$|s(mb/sr)=0.00280 {I42} (at 6|'), 0.00510 {I65} (at 18|'), 0.00580 {I58} (at 31|'), 0.00430 {I55} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0144 {I11} (at 6|'), 0.0420 {I23} (at 18|'), 0.00630 {I59} (at 31|'), 0.0104 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.1740 {I92} (at 6|'), 0.0143 {I10} (at 18|'), 0.0172 {I12} (at 31|'), 0.00720 {I79} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.209 {I11} (at 6|'), 0.1720 {I91} (at 18|'), 0.0650 {I34} (at 31|'), 0.0470 {I31} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.1100 {I59} (at 6|'), 0.0211 {I13} (at 18|'), 0.0205 {I13} (at 31|'), 0.00630 {I95} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0143 {I10} (at 6|'), 0.0670 {I35} (at 18|'), 0.0189 {I11} (at 31|'), 0.0180 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0180 {I11} (at 6|'), 0.0230 {I13} (at 18|'), 0.00670 {I45} (at 31|'), 0.00830 {I65} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.01270 {I81} (at 6|'), 0.0220 {I13} (at 18|'), 0.01410 {I81} (at 31|'), 0.01320 {I96} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.01360 {I91} (at 6|'), 0.056 {I3} (at 18|'), 0.01110 {I69} (at 31|'), 0.0156 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0650 {I34} (at 6|'), 0.0183 {I12} (at 18|'), 0.0177 {I10} (at 31|'), 0.00510 {I65} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.00350 {I53} (at 6|'), 0.01240 {I86} (at 18|'), 0.0088 {I6} (at 31|'), 0.00760 {I89} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.080 {I11} (at 6|'), 0.073 {I7} (at 18|'), 0.1350 {I71} (at 31|'), 0.1060 {I61} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.150 {I13} (at 6|'), 0.1280 {I88} (at 18|'), 0.1245 {I62} (at 31|'), 0.1100 {I59} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.497 {I25} (at 6|'), 0.422 {I21} (at 18|'), 0.1080 {I55} (at 31|'), 0.1170 {I62} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0090 {I11} (at 6|'), 0.0150 {I13} (at 18|'), 0.002 {I1} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0790 {I44} (at 6|'), 0.0510 {I33} (at 18|'), 0.0320 {I19} (at 31|'), 0.0270 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0540 {I34} (at 6|'), 0.0410 {I23} (at 18|'), 0.0240 {I16} (at 31|'), 0.0200 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0140 {I12} (at 6|'), 0.0240 {I16} (at 18|'), 0.0120 {I12} (at 31|'), 0.0140 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0080 {I11} (at 6|'), 0.0180 {I14} (at 18|'), 0.0070 {I11} (at 31|'), 0.0110 {I12} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0180 {I14} (at 6|'), 0.0190 {I14} (at 18|'), 0.005 {I1} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.127 {I7} (at 6|'), 0.061 {I5} (at 18|'), 0.0260 {I17} (at 31|'), 0.0210 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0170 {I13} (at 6|'), 0.0280 {I17} (at 18|'), 0.0070 {I11} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.289 {I15} (at 6|'), 0.319 {I17} (at 18|'), 0.0830 {I43} (at 31|'), 0.0960 {I57} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0230 {I15} (at 18|'), 0.00640 {I68} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.1360 {I74} (at 6|'), 0.1090 {I58} (at 18|'), 0.0283 {I17} (at 31|'), 0.0410 {I29} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0080 {I11} (at 6|'), 0.0110 {I12} (at 18|'), 0.0160 {I13} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0270 {I17} (at 6|'), 0.0210 {I15} (at 18|'), 0.0100 {I11} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.1360 {I71} (at 6|'), 0.1190 {I63} (at 18|'), 0.0266 {I16} (at 31|'), 0.0340 {I26} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0580 {I35} (at 6|'), 0.0160 {I13} (at 18|'), 0.0178 {I11} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0310 {I25} (at 6|'), 0.0630 {I37} (at 18|'), 0.00830 {I73} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0620 {I43} (at 6|'), 0.0280 {I25} (at 18|'), 0.0231 {I15} (at 31|'), 0.0260 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0290 {I25} (at 6|'), 0.0390 {I28} (at 18|'), 0.0150 {I13} (at 31|'), 0.0100 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0640 {I38} (at 6|'), 0.080 {I5} (at 18|'), 0.0240 {I16} (at 31|'), 0.0260 {I24} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0550 {I34} (at 18|'), 0.0170 {I13} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0350 {I27} (at 6|'), 0.0510 {I48} (at 18|'), 0.0160 {I22} (at 31|'), 0.0190 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0190 {I14} (at 6|'), 0.0280 {I25} (at 18|'), 0.01180 {I92} (at 31|'), 0.0140 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0190 {I14} (at 18|'), 0.00680 {I69} (at 31|'), 0.00640 {I96} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.034 {I2} (at 6|'), 0.0270 {I17} (at 18|'), 0.0191 {I13} (at 31|'), 0.0160 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.1040 {I56} (at 6|'), 0.1100 {I59} (at 18|'), 0.0280 {I17} (at 31|'), 0.0360 {I27} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.069 {I4} (at 6|'), 0.0950 {I52} (at 18|'), 0.0246 {I15} (at 31|'), 0.0290 {I25} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0310 {I19} (at 6|'), 0.0400 {I22} (at 18|'), 0.0110 {I12} (at 31|'), 0.0120 {I21} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0160 {I13} (at 6|'), 0.0220 {I15} (at 18|'), 0.0100 {I11} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0400 {I22} (at 6|'), 0.0400 {I22} (at 18|'), 0.0090 {I11} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0240 {I16} (at 6|'), 0.0100 {I11} (at 18|'), 0.0130 {I12} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0650 {I38} (at 6|'), 0.0750 {I43} (at 18|'), 0.0310 {I19} (at 31|'), 0.0300 {I18} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0330 {I19} (at 6|'), 0.0460 {I25} (at 18|'), 0.0370 {I21} (at 31|'), 0.0410 {I29} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.497 {I25} (at 6|'), 0.458 {I23} (at 18|'), 0.351 {I18} (at 31|'), 0.217 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.840 {I43} (at 6|'), 0.444 {I23} (at 18|'), 0.248 {I13} (at 31|'), 0.1620 {I84} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0260 {I17} (at 6|'), 0.0215 {I14} (at 18|'), 0.01500 {I96} (at 31|'), 0.01330 {I97} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0610 {I37} (at 6|'), 0.0580 {I31} (at 18|'), 0.0450 {I25} (at 31|'), 0.0310 {I19} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0860 {I48} (at 6|'), 0.0730 {I38} (at 18|'), 0.057 {I3} (at 31|'), 0.0360 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+&11/2-
level_comment:
$|s(mb/sr)=1.18 {I6} (at 6|'), 0.677 {I34} (at 18|'), 0.385 {I20} (at 31|'), 0.225 {I12} (at 40|') 
E,L$unresolved doublet of 683 (L=5) and 697 (L=4) but resolved in (p,d) in 2017Fr08. 
S$for L=5, deduced from relative C{+2}S from (p,d); 0.203 {I10} fo L=4 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+&7/2-
level_comment:
$|s(mb/sr)=0.0380 {I28} (at 6|'), 0.0130 {I12} (at 18|'), 0.0155 {I11} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0150 {I13} (at 6|'), 0.0120 {I12} (at 18|'), 0.0119 {I10} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.1140 {I61} (at 6|'), 0.0530 {I28} (at 18|'), 0.0370 {I21} (at 31|'), 0.0240 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+&9/2+
level_comment:
$|s(mb/sr)=0.267 {I14} (at 6|'), 0.1680 {I86} (at 18|'), 0.0900 {I49} (at 31|'), 0.0660 {I39} (at 40|') 
E$there are potentially small contributions from a weak, but unresolved L=0 transition (2017Fr08) 
S$for L=4 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0390 {I28} (at 6|'), 0.0400 {I22} (at 18|'), 0.0277 {I17} (at 31|'), 0.0165 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0160 {I13} (at 6|'), 0.00740 {I62} (at 18|'), 0.00450 {I46} (at 31|'), 0.00350 {I72} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.1520 {I79} (at 6|'), 0.0850 {I44} (at 18|'), 0.0490 {I27} (at 31|'), 0.0300 {I18} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0750 {I43} (at 6|'), 0.045 {I3} (at 18|'), 0.0240 {I16} (at 31|'), 0.0170 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0570 {I35} (at 6|'), 0.044 {I3} (at 18|'), 0.0300 {I18} (at 31|'), 0.0180 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0140 {I12} (at 6|'), 0.0130 {I12} (at 18|'), 0.00740 {I79} (at 31|'), 0.00470 {I83} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0320 {I19} (at 6|'), 0.0190 {I14} (at 18|'), 0.0110 {I12} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0110 {I12} (at 6|'), 0.0070 {I11} (at 18|'), 0.005 {I1} (at 31|'), 0.003 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0590 {I36} (at 6|'), 0.0360 {I21} (at 18|'), 0.0220 {I15} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0230 {I23} (at 6|'), 0.0150 {I21} (at 18|'), 0.0060 {I11} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.1370 {I75} (at 6|'), 0.0930 {I51} (at 18|'), 0.0540 {I29} (at 31|'), 0.0350 {I27} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.1020 {I59} (at 6|'), 0.0820 {I46} (at 18|'), 0.0500 {I32} (at 31|'), 0.0300 {I25} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.316 {I16} (at 6|'), 0.209 {I11} (at 18|'), 0.112 {I6} (at 31|'), 0.0580 {I35} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0330 {I26} (at 6|'), 0.0260 {I24} (at 18|'), 0.0170 {I13} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.257 {I14} (at 6|'), 0.1490 {I77} (at 18|'), 0.0790 {I44} (at 31|'), 0.0420 {I29} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0200 {I14} (at 6|'), 0.0130 {I12} (at 18|'), 0.0060 {I11} (at 31|'), 0.003 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0270 {I33} (at 6|'), 0.0170 {I22} (at 18|'), 0.0140 {I12} (at 31|'), 0.0120 {I12} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0760 {I63} (at 6|'), 0.0500 {I32} (at 18|'), 0.0290 {I25} (at 31|'), 0.0160 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0590 {I42} (at 6|'), 0.0360 {I27} (at 18|'), 0.0190 {I14} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=1.124 {I57} (at 6|'), 0.681 {I34} (at 18|'), 0.370 {I19} (at 31|'), 0.237 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0860 {I53} (at 6|'), 0.0600 {I36} (at 18|'), 0.0410 {I23} (at 31|'), 0.0260 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0590 {I85} (at 6|'), 0.0390 {I36} (at 18|'), 0.0170 {I31} (at 31|'), 0.0100 {I31} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0250 {I61} (at 6|'), 0.0170 {I31} (at 18|'), 0.0070 {I11} (at 31|'), 0.004 {I2} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0470 {I31} (at 6|'), 0.0360 {I27} (at 18|'), 0.0230 {I23} (at 31|'), 0.0150 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0390 {I28} (at 6|'), 0.0310 {I25} (at 18|'), 0.0170 {I13} (at 31|'), 0.0090 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0190 {I22} (at 6|'), 0.0120 {I12} (at 18|'), 0.0120 {I12} (at 31|'), 0.004 {I2} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.045 {I3} (at 6|'), 0.0430 {I29} (at 18|'), 0.0220 {I15} (at 31|'), 0.0190 {I32} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0780 {I56} (at 6|'), 0.0360 {I27} (at 18|'), 0.0180 {I14} (at 31|'), 0.0160 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0700 {I46} (at 6|'), 0.0380 {I28} (at 18|'), 0.0200 {I14} (at 31|'), 0.0210 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$from |g(t) measurement (2021Da15). 
MOMM1$from TDPAD measurements with measured {Ig}=-0.114 {I3}{-stat}{I2}{-syst} (2021Da15). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=9.6 {I5} (at 8|'), 1.03 {I5} (at 18|'), 3.26 {I16} (at 27|'), 3.23 {I16} (at 33|'), 1.37 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.86 {I5} (at 8|'), 2.91 {I15} (at 18|'), 1.87 {I10} (at 27|'), 0.92 {I5} (at 33|'), 0.77 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.196 {I12} (at 8|'), 0.305 {I16} (at 18|'), 0.560 {I28} (at 27|'), 0.74 {I4} (at 33|'), 0.443 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.376 {I21} (at 8|'), 0.90 {I5} (at 18|'), 0.513 {I26} (at 27|'), 0.263 {I14} (at 33|'), 0.250 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.92 {I5} (at 8|'), 0.113 {I6} (at 18|'), 0.312 {I16} (at 27|'), 0.330 {I17} (at 33|'), 0.144 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=1.50 {I8} (at 8|'), 3.72 {I19} (at 18|'), 2.11 {I11} (at 27|'), 1.16 {I6} (at 33|'), 1.10 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.084 {I7} (at 8|'), 0.229 {I12} (at 18|'), 0.154 {I8} (at 27|'), 0.083 {I5} (at 33|'), 0.068 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.050 {I5} (at 8|'), 0.081 {I5} (at 18|'), 0.057 {I3} (at 27|'), 0.0280 {I17} (at 33|'), 0.0287 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.065 {I5} (at 8|'), 0.133 {I7} (at 18|'), 0.232 {I12} (at 27|'), 0.297 {I15} (at 33|'), 0.301 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0130 {I21} (at 8|'), 0.0177 {I11} (at 18|'), 0.0440 {I24} (at 27|'), 0.0390 {I22} (at 33|'), 0.0221 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$|s(mb/sr)=0.192 {I12} (at 8|'), 0.278 {I14} (at 18|'), 0.299 {I15} (at 27|'), 0.246 {I13} (at 33|'), 0.130 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.086 {I7} (at 8|'), 0.234 {I12} (at 18|'), 0.145 {I8} (at 27|'), 0.103 {I6} (at 33|'), 0.079 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.440 {I24} (at 8|'), 1.03 {I5} (at 18|'), 0.570 {I29} (at 27|'), 0.288 {I15} (at 33|'), 0.279 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.370 {I21} (at 8|'), 0.058 {I4} (at 18|'), 0.147 {I8} (at 27|'), 0.157 {I8} (at 33|'), 0.094 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.20 {I7} (at 8|'), 0.656 {I33} (at 18|'), 0.465 {I24} (at 27|'), 0.264 {I14} (at 33|'), 0.178 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.183 {I12} (at 8|'), 0.172 {I9} (at 18|'), 0.088 {I5} (at 27|'), 0.100 {I21} (at 33|'), 0.0526 {I28} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0130 {I21} (at 8|'), 0.0182 {I13} (at 18|'), 0.0310 {I19} (at 27|'), 0.0430 {I24} (at 33|'), 0.0261 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.03 {I1} (at 8|'), 0.056 {I3} (at 18|'), 0.0410 {I23} (at 27|'), 0.0285 {I17} (at 33|'), 0.0243 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0110 {I21} (at 8|'), 0.0141 {I10} (at 27|'), 0.0105 {I8} (at 33|'), 0.0056 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.169 {I10} (at 8|'), 0.072 {I4} (at 27|'), 0.076 {I4} (at 33|'), 0.0362 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 8|'), 0.0350 {I19} (at 18|'), 0.0127 {I8} (at 33|'), 0.0092 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0090 {I11} (at 8|'), 0.0165 {I10} (at 18|'), 0.0298 {I17} (at 33|'), 0.0198 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.044 {I3} (at 8|'), 0.119 {I6} (at 18|'), 0.082 {I7} (at 27|'), 0.0377 {I21} (at 33|'), 0.0350 {I19} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0110 {I21} (at 8|'), 0.0160 {I13} (at 18|'), 0.0210 {I15} (at 27|'), 0.0127 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.074 {I6} (at 8|'), 0.123 {I7} (at 18|'), 0.196 {I10} (at 27|'), 0.240 {I13} (at 33|'), 0.246 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.077 {I6} (at 8|'), 0.173 {I9} (at 18|'), 0.098 {I5} (at 27|'), 0.0530 {I28} (at 33|'), 0.0474 {I25} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.096 {I7} (at 8|'), 0.225 {I12} (at 18|'), 0.134 {I7} (at 27|'), 0.074 {I4} (at 33|'), 0.0640 {I34} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0140 {I31} (at 8|'), 0.0280 {I17} (at 18|'), 0.0210 {I23} (at 27|'), 0.0116 {I10} (at 33|'), 0.0087 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.055 {I5} (at 8|'), 0.0260 {I17} (at 18|'), 0.061 {I4} (at 27|'), 0.072 {I4} (at 33|'), 0.034 {I2} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0120 {I21} (at 8|'), 0.0161 {I12} (at 18|'), 0.0170 {I13} (at 27|'), 0.0200 {I14} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.03 {I1} (at 8|'), 0.141 {I8} (at 18|'), 0.096 {I6} (at 27|'), 0.100 {I31} (at 33|'), 0.037 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.180 {I31} (at 8|'), 0.212 {I12} (at 18|'), 0.273 {I14} (at 27|'), 0.19 {I1} (at 33|'), 0.084 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.080 {I11} (at 8|'), 0.0430 {I29} (at 27|'), 0.0480 {I26} (at 33|'), 0.0100 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.170 {I11} (at 8|'), 0.0300 {I18} (at 18|'), 0.0540 {I29} (at 33|'), 0.0330 {I18} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0100 {I21} (at 8|'), 0.0310 {I19} (at 18|'), 0.0270 {I17} (at 33|'), 0.0220 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.046 {I5} (at 8|'), 0.080 {I5} (at 18|'), 0.0530 {I28} (at 33|'), 0.0322 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.099 {I8} (at 8|'), 0.102 {I6} (at 18|'), 0.0500 {I32} (at 33|'), 0.0420 {I23} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.030 {I4} (at 8|'), 0.0410 {I23} (at 18|'), 0.011 {I7} (at 27|'), 0.0140 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.059 {I10} (at 8|'), 0.135 {I7} (at 18|'), 0.079 {I5} (at 27|'), 0.0360 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.170 {I13} (at 8|'), 0.0250 {I24} (at 18|'), 0.069 {I5} (at 27|'), 0.0480 {I26} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.319 {I18} (at 8|'), 0.663 {I34} (at 18|'), 0.398 {I20} (at 27|'), 0.196 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.110 {I8} (at 8|'), 0.202 {I11} (at 18|'), 0.118 {I6} (at 27|'), 0.051 {I6} (at 33|'), 0.0610 {I32} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0190 {I32} (at 8|'), 0.0420 {I23} (at 18|'), 0.0490 {I32} (at 27|'), 0.0350 {I27} (at 33|'), 0.0292 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.033 {I4} (at 8|'), 0.0290 {I18} (at 18|'), 0.0210 {I15} (at 27|'), 0.0190 {I22} (at 33|'), 0.0097 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.018 {I9} (at 8|'), 0.0320 {I26} (at 18|'), 0.0210 {I23} (at 27|'), 0.0090 {I11} (at 33|'), 0.0092 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.014 {I8} (at 8|'), 0.0320 {I26} (at 18|'), 0.0410 {I29} (at 27|'), 0.0460 {I31} (at 33|'), 0.0480 {I26} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.200 {I22} (at 8|'), 0.111 {I6} (at 18|'), 0.110 {I6} (at 27|'), 0.091 {I5} (at 33|'), 0.0410 {I23} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.087 {I6} (at 8|'), 0.083 {I5} (at 18|'), 0.114 {I6} (at 27|'), 0.085 {I4} (at 33|'), 0.081 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.040 {I4} (at 8|'), 0.071 {I5} (at 18|'), 0.0360 {I21} (at 27|'), 0.0169 {I10} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.032 {I9} (at 8|'), 0.0189 {I12} (at 18|'), 0.0260 {I17} (at 27|'), 0.0304 {I17} (at 33|'), 0.012 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.043 {I5} (at 8|'), 0.0550 {I34} (at 18|'), 0.0190 {I14} (at 27|'), 0.0356 {I20} (at 33|'), 0.0274 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.044 {I4} (at 8|'), 0.0170 {I22} (at 18|'), 0.0200 {I14} (at 27|'), 0.0357 {I20} (at 33|'), 0.0206 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.046 {I4} (at 8|'), 0.084 {I5} (at 18|'), 0.069 {I4} (at 27|'), 0.0494 {I26} (at 33|'), 0.0385 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.051 {I4} (at 8|'), 0.066 {I4} (at 18|'), 0.0380 {I28} (at 27|'), 0.0412 {I22} (at 33|'), 0.0323 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.054 {I6} (at 8|'), 0.066 {I4} (at 18|'), 0.0250 {I24} (at 27|'), 0.0300 {I18} (at 33|'), 0.0199 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.15 {I1} (at 8|'), 0.196 {I10} (at 18|'), 0.150 {I8} (at 27|'), 0.095 {I5} (at 33|'), 0.087 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.046 {I5} (at 8|'), 0.034 {I2} (at 18|'), 0.0190 {I22} (at 27|'), 0.0170 {I31} (at 33|'), 0.0198 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.077 {I7} (at 8|'), 0.0540 {I34} (at 27|'), 0.0520 {I33} (at 33|'), 0.0310 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.086 {I7} (at 8|'), 0.076 {I10} (at 18|'), 0.069 {I5} (at 33|'), 0.0410 {I23} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.036 {I6} (at 8|'), 0.044 {I6} (at 18|'), 0.0380 {I28} (at 33|'), 0.0210 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.071 {I7} (at 8|'), 0.063 {I4} (at 18|'), 0.0390 {I28} (at 33|'), 0.0410 {I29} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.031 {I5} (at 8|'), 0.0300 {I25} (at 18|'), 0.0300 {I34} (at 27|'), 0.0160 {I13} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.032 {I4} (at 8|'), 0.0370 {I21} (at 18|'), 0.0230 {I23} (at 27|'), 0.0230 {I32} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.050 {I5} (at 8|'), 0.062 {I4} (at 18|'), 0.0190 {I22} (at 27|'), 0.0310 {I25} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.036 {I4} (at 8|'), 0.0250 {I16} (at 18|'), 0.0110 {I12} (at 27|'), 0.0140 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0180 {I31} (at 8|'), 0.0400 {I22} (at 18|'), 0.0320 {I19} (at 27|'), 0.0130 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.065 {I6} (at 8|'), 0.071 {I4} (at 18|'), 0.0520 {I33} (at 27|'), 0.0240 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.028 {I4} (at 8|'), 0.0400 {I22} (at 18|'), 0.0260 {I17} (at 27|'), 0.0060 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.043 {I5} (at 8|'), 0.0230 {I15} (at 18|'), 0.0190 {I14} (at 27|'), 0.004 {I1} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.035 {I4} (at 8|'), 0.067 {I4} (at 18|'), 0.0510 {I33} (at 27|'), 0.0160 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.048 {I6} (at 8|'), 0.0420 {I23} (at 18|'), 0.0310 {I25} (at 27|'), 0.0320 {I19} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.052 {I6} (at 8|'), 0.061 {I4} (at 18|'), 0.0470 {I31} (at 27|'), 0.0450 {I25} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.062 {I6} (at 8|'), 0.0540 {I34} (at 18|'), 0.0400 {I28} (at 27|'), 0.0450 {I25} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.123 {I9} (at 8|'), 0.132 {I7} (at 18|'), 0.097 {I5} (at 27|'), 0.079 {I5} (at 33|'), 0.0390 {I28} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.055 {I6} (at 8|'), 0.068 {I4} (at 18|'), 0.0550 {I34} (at 27|'), 0.0360 {I21} (at 33|'), 0.0170 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.069 {I7} (at 8|'), 0.067 {I4} (at 18|'), 0.0530 {I33} (at 27|'), 0.0430 {I24} (at 33|'), 0.0280 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.033 {I4} (at 8|'), 0.0560 {I35} (at 18|'), 0.045 {I3} (at 27|'), 0.0310 {I25} (at 33|'), 0.0220 {I23} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.068 {I6} (at 8|'), 0.092 {I5} (at 18|'), 0.074 {I4} (at 27|'), 0.073 {I4} (at 33|'), 0.062 {I4} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.089 {I8} (at 8|'), 0.115 {I6} (at 18|'), 0.095 {I5} (at 27|'), 0.075 {I4} (at 33|'), 0.072 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
J$measurement by optical method (1951Ar29) 
T$T{-1/2}=7.01|*10{+18} y {I+21-17} for 2|n|b|b decay to {+100}Ru g.s. obtained from weighted average of 7.05|*10{+18} y {I+21-17} (2020Ar09, CUPID-Mo, Modane, earlier value of 6.90|*10{+18} y {I40} in 2017Ar18); 6.81|*10{+18} y {I1}(stat) {I+38-40}(syst) (2019Ar04, earlier value of 7.17|*10{+18} y {I54} in 2011Fl06, NEMO-3, see also previous papers e.g. 2005Ar27); 7.15|*10{+18} y {I76} (2014Ca46, NIIC, Russia); 7.2|*10{+18} y {I20} (2001As06, Gran Sasso, see also 2002As05,2001As05 and previous papers); 7.6|*10{+18} y {I26} (1997Al02, Silver mine at Osburn, Idaho); 6.82|*10{+18} y {I86} (1997De40, Valve house, Hoover Dam, USA; note that value listed in 2015Ba11 evaluation from 1997De40 is for {+150}Nd 2|n|b|b decay, not for {+100}Mo). Half-life in 2015Ba11 evaluation is: 7.1|*10{+18} y {I4}, where some of the original values taken from literature seemed erroneous. About 1% 2|n|b|b decay is found to proceed to the 1130, 0+ level in {+100}Ru with weighted averaged partial T{-1/2}=6.9|*10{+20} y {I9}, obtained from 7.5|*10{+20} y {I9} (2014Ar08, NEMO-3); 6.9|*10{+20} y {I12} (2010Be34, ARMONIA, Gran Sasso); 6.0|*10{+20} y {I+20-13} (2009Ki04, TUNL, ITEP); 6.1|*10{+20} y {I+18-11} (1995Ba29, Soudan mine, Minnesota). Value is 6.7|*10{+20} y {I+5-4} in 2015Ba11 evaluation which included somewhat different set of measurements. Note that in all cases, evaluators combined statistical and systematic uncertainties in quadrature. Decays to other excited states of {+100}Ru make almost no contribution, as suggested by recent measurements by 2014Ar08 (NEMO-3) and 2009Ki04 (TUNL, ITEP). 
$2019TrZZ superseded by 2019Ar04 
$Evaluated rms charge radius <r{+2}>{+1/2}=4.4468 fm {I25} (2013An02) 
$Evaluated |dr{+2}({+100}Mo,{+92}Mo)=+1.177 fm{+2} {I1} (2013An02) 
$Measured |d<r{+2}>({+100}Mo,{+92}Mo)=+1.139 fm{+2} {I39} (2009Ch09); uncertainty is systematic. Laser spectroscopy technique at JYFL 
$Measured Isotope shift({+100}Mo,{+92}Mo)=-2645 MHz {I33} (2009Ch09); total uncertainty is given; statistical uncertainty is 1. Laser spectroscopy technique at JYFL 
$|d<r{+2}>({+96}Mo-{+100}Mo)=-0.525 fm{+2} {I6} (1985Go10) 
$From experimental studies of one-neutron removal reactions (d,p), (p,d), ({+3}He,|a) and proton removing reaction ({+3}He,d) on {+100}Mo target, 2017Fr08 deduced following values of neutron and proton vacancies in the g.s. of {+100}Mo: 0.33 {I2} for |n2s{-1/2}, 3.40 {I7} for |n1d, 2.48 {I19} for |n0g{-7/2}, 1.89 {I13} for |n0h{-11/2}, 1.49 {I7} for |p1p, 0.47 {I2} for |p0f{-5/2} and 5.94 {I30} for |p0g{-9/2} orbitals, with a total vacancy of 8.09 {I29} for neutrons and 7.89 {I31} for protons, compared with expected value of 8 for each. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,p')=L(|a,|a')=2 from 0+ 
T$weighted average of 13.6 ps {I7} (recoil-distance Doppler-shift method in Coul. ex.,1975Bo39), and half-lives of 12.56 ps {I22} (1976Pa13), 12.2 ps {I6} (1972Ba90), 10.5 ps {I12} (1962Ga13), 10.2 ps {I16} (1962Er05), 10.5 ps {I11} (1958St32) and 9.7 ps {I15} (1956Te26), deduced from respective B(E2)|^ values determined in the measurement of Coulomb excitation yields. Others: 13.9 ps {I4}, deduced by evaluators from B(E2) in 2012Wr03, where 13.6 ps {I7} (1975Bo39) was used as input data in their GOSIA analysis of Coul. Ex. data; 10.3 ps {I+51-35} (DSAM in {+9}Be({+109}Tc,X|g), 2017Ra05); 16 ps {I5} (2013RuZX, |g|g(t) fast-timing technique in study of prompt |g rays from neutron-induced fission of actinides). 2016Pr01 evaluation gives T{-1/2}=12.1 ps {I5}, from the same original data as here but using |?5% uncertainty in the value given by 1976Pa13. 
MOMM1$from g-factor=+0.471 {I33}, value adopted by 2001Ma17 from weighted average of g=+0.515 {I42} (transient-field technique,2001Ma17) and g=+0.404 {I52} (original g=+0.43 {I6} from 1978HaYJ re-evaluated by 2001Ma17 for consistent field parameters). Other: 0.34 {I18} (IMPAC method, 1969He11, using T{-1/2}(536 level)=10.3 ps {I10}). 
MOME2$reorientation effect in Coul. ex. Other measurements: -0.39 {I8} or -0.13 {I8} (1977Na06); -0.42 {I9} or -0.10 {I9} (1976Pa13) 
$|b{-2}=0.20 (from (p,p') and (|a,|a')) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$L(t,p)=L(p,p')=L(d,d')=0 from 0+; E0 transition to 0+ 
T$weighted average of 1.58 ns {I4} (|b|g|g(t) in |b decay of 1.5-s {+100}Nb,1990Ma01), 1.65 ns {I4} (|b|g(t) quoted by 1990Ma01 from a later report of 1989OhZY), 1.7 ns {I2} (p ce(t) in (p,p'|g) 1972AnZP), 2.2 ns {I3} (B(E2) in Coul. ex.,1972Ba90). Others: 1.52 ns {I+5-8}, deduced by evaluators from B(E2) in 2012Wr03, where 1.580 ns {I40} (1990Ma01) was used as input data in their GOSIA analysis of Coul. Ex. data; 1.53 ns {I30} (2013RuZX, |g|g(t) fast-timing technique in study of prompt |g rays from neutron-induced fission of actinides). Value of 3.0 ns {I1} from (proton)(ce)(t) in (p,t) (1987Es01) seems discrepant 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,p')=L(|a,|a')=2 from 0+ 
T$others: 5.0 ps {I5} from B(E2) value from 1972Ba90 in Coul. ex.; 5.3 ps {I+3-4}, deduced by evaluators from B(E2) (from 536,2+ level) in 2012Wr03, where 6.45 ps {I58} (1985Mu09) was used as input data in their GOSIA analysis of Coul. ex. data 
$|b{-2}=0.037 (from (p,p') and (|a,|a')) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,p')=4 from 0+ 
T$others: 4.9 ps {I+19-14} (DSAM in {+9}Be({+109}Tc,X|g), 2017Ra05); 3.67 ps {I+12-16}, deduced by evaluators from B(E2) (from 536,2+ level) in 2012Wr03, where 3.83 ps {I34} (1985Mu09) was used as input data in their GOSIA analysis of Coul. ex. data 
$|b{-4}=-0.027 (from (p,p')). B(E4)(W.u.)=0.99 {I21} (from (p,p') and (d,d') 1992Pi08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,p')=2 from 0+ 
T$other: 2.25 ps {I+9-10}, deduced by evaluators from B(E2) (from 695, 0+ level) in 2012Wr03, where 2.93 ps {I68} (1985Mu09) was used as input data in their GOSIA analysis of Coul. ex. data 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$471.4|g to 4+, 543.6|g to 2+, and no |g to 0+ suggests 3, 4+. Absence in Coul. ex. and systematics support 3+ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$L(p,p')=(2); possible |g to 0+. In (n,n'|g), 1997Ko62 propose (0+) based on the comparison of experimental and calculated populations of this state. In that case level in (p,p') must be different and possible |g to 0+ will not exist. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J$|gs to 2+, 4+ and population in Coul. ex., probably through a two-step process from 2+ and 4+ states. 
T$other: 1.78 ps {I+17-19}, deduced by evaluators from B(E2) in Coul. Ex.(from 1064,2+ level) in 2012Wr03, where 2.45 ps {I41} (1985Mu09) was used as input data in their GOSIA analysis. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$other: 1.21 ps {I+9-8}, deduced by evaluators from B(E2) (from 1136,4+ level) in 2012Wr03, where 1.20 ps {I17} (1985Mu09) was used as input data in their GOSIA analysis of Coul. ex. data 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(p,p')=L(|a,|a')=3 from 0+ 
$B(E3)=0.143 {I12} (2002Ki06, evaluation) 
T$weighted average of 12 ps {I3} (RDDS in Coul. ex.) and 20 ps {I5} (B(E3) values in Coul. ex.). 2012Wr03 in Coul. Ex. used 12.0 ps {I30} (1985Mu09) in their GOSIA analysis to deduce several matrix elements 
$|b{-3}=0.17 ((p,p') and (|a,|a')) 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J$1281.8|g to 0+; 1+ favored by 1997Ko62 using comparison of experimental and calculated yields in (n,n'|g) reaction 


level_energy_unit: KEV
level_comment:
E$This group may correspond to the 2087 level but L(t,p)=(0,1) and L(p,p')=(3,5) are mutually inconsistent as well as inconsistent with J|p(2086)=0+. If L-transfers are correct, there are two levels near 2082 in addition to the 2086 level. L(t,p)=(0) could correspond to 2086, 0+ level. In (n,n'), J|p=2+ is deduced 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$L(p,p')=5. But L(p,p')=2 is also reported. Also L(|a,|a')=2 
E$The partially resolved group in (t,p) at 2334 with L=0 may be a different level 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E$from particle transfer reactions. 
J$from L(p,p')=(1). However, L(t,p)=2 and L(|a,|a')=5 are inconsistent with this assignments. It is possible that there are different levels near this energy 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$log| {Ift}=5.4 from (5)+; |g to 2+. Also L(p,p')=L(d,d')=(4). But L(|a,|a')=3 and L(p,p')=3 in one of the studies suggest 3- also. (1280|g)(600|g)(|q) measurement in {+100}Nb |b{+-} decay (2.99 s) gives unrealistic |d(M2/E1)<-0.28 for J|p(2416)=3-. There may be two closely spaced levels near this energy 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J$log| {Ift}=5.2 from (5)+; L(p,p')=4, assuming the levels populated in (p,p') at 2563 {I5} and in |b{+-} decay are the same 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E$unresolved in (t,p). This level may correspond to 2663 from (n,n'|g) 
J$in (p,p'), 1987Fr07 assign 4-, treating this as an unnatural parity state. But L(t,p)=2 for a 2652 group is in disagreement. Also, L(|a,|a')=(4,5). L(p,p')=1 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MEV
level_comment:
J$isoscalar giant-quadrupole resonance (ISGQR) 
$%E2 EWSR=79 {I14} for ISGQR in (|a,|a') (2015Yo04) 


level_energy_unit: KEV
level_comment:
L$from 1988Ch29. 1981Fl06 give L=3, 4. This group probably corresponds to the 1908, 3- seen in Coul. ex. 


level_energy_unit: KEV
level_comment:
L$1988Ch29 give L=0 and 1981Fl06 give L=1. The group may be a doublet (see 2082 and 2086 in the Adopted Levels) 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
E$evaluators assume that 2633.3 {I1} in 2006Ru06 and 2632.4 {I3} in 2008RuZW are the same levels 
$Integrated |s=1.5 eVb {I3} (2006Ru06) 
$T{-1/2}=0.51 ps {I10} from |G=0.00090 eV {I18} (2006Ru06) 
$B(E1)(|^)=0.14|*10{+-5} {I3}, B(M1)(|^)=0.013 {I3} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.32 ps {I4} from |G=0.00143 eV {I17} (2006Ru06) 
$B(E1)(|^)=0.17|*10{+-5} {I2}, B(M1)(|^)=0.0152 {I18} (2006Ru06) 
$Integrated |s=2.0 eVb {I2} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.37 ps {I4} from |G=0.00125 eV {I13} (2006Ru06) 
$B(E1)(|^)=0.15|*10{+-5} {I2}, B(M1)(|^)=0.0132 {I14} (2006Ru06) 
$Integrated |s=1.70 eVb {I18} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.207 ps {I19} from |G=0.0022 eV {I2} (2006Ru06) 
$B(E1)(|^)=0.22|*10{+-5} {I2}, B(M1)(|^)=0.0202 {I19} (2006Ru06) 
$Integrated |s=2.8 eVb {I3} (2006Ru06) 
J$1+ in 2005Ru14 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.23 ps {I4} from |G=0.0020 eV {I3} (2006Ru06) 
$B(E1)(|^)=0.17|*10{+-5} {I2}, B(M1)(|^)=0.0157 {I20} (2006Ru06) 
$Integrated |s=2.2 eVb {I3} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.138 ps {I17} from |G=0.0033 eV {I4} (2006Ru06) 
$B(E1)(|^)=0.28|*10{+-5} {I3}, B(M1)(|^)=0.025 {I3} (2006Ru06) 
$Integrated |s=3.6 eVb {I4} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=43 fs {I6} from |G=0.0107 eV {I15} (2006Ru06) 
E$this state decays to g.s. and the first excited 0+ state which indicates that two coexisting configurations are mixed in the 0+ states (2006Ru06) 
$B(M1)(2595|g,1+ to excited 0+)/B(M1)(3290|g,1+ to g.s.)=0.45 {I13} (2006Ru06) 
$Integrated |s=7.6 eVb {I6} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
E,J$level from 2006Ru06 only 
$T{-1/2}=0.175 ps {I20} from |G=0.0026 eV {I3} (2006Ru06) 
$B(E1)(|^)=0.20|*10{+-5} {I2}, B(M1)(|^)=0.018 {I2} (2006Ru06) 
$Integrated |s=2.7 eVb {I3} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=18.9 fs {I15} from |G=0.0242 eV {I19} (2006Ru06) 
$B(E1)(|^)=1.52|*10{+-5} {I12}, B(M1)(|^)=0.138 {I11} (2006Ru06) 
$Integrated |s=21.9 eVb {I16} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
E,J$level from 2006Ru06 only 
$T{-1/2}=0.18 ps {I3} from |G=0.0025 eV {I4} (2006Ru06) 
$B(E1)(|^)=0.16|*10{+-5} {I2}, B(M1)(|^)=0.014 {I2} (2006Ru06) 
$Integrated |s=2.3 eVb {I4} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$T{-1/2}=56 fs {I6} from |G=0.0082 eV {I8} (2006Ru06) 
$B(E1)(|^)=0.50|*10{+-5} {I5}, B(M1)(|^)=0.045 {I5} (2006Ru06) 
$Integrated |s=7.3 eVb {I7} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=32 fs {I3} from |G=0.0144 eV {I14} (2006Ru06) 
$B(E1)(|^)=0.86|*10{+-5} {I8}, B(M1)(|^)=0.078 {I8} (2006Ru06) 
$Integrated |s=12.6 eVb {I12} (2006Ru06) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$T{-1/2}=9 fs {I6} from |G=0.050 eV {I35} 
$|G(g.s.)/|G(total)|<0.85 {I13} (1974Wo05), |<0.88 (1981Sc10) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$Relative population=0.27 
J$1997Ko62 suggest (0+) based on comparison of experimental and calculated population 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
$Relative population=1.44 
J$1997Ko62 give (1+) based on comparison of experimental and calculated population 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
B2$from 1992Ke07 based on reanalysis of data from 1987Fr07. Others: 0.250 {I19} (1992Ke07, reanalysis of data from 1971Lu07), 0.202 (1987Fr07), 0.207 (1975Bu04), 0.184 (1973Ta03), 0.19 (1972Aw03), 0.23 (1971Lu07) 
$G{-2}(W.u.)=27 {I4} (1992Ke07, from |b{-2}=0.196) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$from (p)(ce)(t) (1972AnZP) 
$See 1972Aw03 for deformation parameters 
$I(|g+ce)(695, E0 transition to g.s.)/I(|g+ce)(159|g, E2 to 535)=0.110 {I8} (1972AnZP). This gives I(ce(K)(695,E0))/I(ce(K)(159|g,E2))=0.62 {I5}. 1977Re04 report I(ce(K)(695,E0))/I(ce(K)(159|g,E2))=0.76 {I5} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
B3$others: 0.200 {I15}, 0.220 {I17} (1992Ke07, from reanalysis of data of 1987Fr07 and 1971Lu07, respectively), 0.166 (1987Fr07), 1984Pi01, 1975Bu04, 1972Aw03, 1971Lu07 
1973InZY give I|g(844|g)/I|g(1373|g)=70/30 in (p,p'|g) data 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
L$other: L=2 (1987Fr07,1984Pi01) for 2158 group. |b{-2}=0.022 (1984Pi01) 
E$2516 in 1992Pi08 is a misprint, see 1990Pi14 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
B4$0.053 (1984Pi01) 
$B(E4)(W.u.)=5.7 {I4} (1992Pi08) 
E$the 2470 group (1972Aw03) probably corresponds to 2514 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Model independent quadrupole overall shape parameter and quadrupole asymmetry parameters deduced from E2 matrix elements are <Q{+2}>=0.47 {I3}, <Q{+3}cos3|d>=0.01 {I6}, respectively (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$g-factor: value adopted by 2001Ma17 from weighted average of +0.515 {I42} (transient-field technique,2001Ma17) and +0.404 {I52} (original value of +0.43 {I6} from 1978HaYJ re-evaluated by 2001Ma17 for consistent field parameters). Other: 0.34 {I18} (IMPAC method, 1969He11, using T{-1/2}(536 level)=10.3 ps {I10}). 
MOME2$-0.39 {I8} (for constructive interference) or -0.13 {I8} (for destructive interference) (1977Na06). Other: -0.42 {I9} or -0.10 {I9} (1976Pa13) 
BE2$0.518 {I11} from weighted average of 0.511 {I9} (1976Pa13), 0.526 {I26} (1972Ba90), 0.61 {I6} (1962Ga13), 0.63 {I10} (1962Er05), 0.614 {I62} (1958St32,1955St57), 0.66 {I10} (1956Te26). 
T$weighted average of 13.6 ps {I7} (recoil-distance Doppler-shift method,1975Bo39), and half-lives of 12.56 ps {I22} (1976Pa13), 12.2 ps {I6} (1072Ba90), 10.5 ps {I12} (1962Ga13), 10.2 ps {I16} (1962Er05), 10.5 ps {I11} (1958St32) and 9.7 ps {I15} (1956Te26), deduced from respective B(E2)|^ values determined in the measurement of Coulomb excitation yields. Other: 13.9 ps {I4}, deduced by evaluators from B(E2) in 2012Wr03, where 13.6 ps {I7} (1975Bo39) was used as input data in their GOSIA analysis 
$Reduced E2 matrix element from g.s.=+0.68 {I1} (2012Wr03) 
$Reduced diagonal E2 matrix element=-0.33 {I10} (2012Wr03) 
$Spectroscopic Q=-0.25 {I7} (2011Wr01, deduced from reduced diagonal E2 matrix element=-0.33 {I10}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
$Model independent quadrupole overall shape parameter and quadrupole asymmetry parameters deduced from E2 matrix elements are <Q{+2}>=0.62 {I3}, <Q{+3}cos3|d>=0.42 {I6}, respectively (2012Wr03) 
$B(E2)(from 536,2+)=0.038 {I6} (1972Ba90) 
$B(E2)(from 536,2+)=0.0526 {I+19-8} (2012Wr03) 
$Reduced E2 matrix element from 536,2+=+0.513 {I+9-4} (2012Wr03) 
T$from B(E2) and branching ratio. Other: 1.52 ns {I+5-8}, deduced by evaluators from B(E2) in 2012Wr03, where 1.580 ns {I40} (1990Ma01) was used as input data in their GOSIA analysis 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from weighted average of 7.1 ps {I12} (1975Bo39); 6.5 ps {I6} (1985Mu09), both measurements used recoil-distance Doppler-shift method; and T{-1/2}=5.0 ps {I5} from B(E2) in 1972Ba90; 5.3 ps {I+3-4}, deduced by evaluators from B(E2) (from 536,2+ level) in 2012Wr03, where 6.45 ps {I58} (1985Mu09) was used as input data in their GOSIA analysis. 
$B(E2)(from 536,2+)=0.178 {I21} (1972Ba90, 528|g assumed pure E2). Others: 1961St02, 1962Ga13, 1962Ga10. 
$B(E2)(from g.s.)=0.0113 {I8} (1972Ba90) 
$B(M1(from 536,2+)=0.0013 {I+11-8} (2012Wr03) 
$B(E2)(from g.s.,0+)=0.0106 {I+4-2} (2012Wr03) 
$B(E2)(from 536,2+)=0.177 {I+8-7} (2012Wr03) 
$B(E2)(from 695,0+)=0.102 {I+20-12} (2012Wr03) 
$Reduced E2 matrix element from g.s.,0+=+0.103 {I+2-1} (2012Wr03) 
$Reduced E2 matrix element from 536,2+=+0.94 {I2} (2012Wr03) 
$Reduced E2 matrix element from 695,0+=-0.32 {I+3-2} (2012Wr03) 
$Reduced M1 matrix element from 536,2+=+0.08 {I3} (2012Wr03) 
$Reduced diagonal E2 matrix element=+1.20 {I+10-8} (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from weighted average of 3.8 ps {I5} (1975Bo39) and 3.83 ps {I34} (1985Mu09), both measurements used recoil-distance Doppler-shift method. Other: 3.67 ps {I+12-16}, deduced by evaluators from B(E2) (from 536,2+ level) in 2012Wr03, where 3.83 ps {I34} (1985Mu09) was used as input data in their GOSIA analysis. 
$B(E2)(from 536,2+)=0.444 {I41} (1985Mu09), 0.351 {I30} (1972Ba90) 
$B(E2)(from 1064,2+)<0.008 (1985Mu09) 
$B(E2)(from 536,2+)=0.354 {I+16-11} (2012Wr03) 
$B(E2)(from 1064,2+)=0.119 {I+43-29} (2012Wr03) 
$Reduced E2 matrix element from 536,2+=+1.33 {I+3-2} (2012Wr03) 
$Reduced E2 matrix element from 1064,2+=+0.77 {I+13-10} (2012Wr03) 
$Reduced diagonal E2 matrix element=-0.35 {I18} (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Other: 2.25 ps {I+9-10}, deduced by evaluators from B(E2) (from 695, 0+ level) in 2012Wr03, where 2.93 ps {I68} (1985Mu09) was used as input data in their GOSIA analysis. 
$B(E2)(from g.s.)<0.0009 (1985Mu09) 
$B(E2)(from 536,2+)=0.023 {I10} (1985Mu09) 
$B(E2)(from 694,0+)=0.38 {I16} (1985Mu09) 
$B(E2)(from 1064,2+)<0.072 (1985Mu09) 
$B(E2)(from 1136,4+)=0.03 {I2} (1985Mu09) 
$B(M1)(from 536,2+)=0.00816 {I24} (2012Wr03) 
$B(E2)(from g.s.,0+)=0.00026 {I+11-9} (2012Wr03) 
$B(E2)(from 536,2+)=0.00098 {I+21-16} (2012Wr03) 
$B(E2)(from 695,0+)=0.256 {I+8-6} (2012Wr03) 
$B(E2)(from 1064,2+)=0.032 {I+29-17} (2012Wr03) 
$B(E2)(from 1136,4+)=0.077 {I+13-7} (2012Wr03) 
$Reduced E2 matrix element from g.s.,0+=-0.016 {I3} (2012Wr03) 
$Reduced E2 matrix element from 536,2+=-0.070 {I+7-6} (2012Wr03) 
$Reduced E2 matrix element from 695,0+=+0.506 {I+8-6} (2012Wr03) 
$Reduced E2 matrix element from 1064,2+=+0.40 {I+15-13} (2012Wr03) 
$Reduced E2 matrix element from 1136,4+=+0.83 {I+7-4} (2012Wr03) 
$Reduced M1 matrix element from 536,2+=+0.202 {I3} (2012Wr03) 
$Reduced diagonal E2 matrix element=-0.24 {I+12-7} (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
T$other: 1.78 ps {I+17-19}, deduced by evaluators from B(E2) (from 1064,2+ level) in 2012Wr03, where 2.45 ps {I41} (1985Mu09) was used as input data in their GOSIA analysis. 
$B(E2)(from 1064,2+)=0.158 {I25} (1985Mu09) 
$B(E2)(from 1136,4+)=0.084 {I14} (1985Mu09) 
$B(E2)(from 536,2+)=0.00079 {I+76-27} (2012Wr03) 
$B(E2)(from 1064,2+)=0.208 {I+17-12} (2012Wr03) 
$B(E2)(from 1136,4+)=0.109 {I11} (2012Wr03) 
$Reduced E2 matrix element from 536,2+=0.063 {I+25-12} (2012Wr03) 
$Reduced E2 matrix element from 1064,2+=+1.02 {I+4-3} (2012Wr03) 
$Reduced E2 matrix element from 1136,4+=+0.99 {I5} (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$other: 1.21 ps {I+9-8}, deduced by evaluators from B(E2) (from 1136,4+ level) in 2012Wr03, where 1.20 ps {I17} (1985Mu09) was used as input data in their GOSIA analysis. 
$B(E2)(from 1136,4+)=0.41 {I10} (1985Mu09). Other: 1986Ho25 
$B(E2)(from 1136,4+)=0.372 {I+25-24} (2012Wr03) 
$Reduced E2 matrix element from 1136,4+=+1.83 {I6} (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$other: 20 ps {I5} from B(E3)=0.144 {I15} (weighted average of values from 1985Mu09 and 1972Ba90). 2012Wr03 used 12.0 ps {I30} (1985Mu09) in their GOSIA analysis 
$B(E3)(from g.s.)=0.154 {I15} (1985Mu09), 0.132 {I17} (1972Ba90) 
$B(E1)(from 536)=3.2|*10{+-8} {I16} (1985Mu09) 
$B(E1)(from 1064)=3.9|*10{+-7} {I23} (1985Mu09) 
$B(E1)(from 536,2+)=0.00054 {I+13-10} (2012Wr03) 
$B(E1)(from 1064,2+)=0.0051 {I+14-6} (2012Wr03) 
$B(E3)(from g.s.,0+)=0.194 {I9} (2012Wr03) 
$B(E3)(from 536,2+)=0.022 {I+4-5} (2012Wr03) 
$Absolute reduced E3 matrix element from g.s.,0+=+0.44 {I1} (2012Wr03) 
$Absolute reduced E3 matrix element from 536,2+=+0.33 {I+3-4} (2012Wr03) 
$Absolute reduced E1 matrix element from 536,2+=+0.052 {I+6-5} (2012Wr03) 
$Absolute reduced E1 matrix element from 1064,2+=+0.16 {I+2-1} (2012Wr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=14.8 ps {I+73-50} (statistical uncertainties of +6.1-4.1 ps and systematic uncertainties of +4.0-2.8 ps combined in quadrature). 
$Transition quadrupole moment Q{-t}=2.5 {I4} (2017Ra05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=7.0 ps {I+27-20} (statistical uncertainties of +2.5-1.8 ps and systematic uncertainties of +0.9-0.7 ps combined in quadrature). 
$Transition quadrupole moment Q{-t}=2.3 {I+4-3} (2017Ra05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$from measured 7.12|*10{+18} y {I+18-14}(stat){I10}(syst) for the 2|n2|b decay of {+100}Mo to the g.s. of {+100}Ru. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$upper limit from 111 kg day live exposure at 90% C.L. (2019Kw01) for 0|n2|b decay of {+100}Mo to the g.s. of {+100}Ru. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$upper limit for 0|n|b|b decay mode of {+100}Mo to the g.s of {+100}Ru at 90% C.L, using 1.9 kg of calcium molybdate crystals and 0.68 kg.year exposure with a reduced background respect to previously reported limit in 2019Kw01. Other: > 8.2|*10{+26} y (2023Ki01). Authors of 2023Ki01 state that this valiue is aimed in AMoRE-II experiment, using 100 kg of enriched {+100}Mo with a reduced background level and improved detector setup. With this half life the expected upper limit of Majorana neutrino mass m{-|b|b}<0.013-0.025 eV after 5-year operation. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$from measured 7.5|*10{+18} y {I8}(stat) {I+4-3} (syst) for the 2|n2|b decay of {+100}Mo to the g.s. of {+100}Ru. Others: >4.4|*10{+21} y for 2|n2|b decay to the first 2+ in {+100}Ru, >2.1|*10{+23} y for 0|n2|b decay to the first 2+ in {+100}Ru, and >1.2|*10{+23} y for 0|n2|b decay to the first excited 0+ in {+100}Ru 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$from measured 7.07|*10{+18} y {I+2} (stat) {I11} (syst) for the 2|n2|b decay of {+100}Mo to the g.s. of {+100}Ru (2023Au05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for |b|b|h{-0}, n=1 mode. Others: >5.8|*10{+21} for |b|b|h{-0}, n=2 mode, >2.2|*10{+21} for |b|b|h{-0}, n=3 mode, >2.2|*10{+21} for |b|b|h{-0}x{-0} n=3 mode, >2.0|*10{+21} and |b|b|h{-0}|h{-0} n=7 mode (2024Au02) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MIN
level_comment:
J$L=0 (d,p) 
T$weighted average of: 14.61 {i3} (1990Ab06), 14.6 min (1941Ma03), 14.6 min {i1} (1954Wi04), 14.61 min {i7} (1957Ok01), 14.77 min {i16} (1972Co17) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$M1(+E2) |g to 1/2+, M1+E2 |g from 5/2+ 
T$from (276|g)(13.5|g)(t): (1991Se08). Other: 223 ns {i10} (1977LaZG) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$from (180|g)(K|a| x ray)(t) (1991Se08). Others: 124 ns {i10} (1977LaZG) (semi), 12.5 ns (1965Mc03) 
E$1991Se08 have looked for the possibility of a state near 57 keV without success. See (d,p) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=7.5 {I4} (at 8|'), 0.80 {I4} (at 18|'), 2.49 {I13} (at 27|'), 2.22 {I11} (at 33|'), 1.07 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=1.05 {I5} (at 8|'), 2.95 {I15} (at 18|'), 1.96 {I10} (at 27|'), 0.87 {I4} (at 33|'), 0.77 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0110 {I12} (at 8|'), 0.0307 {I17} (at 18|'), 0.0259 {I15} (at 27|'), 0.0140 {I8} (at 33|'), 0.0089 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+&7/2+
level_comment:
$|s(mb/sr)=0.395 {I21} (at 8|'), 0.557 {I28} (at 18|'), 0.71 {I4} (at 27|'), 0.648 {I33} (at 33|'), 0.402 {I20} (at 43|') 
E,L$unresolved doublet (2017Fr08) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.062 {I4} (at 8|'), 0.153 {I8} (at 18|'), 0.255 {I13} (at 27|'), 0.318 {I16} (at 33|'), 0.340 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.220 {I15} (at 8|'), 0.593 {I31} (at 18|'), 0.416 {I22} (at 27|'), 0.185 {I11} (at 33|'), 0.173 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.87 {I5} (at 8|'), 0.146 {I10} (at 18|'), 0.233 {I15} (at 27|'), 0.274 {I15} (at 33|'), 0.132 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=1.17 {I6} (at 8|'), 2.57 {I13} (at 18|'), 1.48 {I8} (at 27|'), 0.693 {I35} (at 33|'), 0.73 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0140 {I12} (at 8|'), 0.0196 {I11} (at 18|'), 0.0149 {I9} (at 27|'), 0.0086 {I5} (at 33|'), 0.0065 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0520 {I33} (at 8|'), 0.125 {I6} (at 18|'), 0.114 {I6} (at 27|'), 0.099 {I5} (at 33|'), 0.0681 {I35} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.514 {I27} (at 8|'), 1.15 {I6} (at 18|'), 0.70 {I4} (at 27|'), 0.355 {I18} (at 33|'), 0.340 {I17} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.72 {I4} (at 8|'), 0.082 {I4} (at 18|'), 0.268 {I14} (at 27|'), 0.248 {I13} (at 33|'), 0.117 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0100 {I21} (at 8|'), 0.0180 {I22} (at 27|'), 0.0200 {I14} (at 33|'), 0.0136 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0080 {I11} (at 8|'), 0.0220 {I23} (at 27|'), 0.0220 {I15} (at 33|'), 0.0239 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
$|s(mb/sr)=0.0100 {I11} (at 8|'), 0.0250 {I16} (at 27|'), 0.0308 {I17} (at 33|'), 0.0351 {I19} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0160 {I13} (at 8|'), 0.0209 {I13} (at 27|'), 0.0261 {I14} (at 33|'), 0.0284 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0160 {I13} (at 8|'), 0.0298 {I17} (at 27|'), 0.0312 {I17} (at 33|'), 0.0161 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 8|'), 0.0200 {I14} (at 18|'), 0.0162 {I11} (at 27|'), 0.0132 {I8} (at 33|'), 0.0088 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.112 {I7} (at 8|'), 0.201 {I10} (at 18|'), 0.068 {I4} (at 27|'), 0.0520 {I28} (at 33|'), 0.0539 {I28} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.176 {I10} (at 8|'), 0.322 {I16} (at 18|'), 0.120 {I7} (at 27|'), 0.168 {I9} (at 33|'), 0.109 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0170 {I22} (at 8|'), 0.0379 {I21} (at 18|'), 0.0169 {I10} (at 33|'), 0.0143 {I8} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0070 {I11} (at 8|'), 0.0089 {I7} (at 18|'), 0.0098 {I6} (at 33|'), 0.0068 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.066 {I4} (at 8|'), 0.0189 {I10} (at 18|'), 0.0150 {I9} (at 27|'), 0.0105 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0320 {I26} (at 8|'), 0.0146 {I8} (at 18|'), 0.0188 {I11} (at 27|'), 0.0231 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0116 {I11} (at 8|'), 0.0147 {I9} (at 18|'), 0.0127 {I8} (at 27|'), 0.0071 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.200 {I32} (at 8|'), 0.400 {I28} (at 18|'), 0.251 {I13} (at 27|'), 0.112 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0250 {I24} (at 8|'), 0.069 {I4} (at 18|'), 0.0432 {I23} (at 27|'), 0.0196 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0250 {I24} (at 8|'), 0.0156 {I9} (at 18|'), 0.0157 {I9} (at 27|'), 0.0068 {I4} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0071 {I10} (at 8|'), 0.0073 {I5} (at 18|'), 0.0084 {I5} (at 27|'), 0.0074 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0046 {I8} (at 8|'), 0.0064 {I4} (at 18|'), 0.0044 {I4} (at 27|'), 0.00290 {I25} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.058 {I4} (at 8|'), 0.0079 {I5} (at 18|'), 0.0199 {I11} (at 27|'), 0.0191 {I10} (at 33|'), 0.0110 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0081 {I9} (at 8|'), 0.0161 {I9} (at 18|'), 0.0082 {I6} (at 27|'), 0.0052 {I4} (at 33|'), 0.00390 {I22} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0052 {I9} (at 8|'), 0.0111 {I6} (at 18|'), 0.0148 {I9} (at 27|'), 0.0154 {I8} (at 33|'), 0.0082 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.197 {I10} (at 8|'), 0.457 {I23} (at 18|'), 0.378 {I19} (at 27|'), 0.236 {I12} (at 33|'), 0.105 {I5} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.088 {I5} (at 8|'), 0.137 {I7} (at 18|'), 0.129 {I7} (at 27|'), 0.088 {I5} (at 33|'), 0.046 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.145 {I8} (at 8|'), 0.268 {I14} (at 18|'), 0.176 {I9} (at 27|'), 0.096 {I5} (at 33|'), 0.055 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.512 {I27} (at 8|'), 0.315 {I16} (at 18|'), 0.254 {I13} (at 33|'), 0.138 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0220 {I32} (at 8|'), 0.0215 {I14} (at 18|'), 0.0105 {I7} (at 33|'), 0.0083 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0240 {I32} (at 8|'), 0.0211 {I13} (at 18|'), 0.0090 {I11} (at 27|'), 0.0101 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.050 {I7} (at 8|'), 0.0540 {I29} (at 18|'), 0.0510 {I33} (at 27|'), 0.0120 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.120 {I7} (at 8|'), 0.170 {I13} (at 18|'), 0.169 {I9} (at 27|'), 0.0540 {I29} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.352 {I19} (at 8|'), 0.0460 {I31} (at 18|'), 0.132 {I7} (at 27|'), 0.075 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.047 {I4} (at 8|'), 0.0500 {I27} (at 18|'), 0.0410 {I23} (at 27|'), 0.0195 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.080 {I5} (at 8|'), 0.0620 {I33} (at 18|'), 0.0440 {I24} (at 27|'), 0.0410 {I23} (at 33|'), 0.0161 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.086 {I6} (at 8|'), 0.193 {I10} (at 18|'), 0.178 {I9} (at 27|'), 0.119 {I6} (at 33|'), 0.108 {I6} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.066 {I10} (at 8|'), 0.0300 {I18} (at 18|'), 0.0430 {I24} (at 27|'), 0.0370 {I21} (at 33|'), 0.0162 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.095 {I10} (at 8|'), 0.273 {I14} (at 18|'), 0.210 {I11} (at 27|'), 0.102 {I6} (at 33|'), 0.076 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.140 {I12} (at 8|'), 0.0670 {I35} (at 18|'), 0.069 {I4} (at 27|'), 0.0330 {I19} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.072 {I7} (at 8|'), 0.0124 {I9} (at 18|'), 0.0220 {I15} (at 27|'), 0.0137 {I11} (at 33|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.041 {I5} (at 8|'), 0.0379 {I21} (at 18|'), 0.0330 {I19} (at 27|'), 0.0201 {I12} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.074 {I6} (at 8|'), 0.0263 {I16} (at 18|'), 0.0420 {I23} (at 27|'), 0.0455 {I25} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.175 {I10} (at 8|'), 0.116 {I6} (at 18|'), 0.0590 {I31} (at 27|'), 0.0491 {I26} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.150 {I21} (at 8|'), 0.478 {I24} (at 18|'), 0.305 {I15} (at 27|'), 0.171 {I9} (at 33|'), 0.144 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0560 {I35} (at 8|'), 0.0672 {I35} (at 18|'), 0.0596 {I31} (at 27|'), 0.0460 {I24} (at 33|'), 0.0245 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0490 {I32} (at 8|'), 0.085 {I4} (at 18|'), 0.088 {I5} (at 27|'), 0.082 {I4} (at 33|'), 0.0547 {I28} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.084 {I5} (at 8|'), 0.089 {I5} (at 18|'), 0.0660 {I35} (at 27|'), 0.0571 {I30} (at 33|'), 0.0283 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.045 {I3} (at 8|'), 0.0386 {I21} (at 18|'), 0.0330 {I19} (at 27|'), 0.0224 {I13} (at 33|'), 0.0157 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.045 {I3} (at 8|'), 0.0453 {I24} (at 18|'), 0.0280 {I17} (at 27|'), 0.0169 {I10} (at 33|'), 0.0129 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0350 {I27} (at 8|'), 0.0460 {I24} (at 18|'), 0.0430 {I24} (at 27|'), 0.0353 {I19} (at 33|'), 0.0277 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.047 {I4} (at 8|'), 0.083 {I4} (at 18|'), 0.0530 {I28} (at 27|'), 0.0270 {I17} (at 33|'), 0.0221 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.189 {I10} (at 8|'), 0.147 {I8} (at 18|'), 0.134 {I7} (at 27|'), 0.117 {I6} (at 33|'), 0.073 {I4} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.053 {I4} (at 8|'), 0.113 {I6} (at 18|'), 0.075 {I4} (at 27|'), 0.0519 {I28} (at 33|'), 0.0357 {I19} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0170 {I22} (at 8|'), 0.0192 {I11} (at 18|'), 0.0182 {I12} (at 27|'), 0.0218 {I13} (at 33|'), 0.017 {I1} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0360 {I27} (at 8|'), 0.0540 {I29} (at 27|'), 0.0289 {I17} (at 33|'), 0.0194 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0270 {I24} (at 8|'), 0.0412 {I23} (at 27|'), 0.0238 {I14} (at 33|'), 0.0175 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0420 {I29} (at 8|'), 0.0518 {I28} (at 27|'), 0.0351 {I19} (at 33|'), 0.0196 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0260 {I24} (at 8|'), 0.0239 {I14} (at 27|'), 0.0199 {I12} (at 33|'), 0.0119 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.039 {I4} (at 8|'), 0.0360 {I27} (at 18|'), 0.0331 {I18} (at 27|'), 0.0260 {I17} (at 33|'), 0.0134 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.026 {I4} (at 8|'), 0.0510 {I33} (at 18|'), 0.0250 {I16} (at 33|'), 0.0135 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.049 {I5} (at 8|'), 0.058 {I4} (at 18|'), 0.0460 {I25} (at 33|'), 0.0341 {I19} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.061 {I5} (at 8|'), 0.056 {I3} (at 18|'), 0.0380 {I28} (at 27|'), 0.0227 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0230 {I32} (at 8|'), 0.0199 {I14} (at 18|'), 0.0130 {I21} (at 27|'), 0.0058 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0090 {I21} (at 8|'), 0.0205 {I14} (at 18|'), 0.0260 {I24} (at 27|'), 0.0075 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.075 {I6} (at 8|'), 0.0520 {I28} (at 18|'), 0.045 {I3} (at 27|'), 0.0232 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0310 {I34} (at 8|'), 0.0328 {I19} (at 18|'), 0.0280 {I17} (at 27|'), 0.0187 {I12} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.009 {I3} (at 8|'), 0.0066 {I9} (at 18|'), 0.0110 {I21} (at 27|'), 0.0063 {I8} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.031 {I4} (at 8|'), 0.0238 {I15} (at 18|'), 0.0220 {I15} (at 27|'), 0.0102 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.063 {I9} (at 8|'), 0.096 {I6} (at 18|'), 0.071 {I8} (at 27|'), 0.0320 {I34} (at 33|'), 0.0260 {I24} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.079 {I10} (at 8|'), 0.068 {I5} (at 18|'), 0.051 {I8} (at 27|'), 0.062 {I4} (at 33|'), 0.0250 {I24} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.053 {I5} (at 8|'), 0.0630 {I33} (at 18|'), 0.0400 {I22} (at 27|'), 0.0340 {I26} (at 33|'), 0.0248 {I15} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.117 {I8} (at 8|'), 0.093 {I5} (at 18|'), 0.069 {I4} (at 27|'), 0.060 {I4} (at 33|'), 0.0318 {I18} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.097 {I6} (at 8|'), 0.070 {I4} (at 18|'), 0.0540 {I29} (at 27|'), 0.0510 {I28} (at 33|'), 0.0206 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0290 {I33} (at 8|'), 0.0260 {I17} (at 18|'), 0.0170 {I13} (at 27|'), 0.0160 {I13} (at 33|'), 0.0040 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.081 {I6} (at 8|'), 0.0510 {I28} (at 18|'), 0.0410 {I23} (at 27|'), 0.0400 {I22} (at 33|'), 0.0150 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.065 {I8} (at 8|'), 0.0470 {I26} (at 18|'), 0.0380 {I28} (at 27|'), 0.0280 {I25} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.096 {I6} (at 8|'), 0.077 {I4} (at 18|'), 0.0600 {I32} (at 27|'), 0.0580 {I31} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0210 {I32} (at 8|'), 0.0130 {I12} (at 18|'), 0.0150 {I13} (at 27|'), 0.0120 {I12} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.103 {I7} (at 8|'), 0.0400 {I22} (at 18|'), 0.0430 {I24} (at 27|'), 0.0490 {I27} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.053 {I4} (at 8|'), 0.0590 {I31} (at 18|'), 0.0490 {I27} (at 27|'), 0.0370 {I21} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0280 {I33} (at 8|'), 0.0235 {I15} (at 18|'), 0.0160 {I13} (at 27|'), 0.0089 {I9} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.059 {I4} (at 8|'), 0.068 {I4} (at 18|'), 0.0470 {I26} (at 27|'), 0.0320 {I19} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.044 {I7} (at 8|'), 0.0320 {I26} (at 18|'), 0.0250 {I33} (at 27|'), 0.0220 {I32} (at 33|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.041 {I4} (at 8|'), 0.0280 {I17} (at 18|'), 0.0230 {I15} (at 27|'), 0.0260 {I17} (at 33|'), 0.0111 {I9} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.07 {I1} (at 8|'), 0.0420 {I29} (at 18|'), 0.0330 {I26} (at 27|'), 0.0360 {I27} (at 33|'), 0.0195 {I13} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.041 {I9} (at 8|'), 0.044 {I3} (at 18|'), 0.0350 {I35} (at 27|'), 0.0300 {I25} (at 33|'), 0.0162 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0140 {I31} (at 8|'), 0.0185 {I13} (at 18|'), 0.0110 {I12} (at 27|'), 0.0090 {I9} (at 33|'), 0.0056 {I7} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0330 {I34} (at 8|'), 0.0360 {I21} (at 18|'), 0.0250 {I16} (at 27|'), 0.0240 {I16} (at 33|'), 0.0126 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.048 {I6} (at 8|'), 0.0200 {I14} (at 18|'), 0.0180 {I14} (at 27|'), 0.0250 {I16} (at 33|'), 0.0160 {I13} (at 43|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.009 {I4} (at 8|'), 0.0130 {I12} (at 18|'), 0.0110 {I12} (at 27|'), 0.0130 {I12} (at 33|'), 0.0060 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.070 {I8} (at 8|'), 0.113 {I6} (at 18|'), 0.084 {I4} (at 27|'), 0.0610 {I32} (at 33|'), 0.0372 {I20} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|s(mb/sr)=0.0140 {I31} (at 8|'), 0.0200 {I22} (at 18|'), 0.0210 {I23} (at 27|'), 0.0190 {I14} (at 33|'), 0.0080 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0120 {I31} (at 8|'), 0.0330 {I26} (at 18|'), 0.0190 {I22} (at 27|'), 0.0130 {I12} (at 33|'), 0.0110 {I12} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.050 {I5} (at 8|'), 0.077 {I4} (at 18|'), 0.063 {I4} (at 27|'), 0.0400 {I22} (at 33|'), 0.0256 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0170 {I31} (at 8|'), 0.0310 {I25} (at 18|'), 0.0180 {I14} (at 27|'), 0.0099 {I10} (at 33|'), 0.0073 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0160 {I31} (at 8|'), 0.058 {I4} (at 18|'), 0.0350 {I27} (at 27|'), 0.0230 {I15} (at 33|'), 0.0139 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.057 {I5} (at 8|'), 0.0500 {I32} (at 18|'), 0.0370 {I27} (at 27|'), 0.0330 {I19} (at 33|'), 0.0240 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.098 {I7} (at 8|'), 0.135 {I7} (at 18|'), 0.098 {I5} (at 27|'), 0.077 {I4} (at 33|'), 0.0500 {I27} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.056 {I5} (at 8|'), 0.068 {I4} (at 18|'), 0.045 {I3} (at 27|'), 0.0380 {I22} (at 33|'), 0.0250 {I16} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.060 {I5} (at 8|'), 0.093 {I5} (at 18|'), 0.073 {I4} (at 27|'), 0.056 {I3} (at 33|'), 0.0366 {I21} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.046 {I5} (at 8|'), 0.0500 {I32} (at 18|'), 0.0430 {I29} (at 27|'), 0.0330 {I19} (at 33|'), 0.0208 {I14} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.009 {I3} (at 8|'), 0.0200 {I14} (at 18|'), 0.0150 {I13} (at 27|'), 0.0113 {I11} (at 33|'), 0.0099 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0350 {I35} (at 8|'), 0.0300 {I25} (at 18|'), 0.0230 {I15} (at 27|'), 0.0180 {I14} (at 33|'), 0.0105 {I10} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0350 {I35} (at 8|'), 0.0460 {I31} (at 18|'), 0.0360 {I21} (at 27|'), 0.0250 {I16} (at 33|'), 0.0154 {I11} (at 43|') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T weighted average of: 11.2 min {i3} (1980De06), 11.8 min {i4} (1976Ki11), 11.0 min {i5} (1966Ga28), 11.0 min {i3} (1954Wi32), 11.5 min {i5} (1954Fl21). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from |b|g(t) on mass separated fission products (1991Li39). and time-integral perturbed angular correlations with Gammasphere (2005Sm08). Other: 114 ps {i3} from {+100}Mo({+18}O,{+16}O|g), see also 2001Ra27 
$Other: 0.28 {I1} deduced from T{-1/2} (1991Li39) 
J L(t,p)=2 
MOMM1 From PAC measurements of the (401|g-296|g) cascade in the |b{+-} decay of {+102}Nb (high spin + low spin isomer); + from 2005Sm08. Other: +0.8 {I4} (2005Sm08) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B2 Deduced from T{-1/2} (1991Li39) 
J L(t,p)=(4) and J=4 from |g|g(|q) in {+102}Nb |b{+-} decay (4.3 s) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J suggested from level at 2416 keV in (t,p) and (t,p|g|g) results in which a 399.3|g from an observed |g-ray triplet at 400-keV decays to (8+) level 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: PS
level_comment:
J from |g|g and band structure in {+248}Cm SF 
T from Doppler-profile method in {+248}Cm SF (1996Sm04) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_comment:
J from |g|g and band structure in {+248}Cm SF. Following 2007La03 3625 keV level is member of |DJ=2 g.s. Yrast band and not 3622.3 keV level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=186.9 ps {I+183-187} (statistical uncertainties of +17.4-17.8 ps and systematic uncertainties of 5.6 ps combined in quadrature by the authors). This value was compared by the authors to |t=180 ps {I6} in 1991Li39 (Z. Phys. A340, 223). 
$Transition quadrupole moment Q{-t}=3.1 {I+2-1} (2017Ra05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=27.8 ps {I+105-81} (statistical uncertainties of +9.0-6.7 ps and systematic uncertainties of +5.5-4.5 ps combined in quadrature by the authors). This value was compared by the authors to |t=18.0 ps {I36} in 1975Bo39 (Z. Phys. A274, 327). 
$Transition quadrupole moment Q{-t}=2.4 {I+4-3} (2017Ra05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=3.2 ps {I7} (statistical uncertainties of 0.7 ps and systematic uncertainties of 0.2 ps combined in quadrature by the authors). First lifetime measurement in the present work. 
$Transition quadrupole moment Q{-t}=3.5 {I+5-3} (2017Ra05) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
T from |g-decay curves (1977Ti02). Others: 1963Ki12, 1969Ha59, 1976KaYO 
J$1984Sh03 and 1993Li28 suggest g.s. is 3/2[411] Nilsson state. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
$Transitional quadrupole moment Q{-t}=3.84 {I17} (1993Li28) other: if K=3/2, Q{-t}=3.80 {I18} and |b{-2}=0.34 {I2} (only absolute values given) (1985Se02,1990LiZT) 
T$from 1990LiZT in SF decay. Others: 0.45 ns {I16} (1985Se02), 1.7 ns {I3} (1981SeZW) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
$Transitional quadrupole moment Q{-t}=3.84 {i17} (1993Li28) 
T$others: 0.45 ns {I16} (1985Se02), 1.7 ns {I3} (1981SeZW) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
G$from (139|g)(103|g)(|q) and (250|g)(103|g)(|q) 
$ g{-K}=-0.46 {I11}, g{-R}=+0.23 {I3}; assuming Q{-t}=3.84 {I17} 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
G$from (193|g)(139|g)(|q) and (397|g)(139|g)(|q) 
$ g{-K}=-0.73 {I17}, g{-R}=+0.09 {I13}; assuming Q{-t}=3.7 {I3} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
J$even-even nucleus g.s. 
T$from |b{+-} decay (1976KaYO). Others: 66 s {I6} (1962Ki06), 96 s {I6} (1964Te02), 58.8 s {I13} (1981TiZZ) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$from SF decay (2002Sm10). Others: 0.72 ns {I4} (1991Li39), 0.45 ns {I9} (1970Ch11), 1.2 ns {I2} (1970Wa05), 0.91 ns {I3} (1974JaZN), 0.74 ns {I5} (1990LiZZ) 
J$|g(|q) (1972Wi15), stretched E2 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from SF decay (2002Sm10). Others: 28 ps {I8} (1990LiZZ), 26.6 ps {I35} (1986Ma22), 26.8 ps {I35} (1991Li39) 
J$|g(|q) (1972Wi15) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from SF decay (2002Sm10). Other: 6.0 {I23} (2001Kr13),4.2 ps {I6} (2003Hu07) 
J$|g(|q) (1972Wi15) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
$ Q(transition)=3.35 {I14} (2002Sm10) 
T$other: 0.91 ns {I3} (1974JaZN) 
$g factor from integral PAC technique (2004Sm04,2005Sm08,2002Pa14) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$|D<r{+2}>({+104}Mo,{+92}Mo)=+1.82 fm{+2} {I10} (2009Ch09); uncertainty is systematic; statistical uncertainty is 0.001 
$ Isotope shift({+104}Mo,{+92}Mo)=-4353 MHz {I46} (2009Ch09); total uncertainty is given; statistical uncertainty is 6 
T$from 'adopted levels, gammas' dataset for {+104}Mo in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=31.8 ps {I+129-102} (statistical uncertainties of +12.4-9.4 ps and systematic uncertainties of +3.7-3.9 ps combined in quadrature by the authors). This value was compared by the authors to |t=37.7 ps {I11} in 2002Sm10 (J. Phys. G28, 2307). 
$Transition quadrupole moment Q{-t}=3.7 {I+7-6} (2017Ra05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=5.3 ps {I+17-12} (statistical uncertainties of +1.6-1.1 ps and systematic uncertainties of +0.6-0.4 ps combined in quadrature by the authors). This value was compared by the authors to |t=6.83 ps {I21} in 2002Sm10 (J. Phys. G28, 2307). 
$Transition quadrupole moment Q{-t}=3.6 {I4} (2017Ra05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=3.0 ps {I+8-7} (statistical uncertainties of +0.8-0.7 ps and systematic uncertainties of 0.1 ps combined in quadrature by the authors). This value was compared by the authors to |t=3.19 ps {I16} in 2002Sm10 (J. Phys. G28, 2307). 
$Transition quadrupole moment Q{-t}=2.8 {I+4-3} (2017Ra05) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
J$band head of a rotational band and systematics 
T$weighted average of 35.6~s~{I16} (1980TiZX), 36.7~s~{I10} (1977Ti02), 36.0~s~{I20} (1976KaYO); Others: 48~s~{I4} (1972Tr08), 58.1~s~{I14} (1970WiZN), 41~s~{I2} (1969Ha59), 40~s (1962Ki07); Also: |g(t) analysis performed in 1977Ki14, 1976KiZK and 1975KiZH, for a number of transitions in {+105}Tc, suggests two distinctive groups with T{-1/2}|?30~s and 50~s respectively; The existence of a longer-lived state with T{-1/2}=58.1~s~{I14} is also supported by 1970WiZN from 376|g(t), but never confirmed in more recent articles. 
CONF$|n5/2[532] 
MOMM1$from hyperfine structure in 2009Ch09 
$|D<r{+2}> =+1.95 fm{+2} {I11} from isotope shift measurements (2009Ch09) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
J$94.8|g M1+E2 to (5/2-); band member 
T$from |b|g|g(t) (1995Li13) in {+105}Nb |b{+-} decay. Others: 0.54~ns~{I25} (1984LhZZ), 0.80~ns~{I15} (1981SeZW), 1.1~ns~{I2} (1970Wa05) 
MOMM1$from g=-0.064 {I8} in {+252}Cf SF decay (2006Or05) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
J$137.9|g M1+E2 to (7/2-), 232.9|g to (5/2-); band member 
T$from |b-137.9|g(t) in {+105}Nb |b{+-} decay (1995Li13). Other: 0.75~ns {I15} (1981SeZW) 
MOMM1$-0.14~{I18} from g=-0.03~{I4} in {+252}Cf SF decay (2006Or05) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
J$246.9|g to (5/2-); band head of a rotational band 
T$from 246.9|g(t) in 1981SeZW 
CONF$|n3/2+[411] 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$63.5|g to (3/2+), 215.1|g to (7/2-), 309.9|g to (5/2-); band head of a rotational band 
CONF$|n5/2+[413] 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$102.0|g to (3/2+), 253.7|g to (7/2-), 348.5|g to (5/2-); band head of a rotational band 
CONF$|n3/2+[411] 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
J$144.8|g M1+E2 to (9/2-), 283.0|g E2 to (7/2-); band member 
T$weighted average 0.6~ns~{I2} from 283.1|g(t) in 1981SeZW and 0.9~ns~{I+4-2} from 145.0|g(t) in 1981SeZW 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_comment:
J$115.6|g to (5/2+), 231.2 |g to (9/2-), 369.3|g to (7/2-); band head of a rotational band 
CONF$|n5/2+[413], |a=-1/2 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$142.1|g to (7/2+), 272.0|g to (11/2-), 301.4|g to (5/2+), 417.0|g to (9/2-), 555.1|g to (7/2-); band member 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J$139.2|g to (9/2+), 233.9|g to (13/2-), 393.3|g to (7/2+), 479.7|g to (11/2-) and 624.7|g to (9/2-); band member 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
J$177.0 |g to (17/2-), 557.1|g to (15/2-); band member 
T$from the Doppler broadening of the 557.3-keV line in 2012Sm02. The uncertainty is estimated by the evaluators as a sum of the statistical and the systematical uncertainties (2012Sm02) 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
J$165.2|g to (21/2-), 694.0|g to (19/2-); band member 
T$from the Doppler broadening of the 693-keV line in 2012Sm02. The uncertainty is estimated by the evaluators as a sum of the statistical and the systematical uncertainties (2012Sm02) 
MOME2$3.5 eb {I4} from DPM lifetime measurements in {+248}Cm SF decay (2012Sm02) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
T$from the adopted levels; Other: 0.80~ns~{I15} from 94.9|g(t) in 1981SeZW; Also, 1.1~ns~{I2} from x-ray-ce(t) coinc. in 1970Wa05 
MOMM1$-0.224~{I28} from g=-0.064~{I8} in 2006Or05 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
T$from the adopted levels; Other: 0.75~ns~{I15} from 138.1|g(t) in 1981SeZW 
MOMM1$-0.14~{I18} from g=-0.03~{I4} in {+252}Cf SF decay (2006Or05) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
T$weighted average 0.6~ns~{I2} from 283.1|g(t) in 1981SeZW and 0.9~ns~{I+4-2} from 145.0|g(t) in 1981SeZW 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
T$from 556.7|g DPM in {+248}Cm SF (2012Sm02). |DT{-1/2} is the sum of the statistical and the systematical uncertainties given in 2012Sm02 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
T$from 693.5|g DPM in {+248}Cm SF (2012Sm02). |DT{-1/2} is the sum of the statistical and the systematical uncertainties given in 2012Sm02 
MOME2$3.5 eb 4 from DPM lifetime measurements in {+248}Cm SF decay (2012Sm02) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
T$Other: 0.54~ns~{I25} and 0.54~ns~{I25} from centroid-shift method with Ge detectors in 1985Se02 and 1984LhZZ, respectively 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$From |b{+-} decay curves (1995Jo02) Others: 8.4 s {i5} via (55,86,430,466,595,618|g)-decay curves (1977Ti02); 8.2 s {i10} (1976KaYO), 11 s {i2} (1972Tr08), 9.5 s {i5} (1969Ha59), 7.9 s {i12} (1969WiZX) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$from recoil-distance Doppler shift in {+252}Cf SF decay (1974JaZN). Others: 0.75 ns {i15} (1970Ch11); 1.2 ns {I1} from {+252}Cf SF decay (2006Hw01) 
MOMM1$Measured with Gammasphere using time-integral perturbed angular correlations (2004Sm04) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$measured from Doppler-broadened line shapes analysis; value based on the assumption that the transition quadrupole moment=2.85 {I13} for all members of the g.s. band with 8<J<12 (1996Sm04). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$measured from Doppler-broadened line shapes analysis; value based on the assumption that the transition quadrupole moment =2.85 {I13} for all members of the g.s. band with 8<J<12 (1996Sm04). 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$measured from Doppler-broadened line shapes analysis; value based on the assumption that the transition quadrupole moment =2.85 {I13} for all members of the g.s. band with 8<J<12 (1996Sm04).The evaluators assume that the 889.9|g of 1996Sm04 is the same as the adopted 896.7 keV gamma 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
G$Measured with the time-integral perturbed angular correlation technique 
T$ from |g(t) (2006Hw01) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$ from line-shape analysis for 889.9|g (1996Sm04). The evaluators assume that 889.9|g is the same as 896.6|g from 2002Xu03 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$|D<r{+2}>({+106}Mo,{+92}Mo)=+2.04 fm{+2} {I13} (2009Ch09); uncertainty is systematic; statistical uncertainty is 0.002 
$ Isotope shift({+106}Mo,{+92}Mo)=-4836 MHz {I56} (2009Ch09); total uncertainty is given; statistical uncertainty is 8 
T$from 'adopted levels, gammas' dataset for {+106}Mo in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=31.4 ps {I+134-103} (statistical uncertainties of +13.0-9.9 ps and systematic uncertainties of +3.2-2.9 ps combined in quadrature by the authors). This value was compared by the authors to |t=36.6 ps {I74} in 2003Hu07 (Phys.Rev. C67, 054315). 
$Transition quadrupole moment Q{-t}=4.1 {I+8-7} (2017Ra05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$mean lifetime |t=1.86 ns {I13} (2020Ha14, |b|g(t) using plastic scintillator for |b detection and LaBr{-3} for |g detection. First measurement of lifetime of this level 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<3062 {I16}, deduced from Q(|b{+-})=9931 {I10} and S(n)({+106}Mo)=6869 {I13} (2017Wa10) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T 3.5 s {I5} via (64,400,483,784|g) decay curves (1977Ti02). Others: 4 s {I1} (1977Ti02), |?5 s (1972Tr08) from 102.7|g growth-decay curve of chem separated technetium daughter 
J$From 348 |g E1 from 348.3 level assigned (7/2-) (2005Ur02). Earlier (7/2-) was suggested for the g.s. (2004Hu02,1997Hw03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_comment:
E,J,T$ from 2006Pi14. Half-life measured by time spectrum of the isomer.This value updates previous (470 ns 30) from 1999Ge01, same group This level is different from the 66.0, (3/2+) level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
E,J,T$ from 2006Pi14. Half-life measured by time spectrum of the isomer. This level is different from the 66.0, (3/2+) level 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: NS
level_comment:
g-factor from time-differential perturbed angular correlation (1976ChZD) 
T$from 1999Ge01. T{-1/2}(65|g)=238 ns {I7} (1974ClZX), 38 ns {I7} (1974ClZX), 245 ns 15 (1976ChZD) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1995Jo02. Others: 1.5 s {i4} (1972Tr08) from 242|g growth-decay of chem separated technetium daughter, 0.9 s {i4} (1970WiZN), 1.5 s {i5} (1969WiZX) 258|g decay curve 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$ from 2009Pe06; systematic uncertainty=0.065 and statistical uncertainty=0.020 combined in quadrature by compilers 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$|D<r{+2}>({+108}Mo,{+92}Mo)=+2.14 fm{+2} {I14} (2009Ch09); uncertainty is systematic; statistical uncertainty is 0.002 
$ Isotope shift({+108}Mo,{+92}Mo)=-4992 MHz {I63} (2009Ch09); total uncertainty is given; statistical uncertainty is 8 
T$from 'adopted levels, gammas' dataset in ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=29.7 ps {I+115-93} (statistical uncertainties of +11.3-9.1 ps and systematic uncertainties of +2.3-1.9 ps combined in quadrature by the authors). First measurement of lifetime of this state 
$Transition quadrupole moment Q{-t}=3.7 {I+7-6} (2017Ra05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$mean lifetime |t=1.21 ns {I7} (2020Ha14, |b|g(t) using plastic scintillator for |b detection and LaBr{-3} for |g detection. First measurement of lifetime of this level 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<4934 {I18}, deduced from Q(|b{+-})=11210 {I12} and S(n)({+108}Mo)=6276 {I13} (2017Wa10) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$222.2|g E1 from (7/2-) and |g(110.8)|g(222.2)(|q) (2006Ur01) in {+248}Cm SF decay; direct |b{+-} decay feeding to the {+109}Tc ground state (J|p=5/2+) (2012Ku28). Note, that 1997Hw03 ({+252}Cf SF decay) proposed J|p=(7/2-), based on their interpretation, but no experimental evidences were presented by the authors 
T$weighted average of 0.70 s {I+4-6}, using implant-|b|g(t) in 2015Lo04, 0.66 s {I5}, using |b(t) and the maximum likelihood method in 2009Pe06 and 0.53 s {I6} using |b-K|ax(t) in 1992Ay02, and 1992PeZX 
CONF$|n5/2+[402] (g{-7/2}) orbital. The assignment is tentative. The strong |b{+-} feedings to the |pg{-9/2}-dominated levels in the daughter {+109}Tc nuclide would support |ng{-7/2} over |nd{-5/2} assignment 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_comment:
J$Tentative assignment proposed in 2012Ka36 (Be({+238}U,F|g)), based on expectations from the Nilsson model. Similarity to known isomers in neighboring odd-N nuclei 
T$using 69.7|g(t) in 2012Ka36 (Be({+238}U,F|g)). 
CONF$|n1/2+[411] expected from the Nilsson model and similarities to known isomers in neighboring odd-N nuclei. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$78.2|g E1 to (7/2+); proposed configuration 
CONF$|n7/2-[523] orbital. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$The number of implanted {+109}Mo nuclei in the isomeric state was 8.3|*10{+3} (2012Ka36) 
T$using 69.7|g(t) in 2012Ka36. 
CONF$likely |n1/2+[411] orbital from the comparisons with neighboring nucleus {+107}Mo (2012Ka36) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$Weighted average of 0.330 s {I28} (using |b(t) and maximum likelihood method in 2009Pe06), 0.340 s {I11} (using |b(t) and least-squares fit method in 2009Pe06), 0.26 s {I1} (using 121|g-|b(t) in 2004Wa03), 0.28 s {I2} (using 142|g-|b(t) in 2004Wa03), 0.30 s {I4} (using 142|g-|b(t) and K|a| x ray(t) in 1994Lh02), and 0.25 s {I10} (using K|a| x ray(t) in 1992Ay02). Other: 0.30 s {I4} (2002Pf04 compilation) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
E$The doppler broadening observed for the depopulating 748.2|g in {+248}Cm SF decay (2004Ur03) implies a very short lifetime for this state 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
E$The doppler broadening observed for the depopulating 748.2|g implies a very short lifetime for this state 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-N$from Adopted Levels for {+110}Mo in ENSDF database 
$Theoretical T{-1/2}{-1/2}=1.65 s, %|b{+-}n=0.0 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 296 ms {I17} (Adopted Levels of {+110}Mo in ENSDF database; value based on several measurements) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: NS
level_comment:
T$mean lifetime |t=0.84 ns {I4} (2020Ha14, |b|g(t) using plastic scintillator for |b detection and LaBr{-3} for |g detection. First measurement of lifetime of this level 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: NS
level_comment:
T$mean lifetime |t=0.84 ns {I4} (2020Ha14), |b|g(t) using plastic scintillator for |b detection and LaBr{-3} for |g detection. First measurement of lifetime of this level 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=80.8 ms, %|b{+-}n=0.03 (2003Mo09) 
J$from 2011Ku16 from systematics of neighboring nuclides and particle-plus-rotor model calculations. Others: 1/2+ from systematic trends (2012Au07), 7/2- in theoretical prediction (1997Mo25) 
T$weighted average by 2011Ku16 from their decay curves for 10 |g rays and x rays (individual values in ms are: 176 {I35}, 190 {I30}, 266 {I60}, 173 {I17}, 163 {I20}, 196 {I30}, 212 {I25}, 185 {I25}, 180 {I30}, 230 {I40} and 260 {I100}). Others: 196 ms {I5} (2015Lo04, from (implanted ions)|b correlated curves in time and position using maximum likelihood method); 200 ms {I+41-36} (2009Pe06, from maximum likelihood method of time differences of implantations and correlated |b decay events). Values in 2015Lo04 and 2009Pe06 could correspond to both the activities reported in 2011Ku16 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2-,9/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ERR=AP;ISO=M
level_comment:
E$x=100 {I50} (from systematic trends, 2012Wa38) 
T$from 2011Ku16. The half-life is only an estimate by 2011Ku16 since it could not be distinguished from the half-life of the g.s. 
J$from 2011Ku16 from systematics of neighboring nuclides and particle-plus-rotor model calculations. Others: 7/2- from systematic trends (2012Au07), 7/2- in theoretical prediction (1997Mo25) for g.s. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) using maximum-likelihood analysis (2011Ni01). A value of |?103 ms is predicted in 2003Mo09 
%B-N$Calculated %|b{+-}n=4.4 in 2003Mo09 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=580.7, %|b{+-}n=0.31 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 120 ms {I+13-11} (Adopted Levels of {+112}Mo in ENSDF database; value taken from 2011Ni01: Phys. Rev. Lett. 106, 052502; from same lab as 2015Lo04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=121 ms, %|b{+-}n=3.4 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+113}Mo 
J$3/2+ from systematic trends (2012Au07), 5/2- in theoretical prediction (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 78 ms {I+6-5} (2011Ni01, from the analysis of the (ion)|b-correlated decay curve). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=103 ms, %|b{+-}n=4.4 (2003Mo09) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 60 ms {I+13-9} from ion-|b correlations (2011Ni01). See 2015Lo04 for comparison of their experimental value with theoretical values. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=49.2 ms, %|b{+-}n=6.2, %|b{+-}2n=0.02 (2003Mo09) 
$Measured |s=1150 pb (2010Oh02), systematic uncertainty approximately 40%. 
$Probability of misidentification of {+115}Mo isotope<0.001% (2010Oh02) 
E$measured half-life is assumed to correspond to the ground state of {+115}Mo 
J$1/2+ predicted in calculations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 51 ms {I+79-19} from ion-|b correlations (2011Ni01). See 2015Lo04 for comparison of their experimental value with theoretical values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: US
level_comment:
J$the authors state that the measured large isomeric ratio (>0.9) indicates a lower spin for this isomer than that of ground state according to the in-flight fission and fragmentation mechanism. 
T$from 188|g(t) 
$Isomeric ratio>0.9 (2022Wu18) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=50.6 ms, %|b{+-}n=7.8, %|b{+-}2n=0.0 (2003Mo09) 
$Measured |s=72 pb (2010Oh02), systematic uncertainty|?40% 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
$Probability of misidentification of {+116}Mo isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=42.9 ms, %|b{+-}n=16.8, %|b{+-}2n=0.32 (2003Mo09) 
$Measured |s=4 pb (2010Oh02), systematic uncertainty|?40% 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 
$Probability of misidentification of {+117}Mo isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decays, thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=31.9 ms; %|b{+-}n=18; %|b{+-}2n=0.0 (2019Mo01) 
$Theoretical T{-1/2}=27.2 ms; %|b{+-}n=11.6, 11.7; %|b{+-}2n=0.32, 0.25 (2021Mi17, %|b{+-}n and %|b{+-}2n for four different fission barriers) 
$Production |s=0.4 pb for Nb setting, 0.27 pb for Pd setting, 30% systematic uncertainty for |s (2018Sh11) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Authors compared experimental value with theoretical predictions from several models. 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=21.6 ms, %|b{+-}n=28, %|b{+-}2n=1 (2019Mo01) 
$Theoretical T{-1/2}=21.9 ms, %|b{+-}n=31.0, %|b{+-}2n=0.8 (2016Ma12) 
$Only one count was assigned to {+119}Mo, for the spectrometer setting on Pd. Misidentification of this isotope is not likely since no events were observed for neighboring hydrogen-like peaks (2018Sh11). 
$Production |s=0.009 pb for Nb setting, 0.27 pb for Pd setting, 30% systematic uncertainty for |s. 
E$it is assumed that the observed event corresponds to ground-state activity. 
J$3/2- from |W{-|n}=3/2- orbital proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 21.6 ms (2019Mo01) and 21.9 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+119}Mo is expected to be <25 ms, based on measured half-lives of 32 ms for {+116}Mo, 22 ms for {+117}Mo, and 19 ms for {+118}Mo, available in literature. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
T${+85}Tc not detected, only a limiting half-life is estimated by 1999Ja02 from measured upper limits on cross sections. Other: <110 ns (Wefers et al., GSI 2001-1, 2000 annual report, page 10). Theoretical |b decay T{-1/2}=70 ms (1997Mo25) suggests negligible decay through this mode. 
$From structure calculations, 1999Ja02 predict ground state as |p5/2[422] oblate state. Others: 3/2+ (predicted, 1997Mo25), 1/2- (systematics,2012Au07) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: MS
level_comment:
J$possible (T=1,T{-Z}=0) analog of {+86}Mo g.s. (T=1) 
T$weighted average of 44 ms {I12} (2001Ga24) and 59 ms {I+8-7} (2001Ki13,2002Fa13). Earlier value from the same group as 2001Ga24 was 47 ms {I12} (1998Lo17,1999Lo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_lifetime_unit: US
level_comment:
J$from comparison with shell-model calculations (2008Ga04), a 6+ T=0 is predicted near this energy, whereas T=0, 5+ lies lower. Possible configuration=|n5/2[422]~#|p7/2[413], K|p=6+ 2000Ch07 suggested 5+ from possible configuration=|n5/2[303]|p5/2[422] 
T$from |g(t) in {+9}Be({+107}Ag,X|g) (2008Ga04 and erratum), almost the same value of 1.11 |ms {I21} was obtained by 2000Ch07 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_lifetime_unit: US
level_comment:
$S(p) allows proton decay mode also 
$The isomeric ratio R=41 {I7} (2009Ga40), where R=N{-isomer}/(N{-ions}(fragment)|g), N{-isomer}=number of ions observed in the isomeric state, N{-ions}=total number of ions of that nuclear species, F=correction factor for in-flight losses, g=correction factor for finite measuring time period 
J$from comparison with shell-model calculations (2008Ga04), a 6+ T=0 is predicted near this energy. 5- is also possible 
T$from |g(t) (2009Ga40,2008Ga04) 
$Possible configuration=|n5/2[422]~#|p7/2[413], K|p=6+ 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T from 2001Ki13; also given by the same authors as 2.4 {I2} (2000StZU), 1.9 {I2} (2000WeZY) and 1.9 {I+3-2} (2000WeZZ). 
%EC+%B+ assumed by evaluator since Q(|a) is negative. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$Inferred from assuming hindered M1 and E1 transitions from the decay of an 7/2+ oblate shape to 5/2+ and 5/2- prolate shapes and comparison with systematics (2009Ga40) 
T$ measured in 2009Ga40 from decay timing of 64|g and 70|g. Other: |?700 ns (2007Re18) 
$R=11 {I5} (2009Ga40) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$from implant-|b(t) using multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16) 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5+,6+,7+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$from log| {Ift}|?4.8 to 6+ and assuming that the spin difference between the 2 isomers should be at least 3. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (2+,3+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
J$from log| {Ift}|?5.3 to 2+ in {+88}Mo. Positive parity expected as both proton and neutron originate from g9/2 orbitals. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$from implant-|b(t) using multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). Value is combined result for the ground state and the isomer. 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). Value is combined result for the ground state and the isomer. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: S
level_comment:
E$from difference in mass excess values of ME=-61670 keV {I4} for the ground state and -61600 keV {I5} for the isomer (2019Vi05). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$from time decay of 119|g (1991He04). Other: 20 s {I4} for a single activity (1983OxZZ,1981OxZZ, average of 17 s {I5} for 119|g; 23 s {I5} for 269|g) 
$Configuration=|pg{-9/2} (1995Ru03) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$%IT<0.01 from RUL(E4)=100 
T$from decay curve for 269|g (1991He04). Other: 20 s {I4} for a single activity (1983OxZZ,1981OxZZ, average of 17 s {I5} for 119|g; 23 s {I5} for 269|g) 
$Configuration=|pp{-1/2} (1995Ru03) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: S
level_comment:
T$from 809.8|g(t) (1981Ox01). Other: 50.7 s {I63} (2012Ka12, based on analysis of data in 2008We10). 
E$tof spectra in Ni({+40}Ca,X) reaction give population fractions of 89 % {I5} and 11 % {I5} for the ground state and isomer, respectively (2012Ka12). As high-spin levels are more favorably produced in these reactions, the ground state is assigned as the J|p=(8+) level. 
J$from systematics of J|p=8+ states in neighboring odd-odd {+92}Tc(N=43), {+90}Nb(N=49) and {+88}Nb(N=47) nuclei and supported by shell-model calculations (1993Ru03). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$shell-model calculations predict a J|p=6+ state at 106 keV (1993Ru03); in {+90}Nb a 6+ isomeric level lies at 123 keV with T{-1/2} = 60 |ms, which could explain the non-observation of a depopulating 104-keV transition. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
E$from Penning-trap mass measurement (2012Ka12): mass excess=-70724.7 keV {I11} for {+90}Tc g.s. and -70580.6 keV {I13} for {+90}Tc isomer (2012Ka12) 
T$from two component fit to 944.7|g+948.1|g(t) (1981Ox01). Other: 7.9 s {I2} (1974Ia01). 
J$theoretical prediction is 2+ but 1+ is suggested from log {Ift} value to 0+ and 2+ states in {+90}Mo. If g.s. feeding is not properly determined then 2+ is possible (2012Ka11) 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J$based on systematics of J|p=8+ ground states in neighboring odd-odd {+92}Tc(N=49), {+90}Nb(N=49) and {+88}Nb(N=47) nuclei. Shell-model calculations predict J|p=8+ for the g.s. of {+90}Tc. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
T$from the Adopted Levels 
E$from Penning-trap mass measurement (2012Ka12): mass excess=-70724.7 keV {I11} for {+90}Tc g.s. and -70580.6 keV {I13} for {+90}Tc isomer (2012Ka12). Fit to tof spectra yields fractions of lower-mass and and higher mass state as 89 % {I5} and 11 % {I5}, respectively (2012Ka12). As the high-spin state is more favorably produced in the reaction utilized in 2012Ka12, the ground state is most likely the high-spin level and the isomer the low-spin level. 
J$from the Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: MIN
level_comment:
J log| {Ift}=5.2 for |e decay to 9/2+, 2451 level in {+91}Mo; shell-model systematics. Probable configuration=(|p g{-9/2}). 
T from |g(t) of |g lines which could be assigned to the decay of the high-spin {+91}Tc (1976De37). Other measurement: 3.12 min 5 (1974Ia01) from |b{++} activity. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J log| {Ift}=5.7 to 3/2-, 1156 in {+91}Mo; (HI,xn|g) systematics. Probable configuration is (|p p{-1/2}) (1994Ru01). 
T from |g(t) of |g lines assigned to low-spin {+91}Tc |e decay (1976De37). 
%EC+%B+ %IT<1 estimated in {+91}Tc |e decay (1975DeZX) based on absence of growth in decay curves. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J gammas to (9/2)+ and (7/2)+ levels favoring J|p=(5/2+,7/2,9/2,11/2+); stretched Q 1138|g from (11/2+) 1533. 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J |DJ=1 d+Q 1533|g to (9/2)+ g.s.; |DJ=1 411|g from (13/2-) 1943 level; J|p=(9/2-) suggested in ({+40}Ca,|a3p|g) and in ({+40}Ca,3p|g) is not consistent with DCO ratios for 1533|g and 411|g in ({+36}Ar,3p|g). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
J (E1+M2) 108|g to (15/2+) 2045; (E1+M2) 332|g to (17/2+) 1821. 
T Other value: 0.8 ns {I2} from ({+40}Ca,|a3p|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: JAP(51/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES FIT. 
E no connecting transitions to normal deformed structures have been found. 
J from coincidence observation of SD band transitions with 1206|g from 10502, (47/2+) level and assuming an average spin cost of 2 units to connect to the 47/2+ level. 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: NS
level_comment:
T weighted average of 1.09 ns {I6} (1994Ru01) and 1.04 ns {I21}, 0.9 ns {I3}, 0.8 ns {I6} (1995Ka06). 


level_energy_unit: KEV
level_spin_parity: (8)+
level_lifetime_unit: MIN
level_comment:
J log| {Ift}=5.4 for {+92}Tc |e decay to 8+ (89% branch); log| {Ift}=5.7 to 7+; |e decay to 6+ 2612 level is weak or nonexistent; |s(|q) systematics in ({+3}He,t). 
T weighted average of 4.5 min {I5} (1948Mo18), 4.0 min {I1} and 4.4 min {I4} (1964Va05), 4.52 min {I12} (1985Be12), using method of limitation of relative statistical weights. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: US
level_comment:
J 3+,4+ from ({+3}He,t); J=4 based on Hauser-Feshbach analysis in (p,n|g); E2 56|g to J=(6) 214 level. 
T from (p,n|g). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J 5,6+ from ({+3}He,t); J=5 based on Hauser-Feshbach analysis in (p,n|g); |p=+ probable, by analogy to {+88}Y and {+90}Nb. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ERR=LE
level_comment:
J 259|g is D to (4+); 2241|g from 1+ 2771; 3+,4+ from ({+3}He,t); J|p=1,2-,3+ based on Hauser-Feshbach analysis in (p,n|g). 
T from {+92}Ru |e decay. 


level_energy_unit: KEV
level_spin_parity: (4,6+)
level_comment:
J J=(4,6) from |DJ=1 237|g to (5+) 389; 6+ favored by shell-model calculations (1976Se01) which predict a configuration=((|p g{-9/2}){+3}7/2 ~# (|n g{-9/2}){+-1})6+ level near this energy (1983Fi08). 


level_energy_unit: KEV
level_spin_parity: LE 3
level_comment:
J from ({+3}He,t). If J(626 level) were 4, this level would presumably correspond to 1119 level in ({+3}He,2np|g) whose J would then be limited to (2,3). 


level_energy_unit: KEV
level_spin_parity: (0+,1)
level_comment:
J |g from 1+; log| {Ift}=6.3 {I3} (log| {If{+1u}t}=7.6 {I2}) for weak |e branch from 0+; 585|g to (2+) 577. Possible candidate for 0+ anti-analog state (1976Se01). 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J D 669|g to (9+); (E2) 1355|g to (8)+; |p=(+) based on branching in ({+3}He,2np|g); yrast selectivity in ({+3}He,2np|g) favors J=10. 


level_energy_unit: KEV
level_spin_parity: (7,8)
level_comment:
J |g to J|<6; |g(|q) in ({+3}He,2np|g) allows J=4 to 8 if J(626 level)=6, but strong population in ({+3}He,2np|g) favors high spin (1983Fi08). 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: NS
level_comment:
MOMM1 from g-factor=+0.806 {I20} measured using TDPAD, assuming J=11. 
J measured g-factor is close to that calculated for a configuration=((|p p{-1/2})(|p g{-9/2}){+4}(|n g{-9/2}){+-1}) state, and to that known for analogous 11- state in {+90}Nb (1996Tu03). 
T from time differential perturbed angular distribution in ({+28}Si,p3n|g) (1996Tu03). Other T{-1/2}: 1.9 ns {I4} (DSAM, after corrections for prompt component and deorientation effects; 1994Ar33). 


level_energy_unit: KEV
level_spin_parity: (13+)
level_comment:
E the adopted order of the 636|g-663|g cascade is based on I|g in ({+35}Cl,4p3n|g); E(level)=2637.6 in ({+40}Ca,5pn|g) because, there, the order of the cascade |g's is reversed. 


level_energy_unit: KEV
level_spin_parity: (16+,17+)
level_uncertain: ?
level_comment:
E an alternative placement of the 1786|g (between a 7431-keV (18+,19+) level and the 5646 level) was suggested in ({+40}Ca,5pn|g); however, a 627|g? feeds the 5646 level and the 1786|g is absent in ({+35}Cl,4p3n|g). 


level_energy_unit: KEV
level_comment:
E,J 6701.7 {I25}, (17-,18-) in ({+40}Ca,5pn|g) because, there, the 1986|g was placed feeding the (16-) 4716 level. 


level_energy_unit: KEV
level_spin_parity: (13+)
level_comment:
Note that E(level)=2664.7 in Adopted Levels because, there, the order of the 636|g and the 663|g is reversed. 


level_energy_unit: KEV
level_spin_parity: (17-,18-)
level_comment:
Note that in Adopted Levels, Gammas the 1986|g feeds, instead, the (15-) 4048 level, implying E(level)=6033.7. 


level_energy_unit: KEV
level_spin_parity: (18+,19+)
level_uncertain: ?
level_comment:
E,J 1786|g may, alternatively, feed the (15+) 3587 level directly; in that case, E=5373 {I3} and J|p=(16+,17+) for this level (1994Ar33), as shown in Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (12+)
level_comment:
J a second 12+ state in this vicinity is predicted from shell-model calculations, and 1995Gh02 suggest that this level may be that state. However, J|p=(13-) in Adopted Levels, obviating the need for the Q 622|g feeding this level to have mult=M2. 


level_energy_unit: KEV
level_spin_parity: 5,6+
level_comment:
Configuration=((|p 1g{-9/2})(|n 2p{-1/2}){+-1})5-. However, J|p=6+ is favored in Adopted Levels; if correct, configuration must be incorrect. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
Configuration=((|p 1g{-9/2})(|n 1g{-9/2}){+-1})0+; isobaric analog of {+92}Mo g.s., based on strength of excitation, E(level) and |s(|q) (1973Ha02). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: US
level_comment:
E$Isomeric ratio R=10 % {I1} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
J L=4 in (d,n) and ({+3}He,d); comparison of |m with Schmidt values. 
T from 1948Ku26. Others: 2.7 h {I4} (1939De01), 2.7 h {I1} (1948Mo18). 
|m: from g=1.405 {I14} (1995Hi06); NMR on oriented nuclei. Others: 6.26 {I10} from radiative detection of NMR (1989Ra17, from g=1.392 {I22} (1981Ha16)); 6.2 {I+11-4} from 1977Be19, low temperature nuclear orientation in iron (1989Ra17). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J L=1 in (d,n) and ({+3}He,d); M4 392|g to J|p=9/2+ g.s. 
T from 1950Me21. Others: 45 min {I5} (1939De01), 40 min {I5} (1948Mo18). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J (M1+E2) 681|g to J|p=9/2+; shell-model predictions; J|<7/2 from strength of excitation in (p,|g). 


level_energy_unit: KEV
level_comment:
E from (p,|g). 
J |g from J=3/2 {I6576}, so J|<(7/2). Average resonance yield in (p,|g) is consistent with calculated yield for J|p=7/2-, 5/2- and 3/2+, but this may not Be a reliable indicator of J|p. 


level_energy_unit: KEV
level_spin_parity: (17/2)-
level_lifetime_unit: US
level_comment:
J M2+E3 751|g to J|p=(13/2)+ 1434; 40|g to J|p=(13/2)- 2145; configuration assignment. 
|m: from DPAD (1989Ra17, from data of 1977Ha49); value is corrected for diamagnetic shielding and Knight shift. 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: NS
level_comment:
J E2 |g to (17/2)+; configuration assignment. 
T weighted average of 1.82 ns {I10} from direct timing in ({+40}Ca,5p|g), 1.61 ns {I10} from |a-ce(t) in (|a,p2n|g) and 1.44 ns {I9} from recoil distance Doppler shift in ({+35}Cl,|a2p|g). The unweighted average of these data is 1.62 ns {I11}. 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_lifetime_unit: PS
level_comment:
T from recoil distance Doppler shift. Other: 60 ps {I6} from differential decay curve method. 
J Q |g to (21/2-); configuration assignment. 


level_energy_unit: KEV
level_spin_parity: (9/2,11/2)+
level_comment:
E 4650 20 (E), 4690 (C), 4670 30 (B); w.a.=4656 17 
J log| {Ift}=4.7 from J|p=(9/2)+; 3234|g to (13/2)+ 1434. 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T from recoil distance Doppler shift. 
E in ({+31}P,2p2n|g), the order of the 488|g and 818|g is reversed, resulting in E=5267 for the intermediate level energy. 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
T from differential decay curve method in {+64}Zn({+35}Cl,|a2p|g). 
E in ({+31}P,2p2n|g), the order of the 523|g and 1306|g is reversed, resulting in E=4779 for the intermediate level energy. 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T from recoil distance Doppler shift. 
E in ({+31}P,2p2n|g), the order of the 70|g and 2130|g is reversed, resulting in E=3956 for the intermediate level energy. 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
T weighted average of 106 ps {I7} from recoil distance Doppler shift and 100 ps {I10} from differential decay curve method in ({+40}Ca,5p|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2)-
level_comment:
J allowed {+93}Ru |e decay (10.8 s) is observed from (1/2)- to a 6595 {I5} proton-emitting level; J=3/2 favored by |g(|q) in (p,|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2,3/2,5/2(-)
level_comment:
J |g(|q) in (p,|g); 6208|g to 1/2- 392. Allowed {+93}Ru |e decay (10.8 s) is observed from (1/2)- to a 6595 {I5} proton-emitting level. 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_lifetime_unit: PS
level_comment:
T from differential decay curve method. Other: <0.55 ps from recoil distance Doppler shift. 
J (M1) |g to (33/2+); configuration assignment. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
J L=2 in (d,n) and ({+3}He,d); analyzing power in (pol p,p) IAR; isobaric analog of 5/2+ {+93}Mo(g.s.). See {+92}Mo(p,p) fine structure for data on |?19 fragments of this resonance. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
J L=0 in (d,n) and ({+3}He,d). 
Isobaric analog of {+93}Mo(943 level). See {+92}Mo(p,p) fine structure for data on |?180 fragments of this resonance. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
J L=2 in (d,n) and ({+3}He,d); analyzing power in (pol p,p) IAR. 
Isobaric analog of 3/2+ {+93}Mo(1492 level). 
E from (p,|g). E=9906 {I16} in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
J L=2 in ({+3}He,d); analyzing power in (pol p,p) IAR. 
Isobaric analog of 5/2+ {+93}Mo(1695 level). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
T from (|p{++},|p{+-}). 
Collective giant resonance from coupling of GDR and isobaric analog resonance. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
Resonance in (|p{++},|p{+-}) interpreted as double dipole resonance; |s(|q) has Q shape; |G|?8-10 MeV (1994Mo04). 


level_energy_unit: KEV
level_spin_parity: 5/2,7/2
level_comment:
J calculated yield is too high for J|p=1/2- and J=3/2 and too low for J|p=9/2+, but does not rule out J|p=1/2+. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J Note: this value is inconsistent with log| {Ift}=7.4 from (9/2)+ in {+93}Ru |e decay to this state. Yield also consistent with 3/2+ and possibly 1/2+, but 1193|g feeds 9/2+ g.s. Possibly, this is an unresolved doublet in this study. Adopted J|>7/2. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J note that adopted value is (5/2-). Calculated yields for J|p=1/2- and 3/2- are much higher than experimental yield; those for all other J|p are significantly lower. Adopted J|p=(5/2-). 


level_energy_unit: KEV
level_comment:
J experimental and calculated yields are in reasonable agreement for J|p=1/2+, 3/2+, 5/2- and 7/2-. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=4357 {I2} 
S,L,T from 1976Br02. Other E(p): 4355 (1969El08). Other T{-1/2}: 30 eV (1969El08). 
T from 1976Br02. 
|G{-p}: from 1976Br02. Other |G{-p}: 1.5 eV (1969El08). 
Analog of {+93}Mo(g.s.) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=5302 {I3} 
S,T from 1976Br02. Other E(p): 5310 (1966Mo06), 5295.4 (1974Bi02), 5322 (1971Ri11). Other T{-1/2}: 41 eV (1966Mo06), 37.8 eV (1971Ri11), 48 eV {I5} (1974Bi02). 
|G{-p} from 1976Br02. Others: 12 eV (1966Mo06), 11.0 eV (1971Ri11), 10 eV (1974Bi02). 
Analog of {+93}Mo(943 level) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=5875 
S others: 5890 (1966Mo06), 5890 (1969ClZZ), 5872 (1969Li11), 5874 (1969Ej01, no target thickness correction). 
T from 1969Li11. Others: 27 eV (1966Mo06), 25 eV (1969ClZZ), 27 eV (1969El08). 
Other |G{-p}: 3 eV (1966Mo06), 4 eV (1969ClZZ). 
Analog of {+93}Mo(1492 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=6070 
S other: 6058 (1969Li11). 
T from 1969Li11. Other: 30 eV (1969El08). 
Analog of {+93}Mo(1695 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=6550 
S other: 6550 (1969Li11). 
T from 1969Li11. Other: 30 eV (1969El08). 
Analog of {+93}Mo(2181 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=6820 
S other: 6843 (1969Li11). 
T from 1966Mo06. 
|G{-p} from 1966Mo06. 
Analog of {+93}Mo(2437 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=7180 
S other: 7096 (1969Li11). 
T{-1/2}, |G{-p}: from 1966Mo06. 
Analog of {+93}Mo(2743 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=7280 
S other: 7340 (1966Mo06). 
Other |G{-p}: |?3 eV (1966Mo06) 
Possible analog of {+93}Mo(2881 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=7570 
S others: 7570 (1966Mo06), 7600 (1969Li11). 
Other |G{-p}: 5 eV (1966Mo06) 
Possible analog of {+93}Mo(3160 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=8015 
J L=(0) for E(p)=7980 IAR in 1966Mo06 is inconsistent with this. 
Possible analog of {+93}Mo(3596 level). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=8210 
J L=(2) for E(p)=8220 IAR in 1966Mo06 is inconsistent with this. 
Possible analog of {+93}Mo(3790 level). 


level_energy_unit: KEV
level_comment:
E 3980 in 1971Ri12. 
L,S L=3, S=0.060 (f{-5/2}) or 0.031 (f{-7/2}) from 7 MeV data of 1971Bo33; L=(0), S undetermined (1971Ri12). 


level_energy_unit: KEV
level_comment:
E,L,S 1971Ri12 report E=5150+5180 doublet for which L=2 and S=0.064, 0.037, respectively, for d{-3/2}, d{-5/2} transfer. 1971Bo33, however, obtain L=0 based on a more detailed angular distribution. 


level_energy_unit: KEV
level_comment:
E 5300 in 1971Ri12. 
L 1971Bo33 determine L=0 for this state, but this disagrees with L=2 in ({+3}He,d) for a 5305 {I12} state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
Analog of 7/2+ {+93}Mo(1363 level). S shown for this level in 1970Za09 actually belongs with the d{-3/2} analog state. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
S Assuming [S(9906 level): S(9948 level)] is the same in this reaction as in (p,d). 
Analog of {+93}Mo(1493 level). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
S Assuming [S(9906 level): S(9948 level)] is the same in this reaction as in (p,d). 
Analog of {+93}Mo(1520 level). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
L assumed by 1972Sh28 in their analysis, based on J|p({+93}Mo, 2304 level)=11/2-. J|p=11/2- is consistent with correlation data of 1980Ga01. 
Analog of {+93}Mo(2304 level). 


level_energy_unit: KEV
level_comment:
E double-isobaric analog resonance; not a discrete level. E=19.3, |G comparable with |DE due to target thickness in 1994Mo04. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from 1994Mo04. Resonance interpreted by 1994Mo04 as double dipole resonance; |s(|q) has Q shape; |G|?8-10 MeV (1994Mo04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 17/2-
level_comment:
E in Adopted Levels, this level lies at slightly higher energy than does the 17/2+ member of the 2184 doublet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 17/2-
level_comment:
1 |ms<T{-1/2}<10 |ms (1993Gh01), consistent with T{-1/2} for (17/2-) 2184 level reported in other reactions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 33/2+
level_comment:
E misprinted as 6005 in fig. 1 of 1994Gh07. 
Note that different transitions deexcite this state in Adopted Levels, Gammas; the |g placements shown here are not adopted because all |g's are members of 2-photon cascades whose order has been reversed there, and one cascade actually originates at a lower-energy level. 


level_energy_unit: KEV
level_spin_parity: (17/2)-
level_lifetime_unit: US
level_comment:
T weighted average of 10.5 |ms {I7} (1976Br08) and 10.1 |ms {I3} (1977Ha49). 
g factor: from DPAD (1977Ha49); corrected for diamagnetic shielding and Knight shift. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Proposed by 1973Gr31 as isomeric state responsible for delayed component in cascades originating from (13/2)- and (17/2)+ levels; later studies identified the 2185.1 level as the isomeric state. Level omitted from Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (13/2-,15/2+)
level_uncertain: ?
level_comment:
Since the isotopic assignments of both gammas deexciting this level are tentative, and they have not been confirmed in other (HI,xn|g) reactions, this level is not included in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_comment:
J |g(|q) for the 608|g-1096|g cascade in (|a,p2n|g) is consistent with stretched quadrupole transitions; from this and J|p(2185)=(17/2)-, J|p(3889)=(25/2-). 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_comment:
J |g(|q) for the 1722|g-350|g-750|g-1434|g cascade in (|a,p2n|g) is consistent with stretched quadrupole multipolarity for each transition. From this and J|p(g.s.)=9/2+, 1973Gr31 assign J|p(4257)=(25/2+). However, 1722|g(|q) is also consistent with that for a |DJ=0 transition, implying J|p=(21/2+) as in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: MIN
level_comment:
T$from 1963Ma21. Others: 295 m 10 (1965Ba48), 270 m 12 (1962Mo06). 
J$log| {Ift}=5.1 to 6+ and logft=6 to 8+ 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$weighted average of 52.5 min 15 (1950Me21), 53 min 2 (1962Mo06), and 50 min 2 (1948Mo19). 
E$from {+94}Mo({+3}He,t). 
J$log| {Ift}=5.6 to 2+ 


level_energy_unit: KEV
level_spin_parity: 13+
level_lifetime_unit: NS
level_comment:
T$from |g(t) distribution with respect to beam pulse (1981Le11). It is not clear if the half-life is really due to the 2346.9 level or due to a higher-excited state which decays by an unobserved isomeric transition. A 49-keV |g with T{-1/2}|?5 ns was observed but none of the |g's was found to be in coincidence with it. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
J$from L({+3}He,d)=4, atomic beam (1975Ru06) 
T$from 1962Vi04 (|g's; NaI). See 1983Lu03 for other references 
MOMM1$N/RD. 1995Hi06 measured the NMR's for {+94-96}Tc in Fe and {+95,96}Tc in Ni to resolve discrepancies in |b{-HF} and to deduce a more accurate g-factor (1.321 {i13} compared to original 1.308 {i21} from 1981Ha16). Others: 5.89 {i10} (1989Ra17,1981Ha16. N/rd), 5.82 {i12} (1977Wi10. Static (low-temperature) nuclear orientation) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J$from L({+3}He,d)=1; M4 |g to 9/2+ 
T$from 1959Un01 (|g(t),NaI). Others: see 1978LeZA 
%EC+%B+,%IT$see comment on I|g normalization in {+95}Tc |e decay (61 d) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: FS
level_uncertain: ?
level_comment:
J$1/2+,7/2+ from comparison of statistical theory to 2+ res yield in (p,n|g). Possible isotropic D |g to 1/2- 


level_energy_unit: KEV
level_spin_parity: 9/2
level_comment:
J$from |g(|q) in (p,n|g). log| {Ift}=7.1 {I+5-4} (log| {If{+1u}t}=7.9 {I+5-2})? from 5/2+ discrepant 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: FS
level_comment:
J$from L({+3}He,d)=2. {i3}/2+ from av yields in (p,|g). 1/2-,3/2- from comparison of statistical theory to 2+ and 4+ res yields in (p,n|g) is discrepant 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2-)
level_lifetime_unit: PS
level_comment:
J$|<5/2 from |g(|q) in (p,n|g); |=1/2+ from D,E2 |g to 5/2- (1974Sa19); 3/2+,5/2- from av yields of |g's leading from res's in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2(-),7/2-
level_lifetime_unit: FS
level_comment:
J$3/2+,5/2,7/2- from d,E2 |g's to 3/2- and 7/2+. |=5/2+ from comparison of statistical theory to 4+ res yield in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$3/2,5/2,7/2 from |g's to 5/2+ and 5/2-. 5/2- from comparison of statistical theory to 4+ res yield in (p,n|g). |p=+ from log| {Ift}=5.79 {i4} from 5/2+ is discrepant 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$5/2,7/2,9/2 from |g(|q) in (p,n|g). 5/2-,11/2- from comparison of statistical theory to 4+ res yield in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+,7/2+
level_lifetime_unit: FS
level_comment:
J$log| {Ift}=4.9 from 5/2+. Possible D,Q |g to 9/2+ discrepant with 3/2+,5/2- from av yields of |g's leading from res's in (p,|g) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$5/2,7/2 from |g's to 9/2+ and 3/2+. 7/2+,9/2+ from comparison of statistical theory to 4+ res yield in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J$13/2+,15/2,17/2+ from D,E2 |g's to 13/2+ and 17/2+. 15/2,17/2 from yield in (|a,2n|g); |=15/2 from |g(|q) in (|a,2n|g) 
T$from DSAM in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$log| {Ift}=5.2 from 5/2+; |g to 9/2+. 7/2+,9/2+ from comparison of of statistical theory 4+ res yield in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 19/2
level_lifetime_unit: FS
level_comment:
J$15/2,17/2,19/2 from |g(|q) in (|a,2n|g). 19/2,21/2,23/2 from dipole |g to 21/2+ 
T$from DSAM in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: (17/2,19/2+)
level_lifetime_unit: PS
level_comment:
J$17/2,19/2,21/2+ from |g(|q) in (|a,2n|g). |=19/2-,21/2+ from possible D,E2 |g to 15/2+ 
T$from DSAM in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_comment:
J$from stretched E2 |g to 957.15 keV 11/2+ state 
T$lower limit from DSAM (1975Sa09) and upper limit from |a|g(t) (1975Sh02) 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J$13/2+,15/2,17/2+ from D,E2 |g's to 13/2+ and 17/2+. 15/2,17/2 from yield; |=15/2 from |g(|q) (1975Sa09) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$|=5/2 from |g(|q) (1974Sa19). 1/2,7/2+ from comparison of statistical theory to 2+ res yield; |=1/2 from |g to 9/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$|g(|q) consistent with 5/2 or 7/2 (1974Sa19). 3/2+,5/2+ from comparison of statistical theory to 2+ res yield; |=3/2+ from strong |g to 9/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
$1974Sa19 note the presence a small peak in the tof spectra of 1970Ki01 which may correspond to this state 
J$9/2,11/2,13/2 from |g(|q) (1974Sa19). |=5/2-,7/2-,9/2-,11/2- from comparison of statistical theory to 4+ res yield (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$|<5/2- from |g to 1/2-; |>3/2+ from |g to 7/2+; |=5/2- from large 301|g |d required to fit |g(|q) (1974Sa19). 3/2+,5/2+ from from comparison of statistical theory to 2+ res yield (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$11/2 from |g(|q); |p=+ from comparison of |s to statistical theory (1974Sa19). 11/2+,13/2-,15/2- from comparison of statistical theory to 2+ and 4+ res yields; |=15/2- from |g to 9/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: FS
level_uncertain: ?
level_comment:
J$1/2 or |>13/2 from low |s; |=13/2 from possible d |g to 1/2- (1974Sa19). 1/2+,7/2+ from comparison of statistical theory to 2+ res yield; isotropic |g(|q) to 1/2- (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$probably 7/2 but 5/2 could not be excluded from |g(|q) (1974Sa19). 3/2+,5/2+ from comparison of statistical theory to 2+ res yield (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 9/2
level_comment:
J$9/2 from |g(|q) (1974Sa19). 5/2-,7/2+,9/2+,11/2- from comparison of statistical theory to 4+ res yield; |=5/2- from |g to 9/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$7/2-,9/2- from comparison of statistical theory to 4+ res yield; |=7/2- from weak 2+ res yield (1980Mi06). 7/2 from |g(|q) and |p=- from (M1+E2) |g to 5/2- (1974Sa19) discrepant 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: FS
level_comment:
J$1/2,3/2,5/2 from |g(|q); |=1/2 from d |g to 5/2- (1974Sa19). 1/2-,3/2- from comparison of statistical theory to 2+ and 4+ res yields (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: FS
level_comment:
J$7/2 from |g(|q) (1974Sa19). 1/2-,7/2- from comparison of statistical theory to 2+ res yield; |=1/2- from strong |g's to 9/2+ and 7/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$5/2+ from comparison of statistical theory to 4+ res yield and |g's to 9/2+, 7/2+, and 5/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: FS
level_comment:
J$3/2,5/2 from |g(|q) to (3/2+) (1974Sa19). 1/2-,3/2+,13/2+,15/2- from comparison of statistical theory to 4+ res yield and |=13/2+,15/2- from |g to 3/2+,5/2+ (1980Mi06) discrepant 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2+
level_lifetime_unit: FS
level_comment:
J$5/2+,7/2,9/2+ from d,E2 |g's to 5/2+ and 9/2+. 9/2 suggested by |g(|q) and low |s inconsistent with 3/2+,5/2+,7/2+ from log| {Ift}=5.5 from 5/2+ (1974Sa19) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2(-),7/2-
level_lifetime_unit: FS
level_comment:
J$3/2+,5/2,7/2- from d,E2 |g's to 3/2- and 7/2+ (1974Sa19). 5/2-,11/2- from comparison of statistical theory to 4+ res yield; |=11/2- from |g to 3/2- (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2)
level_lifetime_unit: FS
level_comment:
J$1/2-,3/2,5/2,7/2- from d,E2 |g's to 3/2- and 5/2-. |=7/2- from possible d,E2 |g to 3/2+ (1974Sa19) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$9/2 favored from |g(|q) but 5/2 and 7/2 could not be excluded (1974Sa19). 5/2-,11/2- from comparison of statistical theory to 4+ res yield (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2,9/2(-)
level_lifetime_unit: FS
level_comment:
J$7/2 favored by |g(|q) but 5/2 and 9/2 could not be excluded; |=5/2- from d,E2 |g to 9/2+ (1974Sa19) 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2+
level_lifetime_unit: FS
level_comment:
J$5/2,7/2,9/2+ from d,E2 |g to 5/2+ and d,Q |g to 9/2+; |=7/2-,9/2+ from d,E2 |g to 3/2+ (1974Sa19) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: PS
level_comment:
J$5/2-,7/2+,9/2+,11/2- from comparison of statistical theory to 4+ res yield; |=11/2- from |g to 3/2+,5/2+ (1980Mi06) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
T$from 204|g(t), 766|g(t) and 948|g(t) (2020Sz02). Value is average of 19.12 h {I33}, 19.2579 h {I49}, 19.280 h {I56}, 18.84 h {I77}, and 19.65 h {I125} from |g(t) at different energies and with different |g lines. 
J$from the Adopted Levels of {+95}Tc in the ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
T$from |g(t) (2020Sz02). Value is average of 61.949 d {I35}, 61.991 d {I57}, 61.40 d {I39}, 62.05 d {I18}, 61.98 d {I25}, 61.99 d {I16}, 61.82 d {I21}, 61.69 d {I24}, and 62.5 d {I11} from |g(t) at different energies and with different |g lines. 
E,J$from the Adopted Levels of {+95}Tc in the ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: D
level_comment:
T$from the weighted average of 62.17 d, 62.06 d and 61.42 d measured for 204.12|g(t), 582.08|g(t) and 835.15|g(t), respectively (2022We05). The uncertainty in T{-1/2} is determined by the methodology described in Metrologia 52, 51 (2015). 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: D
level_comment:
T$average of 4.20 d {i4} (1950Co69) and 4.35 d {i4} (1950Me21). Other: 4.2 d {i1} (1948Mo06) 
J$J=7 from NMR (1975Sa18), L=4 in ({+3}He,d) on 5/2+ target. 
$|m from 1975Sa18, other value |m=5.09 {I5} (1995Hi06) from NMR on oriented nuclei. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from 1950Me21. Other: 52 min {i2} (1978Ke10) 
J$|g to 7+ is M3; log| {Ift}=5.5 to 3+ 
$%IT, %|e+%|b{++} from 1967Ce01. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$J=2 from strong excitation in (p,n|g), |p=+ from M1/E1 transitions to positive/negative parity states 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: NS
level_comment:
T$other: 25.9 ns {i4} (1988BeYU) 
J$J=2 from strong excitation in (p,n|g), |p=- from M1/E1 transitions to positive/negative parity states 
$|m from TDPAD. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
%IT$from weighted average of 6 measurements at different proton bombarding energies. Branching is calculated from the total effective, g.s. and isomer cross sections (2021He16) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: Y
level_comment:
J$L=4 in ({+3}He,d), (d,n); M4 transition from level with L=1 
T$from 1998Ko27 (by the number of atoms determined by the isotope dilution method); other: 2.6|*10{+6} y {I4} (1958Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J$L=1 in ({+3}He,d), (d,n); M4 transition to level with L=4 
T$weighted average of 91.4 d {I8} (1998Ko27) and 90.5 {I10} d (1954Bo24); others: 87 {I3} d (1959Un01), 92.2 d {I18} (1993Ko64, superseded by 1998Ko27) 
%EC Deduced from log| {Ift} limit (log| {If{+1u}t}>8.5) for first forbidden unique transition. 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_comment:
J$(M1+E2), |DJ=0,1 |g to 9/2+ g.s.; 11/2+ excluded by excitation function in ({+3}He,pn|g) (1996As01) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-,7/2-)
level_comment:
J$(E2) |g to 3/2-, 580, and (M1+E2) |g to 5/2-, 657; if 1179|g belongs to 1274.5 level then J|p=(1/2-,3/2-) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J$(M1+E2), |DJ=0,1 |g to 3/2-, 580; 1/2- excluded by excitation function in ({+3}He,pn|g) (1996As01) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: PS
level_comment:
J$L=2 in ({+3}He,d); |g excit suggests 3/2 (p,n|g) 
T$0.08 ps|<T{-1/2}|<0.69 ps from DSA of 1325.5|g 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_comment:
J$(M1+E2), |DJ=0,1 |g to 7/2+, 216; 9/2+ excluded by excitation function in ({+3}He,pn|g) (1996As01) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$(M1+E2), |DJ=0,1 |g to 7/2+, 970; 7/2+, 9/2+ excluded by excitation function in ({+3}He,pn|g) (1996As01) 


level_energy_unit: KEV
level_spin_parity: (13/2+,15/2+)
level_comment:
J$(M1+E2), |DJ=0,1 |g to 13/2+, 773; 11/2+ excluded by excitation function in ({+3}He,pn|g) (1996As01) 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
J$|DJ=1, (M1+E2) |g to (25/2+), 3530; (23/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
J$|DJ=1, (M1+E2) |g to (25/2+), 3731; (23/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_comment:
J$|DJ=2, (E2) |g to (25/2+), 2530; (21/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_comment:
J$|DJ=2, (E2) |g to (25/2+), 3731; (21/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_comment:
J$|DJ=2, (E2) |g to (25/2+), 3644; (21/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_comment:
J$|DJ=1, (M1+E2) |g to (29/2+), 4681; (27/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (31/2+)
level_comment:
J$|DJ=1, (M1+E2) |g to (29/2+), 4430; (27/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (33/2+)
level_comment:
J$|DJ=2, (E2) |g to (29/2+), 4681; (25/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (33/2+)
level_comment:
J$|DJ=1, (M1+E2) |g to (31/2+), 5461; (29/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (37/2+)
level_comment:
J$|DJ=2, (E2) |g to (33/2+), 5536; (29/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (39/2+)
level_comment:
J$|DJ=1, (M1+E2) |g to (37/2+), 7017; (35/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_spin_parity: (43/2+)
level_comment:
J$|DJ=2, (E2) |g to (39/2+), 7714; (35/2+) unlikely based on the assumption that spins increase with excitation energy in {+82}Se({+19}F,4n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of: 90 ps {I11} (1976Be34, measured (570|g)(215|g)(t)) and 51 ps {I10} (1974Be24, measured (KLM Auger ce)(216 ce(K) and ce(L))(t)). Other: T{-1/2}|<0.15 ns (1973Ch26). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$mean value (with uncertainty covering both values) of: 0.52 ns {I6} (measured (KLM Auger ce)(108 ce(K))(t) (1974Be24)), 0.37 ns {I2} (measured X(325|g)(t) (1973Ch26)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
E,L$1973Me10 observes L=3 level at 1046 {I15} keV, no level at 1053 keV; 1972Sh28 observes L=(2) level at 1.01 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2+
level_comment:
E,L$1973Me10 observes L=4 level at 1360 {I15} keV, no level at 1374 keV. 
S$0.028 if J=3/2, 0.014 if J=5/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
J$(392|g, 469|g) excit support 3/2 assignment (1982Ka26) 
T$DSA of 392.3|g, 469.0|g, 724.9|g (1984Ad06) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E,T$ from adopted dataset for {+97}Ru in ENSDF database; energy kept fixed in least-squares fit of the level scheme 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=?
level_comment:
J,T$from {+97}Tc Adopted Levels in the ENSDF database (Nov 2009 update) 
MOMM1$measured by 2017Ra01 by high-resolution hyperfine structure splittings for {+97}Tc and {+99}Tc, deduced hyperfine structure parameters A for the atomic g.s., first and second excited states in {+97}Tc and {+99}Tc, and using known magnetic moment |m=+5.6847 {I4} for {+99}Tc g.s. as reference, connected by an expression: |m({+97}Tc)=|m({+99}Tc)[I({+97}Tc)/I({+99}Tc)]x[A({+97}Tc)/A({+99}Tc)] where value of |m for {+99}Tc is from {+99}Tc Adopted Levels in the ENSDF database (July 2017 update); I is measured ion count rate, and A is hyperfine structure parameter deduced from atomic transitions from the first and second atomic levels. 
$Isotope shifts: |D|n{-1}({+97}Tc,{+99}Tc)=+312 MHz {I20} for the first atomic transition of 23265.32 cm{+-1}; and |D|n{-2}({+97}Tc,{+99}Tc)=+102 MHz {I20} for the second atomic transition of 48572.10 cm{+-1} (2017Ra01) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=?
level_comment:
J,T$from {+97}Tc Adopted Levels in the ENSDF database (Nov 2009 update) 
MOMM1$from 2020Kr09 by high-resolution hyperfine structure splittings for {+97}Tc and {+99}Tc and using known magnetic moment |m=+5.6847 {I4} for {+99}Tc g.s. as reference. 
MOME2$from 2020Kr09 by high-resolution hyperfine structure splittings for {+97}Tc and {+99}Tc and using known quadrupole moment Q=-0.129 {I6} for {+99}Tc g.s. as reference. 
$|d<r{+2}>{+99,97}=-0.267 fm {+2} {I35} (2020Kr09). 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: Y
level_comment:
$No |e decay has been detected (1993Ko64) 
J$(2J+1) intensity rule in (p,d) and L({+3}He,t)=6 from 0+ suggest J|p=5+, 6+ for g.s. and 21.8 level. J|p=6+ is preferred for g.s. due to log| {Ift}=14 to a 4+ state in {+98}Ru. This would imply 5+ for 21.8 level 
T$from 1966GoZZ (also 1973Ok05 priv. comm.). Others: 6.5|*10{+6} y or 9|*10{+6} y (1993Ko64), 1.5|*10{+6} y {I7} (1956Ok15), |?10|*10{+4} y (1955Ka26) 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$(2J+1) rule in (p,d) with L(p,d)=2 suggests J|p=3+,4+; but (M1) 43.6|g to (5)+ favors 4+. L({+3}He,t)=2 from 0+ (giving 1+,2+,3+) disagrees with 4+ 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,d)=L(d,t)=2 from 9/2+; L({+3}He,d)=4 from 5/2+; 59.8|g to 21.8, (5)+ level not E2 from RUL, although J|p=3+ is suggested from 2J+1 intensity rule; 56.7|g from (3)- 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$47.9|g from (3)- and M1+E2 99.5|g from (3,4)-. No |g ray from this level has been reported to either the g.s., (6)+ or the 21.8, (5)+ level. It is likely that this level decays through a highly converted transition to the 65.4, (4)+ level. 
T$from |g(t) of 43.6|g-21.8|g cascade. Weighted average of 14.8 |ms {I5}, 14.4 |ms {I5} ((|g,p|g),1978Ba18) 14.6 |ms {I7} ((p,n|g),1976We06), 15.5 |ms {I8} ((p,n|g),1961Sc11). This half-life is assumed to correspond to the 90.8 level. The present data, however, do not exclude this to belong to 73.3 level 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=1 from 5/2+; L({+3}He,t)=(3,1) from 0+; Possible configuration=|p2p{-1/2}~#|n2d{-5/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,d)=L(d,t)=0+2 from 9/2+; 138.3|g M1 to (4)+; 148.0|g E1(+M2) from (3)-. But L({+3}He,t)=2 from 0+ is inconsistent 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$212.7|g M1(+E2) to (3)-; L({+3}He,d)=1 from 5/2+. Configuration=|p2p{-1/2}~#|n2d{-5/2}{+-1}. Strongly populated state is expected to be the 3- (1976Ma16). 


level_energy_unit: KEV
level_spin_parity: (1:5)-
level_comment:
J$221.6|g M1(+E2) to (2,3,4)-; 404.6|g to (3)-; L=(1) from 5/2+ target for a weak peak in ({+3}He,d) disfavors J=5 


level_energy_unit: KEV
level_spin_parity: 4+,5+
level_comment:
E$this level may be the same as 713.6, although the energy difference is much larger than the quoted uncertainty 
J$L(d,t)=0+2 from 9/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+)
level_comment:
$E(p)(c.m.)=3480 (1966Mo06), 3505 {I10} (1971Ki06). IAR of 0+, g.s. in {+98}Mo 
$|G=25 keV {I3} (1971Ki06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_comment:
$E(p)(c.m.)=4300 (1966Mo06), 4330 {I10} (1971Ki06). IAR of 2+, 787 in {+98}Mo 
$|G=34 keV {I2} (1971Ki06) 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from 43.6|g(t). Weighted average of 15.5 |ms {I8} (1961Sc11) and 14.6 |ms {I7} (1976We06). It is assumed that this half-life corresponds to the 90.8 level. The present data, however, do not exclude for it to belong to the 73.3 level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$rounded value from Adopted Levels. The position of the isomeric level is uncertain since no transition to 65 level has been reported. It is either at 91 or 73 keV 
T$weighted average of 14.8 |ms {I5} from K| x ray(t), 14.4 |ms {I5} from 43.5|g(t) and 16.4 |ms {I27} from 21.8|g(t) in 1978Ba18 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
$g=0.50 
E$a peak around this energy can be seen in deuteron spectrum at 8|' in Fig.3 of 1976Fi04 but is not labeled. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
$g=0.18 
E$weighted average of 136 {I3} (1976Ma16) and 139 {I3} (1976Fi04). 1976Fi04 state that the 139 level is not resolved from a neighboring level at 148 
J$(3)- in Adopted Levels 


level_energy_unit: KEV
level_comment:
L$1976Sl06 give L=2 for a 631 group, with C{+2}S=0.087. L=0 (1977Em02) may be due to contribution from 609 group 


level_energy_unit: KEV
level_spin_parity: 6
level_comment:
J$from HFS measurements (2020Kr09) 
MOMM1$from 2020Kr09 by high-resolution hyperfine structure splittings for {+98}Tc and {+99}Tc and using known magnetic moment |m=+5.6847 {I4} for {+99}Tc g.s. as reference. 
MOME2$from 2020Kr09 by high-resolution hyperfine structure splittings for {+98}Tc and {+99}Tc and using known quadrupole moment Q=-0.129 {I6} for {+99}Tc g.s. as reference. 
$|d<r{+2}>{+99,98}=-0.229 fm {+2} {I35} (2020Kr09). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: Y
level_comment:
J$from optical spectroscopy (1958Lo62), Electron-paramagnetic Res (1953Ke49); parity from L({+3}He,d)=4. 
T from 1984Co30. Others: 2.16|*10{+5} y {I6} (1960Bo08), 2.12|*10{+5} y {I4} (1951Fr05), 2.14x10{+5} y {I5} (1966Go10). 
MOMM1 from 1952Wa02, NMR 
MOME2 from 1982BuZE Atomic Beam Mag Res. Other: 1953Ke49 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J M1+E2 |g to 9/2+. E3 |g from 1/2-. 
T average of 0.237 ns {I14} (1973Sh21), 0.192 ns {I10} (1969St04), both from Mossbauer line width, 0.16 ns {I2} (1971Mc02) from cece(t). Other: 0.11 ns {I+8-6} from B(E2) in Coulomb excitation if |d(140.5|g)=+0.13 {I4}. 
MOMM1$from (1993Al23) IPAC. Others: 3.6 {I9} (1973Sh21) Moss, +4.35 {I85} (1969In07) IPAC. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From {+99}Tc IT Decay (6.0072 h) 
J from atomic beam magnetic resonance (1974Ru05). M4 |g to +. 
T Value corrected for ionization chamber source-holder instability (2014Un01). 
T$The half-life depends on the electronic environment of the nucleus. Variations up to |?0.3% have been reported (see 1980Ma03). A value of 6.0067 h {I5} is that evaluated and recommended in 2004Wo02. Other values: 6.0076 h {I12} (2004Sc04), 6.0071 h {I21} (2004Da05), 6.0072 h {I9} (saline solution) and 6.012 h {I3} (acid solution) both from (2002Un02), and 6.0016 {I53} measured in (2011Ki45). 6.0072 h {I9} (saline solution) and 6.017 h {I2} (acid solution), both from 1982HoZJ, 6.0062 h {I7} (1983Wa26), 6.006 h {I2} (1980Ho17), 6.02 h {I1}, 6.049 h {I35} (both 1972Em01), 6.031 h {I12} (1970Le07), 6.014 h {I4} (1969Vu03), 6.006 h {I7} (1966Go22), 5.996 h {I11} (1958Be92). Others: Evaluated data (2004WoZZ); 1994Ya02. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
MOMM1$from 1995Hi06, NMR on oriented nuclei, sign from +3.62 {I5} (1993Al23) IPAC, +3.291 {I63} (1971Wi08) TDPAC. Others: +3.6 {I3} (1965An02,1959Bo43,1968Be75) IPAC, +3.8 {I5} (1958Ra16) 
J L({+3}He,d)=2. E2 |g to 9/2+. 
T from |gce(t) (1971Mc02). Some other measurements give values of about 3.4 ns (see |b{+-} decay). Other: 3.8 ns {I3} (|a,2n|g) (1990An21), 3.44 ns 3 (1993Al23). 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J |g to 7/2+ is |DJ=2, E2; |g to 9/2+ is |DJ=1, D+Q 
T from Doppler shift attenuation in Coul excit (1976Sv02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L({+3}He,d)=2; Coulomb excitation excludes 3/2+. 
T from Doppler shift attenuation in Coul excit (1976Sv02) 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_comment:
J$E1 to 5/2+. 1998Cr01 suggest |p=(+) and assign it to 1/2+[431] band but their excitation function lies within the values for |p=- 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_lifetime_unit: PS
level_comment:
J |g to 9/2+ is |DJ=1, D(+Q); |g to 7/2+ is |DJ=2, E2. 
T from Doppler shift attenuation in Coul excit (1976Sv02) 


level_energy_unit: KEV
level_comment:
J$ 7/2,(9/2+) given in Fig. 4 of 1998Cr01, but not in Table should be ignored as suggested by one of the authors (F.A. RICKEY) over a telephone conversation on May 11, 2001 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
E From {+99}Tc IT decay (6.0072 h). 
g=+1.39 {I25} (1969In07, value recalculated in 1993Al23). Other: 1993Zh41. 
T from 1993Al23. Other: 0.16 ns {I2} ce(t) (1971Mc02); T{-1/2}<0.6 ns from |g(t) (1971Be73). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
Other values: g=+1.316 {I25} (1971Wi08); +1.390 {I17} (1995Hi06). 
T from 1993Al23. Other value: ce(t) 3.61 ns 7 (1971Mc02). Others measured |g|g(t) or |b|g(t): 3.36 ns {I7} (1971Be73), 3.60 ns {I9} (1971Bo13), 3.42 ns {I10} (1968Ra22), 3.40 ns {I10} (1968Se02), 3.59 ns {I5} (1965An02), 3.45 ns {I6} (1965Me08), 3.57 ns {I5} (1959Bo43). 


level_energy_unit: KEV
level_comment:
J$ 7/2,(9/2+) given in Figure 4 of 1998Cr01, but not in Table should be ignored as suggested by one of the authors (F.A. RICKEY) over a telephone conversation on May 11, 2001 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_comment:
J$ (17/2-) given in Figure 4 of 1998Cr01, but not in Table should be ignored as suggested by one of the authors (F.A. RICKEY) over a telephone conversation on May 11, 2001 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L L=3, C{+2}S=0.053 from 1977Ch06. However, the 1977Pe18 measurement at higher energy shows clearly L=1. J=1/2 from J dependence (1977Pe18). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T From Adopted Levels. 
T$The half-life depends on the electronic environment of the nucleus. Variations up to |?0.3% have been reported (see 1980Ma03). The adopted value of 6.0072 h {I9} is that evaluated and recommended in 2014Un01. Other values: 6.0076 h {I12} (2004Sc04), 6.0071 h {I21} (2004Da05), 6.0072 h {I9} (saline solution) and 6.012 h {I3} (acid solution) both from (2002Un02), 6.0067 h {I5} (2004Wo02), and 6.0016 h {I53} (saline solution) in (2011Ki45). 6.0072 h {I9} (saline solution) and 6.017 h {I2} (acid solution), both from 1982HoZJ, 6.0062 h {I7} (1983Wa26), 6.006 h {I2} (1980Ho17), 6.02 h {I1}, 6.049 h {I35} (both 1972Em01), 6.031 h {I12} (1970Le07), 6.014 h {I4} (1969Vu03), 6.006 h {I7} (1966Go22), 5.996 h {I11} (1958Be92). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
$Half-life and decay modes from {+99}Tc Adopted Levels in ENSDF database 
$Half-life and decay modes are from Adopted Levels, Gammas. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
$%|e=0.0026 {I4} for {+100}Tc decay (2008Sj01, absolute counting method). Other: 0.0018 {I9} (1993Ga09, x-ray measurement) 
J$log| {Ift}=4.6 to 0+ 
T$unweighted average 15.27 s {I5} (2001Fu21); 15.9 s {I4} (2002Ab03); 15.5 s {I1} (1995Ha46); 15.8 s {I1} (1969Be69); 15.8 s {I2} (1952Bo30). Weighted average is 15.42 s {I11}, but with reduced |h{+2}=7.3. Others: 17.1 s {I7} (1963Cs01), 17.5 s {I10} (1952Ho17) 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
J$E2 28.5|g to 2+; primary 6564.3|g from 4+,5+ 
T$from |g(t) and/or ce(t) using pulsed beam in (p,n|g), (d,2n|g) and (|g,p|g). The Adopted value is unweighted average of 8.18 |ms {I7} (1980Bi01), 8.46 |ms {I5} (1978Ma36) and 8.15 |ms {I20} (1961Sc11) in (p,n|g), and 8.2 |ms {I3} (1978Ba18) in (|g,p|g). Others: 10.2 |ms {I1} (1979Pi08) in (d,2n|g), 11.5 |ms {I2} (1964Br27) in (|g,p|g) are discrepant 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$E2 43.3|g to (4)+; primary 6520.5|g from 4+,5+ 
T$from |g(t) in (p,n|g) (1980Bi01). Others: 4.6 |ms {I5} in (d,2n|g) (1979Pi08); 16 |ms {I3} (1967Iv04) and 15.5 |ms {I8} (1961Sc11) in (p,n|g) seem discrepant 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$M1 43.6|g to (6)+ and M1 86.8|g to (4)+ 
E$in (d,p), the 290 group corresponds to 287.5+294.9+299.6 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_comment:
E$assignment of this level as one component of the doublet in (d,p) is consistent with L(d,p)(444+460)=0+2 from 9/2+ 
J$M1 166.7|g to (5)+, 113.2|g to (3)+ 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
E$assignment of this level as one component of the doublet in (d,p) is consistent with L(d,p)(444+460)=0+2 from 9/2+ 
J$M1 217.1|g to (6)+; 197.5|g to (3)+ 


level_energy_unit: KEV
level_spin_parity: (2:7)+
level_comment:
J$L(d,p)=0+2 for 586+600 from 9/2+ target gives J|p=4+,5+ for both levels or J|p=4+,5+ for one level and J|p=2+ to 7+ for the other 


level_energy_unit: KEV
level_spin_parity: (3,4,5)+
level_comment:
E$639 doublet in (d,p), probably corresponds to 636 and 640 levels 
J$372.0|g to (3)+ and 348.7|g to (5)+; L(d,p)=0+2 for a doublet from 9/2+ target 


level_energy_unit: KEV
level_spin_parity: (3,4,5)+
level_comment:
J$666.3|g to (3)+ and 429.7|g to (4)-; primary 5835.2|g from 4+,5+; L(d,p)=0+2 from 9/2+ target for 936+950 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$unweighted average of 8.18 |ms {I7} (1980Bi01), 8.46 |ms {I5} (1978Ma36), and 8.15 |ms {I20} (1961Sc11). Methods: 172|g(t), ce(L)(28.6|g)(t) (1980Bi01); 28.6|g(t) (1978Ma36); 172|g(t) (1961Sc11). Others: 10.2 |ms {I1} ce(28.6|g)(t) (1979Pi08) seems discrepant 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from 43|g(t) (1980Bi01). Others: 4.6 |ms {I5} (43|g(t),1979Pi08), 15.5 |ms {I8} (1961Sc11) and 16 |ms {I3} (1967Iv04) from 43|g(t) seem discrepant 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$L=1, 0+ to 0- transition can only occur through tensor-exchange term of NN interaction resulting in a cross section reduced by order of magnitude, thus 0- is not considered. J|p=2- is favored due to small mixture of L=3 needed for a better fit. L=1+3 is also assigned by 2017Fr02 from DWBA fit to measured differential cross section 
$d|s/d|W(q{-max})=0.141 mb/sr (2017Fr02) 
$Relative spin-dipole transition strength=1.06 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.289 mb/sr {I6} 
J$note that in the Adopted Levels, a 355.58 {I4} level is assigned (2,3)+ 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$see J|p comment for 223 level. Note that in the Adopted Levels, a 689 {I10} level is assigned (4+,5+). J|p=2- is favored due to small admixture of L=3 needed for a better fit 
$d|s/d|W(q{-max})=0.048 mb/sr (2017Fr02) 
$Relative spin-dipole transition strength=0.37 fm{+2} (2017Fr02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.218 mb/sr {I5} 
$B(>)=0.13 {I2} for a broad peak at 1400 keV in 1997Ak02; assigned as isospin excitation with configuration=|ng{-7/2}{+-1}~#|pg{-9/2} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.128 mb/sr {I3} 
$B(>)=0.23 {I3} for a broad peak at 2600 keV in 1997Ak02; assigned as isospin excitation with configuration=|ng{-7/2}{+-1}~#|pg{-9/2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$centroid of a broad bump (1997Ak02) 
$Giant resonance and spin-dipole resonance 
$B(>)=23 {I4} (1997Ak02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$centroid of a broad bump (1997Ak02) 
$Giant resonance and a sharp IAR peak near 11.5 MeV 
$B(>)=2.9 {I5} (1997Ak02) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
J$from L=4 ({+3}He,d); g.s. of {+99}Tc,{+97}Tc,{+95}Tc are 9/2+ 
T$weighted av: 14.224 {i8} (1990Ab06), 14.0 min {i1} (1957Ok01), 14.3 min {i1} (1954Wi04). Others: 1941Ma03, 1948Pe03, 1948Mo33 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$M1 |g to 9/2+, J|p=7/2+ for the first-excited state is characteristic of {+99}Tc,{+97}Tc,{+95}Tc. |g from 5/2- 
T from 1976SvZY, 1974SvZZ (ce)(ce)(t), s 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J based on E2 |g decay to 9/2+ and M1+E2 |g decay to 7/2+ state. E(level) follows trend of low-lying 5/2+ states of {+99}Tc,{+97}Tc,{+95}Tc 
T from 1976SvZY, 1974SvZZ (ce)(|g)(t) s-scin 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: US
level_comment:
E syst with 1/2- isomerism in {+99}Tc(143 keV, 6.0 h), {+97}Tc(96 keV, 90 d), and {+95}Tc(39 keV, 61 d) 
J from M2 |g decay to 5/2+ state and L=1 ({+3}He,d) 
T 636 |ms {i8} (1978Ba18) 192|g(t) pulsed beam. Others: 760 |ms {i50} (1970Uy01), 710 |ms {i120} (1964Br27), 850 |ms {i120} (1968Ga17), 862 |ms (1968Io01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$only the 211.9|g is seen in all work, evaluator has adopted the scheme from decay, more measurements than in ({+3}He,pn|g) 


level_energy_unit: KEV
level_comment:
E$only the 602.9|g is seen in all work, evaluator has adopted the scheme from decay, more measurements than in ({+3}He,pn|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$({+3}He,d) L=0 excitation at 1608 keV probably corresponds to this level; observed |g decays to J|<3/2 states 


level_energy_unit: KEV
level_comment:
Analog of {+101}Mo g.s., J|p=1/2+; E(level)=13.5 (3/2+) is resolved 
|G(p)=30 keV {i6}, |G=73 keV {i14} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$probably corresponds with 622-keV state populated in {+101}Mo |b{+-} decay. Level=616 is ruled out by deexcitation to 7/2+ state 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
E$probably corresponds with E(level)=1618 populated via {+101}Mo |b{+-} decay. Levels=1599, 1615 are precluded by |g decays to J=9/2 and/or 7/2 states 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.129 {I8} (at 6|'), 0.283 {I15} (at 10|'), 0.626 {I32} (at 14|'), 0.81 {I4} (at 18|'), 0.588 {I30} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$|s(mb/sr)=1.85 {I9} (at 6|'), 1.39 {I7} (at 10|'), 0.420 {I21} (at 14|'), 0.607 {I31} (at 18|'), 0.434 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.81 {I4} (at 6|'), 0.73 {I4} (at 10|'), 0.235 {I12} (at 14|'), 0.326 {I17} (at 18|'), 0.255 {I13} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.441 {I23} (at 6|'), 0.615 {I31} (at 10|'), 0.346 {I18} (at 14|'), 0.173 {I9} (at 18|'), 0.211 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.610 {I31} (at 6|'), 0.433 {I22} (at 10|'), 0.155 {I8} (at 14|'), 0.169 {I9} (at 18|'), 0.135 {I7} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(mb/sr)=0.0330 {I26} (at 6|'), 0.0530 {I33} (at 10|'), 0.0540 {I34} (at 14|'), 0.0480 {I31} (at 18|'), 0.0270 {I17} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0059 {I6} (at 6|'), 0.0090 {I8} (at 10|'), 0.0130 {I8} (at 14|'), 0.0117 {I10} (at 18|'), 0.0069 {I8} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.147 {I8} (at 6|'), 0.19 {I1} (at 10|'), 0.117 {I6} (at 14|'), 0.0470 {I26} (at 18|'), 0.0610 {I32} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0070 {I11} (at 6|'), 0.0240 {I23} (at 10|'), 0.0260 {I17} (at 14|'), 0.034 {I2} (at 18|'), 0.0250 {I16} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0049 {I7} (at 6|'), 0.0116 {I9} (at 10|'), 0.0163 {I10} (at 14|'), 0.0223 {I13} (at 18|'), 0.0120 {I12} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0390 {I22} (at 6|'), 0.0530 {I33} (at 10|'), 0.0303 {I17} (at 14|'), 0.0145 {I10} (at 18|'), 0.0158 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0370 {I21} (at 6|'), 0.0280 {I17} (at 10|'), 0.0077 {I6} (at 14|'), 0.0130 {I9} (at 18|'), 0.0094 {I8} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0460 {I25} (at 6|'), 0.0270 {I17} (at 10|'), 0.0104 {I7} (at 14|'), 0.0168 {I10} (at 18|'), 0.0083 {I7} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.226 {I12} (at 6|'), 0.167 {I9} (at 10|'), 0.0620 {I33} (at 14|'), 0.080 {I4} (at 18|'), 0.0620 {I33} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0360 {I27} (at 6|'), 0.0270 {I24} (at 10|'), 0.0062 {I6} (at 14|'), 0.0095 {I8} (at 18|'), 0.004 {I1} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0060 {I11} (at 6|'), 0.0150 {I13} (at 10|'), 0.0194 {I13} (at 14|'), 0.0201 {I13} (at 18|'), 0.0060 {I11} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0230 {I15} (at 6|'), 0.0480 {I31} (at 10|'), 0.090 {I5} (at 14|'), 0.114 {I6} (at 18|'), 0.082 {I5} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.065 {I4} (at 6|'), 0.093 {I5} (at 10|'), 0.0610 {I32} (at 14|'), 0.0292 {I17} (at 18|'), 0.0310 {I18} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0500 {I27} (at 6|'), 0.069 {I4} (at 10|'), 0.0510 {I28} (at 14|'), 0.0239 {I14} (at 18|'), 0.0275 {I16} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.543 {I28} (at 6|'), 0.375 {I19} (at 10|'), 0.525 {I27} (at 14|'), 0.204 {I11} (at 18|'), 0.182 {I9} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.319 {I16} (at 6|'), 0.411 {I21} (at 10|'), 0.234 {I12} (at 14|'), 0.128 {I7} (at 18|'), 0.143 {I8} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.426 {I22} (at 6|'), 0.521 {I27} (at 10|'), 0.280 {I14} (at 14|'), 0.144 {I8} (at 18|'), 0.165 {I9} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.285 {I15} (at 6|'), 0.302 {I16} (at 10|'), 0.204 {I11} (at 14|'), 0.108 {I6} (at 18|'), 0.114 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.262 {I14} (at 6|'), 0.359 {I19} (at 10|'), 0.208 {I11} (at 14|'), 0.100 {I21} (at 18|'), 0.116 {I6} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.191 {I10} (at 6|'), 0.249 {I13} (at 10|'), 0.142 {I7} (at 14|'), 0.085 {I5} (at 18|'), 0.093 {I5} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0230 {I15} (at 6|'), 0.0240 {I23} (at 10|'), 0.0099 {I10} (at 14|'), 0.0118 {I9} (at 18|'), 0.0097 {I5} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.097 {I5} (at 6|'), 0.134 {I7} (at 10|'), 0.080 {I4} (at 14|'), 0.0380 {I22} (at 18|'), 0.0460 {I25} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.139 {I8} (at 6|'), 0.18 {I1} (at 10|'), 0.131 {I7} (at 14|'), 0.057 {I3} (at 18|'), 0.068 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.137 {I8} (at 6|'), 0.166 {I9} (at 10|'), 0.138 {I7} (at 14|'), 0.0630 {I33} (at 18|'), 0.068 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0550 {I34} (at 6|'), 0.064 {I4} (at 10|'), 0.0470 {I26} (at 14|'), 0.0170 {I13} (at 18|'), 0.0210 {I15} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.040 {I4} (at 6|'), 0.0240 {I23} (at 10|'), 0.0100 {I11} (at 14|'), 0.0090 {I11} (at 18|'), 0.006 {I1} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.091 {I5} (at 6|'), 0.114 {I7} (at 10|'), 0.079 {I4} (at 14|'), 0.0290 {I18} (at 18|'), 0.0360 {I27} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.063 {I4} (at 6|'), 0.091 {I6} (at 10|'), 0.0380 {I22} (at 14|'), 0.0250 {I24} (at 18|'), 0.0220 {I23} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0570 {I35} (at 6|'), 0.087 {I5} (at 10|'), 0.056 {I3} (at 14|'), 0.0280 {I17} (at 18|'), 0.0320 {I19} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.091 {I5} (at 6|'), 0.131 {I7} (at 10|'), 0.085 {I4} (at 14|'), 0.0390 {I22} (at 18|'), 0.0430 {I24} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.120 {I7} (at 6|'), 0.080 {I8} (at 10|'), 0.108 {I7} (at 14|'), 0.0390 {I28} (at 18|'), 0.0300 {I25} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.089 {I6} (at 6|'), 0.132 {I8} (at 10|'), 0.073 {I5} (at 14|'), 0.0370 {I21} (at 18|'), 0.0390 {I22} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.066 {I5} (at 6|'), 0.104 {I7} (at 10|'), 0.065 {I4} (at 14|'), 0.0340 {I26} (at 18|'), 0.0360 {I27} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.040 {I5} (at 6|'), 0.050 {I6} (at 10|'), 0.0350 {I27} (at 14|'), 0.0160 {I22} (at 18|'), 0.0220 {I23} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.037 {I5} (at 6|'), 0.063 {I5} (at 10|'), 0.0530 {I33} (at 14|'), 0.0230 {I23} (at 18|'), 0.0210 {I23} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.158 {I9} (at 6|'), 0.194 {I12} (at 10|'), 0.140 {I8} (at 14|'), 0.072 {I4} (at 18|'), 0.078 {I4} (at 22|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.121 {I7} (at 6|'), 0.148 {I10} (at 10|'), 0.074 {I5} (at 14|'), 0.0470 {I31} (at 18|'), 0.0500 {I32} (at 22|') 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (4,5)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
%IT A very weak it decay is proposed by 1969Bl16 from the observation of a high-energy |b branch, which belongs to |b{+-} decay of {+102}Tc (5.28 s) 
E 300|+200 keV is deduced from E|b measurements by 1969Bl16 (see {+102}Tc it decay). From the observed level density in ({+3}He,p) and (d,|a), this excitation energy becomes improbable as fast |g-decay would be possible. However, as a high spin is proposed for a level at 20 keV, this level should be considered as a primary candidate for this isomeric state. 
J from |b-branches observed in {+102}Tc |b{+-} decay (4.35 min) and |g-deexcitation pattern of the levels fed. 
T from 1970Hu02. Other: 1957Fl14 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E may be same as the 4.35-min {+102}Tc isomer (see its energy discussion) 
J from relative excitation probability in ({+3}He,p) and (d,|a), a high spin was proposed (1982De03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
J from relative excitation probability in ({+3}He,p) and (d,|a), a high spin was proposed (1982De03) 


level_energy_unit: KEV
level_spin_parity: (0+,2+)
level_uncertain: ?
level_comment:
J based on assumption of M1 multipolarity of 211|g and the absence of |b{+-} branching to this level 
E the order of the 211.7 and 148.2 |g's is not well established. If the order is interchanged, there would be a level at 148.19 {i3} rather than at 211.66 {i3}. The position at 211.66 keV is favored from the absence of some |g-transitions (see 1980De06) and the observation of a 213 level in {+104}Ru(d,|a). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J the angular distribution of the p group corresponding to the unresolved 509 and 526 levels is consistent with L=(4+6), J|p=(5+). 


level_energy_unit: KEV
level_spin_parity: (0+,2+)
level_uncertain: ?
level_comment:
E the order of the 211.7 and 148.2 |g's is not well established. If the order is interchanged, there would be a level at 148.19 {i3} rather than at 211.66 {i3}. The position at 211.66 keV is favored from the absence of some |g-transitions (see 1980De06) and the observation of a 213 level in {+104}Ru(d,|a). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J the angular distribution of the p-group, corresponding with the unresolved 509 and 526 levels, is consistent with L=(4+6), J|p=(5+). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_comment:
Suggested Nilsson configuration: 5/2[422] 
T from growth-decay of 210|g in {+103}Ru (1977Ti02,1976KaYO). Others: 55 s {I3} (1975Ba60), 50 s {I2} (1972Tr08), 50 s {I4} (1965FeZZ), 50 s {I5} (1963Ki12) 
J L=2 in (d,{+3}He), L=2 and Ay positive in (pol t,|a). 


level_energy_unit: KEV
level_comment:
E possible unresolved multiplet. Close-lying triplet observed in |b decay of {+103}Mo. 1981Fl02 give E=663 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
1981Fl02 give L=(3), J|p=(5/2-), C{+2}S=0.40, for possible unresolved multiplet. Peak too broad to be a singlet. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
In column with level energies of table 2 of 1983De20 the positions of the 1766 and 1727 levels should be changed 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: MIN
level_comment:
J$shell-model consideration, the observed feeding of the 2+ and 4+ levels suggest J|p=2-,3,4-. 2- is not likely on the basis of systematics (1978Su03) and |p=+ is expected from shell-model arguments 
T$weighted average of 18.0 min {I3} (1972Tr08), 18.2 min {I5} (1975Ti03), 18.4 min {I3} (1978Su03). Others: 18 min {I1} (1956Fl25), 17.3 min {I2} (1969WiZX) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MIN
level_comment:
J$band head of rotational band; direct feeding to 3/2- state in {+105}Ru 
T$weighted average of 7.6~min~{I1} (1976KaYO), 7.86~min~{I18} (1975RaZL) 7.6~min~{I1} (1975Su02), 7.7~min~{I3} (1972Tr08), 7.7~min~{I4} (1967Ka14), and 7.7~min~{I2} (1962Ki07) 
CONF$|p3/2-[301] 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$160.5|g to (5/2-), 236.9|g to (3/2-); strong feeding from the (5/2-) in {+105}Mo; yrast state assumed, however (5/2-) can not be excluded 
CONF$|p5/2-[303] 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$129.0|g M1+E2 to (7/2+), 193.2|g to (5/2+); weak feeding from the (5/2-) in {+105}Mo 
CONF$|p7/2+[413] 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
J$156.0|g to (5/2-), 218.4|g to (5/2+), 303.8|g to (3/2-); band head of a 1/2+ rotational band 
CONF$|p1/2+[431] 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2-)
level_comment:
J$178.2|g to (7/2-), 376.0|g to (5/2-); observed only in {+105}Mo |b{+-} decay (35.6~s), strong feeding from (5/2-) in {+105}Mo 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+,9/2+)
level_comment:
J$321.7|g to (7/2+), 411.1|g to (5/2+); no decay branches to (1/2+) and (3/2+); weak feeding from the (5/2-) in {+105}Mo 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+,9/2+)
level_comment:
J$414.2|g to (7/2+), 478.3|g to (5/2+); no decay branches to (1/2+) and (3/2+); weak feeding from the (5/2-) in {+105}Mo 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$697.7|g to (7/2-), 893.8|g to (7/2+), 895.7|g to (5/2-), 957.7|g to (5/2+), 1043.2|g to (3/2-), weak feeding from (5/2-) in {+105}Mo 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
J$2325.4|g to (9/2-), 2618.5|g to (5/2-), 2681.2|g to (5/2+); direct feeding from (5/2-) in {+105}Mo 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
T$from the adopted levels; Others: 16~ns from FF-|g(t) in 1970Jo20; >6 ns in 1981SeZW 
CONF$|p7/2+[413] 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_lifetime_unit: S
level_comment:
T from 270|g-decay curve (1969WiZX). Others: 36 s {I1} (1972Tr08) semi |g-decay curves, rapid technetium chem; 37 s {I4} (1965Vo06), 36 s {I4} (1970HeZH,1980Su01) 
J |b{+-} branch to J|<2 states ({+106}Ru) predominant 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$From systematics (2004Ur07) 
T$from 1969WiZX. Others: 21.0 s {I10} (1972Tr08) |g-decay curves; 21 s {I2} (1972Tr08) growth-decay of {+107}Ru in technetium activity. Others: 1943Bo03, 1965Vo06 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E$the relative order of the 20.0|g and 45.6|g is not established in {+107}Mo |b{+-} decay so a level at 20.0 instead of at 45.6 could be possible; however, a 2-component T{-1/2} value (6 ns and 194 ns) measured in SF for 45.6|g suggests that it lies below 20.6|g and that T{-1/2}(45.6)=6 ns {I2} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: NS
level_comment:
g-factor: from {+252}Cf SF decay 
T$from |b|g and |g|g coin (1986OhZZ). Others: 238 ns {I7} (1974ClZX), 245 ns {I15} (1976ChZD), 194 ns {I35} (1974ClZX). All from {+252}Cf SF decay. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$E|b=5253 {I90} (1989Gr23) from coin with 301|g and 785|g. E|b=5300 {I85} for coin with 384|g, so 384|g could belong to some other level 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: S
level_comment:
J$M1+E2 |g from 1+, log| {Ift}=6.2 to 2+. Probable |b{+-} branch to (3+) 
T$from 1970WiZN. Others: 5.0 s {i2} (1972Tr08), 5 s {i1} (1980Su01) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
%B-N$Other: |<1 (2009Pe06) 
J$direct feeding in {+109}Mo |b{+-} decay (J|p=(5/2+)); systematics of odd-Z Tc isotopes; configuration assignment 
T$weighted average of 1.04 s 11 (using |b(t) in 2009Pe06 and the maximum likelihood method, but the uncertainty was deduced by the evaluators by taking in quadrature the systematic uncertainty of 0.10 and the statistical uncertainty of 0.05), 0.82 {I10} (using |b(t) in 1996Me09), 0.87 s 4 (using 96.1,128.7,195.6|g-|b(t) in 1992PeZX), 0.93 s 3 (using 96.1,122.2,128.5,376.9,445.0|g-|b(t) in 1969WiZX) and 0.9 s 1 (using 68.7|g(t) in 1990Al43). Other: 1.4 s 4 (1976Tr02, from the growth of 206|g(t) in {+109}Ru) 
CONF$K|p=5/2+, |p5/2[422] Nilsson orbital. The assignment is consistent with the observed g{-K} values from in-band cascade-to-crossover branching ratios, compared to g{-K}=1.49 expected from deformed Woods-Saxon model (|b{-2}=0.322, |b{-4}=-0.003 and |b{-6}=-0.005) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$based on comparisons of the structure of low-lying states in {+109}Tc in {+109}Mo |b{+-} decay (2012Ku28); assigned configuration. The assignment is tentative 
CONF$possible |p5/2[303] Nilsson orbital. The assignment is consistent with the observed g{-K} values from in-band cascade-to-crossover branching ratios, compared to g{-K}=0.45 expected from deformed Woods-Saxon model (|b{-2}=0.322, |b{-4}=-0.003 and |b{-6}=-0.005) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$based on comparisons of the structure of low-lying states in {+109}Tc in {+109}Mo |b{+-} decay (2012Ku28). The assignment is tentative 
CONF$possible |p3/2[301] Nilsson orbital (2012Ku28) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$32.2|g (E1) to (3/2-) and 43.6|g (E1) to (5/2-) 
CONF$Likely a member of the K|p=1/2+, |p1/2[431] band (2012Ku28). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$333.3|g to (5/2+), 314.8|g to (3/2-), 282.5|g to (3/2+); direct |b{+-} feeding from (5/2+); band assignment 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
J$471.0|g to (3/2-), 438.6|g to (3/2+); direct feeding in {+109}Mo |b{+-} decay (J|p=(5/2+)) (5/2+) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$386.6|g to (7/2+), 412.0|g to (3/2+); direct feeding in {+109}Mo |b{+-} decay (J|p=(5/2+)) 
CONF$Likely the K|p=7/2+, |p7/2[413] state (2012Ku28). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From Adopted Levels. 2010Ur03 suggests x<30 keV 


level_energy_unit: KEV
level_spin_parity: (2,3+)
level_lifetime_unit: S
level_comment:
$|b{+-}n; Other: |<4 (2009Pe06) 
J$53.3|g, 142.1|g, 262.9|g, 741.4|g from (1+) levels in {+110}Tc; direct population of 2+ and 4+ levels in the daughter nucleus {+110}Ru, following {+110}Tc |b{+-} decay, albeit the decay scheme suffers from the pandemonium problem. The assignment is tentative 
T$Weighted average of 0.820 s {I56} (using |b(t) and maximum likelihood method in 2009Pe06), 0.910 s {I14} (using |b(t) and least-squares fit method in 2009Pe06), 0.78 s {I15} (using |b(t) in 1996Me09), 0.92 s {I3} (using 241|g-|b(t) in 1990Ay02), 1.0 s {I2} (using 241|g-|b(t) in 1990Al43), 1.0 s {I2} (using 241|g-|b(t) in 1976Tr02) and 0.83 s {I4} in 1969WiZX. Other: 0.90 s {I10} (value quoted in 1990Ay02), 0.92 s {I3} (2002Pf04 compilation) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$Direct |b{+-} decay feeding from {+110}Mo |b-decay (J|p=0+). The assignment is tentative 
T$From 1994Lh02 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
E$ the lowest level populated in the two SF decay studies is probably the ground state, although, such studies do not provide definite evidence for this assignment. 2005Ur01, however, rule out 7/2 or 9/2 for the ground state from systematics and model predictions. Such arguments, however, allow 5/2- ground state. 
T$from 1996Me09. Other: 300 ms 30 (1988Pe13) earlier value from the same group as 1996Me09 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$ it is assumed that the lowest level populated in this study is the g.s., 2005Ur01 rule out 7/2 or 9/2, but 5/2- g.s. is possible from systematics and model predictions 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$level noted as 0.0+y in figure 3 of 2006Lu12, however, there is no evidence of existence of isomerism in {+111}Tc. 2005Ur01 consider the lowest state populated in high-spin study as most probably the g.s. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: MS
level_comment:
%B-N$Other: 4 {I1} (2009Pe06) and 2.6 {I5} (1996Me09); calculated value of 0.9 in (2003Mo09) 
J$Significant direct feeding to 2+ levels in {+112}Ru, following {+112}Tc |b{+-} decay could be misleading given that the decay scheme is incomplete (pandemonium); expected configuration from systematics. The proposed assignment is tentative 
T$Weighted average of 290 ms {I20} (2009Pe09), 290 ms {I20} (1999Wa09), 230 ms {I20} (1996Me09), and 280 ms {I30} (1990Ay02). A value of |?135 ms is calculated in 2003Mo09 
CONF$|p5/2+[422]~#|n1/2+[411]; K|p=2+ is favored by the Gallagher-Moszkowski rule. The assignment is tentative. It should be noted that |n5/2+[402] orbital is a ground state in {+111}Ru, while the |n1/2+[411]) one is located at 9.7 keV. The |p5/2+[422] orbital is assigned to the ground state of {+111}Tc 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$258|g to (2+); expected configuration from systematics 
CONF$|p5/2+[422]~#|n1/2+[411]; K|p=3+. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: NS
level_comment:
J$92|g to (3+); non-observation of 350|g to (2+) in 2010Br15. However, J|p=4- assignment cannot be unambiguously excluded 
T$From 258|g(t) in 2010Br15. Others: 218 ns {I+60-43} in (2012Ka36) and <500 ns using 258|g(t) in 2009Fo05 
CONF$|p5/2+[422]~#|n5/2+[402]; K|p=5+ is favored by the Gallagher-Moszkowski rule. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: NS
level_comment:
T$From 258|g(t) in 2010Br15. Others: 218 ns {I+60-43} in (2012Ka36) and <500 ns using 258|g(t) in 2009Fo05 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n=4 {I1} (2009Pe06), 1.5 {I2} (1999Wa09), and 2.6 {I5} (1996Me09) 
T$Weighted average of 290 ms {I20} (2009Pe09) 280 ms {I30} (1990Ay02), 290 ms {I20} (1999Wa09) and 230 ms {I20} (1996Me09) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from Adopted Levels in ENSDF database taken from 1999Wa09: Phys. Lett. 454B, 1 
J$(2+) from systematics in Adopted Levels of {+112}Tc in ENSDF database, but see also discussion about g.s. J|p in 2010Br15: Phys. Rev. C82, 044312 
$Theoretical T{-1/2}{-1/2}=135.1 ms, %|b{+-}n=0.88 (2003Mo09) 
E$the measured half-life is assumed to correspond to the ground state of {+112}Tc 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 271 ms {I15} (Adopted Levels of {+112}Tc in ENSDF database, value based on several references) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
J$configuration=|p5/2[422], oblate minimum from PES calculations (2010Br15). J|p=5/2+ or >5/2 is also proposed by 2007Ku23 from |b feeding pattern and log| {Ift} values from {+113}Tc decay to levels in the daughter nucleus {+113}Ru 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Others: 160 ms {I+50-40} (2009Pe06, MLH analysis of ion-|b correlated decay curve, systematic uncertainty=5 ms, statistical uncertainty= {+50-40 ms}); 170 ms 20 (1999Wa09, earlier measured values of 110 ms {I30} by 1998Ku17 and 130 ms {I50} by 1992Ay02). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: US
level_comment:
J$proposed by 2010Br15 from PES calculations, which show a deep triaxial minimum at |b{-2}=0.29, |b{-4}=-0.02, |g=29.8|' with J|p=5/2-. Also E1 hindrance factors are consistent with systematics (2010Br05) 
T$from |g(t) (2012Ka36). Other: 0.50 |ms {I10} (2010Br15) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: US
level_comment:
$PES calculations by 2010Br15 show a deep triaxial minimum at |b{-2}=0.29, |b{-4}=-0.02, |g=29.8|' 
$Number of implanted fragments=6.7|*10{+5} (2012Ka36) 
T$from |g(t) (2012Ka36). Other: 0.50 |ms {I10} (2010Br15) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=77.7 ms, %|b{+-}n=8.3 (2003Mo09) 
E,J$the measured half-life is assumed to correspond to the ground state of {+114}Tc, but it could be a mixture of the two activities as in 2011Ri01, who reported two activities in {+114}Tc with half-lives of 100 ms {I20}, J|>4 and 90 ms {I20}, J|p=(1+) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Earlier value: 100 ms {I20} and 90 ms {I20} for two activiries (Adopted Levels of {+114}Tc in ENSDF database, values taken from 2011Ri01) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=34.5 ms, %|b{+-}n=25.6 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+115}Tc 
J$3/2- (syst,2012Au07), 5/2+ from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Others: 83 ms {I+20-13} (2011Ni01, from the analysis of (ion)|b-correlated decay curve); 73 ms {I+32-22} (2006Mo07, from ion-|b correlated decay curve). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
E$it is assumed that the observed activity corresponds to the g.s. of {+115}Tc 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 78 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501); 83 ms {I+20-13} (2011Ni01: Phys. Rev. Lett. 106, 052502); 73 ms {I+32-22} (2006Mo07: Phys. Rev. C 73, 035801). Weighted average of all the four values is 78 ms {I2}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=44.0 ms, %|b{+-}n=17.3, %|b{+-}2n=0.07 (2003Mo09) 
E$it is assumed that the observed activity corresponds to the g.s. of {+116}Tc. 
J$there may be two long-lived states according to 2013So17; a high-spin and low-spin with possible configuration= |p5/2[422]~#|n5/2[532] giving rise to J|p=0- or 5-. 2012Au07 propose 2+ from systematics 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 56 ms {I+15-10} (2011Ni01, from the analysis of the (ion)|b-correlated decay curve). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+116}Tc 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 57 ms {I3} (2015Lo04: Phys. Rev. Lett. 114, 192501); 56 ms {I+15-10} (2011Ni01: Phys. Rev. Lett. 106, 052502). Weighted average of the three values is 57 ms {I3}, as it is heavily weighted by the value in 2015Lo04 (compiler's note) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=39.9 ms, %|b{+-}n=25.2, %|b{+-}2n=0.0 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+117}Tc 
J$3/2- from systematic trend (2012Au07), 5/2+ in theoretical consideration (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Other: 89 ms {I+95-30} (2011Ni01, from the analysis of the (ion)|b-correlated decay curve). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decays, thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=30.4 ms; %|b{+-}n=29; %|b{+-}2n=0 (2019Mo01) 
$Theoretical T{-1/2}=51.6 ms; %|b{+-}n=64.0, 31.4; %|b{+-}2n=1.12, 0.89 (2021Mi17, %|b{+-}n and %|b{+-}2n for four different fission barriers) 
E$measured half-life is assumed to correspond to the ground state of {+118}Tc, although, from systematics, two long-lived activities are expected, a low-spin and a high-spin (2013So17) 
J$there may be two long-lived states according to 2013So17; a high-spin and low-spin with possible configuration= |p5/2[422]~#|n3/2[541] giving rise to J|p=1- or 4-,5-,6-. 2021Ko07 propose 2+ for the g.s. from a systematic trend. 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Authors compared experimental value with theoretical predictions from several models. Observed activity could be a mixture of two activities as suggested by 2013So17 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=25.1 ms, %|b{+-}n=32.0, %|b{+-}2n=0.12 (2003Mo09) 
$Measured |s=24 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+119}Tc isotope<0.001% (2010Oh02) 
E$measured half-life is assumed to correspond to the ground state of {+119}Tc 
J$3/2- from systematic trends (2012Au07), 5/2+ from theoretical considerations (1997Mo25). 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=21.8 ms, %|b{+-}n=31.1, %|b{+-}2n=2.5 (2003Mo09) 
$Theoretical T{-1/2}=34 ms, %|b{+-}n=82.8, %|b{+-}2n=0.8 (2016Ma12) 
$Measured |s=2 pb (2010Oh02), systematic uncertainty|?40%. Probability of misidentification of {+120}Tc isotope<0.001% (2010Oh02) 
E$measured half-life is assumed to correspond to the ground state of {+120}Tc 
J$1- to 4- based on |W{-p}=5/2+ and |W{-n}=3/2- from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=45.45, %|b{+-}2n=0.72 (1997Mo25) 
E$measured half-life is assumed to correspond to the ground state of {+121}Tc 
J$5/2+ from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical T{-1/2}=17.8 ms, %|b{+-}n=44.8, %|b{+-}2n=0.92, %|b{+-}3n=0.0 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=27.1 ms, %|b{+-}n=83.5, %|b{+-}2n=0.7, %|b{+-}3n=0.1 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 36 counts were assigned to {+121}Tc, 6 events with the spectrometer setting on Nb, 3 events for setting on Rh, and 27 events for setting on Pd. Probability of misidentification of this isotope is <0.01% (2018Sh11). 
$Production |s=0.3 pb for Nb setting, 0.09 pb for Rh setting, and 0.27 pb for Pd, with 30% systematic uncertainty for all |s. 
E$it is assumed that the observed events correspond to ground-state activity. 
T$measured by 2015Lo04 at RIBF-RIKEN. 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=13.5 ms, %|b{+-}n=43, %|b{+-}2n=4 (2019Mo01) 
$Theoretical T{-1/2}=21.6 ms, %|b{+-}n=82.0, %|b{+-}2n=1.4 (2016Ma12) 
$Only one count was assigned to {+122}Tc, for the spectrometer setting on Rh. Misidentification of this isotope is not likely since no events were observed for neighboring hydrogen-like peaks (2018Sh11). 
$Production |s=0.020 pb, 30% systematic uncertainty for |s. 
E$it is assumed that the observed event corresponds to ground-state activity. 
J$2- or 3- from |W{-|p}=5/2+ and |W{-|n}=1/2- orbitals proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 14.2 ms (2019Mo01) and 21.6 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+122}Tc is expected to be <25 ms, based on measured half-lives of 22 ms for {+119}Tc, 21 ms for {+120}Tc, and 22 ms for {+121}Tc, available in literature. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E$the observed activity is assumed to be in its ground state 
T$lower limit for assumed time-of-flight=450 ns. Actual half-life is expected to be much longer as suggested by theoretical T{-1/2} of 20.1 ms for |b decay (1997Mo25) 
J$1/2+ in theoretical calculations (1997Mo25) 
$Measured production |s=2|*10{-11} mb (2013Su23) from one count assigned to {+85}Ru isotope (see figure 6 in 2013Su23). 


level_energy_unit: KEV
level_comment:
$T{-1/2}>450 ns from time-of-flight. 
$Measured production |s=2|*10{+-11} mb {I+4-2} (2017Su26) from one count assigned to {+85}Ru isotope (see Fig. 2 in 2017Su26 and Fig. 6 in 2013Su23). 
$Observed fragments were assumed to be in ground state 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E$the observed activity is assumed to be in its ground state 
T$lower limit from tof (2013Su23). Actual half-life is expected to be much longer as suggested by theoretical T{-1/2} of 86.4 ms for |b decay (1997Mo25) 
$Measured production |s=1|*10{-10} mb (2013Su23) from 6 counts assigned to {+86}Ru isotope (see figure 6 in 2013Su23). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$T{-1/2}>438 ns from time-of-flight. 
$Measured production |s=1.0|*10{+-10} mb {I+7-4} (2017Su26) from six counts assigned to {+86}Ru isotope (see Fig. 2 in 2017Su26 and Fig. 6 in 2013Su23). 
$Observed fragments were assumed to be in ground state 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from implant-|b(t) using multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
%ECP$measured by 2019Pa16 from the number of |b{++}p-coin events divided by the total number of decays as determined from the half-life analysis (2019Pa16). Others: 3.0 {I+19-17} (2012Lo08, from observation of six |b{++}p-coin events, uncertainty from assuming a binomial probability distribution with a 95% confidence level); <0.15 (2004De40) 
J$9/2+ (1997He24) proposed from systematics, 3/2+ (2019Mo01, theory). Possible band assignment favors 9/2+ (2004Ma86). From analysis of delayed proton spectrum and relative branching ratio with statistical model calculations, 2005Xu04 proposed J|p=5/2+,7/2 for a very low deformation. But 2004De40 did not confirm observation of delayed proton activity using the same reaction as 1999Li33 or 2005Xu04, although, 2019Pa16 confirmed delayed-proton activity using a different reaction to produce {+89}Ru isotope. 2019Pa16 proposed 7/2+ based on predicted |e+|b{++} feedings of g.s. of {+89}Tc for the two choices of 7/2+ and 9/2+ for the g.s. of {+89}Ru, and observation of strong 179-keV |g ray (from the (7/2+) level in {+89}Tc) observed in {+89}Ru decay, thus leaving only small direct feeding of the g.s. of {+89}Tc, consistent with the predicted value of 8%. However, the decay scheme of {+89}Ru |e+|b{++} decay is poorly known, and in the opinion of evaluator, no firm conclusion can be drawn about preference for (7/2+) for g.s. of {+89}Ru, instead of (9/2+) as proposed by 1997He24 based on band assignment. 
T$from 2019Pa16 (weighted average of 1.31 s {I3} from (implant)|b-correlated decay curve and 1.53 s {I11} from (implant)|b{++}p-correlated decay curve, analyzed using multiparameter fits for the decay chain in Bateman equation). Other: 1.5 s {I2} (2001Ki13, (implants)|b{++}-correlated decay curve, analyzed using complete decay chain, 1.6 s {I+3-2} in 2000WeZZ and 1.45 s {I13} in E. Wefers et al., GSI annual (2000) report 2001-1, p10)); 2.2 s {I12} (2012Lo08, (implants)|b{++}-correlated decay curve fitted with Poisson distribution using log-likelihood function for the complete decay chain); 1.2 s {I2} (1999Li33,2005Xu04). Note that production of {+89}Ru in 1999Li33 and 2005Xu04 was not confirmed by 2004De40 using a similar reaction as in 1999Li33. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$from |e feeding from (6,7,8) parent, 1164|g to 4+, and comparison to shell model calculations in 2019Pa16 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E$This level has been omitted from Adopted Levels; instead a level at 2524.5 keV has been adopted based on more extensive measurement in {+58}Ni({+40}Ca,2|a|g) dataset 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
E$This level has been omitted from Adopted Levels; instead a level at 3037.7 keV has been adopted based on more extensive measurement in {+58}Ni({+40}Ca,2|a|g) dataset 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
J log| {Ift}=4.9 to (9/2)+, 6.5 to (13/2+) and 6.0 to (7/2)+ in |e decay, but these log| {Ift} values may be underestimated; likely dominant configuration=(|n g{-9/2}){+-1} (1994He09). 
T weighted average of 9 s {I1} from activity (1983Ko43) and 7.85 s {I40} from 394|g(t) (2004De40) in |e decay (1.47 s). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%B+P |e+|b{++} delayed p spectrum observed by 1983Ha06. 
E 2012Au07 estimate x=-340 {I500}. 
T from delayed-p activity (1983Ha06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (19/2-)
level_comment:
J M1 |DJ=1 300|g to (17/2-) 2409 from ({+40}Ca, a2png), 509|g to (17/2-) 2200 from ({+36}Ar,2pn|g): E=149 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (39/2-)
level_comment:
J stretched Q 1203|g to (35/2-) 6314 in ({+36}Ar,2pn|g): E=149 MeV. 
E 7197 in ({+40}Ca,|a2pn|g) because 1203|g was placed feeding 5996 level in that study. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (43/2-,45/2-)
level_comment:
J 1481|g to (41/2-) 8149 from ({+40}Ca,|a2pn|g). Differs from J proposed in ({+40}Ca,|a2pn|g) because adopted J(8149 level) differs from that in ({+40}Ca,|a2pn|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$from the analysis of the shape of the overlapping peaks in the revolution time spectrum using exponentially modified Gaussian (EMG) function in 2023Xi01. 
J$based on theb-delayed proton measurement in literature and the systematics of the J|p of the observed isomers in the neighboring nuclei in 2023Xi01. The authors of 2023Xi01 states that the isomeric state is a neutron-hole state. 
T$from the Adopted Levels of {+91}Ru in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
J (E2) 162|g to (6+) 2672; probably feeds lower-J level in ({+40}Ca,2p|a|g). 
T from |g|g(t) in {+58}Ni({+40}Ca,2p|a|g). 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: PS
level_comment:
J E2 565|g to (10+) 3798; probably feeds lower-J level in ({+40}Ca,2p|a|g). 
T unweighted average of 55 ps {I4} (1997Li29) and 86 ps {I9} (1980No06) from RDM in ({+40}Ca,2p|a|g). Source of inconsistency unclear. The weighted average of these data is 60 ps {I12}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
I(|g+ce)=77 {I23}, log| {Ift}=4.6 deduced by 2004De40, inconsistent with a |DJ=2, |D|p=no branch; probably I(|g+ce) is significantly overestimated. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
I(|g+ce)=23 {I10}, log| {Ift}=4.9 deduced by 2004De40; probably unreliable due to incompleteness of the decay scheme. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
E$Isomeric ratio R=32 % {I33} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: S
level_comment:
T from decay of strongest |g rays in {+93}Tc following {+93}Ru |e decay (1976De37). Others: 1976DiZP (54.9 s {I17}), 1973Ni04, 1972Do04, 1955At22. 
J log| {Ift}=5.3 to J|p=9/2+; log| {Ift}=6.3 to J|p=(7/2+); log| {Ift}=7.5, log| {If{+1u}t}=9.0 to J|p=(13/2)-. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J log| {Ift}=4.5 to J|p=1/2-,3/2-; systematics of N=49 isotones; similarity of {+93m}Ru and {+91m}Mo decay schemes. 
T from IT decay. 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: US
level_comment:
|m: from TDPAD (Ag host) (1989Ra17, from g=0.850 {I2} from 1983Gr33 and adopted J); no Knight shift correction applied. 
Q: time differential perturbed angular distribution (1991Ha04, ({+32}S,p3n|g)). 
J E2 146|g to (17/2)+ 1936; band assignment. 
T unweighted average of 2.6 |ms {I2} from ({+40}Ca,4pn|g), 2.6 |ms {I3} and 2.05 |ms {I10} from (|a,3n|g) and 2.7 |ms {I2} from fragment-|g(t) in {+9}Be({+107}Ag,X|g); the weighted average is 2.27 |ms {I17}. 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J D |g to J|p=(17/2)+ and to (13/2)+; band assignment; shell-model predicts a 15/2+ level in {+93}Ru lying |?50 keV above a 21/2+ level (1976Se01). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
MOMM1 From DPAD (1989Ra17) and adopted J; no Knight shift correction applied, but this is expected to be small for the Ag host used. Based on g=0.51 {I2} (1983Gr33). 
J 168|g to J|p=(15/2+) 2113; shell-model predicts a 17/2- level at an energy within 120 keV of this level (1976Se01). 
T from (|a,3n|g). 


level_energy_unit: KEV
level_spin_parity: (37/2+)
level_comment:
Possible configuration: {+88}Sr(2+) ~# (33/2+ 6377 level) (1994Ar33). Supported by preferred decay to 6377 level. 


level_energy_unit: KEV
level_spin_parity: (37/2-,39/2-)
level_comment:
Possible configuration: |p(p{-3/2}){+-1} |p(p{-1/2}{+2}g{-9/2}{+5}) |n(|g{-9/2}){+-1} (1994Ar33); if correct, J=37/2 is preferred. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2)+
level_lifetime_unit: US
level_comment:
Q from 1991Ha04; magnitude from known electric field gradient (EFG) of RuZr, sign from systematics of EFG in metals. 
T weighted average of 2.05 |ms {I10} (1978Br25) (presumed to supersede 2.05 |ms {I8} in 1978HaZO) and 2.6 |ms {I3} (1983Gr33 and 1983Gr01). 
Other g-factor data: 0.838 {I2} (1978HaZO, probably superseded); 0.77 {I1} (Pd host), large Knight shift correction expected to be necessary (1983Gr33). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
E from 1983Gr33. 
|g used for g-factor measurement not stated; note that adopted 176|g placement is from (15/2+) level rather than from this (17/2-) level. 


level_energy_unit: KEV
level_comment:
TI IMBALANCE=90 16. 
J 2004De40 conclude that this level is a likely candidate for the first excited 9/2+ state predicted at ~2 MeV by shell-model calculations. 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_lifetime_unit: US
level_comment:
E$Isomeric ratio R=53 % {I2} (2017Pa35) 
T$From |g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured mass excess=-82531 keV {I72} (2017Ze02), compared to -82584 keV {I3} in 2017Au03: NUBASE-2016 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$value for fully-stripped {+94}Ru isomer in the rest frame (2024Ze04) Other: 102 |us {I17} measured by 2017Ze02, and analyzed in a companion paper 2017Ch37, from analysis of 29 observed fully-stripped {+94}Ru ions in the isomeric state. This value is based on selection of mean lifetime |t=192.3 |ms {I315} in lab system, from cropping scenario using frequentist approach. Relativistic Lorentz factor was 1.302 or |b=v/c=0.64. This value is in agreement with an expected value of 94.7 |ms {I53}, deduced from measured T{-1/2}=71 |ms {I4} for neutral {+94}Ru isomer (from {+94}Ru Adopted Levels in the ENSDF database, Jan 2006 update), and total theoretical conversion coefficient of 0.334 for 146.1 keV, E2 transition from the 2645, 8+ isomer. 
$From the decay of 49 events, half-life of {+94m}Ru{+44+} was obtained as 116 |ms {I79} (2017Ze02), out of which 29 events were were identified, which survived throughout the observation window. Statistical approaches based on Bayesian and frequentist methods to handle half-life measurements involving low statistics and restricted observation times are discussed in detail in a companion paper 2017Ch37, where nine possible scenarios of decay experiments under restricted observation times are discussed, out of which following mean lifetime (|t) values, in the lab system, were obtained in three experimental scenarios: 1. Frequentist approach: 217.5 |ms {I1483} (filtering scenario using 49 events), 192.3 |ms {I315} (cropping scenario using 29 events), and 194.6 |ms {I329} (sorting scenario using 29 events). 2. Bayesian approach: 206.0 |ms {I+884-1205} (filtering scenario using 49 events), 195.9 |ms {I329} (cropping scenario for 29 events), and 198.4 |ms {I342} (sorting scenario for 29 events). In 2017Ze02, authors selected value with the lowest uncertainty i.e. |t=192.3 |ms {I315} from cropping scenario in frequentist approach 
$Measured mass excess=-79905 keV {I132} (2017Ze02), compared to -79940 keV {I3} in 2017Au03: NUBASE-2016 
E$2626 keV {I150} from measured mass excesses in 2017Ze02 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Half-life and decay mode from {+94}Ru Adopted Levels in the ENSDF database (2006 update). Value is 102 |ms {I17} for fully-stripped ions (2017Ze02: Phys. Rev. C 96, 031303(R)) 


level_energy_unit: KEV
level_spin_parity: 18+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t (DSAM for 486.0|g)=0.55 ps {I7} (2018Er01) 
$Proposed dominant configuration=|n(d{-5/2}g{-9/2}{+-1})~#|pg{-9/2}{+-6} (2018Er01) 


level_energy_unit: KEV
level_spin_parity: 19+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t (DSAM for 394.5|g)=3.08 ps {I69} (2018Er01) 
$Proposed dominant configuration=|n(d{-5/2}g{-9/2}{+-1})~#|p(p{-1/2}{+-2}g{-9/2}{+-4}) (2018Er01) 


level_energy_unit: KEV
level_spin_parity: 19-
level_comment:
$Proposed (2018Er01) member of of multiplet with Configuration=|n(d{-5/2}g{-9/2}{+-1})~#|p(p{-1/2}{+-1}g{-9/2}{+-5}) 


level_energy_unit: KEV
level_spin_parity: 20-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t (DSAM for 1113.5|g)=2.20 ps {I31} (2018Er01) 
$Proposed (2018Er01) member of multiplet with Configuration=|n(d{-5/2}g{-9/2}{+-1})~#|p(p{-1/2}{+-1}g{-9/2}{+-5}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$T{-1/2}: From measured mean lifetime {|t}=0.8 ps 4 (2022Pe15) by fitting the Decay Curve. Systematic uncertainty was taken into account for contaminated transitions and short lifetimes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$T{-1/2}: From measured mean lifetime {|t}=87 ps 8 (2022Pe15) by fitting the Decay Curve and performing Differential Decay Curve Method (DDCM), using a subtraction of the contribution of long-lived feeding from higher-lying states [{|t}{-5{+-}}=0.51 ns 5 from ENSDF Adopted dataset for {+94}Ru]. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
J$3/2+,5/2+ from L(p,d)=2; log| {Ift}=5.2 to 7/2+ 
T$weighted av of 1.650 h {i17} (1968Pi03. Ge(Li)) and 1.632 h {i21} (1970Bo22. |b|g-coin; NaI). 
MOMM1$NMR 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_uncertain: ?
level_comment:
J$from |g(|q), comparison to shell-model calculations, and systematics of other odd-a Ru isotopes in ({+6}Li,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: NS
level_comment:
J$From |g(|q) in (|a,3n|g) and E2 cascade to 13/2+ 
T$From |g(t) in ({+6}Li,p2n|g) 
MOMM1$+7.01 {i14} (1978LeZA,1976Le30. DPAD) not adopted since the assignment to 2285 was based on the assumption of only one 255|g. Coincidence data in ({+6}Li,p2n|g) indicate that intensity of 255|g is distributed between two transitions of identical energy. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J$from |g(|q), comparison to shell-model calculations, and systematics of other odd-A Ru isotopes in ({+6}Li,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
J$From |g(|q) in (|a,3n|g) and E2 cascade to 13/2+ 
T$From |g(t) in ({+6}Li,p2n|g) (1985Ch28) 
MOMM1$DPAD. See also comment on |m(2284) 


level_energy_unit: KEV
level_spin_parity: 25/2(+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$25/2 from |g(|q) in (|a,3n|g). |p=+ from membership in band 
T$Determined by recoil-distance Doppler shift (RDDS) method in 2004Ga08 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
T$from 336|g(t), 627|g(t) and 1097|g(t) (2020Sz02). Value is average of 1.6044 h {I18}, 1.6000 h {I55}, 1.6074 h {I64}, 1.6028 h {I32}, 1.5938 h {I87}, 1.5925 h {I94} from |g(t) at different energies and with different |g lines. 
J$from the Adopted Levels of {+95}Ru in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T$With Q(2|e)=2718 keV 8 and Q(2|b{++})=674 keV 8 (2003Au03), {+96}Ru could decay to {+96}Mo by 2|e, 2|b{++} or |e|b{++}. Experimentally, only upper limits were obtained, the shortest value being T{-1/2}(2|b{++})>3.1x10{+16} y with a 68% confidence level (1985No03). 
$<r{+2}>{+1/2}(charge)=4.393 {I5} (2004An14) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$stretched E2 cascade in (|a,2n|g). 
T$Weighted av of 6.8 ps {I7} from {+65}Cu({+36}S,p4n|g), 6.9 ps {I9} from Coulomb excitation and 6.9 ps {I9} from {+95}Mo({+3}He,2n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Weighted av of 0.38 ps {I+15-11} from {+96}Ru(p,p'|g), 0.39 ps {I6} from Coulomb excitation and 0.37 ps {I6} from {+95}Mo({+3}He,2n|g) 
J$E2+M1 |g to 2+. J=2 from p|g(|q) in (p,p'|g) (1979La15,1986Ad04) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$from Hauser-Feshbach analysis, E2 |g to 4+ 
T$Weighted av of 12.7 ps {I10} from {+65}Cu({+36}S,p4n|g) and 26 ps {I2} form {+95}Mo({+3}He,2n) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$stretched E2 cascade in (|a,2n|g). 
T$Weighted av. of 9.5 ps {I8} from {+65}Cu({+36}S,p4n|g) and 20 ps {I2} from {+95}Mo({+3}He,2n) 


level_energy_unit: KEV
level_spin_parity: (5,6,7)+
level_comment:
J$log| {Ift}=5.9 from 6+ {+96}Rh isomer gives (5,6,7)+; |g to 2+ would be an unlikely [M3] and select 5+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|b{-2}=0.163 
$B(E2) weighted average of 0.237 {I6} (2002Kl07, T{-1/2} measurement), 0.202 {I23} (2000Kh02, T{-1/2} measurement), 0.236 {I7} (1980La01), 0.266 {I26} (1980La01), 0.260 {I10} (1978Fa08), 0.268 {I32} (1968Mc08) and 0.254 {I41} (1958St32). 
$Q from 1980La01 
T$from B(E2) value 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$|b{-2}=0.117 
$B(E2) weighted average of 0.098 {I13} (1980La01) and 0.106 {I8} (2001Pi12), for 2+ to 4+ transition 


level_energy_unit: KEV
level_spin_parity: 14(-)
level_comment:
E$An additional gamma ray, with E=745.5 {I4}, Mg=d, and A{-2}=-0.05 {i4}, A{-4}=-0.06 {i6}, was observed from this level. In the adopted levels, this gamma feeds the 5532.7 (13+) level, which was not reported by 1984Pi11. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ average of two measured values of +0.52 {I2} and +0.44 {I2} with statistical uncertainty only. The statistical uncertainty on the average value is 0.01, whereas the uncertainty in the absolute value is 0.03, arising mainly from the calibration value 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3(-)
level_comment:
E$candidate for one-phonon mixed-symmetry octupole state based on comparisons with similar energy states in {+94}Mo and {+92}Zr 
J$a 487|g to 2588, 5- level proposed earlier is not confirmed in this experiment, thus the parity of 3076 level is tentative 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
J$L=2 in (d,p), M1(+E2) |g transition from L=4, 421.54-keV level. 
T$weighted average of 2.79 d {I3} (1998Ko27), 2.88 d {I4} (1958Ka95), and 2.9 d {I1} (1966Cr09) 
MOMM1$from g-factor=0.315 {I3} (1985Ed06) and g-factor=(-)0.315 {I3} (1980Le09, recalculated by 1981Ha11). Others: 0.72 {I5} (1981Ha11), 0.687 {I27} (1976Ba39). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$M1+E2 |g to g.s.; log| {Ift}=6.43 (log| {If{+1u}t}=7.79) from {+97}Rh 1/2- state (J Ne 5/2+, 7/2+) 
T$from {+97}Rh |e decay (46.2 min) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$L=4 in (d,p); M1 |g to L=2 g.s. 
T$weighted average (with external unc.) of 34.6 ps {I21} ({+12}C,3n|g) and 17.9 ps {I19} ({+36}S,p3n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$E2 |DJ=2 |g to 7/2+ level; D+Q to (9/2)+ level; 11/2 from |g excit ((|a,n|g),({+6}Li,p2n|g)) 
T$unweighted average of 3.5 ps {I7} ({+12}C,3n|g) and 10.5 ps {I16} ({+36}S,p3n|g) 


level_energy_unit: KEV
level_spin_parity: (15/2)+
level_lifetime_unit: PS
level_comment:
J$E2 to (11/2)+; 15/2 from ({+7}Li,3n|g), ((|a,n|g),({+6}Li,p2n|g)), (|a,2n|g) 
T$weighted average of 14.6 ps {I21} ({+12}C,3n|g) and 11.6 ps {I16} ({+36}S,p3n|g) 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J$D+Q |g to (15/2)+ level; 17/2 from ({+7}Li,3n|g), from |g(|q), excit ((|a,n|g),({+6}Li,p2n|g)) 
T$from ({+36}S,p3n|g); other: 3.5 ps<({+12}C,3n|g) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: NS
level_comment:
J$E2 |g to (17/2+) level; J|p consistent with g-factor; from ({+7}Li,3n|g), |g(|q) ((|a,n|g),({+6}Li,p2n|g)) 
T$from (|a,2n|g); others: 8.7 ns {I9} ({+12}C,3n|g), 7.3 ps {I8} ({+36}S,p3n|g), whose unit is probably a typographic error 
MOMM1$from g-factor=0.88 {I8}, consistent with configuration=((|p g{-9/2}){++2}{-8+}(|n d{-5/2})) (1982Di18) 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
J$E2 |g to (21/2+) level; 25/2 from ({+7}Li,3n|g), ((|a,n|g), ({+6}Li,p2n|g)), (|a,2n|g) 
T$from ({+36}S,p3n|g) 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_lifetime_unit: PS
level_comment:
J$(E2) |g to (23/2)+ level and (M1(+E2)) |g to (25/2+); 27/2 from ({+36}S,p3n|g) 
T$from ({+36}S,p3n|g) 


level_energy_unit: KEV
level_spin_parity: (29/2+)
level_lifetime_unit: PS
level_comment:
J$(E2) |g to (25/2+) level and (M1(+E2)) |g to (27/2+); 29/2 from ({+36}S,p3n|g) 
T$from ({+36}S,p3n|g) 


level_energy_unit: KEV
level_spin_parity: (33/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$(E2) |g to (29/2+) level and (M1(+E2)) |g to (31/2+); 33/2 from ({+36}S,p3n|g) 
T$from ({+36}S,p3n|g) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$level proposed by 1974Oh07, based on deexciting |g's and coincidence work. However, neither 1975Pl05 nor 1981Gr20 observed these gammas. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
T$deduced from apparent T{-1/2}=15 ps {I4} by estimating the contribution from preceding transitions 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
G$0.88 {I8}; consistent with configuration=((|p g{-9/2}){++2}{-8+}(|n d{-5/2})) (1982Di18) 
T$from 1979HeZQ 


level_energy_unit: KEV
level_comment:
S$unresolved doublet, angular distribution reproduced with L=0 (S=0.04) + L=2 (S=0.19 if J=3/2) transfers 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
T$ measured at room temperature (293K to 298K) (2009Go29). Half-life measured at 19K is 2.8382 d {I14} (2009Go29); difference of 0.0012 d {I18} indicates no change in half-life with temperature 
J$ from adopted dataset for {+97}Ru inn ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius=4.4229 fm {I55} (2013An02) 
$Evaluated |d<r{+2}>({+104}Ru,{+98}Ru)=-0.772 fm{+2} {I5} (2013An02) 
$Hyperfine structure measurements, and deduced changes in rms charge radii by 2014Fo01 with the following results: |d<r{+2}>({+96}Ru,{+98}Ru)=0.2874 fm{+2} {I20}; |d<r{+2}>({+98}Ru,{+100}Ru)=0.2538 fm{+2} {I21}; |d<r{+2}>({+98}Ru,{+99}Ru)=0.0917 fm{+2} {I15} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$652.44|g E2 to 0+ 
T$from 2016Pr01 evaluation, based on weighted average of 5.79 ps {I20} (2012Ra03, RDDS in Coul. ex.); 5.5 ps {I8} (2000Kh02, RDDS in ({+36}S,p2n|g)); 6.42 ps {I12} from B(E2)=0.373 {I7}, and 6.16 ps {I49} from B(E2)=0.389 {I31} in Coul. ex. (1980La01); 5.83 ps {I50} from B(E2)=0.411 {I35} in Coul. ex. (1968Mc08); 5.04 ps {I40} from B(E2)=0.475 {I38} in Coul. ex. (1958St32). 
MOMM1$from transient fields in Coulomb excitation (2011Ch23,2011Ta06). Other: +0.8 {I6} (1974Hu01,1969He11) from |g(|q,H) in Coulomb excitation. Compilation: 2014StZZ 
MOME2$or -0.01 {I9} from reorientation effect in Coulomb excitation (1980La01). Others: -0.03 {I14} from constructive interference in Coulomb excitation (1977Ma41); -0.23 {I14} from re-analysis of data in 1977Ma41 by 1998Hi01 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L({+3}He,n)=0 from 0+; |g(|q) in (p,p'|g) is isotropic 
T$from B(E2)(W.u.)=43 {I11} in Coulomb excitation (2006Wi15). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$745.4|g |DJ=2, E2 to 2+; g.s. band member 
T$from RDDS in Coulomb excitation (2012Ra03). Other: 1.68 ps {I+12-9} from weighted average of all available values including those deduced from B(E2) values in Coulomb excitation; value of 7.6 ps {I16} from RDDS in ({+36}S,p2n|g) (2000Kh02) seems discrepant 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1414.3|g |DJ=2, E2 to 0+ 
T$from RDDS in Coulomb excitation (2012Ra03). Other: 1.2 ps {I4} from B(E2) in Coulomb excitation (1980La01). 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$382.66|g and 1144.2|g M1+E2 to 2+, 399.0|g D+Q to 4+; J=4 from |g excitation function in ({+3}He,2n|g) (1988Sa01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L(d,t)=2 from 5/2+; 1164.8|g M1+E2 to 2+, 1817.1|g to 0+; J=2 from |g|g(|q) in 2016Gi05 in ({+3}He,2n|g); 2004Ca42 in (|a,2n|g) suggest 0+ or 2+ based on decay pattern and level population 


level_energy_unit: KEV
level_spin_parity: 2(+)
level_comment:
J$2 from |g|g(|q) (2016Gi05) and (1,2) from excitation function (1988Sa01) in ({+3}He,2n|g); L(d,t)=(2+0) from 5/2+. other: 0+ proposed by 2004Ca42 in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$253.8|g and 469.5|g M1+E2 to 3+, 868.7|g M1+E2 to 4+; |g excitation functions consistent with J=4 in ({+3}He,2n|g) (1988Sa01) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$2+ from |g(|q,pol) and excitation function (1988Sa01) and 3+,4+ from |g|g(|q) and ce data (2016Gi05, who list (2)+ for 2277 level in Table I) in ({+3}He,2n|g); L(d,t)=2 from 5/2+ for a 2277 group 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$630.0|g M1(+E2) to 3+, 1774.5|g M1+E2 to 2+; J=2 from |g|g(|q) in ({+3}He,2n|g) (2016Gi05); L(d,t)=(2+0) from 5/2+ 


level_energy_unit: KEV
level_spin_parity: (3,5+)
level_comment:
J$(3,5) is suggested by |g|g(|q) and |g(|q) (2016Gi05) and (3) suggested by excitation function (1988Sa01) in ({+3}He,2n|g); 643.9|g to 3+. But (5-) proposed by 1981Du06 in (|a,4n|g) based on possible band structure and theoretical predictions is in disagreement. 


level_energy_unit: KEV
level_spin_parity: (3)
level_comment:
J$(3 to 6) from |g(|q) (2016Gi05) and (2,3) from excitation function (1988Sa01) in ({+3}He,2n|g). But (2+) proposed by 1988Sa01 


level_energy_unit: KEV
level_spin_parity: (6)+
level_comment:
J$320.3|g M1(+E2) to 5+, 644.9|g M1,E2 to 6+; spin not 5 from |g|g(|q) (2016Gi05) and J=(6,7,8) from excitation function (1988Sa01) in ({+3}He,2n|g) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$(3,4,5) from |g(|q) (2016Gi05) and (3,4) from excitation function (1988Sa01); L(d,t)=(2+0) from 5/2+ 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J$967.7|g E2, |DJ=2 to 6+; J=(7,8) from |g|g(|q) and J=8 from excitation function in ({+3}He,2n|g). But J|p=7- proposed (by 1998Kh01) from 967.7|g |DJ=1 to 6+ in ({+36}S,p2n|g) is in disagreement 


level_energy_unit: KEV
level_spin_parity: (6)+
level_comment:
J$978.9|g E2, |DJ=(2) to 4+; (5,6) from |g(|q) (2016Gi05) and (6,7) from excitation function (1988Sa01) in ({+3}He,2n|g) 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J$984.6|g M1+E2 to 2267, 4+; 754.4|g from 4006 level, which is deexcited by a 879.6|g, (M1+E2) to 3126, 8+ level 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_comment:
J$L(d,t)=0 from 5/2+ 
$A previously proposed 1428|g from this level in {+98}Rh |e decay (3.6 min) not confirmed in ({+3}He,2n|g) (2016Gi05). Instead, 2016Gi05 have observed and placed a 1428|g from 2826 level. 


level_energy_unit: KEV
level_spin_parity: (4+:7+)
level_comment:
J$1456.3|g to 6+, 1032.4|g to 5+, 295.1|g to (5,7)+. But (8+) proposed in ({+36}S,|a4n|g) and (7-,8+) in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$725.1|g E1(+M2),|DJ=1 to 8+; band structure 
$Previous placement of a 272|g from this level was not confirmed by 2016Gi05 in their |g|g-coin data, this |g remains unplaced. Previously reported 312|g from this level not seen by 2016Gi05. Previously reported 567.4 and 661.3 |g rays are observed by 2016Gi05 as 569.0 and 662.1 keV, respectively, and both placed from a new level at 3852.3 keV. 
T$from RDDS of the 725.7|g placed from a level at 7626 in ({+36}S,p2n|g) 


level_energy_unit: KEV
level_spin_parity: (7+)
level_comment:
E$only one level near this energy confirmed by 2016Gi05 in ({+3}He,2n|g), and not two at 4006.6 and 4007.4, as in (|a,2n|g) (2004Ca42) 
J$879.6|g (E2+M1) to 3126, 8+, 722.6|g to (5,7)+; 754.4|g to 3251 level, which is deexcited by a 984.6|g, M1+E2 to 2267, 4+ level 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$2016Gi05 in ({+3}He,2n|g) did not confirm a 4221.9 level decaying by a 1030.4|g, as proposed by 2004Ca42in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$(10) from |g(|q) in (|a,2n|g) and ({+3}He,2n|g); 1097.2|g to 8+. Possible member of g.s. band (see 4001 level also) 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
J$821.7|g E2, |DJ=2 to 9-; band member 
T$from RDDS of 821.3|g placed from a level at 4798 in ({+36}S,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 13-
level_lifetime_unit: PS
level_comment:
J$848.4|g E2, |DJ=2 to 11-; band member 
T$from RDDS of 848.9|g placed from a level at 3977 in ({+36}S,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 15-
level_lifetime_unit: PS
level_comment:
J$1070.0|g E2, |DJ=2 to 13-; band member 
T$from RDDS of 1070|g placed from a level at 6900 in ({+36}S,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 17-
level_lifetime_unit: PS
level_comment:
J$1031.7|g E2, |DJ=2 to 15-; band member 
T$from RDDS of 1032|g placed from a level at 5831 in ({+36}S,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured by 2012Ra03, using recoil-distance method. Others: 6.42 ps {I13} from B(E2)=0.373 {I7} and 6.2 ps {I5} from B(E2)=0.389 {I31} (1980La01), 5.8 ps {I+8-7} from B(E2)=0.41 {I5} (1968Mc08), 5.0 ps {I+5-4} from B(E2)=0.475 {I38} (1958St32) 
BE2$from particle yield analyzed using B(E2) for 4+ and 2+ levels as determined from |g-yield (1980La01). Others: 0.389 {I31} (1980La01), 0.41 {I5} (1968Mc08, average of 0.40 {I5} and 0.42 {I5}), 0.475 {I38} (1958St32), all from thick-target |g-ray yield 
MOME2$for constructive interference, Q=-0.01 {I9} for destructive interference (1980La01). Other: -0.03 {I14} (constructive interference) (1977Ma41) 
G$weighted average of +0.408 {I32} (2011Ch23) and +0.47 {I3} (2011Ta06, average of +0.48 {I3} and +0.47 {I2} with statistical uncertainty only, whereas the uncertainty including that in the absolute value is 0.03, arising mainly from the calibration value. Others: g=0.30 {I17} (1969He11), 0.39 {I30} (1974Hu01, reanalysis of data from 1969He11) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from weighted averaged B(E2)(W.u.)=43 {I11}. 
$B(E2) for this level studied by 2006Wi15 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured by 2012Ra03, using recoil-distance method. Others: 2.3 ps {I3} from B(E2)=0.194 {I22} (1980La01), 1.7 ps {I+5-3} from B(E2)(W.u.)=53 {I10} (2006Wi15) 
BE2$from 1980La01. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured by 2012Ra03, recoil-distance method using a plunger device. Others: 1.2 ps {I4} from B(E2) values in 1980La01 
$B(E2)(from g.s.)=0.0067 {I11}; B(E2)(from 652)=0.147 {I25} (1980La01). Other: B(E2)=0.0074 {I11} (1968Mc08) 


level_energy_unit: KEV
level_comment:
E,J$9- in 2004Ca42 inconsistent with 312.7|g to 3540 level with J|p=6+,7+,8+. In Adopted Levels, Gammas, two separate levels near this energy are adopted, where 272.8|g and 312.7|g are not adopted. See comments there for details. 


level_energy_unit: KEV
level_comment:
E,J$(8,9,10)+ in 2004Ca42 inconsistent with 722.9|g to 7-. Only one level near this energy is confirmed by 2016Gi05 in ({+3}He,2n|g) with J|p=(7+), and not two at 4006.6 and 4007.4, as in 2004Ca42 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$2 from |g|g(|q), and 0-3 from |g(|q) (2016Gi05). Parity from mult(1165|g) from |a(K)exp (2016Gi05). J|p=1+,2+ in 1988Sa01 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
J$3,4 from |g|g(|q) (2016Gi05). Parity from mult(879|g) from |a(K)exp in 2016Gi05 who list (2)+ for 2277 level in Table I. J|p=2+ in 1988Sa01 


level_energy_unit: KEV
level_spin_parity: 0:4
level_comment:
$Previously reported 670.2|g from this level was not seen by 2016Gi05. 2468|g from this level could not be confirmed by 2016Gi05 due to the maximum energy limit of 2300 keV in their |g spectra 


level_energy_unit: KEV
level_spin_parity: 4+,6+
level_comment:
J$4 to 7 from |g(|q), and 4,6,7,8 from |g|g(|q) (2016Gi05). Parity from mult(320|g) and mult(645|g) from |a(K)exp (2016Gi05). Authors list (6)+ for 2867 level in Table I. J|p=6+ in 1988Sa01 


level_energy_unit: KEV
level_spin_parity: 1,2+
level_comment:
E$2979.7 in 2016Gi05 is a misprint, as confirmed by e-mail communication of Dec 7, 2016 with A. Giannatiempo by the evaluator( B. Singh) 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
J$5,6 from |g|g(|q). Parity from mult(846.6|g) from |a(K)exp (2016Gi05). Authors list 4+ to 8+ for 3069 level in Table I. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J$7,8 from |g|g(|q), and 5 to 8 from |g(|q) (2016Gi05). Parity from mult(967.7|g) from |a(K)exp (2016Gi05). Authors list (8)+ for 3190 level in Table I. 


level_energy_unit: KEV
level_spin_parity: 5+,6+
level_comment:
J$5,6 from |g(|q) (2016Gi05). Parity from mult(978.8|g) from |a(K)exp (2016Gi05). Authors list (6)+ for 3245 level in Table I. J|p=(6+) in 1988Sa01 


level_energy_unit: KEV
level_spin_parity: 4+,5+
level_comment:
J$3,4,5 from |g(|q). Parity from mult(984.4|g) from |a(K)exp (2016Gi05). Authors list 2+ to 6+ for 3251 level in Table I. 


level_energy_unit: KEV
level_spin_parity: 5+,7+
level_comment:
J$5,7 from |g|g(|q), and 5,6,7 from |g(|q) (2016Gi05). Parity from mult(1061|g) from |a(K)exp (2016Gi05). Authors list (7)+ for 3283 level in Table I. J|p=(5-) in 1988Sa01 
$A 567.4|g from 9- state at 3851.59 was not seen by 2016Gi05. 


level_energy_unit: KEV
level_spin_parity: 6+,7+
level_comment:
J$6,7 from 991.8|g(|q) (2016Gi05). Parity from mult(991.8|g) from |a(K)exp) (2016Gi05). J|p=6+ in 1988Sa01 
$A 312.7|g from 9- state at 3851.59 was not seen by 2016Gi05. 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
$Previous placement of a 272|g from this level was not confirmed by 2016Gi05 in their |g|g-coin data, this |g remains unplaced. Previously reported 312|g from this level not seen by 2016Gi05. Previously reported 567.4 and 661.3 |g rays are observed by 2016Gi05 at 569.0 and 662.1 keV, respectively, and both placed from a new level at 3852.3 keV. 
J$9+ in 1988Sa01 is inconsistent with their |g(|q) and |g(pol) data 


level_energy_unit: KEV
level_spin_parity: 6+,7+
level_comment:
E$2016Gi05 confirmed only one level near this energy, and not a doublet at 4006.6 and 4007.4 keV, as reported by 2004Ca42 in {+96}Mo(|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
E$2016Gi05 did not confirm the existence of a 4221.7 keV level depopulated by a 1030.4|g, as reported by 2004Ca42 in {+96}Mo(|a,2n|g). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$proposed by 1981Du06 based on possible band structure and theoretical predictions. It is in disagreement with (3,5+) based on |g|g(|q) and |g-decay pattern in a recent measurement of ({+3}He,2n|g) by 2016Gi05 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=4.15 mb/sr {I1} at 6|', 0.686 mb/sr {I3} at 15|'. |s(6|')/|s(15|')>2. Integrated |s=93 |mb (1972TaYU) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$from Adopted Levels 
$d|s/d|W=0.0273 mb/sr {I6} at 6|', 0.0444 mb/sr {I6} at 15|'. Integrated |s=9.6 |mb (1972TaYU) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.0158 mb/sr {I5} at 6|', 0.0129 mb/sr {I5} at 15|'. Integrated |s=9.9 |mb (1972TaYU) for 1398+1413 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.0031 mb/sr {I2} at 6|', 0.0071 mb/sr {I2} at 15|'. Integrated |s=9.9 |mb (1972TaYU) for 1398+1413 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1 From atomic beam magnetic resonance; |m({+99}Ru)/|m({+101}Ru)=0.8922344 {I4} (1982Br28) 
MOME2 From atomic beam magnetic resonance (1977Bu04) 
Mossbauer emission (|g|g(|q,H,t): 1995Am09 
Hyperfine interactions (|g|g(|q,H,t): 1994Oh05, 1993Kr28, 1993Oh10 
Gfactor: 1993Ok02 
NMR: 1994Bu30, 1997Is10 
Others: 1997Is10, 1994Bu30, 1994Oh05, 1993Kr28, 1993Oh10, 1993Ok02. 
J from paramagnetic resonance (2013Ma15) and |m 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
MOMM1 From time-differential perturbed angular correlations (see 1965Ma27,1978LeZA). Other: |m=-0.292 {I7} from g-factor(89)/g-factor(g.s.)=0.759 {I16} from Mossbauer spectra (1966Ki02). 
MOME2 Q(89)/Q(g.s.)=+2.93 {I7} from Mossbauer (1976Ki02). Other: Q(89)/Q(g.s.)=+2.82 {I9} from Mossbauer (1974Gi12). 
J from Mossbauer spectra (1966Ki02,2013Ma15). E2+M1 |g to 5/2+. 
T from |g|g(t) in {+99}Rh |b{++} decay (16.1 d) (1972Gu01). Others: 18.9 ns {I10} (1974En02), 21.0 ns {I6} (1973Be72), 20.7 ns {I3} (1965Ma27), 20 ns {I1} (1965Ki01), 19.7 ns {I4} (1964Bo28); 24.7 ns {I27} (Coulex.,1967Ki02, 1974Er04). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 3/2+. J from |g|g(|q) in |b{++} decay (16.1 d). L=0 in (d,t) suggests J|p=1/2+. 
T if B(E2)=0.012 {I2} (see Coulomb excitation). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: PS
level_comment:
J |g from (7/2,9/2)+. Excitation function in (|a,n|g) suggests 5/2; M1+E2 |g's to 3/2+, 5/2+ 
T from Doppler broadening in Coulomb excitation (1974Er04). Note that for the 617 and 719 levels, T{-1/2} from Doppler broadening is significantly smaller than indicated by B(E2). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J log| {Ift}=5.7 from 9/2+. M1+E2 |g to 5/2+. 
T if B(E2)=0.082 {I9} (see Coulomb excitation). T{-1/2}=2.5 ps {I6} from Doppler broadening in Coulomb excitation (1974Er04). 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: NS
level_comment:
J |g to 1/2+. log| {Ift}=7.1 from (1/2-). |g|g(|q). E2 |g to |p=+ 
T from |b|g(t) in |b{++} decay (16.1 d) (1973Be72). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 5/2+. log| {Ift}=6.9 from 9/2+. |g(|q) in (|a,3n|g). 
T if B(E2)=0.207 {I21} (see Coul. ex), T{-1/2}=2.1 ps {I5} (1974Er04); 3.5 ps {i14} in (|a,n|g) (1987Do15) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J log| {Ift}=8.3, log| {If{+1u}t}=9.0 from (1/2-). |g to 5/2+. 
T from {+99}Rh |b{++} decay (16.1 d) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
J log| {Ift}=8.6, log| {If{+1u}t}=9.3 from (1/2-). |g to 5/2+. L=2 in (d,t) is not consistent with J|p=1/2+. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
J E1 |g to 9/2+. |g(|q) in (|a,3n|g). Possible doublet in (d,t). 
T from centroid-shift of |a,|g(t) in (|a,3n|g) (1981Du06). 


level_energy_unit: KEV
level_spin_parity: 31/2-
level_lifetime_unit: PS
level_comment:
T$From Doppler Shift Attenuation in (|a,3n|g) (1999Mr04). 
J from |g(|q), member of the J=11/2- band 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
G From differential perturbed angular correlations (1965Ma27). 
T from |g|g(t) (1972Gu01). Others: 21.0 ns {I6} (1973Be72), 20.7 ns {I3} (1965Ma27), 20 ns {I1} (1965Ki01), 19.7 ns {I4} (1964Bo28). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$From B(E2) in 1987Ar17. Other:B(E2)=0.024 {I3} (1967Ki02) 
T 1.1 ps {I3} from Doppler broadening (1974Er04). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
B(E2)=0.128 {I15} in 1967Ki02 gives T{-1/2}=3.7 ps {I4} 
T 2.1 ps {I5} from Doppler broadening (1974Er04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$measured by 2015Ki14 using fast-timing |g|g-coin technique, and obtained from the slope of the decay curve gated on the 486 and 89-keV lines. Other: 20.5 ns {I1} in {+99}Ru Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T$measured by 2015Ki14 for the first time using fast-timing |g|g-coin technique with gates on 971, 709 and 340 |g rays, and analyzed by centroid shift method 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0290 {I18} (at 6|'), 0.084 {I5} (at 18|'), 0.0174 {I13} (at 31|'), 0.0200 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0126 {I9} (at 6|'), 0.058 {I4} (at 18|'), 0.0130 {I9} (at 31|'), 0.0147 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0520 {I33} (at 6|'), 0.169 {I9} (at 18|'), 0.0420 {I23} (at 31|'), 0.0430 {I29} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.082 {I5} (at 6|'), 0.171 {I9} (at 18|'), 0.0303 {I17} (at 31|'), 0.0490 {I27} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0373 {I21} (at 6|'), 0.092 {I5} (at 18|'), 0.0189 {I10} (at 31|'), 0.0243 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.0153 {I10} (at 6|'), 0.0230 {I14} (at 18|'), 0.0406 {I22} (at 31|'), 0.0541 {I29} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0470 {I31} (at 6|'), 0.122 {I7} (at 18|'), 0.0280 {I17} (at 31|'), 0.0360 {I27} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.472 {I24} (at 6|'), 0.0590 {I31} (at 18|'), 0.107 {I6} (at 31|'), 0.0242 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.0075 {I7} (at 6|'), 0.0084 {I7} (at 18|'), 0.0167 {I10} (at 31|'), 0.0160 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0090 {I11} (at 6|'), 0.0090 {I11} (at 18|'), 0.004 {I1} (at 31|'), 0.003 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0121 {I11} (at 6|'), 0.0150 {I13} (at 18|'), 0.0184 {I12} (at 31|'), 0.0170 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0540 {I34} (at 6|'), 0.0080 {I11} (at 18|'), 0.0145 {I10} (at 31|'), 0.007 {I2} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0240 {I16} (at 6|'), 0.108 {I6} (at 18|'), 0.0227 {I13} (at 31|'), 0.0360 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.259 {I13} (at 6|'), 0.082 {I5} (at 18|'), 0.0620 {I33} (at 31|'), 0.0280 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0220 {I15} (at 6|'), 0.059 {I4} (at 18|'), 0.0168 {I10} (at 31|'), 0.0151 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0086 {I8} (at 6|'), 0.0096 {I9} (at 18|'), 0.00250 {I33} (at 31|'), 0.0024 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.0080 {I9} (at 6|'), 0.0080 {I11} (at 18|'), 0.0182 {I11} (at 31|'), 0.0197 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.063 {I4} (at 6|'), 0.099 {I5} (at 18|'), 0.0210 {I13} (at 31|'), 0.0224 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0073 {I8} (at 6|'), 0.0193 {I13} (at 18|'), 0.0076 {I6} (at 31|'), 0.0050 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.0360 {I21} (at 6|'), 0.0408 {I22} (at 18|'), 0.0147 {I9} (at 31|'), 0.0156 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0180 {I14} (at 6|'), 0.0218 {I13} (at 18|'), 0.0054 {I4} (at 31|'), 0.0047 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0180 {I14} (at 6|'), 0.0217 {I13} (at 18|'), 0.0066 {I5} (at 31|'), 0.0068 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0150 {I13} (at 6|'), 0.0183 {I12} (at 18|'), 0.038 {I2} (at 31|'), 0.034 {I2} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0530 {I33} (at 6|'), 0.0550 {I34} (at 18|'), 0.120 {I6} (at 31|'), 0.108 {I6} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0190 {I22} (at 6|'), 0.0280 {I25} (at 18|'), 0.0095 {I8} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0290 {I25} (at 6|'), 0.0560 {I35} (at 18|'), 0.0064 {I6} (at 31|'), 0.0072 {I9} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.066 {I4} (at 6|'), 0.0150 {I13} (at 18|'), 0.0150 {I13} (at 31|'), 0.0110 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.0120 {I12} (at 6|'), 0.0190 {I14} (at 18|'), 0.0160 {I13} (at 31|'), 0.0170 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.076 {I4} (at 6|'), 0.0120 {I12} (at 18|'), 0.0290 {I18} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0070 {I11} (at 6|'), 0.0140 {I12} (at 18|'), 0.004 {I1} (at 31|'), 0.005 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0150 {I13} (at 6|'), 0.0170 {I13} (at 18|'), 0.003 {I1} (at 31|'), 0.0060 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.059 {I4} (at 6|'), 0.064 {I4} (at 18|'), 0.0170 {I13} (at 31|'), 0.0250 {I16} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.144 {I8} (at 6|'), 0.162 {I8} (at 18|'), 0.0320 {I19} (at 31|'), 0.0390 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.105 {I6} (at 6|'), 0.143 {I8} (at 18|'), 0.0300 {I18} (at 31|'), 0.0390 {I22} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0300 {I25} (at 6|'), 0.0400 {I22} (at 18|'), 0.0080 {I11} (at 31|'), 0.0080 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.104 {I6} (at 6|'), 0.119 {I6} (at 18|'), 0.0240 {I16} (at 31|'), 0.0280 {I17} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0210 {I15} (at 6|'), 0.0310 {I19} (at 18|'), 0.0041 {I6} (at 31|'), 0.0089 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 6|'), 0.0190 {I14} (at 18|'), 0.0018 {I4} (at 31|'), 0.0080 {I7} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0320 {I26} (at 6|'), 0.0310 {I19} (at 18|'), 0.0051 {I5} (at 31|'), 0.0079 {I8} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0350 {I27} (at 6|'), 0.0460 {I25} (at 18|'), 0.0087 {I9} (at 31|'), 0.0105 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0270 {I24} (at 6|'), 0.0290 {I18} (at 18|'), 0.0195 {I12} (at 31|'), 0.0165 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0430 {I29} (at 6|'), 0.0370 {I21} (at 18|'), 0.0174 {I11} (at 31|'), 0.0175 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.651 {I33} (at 6|'), 0.577 {I29} (at 18|'), 0.440 {I22} (at 31|'), 0.268 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|s(mb/sr)=0.0300 {I18} (at 6|'), 0.0240 {I16} (at 18|'), 0.0160 {I13} (at 31|'), 0.0140 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(mb/sr)=0.0130 {I12} (at 6|'), 0.0096 {I8} (at 18|'), 0.0068 {I5} (at 31|'), 0.0048 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.239 {I12} (at 6|'), 0.118 {I6} (at 18|'), 0.076 {I4} (at 31|'), 0.0530 {I28} (at 40|') 
E$there are potentially small contributions from a weak, but unresolved L=0 transition (2017Fr08) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.034 {I2} (at 6|'), 0.0330 {I19} (at 18|'), 0.0192 {I11} (at 31|'), 0.0139 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.0290 {I17} (at 6|'), 0.0310 {I17} (at 18|'), 0.0149 {I9} (at 31|'), 0.010 {I5} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$|s(mb/sr)=0.637 {I32} (at 6|'), 0.431 {I22} (at 18|'), 0.239 {I13} (at 31|'), 0.162 {I9} (at 40|') 


level_energy_unit: KEV
level_comment:
$|s(mb/sr)=0.0190 {I14} (at 6|'), 0.0080 {I11} (at 18|'), 0.004 {I1} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0410 {I23} (at 6|'), 0.0280 {I17} (at 18|'), 0.0160 {I13} (at 31|'), 0.0100 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.0230 {I15} (at 6|'), 0.0110 {I12} (at 18|'), 0.0070 {I11} (at 31|'), 0.004 {I1} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s(mb/sr)=0.091 {I5} (at 6|'), 0.0620 {I33} (at 18|'), 0.0339 {I19} (at 31|'), 0.0245 {I15} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$|s(mb/sr)=0.075 {I4} (at 6|'), 0.0490 {I27} (at 18|'), 0.0286 {I16} (at 31|'), 0.0215 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|s(mb/sr)=0.074 {I4} (at 6|'), 0.057 {I3} (at 18|'), 0.0328 {I19} (at 31|'), 0.0213 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.0300 {I25} (at 6|'), 0.0210 {I15} (at 18|'), 0.0160 {I13} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|s(mb/sr)=0.0250 {I16} (at 6|'), 0.0180 {I14} (at 18|'), 0.0080 {I11} (at 31|'), 0.0070 {I11} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.211 {I11} (at 6|'), 0.127 {I7} (at 18|'), 0.0660 {I35} (at 31|'), 0.0420 {I29} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.102 {I6} (at 6|'), 0.064 {I4} (at 18|'), 0.0320 {I26} (at 31|'), 0.0230 {I23} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(mb/sr)=0.057 {I4} (at 6|'), 0.0330 {I19} (at 18|'), 0.0170 {I13} (at 31|'), 0.0110 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.030 {I5} (at 6|'), 0.0280 {I25} (at 18|'), 0.0180 {I14} (at 31|'), 0.0130 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0200 {I22} (at 6|'), 0.0330 {I19} (at 18|'), 0.0190 {I14} (at 31|'), 0.0120 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0200 {I22} (at 6|'), 0.0200 {I14} (at 18|'), 0.0120 {I12} (at 31|'), 0.0077 {I10} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
$|s(mb/sr)=0.096 {I5} (at 6|'), 0.0520 {I33} (at 18|'), 0.0260 {I24} (at 31|'), 0.0190 {I14} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0490 {I32} (at 6|'), 0.0310 {I25} (at 18|'), 0.0190 {I22} (at 31|'), 0.0170 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.058 {I5} (at 6|'), 0.0340 {I26} (at 18|'), 0.0290 {I33} (at 31|'), 0.0150 {I21} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.0500 {I32} (at 6|'), 0.0310 {I19} (at 18|'), 0.0210 {I15} (at 31|'), 0.0170 {I13} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|s(mb/sr)=0.067 {I4} (at 6|'), 0.0420 {I23} (at 18|'), 0.0240 {I16} (at 31|'), 0.0140 {I12} (at 40|') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius <r{+2}>{+1/2}=4.4531 fm {i31} (2013An02) 
$Evaluated |dr{+2}({+100}Ru,{+104}Ru)=-0.506 fm{+2} {I3} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 539.5|g to 0+ 
T$from B(E2)=0.4938 {I40} in Coul. ex.; weighted average of 0.493 {I4} (1998Hi01,1980HiZV); 0.494 {I6} and 0.482 {I26} (1980La01); 0.520 {I44} (1968Mc08); and 0.572 {I40} (1958St32). B(E2)=0.30 {I6} (1956Te26) seems discrepant. All the values are from determination of Coulomb excitation probability. 2016Pr01 evaluation gives B(E2)=0.4927 {I41} and T{-1/2}=12.51 ps {I10} Other: B(E2)=0.471 {I14}, deduced from |d(charge)=|b{-2}R=1.154 {I17} (1996Go36; (|a,|a')); T{-1/2}=22.0 ps {I17} from RDDS in ({+14}C,2n|g) (2017Ko03) is discrepant 
MOMM1$from g=+0.429 {I23} measured using transient-field in Coulomb excitation (2011Ch23). Other: +0.88 {I6} (2011Ta06, transient-field in Coulomb excitation) from g=+0.44 {I3}, average of two measured values of +0.45 {I2} and +0.43 {I1} with absolute uncertainty of 0.03 in g factor; +1.02 {I13} from |g|g(|q,H,t) in {+100}Rh |e decay (1966Au06, value of g=0.55 {I7} given for T{-1/2}=11.0 ps); 0.94 {I30} from |g(|q,H,t) (1974Hu01) in Coul. ex. 
MOME2$=-0.44 {I4} for constructive or -0.27 {I7} for destructive interference (2016St14 evaluation based on 1998Hi01 (also 1980HiZV) experiment of reorientation effect in Coulomb excitation. 1998Hi01 give respective values of -0.54 {I7} or -0.33 {I7}. Others by the same method: -0.43 {I7} or -0.20 {I7} (1980La01); -0.40 {I12} (1978Fa08); -0.13 {I7} (1977Ma41). 
$|b{-2}(|a,|a')=0.204 {I3} (from |b{-2}R(charge)=1.154 {I17}, |b{-2}R(nuclear)=1.12 {I5} (1996Go36)). |b{-2}(Coul. ex.)=0.209 {I2} (from B(E2) (1980La01,1980HiZV)). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$spin=0 from |g|g(|q) in {+100}Tc |b{+-} decay; |DJ=2, E2 590.8|g to 2+ 
T$from B(E2)=0.0191 {I29} in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$spin=4 from |g(|q) in (|a,xn|g); |DJ=2, E2 686.97|g to 2+; band assignment 
T$from B(E2)=0.260 {I22} in Coulomb excitation. Other: 2.5 ps {I6} from RDDS in ({+14}C,2n|g) (2017Ko03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1362.2|g E2 to 0+ 
T$Other: 1.34 ps {I+19-15}, from B(E2)(from g.s.)=0.0190 {I23} in Coul. ex. and adopted branching %I(1362.2|g)=42.2 {I1} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$638.6|g to 4+ and 734.8|g to 0+ have mult=M1,E2 from ce data; 1865.1|g E2 to 0+ in {+100}Rh |e decay (20.8 h) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(p,p')=3 from 0+; band assignment 
T$from B(E3)=0.053 {I9} in Coul. ex. and adopted |g-ray branching ratio. Other: >0.97 ps from DSA method in (n,n'|g) 
$B(E3)=0.052 {I9} (2002Ki06, evaluation) 
$|b{-3}R(nuclear)(|a,|a')=0.76 {I2} (1996Go36) 
$|b{-3}(Coul. ex.)=0.127 {I11} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(d,p)=2 from 5/2+; spin from |g(|q) in (|a,2n|g) and (n,n'|g); 1701.3|g D to 2+; 228.6|g E1 from 2-; 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=4; |DJ=2, E2 1827.1|g to 2+; 1139.9|g to 4+. In (n,|g) E=th, 1988Co18 assigned J|p=2+ on the basis of a 2366.3|g (I|g=32 {I4}) to g.s. But the placement of 2366.3|g is considered incorrect (evaluators) since no such |g is reported in {+100}Rh |e decay (4.6 min) 
$|b{-4}R(nuclear)(|a,|a')=0.038 {I8} (1996Go36). Large value of |b{-4}(p,p')=0.10 (1989Si15) suggests this state as hexadecapole excitation 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$spin=0 from cross-section ratio in (p,t) and |g|g(|q) in {+100}Tc |b{+-} decay (15.46 s); L(p,d)=2 from 5/2+; allowed |b feeding (log~{Ift}=5.4) from 1+ parent 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_lifetime_unit: PS
level_comment:
E$in (n,n'|g), 248, 1413, 1548 and 2236 gammas are reported from this level (2001Ge03), whereas in (|a,2n|g) 248, 712 and 1548 gammas are reported from this level. In {+100}Rh |e decay (20.8 h), only the 1548 |g is reported. But I|g(248)/I|g(1548)=116/23 in (|a,2n|g) and 13/15 in (n,n'|g). This large discrepancy suggests that there are likely two levels, one high-spin decaying through the 248|g and the other low spin populated in (n,n'|g) and {+100}Rh |e decay. The 248|g is placed from a high-spin level in (|a,2n|g) whereas the 1548|g can be from both the levels. 
J$2236.1|g to 2+ and 1548.7|g to 4+; L(p,d)=2+0 from 5/2+ 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$spin=2 from |g|g(|q) in {+100}Rh |e decay (20.8 h); 1553.3|g and 2375.98|g E1 to 2+; allowed |b feeding from 1- parent 


level_energy_unit: KEV
level_spin_parity: (2,3,4)
level_comment:
J$primary 6614.6|g from 3(+) and 2(+). L(p,d)=2+0 from 5/2+ for a 3051 group suggests 2+,3+ for 3058 and/or 3060 level 


level_energy_unit: KEV
level_spin_parity: 8(+)
level_comment:
J$|DJ=0, D 203.6|g to 8+; |DJ=2, Q 557.98|g and 1188.0|g to 6+; 6 levels; |g from 10+; probable |g to 6+ 


level_energy_unit: KEV
level_spin_parity: (12+)
level_comment:
J$1043|g to 10+; proposed from a band member of the g.s band in (|a,2n|g); |g(|q) in (|a,4n|g) give J=10,11,12 


level_energy_unit: KEV
level_spin_parity: (17-)
level_comment:
E$a 6202 level is proposed in (|a,4n|g) to decay by the 1036.5|g. 
J$|DJ=2, (E2) 1036.5|g to (15-); band assignment 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
E$level considered as questionable by 2000Ge01 since none of the three transitions seen in their (|a,2n|g) experiment 


level_energy_unit: KEV
level_comment:
E$level considered as questionable by 2000Ge01 since 262.3|g is placed from a 2968 level and 1097.8|g is not seen in their (|a,2n|g) experiment 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
|g-ray branching ratios from this level disagree with the adopted values from {+100}Rh |e decay (20.8 h) 


level_energy_unit: KEV
level_spin_parity: (15-)
level_comment:
E,J$ this level corresponds to 7204,(17-) in Adopted Levels, since the 1036.3|g in 1976De33 from 6202 level is considered the same as the 1036.6|g from 7204, (17-) level in the cascade: 1037-1005-933-728 from 2000Ti07 in ({+36}S,|a2n|g). In 1976De33, the same cascade is defined as 1036-932-728, without the intermediate 1005|g. 


level_energy_unit: KEV
level_comment:
$|b{-4}=0.10 
$1989Si15 identify this level as a hexadecapole excitation from large |b{-4} value 
$The |s(|q) data interpreted by a single-step mechanism. The authors did not consider a possible two-step mechanism 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
L$from DWBA analysis of three-point |s(|q) (1976De33) 
$B(E2) deduced from |b{-2}R(charge)=1.154 {I17} (1996Go36). |b{-2}R(nuclear)=1.12 {I5} (1996Go36) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
E$2180 {I20} from 1976De33 
L$from DWBA analysis of |s(|q) in the range 7|' to 13|' (c.m.) (1976De33) 
$|b{-3}R(nuclear)=0.76 {I2} (1996Go36) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.4930 {I40} (1998Hi01,1980HiZV), 0.494 {I6} and 0.482 {I26} (1980La01), 0.520 {I44} (1968Mc08) and 0.572 {I40} (1958St32). B(E2)=0.30 {I6} (1956Te26) seems discrepant. 2016Pr01 evaluation gives B(E2)=0.4927 {I41}. These values correspond to the positive sign of the second 2+ interference term. For negative sign of the interference term, B(E2)=0.493 {I3} (1998Hi01), 0.492 {I6} (1980La01). B(E2)=0.471 {I14}, deduced from |d(charge) in (|a,|a') inelastic data (1996Go36) 
$|b{-2}R(charge)=1.154 {I17} (1996Go36 from (|a,|a')). |b{-2}=0.209 {I2} (1980La01,1980HiZV) 
MOME2$-0.54 {I7}, -0.33 {I7} (1998Hi01,1980HiZV), -0.43 {I7}, -0.20 {I7} (1980La01); -0.40 {I12} (1978Fa08); -0.13 {I7} (1977Ma41). When two values are listed, the first value is for constructive (positive sign) interference (from the second 2+ state) and the second value for the destructive (negative sign) interference. Method: reorientation effect in Coulomb excitation. See also 2016St14 evaluation, where Q=-0.44 {I4} or -0.27 {I7} are recommended from 1998Hi01 measurement 


