# LEVEL

level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 3.69 min {I7} (1972Iz01) and 3.8 min {I1} (1974Ke08). Others: 3.7 min {I3} (1974Fo06), 1970OsZZ, 1956Pa20 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+130}Sn)=+0.240 fm{+2} {I15} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+130}Sn)=+395.9 MHz {I65}(stat) {I37}(syst) for S(p) atomic transition, and +486.6 MHz {I38}(stat) {I31}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: S
level_comment:
T other: 39 s {I2} (1977Sc14; 798|g(t)) 
$ Mean square charge radius: |D<r{+2}>({+131}Sn-{+120}Sn)=+0.52 fm{+2} {I7}; charge radius r=4.708 fm {I7} (2005Le34) 
MOMM1,MOME2$hyperfine structure using LASER spectroscopy 


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:
$From the |b spectrum x=69 {i14}; or x=65.1 {i3} from the level scheme (2004Fo06) 
E level energy held fixed in least-squares adjustment 
$ Mean square charge radius: |D<r{+2}>({+131}Sn-{+120}Sn)=+0.55 fm{+2} {I7}; charge radius r=4.711 fm {I7} (2005Le34) 
MOMM1,MOME2$hyperfine structure using LASER spectroscopy 
T others: 50 s {I2} (1977Sc14; 305, 450, 1226|g(t)) and 61 s {I1} (1981Hu09; 304, 450, 798, 1226|g(t)). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (19/2+,21/2+)
level_comment:
J$log| {Ift}=4.5 from (21/2+); |g's to (17/2+) and (19/2+). Analogy of |b{+-} decay with (|p g{-9/2}){+-1}|)(|n g{-7/2}){+-1} in odd-In isotopes suggests this level as a member of the |n(g{-7/2}g{-7/2}{+-1}h{-11/2}{+-1}) multiplet with J|p=19/2+. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 11/2-
level_comment:
$From the |b-spectrum x=69 {i14}; or x=65.1 {i3} from the level scheme (2004Fo06) 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 


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 
$From the |b-spectrum x=69 {i14}; or x=65.1 {i3} from the level scheme (2004Fo06) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
E$x=69 {i14} from the |b-spectrum or x=65.1 {i3} from the level scheme (2004Fo06) 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
CONF$|nh{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E$from {+131}Sn Adopted Levels in ENSDF database. This level is not seen in the present study which is consistent with theoretical prediction of low cross section 
$|s(theory)=0.03 mb {I2} (2014Al07) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$reported as +0.088 {I2} (stat) {I6} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 11/2-
level_comment:
MOME2$reported as +0.203 {I3} (stat) {I14} (syst); uncertainty added in quadrature by compiler 
J$from hyperfine structure measurements (2020Yo07) 
MOMM1,MOME2$from hyperfine structure measurements (2020Yo07) 
E$from the Adopted Levels of {+131Sn} in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
S$from two component fit fixing S(h{-11/2})=12 for fit to g.s and 65-keV doublet. Other: S=5.0 {I5} for single component fit. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_comment:
T$from |b|g(t) fast-timing measurement (2024Be19). Result is weighted average of 4 measurements of |t=21 ps {I5}, 27 ps {I5}, 39 ps {I8} and 19 ps {I8}. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: PS
level_comment:
T$from (2085|g or 4274|g)-285|g(t) fitted with a Gaussian convoluted exponential function (2024Be19) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$The rms charge radius (<r{+2}>){+1/2}: 4.7093 fm {I76} (2013An02 evaluation). See also 2009An12 for trends in nuclear radii 
$Measured isotope shift=1.140 GHz {I6} (relative to {+120}Sn, 2005Le34) 
$Measured |d<r{+2}>({+120}Sn,{+132}Sn)=0.534 fm{+2} {I69} (2005Le34) 
$Deduced charge radius=4.709 fm {I7} (2005Le34) 
J$hyperfine structure measurement (2005Le34) shows only one peak consistent with J=0 
T$weighted average of 38.0 s {I8} (1975Ba36), 41.0 s {I15} (1974Gr29), 41.1 s {I13} (1972Iz01,1978Iz03), 40 s {I1} (1972Ke20), 39.0 s {I10} (1972Na10), 40.6 s {I8} (1972Nu04). Others: |?47 s (1974Fo06), 1970Li14, 60 s {I10} (1966St25), 50 s {I10} (1963Gr13), 2.2 min (1956Pa20) 
$2011Jo08, 2010Jo03: deduced doubly closed shell nature of {+132}Sn in {+2}H({+132}Sn,p){+133}Sn,E=630 MeV experiment 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$|g to 0+; level is Coulomb excited from 0+ g.s. 
T$from B(E2) value. Other: <0.4 ns (from {+132}Sn IT decay) 
BE2$preliminary result from Coulomb excitation (2005Va31,2005Ra09,2004Be56,2004Ra27) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$(E2) |g to (6+); log| {Ift}=5.7 from (7-) 
T$from |g(t) in IT decay; weighted average of 2.15 |ms {i16} (2017Ch51, (132|g+299|g+374|g)(t) in {+235}U(n,F),E=thermal); 2.088 |ms {I17} (2012Ka36) and 2.03 |ms {I4} (1994Fo14). Other: 1.7 |ms {I2} (1982Ka25) 
$2017Ch51 measured isomeric ratios as a function of kinetic energy of {+132}Sn fragments in {+235}U(n,F),E=thermal using Lohengrin spectrometer at Grenoble 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$0.11 {I3} (2005Ra09, previous value was 0.14 {I5} in 2004Ra27) and 0.11 {I3} (2005Va31, previous value was 0.14 {I6} in 2004Be56). All the values are listed as preliminary by the authors 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from |g(t); weighted average of 2.15 |ms {I16} (2017Ch51, (132|g+299|g+374|g)(t) in {+235}U(n,F),E=thermal); 2.088 |ms {I17} (2012Ka36) and 2.03 |ms {I4} (1994Fo14). Other: 1.7 |ms {I2} (1982Ka25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+132}Sn)=+0.307 fm{+2} {I21} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+132}Sn)=+497.7 MHz {I11}(stat) {I50}(syst) for S(p) atomic transition, and +624.0 MHz {I32}(stat) {I42}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$B(E1)(from 4041,2+ to 4351.9,3-)=9.1|*10{+-6} {I31} (2018Ro30) 
T$deduced by compiler from B(E3)|^ in 2018Ro30 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: NS
level_uncertain: S
level_comment:
T$from {+132}Sn Adopted Levels in the ENSDF database (Feb 2018 update) 
$Gamma rays from this level not seen in the present work, but this level was included in the GOSIA2 analysis by 2018Ro30. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_comment:
T$weighted average of 1.47 s {I4} (1973Bo42), 1.47 s {I7} (1976Lu02), 1.37 s {I7} (1978Si05), and 1.57 s {I14} (2006KeZZ). 
J$L(d,p)=3 in 2010Jo03; systematics of single-particle states in neighboring odd-a nuclei 
CONF$possible |n(f{-7/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_uncertain: S
level_comment:
E$ Estimated in 1999Ur01 from the observed (10+) state at 2434 keV in {+134}Sb, assigned the (|pg{-7/2}|ni{-13/2}){-10+} configuration, and the estimated proton-neutron residual interactions energies of -722 keV ((|pg{-7/2}|ni{-13/2}){-10+}) and -462 keV ((|pg{-7/2}|nf{-7/2}){-7-}) 
J$from systematics (1999Ur01) 
CONF$possible |n(i{-13/2}{++1}). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$Population=50% per |b-n decay of {+134}In (1996Ho16,2000Ho32). 
$Possible configuration |n(f{-7/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$Population=2% per |b-n decay of {+134}In (1996Ho16,2000Ho32). 
$Possible configuration |n(p{-3/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
$Population=10% per |b-n decay of {+134}In (1996Ho16,2000Ho32). 
$Possible configuration |n(h{-9/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$Population=3% per |b-n decay of {+134}In (1996Ho16,2000Ho32). 
$Possible configuration |n(f{-5/2}{++1}) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (11/2-)
level_uncertain: ?
level_comment:
E$observed in the spectrum of |b-delayed neutrons. No deexciting |g observed. 
$Possible configuration: neutron hole at |n(h{-11/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_uncertain: S
level_comment:
E$ Estimated in 1999Ur01 from the observed (10+) state at 2434 keV in {+134}Sb, assigned the (|pg{-7/2}|ni{-13/2}){-10+} configuration, and the estimated proton-neutron residual interactions energies of -722 keV ((|pg{-7/2}|ni{-13/2}){-10+}) and -462 keV ((|pg{-7/2}|nf{-7/2}){-7-}) 
J$from systematics (1999Ur01) 
$Possible configuration |ni{-13/2}{++1}. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$ |s(|q) pattern fits 2f{-7/2} better than 3p{-3/2}. 
CONF$proposed |n(f{-7/2}{++1}) 
$ Asymptotic normalization coefficient C{+2}=0.64 fm{+-1} {I10} 
$ d|s/d|W (mb/sr)=4.3 {I7} at 28.8|', 6.9 {I8} at 31.7|', 6.3 {I7} at 34.7|', 8.2 {I9} at 37.6|', 6.9 {I11} at 42.1|', 9.3 {I15} at 47.5|', 8.8 {I15} at 54.5|', 8.8 {I13} at 59.8|', 8.4 {I9} at 64.1|' (all angles in c.m. system) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$ |s(|q) pattern fits 3p{-3/2} better than 2f{-7/2}. 
CONF$proposed |n(p{-3/2}{++1}) 
$ Asymptotic normalization coefficient C{+2}=5.6 fm{+-1} {I9} 
$ d|s/d|W (mb/sr)=11.5 {I12} at 26.4|', 11.7 {I11} at 29.1|', 13.1 {I11} at 32.1|', 16.5 {I17} at 43.8|', 15.1 {I15} at 50.2|', 11.9 {I13} at 61.6|' (all angles in c.m. system) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
CONF$ proposed |n(p{-1/2}{++1}) 
$ Asymptotic normalization coefficient C{+2}=2.6 fm{+-1} {I4} 
$ d|s/d|W=8.7 mb/sr {I17}, integrated |s for 33.3|'-54.0|' (c.m.) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-)
level_comment:
CONF$ proposed |n(f{-5/2}{++1}) 
$ Asymptotic normalization coefficient C{+2}=(0.0009 fm{+-1} {I2}) 
$ d|s/d|W=11.3 mb/sr {I19}, integrated |s for 48.4|'-54.7|' (c.m.) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$ |s(|q) pattern fits 2f{-7/2} better than 3p{-3/2}. Proposed configuration={+132}Sn(g.s.)~#|nf{-7/2} 
$ Asymptotic normalization coefficient C{+2}=0.64 fm{+-1} {I5} (2011Jo08) 
$ d|s/d|W (mb/sr)=4.3 {I7} at 28.8|', 6.9 {I8} at 31.7|', 6.3 {I7} at 34.7|', 8.2 {I9} at 37.6|', 6.9 {I11} at 42.1|', 9.3 {I15} at 47.5|', 8.8 {I15} at 54.5|', 8.8 {I13} at 59.8|', 8.4 {I9} at 64.1|' (all angles in c.m. system) (2011Jo08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
J$ |s(|q) pattern fits 3p{-3/2} better than 2f{-7/2}. Proposed configuration={+132}Sn(g.s.)~#|np{-3/2} 
$ Asymptotic normalization coefficient C{+2}=5.6 fm{+-1} {I4} (2011Jo08) 
$ d|s/d|W (mb/sr)=11.5 {I12} at 26.4|', 11.7 {I11} at 29.1|', 13.1 {I11} at 32.1|', 16.5 {I17} at 43.8|', 15.1 {I15} at 50.2|', 11.9 {I13} at 61.6|' (all angles in c.m. system) (2011Jo08) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$ proposed configuration={+132}Sn(g.s.)~#|n3p{-1/2} 
E$ this level first reported in 2010Jo03, candidate for 3p{-1/2} state 
$ Asymptotic normalization coefficient C{+2}=2.6 fm{+-1} {I6} (2011Jo08) 
$ d|s/d|W=8.7 mb/sr {I17}, integrated |s for 33.3|'-54.0|' (c.m.) (2011Jo08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-)
level_comment:
J$ proposed configuration={+132}Sn(g.s.)~#|n2f{-5/2} 
$ Asymptotic normalization coefficient C{+2}=0.0009 fm{+-1} {I2} (2011Jo08) 
$ d|s/d|W=11.3 mb/sr {I19}, integrated |s for 48.4|'-54.7|' (c.m.) (2011Jo08) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
$|s=0.58 mb {I10}; |s(theory)=1.1 mb {I4}. C{+2}=5.1 |*10{+-6} fm{+-1} {I15}. Lower |s value could be due to mixing with second 9/2- state from {+132}Sn core excitation (9/2-,2+~#2f{-7/2}) or from weak absolute cross section from poor momentum matching 
$Configuration=|n 1h{-9/2} 


level_energy_unit: KEV
level_comment:
$|s=0.38 mb {I9}. |s(theory)=0.18 mb {I7} assuming a bound |n 1i{-13/2} configuration 
$Configuration: inconclusive evidence for |n 1i{-13/2} state due to inconsistencies between spectroscopic results (|t>1 ps consistent with an E3 transition) and expectations for an {Il}=6 unbound neutron (|t|?0.1 ps) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$extracted from comparison of experimental line shapes with GEANT4 simulations (2017Va09) 
$configuration=|n(2p{-3/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+,11/2+)
level_comment:
J$proposed by 2019Pi04, based on possible member of 3/2+ to 15/2+ multiplet from configuration=|nf{-7/2}{+2}~#|nd{-3/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
E$new level in the present work. 
J$proposed by 2019Pi04, based on possible assignment of Gamow-Teller |b transition from (9/2+) parent state, and assuming that population of 54% {I4} for the {+132}Sn g.s. is entirely due to neutron decay of this level 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<11011 {I200} from Q(|b{+-})({+133}In)-S(n)({+133}Sn), where S(n)({+133}Sn)=2398.7 {I27} and Q(|b{+-}) for {+133}In=13410 {I200}, (2017Wa10: AME-2016). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from |g|g(t), fast timing technique using HPGe and LaBr{-3}(Ce) detectors (2019Pi04). This value is consistent with 21 ps {I11} measured by 2017Va09: Phys. Rev. Lett. 118, 202502 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<11341 {I204} from Q(|b{+-})({+133}In)+level energy of the isomer-S(n)({+133}Sn), where S(n)({+133}Sn)=2398.7 {I27} and Q(|b{+-}) for {+133}In=13410 {I200}, (2017Wa10: AME-2016). 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
MOME2,MOMM1,J$from hyperfine structure measurement. 
MOME2$uncertainty deduced by quadratic addition of statistical uncertainty of 0.004 and systematic uncertainty of 0.010. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1993Ru01. Others: 1.20 s {I10} (1990Fo03), 1.04 s {I2} (1976Lu02), 0.7 s {I2} (1975As04), |?1 s (1974Sh18) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-N$from {+134}Sn Adopted Levels in ENSDF database 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 1.050 s {I11} in {+134}Sn Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+124}Sn,{+134}Sn)=+0.533 fm{+2} {I10} (2019Go12). Uncertainty includes statistical and systematic 
$Measured isotope shift |d|n({+124}Sn,{+134}Sn)=+981.0 MHz {I36}(stat) {I62}(syst) for S(p) atomic transition, and +1196.5 MHz {I74}(stat) {I51}(syst) for PP atomic transition (2019Go12) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=1050 ms {I11} in {+134}Sn Adopted Levels in the ENSDF database (July 2004 update). 2015Lo04 (Phys. Rev. Lett. 114, 192501) measured T{-1/2}=890 ms {I20}. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020) 


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}=890 ms {I20} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=17 {I13} in 1975As04 (Nucl. Phys. A247, 359). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
T$from combined results of 173.8|g-347.4|g(t) in {+134}In |b{+-} decay and |b-725.6|g in {+135}In |b{+-}n decay (2021Pi11) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
%B-N$ others: 25 {I7} (2001Sh12), 22 {I7} (2002Pf04 evaluation). 
$Theoretical T{-1/2}=1070 ms, %|b{+-}n=51.7, %|b{+-}2n=5.5 (2003Mo09) 
J$possible |nf{-7/2}{+3} configuration; systematics of N=85 isotones and shell-model predictions (2001Ko45,2002Ur04). 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Others: 530 ms {I20} (2002Sh08, also 450 ms {I50} in 2001Sh12); 0.6 s {I1} (2001Ko45); 485 ms {I37} (2006KeZZ, preliminary value) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+135}Sn g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=530 ms {I20} in {+135}Sn Adopted Levels in the ENSDF database of Jan 2008 update, whereas re-evaluated in Dec 2016 ENSDF update is 515 ms {I5}, which includes data from 2015Lo04: Phys. Rev. Lett. 114, 192501. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020) 


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}=515 ms {I5} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and %|b{+-}n=21 {I3} in 2002Sh08 (Phys. Rev. C 65, 034313) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 300 ms {I15} from |bn(t) (2011Ar18) and 350 ms {I5} from implant-|b(t) (2015Lo04). Earlier results by same group as 2011Ar18 using similar setup: 0.25 s {I3} (2002Sh08) and <0.4 s (2001Sh12). 
%B-N$from neutron counting (2011Ar18). Earlier result by same group using similar setup: 30 {I5} (2002Sh08). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_comment:
$configuration=|nf{-7/2}{+2} 
T$from implant-|g(t) in {+9}Be({+238}U,F|g); |g(t) was summed for 688|g, 391|g, and 216|g. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_comment:
$configuration=|nf{-7/2}{+2} (2014Si18). 
T$from implant-|g(t), summing |g(t) for 688|g, 391|g and 216|g (2014Si18). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=290 ms {I20} in {+136}Sn Adopted Levels in an earlier version of ENSDF database, whereas April 2018 ENSDF update gives 345 ms {I15}, which includes T{-1/2} from 2015Lo04: Phys. Rev. Lett. 114, 192501. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay. 2020Ju02 observed |b{+-}n decay of {+136}Sn but do not measure the branching. 
T$from 2020Ju02, fitting decay curves with Bateman equations including second-generation daughter decays. Note that authors mention this result is derived from same data set as G. Lorusso et al., PRL 114, 192501 (2015). 


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}=350 ms {I5} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and T{-1/2}=300 ms {I15}, %|b{+-}n=27 {I4} in 2011Ar18 (Phys. Rev. C 84, 061307(R)) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
J$from systematics: 5/2- (1997Au04), 3/2- (1997Mo25) 
T$T{-1/2}|<470 ms from study of |b{+-}n. T{-1/2}=190 ms {I60}, %|b{+-}n=58 {I15} from extrapolation of decay properties of {+133}Sb, {+135}Sb (2002Sh08) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$ measured by 2011Ar18 from decay curve for delayed neutrons 
%B-N$uncertainty of 8 is also listed in the 2011Ar18 paper 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=423 ms, %|b{+-}n=49.5, %|b{+-}2n=23.3 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 190 ms {I60} in {+137}Sn Adopted Levels in ENSDF database. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+137}Sn g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=230 ms {I30} from 2015Lo04: Phys. Rev. Lett. 114, 192501. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-N$from 2020Ju02 based on measurement of intensity of 1726|g in {+137}Te following implantation of {+137}Sn and {+137}Sb, respectively. 
T$from 2020Ju02, fitting decay curves with Bateman equations including second-generation daughter decays. Note that authors mention this result is derived from same data set as G. Lorusso et al., PRL 114, 192501 (2015). 


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}=230 ms {I30} in 2015Lo04 (Phys. Rev. Lett. 114, 192501); and T{-1/2}=273 ms {I7}, %|b{+-}n=50 {I10} in 2011Ar18 (Phys. Rev. C 84, 061307(R)) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=83.3, %|b{+-}2n=3.9 (2003Mo09) 
T$measured by 2015Lo04 from the analysis of the (implanted ions)|b correlated decay curve in time and position. Other: 261 ms {I57} (preliminary value from 2007ArZQ based on neutron decay curve). Theoretical values: 460 ms (2002Pf04), 336 ms (2003Mo09). 
$Measured |s=600 pb (2010Oh02), systematic uncertainty|?30% 
$%|b{+-}n: preliminary value is 36 {I12} (2007ArZQ). Theoretical values: %|b{+-}n=100 (2002Pf04), 83.3 (2003Mo09), 70.3 (2014Mi23); %|b{+-}2n=3.9 (2003Mo09), 0.2 (2014Mi23) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
$Dominant |nf{-7/2}{+2} configuration (2014Si18) 
T$from ({+136}Sn ions)|g(t) in {+138}Sn IT decay (2014Si18) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$from a least-squares fit to the summed time distributions for the 168|g, 461|g and 715|g (2014Si18). 
$Dominant |nf{-7/2}{+2} configuration 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=140 ms {I+30-20} from 2015Lo04: Phys. Rev. Lett. 114, 192501. Value from 2015Lo04 adopted in Sep 2017 ENSDF update of {+138}Sn. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from 2020Ju02, fitting decay curves with Bateman equations including second-generation daughter decays. Note that authors mention this result is derived from same data set as G. Lorusso et al., PRL 114, 192501 (2015). 


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}=140 ms {I+30-20} in 2015Lo04 (Phys. Rev. Lett. 114, 192501) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=236 ms, %|b{+-}n=48.8, %|b{+-}2n=31.9, %|b{+-}3n=0.45 (2003Mo09) 
$Theoretical T{-1/2}=27.6 ms, %|b{+-}n=41.6, %|b{+-}2n=0.7, %|b{+-}3n=0.1 (2016Ma12) 
E$measured half-life is assumed to correspond to the ground state of {+139}Sn 
J$5/2- from theoretical considerations (1997Mo25) 
T$measured by 2015Lo04 from (implanted ions)|b correlated curves in time and position using maximum likelihood method. See 2015Lo04 for comparison of their experimental value with theoretical values 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical T{-1/2}=236 ms, %|b{+-}n=48.8, %|b{+-}2n=31.9, %|b{+-}3n=0.45 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical T{-1/2}=27.6 ms, %|b{+-}n=41.6, %|b{+-}2n=0.7, %|b{+-}3n=0.1 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 101 counts were assigned to {+139}Sn, 28 events with spectrometer setting on Te, and 73 events with setting on Sn. Probability of misidentification of this isotope is <0.01% for both the settings (2018Sh11). 
$Production |s=1.7 pb for Sn setting, and 2.3 pb for Te setting, with 30% systematic uncertainty on both |s values. 
E$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: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+139}Sn g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=130 ms {I60} from 2015Lo04: Phys. Rev. Lett. 114, 192501. Value from 2015Lo04 adopted in Oct 2016 ENSDF update of {+139}Sn. 


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}=130 ms {I60} in 2015Lo04 (Phys. Rev. Lett. 114, 192501) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=68.2 ms, %|b{+-}n=87, %|b{+-}2n=2 (2019Mo01) 
$Theoretical T{-1/2}=21.6 ms, %|b{+-}n=41.7, %|b{+-}2n=0.3 (2016Ma12) 
$A total of five counts were assigned to {+140}Sn, three events with the spectrometer setting on Sn, and two events with setting on Te. Probability of misidentification of this isotope is 0.52% for Sn setting, and 0.32% for Te setting (2018Sh11) 
$Production |s=0.05 pb for Sn setting, and 0.1 pb for Te setting, with 30% systematic uncertainty for both the |s values 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 68.2 ms (2019Mo01) and 21.6 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+140}Sn is expected to be <130 ms, based on measured half-lives of 230 ms for {+137}Sn, 140 ms for {+138}Sn, and 130 ms for {+139}Sn, available in literature. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
T$from time-of-flight and expected 560 counts from cross section calculations, but none observed. Others: >1.5 |ms (1995Ry03); <50 ns (quoted by 2012Au07 from Hinke et al., Leuven conference 2011, p200; <200 ns (quoted by 2012Au07 from Straub et al., GSI report 2010, p151) 
J$1/2+ in theoretical calculations (1997Mo25); 5/2+ from systematics in 2012Au07 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$deduced by 2017Su26 from expected 770 counts from observed production yield curves, time-of-flight of 446 ns, and assumed upper limit of one count for {+103}Sb. Other: <49 ns (2013Su23) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
%P$E(p)=478~{I15} keV and %p |?1 in 1994Ti03, but not confirmed by 1997Sh13. 
J$from systematics 
T$Weighted average of 1.12 s {I16} 1996FaZZ and 1.30 s {I15} from 1995Sc28, 1995Sc33 
CONF$|pd{-5/2}{++1} 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_comment:
J$495.2|g (M1) to (17/2+) 
CONF$|pd{-5/2}{++1}|n(d{-5/2}{++1}g{-7/2}{++1}) and one neutron pair coupled to J=0 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: S
level_comment:
T$ From I|g(t) (1995LeZZ) 
J$Adopted from (1999So08); 2005So06 do not exclude a possible spin-parity assignment of 1+ to the ground state. 


level_energy_unit: KEV
level_spin_parity: (14+)
level_comment:
$Possible configuration=|pg{-7/2}|nd{+3}{-5/2}|ng{+2}{-7/2} 
J$2005So06 assigns (13,14+). The evaluators chose (14+) based on the band assignment. 


level_energy_unit: KEV
level_comment:
$Possible configuration=|pd{-5/2}|nd{+2}{-5/2}|ng{+3}{-7/2}, J|p=14+ or |pg{-7/2}|nd{+2}{-5/2}|ng{+3}{-7/2}, J|p=15+ 


level_energy_unit: KEV
level_spin_parity: (18)
level_comment:
$Level may be interpreted as 18- with fully aligned configuration= |pd{-5/2}|nh{-11/2}|nd{+2}{-5/2}|ng{+2}{-7/2} 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$Adopted from 1999So08; 2005So06 do not exclude a possible spin-parity assignment of 1+ to the ground state. 


level_energy_unit: KEV
level_spin_parity: (18)
level_comment:
$Level may be interpreted as 18- with fully aligned configuration= |pd{-5/2}|nh{-11/2}d{+2}{-5/2}|ng{+2}{-7/2} 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: S
level_comment:
T$weighted av: 7.6 s 3 (1997Sh13), 7.0 s 5 (1976Ox01) 
J$from |g(|q) and model arguments in (HI,xn|g) (1995Ce01). This assignment is inconsistent with |e feeding of a 2+ level; however, as pointed out by 1995Ce01, the large Q value and incomplete decay scheme allow for the possibility of additional feeding of the 2+ state by unplaced or unobserved |g's 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$from analogy to {+111}Sb,{+113}Sb 
T$using Limitation of Relative Statistical Weight method and values of 18.3 s {i5} (using 925.4|g(t) in 1976Ox01), 16.67 s {i15} (|g(t) in 1982Jo03), and 17.3 {I5} (using 545|g(t) and 925|g(t) in 2002Re14) 
CONF$|pd{-5/2} 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$from systematics of similar states in odd-A Sb isotopes; in agreement with shell model calculations (2002Re28) 
CONF$|pd{-5/2}~#2+ multiplet 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$752.3|g to (5/2+); in agreement with shell model calculations (2002Re28). 
CONF$|pd{-5/2}~#2+ multiplet 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$832.2|g D+Q to (5/2+), systematics of similar states in odd-A Sb isotopes 
CONF$|pg{-7/2}, possibly with |pd{-5/2}~#2+ admixtures 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_comment:
J$968|g to (19/2-), 706|g to (21/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_comment:
J$878|g to (19/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (25/2-)
level_comment:
J$275|g to (23/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_comment:
J$384|g to (25/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_comment:
J$756|g to (25/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (29/2-)
level_comment:
J$331|g to (27/2-), 933|g to (25/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_comment:
J$407|g to (29/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_comment:
J$1177|g to (27/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_comment:
J$1308|g to (31/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_comment:
J$762|g to (31/2-); proposed by 1998LaZU in {+54}Fe({+58}Ni,3p|g) based on angular correlation data 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: S
level_comment:
T$Weighted average of 23.0 s 4 (|g(t) in 1972Si28), 23 s 1 (1970SuZY), 23 s 1 (1974De34) and 24.0 s 3 (|g(t) in 1976Ox01). Other: 21.3 s 15 (|b(t) in 1972Mi26) 
J$population of J|p=2+ and 4+ states in {+110}Sb |e+|b{++} decay favor J|p=3+. However, 1997La13 proposed J|p=4+, based on the assigned 195|g (from the (5+) level) as M1(+E2) and the |g-ray decay pattern where the 1153 keV isomeric level is assigned J|p=8- 
CONF$Possible |pd{-5/2}~#|nd{-5/2}. The assignment is tentative 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
J$812|g (M2) to (6+). Systematics of neighboring odd-odd Sb nuclei. 
T$From 812|g(t), 146|g(t), 195|g(t) and 1035|g(t) in 1997La13 
CONF$possible |pd{-5/2}~#|nh{-11/2} configuration, suggested also for the heavier odd-odd Sb isotopes from the measured magnetic moments (1976Ke07) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J$201|g from (9-); observation of strongly coupled bands with a ~200|g from 9- to 8- in neighboring odd-odd Sb isotopes; band member 


level_energy_unit: KEV
level_spin_parity: (15+)
level_comment:
J$1218|g E2 to (13+); band member (|p=+ for the band suggested from 482- and 590-keV gammas assumed being E1) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: NS
level_comment:
T$From 812|g(t), 146|g(t), 195|g(t) and 1035|g(t) deduced by examining data sets from the OSIRIS Spectrometer at Hahn-Meitner Institute 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$allowed |e transitions (log| {Ift}|<5.5) to 3/2+ and 5/2+ states in {+111}Sn imply 3/2+ or 5/2+ parent. Odd-mass {+113}Sb-{+121}Sb g.s. have J|p=5/2+ 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$level not observed in high-spin studies implying spin of <7/2. Assignment of 1/2+ from systematics of neighboring isotope {+113}Sb and intensity balance arguments involving the 1392|g. J|p=3/2+ or 5/2+ cannot be ruled out. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$level not observed in high-spin studies implying spin of <7/2. Assignment of 3/2+ from systematics of neighboring isotope {+113}Sb. J|p=1/2+ or 5/2+ cannot be ruled out 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_uncertain: ?
level_comment:
E$existence of level based on assumption of smoothly varying systematics for second 7/2+ level in neighboring odd-a Sb isotopes. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_uncertain: ?
level_comment:
E$ existence of level based on assumption of smoothly varying systematics for second 7/2+ level in neighboring odd-A Sb isotopes. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: S
level_comment:
J$direct feeding of 2+ and 4+ levels in {+112}Sb following %|e+%|b{++} decay 
T$weighted average for 51.4 {I10} s (1976Wi10), 53.5 {I5} s (1972Si28), 56 {I1} s (1972Mi27), 53 {I1} s (1970SuZY), 54 {I6} s (1959Se56) 
CONF$|pd{-5/2}~#|ng{-7/2} 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$Tentative assignment based on the association of this level as a member of the |pd{-5/2}~#|ng{-7/2} split multiplet 


level_energy_unit: KEV
level_spin_parity: (2+,3+)
level_comment:
J$274.05|g M1+E2 to (3+) and 214.4|g M1 to (2+); Probable member of the |pd{-5/2}x|ns{-1/2} split multiplet; J|p=1+ in {+112}Sn({+3}He,t), but level not observed in {+112}Te |e decay (J|p=0+) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
J$456.4|g M2+E3 to (6+) 
T$from |g(t) in 1982Ma29. Other: 0.56 |ms {I12} from 456.4|g(t) in 1976Ke07 
MOMM1$+2.19 {I4} (1976Ke07) using the perturbed angular correlations technique 
MOME2$0.71 {I8} from |g(|q,t) from abs(Q({+112}Sb,8-)/Q({+123}Sb,5/2+))=1.958 {I10} in 1982Ma29, deduced using the perturbed angular correlations technique, and Q({+121}Sb,5/2+)=-0.36 {I4} (1978Bu24) 
CONF$|pd{-5/2}~#|nh{-11/2} 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (10+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$Possible |g-ray transitions to the (8+) level at 2161.4 keV and the (9+) level at 2569.5 keV. All transitions in the band associated with this level are observed by 1998La14 in coincidence with the 471|g, depopulating the (8+) level at 2161.4 keV and 1385|g, depopulating the (9+) level at 2569.5 keV 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$Possible |g-ray transition to the (10-) level at 1884.4 keV. All in-band transitions are observed by 1998La14 to be in coincidence with the 1059|g,depopulating the (10-) level at 1884.4 keV 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: NS
level_comment:
E$796 {I4} keV in 1976Ka19 
T$from |g(t) in 1982Ma29. Other: 0.56 |ms {I12} from 456.4|g(t) in 1976Ke07 
MOMM1$+2.19 {I4} (1976Ke07) 
MOME2$0.71 {I8} from |g(|q,t) from abs(Q({+112}Sb,8-)/Q({+123}Sb,5/2+))=1.958 {I10} in 1982Ma29, deduced using the perturbed angular correlations technique, and Q({+121}Sb,5/2+)=-0.36 {I4} (1978Bu24) 
CONF$|pd{-5/2}~#|nh{-11/2} 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: NS
level_comment:
T$from |g(t) in 1982Ma29. 
MOMM1$+2.19 {I4} (1976Ke07) 
MOME2$0.071 {I7} from |g(|q,t) in 1982Ma29 (perturbed angular correlations technique) 
CONF$|pd{-5/2}~#|nh{-11/2} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
J${+115}Sb to {+121}Sb have J|p=5/2+. Allowed |e to 3/2+, 5/2+ states in {+115}Sn. 
T$from 1976Wi10. Others: 1962Pa04, 1969Ki16, 1972Si28. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
L$both L=4 and L=5 fit the angular distribution. L=5 is assigned because of sum rule limit for L=4. 
S$J|p=7/2+ gives C{+2}S'=5.0. 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=1.79 mb/sr {I8} (6|'), 0.81 mb/sr {I3} (18|') 
$({+3}He,d): d|s/d|W=1.26 mb/sr {I6} (6|'), 3.45 mb/sr {I14} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=2.59 mb/sr {I10} (6|'), 0.99 mb/sr {I4} (18|') 
$({+3}He,d): d|s/d|W=0.12 mb/sr {I1} (6|'), 0.13 mb/sr {I5} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.36 mb/sr {I2} (6|'), 0.24 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.78 mb/sr {I4} (6|'), 1.82 mb/sr {I8} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.10 mb/sr {I1} (6|'), 0.05 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.16 mb/sr {I5} (6|'); peak too weak to analyze at 15|' 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.07 mb/sr {I1} (6|'), 0.03 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.62 mb/sr {I5} (6|'), 0.16 mb/sr {I13} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.27 mb/sr {I2} (6|'), 0.14 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.26 mb/sr {I4} (6|'), 0.21 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
MOMM1,MOME2,J$from hyperfine structure measurement with |m({+123}Sb)= 2.5457 |m{-N} {I12} and Q({+123}Sb)=-0.692 b {I14} as references. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 3.3 min {I5} (1959Se56), 3.5 min {I5} (1960Ma20), 3.38 min {I8} (1972Mi27), 3.52 min {I8} (1972Si28), 3.51 min {I4} (1976Wi10) 
J$log| {Ift}<6 for |e+|b{++} decay to 2+ and 4+ levels 
MOMM1$from 1992Zi05 (also 1993Bo46) and +1.74 {I12} (1992BaZU,1993BaZJ) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: US
level_comment:
MOMM1$from perturbed angular distributions. 
J$from g factor. Syst of 8- levels in Sb isotopes. 
T$from 1976Ka19; others: 275 |ms {I20} (1973Gi02), 210 |ms {I10} (1976Br40) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
J atomic beam, L=2 in ({+3}He,d) 
MOMM1${+119}Sb g.s. analogous to {+115}Sb g.s. (1968Ja05). Other: +3.457 {I19} (1992BaZV) 
T$unweighted av: 32.1 min {I3} (1976Wi10), 31.8 min {I2} (1968Ra27), 32.3 min 3 (1967Ha27). Others: 1958Se59, 1961Fi05, 1962Se03 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$M1(+E2) |g ray to 5/2+ state, |g ray from 9/2+ state; 1098|g(|q) 
T$from 1995LoZZ, 1998Lo11, DSA method. Other: 320 fs {I+301-110} (1995Bu15) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$from 1978Su05, 1300|g(t) pulsed beam. Others: 6.7 ns {I4} (1977Br08), 7.0 ns {I4} (1980Le05) 
J$L=5 ({+3}He,d); E3 and M2 deexcitations to 5/2+ and 7/2+ states, respectively 
Enhanced M2 and E3 deexcitations are attributed to M2 and E3 phonon admixtures in both initial and final states (1978Su05) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$from 1998Lo11, 1995LoZZ. Other: <5 ps (1977Br08) 
J$stretched E2 |g ray to 5/2+ state, M1 to 7/2+ state 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$from 1998Lo11, 1995LoZZ. Other: <5 ps (1977Br08) 
J$stretched E2 |g ray to 5/2+ state, M1+E2 to 7/2+ state 
E analogous 9/2+ bandheads in {+113}Sb,{+117}Sb,{+119}Sb are, respectively, at 1461, 1160, 971 keV; see 1975Ga11, 1979Sh03 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$stretched E2 |g ray to 11/2- state; 1217|g excit. Interpreted as (|p d5/2) coupled to 5- state of {+114}Sn core; see 1977Br08 
T$from 1998Lo11 in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$from 1998Lo11 in (|a,2n|g) 
J$stretched E2 |g ray to 11/2- state, M1+E2 to (13/2)- state; 322|g excit 


level_energy_unit: KEV
level_spin_parity: (19/2)-
level_lifetime_unit: NS
level_comment:
MOMM1$others: 2.73 {I4} (1979Fa03), 2.76 {I5} (1979Sh03), 2.68 {I6} (1979Ko02) 
T$159 ns {I3} (1979Sh03) 279|g(t) pulsed beam. Others: 156 ns {I3} (1977Br08), 157 ns {I5} (1979Ko02) 
J$stretched E2 |g rays to 15/2- states; 279|g excit. Interpreted as (|p d5/2) coupled to 7- state of {+114}Sn core; see 1979Fa03, 1977Br08 


level_energy_unit: KEV
level_spin_parity: (25/2)+
level_lifetime_unit: NS
level_comment:
T 4.1 ns {I2} unweighted av: 4.17 ns {I14} (1973FrYL), 4.0 ns {I2} (1977Br08) (207|g,214|g)(t) 
J E1 transition to (23/2)- state; HF(E1); 214|g excit. Analog: {+117}Sb at 3130 keV, T{-1/2}=340 |ms, J|p=25/2+, |m=+1.500 {I9}, Q=0.75 {I9}; see 1989Ra17. Interpreted as (|p d5/2) coupled to 10+ state of {+114}Sn core; see 1977Br08, 1979Sh03 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$6.2 ns {I3} from 1300|g(t), 6.4 ns {I10} from 576|g(t) (1978Su05) via {+115}In({+3}He,3n|g) pulsed 25-MeV {+3}He. Others: 6.7 ns {I4} (1976Ka25,1977Br08), 8.4 ns {I7} (1978Ke04), 7.0 ns {I4} (1980Le05) 
g factor=+0.97 {I10} (1978Ke04) |g(|q,H,t) via {+116}Sn(p,2n|g), +1.06 {I10} (1979Fa03) |g(|q,H,t) via {+115}In(|a,4n|g) +1.004 {I13} (1980Le05) 
{+117}Sb analog: 3.9-ns, 1323-keV state, g factor=+1.02 {I7} (1978Ke04) 
Branching: I|g(577|g)/I|g(1300|g)=0.087 {I3} (1978Su05). Others: 0.085 {I4} (1977Br08) via (|a,2n|g), 0.09 {I2} (1977Br08) via (p,2n|g) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: NS
level_comment:
T 159 ns {I3} (1979Sh03) 279|g(t) pulsed beam. Others: 156 ns {I3} (1977Br08), 157 ns {I5} (1979Ko02) 
Branching: I|g(158|g)/I|g(279|g)=0.33 {I4} av of 0.324 {I49} (1979Sh03), 0.338 {I41} (1977Br08) 
g factor=+0.287 {I4} (1979Fa03) |g(|q,H,t). Others: +0.290 {I5} (1979Sh03), +0.282 {I6} (1979Ko02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
Branching: I|g(228|g)/I|g(603|g)/I|g(1327|g)=3.4 {I5}/19.4 {I14}/100 (1975WiZX), 2.7 {I4}/16.1 {I8}/100 (1974Ch51), |<2.4/22.3 {I11}/100 (1972Sh37) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
Branching: I|g(282|g)/I|g(657|g)/I|g(1380|g)=4.3 {I5}/29.6 {I19}/100 (1975WiZX), 4.0 {I6}/26.5 {I12}/100 (1974Ch51), |<4/30.0 {I24}/100 (1972Sh37) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$from 1998Lo11; other:<5 ps (1977Br08) 
Branching: I|g(603|g)/I|g(1327|g)=0.49 {I10} (1977Br08), 0.39 {I4} (1976Ka25), 0.43 {I6} (1979Sh03); lower I|g-ratios observed via decay studies 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T$from 1998Lo11, other:<5 ps (1977Br08) 
Branching: I|g(657|g)/I|g(1380|g)=0.305 {I16} (1977Br08), 0.39 {I4} (1976Ka25), 0.43 {I6} (1979Sh03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 25/2+
level_lifetime_unit: NS
level_comment:
T 4.1 ns {I2} unweighted av: 4.17 ns {I14} (1973FrYL), 4.0 ns {I2} (1977Br08) (207|g,214|g)(t) 
I|g(207|g)(214|g)(442|g)-coin (prompt vs delayed) measured by 1973FrYL establishes ordering of |g-cascade from 4-ns initial state 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=3.61 mb/sr {I14} (6|'), 1.50 mb/sr {I6} (18|') 
$({+3}He,d): d|s/d|W=1.32 mb/sr {I7} (6|'), 3.85 mb/sr {I16} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.19 mb/sr {I1} (6|'), 0.09 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=3.37 mb/sr {I13} (6|'), 1.65 mb/sr {I7} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.77 mb/sr {I3} (6|'), 0.33 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.82 mb/sr {I4} (6|'), 1.79 mb/sr {I8} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.13 mb/sr {I2} (6|'), 0.08 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.20 mb/sr {I2} (15|'); peal at 6|' obscured by an impurity 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 15.5 min {I10} (1953St42), 16.2 min {I12} (1967Ha27). Other: 14 min (1954At34) 
J$atomic beam (1974Ek01). Positive parity deduced from log| {Ift}=4.7 to |p=+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$E2 to 3+; allowed |e transition from J|p=0+ 
T$from 1993Di06; other: 200 ns>(1976Ka19), T{-1/2}>500 ns (1973ChYA) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=2, M1 |g to 3+, |g(|q) rules out J=3; configuration=((|p d{-5/2})(|n s{-1/2})) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T weighted average of 64 min {I4} (1961Fi05), 60.42 min {I24} (1967Ha27), 53.6 min {I21} (1972Pa13). Others: 60 min (1949Te11), 60 min (1954At34). 
J$atomic beam (1974Ek01), log| {Ift}=4.9 to |p=- 
E$from Q(60-M {+116}Sb)=5090 {I40} (1960Je03) and Q(15.8 m 116sb)=4707 {I5} (1995Au04). If one uses Q(60-M)=5113 {I14} (from |e/|b{++} of 1964Bo21) one gets E(8-)=406 {I15} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$(M1,E2) |g to 3+ and 2+, Hauser-Feshbach analysis L({+3}He,d)=2+4; configuration=((|p g{-7/2})(|n s{-1/2})) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$M1,E2 |g to 3+, L({+3}He,d)=4, |g(|q) and Hauser-Feshbach analysis; configuration=((|p g{-7/2})(|n s{-1/2})) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$L({+3}He,d)=0; configuration=((|p s{-1/2})(|n s{-1/2})). Strong branching to 3+, Hauser-Feshbach analysis 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$L({+3}He,d)(4); configuration=((|p g{-7/2})(|n s{-1/2})), M1,E2 |g to 3+, |g(|q) and Hauser-Feshbach analysis 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
J$M1 |g to 8-, M2 |g from 11+ 
T$7.1 ns measured for 752.6|g by 1985BeZH and assigned to a 3731 level. The 752.6|g has been reassigned to the 1135 level. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
T$weighted av: 11.9 ns {I6} (1992Io01), 10.3 ns {I3} (1982Du11). Other: 12.6 ns (1985BeZH) 
J$E1 |g to 8-, E1 |g from 7- 


level_energy_unit: KEV
level_spin_parity: 11+
level_lifetime_unit: NS
level_comment:
T$from 1982Va07 in (|a,3n|g). Other: 4.0 ns {I2} ({+7}Li,4n|g) (1982Du11) 
J$stretched E3 |g to 8-, excit in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
T$7.1 ns measured for 752.6|g by 1985BeZH and assigned to 3731 level. The 752.6|g has been reassigned to the 1135 level. 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ from Adopted Levels of {+116}Sb in ENSDF database. 2012Au07 in NUBASE give 390 {I40} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
MOMM1,MOME2$AB (1974Ek01) 
T$from (1967Ha27). Other: 2.76 h {i6} (1961Fi05). T{-1/2}=3.19 h {i4} reported by 1972Pa13 not used. Others: 1939Li05, 1947Co04 
J$from atomic beam (1976Fu06), L(d,n)=2. Configuration=|pd5/2 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(p)=2, log ft=6.4 from 1/2+ parent 
T$from 1995Bu15 in (p,n|g); other: 520 fs +170-140 (1995LoZZ) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=5, M2 |g to 7/2+, Configuration=|ph11/2 
MOMM1$Atomic beam magnetic res. Others: 5.35 {i9} (1980Le05), { 5.61 {i39}} (1978Ke04) 
T$from 3.8 ns {i2} (1978Ke04), 3.8 {i2} (1980Le05). Others: 3.9 {i2} (1978Su05), 3.5 ns {i3} (1990Ko42); T{-1/2}=1.5 ns {i3} reported by 1975Fr10 not used 


level_energy_unit: KEV
level_spin_parity: (25/2)+
level_lifetime_unit: US
level_comment:
J$M2 |g to 21/2- 
MOMM1$NMR; others: 1.437 {i75} (1975Fr10), 1.450 {i30} (1972Me15), 1.512 {i30} (1975Iv02) 
T$weighted average: 340 |ms {i20} (1970He13), 390 |ms {i30} (1972Me15) 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: NS
level_comment:
J$(E2) |g to (19/2-). Agreement of |m between the calculated and experimental values for configuration=((|p 1g{-9/2}){+-1}(|n 1h{-11/2})(|n 2d{-3/2}){+-7}. 
T$from 1987Io01. 
MOMM1$also given in 1987Io01. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$from 1980Le05. Others: 3.9 ns {i2} (1978Su05), 3.5 ns {i3} (1990Ko42); T{-1/2}=1.5 ns {i3}, reported by 1975Fr10 not used 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
Coulomb displacement energy=13796 {I15} (1966Ha16) 
E E(p)(c.m.)=6862 {I15} (1966Ri06), 6856 {I10} (1966Ha16) 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=4.36 mb/sr {I17} (6|'), 1.51 mb/sr {I6} (18|') 
$({+3}He,d): d|s/d|W=1.26 mb/sr {I8} (6|'), 3.28 mb/sr {I16} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=4.29 mb/sr {I16} (6|'), 1.59 mb/sr {I6} (18|') 
$({+3}He,d): d|s/d|W=0.05 mb/sr {I1} (6|'), 0.11 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.035 mb/sr {I6} (6|'), 0.047 mb/sr {I5} (18|') 
$({+3}He,d): d|s/d|W=3.07 mb/sr {I15} (6|'), 1.39 mb/sr {I6} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.75 mb/sr {I3} (6|'), 0.32 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.55 mb/sr {I5} (6|'), 1.20 mb/sr {I5} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=6.59 mb/sr {I25} (6|'), 2.8 mb/sr {I11} (18|') 
$({+3}He,d): d|s/d|W=0.07 mb/sr {I2} (6|'), 0.13 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.47 mb/sr {I3} (6|'), 0.25 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.65 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.06 mb/sr {I1} (6|'), 0.022 mb/sr {I2} (18|') 
$({+3}He,d): peak at 6|' too weak to analyze; peak at 15|' obscured by an impurity 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.68 mb/sr {I3} (6|'), 0.25 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.08 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.51 mb/sr {I2} (6|'), 0.22 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.38 mb/sr {I5} (6|'), 0.96 mb/sr {I4} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.12 mb/sr {I1} (6|'), 0.061 mb/sr {I4} (18|') 
$({+3}He,d): d|s/d|W=0.12 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.27 mb/sr {I2} (6|'), 0.15 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.21 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
T$weighted average of 2.91 h {I5} and 2.98 h {I1}, from |g(t) (2021Da02). Authors note that small contribution from the decay of the long lived isomer in {+117}Sn may influence their half life determination. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
MOMM1 Atomic beam magnetic res, value relative to {+121}Sb 
Configuration=(|p d{-5/2})(n,d3/2) 
T average of 3.6 min (1940Ri02), 3.5 min (1948Li02), 3.7 min {I3} (1964Va23) 
J atomic beam (1968Ja05) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: US
level_comment:
MOMM1 Differential perturbed angular correlation, value does not include the Knight-shift correction and is relative to |m=-1.378 {I11} for {+115}Sn (11/2- 714 level) 
MOME2$quadrupole interaction from relaxation time, value recalculated based on new measurements and is relative to Q=-0.36 {I4} for g.s. of {+121}Sb (1989Ra17) 
J E2 |g to 1+ and |g from (4)+ allow (2,3)+; measured g-factor is consistent with J=3 
Configuration=((|p d{-5/2})(|n s{-1/2})) 
T pulsed beam |g(t) (1975Pl04) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
Configuration=((|p d{-5/2})(|n h{-11/2})) 
E from E(|b{++} to {+118}Sn 2575 level)=310 {I5} and g.s. Q(|b{++})=3657 {I3}. E(|b{++}) deduced from %|b{++}=0.0016 {I1} (1961Bo13) and %I(|e+|b{++})=98.5. 
T from 1974Ca06. Others: 5.1 h {I3} (1947Co04), 4.96 h {I2} (1967Ha27), 5.15 h {I5} (1968Ki06), 5.11 h {I6} (1972Pa13) 
J atomic beam (1974Ek01), nuclear magnetic resonance (1974Ca06) 
MOMM1 Radiative detection of NMR, value relative to |m=-1.905 {I20} for g.s. of {+122}Sb (1989Ra17) 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$differential perturbed angular distribution; Q: value relative to Q=0.71 {I7} that for {+112}Sb(796 level) and includes the sternheimer correction (1989Ra17) 
Configuration=((|p d{-5/2})(|n h{-11/2})) 
T weighted av of 13.4 ns {I3} (1985Di07) and 13.2 ns {I3} (1974Ch44) 
J E1 |g-M1 |g-E2 |g and d |g-d |g cascades to 1+; no |g to 1+ 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$differential perturbed angular distribution (1989Ra17); Q value relative to Q=0.71 {I7} for {+112}Sb (796 level) and includes the Sternheimer correction (1989Ra17) 
J d |g to 8-, |p=+ from E1+M2 |g-M1,E2 |g cascade relation to 8-; measured g-factor is consistent with J=7 
Configuration=((|p g{-9/2}){+-1}(|n d{-5/2}){+-1}) 
T weighted av of 22.8 ns {I4} (1985Di07) and 22.4 ns {I5} (1983Va14) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J from syst of |DJ=1 band built on 8- state in odd-odd Sb isotopes (1983Va14) 
Configuration=((|p g{-9/2}){+-1}(|n h{-11/2}){+-1}) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$ from Adopted Levels for {+118}Sb in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: H
level_comment:
T$weighted average of 5.13 h {I20}, 5.25 h {I8} (253|g(t)), 5.14 h {I18}, 5.07 h {I10} (1050|g(t)) and 5.15 h {I17}, 5.19 h {I5} (1229|g(t)) (2021Da02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
MOMM1,MOME2$atomic-beam magnetic resonance. Q includes Sternheimer correction (2005St24). 
T weighted av of 38.0 h {I1} (1957Ol05), 39 h {I1} (1947Co04), and 38.5 h {I3} (1967Ha27, |b(t)). All data are from {+119}Sb |e decay 
J J=5/2 from atomic beam (1976Fu06), L({+3}He,d)=2 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
E doublet at 660 keV in ({+7}Li,{+6}He) 
T from >350 fs from DSA in (p,n|g) and <10 ps from |gX(t) in 16.0-h {+119}Te |e decay 
J L({+3}He,d)=0, L({+7}Li,{+6}He)=0+2 for a doublet at 660 keV 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
T from >350 fs from DSA in (p,n|g) and <10 ps from |g|g(t) in 4.7-d {+119}Te |e decay 
J M1+E2 |g to 7/2+,E2 |g to 5/2+ 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E doublet in (p,n). Probably includes 1212.7 level 
J M1(+E2) |g to 7/2+, |g|g(|q) excludes J=5/2 and 7/2 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T from |gX(t) in 4.7-d {+119}Te |e decay 
J L({+3}He,d)=5, J=9/2 is excluded by |g|g(|q) in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: NS
level_comment:
T weighted av of 128 ns {I4} from |g(t) in (d,2n|g) and 134 ns {I6} |g(t) in (HI,xn|g) 
MOMM1,MOME2$TDPAD (1991Io02) 
J (E2) |g to (15/2-), (E1) |g to 17/2+; no |g's to level with J|p<15/2+, |g(|q) in (HI,xn|g) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (27/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T from |g(t) in (HI,xn|g) 
J tentative assignment from syst of lifetime and isomerism in odd Sb nuclei 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E(p)(c.m.)=7258 {I8}; weighted average of 7255 {I15} (1966Ri06), 7261 {I10} (1966Ha16), and 7251 {I20} (1976Be49). Others: 7280 (1966AlZY), 7230 {I60} (1971Mi03) 
|G=39 {I9} keV, |G(p)=10 {I5} keV (1976Be49) 
|G=50 keV, |G(p)=17 keV (1966Ri06) 
|G=60 {I5} keV (1966Ha16) 
|G(p)/|G=0.320 {I15} (1977Fi10), 0.38 {I5} (1971Mi03), |?0.3 (1977Ba52) 
J IAS of the 1/2+ g.s. in {+119}Sn 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E(p)(c.m.)=7276 {I15} (1966Ri06). Other: 7300 (1966AlZY) 
|G=32 keV; |G(p)=5 keV (1966Ri06), |G(p)=7 keV (1968Ve08) 
J IAS of the 23.9-keV 3/2+ level in {+119}Sn 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E(p)(c.m.)=8323 {I9}; weighted average of 8328 {I15} (1966Ri06) and 8321 {I10} (1966Ha16). Other: 8350 (1966AlZY) 
|G=37 keV, |G(p)=3 keV (1966Ri06) 
|G=50 {I5} keV (1966Ha16) 
J IAS of the 1089-keV 5/2+ level in {+119}Sn 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E(p)(c.m.)=8598 {I15} (1966Ri06). Other: 8630 (1966AlZY) 
|G|?40 keV, |G(p)|?1.7 keV (1968Ve08) 
J IAS of the 1355-keV 5/2+ level in {+119}Sn 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (27/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T 0.85 s {I6} from (288.2|g)(t) (1979Sh03) 
J tentative assignment from syst of lifetime and isomerism in odd Sb nuclei 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=5.68 mb/sr {I21} (6|'), 1.86 mb/sr {I7} (18|') 
$({+3}He,d): d|s/d|W=1.08 mb/sr {I6} (6|'), 3.02 mb/sr {I12} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.96 mb/sr {I4} (6|'), 0.38 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.47 mb/sr {I5} (6|'), 0.87 mb/sr {I4} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.27 mb/sr {I3} (6|'), 0.09 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.10 mb/sr {I2} (6|'), 0.20 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=1.30 mb/sr {I5} (6|'), 0.50 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.05 mb/sr {I4} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.57 mb/sr {I2} (6|'), 0.25 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.48 mb/sr {I5} (6|'), 0.17 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.45 mb/sr {I2} (6|'), 0.14 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.20 mb/sr {I3} (6|'), 0.28 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.19 mb/sr {I2} (6|'), 0.08 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.13 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.28 mb/sr {I2} (6|'), 0.13 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.33 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.25 mb/sr {I1} (6|'), 0.10 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.09 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_spin_parity: 25/2+
level_lifetime_unit: S
level_comment:
T$from ion(t) in storage ring (2019Mi18); reported as 776 ms {I181}. Other: 784 ms {I203} from global fit to {+119}Sb isomer decay and all possible daughter nuclides. 
E$from direct mass measurements of ground state and isomer. 
%IT$from non observation of |b{++} or |b{+-} growth. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
MOMM1 atomic beam magnetic resonance, value relative to that of {+121}Sb(g.s. 5/2+) (1989Ra17) 
The assignment of the 1+ isomer to g.s. is tentative 
J atomic beam (1976Fu06); |p=+ from log| {Ift}=4.5 to 0+ 
T value from 1965Eb01. For values in agreement with adopted value, see 1961Ra06, 1968Bo25, 1973ArZI; for values in disagreement, see 1950Jo59, 1967Ha27, 1968Ra14, 1970Pa17. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 8-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
MOMM1 radiative detection of NMR, value recalculated and relative to |m=-1.905 {I20} for {+122}Sb (2- g.s.) (1989Ra17) 
E$0 {I100} is suggested in 1997Au04 as a value from systematics 
J$atomic beam (1974Ek01), NMR (1974Ca06); parity from log| {Ift}=5.17 to (7)- 
T value from 1967Ha27. See also 1958Mc59, 1968Bo25, 1968Ki06, 1972Pa13. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$differential perturbed angular correlation of |g's following nuclear reaction. |m does not include a Knight-shift correction; Q relative to that for g.s. of {+121}Sb and includes the Sternheimer correction (1989Ra17) 
J excit in (p,n|g) suggests 3+,0-; L(p,d),(d,p)=0 rules out 0- 
T weighted average of 241 ns {I3} (1979Ad02) and 247 ns {I1} (1976Io03) in (p,n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 8-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Adopted Levels of {+120}Sb in ENSDF database. The excitation energy of the 8- isomeric level is not known and set to 0.0 on the energy scale given in 2014Li31. 
$Decay mode is from Adopted Levels of {+120}Sb in ENSDF database 
$Configuration=|pd{-5/2}~#|nh{-11/2}~#({+118}Sn,0+ g.s.) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 14+
level_comment:
T$proposed to be isomeric by 2014Li31 since corresponding 7- core state in {+118}Sn is isomeric. This is consistent with non-observation of transitions above this level. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$configuration=(|p 2d{-5/2}) 
MOMM1$from 2005St24; recalculated with the use of |m value of {+23}Na standard (2005St24) 
MOME2$from 2005St24; Sternheimer or other polarization correction included (2005St24). Other: -0.45 {I3} (AB,R) (2005St24) 
J$J=5/2 in optical spectroscopy, microwave absorption in gases (1976Fu06), L=2 in ({+3}He,d), (t,|a) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
E$from (|g,|g') (2006Wi04) 
J$M1 |g to 5/2+. Fed in |e decay and |b- decay from 11/2- 
MOMM1$from 2005St24; consistent with |m value for {+121}Sb g.s. standard 
MOME2$from 2005St24; consistent with Q value of {+121}Sb g.s., Sternheimer or other polarization correction included (2005St24) 
T$from (|b)(K x ray)(t) (1982Ha31). Others: 2.96 ns {I8} from (470|g)(37|g)(t), (1102|g)(37|g)(t) (1973Be18); 3.5 ns {I2} from (1102|g)(ce 37|g)(t) (1964Ch08); 3.47 ns {I39} from (|g,|g')(2000Ki15) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J L=0 in (t,|a). 
T$from unweighted average of 8.5 ps {I10} in (|g,|g') and 11.6 ps {I9} in Coul. ex 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J |g(|q) in (n,n'|g); M1+E2 |g to 5/2+ 
T$weighted average of 0.18 ps {I4} from (|g,|g') and 0.14 ps {I5} from Coul.ex. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J |g(|q) in (n,n'|g); Coul. ex. J|p is consistent with two-particle, one-hole calculation (1975Me23) 
T$from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 9/2+,11/2+
level_comment:
J |g's to 7/2+, 9/2+, no |g to 5/2+; log| {Ift}=7.8 from 11/2-; L=2 in (p,t); two-particle, one-hole calculation of 1975Me23 suggests 11/2+ 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J |g(|q) in (n,n'|g); Coul. ex. 
T$from (|g|g') (1981Ca10); other: 0.21 ps {I7} (1975An16) from Doppler-shift attenuation in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+,7/2+
level_comment:
J$|g's to 3/2+ and 7/2+, L=2 in (p,t). L=1 in (t,|a) is not consistent with this assignment, but the energy resolution is only 30 keV so other levels may be contributing. L=2 in ({+3}He,d) confirms |p=+ 


level_energy_unit: KEV
level_spin_parity: (19/2)-
level_lifetime_unit: NS
level_comment:
T$from {+121}Sb IT decay (179 |ms) 
T$weighted average of 8.5 ns {I5} from {+121}Sb IT decay (179 |ms) and 7.7 ns {I2} from {+120}Sn({+7}Li,|a2n) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (25/2)
level_lifetime_unit: US
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x<60 keV for E2, <80 keV for M2 based on typical Weisskopf estimates 
T$weighted average of 179 |ms {I6} (2009Wa02), 161 |ms {I20} (2008Ko03), 203 |ms {I50} (2008Ko03) and 200 |ms {I30} (2008Jo03) 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: US
level_comment:
T$weighted average of decay curves for 169.8, 286.6 and 323.2 |g rays 
E$from E|g=10-40 keV (if E2) to 2720.9 level, based on Weisskopf estimate (2009Wa02) 
J$(25/2) in adopted levels 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=0.133|*10{+-3} {I13} 
S$Other: 0.00011 eV {I5} (1973B012) 
T$from |G(|g{-0}){+2}/|G and |G(|g{-0})/|G=0.9184 {I20} from adopted gammas 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=0.0173|*10{+-3} {I20} 
S from 1963Me13 
T$from |G(|g{-0}){+2}/|G and |G(|g{-0})/|G=0.984 {I4} from adopted gammas 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=0.05|*10{+-3} {ILT} 
E$rounded-off value from adopted levels 
S$from 1973Bo12 
T$from |G(|g{-0}){+2}/|G and |G(|g{-0})/|G=0.105 {I3} from adopted gammas 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=3.3|*10{+-3} {I7} 
S$Weighted average of 0.00385 eV {I35} (1981Ca10) and 0.0025 eV {I3} (1973Bo12) with external uncertainty 
T$from |G(|g{-0}){+2}/|G 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=0.08|*10{+-3} {ILT} 
E$rounded-off value from adopted levels 
S$from 1973Bo12 
T$from |G(|g{-0}){+2}/|G and |G(|g{-0})/|G=0.007 {I3} from adopted gammas 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=0.88|*10{+-3} {I8} 
S$from 1981Ca10; other: 0.000.9 eV {I2} (1973Bo12) 
T$from |G(|g{-0}){+2}/|G and |G(|g{-0})/|G=0.73 {I8} from adopted gammas 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=4.0|*10{+-3} {I3} 
S$others: 0.0049 eV {I5} (1981Ca10), 0.0046 eV {I6} (1973Bo12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=0.04|*10{+-3} {ILT} 
E,S$from 1973Bo12; 1979Bo12 report E=1446 {I5} with J|p=(11/2-) using an early version of the Nuclear Data Sheets. There is a level at 1447.51 with J|p=3/2+,5/2+,7/2+ and the (11/2-) level is at 1426.88. It isn't clear to which of these levels the authors' width data applies. 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=1.0|*10{+-3} {ILT} 
E$from adopted levels. This level has been reported only in (p,t) and in (d,d'),(|a,|a') 
S$from 1973Bo12 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
$g|G(|g{-0}){+2}/|G (eV)=1.0|*10{+-3} {I2} 
E$1981En03 use a Doppler-shifted 3451|g in {+56}Fe from {+56}Co source to excite the 3451 level. E|g=3451.119 {I4} (2004He14), the resonance energy is 2 eV and the recoil correction is 53 eV. 
S$from 1981En03 
T$from g|G(|g{-0}){+2}/|G and |G(|g{-0})/|G=0.63 {I4} one gets T{-1/2}=0.18g ps {I4}. 
J |g's to 7/2+, 1/2+ 


level_energy_unit: KEV
level_comment:
E$The authors report 1590.5 |g transition whose placement to the 37 level. However, a 1590.4 level is reported in (|g,|g'). Evaluators reassign the |g-ray to a 1590.5 level. 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E$The authors report a 1575.4 transition whose placement is either to gs or to the 37 level. A 1612 level is reported in (p,t), so the placement to the 37 level, giving E(Level)=1612.5 is established 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
BE2 weighted average of 0.007 {I2} (1966Ba45), 0.013 {I4} (1969Ga25), 0.011 {I2} (1975An16), 0.010 {I3} (1979Ho28), 0.0132 {I41} (1989Ja13) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
BE2 weighted average of 0.027 {I3} (1966Ba45), 0.020 {I4} (1969Ga25), 0.028 {I2} (1975An16), 0.024 {I3} (1979Ho28), 0.027 {I4} (1989Ja13) other: 0.012 {I1} (1977Ku23) 
T$from B(E2) and adopted |g branching=0.9896 {I12} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
BE2 unweighted average of 0.0007 {I2} (1975An16), 0.0007 {I2} (1979Ho28), 0.0006 {I2} (1989Ja13); other: 0.0180 {I13} (1977Ku23) 
T$from B(E2) and adopted |g branching=0.105 {I3} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
BE2 weighted average of 0.100 {I16} (1966Ba45), 0.070 {I5} (1975An16), 0.100 {I16}(1979Ho28), 0.0180 {I35} (1989Ja13); other: 0.0300 {I22} (1977Ku23) 
T from Doppler-shift attenuation (1975An16) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
BE2 unweighted average of 0.004 {I1} (1969Ga25), 0.0029 {I3} (1975An16), 0.004 {I1} (1989Ja13); other: 0.0036 {I4} (1977Ku23) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
BE2 unweighted average of 0.120 {I16} (1966Ba45), 0.03 {I1} (1969Ga25) 
$Others: 0.081 {I5} (1975An16), 0.0224 {I33} (1989Ja13) 
T$from Doppler-shift attenuation (1975An16) 


level_energy_unit: KEV
level_comment:
BE2 unweighted average of 0.020 {I5} (1966Ba45), 0.020 {I5} (1979Ho28); 
$Others: 0.007 {I2} (1975An16), 0.0180 {I17} (1977Ku23) 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=6.09 mb/sr {I24} (6|'), 1.75 mb/sr {I7} (18|') 
$({+3}He,d): d|s/d|W=0.96 mb/sr {I5} (6|'), 2.54 mb/sr {I10} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=5.35 mb/sr {I21} (6|'), 2.42 mb/sr {I9} (18|') 
$({+3}He,d): d|s/d|W=0.13 mb/sr {I2} (6|'), 0.23 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=1.25 mb/sr {I5} (6|'), 0.43 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.26 mb/sr {I2} (6|'), 0.60 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.82 mb/sr {I5} (6|'), 0.24 mb/sr {I2} (18|') 
$({+3}He,d): d|s/d|W=0.30 mb/sr {I2} (6|'), 0.82 mb/sr {I4} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=7.84 mb/sr {I30} (6|'), 3.82 mb/sr {I14} (18|') 
$({+3}He,d): d|s/d|W=0.09 mb/sr {I1} (6|'), 0.09 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.16 mb/sr {I1} (6|'), 0.052 mb/sr {I4} (18|') 
$({+3}He,d): d|s/d|W=0.60 mb/sr {I3} (6|'), 0.40 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.39 mb/sr {I2} (6|'), 0.17 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.15 mb/sr {I2} (6|'), 0.39 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.24 mb/sr {I1} (6|'), 0.09 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.34 mb/sr {I3} (6|'), 0.15 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.19 mb/sr {I1} (6|'), 0.08 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.19 mb/sr {I2} (6|'), 0.27 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.34 mb/sr {I2} (6|'), 0.13 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.24 mb/sr {I2} (6|'), 0.53 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.38 mb/sr {I2} (6|'), 0.17 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.07 mb/sr {I1} (6|'), 0.07 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.15 mb/sr {I1} (6|'), 0.07 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.21 mb/sr {I2} (6|'), 0.13 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
MOMM1,MOME2,J$from hyperfine structure measurement using |m({+123}Sb)=2.5457 |m{-N} {I12} and Q({+123}Sb)=-0.692 b {I14} as references. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
$|m: dynamic nuclear orientation, value references to {+121,123}Sb (1958Pi45,2005St24) 
$Q: atomic resonance with magnetic state selection, value is relative to {+121}Sb and includes the Sternheimer correction (1960Fe08,2005St24); other: +0.9 {i2} static nuclear orientation (1985He16,2005St24) 
J atomic beam J=2; |p=- is consistent with the log {If{+1u}t}=9.7 to 0+; this rules out J|p=2+ 
T from 1990Ab06. Others: 2.681 d {i3} (1967Ha27) and 2.714 d {i6} (1972Em01), 2.84 d {i12} (1973Ka45), 2.68 d {i4} (1972Pa13), 2.82 d {i5} (1968Bo25), 2.74 d {i1} (1958Gu09), 2.73 d {i3} (1958Pe17), 2.75 d {i2} (1954Co08), 2.80 d {i2} (1951Bl31) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 3+,4+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E this level is suggested in (d,p) and (p,d) as a composite peak unresolved from g.s. 
J L=0+5 in (p,d), L=(2) in (d,p) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: US
level_comment:
$|m: stroboscopic observation of perturbed angular distributions, value is relative to {+121,123}Sb (1973He10,2005St24) 
$Q: differential perturbed angular distribution of |g rays following nuclear reactions, value is relative to {+121}Sb and includes the Sternheimer correction (1982Ma29,2005St24) 
J L=0 in (p,d); E1 |g to 2- 
T from {+122}Sn(p,n|g) (1973He10). Others: 1.8 |ms {I2} in {+122}Sb IT decay (1962De20), 1.66 |ms {I25} in {+121}Sb(n,|g) (1974Iv02) 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
J see comment on 163.55 level 
T from (ce 26|g)(ce 77|g)(t) in {+122}Sb IT decay (1963De05) 
$|m: differential perturbed angular distribution of |g rays following nuclear reactions (1977Co18,1989Ra17) 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M2
level_comment:
J$(E3)-E2 cascade to 3+ level via the 137.47 level along with T{-1/2} for the 163.55 and 137.47 levels and systematics of 8- state suggests J|p(163.55)=(8)- and J|p(137.47)=(5)+ 
T$from 1990Ab06. Others: 4.21 min {i3} (1963Ke04), 4.15 min {i15} (1963De05), 4.15 min {i20} (1962En04), 4.2 min {i3} (1968Bo25), 3.5 min (1947De06) 


level_energy_unit: KEV
level_spin_parity: (6)-
level_comment:
J M1-M1 cascade to (8)- level via the 265.11 level, and M1-M1-M1-M1 cascade via 264.43, 192.96 and 78.09 levels to 2- (gs) are consistent with only J|p=(6)-; thus J|p(265.11)=(7)-, J|p(264.43)=(5)-, J|p(192.96)=(4)- and J|p(78.09)=(3)- 


level_energy_unit: KEV
level_spin_parity: (3,4)
level_comment:
J L=2+4 in (p,d) and (M1) |g from 3+ resonance in (n,|g) suggest a possibility of exciting |p=+ level, but contradicts with M1,E2 |g to (5)-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
Composite states: E=4.6-10.5 MeV; configuration=(|p1h{-11/2})(|n1h{-9/2}){-(10+)} (|p1h{-11/2})(|n1i{-13/2}){-(12-)} 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
T from (ce(L) 26|g)(ce(K) 76|g+ce(K) 61|g)(t) (1963De05). Other: 0.53 ms {i5} (1962En04) 
g-factor(5+)=+0.61 {i2} (1977Co18) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
Composite states: E=4.6-10.5 MeV; configuration=|p1h{-11/2})(|n1h{-9/2}){-(10+)} (|p1h{-11/2})(|n1i{-13/2}){-(12-)} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: US
level_comment:
g-factor=+0.988 {i4} (stroboscopic resonance curves of the 61.1-keV |g transition) (1973He10) 
T from decay curve of the 61.41-keV |g (1973He10) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$spin=7/2 from optical spectroscopy J=7/2 (1932Ba01, 1934Cr03, 1978Bu24); parity from L(t,|a)=L(|a,t)L({+3}He,d)=4 from 0+ 
MOMM1$from 2014StZZ, deduced from |n({+123}Sb)/|n({+2}H)=0.84423 {I8} measured by NMR (1951Pr02). See also 2014StZZ compilation 
MOME2$from optical spectroscopy (1978Bu24). The 2016St14 compilation quotes a value of -0.692 {I14}, from a calculation by R.L.A. Haiduke et al.: Jour Chem Phys 125, 064301 (2006) 
$Nuclear rms charge radius=4.6879 fm {I25} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$L(t,|a)=L({+3}He,d)=2 from 0+; 160.3|g M1+E2 to 7/2+. 
T$from {+123}Sn |b{+-} decay (40.06 min), as weighted average of 0.60 ns {I8} (1970Si21), 0.64 ns {I5} (1963Sc12), 0.57 ns {I7} (1969Sh12), 0.60 ns {I4} (1973Be18) and 0.62 ns {I21} (1964Sh23). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: PS
level_comment:
J$L(t,|a)=L({+3}He,d)=2 from 0+; spin=3/2 proposed in (|a,p) based on J-dependence 
T$from B(E2)=0.033 {I3} in Coulomb excitation, adopted branching=29% {I3} for 541.9|g, if J=3/2 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$1030.3|g M1+E2 to 7/2+; J=9/2 (favored) or 11/2 (0.13% confidence) from |g(|q) in (n,n'|g) (1979Ho28). 
T$From |G=0.0030 eV {I2} in (|g,|g'). Others: 90 fs {I35} DSAM (1975An16), 0.19~ps~{I3} (1978Ca25). 1978Ca25 superseded by 1981Ca10 whose width is already included in the average in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$1088.6|g E2, |DJ=2 to 7/2+; spin=(9/2,11/2) from |g(|q) in (n,n'|g) (1979Ho28) and 11/2 from |g(|q) in Coulomb excitation (1989Ja13). But spin=9/2 from |g(|q) of 1977Ku23 in Coulomb excitation and 1978Be45 in (|g,|g') is inconsistent 
T$weighted average of 0.53 ps {I+5-4} from width in (|g,|g') and 0.45 ps {I11} from DSAM in Coulomb excitation (1975An16). 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_comment:
J$from |g(|q) in Coulomb excitation (1977Ku23). Other: 11/2 from |g(|q) in (|g,|g') is inconsistent with 1021.2|g to 5/2+ and 1181.1|g D+Q to 7/2+. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$(5/2,7/2,9/2) from dipole excitation in (|g,|g'); 395.3|g from 11/2-; 1100.6|g to 5/2+; 9/2+ proposed in ({+7}Li,|a2n|g) (2009Wa02) and ({+31}P,X|g) (2005Po03). But L(|a,t)=5 from 0+ gives 9/2-,11/2- for a level at 1262 {I1} 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$L({+3}He,d)=2 from 0+; spin=(5/2,7/2,9/2) from dipole excitation from 7/2+ g.s. in (|g,|g') (2002Br05) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$L({+3}He,d)=2+5 for a level at 1644 {I1}, most likely the L=2 component; spin=(5/2,7/2,9/2) from dipole excitation from 7/2+ in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J$L(|a,t)=5 from 0+ for a level at 1644 {I1}; L({+3}He,d)=2+5 from 0+ for a level at 1644 {I1}, most likely the L=5 component; J=11/2 from J-dependence of |s(|q) in (|a,p) for a level at 1643; 11/2- proposed in ({+7}Li,|a2n|g) (2009Wa02) and ({+31}P,X|g) (2005Po03) 


level_energy_unit: KEV
level_spin_parity: (15/2)-
level_lifetime_unit: NS
level_comment:
J$381.1|g E2, |DJ=2 to 11/2- 
T$from |g|g(t) in ({+7}Li,|a2n|g) (2009Wa02). Other: 37 ns {I4} from from |g|g(t) in 2008Jo03 in {+123}Sb IT decay (214 ns) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
J$200.5|g to (15/2)-; 375.7|g from (23/2+) isomer (61 |ms) 
T$from |g|g(t) in ({+7}Li,|a2n|g) (2009Wa02). Others: 190 ns {I30} from |g(t) in {+123}Sb IT decay (214 ns) (2008Jo03), 222 ns {I23} from |g(t) in {+9}Be({+238}U,F|g) (2019Bi04); 110 ns {I10} from |g(t) in ({+31}P,X|g) (2005Po03) is discrepant 


level_energy_unit: KEV
level_spin_parity: (19/2)+
level_lifetime_unit: NS
level_comment:
J$441.8|g E2 to (15/2)+; band assignment 
T$from centroid-shift analysis in ({+7}Li,|a2n|g) (2009Wa02) 


level_energy_unit: KEV
level_comment:
E$since spin of this level in (|g,|g') is expected to be (5/2,7/2,9/2) from dipole excitation from 7/2+ g.s., it could be a different level from the 2522, 1/2+ level in ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$127.8|g (E2), |DJ=(2) to (19/2)+; band assignment. (21/2+) proposed by 2005Po03 in ({+31}P,X|g) 
T$unweighted average of 66 |ms {I4} from {+9}Be({+238}U,F|g) (2019Bi04), 65 |ms {I1} (2009Wa02), 52 |ms {I3} (2008Jo03) and 66 |ms {I4} (2007Ju06), in {+123}Sb IT decay (61 |ms). 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E$weighted average of 2811 {I7} in ({+3}He,d) (2014MiZZ) and 2799 {I10} in (t,|a) (1973Co33) 
J$L({+3}He,d)=0 and L(|a,t)=4 components for a peak at 2811 in 2012MiZY 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$adopted value is weighted average of 0.60 ns {I8} (1970Si21), 0.64 ns {I5} (1963Sc12), 0.57 ns {I7} (1969Sh12), 0.60 ns {I4} (1973Be18) and 0.62 ns {I21} (1964Sh23). 


level_energy_unit: KEV
level_comment:
E$others: 160 {I10} (1966Ba45), 165 {I10} (1966Ba25) 
S$other: 0.8 for J=5/2 (1968Co22) 
$d|s/d|W=0.71 {I4} (6|'), 2.17 {I9} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$others: 537 {I10} (1966Ba45), 541 {I10} (1966Ba25) 
S$others: 0.184 {I22} (2012MiZY), 0.3 (1968Co22), for J=L-1/2 
$d|s/d|W=0.14 {I1} (6|'), 0.45 {I2} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$others: 712 {I10} (1966Ba45), 722 {I10} (1966Ba25) 
S$other: 0.35 (1968Co22) 
$d|s/d|W=0.81 {I4} (6|'), 0.68 {I3} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$other: 1502 {I10} (1966Ba45) 
S$other: 0.123 {I10} for J=L-1/2 (2012MiZY); 0.1 for J=L+1/2 and 0.05 for J=L-1/2 (1968Co22) 
$d|s/d|W=0.31 {I2} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$other: 1574 {I10} (1966Ba45) 
S$other: 0.176 {I8} for J=L-1/2 (2012MiZY) 
$d|s/d|W=0.53 {I2} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$other: 1644 {I10} (1966Ba45) 
L,S$from 1968Co22. C{+2}S=0.15 for J=L+1/2 and 0.07 for J=L-1/2 with L=2, 0.5 for L+1/2 with L=5 
$d|s/d|W=0.08 {I1} (6|'), 0.13 {I1} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$other: 1740 {I30} (1968Co22) 
L$from 1968Co22. Other: (2) from 2012MiZY 
S$for J=L-1/2 (2012MiZY). Others: 0.1 for J=L+1/2 and 0.05 for J=L-1/2 (1968Co22) 
$d|s/d|W=0.26 {I2} (6|') 


level_energy_unit: KEV
level_comment:
E$other: 2100 {I30} (1968Co22) 
S$others: 0.082 {I8} for J=L-1/2 (2012MiZY); 0.2 for J=L+1/2 and 0.12 for J=L-1/2 (1968Co22) 
$d|s/d|W=0.17 {I2} (6|'), 0.25 {I1} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
L$contains L=4 component from (|a,t) data in 2012MiZY 
$d|s/d|W=0.14 {I1} (6|'), 0.06 {I1} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$other: 2520 {I30} (1968Co22) 
L$other: L=2 component also reported in 2012MiZY 
S$others: 0.4 for L=0 (1968Co22); 0.088 {I8} for J=L-1/2 and 0.058 {I5} for J=L+1/2, with L=2 (2012MiZY) 
$d|s/d|W=1.30 {I6} (6|'), 0.84 {I4} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
E$other: 2750 {I30} (probable multiplet, 1968Co22) 
S$others: 0.041 {I5} for J=L-1/2 (2012MiZY); 0.58 for J=L+1/2 and 0.25 for J=L+1/2 (1968Co22) 
$d|s/d|W=0.11 {I8} (6|'), 0.14 {I1} (15|') (mb/sr) 


level_energy_unit: KEV
level_comment:
L$contains L=4 component from (|a,t) data in 2012MiZY 
$d|s/d|W=0.32 {I9} (6|'), 0.27 {I2} (15|') (mb/sr) 


level_energy_unit: KEV
level_spin_parity: 23/2+
level_lifetime_unit: US
level_comment:
T$from summed double gated time spectra for 127-442-956-1089 cascade (2009Wa02). Other: 66 |ms {I4} from 2007Ju06 (pulsed beam timing) 


level_energy_unit: KEV
level_spin_parity: 9/2
level_lifetime_unit: PS
level_comment:
$g|G{-0}{+2}/|G=0.00300 {I23} 
T$from g|G{-0}=0.0030 eV {I23} if |G{-0}/|G=1.0. 
S$weighted average of 0.00302 {I23} (2002Br05), 0.00296 {I27} (1981Ca10) and 0.0030 {I3} (1973Bo12), assuming |G{-0}/|G=1.0. 


level_energy_unit: KEV
level_spin_parity: 9/2
level_lifetime_unit: PS
level_comment:
$g|G{-0}{+2}/|G=0.00107 {I9} 
J$11/2+ in Adopted Levels 
T$from g|G{-0}=0.00107 eV {I7} if |G{-0}/|G=1.0 
S$weighted average of 0.00112 {I15} (2002Br05), 0.00106 {I9} (1981Ca10) and 0.0010 {I2} (1973Bo12), assuming |G(|g{-0})/|G=1.0. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$g|G{-0}{+2}/|G=0.0021 {I4} 
J$(3/2,5/2)+ quoted in 1973Bo12 
$g|G{-0}=0.00295 eV {I39} (2002Br05), 0.0038 eV {I8} (1973Bo12) 


level_energy_unit: KEV
level_comment:
$g|G{-0}{+2}/|G=0.00161 {I23} 
E$other: 1778 {I2} with g|G{-0}{+2}/|G=0.0016 eV {I6} unassigned to {+121}Sb or {+123}Sb by 1973Bo12 


level_energy_unit: KEV
level_comment:
$g|G{-0}{+2}/|G=0.00190 {I24} 
E$other: 1897 {I2} with g|G{-0}{+2}/|G=0.0015 eV {I5} unassigned to {+121}Sb or {+123}Sb by 1973Bo12 


level_energy_unit: KEV
level_comment:
$g|G{-0}{+2}/|G=0.00505 {I43} 
E$other: 2321 {I2} with g|G{-0}{+2}/|G=0.0053 eV {I15} unassigned to {+121}Sb or {+123}Sb by 1973Bo12 


level_energy_unit: KEV
level_comment:
$g|G{-0}{+2}/|G=0.00223 {I30} 
E$other: 2429 {I2} with g|G{-0}{+2}/|G=0.0025 eV {I7} unassigned to {+121}Sb or {+123}Sb by 1973Bo12 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$spin=5/2 supported by |g(|q) in 1977Ku23 
T$from Adopted Levels. 
BE2$unweighted average of 0.0043 {I7} (1966Ba45), 0.0023 {I8} (1969Ga25), 0.0046 {I4} (1977Ku23), and 0.0023 {I4} (1989Ja13). Other: 0.005 (1973Re08) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^=0.033 {I3}, adopted branching=29% {I3} for 541.9|g 
BE2$weighted average of 0.040 {I3} (1975An16), 0.028 {I4} (1966Ba45), 0.028 {I6} (1969Ga25), and 0.030 {I3} (1989Ja13). Other: 0.036 (1973Re08). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
J$spin=11/2 from |g(|q) in 1977Ku23 is considered questionable by the evaluator. 
T$from DSAM in 1975An16. Value from Adopted Levels is 190 fs {I+16-14} 
BE2$weighted average of 0.073 {I9} (1975An16), 0.08 {I1} (1966Ba45), 0.090 {I20} (1969Ga25), 0.0700 {I45} (1977Ku23). Others: 0.0196 {I30} (1989Ja13) seems discrepant; 0.084 (1973Re08) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$spin=9/2 from |g(|q) in 1977Ku23, but 11/2 from |g(|q) in 1989Ja13 
T$from DSAM in 1975An16. Value from Adopted Levels is 0.52 ps {I+5-4} 
BE2$unweighted average of 0.076 {I8} (1975An16), 0.07 {I1} (1966Ba45), 0.042 {I9} (1969Ga25), 0.0300 {I28} (1977Ku23). Other: 0.0206 {I30} (1989Ja13) is discrepant with all other values; 0.087 (1973Re08) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_comment:
J$spin=(5/2,7/2) from |g(|q) in 1977Ku23 
BE2$weighted average of 0.0085 {I8} (from 1181|g yield in 1977Ku23) and 0.008 {I2} (from yield of 1021.8|g in 1975An16). 


level_energy_unit: KEV
level_spin_parity: (19/2)+
level_lifetime_unit: NS
level_comment:
T$from centroid-shift analysis (2009Wa02). Other: 7.9 ns {I4} from 2006JoZY is discrepant; no T{-1/2} is reported for this level by 2008Jo03, which supersedes 2006JoZY 


level_energy_unit: KEV
level_comment:
L$contains L=0 component from ({+3}He,d) data in 2012MiZY 
$d|s/d|W=0.24 {I2} (6|'), 0.12 {I1} (18|') (mb/sr) 


level_energy_unit: KEV
level_comment:
L$contains L=0 component from ({+3}He,d) data in 2012MiZY 
$d|s/d|W=0.54 {I3} (6|'), 0.22 {I1} (18|') (mb/sr) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: D
level_comment:
T from calorimetry of {+124}Sb source using {+123}Sb enriched target (1966Fl01); others: 60.11 d {I7} (2000Kh04), 60.4 d {I2} (1957Ma50), 59.9 d {I5} (1958Jo01), 60.1 d {I3} (1959Ca12), 60.3 d {I2} (1968Re04) 
J atomic beam (1976Fu06); |b{+-} to 2+, 602.7-keV level in {+124}Te indicates 1-yes shape. Expected 3- member of multiplet with configuration=((|p g{-7/2})(|n h{-11/2})) 
MOMM1 From radiative detection of nuclear magnetic resonance, value is referenced to {+122}Sb and recalculated (1974Ca06,1989Ra17). See also 2005St24 compilation. 
MOME2$from static nuclear orientation, value is referenced to {+121}Sb and Sternheimer correction included (1985He16,1989Ra17). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T from |g(t) (1962Va18); others: 78 s (1947De06), 96 s {I12} (1963Br18) 
J log| {Ift}=4.4 to {+124}Te 6+; strong primary |g from 4+ resonance. Expected 5+ member of multiplet with configuration=((|p g{-7/2})(|n d{-3/2})) 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M2
level_comment:
T from |g(t) (1967Ha27); others: 21 min (1947De06), 21 min {I1} (1962Va18) 
J E3 |g to 5+, no |g to 3-; Expected 8- member of multiplet with configuration=((|p g{-7/2})(|n h{-11/2})) 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_lifetime_unit: US
level_comment:
MOMM1 For J=3. From differential perturbed angular distribution of |g rays following nuclear reactions (1981Io04,1989Ra17). See also 2005St24 compilation. 
J E2 |g to 5+, E1 |g to 3-; Expected 3+ member of multiplet with configuration=((|p g{-7/2})(|n d{-3/2})) 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_lifetime_unit: NS
level_comment:
J M1 |g to 3+,4+; |g to 3-; L=0+2 in (d,p); Expected 3+ member of multiplet with configuration=((|p g{-7/2})(|n s{-1/2})) 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
J see for comment to 125.2-keV level; Expected 4- member of multiplet with configuration=((|p g{-7/2})(|n h{-11/2})) 


level_energy_unit: KEV
level_spin_parity: (6)-
level_lifetime_unit: NS
level_comment:
MOMM1 From differential perturbed angular distribution of |g rays following nuclear reactions (1981Io04,1989Ra17). See also 2005St24 compilation. 
J E2-M1 cascade via 87.6-keV level (J|p=4-) to g.s.(J|p=3-), and E2 |g to (8)-; Expected 6- member of multiplet with configuration=((|p g{-7/2})(|n h{-11/2})) 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
J$strong |g from 4+ resonances; M1 |g to 4-; Expected 5- member of multiplet with configuration=((|p g{-7/2})(|n h{-11/2})) 


level_energy_unit: KEV
level_spin_parity: (7,8)-
level_comment:
J M1 |g to (8)-, |g to 6-; Expected 7- member of multiplet with configuration=((|p g{-7/2})(|n h{-11/2})) 


level_energy_unit: KEV
level_spin_parity: 4+,5+
level_comment:
J M1 |g to 3+,4+; M1+E2 |g to 5+; Expected 4+ member of multiplet with configuration=((|p g{-7/2})(|n d{-3/2})) 


level_energy_unit: KEV
level_spin_parity: 3+,4+,5+
level_comment:
J M1 |g to 3+,4+; |g to 5+; L=0+2 in (d,p); Expected 4+ member of multiplet with configuration=((|p g{-7/2})(|n s{-1/2})) 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
J M1 |g to 3+,4+; |g to 5+; L=0+2 in (d,p); Expected 4+ member of multiplet with configuration=((|p g{-7/2})(|n d{-3/2})) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: Y
level_comment:
J L=4 in (d,{+3}He), ({+3}He,d), (t,|a); |DJ=2-yes shape |b{+-} feeds 11/2- daughter (1959Na06,1964Ma30,1966Ma49) 
T$From weighted average of 1007.56 d {I10} (1992Un01), 1008.1 d {I8} (1983Wa26) and 1007.3 d {I3} (1980Ho17)(1y=365.242 d). Others: 2.6 y {I1} (1960Kl04), 2.78 y {I4} (1961Wy01), 2.71 y {I2} (1965Fl02), 2.81 y {I5} (1966La13), 2.7 y (1950Le09) 
MOMM1 $ From nuclear magnetic resonance on oriented nuclei (1989Ra17). 1974Ca06 give measurement. See also 2005St24 compilation. 
Configuration=(|p 1g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in ({+3}He,d), (t,|a); M1+E2 |g to 7/2+ 
T From {+125}Sn |b{+-} decay (9.52 min) 
Configuration=(|p 2d{-5/2}) 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-
level_comment:
J E1 |g to 9/2+ and 11/2+. Large C{+2}S in (d,{+3}He) favors 11/2-; however, this requires the weak gs |g to be M2. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J Log| {Ift}=6.53 from 11/2-, M1+E2 |g's to 11/2+ and 9/2+, |g|g(|q) (1971Ma01,1980Ve04) favors 9/2. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
The closest level of L=(1) is observed at 4060 keV in {+124}Sn(d,p). Energy difference is too large. 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=5.09 mb/sr {I12} (6|'), 2.31 mb/sr {I9} (18|') 
$({+3}He,d): d|s/d|W=0.13 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=9.86 mb/sr {I10} (6|'), 2.78 mb/sr {I3} (18|') 
$({+3}He,d): d|s/d|W=1.02 mb/sr {I4} (6|'), 2.00 mb/sr {I3} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=1.94 mb/sr {I6} (6|'), 0.51 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.20 mb/sr {I1} (6|'), 0.36 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.57 mb/sr {I2} (6|'), 0.17 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.07 mb/sr {I1} (6|'), 0.20 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=1.35 mb/sr {I6} (6|'), 0.32 mb/sr {I5} (18|') 
$({+3}He,d): d|s/d|W=0.27 mb/sr {I2} (6|'), 0.53 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=9.20 mb/sr {I10} (6|'), 4.66 mb/sr {I4} (18|') 
$({+3}He,d): d|s/d|W=0.07 mb/sr {I1} (6|'), 0.11 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.57 mb/sr {I4} (6|'), 0.17 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.13 mb/sr {I1} (6|'), 0.39 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.56 mb/sr {I2} (6|'), 0.18 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.13 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.52 mb/sr {I2} (6|'), 0.16 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.39 mb/sr {I2} (6|'), 0.53 mb/sr {I2} (15|') 


level_energy_unit: KEV
level_comment:
$(|a,t): d|s/d|W=0.31 mb/sr {I2} (6|'), 0.11 mb/sr {I1} (18|') 
$({+3}He,d): d|s/d|W=0.11 mb/sr {I1} (6|'), 0.16 mb/sr {I1} (15|') 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: D
level_comment:
J log| {Ift}=8.57 {I23} to 7- {+126}Te level and (E3) |g from the (5)+, 17.7-keV isomer. 
T from weighted av of 12.2 d {I1} (1961Ha39), 12.5 d {I2} (1962Dr01), 12.4 d {I1} (1967Ha27) and 12.4 d {I1} (1971Or04); Other: 12.47 d (1972Pa13). 
MOMM1$from static nuclear orientation (1972Kr15,2019StZV) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J log| {Ift}=5.74 {I5} to 6+ {+126}Te level limits J|p=5,6,7, but 5+ is preferred since this is the highest spin possible for a positive parity state with the available neutron (h{-11/2},d{-3/2},s{-1/2}) and proton (g{-7/2},d{-5/2},s{-1/2}) shell-model orbitals. For J|p=6+ B(M2)=2.7E-7 is unreasonably small. J|p=7+ is clealy ruled out since an E1 would not have such a long lifetime. 
T weighted av of 19.0 min {I2} (1962Dr01), 19.2 min {I1} (1967Ha27), 19 min {I1} (1970Mu16) 19.0 min {I3} (1971Or04), and 19.6 min {I10} (1972Pa13). Other: 18.8 min (1956Fr31). 
%B-,%IT$from 2010Fe02. Other: %|b{+-}=86 {I4}, %IT=14 {I4} (1971Or04) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: S
level_lifetime_info: ;ERR=AP;ISO=M2
level_comment:
J 22.7-keV, (M2) |g to (5+), no |g to (8-). 
T$The authors of 1976Sm01 give 11.1 s {I10.5} by a computer analysis. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: S
level_lifetime_info: ;ERR=AP;ISO=M2
level_comment:
T from analysis of delayed coin (30-90|g)(14-21|g)(t), (true coin)/(accidental)=0.0002. Computer analysis gave 11.1 s {I10.5}. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: D
level_comment:
J L=4 in (d,{+3}He) and (t,|a) for {+127}Sb g.s., L=2 in (d,t) and ({+3}He,|a) for the 473 level in {+127}Te, and the existing of a |b{+-} branch connecting these levels uniquely establishes J|p({+127}Sb g.s.)=7/2+, and J|p({+127}Te 473)=5/2+ 
T$weighted av of 3.9 d {I1} (1950Sl17), 3.67 d {I9} (1957Bo96), 3.89 d {I7} (1962Dr01), 92 d {I9} (1962Uh01), 3.80 d {I8} (1967Ha27), 3.75 d {I10} (1967Ta05), 3.91 d {I7} (1972Pa13). Others: 3.3 d (1939Ab02), 4.0 d (1946Gr06) 
Configuration=(|p 1g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J L=2 in (d,{+3}He) and (t,|a) and comparison of C{+2}S with values for {+125,129}Sb. 5/2+ is favored from systematics of odd Sb, and the shell model calculation (2007Ji14) supports 5/2+. 
Configuration=(|p 2d{-5/2}) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J L=2 in (d,{+3}He) and (t,|a). C{+2}S for d{-5/2}) is exhausted by the 491 level. 3/2+ is favored from systematics of odd Sb. 
Configuration=(|p 2d{-3/2}) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J logft=7.1 from (3/2+), |g to 7/2+, systematics of odd Sb nuclides 
Configuration=(({+126}Sn 2+)(|p 1g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J from systematics of odd Sb nuclides. log| {If{+1u}t}>7.7 from (11/2-), |g to 5/2,7/2+,9/2. 
Configuration=(({+126}Sn 2+)(|p 1g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J from systematics of odd Sb nuclides. log| {If{+1u}t}=8.1 from (11/2-), |g to 5/2,7/2+. 
Configuration=(({+126}Sn 2+)(|p 1g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J |g to (11/2+), transition in yrast (g.s.) band; systematics of level energies in {+123}Sb,{+125}Sb, and {+127}Sb 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J L=1 in (d,{+3}He) and (t,|a), From C{+2}S and shell model analysis 1/2- is favored 
Configuration=(|p 2p{-1/2}) 


level_energy_unit: KEV
level_spin_parity: 3/2-,1/2-
level_comment:
J L=1 in (t,|a), From C{+2}S and shell model analysis 3/2- is favored. 
Configuration=(|p 2p{-3/2}) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: US
level_comment:
T From (438.2|g)(1095.6|g,1114.3|g)(t) (1971Ap01,1974Ap01) 
J From approximately equal |g branching to the 9/2+ and 11/2+ levels, and from T{-1/2}=11 |ms 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: US
level_comment:
T$From the delayed coincidences between fission fragments and |g's: fission fragment detectors was used to trigger EUROBALL III. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$level is close in energy to previously observed 2124- and 2140-keV levels, both with possible 11/2- J|p assignments (2016En04). 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: H
level_comment:
MOMM1$from static nuclear orientation (1972Kr15) 
J$J=8 from atomic-beam magnetic resonance (1974Ek01). {+128}Sb g.s. |m agrees with theoretical value of 1.3 for configuration=((|p1g{-7/2})(|n1h{-11/2}))8- (1972Kr15). 
T$from weighted average of 9.06 h {I3} (1967Ha27), 8.9 h {I2} (1962Dr01), 9.9 h {I5} (1962Ha16), 8.6 h {I2} (1962Uh01), 9.6 h {I3} (1965Br34), 8.6 h {I6} (1971Ki15), 9.03 h {I9} (1972Pa13). Other: 9.6 h (1967Ha27) 
MOMM1$from |g(|q) in polarized {+128}Sb (1972Kr15) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 5+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E$energy difference between this level and ground state is estimated to be |<20 keV from T{-1/2} systematics for E3 transitions of even Sb isotopes (1975Im01). The fact that no K x ray of {+128}Sb is found in it decay partially supports the above result 
T$weighted average of 10.3 min {I3} (1955Fr11), 10.8 min {I2} (1962De11), 10.1 min {I2} (1962Dr01), 9.9 min {I5} (1962Ha16), 11.0 min {I5} (1962Uh01), 9 min {I1} (1966To02) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 5+
level_lifetime_unit: MIN
level_comment:
E$energy difference between this level and ground state is estimated to be |<20 keV from T{-1/2} systematics for E3 transitions of even Sb isotopes (1975Im01). The fact that no K x ray of {+128}Sb is found in IT decay partially supports the above result. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
$Mass excess=-84564.8 {I25} (2023Ho14) 
E$from difference in measured mass excess of g.s. and isomer 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
J$L(t,|a)=L(d,{+3}He)=4; log| {Ift}=7.78 to 5/2+. 
T$weighted average (LRSW method) of 4.41 h {I1} (1974Fo06), 4.31 h {I3} (1967Ha27), 4.35 h {I5} (1966Ta05), 4.34 h {I7} (1962Uh01). Others: 4.6 h 1 (1953Pa25), 4.2 h (1939Ab02). Uncertainty in LRSW method was increased to 0.024 h in 1974Fo06. Reduced |h{+2}=2.35 
MOMM1$NMR on oriented nuclei (1997St06,1996Li01). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$L(t,|a)=L(d,{+3}He)=2; log| {Ift}=5.86 from (3/2+); shell model predictions; systematics of odd Sb nuclides (1981Sa15). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$L(d,{+3}He)=(0); log| {Ift}=6.8 from (3/2+). Shell-model calculation (1981Sa15) predicts 1/2+ near 1.1 MeV 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E$assigned as isomer by 1987St23. 1982Hu09 also report a 17-min isomer with excitation energy unknown. 
T$from 1982Hu09. Other: 17.1 min (1987St23). 
J$(M4) |g to (11/2+); shell model systematics; possible configuration=|pg{-7/2}~#|nh{-11/2}~#|nd{-3/2} 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$gammas to (9/2+) and (19/2-); no |b feeding from (11/2-); comparison to {+131}Sb and shell-model calculations. 
T$|g(t) in (n,F|g) (2003Ge04,1998GeZX). Other: >2 |ms (1987St23) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J$|g to (15/2-) possibly M1; 296|g between 2568 and 2272 levels disfavors 17/2; no |b feeding from (11/2-) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
T$from coin resolving time (1987St23). 
$1982Hu09 propose a ground-state transition of 1861.2 keV from this level, but in view of implied M4 multipolarity, this transition is unlikely. This |g was not reported in 1987StZO 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$close in energy to previously reported 2031-keV level with tentative J|p=11/2- assignment (2016En04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$possibly corresponds to previously observed 2317-keV level with possible J=11/2 assignment (2016En04). 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from (fragment)(732|g)(t) (2019Bi04), using two-component fit with one component fixed at 0.89 |ms 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$B(E2)|^=0.0248 {I27} from Be(2)(W.u)=6.4 {I7} in 2020Gr01. 
$configuration:2{++}~#|pg{-7/2} multiplet member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_comment:
$B(E2)|^=0.0438 {I27} from Be(2)(W.u)=11.3 {I7} in 2020Gr01. 
$configuration:2{++}~#|pg{-7/2} multiplet member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_comment:
$B(E2)|^=0.0356 {I31} from Be(2)(W.u)=9.2 {I8} in 2020Gr01. 
$configuration:2{++}~#|pg{-7/2} multiplet member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_comment:
J$tentatively assigned based on the energy systematics of the Sb isotopes and from the direct population in the single-step Coulomb excitation in 2020Gr01. 
$B(E2)|^=0.0029 {I3} from Be(2)(W.u)=0.75 {I9} in 2020Gr01. 
$configuration:2{++}~#|pg{-7/2} multiplet member. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: MIN
level_comment:
T$weighted average of 40.0 min {I8} (1974Er07), 40.9 min {I5} (1974Fo06), 40 min {I1} (1971Ki15), 37.2 min {I3} (1967Ha27). Others: 39 min {I3} (1966To02), 35.6 min {I21} (1963Br18), 37 min {I3} (1962Dr01), 33 min {I2} (1962Ha16) 
J$probable shell-model configuration=|pg{-7/2}|nh{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$from 1994WaZU in {+130}Sn |b{+-} decay (1.7 min) <30 from syst (of neighboring odd-odd Sb isotopes). 
J$log| {Ift}=6.6 to 4+; possible first-forbidden transition (log| {Ift}=7.4) to 5-; M1,E2 - M1 cascade from a positive-parity (267) level. 
T$weighted average of 5.7 min {I3} (1974Er07), 6.33 min {I12} (1974Fo06), 6.51 min {I7} (1974Gr29), 6.6 min {I4} (1974Ke08). Others: 1963Br18, 1962Dr01, 1962Ha16 


level_energy_unit: KEV
level_spin_parity: (6,7,8)
level_comment:
J$log| {Ift}=6.2 from (7-). (M1) |g between 733 and 689 levels suggests same parity for both the levels 


level_energy_unit: KEV
level_spin_parity: (4,5)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+130}Sn |b{+-} decay (1.7 min). This level decays by |b{+-} 
T$from adopted levels 
J$4+ (1994WaZU) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MIN
level_comment:
J 3/2,5/2,7/2 from log| {Ift}=6.0 {I2} to 5/2-. (5/2,7/2,9/2,11/2) from log| {Ift}=5.9 {I1} to (7/2+,9/2+). (7/2+) from syst of odd-mass Sb isotopes 
$ |m=2.89 {I1} (1997St06) 
T$from 1967Ha27. Others: 19.4 min {I23} (1966St25) and 25.5 min {I20} (1964Co30) 
$Single-particle state (|p g{-7/2}) (1981ScZL) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J from syst of odd-mass Sb isotopes and odd-even nuclei with N=82 (1977Sc14) 
$Single-particle state (|p d{-5/2}) (1981ScZL) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: US
level_comment:
J from analogy to {+127}Sb and syst of 5- and 7- states in even Sn isotopes (1977Sc14) 
T$weighted average of 88 |ms {I5} (1987Bo19), 95 |ms {I6}(1982Pr01). Others: 80 |ms {I3} (1969Wa29) and 50 |ms {I8} (1977Sc14); 65 |ms {I5} (2000Ge18) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: US
level_comment:
J$from the analogy with {+129}Sb states and decay pattern (2000Ge18) 
$ Configuration=|pg{-7/2}|n(h{-11/2}{+-1}d{-3/2}{+-1}) (2000Ge18) 
T$from 2000Ge18, |gc(t) and c-c(t) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J 13/2-,15/2- proposed by 1988StZQ (no details given). Probably not 15/2- from |b|g coin (evaluators) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_comment:
J$from shell-model calculations; the only E2 transition to 19/2+ 
T$ from 2000Ge18, |gc(t) and c-c(t) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MIN
level_comment:
J,T from the adopted levels 
J$1995St28 suppose 5/2+ 
$Directly populated in 58.4 s 11/2- {+131}Sn |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J from syst of odd-mass Sb isotopes and odd-even nuclei with N=82 (1977Sc14) 
$Directly populated in 56.0 s 3/2+ {+131}Sn |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J M2 |g from (15/2-); |g to (7/2+) 
$Level is presented in fig.3 1995St28, but not connected with any other levels in the scheme 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J E3 |g from (15/2-); |g's to (5/2+) and (7/2+) 
1981Hu09 suggest direct population in 56.0 s |b{+-} decay which seems improbable based on |DJ|p 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: US
level_comment:
J$from analogy to {+127}Sb and syst of 5- and 7- states in even Sn isotopes (1977Sc14) 
T$weighted average of 88 |ms {I5} (1987Bo19), 95 |ms {I6} (1982Pr01). Others: 80 |ms {I3} (1969Wa29) and 50 |ms {I8} (1977Sc14) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: US
level_comment:
J$from the analogy with {+129}Sb states and decay pattern 
Configuration=|pg{-7/2}|n(h{-11/2}{+-1}d{-3/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_comment:
J$from shell-model calculations; the only E2 transition to 19/2+ 
Configuration=|pg{-7/2}|nh{-11/2}{+-2} 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: US
level_comment:
T$from (fragment)(450|g)(t) (2019Bi04), using a three-component fit of the decay curve, with two components fixed at 0.97 |ms and 4.3 |ms 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$from generalized centroid difference method applied to 450-1226|g feeding-decay cascade (2023Bo01) 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: MIN
level_comment:
J$M1+E2 |g from (3)+. Configuration=|pg{-7/2}~#|nd{-3/2}{+-1}. J|p=3+ is not completely ruled out 
T$ weighted average of 2.70 min {I15} (1972Na10), 2.80 min {I10} (1974Ke08), 2.80 min {I7} (1975Ba36), 2.79 min {I10} (1975NuZX). Other: 2.1 min {I3} (1973Er18). Others: 1974Fo06, 1974Gr29, 1973Mc09, 1973Ke25, 1972Ke20, 1966St25, 1956Pa20 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$x=150-250 keV (1989St06). Other: 200 {I30} (2017Au03) 
T$from 1975Ba36. Others: 4.2 min {I1} (1974Ke08) and 4.1 min {I4} (1973Er18,1970ErZZ). Others: 1974Fo06, 1974Gr29, 1972Na10, 1966St25, 1956Pa20 
J$ configuration=|pg{-7/2}~#|nh{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: NS
level_comment:
J$4- is possible but less likely 
T$from |g|g(t) (1974ClZX) in the study of isomers in fission products, value is listed in {+132}Sn |b{+-} decay dataset. Other: 150 ns {I70} (1989St06, |g|g(t) in {+132}Sn |b{+-} decay) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: PS
level_comment:
J$M1+E2 |g from 1+; |g to (4+). J=1 if J({+132}Sb g.s.)=3. Possible member of configuration=|pd{-5/2}~#|nd{-3/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: NS
level_comment:
J$4- is possible but less likely 
T$ from study of isomers in fission products (1974ClZX). Other: 150 ns {I70} (1989St06) 
$It is possible that this level also feeds the 4.10-min, (8-) isomer 


level_energy_unit: KEV
level_spin_parity: (4-)
level_uncertain: ?
level_comment:
E$ reverse ordering of 94-135 cascade is also possible giving a level at 348.4, instead of that at 389.2 
J$3- is possible but less likely 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MIN
level_comment:
J$from |m; systematics of 7/2+ level in neighboring Sb isotopes 
CONF$Probable |p(g{-7/2}{++1}) configuration 
T$from 1984Br31. Others: 2.67 min {I33} (1966St25), 2.3 min {I2} (1973Er18), 2.7 min {I1} (1974Fo06). 
MOMM1$from 1997St06 using the NMR/ON method 
CONF$(|p1g{-7/2}){++1} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$from 962.1|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p(g.s.)=(7/2-)); systematics of 5/2+ level in neighboring Sb isotopes 
CONF$Probable |p(d{-5/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$from 1477.1|g to (5/2+), 2439.5|g to (7/2+); systematics of 3/2+ level in neighboring Sb isotopes 
CONF$Probable |p(d{-3/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: PS
level_comment:
J$from systematics of 11/2- level in neighboring Sb isotopes 
T$from |b|g|g(t) in 1999Sa31 
CONF$Probable |p(h{-11/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J$from 4191.6|g to 7/2+, 272.8|g from (15/2+); non-population in {+133}Sn |b{+-} decay (J|p=7/2-) 
CONF$possible member of the |pg{-7/2}~#|n(f{-7/2}h{-11/2}{+-1}) multiplet (2009Ur01) 


level_energy_unit: KEV
level_spin_parity: (9/2,11/2,13/2)
level_comment:
J$from 1502.6|g to (11/2-) 
CONF$Probably member of |pg{-7/2}~#3{+-} or |pg{-7/2}~#4{++} multiplet (1999Sa31). 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: US
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from direct mass measurements (2010Su11, 2010Su18). 4525+X keV with x|< 20 keV in 2009Ur01. Fed with about 7% of the fission yield of {+133}Sb (1978Si05) 
T$weighted average from 16.6 {I3} (162.3|g(t)) and 16.3 {I3} (1510.1|g(t)) (2009Ur01), 16.7 {I4} (1510.1|g(t)) and 17.6 {I11} (162.3|g(t)) (2000Ge08). Others: 17 |ms {I2} and 15 |ms {I2} using 162.3|g(t) in JOSEF and LOHENGRIN experiments, respectively (1978Si05). 
CONF$possible member of the |pg{-7/2}~#|n(f{-7/2}h{-11/2}{+-1}) multiplet (2009Ur01) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)
level_comment:
J$from 3940.1|g to (5/2+), 4902.2|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)
level_comment:
J$from 4039.5|g to (5/2+), 5001.5|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_comment:
J$from 2685.0|g to (3/2+), and 5124.7|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)
level_comment:
J$from 4228.5|g to (5/2+), 5191.4|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)
level_comment:
J$from 4314.1|g to (5/2+), 5276.6|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)
level_comment:
J$from 4531.0|g to (5/2+), 5493.8|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)
level_comment:
J$from 4597.9|g to (5/2+), 5559.7|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_comment:
J$from 5645.3|g to (7/2+), 3205.4|g to (3/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)
level_comment:
J$from 3089.8|g to (11/2-), and 5881.4|g to (7/2+); direct population in {+133}Sn |b{+-} decay (J|p=7/2-) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: US
level_lifetime_info: ;ERR=?;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from adopted levels 
T$from 2000Ur05, but no information on gating transitions is given 
CONF$Probable |pg{-7/2}|nf{-7/2}h{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: US
level_comment:
$Fed with about 7% of the fission yield of {+133}Sb (1978Si05) 
E$ From adopted levels. x |< 20 keV in 2009Ur01 
T$from |g(t) (2009Ur01). Other: 17 |ms {I2} and 15 |ms {I2} using 162|g(t) in JOSEF and LOHENGRIN experiments, respectively (1978Si05). 
CONF$member of the |pg{-7/2}~#|n(f{-7/2}h{-11/2}{+-1}) multiplet 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2)
level_uncertain: ?
level_comment:
E$Introduced from a questionable 152-keV transition depopulating the 4301.5-keV level; |g-rays depopulating this level were not observed 


level_energy_unit: KEV
level_spin_parity: (21/2)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from adopted levels. The measured X-ray intensities, corrected for the fluorescence yield, suggest that there is no room for an unobserved transition higher than 30 keV (2000Ge08). 
T$weighted average of 16.7 |ms {I4} (1510.5|g(t)) and 17.6 |ms {I11} (162.5|g(t)) in 2000Ge08 
CONF$possible |pg{-7/2}|n(f{-7/2}h{-11/2}{+-1}) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 21/2+
level_lifetime_unit: US
level_comment:
E$x|<30 keV. In {+133}Sb Adopted Levels in the ENSDF database (Oct 2010 update), value is listed as 4560 {I100}, taken from mass measurement by 2010Su11 (Phys Lett B688, 294) 
T$2016Bo19 quote value from 2009Ur01 (Phys. Rev. C79, 037304) 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: S
level_comment:
J$Member of (|p g{-7/2})(|n f{-7/2}) multiplet, feeds mainly 0+ in {+134}Te daughter with log| {Ift}|?5.2, whereas (2+) states are fed with log| {If{+1u}t}|?9 
T weighted average of 0.85 s {I10} (1972Ke21) and 0.75 s {I7} (1990Fo03) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From {+135}Sn |b{+-}n decay (2005Sh23). 
$%|b{+-}n from 1993Ru01. Others: 0.120% {I8} (1980Lu04), 0.084% {I20} (1977Ru04), 0.055% {I13} (1968To19) 
E$can be estimated at |?250-550 keV from Shell Model calculations (2002Ko53) 
T$from 1993Ru01. Others: 11.1 s {I8} (1968De18), 11.3 s {I3} (1968To19), 10.3 s {I5} (1972Ke21), 10.2 s {I3} (1974Gr29), 10.3 s {I4} (1976Lu02), 10.43 s {I14} (1977Ru04), 10.5 s {I3} (1982He06) 
J$Member of (|p g{-7/2})(|n f{-7/2}) multiplet, the (7-) assignment is made based on Shell Model calculations 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
$The 171|g depopulating this level has been seen only in {+248}Cm SF decay, however, its placement in the level scheme is done by 2002Ko53 based on coincidence between 171.3|g and 52.8|g, 317.7|g 


level_energy_unit: KEV
level_spin_parity: (2-)
level_uncertain: ?
level_comment:
J$ 2- assignment consistent with probable M1 |g decay to 331 and 383 levels; log| {Ift} value for the decay and weak population to the 3- state at 384 in both |b- and |g decays. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$Based on strong neutron peak in {+134}Sn |b{+-}n decay this level is presumed to be fed by an allowed transition in {+134}Sn |b decay (1990Fo03) 
$Proposed configuration=((|p h{-11/2})+(|n h{-9/2})) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$ Population of high-spin isomer deduced by 2005Sh23 from |?10% of total |b decay strength observed in intensity of the 318|g and the observation of 115, 297 and 1297 transitions known from its |b-decay into {+134}Te. 
T$ from {+134}Sb in ADOPTED LEVELS. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$114|g from (4-), 162|g to (7-). 
T$ Possible long half-life expected for level based on likely noncollective E2 nature for 162|g. Time-to-amplitude spectrum gated on |b start pulses and 162 stop pulses did not permit lifetime observation due to time resolution and low transition intensity. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$From {+135}Sn |b{+-}n decay (2005Sh23). 
T$From Adopted Levels 
$Configuration=((|p g{-7/2})+(|n f{-7/2})) 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: S
level_comment:
T$from |b(t) (2018Si28). |b decay rate was fit including g.s. and isomeric decay of {+134}Sb as well as the daughter {+134}Te and the time structure of the bunched beam. 2018Si28 report 0.6744 s {I34} (stat) {I19} (syst), compiler added uncertainties in quadrature. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: S
level_comment:
T$weighted average of 9.86 s {I6} (stat) {I4} (syst) from 297|g(t), 9.82 s {I9} (stat) {I16} (syst) from 706|g(t), and 9.92 s {I7} (stat) {I7} (syst) from 1279|g(t) (2018Si28). 2018Si28 report a final value of 9.87 s {I4} (stat) {I7} (syst); compiler has combined uncertainties in quadrature. 
E$From the Adopted Levels of {+134}Sb in the ENSDF database (March 2011 update). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+134}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=780 ms {I60} from Jan 2011 ENSDF update of {+134}Sb. 2018Si28 (Phys. Rev. C 98, 054307) measured T{-1/2}=674.4 ms {I39}, where a 9.87-s isomer was also reported. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_comment:
MOMM1,MOME2,J$from hyperfine structure measurement with |m({+123}Sb)= 2.5457 |m{-N} {I12} and Q({+123}Sb)=-0.692 b {I14} as references. 
MOME2$uncertainty deduced by quadratic addition of statistical uncertainty of 0.008 and systematic uncertainty of 0.017. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
T$weighted average of 1.696 s {I21} (1968To19,1968To18), 1.706 s {I14} (1977Ru04), 1.662 s {I10} (1993Ru01). Others: 1.82 s {I4} (1976Lu02 superseded by 1993Ru01), 2.0 s {I2} (1966To02, superseded by 1968To19), 1964Be06, 1967De01, 1973Bo42, 1978Cr03. 
$%|b{+-}n is adopted from 2002Sh08 (same value in 2002Pf04 evaluation) based on the least-squares fit of their |b-delayed neutron curves. Use of %|b{+-}n=17.6 {I22} recommended by 1993Ru01 (from weighted average of 21.0 {I11} (1993Ru01), 14 {I1} (1978Cr03), 22 {I4} (revision by 1993Ru01 of 19.9 {I21} in 1977Ru04), 25 {I4} (revision by 1993Ru01 of 8 in 1968To19)) gave a very poor fit (by a factor of 10 or so) to the decay curve obtained by 2002Sh08 (according to an e-mail reply of April 30, 2002 by the lead author of 2002Sh08). If one excludes the low value of 14 {I1} in 1978Cr03, the weighted average of other three values quoted by 1993Ru01 is 21.3 {I11}, which is consistent with that obtained by 2002Sh08 and the value adopted by 2002Pf04. Measurements: 1966To02, 1968To19, 1968To18, 1974Sh18, 1974Fr09, 1976Lu02, 1976Kr18, 1977Ru04, 1978Cr03, 1979Kr03, 1980Lu04, 1981Ho07, 1993Ru01. See 2002Pf04, 1993Ru01, 1989BrZI, 1984Ma39, 1982Ru01, 1977Ru10, 1975Iz03 for analysis, reviews and compilations 
$B-N: THEORY: 1981Al25, 1979Pr03, 1978Pe18, 1978Gj02, 1978Gj01, 1977Sh10, 1976Kl08, 1972Pa11 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_comment:
J$shell-model calculations (2005Sh36) predict first 1/2+ at 527 keV 
T$ preliminary value from |b|g|g(t); advanced time-delay method (2007Ma40) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_comment:
J$proposed configuration=|pg{-7/2}~#|n(f{-7/2}h{-9/2}) based on shell-model calculations by 1998Bh09 


level_energy_unit: KEV
level_spin_parity: (21/2,23/2)
level_comment:
J$23/2- suggested from proposed configuration= |ph{-11/2}~#|nf{-7/2}{+2}(6+). However, a 21/2+ state is also predicted (see Figure 3 in 2015Ko05) in shell-model calculations 


level_energy_unit: KEV
level_spin_parity: (21/2,23/2)
level_comment:
J$23/2- suggested from proposed configuration= |ph{-11/2}~#|nf{-7/2}{+2}{-6+}. However, a 21/2+ state is also predicted (see Figure 3 in 2015Ko05) in shell-model calculations 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+135}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=1679 ms {I15} from Dec 2016 ENSDF update of {+135}Sb. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay $ Measured %|b{+-}n=14.6 {I4}(stat) {I12}(syst) from |n{-|bR}) events, and 8.1% {I35} from |n{-|bR}) and |n{-|b} events. 2020Wa04 recommend the former value, where the statistical and systematic uncertainties are added in quadrature. Comparison with five previous measurements of %|b{+-}n values in literature from 1968 to 1993, and evaluations in 1993 (1993Ru01) and 2002 (2002Pf04). Other: %|b{+-}n=20.0 {I29} in 2020Li32 evaluation (Nucl. Data Sheets 168, 1 (2020), which includes the value from 2020Wa04. Note that measured values of %|b{+-}n=24.5 {I10} in 2017AgZZ (Proc. Intern. Conf. Nuclear Data for Science and Technology, ND201) and 21.0 {I11} in 1993Ru01 (At. Data Nucl. Data Tables 53, 1), and the value from 2020Wa04 are in sharp disagreement. 
J$from {+135}Sb Adopted Levels in the ENSDF database (Dec 2016 update) 
T$from 2020Li32 (Nucl. Data Sheets 168, 1) evaluation 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
T$from 1993Ru01. Others: 0.9 s {I1} (1978Cr03), 0.75 s {I20} (1977Ru04), and 0.82 s {I2} (1976Lu02). 
J$a negative parity is expected since with only 1 proton and 3 neutrons away from closed shell, the configuration of {+136}Sb should be |pg{-7/2}|nf{-7/2}{+3}. Assuming a negative parity, the log| {Ift} values of 5.8 and 6.6 to the 0+ and 2+ states of {+136}Te (1997Ho15), respectively, indicate J|p=1-. This assignment is additionally supported following a comparison with {+212}Bi, where the 1- state of the |ph{-9/2}|ng{-9/2}{+3} multiplet is the g.s. 
%B-N$weighted average of 19.2 {I18} (2015CaZM) and 16.3 {I32} (1993Ru01). Others: 32 {I14} (1977Ru04) and 19 {I9} (1978Cr03). These have been adjusted to 44 {I57} and 33 {I40} in 1993Ru01 based on a reassessment of fission yield data. 
%B-2N$preliminary report in 2017CaZZ states observation of |b{+-}2n branch with an upper limit of 1%. 2005Ga61 give a limit of %|b{+-}2n<2.8 {I2}%, with the upper limit corresponding to the case where all the observed two-neutron activity in their experiment originates from {+136}Sb. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: NS
level_comment:
T$weighted average of 540 ns {I30} from implant-|g(t) using 173|g in {+9}Be({+238}U,F|g) and 480 ns {I100} from sum of implant-|g(t) using 173|g and implant-K|a x-ray(t) in {+241}Pu(n,F|g). 
J$E2 53.4|g to (4-) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: NS
level_comment:
T$weighted average of 489 ns {I40} from implant-|g(t) for H-like atom (2015Lo08), 570 ns {I40} from implant-|g(t) (2012Ka36) and 570 ns {I50} from implant-|g(t) (2001Mi22). All measurements used the 173|g. Uncertainty in 2012Ka36 increased from 5 ns to 40 ns, since the former includes only statistical and not systematic uncertainties, per email communication with first author of 2015Lo08 on Sept. 3, 2015 
$configuration=|pg{+1}{-7/2}~#|nf{+3}{-7/2} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
$%|b{+-}n and %|b{+-}2n are beta-delayed one-neutron emission or P{-1n}, and beta-delayed two-neutron emission or P{-2n} deduced by 2018Ca22 from measurement of |b, neutron and (|b)n-time correlated events. Previous experimental %|b{+-}n values: 19.5 {I18} (2015CaZM: Ph.D. thesis, University of Chicago (2015)); 16.3 {I32} (1993Ru01: At. Data Nucl. Data Tables 53, 1); 33 {I+40-33} (1978Cr03: Z. Phys. A287, 45); 44 {I+56-44} (1977Ru04: J. Inorg. Nucl. Chem. 39, 753). Compilations and evaluations give: 23.2 {I68} (2002Pf04: Prog. Nucl. Energy 41, 39); 18.7 {I18} (J. Liang et al., unpublished, 2018). Previous experimental %|b{+-}2n value: 1.4 {I2} (D. Testov et al., Esp-rus congress (2011), reference 17 in 2018Ca22). 
J,T$from {+136}Sb Adopted Levels in the ENSDF database (April 2018 update) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+136}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=923 ms {I14} from 1993Ru01 (At. Data Nuc. Data Tables 53, 1), same value adopted in April 2018 ENSDF update of {+136}Sb. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay $ Measured %|b{+-}n=17.6 {I10}(stat) {I27}(syst) from |n{-|bR}) and |n{-|b} events, where the statistical and systematic uncertainties are added in quadrature. Comparison with four previous measurements of %|b{+-}n values in literature from 1977 to 2018, and evaluations in 1993 (1993Ru01) and 2002 (2002Pf04). Other: %|b{+-}n=24.93 {I73} in 2020Li32 evaluation (Nucl. Data Sheets 168, 1 (2020), which includes the value from 2020Wa04. Note that recently measured %|b{+-}n=32.2 {I15} in 2018Ca22 (Phys. Rev. C 98, 034310) and 2020Wa04 are in disagreement, although measured value of 16.3 {I32} in 1993Ru01 (At. Data Nucl Data Tables 53, 1) is in agreement with that from 2020Wa04 
J,T$from {+136}Sb Adopted Levels in the ENSDF database (April 2018 update) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MS
level_comment:
$t,|b{+-}n: extrapolated values based on properties of {+133}Sb and {+135}Sb (2002Sh08) 
J$from sys (2003Au02) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+137}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=492 ms {I25} from 2011Ar18 (Phys. Rev. C 84, 061307(R)) 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MS
level_comment:
J$from Adopted Levels of {+137}Sb in ENSDF database 
T$from |b|g(t) of 606|g, 608|g, 633|g and 974|g in the decay of {+137}Sb (2021Mo10) 
%B-N,%B-2N$from %|b{+-}n|>22.9 {I36}, %|b{+-}2n|>3.7 {I10} (2021Mo10) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=37.3, %|b{+-}2n=30.5 (2003Mo09) 
J$(3-) tentatively proposed by 2015Le14 based on strong feedings to (2+) and (4+) states in {+138}Te 
T$weighted average of 346 ms {I19} from |b|g(t) in 2015Le14, and 350 ms {I15} measured by 2011Ar18 from decay curve for delayed neutrons. Other 296 ms {I35} from a preliminary analysis of decay curve in 2006KeZZ. Theoretical value: 597 ms (2003Mo09) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+138}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=348 ms {I15} from Sep 2017 ENSDF update of {+138}Sb 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: MS
level_comment:
J$from Adopted Levels of {+138}Sb in ENSDF database 
T$from |b|g(t) of 461|g+442|g (2021Mo10) 
%B-N,%B-2N$from %|b{+-}n|>29.0 {I37}, %|b{+-}2n|>0.74 {I35} (2021Mo10) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=503 ms, %|b{+-}n=76.9, %|b{+-}2n=9.96, %|b{+-}3n=0.02 (2003Mo09) 
$Theoretical T{-1/2}=52.7 ms, %|b{+-}n=44.7, %|b{+-}2n=0.2, %|b{+-}3n=0.1 (2016Ma12) 
E$observed activity of 93 ms is assumed to belong to the g.s. 
J$7/2+ proposed in calculations (2007Ji14) and in systematics (2012Au07); 1/2+ (theoretical prediction,1997Mo25) 
T$measured by 2011Ar18 from decay curve for delayed neutrons and five-component fit to the decay curve, which included daughters 1.4-s {+138}Te and 1.6-s {+139}Te; and grand-daughters, 6.3-s {+138}I and 2.28-s {+139}I. In Table I, 2011Ar18 quote half-life with somewhat different uncertainty: 93 ms {I+14-3} 
$1994Be24 assigned 8 counts to {+139}Sb activity with an estimated |s=3 |mb 
$Measured yield of the low-energy fission component=0.0002 {I2} (1998Do08) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+139}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=93 ms {I+14-3} from 2011Ar18: Phys. Rev. C 84, 061307; same value adopted in Oct 2016 ENSDF update of {+139}Sb, but with an uncertainty of 13 ms. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n and %|b{+-}2n are lower limits deduced by the authors from only the |g-ray data without accounting for any direct feedings to the ground states of {+139}Te and {+138}Te. Value of %|b{+-}2n is deduced more precisely (by B. Singh) from summed intensities of 442.8 and 460.8 gamma rays (Table I). 2017Mo12 quote |?8%. The normalization procedure is not clearly stated in 2017Mo12. 
$For comparison, see the following calculated values: %|b{+-}n=42.5, %|b{+-}2n=16.4 (1997Mo25); %|b{+-}n=58.6 or 100 (2002Pf04); %|b{+-}n=62 (2011Ar18, deformed), 78 (2011Ar18, spherical) 
J$assigned by 2017Mo12 based on possible |b feedings to the (2+) and (4+) states in {+140}Te, but (4-) is not ruled out. 
T$measured by 2017Mo12 from decay curve for combined 271-, 423-, and 425-keV gamma rays, fitted by a single exponential decay with a constant background level, and using maximum likelihood method. Other value: > 407 ns (2010Oh02, from time-of-flight - from T. Kubo e-mail reply of July 14, 2010). Actual half-life is much longer as suggested previously by the calculated values of 37.8 ms (1997Mo25); 38 ms or 645 ms (2002Pf04); 37 ms (2011Ar18, deformed), 364 ms (2011Ar18, spherical) 
$ Measured |s=4.30 nb (2010Oh02), systematic uncertainty|?30% (probability of misidentification of {+140}Sb isotope<0.001% (2010Oh02) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (6-,7-)
level_lifetime_unit: US
level_comment:
$Possible configuration=|pg{-7/2}{+1}~#|nf{-7/2}{+-1} (2016Lo01) 
E$x<30 keV (2016Lo01) 
T$from 70.9|g(t) and 227.3|g(t) (2016Lo01) 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_lifetime_unit: MS
level_comment:
J$adopted values, from |b feedings to (2+) and (4+) of {+140}Te daughter; (4-) not excluded (2017Mo12) 
T$adopted values, from 2017Mo12 (|g(t)) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (6-,7-)
level_lifetime_unit: US
level_comment:
$Possible configuration=|pg{-7/2}{+1}~#|nf{-7/2}{+-1} 
E$x<30 keV (2016Lo01) 
T$from 70.9|g(t) and 227.3|g(t) (2016Lo01) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+140}Sb g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Nov 2018 update of ENSDF for {+140}Sb adopted T{-1/2}=173 ms {I12} from 2017Mo12: Phys. Rev. C 95, 044322; a value derived from the same experiment as in 2020Wu04 (see caption for Table I in 2020Wu04) 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$There is no measurement of any decay mode, but %|b{+-}=100 is assigned by inference as this is the only decay mode allowed, followed by possible delayed neutron emissions. 
$Theoretical %|b{+-}n=44.6, %|b{+-}2n=0.93 %|b{+-}3n=0.012 (2021Mi17, see ref. [62] Supplemental Material) 
$Theoretical %|b{+-}n=95, %|b{+-}2n=2 (2019Mo01) 
$Theoretical %|b{+-}n=45.0, %|b{+-}2n=0.4, %|b{+-}3n=0.1 (2016Ma12) 
$Theoretical %|b{+-}n=92.7, %|b{+-}2n=3.3, %|b{+-}3n=0.76 (2003Mo09, see ref. [42] Supplemental Material) 
$A total of 730 counts were assigned to {+141}Sb, 456 events with spectrometer setting on Sn, and 274 events with setting on Te, with probability of misidentification of this isotope is <0.01% for both settings (2018Sh11). 
$Production |s=22.3 pb for Sn setting, and 28.7 pb for Te setting, with 30% systematic uncertainty on both |s values (2018Sh11). 
E$it is assumed that the observed events correspond to ground-state activity. 
J$7/2+ from systematics (2017Au03); 1/2+ proton orbital proposed in theoretical calculations of 1997Mo25 
T$From 2020Wu04 fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. Data analysis included contributions from the parent, daughter and grand-daughter decays, as well as a constant background. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay, thus 100 |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=42.8 ms, %|b{+-}n=80, %|b{+-}2n=14 (2019Mo01) 
$Theoretical T{-1/2}=23.4 ms, %|b{+-}n=41.9, %|b{+-}2n=2.7 (2016Ma12) 
$In 2018Sh11, a total of 13 counts were assigned to {+142}Sb, eight events with the spectrometer setting on Sn, and five events with setting on Te. Probability of misidentification of this isotope is 0.01% for both the settings (2018Sh11) 
$Production |s=0.2 pb for Sn setting, and 0.3 pb for Te setting, with 30% systematic uncertainty for both the |s values (2018Sh11) 
E$the observed activity is assumed to correspond to {+142}Sb g.s. 
J$2- or 3- from |W{-|p}=1/2+, |W{-|n}=5/2- orbitals proposed in 2019Mo01 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
$%|a decay assumed as 100% in 2018Au04. From theoretical |b-decay half-life of 378.2 ms and |a-decay half-life of 1.4 ps (2019Mo01), |e+|b{++} decay is expected to be negligible. However, 2p decay mode is possible from theoretical S(2p)({+104}Te)=-2130 keV (2019Mo01) 
$2018Au04 reported observation of two recoil-|a correlated events, which were assigned to {+108}Xe |) {+104}Te |) {+100}Sn |a-decay chain, and on this basis half-lives of decays of {+108}Xe and {+104}Te were deduced. 2019Xi06 also reported observation of two recoil-|a correlated events, but with inconclusive assignment to {+108}Xe |) {+104}Te |) {+100}Sn |a-decay chain, as according to the authors the two events could also be due to |b-delayed proton emission from more abundant radioactive isotopes. 
T$from analysis of second derivative of DSSD traces of the two events, corresponding to {+108}Xe - {+104}Te pileup events (2018Au04). Other: T{-1/2}<4 ns (2019Xi06, analysis of the second derivative of either trace of the two events, but no pileup was observed) 
$E|a=4880 keV {I160}, weighted average of measured E|a=4.73 MeV {I24} for the first event, and 5.06 MeV {I25} for the second event in 2018Au04; and 4872 keV {I160} in 2019Xi06. 


level_energy_unit: KEV
level_spin_parity: [5/2+]
level_lifetime_unit: US
level_comment:
T$from |a(t) in 2006Li41; Others: 0.70 |ms {I+25-17} from |a(t) using maximum likelihood method in 2006Se08 
J$assumed |DL=1 |a transition from the [7/2+] {+109}Xe g.s. 
CONF$|nd{-5/2} state 


level_energy_unit: KEV
level_energy_info: ;ERR=GE
level_spin_parity: 0+
level_lifetime_unit: US
level_comment:
%|e+%|b{++}|?0.0008 from the gross |b-decay strength function calculations of 1973Ta30 
T$Weighted average of 60 |ms {I+40-20} (1994Pa11) and 60 |ms {I+30-10} (1981Sc17). Technique used: delayed |a|g coincidences 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%A$from 1979Sc22. Based on gross |b{+-} decay theory of 1973Ta30, one expects %|e+%|b{++}|?0.5. An energy of 3862 {I10} for the decay of {+107}Te (1991He21) 
Populated by 0.9-s {+111}Xe |a decay 
T$from 1994Pa11. Other: 3.6 ms {I+6-4} from time-correlated dependence of I|a({+111}Xe)/I|a({+107}Te) (1979Sc22) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$ %|e+%|b{++}=0.29 {I3} (estimated by 2012Ca03, based on systematics of |b-decay half-lives of odd-A Te nuclei. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from implant-(|a decay) time correlation (2019Au02) 
$|a-decay Q(|b{+-})value=4007 {I10} (2019Au02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1979Sc22 (3288|a decay curve). Others: 2.0 s 3 (1995Sc28) { 2.0 s {i2}} (1973Bo15), 3 s {i1} (1977Ki11), 2.1 s {i2} (1978Ro19) 
$%|a=68 {i12} from I|a({+108}Te)/(I|a({+112}Xe) (1978Ro19) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ from recoil-decay tagging and RDDS method (2011Ba37); mean lifetime |t=11.0 ps {I13} (2011Ba37) 
$ B(E2) deduced by 2011Ba37 from measured lifetime of the 625, 2+ state 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
%A$from 1981Sc17; other: 4 {I3} from 1979Sc22. %|b{++}p is from %|a=3.9 {I13} and I(|b{++}p)/I(|a)=2.40 {I4} in 1985Ti02. %|b{++}|a is from 1985Ti02 
J$systematics of neighboring odd-N Te isotopes; favored |a decay to J|p=(5/2+), {+105}Sn g.s; shell model predicts predominant |nd{-5/2} character 
T$weighted average of 5.3 s 4 (using 3080-keV|a(t) in 1965Ma12 and |b{++}p(t) in 1965Si04. Note, that in the original publications those values were assigned to {+108}Te, but the reported T{-1/2} and E|a are consistent with the adopted properties of {+109}Te), 4.2 s 2 (using (|b{++}p(t)) in 1967Ka01), 4.9 s 4 (unweighted average of 5.3 s 7 (3080-keV|a(t)) and 4.5 s 3 (|b{++}p(t)) in 1977Bo15), 4.1 s 2 (recommended in 1977Ki11 from 4.3 s 3 (3080-keV|a(t)) and 4.03 s 15 (|b{++}p(t))) and 4.6 s 3 from (|e+|b{++})|g(t) in 2002Re28 
CONF$|nd{-5/2}{+1} 
$E|a=3080 {I15} keV (1978Ro19), 3040 keV 30 (1977Ki11) and 3080 keV 30 (1965Ma12) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$2.0|*10{+-3}<%|a<2.0|*10{+-6} (2000De11); %|a|?7.6|*10{+-4} estimated from |a transmission calculations (1981Sc17) 
T$Weighted average of 18.4 s {I8} (using K{-|a}X(t)) and 21 s {I3} (using 219.1|g(t) and 605.9|g(t)) in 1977Ki11 


level_energy_unit: KEV
level_spin_parity: 16(+)
level_comment:
J$1035.5|g E1 to 15-; band member. Authors state that a definitive |p assignment could not be made due to the insensitivity of linear polarization measurements 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (25+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From configuration assignments based on theoretical calculations 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (27-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From configuration assignments based on theoretical calculations and from the observed decay-out intensity below 1533|g transition. However, no discrete transitions were observed carrying this intensity 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: (30-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From configuration assignments based on theoretical calculations and from the observed decay-out intensity below 1654|g transition. However, no discrete transitions were observed to link this band to low-spin level scheme 


level_energy_unit: KEV
level_energy_info: ;OFF=V
level_spin_parity: (29+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From configuration assignments based on theoretical calculations. This band strongly feeds the positive parity band starts at 4655.7 keV through bands at 8344.8 keV (J|p=(20+)) and 6949.8 KeV (J|p=16+). However, no discrete transitions were observed to link these bands 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: (30-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From configuration assignments based on theoretical calculations and from the observed decay-out intensity below 1654|g transition. However, no discrete transitions were observed to link this band to low-spin level scheme 


level_energy_unit: KEV
level_energy_info: ;OFF=V
level_spin_parity: (29+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$From configuration assignments based on theoretical calculations. This band strongly feeds the positive parity band starting at 4655.7 keV through bands at 8344.8 keV (J|p=(20+)) and 6949.8 KeV (J|p=16+). However, no discrete transitions were observed to link these bands 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: S
level_comment:
T$weighted av: 19.0 s {I7} (1967Ka01), 19.5 s {I5} (1967Bo41). Others: 1967Ma44, 1967Bo43 
J$M1,E2 from (7/2)+, 5/2+ proposed by 1967Bo41; 7/2+ for N=59 {+109}Sn g.s. (atomic beam) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
T$723|g(t) (2000St03) 
J$|nh11/2 isomer, syst of isomers T{-1/2}, M2 transition and excit energy (2000St03) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$794.6|g to 2+; direct feeding from the beta-delayed proton decay of {+113}Xe (J|p=(5/2+)) in 2005Ja10, 1985Ti02 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (21+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$tentative assignment based on the observed feeding to the 20+ yrast states and band interpretation 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (21-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$tentative assignment, based on the observed feeding to the (20+) yrast state and band interpretation 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MIN
level_comment:
J$7/2+ probable from log| {Ift}|?5.7 to 5/2+ level and log| {Ift}|?5.9 to (9/2+) level 
T$av of 2.0 min {I2} (1974Ch17), 1.4 min {I2} (1975BuYW), 1.6 min {I2} (1976Wi11). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MIN
level_comment:
T av: 5.7 min {I2} (1976Wi11), 5.76 min {I9} (1976CoYV), 6.0 min {I2} (1974Ch51,1965Re01), 6.0 min {I1} (1972Sh37). Other: 6.0 min {I5} (1960Se04) 
J$log| {Ift}|?6.7 to 5/2+; log| {Ift}|?5.1 to 9/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=LT;ERR=?
level_spin_parity: (1/2)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
%IT$for B(M3)(W.u.)|?0.028 (see {+113}Sn), %IT|<0.06 for E|g=2.2 increasing to |<2.5 for E|g=18 
T$from 1976Wi11, 770|g decay curve. Other: 7.5 min {I3} (1974Ch51) 
E M3 isomeric transition not observed in ce spectra; E|g(M3)<20 keV inferred by 1974Ch51 
J$log| {Ift}|?5.4 to 1/2+ 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
MOMM1 Other: -1.02 {I4} (1989Ra17) 
For near-constant |m values of 11/2- isomers in heavier odd-mass telluriums, see 1989Ra17 
MOME2$estimated 
T$7.5 |ms {I2} (1972Va38) 280|g(t) pulsed beam. Others: 6.3 |ms {I3} (1972Br38), 10 |ms (1974MiZW) 
J$M2 deexcitation to 7/2+ g.s.; B(M2)(W.u.) syst; h11/2 isomerism in {+117}Te,{+119}Te occurs at |?300 keV 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MIN
level_comment:
J the {+115}Te g.s. is assigned 7/2+ as for {+113}Te g.s. rather than 1/2+ as for {+117}Te,{+119}Te,{+121}Te g.s. (1974Ch51,1975WiZX) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
T 280|g(t) pulsed beam: 7.5 |ms {I2} (1972Va38), 6.3 |ms {I3} (1972Br38); other: 10 |ms (1974MiZW) 
g factor: -0.186 {I7} (1972Va38), -0.174 {I40} (1974MiZW) |g(|q,H,t) 
|n h11/2 state; see {+117}Te,{+119}Te,{+121}Te for band structures up to J=23/2- (1983VaZW) 
MOME2$ratio of absolute values of electric quadrupole moments: Q(7/2+,{+121}Te)/Q(11/2-,{+115}Te)=1.1 {I2}, Q(11/2-,{+115}Te)=0.8 estimated (1982Io01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$weighted average of 2.50 h {I2} (1961Fi05), 2.33 h {I8} (1968Ra14). Other measurements: 1953Dr33, 1958Ku79, 1973Ka45 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MIN
level_comment:
J$from atomic beam (1976Fu06), log| {Ift}<5.9 to |p=+ 
T$weighted av.: 60 min {i6} (1973Ka45), 68 min {i5}, 62 min {i3} (1967Be46), 65 min {i5} (1962Kh05,1961Va30), 61 min {i2} (1961Fi05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
MOMM1$DPAD. Other: -0.75 {i5} (1981Ka10), |m and T{-1/2} compatible with 5/2 [402] state. 
J$E2 |g to 1/2+ g.s., d5/2 state. 
T$from 1981Ka10, 1979Ha18 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$1999Mo30 have derived the energy of the 11/2- state. They observe several linking |g between the 25/2+ state at 3315.3 Kev feeding the 23/2- state of the 11/2- band and levels of the band 3 built on the known 7/2+ at 295.8 
T$from 1969Br02 (103 ms {i3}), 1963De37 (104 ms {i15}) 
J$shell model and syst 


level_energy_unit: KEV
level_comment:
E$based on deexciting transition to 274 level. This transition could feed 296 level instead, in which case E(level) would be larger by { 21.6 keV}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from 1963De37 (104 ms {I5}), 1969Br02 (103 ms {I3}), the |g transition unobserved would be M2. 
E$from 1999Mo30 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
%|e|a<2|*10{+-6} (1961Fi05, 1963Ka17) 
T from 1961Fi05. Others: 6.0 d (1948Li02), 6.0 d (1952Dr27), 6.1 d {I1} (1960So02), 6.0 d {I2} (1965An05) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J strong |g to 6+; |g-|g cascade to 2+ allows 5+ and 6+; strong |e+|b{++} feed from (7-) rules out 5+ 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (19)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x is expected to be small. The level decays to 6715 and 6743 levels through, as yet, unidentified transitions 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_comment:
E$ level from figure 2 of 2011Mi08. The |g-rays comprise unresolved doublets with those from this level and 7- 3000.3 level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from |t=7.46 ps {I19} from RDDS method analyzed with differential decay curve (DDC) method (2023Ce04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from |t=4.25 ps {I23} from RDDS method analyzed with differential decay curve (DDC) method (2023Ce04) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: H
level_comment:
MOMM1 atomic-beam magnetic resonance (2005St24) 
T from |g(t) in {+119}Te |e decay (1973Ka45). Other: 15.9 h {I3} (1961Fi05) 
J J=1/2 from atomic beam (1976Fu06); L({+3}He,|a),(d,t)=0 


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 
MOMM1 radiative detection of NMR (2005St24) 
T weighted av of 4.79 d {I12} (1973Ka45), 4.7 d {I3} (1960Ko12) 4.68 d {I5} (1963Ka04), 4.5 d {I3} (1961Fi05) and 4.75 d {I20} (1960So02). All data are from {+119}Te |e decay 
J J=11/2 from atomic beam (1976Fu06), L({+3}He,|a), (pol d,t)=5 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
MOMM1 integral-perturbed angular distribution of |g rays following reactions (2005St24) 
J L(d,t),({+3}He,|a)=2; |g(|q) in (|a,2n|g) 
T from |g(t) in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J L(pol d,t)=(3); |g's to 5/2+ and 11/2-, log {I{ft}}=7.22 (log| {If{+1u}t}=8.55) from 5/2+ excludes 9/2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+ 
MOMM1 transient field integral PAC (1989Ra17). Other: +0.78 {I14} (1989Ra17) 
T from B(E2)|^=0.55 {I11}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E value from {+120}I |e decay. 
T from B(E2) 
G from 1981Sh15. Value assumes T{-1/2}=9.3 ps {I19}; other: g=0.39 {I7} (1985ThZY), g=0.29 {I8} (1969He11 as corrected by 1974Hu01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L from 1972SeZP. The evaluators note that expected L=0 transition is very weak, so that assignment may be incorrect. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (24)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$|g sequence for this band is from 2014Na30. In 2012Na01, it was shown connected to the main level scheme 
E$ x set at 9700 in 2014Na30 
J$from 2014Na30 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$B(E2) determined from ratios of intensities of first 2+ to 0+ gamma transitions in {+120}Te, {+122}Te and {+58}Ni, and using B(E2)=0.660 {I6} (2001Ra27: At. Data Nucl. Data Tables 78, 1) for the first 2+ to 0+ transition in {+122}Te 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$for the 0|n|b{++}|e decay mode at 90% confidence level. The authors also report a value of >2.7|*10{+21} y by combining the results from the Cuoricino experiment (2011An01): Astropart Phys 34, 643 (2011) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: D
level_comment:
J L=0 in (d,p), ({+3}He,|a) 
T from weighted average of 19.16 d {I5} (1995Si30) and 19.2 d {I1} (2008Ea01); others: 16.78 d {I35} (1973Ka45), 17 d {I1} (1963Bh04,1946Ed03) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T from (ce 82|g)(ce 212|g)(t) in IT decay (1963Sc12) 
J L=2 in (d,p), ({+3}He,|a),(pol d,t); M1+E2 |g to 1/2+ 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$N/RD (2005St24); reference to |m=+0.605 {I4} for {+125}Te (36 keV) 
J L=5 in (d,p),(pol d,t); M4 |g to 3/2+ 
T from 2008Ea01. Others: 154 d {7} (1963Bh04), 125 d (1940Se01), 143 d {I5} (1946Ed03), 140 d (1951Co34), 154 d (1951Hi80) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T from |g(t) (1980Io01) 
J$ E2 |g to 3/2+; L=4 in (p,d),(pol d,t), J=7/2 is consistent with band structure 
MOMM1$DPAD (2005St24); others: +0.774 {I11} (DPAD), +0.63 {I7} (DPAD) (2005St24) 


level_energy_unit: KEV
level_spin_parity: (21/2)-
level_comment:
$Probable admixture of non-collective configuration=((|p 1g{-7/2}){++2}{-6+}(|n 1h{-11/2})), J|p=21/2- 


level_energy_unit: KEV
level_spin_parity: (23/2)-
level_comment:
$Probable admixture of non-collective configuration=((|p 1g{-7/2}){++2}{-6+}(|n 1h{-11/2})), J|p=23/2- 


level_energy_unit: KEV
level_spin_parity: (23/2,25/2)
level_comment:
J 25/2- assigned in {+114}Cd({+11}B,p3n|g) from mult.(939|g)=(E1), while 23/2+ assigned in {+116}Cd({+9}Be,4n|g) from mult.(937|g)=(E2) 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_comment:
$Probable admixture of non-collective configuration=((|p 1g{-7/2}){++2}{-6+}(|n 1h{-11/2}){++3}{-25/2-}), J|p=35/2- 


level_energy_unit: KEV
level_spin_parity: (39/2-)
level_comment:
$Probable admixture of non-collective configuration=((|p 1g{-7/2}){++2}{-6+}(|n 1h{-11/2}){++3}{-27/2-}), J|p=39/2- 


level_energy_unit: KEV
level_spin_parity: (47/2)
level_comment:
$Probable admixture of non-collective configuration=((|p 1g{-7/2}){++2}{-6+}(|n 1h{-11/2}){++5}{-35/2-}), J|p=47/2- 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
E$rounded-off value from adopted levels 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$from adopted levels 


level_energy_unit: KEV
level_spin_parity: (23/2,25/2)
level_comment:
$J|p=23/2(+) was proposed in this reaction (1996Si24,1995Si28), this assignment disagrees with J|p=25/2- given in {+116}Cd({+9}Be,4n|g) 


level_energy_unit: KEV
level_spin_parity: (27/2,29/2)
level_comment:
$J|p=27/2(+) was proposed in this reaction (1996Si24,1995Si28), this assignment disagrees with J|p=29/2- given in {+116}Cd({+9}Be,4n|g) 


level_energy_unit: KEV
level_spin_parity: (31/2)
level_comment:
$J|p=31/2(+) was proposed in this reaction (1996Si24,1995Si28), this assignment disagrees with J|p=31/2- given in {+116}Cd({+9}Be,4n|g) 


level_energy_unit: KEV
level_spin_parity: (35/2)
level_comment:
$J|p=35/2(+) was proposed in this reaction (1996Si24,1995Si28), no J|p assignment was given in {+116}Cd({+9}Be,4n|g) 


level_energy_unit: KEV
level_spin_parity: (23/2,25/2)
level_comment:
$J|p=25/2- was proposed in this reaction (1996Pa11), this assignment disagrees with J|p=23/2(+) given in {+114}Cd({+11}B,p3n|g) (1996Si24,1995Si28) 


level_energy_unit: KEV
level_spin_parity: (27/2,29/2)
level_comment:
$J|p=29/2- was proposed in this reaction (1996Pa11), this assignment disagrees with J|p=27/2(+) given in {+114}Cd({+11}B,p3n|g) (1996Si24,1995Si28) 


level_energy_unit: KEV
level_spin_parity: (31/2)
level_comment:
$J|p=31/2- was proposed in this reaction (1996Pa11), this assignment disagrees with J|p=31/2(+) given in {+114}Cd({+11}B,p3n|g) (1996Si24,1995Si28) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$This level is proposed as 13/2- in 1h{-11/2} band in this reaction (1979Ha47), but reinterpreted as band head of |g band based on 1h{-11/2} in {+116}Cd({+9}Be,4n|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: D
level_comment:
T$from decay curve of 573.1|g in {+121}Sb from the decay of {+121}Te (2019Jo03), weighted average of 19.41 d {I7}, 19.30 d {I8}, 19.38 d {I7} and 19.41 d {I4}. Compiler obtains weighted average of 19.39 d {I3} from these four values. This value can be compared with 19.2 d {I1} (2008Ea01: Phys. Rev. C 77, 024303); 19.16 d {I5} (1995Si30: Appl. Radiat. Isot. 46, 865); 16.78 d {I35} (1973Ka45: Radiochim. Acta 19, 1); 17 d {I1} (1963Bh04: Nucl. Phys. 41, 184); 17 d {I1} (1946Ed03: Phys. Rev. 69, 140). Value is 19.17 d {I4} in {+121}Te Adopted Levels in the ENSDF database, taken from 2008Ea01 and 1995Si30 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
%IT$measured by 2019Jo03 from the intensities of the 212.2- and 573.1-keV |g rays, half-lives of the g.s. and isomer of {+121}Te and using equations derived for transient equilibrium. This value can be compared with 88.6 {I11} (from %|e+|b{++}=11.4 {I11} deduced in {+121}Te (164.2 d) |e decay dataset in the ENSDF database, using |g-intensity data from 1975Me23: Phys. Rev. C12, 2010); 90.2 {I5} (1964Ch08: Phys. Rev. 133, No. 6B, 1361); |?81 (1964Au05: Nucl. Phys. 58, 337); 86 (1963Bh04) 
T$from decay curve for 212.2|g (2019Jo03), weighted average of 163.3 d {I16}, 165.1 d {I10}, 166.5 d {I16} and 165.4 d {I19}. This value can be compared with 164.2 d {I8} (2008Ea01); 154 d {I7} (1963Bh04), 140 d (1951Co34: Phys. Rev. 84, 596), 154 d (1951Hi80: Phys. Rev. 81, 470), 143 d {I5} (1946Ed03), 125 d (1940Se01: Phys. Rev. 57, 363). Value is 164.2 d {I8} in {+121}Te Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$|m: transient field integral perturbed angular correlations (1988Du10); others: +0.68 {i4} (1985ThZX), +0.66 {i6} (1981Sh15), +0.56 {i10} (1985Gr17). +0.72 {i4} integral perturbed angular correlation (1988Du10) and reevaluated by 2005St24 
$Q: Coulomb excitation reorientation (1978Be10) and reevaluated in 2005St24. Other: -0.57 {i5} (1978Be10) 
$B(E2) from Coulomb excitation 
J L=2 in (p,t) and (p,p'); stretched E2 |g to 0+ 
T from B(E2); other: 8.4 ps {i8} from total width in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E $unresolved doublet of near-lying levels in (d,d'), (p,p'), ({+3}He,d), (d,t), and ({+3}He,{+4}He) 
J $490|g(|q) and 1183|g(|q) are isotropic in (n,n'|g); J-dependence of excitation function of 1183|g; L=(0) in (p,t); 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
E $unresolved doublet of the near-lying levels in (d,d') 
J stretched E2 |g to 4+, (M1+E2) |g to 6+ in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: PS
level_comment:
E $unresolved doublet of the near-lying levels in (p,t) and ({+3}He,{+4}He) 
J$log {Ift}=5.89 from 1+, M1+E2 |g to 2+, |g to 4+ and 0+ 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: FS
level_comment:
E doublet in (p,t) 
J L=(2) in (p,t); log {Ift}=6.6 from 1+; M1+E2 |g to 2+, |g(|q) excludes J|p=3+ 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
E $unresolved doublet of the near-lying levels in ({+3}He,{+4}He) 
J 1936|g(|q) is isotropic in (n,n'|g); L=0+2+(4) in ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
E $unresolved doublet of the near-lying levels in (d,d') and (d,t) 
J D |g to 0+ in (|g,|g'), |g to 2+ 
T$other: 17 fs {i4} from total width in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1,2,3
level_lifetime_unit: PS
level_comment:
E $admixture of other isotopes in (d,d'), (d,t) and ({+3}He,{+4}He); unresolved doublet of the near-lying levels in (d,d') 
J $D(+Q) |g's to 2+ 


level_energy_unit: KEV
level_spin_parity: 0+,1+,2+
level_lifetime_unit: PS
level_comment:
E doublet in (|a,|a') 
J $log {Ift}=5.56 from 1+; |g's to 2+. Weak feeding in (n,n'|g) suggests J|p=0+ (2005Hi04) 


level_energy_unit: KEV
level_spin_parity: (4,5,6)+
level_lifetime_unit: PS
level_comment:
E$Unresolved doublet of the near-lying levels in (d,d') and ({+3}He,d), 
J $M1+E2 |g to 4+; excitation function and 717|g(|q) in (n,n'|g) (2005Hi04) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: PS
level_comment:
E $unresolved triplet of the near-lying levels in ({+3}He,d) and (d,d'); admixture of other isotope in (d,t) 
J log {Ift}=6.86 from 1+, M1+E2 |g's to 2+, |g to 0+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: PS
level_comment:
E Probable doublet in ({+3}He,d) 
J$|g to 0+, M1(+E2) |g's to 2+; log {Ift}=6.49 from 1+; L=(2) in ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: PS
level_comment:
E $unresolved doublet of the near-lying levels in ({+3}He,d); probable multiplet in (p,t) 
J$M1(+E2) |g to 2+, |g to 0+ 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J $stretched Q |g to 8+ in (|a,2n|g), 1996Pa11 suggested mixture of a possible configuration= (|nh{-11/2}{+2}){-10+} 


level_energy_unit: KEV
level_spin_parity: 1,2+
level_comment:
J excited in (|g,|g'), log {Ift}=6.09 from 1+, (D,Q) |g to 0+ 
$although deexcitation |g rays observed in {+122}I |e decay and in (|g,|g') are different, the evaluator assumes the same level is excited by both reactions, because the detector sensitivity in both experimental conditions are different 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
g-factor=0.38 {I8} deduced from (693|g)(564|g)(|q,h) (weighted average from 1967Mu10,1967Bh06,1966Jo06 and 1966Au05) 


level_energy_unit: KEV
level_comment:
S 0.04 for L=0; 0.15 for L=2; 0.4 for L=(4) 
$|s(10|')=66 {I3}, |s(15|')=44.7 {I21}, |s(20|')=25.2 {I12}, |s(25|')=24.6 {I16}, |s(30|')=15.0 {I10}, |s(35|')=13.3 {I11}, |s(40|')=7.7 {I8}, |s(60|')=1.7 {I4} 


level_energy_unit: KEV
level_comment:
S 0.04 for L=0; 0.15 for L=2; 0.4 for L=(4) 
$|s(10|')=114 {I9}, |s(15|')=100 {I14}, |s(20|')=52.0 {I16}, |s(25|')=63.6 {I25}, |s(30|')=35.4 {I16}, |s(35|')=31.7 {I19}, |s(40|')=20.5 {I13}, |s(60|')=4.7 {I6} 


level_energy_unit: KEV
level_comment:
$|s(10|')=116 {I8}, |s(15|')=84 {I5}, |s(20|')=50.7 {I22}, |s(25|')=52.6 {I23}, |s(30|')=31.6 {I15}, |s(35|')=31.2 {I19}, |s(40|')=18.9 {I13}, |s(60|')=5.1 {I6} 


level_energy_unit: KEV
level_comment:
$|s(10|')=50 {I5}, |s(15|')=48.2 {I29}, |s(20|')=22.9 {I11}, |s(25|')=26.9 {I16}, |s(30|')=16.2 {I11}, |s(35|')=11.4 {I10}, |s(40|')=8.1 {I9}, |s(60|')=1.8 {I4} 


level_energy_unit: KEV
level_comment:
$|s(10|')=30 {I4}, |s(15|')=22.8 {I21}, |s(20|')=14.4 {I9}, |s(25|')=12.4 {I12}, |s(30|')=10.1 {I9}, |s(35|')=8.3 {I8}, |s(40|')=3.4 {I7}, |s(60|')=1.1 {I4} 


level_energy_unit: KEV
level_comment:
E doublet (1751+1752) 
$|s(10|')=136 {I5}, |s(15|'), |s(15|')=130 {I5}, |s(20|')=111 {I4}, |s(25|')=85.6 {I30}, |s(30|')=60.9 {I22}, |s(35|')=48.0 {I20}, |s(40|')=34.9 {I17}, |s(60|')=9.8 {I8} 


level_energy_unit: KEV
level_comment:
$|s(10|')=26.5 {I21}, |s(15|')=22.3 {I23}, |s(20|')=10.1 {I15}, |s(25|')=10.4 {I11}, |s(30|')=6.5 {I9}, |s(35|')=6.2 {I7}, |s(40|')=3.1 {I6}, |s(60|')=0.83 {I30} 


level_energy_unit: KEV
level_comment:
$|s(10|')=13.8 {I20}, |s(15|')=11.0 {I20}, |s(20|')=5.3 {I15}, |s(25|')=6.0 {I10}, |s(30|')=3.9 {I9}, |s(35|')=2.7 {I7}, |s(40|')=1.41 {I30}, |s(60|')=0.78 {I30} (sum for 1940.5+1951.6 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=10.3 {I6}, |s(15|')=8.5 {I19}, |s(20|')=4.1 {I14}, |s(25|')=5.7 {I10}, |s(30|')=3.1 {I9}, |s(35|')=2.7 {I7}, |s(40|')=1.6 {I4}, |s(60|')=0.78 {I30} (sum for 1941+1951.6 levels at 60|') 


level_energy_unit: KEV
level_comment:
E admixture of {+124}Te 2618 level 
$|s(10|')=79 {I4}, |s(15|')=65 {I4}, |s(20|')=35.6 {I26}, |s(25|')=38.1 {I19}, |s(30|')=21.1 {I15}, |s(35|')=17.0 {I12}, |s(40|')=11.1 {I13}, |s(60|')=3.7 {I5} 


level_energy_unit: KEV
level_comment:
$|s(10|')=390 {I8}, |s(15|')=275 {I8}, |s(20|')=158 {I6}, |s(25|')=160 {I4}, |s(30|')=96.1 {I28}, |s(35|')=79.7 {I25}, |s(40|')=57.1 {I21}, |s(60|')=14.3 {I9} 


level_energy_unit: KEV
level_comment:
$|s(10|')=13.1 {I17}, |s(15|')=32.5 {I20}, |s(20|')=42.9 {I16}, |s(25|')=25.6 {I16}, |s(30|')=20.2 {I13}, |s(35|')=14.8 {I13}, |s(40|')=13.4 {I11}, |s(60|')=3.8 {I6} 


level_energy_unit: KEV
level_comment:
$|s(10|')=20.5 {I22}, |s(15|')=31.2 {I18}, |s(20|')=39.1 {I28}, |s(25|')=29.5 {I26}, |s(30|')=20.5 {I15}, |s(35|')=16.1 {I18}, |s(40|')=10.1 {I13}, |s(60|')=5.7 {I6} (sum for 2287.4+2298.3+2311 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=32.7 {I28}, |s(15|')=27.5 {I17}, |s(20|')=19.5 {I24}, |s(25|')=14.3 {I21}, |s(30|')=7.7 {I11}, |s(35|')=10.4 {I16}, |s(40|')=6.4 {I10}, |s(60|')=5.7 {I6} (sum for 2287.4+2298.3+2311 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=31.4 {I27}, |s(15|')=28.1 {I15}, |s(20|')=13.5 {I11}, |s(25|')=16.4 {I17}, |s(30|')=7.1 {I8}, |s(35|')=7.5 {I8}, |s(40|')=6.4 {I7}, |s(60|')=5.7 {I6} (sum for 2287.4+2298.3+2311 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=127 {I6}, |s(15|')=92 {I16} (doublet?), |s(20|')=67 {I7} (doublet?), |s(25|')=71.2 {I25}, |s(30|')=40.8 {I18}, |s(35|')=30.7 {I22}, |s(40|')=25.5 {I15}, |s(60|')=4.7 {I8} 


level_energy_unit: KEV
level_comment:
$|s(10|')=36 {I4}, |s(15|')=31.2 {I15}, |s(20|')=17.0 {I10}, |s(25|')=15.7 {I13}, |s(30|')=8.5 {I9}, |s(35|')=8.1 {I12}, |s(40|')=7.8 {I9}, |s(60|')=0.7 {I5} 


level_energy_unit: KEV
level_comment:
S 0.03 for L=0; 0.12 for L=2; 0.3 for L=(4) 
$|s(10|')=6 {I4}, |s(15|')=7.6 {I11}, |s(20|')=5.9 {I8}, |s(25|')=4.4 {I10}, |s(30|')=3.4 {I9}, |s(35|')=4.1 {I12} 


level_energy_unit: KEV
level_comment:
E admixture of {+124}Te 3091 level 
$|s(10|')=104 {I6}, |s(15|')=81.8 {I24}, |s(20|')=46.5 {I16}, |s(25|')=54.6 {I23}, |s(30|')=29.6 {I16}, |s(35|')=19.0 {I17}, |s(40|')=16.9 {I14}, |s(60|')=3.3 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=215 {I8}, |s(15|')=178 {I4}, |s(20|')=106.1 {I23}, |s(25|')=100 {I4}, |s(30|')=62.8 {I22}, |s(35|')=53.5 {I27}, |s(40|')=34.4 {I21}, |s(60|')=8.8 {I9} 


level_energy_unit: KEV
level_comment:
$|s(10|')=112 {I8}, |s(15|')=90.0 {I24}, |s(20|')=51.3 {I30}, |s(25|')=54.7 {I23}, |s(30|')=32.3 {I16}, |s(35|')=27.4 {I19}, |s(40|')=17.9 {I14}, |s(60|')=4.1 {I7} 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E possible admixture of {+124}Te 3520 level 
$|s(15|')=4.2 {I7}, |s(20|')=5.0 {I7}, |s(25|')=5.5 {I9}, |s(30|')=4.7 {I8}, |s(35|')=2.3 {I7}, |s(40|')=2.5 {I7} 


level_energy_unit: KEV
level_comment:
E possible admixture of {+124}Te 3520 level 
L,S For 2659.2+2671.8 levels 
$|s(10|')=22 {I4}, |s(15|')=14.8 {I13}, |s(20|')=13.0 {I26}, |s(25|')=10.4 {I12}, |s(30|')=5.5 {I8}, |s(35|')=3.6 {I7}, |s(40|')=2.4 {I7} 


level_energy_unit: KEV
level_comment:
E triplet (2671.8+2683.2+2692 levels) 
L,S For 2659.2+2671.8 levels 
$|s(10|')=105 {I6} (for 2672+2683.2 levels at 10|'), |s(15|')=54.0 {I25}, |s(20|')=47 {I4}, |s(25|')=27.4 {I25}, |s(30|')=20.5 {I18}, |s(35|')=16.9 {I17}, |s(40|')=9.0 {I18}, |s(60|')=3.8 {I6} 


level_energy_unit: KEV
level_comment:
E triplet (2671.8+2683.2+2692 levels) 
$|s(10|')=105 {I6} (for 2672+2683.2 levels at 10|'), |s(15|')=80.2 {I28}, |s(20|')=43 {I4}, |s(25|')=48.9 {I30}, |s(30|')=33.3 {I26}, |s(35|')=26.1 {I18}, |s(40|')=22.6 {I21}, |s(60|')=3.5 {I6} (sum for 2683.2+2692 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=21 {I4}, |s(15|')=12.3 {I15}, |s(20|')=7 {I4}, |s(25|')=10.6 {I21}, |s(30|')=4.0 {I16}, |s(35|')=5.5 {I10}, |s(40|')=4.9 {I17}, |s(60|')=3.5 {I6} (sum for 2683+2692 levels at 60|') 
E triplet (2671.8+2683.2+2692 levels) 


level_energy_unit: KEV
level_comment:
$|s(10|')=69 {I4}, |s(15|')=78.5 {I24}, |s(20|')=35.6 {I22}, |s(25|')=47.2 {I23}, |s(30|')=28.6 {I21}, |s(35|')=16.5 {I12}, |s(40|')=12.9 {I12}, |s(60|')=2.0 {I6} (assignment questionable) 


level_energy_unit: KEV
level_comment:
$|s(10|')=90 {I4}, |s(15|')=74.7 {I23}, |s(20|')=32.1 {I22}, |s(25|')=39.9 {I21}, |s(30|')=24.0 {I19}, |s(35|')=20.6 {I13}, |s(40|')=14.4 {I13}, |s(60|')=3.9 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=79 {I4}, |s(15|')=78.8 {I24}, |s(20|')=43.0 {I23}, |s(25|')=57.4 {I25}, |s(30|')=34.2 {I22}, |s(35|')=19.9 {I13}, |s(40|')=17.7 {I14}, |s(60|')=3.9 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=52 {I4}, |s(15|')=29.6 {I18}, |s(20|')=20.6 {I20} (2802 level stronger), |s(25|')=16.5 {I15}, |s(30|')=11.1 {I15}, |s(35|')=7.6 {I10}, |s(40|')=6.6 {I9}, |s(60|')=1.7 {I4} (sum for 2796.6+2814 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=16.5 {I27}, |s(15|')=26.5 {I17}, |s(20|')=13.4 {I18}, |s(25|')=19.3 {I16}, |s(30|')=12.6 {I15}, |s(35|')=8.0 {I13}, |s(40|')=9.1 {I10}, |s(60|')=1.7 {I4} (sum for 2796.6+2814 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(15|')=3.5 {I7}, |s(20|')=14.8 {I14}, |s(25|')=11.1 {I13}, |s(30|')=6.6 {I11}, |s(35|')=4.8 {I11}, |s(40|')=4.0 {I12}, |s(60|')=1.2 {I4} 


level_energy_unit: KEV
level_comment:
$|s(10|')=43 {I4}, |s(15|')=47 {I4}, |s(20|')=25.6 {I17}, |s(25|')=35.3 {I19}, |s(30|')=21.7 {I18}, |s(35|')=11.8 {I18}, |s(40|')=13.9 {I16}, |s(60|')=2.1 {I5} 


level_energy_unit: KEV
level_comment:
E doublet 
$|s(10|')=113 {I6}, |s(15|')=99 {I15}, |s(20|')=64.1 {I26}, |s(25|')=68 {I6}, |s(30|')=43 {I5}, |s(35|')=23.0 {I27}, |s(40|')=21.7 {I19}, |s(60|')=3.2 {I6} 


level_energy_unit: KEV
level_comment:
$|s(10|')=79 {I5}, |s(15|')=60 {I4}, |s(20|')=34.5 {I20}, |s(25|')=44.7 {I22}, |s(30|')=24.6 {I19}, |s(35|')=15.2 {I29}, |s(40|')=19.0 {I18}, |s(60|')=3.1 {I6} 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$|s(10|')=98 {I7}, |s(15|')=78 {I6}, |s(20|')=29 {I4}, |s(25|')=47.2 {I29}, |s(30|')=36.2 {I30}, |s(35|')=13.2 {I5}, |s(40|')=15.8 {I30}, |s(60|')=2.0 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=749 {I16}, |s(15|')=563 {I12}, |s(20|')=324 {I7}, |s(25|')=318 {I6}, |s(30|')=182 {I5}, |s(35|')=135 {I14}, |s(40|')=118 {I8}, |s(60|')=28.1 {I19} 


level_energy_unit: KEV
level_comment:
$|s(10|')=43 {I11}, |s(15|')=30 {I5}, |s(20|')=21.2 {I24}, |s(25|')=33.3 {I29}, |s(30|')=34 {I4}, |s(35|')=32 {I11}, |s(40|')=12.7 {I5}, |s(60|')=3.8 {I15} 


level_energy_unit: KEV
level_comment:
E probably doublet 
$|s(10|')=336 {I10}, |s(15|')=264 {I28}, |s(20|')=154 {I15}, |s(25|')=172 {I19}, |s(30|')=94 {I5}, |s(35|')=7.6 {I4}, |s(40|')=58.9 {I29}, |s(60|')=13.9 {I10} 


level_energy_unit: KEV
level_comment:
$|s(10|')=152 {I7} (assignment and intensity questionable), |s(15|')=61 {I7} (doublet?), |s(20|')=32.3 {I21}, |s(25|')=37.8 {I21}, |s(30|')=19.7 {I14}, |s(35|')=13.8 {I18}, |s(40|')=10.1 {I16}, |s(60|')=1.8 {I5} 


level_energy_unit: KEV
level_comment:
E multiplet (between 3096.6 keV and 3166.9 keV) 
$|s(10|')=133 {I7} (assignment and intensity questionable), |s(15|')=44 {I4}, |s(20|')=27.5 {I18},|s(25|')=33.9 {I19}, |s(30|')=17.6 {I13}, |s(35|')=12.9 {I17}, |s(40|')=11.1 {I17}, |s(60|')=1.3 {I4} 


level_energy_unit: KEV
level_comment:
E multiplet (between 3096.6 keV and 3166.9 keV) 
$|s(10|')=250 {I10} (assignment and intensity questionable), |s(15|')=162 {I10}, |s(20|')=97 {I4}, |s(25|')=102 {I4}, |s(30|')=55.9 {I24}, |s(35|')=44 {I4},|s(40|')=42.3 {I27}, |s(60|')=7.7 {I18} (sum for 3121+3136 levels at 60|') 


level_energy_unit: KEV
level_comment:
E multiplet (between 3096.6 keV and 3166.9 keV) 
$|s(10|')=100 {I8} (assignment and intensity questionable), |s(15|')=46 {I6}, |s(20|')=26.6 {I28}, |s(25|')=21.3 {I26}, |s(30|')=16.3 {I17}, |s(35|')=12.1 {I23}, |s(40|')=6.9 {I17}, |s(60|')=7.7 {I18} (sum for 3121+3136 levels at 60|') 


level_energy_unit: KEV
level_comment:
E multiplet (between 3096.6 keV and 3166.9 keV) 
$|s(10|')=83 {I7} (assignment and intensity questionable), |s(15|')=29 {I4}, |s(20|')=14.4 {I21}, |s(25|')=19.1 {I17}, |s(30|')=12.1 {I12}, |s(35|')=10.5 {I18}, |s(40|')=7.8 {I15}, |s(60|')=2.8 {I6} 


level_energy_unit: KEV
level_comment:
E multiplet (between 3096.6 keV and 3166.9 keV) 
$|s(10|')=60 {I6} (assignment and intensity questionable), |s(15|')=50 {I4}, |s(20|')=78.1 {I28}, |s(25|')=48.7 {I23}, |s(30|')=30.9 {I17}, |s(35|')=27.6 {I23}, |s(40|')=19.8 {I17}, |s(60|')=7.3 {I17} (sum for 3167+3184.6 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=60 {I5}, |s(15|')=22.2 {I27}, |s(20|')=13.3 {I16}, |s(25|')=13.7 {I14}, |s(30|')=9.5 {I11}, |s(35|')=8.5 {I16}, |s(40|')=8.2 {I13}, |s(60|')=7.3 {I17} (sum for 3167+3184.6 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=85 {I5}, |s(15|')=26.5 {I27}, |s(20|')=12.1 {I13}, |s(25|')=13.1 {I13}, |s(30|')=7.3 {I9}, |s(35|')=5.6 {I14}, |s(40|')=4.6 {I11}, |s(60|')=0.8 {I4} 


level_energy_unit: KEV
level_comment:
$|s(10|')=22 {I5}, |s(15|')=14 {I8}, |s(20|')=9.4 {I20}, |s(25|')=9.0 {I4}, |s(30|')=6.4 {I24}, |s(35|')=7.5 {I14} (sum for 3250+3257 levels at 35|'), |s(40|')=4.8 {I11} (sum for 3250+3257 levels at 40|') 


level_energy_unit: KEV
level_comment:
$|s(15|')=13 {I8}, |s(20|')=6.8 {I20}, |s(25|')=11.8 {I5}, |s(30|')=5.8 {I24}, |s(35|')=7.5 {I14} (sum for 3250+3257 levels at 35|'), |s(40|')=4.8 {I11} (sum for 3250+3257 levels at 40|') 


level_energy_unit: KEV
level_comment:
E triplet (3282.7+3295.1+3311.1 levels) 
$|s(|q) are questionable due to multiplet): |s(10|')=46 {I6}, |s(15|')=9 {I7}, |s(20|')=42.6 {I22}, |s(25|')=30.0 {I25}, |s(30|')=18 {I4}, |s(35|')=14.1 {I25}, |s(40|')=10.5 {I16}, |s(60|')=3.5 {I7} (sum for 3282.7+3295.1 levels at 60|') 


level_energy_unit: KEV
level_comment:
E triplet (3282.7+3295.1+3311.1 levels) 
$|s(|q) are questionable due to multiplet): |s(10|')=46 {I6}, |s(15|')=30 {I6}, |s(20|')=16.8 {I18}, |s(25|')=28.2 {I25}, |s(30|')=20 {I4}, |s(35|')=9.8 {I21}, |s(40|')=11.6 {I17}, |s(60|')=3.5 {I7} (sum for 3282.7+3295.1 levels at 60|') 


level_energy_unit: KEV
level_comment:
E triplet (3282.7+3295.1+3311.1 levels) 
$|s(|q) are questionable due to multiplet): |s(10|')=24 {I5}, |s(15|')=20 {I4}, |s(20|')=13.0 {I13}, |s(25|')=15.5 {I16}, |s(30|')=11.5 {I19}, |s(35|')=5.2 {I16}, |s(40|')=4.8 {I12}, |s(60|')=2.0 {I6} 


level_energy_unit: KEV
level_comment:
L,S 0.08 for L=0; 0.22 for L=2, 3331.2+3360.0 levels 
$|s(10|')=13 {I3}, |s(15|')=14 {I3}, |s(20|')=14.4 {I16}, |s(25|')=13.5 {I14}, |s(30|')=8.9 {I14}, |s(35|')=5.4 {I13}, |s(40|')=4.6 {I11}, |s(60|')=1.3 {I5} 


level_energy_unit: KEV
level_comment:
L,S 0.08 for L=0; 0.22 for L=2, 3331.2+3360.0 levels 
$|s(10|')=95 {I6}, |s(15|')=106 {I6}, |s(20|')=55 {I6}, |s(25|')=60.7 {I26}, |s(30|')=41.3 {I26}, |s(35|')=19.1 {I20}, |s(40|')=2.1 {I17}, |s(60|')=3.4 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=41 {I4}, |s(15|')=46 {I5}, |s(20|')=25 {I5} (questionable due to multiplet), |s(25|')=29.3 {I27}, |s(30|')=27.4 {I22}, |s(35|')=12.1 {I17}, |s(40|')=7.2 {I14}, 


level_energy_unit: KEV
level_comment:
L,S 0.05 for L=0; 0.20 for L=2, 3440+3460 levels 
$|s(10|')=58 {I6} (doublet?), |s(15|')=59 {I5}, |s(20|')=42 {I5} (questionable due to multiplet), |s(25|')=26.2 {I29}, |s(30|')=23.0 {I28}, |s(35|')=10.1 {I14}, |s(40|')=9.4 {I15}, |s(60|')=3.2 {I8} 


level_energy_unit: KEV
level_comment:
L,S 0.05 for L=0; 0.20 for L=2, 3440+3460 levels 
$|s(|q=20-30|') are questionable due to multiplet): |s(10|')=77 {I6} (doublet), |s(15|')=59 {I5} (doublet), |s(20|')=38 {I5}, |s(25|')=25 {I4}, |s(30|')=15.5 {I24} (doublet), |s(35|')=8.0 {I13}, |s(40|')=17.2 {I30} (doublet), |s(60|')=3.9 {I8} 


level_energy_unit: KEV
level_comment:
$|s(10|')=38 {I6}, |s(15|')=41 {I4}, |s(20|')=17.9 {I26}, |s(25|')=21 {I5} (doublet), |s(30|')=12.4 {I22}, |s(35|')=6.6 {I20} 


level_energy_unit: KEV
level_comment:
$|s(10|')=81 {I7}, |s(15|')=42 {I3}, |s(20|')=25.5 {I28}, |s(25|')=20.2 {I30}, |s(30|')=13.7 {I22}, |s(35|')=8.3 {I15}, |s(40|')=11.5 {I16} 


level_energy_unit: KEV
level_comment:
$|s(10|')=153 {I8}, |s(15|')=104 {I5}, |s(20|')=76 {I4}, |s(25|')=90 {I4}, |s(30|')=50 {I4}, |s(35|')=40.9 {I22}, |s(40|')=33.8 {I23}, |s(60|')=5.3 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=193 {I9}, |s(15|')=267 {I7}, |s(20|')=131 {I5}, |s(25|')=147 {I6}, |s(30|')=107 {I5}, |s(35|')=50 {I5}, |s(40|')=51.5 {I27}, |s(60|')=9.0 {I9} 


level_energy_unit: KEV
level_comment:
$|s(10|')=7.0 {I24}, |s(15|')=26.4 {I25}, |s(20|')=10 {I4}, |s(25|')=17.1 {I19}, |s(30|')=13.7 {I18}, |s(35|')=3.5 {I15}, |s(40|')=3.5 {I13} 


level_energy_unit: KEV
level_comment:
$|s(10|')=23 {I5}, |s(15|')=44 {I4}, |s(20|')=15.7 {I23}, |s(25|')=15.1 {I19}, |s(30|')=15.8 {I20}, |s(35|')=7.0 {I18}, |s(40|')=11.9 {I21} 


level_energy_unit: KEV
level_comment:
$|s(10|')=78 {I6}, |s(15|')=55 {I6}, |s(20|')=31.0 {I25}, |s(25|')=35.3 {I25}, |s(30|')=23.8 {I22}, |s(35|')=12.1 {I21}, |s(40|')=11.8 {I21}, |s(60|')=5.7 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=67 {I5}, |s(15|')=51 {I4} (overlap due to 3814 levels), |s(20|')=47.3 {I23}, |s(25|')=44.5 {I29}, |s(30|')=39 {I5}, |s(35|')=20.1 {I22}, |s(40|')=20.7 {I18}, |s(60|')=5.8 {I7} 


level_energy_unit: KEV
level_comment:
$|s(10|')=29 {I4} (doublet), |s(15|')=23 {I5} (overlap due to 3788 levels), |s(20|')=12.7 {I5}, |s(30|')=9.3 {I16} 


level_energy_unit: KEV
level_comment:
$|s(10|')=18 {I4}, |s(15|')=25.1 {I24} (doublet), |s(20|')=14.1 {I20}, |s(25|')=12 {I3}, |s(30|')=11.6 {I17}, |s(35|')=9.0 {I16}, |s(40|')=7.4 {I4} 


level_energy_unit: KEV
level_comment:
$|s(10|')=55 {I6}, |s(15|')=25.6 {I23}, |s(20|')=31.3 {I23}, |s(25|')=35.3 {I25} (sum for 3936+3953 levels at this angle), |s(30|')=11.0 {I22}, |s(35|')=8.1 {I20}, |s(40|')=6.5 {I16} 


level_energy_unit: KEV
level_comment:
$|s(10|')=55 {I6}, |s(15|')=42.5 {I26}, |s(20|')=26.2 {I24}, |s(25|')=35.3 {I25} (sum for 3936+3953 levels at 25|'), |s(30|')=16.4 {I23}, |s(35|')=9.3 {I20}, |s(40|')=12.8 {I18} 


level_energy_unit: KEV
level_comment:
$|s(10|')=29 {I6}, |s(15|')=49.2 {I4}, |s(20|')=30.0 {I26}, |s(25|')=51 {I5} (sum for 3983+3998 levels at 25|'), |s(30|')=19.7 {I26}, |s(35|')=14 {I4}, |s(40|')=18.3 {I29} 


level_energy_unit: KEV
level_comment:
$|s(10|')=105 {I13}, |s(15|')=62 {I4}, |s(20|')=32.4 {I22}, |s(25|')=51 {I4} (sum for 3983+3998 levels at 25|'), |s(30|')=25.1 {I26}, |s(35|')=20 {I4}, |s(40|')=21.2 {I29} 


level_energy_unit: KEV
level_comment:
$|s(10|')=54 {I6}, |s(15|')=79 {I4}, |s(20|')=40.0 {I25}, |s(25|')=23.9 {I30}, |s(30|')=28.6 {I23}, |s(35|')=15.2 {I21}, |s(40|')=16.9 {I18} 


level_energy_unit: KEV
level_comment:
$|s(10|')=181 {I11} (sum for 4111+4130 levels at 10|'), |s(15|')=53 {I10}, |s(20|')=39.8 {I29}, |s(25|')=24 {I4}, |s(35|')=6.1 {I20}, |s(40|')=12.6 {I21} (assignment questionable), |s(60|')=7.8 {I12} (sum for 4111+4130 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=181 {I11} (sum for 4111+4130 levels at 10|'), |s(15|')=71 {I10}, |s(20|')=28.6 {I27}, |s(25|')=38 {I4}, |s(30|')=25.9 {I26}, |s(35|')=19.2 {I22}, |s(40|')=18.2 {I24}, |s(60|')=7.8 {I12} (sum for 4111+4130 levels at 60|') 


level_energy_unit: KEV
level_comment:
$|s(10|')=221 {I22}, |s(15|')=243 {I8}, |s(20|')=155 {I10}, |s(25|')=104 {I7} (assignment questionable), |s(30|')=79 {I4}, |s(35|')=56.4 {I28}, |s(40|')=61 {I7} (assignment questionable), |s(60|')=12.5 {I11} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T $weighted average of half-lives (calculated values from total |G): 7.3 ps {i11} (1964Pa17), 9.2 ps {i3} (1963Zi02), 8.3 ps {i21} (1963Sh17), 10.4 ps {i16} ({+122}Sb source, 1963Sh17) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$g|G(|g{-0}){+2}/|G (meV)=56 {I7} 
T |G{-0}=18.4 {i23} from integrated scattering cross section in 1997Sc15 
T |G{-0}/|G=0.84 {i11} from adopted gammas 


level_energy_unit: KEV
level_comment:
E Calibration 
$I(20|')=230 {I30}, I(30|')=110 {I10} (sum for 1751.3+1752.6 levels at 20|' and 30|') 


level_energy_unit: KEV
level_comment:
E$admixture of other isotopes probably doublet 
$I(20|')=44 {I5}, I(30|')=27.6 {I22} (admixture of other isotopes at 20|' and 30|') 


level_energy_unit: KEV
level_comment:
E$doublet (1999Sc19) or triplet (adopted levels) 
$I(20|')=4.1 {I25}, I(30|')=5.4 {I13} (sum for possible triplet: 2756.1+2758.5+2758.8 levels at 20|' and 30|') 


level_energy_unit: KEV
level_comment:
E$triplet (1999Sc19); multiplet (adopted levels) 
$I(20|')=33 {I5} (multiplet), I(30|')=32 {I7} (multiplet) (sum for possible multiplet: 2911.24+2911.24+2913.5+2913.8+2915.9 levels at 20|' and 30|') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2) and branching=1.0 
B(E2)|^=0.664 {I4} 
B(E2) value is weighted average of 0.664 {I20} (1977Sa04), 0.658 {I4} (1976Bo12), 0.667 {I11} (1974Ba45), 0.665 {I4} (1978Be10), 0.53 {I2} (1979Sa05). Others: 0.61 {I3} (1970LaZM), 0.65 {I5} (1959Mc59), 0.47 {I10} (1956Te26) 
Q=-0.57 {I5} or -0.35 {I5} (1978Be10), -0.48 {I5} or -0.22 {I5} (1976Bo12), -0.46 {I10} or -0.20 {I10} (1974Ba45), -0.43 {I8} or -0.21 {I8} (1974La05) 
g-factor(2+)=0.33 {I3} (1981Sh15); others: 0.54 {I4} (1966Bo19), 0.31 {I3} (1967Bh06), 0.32 {I5} (1974Hu01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2) and branching=0.17 {i2} 
B(E2)|^=0.021 {I5} (1961St02). Others: 0.0094 (1974Ba45), 0.01 (1976Bo12). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
1974Ba45 report matrix elements of 0.069 for 1752|g and 0.265 for 1188|g; however, these matrix elements are inconsistent with known branchings, %(1752|g)=60 {i2} and %(1188|g)=31 {i2}. The authors appear to have reversed the branchings of the two |g's. The evaluator assumes that the matrix element of 1188|g is the one deduced by the authors. 


level_energy_unit: KEV
level_comment:
$I(20|')=11.7 {I19}, I(25|')=8.5 {I12}, I(50|')=2.2 {I6} (sum for 2297.5+2310.8 levels at 20|', 25|' and 50|') 


level_energy_unit: KEV
level_comment:
$I(20|')=142 {I14}, I(25|')=105 {I5}, I(50|')=4.2 {I8} (admixture of other isotopes at 20|', 25|' and 50|') 


level_energy_unit: KEV
level_comment:
$I(20|')=13.8 {I22} (doublet), I(25|')=13.5 {I19} (doublet) (sum for 3037.1+3044.7 levels at 20|' and 25|') 


level_energy_unit: KEV
level_comment:
$I(20|')=10.5 {I19}, I(25|')=6.3 {I16} (probably main intensity from other isotopes at 20|' and 25|' 


level_energy_unit: KEV
level_comment:
$I(20|')=41 {I4} (doublet), I(25|')=39.8 {I30} (doublet), I(50|')=1.6 {i7} (doublet); sum for 3211.1+3216 levels at 20|', 25|' and 50|') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ from 'adopted levels, gammas' dataset for {+122}Te in ENSDF database. 2008Hi17 quote a slightly different value of 7.49 ps {I7} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
J$spin=1/2 from hyperfine structure using optical spectroscopy (1949Ma47, 1950Fo08); L(d,p)=L(p,d)=L(d,t)=L({+3}He,|a)=0 from 0+. 
T$from 2003Al02, measured half-life T{-1/2}(|e K)>5|*10{+19} y. Others: T{-1/2}>3.2|*10{+16} y (2003Mu02), T{-1/2}(|e K)>2.4|*10{+19} y (1996Al30), T{-1/2}(|e K)>2|*10{+14} y (1945Ru03), T{-1/2}(|e K)>1|*10{+15} y (1955He13), T{-1/2}(|e L)>5|*10{+13} y (1954Se93), T{-1/2}(|e L)>1|*10{+13} y (1955He13), T{-1/2}(|e K)=1.24|*10{+13} y {I10} (1962Wa15). 
MOMM1$from 2014StZZ compilation, deduced from |m({+125}Te)/|m({+123}Te)=1.205581816 {I48} from Nuclear Magnetic Resonance (NMR) measurement in 1977Bu29 and |m({+125}Te)=-0.8884509 {I10} reference to {+23}Na in 2014StZZ. Others: |m({+125}Te)/|m({+123}Te)=1.20560 {I7} (NMR, 1953We51), 1.208 {60} (hyperfine structure, 1949Ma47); |m({+125}Te)=-0.7 {I2} and |m({+123}Te)=-0.6 {I2} (hyperfine structure, 1952Ro05) 
MOMM1$note that |m({+125}Te)=0.8885051 {I4} (corrected for diamagnetism) in 2014StZZ as quoted from 1977Bu29 is deduced from |m({+125}Te)/|m({+2}H)=2.058849 {I1} in 1977Bu29 (both |m not corrected for diamagnetism), |m({+2}H)=0.857438228 {I9} or 0.857438240 {I12} (both corrected for diamagnetism) in 2014StZZ, and diamagnetic correction factor=1.000025689 for H and 1.006639 for Te in Table A of 1989Ra17 compilation. Similarly, the other |m({+125}Te)=0.8884509 {I10} is deduced from |m({+125}Te)/|m({+23}Na)=1.1947994 {I7} in 1977Bu29 and |m({+23}Na) in 2014StZZ, with diamagnetic corrections. 
$Nuclear rms charge radius=4.7117 fm {I35} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(p,d)=L(d,t)=L({+3}He,|a)=2 from 0+; 159.0|g M1+E2 to 1/2+ 
T$from ce-ce(t) in {+123}Te IT decay, weighted average of 199 ps {I10} (1968Ra02), 186 ps {I20} (1963Sc12), and 190 ps {I30} (1953Gr07). Other: 0.32 ns {I+26-14} from B(E2)|^=0.018 {I5} in Coulomb excitation and adopted |d(E2/M1)=+0.079 {I11} for 158.99|g 
MOMM1$from integral perturbed angular correlation (IPAC) in 1970Ro31 and adopted T{-1/2}=196 ps {I10}, based on original value of 0.72 {I12} in 1970Ro31 using T{-1/2}=199 ps {I10} from 1968Ra02. 0.72 {I12} in 2014StZZ compilation. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J$L(d,p)=L(p,d)=L(d,t)=L({+3}He,|a)=5 from 0+; 88.5|g M4 to 3/2+. 
T$from {+123}Te IT decay, as unweighted average of 119.3 d {I1} (1992Co11), 119.7 d {I1} (1970EmZY) and 118.6 d {I9} (1987Ja13). Others: 117 d {I6} (1965An05), 104 d (1951Hi80), 121 d (1951Co34) 
MOMM1$value from 1987Ni11 using nuclear magnetic resonance of oriented nuclei, sign from 1973Si26 with |m=-1.00 {I5} measured using nuclear orientation with gamma detection (1973Si26). Also in 2014StZZ compilation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$spin=3/2 from |g|g(|q) in {+123}I |e decay (1969Se09); L(p,t)=2 from 1/2+; 439.9|g M1+E2 to 1/2+ 
T$deduced from B(E2)=0.21 {I3} in Coulomb excitation, adopted |d(E2/M1)=-2.1 {I1} and branching ratio 83.2% {I5} for 439.7|g (1974Ro40). Other: 1.23 ps {I21} from DSAM in 1973ErZS is discrepant 
MOMM1$from g-factor=0.34 {I6} by IMPAC using T{-1/2}=27 ps {I3} deduced from their B(E2) in 1974Ro40, with correction by using adopted T{-1/2}=22 ps {I4}. Other: +0.66 {I28}, from g-factor=+0.36 {I15} by transient field technique using T{-1/2}=27 ps in 1989Be22 and corrected by using adopted T{-1/2}=22 ps {I4}. Other: +0.51 {I9} in 2014StZZ compilation, as quoted from 1974Ro40 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$spin=7/2 from |g(|q) in 1981Io05; L({+3}He,|a)=4 from 0+ 
T$from beam-|g(t)-coin in 1981Io05. 
MOMM1$from TDPAD (1981Io03, 1981Io05). Also in 2014StZZ compilation 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$spin=5/2 from particle-|g(|q) in Coulomb excitation (1989Be22) and |g|g(|q) in {+123}I |e decay (1969Se09); L(d,t)=2 from 0+, L(p,t)=2 from 1/2+ 
T$deduced from B(E2)=0.27 {I5} from Coulomb excitation, adopted branching ratio 69.7% {I11} for 505.3|g 
MOMM1$from g-factor=0.040 {I25} by IMPAC using T{-1/2}=18 ps {I2} deduced from their B(E2) in 1974Ro40, with correction by using adopted T{-1/2}=13 ps {I3}. Other: +0.17 {I31}, from g-factor=+0.05 {I9} by transient field technique using T{-1/2}=18 ps in 1989Be22 and corrected by using adopted T{-1/2}. Other: +0.10 {I6} in 2014StZZ compilation, as quoted from 1974Ro40 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$285.3|g to 11/2- and 812.1|g from 1345 level which has L(p,d)=1 (from 0+) together favor 7/2- for 533 level and 3/2- for 1345 level. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$L(d,p)=L(p,d)=L(d,t)=2 from 0+; L(p,t)=2 from 1/2+; spin=3/2 from |g|g(|q) in {+123}I |e decay (1969Se09). But spin=5/2 from |g(|q) anisotropy in 1979Sc13 in {+123}I |e decay is inconsistent. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(d,p)=L(p,d)=2 from 0+; spin=3/2 from |g(|q) anisotropy in {+123}I |e decay (1979Sc13) 
T$from DSAM in (p,n|g) (1990Ja01). 


level_energy_unit: KEV
level_comment:
E$this level in (d,p) should be a different level from 919.8 in ({+11}B,p3n|g), since it would require L(d,p)=(7) for J{+|p}=(13/2-) if same, which is unlikely 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2 from 1/2+; primary 5892.7|g from 1/2+ in (n,|g) E=th; 437.6|g to 1/2+ cannot be E2 or M2 (|DJ=2) based on RUL 
T$from DSAM in (p,n|g) (1990Ja01). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
E$from (p,t). Other: 1211.9 {I7} from (d,p) could also correspond to the 1212.5 level 
J$L(p,t)=(3) from 1/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E$other: 1853.7 {I6} from (d,p) 
J$L({+3}He,|a)=(2) from 0+ for possible 1850 doublet; 976.3|g o (7/2-) 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
E$weighted average of 2066 {I25} from ({+3}He,|a) and 2050 {I15} from (p,t). This level could correspond to the 2065.6 level in (d,p) 
J$L({+3}He,|a)=L(p,t)=4 from 0+ 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$adopted value from this study as weighted average of 190 ps {I30} (1953Gr07), 186 ps {I20} (1963Sc12) and 199 ps {I10} (1968Ra02), with all measured using (ce 88.46|g)(ce 159.00|g)(t). 
MOMM1$from integral perturbed angular correlation (IPAC) in 1970Ro31 and adopted T{-1/2}=196 ps {I10}, based on original value of 0.72 {I12} in 1970Ro31 using T{-1/2}=199 ps {I10} from 1968Ra02. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
T$adopted value from this study as unweighted average of 119.3 d {I1} (1992Co11), 119.7 d {I1} (1970EmZY) and 118.6 d {I9} (1987Ja13). Others: 117 d {I6} (1965An05), 104 d (1951Hi80), 121 d (1951Co34) 
MOMM1$value from 1987Ni11 using nuclear magnetic resonance of oriented nuclei, sign from 1973Si26 with |m=-1.00 {I5} measured using nuclear orientation with gamma detection (1973Si26). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$from B(E2)|^=0.018 {I5}, adopted |d(E2/M1)=+0.079 {I11} 
BE2$weighted average of 0.021 {I5} (1975An16), 0.015 {I6} (1969Ga25) and 0.018 {I5} (1955Fa40) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)|^=0.21 {I3}, adopted |d(E2/M1)=-2.1 {I1} and branching ratio 83.2% {I5} for 439.7|g (1974Ro40). Other: 1.23 ps {I21} from DSAM in 1973ErZS 
BE2$unweighted average of 0.24 {I3} (1975An16), 0.27 {I3} (1970Se03), 0.15 {I5} (1969Ga25) and 0.17 {I2} (1974Ro40). 
MOMM1$from g-factor=0.34 {I6} by IMPAC using T{-1/2}=27 ps {I3} deduced from their B(E2)|^ in 1974Ro40, with correction by using adopted T{-1/2}=22 ps {I4}. Other: +0.66 {I28}, from g-factor=+0.36 {I15} by transient field technique using T{-1/2}=27 ps in 1989Be22 and corrected by using adopted T{-1/2} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$spin=5/2 from particle-|g(|q) in 1989Be22 
T$from B(E2)|^=0.27 {I5}, adopted branching ratio 69.8% {I8} for 505.1|g 
BE2$unweighted average of 0.35 {I4} (1975An16), 0.36 {I3} (1970Se03), 0.17 {I7} (1969Ga25) and 0.20 {I2} (1974Ro40) 
MOMM1$from g-factor=0.040 {I25} by IMPAC using T{-1/2}=18 ps {I2} deduced from their B(E2)|^ in 1974Ro40, with correction by using adopted T{-1/2}=13 ps {I3}. Other: +0.17 {I31}, from g-factor=+0.05 {I9} by transient field technique using T{-1/2}=18 ps in 1989Be22 and corrected by using adopted T{-1/2} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$B(E2)|^ deduced by 1975An16 from their measured yield of 528.8|g and |g-branchings for 528.8|g and 687.7|g from 1972Au10 evaluation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+ 
T from Coul. ex. Other: 4.5 ps {I5} ((|g,|g)) B(E2)=0.567 {I5}. 2001Ra27 evaluation gives 6.23 ps {I7}. 
MOMM1$from transient field integral perturbed angular correlation (2007St24); other: +0.56 {I6}, +0.62 {I8} from ion implantation perturbed correlations, +0.66 {I6}, +0.52 {I6} from transient field integral perturbed angular correlations (1988Du10,1985ThZx,1989Ra17,1981Sh15). See also 2005St24 compilation. 
MOME2$from Coulomb excitation reorientation, weighted average of -0.46 {I10}(1974Ba45),-0.49 {I8}(1974La05) and -0.41 {I8} (1975Kl07) (1989Ra17). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L=2 in (p,t); Coulomb excitation; |g|g(|q) in {+124}Sb |b{+-} decay (60.20 d) and (n,|g) 
T Other: 0.4 ps {I2}(Coul. ex.) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J L=3 in (|a,|a'), (p,p') and |g|g(|q) in {+124}Sb |b{+-} decay (60.20 d) 
T from Coul. ex.: others 100 ps {I5} from |b-|g(centroid shift) (1971BeWP) 
$B(E3) from T{-1/2}. B(E3)=0.12 {I4} (2002Ki06, evaluation). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J L=0 in (d,p) from 1/2+ and |g(|q) in (n,n'|g); 1989GoZK gave 2 or 3 to the spin from |g(|q) but the A{-2} and A{-4} values are consistent with |DJ=0 or 1 to 2+ state. 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: FS
level_comment:
J log| {Ift}=7.49 from 2-; |g(|q) in (n,n'|g); probable E1 |g from capture state suggests negative parity 
T from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J L=2 in (d,p) from 1/2+; |g to g.s.; |g-excitation from 0+ 
T{-1/2}=0.23 ps {I7} if J=1, T{-1/2}=0.21 ps {I7} if J=2 from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
J |g-excitation from 0+; |g to 3- 
T{-1/2}=33 fs {I5} if J=1, T{-1/2}=30 fs {I5} if J=2 from (|g,|g') 


level_energy_unit: KEV
level_comment:
L=2,C{+2}S=0.71 for 2600+2620 level in 1972Au02. The 2600+2620 level in 1972Au02 may be the same as 2618 level in 1995Ge06. 


level_energy_unit: KEV
level_comment:
E reported by 1995Ge06 as 3086.7 {I9} with a comment that the peak happens to be positioned at the edge of the focal plane detector 


level_energy_unit: KEV
level_spin_parity: 1+,0+
level_uncertain: S
level_comment:
E$ statistical uncertainty=0.025 keV, systematic uncertainty=0.1 keV. S(n)=9423.97 {I17} (2003Au03, mass evaluation) 
J$ s-wave capture in {+123}Te, g.s. J|p=1/2+. The 0+ component is estimated as 0.7% by 2006Vo09 


level_energy_unit: KEV
level_comment:
$RELATIVE=130 {I4} 
L=2 and (2J+1)C{+2}S=0.87 for 2320 level in 1977Li05 
$These could correspond to the 2321.6 or 2326.6 levels 


level_energy_unit: KEV
level_comment:
$RELATIVE=17.7 {I19} 
L=(0) and (2J+1)C{+2}S=0.02 for 2730 level in 1977Li05 
$These could correspond to the 2730.6 or 2738.1 levels 


level_energy_unit: KEV
level_comment:
$RELATIVE=63 {I9} 
L=2 and (2J+1)C{+2}S=0.13 for 2859 level in 1977Li05 
$These could correspond to the 2853.2 or 2860.0 levels 


level_energy_unit: KEV
level_comment:
$RELATIVE=42 {I3} 
L=2 and (2J+1)C{+2}S=0.30 for 3220 level in 1977Li05 
$These could correspond to the 3206.6, 3231.2 or 3239.1 levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T weighted average of 4.0 ps {I10} SbCl{-3} source (1961Ak02), 4.6 ps {I8} SbH{-3} source (1963Zi02), 3.1 ps {I23} self-absorption (1963Zi02), 4.8 ps {I6} {+124}SbI{-3} source (1968Sc13) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
$d|s/d|W=13 
Observed (d,d') only. 1970Sh14 proposed this state as a possible member of the 2-phonon triplet with J|p=(0+) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)=0.568 {I5} (for + sign of interference term), 0.566 {I5} (for - sign of interference term) (1975Kl07). Others: 0.47 {I4} (1970Ch14); 0.571 {I11} (for - sign), 0.568 {I11} (for - sign) (1974Ba45); 0.561 {I24} (1977Sa04); 0.48 {I1} (|a,|a') 0.46 {I2} ({+3}He,{+3}He') (1979Sa05) 
Q=-0.41 {I8} (for + sign) or -0.16 {I8} (for - sign) 
Q from 1975Kl07; others: -0.49 {I8} (for + sign), -0.28 {I8} (for - sign) (1974La05); -0.46 {I10} (for + sign), -0.11 {I10} (for - sign) (1974Ba45) 
g factor=0.26 {I10} (1981Sh15) 
T from B(E2)=0.567 {I5} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E From 1979Sa05 
B(E3) from 1979Sa05; others: <0.15 (1970Ch14), <0.45 (1963Ha20) 
T from B(E3) and |g-branching to g.s.=0.0059 {I2} (adopted |g's) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1 From NMR (1977Bu29); value relative to |m for {+2}H (1977Bu29). See also 2005St24 compilation. 
$<r{+2}>{+1/2}=4.7198 fm {i18} (2004An14, evaluation). 
J Optical spectroscopy J=1/2 (1976Fu06); L=0 in (d,p) 
Configuration=(|n 3s{-1/2}) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J L=2 in (d,p), ({+3}He,|a); M1+E2 |g to 1/2+ 
T From weighted av of |g|g(t), X|g(t), ce|g(t),(ce)(ce)(t): 1.55 ns {I3} (1967Vo02), 1.475 ns {I10} (1968Ho05), 1.486 ns {I9} (1970Be47), 1.50 ns {I8} (1970Ba69), 1.51 ns {I5} (1972Sa08), 1.45 ns {I3} (1970Ma20), 1.41 ns {I4} (1971Bo13). Other: 1.32 ns {I21} (1964Ro21); charge state dependence (1995At01,1997At01) 
MOMM1 From Moss (1975Bo51); value relative to |m for {+125}Te. See also 2005St24 compilation. 
MOME2 From Moss (1977La03); value relative to Q for {+129}I. See also 2005St24 compilation. 
Configuration=(|n 2d{-3/2}) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
MOMM1 From radiative detection of NMR (1980Ge02); value relative to |m=+0.605 {I4} for {+125}Te 36-keV level. See also 2005St24 compilation. 
MOME2 From Mossbauer detection of oriented nuclei (1987Be36); value relative to Q=-0.31 {I2} for {+125}Te 36-keV level. 2006Si40 gave +0.02 {I17} from laser spectroscopy. See also 2005St24 compilation. 
J L=5 in (d,p), ({+3}He,|a); M4 |g to 3/2+ 
T From 1978La21. Others: 58 d {I4} (1988GeZS), 58 d {I1} (1965An05), 58 d {I4} (1949Hi27) 
Configuration=(|n 1h{-11/2}) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
J M1+E2 |g to 11/2-, E1 |g from 7/2+ 
T From {+125}Sb |b{+-} decay 
MOMM1 From integral PAC (1970Cr07). See also 2005St24 compilation. 
MOME2 From integral PAC (1976Va28); value relative to Q=-0.31 {I2} for {+125}Te 36-keV level. See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 1/2+, L=2 in (d,t), (t,d), ({+3}He,|a) 
T From B(E2) in Coul. ex. (1975Be04) 
MOMM1$From transient field IPAC (1989Be22). Others: +1.0 {I3} from transient field IPAC (2007St24), +0.59 {I9} from ion implantation PAC (1974Ro40). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in (d,t), log| {Ift}=8.04 from 7/2+ 
T From B(E2) in Coul. ex. (1975Be04). Other: 18.8 ps {I25} in {+125}Sb |b{+-} decay 
MOMM1$From transient field IPAC (1989Be22). Others: +0.85 {I23} from transient field IPAC (2007St24), +0.80 {I23} from transient field IPAC (1985Gr17). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J L=3 in (d,t), ({+3}He,|a); |g|g(|q) in {+125}Sb |b{+-} decay 
T From {+125}Sb |b{+-} decay 
MOMM1 From integral PAC (1971Ro17). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in (d,p), log| {Ift}=6.94 from 7/2+ 
T$from B(E2) in Coul. ex. (1975Be04). Other: 40 ps {I25} in {+125}Sb |b{+-} decay 
MOMM1 From transient field IPAC (1989Be22). Other: -0.5 {I7} from transient field ipac (1989Ra17) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T From weighted average of |b|g(t), |bce(t): 0.695 ns {I15} (1968Ko08), 0.68 ns {I3} (1969Ho42), 0.76 ns {I2} (1970Be47), 0.68 ns {I3} (1970Ma20), 0.65 ns {I3} (1970Be51), 0.704 ns {I21} (1972Sa33), 0.67 ns {I4} (1972Be21), 0.647 ns {I8} (1992De26); Other: 0.87 ns {I8} (1966In02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T From adopted levels. Others: 19 ps {I3} |b|g(t) (1970Be47), 14 ps {I6} |bce(t) (1970Ma20), 26 ps {I8} |b|g(t) (1972Sa08) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T From {+125}Sb |b{+-} decay. Others: 1.45 ns {I3} (1970Ma20), 1.58 ns {I15} (1953Gr07), 1.3 ns {I4} (1958Al98) 


level_energy_unit: KEV
level_comment:
There is a possibility that 3334-keV level in 1969Gr24 is the same level as reported in 1998Ho16 as 3330-keV level. 


level_energy_unit: KEV
level_comment:
L=3 is in conflict with L=2 in (d,t) and ({+3}He,|a). C{+2}S=0.027,0.016. No |s(|q) plot is shown for this level. 


level_energy_unit: KEV
level_comment:
L=2 is in conflict with the property of |g depopulations in (n,|g). C{+2}S=0.007,0.004. No |s(|q) plot is shown for this level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T |?1.5 ns for charge state 44+, |<1.5 ns for charge state 45+, 1.8 {I4} ns for charge state 46+, 5.9 {I5} ns for charge state 47+, 11.0 {I25} ns for charge state 48+ (1997At01) 


level_energy_unit: KEV
level_comment:
S Placement of 0.009 as ({+3}He,|a) in 1984Ro14 seems to be misprinted, because the level energy and cross section are reported in (d,t), not in ({+3}He,|a). 


level_energy_unit: KEV
level_comment:
J=13/2- suggested from combined CCBA analysis in 1984Ro14, which is in disagreement with 15/2- in adopted levels 


level_energy_unit: KEV
level_comment:
1984Ro14 report 1654-keV level with L=(2+5) and C{+2}S=0.08+0.02. Evaluators assume that the 1654-keV level is a doublet of 1643-keV and 1662-keV levels. 


level_energy_unit: KEV
level_comment:
1984Ro14 report 1819-keV level with L=2+4 and C{+2}S=0.11+0.22. Evaluators assume that the 1819-keV level is a doublet of 1814-keV and 1826-keV levels. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$weighted av. of +0.68 {I3} (2007St24, 2020StZV), +0.62 {I8} (1988Du10), +0.68 {I6} (1985ThZX).(transient field technique). Others: +0.64 {I2} (2017St11) using recoil-in-vacuum method and calibration data for Te isotopes (excluding the uncertainty in the parametrization), +0.66 {I2} (2017St11) using calibration data without {+125}Te 3/2+ state, +0.38 {I6} (1981Sh15). 
Q from 2016St14, 2021StZZ 
J E2 |g to 0+ 
T$from B(E2)|^=0.471 {I6} in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from (n,n'|g). Other:0.78 ps {I+25-15} from B(E2)=0.0042 {I10} in Coulomb excitation. 
J E2 |g to 0+. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(p,t)=3. B(E3)=0.117 {I20} in Coulomb excitation. B(E3) and T{-1/2} imply a branching to gs of 0.075% {I13}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+. 
E (p,t) reports 2430 and 2440 keV states, but the assignment of two states seems to be questionable. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: PS
level_comment:
J$|g(|q) and linear pol. in (n,n'|g); negative parity is ruled out by |d(2064.77|g) and T{-1/2}, inconsistent with L(d,p)=(3+5) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T weighted av of 13.5 ns {I10} (1971Ke20), 10.6 ns {I10} (1983Go02) and 10.0 ns {I5} (1998Zh09); other 13 ns {I6} (1970Wa13). All data are from |g(t) 
J |g(|q) in (|a,2n|g) and E2 |g to 8+ 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T unweighted av of 66 ps {I3} from (|?600|b)(|?700|g)(t) (1975Ba46) and 69 ps {I2} from (1370-1500|b)(695|g)(t) (1975So09). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T from (1200|b)(|?700|g)(t) (1975Ba46); other: 0.15 ns {I2} from (610<E|b<720)(695|g,720|g)(t) (1975So09). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)|^=0.471 {I6} 
$B(E2)|^:from weighted av of 0.479 {I11} (1974Ba45), 0.487 {I35} (1967St16), 0.510 {I25} (1970LaZM), 0.457 {I14} (1977Sa04), 0.467 {I7} (1975Kl07), others; 0.420 {I40} (1968La26), 0.532 {I37} (1958St32), 0.32 {I6} (1956Te26). 
Q=-0.28 {I10} or -0.20 {I10} 
Q:from 1974Ba45 for + or - sign of interference term. others: -0.40 {I10} or -0.24 {I8} (1967St16), -0.20 {I9} or -0.10 {I9} (1975Ra24), -0.14 {I11} or +0.02 {I11} (1975Kl07) (for + or - sign of interference term, respectively). 
g(2+)=+0.338 {I17} 
$from 2007St24. others: +0.318 {I10} (2017St11) using recoil-in-vacuum method and calibration data for Te isotopes, +0.332 {I9} (2017St11) using calibration data excluding {+125}Te, 0.31 {I4} (1988Du10), 0.31 {I8} (reanalyzed value by 1974Hu01 from IMPAC data reported by 1969He11), 0.19 {I3} (1981Sh15). 
T from B(E2)|^=0.471 {I6} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
B(E2)|^=0.23 {I10} 
B(E2)|^:(2+ to 4+) was deduced from observation of a weak 693|g in (667|g)(|g) coin (1967St16). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2)|^=0.0042 {I9} 
$B(E2)|^:from weighted av of 0.004 {I1} (1970LaZM) and 0.0047 {I15} (1962Ga13). 
T$for I|g(1420|g)=6.66% {I18} 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.16 
E,S$unresolved from 2391 group, but cross section could be extracted at 5|' by line-fitting procedure 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.15 
$Normalized strength=0.04 (2010Bl06) 
$|s(5|')/|s(17|')=21 
J$Angular distribution in 2010BlZY suggests dominance by L=0 transirion. 
E,S$Three states at 2577.8, 2578.5 and 2585.5 keV could contribute to d|s/d|W (mb/sr). 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.03 
E,S$Probably several unresolved states, such as states at 2731.1 and 2765.8 keV may contribute to d|s/d|W (mb/sr). 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.03 
E,S$Probably several unresolved states, such as states at 2782.7, 2811.6 and 2812.89 keV may contribute to d|s/d|W (mb/sr). 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.03 
E,S$probably several unresolved states, such as states at 2995.9, 2999.4 and 3015.58 keV may contribute to d|s/d|W (mb/sr). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
J$L=2 in (pol d,p); M4 |g from the 88 level which has L=5 in (pol d,p) 
T weighted average of 9.48 h {I13} (1970Bo22), 9.23 h {I13} (1968Qa02), 9.36 h {I20} (1963Ma20), 9.35 h {I10} (1956Kn20), 9.3 h {I5} (1940Se01) 
MOMM1$radiative detection of NMR (1989Ra17); value relative to |m=+0.605 {I4} for the 36 level of {+125}Te 
Configuration=(|n 2d{-3/2}) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M
level_comment:
J see comments on g.s. 
T from 2008Ea01. Others: 109 d {I2} (1965An05), 105 d {I2} (1956Kn20), 115 d (1951Co34), 90 d {I2} (1940Se01) 
MOMM1$radiative detection of NMR (1989Ra17); value relative to |m=+0.605 {I4} for the 36 level of {+125}Te 
Configuration=(|n 1h{-11/2}) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
J L=(5) in (pol d,p),(d,t),({+3}He,|a); D+Q |g from 7/2- 
T from {+127}Sb |b{+-} decay 
MOMM1$integral perturbed angular correlations (1989Ra17) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J L=2 in (pol d,p),(d,t): L=(1) is reported in (t,d), however, later experiments do not confirm L=1 transfer. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Tentatively proposed in 2005Ho15: uncertainty is estimated by evaluator. 1941 (5),and L=(1,2) in 1967Co16 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$T{-1/2}(2|b{+-}) if T{-1/2}({+130}Te)/T{-1/2}({+128}Te)=3.52|*10{+-4} \ {I11} and T{-1/2}({+130}Te)=2.7|*10{+21} {I1} (1992Be30,1993Be04). Others: 2.2|*10{+-24} {I3} for T{-1/2}({+130}Te)/T{-1/2}({+128}Te)=3.52|*10{+-4} {I11} and T{-1/2}({+130}Te)=7.9|*10{+20} {I10} (1996Ta04). <8.6|*10{+22} y (2000Al26), >1.1|*10{+23} y to g.s. (2003Ar02), >8.8|*10{+18} y to g.s., >1.3|*10{+18} y to 443 (2003Ki08), <3.11|*10{+19} y (2006Zu02), 5.4|*10{+19} y to g.s. (2007Bl15), 1.7|*10{+20} y to g.s. (2009Da16), 1.7|*10{+20} y to g.s. (2010Zu02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$weighted average of +0.50 {I6} (1988Du10), +0.62 {I8} (1981Sh15) and +0.70 {I8} (1985ThZX). 
MOME2$from Coulomb excitation reorientation (1978Be10). 1978Be10 also reported -0.14 {I12} as recalculated value. 
J$L(p,p')=2, L(|a,|a')=2, E2 |g to 0+ 
T$from B(E2)=0.377 {I3} in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$E1 |g from 7- 2337 to 1811 and E2 |g's from 1811 to 1497 and from 1497 to 2+ 743 uniquely establish J|p(1811)=6+ and J|p(1497)=4+. 
T$weighted average of 0.48 ns {I3} in {+128}Sb |b{+-} decay (9.01 h) and 0.42 ns {I3} in {+128}Sb |b{+-} decay (10.4 min). 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J$M1+E2 |g from 2395 to 5-, and the E1+M2, M1+E2 cascade from 2395 to 2163 to 2+ uniquely establishes J|p(2395)=4-, J|p(2163)=3+. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: NS
level_comment:
T$from |g(t) in {+238}U({+12}C,F|g), 0.37 |ms {I3} from |g(t) in {+130}Te({+64}Ni,X) and 337ns 59 in 2004Va03. 
J$E2 |g to (8+), high spin ordering in {+238}U({+12}C,F|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$calculated from B(E2) and |a=0.00291. 
BE2$weighted average of 0.376 {I3} (1978Be10), 0.380 {I9} (1977Sa04), 0.378 6 (1975Kl07), 0.387 {I11} (1974Ba45); others: 0.280 {I56} (1956Te26), 0.412 {I33} (1958St32), 0.39 {I3} (1967St16), 0.370 {I5} (1972KlZX). 
G$from {+58}Ni, |g(|q) (2007St24), other: 0.31 {I4} from {+32}S, |g(|q) (1981Sh15). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=741 fs {I+1072-280}(stat) {I+172-124}(syst) from DSA for 754|g (2022Pr02). Deduced mean lifetime=741 fs {I+1086-306} or T{-1/2}=514 fs {I+753-212}. First measurement of lifetime of 1497 level 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=284 fs {I+166-93}(stat) {I+68-46}(syst) from DSA for 1225|g (2022Pr02). Deduced mean lifetime=284 fs {I+179-104} or T{-1/2}=197 fs {I+124-72}. Literature |t=301 fs {I+25-22} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=104 fs {I+28-24}(stat) {I+25-17}(syst) from DSA for 1450|g (2022Pr02). Deduced mean lifetime=104 fs {I+38-30} or T{-1/2}=72 fs {I+26-21}. Literature |t=72 fs {I2} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=257 fs {I+90-62}(stat) {I+61-43}(syst) from DSA for 1609|g (2022Pr02). Deduced mean lifetime=257 fs {I+109-76} or T{-1/2}=178 fs {I+76-53}. Literature |t=198 fs {I+14-10} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=273 fs {I+63-48}(stat) {I+65-44}(syst) from DSA for 1739|g (2022Pr02). Deduced mean lifetime=273 fs {I+91-65} or T{-1/2}=189 fs {I+63-45}. Literature |t=290 fs {I+80-50} (2012Hi10) 
J$no assignment in {+128}Te Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=420 fs {I+43-37}(stat) {I+100-68}(syst) from DSA for 1751|g (2022Pr02). Deduced mean lifetime=420 fs {I+109-78} or T{-1/2}=291 fs {I+76-54}. Literature |t=290 fs {I+80-50} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=167 fs {I+58-43}(stat) {I+40-27}(syst) from DSA for 1887|g (2022Pr02). Deduced mean lifetime=167 fs {I+71-51} or T{-1/2}=116 fs {I+49-35}. Literature |t=137 fs {I+15-14} (2012Hi10) 
J$1+,2+,3+ in {+128}Te Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=481 fs {I+854-225}(stat) {I+116-78}(syst) from DSA for 1900|g (2022Pr02). Deduced mean lifetime=481 fs {I+862-238} or T{-1/2}=333 fs {I+598-165}. Literature |t=230 fs {I+78-120} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=93 fs {I+67-44}(stat) {I+23-15}(syst) from DSA for 1963|g (2022Pr02). Deduced mean lifetime=93 fs {I+71-47} or T{-1/2}=64 fs {I+49-33}. Literature |t=115 fs {I8} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: (1),2+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=347 fs {I+349-141}(stat) {I+85-56}(syst) from DSA for 2869|g (2022Pr02). Deduced mean lifetime=347 fs {I+359-152} or T{-1/2}=241 fs {I+249-105}. Literature |t=410 fs {I+180-99} (2012Hi10) 
J$(1,2+) in {+128}Te Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=244 fs {I+112-70}(stat) {I+58-40}(syst) from DSA for 2891|g (2022Pr02). Deduced mean lifetime=244 fs {I+126-81} or T{-1/2}=169 fs {I+87-56}. Literature |t=270 fs {I+42-34} (2012Hi10) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$this value is for 0|n|b|b decay mode at 90% credibility interval (C.I.), and was derived using Bayesian analysis. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
MOMM1$NMR on oriented nuclei (1979Ge04). Other: 0.66 {i5} (1973Si06, low-temperature nuclear orientation following decay of {+129}Te) 
MOME2$Mossbauer detection of oriented nuclei (1987Be36). 
J$L=2 in (t,d), ({+3}He,|a), (p,d) and (d,p); log| {Ift}=5.8 to 5/2+ level in {+129}I forbids 1/2+ 
$Configuration=|n2d{-3/2} 
T$weighted average of 68.7 min {i4} (1963Br18), 69.5 min {i5} (1963Ha23), 70.2 min {i3} (1970Bo22). Others: 72 min {i3} (1940Se01), 67.5 min {i10} (1963Ma20), 1956Gr10, 1948Wa13, 1939Ab02 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_lifetime_info: ;ISO=M1
level_comment:
$Configuration=|n1h{-11/2} 
%IT,%B-$deduced by the evaluators from the measured ratio I|b(to g.s.)/I|b(to 27 level in {+129}I)=0.58 {i18} in equilibrium between the 33.6-d and 69.6-M {+129}Te activities (1964De10,1969Di01), together with the {+129}I level scheme from 1976Ma35. 
MOMM1$NMR on oriented nuclei (1980Ge02). Others: -1.10 {I3} (2006Si40, laser spectroscopy on resonant ionization of laser-desorbed atoms at COMPLIS facility in ISOLDE-CERN), -1.15 {I5} (1973Si26, low- temperature nuclear orientation following decay of {+129}Te isomer). 2014StZZ cite 1979Ge04 reference incorrectly 
MOME2$laser spectroscopy on resonant ionization of laser-desorbed atoms at COMPLIS facility in ISOLDE-CERN (2006Si40) 
$Charge radius measurement: 2006Si40 
J$L=5 in (t,d), ({+3}He,|a), (p,d) and (d,p); M4 |g to 3/2+ 
T$weighted average of 33.3 d {i1} (1953Pa25), 33.8 d {i3} (1963Ha23), 34.1 d {i2} (1965An05,1972Em01), 33.2 d {i5} (1970Bo22), 33.52 d {i12} (1971Ba28). Others: 32 d {i2} (1940Se01), 1948Wa13, 1951Co34, 1956Gr10, 1963Ma20, 1965Br34 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_comment:
J$gammas to 5/2+ and 11/2-; 5/2 ruled out from |g(|q) of 500|g from 1727 level. 9/2 from |g(|q) of 683|g. 525|g(|q) from 1754 level fits 7/2 somewhat better 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_comment:
J$|DJ=1, dipole |g to 19/2(-); log| {Ift}=6.1 from (19/2-); possible configuration=|pg{-7/2}d{-5/2}~#nh{-11/2} (1998Zh09) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: NS
level_comment:
T$|g(t) in ({+64}Ni,X|g). 
J$|DJ=1, dipole |g to (21/2-); level systematics of {+128}Te and {+130}Te (1998Zh09) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L=2 and analyzing power in (pol d,t). 
E$2395 in (p,d) may correspond to 2377.4, 2379.5 and/or 2379.5 levels, but more likely to 2416 from level populations in similar (d,t) and (p,d) reactions, and energy matching 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: D
level_comment:
%IT,%B-$deduced by the evaluators from the measured ratio I|b(to g.s.)/I|b(to 27 level in {+129}I)=0.576 {I18} (1965Be26), 0.34 (1968Go34) in equilibrium of 33.6-d and 69.6-min {+129}Te activities, along with the {+129}I level scheme. Uncertainty in the ratio from 1965Be26 is estimated in 1972Ho55 Nuclear Data Sheets evaluation 


level_energy_unit: KEV
level_comment:
E$level reported in 2013Ka04 and 2013KaZZ with d|s/d|W=5.16 mb/sr at 5|' and 1.11 mb/sr at 22.5|' 
S$if 1h{-11/2}. 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_comment:
J$from |g(|q). 5/2 ruled out by |g(|q) of 500|g from 1727 level; 9/2 less favorable from |g(|q) of 525|g from 1754 level but not ruled out 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$d|s/d|W=33 
E$1212.7 {i3} in (d,p) (2003Wi02), 1217 (2013Ka04,2013KaZZ) 
J$3/2+,5/2+ quoted by 2013Ka04, 2013KaZZ from earlier Nuclear Data Sheets (1996Te01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=55 
E${ 1303.5 {I3}} in (d,p) 
E,J$1302 with J|p=7/2+,9/2+ given in 2013Ka04, which on the basis of J|p assignment seems to correspond to 1319 level here 


level_energy_unit: KEV
level_comment:
$d|s/d|W=146 
E,J$1752 with J|p=5/2+ given in 2013Ka04, which on the basis of J|p assignment seems to correspond to 1779.9 level here 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$3077 {I15} with (3/2+,5/2+) assignment and 3089.3 {I5} with no J|p assignment in Adopted Levels 
$d|s/d|W=0.12 mb/sr (5|'), 0.017 mb/sr (22.5|') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
J$measurement (1933Ra02) by optical-spectroscopy method 
T$0.79|*10{+21} y {I10} (from geochemical method,1996Ta04). The value is treated as a lower limit, as proposed by 2000Al26. 
T$Neutrinoless |b|b decay: no evidence found by 2000Al26 with T{-1/2}>1.44|*10{+23} y (at 90% confidence level). 2000Al26 (also 1998Al19,1994Al49,1994Al25,1992Al09) used bolometric method with an array of 20 tellurite crystals with a total mass of 6.8 Kilograms. 2000Al26 also found no evidence for neutrinoless decay to first 2+ or excited 0+ states in {+130}Xe. 
T$Geochemical methods: 0.79|*10{+21} y {I10} (1996Ta04), >1.25|*10{+21} y (1988Li11), 2.60|*10{+21} y {I28} (1983Ki02,1983Ki03), 2.51|*10{+21} y {I24} (1972Sr03), 2.03|*10{+21} y {I30} (1969Al22), 2.2|*10{+21} y {I6} (1968Ki02) and |<1.00|*10{+21} y {I12} (1986Li10), 1.0|*10{+21} y {I3} (1986Ri02), 0.97|*10{+21} y {I11} (1975He04), 0.82|*10{+21} y {I6} (1966Ta02), 1.4|*10{+21} y (1950In03,1949In03). See also 1993Be04, 1992Be30, 1988Mi13, 1987Be13, 1985HoZN, 1984Fi16, 1980Zd02, 1980Zd03, 1980Zd01, 1970Ki21, 1969Va39, 1967Ge12, 1967Ki04. 
$Compilation and analysis of |b|b data: 2001Ej01, 1998Kl25 
THEORY (BB DECAY): 2000Ve05, 2000Pa25, 2000Pa47, 2000Ne05, 2000Ki24, 2000Fa14, 2000Ba54, 2000Ba68 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$|g(|q,H) in Coul. ex. (1988Du10). See other measurements in Coulomb excitation 
MOME2$reorientation method in Coul. ex. for positive sign of the interference term (1976Bo12). See other details in Coulomb excitation 
BE2$from Coul. ex. 
J$L(p,p')=2; E2 |g to 0+ 
T$from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
J$systematics, probable |nh{-11/2}{+-2} configuration in N=78,80 and Z=52,54 nuclides 
T$from timing of 182|g in {+239}Pu(n,F|g) (2001Ge07). Other: 4.2 |ms {I9} (from delayed |g rays in ({+64}Ni,X|g),1998Zh09) 
E$x<25 keV (2001Ge07). Other: x<90 keV (1998Zh09) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
B3$from (p,p'). Others: 0.10 (n,n'); 0.06 (|a,|a') 
J$L(p,p')=L(|a,|a')=3 
E$from (p,p') 
BE3$from Coul. ex. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E$from 1969ScZX 
|G{-|g}=0.06 eV {I3}, |G{-|g0}=0.03 eV {I1} (1974Wo05) 
|G{-|g0}/|G{-|g}=0.45 {I10} (1974Wo05), 0.41 {I7} (1969ScZX) 
J$from |g(|q) and |g(lin pol) (1974Wo05) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (10+)
level_lifetime_unit: US
level_comment:
T$from observation of delayed 6+ to 4+ to 2+ cascade between beam bursts (1998Zh09). This value is in disagreement with 1.90 |ms {I8} from 2001Ge07 
E$x<90 keV. Other: x<25 keV (2001Ge07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.296 {I6} (1976Bo12), 0.290 {I11} (1974Ba45), 0.302 {I16} (1970LaZX). Others: 0.30 {I3} (1970Ch01), 0.34 {I3} (1962Ga13,1958St32), 0.26 {I5} (1956Te26) 
G$from |g(|q,H) in Coul. ex. (1988Du10,1981DuZX). Others: +0.33 {I8} (1985Gr17), +0.29 {I6} (1981Sh15), +0.32 {I9} (1974Hu01,reanalyzed value of 1969He11) 
MOME2$from reorientation method in Coul. ex. for positive sign of the interference term (1976Bo12). Others: -0.14 {I12} (1974Ba45), -0.08 {I8} (1974La05), -0.19 {I15} (1970Ch01). For negative sign of the interference term, the values are: -0.07 {I12} (1976Bo12), -0.09 {I12} (1974Ba45), 0.00 {I8} (1974La05), -0.12 {I15} (1970Ch01) 
T$from B(E2) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: US
level_lifetime_info: ;ERR=?
level_comment:
T$From 2004Br19; 4.2 |ms 9 in 1998Zh09 (from observation of delayed 6+ to 4+ to 2+ cascade between beam bursts). 
E$From 2004Br19; 2649+x in 1998Zh09, where x<90 keV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$ listed as <2.08 ps in table III and >2.01 ps in table IV of 2008Hi17. It should be >2.01 ps according to e-mail reply of May 18, 2009 from the first author of 2008Hi17 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$105.4 fs {I14} in table IV of 2008Hi17 is incorrect. It should be 104 fs {I7} according to e-mail reply of May 18, 2009 from the first author of 2008Hi17 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
T$451 fs {I+42-35} in table IV of 2008Hi17 is a misprint, it should be 457 fs {+42-35} according to e-mail reply of May 18, 2009 from the first author of 2008Hi17 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2) is listed by 2013St24 as an average of two measurements: 0.280 {I12} at 343 MeV and 0.292 {I10} at 390 MeV. But the compiler obtains a weighted average of 0.287 {I8} and unweighted average of 0.286 {I6} 
T$deduced by 2013St24 from B(E2) value 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$this value is for 0|n|b|b decay mode at 90% confidence level (C.L.), and was derived from a Bayesian analysis (2018Al13). Authors' frequentist analysis gave T{-1/2}>2.1|*10{+25} y at 90% C.L. and a sensitivity of >0.76|*10{+25} y at 90% C.L. Combining the earlier results of >2.7|*10{+24} y (CUORE-0 value from 2015Al20: Phys. Rev. Lett. 115, 102502; and >2.8|*10{+24} y (CUORICINO value from 2011An08: Astropart. Phys. 34, 822), authors obtain T{-1/2}>1.5|*10{+25} y at 90% C.L. using profile likelihood or Bayesian approach, and >2.2|*10{+25} y using frequentist technique. 
$Corresponding upper limit of Majorana neutrino mass m{-|b|b}<0.11-0.52 eV (2018Al13) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$level energy held fixed in least-squares adjustment 
T$2022Hi01 take value from {+130}Te Adopted Levels in the ENSDF database (May 2001 update) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=2600 fs {I+2400-900} (2022Hi01); Doppler shift from 1125.2|g(|q) distribution for E(n)=3.3 MeV 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$2022Hi01 take value from {+130}Te Adopted Levels in the ENSDF database (May 2001 update) 
J$|g(|q) data in 2022Hi01 consistent with J=7 or 5, the former assignment is supported in authors' excitation function data and comparison with SMC 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=120 fs {I10} (2022Hi01) 
$|g branching ratio from excitation function data (2022Hi01) 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=670 fs {I+80-70} (2022Hi01) 
J$|g(|q) data in 2022Hi01 consistent with J=1 or 2, the former assignment is supported in authors' excitation function data and comparison with SMC, but 2+ is not ruled out completely 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=860 fs {I+200-140} (2022Hi01) 
J$|g(|q) in (n,n'|g) rules out J=3 
$|g branching ratios deduced by 2022Hi01, using SMC iteratively to obtain a consistency with |g(|q) and excitation functions data and comparison with SMC for the 2330.7, 4+ level, since the 349.35|g could not be resolved from the strong 348.5|g from 1981.4 keV level. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J$303.9|g(|q) allows J=3,4,6,(5); 258.8|g(|q) allows J=5,6. Excitation function data compared with SMC strongly supports 6 


level_energy_unit: KEV
level_spin_parity: (6+,7-)
level_comment:
J$286.2|g(|q) supports J=5,6 and 331.1|g(|q) supports J=3,4,6; with no multipole mixing for J=6 in both cases. Excitation functions data compared with SMC give spin above 6 or 7. Systematics of even-A Te isotopes support second 6+ near this energy. However, J=7 cannot be ruled out 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=380 fs {I+50-40} (2022Hi01) 
$An 861.6|g reported earlier in |b{+-} decay was weakly observed in the present work but with a threshold of E(n)>2.6 MeV 
J$816.4|g(|q) consistent with 4+; excitation function of the 816.4|g consistent with 4+ from SMC for an 80% branch 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=820 fs {I+130-100} (2022Hi01) 
J$2+ supported by |g(|q) for all the transitions which are also seen in appropriate |g|g-coin gates. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=1800 fs {I+2600-700} (2022Hi01) 
J$from shell-model predictions (Fig. 13 in 2022Hi01) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=740 fs {I+180-130} (2022Hi01) 
J$|g(|q) forbid 4+, and J=5 and 6 less likely as large angular momentum transfer not supported in the present work. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=300 fs {I20} (2022Hi01) 
J$993|g(|q) and 1742|g(|q) allow J=2,3,4; excitation function data are above the SMC, but closest to J=2. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=500 fs {I+190-110} (2022Hi01) 
J$from shell-model prediction (Fig. 13 in 2022Hi01) 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=100 fs {I10} (2022Hi01) 
J$positive parity is preferred from comparison of excitation function data to SMC, and from systematics of stable Te isotopes 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J$614|g(|q) favors J=4 or 6, with non-zero mixing ratios. 576|g(|q) consistent with J=2-5, with no mixing for J=4 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$two separate levels of 2733.4, 4+ and 2736.3, 5+ are proposed in the present work based on excitation functions and |g|g-coin data, in contrast to only one level 2736, 4+ in {+130}Te Adopted Levels in the ENSDF database (2001 update) 
T$measured mean lifetime |t=220 fs {I+60-40} (2022Hi01) 
J$1145.2|g(|q) and 1894.0|g(|q) suggest J=4; positive parity from population in |b decay. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E$two separate levels of 2733.4, 4+ and 2736.3, 5+ are proposed in the present work based on excitation functions and |g|g-coin data, in contrast to only one level 2736, 4+ in {+130}Te Adopted Levels in the ENSDF database (2001 update) 
J$from 1103.4|g(|q) and excitation function for 920.9|g 1894.0|g(|q) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=150 fs {I10} (2022Hi01) 
J$1155.8|g(|q) gives J=1,2,3, while the excitation function and SMC slightly favor positive parity. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=740 fs {I+140-110} (2022Hi01) 
J$859.3|g(|q), 1111.7|g(|q) and 1905.3|g(|q) strongly support J=3. Negative parity is from previous scattering experiments 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=360 fs {I40} (2022Hi01) 
J$no pure multipole decays from |g(|q) strongly support J|p=3+ 
$A previously assigned 949.8|g from this level is not observed in the present experiment, except possibly with a threshold above E(n)=3.1 MeV (2022Hi01). 


level_energy_unit: KEV
level_spin_parity: (5,6,7)-
level_comment:
J$669.7|g(|q) gives J=3-7 with preference for J=7, and then for J=5, with negative parity supported for all the spin choices. Excitation functions agree well with SMC for J=5 
$A previous tentatively assigned 1137|g from this level is not supported in the present experiment, although a small contribution cannot be excluded, while an 1135.6| is observed in this work with a threshold above E(n)=3.1 MeV (2022Hi01). 


level_energy_unit: KEV
level_spin_parity: (7-)
level_comment:
J$680.6|g(|q) gives J=3-7; excitation function and SMC support J=7 
$A previously assigned 635.6|g from this level is neither supported by excitation function nor by the |g|g-coin data in 2022Hi01 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=250 fs {I+30-20} from DSA for 1949.7|g (2022Hi01) 
J$1949.7|g(|q) gives J=2,3,(1); 903.4|g(|q) and 1201.2|g(|q) give J=0-4; excitation functions and SMC for 903.4|g and 1949.7|g support J=2. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$1018.0|g(|q) excludes J=4, pure E2 to 1815, 6+ level; excitation function and SMC support J=5, using the listed branching ratios 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=740 fs {I+650-250} (2022Hi01) 
J$1323.3|g(|q), 1368.6|g(|q), and 2117.2|g(|q) support J=4; |g to 2+ suggests positive parity 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=280 fs {I+70-50} (2022Hi01) 
J$2314.8|g(|q) gives J=4,(2,3); 1566.0|g(|q) gives J=1,2,3,(4); 1521.6|g(|q) gives J=2-5; excitation function and SMC support J=4; |g to 2+ suggests positive parity. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=660 fs {I+7000-340} (2022Hi01) 
J$from 1291.2|g(|q) and excitation function compared with SMC; |g to 5- 


level_energy_unit: KEV
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$at 90% confidence level for 2|n decay to first excited 0+ state in {+130}Xe (2019Al27). For 0|n decay mode, T{-1/2} > 7.9|*10{+23} y for decay to first excited 0+ state in {+130}Xe (2019Al27). Authors also combine their results with those from CUORICINO experiment to obtain T{-1/2}{+0|n} > 1.4|*10{+24} y and T{-1/2}{+2|n} > 2.5|*10{+23} y, both for decay to the first excited state in {+130}Xe. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=5 ps {I3} from 794|g-840|g(t) (2022Ku31). Compared with T{-1/2}=2.30 ps {I5} (|t=3.32 {I7}) in the ENSDF database; and measured B(E2)(up)=0.291 e{+2}b{+2} {I10} from Coulomb excitation, which translates to |t=3.38 ps {I12} (2013St24: Phys. Rev. C 88, 051304(R) (2013)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=6 ps {I4}, from combined lifetimes for the first 2+ and 4+ states |t=11 ps {I3} and 14 ps {I3} from 182|g-840|g(t), subtracting lifetime of the first 2+ state (2022Ku31). Authors compared their result to |t=4.7 ps {I10} (from B(E2) in Coul. Ex. in 2020CoZY: EPJ Web of Conf. Vol. 232 (2020)); and tau=1.395 {I+342-237} (stat) {I+150-124} (syst) (from DSA in 2022Pr02: Phys. Rev. C 105, 034319) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
$Measured mean lifetime |t=13.5 ns {I8} and 14.5 ns {I2} from 331|g-182|g(t) (2022Ku31). Compared with T{-1/2}=9.8 ns {I5} (|t=14.1 ns {I7}) in the ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
$Measured mean lifetime |t=155 ns {I24} from 502|g-331|g(t) (2022Ku31). Compared with T{-1/2}=115 ns {I8} (|t=166 ns {I11}) in the ENSDF database. Newer measurement: T{-1/2}=186 ns {I11} (2004Va03: Phys. Rev. C 69, 024316); 110 ns {I5} (2014As01: Eur. Phys. Jour. A50, 2) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E$from 2004Br19 (Eur. Phys. Jour. A20, 145); and 2014As01 (Eur. Phys Jour. A50, 2) 
$Measured mean lifetime |t<120 ns (2022Ku31). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
E$from 2004Br19 and 2014As01. 
$Measured mean lifetime |t=2.76 |ms {I12} from (794|g+840|g)(t) (2022Ku31). Compared with T{-1/2}=1.90 |ms {I8} (|t=2.74 |ms {I11}) in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$For 0|n|b|b from 2020Nu01 with a 90% C.L. The authors stated that T{-1/2} > 1.5|*10{+25} yrs (90% C. L.), combined with the CUORE-0 (2015Al20, 2016Al11) and Cuoricino (2011An08) results. 
T$7.9 {I1} (stat) {I2} (syst) |* 10{+20} yrs for 2|n|b|b from 2020Nu01. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=1395 fs {I+342-237}(stat) {I+150-124}(syst) from DSA for 794|g (2022Pr02). Deduced mean lifetime=1395 fs {I+373-268} or T{-1/2}=967 fs {I+259-186}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=283 fs {I+93-65}(stat) {I+30-26}(syst) from DSA for 1046|g (2022Pr02). Deduced mean lifetime=283 fs {I+98-70} or T{-1/2}=196 fs {I+68-49}. Literature |t=470 fs {I+40-30} (2008Hi17) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=439 fs {I+255-135}(stat) {I+46-42}(syst) from DSA for 1125|g (2022Pr02). Deduced mean lifetime=439 fs {I+259-141} or T{-1/2}=304 fs {I+180-98}. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=960 fs {I+186-139}(stat) {I+99-89}(syst) from DSA for 1142|g (2022Pr02). Deduced mean lifetime=960 fs {I+211-165} or T{-1/2}=665 fs {I+146-114}. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
$Measured mean lifetimes |t=523 fs {I+145-100}(stat) {I+55-48}(syst) from DSA for 1351|g; 615 fs {I+151-107}(stat) {I+65-67}(syst) from DSA for 2191|g, with weighted averaged |t=576 fs {I+100-78}(stat) {I+61-53}(syst) (2022Pr02). Deduced averaged mean lifetime=576 fs {I+117-94} or T{-1/2}=399 fs {I+81-65}. Literature |t=590 fs {I50} (2008Hi17) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
$Measured mean lifetimes |t=90 fs {I+20-18}(stat) {I+9-8}(syst) from DSA for 1443|g; 79 fs {I+24-20}(stat) {I+8-7}(syst) from DSA for 2283|g, with weighted averaged |t=85 fs {I+15-13}(stat) {I+9-8}(syst) (2022Pr02). Deduced averaged mean lifetime=85 fs {I+18-15} or T{-1/2}=59 fs {I+13-10}. Literature |t=150 fs {I10} (2008Hi17) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=446 fs {I+64-52}(stat) {I+48-40}(syst) from DSA for 816|g (2022Pr02). Deduced mean lifetime=446 fs {I+80-66} or T{-1/2}=309 fs {I+56-46}. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=581 fs {I+76-63}(stat) {I+60-55}(syst) from DSA for 1627|g (2022Pr02). Deduced mean lifetime=581 fs {I+97-84} or T{-1/2}=403 fs {I+67-58}. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=1749 fs {I+2058-651}(stat) {I+184-162}(syst) from DSA for 1688|g (2022Pr02). Deduced mean lifetime=1749 fs {I+2066-671} or T{-1/2}=1212 fs {I+1432-465}. 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=112 fs {I+132-68}(stat) {I+12-10}(syst) from DSA for 942|g (2022Pr02). Deduced mean lifetime=112 fs {I+133-69} or T{-1/2}=78 fs {I+92-48}. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=279 fs {I+33-28}(stat) {I+30-26}(syst) from DSA for 1741|g (2022Pr02). Deduced mean lifetime=279 fs {I+45-38} or T{-1/2}=193 fs {I+31-26}. 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=66 fs {I+31-25}(stat) {I+6-6}(syst) from DSA for 2689|g (2022Pr02). Deduced mean lifetime=66 fs {I+32-26} or T{-1/2}=46 fs {I+22-18}. 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=109 fs {I+102-59}(stat) {I+11-10}(syst) from DSA for 2743|g (2022Pr02). Deduced mean lifetime=109 fs {I+103-60} or T{-1/2}=76 fs {I+71-42}. 


level_energy_unit: KEV
level_spin_parity: (2+,3)
level_lifetime_unit: FS
level_comment:
$Measured mean lifetimes |t=811 fs {I+283-177}(stat) {I+83-74}(syst) from DSA for 859|g; 664 fs {I+63-55}(stat) {I+68-60}(syst) from DSA for 1905|g, with weighted averaged |t=679 fs {I+61-53}(stat) {I+69-62}(syst) (2022Pr02). Deduced averaged mean lifetime=679 fs {I+92-82} or T{-1/2}=471 fs {I+64-57}. 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
$Measured mean lifetimes |t=165 fs {I+159-79}(stat) {I+18-15}(syst) from DSA for 1156|g; 307 fs {I+55-44}(stat) {I+33-28}(syst) from DSA for 1950|g, with weighted averaged |t=296 fs {I+51-41}(stat) {I+32-27}(syst) (2022Pr02). Deduced averaged mean lifetime=296 fs {I+60-49} or T{-1/2}=205 fs {I+42-34}. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
$Measured mean lifetime |t=250 fs {I+13-12}(stat) {I+28-22}(syst) from DSA for 1478|g (2022Pr02). Deduced mean lifetime=250 fs {I+31-25} or T{-1/2}=173 fs {I+22-17}. 
E$from 2022Pr02. Other: 3360 {I10} in ENSDF from (p,p') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GT
level_comment:
T$this value is for 0|n|b|b decay mode at 90% credibility interval (C.I.), and was derived using Bayesian analysis. The authors also reported the same half-life limit at an earlier publication (2022Ad14). 
$Corresponding upper limit of Majorana neutrino mass m{-|b|b}<0.090-0.305 eV. s 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$this value is for 2|n|b|b decay mode and reported as 7.9|*10{+20} y {I1} (stat) {I2} (syst) (2019Ca21). Authors also report limit for 0|n|b|b decay mode as T{-1/2} > 1.3|*10{+25} y at 90% C.L. (2019Ca21) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
$Configuration=|nh{-3/2}{+-1} 
J$log| {Ift}=7.1 to 877, 1/2+ in {+131}I 
MOMM1$NMR on orientated nuclei; {+125}Te(36-keV state) standard 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$NMR on orientated nuclei; {+125}Te(36-keV state) standard. Other:(-)1.123 {I7} (1998Wh05) 
$%IT from 2002Re30. Others: of 22.2 % {I16} (1975Ja03), 18.3 % {I12} (1961Be20), 21 % (1955He88) 
$Configuration=|nh{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
$Configuration=|nh{-11/2}~#(2{++} {+130}Te core) from 1998FoZY 
J$E2 |g from (17/2)- level, M1,E2 |g to 11/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+,(7/2)+
level_comment:
J$(7/2+,9/2+) from L(d,p)=(4) (2003To08); 5/2+,7/2+ from L(d,p)=2 (1967Gr21) and L(t,p)=2. |=(9/2+) from |g to 3/2+ 
E$1274 {I5} in (t,d) 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: PS
level_comment:
J$E3 |g from (23/2)+ state, E2 |g to (13/2)- 
$Configuration=|nh{-11/2}~#(4{++} {+130}Te core) from 1998FoZY 
T$from IT Decay (93 ms), |g|g(t) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$7/2-,5/2+ from Ay in (d,p), L(d,p)|=0; |g to (9/2-) suggests J|p|=5/2+; L(t,d)=0 in (t,d) discrepant 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
$Configuration=|nh{-11/2}~#(7{+-} {+130}Te core) from 1998FoZY 
J$from systematics and decay pattern 
T$from |g|g(t) IT Decay (93 ms) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$from L(d,p)=2 (2003To08) and log| {Ift}=7.09 from (7/2+) state; L(d,p)=1 (1967Gr21) and (t,d)=(1) discrepant 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
$Total |b{+-}+|g feeding to state is 6.5% {I9} recalculated by evaluators from data from 1965Sa23 and current T{-1/2}=33.25 h and %IT 
T$from adopted levels 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T$from 2002Re30. Other: 1.2 d {I2} (1940Se01) 
$ %IT from 2002Re30. Others: of 22.2 % {I16} (1975Ja03), 18.3 % {I12} (1961Be20), 21 % (1955He88) 
$Configuration=|nh{-11/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
$Configuration=|nh{+2}{-11/2}~#(7{+-} {+130}Te core) (1998FoZY), also =|nh{+2}{-11/2}d{-3/2} (1998Zh09) 
T$from 1998FoZY. T{-1/2}>1 |ms from 1998Zh09 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
$ %IT from ENSDF database 
T$ from timing of 773.7|g and 852.2|g (2008Ea01). Literature value: 30 h {I2}}, 33.25 h {I25}} 
$ |s(thermal)=0.0106 b {I4}} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
T$ from 1983Wa26. Others: 3.26 d {I3} (1965An05), 3.283 d {I19} (1971BaZW), 1974Ca26, 1958Ch28, 1956Fl15, 1951Pa33, 1939Ab02, 1939Ha13 


level_energy_unit: KEV
level_spin_parity: (7)-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M1
level_comment:
J$ E1 |g to 6+; probable configuration=(|nd{-3/2}{+-1})(|nh{-11/2}{+-1}) 
T$ from {+132}Te IT decay 


level_energy_unit: KEV
level_comment:
J$|g to (5)-. 
J$ 2+ IN 2004Hu08 IS INCORRECT AS PER E-MAIL REPLY OF JUNE 23, 2004 FROM AUTHORS OF 2004Hu08 


level_energy_unit: KEV
level_spin_parity: (2+,3,4+)
level_comment:
J$ |g's to 2+ and 4+. From systematics of first 3- states in N=80 isotones and Z=52 isotopes, this level is a possible candidate for the first 3- state in {+132}Te 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$ |g's to (8+) and (7)-; systematics; configuration=|nh{-11/2}{+-2} 
T$ from 2001Ge07. Other: 3.9 |ms {I3} (1979Si18) 


level_energy_unit: KEV
level_comment:
$A level at 3350.6 is established by 2004HuZX with deexciting |g rays of 383.3 and 1425.3, these |g's not reported by 1974Ke06 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$g-factor deduced as weighted average of +0.33 {I18} (the gadolinium backed target) and +0.16 {I28} the iron backed target) (2008Be14). Earlier value of 0.38 {I4} from 2007St25 (Phys Rev C 76, 034307; also 2005St18: Phys Rev Lett 94, 192501) using recoil-in-vacuum technique was more precise but without determination of the sign of g factor. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$ Value of 0.35 {I5} reported in 2005St18: Phys Rev Lett 94, 192501 was updated to 0.38 {I5} in 2007St25: Phys Rev C 76, 034306. It is further revised by 2011Da21 to (+)0.46 {I5} as the B(E2)(up)(g.s. to first 2+) has been corrected (for correct target thickness in 2002Ra21) to 0.216 {I22} from the original value of 0.172 {I17} reported in 2002Ra21: Phys Rev Lett 88, 222501. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ B(E2) has been corrected in 2011Da21 (for correct target thickness in 2002Ra21) to 0.216 {I22} from the original value of 0.172 {I17} reported in 2002Ra21 
T$ deduced by compiler from B(E2)=0.216 {I22} 


level_energy_unit: KEV
level_spin_parity: (11-)
level_comment:
$2016Bi02 note that a 518-keV |g ray from this level reported by 2015Le03 (Acta. Phys. Pol. B46, 637) in delayed |g-ray detection from {+235}U,{+241}Pu(n,F) reaction at PF1B cold-neutron facility at ILL-Grenoble, was not observed in the present experiment 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=5 ps {I3} from 697|g-974|g(t) (2022Ku31). Compared with T{-1/2}=1.83 ps {I18} (|t=2.64 {I26}) in the ENSDF database; and |t=2.15 ps {I+25-20} from B(E2)(up)=0.216 {I22} from Coulomb excitation in 2011Da21 (Phys. Rev. C 84, 061306(R) (2011)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$Measured mean lifetime |t=61 ps {I5} from 163|g-697|g(t) (2022Ku31); adopted from three different values: 60 ps {I5} and 55 ps {I5} from 103|g-697|g(t) using two different methods of analyses; and 62 ps {I8} from combined |t=67 ps {I7} combined for the first 2+ and 4+ states, and subtracting |t=5 ps {I3} for the first 2+. Compared with |t|<58 ps from |g|g(t) in 2013Ro07 (Acta Phys. Pol. B44, 403) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
$Measured mean lifetime |t=192 ns {I5} from 151|g-103|g(t) (2022Ku31). Compared with T{-1/2}=145 ns {I8} (|t=209 ns {I11}) in the ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
$Measured mean lifetime |t=41.1 |ms {I13} from 151|g(t) (2022Ku31). Compared with T{-1/2}=28.1 |ms {I15} (|t=40.5 |ms {I22}) in the ENSDF database; and with |t=41.3 |ms {I+17-16} in 2017Ki09 (Eur. Phys. J. A53, 162) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M3
level_comment:
$Measured mean lifetime |t=5.4 |ms {I12} from 926|g(t) (2022Ku31). Compared with T{-1/2}=3.70 |ms {I9} (|t=5.34 |ms {I13}) in the ENSDF database; and |t=5.10 |ms {I13} in 2017Ki09 (Eur. Phys. J. A53, 162) 
$A 798|g with implied mult=[E3] has been reported in 2001Ge07 (Phys. Rev. C63, 054315). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MIN
level_comment:
MOMM1,MOME2$using laser spectroscopy technique (2006Si40) 
J$ |m; systematics in neighboring odd-A nuclei 
T$|b|g(t) in 1965Pr08 
CONF$possible |n(d{-3/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$using NMR/ON technique (1998Wh05). Other: |m=-1.15 {I9} using laser spectroscopy technique (2006Si40) 
MOME2$using laser spectroscopy technique (2006Si40) 
J$334.3|g M4 to (3/2+). 
T$from |g(t) 1968Be64. Other: 53 min {I4} (1957Al35) 
CONF$possible |n(h{-11/2}{+-1}) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: ?
level_comment:
J$from 1113.1|g to (1/2+), 1421.3|g to (3/2+), population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2+)
level_comment:
J$from 1728.6|g to (3/2+), 632.4|g to (7/2+,5/2-), population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_comment:
J$from 1579.2|g to (11/2-), 817|g to (7/2+,5/2-), population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2,9/2-)
level_comment:
J$from 927.7|g to (7/2+,5/2-), 523.4|g to (5/2-,7/2,9/2-), population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_comment:
J$from 1877.2|g to (11/2-), 1115.2|g to (7/2+,5/2-) population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2)
level_comment:
J$from 1236.0|g to (7/2+,5/2-), 308.2|g to (5/2-,7/2,9/2-), population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_comment:
J$from 2416.2|g to (11/2-), 1654.2|g to (7/2+,5/2-), population in {+133}Sb |b{+-} decay (J{+|p}=(7/2+)). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: MIN
level_comment:
E$from adopted levels. In 2001Bh06, the level energy was put equal to zero in calculations of energies of higher levels (Fig. 3). 
T$from 2001Bh06 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
B(E2) from Coulomb Excitation. 
J$from systematics of N=82 Nuclei 
T$from B(E2) value; other: <0.17 ns (1980Ka31) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$E2 |g to 4+ 
T$weighted average of 165 ns {I6} (2001Mi22), 164 ns {I1} (1995Om01), 163 ns {I7} (1970Jo20), 163 ns {I4} (1974ClZX), 170 ns {I4} (1974Su04), 161 ns {I4} (1976ChZD). Other: 196 ns {I7} (1974Bl03), 197 ns {I20} (2004Hw02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_lifetime_unit: NS
level_comment:
$ g factor=0.36 {I+23-9} for hyperfine magnetic field(Te-Fe)=69 T; 0.70 {I+55-38} for 34 T {I16}; 1.31 {I+31-14} for 19 T {I6} 
T$from 'adopted levels' dataset for {+134}Te in ENSDF database 
T$ 2008Go28 quote |t=1.96(6) ns, it should be 1.96(16) ns 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ B(E2) has been corrected in 2011Da21 (for correct target thickness in 2002Ra21) to 0.114 {I13} from the original value of 0.096 {I12} reported in 2002Ra21 
T$ deduced by compiler from B(E2)=0.114 {I13} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$measured by 2017Ur03 from decay curve for 115|g. Value is 164.1 ns {I9} in {+134}Te Adopted Levels in the ENSDF database (July 2004 update) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
T$from sum of 1064|g and 2865|g time distributions in HPGe fitted with an exponential decay plus constant background (2021Ha13). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
MOMM1,MOME2$from hyperfine structure study using laser spectroscopy at COMPLIS-ISOLDE-CERN facility. 
J$this assignment is also consistent with N=83 isotones (7/2- g.s. in {+137}Xe, {+139}Ba, {+141}Ce, {+143}Nd, {+145}Sm) as well as with strong |b transition from (7/2+) g.s. in {+135}Sb to this state, possibly from |pg{-7/2} to |nf{-7/2} orbitals 
$Configuration=|nf{-7/2} 
T$weighted average of 18.6 s {I4} (1985Sa15), 19.2 s {I2} (1974Gr29), 18 s {I1} (1973Bo42), 18 s {I2} (1969De13). Others: 11 s {I3} (1970De15), 16.6 s {I9} (1969ScZY). Method: |g timing 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$|g's to (7/2-) and (3/2-); log| {Ift}=6.55 from (7/2+); systematics support 5/2 with configuration=|nf{-5/2} 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$|g to (7/2-); log| {Ift}=6.5 from (7/2+); systematics support 9/2 with probable configuration of |nh{-9/2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$from systematics, 2002Ra46 state that this tentative level may be a better candidate for |nf{-5/2} state than the 1127 level. 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
MOMM1 DPAC (1989Ra17 quote from abstract Particle normalization-13 in Sixth International Conference on Hyperfine Interactions, Groningen, Netherlands, July 1983.). See also 2005St24 compilation 
T$from delayed |g timing, weighted average of 0.512 |ms {I22} (2001Mi22) and 0.510 |ms {I20} (1980Ka30). 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g's to (19/2-) and (21/2-); probable configuration=|pg{-7/2}|ph{-11/2}|nf{-7/2} (1997Bh06) 
T$ |g|g(t) in {+248}Cm SF decay (2001Fo02) 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_comment:
J$|g's to (19/2-) and (21/2-); possible (21/2+) member of configuration=|pg{-7/2}|ph{-11/2}|nf{-7/2} (2001Fo02) 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
J$|g to (25/2+); probable configuration=|pg{-7/2}{+2}~#|ni{-13/2} or configuration=|p(g{-7/2}|h{-11/2})~#|nh{-9/2} (1997Bh06) 


level_energy_unit: KEV
level_spin_parity: (31/2-)
level_comment:
J$|g's to (25/2+) and (27/2+); possible configuration=|pg{-7/2}{+2}~#|nf{-7/2}{+2}~#|nh{-11/2}{+-1} (1997Bh06) 


level_energy_unit: KEV
level_spin_parity: (35/2-)
level_comment:
J$|g to (31/2-), it should Be noted that the dipole (M1) transition to (33/2-) level is not reported, which is expected if this level is a member of the magnetic-rotational band 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
E(n) (I(n)): 1042 {I2} (88), 1458 {I2} (100) (1979Kr03). It is possible that 1042 transition is misplaced, it may be from 5810 level. See {+135}Sb |b{+-}n decay ({+134}Te in A=134) for details 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
E(n) (I(n)): 499 {I3} (12), 1201 {I2} (54), 1322 {I4} (24), 1618 {I5} (10) (1979Kr03). 499 transition is probably misplaced as the |g-ray study (1989Ho08) suggests no feeding of second 6+ state in {+134}Te 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
$Configuration=(|pg{-7/2}{+2}){-2+}~#|nf{-7/2} (1980Ka30); 2+ refers to first 2+ state in {+134}Te 
T$|g|g(t) (1980Ka30) 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
$Configuration=(|pg{-7/2}{+2}){-4+}~#|nf{-7/2} (1980Ka30); 4+ refers to first 4+ state in {+134}Te 
T$|g|g(t) (1980Ka30) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$ 1554.89 {I16} in 'adopted levels' 
$Configuration=(|pg{-7/2}{+2}){-6+}~#|nf{-7/2} (1980Ka30); 6+ refers to first 6+ state in {+134}Te 
T$from delayed |g timing, weighted average of 0.512 |ms {I22} (2001Mi22) and 0.510 |ms {I20} (1980Ka30). Others: 1970Gr38, 1970Jo20, 1974ClZX, 1977SeZJ, 1978Ba47 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$ from 2001Fo02, but no details available for this measurement. Probably estimated from |g|g(t) 
Probable configuration=|pg{-7/2}|ph{-11/2}~#|nf{-7/2} (1997Bh06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
$RELATIVE INTENSITY=1.00 {I8} 
$Probable |np{-3/2} 
$Relative intensity=1.00 {I7} in {+134}Te({+9}Be,{+8}Be) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-)
level_comment:
$RELATIVE INTENSITY=0.22 {I2} 
$Probable |np{-1/2} 
$Relative intensity=0.92 {I4} in {+134}Te({+9}Be,{+8}Be) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-)
level_comment:
$RELATIVE INTENSITY=0.17 {I3} 
$Probable |nf{-5/2} 
$Relative intensity=0.59 {I4} in {+134}Te({+9}Be,{+8}Be) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_comment:
$RELATIVE INTENSITY=0.13 {I5} 
$Probable configuration=|pg{-7/2}{+2}|nf{-7/2} 
$Relative intensity=0.22 {I2} in {+134}Te({+9}Be,{+8}Be) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2-)
level_comment:
$RELATIVE INTENSITY=0.042 {I12} 
$Probable |nh{-9/2} 
$Relative intensity=0.054 {I13} in {+134}Te({+9}Be,{+8}Be) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2+)
level_comment:
$RELATIVE INTENSITY=0.22 {I2} 
E$possible |ni{-13/2} from systematics of N=83 isotones 
$Relative intensity=0.04 {I3} in {+134}Te({+9}Be,{+8}Be) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2-)
level_lifetime_unit: PS
level_comment:
T$weighted average of 552 ps {I22} from K-xray -325|g(t) and 571 ps {I22} from 50|g-325|g(t) (2019Si32) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$weighted average of 17.66 s {I9} (1993Ru01), 17.5 s {I2} (1978Cr03), and 17.5 s {I4} (1976Lu02). Others: 18.1 s {I3} (1978Ze08), 25 s {I5} (1977Ru04), 24 s {I2} (1974Gr29). 
$%|b{+-}n: weighted average of 1.31 {I5} (1993Ru01) and 1.34 {I13} (2012Ma63). Others: 1.7 {I8} (updated value of 2.0 {I10} from 1978Cr03 by 1993Ru01 based on new measurement of {+136}Sb %|b{+-}n value), 0.7 {I4} (1977Ru04) 
$|d<r{+2}>=0.389 fm{+2} {I19} (2013An02,2006Si40). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 607|g to 0+. 
T$from B(E2) and adopted |g-ray properties. Other: 42 ps {I8} (preliminary result from centroid shift technique in {+136}Sb |b{+-} decay). 
BE2$weighted average of 0.181 {I15} (2017Al06) and 0.122 {I18} (2011Da21), both from Coulomb Excitation. Value from 2011Da21 supersedes value of 0.103 {I15} from 2002Ra21 which was calculated using an incorrect value for the target thickness. 
MOMM1$from recoil-in-vacuum (2017Al06). Sign is not measured and from systematics. 
MOME2$from reorientation method (2017Al06) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$962|g to 2+, systematics of N=84 isotones 
$B(E2)(607 to 1568) < 0.09 in Coulomb Excitation (2017Al07). 
BE2$from Coulomb Excitation (2017Al07). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(n)({+136}Te)=4768 {I3} (2017Wa10), with x < 5150 from Q(|b{+-})({+136}Sb decay)=9918 {I6} and S(n)({+136}Te) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.181 {I15} (2017Al06) and 0.122 {I18} (2011Da21). Value from 2011Da21 supersedes value of 0.103 {I15} from 2002Ra21 which was calculated using an incorrect value for the target thickness. 
T$deduced by evaluator from B(E2) and adopted gamma-ray properties. 
G$from recoil-in-vacuum (2017Al06). Sign is not measured and from systematics. 
MOME2$from reorientation method (2017Al06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE2$from B(E2)|_=0.060 {I9} (2017Al06) 
T$deduced by evaluator from B(E2) and adopted gamma-ray properties. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$%|b{+-}n is beta-delayed one-neutron emission or P{-1n}, deduced by 2018Ca22 from measurement of |b, neutron and (|b)n-time correlated events. Previous experimental values: 1.34 {I13} (2012Ma63: J. Instrum. 7, P08029); 1.31 {I5} (1993Ru01: At. Data Nucl. Data Tables 53, 1); 1.7 {I8} (1978Cr03: Z. Phys. A287, 45); 0.7 {I4} (1977Ru04: J. Inorg. Nucl. Chem. 39, 753). Compilations and evaluations give: 1.26 {I20} (2002Pf04: Prog. Nucl. Energy 41, 39); 1.31 {I5} (J. Liang et al., unpublished, 2018) 
T$from {+136}Te Adopted Levels in the ENSDF database (April 2018 update) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from B(E2)=0.191 {I26} (2019Va03). Other: 23 ps {I11} from lineshape analysis in 2019Va03 compared to GEANT4 simulations. This gives a B(E2) consistent with the result from Coulomb excitation yields in 2019Va03, but with considerably larger uncertainty. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
T from 1985Sa15. Other: 2.1 s {I5} (1975As04); see also T{-1/2}=3.5 s {I5} (1969ScZY), |?4 s (1977Pf01) 
%|b{+-}n: evaluated result from 1993Ru01 
J$From syst of N=85 isotones expected configuration=(|n f{-7/2}){+3} (2000Ur01,2002Ur04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+137}Te g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared with half-life of 2490 ms {I50} from 1985Sa15 (Zeit. Phys. A321, 255), the same value adopted in Oct 2006 ENSDF update of {+137}Te. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
J$from Adopted Levels of {+137}Te in ENSDF database 
T$from |g(t) in 2022Si16. 
%B-N$deduced by 2022Si16 from measured I|g of 87.3|g in {+136}I, assumed from |b{+-}n decay of {+137}Te; considered as a lower limit by 2022Si16 due to possible unobserved weak transitions. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 1975As04, weighted average of T{-1/2} values from |b{+-} and delayed neutrons. Other: 1.15 s {I3} from a preliminary analysis of decay curve in 2006KeZZ. 
$Theoretical T{-1/2}=7.9 s, %|b{+-}n=1.5 (2003Mo09) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared with half-life of 1400 ms {I400} from 1975As04 (Nucl. Phys. A247, 359), the same value adopted in Sept 2017 ENSDF update of {+138}Te. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
$Theoretical T{-1/2}=2.10 s, %|b{+-}n=26.6 (2003Mo09). 
$Theoretical T{-1/2}=0.115 s, %|b{+-}n=0.7 (2016Ma12). 
J$from the systematic trend of yrast excitations in N=87 isotones. Alternate assignment of 5/2- is less likely since the 271 level fits the systematics for the 9/2- levels in N=87 isotones and the 271|g has a stretched dipole character. 2007Ji14 give 5/2- from their theoretical calculations, also the same in 2012Au07 from systematics. 1997Mo25 give 3/2- from theoretical predictions 
T$1.6 s {I3} from analysis of composite integral decay curve for {+139}Sb, {+139}Te, {+138}Te and {+137}I background (2007ArZQ thesis, same value also cited in 2011Ar18). The statistics is very weak in the decay curve shown in figure 77 of 2007ArZQ. In the opinion of the evaluators this half-life should be viewed with caution. Systematic value=0.5 s (2012Au07), and theoretical half-life=2.10 s (2003Mo09). In 2006KeZZ (GSI annual report), half-life is listed as 598 ms {I20} from integral |b counting, but in e-mail reply of Sept 29, 2008 from K.L. Kratz, the half-lives in the report were pointed out as questionable due to calibration issues. Perhaps based on this report, value of 0.60 s is listed in KAPL 2009 Wall Chart of Nuclides. 
$Configuration=|n2f{-7/2}{+3}~#|ni{-13/2}{+2}(0+) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$from the systematic trend of yrast excitations in N=87 isotones. Alternate assignment of 5/2- less likely since the 271 level fits the systematics for the 9/2- levels in N=87 isotones and the 271|g has a stretched dipole character. 
$Configuration=|n2f{-7/2}{+3}~#|ni{-13/2}{+2}{-0+} 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+137}Te g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Tentative half-life of 1.6 s {I3} is adopted in Oct 2016 ENSDF update of {+139}Te, from 2007ArZQ (Thesis, O. Arndt, Mainz Univ.). Another tentative value is 598 ms {I20} in 2006KeZZ (Annual Rept. GSI 2006-1, p.154). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 335 {I14} ms from 2006KeZZ (|b(t), quoted as preliminary) and 350 {I5} ms from 2017Mo19 (from analysis of |g(t) decay curve of summed 342, 740, and 875 |g transitions in {+140}I, and using maximum likelihood method for fitting a function of a single-component exponential decay and a constant background) 
$Branching ratios were not measured for this nucleus. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<Q(|b{+-})-S(n)({+140}Te) or x<8200 {I600}, where Q(|b{+-})=12640 {I600} and S(n)=4440 {I60}, both from 2017Wa10 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_comment:
E$y<Q(|b{+-})-S(2n)({+140}Te) or x<5620 {I600}, where Q(|b{+-})=12640 {I600} and S(2n)=7020 {I60}, both from 2017Wa10 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Half-life of 348 ms {I5} is adopted in Nov 2018 ENSDF update of {+140}Te, based on 350 ms {I5} from 2017Mo19 (Phys. Rev. C 96, 014325); a value derived from the same experiment as in 2020Wu04 (see caption for Table I in 2020Wu04); and and a tentative value of 335 ms {I14} from 2006KeZZ (Annual Rept. GSI 2006-1, p154) 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$From 2020Wu04 fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods and confirmed by the method of gating the |b-delayed |g rays. Data analysis included contributions from the parent, daughter and grand-daughter decays, as well as a constant background. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Measured |s=300 pb (2010Oh02), systematic uncertainty|?30% 
T$ lower limit from time-of-flight in 2010Oh02. Actual half-life is expected to be much longer as suggested by the calculated values of 75 ms (1997Mo25); 67 ms (2002Pf04). 
J$ 3/2+ predicted in calculations of 1997Mo25 
$ Probability of misidentification of {+145}I isotope<0.001% (2010Oh02) 
$Calculated %|b{+-}n=15.91, %|b{+-}2n=1.59 (1997Mo25). Calculated %|b{+-}n=16.3 (2002Pf04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+143}Te g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$There is no measurement of any decay mode, but %|b{+-}=100 is assigned by inference as this is the only decay mode allowed, followed by possible delayed neutron emissions. 
$Theoretical T{-1/2}=59.2 ms, %|b{+-}n=25.9, %|b{+-}2n=0.08 (2003Mo09) 
$Theoretical T{-1/2}=28.7 ms, %|b{+-}n=26.8, %|b{+-}2n=0.2 (2016Ma12) 
E$observed fragments are assumed to correspond to the ground state 
T$from time-of-flight, half-life is implied as >300 ns. From systematic trend of decreasing half-life with increasing neutron number in an isotopic chain, half-life is expected to be <0.5 s from known half-lives of 1.4 s for {+138}Te, 2.49 s for {+137}Te and 17.6 s for {+136}Te 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay 
$Theoretical %|b{+-}n=25.9, %|b{+-}2n=0.08 (2003Mo09: Phys. Rev. C67, 055802) 
$Theoretical %|b{+-}n=26.8, %|b{+-}2n=0.2 (2016Ma12: Phys. Rev. C93, 025805) 
$A total of 44 counts were assigned to {+144}Te, 16 events with spectrometer setting on Sn, and 28 events with setting on Te. Probability of misidentification of this isotope is <0.01% for both the settings (2018Sh11). 
$Production |s=2.7 pb for Te setting, with 30% systematic uncertainty on |s value. 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08 (Jour. Phys. Soc. Japan 87, 014202). Actual half-life is expected to be much longer as suggested by the theoretical values of 59.2 ms (2003Mo09) and 28.7 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+144}Te is expected to be <1.5 s, based on measured half-lives of 2.49 s for {+137}Te, 1.4 s for {+138}Te, and 1.6 s for {+139}Te. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=24.4 ms, %|b{+-}n=21, %|b{+-}2n=1 (2019Mo01) 
$Theoretical T{-1/2}=22.8 ms, %|b{+-}n=40.4, %|b{+-}2n=0.5 (2016Ma12) 
$A total of two counts were assigned to {+145}Te, with the spectrometer setting on Te. Probability of misidentification of this isotope is 0.04% (2018Sh11) 
$Production |s=0.1 pb for Te setting, with 30% systematic uncertainty for |s value 
E$it is assumed that the observed events correspond to ground-state activity. 
J$3/2- from |W{-|n}=3/2- orbital proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 24.4 ms (2019Mo01) and 22.8 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+145}Te is expected to be <100 ms, based on measured half-lives of 193 ms for {+141}Te, 147 ms for {+142}Te, 120 ms for {+143}Te, and 93 ms {I60} for {+144}Te, available in literature. 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: MS
level_comment:
E$the |a decay of {+108}I was observed using the reaction {+54}Fe({+58}Ni,xnyp) E=260 MeV and the Daresbury recoil-mass separator (1994Pa11,1991Pa05). The measurement was performed with the residue implantation detection system. Two |a decay lines were identified by 1991Pa05 at 3730 keV {i25} and 3885 keV {i25} but were not confirmed by 1994Pa11 who report 3947 keV {i5} and state that any lower-energy line would be |<13% of the main 
T$from 1994Pa11. Also reported in 1994Pa12 
J$from systematics 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: US
level_comment:
%A$from 2007Ma35 
J$from comparison between experimental and theoretical proton-decay half-lives using a deformed single particle Nilsson model (1999Ma05). non-favored |a-decay (HF=37 {I12} with r{-0}({+105}Sb)=1.67 {I3}, unweighted average of 1.632 {I14} ({+104}Sn) and 1.70 {I6} ({+106}Te)) to J|p=(5/2+) in {+105}Sb. Note, that J|p=5/2+ (d{-5/2}), if a spherical shape is assumed 
T$unweighted average of 93.5 |ms 3 (2007Ma35) and 92 |ms 1 (2007Pe32). Others: 103 |ms {I5} (1995Ho26), 100 |ms {I5} (1993Se04), 109 |ms {I17} (1987Gi02) and >25 |ms (1984Fa04) 
$E(|a)=3774 keV 20 (2007Ma35). E(p)=813 keV 4 (1995Ho26) and 830 keV 80 (1984Fa04) 
CONF$|p1/2+[420] (g{-7/2}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$proposed by 2007Pe32 based on systematics of odd-A iodine isotopes and self-consistent cranking calculations 
CONF$|p1/2+[420] (g{-7/2}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
J$proposed by 2007Pe32 based on systematics of odd-A iodine isotopes and self-consistent cranking calculation; 548.2|g (E1) to (11/2+) 
CONF$|p1/2-[550] (h{-11/2}). The assignment is tentative 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ it is not clear whether this level corresponds to the g.s. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2+)
level_lifetime_unit: PS
level_comment:
T$from recoil-distance doppler-shift technique using the differential decay curve method and the 594|g (2011Pr12) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (11/2-)
level_uncertain: ?
level_comment:
$The lower intensity of the depopulating 643.4|g, compared to the 593.4|g that feeds this level indicates that this level may be isomeric 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
J$From HF=3.1 {I13} in {+114}Cs |a decay (J{+|p}=(1{++})). It should be noted, however, that the HF value is very sensitive to the r{-0} parameter, which is not well defined in the case of {+114}Cs |a decay 
T$Weighted average of 0.69 s {I4} (|a(t) in 1977Ki11) and 0.65 s {I3} (weighted average of 0.62 s {I2} using |a(t), 0.68 s {I2} using |bp(t) and 0.81 s {I9} using |b|a(t) in 1981Sc17) 
$E|a=3392 {I25} (1977Ki11), 3424 {I15} (1978Ro19), 3444 {I10} (1981Sc17) and 3456 {I5} (1991He21) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$It is not clear, if the g.s. or an isomeric state is populated in {+58}Ni({+58}Ni,|apn|g) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$It is not clear, if the g.s. or an isomeric state is populated 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T$from 1977Ki11: 2.5 s {I2} (tellurium K|a| x ray), 2.3 s {I3} (3120|a), 2.7 s {I2} (266,321,341 |g's) 
J$from syst 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
%A$from 1978Ro19 
%ECP,%ECA$from %|ep/%|a=735 {I80} and %|ep/%|e|a=8.5 {I2} in 1985Ti02 
J$from the predicted |p1/2+[420](d{-5/2}) and |n3/2+[422](g{-7/2}) orbitals near the Fermi surface in 1997Mo25. Note, that J|p=1/2+ and configuration=|p1/2+[420](d{-5/2}) in {+109}I. Assignment is tentative. 
T$weighted average of 3.42 s {I11} from |b+p(t) in 1985Ti02, 2.80 s {I25} from |b+|a(t) in 1985Ti02, 3.3 s {I2} from K{-|a}(t) in 1977Ki11, 3.3 s {I3} from 688.9|g(t) and 786.9|g(t) in 1977Ki11, and 3.7 s {I3} from p(t) in 1977Ki11 
CONF$probably |p1/2+[420](d{-5/2})~#|n3/2+[422](g{-7/2}). The assignment is tentative 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$From |t=124 ps {I30} (value in abstract - confirmed by 1st author of 2018Gi11 (e-mail communication - dated: Nov 13, 2018)). Other value: 124 ps {I20} (in Fig. 1 and text). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_comment:
%A$from 1981Sc17 
E$tentative g.s. assignment for 6.6-s activity (1980GoZX). 
T$from 1980GoZX. Other: 5.9 s {i5} (1979Sc22). 
J$from systematics. All odd-a isotopes have J|p=5/2+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
%B+P$1978Ka17 give theoretical calc for % delayed protons and |a's 
T$from 1977Ki11 
J$log| {Ift}=4.8 to the 0+ {+114}Te 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
T from 1969Ha03, {+115}I |b{++} decay curve; ms 18-s {+115}Xe parent source 
J$from syst of J|p(g.s.) (1977Ek02,1979Au01,1979Ta01) in iodine isotopes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2+)
level_comment:
E $the 318-keV |g ray observed in coin with emission via the {+116}Cs precursor (1978Da07) may correspond with the 322.5|g but the 275.3|g, which also deexcites the 322 level in the scheme of 1973Co32, is not observed by 1978Da07. This level, thus, appears as questionable. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: US
level_comment:
E$low-lying 11/2- states in {+117}I, {+119}I, {+121}I occur, respectively, at 661,687,812 keV (1977Go04,1977Fo03) 
T av of K| x ray, 91|g, 322|g decay curves 
J $in disagreement with the (11/2-) bandhead level observed at 837.5 keV by 1985Pi02 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
J$from adopted levels 
T 1.3 min {I2} (1969Ha03) on-line ms of {+115}Xe produced by 600-MeV p spall. Other: 24 s {I3} (1973LiZB,1974SpZX) on-line ms 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: MIN
level_comment:
MOMM1$static nuclear orientation, (1986Gr06,1987Gr15,1987St20) compatible with the |p[402] 5/2 state with weak component of the |p[413] 5/2 
T$from 1985Le10. Others: 2.2 min {i5} (1974Ha10), 2.4 min {i1} (1969Ha03), 2.4 min {i3} (1969Se05). Other: 1969La33 
J$|p from log| {Ift}=4.8 to (3/2)+, predominately d5/2 orbital (1999Pa13) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
J$9/2+ bandhead level from the 1g9/2 state (1985Pi02), M1 |g to |p=+ 
T$from 1982Ga21. Other: 17.5 ns (1993Wa21) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_comment:
Since the 663-keV transition has no delayed component (T{-1/2}>10 ns), it does not decay directly from the 11/2- bandhead. An unobserved E1 transition (x) between the 11/2- bandhead and the 663-keV 9/2+ level is suggested by 1985Pi02 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
MOMM1$static low-temperature nuclear orientation (1989Ra17) 
T average of 13.9 min {I5} (1965An05), 13.0 min {I3} (1968La18), 14.3 min {I1} (1969Ha03). Others: |?10 min (1957Aa04), 17 min {I2} (1960Za07), 17.2 min {I7} (1965Bu08) 
J from |g(|q) from oriented nuclei; log| {Ift}=6.6 to 2+ 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E 1993Au05 indicated E(level)=90 {I310} as adjusted value 
MOMM1$static low-temperature nuclear orientation (1989Ra17) 
J on-line nuclear orientation (1985Sh16) 
T from 1968La18 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_comment:
E level energy held fixed in least-squares adjustment 
E$y=3528.7+x from its decay to 3528.7 level through a |g-ray of unknown energy 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
MOMM1$static low-temperature nuclear orientation (2005St24) 
J log| {Ift}=5.0 to 3/2+ and 6.6 to 7/2+ 
T weighted av of 19.3 min {I2} (1968Se05) and 18.2 min {I3} (1969La33). Others: 21 min {I1} (1960Za07), 19.5 min {I5} (1965An05), 18 min {I1} (1954Ro03) 25.8 min {I19} (1965Bu08). All data are from {+119}I |e decay 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
MOMM1$differential-perturbed angular distribution of |g rays following reactions (2005St24). Others: +5.45 {I36} (2005St24), 5.36 {I23} (1978VaZY) 
J M1+E2 |g to 7/2+, E2 |g to 5/2+ 
T from |g(t) in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
MOMM1$differential-perturbed angular distribution of |g's following reactions (1989Ra17). Others: +5.45 {I36} (1989Ra17), 5.36 {I23} (1978VaZY) 
T from 1982Da17. Other: 28.8 ns {I10} (1982Ga21) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
J log| {If{+1u}t}=9.27 to 0+ 
T weighted av of 81.0 min {I6} (1965An05) and 81.7 min {I2} (2000Ho19). 81.7 min {I2} is that from 81.5 min {I2} (511|g counting) and 81.9 min {I2} (1523|g counting) (2000Ho19). Others: 78 min {I3} (1965Bu03), 82.8 min {I42} (1968La18), 85 min {I5} (1970Ga32) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J log| {Ift} 6.41 to 6+, M1 |g from (8-) 
E from E|b from (600|g)(|b{++})- and (612|g)(|b{++})-coin in {+120}I |e decay (53 min) 
T from 1968La18. Other: 40 min {I2} (1967La18) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J$from syst of head of the 8- band, based on the configuration=((|p g{-9/2}){+-1}(|n h{-11/2})) in lighter even iodine-isotopes 


level_energy_unit: KEV
level_energy_info: ;OFF=X+953.3
level_spin_parity: (9-)
level_comment:
J$from syst of the bandhead based on configuration=((|p g{-7/2})(|n h{-11/2})) in lighter iodine isotopes 


level_energy_unit: KEV
level_energy_info: ;OFF=X+1016.5
level_spin_parity: (10-)
level_comment:
J$from syst of the bandhead based on configuration=((|p h{-11/2})(|n d{-5/2})) in lighter iodine isotopes 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$ |g(t) (2012MoZZ); uncertainties of 2, 3 and 5 ns are also stated in different places in text of 2012MoZZ. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7-)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J,T$ from Adopted dataset for {+120}I in ENSDF database 
E$ x=320 {I150} from Adopted Levels in ENSDF database. From systematics of 8- states in even-A iodine nuclei, 2012MoZZ suggest and use x=132 {I30} in their level-scheme figure. Uncertainty of 15 keV quoted in 2011AuZZ and 2003Au02 seems incorrect 
$ Configuration=|p9/2[404]~#|n5/2[532] (2012MoZZ) 


level_energy_unit: KEV
level_comment:
J$proposed by 2013Li27 to be a (25+) state, based on spectral behavior of 506-keV transition with gate at 1182 keV. It is also speculated to be an isomer with M3 multipolarity for 506|g 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 7-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
T$from Adopted Levels of {+120}I in the ENSDF database 
E$x=132 {I30} in 2018Mo16. Value is 320 {I150} in {+120}I Adopted Levels in the ENSDF database (Dec 2001 update), deduced from E|b values. 2017Au03 (NUBASE-16) give 320 {I15}, where the uncertainty seems erroneous by a factor of 10. In contrast, 2013Li27 (Chinese Physics Letters 30, 062301) give x=73.2 keV {I18}, based on the connection of the level scheme built on this isomer with the main level scheme. An e-mail reply of June 20, 2018 from C.B. Moon (corresponding author of 2018Mo16) mentioned that no observation of the linking transitions in their experiments would be due seen due to poor statistics, and that they have plans to conduct future experiments, including perhaps conversion electron measurements. 
$Configuration=|p9/2[404]~#|n5/2[532] (2012MoZZ) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$|g(t) (2012MoZZ,2011Mo27,2003Mo22), and as listed in 2018Mo16. Uncertainties of 2, 5 and 10 ns were also stated in different places in text of 2012MoZZ. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$|g(t) (2012MoZZ,2011Mo27,2003Mo22), and as listed in 2018Mo16. Uncertainties of 0.6 ns was also stated in 2012MoZZ. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J$from level-scheme Figure and for final level in supplemental material (2018Mo16), not listed for initial level in authors' Table in supplemental material. 


level_energy_unit: KEV
level_energy_info: ;OFF=Z;ERR=?
level_spin_parity: (25+)
level_lifetime_unit: NS
level_comment:
E$z<30 keV (2018Mo16) 
E$this state interpreted by 2018Mo16 as a noncollective fully aligned oblate structure with possible configuration of |p(g{-7/2},d{-5/2},h{-11/2}~#|n(h{-11/2}{+3}, the three protons and the three neutrons as the valance particles outside the {+114}Sn core. 
T$from |g(t) (2018Mo16), with gates on 506, 872, and 1067 |g rays. The analysis used maximum likelihood method with an exponential decay function and a constant background. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
J from atomic beam J=5/2 (1974EkZX). L=2 in ({+3}He,d) 
T from 1965An05. Others: 1.8 h (1950Ma29), 2.1 h {I1} (1960Za07) 2.07 h {I9} (1964BlZZ), 1.95 h {I17} (1965Bu03), 2.1 h {I1} (1968Jo02) 
MOMM1$NO/S (2005St24); relative to |m=+2.742 {I1} for {+131}I g.s. and |m=+3.088 {I7} for {+132}I g.s. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
J E2 |g to 5/2+, M1+E2 |g to 7/2+; J=9/2 is consistent with being the band head of 9/2+[404] orbital 
T $unweighted average of 9.4 ns {I4} (1982Ga21), 9.5 ns {I4} (1994Ko13) in {+118}Sn({+6}Li,3n|g), and 10.0 ns {I4} in {+121}Sb({+3}He,3n|g) (1982Ha46) 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J M1+E2 |g to 5/2+; possible band head of g{-7/2} band 
T $upper limit was deduced from centroid shift in |g-rf coincidence in {+118}Sn({+6}Li,3n|g) (1994Ko13) 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: NS
level_comment:
T$from recoil-distance in {+114}Cd({+11}B,4n|g) (1994Wa08); other: 0.35 ns {I20} from |g(t) in {+118}Sn({+6}Li,3n|g) (1994Ko13) 
J L=5 in ({+3}He,d) and syst. 


level_energy_unit: KEV
level_spin_parity: (21/2)
level_lifetime_unit: NS
level_comment:
J T{-1/2} is compatible with mult.=M1 or E2, for the 134.8|g, thus J=21/2 is suggested 
T from |g(t) in {+121}Sb({+3}He,3n|g) 
MOMM1 DPAD (2005St24) 


level_energy_unit: KEV
level_spin_parity: (39/2-)
level_lifetime_unit: PS
level_comment:
$Probable admixture of non-collective configuration=((|p 1h{-11/2})(|p 1g{-9/2}){++2}(|n 1h{-11/2}){++2}{-8+}), J|p=39/2- 


level_energy_unit: KEV
level_spin_parity: (43/2-)
level_comment:
$Probable admixture of non-collective configuration=((|p 1h{-11/2})(|p 1g{-9/2}){++2}(|n 1h{-11/2}){++2}{-10+}), J|p=43/2- 


level_energy_unit: KEV
level_spin_parity: (55/2-)
level_comment:
$Probable admixture of non-collective configuration=((|p 1h{-11/2})(|p 1g{-9/2}){++2}(|n 1h{-11/2}){++4}{-16+}), J|p=55/2- 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_comment:
$Probable admixture of non-collective configuration=((|p 1h{-11/2})(|n 1h{-11/2})(|n 1g{-7/2})), J|p=25/2+ 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: NS
level_comment:
T $unweighted average of of 9.4 ns {I4} (1982Ga21), 9.5 ns {I4} (1994Ko13) and 10.0 ns {I4} from {+121}Sb({+3}He,3n|g) (1982Ha46) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
|m: from static nuclear orientation, value relative to {+131}I,{+132}I (1986Gr06,1989Ra17); positive sign (1988As06) 
J log {Ift}=5.19 from 0+ 
T from 1970LaZX. Others: 3.6 min (1951Yo06), 3.4 min {i1} (1952Dr18), 3.5 min (1954Ma75) 


level_energy_unit: KEV
level_spin_parity: 0+,1+
level_lifetime_unit: NS
level_comment:
J log {Ift}=7.04 from 0+, M1 |g to 1+ 
T weighted average of 7.55 ns {i40} from (61.8|g)(K| x ray)(t) and 7.2 ns {i7} from (61.8L+90.5K)(K| x ray)(t) (1973Lo10) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: NS
level_comment:
J M1+E2 |g to 1+ 
T average value of (90.6|g)(K| x ray)(t) and (61.8L+90.5K)(K| x ray)(t) (1973Lo10) 


level_energy_unit: KEV
level_spin_parity: 0+,1+
level_lifetime_unit: NS
level_comment:
T $weighted average of 7.55 ns {i40} from (61.8|g)(K| x ray)(t) and 7.2 ns {i7} from (61.8L+90.5K)(K| x ray)(t) (1973Lo10) 


level_energy_unit: KEV
level_spin_parity: 8-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$ from Adopted dataset for {+122}I in ENDSF database. 2012Si09 list this energy as 444.2 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: US
level_comment:
T$ 64.5|g(t) (2012MoZZ). Value of 80 |ms is quoted in authors' text 
$ Configuration=|p9/2[404]~#|n5/2[532] (2012MoZZ) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
E$g.s. of {+122}I{++53} ion (fully-ionized charge state) 
J$from {+122}I Adopted Levels in ENSDF database 
T$from |l(|b{++})=2.63 |*10{+-3} s{+-1} {I17} and |l{-{Iloss}}= 1.5 |*10{+4} s{+-1} {I5} (2012At01) for fully-ionized {+122}I, the values are weighted averages of five measurements. The value for |b{++} decay agrees within 2|s of |l(|b{++})=2.48 |*10{+-3} s{+-1} {I23} for neutral {+122}I atom. Half-life of neutral atom is 3.63 min {I6} (from {+122}I Adopted Levels in ENSDF database) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
E$g.s. of {+122}I{++52} ion (H-like ion with single bound electron) 
T$from |l{-|b{++}}=2.80 |*10{+-3} s{+-1} {I15}, |l{-|e}=7.35 |*10{+-4} s{+-1} {I33}, and |l{-{Iloss}}=1.5 |*10{+4} s{+-1} {I5} (2012At01), the values are from weighted average of nine measurements. The decay constant for |b{++} agrees within 2|s of |l{-|b{++}}=2.48 |*10{+-3} s{+-1} {I23} for neutral {+122}I atom. Neutral atom half-life=3.63 min 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7-)
level_lifetime_unit: NS
level_comment:
T$from sum of 61|g, 94|g, and 159|g(t) (2019Mo28). Fits to individual gammas: 194.2 ns {I14} (61|g(t)), 192.9 ns {I19} (94|g(t)), 192.5 ns {15} (159|g(t)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: US
level_comment:
T$from sum of 51|g and 187|g(t) (2019Mo28). Fits to individual gammas: 78.6 |ms {I7} (51|g(t)) and 77.9 |ms {I5} (187|g(t)). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: H
level_comment:
J$spin=5/2 from atomic beam (1958Ga18); L({+3}He,d)=2 from 0+ 
T$Weighted average of 13.25 h {I3} (2018Bo02), 13.218 h {I7} (2012Re25), 13.232 h {I7} (2004Sc04), 13.2216 h {I24} (2004Da05), 13.2235 h {I19} (2002Un02, 1992Un01), 13.21 h {I3} (1987Ja13), 13.21 h {I2} (1982La25), 13.4 h {I5} (1968Jo02), 13.30 h {I5} (1965An05). Others: 13.50 h {I11} (1973Ka45) and 13.02 h {I4} (1968Hu01) are discrepant. 
MOMM1$from nuclear magnetic resonance on oriented nuclei (1979Sc13). Also in 2014StZZ compilation. 
$1992Oh03 measured magnetic hyperfine splitting frequency by NMR-ON method. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$138.4|g M1+E2, |DJ=1 to 5/2+, 532.6|g from 9/2+; L({+3}He,d)=0+4 from 0+ for a composite peak at 144 keV 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
J$148.99|g E2, |DJ=2 to 5/2+, 899.6|g M1 from 1/2+; L({+3}He,d)=0+4 from 0+ for a composite peak at 144 keV gives 1/2+ for one component and 7/2+ for the other 
T$from |g|g(t) and |g-ce(t) in {+123}Xe |e decay 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=2 from 0+; 178.1|g M1(+E2) to 5/2+, 870.7|g M1(+E2) from 1/2+ 
T$from |g-ce(t) in {+123}Xe |e decay. Other: 0.3 ns {I1} from generalized centroid-shift method (1988Ko16) in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$912.0|g M1 from 1/2+; 192.3|g to 7/2+ must be D or E2, required by RUL 
T$from |g-ce(t) in {+123}Xe |e decay 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$641.3|g E2, |DJ=2 to 5/2+, 502.9|g M1+E2, |DJ=1 to 7/2+ 
T$from generalized centroid-shift in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=5 from 0+; 272.5|g E1, |DJ=1 to 9/2+. 
T$from generalized centroid-shift in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
J$331.2|g M1+E2, |DJ=1 to 9/2+; no |g decays to 5/2+, 7/2+ and 3/2+ low-lying levels; band assignment 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_uncertain: ?
level_comment:
J$L({+3}He,d)=2 from 0+ for a level at 1152; probable |e feeding (|DJ=0,1) from 1/2(+) parent in {+123}Xe 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: NS
level_comment:
J$298.1|g (M1), |DJ=1 to (19/2+). Other: (19/2-) proposed by 2011Mo28 in ({+7}Li,6n|g) 
T$weighted average of 24 ns {I3} in ({+7}Li,6n|g) (2011Mo28), 28 ns {I2} in (|a,2n|g) (1977Ha36) and 26.3 ns {I21} in ({+6}Li,3n|g) (1982Sh20). Note apparent error in authors' value of T{-1/2}=24.3 ns {I20} in figure 3 (1982Sh20). 
MOMM1$from TDPAD, quoted in the 2014StZZ compilation, from a conference proceeding abstract (Proceeding of the 6th Hyperfine Interaction Conference in Groningen, page NP14, 1983) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$this level is proposed by 2011Mo28 in ({+7}Li,6n|g), based on a 399|g-310|g cascade to 2362 level. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$this level perhaps decays to 5002 and 2614 levels as tentatively proposed by 1997Ba56 in ({+18}O,p4n|g), but the |g rays have not been observed. 


level_energy_unit: KEV
level_spin_parity: (47/2-)
level_comment:
E$The order of the 991|g-801|g cascade in ({+18}O,p4n|g) is reversed in ({+48}Ca,p4n|g), resulting in the level at 7766, instead of a level at 7579 in ({+18}O,p4n|g), with the former being adopted. 
J$990.5|g Q, |DJ=2 to (43/2-); band assignment in ({+48}Ca,p4n|g). (45/2-) proposed in ({+14}N,|a3n|g) based on Mult(990.5|g)=D from |g|g(ADO) data. The former is adopted considering more complete level scheme in ({+48}Ca,p4n|g). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (55/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x estimated at 11250 keV (2012Si21) 
J$band head; proposed in ({+48}Ca,p4n|g) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (59/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$y estimated at 13000 keV (2012Si21) 
J$band head; proposed in ({+48}Ca,p4n|g) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (61/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$z estimated at 13300 keV (2012Si21) 
J$band head; proposed in ({+48}Ca,p4n|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$weighted average of 2.34 ns {I3} from (|b{++})(ce of 148.9|g)(t) (1971Ch43); 2.44 ns {I9} from (|g{+|+})(148.9|g)(t), (899|g)(148.9|g)(t) (1970Sc21); 2.35 ns {I8} from (600-800|g)(ce of 148.9|g)(t) (1971Ho02) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.77 
E$doublet. 1977Sz01 report an unsolved triplet of 138+148+178; 1979Sz05 report a 138+149 doublet 
$Other: (2J+1)C{+2}S'=0.16, d|s/d|W(35.7|')=0.049 |mb/sr for J=1/2 (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.083 
E$from 1979Sz05. other: 176 {I10} (1977Li10) 
$Other: (2J+1)C{+2}S'=0.20, d|s/d|W(35.7|')=0.046 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.017 
E$weighted average of 327 {I4} (1979Sz05), 332 {I10} (1977Li10), and 330 {I10} (1977Sz01) 
$Other: d|s/d|W(35.7|')=0.006 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.18 
E$from 1979Sz05. Others: 942 {I10} (1977Li10), 940 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=4.2, d|s/d|W(51.0|')=0.078 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.74 
E$others: 1010 {I6} (1979Sz05), 1010 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=1.32, d|s/d|W(35.7|')=0.233 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=1.1 
E$others: 1046 {I6} (1979Sz05), 1050 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=0.34, d|s/d|W(46.0|')=0.135 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.43 
E$others: 1152 {I6} (1979Sz05), 1150 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=1.1, d|s/d|W(35.7|')=0.148 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.19 
E$from 1979Sz05. Others: 1240 {I10} (1977Sz01, 1977Li10) 
$Other: (2J+1)C{+2}S'=0.10, d|s/d|W(41.0|')=0.04 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.066 
E$from 1979Sz05. Others: 1307 {I10} (1977Li10), 1310 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=0.16, d|s/d|W(41.0|')=0.029 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.050 
E$from 1979Sz05. Others: 1368 {I10} (1977Li10), 1370 {I10} (1977Sz01) 
L$other: (0) from 1977Sz01 
$Other: (2J+1)C{+2}S'=0.08, d|s/d|W(35.7|')=0.029 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.35 
E$others: 1493 {I6} (1979Sz05), 1490 {I10} (1977Sz01) 
L$other: 2 from 1977Sz01 
$Other: (2J+1)C{+2}S'=0.28, d|s/d|W(41.0|')=0.045 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.053 
E$from 1979Sz05. Others: 1583 {I10} (1977Li10); 1570+1630 unresolved doublet in 1977Sz01, with d|s/d|W(46.0|')=0.028 |mb/sr 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.12 
E$weighted average of 1718 {I10} (1977Li10) and 1710 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=0.28, d|s/d|W(41.0|')=0.049 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.67 
E$other: 1870 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=0.34, d|s/d|W(41.0|')=0.17 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.14 
E$weighted average of 1928 {I10} (1977Li10) and 1930 {I10} (1977Sz01) 
L$not reported in 1977Sz01 
$Other: d|s/d|W(41.0|')=0.025 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.042 
E$other: 1950 {I10} (1977Sz01) 
L$other: 0 from 1977Sz01 
$Other: (2J+1)C{+2}S'=0.08, d|s/d|W(46.0|')=0.042 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=0.16 
E$weighted average of 2282 {I10} (1977Li10) and 2270 {I10} (1977Sz01) 
$Other: (2J+1)C{+2}S'=0.10, d|s/d|W(41.0|')=0.056 |mb/sr (1977Sz01) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
T from |g(t) with ionization chamber (1992Wo03); others: 4.24 d {I5} (1958Dy88), 4.1 d {I1} (1959Gi59), 4.2 d {I2} (1959Mi22), 4.15 d {I3} (1968An05), 4.30 d {I8} (1967Ru04), 4.1 d {I2} (1968Jo02), 4.15 d {I8} (1973Ka45) 
J atomic beam (1976Fu06); 2-yes |b to {+124}Te g.s. 
MOMM1 From nuclear magnetic resonance on oriented nuclei (1992Oh01); Other: 1.14 {|8} (1983De55,1989Ra17). See also 2005St24. 
Configuration=((|p g{-7/2})(|n h{-11/2})) (1982Bu12) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: NS
level_comment:
J |g(|q) and (E1) |g to 2- 
T from |g|g(t) (1982Bu12); others: 26 ns {I2} (1986LuZW), 62 ns (2003MoZQ) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
J from (HI,xn|g). (HI,xn|g) gave no arguments, but A{-2} value in (p,n|g) is consistent with |DJ = 2, although 1982Bu12 gave 2- or 3-. 
T from |g|g(t) (1982Bu12); others: 9.7 ns {I8} (1986LuZW), 10 ns (2003MoZQ) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
J 1997DaZY gives 4- without any discussions. 1982Bu12 gave 2- or 3- from |g(|q) data, but A{-2} value is consistent with |DJ = 2. 
T from (152|g,168|g,174|g)(123|g)(t) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
J$from Adopted Levels of {+124}I in ENSDF 
T$from 2021Pi01. 4.1760 d {I3} from Adopted Levels of {+124}I in ENSDF 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: D
level_comment:
J Microwave spectroscopy J=5/2 (1976Fu06) L=2 in ({+3}He,d), (|a,t) 
T Weighted average of 59.37 d {I6} (1991Al05), 59.416 d {I10} (1990Wo03), 59.38 d {I3} (1990De09), 59.39 d {I2} (1989Sc17), and 59.40 d {I5} (1989Si19) Others: 59.156 d {I20} (1980Ho17), 59.47 d {I21} (1982HoZF), 59.83 d {I11} (1965An07), 59.89 d {I18} (1968La10), 60.18 d {I17} (1972Em01), 60.0 d {I5} (1951Fr21), 57.4 d {I2} (1960Ma36), 58.76 d {I13} (1966Ri14) 
MOMM1 From nuclear magnetic resonance on oriented nuclei. See also 2005St24 compilation. 
MOME2 From microwave absorption. See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J L=2 in ({+3}He,d), (|a,t); M1+E2 |g from 1/2+ 
T From X|g(t) in {+125}Xe |e decay 
MOMM1 From integral perturbed angular correlation. See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T From (K| x ray)(ce(K) 114|g)(t) (1968Ko01); Other: 0.60 ns {I4} (K| x ray)(ce(K) 114|g)(t) (1966Ge13) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T Weighted average of 0.354 ns {I7} (K| x ray)(ce(K) 188|g)(t) (1966Ge13), 0.34 ns {I2} (ce(K) 55|g)(ce(K) 188|g)(t) (1967Ho04), 0.325 ns {I10} (ce(K) 55|g)(ce(K) 188|g)(t) (1968Ko01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T From (E|g|>600|g)(ce(L) 243|g)(t) (1968Ko01); Others: |<0.19 ns (K| x ray)(ce(K) 243|g)(t) (1966Ge13), 0.21 ns {I2} (Auger E)(ce(K) 243|g)(t) (1967Ho04) 


level_energy_unit: KEV
level_comment:
L From 1979Sz05; L=(0)+(2) (1977Li10) 
S 0.24 if 3s1/2 for L=0 component; 0.48 if 2d3/2 for L=2 component 


level_energy_unit: KEV
level_spin_parity: 41/2+
level_comment:
$ It is not clear whether 6887.9, 41/2+ or 6907.8, 41/2+ level is is associated with the band based on 9/2+, or both 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: D
level_comment:
T from weighted av of 13.1 d {I3} (1968Jo02), 13.02 d {I7} (1968Qa02), 13.1 d {I5} (1957Aa04), 13.5 d {I6} (1957Er25), 13.3 d {I1} (1954Pe18), 13.1 d {I5} (1948Mo33), 13.0 d {I3} (1938Li05), 12.8 d {I1} (1965An05), 12.93 d {I6} (1975Ok04), 12.82 d {I5} (1998Fo05) 
J atomic beam (1960Ga12); first-forbidden unique |b{+-} to 0+. 
MOMM1 nuclear static orientation and radiative detection of nuclear magnetic resonance (2019StZV,1992Oh01) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1983Bu11). other; 20 ns from |g(t) (2012MoZZ) 
J J=1 from |g(|q) and E1 |g to 2- in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: NS
level_comment:
MOMM1 differential perturbed angular distribution (1975BlZY,2020StZV) 
T$from |g|g(t) (1983Bu11). other; 128 ns from |g(t) (2012MoZZ) 
J$E1 |g to 2- and M1+E2 |g from (4+) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) (1983Bu11). other; 11 ns from |g(t) (2012MoZZ) 
J$stretched E2 |g to 2- in ({+7}Li,5n|g) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
$This level seems to be same the 237.38 level from {+126}Te(p,n|g). However, the suggested spin 6- value is different with that of 3+. The valuators assumed the different level. 
J$stretched E2 |g to 4- in ({+7}Li,5n|g) 
T$from |g(t) (2012MoZZ) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
T$from |g(t) (2012MoZZ). 13.5 ns {I11} in Adopted levels. 
$ In-out intensity is imbalance. 
J$stretched E2 |g to 2-. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J$M1,E2 |g from 2+ in (p,n|g) |g and |g from (6+). 2012Zh30 and 2012MoZZ propose (5-) and 5, respectively. 


level_energy_unit: KEV
level_spin_parity: (9+)
level_comment:
J$M1+E2 |g to (8+), E1+M2 |g to (8-) from DCO and |g|g(linear pol) (2013Ka50). 2012MoZZ proposed spin-parity of (9-). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1$nuclear magnetic res and optical spectroscopy; value relative to |m for {+1}H (1989Ra17) 
MOME2$atomic beam magnetic res (1989Ra17). Others: -0.722 {I21} (2004Al08), -0.710 {I10} (2001Bi17), -0.69 {I3} (2000Va33) and -0.689 {I15} (2000Ha64): The value from 1989Ra17 is the result of systematic treatment on wide range of nuclides. However, the recent values are significantly smaller than adopted. The weighted mean of the above 4 values is -0.705 {I8} (evaluator). 
<r{+2}>{+1/2}(charge)=4.750 {I4} (2004An14) 
J atomic beam J=5/2 (1976Fu06); L=2 in ({+3}He,d),(|a,t) 
Configuration=(|p 2d{-5/2}) 
T The lower limit of half-life due to unusual decay mode is 1.5|*10{+24} y (2005Be17), 1.1|*10{+25} y (1993Ej01); others: (2005Be03), (1999Be61), (1991Ej01), (1991Ke05), (1987Ho02). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J L=4 in ({+3}He,d),(|a,t); M1+E2 |g to 5/2+ 
T from |b|g(t) in {+127}Te |b{+-} decay (106.1 d) (1976Sa20): others: 1.90 ns {I15} (1969BeZH), 1.93 ns {I7} (1967Sv01), 1.5 ns {I3} (1964Jh02) in {+127}Te |b{+-} decay (106.1 d); 1.86 ns {I11} (1965Ge04), 1.0 ns {I2} (1964Jh02), 2.0 ns {I2} (1962Th12) in {+127}Xe |e decay 
MOMM1,MOME2$Moss; values relative to those of g.s. for {+127}I (1989Ra17) 
Configuration=(|p 1g{-7/2}) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J L=4 in ({+3}He,d),(|a,t), M1+E2 |g from 1/2+ 
T from |e decay. Others: 0.39 ns {I6} from (|g,|g'), 0.52 ns {I10} from DSA in Coul. ex (1975An19) 
MOMM1$integral PAC; value recalculated based on new measurements (2005St24) 
Configuration=(|p 2d{-3/2}) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J L=0 in ({+3}He,d),(|a,t) 
T from unweighted av of 15 ps {I3} from (|g,|g'), 34 ps {I3} from B(E2) and 43 ps {I4} from DSA in Coul. ex. Other: |<0.135 ns from (K| x ray)|g(t) and ce|g(t) in |e decay (1968Ko01) 
Configuration=(|p 3s{-1/2}) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J L=2 in ({+3}He,d),(|a,t); linear pol of (|g,|g') is compatible only with J=5/2 
T weighted average of 3.4 ps {I3} from (|g,|g') and 3.0 ps {I6} from DSA in Coul. ex. 
BE2 B(E2)=0.0082 {I12} from Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J fed in |b{+-} decay from 11/2-, D+Q |g to 5/2+ 
T from DSA in Coul. ex., other; |43.1 ps in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_lifetime_unit: PS
level_comment:
J D+Q |g to 7/2+; 9/2 supported by |g(|q) in Coul. ex. 
T from B(E2) in Coul. ex., Other: 1.5 ps {I3} in DSA 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_lifetime_unit: PS
level_comment:
J D+Q |g to 7/2+; 9/2 supported by |g(|q) in Coul. ex. 
T from B(E2) in Coul. ex., others: 1.6 ps {I3} from DSA, <3.5 ps in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
T from (ce(K) 145|g)(K| x ray)(t) (1965Ge04). Others: 1.5 ns {I3} (1964Jh02), 2.0 ns {I2} (1962Th12) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
(|eK)(|w(K))=0.750 {I16} (1964Br26) 
T unweighted av of 0.38 ns {I1} (1966Ge13) and 0.40 ns {I1} (1968Ko01) from |g|g(t) 


level_energy_unit: KEV
level_comment:
E IAR of 1815.3 level in {+127}Te; L=(2),3 in {+126}Te(d,p) 
|G(total)=38 keV {I5}, |G(p)=0.9 keV {I4} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E IAR of 1919.57 {I7}/2- level in {+127}Te; L=(2),3 in {+126}Te(d,p) 
|G(total)=29 keV {I5}, |G(p)=1.1 keV {I4} 


level_energy_unit: KEV
level_comment:
E IAR of 1956.27 level in {+127}Te; L=(1,2) in {+126}Te(d,p) 
|G(total)=42 keV {I7}, |G(p)=1.5 keV {I4} 


level_energy_unit: KEV
level_comment:
E IAR of 2167.1 and/or 2175.66 level in {+127}Te; no L=1 level in {+126}Te(d,p) 
|G(total)=80 keV {I10}, |G(p)=6.9 keV {I7} 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E IAR of 2438.36 (3/2-) level in {+127}Te; L=(1) in {+126}Te(d,p) 
|G(total)=70 keV {I6}, |G(p)=4.6 keV {I5} 


level_energy_unit: KEV
level_comment:
S if 2d{-5/2}, value is av 0.60 (|a,t) and 0.55 ({+3}He,d). Other: if 2d{-3/2}, 1.20 (|a,t) and 1.10 ({+3}He,d) 


level_energy_unit: KEV
level_comment:
S av of 0.10 (|a,t) and 0.12 ({+3}He,d) if 2d{-5/2} for L=2 component; 0.23 for L=0 component ({+3}He,d) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T from |G{-0}{+2}/|G=9.9|*10{+-5} eV {I4} and g|G{-0}=1.13|*10{+-4} eV {I6} (1965La01), and |G{-0}/|G=0.85 {I3} from adopted branching 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
BE2 Weighted av of 0.035 {I5} (1969De03), 0.033 {I5} (1969Wa09), 0.043 {I5} (1973Re08), and 0.037 {I5} (1975An19). Others: 0.042 {I14} (1973Re08), 0.072 {I14} (1967Im01) 
T from B(E2). Other: 0.52 ns {I10} from DSA 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted av of 0.029 {I5} (1969Wa09), 0.027 {I3} (1973Re08), and 0.026 {I2} (1975An19). Other: 0.015 {I2} (1969De03) 
T from B(E2). Others: 41 ps {I3} from DSA 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_lifetime_unit: PS
level_comment:
BE2 Weighted av of 0.0235 {I35} (1969Wa09), 0.023 {I2} (1975An19), and 0.023 {I3} (1973Re08) 
T from B(E2). Other: 1.5 ps {I3} from DSA 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_lifetime_unit: PS
level_comment:
BE2 Weighted av of 0.135 {I20} (1969Wa09), 0.110 {I8} (1975An19), and 0.120 {I13} (1973Re08) 
T from B(E2). Other: 1.6 ps {I3} from DSA 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$ A 684.3|g shown from this level in table I and level-scheme figure 1 of 2012Di06 is incorrect as per e-mail reply of April 26, 2012 from Y.H. Zhang. Instead, this |g is 683.7 from 4641.6 level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 15/2-
level_comment:
$B(E1)/B(E2)=0.18|*10{+-6} {I2}; D{-0}=0.058 efm {I3} using Q{-0}=2.46 b {I4} from the average of that for {+126}Te and {+128}Xe. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 19/2-
level_comment:
$B(E1)/B(E2)=0.22|*10{+-6} {I6}; D{-0}=0.065 efm {I9} using Q{-0}=2.46 b {I4} from the average of that for {+126}Te and {+128}Xe. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J$atomic beam J=1; L(d,p)=2 for 5/2+ target, configuration=(|p2d{-5/2})(|n2d{-3/2}) 
T$weighted average of 24.99 min {I2} (1941Hu04), 25.03 min {I4} (1958Gu09), 25.0 min {I5} (1959Gi42), 25.5 min {I3} (1968Qa02), 25.08 min {I5} (1968Re04), 24.97 min 3 (1972Em01). Other: 24.92 min {I6} (1994Ya02); value is an average from three values given in the authors' table. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$E1 |g's to 1+ and 3+. 
T$from |g|g(t) in (p,n|g); other: 12.5 ns {I19} in {+127}I(n,|g) E=thermal:secondary. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=0 for 5/2+ target, no |g to 1+. 
T$from |g|g(t) in (p,n|g); other: <5 ns in {+127}I(n,|g) E=thermal:secondary. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$M1 |g's to 1+ and 2+. 
T$from |g|g(t) in (p,n|g). Other: <5 ns in {+127}I(n,|g) E=thermal:secondary. 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$M1 |g to (5)-, |g to (3)-, population by primary |g in {+127}I(n,|g) E=thermal:secondary rejects J|p|>5-. 


level_energy_unit: KEV
level_spin_parity: (3,4)-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$M1,E2 |g to (2,3)-, |g to (5)-; primary |g from 2+,3+ in {+127}I(n,|g) E=thermal:primary rejects J|p=5-. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: Y
level_comment:
MOMM1$From NMR (1951Wa12). 
MOME2$quadrupole resonance, microwave absorption (1953Li16). Value recommended in 2013StZZ evaluation based on original value of -0.553 from 1953Li16. Others: -0.498 {I7} (2001Bi17, re-evaluated from measured Q({+129}I)/Q({+127}I)=0.701213 {I15} (1953Li16)); -0.482 {I10} (reanalysis of Q{-2} for {+127}I by 2000Ha64) 
J$spin from microwave spectroscopy (1949Li09). Parity from L({+3}He,d)=4 
T$from specific activity (1972Em01). Others: 1.97|*10{+7} y 14 (1973Ku17), 1.56|*10{+7} y {I6} (1957Ru65), 1.72|*10{+7} y {I9} (1951Ka16), 3.0|*10{+7} y (1949Pa19), |?10{+8} y (S. Katcoff, Phys. Rev. 71, 826 (1947) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
MOMM1$Mossbauer effect (1981De35). 
MOME2$Mossbauer effect, value recommended by 2013StZZ evaluation based on original value of -0.685 from 1972Ro41. Others: -0.616 {I9} (2001Bi17, re-evaluated data from 1972Ro41); -0.598 {I13} (reanalysis of 1972Ro41 data and Q{-2} for {+127}I by 2000Ha64); -0.42 {I2} (1987Gr28, Mossbauer effect measurement) 
J$L({+3}He,d)=2; M1+E2 |g to 7/2+. 
T$from (|b)(0.0278 ce(L))(t) (1966Sa06). Others (from |b|g(t) or |g|g(t)): 16.4 ns {I11} (1965Pa04), 14.4 ns 5 (1964Ka09), 14.4 ns {I7} (1964Jh02), 15.9 ns 13 (1963Go17), 18.6 ns 11 (1962De18) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$L({+3}He,d)=2; E2 |g to 7/2+; |g from 1/2+. 
T$from delayed |g (1969BoZR). 0.27 ns is deduced from B(E2) in Coulomb ex. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=2; M1+E2 gammas to 7/2+, 5/2+ and 3/2+. 
T$deduced by compilers from B(E2)(|^)=0.016 {I3} in Coulomb excitation. Other: 0.05 ns (from |g(t),1969BoZR). 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, (E2) g to 7/2+; Coulomb excited; population in ({+7}Li,2n|g) supports 11/2 over 3/2 
T$deduced by compilers from B(E2)=0.122 {I13} in Coulomb ex. 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_lifetime_unit: PS
level_comment:
J$log| {Ift}=9.9 from 11/2-; M1+E2 |g to 7/2+. 
T$deduced by compilers from B(E2)=0.078 {I8} in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$log| {If{+1u}t}=11.9 from 11/2-; M1+E2 |g to 5/2+; Coulomb excited. J=(9/2) proposed in ({+7}Li,2n|g) is inconsistent with M1+E2 G to 5/2+ 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
J$L(|a,t)=5; |DJ=1, dipole |g to (7/2)+. J=(11/2) proposed in ({+7}Li,2n|g) is not likely with (7/2) assignment for 845 level 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$from (|b)(0.0278 ce(L))(t) (1966Sa06). Others (from |b|g(t) or |g|g(t)): 16.4 ns {I11} (1965Pa04), 14.4 ns 5 (1964Ka09), 14.4 ns {I7} (1964Jh02), 15.9 ns 13 (1963Go17), 18.6 ns 11 (1962De18) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$IAR of 2108-keV 5/2-, 7/2- state in {+129}Te. |G(total)=50 keV {I5}, |G(p)=3.6 keV {I5}. 
J$from L=3. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$IAR of 2221-keV 5/2-, 7/2- state in {+129}Te. |G(total)=47 keV {I5}, |G(p)=3.9 keV {I6}. 
J$from L=3. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$IAR of 2361-keV 1/2-, 3/2- state in {+129}Te. |G(total)=95 keV {I10}, |G(p)=10 keV {I15}. 
J$from L=1. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$IAR of 2705-keV 1/2-, 3/2- state in {+129}Te. |G(total)=88 keV {I10}, |G(p)=4.3 keV {I7}. 
J$from L=1. 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
E$IAR of 2975-keV, 5/2-,7/2- state in {+129}Te. |G(total)=35 keV {I10}, |G(p)=1.0 keV {I4}. 
J$from L=(3). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
$|m(27.8 level)/|m(g.s.)=1.0687 {I11} (1970De37) 
MOME2$reanalyzed result is -0.604 {I10} (2013StZZ); see also 2001Bi17 and 2000Ha64 for re-analysis of 1972Ro41 data. Other measurement: -0.42 {I2} (1987Gr28) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$tentatively assigned as L=5, J|p=9/2- in Adopted Levels of {+129}I in the ENSDF database, but 2016En04 state that it is highly likely to have L=5, J|p=11/2- assignment. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: Y
level_comment:
T$from activity and mass concentration measurements (2018Ga37). Other: ENSDF database for {+129}I (August 2014 update) gives 15.7|*10{+6} y {I4}. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: H
level_comment:
J$atomic beam-NMR (1958Ga20,1959Sh63); log| {Ift}=5.8 to |p=+ 
MOMM1$low-temperature nuclear orientation and NMR (1992Oh01) 
CONF$|pg{-7/2}{+3}|nd{-3/2} gives |m(theory)=-3.43 (1992Oh01) 
T$weighted average of 12.34 h {I4} (1996Na23), 12.36 h {I1} (1973Ho25), 12.4 h {I1} (1972Ba51), 12.30 h {I7} (1970Qa02), 12.3 h {I1} (1968Re04), 12.3 h {I1} (1965An05), 12.5 h {I1} (1957Aa04). Others: 12.5 h (1968Le25), 12.5 h {I5} (1939Ta01), 12.6 h {I10} (1938Li05) 
$1968Le25: LEVKOVSKII ET AL., YADERNAYA FIZIKA 8, 7 (1968) 
$1939Ta01: TAPE, G.F., PHYS REV 56, 965 (1939) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$M3 |g to 5+; log| {Ift}=6.6 to 2+ 
T$weighted average of 8.78 min {I2} (1996Na23), 8.9 min {I2} (1974Di03), 9.16 min {I5} (1972Ba51), 9.2 min {I2} (1970Qa02,1970Qa03), 8.82 min {I4} (1968Re04), 9.2 min {I1} (1966Wi15). Others: 8.3 min {I10} (1984RoZO), 9.2 min (1967Ke12), 1974Me17 
%B-$average of 17 {I3} (1973Ho25), 16 {I3} (1970Qa03), 15 {I4} (1967Ke12). Other: 15 (1972Ba51) 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$E1 |g from 3+, M1-M1 |g cascade from (5)-, |g to 2+ establish J|p(43.93)=(3)- and J|p(91.76)=(4)- 


level_energy_unit: KEV
level_spin_parity: (6)-
level_lifetime_unit: NS
level_comment:
J$E1 |g to 5+, no primary |g from 3+,4+ 
T$other: 229 ns {I14} from (p,n|g) 
MOMM1$from |g(|q,H,t) in (p,n|g) (1975BlZY). 
MOMM1$ 1975BlZY (ALSO COMPILATION BY 1989Ra17) ASSOCIATED MEASURED G=-0.048 5 TO A 203, (5-) LEVEL DUE TO INCORRECT ASSIGNMENT OF 85.1G. THE PRESENT PLACEMENT IS FROM (N,G) RESULTS 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$M1 |g to 2+, M1-M1 |g cascade to 5+ through 48.83 level establish J|p(93.71)=3+ and J|p(48.83)=4+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$used as a reference peak for calibration of neutron spectra. This probably corresponds to the 40-keV isomer with J|p=2+ 


level_energy_unit: KEV
level_spin_parity: (6)-
level_lifetime_unit: NS
level_comment:
T,G$|g(t) and |g(|q,H,t); assigned by 1975BlZY to 202.9 level based on incorrect placement of 85.1|g 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: D
level_comment:
T from 2004Sc04. Others: 8.0197 d {I22} (2002Un02), 8.02070 d {I11} (1983Wa26), 8.0213 d {I9} (1980Ho17), 8.020 d {I3} (1978La21), 8.040 d {I1} (1972Em01),8.116 d {I26} (1971Zo02), 7.999 d {I9} (2004Da05) 
J=7/2 from atomic beam method (1976Fu06); |p=+ from L({+3}He,d)=4 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_comment:
J$9/2 from |g(|q) in {+131}Te |b{+-} decay (33.25 h); |p=(+) from |g to 7/2+ which is probably (M1+E2) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_comment:
J$1/2, 3/2, 5/2 from log| {If{+1u}t}<8.5 in {+131}Te |b{+-} decay (25.0 min) from 3/2+; J=1/2 less likely from |g to 7/2+ 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-,13/2-
level_lifetime_unit: NS
level_comment:
J$9/2, 11/2, 13/2 from log| {If{+1u}t}<8.5 from 11/2-; |p=- from M1 |g from J|p=9/2-, 11/2-, 13/2- level 
MOMM1$for J|p=(15/2)- 
T from |g|g(t) in {+131}Te |b{+-} decay (33.25 h) 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-,13/2-
level_comment:
J$9/2, 11/2, 13/2 from log| {Ift}=6.5 from 11/2-; |p=- from M1 |g from J|p=9/2-, 11/2-, 13/2- level 


level_energy_unit: KEV
level_spin_parity: 9/2,11/2
level_comment:
J$9/2, 11/2, 13/2 from log| {If{+1u}t}<8.5 in {+131}Te |b{+-} decay (33.25 h) from 11/2-; |g|g(|q) in {+131}Te |b{+-} decay (33.25 h) rules out 13/2 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_comment:
J$1/2, 3/2, 5/2 from log| {If{+1u}t}<8.5 in {+131}Te |b{+-} decay (25.0 min) from 3/2+; |g to 7/2+ makes J=1/2 not likely 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$1/2+, 3/2+, 5/2+ from log| {Ift}=5.66 in {+131}Te |b{+-} decay (25.0 min); |g to 7/2+ makes J|p=1/2+ not likely 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: D
level_comment:
T from 1983Wa26. Others: 8.0213 d {I9} (1980Ho17), 8.020 d {I3} (1978La21), 8.116 d {I26} (1971Zo02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T from |g|g(t) (1965De22). Others: 0.9 ns {I1} (1956De57), 0.8 ns {I1} (1959So16), and 0.76 ns {I5} (1971Ma04) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: D
level_comment:
T from 1983Wa26. Others: 8.0213 d {I9} (1980Ho17), 8.020 d {I3} (1978La21), 8.116 d {I26} (1971Zo02), 8.040 d {I1} (1972Em01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T from |g|g(t) (1965De22). Others: 0.9 ns {I1} (1956De57), 0.76 ns {I5} (1971Ma04), and 0.8 ns {I1} (1959So16) 


level_energy_unit: KEV
level_spin_parity: 9/2-,11/2-,13/2-
level_lifetime_unit: NS
level_comment:
J=11/2 if J(774)=11/2, J=13/2 if J(774)=9/2 (1975Lu01); J=13/2 or 15/2 from |g|g(|q), J=15/2 if J(1980)=11/2 (1975Lh01) 
T from |g|g(t) (1965De22) 


level_energy_unit: KEV
level_spin_parity: (31/2-,33/2-)
level_lifetime_unit: NS
level_comment:
T$ from |g|g(t) (2009Wa11) 
$ The configuration probably involves a proton coupled to |n(h{-11/2}{+-3}d{-3/2}{+-1}){-15-} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) measured with LaBr3(Ce) detectors (2020Al17). 
MOME2$from TDPAC measurements (2020Al17). 


level_energy_unit: KEV
level_spin_parity: 19/2+
level_comment:
$Compiler's note: there seems a large in-out negative intensity imbalance at this level, with incoming I|g(491|g+692|g+358|g)=95 {I3} versus outgoing I|g(352|g+678|g)=40 {I3} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: H
level_comment:
J$ atomic beam (1960Ga12,1959Sh64); E2-M1 |g cascade from 1+ 
T$ unweighted average of 2.259 h {I8} (1954Em27), 2.30 h {I5} (1955Wa35), 2.292 h {I7} (1958Ke26), 2.34 h {I2} (1965An05), 2.2846 h {I4} (1966Ma56). Others: 1965Si17, 1962Wi14, 1957Aa04, 1939Ab02, 1939Ha13. 
$ 1939Ha13: Hahn and Strassmann: Naturwissenschaften 31, 201 (1939) 
T$ Other: 1961Ne15 (priv. comm.) 
MOMM1,MOME2$atomic beam (1960Wh06,1962Wh11); signs of |m and Q are opposite. Q recalculated by 2001StZZ based on revised Q=0.689 {I15} (2000Ha64) for {+127}I g.s. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
J$ M1 |g to 4+; E2 |g from 1+ 
T$|g|g(t) (1981Yo02). Others: 2.94 ns {I11} (1999Da03), 0.93 ns {I4} (1969Ho42), 0.96 ns {I4} (1966Go23) 
MOMM1$g=+0.74 {I10} was obtained using IPAC (1969Si06) and T{-1/2}=0.951 ns {i22}, which gives |m=+2.24 {I30} (also adopted by 1989Ra17). However, |g|g(t) and |g|g(|q,t) measurements of 1981Yo02 cast doubt on this value, since 1981Yo02 obtain T{-1/2}=7.14 ns {I14} and perturbation coefficient of 0.41 {I9} for the 228-49 cascade as opposed to unperturbed correlation assumed by 1969Si06. 
MOME2$from IPAC (1979Oo01). Q recalculated by 2001StZZ based on revised Q=0.689 {I15} (2000Ha64) for {+127}I g.s. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E$ from difference in Q(|b{+-}) values for {+132}I isomers 
J$ from systematics of 8- levels in neighboring nuclei 
T$ weighted average of 1.385 h {I17} (1976La14) and 1.393 h {I28} (1974Di03,1973Di14) 
$ %IT: obtained by 1974Di03 from relative intensities of pairs of |g-rays from decay of only isomer and from decay of both isomer and ground state 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J$ M1+E2 |g from 1+; M1+E2 |g to 3+ 
T$from 1981Yo02. Other: 0.55 ns {I4} (1999Da03), although, slope in authors' figure 1b seems to correspond to 1.14 ns 
T$ from {+132}Te |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J$ log| {Ift}=4.7 from 0+ 
T$ from 1981Yo02. Others: 1.42 ns {I5} (1966Go23), 1.41 ns {I7} (1969Ho42) 
MOMM1,MOME2$TDPAC (1979Oo01). Q recalculated by 2001StZZ based on revised Q=0.689 {I15} (2000Ha64) for {+127}I 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
T$ from 1981Yo02, used plastic with lead-iron filter for 228|g and NaI(Tl) or Ge(Li) for 49|g, integral and differential directional correlations of 228|g - 49|g cascade confirms value obtained. Others: 0.96 ns {I4} (1966Go23, used two plastics for registration of 232|b,|g-28.5 X-ray), 0.93 ns {I4}(1969Ho42), 2.94 ns {I11} (1999Da03, used two NaI(Tl) detectors for detecting 228|g and 49|g) 
G$+0.74 {I10} was obtained using IPAC (1969Si06) and T{-1/2}=0.951 ns {i22}. However, |g|g(t) and |g|g(|q,t) measurements of 1981Yo02 cast doubt on this value, since 1981Yo02 obtain T{-1/2}=7.14 ns {I14} (g=0.099 {I13}) and perturbation coefficient of 0.41 {I9} for the 228-49 cascade as opposed to unperturbed correlation assumed by 1969Si06. 
G$for T{-1/2}=0.951 ns {I22}; 0.099 {I13} for T{-1/2}=7.14 ns 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$ from 1981Yo02, used plastic for 116 |g and NaI(Tl) for 111 |g, uranium shield used non-simultaneously for each detector. Others: 0.55 ns {I4} 1999Da03, used two CsI for detecting 116 |g and 111 |g, fig. 1b corresponds to half-life of 1.14 ns 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
T$ from 1981Yo02. Others: 1.42 ns {I5} (1966Go23), 1.41 ns {I7} (1969Ho42) 
$ Configuration=|pd{-5/2}|nd{-3/2}{+-1} 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
E$ from difference in Q(|b{+-})=3680 {I15} for {+132}I isomer (1974Di03) and Q(|b{+-})=3560 {I15} for {+132}I g.s. (1965Jo13) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
$ Configuration=|pg{-7/2}~#|nd{-3/2}{+-1} (2009Ta23) 
T$ from |g|g(t) (2009Ta23). Previous values: 0.96 ns {I4} (1966Go23), 0.95 ns {I3} (1967Sc39), 0.93 ns {I4}(1969Ho42), 7.14 ns {I14} (1981Yo02), 2.94 ns {I11} (1999Da03). 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
$T{-1/2} and decay modes from {+132}I Adopted Levels in the ENSDF database (Feb 2005 update). Half-life of 89.4 min {I47} was also measured by 2014BhZZ (EPJ Web Conf. 66, 2009) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (11+)
level_lifetime_unit: NS
level_comment:
T$from 762|g(t) in the present work 
$The isomer probably depopulated through a low-energy transition to connect to the 1644-keV level 
$Level defined as 605|g is observed in coincidence with both the 762-keV |g rays. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
J$Atomic beam (1960Ga12) 
T$weighted average of 20.9 h {I1} (1968Re04), 20.8 h {I2} (1966Ei01), 20.3 h {I3} (1965An05), 20.9 h {I3} (1955Wa35), and 20.8 h {I2} (1953Ka28). 
CONF$|p(g{-7/2}{++1})~#(g{-7/2}{++2}){-0+} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$from 719.71|g to 7/2+, 407.63|g to (5/2+); branching ratios favor 3/2+ 
CONF$|p(g{-7/2}{++1})~#2{++} 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$587.6|g to (3/2+), 394|g to 11/2+; not populated directly in {+133}Te (J|p=(3/2+)) |b{+-} decay and in {+133}Te (J|p=(11/2-)) |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J$74.05|g (M2) to 15/2+ 
T$from I|g(t), I|b(t) in 1970OsZZ 
CONF$|p(g{-7/2}{++1})~#|n(h{-11/2}{+-1},d{-3/2}{+-1}){-7-} 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
J$94.989|g E2 to (19/2-), 169.025|g (E1) to (15/2+) 
T$from |g|g(t) in 1984Wa04 
CONF$|p(g{-7/2}{++1})~#|n(h{-11/2}{+-1},d{-3/2}{+-1}){-5-} 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J$88.064|g M1+E2 to (11/2+), 1885.62|g to 7/2+, no |g-ray transition to the 312.1-keV level (J=(5/2+)) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$667|g to (1/2+), 368.9|g to (3/2+), 1254.2|t to (5/2+); no |g-ray transitions to 7/2+ and 9/2+ levels 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$2053.43|g to 7/2+, 679.8|g to (1/2+), no |g-ray transition to the 914.8-keV level (J{+|p}=(9/2+)) 


level_energy_unit: KEV
level_spin_parity: (11/2,13/2)
level_comment:
J$363.06|g to (11/2+), 257.82 to (11/2-,13/2-) no |g-ray transitions to the 312.1-keV (J{+|p}=(5/2+)) and g.s. (J{+|p}=7/2+) levels 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$from 2255.4|g to 7/2+, 690.8|g to (1/2+), no |g-ray transition to the 914.8-keV level (J{+|p}=(9/2+)) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2)
level_comment:
J$910.0|g to (1/2+), 971|g to (5/2+), no |g-ray transitions to the 7/2+ g.s. and the 914.8-keV level (J{+|p}=(9/2+)) 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$874.9|g E2(+M3) to (15/2+) 
T$from 913-648|g|g(t) and 913-875|g|g(t) in 2004Va03 
CONF$|p(g{-7/2}{++3})~#|n(h{-11/2}{+-2}){-10+} or |p(g{-7/2}{++2},d{-5/2}{++1}) 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M3
level_comment:
J$58.7|g E2 to (19/2+) 
T$from 875-647|g|g(t) in {+176}Yb({+136}Xe,X|g) (2009Wa11) 
CONF$|p(g{-7/2}{++3})~#|n(h{-11/2}{+-2}){-10+} 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$Assumed that the isomer decays directly by 875|g, but possibility of a low-energy |g transition preceding 875|g is not ruled out 
T$from (beam like recoil fragments)|g(t)-coin (2004Va03); 913|g and pair of 648|g-875|g used as gates 


level_energy_unit: KEV
level_spin_parity: 23/2+
level_lifetime_unit: NS
level_comment:
T$from (353|g+874|g+1168|g)(t) (2020Ba52). This value can be compared with 469 ns {I15} from 2009Wa11 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: MIN
level_comment:
J$278-435-210 cascade of M1,E2 transitions gives positive parity, no |g from 1+ points to a J=4 assignment. Additionally, it mainly feeds 4+ levels in {+134}Xe after |b decay 
T weighted average of 52.5 min {I5} (1953Pa25), 52.8 min {I3} (1961Jo08), 52.0 min {I2} (1965An05), 52.5 min {I1} (1969Ta10), 53.2 min {I2} (1971Ac01), and 51.3 min {I7} (1974OhZR) 


level_energy_unit: KEV
level_spin_parity: (8)-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J E3-M1 |g cascade to (4)+ g.s., lack of crossover |g establishes J|p(316.3)=(8)- and J|p(44.4)=(5)+. Feeds only 7- level in {+134}Xe after |b decay 
T weighted average: 3.80 min {I10} (1970Ca16), 3.56 min {I8} (1971Ac01), 3.8 min {I2} (1972Co04), 3.8 min {I1} (1974Di03), 3.50 min {I2} (1976La14) 
%IT, %|b{+-}: from I(234.3|g, {+134}Xe)/I(272.1|g, {+134}I)=0.020 {I10} (1972Co04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8-)
level_lifetime_unit: MIN
level_comment:
$ Configuration=|p(1g{-7/2})~#|n(1h{-11/2}){+-1} 
%IT,%B-$ from Adopted Levels, Gammas dataset for {+134}I in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
J$spin from atomic beam (1960Ja12); parity from L(d,{+3}He)=4 
MOMM1$ NMR on oriented nuclei, measured |g(|q,H,temp) (1998Wh04). The positive sign is from systematics of odd-A I nuclides where the magnetic moment of the 7/2+ g.s. has been measured as positive. See also compilation by 2005St24 
T$unweighted average of 6.55 h {I3} (1982Wa21) and 6.61 h {I1} (1974LaZV). Others: 6.585 h {I2} (quoted by 1971Ha13 from their 'to be published' paper, but which never appeared), 6.7 h {I2} (1953Pa25), 6.7 h {I1} (1950Gl09), 6.6 h {I3} (1940Do07), 1955Wa35, 1950Ka06, 1945Wu05. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2+)
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) and |g|g|g(t) (2017Sp02), weighted average of 1.81 ns {I18}, 1.85 ns {I14}, 1.67 ns {I14}, and 1.65 ns {I14}; the first two values obtained from exponential fitting of (288.1|g)(572.4|g)(t) decay curves, and the second two from fits to (1133.4|g)(572.4|g)(288.1|g)(t) triple coincidence decay curves. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$due to larger width, peak is suspected to be a doublet. 2016En04 suggest peak could also include 2312-keV level reported in literature with unassigned J|p. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
J$log| {Ift}=6.46 for |b{+-} decay to 2+ state, no decays to 3- states (1991Ma07), supported by Shell Model calculations (2009Co15,2010Co17) 
T$weighted average of 85.1 s {I20} (|g(t), 1977We04), 83.4 s {I4} (1972Wa21), 83 s {I2} (|g(t), |b(t), 1971Lu02), 83 s {I3} (|g(t), 1970Ca25), and 82.8 s {I15} (|b(t), 1959Jo37). 


level_energy_unit: KEV
level_spin_parity: (2-,1-,0-)
level_lifetime_unit: NS
level_comment:
J$M1(+E2) 87.3|g to (1-), population in {+248}Cm SF decay favors J|p=2-. 
T$from ce(t) in {+252}Cf SF decay 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$from |b endpoint energies in 2007Fo02. Note that 2007Fo02, interpreted this as 7- isomer, however, observation of prompt, 42.6 keV transition from (7-) level by 2006Ur02 indicates that the isomer is J|p=(6-). Other: 640 {I110} from 1985Wa04, based on |b|g coincidence data of 1980KeZQ. 
T$weighted average of 44.8 s {I10} (|g(t), 1977We04), 48 s {I2} (|g(t), |b(t), 1971Lu02), 48 s {I1} (|g(t), 1970Ca25) 
J$from log| {Ift}=6.4 for |b decay to 6+, weak or no |b decay to 4+, no observed IT decay, supported by shell model calculations (2006Ur02). 
$configuration=|pg{-7/2}{+2}d{-5/2}|nf{-7/2} (2006Ur02) 


level_energy_unit: KEV
level_comment:
J$(3-) proposed in {+248}Cm SF decay based on assignment to |g-cascade, feeding from 0+ parent in |b{+-} decay suggests J=0,1,2 


level_energy_unit: KEV
level_spin_parity: (11-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
T$unplaced 261|g in {+252}Cf SF decay observed with T{-1/2}=4 ns (1970Jo20). Other: 3.4 ns {I6} also for unplaced 261|g (1974ClZX) 
J$(E2) 261|g to (9-) 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (11-)
level_comment:
T$unplaced 261|g was observed in 1970Jo20 with T{-1/2}=4 ns and in 1972ClZN with T{-1/2}=3.4 ns {I6}. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
%|b{+-}n from 1993Ru01. Other: 6.97 {I42} (1989BrZI) from 1989BrZI. 
J$from systematics. Possible configuration=(|p g{-7/2}){+3}. 
T from 1974Ru08, 1974Gr29, 1970OsZZ. Others: 24.4 s {I4} (1959Pe28), 24.7 s {I2} (1971De35), 24.3 s {I8} (1974Kr21), 24.8 s {I2} (1975As04), 24.25 s {I12} (1976Lu02) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
%B-N$from ratio of total number of decays resulting in {+136}Xe recoil ions over the total number of |b decays; weighted average of results from different methods to determine the total number of |b decays: 6.80 {I88} from number of {+137}Xe recoil ions, 6.88 {I105} from number of |b-delayed |g rays (1218|g and 1220|g following {+137}I |b-decay) and 6.95 {I76} from number of |b singles events from trapped {+137}I. Other: Adopted Levels of {+137}I in ENSDF database give %|b{+-}n=7.14 {I23}. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
%B-N$measured by 2016Ag03 from the number of neutrons detected in coincidence with |b particles by measuring precise ratio of detection efficiencies of |b and neutrons using well-known %|b{+-}n values from the decays of {+88}Br, {+94}Rb, and {+95}Rb. Other: 7.14 {I23} in Adopted Levels of {+137}I in the ENSDF database, taken from 1993Ru01 (At. Data and Nuc. Data Tables 53, 1) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
%B-N$recommended value by 2020Cz01 from the ratio of the total number of decays resulting in {+136}Xe recoil ions over the total number of |b decays |b{-nr}, the latter determined by |b-ion coin with longer TOFs typical of |b and |g events. Other values from 2020Cz01: 6.13 {I49} (for total number of |b decays from trapped {+137}I ions n{-|b}; and 7.16 {I96} (for |b|g-coin events from trapped {+137}I ions |n{-|b|g}). Compiler's note: weighted average of all the three values is 6.66 {I49}. The recommended value of %|b{+-}n=7.18 {I56} in 2020Cz01 can be compared with 7.63 {I14} in 2020Li32 (Nucl. Data Sheets 168, 1) evaluation, where value from 2020Cz01 was considered. 
J$From {+137}I Adopted Levels in the ENSDF database (Oct 2006 update) 
T$from 2020Li32 evaluation 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<2171 {I18} from Q(|b{+-})({+137}Te)-S(n)({+137}I), where Q(|b{+-})=7053 {I9} and S(n)=4882 {I16} from 2021Wa16. This represents a range of unobserved levels that subsequently decay to {+136}I via one-neutron emission. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
J$from direct |b feeding to 0+ and 2+ levels in {+138}Xe and shell-model calculations (2007Rz01) 
T$weighted average of 6.23 s {I3} (1993Ru01), 6.46 s {I15} (1976Lu02), 6.5 s {I2} (1975As04), 6.33 s {I8} (1975Kr17,1971Kr22), 6.40 s {I17} (1974NoZR), 6.21 s {I20} (1974Kr21), 6.30 s {I29} (1970WiZN). Others: 6.62 s {I9} (1974Gr29), 6.9 s {I24} (1970Lu05), 6.3 s {I7} (1959Pe28), 5.6 s {I1} and 6.5 s {I4} (1949Su14) 
$%|b{+-}n: weighted average of 5.32 {I20} (2011Go37), 5.56 {I22} (1993Ru01), 5.5 {I4} (1980Lu04), 5.1 {I30} (1980ReZQ). Others: 5.3 {I2} (1979RuZQ, compilation), |?5.4 (2010MaZS), 2.58 {I22} (1975As04), 4.5 {I9} (1974Kr21,corrected), 4.5 {I10} (1972Sc48,corrected) 
$Configuration=|pg{-7/2}~#|nf{-7/2} (2007Rz01) 
$Theoretical T{-1/2}=11.5 s, %|b{+-}n=2.4 (2003Mo09) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: S
level_comment:
%B-N$recommended value by 2020Cz01 from the ratio of the total number of decays resulting in {+136}Xe recoil ions over the total number of |b decays |b{-nr}, the latter determined by |b-ion coin with longer TOFs typical of |b and |g events. Other values from 2020Cz01: 5.82 {I55} (for total number of |b decays from trapped {+138}I ions n{-|b}; and 6.34 {I86} (for |b|g-coin events from trapped {+138}I ions |n{-|b|g}). Compiler's note: weighted average of all the three values is 6.13 {I50}. The recommended value of %|b{+-}n=6.18 {I50} in 2020Cz01 can be compared with 5.30 {I21} in 2020Li32 (Nucl. Data Sheets 168, 1) evaluation, where value from 2020Cz01 was considered. 2020Cz01 compared their recommended value with six previous measurements from 1964 to 2011. Note that measured values of %|b{+-}n=4.98 {I18} in 2017AgZZ (Proc. Intern. Conf. Nuclear Data for Science and Technology, ND201) and 5.56 {I22} in 1993Ru01 (At. Data Nucl. Data Tables 53, 1), and the recommended value from 2020Wa04 are in disagreement. 
J$From {+138}I Adopted Levels in the ENSDF database (Sept 2017 update) 
T$from 2020Li32 evaluation 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
J$syst of {+137}I, {+139}Cs, and {+141}Cs. Supported by suggestion of 1980KeZQ that there is no direct feeding of the {+139}Xe 3/2- g.s. based on agreement of E{-|b} from singles and from |b-528|g and by <E{-|b}> measurement of 1982Al01. 
T$from timing of |b and neutrons (1993Ru01). Others: 2.29 s {I2} (1980Al15, timing of |b, |g and neutrons); 2.30 s {I5} (1976Lu02), 2.4 s {I2} (1975As04), 2.47 s {I15} (1974Gr29), 2.27 s {I27} (1974Kr21), 2.0 s {I5} (1971BrXW), 2.0 s {I4} (1958Co72), 2.7 s {I1} (1949Su14). Weighted average of all the values, except from 1949Su14, is 2.284 s {I10} with a |h{+2}=0.5. 
%B-N$weighted average of 15% {I3} (1972Sc48), 10% {I3} (1974Kr21), 10.2% {I9} (1975As04), 9.5% {I6} (1980Lu04,1976Lu02,1974Ru07), 9.1% {I7} (1980Al15,1981Ho07), and 10.3% {I4} (1993Ru01). Others: 1959Pe28, 1958Co72 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: S
level_comment:
J assigned by 1999Li18 based on significant |b{+-} to {+140}Xe 2+, 4+, and 6+ levels (|b|g|g(t) method), for which no values are given (possibly in their Ref. [16] "to be published", not retrieved by evaluator, probably unpublished; H. Mach confirmed to evaluator in Dec. 2005 that there is supplementary unpublished data). This value updates the formerly evaluated values, (3) (1994Pe19), and (3)(-) (2003Au02) 
T from 1976Ah01. Others: 0.88 s {I13} (1974Kr21), 0.86 s {I14} (1970HeZH), 0.88 s {I12} (1970WiZN) 
$Delayed neutron emission probability=7.60% {I28} (2017AgZZ); Others: 9.3% {I10} (1993Ru01,1983ReZX,1984Ma39), 9.2% {I6} (1980Al15), 21.7% {I56} (1978Kr15); see also 1976NiZZ, 1975Is03, 1974Kr21, 1973To16 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2-)
level_comment:
$Decay modes of this state are not known 
E,J$based on beta-decay feeding from {+140}Te parent 0+ g.s. and |g transitions from the levels populated by |b{+-} decay, 2017Mo19 propose this level with J|p=(2-), different from the known (4-) {+140}I g.s. with half-life of 0.86 s. Energy and half-life of the (2-) state are not given by 2017Mo19, but the authors refer about this state to a private communication (their reference 17). Consequently this level is assumed at higher energy than the (4-) g.s. (hence this level scheme is built on the 0.0+x level) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (2-)
level_comment:
E,J$based on beta-decay feeding from {+140}Te parent 0+ g.s. and |g transitions from the levels populated by |b{+-} decay, 2017Mo19 propose this level with J|p=(2-), different from the known (4-) {+140}I g.s. with half-life of 0.86 s. Energy and half-life of the (2-) state are not given by 2017Mo19, but the authors refer about this state to a private communication (their reference 17). Consequently this level is assumed at higher energy than the (4-) g.s. (hence this level scheme is built on the 0.0+x level) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+140}I g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with T{-1/2}=860 ms {I40} from 1976Ah01 (Jour. Inorg. Nucl. Chem. 38, 191), same value adopted in Nov 2018 ENSDF update of {+140}I. 
$2020Li32 (evaluation): Nucl. Data Sheets 168, 1 (2020). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay $ Measured %|b{+-}n=7.6 {I9}(stat) {I27}(syst) from |n{-|bR} events; and 8.1% {I35} from |n{-|bR}) and |n{-|b} events. 2020Wa04 recommend the former value, where the statistical and systematic uncertainties are added in quadrature. Comparison with four previous measurements of %|b{+-}n values in literature from 1970 to 1980, and an evaluation in 2002 (2002Pf04). Other: %|b{+-}n=7.88 {I43} in 2020Li32 evaluation (Nucl. Data Sheets 168, 1 (2020), which includes the value from 2020Wa04 
E$the observed activity is assumed to correspond to {+140}I g.s. 
J$from {+140}I Adopted Levels in the ENSDF database (Nov 2018 update) 
T$from 2020Li32 (Nucl. Data Sheets 168, 1) evaluation 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (0-,1)
level_lifetime_unit: S
level_comment:
T$from 3 component fit to {+140}Te-377|g(t) fixing the {+140}Te and {+140}I g.s. half-lives (2022Ya13). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
Delayed neutron emission probability=21.2% {I30} (1980Al15), 21.3% {I32} (1989BrZI). Others: 39% {I13} (1978Kr15), 30% {I17} (1974Kr21); see also 1977Ru10, 1974Ru07, 1969ScZY 
T$From 2020Wu04 fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods and confirmed by the method of gating the |b-delayed |g rays. Data analysis included contributions from the parent, daughter and grand-daughter decays, as well as a constant background. Others: 0.43 s {I2} (1980Al15), 0.48 s {I3} (1976Lu02, same group), as well as (common authors) 0.42 s {I8} (1976Ah01), 0.45 s {I10} (1975Kr17), 0.41 s {I8} (1974Kr21), 0.43 s {I8} (1970HeZX) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}=100 %|b{+-}n=? 
T$from 2006KeZZ 
From systematics of neighboring nuclides 2003Au02 suggest J|p=2- 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+142}I g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with preliminary T{-1/2}=222 ms {I12} from 2006KeZZ (Annual Rept. GSI-2006-1, p154), same value adopted in Aug 2011 ENSDF update of {+142}I. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
J|p=7/2+ expected from systematics of odd-A Iodine nuclides. 
T Measured decay of |b{+-} radiation (2006KeZZ). Other value: T{-1/2}>300 ns, from time-of-flight measurements (1994Be24, 2003Au02). 
|b{+-} decay from 1994Be24, 2006KeZZ. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+143}I g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. Authors compared their result with preliminary T{-1/2}=130 ms {I45} from 2006KeZZ (Annual Rept. GSI-2006-1, p154), same value adopted in May 2011 ENSDF update of {+143}I. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T$it has to be of the same order or larger than the flight time through the spectrograph, which for this experiment was 300 ns 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+144}I g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Measured |s=3.10 nb (2010Oh02), systematic uncertainty|?30% 
T$ lower limit from time-of-flight in 2010Oh02, as communicated to the evaluator by T. Kubo in an e-mail reply of July 14, 2010. Actual half-life is expected to be much longer as suggested by the calculated values of 53 ms (1997Mo25), 57 ms (2002Pf04) 
J$ 1/2- predicted in calculations of 1997Mo25 
$ Probability of misidentification of {+145}I isotope<0.001% (2010Oh02) 
$Calculated %|b{+-}n=42.80, %|b{+-}2n=0.26 (1997Mo25). Calculated %|b{+-}n=46.4 (2002Pf04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay 
E$the observed activity is assumed to correspond to {+145}I g.s. 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b|g-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
%B-$only the |b{+-} decay mode is expected and detected, followed by |b-delayed neutron decay, thus 100 |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=36.6 ms, %|b{+-}n=54, %|b{+-}2n=2 (2019Mo01) 
$Theoretical T{-1/2}=34.4 ms, %|b{+-}n=41.0, %|b{+-}2n=0.7 (2016Ma12) 
$A total of 128 counts were assigned to {+146}I, four events for spectrometer setting on Sn, and 124 for setting on Te. Probability of misidentification of this isotope is <0.01% for both the settings (2018Sh11) 
$Production |s=18.6 pb for Te setting, with 30% systematic uncertainty for |s value (2018Sh11) 
E$it is assumed that the observed events correspond to ground-state activity. 
J$0- or 3- from |W{-p}=3/2- and |W{-|n}=3/2- orbitals proposed in 2019Mo01 
T$from 2020Wu04, fitting the time distribution of (implanted ions)|b-correlated decay curves to the sum of activities of parent nuclei, daughter nuclei, grand-daughter nuclei, |b{+-}n daughter and grand-daughter nuclei, and a constant background. 


level_energy_unit: KEV
level_comment:
$Only |b{+-} decay mode is expected, followed by delayed-neutron decay, thus 100% |b{+-} decay mode is assigned by inference. 
$Theoretical values: T{-1/2}=48.1 ms, %|b{+-}n=90, %|b{+-}2n=1, %|b{+-}3n=0 (2019Mo01) 
$Theoretical values: T{-1/2}=27.7 ms, %|b{+-}n=39.8, 40.6; %|b{+-}2n=0.47, 0.55; %|b{+-}3n=0 (2021Mi17) 
$A total of 2 counts were assigned to {+147}I, for spectrometer setting on Te. Probability of misidentification of this isotope is 0.73% (2018Sh11) 
$Production |s=0.2 pb for Te setting, with 30% systematic uncertainty for |s value 
E$it is assumed that the observed events correspond to ground-state activity. 
T$>550 ns lower limit can be extracted from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 48.1 ms (2019Mo01) and 27.7 ms (2021Mi17). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+147}I is expected to be <0.5 s, based on measured half-lives of 2.28 s for {+139}I, 0.86 s for {+140}I, and 0.43 s for {+141}I, available in literature. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: US
level_uncertain: ?
level_comment:
$%|a decay assumed as 100% in 2018Au04. From theoretical |b-decay half-life of 184.4 ms and |a-decay half-life of 8.3 ps (2019Mo01), |e+|b{++} decay is expected to be negligible. However, 2p decay mode is possible from theoretical S(2p)({+108}Xe)=-1800 keV (2019Mo01) 
$2018Au04 reported observation of two recoil-|a correlated events, which were assigned to {+108}Xe |) {+104}Te |) {+100}Sn |a-decay chain, and on this basis half-lives of decays of {+108}Xe and {+104}Te were deduced. 2019Xi06 also reported observation of two recoil-|a correlated events, but stated that these may be due to {+108}Xe |) {+104}Te |) {+100}Sn |a-decay chain, or could also be due to |b-delayed proton emission from more abundant radioactivities 
T$weighted average of 58 |ms {I+106-23} (2018Au04, from time difference between a recoil implantation and subsequent decay event in the same pixel of DSSD using maximum-likelihood method); 30 |ms {I+57-12} (2019Xi06, from analysis of time distribution of implant-|a correlated curve by maximum-likelihood method). In each experiment, two correlated events were observed, with a tentative assignment in 2019Xi06. 
$E|a=4320 keV {I160} from weighted average of measured E|a=4.56 MeV {I26} and 4.23 MeV {I20} (for two correlated events in 2018Au04); and measured 4290 {I160} (from the two correlated events in 2019Xi06) 
$Measured production |s<130 pb (2019Xi06) for {+108}Xe, which, according to the authors is about an order of magnitude below the expected value of |?1 nb, based on earlier cross section measurements for neighboring isotopes, and theoretical predictions of the HIVAP fusion-evaporation code 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: MS
level_comment:
J$HF=3.8 {I11} to the excited J|p=(7/2+) level in the daughter {+105}Te nucleus, deduced using r{-0}({+105}Te)=1.672 {I22}, from HF=1.00 in {+110}Xe |a decay. Note that HF=9.0 {I18} to the J|p=(5/2+) ground state; systematics of neighboring odd-A Xe,Te and Sn isotopes 
CONF$|ng{-7/2} orbital 
T$From recoil-|a(|Dt) decay in 2006Li41 
$E|a=3918 {I9} (I|a=30 {I6}) and 4062 {I7} (I|a=70 {I6}) (2006Li41); E|a=3910 {I10} (I|a=31 {I7}) and 4063 {I4} (I|a=69 {I7}) (2010Da17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%A$from 2002Ma19, deduced by assuming %|a({+114}Ba)=0.9 {I3} and %|a({+106}Te)=100 
T$From recoil-|a(t) in 2007Sa36. Others: 110 ms {I+30-20} (from the least-squares fit of the theoretical time distribution to the experimental data) and 100 ms {I+30-20} (using grow-in and decay pattern) in 2005Ja03 (note that a value of 105 ms +35-25 was adopted in 2005Ja03) and 160 ms {I+290-60} (from the analysis of time correlations between {+114}Ba and {+110}Xe-{+106}Te |a-decay events) in 2002Ma19 
$E|a=3717 {I19} (2007Sa36), 3737 {I30} (1981Sc17) and 3730 {I30} (2002Ma19) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|a=64 {I35} (2002Ma19), deduced by assuming %|a({+114}Ba)=0.9 {I3} and %|a({+106}Te)=100 
$E|a=3737 {I30} (1981Sc17) and 3730 {I30} (2002Ma19) 
T$From adopted levels. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2016Ca33. Others: 93 ms {I3} (2007Sa36: Phys. Rev.Lett. 99, 022501); 105 ms {I+35-25} (2005Ja03: Eur. Phys.J. A23, 197); 160 ms {I+290-60} (2002Ma19) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$from 3480|a(t)(1981Sc17). Other: 0.89 s {I20} from 3580|a(t) (1981Sc17). Overlapping half-lives for the two |a groups do not allow interpretation as |a decay of two isomeric states in {+111}Xe, or |a decay of one {+111}Xe state to two levels in {+107}Te. No isomer are known in odd Xe with |a<121. 
%A$from 1994Pa11. From Gross |b decay theory of 1973Ta30, T{-1/2}(|e+|b{++})|?0.2 s to 1 s, so one expects roughly comparable |a and |b{++} decay modes. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
%A$symmetrized from %|a=0.8 +1.1-0.5 (1994Pa12) using the procedure adopted in 2012Wa38. Other: |?0.84 in 1978Ro19, but this value is tentative 
T$from 3185|a(t) in 1979Sc22. Other: 2.8 s {I2} from (|e+|b{++})-delayed |a(t) in 1978Ro19, but this value is more uncertain given the complexity of the spectra, as discussed in 1979Sc22. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
%A$from 1985Ti02, based on estimated limit for the reduced width. |ep and |b+|a derived from |ep/|a=500-1500 in 1985Ti02. Other: |ep=4.2 (1978Ro19). 
E$tentative g.s. assignment for 2.8-s activity (1973Ha37), the proton-to-|a intensity in |b-delayed particle is 830 {i50} (1979Ew02). 
T$from 1985Ti02. Other: 2.8 s {i2} (1973Ha37). 
J$tentative J|p from syst 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$ from Doppler-shifted intensities of 657|g (2013Pr01), assuming any feeding transitions had the same deformation as 1476 level 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
J$from comparison between measured and calculated absolute (|b{++})-delayed p intensity and p|g (709|g, {+114}Te) coin (1972Ho18,1972Ho19) 
T 18 s {I4} (1971Ho07) proton counting. Others: 19 s {I5} (1969Ha03), 12 s {I2} (1973LiZB) K| x ray (iodine) counting 
|b{++}p/|b{++}|a ratio=1100 {I300} (1979Ew02) on-line ms 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: ZS
level_lifetime_info: ;ERR=?
level_comment:
E$other: 3900 from Bayesian method analysis 
T$other: 2.3 zs from Bayesian method analysis 
$|G=289 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: ZS
level_lifetime_info: ;ERR=?
level_comment:
E$other: 4900 from Bayesian method analysis 
T$other: 0.8 zs from Bayesian method analysis 
$|G=702 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: ZS
level_lifetime_info: ;ERR=?
level_comment:
E$other: 5600 from Bayesian method analysis 
T$other: 2.3 zs from Bayesian method analysis 
$|G=364 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: ZS
level_lifetime_info: ;ERR=?
level_comment:
E$other: 6100 from Bayesian method analysis 
T$other: 2.5 zs from Bayesian method analysis 
$|G=532 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: ZS
level_lifetime_info: ;ERR=?
level_comment:
E$other: 6600 from Bayesian method analysis 
T$other: 0.6 zs from Bayesian method analysis 
$|G=817 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: ZS
level_lifetime_info: ;ERR=?
level_comment:
E$other: 7300 from Bayesian method analysis 
T$other: 0.8 zs from Bayesian method analysis 
$|G=690 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from weighted average of |t=38.0 ps {I6} and |t=37.9 ps {I6} from ring 1 and ring 2 analysis, respectively (2023La11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from weighted average of |t=5.3 ps {I4} and |t=5.5 ps {I3} from ring 1 and ring 2 analysis, respectively (2023La11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$from a chi-squared minimization of experimental/simulated spectrum. Other: |t=1.4 ps {I9} from DDCM analysis, not adopted by 2023La11 because lifetime is similar to slowing down time. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
T$from a chi-squared minimization of experimental/simulated spectrum. Other: |t=0.7 ps {I5} from DDCM analysis, not adopted by 2023La11 because lifetime is similar to slowing down time. 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: S
level_comment:
$%|b{++}=35 {i10} (1975Ho03) disagrees with %|b{++}=72 (1986Ma41) 
T$61 s {i2} (1974Ha10), 65 s {i6} (1969Ha03) 
J$from LASER spectroscopy (1990NeZY), |p suggested by analogy with {+117,119,121}Xe 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$d |g to (5/2+). Could be (9/2+) as bandhead of the g7/2 band (1994To05), analogy with {+119}Xe and {+121}Ba (5/2+) [413] band 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T from 1976Be61. Previously reported values of 6 min {I1} (1965An05) and 6 min (1969Ho03) seem to belong to {+119}Xe 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=68.6 ps {I10} (2020Mu17), weighted average of 67.6 ps {I7} and 69.6 ps {I7} for two forward rings, as at backward rings, there was contamination from a 337.5-keV line in {+117}I. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=8.46 ps {I17} (2020Mu17), weighted average of 7.9 ps {I2}, 8.3 ps {I2}, 8.51 ps {I14} and 8.75 ps {I14}, for gate on 586.4|g, 6+ to 4+ transition. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=2.18 ps {I9} (2020Mu17), weighted average of 2.06 ps {I14}, 2.1 ps {I2}, 2.4 ps {I2} and 2.5 ps {I3}. Compiler's note: weighted average is 2.19 {I10}, or T{-1/2}=1.52 ps {I7} with an external uncertainty 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=1.17 ps {I13} (2020Mu17), weighted average of 0.8 ps {I3}, 0.9 ps {I8}, 1.0 ps {I6}, 1.0 ps {I3}, 1.2 ps {I3}, 1.3 ps {I3}, 1.4 ps {I4} and 1.8 ps {I4}. Two gates were set from above: one on 742.2|g from 10+ to 8+ and the other on 845.9|g from 9- to 8+ 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MIN
level_comment:
MOMM1 Corrected for diamagnetism (2005St24). Other value: -0.59 {I6}, static low-temperature nuclear orientation (1986ShZM,1989Ra17). 
%|b{++}=79 {I5} 
J strong |e+|b{++} feeding to 7/2+; syst of 5/2[402] state in the neighboring Xe isotopes 
T from 1976Be61. Other: 6 min {I1} (1965An05) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
J |g to (7/2-) and no |g to 5/2+ suggest (9/2-,11/2), and 11/2- expected band structure 
T from |g|g(t) in (HI,xn|g) (1982Ba31) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J E2 |g's to (5/2+) levels, no |g to (7/2+) and expected band structure 
T from |g|g(t) in (2001Ge01). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J (M1+E2) |g to (7/2-), no |g to (5/2+) and expected band structure 
T from |g|g(t) in (HI,xn|g) (1982Ba31) 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J From expected band structure; log| {Ift}>6.85 from 9/2+ is consistent with J|p=(13/2-) assignment 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
Negligible |e feeding is expected to this level. Experimental value from |g-ray transition intensity balance is 3% {I1}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+ 
T value from weighted av of 52.0 ps {I49} (from A. Dewald as quoted by 1995Wa25), 44.4 ps {I35} (1995Wa25), and 44.4 ps {I28} (1996Ma16); these values are based on RDM, except for 1995Wa25 (|g|g(t) in {+120}Cs |e decay). Others: 86 ps {I10} (1972Ku14), 84 ps {I8} (1980KaZT), and 84 ps {I18} (1985ChZY); these values based on RDM are in error due to an incorrect treatment of side feeding (1995Wa25) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J E2 |g to 2+ 
T based on RDM in (HI,xn|g). Value from weighted av of 6.1 ps {I12} (1972Ku14), 6.0 ps {I6} (from A. Dewald as quoted by 1995Wa25), and 5.6 ps (1995Wa25). Other: 7.6 ps {I9} (1980KaZT) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J E2 |g to 4+ 
T based on RDM, value is from 1995Wa25. Others: <3.5 ps (1972Ku14), 2.1 ps {I7} (1980KaZT), and 1.0 to 2.0 ps (from A. Dewald as quoted by 1995Wa25), 1.42 ps {I+45-28} (2000Pa63) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J E0 transition to 0+ 
T$from 1996Ma16 based on RDM. Other: 600 ns {I21} from (|b)(ce)(t) (1992Bh02) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J E2 |g to 6+ 
T weighted av of 0.91 ps {I17} from DSA (2000Pa63) and 1.3 ps {I4} from RDM (1987Ha17), in (HI,xn|g). Others: <1.4 ps (1980KaZT), <1.80 ps {I21} (1995Wa25) 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: MIN
level_comment:
$|m and Q from CFBLS (1990NeZY), reevaluated by 2005St24. Other: |m=-0.65{I3} (NO/S) (2005St24) 
T from 1972Mu03. Others: 38.8 min {I20} (1965An05), 40 min {I2} (1952Dr18), 34.0 min {I25} (1965Bu03), 38.8 min {I6} (1969Bu07) 
J$log| {Ift}|<5.7 from 3/2(+), M1+E2 |g from the 179.55 level, and log| {Ift}<6.0 from 9/2(+) give J|p=5/2(+) and 7/2(+) for the g.s. and 179.55 levels,respectively. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_comment:
J$E2 |g to 5/2(+); M1+E2 |g from (3/2+); Proposed as the band head of a 1/2+ band. 
T from |g(t) in ({+12}C,3n|g) 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: NS
level_comment:
J E1 |g to 5/2(+); log| {Ift}|<6.3 from 9/2(+) 
T unweighted average of 5.5 ns {I5} ({+112}Cd({+12}C,3n|g)) and 8 ns {I2} ({+121}Cs |e+|b{++} decay (155 s, 122 s)) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
Nuclear rms charge radius=4.7555 fm {i61} (2004An14) 
T from 1965An05. Others: 20 h {i1} (1952Dr18), 19.5 h (1952Ti25), 19.0 h {i5} (1954Ma75), 18.5 h {i5} (1960Mo09) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J J(1149):J(331):J(0)=0:2:0 sequence is established in (331.1|g)(817.9|g)(|q) in {+122}Cs |b{++} decay (21.18 s) (1979Si11); M2 character for 817.9 keV is unlikely rather than E2 character. 


level_energy_unit: KEV
level_spin_parity: (7)-
level_comment:
E$decay pattern of this level is different for 3.70-min Cs |b{++} decay and {+122}Te({+3}He,3n|g),{+110}Pd({+16}O,4n|g) 
J E1 |g to 6+, D |g to 8+; log| {Ift}=6.1 from 8(-) 


level_energy_unit: KEV
level_spin_parity: (20+)
level_comment:
E 843|g and 1020|g from this level establish the position of this level together with the cascade relations associated with the 6125 and 5851 levels. 
J |g's to (18+) 


level_energy_unit: KEV
level_spin_parity: (23+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-15+} ~#[|n(h{-11/2}){+4}]{-8+} 
J D(+Q) |g to (22+) 


level_energy_unit: KEV
level_spin_parity: (24+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}]{-8+} 
J Q |g to (22+) 


level_energy_unit: KEV
level_spin_parity: (25-)
level_comment:
J stretched Q |g to (23-) 
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+1}(g{-7/2}+d{-5/2}){+3}]{-9-} ~#[|n(h{-11/2}){+4}]{-16+} 


level_energy_unit: KEV
level_spin_parity: (25+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-15+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-1}(s{-1/2}){+1}]{-10+} 
J D(+Q) |g to (24+) 


level_energy_unit: KEV
level_spin_parity: (26+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-15+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-1}(s{-1/2}){+1}]{-11+} 
J |g to (24+) 


level_energy_unit: KEV
level_spin_parity: (27-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}]{-11-} 
J stretched Q |g to (25-) 


level_energy_unit: KEV
level_spin_parity: (28+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-1}(s{-1/2}){+1}]{-12+} 
J stretched Q |g to (26+) 


level_energy_unit: KEV
level_spin_parity: (29-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}{-13-} 
J stretched Q |g to (27-) 


level_energy_unit: KEV
level_spin_parity: (30+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-2}(s{-1/2}){+1} (d{-3/2}){+1}]{-14+} 
J stretched Q |g to (28+) 


level_energy_unit: KEV
level_spin_parity: (29-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}]{-13-} 
J (D) |g to (29-), |g to (27-) 


level_energy_unit: KEV
level_spin_parity: (30-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}]{-14-} 
J D(+Q) |g to (29-) 


level_energy_unit: KEV
level_spin_parity: (31-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+3}(d{-3/2}){+1}){-15-} 
J D(+Q) |g to (30-) 


level_energy_unit: KEV
level_spin_parity: (32+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}]{-16+} 
J |g to (30+) 


level_energy_unit: KEV
level_spin_parity: (23+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-15+} ~#[|n(h{-11/2}){+4}]{-8+} 


level_energy_unit: KEV
level_spin_parity: (24+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}]{-8+} 


level_energy_unit: KEV
level_spin_parity: (25-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+1}(g{-7/2}+d{-5/2}){+3}]{-9-} ~#[|n(h{-11/2}){+4}]{-16+} 
J (Q) |g to (23-) 


level_energy_unit: KEV
level_spin_parity: (25+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-15+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-1}(s{-1/2}){+1}]{-10+} 


level_energy_unit: KEV
level_spin_parity: (26+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-15+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-1}(s{-1/2}){+1}]{-11+} 


level_energy_unit: KEV
level_spin_parity: (27-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}]{-11-} 


level_energy_unit: KEV
level_spin_parity: (28+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-1}(s{-1/2}){+1}]{-12+} 


level_energy_unit: KEV
level_spin_parity: (29-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}{-13-} 


level_energy_unit: KEV
level_spin_parity: (30+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}(g{-7/2}+d{-5/2}){+-2}(s{-1/2}){+1} (d{-3/2}){+1}]{-14+} 


level_energy_unit: KEV
level_spin_parity: (29-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}]{-13-} 


level_energy_unit: KEV
level_spin_parity: (30-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+5}(g{-7/2}+d{-5/2}){+-1}]{-14-} 


level_energy_unit: KEV
level_spin_parity: (31-)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+3}(d{-3/2}){+1}){-15-} 


level_energy_unit: KEV
level_spin_parity: (32+)
level_comment:
$Possible admixture of non-collective state is suggested in 1994Ti01: configuration= [|p(h{-11/2}){+2}(g{-7/2}+d{-5/2}){+2}]{-16+} ~#[|n(h{-11/2}){+4}]{-16+} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 62 ps {i6} (1972Ku14), 48.5 ps {i14} (1994Pe02,1995Pe07), 50 ps {i3} (1998Go03); other: 35 ps {I+7-4} (1992Dr05) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$weighted average of 5.5 ps {i8} (1972Ku14), 3.7 ps {I+20-4} (1992Dr05), 4.5 ps {i2} (1994Pe02,1995Pe07), 5.5 ps {i10} (1998Go03) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.7 ps {i5} (1972Ku14), 1.04 ps {i14} (1994Pe02,1995Pe07), 2.0 ps 2 (1998Go03) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_comment:
E This level was displaced by +781 keV higher than from the placement in 1987Ha03, as proposed by 1997Se06, and as confirmed by 2003Mo27. 
J from 2003Mo27; DCO ratio for the 1007.4|g indicated mult.=Q 


level_energy_unit: KEV
level_spin_parity: 1/2(+)
level_lifetime_unit: H
level_comment:
J$spin from Collinear Fast Beam Laser Spectroscopy (1990NeZY); strong |b{++}+|e feeding from 1/2(+) in {+123}Cs; systematics of odd-mass xenon isotopes favors 1/2+ 
T$weighted average of 2.040 h {I9} (2021Ze01), 2.10 h {I3} (1969Bu07), and 2.08 h {I2} (1965An05). Others: 1.85 h {I3} (1960Mo09), 1.85 h {I10} (1962Pr09), 1.85 h {I5} (1965Bu03), 1.83 h {I15} (1967DaZY), and 2.23 h {I2} (1974Jo16), are discrepant 
MOMM1$from Collinear Fast Beam Laser Spectroscopy (1990NeZY) and 2014StZZ compilation. 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: PS
level_comment:
J$97.4|g M1, |DJ=1 to 1/2(+); strong |b{++}+|e feeding from 1/2(+) in {+123}Cs; spin=3/2 proposed by 1981Lu01 in ({+3}He,3n|g) and 1982Ze05 in ({+12}C,3n|g) based on |g(|q); systematics of odd-mass xenon isotopes also favors 3/2+ 
T$from ce-|g-coin in {+123}Cs |e decay (1987Fr10). 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: NS
level_comment:
J$180.6|g E2, |DJ=2 to 1/2(+), 83.4|g M1, |DJ=1 to 3/2(+) 
T$from ce-|g-coin in {+123}Cs |e decay (1987Fr10) 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E$the position of this isomeric state is proposed by 1981Lu01 in ({+3}He,3n|g), based on their observation of the 66.8|g from the 252 level in coincidence with the 266.4|g and 515.7|g both feeding the 252 level. It is proposed as 180+x by 1982Ze05 in ({+12}C,3n|g), feeding the 180 level with an unobserved transition of E=x. 
J$spin=7/2 from analysis of the quadrupole modulation spectra by 1982Ze05 in ({+12}C,3n|g); negative parity proposed in 1981Lu01 based on possible 57|g(M1)-21|g(M1) cascade from 263,(11/2-) level 
T$weighted average of 5.2 |ms {I5} (1982Ze05) in ({+12}C,3n|g), 5.6 |ms {I3} (1981Lu01) and 6.3 |ms {I5} (1970Ke01) in ({+3}He,3n|g). 
MOMM1,MOME2$from TDPAD in 1982Ze05. Value of |m does not include correction for dia-magnetic shielding or Knight shift; value of Q is relative to {+125}Xe (296,7/2+ level) (1982Ze05). See also 2014StZZ compilation 
MOMM1$quoted as -0.902 {I7} in 2014StZZ compilation 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
J$21.1|g to 7/2(-), 57|g M1+E2, |DJ=1 from (11/2-); systematics of 9/2- levels in neighboring odd-mass xenon isotopes. 
T$from |g(t) in ({+12}C,3n|g) (1982Ze05) 
MOME2$from model-independent ratio of Q(9/2-)/Q(7/2-)=0.80 {I40} from the analysis of the amplitude reduction and phase shift and Q(9/2-)=1.4 {I3} measured by TDPAD (1982Ze05). But 1.1 {I7} is quoted in 1982Ze05 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: NS
level_comment:
J$proposed as the band head of the h{-11/2} band by 1981Lu01 in ({+3}He,3n|g) based on systematics of observed h{-11/2} bands of neighboring odd-mass xenon isotopes 
T$from recoil-distance method (1982Ze05). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_comment:
J$261.8|g M1,E2 to 5/2(+), 442.6|g to 1/2(+); possible direct |b{++}+|e feeding from 1/2(+) in {+123}Cs 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_lifetime_unit: PS
level_comment:
J$455.8|g E2, |DJ=2 to (11/2-); probable band assignment 
T$from recoil-distance method in ({+12}C,3n|g) (1982Ze05). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2)
level_comment:
E$there is no evidence for two separate levels of 847.9 and 848.5 proposed by 2001Ga25 in ({+3}He,3n|g). So only a single level is adopted based on {+123}Cs |e decay 
J$848.0|g to 1/2(+), 667.8|g to 5/2(+); possible |b{++}+|e feeding from 1/2(+) in {+123}Cs 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$possible |b{++}+|e feeding from 1/2(+) in {+123}Cs; 610.3|g to 5/2(+), possible 481.0|g to 7/2(+) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J$617.0|g E2, |DJ=2 to (15/2-); probable band assignment 
T$from recoil-distance method in ({+12}C,3n|g) (1982Ze05). 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J$879.0|g D+Q, |DJ=1 to (13/2-), 821.9|g to (15/2-), 499.6|g to (11/2-), possible 247.1|g to (17/2-) 


level_energy_unit: KEV
level_energy_info: ;OFF=U;ERR=?
level_spin_parity: (31/2-)
level_uncertain: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$Decays to 2965, 27/2- and 3350, 27/2+ levels through unknown transitions. Level energy should be about 5.5 MeV (2002Ra34). 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: US
level_comment:
E$180+x in 1982Ze05. The position of this isomer is proposed by 1981Lu01 in {+123}Te({+3}He,3n|g), which is adopted in Adopted Levels. 
J$spin=7/2 from analysis of the quadrupole modulation spectra (1982Ze05) 
MOMM1$from g-factor=-0.256 {I2} and spin=7/2, without correction for dia-magnetic shielding or Knight shift (TDPAD,1982Ze05). See also 2014StZZ compilation 
T$from |g(t) of 97|g, 83|g and 180|g in 1982Ze05 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: NS
level_comment:
E$201+x in 1982Ze05 
T$from 21|g(t) in 1982Ze05 
MOME2$from model independent ratio of Q(9/2-)/Q(7/2-)=0.80 {I40} from the analysis of the amplitude reduction and phase shift and Q(9/2-)=1.4 {I3} (1982Ze05). But 1.1 {I7} is given in 1982Ze05 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: US
level_comment:
E$the position of this isomeric state is proposed by 1981Lu01 based on their observation of the 66.7|g in coincidence with 266.4|g and 515.7|g both feeding the 252 level. 
J$other: 1970Ke01 tentatively assign J|p=9/2- and E<250 keV to this isomer and proposed that this isomer feeds the 181 level by a M2 transition 
T$weighted average of 5.6 |ms {I3} from |g(t) of 97.3|g, 83.2|g and 180.6|g in 1981Lu01, and 6.3 |ms {I5} from 97.3|g(t) and 83.2|g(t) in 1970Ke01 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
$<r{+2}>{+1/2}=4.762 fm {i5} (2004An14, evaluation) 
T from 1990Ba22 for 2|b{++}(2|n) decay which is the fastest decay mode. The measurement was performed with ionization chamber filled with a mixture Xe+0.8%H2 gas. 1989Ba22 also reported T{-1/2}>2.0|*10{+14} y for the decay mode. For more details, see the table above. 
|D<r{+2}>=-0.242 {I5} fm{+2} (relative to {+136}Xe; 1989Bo03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+ 
T others: 44 ps {I+7-6} in Coul. ex.; 57 ps {I3}(1998Go03); 33 ps {I12}(1982GaZH). 2001Ra27 evaluation gives 52 ps {I3}. 
MOMM1 Ion implantation PAC (1975Go18,1989Ra17). Value relative to |m=+0.78 {I10} for 668 level in {+132}Xe. See also 2005St24 compilation. 
BE2 0.17(1998Go03) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J from |g(|q), E2 |g to 2+; g.s. band member 
T$ Others:2.1 ps {I2}(1998Go03); 3.5 ps {I4}(1982GaZH). 
BE2 0.67(1998Go03) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J from |g(|q), E2 |g to 4+; g.s. band member 
T$ Others:0.7 ps {I1}(1998Go03); 1.0 ps {I4}(1982GaZH). 
BE2 0.60(1998Go03) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J from |g(|q), E2 |g to 6+; g.s. band member 
T$ Others:0.5 ps {I2}(1998Go03); 1.0 ps {I4}(1982GaZH). 
BE2 0.39(1998Go03) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J from |g(|q), E2 |g to 8+ 
T Others: <0.4 ps deduced from lifetime <0.6 ps(1998Go03); 1.5 ps {I3}(1982GaZH). 
BE2 0.32(1998Go03) 


level_energy_unit: KEV
level_spin_parity: 13(-)
level_lifetime_unit: PS
level_comment:
J |DJ=2 |g to 11(-); |DJ=1 |g to 12(-); band assignment 
J from |g(|q), (E2) |g to 11(-) 
T other: 1.7 ps {I10}(1982GaZH). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G From ion implantation PAC 
T from B(E2) (1975Go18); others: 56 {I5} (2006Ch26) 
B(E2) from 2006Mu04; other: 0.90 {I7} (1975Go18) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From Adopted levels for {+124}Xe in ENSDF, based on value reported by 2004Sa47: Phys Rev C 70, 034313. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 6.1 ps {I5} and 6.0 ps {I5}, deduced using B(E2)(W.u.)(493|g)=64 {I5} and B(E2)(W.u.)(847|g)=1.45 {I12}, respectively in 2010Ra05. Other: 12.3 ps {I21} in Adopted levels for {+124}Xe in ENSDF (2004Sa47). The authors in 2010Ra05 communicated to the compiler that they were unable to reproduce the Coulomb excitation yield using the T{-1/2} value from Adopted levels for {+124}Xe in ENSDF (2004Sa47). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 5.8 ps {I12} and 6.0 ps {I15}, deduced using B(E2)(W.u.)(894|g)=2.33 {I38} and B(E2)(W.u.)(401|g)=95 {I19}, respectively in 2010Ra05. Other: 6.2 ps 7 in Adopted levels for {+124}Xe in ENSDF (2004Sa47) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 1.6 ps {I4} and 1.6 ps {I4}, deduced using B(E2)(W.u.)(915|g)=13.2 {I31} and B(E2)(W.u.)(422|g)=21 {I18}, respectively in 2010Ra05. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 2.1 ps {I4} and 2.2 ps {I4}, deduced using B(E2)(W.u.)(591|g)=66 {I12} and B(E2)(W.u.)(560|g)=35 {I6}, respectively in 2010Ra05. Other: 2.1 ps 7 in Adopted levels for {+124}Xe in ENSDF (1982GaZH: Thesis, Univ. Koln (1982)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$From B(E2)(W.u.)(670|g)=90 {I18} in 2010Ra05. Other: 1.29 ps 11 in Adopted levels for {+124}Xe in ENSDF (2004Sa47) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 1.8 ps {I3}, 1.75 ps {I25}, 1.8 ps {I3} and 1.8 ps {I4}, deduced using B(E2)(W.u.)(1629|g)=0.315 {I49}, B(E2)(W.u.)(1274|g)=0.613 {I68}, B(E2)(W.u.)(750|g)=5.55 {I79} and B(E2)(W.u.)(782|g)=3.54 {I71}, respectively in 2010Ra05. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.26 ps {I4} and 0.27 ps {I5}, deduced using B(E2)(W.u.)(1336|g)=11.9 {I17} and B(E2)(W.u.)(843|g)=18.5 {I17}, respectively in 2010Ra05. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 1.16 ps {I48}, 1.16 ps {I45}, 1.19 ps {I57} and 1.19 ps 46, deduced using B(E2)(W.u.)(1131|g)=2.75 {I84}, B(E2)(W.u.)(1978|g)=0.11 {I2}, B(E2)(W.u.)(1624|g)=0.21 {I7} and B(E2)(W.u.)(1100|g)=1.47 {I38}, respectively in 2010Ra05. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>{+136,124}=0.269 fm{+2} {I42} (2018Si30). Uncertainty includes experimental shift, mass-shift correction, field-shift calculation and higher-order nuclear moments. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$from measured 1.18|*10{+22} y {I13}(stat){I14}(syst) for the 2|nECEC |e decay of {+124}Xe. Uncertainty combined in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 1/2(+)
level_lifetime_unit: H
level_comment:
J From collinear LASER-fast-beam spectroscopy (1990NeZY); log| {Ift}=5.6 from 1/2(+) 
T Weighted average of 16.8 h {I2} (1965An05), 17.3 h {I4} (1969Lu09). Others: 20 h {I1} (1950An05), 18.0 h {I4} (1952Be55), 17 h {I1} (1960Mo09) 
MOMM1 From collinear LASER-fast-beam LASER spectroscopy (1990NeZY). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 9/2(-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
J From collinear LASER-fast-beam LASER spectroscopy (1990NeZY); E3 |g to 3/2(+) 
T From {+125}Xe IT decay 
MOMM1 From collinear LASER-fast-beam LASER spectroscopy (1990NeZY). See also 2005St24 compilation. 
MOME2 From collinear LASER-fast-beam LASER spectroscopy (1990NeZY). See also 2005St24 compilation. 


level_energy_unit: KEV
level_spin_parity: 7/2(+)
level_lifetime_unit: US
level_comment:
T From {+122}Te(|a,n|g),{+123}Te(|a,2n|g) data set 
J From differential perturbed angular distribution (1983Al21) 
MOMM1 From g-factor of +0.264 by differential perturbed angular distribution (1983Al21). See also 2005St24 compilation. 
MOME2 Estimated from the relationship between B(E2) and Q using triaxial-rotor-plus-particle model (1983Al21) See also 2005St24 compilation. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (47/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x |? 8500 from level-scheme figure 2 of 2007Al37 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (49/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ y |? 9000 from level-scheme figure 2 of 2007Al37 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (53/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ z |? 10750 from level-scheme figure 2 of 2007Al37 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: (55/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ u |? 10750 from level-scheme figure 2 of 2007Al37 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (49/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ x |? 10020 from data sent as e-mail reply of Mar 11, 2011 and level-scheme figure 2 of 2011Al02 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (55/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ y |? 11010 from data received as e-mail reply of Mar 11, 2011 and from level-scheme figure 2 of 2011Al02 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (61/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ z |? 12605 from data received as e-mail reply of Mar 11, 2011 and from level-scheme figure 2 of 2011Al02 


level_energy_unit: KEV
level_spin_parity: 1/2(+)
level_lifetime_unit: H
level_comment:
T$from 188|g(t) and 243|g(t) reported as 16.87 h {I3} (stat) {I7} (syst) (2019Sz01); uncertainty added in quadrature by compiler. Value is average of 16.81 h {I8}, 16.84 h {I33}, 17.27 h {I31}, 16.87 h {I13}, 16.71 h {I11}, 17.02 h {I12}, 16.79 h {I8}, 16.94 h {I8} from 188|g(t) and 16.73 h {I9}, 16.97 h {I45}, 17.36 h {I32}, 17.17 h {I22}, 17.05 h {I19}, 16.95 h {I10}, 16.68 h {14}, and 17.02 h {I12} from 243|g(t), all from sources produced at different proton bombarding energies. 
J$from the Adopted Levels of {+125}Xe in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T lower limit is given as 1.9|*10{+22} y for the 2|n2K decay mode from the measurement with liquid xenon scintillation detector (2018Ab04) 


