# LEVEL

level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=80 ms, %|b{+-}n=6.9 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 14.6 {I15} (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI); P{-n} values measured for {+123},{+124},{+125},{+126}Pd and {+125},{+126},{+127},{+128}Ag in this work are systematically much larger as compared to corresponding values in 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+127}Ag 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier value: 89 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: 102 ms {I5} (2014SmZZ); 79 ms {I3} (1996WoZZ: Conf. Proc. NWE'96, Amsterdam, p107); 109 ms {I25} (1995Fe12: Z. Phys. A353, 9). Weighted average of values from 2021Ha19 and 2015Lo04 is 89.1 ms {I9} (compiler's note). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from time distribution of |g rays (1996WoZZ). 
$%|b{+-}n: delayed-neutrons not observed (1995Fe12) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
J$expected configuration=|pg{-9/2} (2000Kr18). 2012Au07 propose 7/2+ from systematics; 9/2+ in predictions by 1997Mo25 
T$from decay curve for delayed neutrons (2000Kr18) 
$Theoretical %|b{+-}n=12.1 (1997Mo25), 11.8, 9.0 (2002Pf04) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ERR=AP;ISO=M
level_uncertain: ?
level_comment:
E$x=20 {I20} (from syst, 2012Au07) 
T$crude estimate from composite decay curve of delayed neutrons from {+129}Ag g.s. and {+129}In (2000Kr18). Other: 10 ms from systematics (2012Au07) 
J$expected configuration=|pp{-1/2} (2000Kr18); also 1/2- from systematics (2012Au07) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}{-1/2}=31.7 ms, %|b{+-}n=9.8 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 46 ms {I+5-9} in {+129}Ag Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: <20 (2014SmZZ: thesis, Univ. of Notre Dame, work at GSI). No events for |b{+-}2n decay mode were detected by 2021Ha19 
E$it is assumed that the observed activity corresponds to the g.s. of {+129}Ag 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 52 ms {I4} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: 95 ms {I+35-29} (2014SmZZ); 46 ms {I+5-9} (2000Kr18: Hyperfine Int. 129, 185). Weighted average of values from 2021Ha19 and 2015Lo04 is 53.9 ms {I24} (compiler's note). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$possible mixture of g.s. and a millisec isomeric state. 
$T{-1/2}, %|b{+-}n and %|b{+-}2n measured by 2022Ph01 for possible mixture of g.s. and a millisec isomeric state 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. These values are compared with T{-1/2}=52 ms {I4} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=17.9 {I14} in 2021Ha19 (Phys. Lett. B 816, 136266). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=31.8 ms, %|b{+-}n=64.4, %|b{+-}2n=2.5 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+130}Ag 
J$2- to 5- from theoretical considerations with neutron in 3/2+ orbital and proton in 7/2- orbital (1997Mo25). J|p=0+ in 2012Au07 is a misprint 
T$measured by 2015Lo04, from (implanted ions)|b correlated curves in time and position using maximum likelihood method. Others: 35 ms {I10} (2005Kr20), |?50 ms (estimated value, 2000Ka48). See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity belongs to the g.s. 
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. T{-1/2} is compared with 42 ms {I5} in 2015Lo04 (Phys. Rev. Lett. 114, 192501). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=33.4 ms, %|b{+-}n=85.3, %|b{+-}2n=11.3 (2003Mo09) 
E$measured half-life is assumed to correspond to the ground state of {+131}Ag 
J$5/2+ in theoretical considerations (1997Mo25) 
T$measured by 2015Lo04, from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo05 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity belongs to the g.s. 
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. T{-1/2} is compared with 35 ms {I8} in 2015Lo04 (Phys. Rev. Lett. 114, 192501). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=28 ms, %|b{+-}n=3.3, %|b{+-}2n=88, %|b{+-}3n=4.0 (2003Mo09) 
$Theoretical T{-1/2}=29.8 ms, %|b{+-}n=28, %|b{+-}2n=61, %|b{+-}3n=0.7 (2016Ma12) 
E$measured half-life is assumed to correspond to the ground state of {+132}Ag 
J$3- or 6-, suggested from |W(odd proton)=9/2+ and |W(odd neutron)=3/2- in the theoretical considerations (1997Mo25) 
T$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}=28.3 ms, %|b{+-}n=3.3, %|b{+-}2n=88.1, %|b{+-}3n=4.0 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=29.8 ms, %|b{+-}n=28.1, %|b{+-}2n=60.7, %|b{+-}3n=0.7 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 11 counts were assigned to {+132}Ag, with the spectrometer setting on Sn. Probability of misidentification of this isotope is <0.01% (2018Sh11). 
$Production |s=0.12 pb for Sn setting, with 30% systematic uncertainty |s. 
E$it is assumed that the observed events correspond to ground-state activity. 
T$measured by 2015Lo04 at RIBF-RIKEN. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$A total of three events were assigned to {+94}Cd 
$Measured production |s=0.02 pb {I+3-1} (2016Ce02) 
T$lower limit of half-life assigned by evaluator from time-of-flight of 760 ns (2016Ce02) through the BigRIPS fragment separator and ZDS spectrometer. Since {+94}Cd is expected to be a bound nucleus from S(p)=1.48 MeV, S(2p)=0.99 MeV (theory, 1997Mo25), actual half-life is expected to be much longer, e.g. theoretical T{-1/2}=73 ms in 1997Mo25 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$|e decay considered as negligible by 2018Pa20 
%B+P$from number of single-pixel events with |DE>1500 keV (2018Pa20). 
$476 implantation counts were assigned to {+95}Cd by 2018Pa20. 
$|b-decay correlation fraction=68% {I3} 
$As no beta-delayed |g rays were observed, 2018Pa20 assumed 100-(%|b{++}p)=95.5 {I+10-12} |b{++} feeding to the g.s. of {+95}Ag, implying log| {Ift}=3.1 {I5} for this transition. 
J$(9/2+) proposed by 2017Da07, based on g{-9/2} neutron orbital. 7/2+, from |W{-n}=7/2+ orbital proposed in 2019Mo01. 
T$measured by 2018Pa20, using maximum likelihood method (MLH) for (implant)(|b{++})-correlated decay curve, where the fit function contained the parent, |b-daughter, and |bp-daughter decay components with half-lives and %|bp branching ratios, and a constant background for random correlations. Two generations of isotopes were considered in the Bateman equation. Decay constants for {+95}Ag and {+94}Pd daughters were taken from literature. Others: 29 ms {I8} (2017Da07), 73 ms {I+53-28} (2011StZV, from 17 correlated events, and using maximum likelihood method (MLH)). Theoretical T{-1/2}=54 ms (2019Mo01), 31.7 ms (1997He24, shell-model calculations) 
$Measured production |s=1.0 pb {I1} (2016Ce02), 5.4 pb {I28} (2011StZV) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$ from |b decays correlated with implanted nuclei (2008Ba53) 
$ Production |s=5.5 pb {I14} (2008Ba53) from 274|+24 events assigned to {+96}Cd 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$ from the time distribution of 421|g (assigned by 2011Na34 tentatively to the |b{++}+|e decay of {+96}Cd to {+96}Ag levels) correlated with {+96}Cd nuclei using maximum likelihood method (2011Na34). 2011Na34 compare T{-1/2} with the earlier value of 1.03 s {+24-21} from NSCL (2008Ba53: Phys Rev Lett 101, 252501) 
$ Percent population is estimated as |?90% (2011Na34) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 16+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$ Percent population of the isomer is estimated as <10% (2011Na34) 
$ Deduced B(G-t)=0.19 {I+10-6} from above T{-1/2}, 100% |b{++}, and Q value of 11.51 MeV {I26} (2011Na34) 
$ Configuration=|pg{-9/2}{-2}~#|ng{-9/2}{+-2}, 76% component is estimated from shell-model calculations. This mainly decays to to the 15+ state in {+96}Ag with configuration=|p|n(p{-1/2}{+2} |p(g{-9/2}{+7})|n(g{-9/2}{+9}); |p(g{-9/2}{+-3}|n(g{-9/2}{+-1} holes coupled to maximum spin of 15+ 
E$ x=3771 predicted from T=0 shell-model calculations, this is lower than the energies of the first 12+ and 14+ states in {+96}Cd 
T$ from the combined time distribution of 470|g, 667|g and 1506|g (assigned by 2011Na34 to the |b{++}+|e decay of {+96}Cd isomer to {+96}Ag levels), correlated with {+96}Cd nuclei using maximum likelihood method (2011Na34) 
$ Isomeric decay mode is hindered by E6 |g required to the 10+ state in {+96}Cd. Thus |b{++}+|e and delayed-proton decay are the most likely decay modes. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$ measured by 2008Ba53: Phys Rev Lett 101, 252501; same experimental as 2012Lo08. 
%B+P$ Measured by 2012Lo08 based on observation of 12 |bp coincidence events. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from |b-p(t) with fit including contributions from {+96}Cd ground state and isomer, as well as the isomer and ground state in {+96}Ag (2017Da07). 
%B+P$from 2017Da07 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 16+
level_lifetime_unit: S
level_comment:
T$from sum of all |b and |b-p gamma rays; time distribution is fit using the Schmit method (2017Da07) 
%B+P$from 2017Da07 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: S
level_comment:
T$weighted average of 0.54 s {I4} from implant-|b(t) and 0.52 s {I7} from implant-|bp(t); both analyses used a multiparameter fit to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 
J$from 2011Na34 
E$from measured difference in endpoint energies of ground state and isomer (2019Pa16). Reported as 5.81 MeV {I+156-122} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: NS
level_comment:
T$from sum of gates on eight main gamma rays depopulating the isomer (2019Da02). Value is a weighted average of 198 ns {I+28-22} from RIBF83 experiment and 195 ns {I26} from RIBF9 experiment (2019Da02) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
E,J,T$T{-1/2} measured by |bp coin (1997Sc30); p|g coin data showed coin with 6+ - 4+ - 2+ cascade in {+97}Cd, whence the conclusion that the observed T{-1/2} is that of the {+97}Cd g.s. (while admixture of other activities is not excluded, especially from the hypothetical 25/2+ isomer of {+97}Cd); this also suggests the tentative J|p assignment for {+97}Cd g.s.. Other value: 3 s {I+4-2} (1982Ku15) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
T$weighted average of 1.22 s {I7} from implant-|b(t) and 1.08 s {I16} from implant-|bp(t); both analyses used a multiparameter fit 
%B+P$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: (25/2+)
level_lifetime_unit: S
level_comment:
T$weighted average of 3.88 s {I8} from implant-|b(t) and 3.83 s {I8} from implant-|bp(t); both analyses used a multiparameter fit to total decay time distribution with a Bateman equation (2019Pa16). 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 
E$from measured endpoint energy difference between isomer and ground state (2019Pa16) 
J$from 2012Lo08 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_comment:
T$from implant-|b(t) using multiparameter fit to total decay time distribution with a Bateman equation (2019Pa16). 
E,J$from 2019Pa16 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 9.3 s {I1} (2019Pa16, |b|g(t)) and 9.2 s {I3} (1992Pl01). Others: 8.1 s {I5} (1988RyZY), |?8 s (1978El09), 2002StZU 
$%|ep from 2019Pa16. Other: <0.025 (1996He25,1997Ra22) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
T$from (147|g)(198|g+688|g+1395|g)(t) in ({+124}Xe,X|g) (2017Pa35). Other: <20 ns in ({+58}Ni,|a2n|g) (2004Bl10, centroid shift method) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
T$from |g|g(t) in ({+124}Xe,X|g) (2017Pa35, note that 149 ns {I14} is also quoted in authors' text). Others: 0.17 |ms {I+6-4} (2004Bl10) and 0.48 |ms {I16} (1997Go18) in |g|g(t) in ({+58}Ni,|a2n|g); 0.20 |ms {I+30-17} (1997Gr02) and 0.19 |ms {I2} (1998GrZS). Note that values from 1997Go18, 1997Gr02 and 1998GrZS could have contribution from the 224-ns isomer at 6635 also, first identified by 2004Bl10, since that isomer could have been also populated, but was not identified by 1997Go18, 1997Gr02 and 1998GrZS. 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
$Core-excited state as intrepreted by 2017Pa35, 2010Bl13 and 2004Bl10 in ({+124}Xe,X|g) and ({+58}Ni,|a2n|g) 
J$tentatively assigned by 2004Bl10 in ({+58}Ni,|a2n|g) based on shell-model predictions and observed isomeric decay. The same assignment is given in 2017Pa35, 2010Bl13, 2006Ve09 and 2004Bl10 
T$from |g|g(t) in ({+124}Xe,X|g) (2017Pa35). Others: 0.21 |ms {I2} (2019Ha26, |g(t) at RIBF-RIKEN); 0.23 |ms {I+4-3} (2004Bl10) in ({+58}Ni,|a2n|g), 0.23 |ms {I8} (2010Bl13) in ({+124}Xe,X|g), 0.23 |ms {I+8-9} (2006Ve09) in ({+46}Ti,|a2n|g) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
T$from single exponential fit to |g|g(t) (2004Bl10). Others: 0.48 |ms {I16} (1997Go18), 0.20 |ms {I+30-17} (1997Gr02) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
E$core-excited state (2004Bl10) 
J$tentatively assigned by 2004Bl10 based on shell-model predictions and observed isomeric decay. 
T$from single exponential fit to background-subtracted |g(t) (2004Bl10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
T$value is from Table I in 2017Pa35, but T{-1/2}=149 ns {I14} is also quoted in text. 
$Measured isomeric ratio R=58% {I7} (2019Ha26), 97% {I36} (2017Pa35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (12+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
$Core-excited state as intrepreted by 2017Pa35 and earlier authors 
T$from |g|g(t) in 2017Pa35, but the gating |g-ray transitions were not given by the authors. Others: 0.21 |ms {I2} (2019Ha26, |g(t)); 0.23 |ms {I8} from a single exponential fit to 4157|g(t) (2010Bl13) 
$Measured isomeric ratio R=18% {I4} (2019Ha26), 10% {I1} (2017Pa35) 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: PS
level_comment:
T$from comparison of the simulated response function to measured |g spectrum (2021Ji11) 
$population=100% {I8} (2021Ji11) 
$Configuration=|pg{+-1}{-9/2}p{+-1}{-1/2} (2021Ji11) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
$%|b{++}p: 1978El09 and 1982Ku15 used the statistical model to calculate the p and |a branching ratios. In these calculations the spin and parity of {+99}Cd were assumed to be 5/2+ in agreement with systematics for odd nuclei with N=51 ({+93m}Mo, {+95}Ru, {+97}Pd, {+110}Sn) 
T from delayed-p activity (1978El09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1989Ry02. Other: 66 s {I18} (from |b(t),1970Hn03) 
$Measured isotope shift |n({+114}Cd,{+100}Cd)=6371.6 MHz {I31}(stat) {I114}(syst) (2018Ha30, high-resolution collinear laser spectroscopy at ISOLDE-CERN). 
$Measured |d<r{+2}>({+114}Cd,{+100}Cd)=-1.421 fm{+2} {I5}(stat) {I43}(syst) (2018Ha30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$level populated strongly in Coul. ex. 
T$from B(E2)|<0.21 {I7} in Coul. ex. (2009Ek01), assuming Q{-0}=0 from shell-model calculations 
$B(E2) and comment edited, T{-1/2} revised, B. Singh, Sept 15, 2021, in response to e-mail query of Aug 18, 2021 from Dr. M.L. Cortes (T.U. Darmstadt) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
T$from |g(t), unweighted average of 60 ns {I3} (1994Go38) and 52 ns {I5} (1992Al17) in ({+58}Ni,2p2n|g), and 73 ns {I5} (1988Pi03) in ({+40}Ca,2p2n|g). 
MOMM1$from g factor=1.24 {I6} measured using DPAD method in ({+58}Ni,2p2n|g), corrected for Knight shift and diamagnetic shift (1992Al17) 
$Proposed configuration=|pg{-9/2}{+-2}, consistent with measured g factor (1992Al17) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
T$from |g(t), weighted average of 60 ns {I3} (1994Go38) and 52 ns {I5} (1992Al17). Other: 40 ns {I+20-10} (1987Al08) 
$g factor from DPAD method with correction for Knight shift and diamagnetic shift (1992Al17) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
BE2$Q{-0} fixed as 0 to deduce B(E2) value 
T$deduced from B(E2)|<0.21 {I7} 
$|s=0.20 b {I6} (2009Ek01) 


level_energy_unit: KEV
level_spin_parity: (4+,5,6+)
level_comment:
J$ 2002Pl03 suggest (5-,6+) based on shell-model predictions and decay modes. But figure 12 in 2002Pl03 gives calculated positive parity levels, not the negative parity levels. Amongst the calculated levels, 4+, two 5+ and 6+ levels lie close together. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$this level may be the second 2+ state, but statistics for |g|g-coin were too low to make a definite assignment. The 1930|g could feed the first 2+ and 4+ states, but then the latter states would not be fed directly, an unlikely scenario. 
E$listed as 1930+x in 2018Co07 
$Measured |s=3 mb {I3} (2018Co07) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
T$weighted average of: 1.37 min {I5} (1980Ka05) and 1.2 min {I2} (1969Ha03) |b+ decay; on-line ms of Sn(p,spallation) products 
J$based on syst with {+105}Cd, {+107}Cd, {+109}Cd g.s. and |g decays. 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
J$spin from fit to measured optical spectrum using Collinear Laser Spectroscopy 
MOMM1,MOME2$deduced from measured hyperfine parameters. 
MOMM1$-0.8278461 {I15} is used for calibration; uncertainties are statistical only (2018Yo07) 
MOME2$from -0.177 {I2}(stat) {I7}(syst) in 2018Yo07, with two uncertainties added in quadrature. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+101}Cd)=+5859.9 MHz {I22} {I105} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+101}Cd)=-1.307 fm{+2} {I4} {I40} 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
MOME2 From 1992Al17 
MOMM1 From 1992Al17 
T$2001Li24 quote from 1992Al17.Also 38.8 ns 28 2007Bo17), 17 ns {i7} (1982Tr04) 
J from PAD in (HI,xn|g) 157|g stretched E2 to 6+ (1992Al17). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$Ordering of the 1081-952-849-511 cascade is not certain in this band so no J|p values given here by 2001Li24 


level_energy_unit: KEV
level_spin_parity: (11)+
level_lifetime_unit: PS
level_comment:
J$|p=+ from measured short lifetime of yrast states above the 10+ level which rules out any change of parity and determines the stretched M1 character of the upper transitions in the cascade (2001Li24) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$ for {+64}Zn target, statistical uncertainty of 0.11 and systematic of 0.15 have been combined in quadrature. Other: +0.20 {I43} with {+109}Ag target 
BE2$with {+64}Zn target. The quoted uncertainties of 0.02 each for statistical and systematic have been combined in quadrature. The known lifetime of the 776.6 level was not included in the analysis. Other: B(E2)=0.28 {I4} with {+109}Ag target where known lifetime of the 776.6 level was included in the analysis. 
T$ deduced by compiler from B(E2)=0.28 {I3} 
$ |s=0.20 b {I4} with {+64}Zn target, 0.60 b {I5} with {+109}Ag target (2009Ek01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+102}Cd)=+5037.2 MHz {I22} {I96} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+102}Cd)=-1.144 fm{+2} {I3} {I25} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=5.6 ps {I6} from DDCM (2021Si26). Authors compared their result with |t=5.9 ps {I5} from 2007Bo17 (Phys. Rev. C 75, 054311), and 5.2 ps {I7} from 2009Ek01 (Phys. Rev. C 80, 054302). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=3.6 ps {I12} from DDCM (2021Si26). Authors compared their result with |t<8.1 ps from 2001Li24 (Phys. Rev. C 63, 054304) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: MIN
level_comment:
$<r{+2}>{+1/2}=4.4860 fm {i88} (2004An14, evaluation) 
J$from analogy to {+105}Cd, {+107}Cd, {+109}Cd g.s.|p=+ from log| {Ift}=6.0 to J|p=7/2+ of {+103}Ag g.s. No direct measurement of J has been performed. 
T from decay curves: |b{++}, 1080|g, 1449|g, 1463|g (1969Ha03). Other: 7.70 min {I17} (1980Ka05) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J$stretched E2 to (5/2)+ and M1 to (7/2)+. Member of a |DJ=2 cascade on (5/2)+ g.s. log| {Ift}=5.9 from (9/2+) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$D to (11/2)+ and Q to (9/2)+ Member of a |DJ=2 cascade on (5/2)+ g.s. log| {Ift}=6.0 for |e decay from (9/2+) {+103}In g.s. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: NS
level_comment:
T$From |g(t) in {+58}Ni({+50}Cr,4pn|g) (1997Pa25) Not excluded that T{-1/2} is associated with 2571 keV level (1997Pa25) 
J member of |DJ=2 cascade based on (7/2)+ state 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
J$spin from fit to measured optical spectrum using Collinear Laser Spectroscopy 
MOMM1,MOME2$deduced from measured hyperfine parameters. Uncertainties are statistical only. |m=-0.8278461 {I15} is used for calibration 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+103}Cd)=+4621.6 MHz {I24} {I87} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+103}Cd)=-1.046 fm{+2} {I3} {I24} 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
|g's seen in |e decay and (|a,2n|g) suggest that same level is populated in both; however, if direct |e feeding is correct then J|p(parent)=7+. See 1989Va05 
J$from |g(|q) in {+102}Pd(|a,2n|g), stretched E2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$ for {+64}Zn target, statistical uncertainty of 0.10 and systematic of 0.11 have been combined in quadrature. Other: -0.52 {I19} with {+109}Ag target 
BE2$with {+64}Zn target. The quoted uncertainties of 0.01 statistical and 0.02 systematic have been combined in quadrature. The known lifetime of the 658.0 level was not included in the analysis. Other: B(E2)=0.39 {I1} with {+109}Ag target where known lifetime of the 658.0 level was included in the analysis. 
T$ deduced by compiler from B(E2)=0.33 {I2} 
$ |s=0.31 b {I4} with {+64}Zn target, 1.01 b {I6} with {+109}Ag target (2009Ek01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+104}Cd)=+3922.7 MHz {I24} {I79} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+104}Cd)=-0.904 fm{+2} {I2} {I16} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=9.6 ps {I3} from DDCM, 10.0 ps {I+6-4} from DCM (2021Si26). T{-1/2} from compiler's weighted average of |t=9.7 ps {I3} of the two values. Authors compared their result with |t=9 ps {I3} from 2001Mu19 (Phys. Rev. C 64, 014305), 8.5 ps {I12} from 2007Bo17 (Phys. Rev. C 75, 054311), and 8.5 ps {I2} from 2009Ek01 (Phys. Rev. C 80, 054302). Compiler's note: 2009Ek01 also give B(E2)(up)=0.33(2) giving |t=10.0(6) ps, an independent value. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=1.6 ps {I5} from DDCM, 1.44 ps {I+33-24} from DCM (2021Si26). T{-1/2} from compiler's weighted average of 1.49 ps {I+33-24} of the two values. Authors compared their result with |t<6 ps from 2001Mu19 (Phys. Rev. C 64, 014305), 1.5 ps {I5} from 2007Bo17 (Phys. Rev. C 75, 054311) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$mean lifetime |t<6 ps from DCM (2021Si26). Authors compared their result with |t<6 ps from 2001Mu19 (Phys. Rev. C 64, 014305) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
J$from optical double resonance measurements (1969La06), |p=+ from log| {Ift}=5.3 to 7/2+ 25-keV level in {+105}Ag 
T$weighted average of: 54.7~min~{I8} (1953Jo20), 55.0~min~{I6} (1968Bo25), 56.0~min~{I5} (1969St18); Others: 57~min~{I2} (1950Gu54), 50.7~min~{I10} (1961Ra06) 
$<r{+2}>=4.5157 fm{+2} {I71} (2004An14) 
CONF$|nd{-5/2}{++1} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$131.36|g M1 to 5/2+; L(d,t)=4; L({+3}He,|a)=(4,2) 
T$weighted average of 1.75 ns {I11} from |g-131|g(t) in {+105}In |e decay (5.07~min) (1973Ro30) and 1.66 ns {I12} in {+96}Mo({+12}C,3n|g) (2011Ki17) 
CONF$|ng{-7/2}{++1} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$L({+3}He,|a)=2; 570.40|g (E2) to (5/2+) in {+102}Pd(|a,n|g) (1978Ge05), 635.44|g to 7/2+; log| {Ift} supports (5/2+) assignment 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_comment:
J$331|g E1 to 9/2+, 363|g E1 to 11/2+; L({+3}He,|a)=5; However, 9/2- can not be excluded 
CONF$|nh{-11/2}{++1} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$no direct feeding from 9/2+ in {+105}In |e decay (5.07~min); |g decay to (7/2+,9/2+) states; |g feeding from (7/2+,9/2+) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$126.4|g E2 to (17/2)+; band member 
T$from 1976HaXS and 1976SpZQ, but not assigned to this particular level. Assignment made by the evaluators 
CONF$|pg{-9/2}{++2}|ng{-7/2}{++1} 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$Others: 9/2+ in 2015Ra02 does not fit to |g-ray multipolarity; 5/2+ in 1978St01 
CONF$|nd{-5/2}{+1}x2{++}{-1} (2011Ki17) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: US
level_lifetime_info: ;ERR=?
level_comment:
T$from 1978Ge05, based on cyclotron off-beam activity, but the value seems to be from Heiser,C. et al., Symp. on Nuclear Spectroscopy and Nuclear Theory, Dubna, June 19-23, p.18 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2 Based on reorientation effect. Others: see Coul. ex. 
T from B(E2)=0.384 {I4} (1976Es02) 
J E2 |g to 0+ 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from B[E2; 2+(632 keV) to 4+(1493 keV)]=0.247 {I31} Coul. ex. (1969Mi07) 
J |DJ(861|g,E2)=2. J=4 preferred above J=0 because member of a |DJ=2 band 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
From E2 to 0+ in ((p,p'|g). After discussions with authors of (n,n'|g) data (1988BeYC) from which J=1 was suggested, they cannot exclude J=2 for this level 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J L(p,p')=3 for 2366-keV level which is probably the same level; E1 to 2+, |DJ=1 from negative A{-22} |g(|q) coefficient. J=3 from (p,2n) excitation function 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
T weighted average of 0.4 ns {I1} (1985An27) and 0.38 ns {I14} (1983Gu14) 
J |p=+ from allowed |b transition (log| {Ift}=5.1) from J|p(initial)=(7)+. J=8 from |DJ(541|g,E2)=-2 and |DJ(552|g,E2)=-2 to 6+ levels 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J |p=+ from M1+E2 to 6+. J=7 from |DJ(581|g,M1+E2)=-1 to 6+ 2503 keV level, |DJ(753.8|g,E2)=-2 to 5+ 2331 keV level 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: NS
level_comment:
J |DJ(171.10|g,M1+E2)=-1 to 8- 
T from ({+13}C,3n|g). Other: 0.15 ns {I+8-2} (1983Gu14). Systematics of B(E2)(W.u.) values in this region suggest that this value is not correct (1985An27) 


level_energy_unit: KEV
level_spin_parity: 12(+)
level_lifetime_unit: NS
level_comment:
T |a,|g(t) pulsed beam (1977Da08): average of 65 ns {I8}, 73 ns {I16}, 55 ns {I10}, 53 ns {I16} for (335,646,1069,875|g)(t), respectively 
J |DJ(223.61|g,E2)=-2 to 10(+) 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
E$Different interpretation of level by 1994Je05 who claim this is the 12+ member of the |DJ=2 band on the 4+ level and not the 5418.7 keV level as proposed by 2003Si14, 2005Si23. 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
T$From |g(t) in (HI,xn|g) (1994Je05) 
E,T$No evidence found in {+94}Zr({+16}O,4n|g) by 1995Re07 although this is the most complete study 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 26+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
T$Effective half-life (2005Si23). Effective half-life is obtained assuming 100% side-feeding into the top of the band via a cascade of 5 transitions with the same moment of inertia as the in-band transitions The highest |g ray for which a line shape was observed was then fitted and the extracted life time is called effective lifetime. This lifetime was used as input parameter to extract the lifetimes of the states lower in the cascade 
E$Different interpretation of level by 1995Re07. Considered as a member of a |nh{-11/2}~#|ng{-7/2} band 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
E$In |e decay. Observed only by (2007Li07). Also observed in (|g,|g). No |e information given by these authors. 
J$possible quadrupole-octupole coupled state with J|p=1- 


level_energy_unit: KEV
level_spin_parity: 12(+)
level_lifetime_unit: NS
level_comment:
T |a|g(t) pulsed beam (1977Da08): average of 65 ns {I8}, 73 ns {I16}, 55 ns {I10}, 53 ns {I16} for (335,646,1069,875|g)(t), respectively 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.384 {I4} (1976Es02) 
BE2 Others: 0.408 {I24} (1970Kl12), 0.426 {I17} (1969Mi07) 0.47 {I5} (1958St32) 
MOME2 Constructive interference from higher 2+ states assumed; others: -0.32 {I8} (1976Es01), -0.15 {I11} (1974Ha08), -0.76 {I15} (1970Kl12), -0.77 {I26} (1970St17) 


level_energy_unit: KEV
level_spin_parity: (4,5+)
level_comment:
J from |DJ=0 or -1 for 1028|g to 1493-keV level and |D|p=no if J=5 in {+96}Mo({+13}C,3n|g) (1979Sa01) 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
T$From |g(t) in (HI,xn|g) (1994Je05) 
E,T$No evidence found in {+94}Zr({+16}O,4n|g) by 1995Re07 although their data are the most complete. Therefore the existence of that level becomes doubtful. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$this level may be the same as 8099.7, thus x may be zero 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 26+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
T$Effective half-life (2005Si23). Effective half-life is obtained assuming 100% side-feeding into the top of the band via a cascade of 5 transitions with the same moment of inertia as the in-band transitions The highest |g ray for which a line shape was observed was then fitted and the extracted life time is called effective lifetime.This lifetime was used as input parameter to extract the lifetimes of the states lower in the cascade 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
G$from the transient-field technique (2016Ku06). E{-beam} = 400 MeV was used in the analysis since the feeding contribution from the higher excited states populated to the 2{++} state was the lowest at this beam energy. T{-1/2}= 7.7 ps {I8} from the Adopted Levels of {+106}Cd in the ENSDF database was used to deduce the g-factor 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
G$from the transient-field technique (2016Ku05). E{-beam} = 410 MeV was used in the analysis. The T{-1/2} = 0.87 ps {I11} from the Adopted Levels of {+106}Cd in the ENSDF database was used to deduce the g-factor. 
T$2016Ku05 state that their lineshape analysis of the current data favors a longer lifetime of T{-1/2} = 1.73 ps {I14} compared with 0.87 ps {I11} in the Adopted Levels of {+106}Cd in the ENSDF database, but that additional details will be presented in a forthcoming paper. This new T{-1/2} would reduce the measured g-factor value by ~25% (2016Ku05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$from the transient-field technique. E{-beam} = 400 MeV was used in the analysis since the feeding contributions from the higher excited states populating the 2{++} state were the lowest at this beam energy. See 2016Ku05 and XUNDL-8 for more information. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
G$from the transient-field technique. E{-beam} = 410 MeV was used in the analysis. Please see 2016Ku05 and XUNDL-8 for the explanation of the expected differences in T{-1/2} and g-factors. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+106}Cd)=+2991.1 MHz {I22} {I62} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -800.9 MHz {I18} {I31} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+106}Cd)=-0.695 fm{+2} {I2} {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from RDDM using a gate on the 861|g and analyzing shifted and unshifted components of the 633|g (2020Zh26) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for 2|n2|e capture to the ground state of {+106}Pd, obtained by searching for K-xray-K-xray coincidences in Pd (2015Br14) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$<0+ || E2 || 2+ > = 0.169 eb {I4} 
$<2+ (633) || E2 || 2+ (1717) > = 0.415 eb {I15} 
$<2+ (1717) || E2 || 2+ (1717) > = 1.33 eb {I6} 
$<2+ (633) || M1 || 2+ (1717) > = -0.263 |m{-N} {I17} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=10.4 ps {I2} from DDCM, 10.7 ps {I4} from DCM reported in authors' earlier paper based on the same experiment as the present one: 2017-Sicliano et al, Nuovo Cimento C 40, 84 (2017), 10.1 ps {I3} from DCM (2021Si26). T{-1/2} from compiler's weighted average of |t=10.37 ps {I20} of the three values. Authors compared their result with |t=10.5 ps {I1} from 1976Es02 (Nucl. Phys. A274, 237); 9.4 ps {I4} from 1969Mi07 (Nucl. Phys. A129, 687); 10.1 ps {I8} from 1970Kl12 (Nucl. Phys. A158, 81); 7.0 ps {I3} from 2016Be24 (Phys. Rev. C 94, 034303); 9.5 ps {I3} (2021Rh01: Phys. Rev. C 103, L051301) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=1.4 ps {I2} from DDCM (2021Si26). Authors compared their result with |t=1.26 ps {I16} from 1969Mi07, 2.5 ps {I2} from 2016Be24, 1.42 ps {I7} (2021Rh01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=0.46 ps {I10} from DDCM, 0.51 ps {I2} from DCM for 1717|g, 0.41 ps {I4} from DCM and 0.55 {I3} from DCM for 1084|g (2021Si26). T{-1/2} from compiler's weighted average of |t=0.51 ps {I3} of the four values. Authors compared their result with |t=0.45 ps {I7} from 1969Mi07; 0.28 ps {I2} from 2016Be24; 0.50 ps {I3} (2021Rh01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=1.7 ps {I5} from DDCM, 1.3 ps {I1} from DCM (2021Si26) for 1163|g. T{-1/2} from compiler's weighted average of |t=1.3 ps {I1} of the two values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Direct population of this state was determined as 59% {I4} (2021Si26) 
T$mean lifetime |t=4.1 ps {I7} from DCM (2021Si26) for 1472|g. Authors compared their result with |t|<2.9 ps from 1983Gu14 (Izv. Akad. Nauk SSSR, Ser. Fiz. 47, 862); >10 ps from 2016Be24 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=1.1 ps {I1} from DCM (2021Si26) for 811|g. Authors compared their result with |t=1.1 ps {I1} from 2016Be24. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+
level_lifetime_unit: NS
level_comment:
T$from {+106}Cd Adopted Levels in the ENSDF database 
$Direct population of this state was determined as 28% {I3} (2021Si26) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$mean lifetime |t<0.3 ps from DCM (2021Si26) for 1746|g. Authors compared their result with |t=0.16 ps {I1} from 2016Be24. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+,3+,4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=2.2 ps {I3} from DCM, 2.4 ps {I2} from DCM for 1853|g (2021Si26). T{-1/2} from compiler's weighted average of |t=2.3 ps {I2} of the two values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=1.3 ps {I6} from DDCM, 1.21 ps {I15} from DCM (2021Si26) for 1009|g. T{-1/2} from compiler's weighted average of |t=1.22 ps {I15} of the two values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
$Direct population of this state was determined as 14% {I3} (2021Si26) 
T$mean lifetime |t=8.2 ps {I4} from DCM (2021Si26) for 525|g by gating on the 691|g from 3320, 6- level. Authors compared their result with |t=7 ps {I+6-3} from 1983Gu14 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$<Q{+2}>=0.443 e{+2}b{+2} {I13} (2022Gr08); if a less likely P{-3}<0, <Q{+2}>=0.428 e{+2}b{+2} {I12} (2022Gr08) 
$<Q{+3}cos(3|d)>=+0.01 e{+3}b{+3} {I6} and <|d>=29 |' {I4} (2022Gr08); if a less likely P{-3}<0, <Q{+3}cos(3|d)>=+0.20 e{+3}b{+3} {I5} and <|d>=15 |' {I5} (2022Gr08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Q{-s}=-0.29 eb {I13} (2022Gr08) 
$<Q{+2}>=0.375 e{+2}b{+2} {I29} (2022Gr08); if a less likely P{-3}<0, <Q{+2}>=0.373 e{+2}b{+2} {I31} (2022Gr08) 
$<0+{-1}|| E2 ||2+{-1}> = 0.636 eb {I9} 
$<2+{-1}|| E2 ||2+{-1}> = -0.38 eb {I17} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$<Q{+2}> >0.28 e{+2}b{+2} {I3} (2022Gr08) 
$<2+{-1}|| E2 ||4+{-1}> = 1.05 eb {I3} 
$<4+{-1}|| E2 ||4+{-1}> = -0.15 eb {I18} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Q{-s}=+0.61 eb {I29} (2022Gr08) 
$<Q{+2}> >0.21 e{+2}b{+2} {I13} (2022Gr08) 
$<0+{-1}|| E2 ||2+{-2}> = 0.195 eb {I15} 
$<2+{-1}|| E2 ||2+{-2}> = 0.44 eb {I3} 
$<2+{-2}|| E2 ||2+{-2}> = 0.81 eb {I38} 
$<2+{-1}|| M1 ||2+{-2}> = -0.31 |m{-N} {I3} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
$<Q{+2}> >0.031 e{+2}b{+2} {I5} (2022Gr08) 
$<2+{-1}|| E2 ||0+{-2}> = 0.176 eb {I14}, determined in 2022Gr08 using the level meanlife of 1.3 ps {I1} from 2021Si26 as a constraint to the GOSIA fit of observed intensities 
$<2+{-2}|| E2 ||0+{-2}> < -0.02 eb 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
J$from optical double resonance (1976Fu06) and |p from L(d,p)=2, configuration=d5/2 
E$|D<r{+2}>=-0.53 (fm{+2}) 
T$from 1974Co16. |g-decay curves. Others: 6.49 h {I5} (1962La10), 6.56 h {I3} (1974Pa15). See also 1939De01, 1939Va02, 1941He01 
|m=-0.615 exp optical double res, -0.62 theory confirms d5/2 single-particle character 
Isotope shift: relative to {+114}Cd (1981Bu15) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T$from (|b{++})(205|g)(t) in {+107}In |e decay (1973Ro30), scin 
J$L=4 (d,p); M1+E2 transition to 5/2+ g.s., configuration=g1/2 
HF(M1,205|g) is in accord with predictions for |DL=2 forbidden transitions (1g7/2 to 2d5/2); see 1973Ro30 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$L=0 (d,p) 
E$low-lying 1/2+ states occur in {+109}Cd, {+111}Cd at 60, 0 keV, respectively; this level needs confirmation. 1973Ny03 in (p,n|g) state that they looked for this level and did not see it. But more 1990Vi07 (p,n|g) found 2 gammas deexciting this level. 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$L=2 (d,p); M1 |g decay to 5/2+ state; J|p=3/2+ determined from excitation function in {+106}Cd(p,p') for probable IAR of 702 level. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$|m: |g(|q,H,t), Q using DPAD method 
E$see 1973Ri14 for near-constant |m measurements of 11/2- isomers in odd-mass cadmium isotopes 
T$from |a|g(t) in (|a,xn|g) (1974Ha41,1974Be17), other: 74 ns {I2} (1995Re15) 
J$E1 transition to 9/2+ state, M2 to 7/2+ state; HF(E1,M2); excit 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$from recoil-distance Doppler shift (1974Ha48), T{-1/2}>2 ps (1991Vi07) 
J$E2 transition to 7/2+ state; excit 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T$from 2007As05, 2007As07, recoil-distance Doppler shift in (HI,xn|g). Others: 16.3 ps {I10} (1974Ha48), 18.3 ps {I7} (2005An26) 
J$E2 transition to 11/2- state; excit 
$|b{-2}=0.12 {i1} (2007As05,2007As07) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
J$E2 transition to 15/2- state; 798|g(|q, linear pol); excit 
T$from 2005An26 using RDM lifetime measurements. Same value from 1991Vi07 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$|m: |g(|q,H,t), Q using DPAD method. 
T$from |a|g(t) in (|a,xn|g) (1974Ha41), Other: 54 ns {I3} (1995Re15) 
J$E1 transition to 19/2- state; 520|g(|q, linear pol); excit interpreted by 1974Ha48 as a 3-particle configuration=((|p g{-9/2}){+-2}{-8+}(|n d{-5/2}){++1}{-5/2+})21/2+. Using empirical g-factors for (|p)g9/2, (|n)d5/2 states, calculated |g(21/2+)=+0.87 {I1}, as for exp g=+0.866 {I10} 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_comment:
J$1076|g (E1) transition to 23/2- state interpreted by 1978St01 as a 3-particle configuration=((|n h{-11/2}){++2}{-10+}(|n d{-5/2}){++1}{-5/2+})25/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T from (>1940|b{++})(205|g)(t) 1973Ro30, scin 
E low-lying 7/2+ states in {+105}Cd, {+109}Cd occur, respectively, at 131, 203 keV 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
Branching: I|g(303|g)/I|g(604|g)/I|g(809|g)=19 {I2}/41 {I3}/100 (1973Ny03), 18 {I2}/48 {I4}/100 (1972Dr09) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J possibly 9/2+ band member based on 5/2+ g.s. (1976Do01). Consistent with E2 and M1 |g-decays to 5/2+ and 7/2+ states, respectively 
Branching: I|g(416|g)/I|g(922|g)/I|g(716|g)=100/72 {I10}/|?20 (1973Ny03) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
Branching: I|g(456|g)/I|g(1377|g)=0.37 {I4} (1973Ny03), 0.60 {I13} (1972Dr09), 0.54 {I6} (1971Ri05) 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
Branching: I|g(499|g)/I|g(611|g)/I|g(915|g)=20 {I3}/50 {I5}/100 (1973Ny03), 10 {I3}/54 {I10}/100 (1972Dr09) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
1976Do01 propose band structure of d3/2 neutron coupled to {+106}Cd core; E(levels) compared (exp vs theory) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$from Doppler shift (1991Vi07) 
Branching: I|g(303|g)/I|g(604|g)/I|g(809|g)=23.5 {I13}/65 {I5}/100 (1974Ha41), 16 {I3}/56 {I10}/100 (1979Oh02) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T weighted average of 67 ns {I6} (1974Ha41) and 77 ns {I7} (1974Be17) from |a|g(t) 
Branching: I|g(36|g)/I|g(640|g)/I|g(845|g)=11.2 {I12}/100/2.3 {I7} (1974Ha41) 
g-factor: -0.184 {I2} (1974Be17), -0.195 {I8} (1974Ha48), -0.201 {I4} (1976Le13) via |g(|q,H,t) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
T$from Doppler shift (1991Vi07) 
Branching: I|g(921.8|g)/I|g(416|g)=0.71 {I8} (1974Ha41), 0.25 {I12} (1979Oh02) is ascribed to I|g doublets; compare I|g-branching=0.72 {I10} via {+107}In decay 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T 16.3 ps {I10} (1974Ha48) recoil-distance Doppler shift 
B(E2)(15/2- to 11/2-)=0.095 {I6}; compare with 1976Es02 measurements B(E2)(2+ to 0+,{+106}Cd)=0.077 {I1}, B(E2)(2+ to 0+,{+108}Cd)=0.081 {I1}, and calculated B(E2)=0.110 {I7} (1976Do01) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T from |a|g(t) (1974Ha41) 
g-factor: +0.866 {I10} (1974Ha48), +0.876 {I15} (1976Le29) via |g(|q,H,t) 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: PS
level_comment:
T$from Doppler shift (1991Vi07) 
Branching: I|g(128|g)/I|g(884|g)=0.40 {I7} (1974Ha41), 0.15 {I5} (1979Oh02) undetermined discrepancy 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
Branching: I|g(303|g):I|g(604|g):I|g(809|g)=20:34:100 (6-MeV p), 14:37:100 (11-MeV p), 26:45:100 (10-MeV p) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
Probably corresponds with L=0 (d,p) excitation at 911 keV 
Branching: I|g(905|g)/I|g(540|g)=0.75 (6-MeV p), 0.82 (11-MeV p) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
Branching: I|g(922|g)/I|g(416|g)=0.63 (6-MeV p), 0.95 (11-MeV p), 0.40 (10-MeV p). Deviation is attributed to |g-ray doublets 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
MOME2$ uncorrelated uncertainty of 0.003, and correlated uncertainty of 0.024 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 47/2+
level_lifetime_unit: PS
level_comment:
T$ effective half-life, not corrected for side feeding. It should be considered as upper limit 
$Q(transition)=1.13 {I9} 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$From 640|g(t) in 2017Gr19. The result accounts for 20% feeding from the J|p=21/2+, T{-1/2}=55 ns isomer. If the feeding from the J|p=21/2+ isomer is neglected, then T{-1/2}=74.9 ns {I14} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
$Spin from 2013Yo02: Phys. Rev. Lett. 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+107}Cd)=+2730.9 MHz {I23} {I54} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -724.0 MHz {I13} {I25} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+107}Cd)=-0.625 fm{+2} {I2} {I12} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
MOME2$statistical uncertainty of 0.007 and systematic uncertainty of 0.025 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$from B(E2)=0.406 {i4}. Other: 7.0 ps {i6} in (HI,xn|g) 
MOMM1$|m, Q are from Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
J$from |g(|q) and |g(pol) for the 569|g in (HI,xn|g), 1978Sa13 conclude |DJ(3110-2541 levels)=2 (J|p 2541=6+). Another solution allowed by |g(|q), namely |DJ=0, is ruled out by the authors on the basis of |g(pol) (pol exp)=0.60 {i20}, pol=0.60 {i5} for |DJ=2 and pol=0.007 to 0.32 for |DJ=0). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2) 
BE2 from 1976Es02. Other: 0.442 {i18} (1969Mi07) x=p 
G from 1980Br01, |g(|q), recoil through thin magnetized Fe layer on Cu backing. Dynamic field calibrated using g-factor=0.285 {i55} for 2+ level in {+110}Cd (1989Ra17) 
MOME2 from 1976Es02, reorientation effect. Value given is for constructive interference from excitation via the second 2+ level. If the interference is destructive, Q=-0.20 {i8} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E authors take E(level) from a now superseded {+108}In |e decay study. This level is not present in the decay scheme adopted here. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+108}Cd)=+2194.0 MHz {I22} {I46} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -588.2 MHz {I13} {I23} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+108}Cd)=-0.510 fm{+2} {I1} {I9} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=10.8 ps {I9} from DDCM, 10 ps {I+3-2} from DCM (2021Si26). T{-1/2} from compiler's weighted average of |t=10.7 ps {I9} of the two values. Authors compared their result with |t=9.9 ps {I1} from 1976Es02 (Nucl. Phys. A274, 237); 9.1 ps {I4} from 1969Mi07 (Nucl. Phys. A129, 687); 10.1 ps {I8} by RDDS method from 1994Th01 (Nucl. Phys. A568, 306) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=1.4 ps {I5} from DDCM (2021Si26). Authors compared their result with |t=1.28 ps {I16} from 1969Mi07, <5 ps (1994Th01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
J$optical-double resonance (1976Fu06); direct |e to 7/2+ level in {+109}Ag; L(d,t)=2 
T$using the Limitation of Relative Statistical Weight method and 462.3 d {I8} (2014Un01), 462.36 d {I33} and 461.92 d {I76} (2011Va02), 459.6 d {I17} (2004Sc04), 460.2 d {I4} (1997Ma75), 463.1 d {i4} (1982La25), 461.9 d {i3} (1981Va11), 450 d {i5} (1968Re04), 459 d {i6} (1968Ea01),453 d {i2} (1965Le06) and 470 d {I8} (1950Gu54). Other: 330 d (1947Br05). Values of 463.2 {i6} (1982HoZJ), 463.26 {i63} (1992Un01,2002Un02) and 462.6 {i6} (2012Fi12) are superseded by 2014Un01 
MOMM1$from 2014StZZ, based on 1972Sp09 and 1963By02 data 
MOME2$from 2013Yo02 by collinear laser spectroscopy. Other: +0.69 {I7} from 1969La06 by optical double resonance. 
CONF$a mixture between |nd{-5/2} and |ng{-7/2} orbitals 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: US
level_comment:
J$L(d,t)=0; 59.6|g E2 to 5/2+ 
T$weighted average of 11.7 |ms {i18} (1968Iv02) and 12 |ms {i3} (1956Pe56) in {+109}Cd IT decay 
CONF$|ns{-1/2} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$L(d,t)=4, 203.5|g M1 to 5/2+ 
T$from microwave modulation of beam and lens spectrometer (1969Be37) 
CONF$|ng{-7/2} 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
J$L(d,t)=5, 259.7|g M2 to 7/2+ 
T$weighted average of 10.4 |ms {i6} (1964Br27), 10.4 |ms {i10} (1966Mc06), 10.8 |ms {i16} (1968Iv02), and 10.8 |ms {i7} in 1975Me22 
MOMM1$from a measurement by the Stroboscopic Observation of Perturbed Angular Distribution (SOPAD) method (2014StZZ) 
MOME2$from 1978Sp09 by the Time Dependent Perturbed Angular Distribution (TDPAD) method. Value measured relative to Q for {+107}Cd and {+111}Cd and by assuming that the magnitude of Q follows the relative h{-11/2} shell filling with an increasing neutron number. 
CONF$|nh{-11/2} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(d,t)=2; J=3/2 is ruled out based on measured 721.8|g(|q) compared with theoretical values using the |h{+2} fits method in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L(d,t)=2; measured C{+2}S=1.3 in (d,t) is considered too large for J=3/2 assignment based on comparisons with theoretical values of neighbouring nuclei by 1975Ch07 in (d,t). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$possible |e feeding from 9/2+; J=7/2 from measured 929.5|g(|q) compared with theoretical values using the |h{+2} fits method in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_lifetime_unit: PS
level_comment:
J$1029.6|g (E2) to (27/2-), 754.7|g E2 to to (27/2-) 
T$from 2000Ch04 in {+96}Zr({+18}O,5n|g) using DSAM, weighted average of 1.26 ps {I+12-8}, 1.25 ps {i5} and 0.85 ps {I+7-6}. 


level_energy_unit: KEV
level_spin_parity: (33/2-)
level_lifetime_unit: PS
level_comment:
J$289.9|g (M1) to (31/2-) 
T$from 2000Ch04 in {+96}Zr({+18}O,5n|g) using DSAM, weighted average of 0.96 ps {i3}, 0.81 ps {I+1-8}, and 1.12 ps {i5}. 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_lifetime_unit: PS
level_comment:
J$920.7|g E2 to (31/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.214 ps {I+14-21}, 0.277 ps {I+21-14}, and 0.236 ps {I+42-7}. 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_lifetime_unit: PS
level_comment:
J$433.3|g (M1) to (33/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.173 ps {i7}, 0.183 ps {I+5-6}, and 0.202 {I+4-6} 


level_energy_unit: KEV
level_spin_parity: (33/2+)
level_comment:
J$301.1|g (M1) to (31/2+) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), 0.248 ps {I+10-8}, weighted average of 0.284 ps {I+27-21}, 0.263 ps {i14}, and 0.222 ps {i14} 


level_energy_unit: KEV
level_spin_parity: (35/2+)
level_lifetime_unit: PS
level_comment:
J$band assignment 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.187 ps {i7}, 0.173 ps {I+6-5} and 0.166 ps {I+5-9} 


level_energy_unit: KEV
level_spin_parity: (37/2-)
level_lifetime_unit: PS
level_comment:
J$631.5|g (M1) to (35/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.215 ps {I+14-21}, 0.194 ps {I+7-14}, and 0.142 ps {I+2-5} 


level_energy_unit: KEV
level_spin_parity: (39/2-)
level_lifetime_unit: PS
level_comment:
J$1039.0|g (E2) to (35/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.28 ps {i3}, 0.284 ps {I+14-7}, and 0.24 ps {i2} 


level_energy_unit: KEV
level_spin_parity: (37/2+)
level_lifetime_unit: PS
level_comment:
J$463.0|g (M1) to (35/2+) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.148 ps {I+5-6}, 0.146 ps {i3}, and 0.141 ps {I+3-15} 


level_energy_unit: KEV
level_spin_parity: (39/2-)
level_lifetime_unit: PS
level_comment:
J$759.0|g (M1) to (37/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.187 ps {I+14-21}, 0.235 ps {i14}, and 0.249 ps {I+14-21} 


level_energy_unit: KEV
level_spin_parity: (39/2+)
level_lifetime_unit: PS
level_comment:
J$540.6|g (M1) to (37/2+) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.067 ps {i4}, 0.078 ps {I+3-7}, and 0.091 ps {I+4-6} 


level_energy_unit: KEV
level_spin_parity: (43/2-)
level_lifetime_unit: PS
level_comment:
J$1191.6|g (E2) to (39/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.110 ps {I+7-14}, 0.130 ps {I+3-13}, and 0.133 ps {I+6-4} 


level_energy_unit: KEV
level_spin_parity: (41/2+)
level_lifetime_unit: PS
level_comment:
J$band assignment 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.059 ps {I+4-6}, 0.049 ps {I+4-5}, and 0.067 ps {I+3-9} 


level_energy_unit: KEV
level_spin_parity: (47/2-)
level_lifetime_unit: PS
level_comment:
J$1367.0|g (E2) to (43/2-) 
T$from 2000Ch04 using DSAM in {+96}Zr({+18}O,5n|g), weighted average of 0.126 ps {i5}, 0.119 ps {I+6-5}, and 0.126 ps {I+5-6} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (37/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$band assignment 
E$x >5730, since transitions from this level feed members of bands #10 and #11 as labeled by 2000Ch04 


level_energy_unit: KEV
level_spin_parity: 31/2-
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.85 ps {I+7-6} 1.26 ps {I+11-8}, and 1.25 ps {I+10-8} 


level_energy_unit: KEV
level_spin_parity: 35/2-
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.214 ps {+14-21}, 0.277 ps {I+21-14}, and 0.236 ps {I+42-7} 


level_energy_unit: KEV
level_spin_parity: 35/2-
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.173 ps {I7}, 0.183 ps {I+5-6}, and 0.202 ps {I+4-6} 


level_energy_unit: KEV
level_spin_parity: 33/2+
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.284 ps {I+27-21}, 0.263 ps {I+14-14}, and 0.222 ps {I+14-14} 


level_energy_unit: KEV
level_spin_parity: 35/2+
level_lifetime_unit: PS
level_comment:
T$ using DSAM in 2000Ch04, weighted average of 0.187 ps {I7}, 0.173 ps {I+6-5}, and 0.166 ps {I+5-9} 


level_energy_unit: KEV
level_spin_parity: 37/2-
level_lifetime_unit: PS
level_comment:
T$ using DSAM in 2000Ch04, weighted average of 0.215 ps {I+14-21}, 0.194 ps {I+7-14}, and 0.142 ps {I+2-5} 


level_energy_unit: KEV
level_spin_parity: 37/2+
level_lifetime_unit: PS
level_comment:
T$ using DSAM in 2000Ch04, weighted average of 0.148 ps {I+5-6}, 0.146 ps {I3}, and 0.141 ps {I+3-15} 


level_energy_unit: KEV
level_spin_parity: (39/2-)
level_lifetime_unit: PS
level_comment:
T$ using DSAM in 2000Ch04, weighted average of 0.187 ps {I+14-21}, 0.235 ps {I14}, and 0.249 ps {I+14-21} 


level_energy_unit: KEV
level_spin_parity: 39/2+
level_lifetime_unit: PS
level_comment:
T$ using DSAM in 2000Ch04, weighted average of 0.067 ps {I4}, 0.078 ps {I+3-7}, and 0.091 ps {I+4-6} 


level_energy_unit: KEV
level_spin_parity: 43/2-
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.110 ps {I+7-14}, 0.130 ps {I+3-13}, and 0.133 ps {I+6-4} 


level_energy_unit: KEV
level_spin_parity: 41/2+
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.059 ps {I+4-6}, 0.049 ps {I+4-5}, and 0.067 ps {I+3-9} 


level_energy_unit: KEV
level_spin_parity: 47/2-
level_lifetime_unit: PS
level_comment:
T$using DSAM in 2000Ch04, weighted average of 0.126 ps {I+5-5}, 0.119 ps {I+6-5}, and 0.126 ps {I+5-6} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (37/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x >5730, since transitions from this level feed members of bands #10 and #11 as labeled by 2000Ch04 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_uncertain: ?
level_comment:
E$proposed by 1994Ju05 in {+100}Mo({+13}C,4n|g) based on the 999.0|g, but not observed in {+96}Zr({+18}O,5n|g) by the same authors. Evaluators have considered this assignment questionable. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$from 1992Si05 only, J=3/2 is ruled out based on 721.8|g(|q) using the |h{+2} fits method. 
T$Weighted average of 104 fs {I+49-28} (using 721|g) and 69 fs {I+21-17} (using 518|g) in 1982Av07. 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: FS
level_comment:
J$5/2+ from 1992Si05 
T$ weighted average of 47 fs {I+15-11} (using 891|g) and 31 fs {I+10-7} (using 831|g) in 1982Av07. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$9/2+ in 1992Si05 
T$weighted average of 76 fs {I35-21} (using 794|g(t)) and 59 fs {I+24-14} in 1982Av07. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_uncertain: ?
level_comment:
E$not confirmed in 1988Vi03 
J$from 1992Si05 based on measured 929.5|g(|q) 
T$weighted average of 83 fs {i+55-28} (using 932|g in 1982Av07) and 49 fs {i+38-26} (using 932|g in 1988Ch35). 


level_energy_unit: KEV
level_spin_parity: 5/2+,3/2+
level_comment:
L$1975Ch07 state in text that L=0+2 (70% L=2, 30% L=0) provides best fit to the angular distribution of the 890-keV peak. However, in authors' table of results only L=2 is given. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
T$weighted average of 10.4 |ms {i6} (1964Br27), 10.4 |ms {i10} (1966Mc06), 10.8 |ms {i16} (1968Iv02), 10.8 |ms {i7} in 1975Me22 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+109}Cd)=+1958.3 MHz {I22} {I38} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -515.3 MHz {I6} {I21} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+109}Cd)=-0.445 fm{+2} {I1} {I9} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
T$from 2016Fe04 from weighted least-squares exponential fit to 13 measurements taken over 223 days and 141 measurements taken over 930 day, with the two measurements separated by 1036 days. Uncertainty includes standard deviation of the residuals (0.07%), trend in residuals (0.10%), geometric reproducibility (0.07%), background subtraction (0.0002%), impurities (0.01%), efficiency stability (0.08%) and linearity (0.02%), combined in quadrature. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L((pol d,t),(d,t))=L(|a,|a')=L(p,t)=2; 657.7600|g E2 to 0+ 
T$Weighted average of 6.4 ps {I4} (recoil-distance technique in 1993Pi16), 6.0 ps {I8} (recoil-distance technique in 2001Ha09) and 5.36 ps {I9} (extracted from the adopted B(E2)|^=0.427 {I3}) 
MOMM1$Weighted average of 0.57 {I11} (using dynamic field technique (1980Br01)), 0.50 {I4} (reevaluated value based on the strength of the hyperfine field and the precession angle given at nuclear orientation measurement in {+110}Ag |b{+-} decay (249.83 d) (1978Wa07), using adopted T{-1/2}=5.42 {I16}), 0.62 {I14} (using recoil gas into vacuum technique in Coulomb excitation (1979LaZL)) and 0.50 {I20} (reevaluated value from the reference within 1989Be22, using adopted T{-1/2}=5.42 {I16}). Other: 0.81 {I6} from transient filed technique in 2011Ch23 
MOME2$Weighted average of -0.39 {I4} (weighted average of -0.39 {I6} (1977Ma41), -0.36 {I8} (1976Es02) and -0.42 {I10} (1971Be36) in Coulomb excitation) and -0.40 {I4} (deduced from fits to the inelastic electron scattering cross sections within the framework of the anharmonic vibrational model in {+110}Cd(e,e') (1977Gi13)). Others: -0.55 {I8} (or -0.31 {I7} in 1971Ha08) and -0.24 {I9} (relative to {+114}Cd in 1970St17) 
BE2$Weighted average of 0.45 {I4} (1991We15), 0.454 {I43} (1977Gi13) from {+110}Cd(e,e'), 0.427 {I3} (weighted average of 0.415 {I6} (1985Si01), 0.432 {I6} (1972Be66 and 1971Be36) and 0.427 {I4} (1976Es02), 0.44 {I4} (1971Ha08), 0.467 {I19} (1969Mi07), 0.50 {I4} (1958St32), 0.41 {I6} (1956Te26) and 0.436 {I22} (relative to B(E2)|^({+114}Cd) in 1970St17), in Coulomb excitation). Others: 0.459 (average of 0.474, 0.444, 0.460 and 0.456 in 1965Mc05) and 0.42 (1958Sh01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$E0 to g.s.; 815.31|g E2 to 2+; |g|g(|q) in {+110}Ag |b{+-} decay (24.56 s) is only consistent with J=0, with J(657 keV level)=2 (1972Ka34) 
$B(E0; 0+ to 0+ g.s. level)/B(E2; 0+ to 657 keV, 2+ level)=0.027 {I4} (1990Gi01, {+110}In |e decay (69.1 min)) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1475.7792|g E2 to 0+; 818.0244|g M1+E2 to 2+ 
BE2$Weighted average of 0.021 {I3} (1969Mi07) and 0.023 {I7} (1961St02) in Coulomb excitation. Other: 0.014 {I3} (1991We15) in {+110}Cd(e,e') 
T$From adopted B(E2)|^=0.021 {I3} and |g branching. Others: 1.02 ps {I22} (from B(E2)|^=0.014 {I3} (1991We15) in {+110}Cd(e,e')), 0.8 ps {I+4-2} (1995KuZX) and 0.74 {I19} (1999Lo15) (using Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(pol d,t)=4; 884.6781|g E2 to 2+; band member 
T$Weighted average of 0.7 ps {I4} (2001Ha09) (from recoil-distance method, differential decay-curve analysis in (HI,xn|g)) and 0.82 ps +22-12 (1999Lo15) (from {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)). Other: <2.1 ps (1993Pi16) from (HI,xn|g) 
MOMM1$5.4 {I+14-13} 
MOMM1$From g-factor=1.36 +34 -33 deduced using the strength of the hyperfine field and the precession angle given at nuclear orientation measurement in {+110}Ag |b{+-} decay (249.83 d) (1978Wa07), and adopted T{-1/2}=0.80 {I+17-16} 
BE4$0.5|*10{+-3} {I5} (1991We15) from {+110}Cd(e,e') 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$E0 to g.s.; 1073.55|g E2 to 2+; L({+3}He,d)=1 
$B(E0; 0+ to 0+ g.s. level)/B(E2; 0+ to 657 keV, 2+ level)<0.049 (1990Gi01) from {+110}In |e decay (69.1 min) 
$B(E2; 0+ to 657 keV, 2+ level)|*B(E2; 0+ to 0+ g.s. level)/B(E2; 0+ to 657 keV, 2+ level)|*B(E2; 0+ to 1475 keV, 2+ level)<0.00029 (1990Gi01) from {+110}In |e decay (69.1 min) 
$B(E0; 0+ to 1473 keV, 0+ level)/B(E2; 0+ to 657 keV, 2+ level)<7.2 (1990Gi01) from {+110}In |e decay (69.1 min) 
$B(E0; 0+ to 1473, 0+ level)/B(E2; 0+ to 1475 keV, 2+ level)<0.042 (1990Gi01) from {+110}In |e decay (69.1 min) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1783.49|g E2 to 0+; 1125.709|g M1+E2 to 2+; band member; |g|g(|q) in {+110}Ag |b{+-} decay (24.56 s) is only consistent with J=2, with J(657 keV level)=2 (1972Ka34) 
$B(E2)|^=0.005 {I3} (1990We08) from {+110}Cd(e,e') 


level_energy_unit: KEV
level_spin_parity: 4+
level_uncertain: ?
level_comment:
E,J$From {+110}Cd(e,e'). E|g=1151.9 keV was assigned in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1990Ke02) to depopulate the 1809.66-keV state (J|p=(2+)). However, this level was not observed in 1992Ku01, where it was stated that this |g-ray belongs to {+111}Cd 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$From L(|a,|a')=3; 1421.06|g E1 to 2+ 
T$From Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1995KuZX and 1999Lo15). Other: 0.46 ps {I+15-9} in {+110}Cd(n,n'|g) (2001Co01) (using Doppler shift attenuation method) 
$B(E3)|^=0.11 {I1} (weighted average of 0.10 {I2} (from 1965Mc05, under assumption that only direct E3 excitation is involved) and 0.115 {I13} (1985Fe05) in Coulomb excitation). Other: 0.63 (1963Ha20) in {+110}Cd(|a,|a') 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$E0's to 0+; 295.30|g E2 to 2+; |g|g(|q) in {+110}Ag |b{+-} decay (24.56 s) is only consistent with J=0, with J(657 keV level)=2 (1972Ka34) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$677.6217|g M1+E2 to 4+; 744.2755|g E2 to 2+ 
$B(E4)|^=6.2|*10{+-3} {I16} (1991We15) from {+110}Cd(e,e') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1629.65|g E2(+M1) to 2+; assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) and {+110}Cd(p,p'),{+110}Pd(d,d'); L({+3}He,d)=(1) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=(6); 937.485|g E2 to 4+; band member 
T$Using recoil-distance method, differential decay-curve analysis in (HI,xn|g) (2001Ha09). Others: 0.40 ps {I+15-9} (in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1999Lo15) using Doppler shift attenuation method), 0.2 ps {I+8-1} (in {+110}Cd(n,n'|g) (2001Co01) using Doppler shift attenuation method), <2.1 ps (in (HI,xn|g) (1993Pi16) using recoil-distance method) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.6 ps {I+4-2} (in {+110}Cd(n,n'|g) (2001Co01), using Doppler shift attenuation method) and 0.6 ps {I+3-2} (in {+108}Pd(|a,2n|g), {+110}Pd(|a,4n|g) (1995KuZX and 1999Lo15), using Doppler shift attenuation method) 
J$460.85|g E2 to 3-; 997.256|g E1 to 4+; L({+3}He,d)=4 


level_energy_unit: KEV
level_spin_parity: (2-,3)
level_comment:
J$782.8|g and 1908.7|g to 2+; branching ratios would favor dipole transitions; the absence of |g's to 0+ would argue against J|p=1 and 2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1090.83|g to 4+; 1975.2|g E2+M1 to 2+; assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) and {+110}Cd(p,p'),(d,d') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
J$2649.92|g E1 to 0+ 
T$Other: 0.0203 ps {I5} from {+110}Cd(|g,|g'), deduced using ground state transition width |G{-0} and adopted branching ratios. Note that authors of 2005Ko32 only quote depopulating 2649.92|g, but not the 1176.8|g one resulting in T{-1/2}=0.0298 ps {I8}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$2004.40|g E2 to 2+; direct population in {+110}Ag |b{+-} decay (24.56 s) (J|p=1+); |g|g(|q) in {+110}Ag |b{+-} decay (24.56 s) is only consistent with J=0, with J(657 keV level)=2 (1972Ka34). Note that L((pol d,t),(d,t))=2+4 would suggest J|p=3+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J$2211.33|g M1+E2 to 2+; 2869.28|g to 0+; direct population in {+110}In |e decay (69.1 min) (J|p=2+) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$339.498|g E2 to 5-; 399.254|g E1(+M2) to 6+ 
T$Weighted average of 0.69 ns {I42} (from recoil-distance measurement in (HI,xn|g) (1993Pi16)), 0.62 ns {I14} (deduced using |g|g(t) in (HI,xn|g) (1994Ju04)), 0.60 ns {I10} (from generalized centroid-shift method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)(1998Ko35)). Other: <0.87 ns in (HI,xn|g) (2001Ha09) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$369.20|g E2 to 5-; 149.88|g M1(+E2) to 7-; band member 
T$From centroid-shift method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1998Ko35) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$3042.98|g M1 to 0+ 
T$Deduced from the ground state transition width |G{-0} in {+110}Cd(|g,|g') (2005Ko32) and the adopted branching ratios 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: NS
level_comment:
J$159.746|g E2 to 6-; 176.517|g M1+E2 to 7-; band member 
T$Weighted average of 2.25 ns {I10} (from centroid-shift method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1998Ko35)) and 2.4 ns {I4} (from |g|g(t) in (HI,xn|g) (1994Ju04)) 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: FS
level_comment:
J$3078.42|g (M1) to 0+; 2420.51|g to 2+; direct population in {+110}In |e decay (69.1 min) (J|p=2+) 
T$Deduced from the ground state transition width |G{-0} in {+110}Cd(|g,|g') (2005Ko32) and the adopted branching ratios 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J$3128|g to 0+; 1344.88|g to 2+; direct population in {+110}In |e decay (69.1 min); assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) 


level_energy_unit: KEV
level_spin_parity: 2+,3+,4+
level_comment:
E$Weighted average of 3141 {I3} (from {+111}Cd(pol d,t),{+111}Cd(d,t)) and 3143 {I3} (from {+110}Cd(p,p'),(d,d')) 
J$From {+111}Cd(pol d,t),{+111}Cd(d,t) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$1+,2+,3+ in {+111}Cd(pol d,t),{+111}Cd(d,t); 1030.0|g to 3+ and 1410.08|g to 2+. The absence of |g's to 0+ would argue against J|p=1+ and 2+ 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_comment:
E$Probably a component of unresolved doublet in {+111}Cd(pol d,t),{+111}Cd(d,t) 
J$1666.23|g to 4+; direct population in {+110}In |e Decay (69.1 min) (J|p=2+); assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=(8); 795.5|g E2 to 6+; band member 
T$Weighted average of 0.62 ps {I21} in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (using Doppler shift attenuation method (1995KuZX)) and 1.0 ps {I4} in (HI,xn|g) (using recoil-distance method, differential decay-curve analysis (2001Ha09)). Others: <2.8 ps in (HI,xn|g) (1993Pi16), (using recoil-distance method), >0.83 ps in (1999Lo15) (using Doppler shift attenuation method) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: FS
level_comment:
J$3281|g (M1) to 0+; 2620.00|g to 2+ 
T$From {+110}Cd(|g,|g') (2005Ko32), by assuming that only 3281|g depopulate this level 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$3298.1|g D to 0+; 2640.1|g to 2+; assignment in {+110}Cd(p,p'), {+110}Cd(d,d') 
T$From {+110}Cd(|g,|g') (2005Ko32), by assuming that only 3298|g depopulate this level 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$1235.67|g to 3-; 1583.18|g to 0+; 1151.70|g to 3+; direct population in {+110}In |e Decay (69.1 min) (J|p=2+) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$L({+3}He,d)=2, 3403.48|g to 0+; 2745.45|g to 2+. However, assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) suggests J|p=1+,2+,3+ 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$959.785|g E2 to 6+; 164.26|g M1(+E2) to 8+ 
T$From Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1995KuZX). Others: <2.8 ps in (HI,xn|g) (from recoil distance method (1993Pi16)) and >1.11 ps from Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g)(1999Lo15) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$3475.34|g (M1) to 0+; direct population in {+110}In |e Decay (69.1 min) (J|p=2+). Note that J|p=1- in {+110}Cd(p,p'),(d,d') 
T$Deduced from |G{-0} in {+110}Cd(|g,|g') (2005Ko32), by assuming that only 3475|g depopulate this level 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J$460.85|g E2(+M1) to 6+; 1982.77|g to 4+; direct population in {+110}In |e decay (4.92 h) (J|p=7+) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$3596.9|g M1 to 0+ 
T$Deduced using ground state transition width |G{-0} in {+110}Cd(|g,|g') (2005Ko32) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T$Weighted average of 0.45 ns {I10} (from generalized centroid shift method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1998Ko35)), 0.56 ns {I3} (from recoil distance method in (HI,xn|g) (1993Pi16)), 0.49 ns {I14} (from |g|g(t) in (HI,xn|g)(1994Ju04)) and 0.464 ns {I17} (using recoil-distance method, differential decay-curve analysis in (HI,xn|g) (2001Ha09)) 
J$335.596|g E2 to 8+; 265.218|g E1(+M2) to 9- 
MOMM1$From g-factor=-0.09 {I3} in 1995Re15, deduced using the perturbed angular-correlation technique and T{-1/2}=0.56 ns {I3}, and the adopted T{-1/2}=0.487 ns {I24} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$3772|g M1 to 0+. Note, that 1+,2+,3+ in {+111}Cd(pol d,t),{+111}Cd(d,t) and (2+,3-) {+110}Cd(p,p'),(d,d') 
T$Deduced using ground state transition width |G{-0} given in {+110}Cd(|g,|g') (2005Ko32) and the adopted branching ratios 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: PS
level_comment:
J$767.532|g E2 to 8-; 477.45|g M1 to 9-; band member 
T$Other: >2.1 ps from Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) ((1995KuZX) and (1999Lo15)) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: FS
level_comment:
E$From {+111}Cd(pol d,t),{+111}Cd(d,t) 
J$3854|g (M1) to 0+; 1+,2+,3+ assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: FS
level_comment:
J$3862|g (M1) to 0+; 1+,2+,3+ assignment in {+111}Cd(pol d,t),{+111}Cd(d,t) 
T$Deduced using ground state transition width |G{-0} given in {+110}Cd(|g,|g') (2005Ko32) and adopted branching ratios 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$801.724 E2 to 8+ 
T$Weighted average of 0.69 ps {I21} (from recoil-distance method in (HI,xn|g) (1993Pi16)) and 0.8 ps {I+4-2} (from Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1999Lo15)). Others: >1.4 ps (from Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1995KuZX)), <3.5 ps (from recoil-distance Doppler shift technique, using the differential decay curve method in (HI,xn|g) (2001Ha09)) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$561.034|g E2 to 10+; band member 
T$Weighted average of 8.3 ps {I4} (from recoil-distance method in (HI,xn|g) (1993Pi16)) and 7.9 ps {I4} (from recoil-distance Doppler shift technique, using the differential decay curve method in (HI,xn|g) (2001Ha09)) 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
J$826.893|g E2 to 9-; band member 
T$Other: 1.7 ps {I+14-7} from Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1995KuZX and 1999Lo15) 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: PS
level_comment:
J$736.7|g M1 to 10-; 877.0|g E2 to 9-; band member 
T$From Doppler shift attenuation method in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g) (1995KuZX and 1999Lo15) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$811.093|g E2 to 10+; band member. Other: J|p=12+ in {+108}Pd(|a,2n|g),{+110}Pd(|a,4n|g), interpreted as a member of the g.s. band 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
J$854.25|g E2 to 12+; band member. 
T$Other: <2.8 ps (from recoil-distance method, differential decay-curve analysis in (HI,xn|g) (2001Ha09)) 


level_energy_unit: KEV
level_spin_parity: 22+
level_lifetime_unit: PS
level_comment:
J$1314.1|g E2 to 20+; band member 
T$From Doppler shift attenuation method using the line-shape analysis in (HI,xn|g) (2011Ro01). The quoted uncertainty does not include additional systematics error in the stopping powers that may be as large as 20%. Note that T{-1/2}=0.11 ps {I4} was deduced by including 1100|g. However, authors of 2011Ro01 stated that 1100-keV |g was not confirmed in their |g|g-coincidence gated spectra (see XUNDL compilation dated on January 5th, 2011) and they reported T{-1/2}=0.15 ps {I5} 


level_energy_unit: KEV
level_spin_parity: 26+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
J$1443|g E2 to 24+; band member 
T$Effective T{-1/2} from Doppler shift attenuation method using the line-shape analysis in (HI,xn|g) (2011Ro01). 1443|g which depopulate 12763 keV J|p=26+ and 14206 keV J|p=28+ levels was used to deduce the effective T{-1/2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$B(E0; 0+ to 0+ g.s. level)/B(E2; 0+ to 657 keV, 2+ level)<0.049 (1990Gi01) 
$B(E2; 0+ to 657 keV, 2+ level)|*B(E2; 0+ to 0+ g.s. level)/B(E2; 0+ to 657 keV, 2+ level)|*B(E2; 0+ to 1475 keV, 2+ level)<0.00029 (1990Gi01) 
$B(E0; 0+ to 1473 keV, 0+ level)/B(E2; 0+ to 657 keV, 2+ level)<7.2 (1990Gi01) 
$B(E0; 0+ to 1473, 0+ level)/B(E2; 0+ to 1475 keV, 2+ level)<0.042 (1990Gi01) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=1 member C{+2}S'=0.032 (J|p=0+,1+,2+), for L=2 member C{+2}S'=0.053 (J|p=1-,2-,3-) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=(1) member C{+2}S'=(0.023) (J|p=(0+,1+,2+)), for L=2 member C{+2}S'=0.067 (J|p=1-,2-,3-) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=0 member C{+2}S'=0.019 (J|p=0-,1-), for L=4 member C{+2}S'=0.68 (J|p=4-,5-) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=(1) member C{+2}S'=(0.007) (J|p=(0+,1+,2+)), for L=2 member C{+2}S'=0.015 (J|p=1-,2-,3-) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=(2) member C{+2}S'=(0.011) (J|p=(1-,2-,3-)), for L=4 member C{+2}S'=0.40 (J|p=3-,4-,5-) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=(2) member C{+2}S'=(0.02) (J|p=(1-,2-,3-)), for L=(4) member C{+2}S'=(0.04) (J|p=(3-,4-,5-)) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=(0) member C{+2}S'=(0.049) (J|p=(0-,1-)), for L=2 member C{+2}S'=0.29 (J|p=1-,2-,3-) 


level_energy_unit: KEV
level_comment:
$Unresolved doublet. For L=(0) member C{+2}S'=(0.09) (J|p=(0-,1-)), for L=2 member C{+2}S'=0.39 (J|p=1-,2-,3-) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
BE1$deduced using |G{-0}=0.0153 eV {I4} (2005Ko32) 
$Interpreted as member of two-phonon quintuplet (2+~#3-) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
T$18 fs 3 from author's deduced transition probabilities 
BM1,BE1$Deduced using |G{-0}=0.0078 eV {I12} (2005Ko32) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
BE2$0.45 {I4} (1991We15), 0.454 {I43} (1977Gi13) 
MOME2$-0.40 {I4} 
MOME2$Deduced from fits to the inelastic electron scattering cross sections within the framework of the anharmonic vibrational model in 1977Gi13 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|b{-3}=0.146 {I15} (1989Va02), 0.16 (1969Ko01), 0.168 (1969Lu02), 0.138, 0.122 (from (p,p') and (d,d'), respectively in 1990Pi14) 


level_energy_unit: KEV
level_comment:
BE3$0.63, uncertainty 30% to 50% (1963Ha20) 
$1400 keV {i3} |g-ray depopulating this state was observed by 1963Ha20 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
BE2$Weighted average of 0.415 {I6} (1985Si01), 0.427 {I4} (1976Es02), 0.432 {I6} (1972Be66 and 1971Be36), 0.44 {I4} (1971Ha08), 0.467 {I19} (1969Mi07), 0.50 {I4} (1958St32), 0.41 {I6} (1956Te26) and 0.436 {I22} (relative to B(E2)|^({+114}Cd) in 1970St17). Others: 0.459 (average of 0.474, 0.444, 0.460 and 0.456 in 1965Mc05), and 0.42 (1958Sh01) 
MOMM1$0.57 {I11} using dynamic field technique (1980Br01) and 0.62 {I14}, using recoil gas into vacuum technique (1979LaZL) 
MOME2$Weighted average of -0.39 {I6} (1977Ma41), -0.36 {I8} (1976Es02) and -0.42 {I10} (1971Be36). Others: -0.55 {I8} (or -0.31 {I7} in 1971Ha08) and -0.24 {I9} (relative to {+114}Cd in 1970St17) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3$Weighted average of 0.10 {I2} (from 1965Mc05, under assumption that only direct E3 excitation is involved) and 0.115 {I13} (1985Fe05) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T$From 2001Ha09. Other: 0.7 ns {I2} (1994Ju04) and 0.55 ns {I3} (1993Pi16) 
MOMM1$Using ion-implantation perturbed-angular-correlation (IMAP) technique in 1995Re15 (g-factor=-0.09 {i3} deduced using T{-1/2}=0.56 ns 3) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
MOMM1$0.52 {I3} from adopted levels. Other: 0.56 {I10} (from g=0.28 {I5}, deduced using T{-1/2}=5 ps {I1} in nuclear orientation (1978Wa07)) in {+110}Ag |b{+-} Decay (249.83 d) 


level_energy_unit: KEV
level_spin_parity: 2+
level_uncertain: ?
level_comment:
A 2287.41 level is fed from J|p=1+ {+110}Ag |b{+-} decay (24.6 s). Because no |g feeding from higher levels is observed here from J|p=6+ {+110}Ag |b{+-} decay (249.76 d), the weak |b feeding to this level suggests a high spin (J|>4); therefore, the possibility of a close-lying doublet is not excluded. 


level_energy_unit: KEV
level_spin_parity: 0+
level_uncertain: ?
level_comment:
$Observation in this decay is questionable because of J|p=0+ assignment in {+110}Ag |b{+-} decay (24.6 s), and no |g feeding to this level is observed here. Otherwise, this must be a close-lying doublet 


level_energy_unit: KEV
level_comment:
$C{+2}S(d3/2)=0.027 for J|p=1+,2+,3+ component, C{+2}S(d5/2)=0.021 for for J|p=1+,2+,3+ component, C{+2}S(h11/2)=0.094 for J|p=5-,6- component 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$ 657.765 {I2} in table III of 2012Ga41, even though it is stated that the value is from Nuclear Data Sheets (or ENSDF) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
MOMM1$From g=-0.29 {I16}, deduced in 2017Gr19 from re-evaluation of previous data (1995Re15), T{-1/2}=485 ps {I21} and the field distribution data from the measurements of {+107}Cd in 2017Gr19. 
CONF$Seniority-two |n(h{-11/2}){+2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+110}Cd)=+1432.2 MHz {I23} {I30} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -382.4 MHz {I5} {I15} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+110}Cd)=-0.334 fm{+2} {I1} {I6} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
MOME2$others: +0.80 {i10} (1983Er01), +0.83 {i13} (1983He02) 
MOMM1$other: -0.76 {i5} (1989Be22) 
T$weighted average: 84.1 ns {i5} (1957Ma26) |g|g(t), 84.8 ns {I+8-5} (1957Si63) |g|g(t) from |e decay, and 85.0 ns {i7} (1968Mc04) from |b{+-} decay 
J$E2 |g decay to ground state; E3 |g from J=11/2 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.110 {i9} in Coul. ex. and |d(342|g)=0.36 {i2}. Others: 59 ps {i12} (1970Ra16) 62 ps {i17} (1961Fr08), 42 ps {i6} (1971Sh21) res scattering cross section as a function of temperature. A weighted av of these other values gives 47 ps {i5} which requires |d(342|g)=0.53 {i5} if B(E2)=0.110 {i9} 
J$M1+E2 |g decay to 1/2+ state 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$optical double resonance (1976Fu06), L(d,p)=5. Measured moments of odd-mass {+105}Cd-{+115}Cd are compared with theoretical predictions (1989Be22). 
T$from weighted average with Limitation of Relative Statistical Weight, lrsw, method (1985ZiZY,1992Ra09) of 48.7 m {i3} (1945Wi11), 50 m {i2} (1948Ho37), 48.6 m {i3} (1949He06), 49.4 m {i7} (1968Bo28), 48.54 m {i5}, (1987Ne01), and 48.30 m {i15} [Xiao-qiong Wen et al. Nucl. Instr. Meth. A379 (1997) 478]. In the lrsw process the uncertainty for the value of 1987Ne01 is increased from 0.05 to 0.12 to decrease its relative weight to 50%. 
MOMM1$other: -1.1055 (1989Be22) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
T$from |g|g(t) in Coul. ex. Other: 11 ps {i2} (1968Mc04) 
J$L=2 and cross-section ratio (d,p)/(d,t); allowed |b{+-} transition from 7/2+ excludes 3/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$based on probable |g decay to 1/2+ g.s. and allowed (log| {Ift}=4.6) |b{+-} transition from 7/2+ {+111}Ag isomer 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$M1+E2 |g to 1/2+ g.s., |g(|q) and linear polarization in (n,n'|g). 
E$1991NeZX suggest correspondence with the 1020 level, but this would require the |g(|q) and |g(pol) for the 1016|g giving mult=M1+E2 to be in error 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$from |b|g(t) (1970Ra16) scin 
E$branching: I|g(97|g)/I|g(342|g)=0.03 {I1} av of 0.042 {I1} (1970Hn04), 0.038 (1974BuZU), 0.034 {I2} (1975PuZZ), 0.018 {I2} (1975Sh29), 0.016 (1974HeYW) via {+111}Ag g.s. decay (690|b)(340|g)(|q); deduced nuclear matrix element (1960Ha29) (690|b)(340|g,CP)(|q); deduced nuclear matrix element (1966De03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$48.6 min {I3} (1949He06), 48.7 min {I3} (1945Wi11). Others: 49.6 min {I7} (1968Bo28), 50 min {I2} (1948Ho37) 
J$consistent with A{-2}=+0.175 {I14} (1953Kr48) via (151|g)(245|g)(|q) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
g=+0.02 {i79} (1989Be22) 
BE2$B(E2)=0.087 {i10} (1968Mc04), 0.11 {i2} (1969Ga25), 0.098 {i5}(1985Si01) 
T$from B(E2) and |d(342)=0.36 {i2} 
Branching: I|g(97|g)/I|g(342|g)=0.017 (1958Mc02), 0.014 (1968Mc04). Other: 0.03 {i1} av ({+111}Ag g.s. decay) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
g=+0.11 {i5} (1989Be22) 
BE2$others: 0.133 {i11} (1985Si01), 0.126 {i17} (1968Mc04), 0.14 {i3} (1969Ga25) 
Branching: I|g(620|g)/I|g(375|g)/I|g(279|g)=76/19/4.4 (1969Ga25), 71/25/3.8 (1968Mc04), 79/18/3 (1958Mc02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
Branching: I|g(413|g)/I|g(508|g)/I|g(755|g)=12/56.6/31.4 (1968Mc04), 17/41/42 (1975AnYZ) 
BE2$others: 0.022 {i7} (1969Ga25), 0.027 {i8} (1985Si01) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
MOME2$ uncorrelated uncertainty of 0.004, and correlated uncertainty of 0.030 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$doublet of two 3/2+ levels at 864.8 and 866.6 keV in the ENSDF database for {+111}Cd (Adopted as well as decay datasets) is not supported by the results in 2015Kr07; only one level is proposed here based on close inspection of width of the |g-ray peaks. Results in 2015Kr07 are in agreement with those from (n,n'|g) as given in the ENSDF database, and {+111}Ag decay study by 2014Co08 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$spi from 2013Yo02: Phys Rev Lett 110, 192501. Parity from {+111}Cd Adopted Levels in the ENSDF database (Feb 2008 update) 
$Measured isotope shift |d|n({+114}Cd,{+111}Cd)=+1314.3 MHz {I22} {I23} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -334.4 MHz {I13} {I10} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+111}Cd)=-0.288 fm{+2} {I1} {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$statistical uncertainty of 0.005 and systematic uncertainty of 0.031 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=2; 617.52|g E2 to 0+ 
T$from B(E2)|^(617.52|g)=0.486 {I3}; weighted average of 0.486 {I5} (1985Si01), 0.524 {I50} from {+112}Cd(e,e') in (1977Gi13), 0.484 {I4} (1976Es02), 0.478 {I33} (1970St17), 0.524 {I21} (1969Mi07), 0.514 {I60} (1965Mc05) and 0.546 {I39} (1962Ec03) 
MOME2$-0.38 {I3}; weighted average of -0.37 {I4} (1977Gi13), -0.39 {I8} (1976Es02), -0.42 {I8} (1976Es01), -0.38 {I11} (1977Ma41). Others: -0.40 {I+13-20} (1971Ha47), -0.15 {I7} (1970St17) 
MOMM1$+0.71 {I3}; weighted average of +0.71 {I5} (conventional kinematics in 2011Ch33), +0.73 {I4} (inverse kinematics in 2011Ch33), 0.60 {I12} (1970St17), 0.72 {I22} via IMPAC (1974Hu01), 0.74 {I22} (1978BrZX) and 0.64 {I16} (1980Br01) from |g|g(|q,H,t) 
$|b{-2}=0.173 {I11} (1968Ma34), 0.20 {I1} (1968St18) and 0.19 (1967BaZV) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$694.87|g E2+M1 to 2+; 1312.41|g E2 to 0+; L(p,p')=2; 
T$from B(E2)(|_)=0.0021 {I3} in Coulomb excitation (1969Mi07). Other: 1.5 ps {I+22-5} from DSAM in {+112}Cd(n,n'|g) (2007Ga22) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$798.04|g E2 to 2+; L(p,p')=4; band assignment 
T$from B(E2)|^=0.36 {I4}, weighted average of 0.34 {I5} (1978Jo07), 0.356 {I42} (1965Mc05), and 0.41 {I8} (1962Ec03); Others: 0.7 ps {I+7-2} from DSAM in {+112}Cd(n,n'|g) (2007Ga22) 
$B(E4)|^=0.09 {I1} W.u. (1992Pi08) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$815.79|g E2 to 2+; 1433.27 E0 to 0+; L(d,p)=0 
T$from Rf-ce(t) in {+111}Cd(d,p|g) (1979Lu10,1980Ju05). Others: 2.9 ps {I9} using B(E2)(W.u.)(120.68|g)=66 {I20} and 1.4 ps {I3} using B(E2)(W.u.)(815.79|g)=0.017 {I4} 
$Ice(K)(1433.27):Ice(K)(815.79):Ice(K)(208.93):Ice(K)(120.68)= 0.79 {I8}: 0.10 {I3}: 2.5 {I4}: 11 {I2} (1980Ju05) and Ice(K)(1433.27):Ice(K)(815.79)=19.0 {I17}, Ice(K)(1433.27):Ice(K)(120.68)= 0.051 {I7}, Ice(K)(208.93):Ice(K)(815.79)=45 {I5} and Ice(K)(208.93):Ice(K)(120.68)=0.13 {I2} in 1997Dr03 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1468.836|g E2 to 0+; L(p,p')=2; band member 
T$from B(E2)|^=0.0055 {I10} in Coulomb excitation (1969Mi07); Other: 1.4 ps {I+30-6} {+112}Cd(n,n'|g) (2007Ga22) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$1387.68|g E1 to 2+; L(p,p')=3 
$B(E3)=0.0207 (1985De57) in {+112}Cd(p,p') and 0.114 {I9} (1985Fe05), 0.158 {I27} (1978Jo07), 0.106 {I22} (1965Mc05) and 0.37 {I18} (1963Ha20) in Coulomb excitation 
$|b{-3}=0.164 {I11} (1968Ma34), 0.15 {I2} (1968St18), 0.049 {I5} (1985De57) and 0.147 (1984Pi01) from {+112}Cd(p,p'), 0.146 (1965Mc05) in Coulomb excitation, 0.15 (1967BaZV) from {+112}Cd(|a,|a') 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$1464.04|g E2 to 2+, 666.15|g M1+E2 to 4+; L(p,p')=4; band member 
$B(E4)|^=8.2 {I10} W.u. (1992Pi08) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$957.72|g E1 to 4+ and 367.9|g E2 to 3-; L(p,p')=5; band member 
$|b{-5}=0.048 or 0.044 if two-step contributions through 2+ and 3- states are included (1984Pi01) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J$987.89|g M1+E2 to 4+, 1785.48|g to 2+; 6991.18|g from (1+) in {+111}Cd(n,|g) E=th:primary (1997Dr03) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$946.92|g E1 to 2+; L(p,p')=3 
$B(E3)=0.0019 (1985De57) 
$|b{-3}=0.0148 {I17} (1985De57), and 0.035 or 0.038 if two-step contributions via the 2+ and 3- states are included (1984Pi01) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$2506.70|g E1 to 0+, 1037.8|g E1 to 2+ and L(p,p')=(1); 
T$from {+112}Cd(|g,pol |g'). Other: 44 fs {I8} in {+112}Cd(n,n'|g) (2007Ga22) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
J$1154.75|g E1 to 4+ and 565.10|g E2 to 3-; band member 
CONF$possible |n(s{-1/2},h{-11/2}). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: PS
level_comment:
J$1356.522|g E1 to 2+, 663.59|g M1+E2 to 3-; L(t,p)=(2,6); direct population in {+111}Cd(n,|g) E=th:primary (J|p=(1)+) makes J|p=3- unlikely 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$2056.48|g M1+E2 to 2+ and L(pol d,t)=2 
CONF$possible |n(s{-1/2},d{-3/2}). The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
J$2448.76|g E1 to 2+; {+112}Cd(pol d,d') (1994He22) and {+112}Cd(n,n'|g) (2001Ga44) support 3- assignment 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: PS
level_comment:
J$3300.94|g to 0+; population in {+112}Cd(|g,pol |g') 
T$Other: 40.6 fs {I22} in {+112}Cd(|g,pol |g') 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: FS
level_comment:
J$3375.40|g to 0+, 2758.02 to 2+; population in {+112}Cd(|g,pol |g') 
T$Other: 87 fs {I13} in {+112}Cd(|g,pol |g') 


level_energy_unit: KEV
level_spin_parity: (1)+
level_uncertain: S
level_comment:
J$s-wave capture on J|p=1/2+ in {+111}Cd suggests 0+,1+; 9393.63|g to the g.s. and other decay branches to 0+ states support 1+ assignments. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$from RF-ce(t) (1979Lu10,1980Ju05) 
$Ice(K)(1432):Ice(K)(815|g):Ice(K)(209):Ice(K)(120)=0.79 8:0.10 {I3}:2.5 {I4}:11 {I2}. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$Possible doublet structure with J|p=1+ for the second state (1973Ar02) 
T$from |G{-|g}=0.086 eV {I15} (1970Mo26). Others: 0.6 eV {I+2-1} (1966Mi13) 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: FS
level_comment:
J$from the adopted levels. J|p=3+ in 2001Ga44 seems to be a missprint since 2869.99|g is claimed to be a stretched E2 transition to 2+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
|b{-3}=0.0148 {I17} (1985De57); 0.035 or 0.038 if two-step contributions through 2+ and 3- states are included (1984Pi01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)|^(617.52|g)=0.486 {I5} (1985Si01), 0.524 {I50} (1977Gi13), 0.484 {I4} (1976Es02), 0.478 {I33} (1970St17), 0.524 {I21} (1969Mi07), 0.514 {I60} (1965Mc05) and 0.546 {I39} (1962Ec03) 
MOME2$-0.38 {I3}, weighted average of -0.37 {I4} (1977Gi13), -0.39 {I8} (1976Es02), -0.42 {I8} (1976Es01), -0.38 {I11} (1977Ma41). Others: -0.40 {I+13-20} (1971Ha47), -0.15 {I7} (1970St17) 
MOMM1$+0.71 {I3}, weighted average of +0.71 {I5} (conventional kinematics in 2011Ch23), +0.73 {I4} (inverse kinematics in 2011Ch23), 0.60 {I12} (1970St17), 0.72 {I22} via IMPAC (1974Hu01), 0.74 {I22} (1978BrZX) and 0.64 {I16} (1980Br01) from |g-|g(|q,H,t) coinc. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$B(E3)|^=0.114 {I9} (1985Fe05), 0.158 {I27} (1978Jo07), 0.106 {I22} (1965Mc05), 0.37 {I18} (1963Ha20) 
B3$0.146 (1965Mc05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_uncertain: ?
level_comment:
S$for |ns{-1/2} transfer 
Not observed in any other data set; In particular, it was not observed in {+112}Cd(n,n'|g) (2001Ga44) and hence suggested to be due to {+114}Cd presence in the target composition 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=(1+,2+) and J|p=5-,6- with C{+2}S=0.004 and 0.013 for |nh{-11/2} and |nd{-3/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=1+,2+ and J|p=5-,6- with C{+2}S=0.038 and 0.562 for |nd{-3/2} and |nh{-11/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=2+,3+ and J|p=3+,4+ with C{+2}S=0.019 and 0.060 for |nd{-5/2} and |ng{-7/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=1+,2+ and J|p=3+,4+ with C{+2}S=0.016 and 0.043 for |nd{-3/2} and |ng{-7/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=2+,3+ and J|p=5-,6- with C{+2}S=0.004 and 0.015 for |nd{-5/2} and |nh{-11/2}transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=1+,2+ and J|p=5-,6- with C{+2}S=0.004 and 0.048 for |nd{-3/2} and |nh{-11/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=1+,2+ and J|p=3+,4+ with C{+2}S=0.032 and 0.079 for |nd{-3/2} and |ng{-7/2} transfers, respectively 


level_energy_unit: KEV
level_spin_parity: (0+,3+)
level_comment:
S$for |ng{-7/2} transfer; Otherwise, 0.002 for |ns{-1/2} and 0.009 for |nd{-5/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=1+,2+ and J|p=5-,6- with C{+2}S=0.014 and 0.090 for |nd{-3/2} and |nh{-11/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=0+ and J|p=1+,2+ with C{+2}S=0.005 and 0.007 for |ns{-1/2} and |nd{-3/2} transfers, respectively 


level_energy_unit: KEV
level_comment:
Doublet consisting of J|p=0+ and J|p=1+,2+ with C{+2}S=0.004 and 0.020 for |ns{-1/2} and |nd{-3/2} transfers, respectively 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+112}Cd)=+674.6 MHz {I22} {I15} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -182.8 MHz {I4} {I7} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+112}Cd)=-0.159 fm{+2} {I1} {I4} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$s{-1/2} neutron transfer 
$S{-jl}(DWBA)=0.0736 {I12} 
$d|s/d|W(at 30|')=0.037 mb/sr {I1} 
E$a doublet is known at this energy, the other level is 4+, which is not evident in the present work from the shapes of angular distributions and analyzing powers. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$f{-7/2} neutron transfer. Octupole phonon level. 
$S{-jl}(DWBA)=0.0119 {I18}. 
$d|s/d|W(at 30|')=0.0046 mb/sr {I2} 
$For high-momentum bite values are: E(level)=2005.20 {I12}, d|s/d|W(at 30|')=0.0048 mb/sr {I3}, S{-jl}(ADWA)=0.01360 {I2}, S{-jl}(DWBA)=0.0095 {I16} 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$g{-7/2} neutron transfer 
$S{-jl}(DWBA)=0.0083 {I6} 
$d|s/d|W(at 30|')=0.0011 mb/sr {I2} 
$For high-momentum bite values are: E(level)=2064.7 {I5}, d|s/d|W(at 30|')=0.0010 mb/sr {I1}, S{-jl}(ADWA)=0.0124 {I8}, S{-jl}(DWBA)=0.0097 {I6} 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$g{-7/2} neutron transfer 
$S{-jl}(DWBA)=0.085 {I13} 
$d|s/d|W(at 30|')=0.0116 mb/sr {I5} 
$For high-momentum bite values are: E(level)=2081.65 {I14}, d|s/d|W(at 30|')=0.0122 mb/sr {I5}, S{-jl}(ADWA)=0.1440 {I3}, S{-jl}(DWBA)=0.094 {I18} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$S{-jl}(DWBA)=0.0694 {I9} 
$d|s/d|W(at 30|')=0.0171 mb/sr {I6} 
$For high-momentum bite values are: E(level)=2121.56 {I10}, d|s/d|W(at 30|')=0.0178 mb/sr {I7}, S{-jl}(ADWA)=0.0986 {I13}, S{-jl}(DWBA)=0.0697 {I10} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$S{-jl}(DWBA)=0.0446 {I6} 
$d|s/d|W(at 30|')=0.0108 mb/sr {I4} 
$For high-momentum bite values are: E(level)=2156.19 {I11}, d|s/d|W(at 30|')=0.0105 mb/sr {I4}, S{-jl}(ADWA)=0.0654 {I9}, S{-jl}(DWBA)=0.0458 {I7} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$S{-jl}(DWBA)=0.0219 {I3} 
$d|s/d|W(at 30|')=0.0056 mb/sr {I3} 
$For high-momentum bite values are: E(level)=2231.04 {I15}, d|s/d|W(at 30|')=0.0056 mb/sr {I6}, S{-jl}(ADWA)=0.0230 {I6}, S{-jl}(DWBA)=0.0209 {I5} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$s{-1/2} neutron transfer 
$S{-jl}(DWBA)=0.132 {I18} 
$d|s/d|W(at 30|')=0.069 mb/sr {I3} 
$For high-momentum bite values are: E(level)=2300.73 {I10}, d|s/d|W(at 30|')=0.068 mb/sr {I3}, S{-jl}(ADWA)=0.166 {I2}, S{-jl}(DWBA)=0.139 {I2} 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
$h{-11/2} neutron. Assigned as 5- member of |n3s{-1/2}~#|n1h{-11/2} configuration. It is not a candidate for quadrupole-octupole coupled quintplet 
$S{-jl}(DWBA)=1.59 {I19} 
$d|s/d|W(at 30|')=0.200 mb/sr {I7} 
$For high-momentum bite values are: E(level)=2373.30 {I10}, d|s/d|W(at 30|')=0.196 mb/sr {I7}, S{-jl}(ADWA)=2.63 {I4}, S{-jl}(DWBA)=1.70 {I2} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$f{-7/2} neutron transfer. 
E$this level was previously (1997Dr03: Nucl. Phys. A 614, 137; and 1999Ga15: Phys. Rev. C 59, 2455) assigned as a candidate for quadrupole-octupole coupled quintplet 
$S{-jl}(DWBA)=0.0166 {I3} 
$d|s/d|W(at 30|')=0.0058 mb/sr {I4} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$S{-jl}(DWBA)=0.201 {I3} 
$d|s/d|W(at 30|')=0.051 mb/sr {I2} 
E$a doublet is known at this energy, the other being 1-, which has not been seen in the present work. Due to required |np{-1/2} or |np{-3/2} transfer strengths for a 1- level, this level is expected to be only weakly populated in this reaction. 


level_energy_unit: KEV
level_spin_parity: 0+
level_uncertain: ?
level_comment:
E$weakly populated level with s{-1/2} neutron transfer. As this level was not seen in (n,n'|g) work (2001Ga44), its existence is considered questionable by 2018Ja16, could be due to target impurity, although none could be assigned 
$S{-jl}(DWBA)=0.00223 {I12} 
$d|s/d|W(at 30|')=0.0018 mb/sr {I6} 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
$f{-7/2} neutron transfer. Possible candidate for quadrupole-octupole coupled quintplet 
$S{-jl}(DWBA)=0.0106 {I19}. S{-jl}(ADWA)=0.0126 {I2} in 2014Ja19 
$d|s/d|W(at 30|')=0.0045 mb/sr {I2} 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_uncertain: ?
level_comment:
$g{-7/2} neutron transfer 
E$weakly populated level with J|p=3+,4+ in this work was not seen in (n,n'|g) work (2001Ga44), thus its existence is considered questionable by 2018Ja16, could be due to target impurity, although none could be assigned 
$S{-jl}(DWBA)=0.058 {I15} 
$d|s/d|W(at 30|')=0.0045 mb/sr {I3} 
J$2+,4+ listed in A{-y}(|q) plot on p121 in 2014JaZZ seems a misprint 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
$h{-11/2} neutron transfer with largest spectroscopic strength in this work. Assigned as the 6- member of |n3s{-1/2}~#|n1h{-11/2} configuration, and not a candidate for quadrupole-octupole quintplet 
$S{-jl}(DWBA)=3.47 {I4} 
$d|s/d|W(at 30|')=0.47 mb/sr {I2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$s{-1/2} neutron transfer 
$S{-jl}(DWBA)=0.0343 {I6} 
$d|s/d|W(at 30|')=0.0178 mb/sr {I8} 
E$a 2+ level at 2853 seen in (n,n'|g) (2001Ga44) may be weakly populated in the present work. The 0+ level proposed here and also seen in (pol d,t) (1990Bl19) was not seen in (n,n'|g) (2001Ga44) 


level_energy_unit: KEV
level_spin_parity: 3+&3-
level_comment:
E$doublet 
$g{-7/2} and f{-5/2} neutron transfers 
$S{-jl}(DWBA)=0.277 {I4} for L=4,g{-7/2}; 0.042 {I3} for L=3,f{-5/2} 
$d|s/d|W(at 30|')=0.099 mb/sr {I4} 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
$f{-7/2} neutron transfer 
$S{-jl}(DWBA)=0.0329 {I10} 
$d|s/d|W(at 30|')=0.014 mb/sr {I2} 
E$no evidence was found for a 2924, 0+ level reported in (pol d,t) (1990Bl19) 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_uncertain: ?
level_comment:
$f{-7/2} neutron transfer 
$S{-jl}(DWBA)=0.0692 {I9} 
$d|s/d|W(at 30|')=0.029 mb/sr {I1} 
E$levels at 2944.9, 2+ and 2947.8, 3+ in (n,n'|g) (2001Ga44); and a doublet at 2945 with (2+,3+) and (3+,4+) in (pol d,t) (1990Bl19) were not seen in the present work. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$s{-1/2} neutron transfer 
$S{-jl}(DWBA)=0.0655 {I13} 
$d|s/d|W(at 30|')=0.038 mb/sr {I2} 
E$no evidence was found in the present work for levels at 3066, (2,3)- and 3069, 4+, as given in {+112}Cd Adopted Levels in the ENSDF database (August 2014 update) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
$S{-jl}(DWBA)=0.053 {I16} 
$d|s/d|W(at 30|')=0.018 mb/sr {I1} 
E$doublet at 3069 was tentatively assigned as (1+,2+) and (3+,4+) in (pol d,t) (1990Bl19). No evidence was found in the present work for J|p=3+,4+ component. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$f{-7/2} neutron transfer 
$S{-jl}(DWBA)=0.0599 {I8} 
$d|s/d|W(at 30|')=0.030 mb/sr {I1} 
E$no evidence was found for a 5- component at 3131 keV or for a 1- state at 3133, as given in {+112}Cd Adopted Levels in the ENSDF database (August 2014 update) 


level_energy_unit: KEV
level_spin_parity: 2-,3-&2+,3+
level_comment:
E$doublet 
$f{-5/2} neutron transfer, and d{-5/2} transfer (also possible d{-3/2}) 
$S{-jl}(DWBA)=0.022{I2} for L=3,f{-5/2}; 0.006 {I2} for L=2,d{-5/2} 
$d|s/d|W(at 30|')=0.0135 mb/sr {I10} 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$g{-7/2} neutron transfer, and d{-5/2} transfer (also d{-3/2} possible) 
$S{-jl}(DWBA)=0.12 {I2} for L=4,g{-7/2}; 0.003 {I1} for L=2,d{-5/2} 
$d|s/d|W(at 30|')=0.022 mb/sr {I1} 


level_energy_unit: KEV
level_spin_parity: 2+,3+,4+
level_comment:
$g{-7/2} neutron transfer, and d{-5/2} transfer (also d{-3/2} possible) 
$S{-jl} for L=4,g{-7/2}; 0.0013 {I2} for L=2,d{-5/2} 
$S{-jl}(DWBA)=0.118 {I5} for L=4,g{-7/2}; 0.0022 {I3} for L=2,d{-5/2} 
$d|s/d|W(at 30|')=0.0195 mb/sr {I8} 


level_energy_unit: KEV
level_spin_parity: 2+,3+,4+
level_comment:
$Dominant g{-7/2} neutron transfer with possible d{-5/2} (and d{-3/2}) transfer 
$S{-jl} for L=4,g{-7/2}; 0.0037 {I3} for L=2,d{-5/2} 
$S{-jl}(DWBA)=0.113 {I6} for L=4,g{-7/2}; 0.0056 {I5} for L=2,d{-5/2} 
$d|s/d|W(at 30|')=0.020 mb/sr {I1} 


level_energy_unit: KEV
level_spin_parity: 2+,3+,4+
level_comment:
$g{-7/2} neutron transfer, and d{-5/2} transfer (also d{-3/2} possible) 
$S{-jl} for L=4,g{-7/2}; 0.0057 {I3} for L=2,d{-5/2} 
$S{-jl}(DWBA)=0.134 {I7} for L=4,g{-7/2}; 0.0090 {I6} for L=2,d{-5/2} 
$d|s/d|W(at 30|')=0.025 mb/sr {I1} 


level_energy_unit: KEV
level_spin_parity: 5-,6-&2+,3+
level_comment:
E$doublet 
$h{-11/2} neutron transfer, and d{-5/2} transfer (also d{-3/2} possible) 
$S{-jl} for L=5,h{-11/2}; 0.0040 {I2} for L=2,d{-5/2} 
$S{-jl}(DWBA)=0.076 {I3} for L=5,h{-11/2}; 0.00560 {I5} for L=2,d{-5/2} 
$d|s/d|W(at 30|')=0.0123 mb/sr {I7} 


level_energy_unit: KEV
level_spin_parity: 5-,6-&2-,3-
level_comment:
E$doublet 
$h{-11/2} and f{-5/2} neutron transfers 
$S{-jl} for L=5,h{-11/2}; 0.0126 {I5} for L=3,f{-5/2} 
$S{-jl}(DWBA)=0.126 {I8} for L=5,h{-11/2}; 0.0134 {I7} for L=3,f{-5/2} 
$d|s/d|W(at 30|')=0.031 mb/sr {I1} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: Y
level_comment:
MOMM1$optical pumping, NMR. 
J$NMR and optical spectroscopy (1976Fu06), L(d,p)=0. 
T$From 2007Be61 Measured in CdWO{-4} crystal at Gran Sasso National Lab of INFN. Measured half-life of {+113}Cd using the low-background CdWO{-4} crystal scintillator of mass 434g. Others: 7.7|*10{+15} y {I3} (1996Da11) using scintillation crystals of cdw04. 9.3|*10{+15} y {I19} (1970Gr20) from activity measurements on enriched and natural cadmium samples. Others: 1962Wa15, 1994Al49 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$; |m=-1.0877842 {I17} (1989Ra17) NMR. 
MOME2$optical double res, recalculated (1989Ra17). 
J$optical double res (1976Fu06), 264|g is E5. 
T$unweighted av of 13.6 y {i2} (1965Fl02) and 14.6 y {i5} (1972Wa11), |b(t) for about one half-life. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$L(d,p)(316)=2, L(d,p)(458)=4, and M1+E2 |g from 459 to 316 gives J|p(316)=5/2+ and J|p(458)=7/2+ 
T$weighted av of 10.7 ns {i4} (1980Oh01), 11.0 ns {i6} (1972RaZM). Other: 4.9 ns {i7} from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
E$1991NeZX suggested a 1423-keV level with J|p=11/2- based on syst, not confirmed by 1997Wa20 in (|a,n|g)but given by 2005Bu20 
J$L(pol d,p)=5 


level_energy_unit: KEV
level_comment:
J$authors assign J|p=7/2+ but it is not compatible with given L. A level at 1195.4 has been adopted with J|p=5/2+,7/2+,9/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M
level_comment:
T$ measured by 2011Ko01 from decay curve of |b radiation detected in a liquid scintillation detector. 2011Ko01 give weighted average value of 13.89 y {I16} using their measured value and previous values of 13.6 y {i2} (1965Fl02) and 14.6 y {i5} (1972Wa11). 2011Ko01 define 1 year as 365.242 days. Compiler's note: 2011Ko01 followed the activity for 11 months, 1965Fl02 for 11 years and 1972Wa11 for 18 years 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M
level_comment:
MOME2$ uncorrelated uncertainty of 0.003, and correlated uncertainty of 0.025 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: Y
level_comment:
J$spin from 2013Yo02: Phys Rev Lett 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+113}Cd)=+555.2 MHz {I23} {I8} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and -134.3 MHz {I8} {I9} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+113}Cd)=-0.114 fm{+2} {I1} {I10} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$statistical uncertainty of 0.004 and systematic uncertainty of 0.025 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
E$g-factor=+0.321 {I21} (2011Ch23) 
T$an upper limit is given for the double |b decay: >92.|*10{+15} y (1995Tr07), >6.0*10{+17} y (2003Da24), >1.3*10{+18} y (2008Be22) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(d,p)=4, E2 |g to 2+ 
T$from |g|g(|q) in {+114}In |b{+-} decay (1970Mu11); other: 5.2 ps {I+8-18} from (|g,|g') (1962Ak01) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$J=3 from |g(|q) in (n,n'|g). L(d,{+3}He)=1 for E=2390 {i15} yields |p=-. 1976De42 in (n,n'|g) suggest |p=+, but |d discrepant with 1987Ar24 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
T$From 2007Ba73 
J$L(e,e')=4. |g(|q) data in (e,e') analyzed as L=2+4 doublet, possibly distorted by 2387 J=(3) level 


level_energy_unit: KEV
level_spin_parity: 1-,2-,3-
level_lifetime_unit: FS
level_comment:
T$From 2007Ba73 
J$E1 |g to 2+. Tentative |g to 0+ would rule out 2-,3-. Doubly placed E1 to 3+ would rule out 1-. Doubly placed |g to 4- would rule out 1- 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$deduced from form factor using anharmonic vibrational model. Others: B(E2)=0.472 {I48} (1973Ho05), 0.553 {I18} (1974Ye01), 0.575 {I48} (1976Li19) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2). Other B(E2) values: 0.584 {I41}, (1958St32), 0.571 {I67} (1965Mc05), 0.567 {I18} (1967Gl02), 0.480 {I50} (1967Si03), 0.503 {I13} (1967St03), 0.509 {I9} (1968Si05), 0.576 {I23} (1969Mi07), 0.560 {I17} (1969Sa27), 0.506 {I27} (1970Kl12), 0.547 {I13} (1970Wa04), 0.553 {I14} (1970Pr07), 0.513 {I5} (1972Be66), 0.528 {I4} (1976Es02) 
Other Q values: -0.53 {I17} (1970An09), -0.28 {I9} (1971Be36), -0.35 {I7} (1972La17), 0.574 {I18} (1985Si01). All Q values are for constructive multiple Coulomb interference 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
E$from 1994Ge07, energy of 3110 in 2005Ko32 is 3109+3110 unresolved doublet 
J$1(+) for composite 3109+3110 
T$0.0172 eV {I13} (2005Ko32) for doublet 
$|G=0.0067 eV {I40} (1994Ge07), with R(exp)=0.54 {I36} (1994Ge07) 
S$for 3109+3110 doublet (2005Ko32) 
$B(M1)=0.148 {I12}, B(E1)=1.64|*10{+-5} {I13}: for 3109+3110 doublet (2005Ko32) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W(at 8|')=0.015 mb/sr {I1} 
$At 15|', only an upper limit of cross section could be determined due to low yield, yet L-transfer is larger than that expected for L=0. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s(8|')/|s(15')|<1 in authors' Fig. 3 suggests L>0 
$New level in the present work. It is unlikely that this level corresponds to a previously known level at 2701.066, 3+ in {+114}Cd Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$firm 0+ assignment in the present work. In {+114}Cd Adopted Levels in the ENSDF database, J|p=0+,1+ was assigned to a 2828 level 
$d|s/d|W(at 8|')=0.015 mb/sr {I1} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$firm 0+ assignment in the present work. In {+114}Cd Adopted Levels in the ENSDF database, for a level at 3254, J|p=(0+) and/or (5-) implied from L(p,t)=(5+0) 
$d|s/d|W(at 8|')=0.026 mb/sr {I2} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: H
level_comment:
MOMM1 Optical double resonance 
T weighted av: 53.38 h {I4} (1971Ba28), 53.53 h {I4} (1968RoZZ), 53.50 h {I10} (1961Wy01). Other: 1964Be44 
J$L=0 (d,p) 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
%IT Decay unobserved. %IT<0.003|*B(E5)(W.u.) 
MOMM1 Optical double resonance 
T weighted av: 44.8 d {I3} (1971Ba28), 44.1 d {I6} (1969MoZS), 44.2 d {I5} (1959Wa13) 
J L=5 (d,p); syst of h11/2-isomerism in {+111}Cd (at 396), {+113}Cd (at 264), and {+117}Cd (at 136) 
Measured moments of odd-mass {+105}Cd-{+115}Cd 11/2- isomers agree well with theory (1969La06) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$may correspond to 695-keV L=(3) (d,p) excitation. Low-lying 5/2- states occur in {+113}Cd at 855 keV and in {+117}Cd at 606 keV 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$log| {Ift}=7.0 from 1/2- {+115}Ag, |g to (7/2)-. Low-lying 3/2- states occur in {+113}Cd at 1195 keV and in {+117}Cd at 1073 keV 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
E$deduced from cascade and crossover |g rays originating from higher lying |p=- states. 719.9=472.7+247=326.1+236.1+181.0 
Yield of 44.6-d isomer via 20 min {+115}Ag decay=5.7% {I7} from level scheme. Others: 10.7% (1970Hn01), 8.5% (1968Kj01), 8% (1955Hi66), 9% (1952Wa06) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J$ (11/2)- in {+115}Cd Adopted Levels in ENSDF database 
MOME2$ uncorrelated uncertainty of 0.005, and correlated uncertainty of 0.019 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: H
level_comment:
$Spin from 2013Yo02: Phys. Rev. Lett. 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+115}Cd)=+47.3 MHz {I11} {I6} for 5s5P {+3}P{-2} |) 5s6s {+3}S{-1} transition; and -110.4 MHz {I29} {I7} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+115}Cd)=+0.043 fm{+2} {I1} {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2)-
level_comment:
MOME2$statistical uncertainty of 0.004 and systematic uncertainty of 0.020 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$From 2002Ba52 the lower limits of the T{-1/2} for 2|b- decay is 4|*10{+19} y {I1}(2005Ra13). Other values: 1.7|*10{+20} y (1990Ba52), 2.6|*10{+20}y (1994Ku25), 2.7|*10{+20} y (1995Da09). Others: 1991Zd01, 1993Kl01, 2000Ar16, 1998Da23, 2003Da09, 2003Da24, 2005Ba01, 2005Ba33, 2005Da03,2006Wi12, 2006Sh31, 2006Ba35 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=2 
T$from Coul. ex., B(E2)(0-2)=0.560 {i20} (1987Ra01) 
MOME2$average of 1976Es02 and 1977Gi13 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|g(|q) in Coul. ex., |p=+ from L=2+4 (p,p') and (t,p) 
T$from Coul. ex., B(E2)=0.019 {i3} (1969Mi07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$|g(|q) in (n,n'|g), J=2 in (p,p') could be different level 
T$from 1989Ma33, measured |b|g|g with BaF{-2} and plastic detector. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$from text and tables vi and vii. Other: (2+) in figure 5. log| {Ift}=8.5 from (0-) is too low to be realistic for |DJ=3 |b transition 


level_energy_unit: KEV
level_comment:
J$2009Ba52 propose 2+,3,4+ based on |g's to 2+ and 4+, which disagrees with 1- assignment in Adopted Levels, but log {Ift}=8.1 from (0-) does not allow 3,4+. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J$4- in figure 5 and Table I of 2009Ba52; but this assignment is inconsistent with multipolarities assigned to 418 and 424 |g rays 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$from table iv of 2009Ba52 and discussion in text; 2+ in figure 5, not listed in Table I of 2009Ba52. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$J=2- in Table I of 2009Ba52. 
$Compilers' note: there seems problem with the inventory of |g rays from this level as listed in table I of 2009Ba52. Strong transitions as seen in the decay of the ground state are not listed here. It is not clear how the |b feeding of 2.2 has been obtained. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
B(E2): deduced from form factor by use of anharmonic-vibrational model 
E$rounded-off value from adopted levels 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.560 {I20} (1987Ra01). Values included in 1987Ra01 are B(E2): 0.65 {I4} (1970St17), 0.581 {I23} (1969Mi07), 0.621 {I8} (1967St03), 0.58 {I7} (1965Mc05) 0.532 {I4} (1976Es02), 0.608 {I30} (1985Si01) 
MOME2$others: -0.42 {I8} (1976Es02), -0.88 {I25} (1970St17) 0.81 {I14} (1967St03) 
g-factor: 0.7 {I4} (1969He11), 0.30 {I7} (1980Br01), 0.4 {I3} (1974Hu01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+116}Cd)=-526.5 MHz {I22} {I15} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition; and +151.5 MHz {I7} {I7} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition. 
$Measured |d|4r{+2}|5({+114}Cd,{+116}Cd)=+0.134 fm{+2} {I1} {I8} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$measured by 2017Ar01 for 2|n|b|b decay mode, considering the double |b decay process to be single step (through intermediate 1+ state in {+116}In) dominated decay. Statistical uncertainty of 0.04|*10{+19} y and systematic uncertainty of 0.18|*10{+19} y given by 2017Ar01 have been combined in quadrature. For a two step dominated process (through the higher excited states in {+116}In), T{-1/2}=2.96|*10{+19} y {I4}(stat) {I20}(syst) (2017Ar01). Values are compared by authors to previous measurements: 2.62|*10{+19} y {I14} (F.A. Danevich et al., J. Phys. Conf. Series 718, 062009 (2016) using Aurora detector); 2.9|*10{+19} y {I+4-3} (2003Da24: Phys. Rev. C 81, 035501 using Solotvina detector); 2.9|*10{+19} y {I3}(stat) {I2}(syst) using NEMO-2 detector; this value is also quoted in evaluation by 2010Ba07: Phys. Rev. C 81, 035501); and 2.6|*10{+19} y {I+9-5} (1995Ej01: J. Phys. Soc. Japan 64, 339 using ELEGANT-V detector). 
T$measured lower limit for 0|n|b|b decay mode is >1.0|*10{+23} y at 90% confidence level (2017Ar01), and the corresponding upper limit for mass of Majorana neutrino is <1.4-2.5 eV. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$measured by 2018Ba44 for 2|n|b|b decay mode, with statistical uncertainty of 0.011|*10{+19} y and systematic uncertainty of {I+0.113-0.123}|*10{+19} y given by the authors. Value is compared by authors to previous measurements: 2.90|*10{+19} y {I6}(stat) {I+40-30}(syst) (2003Da24: Phys. Rev. C 81, 035501 using Solotvina detector; values also quoted from papers in 1995 and 2000); 2.74|*10{+19} y {I4}(stat) {I18}(syst) using NEMO-3 detector (2017Ar01: Phys. Rev. D 95, 012007; value also quoted from NEMO-2 result in a 1995 paper); and 2.6|*10{+19} y {I+9-5} (1995Ej01: J. Phys. Soc. Japan 64, 339 using ELEGANT-V detector). See Table I of 2018Ba44 for details 
T$measured lower limit for 0|n|b|b decay mode is |>2.2|*10{+23} y at 90% confidence level (2018Ba44), and the corresponding upper limit for mass of Majorana neutrino as |<1.0-1.7 eV. Value compared with previous measurements using Solotvina detector, NEMO-2, NEMO-3, and ELEGANT-V detector systems. See Fig. 14 in 2018Ba44 for details. 
$Measured half-life limits for exotic modes of double-|b decay to {+116}Sn g.s., where |h=majoron (massless Goldstone boson) emission, and LV=Lorentz-violating, n=spectral index defined by the phase space of the emitted particles 
$Measured T{-1/2}|>1.2|*10{+21} y for 2|n|b|b(LV),n=4 decay. 
$Measured T{-1/2}|>8.2|*10{+21} y for 0|n|h{+0}|b|b,n=1 decay. 
$Measured T{-1/2}|>4.1|*10{+21} y for 0|n|h{+0}|b|b,n=2 decay. 
$Measured T{-1/2}|>2.6|*10{+21} y for 0|n|h{+0}|b|b,n=3 decay. 
$Measured T{-1/2}|>2.6|*10{+21} y for 0|n|h{+0}|h{+0}|b|b,n=3 decay. 
$Measured T{-1/2}|>8.9|*10{+20} y for 0|n|h{+0}|h{+0}|b|b,n=7 decay. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$From 2016Eb03 with a 90 % C.L. The authors stated that switching to a prior uniform effective neutrino Majorana mass increased the limits on the T{-1/2}. The Adopted levels of {+116}Cd shows T{-1/2} as stable. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: H
level_comment:
T$weighted average from 2.4 h {i1} (1975Ta06), 2.42 h {i7} (1972Pa13), 2.5 h {i2} (1972Gr24), 2.60 h {i8} (1969Mo21), 2.52 h {i12} (1967Sc37), 2.5 h {i1} (1967Ba18), 2.5 h {i2} (1966De16). Others: 1939Go02, 1939Li04, 1940La07, 1940Ni03, 1952At25, 1953Co04 
J$L=0 (d,p) 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
J$L=5 (d,p), h11/2 configuration favored by shell model for the isomeric state. 
$%IT negligible from B(E5)(W.u.)|?4|*10{+5} 
T$weighted average from 3.4 h {i1} (1975Ta06), 3.31 h {i7} (1972Pa13), 3.4 h {i2} (1972Gr24), 3.50 h {i8} (1969Mo21), 3.10 h {i12} (1967Sc37), 3.3 h {i3} (1966De16) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: NS
level_comment:
J$log| {Ift}<5.9 to 2382.6 and 3032.4 levels, |g decay from these levels to 293.5 and decay of 293.5 via an E2 to (11/2)- uniquely establishes J|p(293.5)=(7/2)- and J|p(2382.6, 3032.4)=(3/2-) 
T$from 1976Fo10 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$M1,E2 |g to 1/2+, M1 |g from (5/2+) 
E$E=434 {i10}, L=(2) reported in {+116}Cd(d,p). May include both the 426.2 and 442.6 levels. 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J,T$ from Adopted Levels for {+117}Cd in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
MOME2$ uncorrelated uncertainty of 0.006, and correlated uncertainty of 0.013 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: H
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+117}Cd)=+192.9 MHz {I11} {I21} for 5s5P {+3}P{-2} |) 5s6s {+3}S{-1} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+117}Cd)=+0.171 fm{+2} {I2} {I20} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2)-
level_comment:
MOME2$statistical uncertainty of 0.002 and systematic uncertainty of 0.013 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J 4+,5+,6+ from |g|g(|q) in {+118}Ag |b{+-} decay; systematics of the yrast states in Cd isotopes suggests 6+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+118}Cd)=+275.5 MHz {I20} {I14} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+118}Cd)=+0.243 fm{+2} {I3} {I22} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MIN
level_comment:
J$from recent hyperfine structure measurement, prl 110, 192501 (2013) Earlier assignment of 3/2+ was based on log| {Ift} arguments and syst. 
T$from |g(t). Value from 1976Sc30. Others: 2.6 min (1974Mc09), 3.3 min {i10} (1974Gr29) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$M1 |g to 3/2+. If J|p(g.s.)=3/2+, 1/2+ is favored from syst of low-lying state for odd Cd isotopes, but |g from (7/2+) level allows only 3/2+. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$I(|g+ce)(119.5|g)<0.02% from B(M4)(W.u.)<30, thus, %|b{+-}=100 
J$syst of lighter odd-mass Cd isotopes for the high-spin isomer 
T$from |g(t). Value from 1976Sc30. Other: 1.9 min (1974Mc09). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J,T$ from Adopted Levels for {+119}Cd in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$ (11/2-) in {+119}Cd Adopted Levels in ENSDF database 
MOME2$ uncorrelated uncertainty of 0.003, and correlated uncertainty of 0.005 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MIN
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+119}Cd)=+319.0 MHz {I10} {I32} for 5s5P {+3}P{-2} |) 5s6s {+3}S{-1} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+119}Cd)=+0.283 fm{+2} {I3} {I33} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_comment:
MOME2$statistical uncertainty of 0.003 and systematic uncertainty of 0.006 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+120}Cd)=+386.5 MHz {I10} {I21} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+120}Cd)=+0.342 fm{+2} {I3} {I37} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
J systematics of J|p in odd Cd isotopes suggests 1/2+ or 3/2+, but 3/2+ is more likely because log| {Ift}=5.7 to the 1315-keV, (5/2+) state in {+121}In 
T weighted average of 12.8 s {I4} (1965We09), 12.7 s {I5} (1974Sc05), 13.8 s {I2} (1974Gr29), 12.5 s {I15} (1982Fo04) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
Decay mode is not known; however, one can assume a conservative estimate of log| {Ift}|>5 for any |b branch to a level in {+121}In. For a branch of 1% to the 313 level for example, one gets T{-1/2}(parent)>0.1s, leading to B(M1)(W.u.)<4|*10{+-9} or B(E2)(W.u.)<7|*10{+-5}. These are both unreasonably small. Any larger |b branching would give even smaller Weisskopf estimates, as would 1% branches to higher lying levels. Any possible |b branching must thus be <<1%. 
J systematics of J|p in odd Cd isotopes 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$no |g to (1/2+), (3/2+); the upper limit of I|g to (3/2+) is estimated to be 1%, systematics of J|p in odd-Cd isotopes suggests 11/2- based on 1h{-11/2}, J=11/2 is consistent with log| {Ift}|<6.5 to 1182, 13/2+ state in {+121}In 
T from 1982Fo04 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g's to (11/2-) and (9/2-,11/2-,13/2-); log| {Ift}=6.1 from (7/2+) 
T from |b|g(t) in {+121}Ag |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E deduced from |g-cascade relations at 744.75-, 1510.45-, 1812.03-keV levels; E=70 {I170} was deduced from observed Q(|b{+-}) value (1982Fo10) 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
MOME2$ uncorrelated uncertainty of 0.007, and correlated uncertainty of 0.011 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
$Spin from 2013Yo02: Phys. Rev. Lett. 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+121}Cd)=+420.9 MHz {I9} {I31} for 5s5P {+3}P{-2} |) 5s6s {+3}S{-1} transition; and -1309.3 MHz {I40} {I50} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+121}Cd)=+0.375 fm{+2} {I4} {I49} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
MOME2$statistical uncertainty of 0.015 and systematic uncertainty of 0.012 from electric field gradient combined in quadrature by compiler 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_comment:
MOME2$statistical uncertainty of 0.006 and systematic uncertainty of 0.001 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from |b{+-}-multiscaler counting, |DT{-1/2}: statistical uncertainty only (1981Ru07). Others: 3.13 s {I12} (1974Gr29), 5.78 s {I9} (1973Sc19) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2|^ from Coulomb excitation (2005BeZS); other: BE2|^=0.58 {I27} deduced from |t=15 ps {I7} (1995Za01) 
J$ (1135|g)(569|g)(|q) and (1422|g)(569|g)(|q) clearly indicate 0-2-0 spin sequences, RUL assigns mult.(569|g)=E2 
T$from centroid-shift analysis of |b|g(t) coincidence (1995Za01); other: 14 ps {i5} from B(E2) in Coulomb excitation (2005BeZS) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T $ Centriod-shift analysis of |b|g(t) coincidence spectra using NE111A and BaF{-2} scintillators with time-to-amplitude converter. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+122}Cd)=+484.9 MHz {I11} {I27} for 5s5p {+3}P{-2} |) 5s6s {+3}S{-1} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+122}Cd)=+0.431 fm{+2} {I5} {I54} 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
J$spin=3/2 from collinear laser spectroscopy in 2013Yo02 and 2018Ha30; systematics of odd Cd isotopes indicates 1/2+ or 3/2+; parity also supported by possible allowed |b feeding (log {Ift}=5.5) to parity=(+) state at 1052 in {+123}In 
T$weighted average of 2.07 s {I3} (1983Re05), 2.19 s {I10} (1986Go10), 2.11 s {I6} (1986Ma42) and 2.12 s {I3} (1989Hu03). Other: 2.35 s {I5} (2014TeZY) is in disagreement. 
MOMM1,MOME2$from collinear laser spectroscopy in 2013Yo02. See also 2014StZZ and 2016St14 compilations 
$|d<r{+2}>=-0.028 mb {I3}(stat) {I2}(syst), or -0.042 mb {I13}(stat) {I3}(syst), for difference between the (11/2-) state and the g.s. (2016Yo01). 
$|d<r{+2}>=0.457 fm{+2} {I6}(uncorrelated) {I67}(correlated), with respect to {+114}Cd (2018Ha30) 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$from the direct mass measurement by 2013Ka08. Other: an energy of 316 keV proposed by 1989Hu10 in {+123}Ag |b{+-} decay from |g-cascade relations. See detailed comments in that dataset for the position of this isomer 
J$spin=11/2 from collinear laser spectroscopy in 2013Yo02; 11/2- from systematics of h{-11/2} states in odd-A Cd isotopes 
T$weighted average of 1.81 s {I3} (1989Hu03) and 1.88 s {I6} (1986Ma42), and 1.74 s {I4} (2014TeZY) 
MOMM1,MOME2$from collinear laser spectroscopy in 2013Yo02. See also the 2014StZZ and 2016St14 compilations. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_comment:
J$possible allowed |b feeding (log {Ift}=5.1) from (7/2+); 263.9|g to 3/2(+); possible 123.7|g to 11/2(-) 
T$from |g|g(t) (1989Hu10) in {+123}Ag |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$from the mass measurement by 2013Ka08. Other: 316 keV in 1989Hu10. See detailed comments above on the position of this isomer. 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
MOME2$statistical uncertainty of 0.007 and systematic uncertainty of 0.003 from electric field gradient combined in quadrature by compiler 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
MOME2$statistical uncertainty of 0.011 and systematic uncertainty of 0.005 from electric field gradient combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T weighted average of following values from |g multiscaling: 1.23 s {I2} (1984Hi03), 1.26 s {I6} (1986Go10) and 1.29 s {I3} (1986Ma42); others: 0.9 s {I2} (1974Fo23), 1.7 s {I6} (|b multiscaling) (1981Ru07), 1.2 s {I1} (|b multiscaling) (1983Re05) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$(3+) in Table IV and (4+) in Table I of 2014Ba18. In the text on p7, authors prefer 3+ from systematics but do not rule out 2+ and 4+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+124}Cd)=+574.9 MHz {I33} {I34} for 5s5P {+3}P{-2} |) 5s6s {+3}S{-1} transition; and -1748.2 MHz {I22} {I72} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+124}Cd)=+0.510 fm{+2} {I6} {I72} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
T From |g decay curve (1989Hu03) and 0.64 s {I3} from |g decay curve (1986Ma42). Other: 0.64 s {I3} (1986Ma42), 0.75 s {I4} (1986Ho24,1986Go10; not divide two components of the decays from g.s. and 50-keV level) 
J Systematics of 3/2+ in odd-cadmium isotopes 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x=186 {I4} (2012Au07) from mass measurement 
E$From systematics of the 11/2-, 3/2+ energy difference for Cd isotopes with N=67 to 75, X is expected to be |=350 keV. This value is consistent with statements made in 1987Sp09, whose Q(|b{+-})determinations were based on the assumption of a single parent source (data of 1986Ho24), now known to be a mixed gs+isomer source (data of 1989Hu03). 
T From |g decay curve (1989Hu03). Other: 0.66 s {I3} from |g decay curve (1986Ma42). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (33/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ Possible microsecond isomer. T{-1/2}=14 |ms {I2} for the 720 and 743 |g's (2003HeZT). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (33/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ Possible configuration=[|nh{-11/2}~#(|nh{-11/2}~#|nd{-3/2}){-7-}~# (|pg{9/2}|pp{-1/2}){-5-}]{-33/2-} 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
MOME2$ uncorrelated uncertainty of 0.004, and correlated uncertainty of 0.009 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-73347 keV {I24} (2017La16). Value is -73348.1 keV {I29} in 2012Wa38: AME-2012 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$deduced by 2017La16 from mass excesses of {+125}Cd g.s. and isomer. Literature value=186 keV {I4} (2012Wa38: AME-2012) based on mass measurements. 
$Measured mass excess=-73157.9 keV {I90} (2017La16). Value is -73162 keV {I4} in 2013Ka08 (Phys. Rev. C 87, 024307). 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
$Spin from 2013Yo02: Phys. Rev. Lett. 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+125}Cd)=-1757.3 MHz {I35} {I79} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+125}Cd)=+0.533 fm{+2} {I7} {I86} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
$Half-life from {+125}Cd Adopted Levels in the ENSDF database (Jan 2010 update) 
J$spin from 2013Yo02 (Phys. Rev. Lett. 110, 192501; hyperfine structure studies). Parity from systematics in 2013Yo02 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Half-life and decay mode from {+125}Cd Adopted Levels in the ENSDF database (Jan 2010 update) 
J$spin from 2013Yo02 (Phys. Rev. Lett. 110, 192501; hyperfine structure studies). Parity from systematics in 2013Yo02 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$spin from 2013Yo02 (Phys. Rev. Lett. 110, 192501; hyperfine structure studies). Parity from systematics in 2013Yo02 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T from weighted av of 0.506 s {I15} (1978Ga18), 0.51 s {I1} (1981Ru07), 0.60 s {I3} (1986Go10) and 0.513 s {I6} (2015Lo04). All data are from |g(t) except data of 2015Lo04 from ion-|b decay curve. 
$|4r{+2}|5({+126}Cd)-|4r{+2}|5({+114}Cd)=0.585 fm{+2} {I8} (uncorrelated) {I90} (correlated) from collinear laser spectroscopy (2018Ha30) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$ Isomer in the microsecond range from observation of delayed |g rays 


level_energy_unit: KEV
level_comment:
$In table VIII in 2014Ba18 the 3755 keV level belongs to the low spin decay, but in figure 12 and in table VII it belongs to the high spin decay. The designation in table VIII seems to be misplaced. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
$ Isomer in the microsecond range from observation of delayed |g rays 
J$2007Ho22 proposed spin-parity of (12+) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
J syst of odd-Cd isotopes 
T from |g multiscaling. Value from weighted av of 0.43 s {I3} (1986Go10,1986Ho24) and 0.30 s {I3} (1986Ma42). Other: 1.3 s (1981Al25) 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
MOME2$ uncorrelated uncertainty of 0.005, and correlated uncertainty of 0.010 from electric field gradient combined (by compilers) in quadrature 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 11/2-
level_comment:
MOME2$ uncorrelated uncertainty of 0.010, and correlated uncertainty of 0.014 from electric field gradient combined (by compilers) in quadrature 
T$ not known, but according to e-mail reply of May 7, 2013 from D. Yordanov, the half-lives of the g.s. and the 11/2- isomer are expected to be similar, since both states were seen equally well, otherwise one of the states would have decayed considerably during release from the ISOL-target. 
$ Decay mode of 11/2- isomer is not known 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: MS
level_comment:
J$spin from 2013Yo02 (Phys. Rev. Lett. 110, 192501); |p from {+127}Cd Adopted Levels in ENSDF database 
$Theoretical T{-1/2}=1.31 s, %|b{+-}n=0.16 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 0.37 s {I7} in {+127}Cd Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: MS
level_comment:
T$from 2015Lo04 (Phys. Rev. Lett. 114, 192501) 
$Parity and decay mode are from {+127}Cd Adopted Levels in the ENSDF database (Oct 2009 update) 
$Measured mass excess=-68743.4 keV {I56} (2017La16). Value is -68491 keV {I13} in 2012Wa38: AME-2012, which is closer to that for the isomer in 2017La16 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_comment:
$Half-life of the expected isomer is unknown. The decay mode is expected to be 100% |b{+-} 
E$deduced by 2017La16 from mass excesses of {+127}Cd g.s. and isomer. Literature value=276 keV {I15} (2017Au03: NUBASE-2016) based on mass measurements. 
$Measured mass excess=-68460.1 keV {I47} (2017La16). 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: S
level_comment:
$Spin from 2013Yo02: Phys. Rev. Lett. 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+127}Cd)=-1912.3 MHz {I30} {I94} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+127}Cd)=+0.599 fm{+2} {I9} {I106} 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
E$from the half-life of 340-ms, observed activity in 2021Ha19 is arbitrarily assigned by compiler to the 11/2(-) isomer, although it could be a mixture of the two activities, as 2013Yo02 (Phys. Rev. Lett. 110, 192501) measured spins, magnetic dipole and electric quadrupole moments of the two activities with spin assignments of 3/2 and 11/2, with likely positive parity for the 3/2 level and negative for the 11/2 level; 2017La16 (Phys. Rev. C 96, 044323) measured the energy of the 11/2 isomer as 283.3 keV {I56}; and 2019Lo004 (Phys. Rev. C 99, 044310) measured two separate half-lives of 0.45 s {I+12-8} for the 3/2(+) level and 0.36 s {I4} for the 11/2(-) isomer (Compiler's note). 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. This half-life is closer to T{-1/2}=0.36 s {I4} in 2019Lo04 for the 11/2(-) isomer. Earlier values: 0.45 s {I+12-8} for the 3/2(+) g.s. and 0.36 s {I4} for the 11/2(-) isomer (2019Lo04); 330 ms {I20} (2015Lo04: Phys. Rev. Lett. 114, 192501, could be for a mixture, although closer to the half-life of 11/2(-) isomer). Three older half-life measurements, two consistent values in 1986, and a discrepant value in 1974. Weighted average of values from 2021Ha19, 2019Lo04 and 2015Lo04 (assuming all belong to 11/2(-) isomer) is 337 ms {I20} (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from {+127}Cd Adopted Levels in the ENSDF database (2009 update) 
$Measured mass excess=-68737 keV {I11} (2020Ma09). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J$from {+127}Cd Adopted Levels in the ENSDF database (2009 update) 
E$deduced by 2020Ma09 from mass excesses of {+127}Cd g.s. and isomer. 
$Measured mass excess=-68453.8 keV {I54} (2020Ma09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from |g-multiscaling. Value is weighted average of 0.34 s {I3} (1986Go10) and 0.26 s {I2} (1986Ma42) 
J$ground state of even-even nucleus. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
T$time distribution of 69|g, 238|g and 538|g in ({+136}Xe,X|g), other: 3.76 |ms {I+44-37} from {+9}Be({+238}U,F|g):isomer 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
T$time distribution of 237.9|g, centroid shift method 
$Dominant |nd{-3/2}{+-1}h{-11/2}{+-1} configuration can possibly be traced to |pg{-9/2}|nd{-3/2} monopole 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2016Du13 from decay curves for 857|g and 925|g, analyzed from |b|g-coin spectra. The respective half-lives obtained were 245.8 ms {I21} and 257 ms {I11}. Weighted average of these two values is 246.2 ms {I21}. A fit of the summed time distribution of the above two |g rays gave T{-1/2}=246.2 ms {I21}. Systematic uncertainties were discussed by the authors. This value can be compared with 245 ms {I5} (2015Lo04: Phys. Rev. Lett. 114, 192501) and 280 ms {I40} (1986Go10: Z. Phys. A324, 117; also 1988FoZX: Proc. Intern. Conf.Nuclear Data for Science and Technology, Mito, Japan, p.837) 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M4
level_comment:
$Proposed configuration (2017Ju02)= |p(0g{-9/2}{+-2}){-8+}~#|n(0h{-11/2}{+-1},1d{-3/2}{+-1}){-7-} 
T$measured by 2017Ju02 from decay curve for summed 203, 238, 309, 440, 538, 646, 785, 1060 and 1263 |g rays. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+128}Cd)=-2171.6 MHz {I23} {I100} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+128}Cd)=+0.660 fm{+2} {I9} {I107} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 246.2 ms {I21} (2016Du13: Phys. Rev. C93, 062801(R)); 245 ms {I5} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: five older from from 1974 to 1986, either less precise or discrepant. Weighted average of values from 2021Ha19, 2016Du13 and 2015Lo04 is 245.9 ms {I21} (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=0.07 (1997Mo25), 0.77, 0.94 (2002Pf04) 
%B-N$there is some experimental evidence of delayed-neutron emission from {+129}Cd decay from the work of 2003ArZX (also 2005Kr20), but their half-life measurement is in sharp disagreement with that from 2015Ta13 
T$others: 154.5 ms {I20} (2015Lo04, from ion-|b correlated curves), 104 ms {I6} (2003ArZX,2005Kr20, from decay curves for delayed neutrons). The value from 2015Lo04 may correspond to mixture of the two activities of {+129}Cd 
J,MOMM1,MOME2$hyperfine structure in collinear laser spectroscopy (2013Yo02). For Q, uncorrelated uncertainty of 0.013, and correlated uncertainty of 0.023 from electric field gradient combined in quadrature. See 2014De06 and 2014Zh02 for theoretical calculations of single-particle occupation probabilities using experimental values of quadrupole moments 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
%B-N$there is some experimental evidence of delayed-neutron emission from {+129}Cd decay from the work of 2003ArZX (also 2005Kr20), but their half-life measurement is in sharp disagreement with that from 2015Ta13 
E$x|?290 keV (2014Ta29) from shell-model calculations 
J,MOMM1,MOME2$hyperfine structure in collinear laser spectroscopy (2013Yo02). For Q, uncorrelated uncertainty of 0.007, and correlated uncertainty of 0.005 from electric field gradient combined in quadrature. See 2014De06 for theoretical calculations of single-particle occupation probabilities using experimental values of quadrupole moments 
T$others: 242 ms {I8} (2003ArZX,2005Kr20, from decay curves for delayed neutrons), 0.27 s {I4} (1986Go10, from decay curve for a 281-keV |g ray, but no such |g is reported in the detailed study of decay of activities of {+129}Cd by 2015Ta13) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2-)
level_comment:
$Ordering of the 406-1181 |g cascade is not established experimentally, but the level ordering in energies and spins is predicted by shell-model calculations 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
T$from summed time difference distribution of the 406- and 1181-keV |g rays (2014Ta29) 
$Configuration=|nh{-11/2}{+-1}~#|p(g{-9/2}{+-1}p{-1/2}{+-1}) mixed with |nh{-11/2}{+-1}~#|p(g{-9/2}{+-1}p{-3/2}{+-1}) and |nh{-11/2}{+-1}~#|p(g{-9/2}{+-1}f{-5/2}{+-1}) (2014Ta29) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (21/2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
T$from summed time difference distribution of the 406- and 1181-keV |g rays (2014Ta29) 
$Configuration=|nh{-11/2}{+-1}~#|p(g{-9/2}{+-1}p{-1/2}{+-1}) mixed with |nh{-11/2}{+-1}~#|p(g{-9/2}{+-1}p{-3/2}{+-1}) and |nh{-11/2}{+-1}~#|p(g{-9/2}{+-1}f{-5/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_comment:
T$measured by 2016Du13 from decay curves for 358.9|g, 1796.5|g, and 2155.6|g, analyzed from |b|g-coin spectra. The respective half-lives obtained were 148 ms {I3}, 143 ms {I6} and 136 ms {I12}. The weighted average of these three values is 146.5 ms {I26}. A fit of the summed time distribution of the above three |g rays gave T{-1/2}=147 ms {I3}. Systematic uncertainties were investigated by the authors. This value can be compared with 154 ms {I2} (2015Ta13: Phys. Rev. C91, 054324; also 155 ms {I3} in thesis by J. Taprogge, Universidad Autonoma de Madrid, 2015), where 995.1|g and 1354.2|g were also used for T{-1/2} analysis. 2016Du13 point out that 995.1|g potentially contains contribution from both the activities, and that 1354.2|g is a doublet with a |g ray from the decay of {+129}In, thus they did not use these two |g ray in their T{-1/2} analysis. 2016Du13 obtain T{-1/2}=151.8 ms {I23} from 995.1|g and 192 ms {I12} from 1354.2|g, as compared to 152.0 ms {I27} and 158.6 ms {I81}, respectively in thesis by J. Taprogge (2015) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$measured by 2016Du13 from decay curves for 1422.9|g and 1586.2|g, analyzed from |b|g-coin spectra. The respective half-lives obtained were 158 ms {I8} and 157 ms {I19}. The weighted average of these two values is 157.9 ms {I75}. A fit of the summed time distribution of the above two |g rays gave T{-1/2}=157 ms {I8}. Systematic uncertainties were investigated by the authors. This value can be compared with 146 ms {I8} (2015Ta13: Phys. Rev. C91, 054324) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
$Spin from 2013Yo02: Phys. Rev. Lett. 110, 192501. 
$Measured isotope shift |d|n({+114}Cd,{+129}Cd)=-1911.1 MHz {I55} {I108} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+129}Cd)=+0.638 fm{+2} {I12} {I133} 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} first measured by 2021Ha19 from (implanted ions)-|b-n correlated events. 2005Kr20 (Eur. Phys. J. A25, s{+-1}, 633) found evidence for delayed neutron decay but %|b{+-}n was not measured 
E,J,T$the 155.9-ms activity in 2021Ha19 is arbitrarily assigned by compiler to the g.s., although it could be a mixture of the two activities comprising g.s. J|p=11/2-, and 0+x level with J|p=3/2+ as measured in 2013Yo02 (Phys. Rev. Lett. 110, 192501); later 2015Ta13 (Phys. Rev. C 91, 054324) measured half-lives as 155 ms {I3} (or 154 ms {I2}) for the 11/2- g.s. and 146 ms {I8} for the 3/2+ isomer; 2016Du13 (Phys. Rev. C93, 062801(R)) measured the respective half-lives as 147 ms {I3} and 157 ms {I8}; 2015Lo04 (Phys. Rev. Lett. 114, 192501) measured T{-1/2}=154.5 {I20}, probably for a mixed activity. Other: 2005Kr20 measured very different half-lives of 104 ms {I6} and 242 ms {I8}. (Compiler's note) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J$from {+129}Cd Adopted Levels in the ENSDF database (2015 update) 
$Measured mass excess=-63122.1 keV {I54} (2020Ma09). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from {+129}Cd Adopted Levels in the ENSDF database (2015 update) 
E$deduced by 2020Ma09 from mass excesses of {+127}Cd g.s. and isomer. 
$Measured mass excess=-62779.1 keV {I56} (2020Ma09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from 2001Ha39 (also 2001Pf04). Other: 0.20 s {I4} (1986Kr17). 
$Other %|b{+-}n|?4 (1986Kr17) 
$ %B-N, T1/2: THEORY: 1999Ma88, 1999En03, 1997Bo24, 1988Kr08, 1981Al25 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$ this level is not confirmed by 2007Ju05 in {+130}Cd isomer study, thus its existence is suspect. It is not included in 'adopted levels, gammas' dataset. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-N$from {+130}Cd Adopted Levels in ENSDF database. 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 162 ms {I7} in {+130}Cd Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Decay modes from {+130}Cd Adopted Levels in ENSDF database (May 2008 update) 
T$measured by 2016Du13 from decay curves for 451.0|g, 1170.3|g, and 1669.2|g, analyzed from |b|g-coin spectra. The respective half-lives obtained were 123 ms {I5}, 138 ms {I20} and 126 ms {I6}. Weighted average of these three values is 125 ms {I4}. A fit of the summed time distribution of the above three |g rays gave T{-1/2}=126 ms {I4}. Systematic uncertainties were discussed by the authors. This value agrees with 127 ms {I2} from 2015Lo04 (Phys. Rev. Lett. 114, 192501) but not with 162 ms {I7} from 2001Ha39 (Nucl. Phys. A688, 578). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Measured isotope shift |d|n({+114}Cd,{+130}Cd)=-2208.1 MHz {I33} {I115} for 5s {+2}S{-1/2} |) 5p {+2}P{-3/2} transition 
$Measured |d|4r{+2}|5({+114}Cd,{+130}Cd)=+0.705 fm{+2} {I11} {I132} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n or P{-n} measured by 2021Ha19 from (implanted ions)-|b-n correlated events. Other measurement: 3.5 {I10} (2001Ha39: Nucl. Phys. A688, 578c). Weighted average of the two values is 3.0 {I2} (compiler's note) 
T$measured by 2021Ha19 from the decay curves of (implanted ions)-|b and (implanted ions)-|b-n correlated events. Earlier values: 126 ms {I4} (2016Du13: Phys. Rev. C93, 062801(R)); 127 ms {I2} (2015Lo04: Phys. Rev. Lett. 114, 192501). Others: 162 ms {I7} (2001Ha39); 195 ms {I35} (1986Kr17: Z. Phys. A325, 489). Weighted average of values from 2021Ha19, 2016Du13 and 2015Lo04 is 129 ms {I2} (compiler's note) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. These values are compared with T{-1/2}=127 ms {I2} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=3.0 {I2} in 2021Ha19 (Phys. Lett. B 816, 136266). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
E$assumed as the ground state 
J$probable configuration=|nf{-7/2} (2000Ha55), syst. (2003Au02) 
%|b{+-}n from 2000Ha55 (also 2001Ha39) 
T$from timing of delayed neutrons (2000Ha55,2001Ha39) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from {+131}Cd Adopted Levels in ENSDF database 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Value of 98.0 ms {I2} quoted in Table I of 2015Lo04 should be 98 ms {I2} as per e-mail reply of May 11, 2015. Other: 68 ms {I3} in {+131}Cd Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity corresponds to the g.s. 
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. These values are compared with T{-1/2}=98 ms {I2} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); 68 ms {I3} in 2000Ha55 (Phys. Rev. C62, 054301); and %|b{+-}n=3.5 {I1} in 2000Ha55. Compiler's note: uncertainty of 0.2 ms in 2015Lo04 should be 2 ms, according to e-mail reply of May 11, 2015 from the first author of 2015Lo04 to the XUNDL compiler. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n from 2000Ha55 (also 2001Ha39) 
$Theoretical T{-1/2}=244 ms, %|b{+-}n=64.3, %|b{+-}2n=0.23 (2003Mo09) 
$Theoretical T{-1/2}=61 ms, %|b{+-}n=61.7, %|b{+-}2n=0.5 (2016Ma12) 
T$weighted average of 82 ms {I4} (2015Lo04, analysis of the (implanted ions)|b correlated decay curve in time and position) and 97 ms {I10} (2000Ha55, 2001Ha39, from delayed neutrons decay curve) 
$Probable configuration=|nf{-7/2}{+2}~#|pg{-9/2}{+-2} (2000Ha55) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$from systematic trend of neighboring nuclides (2016Wa28) 
$Proposed (2016Wa28) configuration=mixture of |p{+-2}~#|n{+2} excitations around the robust {+132}Sn core 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. These values are compared with T{-1/2}=82 ms {I4} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and T{-1/2}=97 ms {I10}, %|b{+-}n=60 {I15} in 2000Ha55 (Phys. Rev. C62, 054301). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$Calculated %|b{+-}n=0.47, %|b{+-}2n=98.6 (1997Mo25). 
T$from |b{+-}n(t) in 2003ArZX, 2005Kr20 
J$from the isotone {+135}Sn, based on shell-model predictions (|n(f{-7/2}{++1}) orbital). Other: J|p=3/2- (|n(p{-3/2}{++1})) predicted in 1997Mo25 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=186 ms, %|b{+-}n=21.1, %|b{+-}2n=50.3 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 57 ms {I10} in {+133}Cd Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity corresponds to the g.s. 
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=64 ms {I8} in 2015Lo04 (Phys. Rev. Lett. 114, 192501) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=0.17, %|b{+-}2n=93.32 (1997Mo25) 
T$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_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical T{-1/2}=14.5 ms, %|b{+-}n=31.3, %|b{+-}2n=43.4, %|b{+-}3n=3.7 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=35.2 ms, %|b{+-}n=50.9, %|b{+-}2n=3.1, %|b{+-}3n=0.5 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 68 counts were assigned to {+134}Cd, 2 events with spectrometer setting on Pd, and 66 events with setting on Sn. Probability of misidentification of this isotope is 0.10 for Pd setting and <0.01% for Sn setting (2018Sh11). 
$Production |s=0.99 pb for Sn setting, with 30% systematic uncertainty |s. 
T$measured by 2015Lo04 at RIBF-RIKEN. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=65 ms {I15} in 2015Lo04 (Phys. Rev. Lett. 114, 192501) 


level_energy_unit: KEV
level_comment:
$decay mode assigned by the compiler as {+96}In is expected to be proton-unbound nucleus from theoretical S(p)=-0.38 MeV (1997Mo25) 
$A total of two events assigned to {+96}In in 2016Ce02 are assumed by the evaluator to correspond to the g.s. activity of {+96}In 
$Theoretical |b-decay half-life=24.8 ms (1997Mo25) 
J$1-8, |p=+ from proton in 9/2+ and neutron in 7/2+ orbital (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
$|e decay considered negligible by 2018Pa20. 
$Production |s=0.86 pb {I41} in {+9}Be({+124}Xe,X),E=1 GeV/nucleon reaction (2011StZV), 0.13 pb {I2} in {+9}Be({+124}Xe,X),E=345 MeV/nucleon at RIBF-RIKEN (2016Ce02). A total of 278 counts were assigned to {+97}In in 2018Pa20 (also 2019Pa16, 2016Ce02) 
%B+P$from number of single-pixel events with |DE>1500 keV (2018Pa20); value is combined for g.s. and an hypothesized isomer. 
$Deduced S(p)=-0.10 MeV {I19} (2018Pa20) for g.s. of {+97}In, based on experimental data, semiempirical theory of proton emission and shell-model calculations. 2017Wa10 give -1.09 MeV {I57} from systematic trend. Theoretical S(p)=-300 keV (2019Mo01) 
T$measured by 2018Pa20, using maximum likelihood method (MLH) for (implant)(positron)-correlated decay curve, where the fit function contained the parent, |b-daughter, and |bp-daughter decay components with half-lives and %|bp branching ratios, and a constant background for random correlations. Two generations of isotopes were considered in the Bateman equation. Decay constants for {+97}Cd and {+96}Ag daughters were taken from literature. Value of 28 ms {I5} was obtained by 2018Pa20 when the analysis of decay curve included the hypothesized isomer, and subsequent decay of {+96}Cd to {+96}Ag. Other: 26 ms {I+47-10} (2011StZV) 
$Measured Q(|e)({+97}In)=10.0 MeV {I30} (2018Pa20), from (implants)|b correlated energy curve, by taking into account contribution from {+97}Cd daughter activity, and assuming that the observed endpoint energy corresponds to g.s. to g.s. |b{++} transition. Other: 13.26 MeV {I50} (syst, 2017Wa10) 
$278 implantation counts were assigned to {+97}In by 2018Pa20. 
$2018Pa20 assumed 100-(%|b{++}p)=98.3 {I+8-17} |b{++} feeding of the g.s. of {+97}Cd, implying log| {Ift}=3.0 {I9} for this |b transition. 


level_energy_unit: KEV
level_energy_info: ;ERR=CA;ERR=?
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_uncertain: ?
level_comment:
$Isomeric activity proposed by 2018Pa20 from observed |b-decay correlation percentage of 50% {I4}, lower than the expected value of 66% {I4}, from values obtained from the decays of {+91}Pd, {+95}Cd, and {+99}Sn 
$In beta-delayed gamma-ray spectrum, a peak at 421 keV was observed with 9 {I4} counts, with the decay curve giving a half-life of 1.7 s {I7}, consistent with the tentative assignment of 421|g as a (1+) to (2+) transition in {+96}Ag from the decay of {+96}Cd, as reported by 2011Na34. A strong 421-keV |g was also seen by 2017Da07, and assigned as a low-lying transition in {+96}Ag. 2018Pa20 proposed that the isomer decayed by direct proton decay to {+96}Cd. 
E$between 568 and 763 keV calculated by 2018Pa20 from shell-model and different interactions 
T$1.3 |ms to 230 |ms deduced by 2018Pa20, the upper limit from solution of the exponential decay equation with an elapsed time of 600 |ms (dead time of WAS3ABi after implantation), and the lower limit from assumption of 2|s reduction of {+97m}In counts during the 600-ns flight time through the separator. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: MS
level_comment:
%ECP$measured by 2019Pa16. Other: 5.5 {I+30-20} (2012Lo08, based on observation of 20 |bp coincidence events. Uncertainty from e-mail reply of August 1, 2012 from G. Lorusso). 2019Pa16 suggest that large %|ep reported in 2012Lo08 probably contributed by the (9+) isomeric activity. 
J$|b{++} decay proceeds mostly to the ground state of {+98}Cd with T=1 through a superallowed |b transition as log| {Ift}=3.57 {I8}. Also J|p=0+ and T=1 from shell-model predictions in 1997He24. See also shell-model calculations by 2012Co07 for energies of proton hole-neutron hole multiplet in {+98}In. 
T$weighted average of 30 ms {I1} (2019Pa16, |b|g-correlated decay curve); 47 ms {I13} (2012Lo08 and 2008Ba53, decay curves of time correlations between implantations and decay radiation); 32 ms {I6} (2011StZV, implants-|b-correlated decay curve); 32 ms {I+32-11} (2001Ki13,2002StZZ,2002Fa13,2007WeZX). 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%ECP$measured by 2019Pa16. Other measurement: 19 {I2} (2012Lo08, from observation of 40 |bp-coin events). 
E$from |b{++}|g-coin data (2019Pa16). Other: <500 keV from systematics (2017Au03) 
T$weighted average of 0.89 s {I2} (2019Pa16, weighted average of 0.99 s {I7} from |b|g-decay curve and 0.88 s {I2} from |bp-decay); 1.27 s {I30} (2012Lo08, decay curves of time correlations between implantations and decay radiation), 0.86 s {I21} (2011StZV, implants-|b-correlated decay curve), and 1.2 s {I+12-4} (2001Ki13,2002StZZ,2002Fa13). Other: 0.66 s {I40} reported in 2008Ba53 (earlier publication of 2012Lo08) 
J$proposed by 2019Pa16 from |b feeding to (8+) state in {+98}Cd with log| {Ift}|?5.0, and strong population of (15/2+), (17/2+) and (21/2+) levels in {+97}Ag from |b{++}p decay through minimum angular momentum for the proton, which for 9+ assignment would be L=1. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$from implant-|b|g(t) using multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16) 
%B+P$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_lifetime_unit: S
level_comment:
T$weighted average of 0.99 s {I7} from implant-|b|g(t) and 0.88 s {I2} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation (2019Pa16) 
%B+P$from the number of |bp events divided by the total number of decays as determined from the T{-1/2} analysis (2019Pa16). 
E$from measured difference in endpoint energies of ground state and isomer (2019Pa16). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$From 2012Lo08 in |b-decay data in {+9}Be({+112}Sn,X|g) reaction. T{-1/2}=3.05 s {I60} is also listed in 2012Lo08 which may be from |b{++}p decay curve 
J$9/2+ from syst (2017Au03) 
%B+P$ Measured by 2012Lo08 based on observation of 183 |bp coincidence events. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$ measured by 2012Lo08 from decay curves of time correlations between implantations and decay radiation. Decay curves were fitted with Poisson distribution using log-likelihood function by consideration of decay of parent, daughter and grand-daughter. Value is from |b-decay data. T{-1/2}=3.05 s {I60} is also listed which may be from |b{++}p decay curve 
J$9/2+ from syst (2017Au03) 
%B+P$ Measured by 2012Lo08 based on observation of 183 |bp coincidence events. 


level_energy_unit: KEV
level_comment:
E$reported as 671 {I33} (stat) {I16} (syst); uncertainty added in quadrature (2023Ni08). Energy is extracted from simultaneous fit of {+80}Sr{+19}F{++} and both In states 
J$from systematics the isomer is extrapolated as 1/2- 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
$%|ep: from weighted average of 1.66 {I3} (2019Pa16); 1.7 {I4} (2012Lo08, observation of 756 |bp coincidence events); and 1.6 {I3} (2002Pl03, proton-TAS coin spectrum). Other: >3.9 (1995Sz01, estimated from singles proton spectrum) 
T$weighted average of 5.62 s {I6} (2019Pa16, weighted average of 5.60 s {I6} from |b-correlated decay curve and 5.70 s {I16} from |bp-correlated decay curve); 5.8 s {I2} (2019Lu08, (implant)|g-correlated decay curve); 5.7 s {I3} (2012Lo08, |b|g- and |bp-implants-correlated decay curves); and 5.9 s {I2} (2002Pl03). Others: 6.1 s {I9} (1995Sz01), 7.8 s {I8} (1995Sc33). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2+)
level_uncertain: S
level_comment:
E$level proposed from deexcitation of 1297|g from the 2720+x level, but no deexciting |g transitions reported in either 2012Hi07 or 2019Lu08. From large-scale shell-model calculations, 2012Hi07 proposed decays to 236+x, a (3+) level below the 672+x level, and 672+x level with branching ratios of 78%, 11% and 11%, respectively. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 1+
level_comment:
J$Gamow-Teller transition from 0+ parent state with log| {Ift}|?2.6 for 100% |b{++}+|e feeding 
$From observation of a single proton event attributed to delayed proton decay in 2012Hi07, %p decay of this level is estimated by 2012Hi07 as <1%. Other: <17% (1997Su06,1996Ki23) 
$Dominant configuration=|pg{-9/2}{+9}~#|ng{-7/2}{+1} 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
T$weighted average of 5.62 s {I6} (2019Pa16, weighted average of 5.60 s {I6} from |b-correlated decay curve and 5.70 s {I16} from |bp-correlated decay curve); 5.8 s {I2} (2019Lu08, (implant)|g-correlated decay curve); 5.7 s {I3} (2012Lo08, |b|g- and |bp-implants-correlated decay curves); and 5.9 s {I2} (2002Pl03). Others: 6.1 s {I9} (1995Sz01), 7.8 s {I8} (1995Sc33). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2+)
level_uncertain: S
level_comment:
E$level proposed from deexcitation of 1297|g from the 2721+x level, but no deexciting |g transitions reported in either 2012Hi07 or 2019Lu08. From large-scale shell-model calculations, 2012Hi07 proposed decays to 236+x, a (3+) level below the 672+x level, and 672+x level with branching ratios of 78%, 11% and 11%, respectively. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 1+
level_comment:
E$value is consistent with measured E(|b-endpoint)=2.6 MeV {I10}, 2.93 MeV {I34} from observation of a single event of |b-delayed proton emission (2012Hi07), and 2.76 MeV {I43} from TAGS data (1996Ki23, 1997Su06). Theoretical calculations suggest 1+ level at 2533 (1996Ki23), 2963 (2012Hi07) 
J$Gamow-Teller transition from 0+ parent state with log| {Ift}=2.85, assuming 100% |b{++}+|e feeding to this level 
$From observation of a single proton event attributed to delayed proton decay in 2012Hi07, %p decay of this level is estimated by 2012Hi07 as <1%. Other: <17% (1997Su06,1996Ki23) 


level_energy_unit: KEV
level_comment:
E$reported as 658 {I14} (stat) {I7} (syst); uncertainty added in quadrature (2023Ni08). 
J$from systematics the isomer is extrapolated as 1/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$from ME(g.s)=-68550 {I13} (stat) {I6} (syst) and ME(isomer)= -67891 {I48} (stat) {I6} (syst) (2019Xu13) 
J$As proposed in 2019Xu13 based on systematics of 1/2- isomers in In isotopes. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: S
level_comment:
T$From delayed gammas (2003Gi06) 
T$Others: 22 s 1 (1995Sz01), 24 s {i3} (1981Be16), 21 s {i7} (1981CeZX) 
J based on J|p=6+ for {+104}In (1995Se08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_comment:
J$5+ is less probable as the best fit for the tas spectrum in 102Sn |e decay is obtained with 94 keV |g being E2 and 69 keV |g being M1 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: S
level_comment:
T from 188|g-, 202|g-decay curves (1978Lh01); on-line mass spectrometry 
J$ J=9/2 from analogy to {+111}In, {+109}In, {+107}In and {+105}In g.s. |p=+ from logft=5.9 to (7/2)+ 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MIN
level_comment:
T$from 1995Sz01. Others: 1.8 min {I2} (1989Va05), 1.8 min {I2} (1978Hu06), 1.5 min {I2} (1977Va06) and 1.7 min {I3} (1976CoYX) 
%B+$ratio: |b{++}/(|e+|b{++})=0.44 {I3} from coin method, 0.45 {I1} from singles (1995Sz01) 
J$could be (5+,6+,7+) from the strong feeding to 6+ levels in {+104}In |e+|b{++} decay. Assumed to be (6+) to be consistent with the |g's decay with known mult from the 1+ levels, but if feeding to 3210, 8+ level is definite then J|p>6+ would be required. However, J was measured as 5,6 by 1987Eb02. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
J$|p=+ from log| {Ift}=5.77 to 7/2+ 131 level; J from isotope shift and hfs measurements (1987Eb02) 
T$from |g(t) in {+105}In |e decay (1984Ve01); others: 5.1 min {I3} (1975Ri06,1974Bu20), 4.8 min {I2} (1980Wi20) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%IT$Only IT decay has been reported 
J$674.1|g M4 to 9/2+; systematics 
T$ weighted average of 55 s {I5} in 1975Ri06 and 43 s {I4} in 1980Wi20 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J$484.7|g E2 to 13/2+; band member 
T$Others: 48~ps~{I15} (1992Is02) via recoil distance method; 330~ps~{I100} (1995Is06) via recoil distance method 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_comment:
E$due to reversed ordering of 1730-131 cascade in later studies (1997Ko51,1999De50), this level is non-existent, instead the level is defined at 3829 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: MIN
level_comment:
$rms charge radius: 4.5364 fm 96 (2004An14) 
T from |g-decay curves (1978Hu06). Others: 6.35 min {I20} (1976Fl14), 6.26 min {I24} (1972Me02); |g-decay curves 
J J from NMR of on-line oriented {+106}In (1987Va27) |p from log| {Ift}=5.77 and 5.90 to 6+ levels 
MOMM1 From optical hfs, isotope shifts. Other: 4.921 {I13} (1985Va06) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
From B(E4)(W.u.)|<30 and |a(28.6|g)=8.17|*10{+5} one gets branching (IT)<0.04% 
T from |g-decay curves (1978Hu06). Others: 5.3 min {I2} (1976Fl14), 5.33 min {I6} (1972Me02), 5.32 min {I5} (1969St18), 5.3 min {I1} (1966Ca09); |g-decay curves 
J J|p=2+ suggested from strong |g feeding from 1+ levels; |e decay to 1795-keV level (J|p=0+) with log| {Ift}=7.10 almost excludes J|p=3+ if decay schemes is complete, which is very probably not the case due to large Q value in {+106}Sn |e,|b{++} decay. log| {If{+1u}t}<8.5 for |b branches to 632, 1494, 1716, 2104, 2253, and 2347 levels almost excludes |p=-. J|p=3+ suggested from Hauser-Feshbach calculations. 1988Ba10 suggest 2+ from {+106}Sn |e decay 
E from observation of |g decay of 390-keV level to J|p=7+ g.s. and 28.6-keV levels in {+106}Cd(p,n|g) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J J=1 or 2 from Hauser-Feshbach calculation. |p=+ from allowed |b transition (log| {Ift}=5.1) and M1 to 28.6 level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$ from adopted dataset for {+106}In in ENSDF database 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
MOMM1,MOME2$others: 5.58 {I53} (1982Va21) NO/S method, Q CFBLS method 
T 32.4 min {I3} (1973Ny03) |g-decay curves. Others: 33 min {I2} (1949Ma20), 31 min {I3} (1963Ba41), 33 min {I1} (1971Ri05) 
J L({+3}He,d)(g.s.)=4, L({+3}He,d)(678 level)=1. M4 |g connects these two states. B(E3)(W.u.)<5|*10{+-9} for |DJ=3 (if |d>10) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T 50.4 s {I6} (1976Hs01) |g-decay curve. Other: 51.8 s {I20} (1973Ny03) 
E 1/2- isomerism occurs at 674,650,537,392,336 keV in {+105}In, {+109}In, {+111}In, {+113}In, {+115}In, respectively 
J$see g.s. 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
E low-lying 11/2+ states occur regularly at 1026,1153,1173,1133 keV in {+109}In,{+111}In,{+113}In,{+115}In, respectively 
J$E2 |g decay to g.s., excit consistent with 11/2 in (d,n|g) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$low-lying 3/2- states occur at 981,803,647,597 keV in {+109}In,{+111}In,{+113}In,{+115}In, respectively 
J$M1 |g decay to 1/2- state, excit consistent with 1/2 in (d,n|g) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E low-lying 5/2+ states occur regularly at 1099,1102,1132,1078 keV in {+109}In,{+111}In,{+113}In,{+115}In, respectively 
J$E2 |g decay to g.s., excit consistent with 5/2 in (d,n|g) 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_comment:
E low-lying 1/2+ states occur regularly at 1172,1188,1030 keV in {+109}In,{+111}In,{+113}In, respectively 
J$E1 |g decay to 1/2- state, excit consistent with 1/2 in (d,n|g) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
E$low-lying 13/2+ states occur regularly at 1428,1401,1345,1291 keV in {+109}In,{+111}In,{+113}In,{+115}In, respectively 
J$stretched E2 |g to 9/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$may correspond with (d,n|g) excitations at 1107, 1129, 1166 keV |s(|q) can also be fit by 4+0 with S=7.5+0.75 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (21/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ probably feeds 1854, 17/2+ and 2003, 19/2+ levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_comment:
$B(E2) measured by 2013Di01 and normalized to B(E2)(0+ to 2+)=0.0704 {I15} in {+58}Ni (2010Ne01: Nuclear Data Sheets evaluation, also in ENSDF database) 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: MIN
level_comment:
J$J=7 from NMR (1986Va27), |p from log| {Ift}=5.0 to 6+. 
T$from 1975Fl01. Others: 59 min {i5} (1963Ka18), 58 min {i2} (1962Ka23), 55 min (1956Me94) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$J=2 from collinear LASER spectroscopy (1986Eb01). |p from M1,E2 |g from 1+ 
T$from 1975Fl01. Others: 39 min {i2} (1963Ka18), 40 min {i2} (1962Ka23), 40 min {i2} (1956Me94) 
E$from 1989Kr07 in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (6,7,8)
level_comment:
J$J>5 from Hauser-Feshbach analysis, |g transition to 7+ is probably not pure Q since its presence in |g|g spectrum with resolving time |?6 ns implies B(E2)(W.u.)>130 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
J$M1, E2 |g's to J|p=2+ and 3+ states, |g's to J|p=4+ and 4+,5+, |g(|q) and Hauser-Feshbach analysis. 


level_energy_unit: KEV
level_spin_parity: (9)-
level_comment:
J$M1 |g to 8-. |s(1332 level)/|s(1119 level) much smaller in ({+3}He,2np|g) than in ({+14}n,4n|g). |g(|q) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T 237-1396 cascade observed to have a lifetime >100 ns with an upper limit of |?100 |ms. Since the 237|g appears to be E2 and would have B(E2)(W.u.)<0.25 if this lifetime were associated with the 1633 level, the authors propose an additional unobserved level which would feed the 237-1396 cascade 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$ from adopted dataset for {+108}In in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: H
level_comment:
J$from atomic-beam magnetic-resonance flop-in technique (1958Ma43,1959Ma19); |p=+ from |m, L({+3}He,d)=4 
T$weighted average of 4.167 h 18 (203|g(t) in 2005Gy02, uncertainty is statistical only), and 4.155 h 12 (203|g(t) in 2009Ra17, weighted average of 4.143 h {I4} (Au catcher), 4.184 h {I6} (Pb catcher) and 4.151 h {I7} (Al catcher); uncertainty is statistical only). Others: 4.30 h {I15} (|b(t) in 1949Ma20), 4.2 h 2 (ce(t) in 1951Mc11), 4.3 h {I3} (momentum plot of positron in 1962No06), and 4.2 h {I1} (203|g(t) in 1968Sm08). 
MOMM1$from collinear fast-beam LASER spectroscopy (1985Ul03,1987Eb02) Other: +5.538 {I11} from nuclear magnetic resonance on oriented nuclei (1981Ha26), 5.53 {I6} (from atomic beam in 1959Ma19), 
MOME2$from collinear fast-beam LASER spectroscopy (1985Ul03,1987Eb02) 
CONF$|p(g{-9/2}){+-1} 
$|d<r{+2}>(115,109)=-0.410 {I7} (1985Ul03). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J$649.87|g M4 to 9/2+; L({+3}He,d)=1 
T$weighted average of 1.34 min {i7} (651|g(t) in 1968Sm08), 1.35 min {i20} (658|g(t) in 1966Ma39) and 1.3 min {i2} (1956Ku51) 
CONF$|p(p{-1/2}){+-1} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L({+3}He,d)=(2); 785.3|g to 1/2+ and 1956.9|g to 9/2+; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
J$673.52|g M3 to 13/2+ 
T$weighted average: 214 ms {i12} (|g(t) in 1994ByZZ), 210 ms {i4} (using 402-,673-,1026-,1428|g(t) in 1979Va13), 210 ms {i1} (using 405-,680-,1035-,1435|g(t) in 1966We01), 204 ms {i10} (|g(t) in 1965Al15), and 210 ms {i2} (1963Po10) 
CONF$|n(g{-9/2}){+-1}~#|n6{++}, where |n6{++} is a mixture of |n(d{-5/2},g{-7/2}) and |n(g{-7/2}){++2}. Shell model would suggest configuration=|pg{-9/2}{+-3}; However, no such isomer was observed in other odd-A In isotopes 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$L({+3}He,d)=(2); 1039.0|g to 5/2+, 1488.7|g to 1/2-; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_comment:
J$710.7|g to 5/2-, 1501.7|g to 1/2-, 1170.2|g to 3/2-; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$L({+3}He,d)=(2), 1621.7|g to 1/2-, 1290.0|g to 3/2-; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_comment:
J$L({+3}He,d)=(0,2,3); 1655.7|g to 1/2-, 1205.6|g to 5/2+; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$L({+3}He,d)=(0,2); 1911.1|g to 1/2-, 1462.0|g to 5/2+; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$L({+3}He,d)=(4), 1565.6|g to 11/2+, 452.8|g to 3/2+; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
J$336.36|g M1+E2 to 15/2-, band assignment 
T$weighted average of 0.38 ps {i17} (1987KuZV) in {+107}Ag(|a,2n|g) and 0.42 ps {i17} (also 1987KuZV) in {+97}Mo({+16}O,3pn|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$1889.8|g to 3/2-, 1157.8|g to 9/2+, 1700.7|g to 1/2+; direct feeding in {+109}Sn |e decay (J|p=5/2+) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
J$534.9|g M1+E2 to 15/2- 
T$weighted average of 0.17 ps {i10} (1987KuZV) in {+107}Ag(|a,2n|g) and 0.31 ps {i17} (also 1987KuZV) in {+97}Mo({+16}O,3pn|g) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
J$990.25|g E1 |DJ=0 to 19/2+, 223.4|g M1 to 17/2-; band assignment 
T$weighted average of 0.49 ps {i21} (1987KuZV) in {+107}Ag(|a,2n|g) and 0.42 ps {i14} (also 1987KuZV) in {+97}Mo({+16}O,3pn|g) 


level_energy_unit: KEV
level_spin_parity: 23/2-
level_lifetime_unit: PS
level_comment:
J$207.90|g M1(+E2) to 21/2-; band assignment 
T$from {+97}Mo({+16}O,3pn|g) (1987KuZV); Other: 0.42 ps {i14} (1987KuZV) in {+107}Ag(|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
J$231.3|g (M1) to 19/2- 
T$weighted average of 0.45 ps {i14} (1987KuZV) in {+107}Ag(|a,2n|g) and 0.42 ps {i14} (also 1987KuZV) in {+97}Mo({+16}O,3pn|g) 


level_energy_unit: KEV
level_spin_parity: 25/2-
level_lifetime_unit: PS
level_comment:
J$389.80|g M1+E2 to 23/2-, band assignment 
T$weighted average of 1.4 ps {i7} (1987KuZV) in {+107}Ag(|a,2n|g) and 2.7 ps {i14} (also 1987KuZV) in {+97}Mo({+16}O,3pn|g) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (25/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$feeding to J|p=19/2- (band 8) and J|p=23/2- and 25/2- (band 11) levels in {+76}Ge({+37}Cl,4n|g) (1997VaZS). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 1.34 min {i7} (651|g(t) in 1968Sm08), 1.35 min {i20} (658|g(t) in 1966Ma39) and 1.3 min {i2} (1956Ku51) 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_lifetime_unit: MS
level_comment:
T$using 673|g(t) (216 ms 2), 402|g(t) (202 ms 5), 1026|g(t) (204 ms 6) and 1428|g(t) (218 ms 3) in 1979Va13 
CONF$|n(g{-9/2}){+-1}~#|n6{++}, where |n6{++} is a mixture of |n(d{-5/2},g{-7/2}) and |n(g{-7/2}){++2} 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (25/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$feeding to 19/2- level of band 8; also feeding 23/2- and 25/2- levels of band 11. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: H
level_comment:
J$J=7 from atomic-beam magnetic-resonance flop-in technique (1958Ma43,1959Ma19); direct population of J|p=6+ level of {+110}Cd in {+110}In |e decay (4.92 h) 
T$Weighted average of 4.9 h 2 (ce(t) in 1953Bl44), 4.9 h 1 (|g(t) in 1975Bu24) and 5.0 h 2 (ce(t) in 1951Mc11). Others: 4.9 h (1962Ka08) and 4.9 h (1974Bo61) 
MOMM1$From collinear fast-beam LASER spectroscopy (1985Ul03). Other: 4.719 {I13} from nuclear magnetic resonance on oriented nuclei (1981Ha26), 4.73 {I4} (from 1989Ra17), 4.64 {I35} from nuclear orientation (1977Be19), 5.1 {I3} from nuclear orientation (1976Ha63) 
MOME2$From collinear fast-beam LASER spectroscopy (1985Ul03) 
CONF$|pg{-9/2}~#|nd{-5/2} 
$|d<r{+2}>(115,110)=-0.361 {I5} (1985Ul03). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$J=2 from atomic beam (1968CaZX); direct population of J|p=2+ level of {+110}Cd in {+110}In |e decay (69.1 min); 
T$From |g(t) in 1969Sa20. Others: 66 min {I4} (1975Bu24), 69 min (1974Bo61), 69 min {I2} (1963Ha45), and 66 min (1962Ka08) 
MOMM1$From atomic beam (1968CaZX) 
MOME2$From atomic beam (1968CaZX) 
CONF$|pg{-9/2}~#|nd{-5/2} 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_lifetime_unit: PS
level_comment:
J$From adopted levels, but 2+,3+,4+,5+,6+ in 1989Kr12 
T$Weighted average of T{-1/2}(390|g)=1.0 ps {I+8-3} and T{-1/2}(410|g)=1.0 ps {I+4-2} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: D
level_comment:
Configuration=((p,g9/2,-1) 
J$from atomic beam 
Configuration=((p,g9/2,-1) 
T from values of 2.84 d {I3} (1949He06), 2.81 d {I1} (1957Ma26), 2.84 d {I11} (1968Li08), 2.96 d {I8} (1968Sm08), 2.83 d {I1}(1972Em01), 2.802 d {I1} (1978La21, with quoted uncertainty divided by 3 to convert to 1|s value), 2.8071 d {I15} (1980Ho17), 2.8049 d {I1} (1983Wa26), 2.8048 d {I1} (1986Ru09), and 2.8048 d {I5} (1992Un01). Since the reduced-|h{+2} for the weighted average for this set is 2.45, the data set is not consistent and the Limitation of Relative Statistical Weight, LRSW, method (1985ZiZY,1992Ra08) increases the uncertainty of the 1986Ru08 value from 0.0001 to 0.00033 to reduce its relative weight from 91% to 50%. The weighted average is then 2.8047 with an internal uncertainty of 0.00024, a reduced-|h{+2} of 2.4, and in external uncertainty of 0.00037. This average is adopted along with an uncertainty of 0.0004, which corresponds to the external uncertainty and to that from the modified Bayesian method (1992Ra08). The Normalized Residual method (1992Ja06) and RAJEVAL method (1992Ra08) which adjust the uncertainties of the most discrepant values, those of 1972Em01 and 1978La21, give the same weighted average and uncertainties of 0.0004 and 0.0002, respectively. So, the adopted value does not depend on the analysis method. Other reported values: 2.84 d (1972Gu19) and 2.8048 d {I5} (1982HoZY, replaced by 1992Un01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted av: 7.3 min {I5} (1966Ma39), 8.5 min {I4} (1968Sm08), 7.6 min {I2} (1969Sh11) 
J$M4 |g decay to g.s. and L=1 (d,{+3}He) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
Configuration=|pg{-9/2}{+-1} coupled to 2+ in {+112}Sn 
J$M1+E2 |g to 9/2+, member of g.s. rotational band 
T$from 1991ViZY in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
Configuration=|pg{-9/2}{+-1} coupled to 2+ in {+112}Sn 
J$based on E2 and M1+E2 |g decays to 9/2+ and 11/2+ states, respectively, and excit via (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
Configuration=|pg{-9/2}{+-1} coupled to 4+ in {+112}Sn 
J$based on E2 and M1+E2 |g decays to 11/2+ and 13/2+ states, respectively, and excit via (|a,2n|g) 
T$from 1991ViZY in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
T$from 1991ViZY in (|a,2n|g) 
J$based on E2 and M1+E2 |g decays to 13/2+ and 15/2+ states, respectively, and excit via (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T$weighted av: 14.8 ns {I8} (1980Le05), 13.8 ns {I5} (1978He10), 13.3 ns {I4} (1981Va15) 
J$observed E2 |g-decay only to 17/2+ state and excit via (|a,2n|g) 
MOMM1$other: |m=4.94 {I21} (1981Va15) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted av: 7.6 min {I2} (1969Sh11), 8.5 min {I4} (1968Sm08), 7.3 min {I5} (1966Ma39) 
E$|b{++} unobserved (|<2%) (1966Ma39) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: D
level_comment:
T from 1972Em01. Others: 2.84 d {i3} (1949He06), 2.81 d {i1} (1957Ma26), 2.84 d {i11} (1968Li08), 2.96 d {i8} (1968Sm08) 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: NS
level_comment:
T$weighted av of: 13.8 ns {i5} (1978He10), 14.8 ns {i8} (1980Le05), 13.3 ns {i4} (1981Va15) 
J$g9/2 proton-hole state coupled to two-proton 2d{-5/2},1g{-7/2} configuration associated with 14-ns, 6+ state in {+112}Sn (1978He10) 


level_energy_unit: KEV
level_comment:
J$the 3028 level is given with L=2 by 1988Ta01 but assigned as 1/2+. The L=2 is apparently a misprint. In the authors' Fig. 2, |s(|q) for 3015+3028 (mislabelled as 3028 and 3074) is fitted with L=0. See also Fig. 3 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$from adopted levels 
J from n angular distribution compared with Hauser-Feshbach prediction (1969Ki08) 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)
level_comment:
J$(11/2+,13/2+) suggested in {+111}Sn decay studies. Branching: I|g(1543|g)/I|g(441|g)=9 (1974Ki02), 13 {i4} (1977Za03) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: D
level_comment:
T$from time series measurements in 2016Dz01. Results are consistent with Decay Data Evaluation Project recommended value of 2.8049 d {I4} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
%EC+%B+$From I|b{++}(tot)=24% {I2} in 1983Ry06 and I|b{++}(617.37)/I|b{++}(g.s.)=0.029 (1962Ru05), and by assuming that the I|b{++} feedings to the higher-lying levels are negligible. 
J$L=4 in {+113}In(p,d) (1978EmZT); Direct feeding of 0+ and 2+ states in {+112}Cd following {+112}In |e Decay 
T$weighted average of 14.97 min {I10} (1983Ry06), 14.5 min {I1} (1953Bl44), 14.4 min {I4} (1965Fu07), 15.2 min {I1} (1980Ad04), 14.5 min {I6} (1968Ro03); Other: 13.8 min (1974Ku10) and 14.4 min (1998Ko24) 
MOMM1,MOME2$Using atomic beam magnetic resonance technique in 1968CaZX 
CONF$|p(1g{-9/2}){+-1}~#|n(1g{-7/2}){++1} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1,MOME2$Using colinear fast-beam laser spectroscopy technique in 1987Eb02 
J$L=0 in {+113}In(d,t) (1967Hj03); 156.56|g M3 to 1+ 
T$weighted average of 20.56 min {I6} (1983Ry06), 20.7 min {I3} (1953Bl44), 21.0 min {I5} (1962Ru05), 20.9 min {I2} (1968Ko25), 20.9 min {I1} (1980Ad04); Others: 20.7 min (1974Ku10) and 20.4 min {I4} (1968Ro03) 
CONF$|p(1g{-9/2}){+-1}~#|n(1s{-1/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$L=2 in {+113}In(p,d) (1978EmZT); multiplet member 
T$from 263.01|g-187.93|g(t) in {+109}Ag(|a,n|g) (1976Io04); Other: 2.1 |ms {I2} from 188|g(t) in {+112}Cd(d,2n|g) (1972BrYL) and 1.48 |ms from 187|g(t) in {+112}Cd(d,2n|g) (1973FrYM) differ significantly from adopted value 
MOMM1$+4.73 {I4}, from g=+0.675 {I6} in 1976Io04 
MOME2$1.03 {I3} from TDPAD in {+112}Cd(d,2n|g) (1993Io02); Also from the same group: 0.75 {I15} from PAD in {+109}Ag(|a,n|g)(1981Io07) 
CONF$|p(1g{-9/2}){+-1}~#|n(2d{-5/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$249.68|g M1 to (2)+; L=2+4 in {+113}In(d,t) (1967Hj03); multiplet member 
CONF$|p(1g{-9/2}){+-1}~#|n(1g{-7/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J$399.87|g M1,E2 to (5)+; 406.20|g M1,E2 to 4+; L=2 in {+113}In(p,d) (1978EmZT); Member of the |pg{-9/2}~#|nd{-3/2} multiplet 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J$135.64|g M1 to (3)+, 385.5|g to (2)+, 429.17|g to (5)+; L=(2+4) in {+113}In(d,t) (1967Hj03); member of the |pg{-9/2}~#|ng{-7/2} multiplet 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$388.20|g M1 to (2)+, 594.85|g M1+E2 to 1+; L=2+4 in {+113}In(p,d) (1978EmZT); multiplet member 
CONF$|p(1g{-9/2}){+-1}~#|n(2d{-5/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
J$263.01|g E1+M2 to (7)+; member of the split |pg{-9/2}~#|nh{-11/2} multiplet 
T$from 187.93|g(t) in {+109}Ag(|a,n|g) (1976Io04); 2.81 |ms {I6} in {+112}Cd(p,n|g) (1976Io05); Others: 1.6 |ms {I2} in {+110}Cd(|a,np|g) (1972BrYL) 
MOMM1$+3.08 {I3} (1976Io02) 
MOME2$0.095 {I3} from |g(t,|q) in (1993Io02) 
CONF$|p(1g{-9/2}){+-1}~#|n(1h{-11/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J$573.29|g M1+E2 to 4+, 523.13|g to (2)+; Member of the split |pg{-5/2}~#|ns{-1/2} multiplet; However 4+ can not be excluded; L=2 in {+111}Cd({+3}He,d) (1978EmZT) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$288.81|g M1+E2 to 2+ and 727.16|g to 4+; Member of the split |pg{-9/2}~#|nd{-5/2} multiplet 
CONF$|p(1g{-9/2}){+-1}~#|n(2d{-5/2}){++1} 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$1062.92|g E2 to 1+; 856.22 M1 to (2)+; L=4 in {+111}Cd({+3}He,d) (1978EmZT); However, 1+,(2)+ in {+109}Ag(|a,n|g) and {+112}Cd(p,n|g) (1988Ki04) 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_comment:
J$421.39|g to (3)+; L=2 in {+113}In(d,t) (1967Hj03); possible L=2(+0) doublet in {+113}In(p,d) (1978EmZT) 


level_energy_unit: KEV
level_spin_parity: (0-,1-,2-)
level_comment:
possibly unresolved doublet in {+113}In(d,t) and {+111}Cd({+3}He,d) 
J$293.32|g E2,M1 to (1,2)-; L=1 in {+111}Cd({+3}He,d) (1978EmZT) 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3+)
level_comment:
possibly unresolved doublet in {+113}In(p,d) 
J$L=2(+0) in {+113}In(p,d) (1978EmZT); 149.46|g to 3+ 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: US
level_comment:
J$6+ in 1976Io04 
T$from 263.01|g-187.93|g(t) in 1976Io04 
MOME2$0.75 {I15} from PAD in (1981Io07) 
CONF$|p(1g{-9/2}){+-1}~#|n(2d{-5/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: US
level_comment:
T$from 187.93|g(t) in 1976Io04; Other: 2.8 |ms (1987Iw04), 1.25 |ms (1973FrYM), 1.6 |ms {I2} (1972BrYL) 
MOMM1$+3.08 {I3} from DPAD in 1976Io04 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$2.1 |ms 2 from 188|g(t) in 1972BrYL and 1.48 |ms from 187|g(t) in 1973FrYM differ significantly from the adopted value 
MOME2$1.03 {I3} from TDPAD in 1993Io02 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
T$1.6 |ms 2 from 263|g(t) in 1972BrYL and 1.25 |ms from 263|g(t) in 1973FrYM differ significantly from the adopted value 
MOME2$0.093 {I6} from DPAD analysis in 1976Io02 
CONF$(|pg{-9/2}){+-1}~#(|nh{-11/2}){+n} (1976Io02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
T$weighted mean of 14.97 min {I10} (1983Ry06), 14.5 min {I1} (1953Bl44), 14.4 min {I4} (1965Fu07), 15.2 min {I1} (1980Ad04), 14.5 min {I6} (1968Ro03); Other: 13.8 min (1974Ku10) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 20.56 min {I6} (1983Ry06), 20.7 min {I3} (1953Bl44), 21.0 min {I5} (1962Ru05), 20.9 min {I2} (1968Ko25), 20.9 min {I1} (1980Ad04); Others: 20.7 min (1974Ku10) and 20.4 min {I4} (1968Ro03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: MIN
level_comment:
IR=Y{-m}/Y{-g}=3.9 {I3}, 4.5 {I3} and 4.9 for E(|g)=50, 60, and 70 MeV in 2010Ra01, respectively. Here Y{-m} and Y{-g} are the isomeric and the ground state yields, respectively. Others: 0.77 {I1} for E=16 MeV in 2008Ma25; 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1$|m=+5.5289 (1989Ra17), NMR. 
MOME2$atomic beam. Value includes pol correction. 
J$atomic beam (1976Fu06), L({+3}He,d)=4. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
%IT$K-electron capture <0.0036% (1970De22). 
MOMM1$atomic beam. 
J$atomic beam (1976Fu06), M4 |g to 9/2+ 
T$From weighted average of 99.3 min {I2} (1967Ok02), 99.2 min {I6} (1969Va04), 99.48 min {I3} (1970Go48), 99.48 min {I8} (1970Le07), 99.8 min {I2} (1970Ro29), 99.47 min {I7} (1971Ha18), 99.2 min {I6} (1971Oo01), 99.78 (18) (1971Em01), 102 min {I2} (1975Bu24), 99.21 min {I13} (1982HoZJ), 99.49 min {I6} (1982RuZV), 99.45 min 7 (1984Iw06), and 99.6 min {I3} (1987Ne01). In the Limited Relative Statistical Weight method, the uncertainty for the 1970Go48 value is increased from 0.03 to 0.0316 to reduce its relative weight from 53% to 50%. For either weighting, the results are the same, with the internal uncertainty of 0.022 and the reduced-|h{+2}=1.07. Since these data are consistent, the Rajeval and Normalized Residual methods give the same result. Others: 105 min {I10} (1939Ba03), 104 min {I2} (1940La07), 102 min {I2} (1958Gi06), 114 min (1965Ca13), 102.4 min (1975Ku10), and 99.8 min {I7} (1997We13). 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$|g(|q) of 1509|g in Coul. ex., L(p,t)=2, 7/2+ preferred in analogy with {+115}In 
T$from {+113}In Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_lifetime_unit: PS
level_comment:
J$|g(|q) of 1567|g in Coul. ex., 9/2+ preferred in analogy with {+115}In, L({+3}He,d)=4 
T$from {+113}In Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$L({+3}He,d)=0 
E$probably not the same as 1706.99 level, since E(levels) from ({+3}He,d) in the range 393 to 1567 appear to be about 1-4 keV too high 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_uncertain: ?
level_comment:
E$from (p,t), possibly same as 2104 level, 2120 level (d,d') could also correspond to 2104 or 2116 level, L(p,t)=(3). 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
J$L(|a,t)=5, 11/2- preferred from shell-model syst. 
E$a 2380 level (d,d') could be 2376, 2391, or 2396 level 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T$From weighted average of 99.3 min {I2} (1967Ok02), 99.2 min {I6} (1969Va04), 99.48 min {I3} (1970Go48), 99.48 min {I8} (1970Le07), 99.8 min {I2} (1970Ro29), 99.47 min {I7} (1971Ha18), 99.2 min {I6} (1971Oo01), 99.78 (18) (1971Em01), 102 M 2 (1975Bu24), 99.21 min {I13} (1982HoZJ), 99.49 min {I6} (1982RuZV), 99.45 min 7 (1984Iw06), and 99.6 min {I3} (1987Ne01). In the Limited Relative Statistical Weight method, the uncertainty for the 1970Go48 value is increased from 0.03 to 0.0316 to reduce its relative weight from 53% to 50%. For either weighting, the results are the same, with the internal uncertainty of 0.022 and the reduced-|h{+2}=1.07. Since these data are consistent, the Rajeval and Normalized Residual methods give the same result. Others: 105 min {I10} (1939Ba03), 104 min {I2} (1940La07), 102 min {I2} (1958Gi06), 114 min (1965Ca13), 102.4 min (1975Ku10), and 99.8 min {I7} (1997We13). 
$From the presence of Cd K x rays from a {+113}In (99 min) source, 1970Ra05 (and 1969RaZP) reported |e decay of this level with I(|e)=0.07% {I1}. Such a transition to {+113}Cd would be 1st forbidden, 1/2- to 1/2+, and would have a log| {Ift} of 5.1. This |e intensity is unlikely since the log| {Ift} systematics (1973Ra10) indicate that such transitions have log| {Ift}'s of >5.9. Also, 1970De22 (see also 1969De25) repeated the experiment and placed a limit of <0.0036% on this |e transition for which the log| {Ift} is >6.5. Such an electron capture branch is therefore negligible and has not been included in this scheme. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$x,|g(|q) gives 9/2+ or 13/2+. T{-1/2}(DSA) and B(E2) not mutually consistent with 9/2+ 
T$from B(E2). 0.28 ps {I7} from DSA. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (19/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Tentative 457|g and 378-572 |g cascade from this level; and other possible feeding |g rays to lower levels 


level_energy_unit: KEV
level_spin_parity: (29/2-)
level_comment:
E$populated from decay out of band 6 through 297|g and 388|g. May feed 3279 keV as shown by 1997VaZS 


level_energy_unit: KEV
level_comment:
MOMM1,MOME2$derived from measured hyperfine-structure constants A{-hf} and B{-hf} using collinear laser spectroscopy and calculated A{-hf}/g=+1847 MHz {I20} and B{-hf}/Q=+576 MHz/b {I4} using the Coupled-Cluster Singles Doubles method (CCSD) (2018Ga36) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
$ Configuration=|pg{-9/2}~#|ng{-7/2} 
J$log| {Ift}=4.5 to 0+ {+114}Sn 
T$from 1968Ko25. Others: 1937La05, 1956Br87, 1956Gr35 
%B-$I|b{++} is from 1956Gr35 and |e/|b{++}=142 from theory. Note that 1956Gr35 deduce I|e|?1.9% 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
T$from 1972Me01. Others: 1939Ba03, 1940La07, 1949Bo52, 1949Ma38, 1957Wr37, 1959Ca12 
J$atomic beam (1969Fu11), E4 |g to 1+ 
%IT$from I|g(190|g)=15.56% {I15} (1994Co02. Value revised in Priv. Comm. from F. Schima, May 1995), I|g(725|g)/I|g(190|g)=0.209 {I15} and the requirement that %IT+%(|e+|b{++})=100. The I|g ratio is an unweighted average of 0.150 {I20} (1949Bo52), 0.211 {I15}, 0.211 {I15} (1967Ro22), 0.189, 0.185 (1952Jo22), 0.268, 0.250 (1957Go82). The two sets of values are from separate measurements of I|g(725|g) and I|g(558|g), with the assumption of negligible feeding of the 558 level from the {+114}In g.s. via IT decay 
$ Configuration=|pg{-9/2}~#|ns{-1/2} 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
$ Configuration=|pg{-9/2}~#|nh{-11/2} 
J$E3 |g to 5+ 
T weighted average: 43.5 ms {I10} (1968Ko25), 43.5 ms {I20} (1966MoZZ), 42 ms {I2} (1968Al08), 39.4 ms (1967Iv04), 42 ms {I5} (1958Du80), 41.8 ms {I14} (1960Mo19), 46.5 ms {I20} (1966Me02), 42 ms {I2} (1959Gl56) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$ Configuration=|pg{-9/2}~#|ng{-7/2}+|pg{-9/2}~#|nd{-3/2} 
J$M1 |g to 3+ and E2 |g to 2+, L(n)=(4) (d,p) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
T weighted average: 43.5 ms {I10} (1968Ko25), 43.5 ms {I20} (1966MoZZ), 42 ms {I2} (1968Al08), 39.4 ms (1967Iv04), 42 ms {I5} (1958Du80), 41.8 ms {I14} (1960Mo19), 46.5 ms {I20} (1966Me02), 42 ms {I2} (1959Gl56) 


level_energy_unit: KEV
level_spin_parity: 5+&8-
level_comment:
E$unresolved doublet of 497.2, 5+ and 501.9, 8- states. 
$E=497.20 {I8}, L=2, S=0.85; E=502.02 {I25}, L=5, S=2.32 (1974GlZO). 
$ Configuration=|pg{-9/2}~#|nd{-3/2} for 5+ and |pg{-9/2}~#|nh{-11/2} for 8- 
J$in Table 4 of 2002SaZO negative parity of 497.2 level is a misprint 


level_energy_unit: KEV
level_spin_parity: 9-&7+
level_comment:
E$unresolved doublet of 639.9, 9- and 641.7, 7+ states. 
$E=640.90 {I9}, L=5, S=1.87; E=641.7, L=2, S=0.13 (1974GlZO) 
$ Configuration=|pg{-9/2}~#|nh{-11/2} for 9- state and |pg{-9/2}~#|nd{-5/2} for 7+ state 
J$in Table 4 of 2002SaZO negative parity of 641.7 level is a misprint 


level_energy_unit: KEV
level_spin_parity: 8+&5-
level_comment:
E$unresolved doublet of 687.5, 8+ and 696.4, 5- states. 
$E=687.59 {I15}, L=4, S=0.58; E=696.35 {I13}, L=5, S=1.91 (1974GlZO) 
$ Configuration=|pg{-9/2}~#|ng{-7/2} for 8+ and |pg{-9/2}~#|nh{-11/2} for 5- 
J$in Table 4 of 2002SaZO negative parity of 687.5 level is a misprint 


level_energy_unit: KEV
level_spin_parity: 3+&4+
level_comment:
E$unresolved doublet of 725.1, 3+ and 728.5, 4+ states. 
$E=725.28 {I17}, L=2+0, S=0.83; E=728.55 {I14}, L=2+0, S=0.83+0.11 (1974GlZO) 
$ Configuration=|pg{-9/2}~#|nd{-3/2} for 3+ and |pg{-9/2}~#|nd{-3/2}+|pg{-9/2}~#|ns{-1/2} for 4+ 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$E=775.66 {I21}, L=4+2, S=0.75+0.14 (1974GlZO) 
$ Configuration=|pg{-9/2}~#|ng{-7/2}+|pg{-9/2}~#|nd{-3/2} 


level_energy_unit: KEV
level_spin_parity: 2+&4-
level_comment:
E$unresolved doublet of 825, 2+ and 835.7, 4- states. 
$E=825.23 {I14}, L=2, S=0.20; E=835.80 {I17}, L=5, S=1.72 (1974GlZO) 
$ Configuration=|pg{-9/2}~#|nd{-5/2} for 2+ and |pg{-9/2}~#|nh{-11/2} for 4- 
J$in Table 4 of 2002SaZO negative parity of 825 level is a misprint 


level_energy_unit: KEV
level_spin_parity: 3-&6+
level_comment:
E$unresolved doublet of 1032, 3- and 1044.9, 6+ states. 
$ Configuration=|pg{-9/2}~#|nh{-11/2} for 3- and |pg{-9/2}~#|nd{-5/2} for 6+ 


level_energy_unit: KEV
level_spin_parity: 5+&8-
level_comment:
E$unresolved doublet of 497.2, 5+ and 501.9, 8- states. 
$Configuration=|pg{-9/2}~#|nd{-3/2} for 5+, and |pg{-9/2}~#|nh{-11/2} for 8- 
J$in Table 4 of 2002SaZO, negative parity of 497.2 level is a misprint 


level_energy_unit: KEV
level_spin_parity: 8+&5-
level_comment:
E$unresolved doublet of 687.5, 8+ and 696.4, 5- states. 
$Configuration=|pg{-9/2}~#|ng{-7/2} for 8+ and |pg{-9/2}~#|nh{-11/2} for 5- 
J$in Table 4 of 2002SaZO, negative parity of 687.5 level is a misprint 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: Y
level_comment:
MOME2$others: +0.810, 0.79 {I20}, 0.83 {I10}, 0.58 {I9}, all from (1989Ra17) 
J$L=4 ({+3}He,d),(d,{+3}He),(p,|a), M4 |g from 1/2- 
T$from measured |b spectrum of scin solution spiked with indium salt (1978Pf01,1979Pf01). Others: 5.1|*10{+14} y {I4} (1962Wa15), 6.9|*10{+14} y 15 (1961Be15), 6|*10{+14} y {I2} (1950Ma76), |?1|*10{+14} y (1951Co19) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
J$atomic beam (1961Ki02), L=1 ({+3}He,d),(d,{+3}He),(p,|a) 
T$from (1974Ha39), agrees with 4.485 h {I4} (1987Ne01) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T$from |b|g(t), |g|g(t) (1967Na04) 
J$M1+E2 decay to 1/2- state, |b|g(|q) 
$L=1 ({+3}He,d),(d,{+3}He),(p,|a) 
$B(E3)=0.0057 {I4} Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
$Analog: 660-keV {+117}In 3/2+ state; |m=+0.938, Q=-0.64 
T$from 1971Sv01, |b|g(t) scin-semi. Others: 5.73 ns {I7}, 6.09 ns {I10} via alternate data analyses 
J$E1 |g to 1/2- from 828, M1(+E2) |g to 9/2+ from 934 and E2 |g connecting 934 and 828 uniquely establish J|p(828)=3/2+ and J|p(934)=7/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$av: 1.12 ps {I17} res fluorescence (1981Ca10), 0.86 ps {I5} (1976Tu02) from B(E2)=0.0227 and I|g(1078|g)-branching=83.7% 
J$L=2 (p,|a); E2 to 9/2+ 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$average of 0.064 ps {I4} (1977Ca14) and 0.065 ps {I3} (1975Bo40) res fluorescence. 
J$L=6 (p,|a); M1+E2 decay to 9/2+ g.s. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T$average of 0.46 ps {I4} (1981Ca10) res fluorescence, 0.38 ps {I3} from B(E2)=0.0565 and I|g(1291|g)-branching=97.6% 
J$L=6 (p,|a). Adopted T{-1/2} inconsistent with measured B(E2) if J=11/2 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
E$from band assignment 
J$|g to 5/2+ not consistent with 11/2+; (484|g)(934|g)(|q) is consistent with J(initial)=9/2 (1975Bo29) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T$average of 0.066 {I8} (1977Ca14) and 0.059 ps {I15} (1973Bo17) res fluorescence 
J$M1+E2 decays to 5/2+,9/2+ states, Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$from 1981Ca10. Other: 0.52 ps {I22} (1973Bo17) res fluorescence 
J$L=4 (p,|a), M1+E2 decay to 11/2+ state, Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
J$L=1 (d,{+3}He),(p,|a). L=2 ({+3}He,d) could be a separate level. It is not adopted since those results are as yet unpublished 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$from |b|g(t) (1971Sv01). Others: 5.99 ns {I3} (1967Na04), 5.65 ns {I15} (1967Mc13), 6.00 ns {I12} (1967Hr02), 5.6 ns {I1} (1967Be57), 5.4 ns {I2} (1967Ba18), 5.5 ns {I2} (1964Ta09), 5.9 ns {I3} (1960Go21) 
$g factor=+0.50 {I8} if T{-1/2}=5.78 ns (1974Ba24) (35|g)(492|g)(|q,H) 
$Deduced electric quadrupole interaction (1976Lu06,1973RaZG) |b|g(|q,H,t) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$from |b|g(t) (1971Sv01). Others: 1.15 ns {I4} (1967Na04), 0.95 ns {I3} (1967Mc13), 1.13 ns {I6} (1967Hr02), 1.52 ns {I8} (1967Be57), 1.1 ns {I1} (1967Ba18) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_uncertain: ?
level_comment:
$Level added in this update. Population of this level in this decay is tentative, although, definite in Coulomb excitation, (|g,|g'); (n,n'|g) and (d,d'). See Adopted Levels for details. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T from (484|g)(934|g)(t) scin (1973Se06). Other: |<130 ps (1967Mc13) 
Branching: I|g(105|g)/I|g(934|g)=0.0022 {I1} (1978He08), 0.0024 {I4} (1973Se06), 0.0023 {I4} (1973Is03) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
Branching: I|g(477|g):I|g(484|g):I|g(1418|g)=0.034 {I7}:100:0.63 {I3} (1978He08), 0.06 {I3}:100:0.61 {I7} (1973Se06) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
Branching: I|g(1449|g):I|g(515|g):I|g(507|g):I|g(316|g)=100:0 \.6 {I2}:1.5 {I1}:14.6 {I6} (1978He08), 100:--:2.4 {I13}:18 {I3} (1973Se06) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T 4.486 h {I4} (1974Ha39) av: 4.485 h {I3} scin, 4.485 h {I2} scin, 4.487 h {I3} semi, 4.491 h {I4} 4|p|b pc. Others: 4.34 h (1975Ku10), 4.5 h {I1} (1975Bu24), 4.20 h {I7} (1973Fo15), 4.49 h {I8} (1972Pa13), 4.8 h (1968Bo28), 4.48 h (1965Sa09), 4.50 h {I2} (1947Du03), 4.53 h (1940La07) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=0.42 {I15} 
T$from 1981Ca10. Others: 1.1 ps {I2} (1977Ca14), 0.47 ps (1971Bo46), 0.64 ps {I13} (1969Al19) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=9.4 {I7} 
T$0.065 ps {I3} (1975Bo40). Others: 0.064 ps {I4} (1977Ca14), 0.072 ps {I7} (1973Bo17), 0.075 ps {I10} (1969Al19) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=1.2 {I3} 
T from 1981Ca10. Others: 0.46 ps {I4} (1977Ca14), 0.48 ps {I22} (1973Bo17), |?0.45 ps (1969Al19) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=1.7 {I4} 
T from 1981Ca10. Others: 0.50 ps {I21} (1973Bo17); |?0.35 ps (1969Al19) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=4.0 {I6} 
T$average of 0.066 {I8} (1981Ca10), 0.059 ps {I15} (1973Bo17) res fluorescence 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=0.49 {I18} 
T$from 1981Ca10. 1981Ca10 report g|G{+2}{-|g0}/|G=1.33 MeV {I16}. For J=7/2 and adopted g.s. branching=0.781. T{-1/2}=0.17 ps {I2} 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_comment:
$g|G{+2}{-|g0}/|G (MeV)=1.0 {I3} 
T$from 1981Ca10. 1981Ca10 report g|G{+2}{-|g0}/|G=1.54 MeV {I24}. For J=7/2 and adopted g.s. branching=0.690. T{-1/2}=0.11 ps {I2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
E probably corresponds with 1040-keV L=3 (d,{+3}He) state (see 1974He11) 
Branching: I|g(444|g)/I|g(705|g)=0.14 (1978VaZW,1976AvZV) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.00272, I|g(941|g)-branching=89.8%. Other: |>3.5 ps (1976Tu02) Doppler-line shape 
Branching: I|g(345|g)/I|g(942|g)=0.114 {I7} (1976Tu02), 0.15 (1970Di11) 
B(E2)=0.00272 {I18} (1976Tu02). Others: 0.0027 {I3} (1970Di11), 0.0023 {I8} (1970Be02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T 0.86 ps {I5} from B(E2)=0.0227, I|g(1078|g)-branching=83.7%. Others: 0.80 ps {I14} (1974Er06) DSA, 0.90 ps {I14} (1976Tu02) Doppler-line shape, 1.1 ps {I2} (1977Ca14) res fluorescence 
Branching: I|g(136|g)/I|g(480|g)/I|g(1078|g)=1.2 {I2}:18.7 {I3}:100 (1976Tu02), --:23:100 (1970Di11) 
B(E2)=0.0227 {I12} (1976Tu02). Others: 0.0220 {I20} (1970Di11), 0.0151 {I20} (1970Be02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T res fluorescence: 0.065 ps {I3} (1975Bo40), 0.064 ps {I4} (1977Ca14), 0.072 ps {I7} (1973Bo17), 0.075 ps {I10} (1969Al19). Others: 0.07 ps {I4} (1976Tu02) Doppler-line shape, 0.042 ps {I14} (1974Er06) DSA, 0.075 ps {I9} from B(E2)=0.100, |d(1132|g)=+0.51 
B(E2)=0.100 {I5} (1976Tu02). Others: 0.100 {I11} (1970Di11), 0.108 {I12} (1970Be02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T$0.38 ps {I3} from B(E2)=0.0565, I|g(1291|g)-branching=97.6%. Others: 0.31 ps {I7} (1974Er06) DSA, 0.38 ps {I7} (1976Tu02) Doppler-line shape, 0.46 ps {I4} (1977Ca14) res fluorescence 
Branching: I|g(158|g):I|g(1290|g)=0.0246 {I6} (1976Tu02), 0.0217 (1970Di11) 
B(E2)=0.0565 {I30} (1976Tu02). Others: 0.050 {I5} (1970Di11), 0.060 {I9} (1970Be02) 


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 0.10 ps {I+4-4} (1976Tu02) Doppler-line shape, 0.49 ps {I3} from B(E2)=0.0151, I|g(1449|g)-branching=86%, |d(1449|g)|?-8 
Branching: I|g(316|g):I|g(1449|g)=0.163 {I6} (1976Tu02), |?0.21 (1970Di11) 
B(E2)=0.0151 {I10} (1976Tu02). Other: 0.0124 {I20} (1970Di11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
Branching: I|g(386|g):I|g(1463|g)=0.062 {I5} (1976Tu02), 0.067 (1970Di11) 
B(E2)=0.0096 {I13} (1976Tu02). Other: 0.0124 {I30} (1970Di11) 


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 0.21 ps {I14} (1976Tu02) Doppler-line shape, 0.33 ps {I3} from B(E2)=0.0087, I|g(1486|g)-branching=78.7%, |d(1486|g)|?-0.95 
Branching: I|g(353|g):I|g(544|g):I|g(1486|g)=22.4 {I18}:4.7 {I8}:100 (1976Tu02), 35:--:100 (1970Di11) 
B(E2)=0.0087 {I9} (1976Tu02). Other: 0.0060 {I15} (1970Di11) 


level_energy_unit: KEV
level_comment:
J tentative J=9/2 from angular distribution shape; incompatible with L=1 (d,{+3}He) state at 2450 keV 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
T$from 1963Be23. Others: 13 s (1935Am01,1937La05), 12.5 s {I20} (1953Wi42), 14.5 s {I4} (1957Ca71), 15.9 s {I28} (1958Gu09), 13.4 s {I4} (1960Do02), 14.05 s {I26} (1960Du04), 15.6 s {I5} (1965Br34) 
J$log| {Ift}=4.7 to 0+ level 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 54.31 min {I7} (1945Ru02), 54.05 min {I16} (1947Gr16), 53.93 min {I13} (1949Si02), 54.14 min {I7} (1953Do09), 53.99 min {I6} (1953Lo09), 55.13 min {I27} (1957Ca71), 54.12 min {I5} (1963Be23), 56.6 min {I11} (1965Br34), 55.3 min 4 (1972Pa13), 54.34 min {I9} (1972Em01), 55.77 {I10} (1986Ne01), agrees with the new value 54.20 {I7} (2006Vo12) 
J$atomic beam (1976Fu06), M1 |g from 4+ 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
J$E3 |g to 5+ 
T$weighted average: 2.46 s {I8} (1960Al27), 2.17 s {I7} (1961He08), 2.3 s {I3} (1962Wh02), 2.16 s {I2} (1963Al32). Other: 2.5 s (1950Ca72) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
$B(Gt) from {+116}In |b{+-} decay 
$d|s/d|W(|DL=0,q=0)=62 |mb/sr {i12}; d|s/d|W(|q{-min})=58 |mb/sr {i12} 


level_energy_unit: KEV
level_comment:
E$listed as 1200-2000 by 2005Ra13 
$d|s/d|W(|DL=0,q=0)=90 |mb/sr {i18}; d|s/d|W(|q{-min})=90 |mb/sr {i18} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
MOMM1,MOME2$From 2005St24,collinear fast beam LASER spect.(1987Eb02) 
T$weighted av: 43.1 min {i2} (1982Fu07), 42 min {i2} (1975Bu24), 42.3 min {i13} (1972Pa13), 40 min {i2} (1967Sc37), 44.6 min {i6} (1963Ne04), 43 min {i4} (1961Wo07). Others: 1953Co04, 1955Mc17 
J$atomic beam (1976Fu06), L=4 in {+116}Cd({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$atomic beam (1962Ca14) 
T$weighted av: 116.1 min {i2} (1982Fu07), 117 min {i2} (1975Bu24), 114 min {i3} (1972Pa13), 117 min {i2} (1967Sc37), 117.5 min {i10} (1963Ne04), 115.7 min {i10} (1965Br34), 116 min {i3} (1961Du07). Others: 1940La07, 1955Mc17 
J$atomic beam (1976Fu06), L=1 in {+116}Cd({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
MOMM1$ipad (1986Bo36) 
E$1985Al05 suggest that the level could be the first rotational state built up on the single proton [301] 1/2- Nilsson orbital in a strongly deformed core of prolate shape 
T$av: from 0.20 ns {i5} (1968Be58), 0.17 ns {i3} (1968Ch08), {0.20 ns {i2}} (1967Ba18) 
J$L=1 in {+116}Cd({+3}He,d), not 1/2 from |g|g(|q) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$weighted av.: 55.0 ns {i20} (1968Be58), 59.7 ns {i20} (1968Ch08), 58.7 ns {i20} (1967Ba18), 53.3 ns {i3} (1976Pi18), Other: 53.5 ns (1972Ra27) 
MOMM1,MOME2$DPAD (1976Pi18) 
J$L=2 in {+116}Cd({+3}He,d), not 5/2 from |g|g(|q) (1979Gl09) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$L=0+4 for 748+749 levels in {+116}Cd({+3}He,d), not 1/2+ from |g decay to g.s., C{+2}S' favors 7/2+, |g feeding from (3/2+) and (9/2-) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$from 4.82 ns {i10} (1968Be58), 4.55 ns {i32} (1968Ch08), { 4.3 ns {i2}} (1967Ba18), 4.9 ns {i2} (1966Pa07) 
J$L=0+4 for 748+749 levels in {+116}Cd({+3}He,d), not 7/2+ or 9/2+ from |g decay (1979Gl09) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$|g from 1028 to 1/2-, log| {Ift}(1957)=7 from (11/2) and |g from 1957 to 1028 give J|p(1028)=(5/2-) and J|p(1957)=(9/2-) 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2,9/2+
level_comment:
J$|g to 1/2+ from 2112, |g to 9/2+ from 1468 and |g from 2112 to 1468 establishes J|p(2112)=1/2+,3/2,5/2+ and J|p(1468)=5/2+,7/2,9/2+. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J log| {Ift}=4.7 to 0+, log| {Ift}=5.5 to 2+ 
T$from 1964Ka10, 1968Sc24. Others: 5.1 s {I5} (1961Gl02), 5.7 s {I3} (1965Br34) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 5+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1,MOME2$collinear fast-beam LASER spectroscopy (1989Ra17); |m value relative to |m=+5.5408 {I2} for {+115}In (9/2+ g.s.), Q value relative to Q=+0.81 for {+115}In (9/2+ g.s.) and includes the Sternheimer correction (1989Ra17) 
J atomic beam (1984Be40) 
T from 1969Do11. Others: 4.35 min {I5} (1964Ka10), 4.9 min {I1} (1965Br34), 4.7 min {I3} (1965Me11), 4.4 min {I1} (1968Sc24) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 8-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
%B-,%IT From {+118}In |b{+-} decay (8.5 s) 
MOMM1,MOME2$collinear fast-beam LASER spectroscopy (1989Ra17); |m value relative to |m=+5.5408 {I2} for {+115}In (9/2+ g.s.), Q value relative to Q=+0.81 for {+115}In (9/2+ g.s.) and includes the Sternheimer correction (1989Ra17) 
J atomic beam (1984Be40) 
T from 1969Ha08 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MIN
level_comment:
J atomic-beam magnetic resonance (1984Be40); L(d,{+3}He)=4 
MOMM1,MOME2$collinear fast-beam LASER spectroscopy (2005St24); |m value relative to |m=+5.5408 {I2} for {+115}In (9/2+ g.s.), Q value relative to Q=0.81 for {+115}In (9/2+ g.s.) and includes the Sternheimer correction (2005St24) 
T from |b(t) in {+119}In |b{+-} decay (1976Sc30) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T from |b(t) (1976Sc30). Other: 18.0 min {I5} from |g(t) (1973Ra17). 
J atomic-beam magnetic resonance (1984Be40); L(d,{+3}He)=1 
MOMM1$collinear fast-beam LASER spectroscopy (2005St24); |m value relative to |m=+5.5408 {I2} for {+115}In (9/2+) (2005St24) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: NS
level_comment:
J E1 |g ray to 1/2- 
MOMM1,MOME2$differential perturbed angular distribution of |g's following reactions (2005St24); |m value is that from original authors (2005St24). Q value relative to Q=+0.810 for {+115}In (9/2+ g.s.) 
T from |g|g(t) in {+119}Cd |b{+-} decay (2.69 min) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J |g ray to 9/2+, |g ray to (11/2+) 
E a level at 1203.7 was observed weakly populated in the (d,{+3}He) reaction with L=3. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J log| {Ift}=7.4 from (11/2-) and |g ray to 5/2+ allows (7/2-,9/2+), log| {If{+1u}t}=8.3 from (11/2-) rules out (7/2-) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J log| {Ift}=5.2 from (11/2-), |g ray to (13/2+), |g ray to (9/2-,11/2-). 
J$Previous assignment (9/2-,11/2-) was wrong. G ray to 7/2- also wrong 


level_energy_unit: KEV
level_spin_parity: (9/2,11/2)
level_comment:
J log| {Ift}=5.2 from (11/2-), |g ray to 9/2+, |g ray to (13/2+). 
J$Previous assignment (9/2-,11/2-) is wrong. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J log| {Ift}=5.3 from (11/2-), |g rays to (7/2+), 9/2+, and (11/2+). 
J$Previous assignment (9/2-, 11/2-) is wrong. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J log| {Ift}=5.7 from (11/2-), |g rays to (11/2-) and (13/2+). 
J$Previous assignment was (9/2-,11/2-). G ray to 7/2- is wrong. 


level_energy_unit: KEV
level_spin_parity: (9/2,11/2)
level_comment:
J log| {Ift}=5.5 from (11/2-), |g ray to 7/2+,9/2+. 
J$Previous assignment was (9/2-,11/2-). G ray to 7/2- is wrong. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E unresolved peak consisting of known levels at 1044 and 1050 (1989La21). Authors suggested that the peak could also contain the known 1025 level 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
T$non-observation of 60|g and 64|g suggests a lifetime for this state, which is estimated to be 3 ns<T{-1/2}<10 ns from measured T{-1/2}(2656 level)=304 ns {I10} gating on 928|g+1204|g and 270 ns {I11} gating on 152|g (2020Bi06) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J log| {Ift}=5.02 to 0+ 
T from weighted av of 3.0 s {I8} (1960Po06), 3.2 s {I4} (1964Ka10), 2.87 s {I5} (1970OsZZ), and 3.08 s {I8} (1973Sc19) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$300 {I200} is suggested in 1997Au04 as a value from systematics 
J from log| {Ift}=4.68 to (7-,8-) and syst of low-lying 8- states in even-A indium isotopes 
T other: 50 s {I1} (1960Po06) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$mass excess=-85709.1 {I31} (2023Ne13) 
E,J$assignment of 1+ to the ground state is based on 5.5 to 1 ratio of isomer to ground state population following proton induced fission. 


level_energy_unit: KEV
level_spin_parity: 5+,8+
level_comment:
E$from difference in mass excess. The 5+ and 8+ isomers could not be resolved and based on the spot width the energy difference between the two isomers was estimated as <15 keV (2023Ne13). 
$mass excess=-85619.0 {I16} (2023Ne13), uncertainty is statistical only. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_comment:
J from on-line atomic beam magnetic resonance (1984Be40) and L=4 in (d,{+3}He) and (p,|a) 
T from 1974Gr29. Others: 30 s {I3} (1960Yu01), 29 s {I8} (1963Wa30), 30.0 s {I2} (1974Sc05) 
MOMM1$from 2005St24; value relative to |m=+5.5408 {I2} for {+115}In. 
MOME2$from 2005St24; Sternheimer correction or other correction included 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E$from weighted average from decay (13.5 s, 3.88 m) 
%|b{+-}, %IT from 1976Fo02 
J from on-line atomic beam magnetic resonance (1984Be40) and L=1 in (d,{+3}He), (p,|a). 
T from 1974Gr29. Others: 3.1 min {I3} (1960Yu01), 3.3 min {I10} (1963Wa30), 3.1 min {I4} (1965We04) 
MOMM1$from 2005St24; value relative to |m=+5.5408 {I2} for {+115}In. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
J log| {Ift}=6.3 from (3/2+); systematics suggest (3/2+) in odd indium isotopes 
T from |b |g(t) in {+121}Cd |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J |g to 3/2-, (3/2+); systematics of odd mass indium suggests 1/2+ 
T from |b|g(t) in {+121}Cd |b{+-} decay 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (17/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$systematics of high spin states of odd mass indium 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (19/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$non-observation of 953|g and 1181|g in prompt |g|g-coin with sum gate on 110|g, 169|g and 361|g, and observation of the two gammas in delayed spectra suggest this state has a short half-life, which below the sensitivity of the present setup (2020Bi06) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (25/2+)
level_lifetime_unit: US
level_comment:
T$from 99|g(t). Others: 7.5 |ms {I2} from 214|g(t), 7.0 |ms {I2} from 953|g(t), 7.2 |ms {I2} from 1181|g(t) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
Nuclear rms charge radius=4.6557 fm {I50} (2004An14) 
J log {Ift}=5.1 to 0+ 
T from |g-multiscaler counting (1971Ta07) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1$from collinear fast-beam laser spectroscopy (1987Eb02,2005St24) 
MOME2$from collinear fast-beam laser spectroscopy and includes the Sternheimer correction (1987Eb02,2005St24) 
No significant IT decay branching is expected because of |DJ=4 for E(IT)=40 keV 
E $Q{-|b} systematics: E(5+)-E(1+)=40 keV 60 in NUBASE (2003Au02) 
J from collinear fast-beam laser spectroscopy (1987Eb02); |p=+ from log {Ift}=4.9 to 4+ 
T from |g-multiscaler counting (1979Ch10) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
MOMM1$from collinear fast-beam laser spectroscopy (1987Eb02,2005St24) 
MOME2$from collinear fast-beam laser spectroscopy and includes the Sternheimer correction (1987Eb02,2005St24) 
E $Q{-|b} systematics: E(8-)-E(1+)=290 keV {I140} in NUBASE (2003Au02) 
J$From collinear fast-beam laser spectroscopy (1987Eb02,2005St24); systematics of (8)- isomers in {+120-128}In (1979Fo10) 
T from |g-multiscaler counting (1979Ch10) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_lifetime_unit: S
level_comment:
E,T$From the Adopted Levels for {+122}In in the ENSDF database. 
J$other: (8-) in the Adopted Levels for {+122}In in the ENSDF database. 2016Re03 suggest (9-) based on shell model calculations and observed staggering in B(M1)/B(E2) ratios. 


level_energy_unit: KEV
level_spin_parity: 5+,8-
level_comment:
$mass excess=-83550.7 {I12} (2023Ne13), uncertainty is statistical only. 
E$doublet consisting of 5+ and 8- levels which 2023Ne13 deduce are separated by < 15 keV. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$mass excess=-83473.45 {I92} (2023Ne13) 
E$from difference in mass excess. Note that this value is the energy difference between the 1+ and the 8- and 5- states. 
E,J$assignment of 1+ to the isomer is based on 1 : 20 ratio of isomer to ground state population following proton induced fission. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_comment:
J$L(d,{+3}He)=L(t,|a)=4 from 0+; spin=9/2 from collinear laser spectroscopy (1987Eb02) 
T$unweighted average of 5.98 s {I6} (1974Gr29), 6.68 s {I20} (1986Go10), and 5.8 s {I2} (2011Hi15). 
MOMM1,MOME2$from collinear fast beam laser spectroscopy, relative to {+115}In (1987Eb02). Quoted value of Q is from the original Q=+0.757 {I9} relative to Q({+115}In)=0.81 used in 1987Eb02, scaled using the adopted Q({+115}In)=0.770 {I8} (2008Py02). See also 2014StZZ and 2016St14 compilations 
$Nuclear rms charge radius=4.6594 fm {I56} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(d,{+3}He)=L(t,|a)=1 from 0+; spin=1/2 from collinear laser spectroscopy (1987Eb02) 
T$weighted average of 47.8 s {I5} (1974Gr29), 45.9 s {I10} (1986Go10) using |b counting. Other: 36 s {I3} (1960Yu01) seems discrepant 
MOMM1$from collinear fast beam laser spectroscopy, relative to {+115}In (1987Eb02). See also 2014StZZ compilation 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$L(d,{+3}He)=L(t,|a)=1 from 0+; spin=3/2 from systematics of neighboring odd-mass In isotopes; 371.3|g M1 to 1/2- 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J$1027.5|g to 9/2+; possible |b-feeding (log {Ift}=6.2) from 11/2(-) parent; 11/2+ is favored from systematics of neighboring odd-mass In isotopes 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J$438.7|g to (3/2)-, 810.3|g to 1/2-, 883.0|g from (7/2-); possible |b-feeding (log {Ift}=6.0) from 3/2(+) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$1165.9|g to 9/2+; possible |b-feeding (log {Ift}=6.2) from 11/2(-); 13/2+ is favored from systematics of neighboring odd-mass In isotopes 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$1566.1|g to 9/2+, 454.3|g from (7/2-), 827.2|g from (5/2+); possible |b-feeding (log {Ift}=6.4) from 11/2(-) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$2020.7|g to 9/2+, 334.0|g from (11/2-), 480.3|g from (9/2-,11/2-), possible |b-feeding from 3/2(+) suggest (7/2-). But log {Ift}=6.2 from 3/2(+) would suggest (5/2+), which cannot be completely ruled out. It could be that the |b-feeding to this level is overestimated probably due to unobserved or unplaced |g feedings to this level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (21/2-)
level_lifetime_unit: US
level_lifetime_info: ;ERR=GE;ISO=M3
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$this isomer is proposed by 2010Re01 based on their observation of delayed |g transitions seen in the decay of the 1.4-|ms isomer in 2004Sc42, which however is less likely originated from the relatively short-lived 1.4-|ms isomer due to the particle-|g correlation time from 5 to 175 |ms in their setup, but is likely from a longer-lived isomer above the 1.4-|ms isomer to further delay the decays as observed. 
J,T$from 2010Re01 in ({+6}Li,F|g), with the half-life limit suggested from intensity in time spectra. 
$This isomer is suggested to arise from |n(h{-11/2}~#d{-3/2})7{+-} and |n(h{-11/2}~#s{-1/2})5{+-} neutron core excitation coupling with the valence proton (2010Re01) 


level_energy_unit: KEV
level_spin_parity: (11/2-,13/2-)
level_comment:
J$1143.8|g to (13/2+), 1282.2|g to (11/2+); possible allowed |b-feeding (log {Ift}=5.3) from 11/2(-) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$2393.5|g to 9/2+, 1694.8|g to (3/2)-, 256.7|g to (1/2+,3/2+); possible allowed |b-feeding (log {Ift}=4.7) from 3/2(+). 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$the simultaneous feeding of the 11/2+ and 13/2+ levels at 1027.5 and 1165.9, respectively, (and no feeding to 9/2+ g.s. and 11/2+ level at 1027.5), suggests a spin and parity assignment 13/2- or 15/2+ for this level. The negative parity assignment is preferred by analogy with the heavier In isotopes, but a positive parity cannot be completely ruled out (2004Sc42). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$proposed by 2004Sc42 based on 31.5|g probably (E2) to (13/2-) 
T$from 880.7|g(t)+1166.0|g(t) (2004Sc42) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (21/2-)
level_lifetime_unit: US
level_lifetime_info: ;ERR=GE;ISO=M2
level_comment:
E$this isomer is proposed by 2010Re01 based on their observation of delayed |g transitions seen in the decay of the 1.4-|ms isomer in 2004Sc42, which however less likely originates from the relatively short-lived 1.4-|ms isomer due to the particle-|g correlation time from 5 to 175 |ms in their setup, but is likely from a longer-lived isomer above the 1.4-|ms isomer to further delay the decays as observed. 
J,T$from 2010Re01, with the half-life limit suggested from intensity in time spectra. 
$This isomer is suggested to arise from |n(h{-11/2}~#d{-3/2})7{+-} and |n(h{-11/2}~#s{-1/2})5{+-} neutron core excitation coupling with the valence proton (2010Re01) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_lifetime_unit: S
level_comment:
$<r{+2}>{+1/2}=4.665 fm {i6} (2004An14, evaluation) 
J from systematics in even A In isotopes, log| {Ift}=5.14 to 3214.4-keV 2+ state in {+124}Sn 
T weighted average of 3.3 s {I3} (|g multiscaling) (1983Ta02), 3.09 s {I10} (|g multiscaling) (1986Go10) and 3.2 s {I3} (|g multiscaling) (1974Fo23); others: 3.6 s {I10} (1964Ka20) 
MOMM1 $ from collinear fast-beam LASER spectroscopy (1989Ra17). 1987Eb02 gave measurement. See also 2005St24 compilation. 
MOME2 $ from collinear fast-beam LASER spectroscopy (1989Ra17). 1987Eb02 gave measurement. Sternheimer correction was included. See also 2005St24 compilation. 


level_energy_unit: KEV
level_energy_info: ;ERR=LT;ERR=?
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E Q(|b{+-}) difference of the 3.11-s and 3.7-s {+124}In isomers (1987Sp09); systematics of odd-odd In isotopes strongly supports E(level) above the ground state. Other: 190 {I220} (1978Al18) 
J J|p=7,8,9 was proposed by 1987Eb02 from collinear fast-beam LASER spectroscopy; systematics of odd-odd In isotopes strongly support 8- 
T from |g multiscaling (1986Go10); other: 2.4 s {I3} (1974Fo23) 
MOMM1 $ from collinear fast-beam LASER spectroscopy (1987Eb02,1989Ra17). 1987Eb02 gave measurement. Evaluation of hyperfine structure was made under assumption of J=8. See also 2005St24 compilation. 
MOME2 $ from collinear fast-beam LASER spectroscopy (1987Eb02,1989Ra17). 1987Eb02 gave measurement. Sternheimer correction was included. Evaluation of hyperfine structure was made under assumption of J=8. See also 2005St24 compilation. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9-)
level_lifetime_unit: S
level_comment:
E$x <50 from the Adopted Levels for {+124}In in the ENSDF database. 
J$other: (8-) in the Adopted Levels for {+124}In in the ENSDF database. 2016Re03 suggest (9-) based on shell model calculations and observed staggering in B(M1)/B(E2) ratios. 
T$From the Adopted Levels for {+124}In in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_comment:
T Weighted average of 2.50 s {I10} (1986Go10), 2.43 s {I15} (1983Sh07) and 2.33 s {I4} (1974Gr29) 
J$J from LASER spectroscopy (1987Eb02); log| {Ift}=4.4 to 7/2+, 1362.5 level in {+125}Sn 
MOMM1,MOME2$From collinear fast-beam LASER spectroscopy (1987Eb02). See also 1989Ra17 and 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 1/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T Weighted average of 12.2 s {I3} (1986Go10), 15.1 s {I11} (1983Sh07) and 12.2 s {I1} (1974Gr29) 
J$J from LASER spectroscopy (1987Eb02); |p from systematics 
MOMM1$From collinear fast-beam LASER spectroscopy (1987Eb02). See also 1989Ra17 and 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: MS
level_comment:
J M2 |g to (19/2+); 2004Sc42 assign 25/2+. This assignment, however, leads to 15/2- assignment of 1910-keV level to which relative strong beta feed is observed from (11/2-) state. 
T$From 1998FoZY 
Configuration=(|p g{-9/2} hole ~# 7{+-} Sn Core) 


level_energy_unit: KEV
level_spin_parity: 1/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Measured mass excess=-80061 {I13} (2018Ba08) 
E$from measured mass excesses of the isomer and ground state (2018Ba08). This value can be compared with 360.12 keV {I9} in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: S
level_comment:
$measured mass excess=-80511 {I110} with {+125}In{+m} unresolved from {+125}In assuming an equal ratio of ground and isomeric states in the beam with the uncertainty inflated accordingly (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_lifetime_unit: S
level_comment:
MOMM1,MOME2$from collinear fast beam laser spectroscopy (1987Eb02, 2019StZV, 2021StZZ). 
CONF from comparison of |m and Q with proton and neutron orbits by coupling of moments (1987Eb02). 
T from 1974Gr29. Others: 1.60 s {I10} (1986Go10), 1970OsZZ, 1979Fo10. 
J from laser spectroscopy and comparison of measured moments with configuration of proton and neutron orbits (1987Eb02). 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1,MOME2$from collinear fast beam laser spectroscopy (1987Eb02, 2019StZV, 2021StZZ). 
E from measured masss excesses of -77719.6 keV {I50} for high spin state and -77809.5 keV {I41} for low spin state (2018Ba08). Other: 102 keV {I64} from difference in Q(|b{+-}) for high spin state and low spin state (1987Sp09). 
J$from systematics 
T from |g counting (1986Go10). Others: 1979Fo10, 1970OsZZ. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$ Weighted av. of 22 |ms {I2} (2004Sc42) and 29 |ms {I2} (2003HeZT) 
$Configuration=(|pg{-9/2}){+-1}(|nh{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
%B-N$ others: <0.15 (1981En05), <0.04 (1980Lu04) 
J syst for g.s. of odd-In isotopes 
J configuration=(|p g{-9/2}){+-1} 
T$weighted av of following data: |g-multiscaling: 1.15 s {I5} (1980De35) 1.22 s {I5} (1986Go10); |b{+-} or delayed neutron counting: 1.3 s {I2} (1974Gr29) 1.12 s {I2} (1980Lu04), 1.10 s {I4} (1981En05), 1.083 s {I7} (1993Ru01) 
<r{+2}>{+1/2}(charge)=4.676 {I7} (2004An14) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$420 {I65} from the end point energy of |b, using |b|g coincidence (2004Ga24) 
Delayed neutron precursor; %|b{+-}n from weighted av of 0.68 {I6} (1980Lu04), 0.54 {I11} (1986ReZU), and 0.72 {I4} (1993Ru01) 
J$syst for isomers of odd-In isotopes suggest 1/2- 
Configuration=(|p p{-1/2}){+-1} 
T$weighted av of following data: |g-multiscaling: 3.7 s {I1} (1980De35), 3.8 s {I2} (1986Go10); |b{+-} or delayed neutron counting: 3.7 s {I1} (1974Gr29), 3.76 s {I3} (1976Lu02), 3.70 s {I4} (1986ReZU), 3.580 s {I25} (1993Ru01) 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$From |b end point energy, using |b|g coincidence (2004Ga24) 
J log| {Ift}|=4.5 to (19/2-) 
T From (2004Ga24) 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_uncertain: ?
level_comment:
From systematics of E(level) and J|p of odd-In isotopes and comparison to shell model (2004Sc42). 
E$The order of 221.3-233.4 |g-ray cascade is uncertain. E(level)=2097 is possible. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E$other: 420 {I65} from the end point energy of |b, the value is obtained by using |b|g coincidence (2004Ga24) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$Measured mass excess=-76487 {I15} (2018Ba08) 
E$from measured mass excesses of the isomer and ground state (2018Ba08). This value can be compared with 408.9 keV {I3} in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$Measured mass excess=-75179 {I48} (2018Ba08) 
E$from measured mass excesses of the isomer and ground state (2018Ba08). This value can be compared with 1863 keV {I58} in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$measured mass excess=-76469 {I37} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$measured mass excess=-75126 {I36} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: S
level_comment:
$%|b{+-}n given for mixture of g.s. and 340-keV, 8- state. Value is weighted average of 0.059 {I8} from n and |b counting (1980Lu04), 0.030 {I7} from |bn coincidence (1986ReZU), and 0.040 {I3} from n- and |b-counting (1993Ru01). 1993Ru01 suggest %|b{+-}n=0.06 if all neutrons originate from the decay of the g.s. Other: <0.2 from n and |b counting (1981En05). 
J$|g from 1+, no |b{+-} feeding from 0+, and systematics for the g.s. in lighter In isotopes (1988FoZX). 
T$from |g-multiscaling (1986Go10). Other reported values of 0.80 s {I3} (1974Gr29), 0.94 s {I5} (1976Lu02), 0.9 s {I1} (1977FoZR), 0.83 s {I2} (1981En05), and 0.776 s {I24} (1993Ru01) were given for the mixture of g.s. and (8)- state. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: US
level_comment:
T$from time distribution of 248 keV |g (2004Sc42). Other: 10 |ms<T{-1/2}<20 ms (1988FoZX). 
J$comparison to shell-model. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_comment:
$No IT decay is expected, since the multipolarity of the isomeric transition is expected to be high. 
$%|b{+-}n given for mixture of g.s. and 340-keV (8-) state. 1993Ru01 suggest %|b{+-}n=0.121 if all neutrons originate from the decay of this (8-) level. See the comment on %|b{+-}n for g.s.. 
E$from |b|g (1990St13). 
J$log| {Ift}|?5.8 to (7-), systematics of the 8- states in lighter In isotopes. 
T$from |g-multiscaling (1986Go10). Others: see the comment given under the g.s.. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Measured mass excess=-73908.8 {I91} (2018Ba08) 
E$from measured mass excesses of the isomer and ground state (2018Ba08). This value can be compared with 340 keV {I60} in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: S
level_comment:
J,T,%B-$From {+128}In Adopted Levels in the ENSDF database (Feb 2015 update) 
$Measured mass excess=-74190.0 keV {I14} (2020Ne06), with reference to mass excess for {+128}Te, using the tof-ICR method. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J,T,%B-$From {+128}In Adopted Levels in the ENSDF database (Feb 2015 update) 
$Measured mass excess=-73904.9 keV {I21} (2020Ne06), with reference to mass excess for {+128}Te, (5+), using the tof-ICR method. 
E$from difference of mass excesses for the g.s. and the (8-) isomer (2020Ne06). The value in 2020Ne06 can be compared with 262 keV {I13} (2018Ba08: Phys. Rev. C 97, 024312; from mass measurement at TRIUMF). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: S
level_lifetime_info: ;ERR=GE;ISO=M2
level_comment:
J,T$from 2020Ne06, new isomer discovered in this work. See also {+128}In |b{+-} decay to {+128}Sn dataset compiled from 2020Ne06 for this isomer in the XUNDL database. 
$Measured mass excess=-72392.4 keV {I15} (2020Ne06), with reference to mass excess for {+128}Te, using the tof-ICR method. 
E$from difference of mass excesses for the g.s. and the (16+) isomer (2020Ne06). 
$Configuration=|p0g{-9/2}{+-1}~#|n(1d{-3/2}{+-1},0h{-11/2}{+-2}), 92%, proposed by 2020Ne06, based on shell model calculations 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$measured mass excess=-73924 {I44} (2021Iz01). 
E$deduced from two-state fits of overlapping ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: S
level_lifetime_info: ;ERR=GE;ISO=M2
level_comment:
J,T$from 2020Ne06. 
$measured mass excess=-72370 {I39} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n: value recommended in 1993Ru01 and 2002Pf04 based on the following measurements: 0.25 {I5} (1980Lu04), 0.13 {I3} (1986ReZU), 0.331 {I32} (1993Ru01) 
T$weighted average of 611 ms 5 (1993Ru01) and 610 ms 10. (1986Wa17,1986ReZU). Others: 590 ms 20 (1980Lu04), 0.8 s 3 (1970OsZZ, 1974Gr29,1975Al11) for either or both 0.61-s and 1.23-s activities 
$Configuration=|nh{-11/2}{+-2}~#|pg{-9/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$%|b{+-}n: value recommended in 1993Ru01 and 2002Pf04 based on the following measurements: 2.5 {I5} (1980Lu04), 2.52 {I52} (1986ReZU), 3.92 {I19} (1993Ru01) 
%IT$Estimated by the evaluators assuming only M4 |g directly to g.s., and B(M4)(W.u.)<30 from general policies in Nuclear Data Sheets 
E$from measured mass excess=-72379 keV {I4} (2013Ka08) for (1/2-), 1.3-s isomer using JYFL Penning-trap system (2013Ka08), and mass excess=-72837.9 keV {I26} (2012Wa38,2012Ha25) for g.s. of {+129}In. Earlier value of 369 keV {I46} (2004Ga24) determined from |b{+-} end-point energies from the decay of the 1.3-s and 611-ms activities is much less precise and deviates by |?2|s from value deduced from direct mass measurements by 2013Ka08 and 2012Ha25 
T$average value of 1.26 s 2 (1980Lu04) and 1.18 s 2 (1986ReZU). Other: 0.8 s 3 (1970OsZZ,1974Gr29,1975Al11) for either or both 0.61-s and 1.23-s activities 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
T$weighted average of 8.5 |ms {I5} (2003Ge04) and 11.3 |ms {I+22-16} (2012Ka36) 
J$(M2) |g to (13/2+). Configuration=|n(d{-3/2}){+-1}(h{-11/2}){+-1}~#|pg{-9/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from mass measurement using JYFL Penning-trap system (2013Ka08). Earlier value: 369 keV {I46} (2004Ga24) determined from |b{+-} end-point energies from the decay of the 1.23-s and 611-ms activities is about 2|s lower than the value from direct mass measurements 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: US
level_comment:
T$weighted average of 8.5 |ms {I5} (2003Ge04) and 11.3 |ms {I+22-16} (2012Ka36) 
$Configuration=|n(d{-3/2}{+-1},h{-11/2}{+-1})~#|pg{-9/2}{+-1} 
$M2 |g to (13/2+) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$measured mass excess=-72399 {I37} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$measured mass excess=-71196 {I89} (2021Iz01). 
E$Two unresolved isomeric states of {+129}In{+m2} and {+129}In{+m3} were fit into a single peak with the reported mass of {+129}In{+m2} adjusted (2021Iz01). 


level_energy_unit: KEV
level_comment:
$this level is shown by compilers only from the decay of the 3/2+ isomer, since it is populated by 967.6|g and 1130.6|g, both of which deexcite levels populated in the decay of the 3/2+ isomer. In 2015Ta13, and according to e-mail reply of June 3, 2015 from J. Taprogge, this level is tentatively associated with the decay of the 11/2- g.s. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
J,%B-N$from {+129}In Adopted Levels in ENSDF database 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 611 ms {I5} in {+129}In Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Measured mass excess=-72392 {I14} (2018Ba08) 
E$from measured mass excesses of the isomer and ground state (2018Ba08). This value can be compared with 459 keV {I5} in the ENSDF database, and 450.72 keV {I16} in 2015Ta13 (Phys. Rev. C 91, 054324) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: S
level_comment:
J$|b{+-} decay to 0+ and (2+); shell-model prediction, probable configuration=|p1g{-9/2}{+-1}~#|n1h{-11/2}{+-1} 
%B-N$weighted average of 1.49 {I22} (1993Ru01) and 0.90 {I5} (1986Wa17). Other: 0.91 {I10} (1986ReZS) 
T$weighted average of 0.256 s {I18} (1993Ru01, uncertainty increased by the evaluator by a factor of 2), 0.32 s {I2} (1986Wa17), 0.33 s {I3} (1981Fo02). 1986Wa17, in another report (1986ReZU), also quoted T{-1/2}=0.278 s {I3}, it is not used in averaging. Other: 1970OsZZ 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
%B-N$combined for (10-) isomer and (5+) isomer at 400. Weighted average of 2.03 {I12} (1993Ru01), 1.67 {I9} (1986Wa17), 4.3 {I15} (1981En05), 1.40 {I9} (1980Lu04) 
T$combined value for (10-) isomer and (5+) isomer at 400 is from weighted average of 0.542 s {I9} (1993Ru01), 0.55 s {I1} (1986Wa17), 0.51 s {I4} (1983Sh07), 0.51 s {I2} (1981En05), 0.53 s {I3} (1981Fo02), 0.53 s {I5} (1973Ke12). Others: 0.532 s {I6} (1986ReZS), 0.58 s {I1} (1976Lu02) 
J$shell-model prediction, probable configuration=|p1g{-9/2}{+-1}~#|n1h{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$ shell-model prediction (2003Di06); configuration=|pg{-9/2}{+-1}~#|nd{-3/2}{+-1} (2004Sc42) 
T$from 2004Sc42. Others: <6 |ms (2003HeZT), 2003Di06 quote <10 |ms from a study by the same group as 2003HeZT 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M3
level_comment:
%B-N,T$combined for (5+) isomer and (10-) isomer at 50 keV. See comment for (10-) isomer above 
J$|b{+-} decay to (4+); no |g to 1(-), T{-1/2}=0.55 s rules out assignment of J|p=4+; parity from shell-model prediction 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ERR=LT
level_comment:
T$from 2003HeZT. 2003Di06 quote |t<10 |ms from an article by the same authors as 2003HeZT in a conference proceedings 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: MS
level_comment:
J,%B-N$from {+130}In Adopted Levels in ENSDF database 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 0.29 s {I2} in {+130}In Adopted Levels in ENSDF database. Note that there is also an isomer known at |?50 keV with T{-1/2}=0.54 s {I1} 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: MS
level_comment:
T$from 2015Lo04: Phys. Rev. Lett. 114, 192501 
$Configuration=|pg{-9/2}{+-1}~#|nh{-11/2}{+-1} (2016Ju03) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from 388|g(t) (2016Ju03) 
$Configuration=|pg{-9/2}{+-1}~#|nd{-3/2}{+-1} (2016Ju03) 
$2016Ju03 suggest that there may be a low-energy transition from this level to a |b-decaying 0.54-s, (5+) isomer at about 50 keV below the 388-keV level 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<3230 {I165} from Q(|b{+-})=8350 {I160} for {+130}Cd |b{+-} decay and S(n)({+130}In)=5120 {I40} (2012Wa38) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-69862 {I20} (2018Ba08), probably for a mixture of (10-) isomer at 50 keV {I50} (with combined half-life of 0.54 s {I1} for (10-) and (5+) isomers), and 1(-) g.s. (as given in the ENSDF database). The tof-ICR frequency spectrum for the g.s. and (10-) isomers could not be resolved in the present mass measurements. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Measured mass excess=-69503 {I28} (2018Ba08) 
E$from measured mass excesses of the isomer and ground state (2018Ba08). This value can be compared with 400 keV {I60} in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: S
level_comment:
$Measured mass excess=-69909.2 keV {I75} (2020Ne06), with reference to mass excess for {+130}In, (5+) isomer, using the |p{+-}ICR method, which enabled the g.s. and the (10-) isomer as resolved structures. 
$Configuration=|p0g{-9/2}{+-1}~#|n0h{-11/2}{+-1}, |?80% with antiparallel coupling proposed by 2020Ne06, based on shell model calculations. Other contributing configurations: |?8% of |p1p{-3/2}{+-1}~#|n1d{-5/2}{+-1}, and 6% of |p1p{-1/2}{+-1}~#|n2s{-1/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (10-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$Measured mass excess=-69850.6 keV {I71} (2020Ne06), with reference to mass excess for {+130}In, (5+) isomer, using the |p{+-}ICR method, which enabled the g.s. and the (10-) isomer as resolved structures. 
$Measured mass excess=-69842.7 keV {I64} (2020Ne06), with reference to mass excess for {+130}Te, using the tof-ICR method which did not resolve the g.s. and (10-) activities. 
E$from difference of mass excesses for the g.s. and the (10-) isomer (2020Ne06, |p{+-}ICR method). Other: 66.5 keV {I99} (2020Ne06) from the tof-ICR. The value from the |p{+-}ICR method is preferred by the authors as the two activities could be resolved in this method. Note: compiler obtains 58.6 keV {I103} from the listed mass excesses in Table 1 of 2020Ne06. This value can be compared with 50 keV {I50} in {+130}In Adopted Levels in the ENSDF database. 
$Configuration=|p0g{-9/2}{+-1}~#|n0h{-11/2}{+-1} with parallel coupling proposed by 2020Ne06, based on shell model calculations 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$Mass excess=-69524.1 keV {I33} (2020Ne06), as weighted average of measured mass excess=-69525.6 keV {I49} (2020Ne06, tof-ICR method, with reference to mass excess for {+130}Te), and -69522.8 keV {I45} (2020Ne06, |p{+-}ICR method, with reference to mass excess for {+133}Cs). 
E$from 2020Ne06, weighted average of 384 keV {I9} (tof-ICR) and 386.3 keV {I60} (|p{+-}ICR), from difference of respective mass excesses for the g.s. and the (5+) isomer. Note: compiler obtains the following values from the listed mass excesses in 2020Ne06: 383.6 keV {I90} (tof-ICR), 386.4 keV {I88} (IP-ICR), and 385.1 keV {I82} using weighted averaged mass excess for the (5+) isomer. Weighted average of the first two energy values is 385.0 keV {I63}. The value in 2020Ne06 can be compared with 359 keV {I34} (2018Ba08: Phys. Rev. C 97, 024312; from mass measurement at TRIUMF). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$measured mass excess=-69523 {I38} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
%|b{+-}n: unweighted average of 1.72 {I23} (1980Lu04), 1.55 {I7} (1986Wa17), and 2.64 {I13} (1993Ru01). Other: 5.5 {I19} (1981En05). Similarity in T{-1/2}'s does not allow decomposition of the decay curves. From the measured fission yield ratios of E(302):E(3764):g.s.=0.82/0.014/0.16 (1993Ru01) in {+235}U(n,F) reaction, the evaluators estimate |?0.3% for g.s., |?1.6% for (1/2-) isomer and |?0.03 for (21/2-) isomer. This branching between the g.s. and the first isomer is consistent with that in {+127}In and {+129}In. 
J$9/2+ is most probable from the depopulation ratios to {+131}Sn levels. 
T from 1984Fo19 (2434|g(t),3990|g(t)). Others: 0.276 s {i3} (1986Wa17), 0.287 s {i4} (1993Ru01). The more precise, but discrepant, values from 1986Wa17 and 1993Ru01 were not used since the experimental techniques would not distinguish between contributions from the three isomers. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
%B-N see comment for g.s. 
%IT estimated by the evaluators; see U(n,F) dataset 
T$from 1984Fo19 (timing of 332|g from {+131}In decay) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
%B-N see comment for g.s. 
%IT no isomeric transitions observed 
J$log| {Ift}=5.4 to (23/2-) and 5.8 to (19/2-); excitation energy and angular momentum restricts the configuration, within the shell model, to |p g{-9/2}{+-1}|n(h{-11/2}){+-1}f{-7/2} implying |p=+; J|p=21/2+ is most probable from lack of isomeric transition (2004Fo06) 
T from 1984Fo19 (173|g(t), 4273|g(t)) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
%|b{+-}n: unweighted average of 1.72 {I23} (1980Lu04), 1.55 {I7} (1986Wa17), and 2.64 {I13} (1993Ru01). Other: 5.5 {I19} (1981En05). Similarity in T{-1/2}'s does not allow decomposition of the decay curves. From the measured fission yield ratios of E(302):E(3764):g.s.=0.82/0.014/0.16 (1993Ru01) in {+235}U(n,F) reaction, the evaluators estimate |?0.3% for g.s., |?1.6% for (1/2-) isomer and |?0.03 for (21/2-) isomer. This branching between the g.s. and the first isomer is consistent with that in {+127}In and {+129}In. 
J$J|p=9/2+ is most probable from the depopulation ratios to {+131}Sn levels 
T from 1984Fo19 (2434|g(t),3990|g(t)). Others: 0.276 s {i3} (1986Wa17), 0.287 s {i4} (1993Ru01). The more precise, but discrepant, values from 1986Wa17 and 1993Ru01 were not used since the experimental techniques would not distinguish between contributions from the three isomers. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
%B-N see comment for g.s. 
%IT estimated by the evaluators assuming M4 |g to g.s., no states of intermediate J|p between g.s. and 302 state (syst of odd-A In), and RUL(M4)=30; 
J$J|p=1/2- is most probable from the depopulation ratios to {+131}Sn levels (2004Fo06) 
T from 1984Fo19 (332|g(t)) 


level_energy_unit: KEV
level_spin_parity: (19/2:23/2)(+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
%B-N see comment for g.s. 
%IT no isomeric transitions observed 
J J|p|>19/2+; excitation energy and angular momentum restricts the configuration within the shell model to (|p g{-9/2}){+-1}(|n h{-11/2}){+-1}(|n f{-7/2}) implying |p=+; J|p=21/2+ is most probable from lack of isomeric transition (2004Fo06) 
T from 1984Fo19 (173|g(t), 4273|g(t)) 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
J$ tentative assignment from 2009Go40 where 3782|g is proposed to have E4 multipolarity. 
T$ from 3782|g(t) (2009Go40) 
$Measured isomeric ratio defined as the ratio of nuclei in the excited state to the total number of nuclei is 4.0% {I4} (2009Go40) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Decay modes from {+131}In Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$Based on systematics of the proton 1{Ip}, 1{Id}, and 1{If} pairs in {+78}Ni, {+132}Sn, and {+208}Pb. 
$Possible configuration=|p 1p{-3/2}{+-1} (2014Ta07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
J$based on systematics of the proton 1{Ip}, 1{Id}, and 1{If} pairs in {+78}Ni, {+132}Sn, and {+208}Pb. 
$Possible configuration=|p 1p{-3/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
J,%B-N$from {+131}In Adopted Levels in ENSDF database 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 0.28 s {I3} in {+131}In Adopted Levels in ENSDF database. Note that there is also an isomer known at 302 keV with T{-1/2}=0.35 s {I5} 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
$measured mass excess=-67675 {I39} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
$measured mass excess=-64280 {I38} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$possible mixture of g.s. and a millisec isomeric state. 
$T{-1/2}, %|b{+-}n and %|b{+-}2n measured by 2022Ph01 for possible mixture of g.s. and a millisec isomeric state 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=261 ms {I3} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=2.3 {I3} in 2019Du12 (Phys. Rev. C 99, 045805), combined for 9/2+ g.s. and 1/2- isomeric state, and %|b{+-}n=12 {I7} in 2019Du12 for 21/2+ isomeric state. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
T$from (171|g+173|g+285|g)|g(t) (2019Du12) 
%B-N$from analysis of |g ray intensities in {130}Sn and total number of |b decays (2019Du12) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_comment:
$Theoretical T{-1/2}=81 ms, %|b{+-}n=10.6, %|b{+-}2n=0.01 (2003Mo09) 
$Theoretical T{-1/2}=173 ms, %|b{+-}n=59.8, %|b{+-}2n=0.2 (2016Ma12) 
$%|b{+-}n: weighted average of 6.8% {I14} (1986ReZU) and 10.7% {I33} (1993Ru01, earlier value was 4.2 {I9} in 1980Lu04). Others: 1986ReZU and 1986ReZS (1986Wa17 from the same group), 1984Ma39, 1982Ru01 and 1976Lu02 (same group as 1980Lu04 and 1993Ru01). 1993Ru01 recommend 5.2% {I12} from average of 4.2% {I9} (1980Lu04), 6.8% {I14} (1986ReZU) and 10.7% {I33} (1993Ru01) 
T$weighted average of 0.198 s {I2} (2015Lo04, analysis of the (implanted ions)|b correlated decay curve in time and position); 0.206 s {I6} (2002Di12); 0.221 s {I11} (1993Ru01); 0.186 s {I22} (1986Bj01); 0.204 s {I6} (1986Wa17,1986ReZU,1986ReZS). Others: 0.22 s {I3} (1980Lu04), 0.12 s {I2} (1973Ke06,1973Ke27), 0.3 s {I1} (1976Lu02) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_uncertain: ?
level_comment:
E$note that a level of energy |?800 keV, J|p=(1-) in {+132}In was proposed from {+132}Cd |b{+-} decay study by 2000Ha55 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: MS
level_comment:
T$from |g(t) using summed spectra with 300|g, 375|g, 2269|g, 2380|g, 4041|g, 4352|g, and 4416|g (2020Wh02) 
%B-N$from measurement of |g ray intensities in A=132 and A=131 daughter nuclei (2020Wh02). Other: > 0.50 {I2}, lower limit as any decay directly to (11/2-) isomer would not be detected. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity is for the g.s. 
T$measured by 2022Ph01. 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=192 ms {I2} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=12.3 {I4} in 2020Wh02 (Phys. Rev. C 102, 024327). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
J$from systematics of odd mass In isotopes 
T$from |b{+-}n(t) in 2002Di12, 2003DiZX. Other: 180 ms {I15} from |b{+-}|g(t) 1996Ho16 
CONF$possible |p(g{-9/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
E$existence of that state is based on the population pattern of {+133}Sn levels in {+133}In |b{+-} and {+134}In |b{+-}n decays (1996Ho16,2000Ho32). 
J$from systematics 
T$possible isomeric state, but this value was assigned to the ground state by 1996Ho16. 
CONF$possible |p(p{-1/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
J,%B-N$from {+133}In Adopted Levels in ENSDF database 
$Theoretical T{-1/2}=109 ms, %|b{+-}n=92.7, %|b{+-}2n=0.21 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 165 ms {I3} in {+133}In Adopted Levels in ENSDF database. . Note that there is also an isomer known at 330 keV with T{-1/2}=180 ms {I15} 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
T$measured by 2019Pi04: weighted average of 161 ms {I3} from decay curve of 375|g, 162 ms {I4} from that of 4041|g and 167 ms {I7} from 3564|g. The 375 and 4041 |g rays are vin {+132}Sn from {+133}In |b{+-}n decay, and 3564|g in {+133}Sn from {+133}In |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$measured mass excess=-57036 {I69} (2021Iz01). 
E$sufficiently separated from the ground state, determined from the mass difference between ground and isomeric states (2021Iz01). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$possible mixture of g.s. and a millisec isomeric state. 
$T{-1/2}, %|b{+-}n and %|b{+-}2n measured by 2022Ph01 for possible mixture of g.s. and a millisec isomeric state 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=163 ms {I7} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=90 {I3} in 2020Be16 (Phys. Rev. C 102, 014328) for 9/2+ g.s., and %|b{+-}n=93 {I3} in 2020Be16 for 21/2+ isomeric state. 


level_energy_unit: KEV
level_spin_parity: (4- : 7-)
level_lifetime_unit: MS
level_comment:
J$from {+134}In |b{+-}n decay, which mostly populates the 7/2- ground state in {+133}Sn; the parity assignment is based on the expected configuration: configuration=((|p g{-7/2}){+-1}+(|n f{-7/2})) 
T$weighted average of 141 ms {I5} (2002Di12) and 138 ms {I8} (1996Ho16) 


level_energy_unit: KEV
level_spin_parity: (4-:7-)
level_lifetime_unit: MS
level_comment:
J,%B-N$from {+134}In Adopted Levels in ENSDF database 
$Theoretical T{-1/2}=77 ms, %|b{+-}n=6.5, %|b{+-}2n=86.7 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 140 ms {I4} in {+134}In Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity is for the g.s. 
T$measured by 2022Ph01 for g.s. and possible isomeric state 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=126 ms {I7} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=89 {I3}, %|b{+-}2n=9 {I2} in 2021Pi11 (Phys. Rev. C 104, 044328) 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: US
level_comment:
T$from 56.7|g(t) using a Poisson probability log-likelihood function that considered an exponential decay and constant background (2019Ph02). 


level_energy_unit: KEV
level_spin_parity: (6-,7-)
level_lifetime_unit: MS
level_comment:
J$as given in 2021Pi11. (4- to 7-) from Adopted Levels of {+134}In in the ENSDF database 
T$from |b-1561|g(t) in {+134}In decay (2021Pi11). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=69.8 ms, %|b{+-}n=23.5, %|b{+-}2n=64.3 (2003Mo09) 
$Theoretical %|b{+-}n=95 (2002Di12, QRPA calculations) 
E$101-ms activity assumed as belonging to the ground state of {+135}In. 
J$9/2+ from systematics of Z=49 nuclides (1997Mo25,2012Au07) 
T$weighted average of 103 ms {I5} (2015Lo04 from (implanted ions)|b correlated decay curve) and 92 ms {I10} (2002Di12, from |b-delayed neutron curve) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity corresponds to the g.s. 
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=103 ms {I5} in 2015Lo04 (Phys. Rev. Lett. 114, 192501) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
J$as given in 2021Pi11 based on systematics. 
T$from |b-347|g(t) and |b-726|g(t) in {+135}In decay (2021Pi11). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$assuming observed events correspond to the ground state. 
T$from implant-|b(t) (2015Lo04). Measured T{-1/2} is assumed to correspond to the ground state of {+136}In. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
E$it is assumed that the observed activity corresponds to the g.s. 
T$measured by 2022Ph01 
$T{-1/2}, %|b{+-}n and %|b{+-}2n were simultaneously extracted by 2022Ph01 from fitting of (implanted ions)-|b correlated events, and associated neutron multiplicity distributions using the maximum likelihood method, with the inclusion of probability density functions for decays of parent and subsequent all the daughter activities, neutron background, and efficiencies of neutron and |b detectors. This value is compared with T{-1/2}=85 ms {I+10-8} in 2015Lo04 (Phys. Rev. Lett. 114, 192501) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=0.00, %|b{+-}2n=88.00 (1997Mo25) 
E$measured half-life is assumed to correspond to the ground state of {+137}In 
J$9/2+ from theoretical considerations (1997Mo25) 
T$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}=39.5 ms, %|b{+-}n=14.9, %|b{+-}2n=67.4, %|b{+-}3n=14.3 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=28.5 ms, %|b{+-}n=49.2, %|b{+-}2n=42.4, %|b{+-}3n=1.0 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 25 counts were assigned to {+137}In, 3 events with spectrometer setting on Te, and 22 events with setting on Sn. Probability of misidentification of this isotope is <0.01% for Sn setting and 0.10% for Te setting (2018Sh11). 
$Production |s=0.35 pb for Sn setting, and 0.5 pb for Te setting. with 30% systematic uncertainty on both |s values. 
E$it is assumed that the observed events correspond to ground-state activity. 
T$measured by 2015Lo04 at RIBF-RIKEN. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Expected decay mode assigned by the evaluator 
T$lower limit of half-life assigned by evaluator from time-of-flight of 760 ns (2016Ce02). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Expected decay mode assigned by the evaluator 
$About 30 events assigned to {+99}Sn by 2016Ce02, which are assumed by the evaluator to correspond to the g.s. activity of {+99}Sn 
$Measured production |s=0.042 pb {I8} (2016Ce02) 
T$lower limit of half-life assigned by evaluator from time-of-flight of 760 ns (2016Ce02) through the BigRIPS fragment separator and ZDS spectrometer. Since {+99}Sn is expected to be a bound nucleus from S(p)=1.89 MeV, S(2p)=2.78 MeV (theory, 1997Mo25), actual half-life is expected to be much longer, e.g. theoretical T{-1/2}=41.8 ms (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$|e decay considered as negligible by 2018Pa20 
%B+P$from number of single-pixel events with |DE>1500 keV (2018Pa20). 
T$measured by 2018Pa20, using maximum likelihood method (MLH) for (implant)(positron)-correlated decay curve, where the fit function contained the parent, |b-daughter, and |bp-daughter decay components with half-lives and %|bp branching ratios, and a constant background for random correlations. Two generations of isotopes were considered in the Bateman equation. Decay constants for {+99}In and {+98}Cd daughters were taken from literature. The half-life measured in this work is compared with theoretical value of 20.6 ms from shell-model calculations by 1997He24 (Nucl. Phys. A627, 35) 
$Measured Q(|e)({+99}Sn)=14.7 MeV {I36} (2018Pa20), from (implants)|b correlated energy curve, by taking into account contribution from {+99}In daughter activity, and assuming that the observed endpoint energy corresponds to g.s. to g.s. |b{++} transition. Other: 13.43 MeV {I59} (syst, 2017Wa10: AME-2016) 
$77 implantation counts were assigned to {+99}Sn by 2018Pa20. 
$|b-decay correlation fraction=62% {I6} (2018Pa20) 
$As no beta-delayed |g rays were observed, 2018Pa20 assumed 100-(%|b{++}p)=96.1 {I+17-34} |b{++} feeding to the g.s. of {+99}In, implying log| {Ift}=3.8 {I7} for this transition. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$%|ep<17 (1996Ki23,1997Su06); <35% from 2012Lo08 based on analysis of seven {+100}Sn implantations, with no delayed proton events observed; upper limit of 35% given with 95% confidence limit. Other: from observation of a single proton event attributed to delayed proton decay in 2012Hi07, %p decay of the 2720+x level in {+100}In is estimated by 2012Hi07 as <1%. 
T$weighted average of 1.18 s {I8} (2019Lu08, average of 1.17 s {I10} from decay correlations of 2500 {+100}Sn implantations, and 1.19 s {I10} from implant-|g correlations); and 1.16 s {I20} (2012Hi07, from time distribution of decay events correlated with 163 {+100}Sn implantations analyzed by maximum likelihood method taking into account half-life of daughter nuclei and small background). Others: 0.55 s {I+70-31} (2008Ba53, from |b decays correlated with 14 {I5} implanted nuclei); 1.00 s {I+54-26} (2002Fa13, from one event in 2002Fa13 and six in 1996Ki23,1994Sc22; also 0.94 s {I+54-27} from analysis of seven events in 1997Su06,1996Ki23, 1994Sc22); 0.66 s {I+59-22} (1995Sc28,1995Sc33, from four events). Weighted average of all the measured values from 2019Lu08, 2012Hi07, 2008Ba53, 2002Fa13, and 1995Sc28 is 1.16 s {I8}, close to the Adopted value here. 
$Production |s=5.8 pb {I21} (2012Hi07) from 259 nuclei assigned to {+100}Sn, 0.25 pb {I15} (2008Ba53) from 14|+5 events assigned to {+100}Sn in {+9}Be({+112}Sn,X) at 120 MeV/nucleon, NSCL-MSU facility. Production cross section=11 pb {i4} (1997Su06) from seven events in {+9}Be({+124}Xe,X) at 1095 MeV/nucleon, GSI facility 
$Measured E(|b endpoint)=3.29 MeV {I20} (2012Hi07), 3.8 MeV {I+7-3} (2002Fa13), 3.4 MeV {I+7-3} (1996Ki23, 1997Su06), 3.5 MeV {I+13-2} (1995ScZZ), observed |b energies=700-2700 keV from seven events (1995Sc28,1995Sc33). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
$%|ep from comparison of experimental proton spectrum with calculations, assuming J|p=5/2+ for g.s. of {+101}Sn 
T$ weighted average of 1.9 s {I3} (2007Ka15, timing of delayed protons) and 1.3 s {I5} (2007Se04, recoil-decay tagging method). Other: 3 s {I1} (1995Ja16, timing of delayed proton spectra). 
$ d{-5/2} orbital 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T$ measured by 2012Lo08 from decay curves of time correlations between implantations and decay radiation. Decay curves were fitted with Poisson distribution using log-likelihood function by consideration of decay of parent, daughter and grand-daughter. correlated with implanted nuclei 
J$ from {+101}Sn Adopted Levels in ENSDF database 
%B+P$ Measured by 2012Lo08 based on observation of 458 |bp coincidence events. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$weighted average of 2.18 s {I9} from implant-|b(t) and 2.24 s {I6} from implant-|bp(t); both analyses used multiparameter fits to total decay time distribution with a Bateman equation 
%B+P$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: 0+
level_lifetime_unit: S
level_comment:
T from decay of implanted {+102}Sn ions from 1.|a GeV {+112}Sn spallation (2002Fa13). Other: 4.5 s {I7} from 1995Sc28 in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$From 2018Co07, based on the observed 1020|g and 2470|g to the 2+ and 0+ levels, respectively, and systematics of 2+{-2} levels in Sn nuclei 
$|s(2n removal)=1.4 mb {I9}. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T$ from 2005Ka34 (also 2005Ka48,2004Mu32). Others: 7 s {I3} (1981Ti03, time distribution of |b-delayed protons), 7.5 s {I15} (GSI annual report 1995, p9), 8.7 s {I6} (thesis by A. Stolz, Munich, 2001). The last two values are also quoted by 2005Ka34. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2+)
level_comment:
$ Population of this level from 2002Se10. 
E$ 162 {I4} (2002Se10) from energy interval between two |a peaks. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$ value is relative to B(E2)=0.28 {I3} for first 2+ state in {+102}Cd taken from 2009Ek01: Phys. Rev. C80, 054302 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$ value is relative to B(E2)=0.242 {I8} for first 2+ state in {+112}Sn taken from 2010Ku07: Phys. Rev. C81, 024306 
T$ deduced by compiler from B(E2)=0.10 {I4} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Feeding correctrion from higher levels is applied with reference to Coulomb excitation experiment on 
J$From {+104}Sn Adopted Levels in ENSDF database 
T$deduced by compiler from B(E2)=0.173 {I28} and E|g=1260.2 {I2} taken from Adopted dataset for {+104}Sn in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
S$a systematic uncertainty of +0-1.0 is not included (2015Co03) 
S$3.5 mb {I13} on the C target (2015Co03) 
$|s{-th}=0.7 mb {I1} from QRPA calculations (2015Co03) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
S$0.88 mb {I155} on the C target (2015Co03) 
$|s{-th}=0.3 mb {I1} from QRPA calculations (2015Co03) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
S$a systematic uncertainty of +1.0-0 is not included (2015Co03) 
S$5.0 mb {I27} on the C target (2015Co03) 
$|s{-th}=3.0 mb {I6} from QRPA calculations (2015Co03) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$Direct feeding from (5/2+) in {+109}Te |a decay (4.4~s); systematics 
T$from |g(t) and X-ray(t) in 2006Ka44; Others: 34~s~{I1} in 1995Pf01, 31~s~{I4} in 1981Ti03 and |?30~s in 1978AuZY 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: NS
level_comment:
J$200.0|g to (5/2+); systematics; yrast state assumed; Also, B(M1)(W.u.)=0.0077~{I19} consistent with the l-forbidden nature of the 200.0|g 
T$from RDDS in 1994IsZX 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T$from |t=0.61 ns {I3}, measured in |g|g-1p coincidence by gating on the in-flight component of the direct feeding transition (2023Pa30) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$from |t=7 ps {I2} and merging statistics on all 5 GALILEO rings after gating on the in-flight component of the direct feeding transition (2023Pa30). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
$g factor=-0.14 {I9} (1994Ma47), measured relative to 6+ state of {+108}Sn 
T$ Weighted average of 2.3 ns 5 from (particle)|g(t) (1994Ma47) and |g|g(t) (1988IsZW) and 2.8 ns 5 from {+106}Cd({+3}He,3n) (1989An14) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$Observed only by 1989Az02. Level energy recalculated by evaluators using decaying gamma to level energy taken from 1997Ju01 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
$g factor=-0.14 {I9} (1994Ma47), measured relative to 6+ state of {+108}Sn 
T$ from (particle)|g(t) (1994Ma47)and |g|g(t) (1988IsZW) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$from 'adopted levels, gammas dataset for {+106}Sn in ENSDF database 
T$deduced by compilers using measured B(E2)(|^) value 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
T$2.90 min {I5} (1976Hs01) 1129|g decay curve. Others: 1.3 min {I3} (1972Ri16), 2.93 min {I3} (1976VaYY), 3.0 min {I2} (1976BuZF) 
J$empirical syst presented by 1974Ho17 suggest 5/2+ or 7/2+ {+107}Sn decay feeds the 3/2+ and 5/2+ in {+107}In, so 7/2+ is ruled out. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$from 1978Hs01. Others: 10.8 min {i3} (1977Va14), 10.5 min {i4} (1970Ki04). For earlier measurements see 1956Me94 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$stretched E2 to 4+ 
T$from centroid shift in (HI,xn|g) (1983Ha37). Other: (HI,xn|g) 7 {i4} from recoil-distance pulsed beam in (HI,xn|g) (1982AnZY) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+108}Sn)=-1.081 fm{+2} {I18} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+108}Sn)=-2416.3 MHz {I94}(stat) {I98}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
J$From hyperfine structure splitting measurement in 1987Eb01. The value is in conflict with J=7/2+, measured using the atomic-beam magnetic resonance method in 1974Ho17, where no isotope selection between {+109}Sn and {+111}Sn was made. |p from |m and shell model 
T$Weighted average of 19 min {i2} (using 625|g,648|g ce(t) in 1965Kh04), 18.1 min {i3} (using 650|g(t) in 1956Pe56), 18.3 min 3 (1972Bu41, using weighted average of 330.5|g(t),649.8|g(t), 1098.1|g(t), 1321.5|g(t) and 1463.9|g(t)), 18.0 min {i2} (1969Bu04) 
MOMM1$From collinear fast-beam laser spectroscopy technique (1987Eb01) |m=1.086 {i5} for J=7/2+ (1987Ku09,1987Eb01) 
MOME2$From collinear fast-beam laser spectroscopy (1987Eb01) 
CONF$|nd{-5/2} 
$|d<r{+2}>(116,109)=-0.506 {I4} (1987Eb01) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
CONF$|ng{-7/2} 
E$the existence of this level is confirmed by 1999Da05 in (|a,n|g) and 2002Re14 in {+109}Sb |e decay, based on |g|g-coincidence measurements. 
J$13.9|g to 5/2+; systematics in neighboring nuclei; shell-model predictions 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$not populated directly in {+109}Sb |e decay (J|p=(5/2+)), non-observation of a |g ray to the 7/2+ state at 14 keV and shell-model predictions; 544.8|g(|q) in (|a,n|g) (1981JoZX,1999Da05) suggest D transition, and hence, J|p=3/2,5/2; |a(K)exp in (|a,n|g) (1976Ma09,1999Da05) is consistent with both M1 and E2 
T$6.9 ns 6 could be expected using B(E2)(W.u.)=0.054 {I5} in {+111}Sn 
CONF$|ns{-1/2} (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$664.0|g to 5/2+, 650.1|g to (7/2+), direct feeding in {+109}Sb |e decay (J|p=(5/2+)); systematics in neighboring Sn nuclei and shell-model predictions (2002Re14). 
$B(E2)=0.013 {I+8-11} in Coulomb excitation (2012Di13) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$664.5|g M1 to (7/2+), 678.6|g M1(+E2) to 5/2+; excitation functions in (|a,n|g) (1999Da05) suggests J<7/2; direct population in {+109}Sb |e decay (J|p=(5/2+)) and shell-model predications (2002Re14) 
$B(E2)<0.012 (2012Di13, Coulomb Excitation) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$925.3|g M1(+E2) to 5/2+, 910.9|g to (7/2+), 381.3|g to (1/2+); strong direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 
$B(E2)=0.029 {I+14-15} in Coulomb excitation (2012Di13) 
CONF$|nd{-3/2} state 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$991|g M1(+E2) to 5/2+, 446.3|g to (1/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); 
$B(E2)<0.028 in Coulomb excitation (2012Di13) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$1061.8|g M1(+E2) to 5/2+, 516.5|g to (1/2+) and 1047.7|g to (7/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$1078.0|g M1(+E2) to 5/2+, 1064.0|g M1(+E2) to (7/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14); excitation functions in (|a,n|g) suggests J=7/2 (1999Da05) 
$B(E2)=0.060 {I+20-22} (2012Di13, Coulomb Excitation) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$1229.3|g to 5/2+, 1214.4|g to (7/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
J$1255.85|g M2 to (7/2+); not populated in {+109}Sb |e decay (J|p=(5/2+)) 
T$from 1995Ka09 in (HI,xn|g) Other: 2.0 ns {i3} (Centroid shift method in 1982An17) 
CONF$|nh{-11/2} state 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$ 1343.64|g M1 to 5/2+; excitation functions in (|a,n|g) suggests J=7/2 (1999Da05); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$951.1|g to (1/2+), 1482.2|g to (7/2+); strong direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$1601.4|g to (7/2+), 687.3|g to (3/2)+; J |< 5/2 from excitation function in (|a,n|g) (1999Da05); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$1636.3|g to (7/2+), 1104.4|g to (1/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$835.0|g to (7/2)+, 1369.6|g to (1/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
J$690.3|g E2 to 9/2+, 672.43|g M1 to 11/2+. J=13/2 is also suggested from side-feeding excitation function of this state in (|a,n|g) (1999Da05) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$1024.4|g to (3/2)+, 2016.2|g to 5/2+; direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_comment:
J$813.44|g M1,E2 to 11/2+; J=13/2 based on side-feeding excitation function of this state in (|a,n|g) (1999Da05) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$2127.1|g to 5/2+, 1581.8|g to (1/2+); direct feeding in {+109}Sb |e decay (J|p=(5/2+)); shell-model predictions (2002Re14) 


level_energy_unit: KEV
level_spin_parity: (15/2)+
level_comment:
J$288.17|g M1,E2 to 13/2+, 960.5|g M1,E2 to 11/2+; J=15/2 based on excitation function data in (|a,n|g) (1999Da05) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$from 2002Re14 based on the non-observation of |g to the 7/2+ state and shell-model predictions 
CONF$|ns{-1/2} proposed in 2002Re14 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$the existence of this level is confirmed by 1999Da05, based on |g|g-coincidences. 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: NS
level_comment:
T$from |g(t) in 1986En06. The same value is also reported in 1984Ka16, 1995Ka09 using 833|g(t) and 1244|g(t), as well as the 185.6|g(t). However, the latter |g rays is not in coincidence with the 883| and 1244|g 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
MOME2$given as 0.218 {I7} (stat) {I15} (syst), uncertainties added in quadrature. 
J$from hyperfine structure measurements (2020Yo07) 
MOME2,MOMM1$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$Weighted average of 4.15 h {I12} (1973Ka45), 4.0 h {I2} (1956Me94), 4.173 h 23 (280|g(t) in 2005Gy02, uncertainty is statistical only), and 4.153 h 4 (280|g(t) in 2009Ra17, uncertainty is statistical only), weighted average of 4.145 h {I6} (Au catcher), 4.165 h {I9} (Pb catcher) and 4.156 h {I7} (Al catcher). Other: 4.1 h (1967Bo43) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1212.01|g E2 to 0+ 
BE2$Weighted average of 0.240 {I32} from 2007Va22, measured relative to B(E2)|^(3/2+ (g.s.) to 7/2+ (547 keV level))=0.449 {I41} for {+197}Au, and 0.220 {I22} from 2007Ce02, measured relative to B(E2)|^(0+ to 2+)=0.0695 {I20} for {+58}Ni. 
T$From adopted B(E2)|^ 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$261.5|g to 4+; 1246.4|g E1 to 2+; L(p,t)=3+4 
CONF$possible |n(h{-11/2},d{-5/2}) or octupole structure 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$L(p,t)=6; 280.2|g E2 to 4+ 
T$Weighted average of 5.6 ns 4 (280|g(t), slope analysis in {+104}Pd({+12}C,|a2n|g), by taking into account the decay of the 8- isomer at 3765 keV), 5.2 ns {I8} (280|g(t), centroid-shift analysis in {+110}Cd({+3}He,3n)) and 5.8 ns {I4} (280|g(t), slope analysis in {+110}Cd({+3}He,3n)) in 1989An14. Others: 8.0 ns {I2} (1212|g(t)), 8.4 ns {I2} (985|g(t)) and 8.5 ns {I4} (282.9|g(t)) in 1980Va13; <7 ns 282.9|g(t) in 1969Ya05 
MOMM1$From g=0.012 {I3} using |g(|q,H,t) in {+108}Cd(|a,2n) (1989Vo17) 
MOME2$Using |g(|q,H,t) in {+108}Cd(|a,2n) (1989Vo17) 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J$751.5|g to 4+; 1735.9|g 2+; direct population in {+110}Sb |e decay (J|p=(3+)); the absence of |g to 0+ 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J$1025.8|g to 4+; 2010.1|g to 2+; direct population in {+110}Sb |e decay (J|p=(3+)); the absence of |g to 0+ 


level_energy_unit: KEV
level_spin_parity: (3,4+)
level_comment:
J$796.2|g to 2+; 1432.6|g to 4+; direct population in {+110}Sb |e decay (J|p=(3+)); the absence of |g to 0+ 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J$1191.1|g to (6+); band member 
$Member of |n[g{+2}{-7/2}h{+2}{-11/2}] or |n[d{+2}{-5/2}h{+2}{-11/2}] multiplets. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J$945.4|g to (6+) 
CONF$possible member of |n(g{-7/2}{+2},h{-11/2}{+2}) or |n(d{-5/2}{+2},h{-11/2}{+2}) multiplets. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$1227.4|g to (8+); band member 
CONF$possibly a competition between the |n(g{-7/2}{+2},d{-5/2}{+2}) and |n(h{-11/2}{+2}) multiplets. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
T$Weighted average of 8.0 ns {I2} (1212|g(t)) and 8.4 ns {I2} (985|g(t)) in 1980Va13. Other: 8.5 ns {I4} (282.9|g(t)) in 1980Va13, but the transition is contaminated with similar one in {+110}In 
MOME2 from |g(|q,H,t) (1989Vo17) 
MOMM1$From |g(|q,H,t) (g=0.012 {I3}) (1989Vo17) 
CONF$Possible admixture of |n(g{-7/2}){+2} and |n(g{-7/2},d{-5/2}) configurations 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From B(E2)|^=0.226 {I18} 
$B(E2)|^=0.226 {I18}, weighted average of 0.240 {I32} from 2007Va22, measured relative to B(E2)|^(3/2+ (g.s.) to 7/2+ (547 keV level))=0.449 {I41} for {+197}Au taken from 1995Zh27 (communicated by the first author of 2007Va22 with an e-mail reply on October 25, 2007) (statistical uncertainty of 0.020 and systematic uncertainty of 0.025 were combined in quadrature by the evaluators) and 0.220 {I22} from 2007Ce02, measured relative to to B(E2)|^(0+ to 2+)=0.0695 {I20} for {+58}Ni 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from Doppler shift attenuation method via lineshape analysis in 2016Ku05. ~40% feeding from the long-lived 4{++} and 6{++} states and ~8% feeding from the 3{+-} state were measured and included in the analysis 
G$from the analysis of |g spectra in coincidence with 2|a-peak. Due to the higher feeding contributions from 4{++} and 6{++} states populated, only Doppler-shifted part of the 1212.0|g was used in the analysis. The authors of 2016Ku05 state that, adopting the T{-1/2}= 0.48 ps {I2} from the Adopted Levels of {+110}Sn in ENSDF database would increase the value of g-factor by 7%. g-factor = +0.24 from the Shell Model calculations. The calculated value is the average of two g-factor values obtained for two configurations including 2 neutrons; (g{-7/2}){+2} (gives g-factor = +0.208) and mixed [(g{-7/2}){+1}, (d{-5/2}){+1}] (gives g-factor = +0.28). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$from Doppler shift attenuation method via lineshape analysis in 2016Ku05. No discernible Doppler-shifted component was observed in the lineshape analysis. 
G$from the analysis of |g-spectra gated on |a-peaks. T{-1/2} = 4 ps was used in the analysis. g-factor = +0.07 from the Shell Model calculations. The calculated value is the average of two g-factor values obtained for two configuration including 2 neutrons; (g{-7/2}){+2} (gives g-factor = +0.208) and mixed [(g{-7/2}){+1}, (d{-5/2}){+1}] (gives g-factor = -0.07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$from Doppler shift attenuation method via lineshape analysis using the segments of clover detectors at 52{+|o} and 68{+|o} together with the reaction kinematics and energy loss in the multilayer target in 2016Ku05. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
G$from the analysis of |g-spectra gated on |a-peaks. T{-1/2}=5.614 ns {I69} from the Adopted Levels of {+110}Sn in the ENSDF database was used in the analysis. g-factor = +0.03 from the Shell Model calculations. The calculated value is the average of two g-factor values obtained for two configurations including 2 neutrons; (g{-7/2}){+2} (gives g-factor = +0.208) and mixed [(g{-7/2}){+1}, (d{-5/2}){+1}] (gives g-factor = -0.151). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-,4+
level_comment:
E,J$Two levels are known in the adopted levels of ENSDF database at 2455.3 (J|p=4+) and 2458.42 keV (J|p=3-), but those cannot be resolved in 2018Co07 
$|s(2n removal)=8.7 mb {I12}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+110}Sn)=-0.907 fm{+2} {I11} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+110}Sn)=-2014.9 MHz {I75}(stat) {I84}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_comment:
J$from atomic beam (1974Ho17), |p=+ from L=4 (p,d) 
T$weighted av: 35.0 min {I5} (1949Hi10), 35 min {I1} (1951Mc11), 35.5 min {I8} (1967Da11), 35.8 min {I8} (1969Sh11). Other: 1961Ra06 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: US
level_comment:
T$from (1978Ho06) |g(t) pulsed beam. Other: 18 |ms {I1} (1972Br38) |g(t) pulsed beam 
J$L=0 (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
J$L=5 in (pol d,t), M2 |g to 7/2+ 
E$The state results from the occupation of the |nh11/2 orbital coupled to the core g.s. of {+110}Sn (1995La11) Analogs {+113}Sn at { 740 keV}, 159-|ms, {+115}Sn at 714 keV 
T$from (1984Pr06). Others: 9.2 ns {i10} (1974Br29), 7.9 ns {i8} (1972Br38) |g(t) pulsed beam 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_comment:
E$The state results from the occupation of the |nh11/2 orbital coupled to the 2+ of the core of {+110}Sn (1995La11) 
J$stretched E2 |g to 11/2- state and excit in (|a,n|g) 


level_energy_unit: KEV
level_comment:
J$L=(1) (p,d), but L=4+1, J=9/2,7/2 from (pol d,t) for a complex peak at 3270 assumed by the authors to be 3238+3262 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$from 1984Pr06. Others: 9.2 ns {i10} (1974Br29), 7.9 ns {i8} (1972Br38) 
g-factor=-0.23 {i2} (1974Br29) 979|g(H,T) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_comment:
J$From {+111}Sn Adopted Levels in the ENSDF database (Feb 2008 update) 
T$From measured half-lives of 35.1 min {I5} and 35.2 min {I6} from decay curves for 761|g and 1152|g, respectively (2022Ch11). This value can be compared with 35.3 min {I6} in {+111}Sn Adopted Levels in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=2; 1256.68|g E2 to 0+ 
T$from B(E2)|^ in Coulomb excitation. Others: 0.451 ps {I28} from DSAM in 2011Ju01 and 0.37 ps {I+7-6} in from DSAM in 2007Or04 (note that the value was initially reported as 0.52 ps {I+9-6}, but it was retracted by the authors. 
BE2$0.240 {I3}, weighted average of 0.242 {I8} (2011Ku05,2010Ku07), 0.240 {I20} (2007Va22), 0.229 {I5} (1975Gr30), and 0.256 {I6} (1970St20). Other: 0.240 {I14} (1987Ra01), weighted average of the data in 1975Gr30 and 1970St20 
$|b{-2}=0.143 {i5} (for r{-0}=1.26 fm) (1980Bl07). Other: 0.152 {i10} (1968Ma34) 
MOMM1$+0.21 {I7} from g-factor=+0.104 {I35} in 2011Wa15. Other: +0.7 {I3} in 1980Ha19 
MOME2$-0.09 {I10} in 1975Gr30 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,p')=2; 2150.9|g E2 to 0+ and 894.17|g M1+E2 to 2+ 
T$from B(E2)|^=0.00065 {I20} in Coulomb excitation (1981Jo03) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4; L(p,p')=4; 990.69|g E2 to 2+ 
T$from B(E2)(2+ to 4+)=0.032 {I5} in Coulomb excitation (1981Jo03) 
MOMM1$+1.5 {I7} from g-factor=+0.38 {I18} in 2011Wa15 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(p,p')=3; L(p,t)=3; L(|a,|a')=3; 1097.38|g E1 to 2+ 
T$From DSAM in 2011Ju01; Other: 0.35 {I+14-8} ps from DSAM in {+112}Sn(n,n'|g) (2005Ku28) 
$|b{-3}=0.146 {i5} (for r{-0}=1.26 fm) (1980Bl01). Other: 0.203 {i15} (1968Ma34). 
$B(E3)=0.087 {I12} (1981Jo03) in Coulomb excitation (1981Jo03) and 0.050 {I10} in {+112}Sn(|a,|a') (1970Br07) 
MOMM1$-1.4 {I28} from g-factor=-0.48 {I92} in 2011Wa15 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4; 1264.07|g E2 to 2+ 
T$from DSAM in {+103}Rh({+12}C,p2n|g) (1990ViZW). Other: >0.8 ps in {+112}Sn(n,n'|g) (2005Ku28) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$L(p,t)=6; 301.84|g E2 to 4+ 
T$weighted average of of 13.9 ns {I2} (1980Va13), 14.0 ns {I4} (1969Ya05), 13.2 ns {I4} (1981Go17) and 13.7 ns {I1} (1981Va15) in {+110}Cd(|a,2n|g) and 12.1 ns {I15} (1989An14, 1988Pe17) and 13.6 ns {I4} (1989An14) in {+110}Cd({+3}He,n|g),{+112}Cd({+3}He,3n|g). Other >0.5 ps from DSAM in {+112}Sn(n,n'|g) (2005Ku28) 
MOMM1$+0.53 {I3} (1983Le18), +0.61 {I5} (1981Go17), and +0.2 {I2} (1981Va15) 
MOME2$0.29 {I6} (1975Vi03) 
CONF$most likely a mixture between (|ng{-7/2}{+-1},|nd{-5/2}{+-1}) and (|ng{-7/2}){+-2} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4; L(p,p')=4; 1527.2|g E2 to 2+ 
T$wt. average of 0.35 ps {I14} in {+103}Rh({+12}C,p2n|g) (1990ViZW) and 0.31 ps {I+10-6} in {+112}Sn(n,n'|g) (2005Ku28) 


level_energy_unit: KEV
level_spin_parity: (7)-
level_comment:
J$805.11|g E1 to 6+; yrast state, but 5- and 6- cannot unambiguously be excluded 
CONF$possible |nd{-3/2}h{-11/2} configuration 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4,6; 1166.9|g E2 to 4+; member of |DJ=2 sequence 
T$From DSAM in {+103}Rh({+12}C,p2n|g) (1990ViZW) 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: NS
level_comment:
J$76.3|g M1+E2 to (7)-; no transitions to the 6+ states 
T$weighed average of 0.58 ns {I6} from |g|g(t) in {+110}Cd(|a,2n|g) (1980Va13) and 0.62 ns {I4} from recoil distance method in {+100}Mo({+16}O,4n|g) (1986Ka25) 


level_energy_unit: KEV
level_spin_parity: (9)-
level_lifetime_unit: PS
level_comment:
J$263.03|g M1+E2 to (8)- 
T$From recoil-distance measurements in {+100}Mo({+16}O,4n|g) (1986Ka25); Other: 0.69 ps {I14} in {+103}Rh({+12}C,p2n|g) (1990ViZW) 


level_energy_unit: KEV
level_spin_parity: (10)-
level_lifetime_unit: PS
level_comment:
J$1151.94|g E2 to (8)- 
T$from DSAM in {+103}Rh({+12}C,p2n|g) (1990ViZW). Other: <21 ps from RDDS in {+100}Mo({+16}O,4n|g) (1986Ka25); 


level_energy_unit: KEV
level_spin_parity: (11)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$1235.3|g E2 to (9)-, 345.9|g M1+E2 to (10)- 
T$from recoil distance method in {+100}Mo({+16}O,4n|g) (1986Ka25) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$745.0|g E2 to 10+; band member 
T$from DSAM in {+100}Mo({+20}Ne,|a4n|g) (2007Ga45). Other: <0.14 ps in {+103}Rh({+12}C,p2n|g) (1990ViZW) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
T$weighted average of 13.9 ns {i2} (1980Va13); 14.0 ns {i4} (1969Ya05); 13.2 ns {i4} (1981Go17) and 13.7 ns {i1} (1981Va15) 
G$+0.097 {I9} (1981Go17); Other: +0.04 {I3} from TDPAD in 1981Va15 
MOME2$0.29 {I6} (1975Vi03); 
CONF$|ng{-7/2}|nd{-5/2}, (|ng{-7/2}){+2} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^ 
BE2$0.240 {I3}, weighted average of 0.242 {I8} (2011Ku05,2010Ku07), 0.240 {I20} (2007Va22), 0.229 {I5} (1975Gr30), and 0.256 {I6} (1970St20). Other: 0.240 {I14} (1987Ra01), weighted average of the data in 1975Gr30 and 1970St20 
MOMM1$+0.21 {I7} from g-factor=+0.104 {I35} in 2011Wa15 
MOME2$-0.06 {I9}, weighted average of-0.03 {I11} (1975Gr30) and -0.15 {I18} (1970St20) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$From B(E2)|^ 
$B(E2)|^=0.032 {I5} (1981Jo03) 
MOMM1$+1.5 {I7} from g-factor=+0.38 {I18} in 2011Wa15 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
T$weighted average of 12.1 ns {I15} (1989An14,1988Pe17) and 13.6 ns {I4} (1989An14) from centroid shift and slope analysis, respectively. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
|b{-2}=0.147 {I4}, weighted average of 0.143 {I5} and 0.150 {I5} in 1980Bl01; Other: 0.152 in 1968Ma34 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
|b{-3}=0.152 {I6}, weighted average of 0.146 {I5} and 0.157 {I5} in 1980Bl01; Other: 0.203 {I15} in 1968Ma34 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$From recoil-in-vacuum method with sign taken from transient field measurements (see reference in 2015Al24) 
$Transitional E2 matrix element=(+)0.500 {I10} 
$Diagonal E2 matrix element=+0.05 {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)({+112}Sn)/B(E2)({+58}Ni)=3.72 {I16} (2017Ku28) 
$B(E2) relative to B(E2)=0.0650 {I12} for the first 2+ state in {+58}Ni, value taken from 2016Pr01 evaluation (At. Data and Nucl. Data Tables 107, 1). Earlier B(E2)=0.242 {I8} (2010Ku07: Phys. Rev. C81, 024306) from the same group as 2017Ku28. These values can be compared with B(E2)=0.250 {I10} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); and 0.200 {I12} (from mean lifetime |t=0.65 ps {I4} by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+112}Sn)=-0.747 fm{+2} {I7} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+112}Sn)=-1383.3 MHz {I22}(stat) {I84}(syst) for S(p) atomic transition, and -1652.1 MHz {I56}(stat) {I71}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) = 0.240 {I12}, average of 0.239 {I9} (2019Ku06) and 0.242 {I23} (2019Ku15) deduced from the transition matrix elements. 
$B(IS2) = 0.241 {I28} (2019Ku06) and 0.251 {I25} (2019Ku15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$measured relative to {+59}Co and {+27}Al (2024Be28) 
$|G{-0}=1.18 meV {I6} (2024Be28) 
$I{-s}=14.4 eVb {I8} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
S$22.5 mb {I35} on the C target (2015Co03) 
$|s{-th}=6.5 mb {I13} from QRPA calculations (2015Co03) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: D
level_comment:
MOMM1$atomic beam. 
T from weighted average of 115.2 d {I8} (1972Em01), 115.07 d {I10} (1972La14), 115.09 d {I4} (1980Ho17), 115.12 d {I13} (1982RuZV), and 115.08 d {I8} (1992Un01). The reduced-|h{+2} = 0.03. Because this set of values is consistent, the Limited Relative Statistical Weight method (1985ZiZY, 1992Ra09) does not increase the uncertainty for the 1980Ho17 value even though it contributes 66% of the relative weight. If the 1980Ho17 uncertainty were increased from 0.04 to 0.056 in order to decrease its relative weight to 50%, the weighted average average would still be 115.09 with an uncertainty of 0.04. The very small reduced-|h{+2} value suggests that the reported uncertainties are overestimated. Other measurements: 107 d (1959Bu08), 115.12 d {I20} (1976MeZR, replaced by 1982RuZV), and 115.06 d 7 (1982HoZJ, replaced by 1992Un01). 
J$atomic beam (1976Fu06), L(d,p)=0. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from 1974Ho17. Others: 21 min {I1} (1961Se08), 20 min {I1} (1961Sc12). 
%IT from I(K|a| x ray,{+113}In)/I(K|a| x ray,{+113}Sn). 
J$atomic beam (1976Fu06), 77|g is M3(+E4). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
MOMM1$|m and Q: differential perturbed angular distribution 
J$L(d,p)=5, M2(+E3) |g to 7/2+ 
T$unweighted av of 88 ns {I3} (1973IsZQ), 89 ns {I3} (1974Di18), 82.1 ns {I17} (1974Br29) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
E$a level with L(d,p)=2 observed at 1014 {I5}, may correspond to either 1013.22 or 1018.09 level 
J$log| {Ift}=5.86 {I3} from 5/2+, M1+E2 |g to 1/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$L(d,p)=2 at 2129 {I5}, the 2129 level in (d,p) does not seem to correspond to the 2134 level (no |g to g.s.). 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: NS
level_comment:
J$E1 |g to 23/2-, a three quasi-particle neutron configuration proposed by 1997Ka40 
T$from |g-rf(t) in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 27/2-
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=3.94 eb {I+11-15}. Quadrupole deformation |b{-2}=0.27 {I1} (deduced assuming |g=0|'). 


level_energy_unit: KEV
level_spin_parity: 31/2-
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=3.38 eb {I32}. Quadrupole deformation |b{-2}=0.24 {I2} (calculated assuming |g=0|'). 


level_energy_unit: KEV
level_spin_parity: 35/2-
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=3.09 eb {I+41-36}. Quadrupole deformation |b{-2}=0.22 {I+3-2} (calculated assuming |g=0|'). 


level_energy_unit: KEV
level_spin_parity: 39/2-
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=2.39 eb {I18}. Quadrupole deformation |b{-2}=0.17 {I1} (calculated assuming |g=0|'). 


level_energy_unit: KEV
level_spin_parity: 43/2-
level_lifetime_unit: PS
level_comment:
$Transition quadrupole moment Q{-t}=2.56 eb {I16}. Quadrupole deformation |b{-2}=0.18 {I1} (calculated assuming |g=0|'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ 
T$From 2011Ju01 in Coulomb excitation; Others:T{-1/2}=0.31 ps {i10} (1991ViZW), T{-1/2}=0.39 ps {i8} (2001Ga52), 0.30 ps {i6} (1961An07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=4, E2 |g to 2+. log| {Ift}=5.9 from 3+ {+114}Sb g.s. 
T$from (2001Ga52). Other: 1.4 ps>(1991ViZW) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: NS
level_comment:
T$from a,|g(t) in {+112}Cd(|a,2n|g) (1978BrZU) 
J$probable M1 |g to 7-, no |g's to 6+ or 5-. M1+E2 from 8- 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 8+, |g(|q), |a(K), |g-pol (1979Br07) 
T$from (2001Ga52). Other: 0.60 ps {i18} (1991ViZW) 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 10+, |g(|q), |a(K), |g-pol (1979Br07) 
T$from (2001Ga52). Other: 0.67 ps {i18} (1991ViZW) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From 2011Ju01. Other: 0.390 ps from B(E2)(2008Do19) 
Other B(E2)=0.20 {I7} (1957Al43) 0.25 {I5} (1961An07) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$deduced from the lineshape of the 3{+-} to 2{++} E1 transition, and hence it should be considered as an upper limit. Note that this value disagrees with that of 1.7 ps +10-7, quoted in the Adopted Levels from the unpublished work of 1991ViZX 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$From recoil-in-vacuum method with sign taken from transient field measurements (see reference in 2015Al24) 
$Transitional E2 matrix element=(+)0.479 {I10} 
$Diagonal E2 matrix element=+0.12 {I11} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)=0.232 {I8} (2008Do19, normalized to B(E2)=0.209 {I6} for {+116}Sn (value from 2001Ra27: At. Data and Nucl. Data Tables 78, 1). Here the value in 2008Do19 is re-normalized to B(E2)=0.200 {I7} for {+116}Sn, determined in the present work. This value can be compared with B(E2)=0.229 {I9} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); and 0.183 {I12} (from mean lifetime |t=0.60 ps {I4} by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+114}Sn)=-0.605 fm{+2} {I5} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+114}Sn)=-1115.3 MHz {I19}(stat) {I69}(syst) for S(p) atomic transition, and -1335.6 MHz {I62}(stat) {I58}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
See 1973Ri14 for near-constant |m measurements of 11/2- isomers in odd-mass tin, cadmium, tellurium isotopes 
T$from |g(t) pulsed beam (1964Iv01). Others: 165 |ms {I15} (1958Du80), 155 |ms {I10} (1964Br27), 166 |ms {I10} (1966Mc06) 
J$L=5 (d,p),(d,t),(p,d),(p,t); M2 decay to 7/2+ state 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.0227 {I10} and I|g(986|g)-branching=24.7%; other: 1.25 ps {I28} Doppler-broadened 986|g peak 
J$L=2 (d,p),(d,t),(p,d),(p,t); J=5/2 from (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T Doppler-broadened 1280|g peak (1977Da12); others: 0.53 ps {I5} if B(E2)=0.0444, I|g(1280|g)-branching=86%, |d(1280|g)=-2.2; 0.6 ps {I+4-3} (1999Lo04) 
J$M1+E2 decay to 1/2+ state 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.0607 and I|g(1417|g)-branching=72%:0.97 ps<(1999Lo04) 
J$L=2 (d,t),(p,d),(p,t); J=5/2 from (pol d,t); 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J from L=4 (d,t),(p,d) and E2 transition to 3/2+ state; J=7/2 from (pol d,t). 1857 |g to 1/2+ g.s. in (|a,n|g) is not compatible, suggesting |g is misplaced in (|a,n|g) 
T$from 1999Lo04 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: US
level_comment:
T 3.26 |ms {I8} (1967Iv05) |g|g(t) scin. Others: 3.45 |ms (1968Iv02) |g(t) pulsed beam, 3.8 |ms {I4} (1978Ho06) |g(t) pulsed beam 
g factor: +0.195 {I3} (1975Iv02) |g(|q,H,t) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
T from 1964Iv01 |g(t) pulsed beam. Others: 165 |ms {I15} (1958Du80), 155 |ms {I10} (1964Br27), 166 |ms {I10} (1966Mc06) 
g factor: -0.250 {I2} (1975Iv02), 0.255 {I15} (1972Me15), 0.247 {I1} (1971Br03) 
%IT decay=100 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
Branching: I|g(1280|g):I|g(783|g):I|g(668|g):I|g(294|g)=86.2 {I12}:7.8 {I7}:3.0 {I7}:3.0 {I4} (1977Da12) Coul. ex. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$Branching: I|g(1417|g):I|g(920|g):I|g(804|g):I|g(430|g):I|g(137|g) =72.1 {I28}:21.0 {I19}:5.1 {I7}:0.6 {I4}:1.2 {I5} (1977Da12) Coul. ex. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2+
level_comment:
E may correspond with L=2, 2355-keV (d,t) and 2360-keV (p,d) excitations 
J based on |g-decays to 1/2+,3/2+,5/2+ states and log| {Ift}=6.4 
Branching: I|g(1378|g)/I|g(1867|g)/I|g(2365|g)=14 {I2}/100/23 {I9} (1974Ki07), 7 {I3}/100/21 {I5} (1975WiZX); I|g-ratios via in-beam (1975Ma38) are different 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2,5/2)+
level_comment:
I|g(1021|g)/I|g(1136|g)/I|g(1633|g)=11 {I4}/18 {I2}/100 (1975Ma38), 12 {I2}/36 {I2}/100 (1975WiZX, {+115}Sb decay) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2,5/2)+
level_comment:
Branching: I|g(1236|g)/I|g(1121|g)/I|g(747|g)=100/52 {I14}/49 {I13} (1975Ma38) via (|a,n|g), 100/80 {I22}/44 {I12} (1975Ma38) via (p,n|g), 100/27 {I2}/34 {I4} (1975WiZX, {+115}Sb decay) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2,5/2+)
level_comment:
Branching: I|g(1379|g)/I|g(1752|g)/I|g(1867|g)=100/88 {I37}/75 {I32} (|a,n|g), 100/83 {I24}/<78 (p,n|g); I|g-ratios via {+115}Sb decay are different 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T 11 ps {I2} if B(E2)=0.0140 and |d(497|g)=+0.21 {I2} 
B(E2)=0.0140 {I8} (|a,|a'|g) semi; 0.0140 {I4} (|a,|a') E|a=10.2 MeV, 0.0139 {I11} (|a,|a') E|a=9.5 MeV (s); other: |?0.015 (1962Va20) via ({+14}N,{+14}N'|g) E=42 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.0227 and I|g(986|g)-branching=24.7% 
T 1.25 ps {I28} (1977Da12) Doppler-broadened 986|g-line shape 
B(E2)=0.0227 {I10} (|a,|a'|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T from B(E2)=0.0607 and I|g(1417|g)-branching=74%; other: 0.25 ps {I5} Doppler-broadened 1417|g peak 
B(E2)=0.060 {I3} (|a,|a'|g), 0.061 {I3} (|a,|a') E|a=10.2 MeV 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$from hyperfine structure measurements (2020Yo07) 
MOMM1$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$others: +0.07 {i10} (1975Gr30), +0.09 {i13} (1970Kl06) 
J$E2 |g to 0+ 
T$from 1987Ra01 based on an average of available B(E2) and T{-1/2} data; values included in 1987Ra01: 0.49 ps {i9} (1962Li10), 0.44 ps {i19} (1962Ka28), 0.195 (1975Gr30), 0.33 ps {i7} (1963Be14), 0.37 ps {i4} (1977Ca14,1981Ca10) via res fluorescence The recent value: 0.51 ps {I+20-14} (2007Or04) in (n,n'|g) is in agreement 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J$E2 |g to 3-, E3 |g to 2+, L(p,p')=5 
T$weighted av of 335 ns {i50} from (|a,2n|g) (1980Va13) and 350 ns {i20} from |e decay (1966Rg02). Others: 370 ns from (|a,2n|g) (1973IsZQ), 230 ns {i20} from |e decay (1964Bo21) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 2+ (1097|g)(1293|g)(|q), L=4 (d,t) 
T$from 1972Ka66, res fluorescence, T{-1/2}=0.47 ps {i9} from Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$M1 |g to 6-, log| {Ift}=4.9 from 8- parent 
T$from (|a,2n|g) (1980Va13). Other: |<0.5 ns from |e decay (1966Rg02) 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
E$1987Va30 have studied the role of core polarization and of the quenching of the leading shell model configuration in stretched spin states for this state. 
J$from |g(|q) for M1+E2 |g to 8- 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
J$probably different from the 3850.9 level (1,2+) since |s(|q) in (p,p') requires a high -L component (see comment in (p,p')) 


level_energy_unit: KEV
level_spin_parity: (8,10-)
level_comment:
J$strong feeding to 8-. L({+3}He,d)=4,5. 1992Sc20 suggest that this state contains part of the fragmented 10-,8- or 8+ configurations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T from 1980Va13. Others: 904 ns (1973IsZQ), 750 ns {I100} (1969Ch15), 900 ns {I100} (1987Lu06) 
G$value not corrected for Knight shift or diamagnetism 


level_energy_unit: KEV
level_comment:
L$|s(|q) cannot be fit with any L value, suggests unnatural parity, similar to that for a known 1+ state in {+58}Ni(p,p') (1983Wi07) 


level_energy_unit: KEV
level_comment:
L$|s(|q) cannot be fit with any L value by 1983Wi07, L given by 1970Be20 is discrepant. Could be associated with the adopted 3+ (2996), the shape is similar with 3+ state in {+58}Ni(p,p') 


level_energy_unit: KEV
level_comment:
L$from 1983Wi07, L=(6) (1970Be20). The evaluators assume that the peak corresponds to the known 5- level at 3105 but could include a contribution from the 3097 {I4}+ level. 


level_energy_unit: KEV
level_comment:
L$from 1970Be20. Value is discrepant with adopted J|p=6+, but peak is probably not a separate level. Could include the 3256 with J|p=(3-,4,5-) and/or 3289 level with J<5 


level_energy_unit: KEV
level_comment:
L$from 1970Be20; 1983Wi07 do not report L but the shape of their fit is almost identical to the 2586 level which has J|p=1+ 


level_energy_unit: KEV
level_comment:
L$from 1983Wi07. L=(6) (1970Be20). The fit of 1983Wi07 is good at small angles but requires a higher component at |q>50|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$authors' value of 2970 is probably a misprint. Using the known 2+ and 3- states, the evaluators recalculate the energy to be 2810. Note that 1968Ku20 report 2870 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Calculated B(E2)=0.229 {I+7-24} (DP model), 0.182 {I+6-19} (DIF model), 0.233 {I+7-24} (DDF model). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$Calculated B(E3)=0.116 {I+3-12} (DP model), 0.101 {I+3-11} (DIF model), 0.133 {I+4-14} (DDF model) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MEV
level_comment:
E$14340 {I+206-200} quoted for isoscalar quadrupole E2 (ISGQR) resonance; E2 EWSR=94% {I+14-10}. Gaussian fit gives energy of 14.09 MeV {I27} and |G=5.48 MeV {I35} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MEV
level_comment:
E$15390 {I+305-200} quoted for isoscalar monopole E0 (ISGMR) resonance; E0 EWSR=106% {I+27-11}. Gaussian fit gives energy of 15.58 MeV {I19} and |G=5.46 MeV {I18} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: MEV
level_comment:
E$ isoscalar dipole E1 (ISGDR) resonance; E1 EWSR=52% {I+20-14} 
$ Total E1 (ISGDR) EWSR=118% {I+20-14} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from adopted levels. Other: B(E2): 0.216 (1970St20), 0.23 {I1} (1970Kl06,1968St14) 
$Q=+0.09 {I13} (1970Kl06), +0.07 {I10} (1975Gr30), 0.07 {I16} (1970St20) 
G$2008Ea02 give adopted g factor=-0.16 {I9} from their measurement -0.15 {I26} and earlier g-factor=-0.16 {I10} from 1980Ha19 deduced using the transient field integral PAC technique 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$deduced from the lineshape of the 3{+-} to 2{++} E1 transition, and hence it should be considered as an upper limit. 


level_energy_unit: KEV
level_spin_parity: 3-&(8+,9-)
level_comment:
L$ |s(|q) is accurately reproduced by considering 30% admixture of L=3 and 70% that of L=8 or 9 for a doublet 


level_energy_unit: KEV
level_spin_parity: 4+&2+
level_comment:
L$ |s(|q) is accurately reproduced by considering 60% admixture of L=4 and 40% that of L=2 for a doublet 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
MOMM1$ deduced from g-factor=+0.006 {I19} (2011Wa15), which is the average of the results +0.015 {I27} and -0.003 {I27} from the inner and outer pairs of Si detectors, respectively, both of which were corrected for feeding from the higher-lying states. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
MOMM1$ deduced from g-factor=-0.01 {I23} (2011Wa15), which is the average of the results -0.05 {I25} and +0.19 {I58} from the inner and outer pairs of Si detectors, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
MOMM1$ deduced from g-factor=0.00 {I35} (2011Wa15), which is the average of the results +0.17 {I39} and -0.63 {I74} from the inner and outer pairs of Si detectors, respectively. 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$isoscalar giant quadrupole resonance (ISGQR) (2014Pa29) 
$%EWSR=73 {I23} (stat) (2014Pa29) 
L$dominant component among L=0,1 and 2 (2014Pa29) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Transitional E2 matrix element=(+)0.453 {I9} 
$Diagonal E2 matrix element=+0.22 {I11} 
G$From recoil-in-vacuum method. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)({+116}Sn)/B(E2)({+58}Ni)=3.08 {I9} (2017Ku28) 
$B(E2) relative to B(E2)=0.0650 {I12} for the first 2+ state in {+58}Ni, value taken from 2016Pr01 evaluation (At. Data and Nucl. Data Tables 107, 1). This value can be compared with B(E2)=0.205 {I8} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); 0.170 {I10} and 0.165 {I10} (from mean lifetime |t=0.66 ps {I4} and 0.68 ps {I4}, respectively, by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+116}Sn)=-0.461 fm{+2} {I4} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+116}Sn)=-841.8 MHz {I14}(stat) {I55}(syst) for S(p) atomic transition, and -1007.6 MHz {I79}(stat) {I45}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$from weighted average of 56 ps {I17}, 48 ps {I15}, 51 ps {I14} all from |g|g fast-timing technique (2019Pe06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) = 0.207 {I10}, average of 0.207 {I6} (2019Ku06) and 0.207 {I20} (2019Ku15) deduced from the transition matrix elements. 
$B(IS2) = 0.211 {I18} (2019Ku06) and 0.211 {I28} (2019Ku15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$B(E3) = 0.098 {I13} from 2019Ku15. Other: 0.095 in 2019Ku06. 
$B(IS3) = 0.053 {I8} (2019Ku06) and 0.090 {I19} (2016Ku15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$measured relative to {+112}Sn, from the ratio B(E2)({+116}Sn)/B(E2)({+112}Sn)=0.83 {I4} (2024Be28) 
$|G{-0}=1.13 meV {I8} (2024Be28) 
$I{-s}=13.0 eVb {I9} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$from 1972Jo13. Other: 0.31 ns {i3} (1963Sc12) 
MOMM1$integral perturbed angular correlations. 
J$L(d,p)=2, 158|g is M1+E2 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
MOMM1,MOME2$LASER induced resonance fluorescence from an atomic beam (1986An24) 
T$From 2002Un02. Others: 13.98 d {I7} (2003Po21), 13.60 d {I4} (1977Ka16), 14.0 d {i5} (1951Co34), 14.0 d {i3} (1950Mi52) 
J$L(d,p)=5 156|g to 3/2+ is M4 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.062 {i3} and branching. Other: 0.49 ps {i10} from DSA 
J$L=2 in (|a,{+3}He), |g(|q) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$0.35 ps {i10} from DSA, 0.43 ps {i3} from B(E2)=0.0360 {i20} and branching 
J$|g|g(|q) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_comment:
T$From 2002Un02. Others: 13.98 d {I7} (2003Po21), 13.60 d {I4} (1977Ka16), 14.0 d {i5} (1951Co34), 14.0 d {i3} (1950Mi52) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E 314.58 {i10} from adopted levels. 1979Ha12 report T{-1/2}=140 d, probably a misprint 
T from adopted levels 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
Ground-state decay |G (g|G{-0})=0.0027 eV {I8} 
B(E1)=0.071|*10{+-5} {I17}. B(E1)=0.16|*10{+-5} {I5} (corrected for possible inelastic transition) 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
Ground-state decay |G (g|G{-0})=0.0092 eV {I11} 
B(E1)=0.224|*10{+-5} {I23}. B(E1)=0.34|*10{+-5} {I4} (corrected for possible inelastic transition) 


level_energy_unit: KEV
level_spin_parity: 1/2,(3/2)
level_lifetime_unit: EV
level_comment:
Ground-state decay |G (g|G{-0})=0.0203 eV {I6} 
B(E1)=0.44|*10{+-5} {I4}. B(E1)=0.577|*10{+-5} {I17} (corrected for possible inelastic transition) 


level_energy_unit: KEV
level_spin_parity: 1/2,(3/2)
level_lifetime_unit: EV
level_comment:
Ground-state decay |G (g|G{-0})=0.0163 eV {I16} 
B(E1)=0.28|*10{+-5} {I3}. B(E1)=0.44|*10{+-5} {I4} (corrected for possible inelastic transition) 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
Ground-state decay |G (g|G{-0})=0.011 eV {I4} 
B(E1)=0.092|*10{+-5} {I25}. B(E1)=0.18|*10{+-5} {I6} (corrected for possible inelastic transition) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
T$From 158.6|g(t), over time period of ~~5.5|*T{-1/2}, using a single exponential fit (2016Do10). Other: 13.8 d {I12} from 314.3|g(t), but 96% {I4} of the intensity of this |g ray was found to be due to |g-ray coincidence summing. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$from two separate measurements, weighted average of 0.281 ns {I28} and 0.258 ns {I18} (2021Da02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as -0.263 {I6} (stat) {I19} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+117Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$transient field integral PAC (1989Ra17) 
MOME2$Coul. ex. reorientation (1989Ra17) 
Deformation parameter=0.108 {I7} 
T from Coul. ex. other: 0.46 ps {I3} in (|g,|g') 
J L=2 in (t,p) and (|a,|a'),(d,d'),({+3}He,{+3}He') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J E0 to 0+ 
T from centroid shift measurement in {+117}Sn(d,p) (1981Ba05). Other: >0.7 ps in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L=4 in (p,p'),(p,p'|g) 
T from Coul. ex. others: <0.7 ns in {+118}Sb |e decay (5.00 h), >1.5 ps in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J J=5 from |g|g(|q) in {+118}Sb |e decay (3.6 min), E1 |g to 4+ 
T from {+118}Sb |e decay (5.00 h). Other: 22 ns {I5} in {+118}In |b{+-} decay (8.5 s) 
MOMM1$differential PAC (1989Ra17). Other: -0.342 {I35} from integral PAC (1989Ra17) 
MOME2$differential PAC, value relative to Q=0.50 for {+116}In (10+ 3548 level) and recalculated (1989Ra17) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
B(E3) from Coul. ex. 
J L=3 in (d,{+6}Li) and (|a,|a'),(d,d'),({+3}He,{+3}He') 
T other: 2.1 ps {I2} from B(E3) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
MOMM1$differential perturbed angular distribution, value does not include the Knight-shift correction (1989Ra17) 
MOME2$differential perturbed angular distribution, value relative to Q=0.41 for 3108 level (1989Ra17) 
J L=7 in (t,p) and (p,p'),(p,p'|g) 
T from in {+118}Sb |e decay (5.00 h). Other: 245 ns {I40} in (|a,2n|g),({+7}Li,p4n|g) 


level_energy_unit: KEV
level_spin_parity: 9+,10+
level_lifetime_unit: US
level_comment:
g-factor: differential perturbed angular distribution, value does not include the Knight-shift correction (1973IsZQ) 
MOME2$differential perturbed angular distribution, value derived from experimental B(E2) (1989Ra17) 
J E2 |g to 7+,8+; no |g to 6+ 
T from (|a,2n|g),({+7}Li,p4n|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
T from (254|g)(1044|g+1229|g)(t) (1962Bo16), (1961Bo13) 
g=-0.063 {I4} 
g: weighted av of -0.060 {I5} (1964DeZZ), -0.068 {I7} (1962Bo16) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: US
level_comment:
T from 1987Lu06. Others: 2.50 |ms {I14} (1980Va13), 2.93 |ms (1973IsZQ), 2.65 |ms {I10} (1986Da05) 
g=0.2432 {I7} (1973IsZQ) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G{-|g0}=0.128 eV {I3} (1974Wo05), 0.135 eV {I8} (1982Be35); |G=0.152 eV {I5} (1974Wo05), 0.340 eV {I25} (1982Be35); 0.84 {I13} as upper limit of |G{-|g0}/|G (1974Wo05) 
J from A{-2} in |g(|q) and |g(pol) (1974Wo05) 
T from weighted av of widths from 1974Wo05 and 1982Be35 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
Deformation parameter=0.120 {I10} from (|a,|a') (1968Ku20) 
E others: 2310 (1961Co07), 2320 (1968Ku20), 2300 (1970Br07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E others: 2920 (1961Co07), 2970 (1968Ku20) 
Deformation parameter(2720+2970)=0.073 {I20} (1968Ku20) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)|^=0.209 {I9} 
Weighted average of 0.216 {I5} (1981Jo03) and 0.199 {I6} (1975Gr30) 0.204 {I4} (1989Sp03) 
Other: Q=-0.23 {I16} (1970St20) 
g(2+)=+0.02 {I10} 
g-factor is based on dynamic magnetic field technique for fast ion in polarized thin iron foil (1980Ha19) 
T from B(E2) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$from B(E3) with E|g=2324.9 keV and Branching given in the adopted levels 
B(E3)|^=0.118 {I10}. From weighted av of 0.097 {I14} (1981Jo03), and 0.122 {I6} (1989Sp03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$2008Ea02 give adopted g factor=+0.10 {I7} from their measurement and earlier g-factor=+0.02 {I10} from 1980Ha19 deduced using the transient field integral PAC technique 
$ Note that g factor has a positive sign in {+118}Sn whereas in {+116}Sn, {+120}Sn, {+122}Sn and {+124}Sn, the sign is negative. This behavior is investigated by 2008Ea02 through shell-model calculations 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J$ ENSDF database lists 7+,8+; but level systematics of even-A Sn nuclei and a recent high-spin study (2010Wa05: Phys Rev C 81, 017301) suggests 8+ 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$ from Adopted Levels of {+118}Sn in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (15,16,17-)
level_comment:
J$assigned by compilers based on suggested |<18+ (2014Is01), and 1087 |g to (15-) suggesting J|>15 from yrast type of excitation in the reaction used in this study 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Transitional E2 matrix element=(+)0.451 {I10} 
$Diagonal E2 matrix element=+0.09 {I12} 
G$From recoil-in-vacuum method 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)({+118}Sn)/B(E2)({+58}Ni)=3.05 {I7} (2017Ku28) 
$B(E2) relative to B(E2)=0.0650 {I12} for the first 2+ state in {+58}Ni, value taken from 2016Pr01 evaluation (At. Data and Nucl. Data Tables 107, 1). This value can be compared with B(E2)=0.203 {I9} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); 0.183 {I9} (from mean lifetime |t=0.79 ps {I4} by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+118}Sn)=-0.324 fm{+2} {I5} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+118}Sn)=-585.6 MHz {I19}(stat) {I40}(syst) for S(p) atomic transition, and -695.0 MHz {I67}(stat) {I33}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) = 0.207 {I9}, average of 0.205 {I7} (2019Ku06) and 0.208 {I16} (2019Ku15) deduced from the transition matrix elements. 
$B(IS2) = 0.214 {I18} (2019Ku06) and 0.246 {I31} (2019Ku15). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J from NMR (1976Fu06); L(d,p),({+3}He,|a)=0 
MOMM1$NMR (2005St24); value relative to |m=+2.2176556 {I6} {+23}Na(g.s.) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
MOMM1$Moss (1973Cr01, 2005St24). Value relative to |m=-1.04728 {I7} for {+119}Sn(g.s.). Other: +0.682 {I3} (Moss (2005St24)) 
MOME2$Moss (2006Ma35). Other values: 0.094 {I4} (Time dependent perturbed angular distributions, 1975Di02, 2005St24); -0.065 {I5} (Moss, 1972Mi02, 2005St24); -0.061 {I3} (Moss, 1987Gr28, 2005St24); -0.109 {I8} (Moss, 1983Ha50, 2005St24). Other: 0.121 {I1} (1997Sv03), 0.094 {I11} ( 
T from 1980La03. Others: 17.87 ns {I11} and 18.48 ns {I30} (1976Ab01), 18.29 ns {I9} (1975Ro14), 18.45 ns {I20} (1971Dr04), 17.75 ns {I12} (1971Be04), and 18.5 ns {I10} (1957Ol05). All data are from IT decay. Note that the weighted av of these values gives T{-1/2}=18.06 ns {I8}, but that of 1980La03 is somewhat more precise. See 1977Do07, 1976Ha66, 1983Ma81 for physical and chemical effects 
J L(d,p),({+3}He,|a)=2; M1 |g to 1/2+ 
Isomer shift |D' r/r=0.00087 {I25} (1984Mu28) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J L(d,p),({+3}He,|a)=5; M4 |g to 3/2+ 
MOMM1 Moss (2005St24). 
MOME2 Value relative to Q=+0.094 {I4} for {+119}Sn (23.87 level) (1975Di02,2005St24). 
T from 1988GeZS. Others: 293.0 d {I13} (1976Ma63), 245 d {I20} (1950Ne52). All data are from IT decay 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J |g(|q) for a composite 921|g from the 920.5 and 921.4 levels, and T{-1/2} from Doppler shift measurement for these levels are mutually consistent with J|p(920.5)=3/2+, and J|p(921.4)=5/2+, not with J|p(921.4)=3/2+ and J|p(920.5)=5/2+, or with J|p=3/2+ or 5/2+ for both states 
T Doppler-broadening in Coul. ex. 
E from (p,p') 


level_energy_unit: KEV
level_spin_parity: GE7/2
level_comment:
J |g to 11/2-; but inconsistent with L=(2) assigned in (d,p); an L=3 or L=4 admixture cannot be ruled out from authors' drawing 


level_energy_unit: KEV
level_comment:
E doublet or broad peak in (p,p'). |?1385 in ({+3}He,|a), reported as peak populated with probably L>2 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
J$|g's to 13/2- and 15/2-; from systematics of the 19/2+ state in {+117-123}Sn 
T off-beam |g|g(t) in ({+80}Se,{+80}Se') 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
J$E2 |g to 23/2-; from energy calculation of h{-11/2} seniority scheme 
T from |g|g(t) in ({+80}Se,{+80}Se') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
T$Weighted average of 285 d {I8} (2003Po21), 293.1 d {I7} (1988GeZS), 293.0 d {I13} (1976Ma63), 245 d {I20} (1950Ne52). 
T For variation of the half-life of 119mSn(293 d) possibly caused by radiation from Mossbauer excitation of the intermediate 23.87-keV level see: 1998Go25, 1999Go25, 1998ViZY, 2002Go20, 2007LoZZ, and 2008Al24. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J |g(|q) for composite 921|g is for the 920.5 and 921.4 levels, and T{-1/2} from Doppler shift measurement for these levels are mutually consistent with J|p(920.5)=3/2+, and J|p(921.4)=5/2+, but not with J|p(921.4)=3/2+ and J|p(920.5)=5/2+, or with J|p=3/2+ or 5/2+ for both states 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
|G=36 {I10} keV (1980Ta04) 
|G=40 {I15} keV (1980Ge01) 
J IAS of the 1/2- 311-keV level in {+119}In 


level_energy_unit: KEV
level_comment:
|G=70 {I20} keV (1980Ge01) 
E from level energy, this state corresponds to the 1044-keV (5/2-) or 1050-keV (5/2+) level in {+119}In. But either assignment is inconsistent with L({+3}He,|a)=(1) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$From Adopted Levels of {+119}Sn in the ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as -0.175 {I4} (stat) {I12} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+119Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L(p,p')=2 
MOMM1$transient field integral PAC (1989Ra17) 
MOME2$Coulomb excitation orientation (1989Ra17) 
T weighted av of 0.652 ps {I10} (from B(E2) in Coul. ex.), 0.617 ps {I14} (from DSA in Coul. ex.), and 0.63 ps {I8} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L(d,{+3}He)(t,|a)=2; |g to 0+; Coul. ex. 
T$from B(E2) (Coul. ex.) in 1981Ba05. Other: 0.7 ps {I+4-2} (n,n'|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J this level is not confirmed in (n,n'|g), where the authors claim that all levels with J=1 to 5 below E=3100 and with J=0 below 2900 are expected to be populated 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
MOMM1$differential PAC (1989Ra17). Other: -0.37 {I5} from integral PAC (1989Ra17) 
MOME2$differential PAC; value recalculated and relative to |m=0.094 {I4} for {+119}Sn (24 level, 3/2+) (1989Ra17) 
J L(p,t)=5; |g|g(|q) and |g|g(pol) in |e decay (5.76 d). 
T from |g|g(t) in |e decay; weighted average of 6.05 ns {I20} (1960Ik01), 5.2 ns {I4} (1961Bo13), 5.53 ns {I6} (1962Bo16), 5.55 ns {I25} (1967Ra26), and 5.55 ns {I3} (1980Mi13). Other: 8.24 ns {I23} (1963Cu04). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
T from |g|g(t); weighted average of 6.05 ns {I20} (1960Ik01), 5.2 ns {I4} (1961Bo13), 5.53 ns {I6} (1962Bo16), 5.55 ns {I25} (1967Ra26), 5.55 ns {I3} (1980Mi13); other 8.2 ns {I23} (1963Cu04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|G{-0}=0.90 {I11} 
T weighted av of 0.72 ps {I6} (1977Ca14,1981Ca10), 0.87 ps {I17} (1966Hr03), and 0.51 ps {I6} (2000Br05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{-0}=5.3 {I5} 
T branching ratio(3157|g)=0.841 {I6} from (n,n'|g), value of 0.825 {I16} cited is a typo by authors 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
|G=0.030 eV {I12} (1978Ka30). 
J from |g(|q) (1978Ka31) 
E uncertainty is assigned by the evaluators 


level_energy_unit: KEV
level_comment:
E other: 1180 (|a,|a') 
BE2 from ({+17}O,{+17}O'). Other: 0.1508 in ({+3}He,{+3}He') (1988Bu21) 
S others: 0.134 {I19} in (|a,|a') (1970Br07), 0.005 in ({+3}He,{+3}He') (1988Bu21), 0.119 {I10} in (p,p') (1968Ma34) 
S=0.11 (|a,|a') (1968Ku20) 


level_energy_unit: KEV
level_comment:
E 2390 in (|a,|a') (1968Ku20) 
S=0.12 in (|a,|a') (1968Ku20) B(E2)=0.090 {I24} 
BE2 Weighted av of 0.159 {I14} in (p,p') (1970Be20), 0.069 {I14} in (|a,|a') (1970Br07), and 0.075 {I8} in ({+17}O,{+17}O') 
S other: 0.126 {I18} (|a,|a') 
%EWSR=9.5 {I18} ({+3}He,{+3}He') (1981Ya02) 


level_energy_unit: KEV
level_comment:
E from 1980Be50 in (|a,|a'). Other: 13100 {I500} ({+17}O,{+17}O') 
(GQR) |G=3.7 {I5} MeV, %EWSR=70 {I15} (1980Be50); |G=3.2 MeV {I4}; %EWSR=50 {I10} ({+17}O,{+17}O') 
E 13240 {I130}; GQR, |G=2.88 {I20}, %EWSR=135 {I27} (1988Sh38) 


level_energy_unit: KEV
level_comment:
E from 1988Sh38. Other: 15700 {I500} ({+17}O,{+17}O') 
(GMR) |G=3.92 {I35}, %EWSR=94 {I20} (1988Sh38) 


level_energy_unit: KEV
level_comment:
E from 1980Be50 
(GMR) |G=3.3 {I5} MeV. %EWSR=100 {I20} (1980Be50); |G=4.1 MeV {I5}; %EWSR=135 {I30} 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E from (1981Be33). Other: 24500 {I1500} in ({+3}He,{+3}He') (1981Ya02) 
|G=8 MeV {I1}, %EWSR=14 {I3} (1981Be33). 
(GDR) |G|?7 MeV. %EWSR=95 {I29} (1981Ya02) 
L from ({+3}He,{+3}He') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted av of 0.203 {I4} (1970St20), 0.197 {I4} (1975Gr30), and 0.194 {I3} (1989Sp03) 
G other: 0.05 {I20} (1972SiZI). 
T from B(E2). Other: 0.617 ps {I14} from DSA (1972SiZI). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 for the transition from 1171 level to 2097 level. Value normalized to B(E2)(g.s. to 1171 level)=0.203 {I4}, and I|g(925|g)/I|g(2097|g)=1.0 {I1} and |d=-1.43 {I25} for 925|g assumed (1981Jo03) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
BE2 for the transition from 1171 level to 2159 level. Value normalized to B(E2)(g.s. to 1171 level)=0.203 {I4} (1981Jo03) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2 for the transition from 1171.5 level to 2194 level. Value normalized to B(E2)(g.s. to 1171 level)=0.203 {I4}, and negligible branching to 2097 level assumed (1981Jo03). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3 Weighted av of 0.131 {I10} (1989Sp03), 0.090 {I17} (1981Jo03), and 0.13 {I6} (1964Al26). Value from 1981Jo03 is normalized to B(E2)(g.s. to 1171 level)=0.203 {I4} 


level_energy_unit: KEV
level_spin_parity: (2+&6+)
level_comment:
E unresolved peak. DWBA shows the doublet with components having L=2 (10%) and L=6 (90%) respectively 


level_energy_unit: KEV
level_spin_parity: (1-&8+)
level_comment:
E unresolved peak. DWBA shows the doublet with components having L=1 (3%) and L=8 (97%) respectively 


level_energy_unit: KEV
level_spin_parity: (3-&4+)
level_comment:
E unresolved peak. DWBA shows the doublet with components having L=3 (40%) and L=4 (60%) respectively 


level_energy_unit: KEV
level_spin_parity: (3-&7-)
level_comment:
E unresolved peak. DWBA shows the doublet with components having L=3 (10%) and L=7 (90%) respectively 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$2008Ea02 give adopted g factor=-0.12 {I5} from their measurement and earlier g-factor=-0.14 {I7} from 1980Ha19 deduced using the transient field integral PAC technique 


level_energy_unit: KEV
level_spin_parity: 13-
level_lifetime_unit: NS
level_comment:
T$measured from time distribution of double coincidence gates on 241.7|g and 556.9|g, 1190.3|g (2014Is04) 


level_energy_unit: KEV
level_spin_parity: 15-
level_lifetime_unit: NS
level_comment:
J$higher spin value excluded by the presence of the strong decay sequence of 241.7|g, 253.2|g, 661.0|g, and 1253.6|g transitions connecting it to 7- isomer. Please see footnotes associated with this |g sequence. 
T$measured from time distribution of prompt and delayed gates on 783.2|g, 1622.1|g and 241.7|g, 556.9|g, 1190.3|g (2014Is04) 


level_energy_unit: KEV
level_spin_parity: 16+
level_comment:
J$the strong yrast population favors J|p=16+, as this is consistent with the observed decay and favors J|p=14+ proposed for the 5220-keV level depopulated by 1127.6|g to the lowest 12+ state (2014Is04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$From recoil-in-vacuum method with sign taken from transient field measurements (see reference in 2015Al24) 
$Transitional E2 matrix element=(+)0.458 {I10} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)({+120}Sn)/B(E2)({+58}Ni)=2.90 {I9} (2017Ku28) 
$B(E2) relative to B(E2)=0.0650 {I12} for the first 2+ state in {+58}Ni, value taken from 2016Pr01 evaluation (At. Data and Nucl. Data Tables 107, 1). This value can be compared with B(E2)=0.210 {I9} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); 0.191 {I10} (from mean lifetime |t=0.97 ps {I5} by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+120}Sn)=-0.206 fm{+2} {I5} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+120}Sn)=-360.5 MHz {I13}(stat) {I27}(syst) for S(p) atomic transition, and -448.6 MHz {I80}(stat) {I22}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$transition quadrupole moment, Q{-02}=1.468 {I-24+33} (2019Ku17) 
T$2019Ku17 state that feedings from 4{-1}{++}, 0{-2}{++} and 2{-2}{++} states are included in the DSAM analyis. The feeding from the 4{-1}{++} is expected to be largest at |? 10%, and changes the deduced lifetime within the quoted uncertainties (2019Ku17). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) = 0.216 {I11}, average of 0.215 {I9} (2019Ku06) and 0.217 {I21} (2019Ku15) deduced from the transition matrix elements. 
$B(IS2) = 0.209 {I21} (2019Ku06) and 0.242 {I38} (2019Ku15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$measured relative to {+112}Sn, from the ratio B(E2)({+120}Sn)/B(E2)({+112}Sn)=0.80 {I4} (2024Be28) 
$|G{-0}=0.67 meV {I5} (2024Be28) 
$I{-s}=8.1 eVb {I6} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
MOMM1$ABLFS (2005St24); value relative to |m for {+115}Sn, {+117}Sn, {+119}Sn 
MOME2$ABLFS (2005St24) 
J atomic beam J=3/2 (1978LeZA). L=2 in (t,p), (t,d), (p,d). 
T from weighted average of 27.06 h {I4} (1968Er03), 27.5 h {I5} (1950Ne52), 27.0 h {I6} (1963Ma20), 26.85 h {I20} (1966La13); others: 28 h (1948Li02), 25.5 h {I1} (1968Sn01) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1$ABLFS (2005St24); value relative to |m=-1.04728 {I7} for {+119}Sn 
MOME2$ABLFS (2005St24) 
T from 2002Re18. Others: 55 y {I5} (1971Fl03), 40 y {I10} (1971Or01), 25 y (1962Dr01) 
J from LASER spectroscopy (1986An24). F-K-plot for the |b{+-} decay to 7/2+ level has |DJ=2 yes shape (1968Sn01). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L=2 in (t,d), (t,p), (p,d). Fed from only one of sixteen J|p=1/2+, 1/2-, or 3/2- (n,|g) resonances rules out J|p=3/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$L=3 in (d,p). |g to 11/2-. For J|p=5/2-, the 943|g would be M3, and the T{-1/2}>17 |ms from B(M3)(W.u.)<10. But J|p contradicts L=0 in (t,d). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2-)
level_comment:
J$from |g to 11/2- and analogy of the 19/2+ and 15/2- states in odd-mass Sn excitation in in-beam spectroscopy 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2-)
level_comment:
J$from from |g to 11/2- and analogy of the 13/2- states in odd-mass Sn excitation in in-beam spectroscopy 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
J$from |g's to (13/2-) and (15/2-), T{-1/2}, and analogy of the 19/2+ and 15/2- states in {+117}Sn in in-beam spectroscopy 
T$from |g decay in {+124}Sn({+80}Se,{+80}Se{+3}n|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J L=3 in (t,p); J=7/2 is consistent with analyzing power in (pol p,p) IAR 
E$average of 3326 {I15} from (t,p) and 3314 {I15} from (t,d) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
E$From Adopted Levels of {+121}Sn in ENSDF database. 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$reported as -0.056 {I4} (stat) {I4} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as -0.093 {I3} (stat) {I7} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+119Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
Nuclear rms charge radius=4.6657 fm {I10} (2004An14) 
T$>5.8|*10{+13} y for neutrino-less decay mode (1952Fr23) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$from transient field integral perturbed angular correlation (1980Ha19,2005St24), Q from Coulomb excitation reorientation (1975Gr30,2005St24), reported as Q < +0.14 > -0.28 
J L=2 in (p,p') 
T from B(E2) in Coulomb excitation; other: 0.62 ps {I12} from |G in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L=2 in (p,p') 
T$others: 0.19 ps {i5} from |G in (|g,|g'); >0.78 ps from B(E2) in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: US
level_comment:
T$weighted average of 7.2 |ms {i10} (1979Ch10) and 9.3 |ms {i23} (1979Fo10); measured from (1121|g)(|g)(t) (1979Fo10, 1979Ch10) 


level_energy_unit: KEV
level_comment:
In 1970Be20, the 2390-keV level was not separated from 2412-keV level, but authors suggested L=7 for the 2390-keV level based on the energy systematics and the cross-section value 


level_energy_unit: KEV
level_comment:
$BE3|^: weighted mean of 0.146 (1968Ma34), 0.140 (1970Be20) and 0.1259 (1989Va02) from (p,p') 
$others: 0.146 {i28} (1968Ma34), 0.12 {i6} (1966Ba11,2002Ki06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 Average of 0.196 {i4} (1970St20), 0.188 {i4} (1975Gr30) and 0.182 {I3} (1989Sp03); recommended value B(E2)=0.192 {i4} (2001Ra27) 
T From B(E2)=0.189 {i4}; branching=1.0 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$deduced from the lineshape of the 3{+-} to 2{++} E1 transition, and hence it should be considered as an upper limit. If all decay branches are taken into account, then T{-1/2}=0.073 ps {I14}, which is in better agreement with the value of 0.079 ps {I+5-3} adopted in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 2+&7-
level_comment:
L$ |s(|q) is accurately reproduced by considering 30% admixture of L=7 and 70% that of L=2 for a doublet 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
MOMM1$ deduced from g-factor=-0.044 {I19} (2011Wa15), which is the average of the results -0.048 {I20} and -0.017 {I50} from the inner and outer pairs of Si detectors, respectively, both of which were corrected for feeding from the higher-lying states with an adopted value of 0.0 {I5} as the g-factor for the 3- state since it was not measured in the present work. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
MOMM1$ deduced from g-factor=-0.18 {I17} (2011Wa15), which is the average of the results -0.20 {I18} and -0.03 {I52} from the inner and outer pairs of Si detectors, respectively. 


level_energy_unit: KEV
level_spin_parity: 15-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M4
level_comment:
T$from |g|g(t) (2014Is04), compared with 146 ns {I15} in 2012As05: Phys. Rev. C 85, 054316. This half-life required that the level be assigned to {+122}Sn based on cross-coincidence with complementary fission fragments 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Transitional E2 matrix element=(+)0.445 {I10} 
$Diagonal E2 matrix element=-0.11 {I12} 
G$From recoil-in-vacuum method 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)({+122}Sn)/B(E2)({+58}Ni)=2.70 {I6} (2017Ku28) 
$B(E2) relative to B(E2)=0.0650 {I12} for the first 2+ state in {+58}Ni, value taken from 2016Pr01 evaluation (At. Data and Nucl. Data Tables 107, 1). This value can be compared with B(E2)=0.198 {I9} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); 0.164 {I10} (from mean lifetime |t=1.29 ps {I8} by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+122}Sn)=-0.097 fm{+2} {I3} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+122}Sn)=-167.3 MHz {I16}(stat) {I13}(syst) for S(p) atomic transition, and -206.3 MHz {I75}(stat) {I10}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) = 0.191 {I9}, average of 0.191 {I4} (2019Ku06) and 0.191 {I17} (2019Ku15) deduced from the transition matrix elements. 
$B(IS2) = 0.189 {I15} (2019Ku06) and 0.216 {I30} (2019Ku15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$B(E3) = 0.082 {I14} from 2019Ku15. Other: 0.077 (2019Ku06). 
$B(IS3) = 0.043 {I8} (2019Ku06) and B(IS3) = 0.074 {I18} (2019Ku15). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_comment:
J$spin from atomic beam laser spectroscopy (1986An24); |p=- from L(d,p)=L(d,t)=5 from 0+ 
T$weighted average of 129.0 d {I5} (1966La13) and 129.6 d {I6} (1968Er03). Others: 130 d {I5} (1949Le05), 126 d {I5} (1950Ne52), 125 d {I3} (1951Co34). 
MOMM1,MOME2$from thermal atomic beam LASER spectroscopy (1986An24). See also 2014StZZ and 2016St14 compilations 
$Nuclear rms charge radius=4.6665 fm {I23} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin from atomic beam (1968Ch38); |p=+ from L(d,p)=L(d,t)=2 from 0+ 
T$weighted average of 40.06 m {I1} (1990Ab06), 40.08 m {I7} (1968Er03), 41.5 m {I5} (1948Mo33), and 40 m {I1} (1949Le05). Others: 41.8 m {I5} (1977Ti03), 38.9 m {I4} (1970OsZZ), 39.5 m (1949Du15). 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
J$619.0|g M1,E2 to 11/2-; 536.4|g from 7/2+; possible |b{+-} feeding from 9/2+ parent; level systematics of 9/2- in odd Sn isotopes. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$719.5|g to 1/2+, 284.7|g from 7/2+, 1331|g from (9/2)+. 1970Ca01 also suggest J=5/2 in (p,d) for a level at 899. 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$769.5|g M1 to 1/2+; excitation function in (d,p|g) favors 3/2+. Other: 1970Ca01 suggest J=5/2 in (p,d). 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,t)=4 and L(p,d)=(4) from 0+; 1019.7|g to 3/2+. 
T$from (|b)(1019.7|g)(t) (1976Fo02) in {+123}In |b{+-} decay (6.15 s). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E$L=4 component of 1185 level in (p,d) suggest excitation of 1155 level 
J$L(d,p)=L(d,t)=4 from 0+; 1130.5|g E2 to 3/2+ 
T$From (|b)(1130.5|g)(t) (1976Fo02). 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$from (d,t). Others: 1784 from (d,p), 1780 from (p,d) 
J$L(p,d)=L(d,t)=2 from 0+; 1970Ca01 in (p,d) suggest J=5/2 from possible J-dependence of |s(|q). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2+
level_comment:
J$L(p,d)=2 and L(d,p)=(2) from 0+; 1970Ca01 in (p,d) suggest J=3/2 from possible J-dependence of |s(|q) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
J$allowed |b{+-} feeding from 9/2+ parent gives 7/2+,9/2+,11/2+; 1131|g-719.5|g cascade to 1/2+ disfavors 11/2+; 2001.2|g to 11/2- disfavors 7/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2+
level_comment:
E$from (d,p). Others: 2020 from (p,d), 2010 {I20} from (d,t) 
J$L(p,d)=L(d,t)=2 from 0+; 1970Ca01 in (p,d) suggest J=3/2 from possible J-dependence of |s(|q) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_lifetime_info: ;ERR=?;ISO=M2
level_comment:
J$band assignment 
T$from delayed |g versus beam pulse (1994Ma48,1995Da26) in ({+80}Se,X|g). No |DT{-1/2} value have been given. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$from (d,p). Other: 2615 {I3} from (n,|g) E=res is questionable; 2620 from (p,d) 
J$L(p,d)=0 for a level at 2620 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
E$other: 3130 from 1972Ca33 could correspond to 3113+3151; 3150 (1964Ne10) 
S$other: 0.12 for a level at 3140 (1967Sc12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
E$other: 4033 {I15} in 1972Ca33 could correspond to this level; 4043 (1964Ne10) 
S$other: 0.11 for a level at 4050 with L=(1) (1967Sc12) 


level_energy_unit: KEV
level_comment:
E$Unresolved doublet (1982Fl02) 
S$4.5 {I15} for L=5, 3.0 {I4} for L=2 obtained by 1982Fl02 from peak angle systematics. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E,L$from 1982Fl02. 1970Ca01 report L=2+4, suggesting a possible contribution from 7/2+ level at 1155. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$reported as -0.024 {I4} (stat) {I2} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as -0.012 {I3} (stat) {I1} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+123Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$<r{+2}>{+1/2}=4.6759 fm {i12} (2004An14, evaluation) 
$ Mass excess=-88228 {I20} with Penning trap mass spectrometer ISOLTRAP (2005Si34) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 transition to 0+ 
MOMM1 From transient field integral PAC (1980Ha19,1989Ra17). See also 2005St24 compilation. 
MOME2 From Coul. ex. reorientation (1975Gr30,1989Ra17). See also 2005St24 compilation. 
T from B(E2) in Coul. ex. Others: 0.93 ps {I13} from (|g,|g'); > 1.2 ps from (n,n'|g). 2001Ra27 evaluation gives 0.917 ps {I22}. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L=4 in (p,p'); L=5 in (t,p) but its assignment is questionable. 
T from B(E2) in Coul. ex. Other: >0.8 ps from DSA in (n,n'|g) 
B(E4)(e,e')=0.014 {I3} 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
J systematics of 10+ state in {+116}Sn-{+130}Sn isotopes 
T from measurements with pulsed beam in {+124}Sn IT decay (1992Br06) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J p(|q) in (p,p') through f{-7/2} analog resonance allows (3-,5-). log| {Ift}=6.26 from (1)+ rules out 5- 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|G{+2}{-|g0}/|G{-|g}=0.41 {I10} 
T from |G{+2}{-|g0}/|G{-|g} and branching(2426|g)=0.65 {I5} (see adopted gammas) 
|G{+2}{-|g0}/|G{-|g} from 1994Go25. 2005Br05 gives 2.1 {I11} but it seems to be misprinted. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|G{+2}{-|g0}/|G{-|g}=8.9 {I10} 
T from |G{+2}{-|g0}/|G{-|g} and branching(3214|g)=0.85 {I7} (see adopted gammas) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: PS
level_comment:
$|G{+2}{-|g0}/|G{-|g}=11.3 {I17} 
T from |G{+2}{-|g0}/|G{-|g} and branching(3697|g)=0.85 {I8} (see adopted gammas) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|G{+2}{-|g0}/|G{-|g}=6.6 {I10} 
T from |G{+2}{-|g0}/|G{-|g} and branching(3697|g)=0.78 {I7} (see adopted gammas) 


level_energy_unit: KEV
level_comment:
|b{-2}=0.140 {I10} (1992Ke07). Others: 0.108 {I7} (1968Ma34), 0.109 {I11} (1989Va02); and 0.119 {I4} (1970Be20), see comment on |b{-2} for 2428L 


level_energy_unit: KEV
level_comment:
|b{-3}=0.140 {I10} (1992Ke07); others: 0.133 {I20} (1968Ma34), 0.123 {I12} (1989Va02); and 0.138 {I7} (1970Be20) 


level_energy_unit: KEV
level_comment:
E others: 3485 {I10} (1965Al11), 3509 {I10} (subtracted 7 keV from 1970Be20) 
|b{-3}=0.038 (1970Be20) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
|b{-2}=0.098 (1990Bu25). Others: 0.119 {I12} deduced from deformation length (1970Br07); 1979Sa05 give 0.076 {I2} for nuclear deformation and 0.082 {I2} for charge deformation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from 1979Sa05; other: 2530 (1970Br07) 
|b{-3}=0.118 (1990Bu25). Others: 0.104 {I10} deduced from deformation length (1970Br07); 1979Sa05 give 0.072 {I3} for nuclear deformation and 0.15 {I2} for charge deformation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 Average of 0.161 {I4} (1970St20) and 0.170 {I4} (1975Gr30). Others: 0.22 {I4} (relative value to B(E2)(0+ to 2+, {+122}Sn)=0.26 {I5}) (1961An07), 0.18 {I2} (1968La26), 0.188 {I13} (1970Kl06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B(E2)(2+ to 4+)=0.032 {I4} 
BE2 From 1981Jo03, value renormalized to B(E2)(0+ to 2+)=0.166 (evaluators) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
MOMM1$ deduced from g-factor=-0.067 {I14} (2011Wa15), which is the average of the results -0.055 {I18} and -0.083 {I21} from the inner and outer pairs of Si detectors respectively, both of which were corrected for feeding from the higher-lying states with an adopted value of 0.0 {I5} for the g-factors of both the 4+ and 3- states since they were not measured in the present work. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$ E2 matrix element=(+)0.403 {I7} (2011Al25). Input E2 matrix elements for other states are listed in table I of 2011Al25 
$ Diagonal E2 matrix element=+0.04 {I9} without including high-lying states; -0.08 {I11} (positive interference term) and -0.05 {I11} (negative interference term) with high-lying states included 
$ Q=+0.03 {I7} without including high-lying states; -0.06 {I8} (positive interference term) and -0.04 {I8} (negative interference term) with high-lying states included 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ from g|t=0.143 {I13}, average of six values obtained using carbon and titanium targets. Sign is not given by this method, it is taken from transient-field technique (2012Ku41: Phys. Rev. C86, 034319) 
T$ from B(E2)(up)=0.162 {I6} (2011Al25: Phys. Rev C84, 061303(R)) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$From recoil-in-vacuum method with sign taken from transient field measurements (see reference in 2015Al24) 
$Transitional E2 matrix element=(+)0.406 {I8} 
$Diagonal E2 matrix element=-0.11 {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2)({+124}Sn)/B(E2)({+58}Ni)=2.22 {I5} (2017Ku28) 
$B(E2) relative to B(E2)=0.0650 {I12} for the first 2+ state in {+58}Ni, value taken from 2016Pr01 evaluation (At. Data and Nucl. Data Tables 107, 1). This value can be compared with B(E2)=0.165 {I7} (from Coul. Ex., 2015Al24: Phys. Rev. C92, 041303(R)); 0.148 {I15} (from mean lifetime |t=1.48 ps {I15} by DSAM, 2011Ju01: Phys. Lett. B695, 110) 
T$deduced by compiler from B(E2) in 2017Ku28 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) = 0.166 {I11}, average of 0.165 {I4} (2019Ku06) and 0.167 {I21} (2019Ku15) deduced from the transition matrix elements. 
$B(IS2) = 0.166 {I14} (2019Ku06) and 0.185 {I29} (2019Ku15). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_comment:
J L=5 in (d,p), (|a,{+3}He); |DJ=2, yes shape to 7/2{++} from F-K plot. 
T Value recommended by 1968Er03 based on their value of 9.67 d {I4}, along with 9.4 d {I1} from 1950Ne52 and 9.625 d {I25} from 1966La13. Others: 10 d (1939Li04), 9.5 d (1949Ne06), 10.0 d {I3} (1949Le05) 
MOMM1$LASER spectroscopy (1986An24). See also 2005St24 compilation. 
MOME2$LASER spectroscopy (2004Le13,2005Le34). See also 2005St24 compilation. 
$<r{+2}>{+1/2}=4.678 fm {i3} (2004An14, evaluation). 2005Le34 gave measured value of 4.677 fm {i3}. 
Configuration=(|n 1h{-11/2}) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J L=2 in (d,p), M1+E2 |g from 1/2+ 
T From 1968Er03. Others: 9 min (1939Li04), 10 min (1947Su21), 9.8 min {I2} (1949Le05), 9.5 min {I1} (1950Ne52) 
MOMM1$LASER spectroscopy (2004Le13,2005Le34). See also 2005St24 compilation. 
MOME2$ LASER spectroscopy (2004Le13). 2004Le13 gave measured Q value of +0.79 {I7}, but 2005Le34 by the same author gave no value because the weakest line was buried in the strongest component of the 11/2{+-} state and could not be isolated. See also 2005St24 compilation. 
$<r{+2}>{+1/2}=4.676 fm {i3} (2005Le34). 
Configuration=(|n 2d{-3/2}) 


level_energy_unit: KEV
level_comment:
L $ For 3830 (possible doublet for 3820+3850) in 1973Bi09 
S $ For 3830 (possible doublet for 3820+3850) in 1973Bi09. 0.10 for L=1 component; 0.02 for L=5 component 


level_energy_unit: KEV
level_comment:
L $For 3940 (possible doublet for 3920+3970) in 1973Bi09 
S 0.02 for L=(3) component; 0.01 for L=5 component 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$reported as +0.018 {I6} (stat) {I1} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as +0.061 {I2} (stat) {I4} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+125Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$weighted av. of 1.98|*10{+5} y {I6} from plasma-mass spectrometry (2009Bi07), 2.35|*10{+5} y {I7} from thermo-ionnisatio mass spectrometry (1999Ob04), 2.33|*10{+5} y {10} from plasma-mass spectrometry (2005Ca14), 2.07|*10{+5} y {I21} from specific activity measurement (1996Ha45) and 2.5|*10{+5} y {I2} from radiochemical method (1996Zh16). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L(t,p)=2. 
T$weighted av. of 1.15 {I7} ps deduced from B(E2)=0.127 {I8} (2011Al25) and 1.04 {I14} ps from DSAM (2012Ku24) in Coulomb ex. 
MOMM1$from Coulomb ex. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J$ L(d,{+6}Li)=5, see comment in footnote ; L(t,p)=6 is inconsistent with 5- 
T$ from |b|g(t) in {+126}In |b{+-} decay (2012As05) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: US
level_comment:
J L(d,{+6}Li)=7. 
T$weighted av. of 6.6 |ms {I14} from |g|g(t) in {+126}In |b{+-} decay (1979Fo10) and 5.9 |ms {I8} in {+9}Be({+238}U,X|g) (2010Il01). 
MOMM1$ in {+9}Be({+238}U,X|g) (2010Il01) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
J$ systematics 
T$weighted av. of 7.7 |ms {I5} in {+124}Sn({+136}Xe,X|g), ({+238}U,X|g) (2000Zh47), 7.5 |ms {I3} in {+9}Be({+238}U,X|g) (2010Il01) and 7.6 |ms {I4} (1998GeZX). 


level_energy_unit: KEV
level_spin_parity: (16+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$a member of higher-seniority positive high-spin levels 
T$estimated in 2012As05 from non-observation of any delayed component below the 16+ state 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7-
level_lifetime_unit: US
level_comment:
T$from 909|g(t) + 1141|g(t) using a two-component fit (2010Il01). The half-life of the topmost 10+ isomer at 2565 keV was fixed to T{-1/2}=7.5 |ms {I3} 
MOMM1$from g=-0.098 {I9}, measured using the time-differential perturbed angular distribution technique 
CONF$|n{+2} (h{-11/2}{+-1},d{-3/2}{+-1}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$from g factor=0.12 {I3} (2013Al10), Sign from g factor=-0.25 {I21} (2012Ku24) 
BE2$from 2011Al25. 
T$from DSAM (2012Ku24) 
$Q=+0.08 {I11} without including high-lying states; -0.02 {I11} (positive interference term) and +0.01 {I11} (negative interference term) with high-lying states included (2011Al25) 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: NS
level_comment:
T$from |g(t) (2012As05); time distribution of 570 or 1030 transition. ;See 126 ns {|20} in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: NS
level_comment:
T$measured from time distribution of double coincidence gates on 181|g and 571|g, 1031|g (2014Is04). The half-life for this level is significantly shorter compared to 160 ns {I20} (2012As05) in {+238}U({+12}C,F|g). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_comment:
MOMM1$laser spectroscopy (2004Le13,2005Le34) 
Configuration=(|n h{-11/2}) 
J log| {If{+1u}t}=9.45 to 7/2+, syst of 11/2- states in odd-Sn isotopes. The result of theoretical calculation of |m=-1.225 (2005Le34) confirms the h{-11/2} assignment. 
T weighted av of 2.05 h {I5} (1956Ca32), 2.15 h {I10} (1962Dr01), 2.2 h {I2} (1962Ha16), 2.10 h {I5} (1962Uh01), 2.22 h {I15} (1963La15), 2.45 h 30 (1963Ma20). Other: 1.5 h (1951Ba41) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
MOMM1,MOME2$laser spectroscopy (2004Le13,2005Le34) 
Configuration=(|n d{-3/2}) 
J log| {Ift}=5.6 to 5/2+, syst of 3/2+ states in odd-Sn isotopes. The result of theoretical calculation of |m=+0.831 (2005Le34) confirms the d{-3/2} assignment. 
T from (1974Gr29). Others: |?2.5 min (1962Dr01), 4.6 min {I4} (1962Ha16), 4.1 min {I8} (1963Tr10), 4.4 min {I5} (1965Ka08), 4.0 min {I3} (1965Ka08), 4.4 min {I1} (1970OsZZ), 3.5 min {I5} (1977Lu06) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
Configuration=({+128}Sn 2+)(|n (h{-11/2}){+-1}) 
J M1,E2 |g to 11/2-, systematics of odd-Sn isotopes favors 9/2- 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J In {+127}In(1.09 s, 9/2+) decay, 11 levels assigned (7/2 or 9/2) make |g transitions to this level, and this level goes to 3/2+ level by |g. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
Configuration=({+128}Sn 2+)(|n (d{-3/2}){+-1}) and/or ({+128}Sn 2+)(|n (s{-1/2}){+-1}) 
J log| {Ift}=7.0 from (1/2-), |g to (1/2+) and (5/2+) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
Configuration=({+128}Sn 2+)(|n (h{-11/2}){+-1}) 
J |g to 11/2- and (9/2-), systematics in odd-Sn isotopes favors 7/2- 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
Configuration=({+128}Sn 2+)(|n (d{-3/2}){+-1}) and/or ({+128}Sn 2+)(|n (s{-1/2}){+-1}) 
J log| {Ift}=6.5 from (1/2-) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
Configuration=({+128}Sn 2+)(|n (d{-3/2}){+-1}) and/or ({+128}Sn 2+)(|n (s{-1/2}){+-1}) 
J log| {Ift}=7.1 from (1/2-) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J |g from (15/2+), |g to (11/2-): from systematics of Sn isotopes (2000Pi03). Though 2004Ga24 have also proposed that this level is 13/2-, the |b-ray feeding intensity obtained from in and out |g-ray balance (log| {Ift}=6.4 from (21/2-)) contradict this assignment. 2004Ga24 suggest this contradiction is due to unobserved |g-rays. 
Configuration=({+128}Sn 2+)(|n (h{-11/2}){+-1}) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
The order of feeding 2103.8|g and 406.9|g is not known, and so this level may actually be at 3198.3. 


level_energy_unit: KEV
level_comment:
J log| {Ift}=6.9 from (21/2-), |g to (9/2+): In view of the difference of large Q value (6510) and maximum energy of level proposed (3899.5) in the T{-1/2} =1.04 s |b-decay, it is likely that the decay scheme is not yet complete. Only one |g feeding to this level from decay process of the 4.52 |ms isomer is reported. The discrepancy between the log {Ift} and possible multipolarity of decaying |g could be attributed to not yet reported feeding |g 's to this level (evaluator). 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
Configuration=(|n (d{-3/2}){+-1})(|n (h{-11/2}){+-2}) (2008Lo07) 
J from systematics of odd Sn isotopes (2000Pi03), |g to (15/2+) 
T$weighted average of 4.4 |ms {I2} (2008Lo07), 4.8 |ms {I3} (2004Ga24) and 4.5 |ms {I3} (2000Pi03); other: 3.1 |ms {I9} (1980De35) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_comment:
Configuration=(|n (d{-3/2}){+-1})(|n (h{-11/2}){+-2}) (2008Lo07) 
J (E2) |g to (19/2+), from systematics of odd Sn isotopes 
T weighted average of 0.9 |ms {I3} (2008Lo07) and 1.26 |ms {I15} (2004Ga24) 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_comment:
J$members of configuration=(|n (h{-11/2}){+-3}) quasiparticle multiplet from shell model calculation (2008Lo07) 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: US
level_comment:
T$From (2008Lo07) 
J$member of configuration=(|n (h{-11/2}){+-3}) quasiparticle multiplet from shell model calculation (2008Lo07) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
Configuration=(|n h{-11/2}{+-1}d{-3/2}{+-1}){-7-}) (|n g{-7/2}){+-1}) 
J log| {Ift}=4.5 from (21/2-), |g to (15/2-) 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
Configuration=(({+128}Sn 5-)(|n h{-11/2}{+-1})) 
T$weighted average of 4.4 |ms {I2} (2008Lo07), 4.8 |ms {I3} (2004Ga24) and 4.5 |ms {I3} (2000Pi03); other: 3.1 |ms {I9} (1980De35) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_comment:
T weighted average of 0.9 |ms {I3} (2008Lo07) and 1.26 |ms {I15} (2004Ga24) 
Configuration=(({+128}Sn 7-)(|n h{-11/2}){+-1}) 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
T$weighted average of 4.4 |ms {I2} (2008Lo07), 4.8 |ms {I3} (2004Ga24) and 4.5 |ms {I3} (2000Pi03); other: 3.1 |ms {I9} (1980De35) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$reported as +0.053 {I3} (stat) {I4} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as +0.111 {I3} (stat) {I8} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+127Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 59.1 min {I5} (1976Nu01), 60.0 min {I4} (1968Er03), 59.0 min {I1} (quoted in 1968Er03), 59.8 min {I8} (1964St28). Others: 59 min {I1} (1962Uh01), 62 min {I2} (1962Dr01), 57 min {I4} (1962Ha16), 58 min {I5} (1962Dr01). 
T$isotope shift=0.801 GHz {I12}, charge radius=4.692 fm {I4} was measured in 2005Le34 
MOME2$from Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: PS
level_comment:
J$log| {Ift}=5.86 from (3)+; |g to 0+; syst of the first excited state of even-even Sn isotopes. 
T$from B(E2) in Coulomb excitation (2011Al25) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_comment:
$No |b{+-} transition to {+128}Sb (8-) g.s. was observed (1979Fo10), and the authors do not give any limit 
T$from {+128}Sn IT decay (6.5 s) (1979Fo10) 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
T$weighted average of 2.69 |ms {I23} in {+128}In |b{+-} decay (0.72 s) and 3.00 |ms {I15} in {+9}Be({+136}Xe,X|g) 
G$TDPAD method (2010At03). Comparison with shell-model calculations confirm dominance of |nh{-11/2}{+-2} configuration. 
J$E2 |g to (8+); high spin ordering. However, log| {Ift}=5.97 from (8-) suggest (7-,8-,9-) 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: NS
level_comment:
J$from comparison to shell-model calculation in {+9}Be({+136}Xe,X|g) 
T$from time distribution of delayed |g rays in {+9}Be({+136}Xe,X|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
G$TDPAD method (2010At03). Comparison with shell-model calculations confirm dominance of |nh{-11/2}{+-2} configuration. 
T$from {+128}Sn |b{+-} decay (0.72 s). 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: NS
level_comment:
T$from time distribution of delayed |g rays (2011Pi05) 
$Proposed configuration=|nh{-11/2}{+-3}d{-3/2}{+-1}, with four neutron holes in {+132}Sn maximally aligned to J|p=15-. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: PS
level_comment:
$E2 matrix element=(+)0.282 {I9} (2011Al25). Input E2 matrix elements for other states are listed in Table I of 2011Al25 
$Diagonal E2 matrix element=-0.0 {I24} without including high-lying states; -0.17 {I25} (positive interference term) and +0.11 {I25} (negative interference term) with high-lying states included 
$Q=-0.02 {I18} without including high-lying states; -0.13 {I19} (positive interference term) and -0.08 {I19} (negative interference term) with high-lying states included 
T$from B(E2) (2011Al25) 
G$from g|t=0.55 {i12}, average of six values obtained using carbon and titanium targets. Sign is not given by this method, it is taken from systematics of even-A Sn nuclei 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+128}Sn)=+0.165 fm{+2} {I10} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+128}Sn)=+273.2 MHz {I53}(stat) {I26}(syst) for S(p) atomic transition, and +338.9 MHz {I49}(stat) {I21}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$level energy, with its uncertainty, kept fixed in least-squares adjustment 
$Energy and decay mode from {+128}Sn Adopted Levels in the ENSDF database (Feb 2015 update) 


level_energy_unit: KEV
level_spin_parity: (15+)
level_comment:
E$new level proposed by 2020Ne06 
J$from 2020Ne06 
$Configuration=|n[0g{-7/2}{+-1},1d{-3/2}{+-1},0h{-11/2}{+-2}], 97% proposed by 2020Ne06, based on shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius=4.6934 fm {I58} (2013An02) 
$|d<r{+2}>(relative to {+120}Sn)=+0.384 fm{+2} {I52}; charge radius=4.693 fm {I5} (2005Le34) 
MOMM1,MOME2$atomic beam laser fluorescence spectroscopy (2005Le34); 2004Le13 and 2002Le30 are conference articles from the same group as 2005Le34. 2004Le13 give Q{-2}=+0.05 {I11}, but this value is not listed in authors' later publication 2005Le34. 
J$agreement of measured |m with shell model calculations for semi-closed nucleus (2005Le34,2004Le13); 2d{-3/2} neutron orbital 
T$weighted average of 2.4 min {I1} (1982Hu09), 2.16 min {I4} (1980De35), 2.23 min {I3} (1974Gr29), 2.5 min {I3} (1974Fo06) and 2.52 min {I12} (1972Iz01). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
$|d<r{+2}>(relative to {+120}Sn)=+0.411 fm{+2} {I53}, charge radius=4.696 fm {I6} (2005Le34) 
%IT$Calculated from the upper limit of B(M4)(W.u.)<30 recommended in Nuclear Data Sheets policies. 
MOMM1,MOME2$atomic beam laser fluorescence spectroscopy (2005Le34); 2004Le13 and 2002Le30 are conference articles from the same group as 2005Le34. 
J$agreement of measured |m with shell model calculations for semi-closed nucleus (2005Le34,2004Le13); 1h{-11/2} neutron orbital 
T$from 1982Hu09. Others: 6.7 min {I4} (1980De35), 7.3 min {I2} (1974Fo06), 8.9 min 6 (1974Gr29), 7.5 min {I1} (1967Bi15), 6.2 min {I12} (1962Dr01), 8.8 min {I6} (1962Ha16). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$odd tin systematics (one phonon+d{-3/2} multiplet); weak |b feeding from (1/2-) and (9/2+) parents 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$log| {Ift}=6.34 from (9/2+); M1,E2 |g to (5/2+); odd tin systematics (one phonon+d{-3/2} multiplet). 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J$energy systematics arguments deduced from comparison with the known lighter Sn isotopes and shell model considerations (2000Pi03); |nh{-11/2}{+-1}~#(2+ core) (2004Ga24). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$log| {Ift}=7.24 from (1/2-); odd tin systematics (one phonon+d{-3/2} multiplet); gammas to (1/2)+, 3/2+ and (5/2+). 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$based on the energy systematic arguments deduced from comparison with the known lighter Sn isotopes and shell model considerations (2000Pi03); |nh{-11/2}{+-1}~#(2+ core) (2004Ga24). 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$weighted average of values in {+129}In |b{+-} decay (0.67 s), {+129}Sn IT decay (0.27 |ms) and {+239}Pu(n,F|g). 
J$(E2) |g from (23/2+); (E2) |g to (15/2+). 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
T$weighted average of values in {+129}In |b{+-} decay (0.67 s), {+129}Sn IT decay (0.27 |ms) and {+239}Pu(n,F|g). 
J$energy systematic arguments deduced from comparison with the known lighter Sn isotopes and shell model considerations (2000Pi03) 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M4
level_comment:
T$from |g(t) in {+129}Sn IT decay (2011Pi05). Other: 0.27 |ms 7 (2008Lo07) 
J$shell model and odd tin systematics. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2)+
level_lifetime_unit: PS
level_comment:
$Dominant configuration=|ns{-1/2} (2016Li20) 
T$from fast timing |b|g(t) and centroid-shift analysis (2016Li20), using LaBr{-3}(Ce) for |g rays and plastic scintillator for |b particles. Due to the low statistics, |b|g|g(t) method could not be applied. For calibration, determination of prompt time centroids, and walk correction of the |b detector, several |g transitions in {+138}Ba from the decay of {+138}Cs were used in |b|g|g(t) measurement. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$reported as +0.090 {I6} (stat) {I6} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
MOME2$reported as +0.166 {I3} (stat) {I12} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+129Sn} in the ENSDF database. 


