# LEVEL

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}=671.9 ms, %|b{+-}n=13 (2019Mo01) 
$Theoretical T{-1/2}=1.305 s, %|b{+-}n=1.9 (2016Ma12) 
$A total of 15 counts were assigned to {+173}Tb for spectrometer setting on Pr, and 23 counts for setting on Gd. 
$Production |s=0.11 nb {I+7-4} for Pr setting, and 51 pb {I11} for Gd setting, with 50% systematic uncertainty on |s values (2018Fu08) 
E$it is assumed that the observed events correspond to ground-state activity. 
J$3/2+ from |W{-|p}=3/2+ orbital proposed in 2019Mo01 
T$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 672 ms (2019Mo01) and 1.31 s (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+173}Tb is expected to be <1 s, based on measured half-lives of 0.96 s for {+170}Tb, 1.24 s for {+171}Tb, and 0.76 s {I19} for {+172}Tb, available in literature. 


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}=460.8 ms, %|b{+-}n=21 (2019Mo01) 
$Theoretical T{-1/2}=870.2 ms, %|b{+-}n=4.4 (2016Ma12) 
$Only one count was assigned to {+174}Tb for spectrometer setting on Pr, and four counts for setting on Gd. 
$Production |s=10 nb {I+23-8} for Pr setting, and 8.2 pb {I+65-39} for Gd setting, with 50% systematic uncertainty on |s values (2018Fu08) 
E$it is assumed that the observed events correspond to ground-state activity. 
J$1- or 2- from |W{-|p}=3/2+ and |W{-|n}=1/2- orbitals proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 461 ms (2019Mo01) and 870 ms (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+174}Tb is expected to be <1 s, based on measured half-lives of 0.96 s for {+170}Tb, 1.24 s for {+171}Tb, and 0.76 s {I19} for {+172}Tb, available in literature. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: S
level_comment:
J$from comparison of experimental delayed proton spectrum to statistical model calculations (1999Xu05,2005Xu04) 
T$from the decay curve of p-221|g in {+138}Gd (1999Xu05,2005Xu04) 
$|b{-2}|?0.3 (from comparison of J|p to Nilsson diagrams, 1999Xu04) 
$Measured partial reaction cross sections via |b{++}p decay=160 nb (1999Xu05) with a quoted uncertainty of a factor of 2 
$Observed 221|g and 384|g, assigned to the decay of first 2+ and 4+ states, respectively in {+138}Gd (1999Xu05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
B2$other values: |?0.24 (2005Bi24) 0.244 (2003Fi05,2002Kr04), 0.23-0.24 (2003BaZZ,2002RyZX). Also, from the analysis of the proton radioactivity data, |b|?0.3 was deduced (1998Da03, 1999Ry04, 1999Ma05, 2000Bb02, 2000Kr07, 2001Es01). A similar conclusion was reached following the study of the high-spin data (2001Se03) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_uncertain: ?
level_comment:
E$according to {+140}Dy IT Decay dataset, the ordering of the 574-550 cascade is not well established. Alternate ordering gives E(level)=1616.1 


level_energy_unit: KEV
level_spin_parity: (8+)
level_uncertain: ?
level_comment:
E$ordering of the 574-550 cascade is not well established. Alternate ordering gives E(level)=1616.1 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: US
level_comment:
T$weighted average of 7.0 |ms {I5} (2002Kr04) and 7.3 |ms {I15} (2002Cu01) 
$Two-quasineutron configuration |n9/2{+-}[514]|n7/2{++}[404], K|p=8-, from 1999Xu01, 2002KrZU, 2003Kr22. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: S
level_comment:
$Produced in {+92}Mo({+54}Fe,|an) E=274 MeV (1984Ni03); and {+106}Cd({+40}Ca,|an) at E=232 MeV (2006Xu03) 
Measured |b-delayed protons in coincidences with Tb K| x ray (1984Ni03), observed |b-delayed protons in coin with {+140}Gd |g's: 329|g (2+ to 0+), 508|g (4+ to 2+) (1986Wi15); |g(x-rays) gated on |b-delayed protons and |b-delayed protons gated on 329|g of {+140}Gd daughter (2006Xu03) 
$E(p)=2.1-7.2 MeV (1986Wi15), E(p)=3.0-7.0 MeV (2006Xu03); other: 1984Ni03 
J from analysis of feeding of 2+ and 4+ in {+140}Gd by delayed protons from {+141}Dy |e decay and Nilsson model (1989Gi06); and respectively of 0+ g.s., 2+, 4+, and 6+, and configuration-constrained nuclear potential energy surfaces using Woods-Saxon-Strutinsky method (2006Xu03; they also allow 9/2+) 
T$from 1986Wi15 and 2006Xu03. Others: 1.0 s {I2} (1984Ni03), 0.8 s {I2} (1988WiZN) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
Delayed proton emission from observation of p-K| x ray(Tb) coin, %|e=10, %|b{++}=90 (1991Fi03,1988GiZV) 
T from 1991Fi03 (preliminary results 1988GiZV), 1986Wi15 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
T$From 2003Xu04. Other values: 4.1 s {I3} (1984Ni03), 3.2 s {I6} (1983Ni05). 
J$from systematics of N=77 nuclides (1997Au04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: US
level_comment:
T$From the decay of the 95-keV |g ray. Other value: 3 |ms {I2}, from the decay of the 86-keV |g ray. Both from 2005Ri17. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (23-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ possibly feeds 7272,22 and 6872,21 levels 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
Observed delayed protons with T{-1/2}=10 s and suggested that they may be assigned to |e decay of low-spin isomer (1984ScZT) 
T$from 108.1|g(t) in {+145}Tb. Others: 10.5 s {I15} (1993Al03), 10 s {I1} (1984ScZT) 
J$configuration=(|n 3s{-1/2}){+-1} (1989Vi02) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$wt av: 14.5 s {I10} (1993To04), 13.6 s {I10} (1982No08). Other: 18 s {I3} (1982Al07) 
J$configuration=(|n 1h{-11/2}){+-1} (1989Vi02) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J$10+ state is the only possible seniority-two configuration for the T{-1/2}=150 ms half-life (1982Gu07). 
T$from I|g(t) (1982Gu07) 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: MS
level_comment:
J$10+ state is the only possible seniority-two configuration for the T{-1/2}=150 ms half-life. Transitions feeding this state are not identified. If the 10+ state is populated by direct |b-feeding the value log| {Ift}=4.8 would be typical for an allowed |b-transition which corresponds 9+, 10+, or 11+ for {+146}Ho (3.9 s) (1982Gu07). Evaluators suppose this as less probable, see {+146}Ho 'Adopted Levels' dataset. 
T$from |g(t) (1982Gu07) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
%B+P$other values: 2|*10{+-3} {I1} (1988WiZN); >0 (1984ScZT) 
MOMM1$measured by collinear fast beam laser spectroscopy - accelerated beam (quoted by 2019StZV from R. Neugart, Private Communication, 1987) 
T$from 1985Al08 other values: 40 s {I10} (1984ScZT), 67 s {I7} (1983ByZZ), 75 s {I4} (1983Al06). 1984ScZT is discrepant (this was adopted by 1992De38); the other values are in agreement but they are at least partially interrelated to each other as well as with 1985Al08 by authorship and experimental setup (1985Al08 and 1983ByZZ give identical results), reason for which the result of 1985Al08 is adopted. The average value by the limitation of statistical weights method of the three distinct values is 67 s {I9} close to the adopted value 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$(1/2+,3/2+) from M1 |g to (1/2+) g.s. (IT decay dataset); (3/2+) from nuclear structure configuration (d3/2+ orbital) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$750.5 measured by 2005Ge10 and 2006Bo41 from mass differences of {+147m}Dy and {+147g}Dy 
%IT$value from 1997Co21 by total absorption spectrometer; other values: 31 {I3} (1985Al08), |?40 (1976Ra07) 
MOMM1$measured by collinear fast beam laser spectroscopy - accelerated beam (quoted by 2019StZV from R. Neugart, Private Communication, 1987) 
MOME2$measured by collinear fast beam laser spectroscopy - accelerated beam (quoted by 2019StZV from R. Neugart, Private Communication, 1987) 
J$(M4) |g to (3/2+), 72; analog to 11/2-, 83 s, 748 isomer in {+145}Gd (see Adopted Levels) 
T$weighted average of 55.7 s {I7} (1993Al03,1985Al08), 54.4 s {I5} (1984ScZT), 55.7 s {I5} (1983ByZZ); other values: 57 s {I4} (1982Kl03), 59 s {I3} (1976Ra07) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$log| {Ift}|?5.1 from (11/2-) parent (|b{++} dataset, 1982No08); |g's to (7/2-), 1145 and to (7/2+), 1336, respectively 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T unweighted average of 3.1 min {I1} (1975To03) and 3.5 min {I2} (1974GrYZ,1974La32,1975Gr35) 
$Rms charge radius <r{+2}>{+1/2}=5.0538 fm {I2030} (2004An14); others: see 2000Ga58 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius=5.06 fm {I24} (2013An02) 
$Evaluated difference in charge radius: |d<r{+2}>({+148}Dy,{+149}Dy)=+0.119 fm{+2} {I13} (2013An02) 
J$f{-7/2} neutron state (1994Me13); allowed |e feeding to 5/2- levels (1728, 1876) levels and 9/2- level (1841) in {+149}Tb 
T$weighted average of 4.2 min {I2} (1993Al03), 4.1 min {I2} (1975To03), 4.6 min {I4} (x ray(t)) and 5.1 min {I9} (|a(t)) (1973Bi06). Other: 8 min {I2} (1958To27,1959To27) 
T$decay of fully-ionized atoms (where %|b{++}=100) was detected by 2003Li42; but half-life could not be measured since it is too long compared to the storage times possible in their experiment. With %|e=0, predicted T{-1/2} of bare atom is 40 min {I5} (2003Li42) 
MOMM1,MOME2$1989Ra17 compilations quotes |m and Q from Neugart et al. (priv. comm. 1987) who used collinear laser-spectroscopic technique. The same values are quoted by 2019StZV and 2021StZZ. 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: NS
level_comment:
J$E3 1073.2|g to 7/2-; probable member of configuration=|nf{-7/2}~#(3- in {+148}Dy) multiplet (1994Me13,1980Da18). This state is also mixed with i{-13/2} neutron state (1980Da18) 
T$from |g|g(t) in ({+16}O,3n|g) (1980Da18). Other: 13 ns {I3} in (1976St01) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J$probable member of configuration=|nf{-7/2}~#(2+ in {+148}Dy) multiplet (1994Me13); evidence of |e+|b{++} feeding from (11/2-) parent 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
J$probable member of configuration=|nf{-7/2}~#(3- in {+148}Dy) multiplet (1994Me13); evidence of |e+|b{++} feeding from (11/2-) parent 


level_energy_unit: KEV
level_spin_parity: (11/2)+
level_comment:
J$probable member of configuration=|nf{-7/2}~#(3- in {+148}Dy) multiplet (1994Me13); 630.3|g M1(+E2) to (13/2)+ 


level_energy_unit: KEV
level_spin_parity: (17/2)+
level_comment:
J$E2 1178.6|g to (13/2)+ 
$Configuration=|ph{-11/2}~#|ps{-1/2}~#|nf{-7/2} (1983JuZY) or configuration=|nf{-7/2}~#(5- in {+148}Dy) (1980Da18) 


level_energy_unit: KEV
level_spin_parity: (21/2)+
level_comment:
J$E2 298.6|g to (17/2)+ 
$Configuration=|ph{-11/2}~#|pd{-3/2}~#|nf{-7/2} (1983JuZY) or configuration=|nf{-7/2}~#(7- in {+148}Dy) (1980Da18) 


level_energy_unit: KEV
level_spin_parity: (27/2)-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$E3 110.5|g to (21/2)+ 
T$from |g|g(t) and |g(t) in {+149}Dy IT decay. For fully-ionized {+149}Dy{+66+}, T{-1/2}=11 s {I1} (2003Li42) 
$%IT from %|e+%|b{++}=0.7 {I3} in 1988Ba02 
$Configuration=|ph{-11/2}{+2}~#|nf{-7/2} (1983JuZY) or configuration=|ph{-11/2}{+2}~#(10+ in {+148}Dy) (1980Da18) 
$For fully-ionized atom, %|e=0 (2003Li42) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_comment:
J$probable member of configuration=|ph{-11/2}~#|nh{-9/2}~#|ps{-1/2} multiplet (1994Me13); possible allowed |b feeding from (1/2+) parent 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J$1753.4|g to (13/2)+, 2827.4|g to 7/2-; allowed |e+|b{++} transition from (11/2-) parent; probable member of configuration=|ph{-11/2}{+2}~#|nh{-9/2} multiplet (1994Me13) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J$3079.1|g to 7/2-, 2006.0|g to (13/2)+; allowed |e+|b{++} transition from (11/2-) parent; probable member of configuration=|ph{-11/2}{+2}~#|nh{-9/2} multiplet (1994Me13) 


level_energy_unit: KEV
level_spin_parity: (29/2)+
level_comment:
J$|DJ=1, E1 984.2|g to (27/2)- 
$Configuration=|ph{-11/2}{+2}~#|nf{-7/2}~#(3- in {+148}Dy) (1983JuZY,1980Da18) 


level_energy_unit: KEV
level_spin_parity: (49/2+)
level_lifetime_unit: NS
level_comment:
J$from systematics of N=83 isotones, see figure 4 of 2002Go06 in {+141}Pr({+16}O,p7n|g). The location of this isomer proposed by 2002Go06 is still tentative due to tentative connections of the 28-ns isomer with the low-lying levels 
T$|g|g(t); weighted average of 29 ns {I3} (1979Ha29), 36 ns {I8} (1980Da18), 25 ns {I5} (1980Ja16) and 28 ns {I3} (1981Ha17). Other: 50 ns {I15} (1976St01). See {+152}Gd(|a,7n|g) dataset 
MOMM1$from TDPAD (2003Wa28) using pulsed {+132}Xe beam 
$Configuration=|p(h{-11/2}){+2} ~# |n(f{-7/2},h{-9/2},i{-13/2},d{-3/2}{+-2}(0)) gives calculated g=0.46 (2002Go06) 


level_energy_unit: KEV
level_spin_parity: (27/2)-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$adopted value from weighted average of 0.500 s {I30} (1976St08), 0.510 s {I10} (1980Ja16), 0.47 s {I1} (1987BaZV). Other: for fully-ionized atom, T{-1/2}=11 s 1 (2003Li42) 
$Configuration=|ph{-11/2}{+2}~#|nf{-7/2} (1976St08,1980Da18) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (45/2-)
level_lifetime_unit: NS
level_comment:
E$x assumed as 80 (1996Gu17); but in 2002Go06 two tentative cascades have been proposed, defining the isomer at 8520 (see the Adopted Levels), implying x=1108 
J$(49/2+) in the Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (61/2)
level_uncertain: ?
level_comment:
E$this level is not included in the Adopted Levels, as the level proposed by 1996Gu17 from the placement of 1143.6|g, which has been placed from the 6893 level by 2002Go06 in ({+16}O,p7n|g), with the latter being adopted 


level_energy_unit: KEV
level_spin_parity: (49/2+)
level_lifetime_unit: NS
level_comment:
G$TDPAD method (2003Wa28) with a pulsed {+132}Xe beam; 984.9|g and 1393.5|g used for measurement 
$Configuration= |ph{-11/2}{+2}~#|n(f{-7/2}h{-9/2}i{-13/2}d{-3/2}{+-2}(0)) gives calculated g=0.46 


level_energy_unit: KEV
level_spin_parity: 27/2-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$adopted value from weighted average of 0.500 s {I30} (1976St08), 0.510 s {I10} (1980Ja16), 0.47 s {I1} (1987BaZV) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (49/2+)
level_lifetime_unit: NS
level_comment:
E$1983JuZY suggest x<80. {I8520} level in the Adopted Levels 
T$weighted average of 36 ns {I8} (1980Da18) and 50 ns {I15} (1976St01) 


level_energy_unit: KEV
level_spin_parity: 45/2,47/2,49/2
level_lifetime_unit: NS
level_comment:
E$this isomer corresponds to the 8520 level in the Adopted Levels 
T$weighted average of 29 ns {I3} (1979Ha29), 25 ns {I5} (1980Ja16) and 28 ns {I3} (1981Ha17). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
%A$|a-branch was determined by a comparison of |a-lines from parent and daughter in equilibrium (1977Ha48). 1974To07 give %|a=36 {I3} assuming 397 |g ray is 100% branch. Other: 1973Bi06. 
T$from 1973Bi06. 7.3~min {I1} given by 1982Bo04. 


level_energy_unit: KEV
level_spin_parity: (29-)
level_lifetime_unit: NS
level_comment:
T$the halflife of the isomeric state is determined using the centroid-shift method with the {+141}Pr({+16}O,p6n){+150}Dy reaction. 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: MIN
level_comment:
$ <r{+2}>{+1/2}=5.09 fm {I21} (2004An14 evaluation) 
MOMM1,MOME2$ from collinear fast-beam LASER spectroscopy (priv. comm. from Neugart to 1989Ra17). See also 2005St24 compilation 
J$spin from atomic beam magnetic resonance (1970Ro21). parity from probable shell model configuration=|nf{-7/2} 
T$from |a(t). Weighted average of values: 19.8~min~{I5} (1982Bo04), 17.5~min~{I5} (1978MoZH), 17~min~{I2} (1974PeZS), 16.9~min~{I5} (1973Bi06), 17.7~min~{I5} (1965Ma51) and 18.0~min~{I2} (1964Ma19). 


level_energy_unit: KEV
level_spin_parity: (41/2)
level_lifetime_unit: NS
level_comment:
J$|DJ=2, E2 |g to (37/2) 
T$from centroid-shift method in |g|g(t): weighted average of 6.0~ns~{I9} (1981Ha17), 5.5~ns~{I10} (1979Pi07) and 7~ns~{I2} (1979Li14). 


level_energy_unit: KEV
level_spin_parity: (49/2+)
level_lifetime_unit: NS
level_comment:
J$from theoretical considerations, This state is described as the maximally aligned valence nucleon state in analogy to {+148}Dy-{+152}Dy isotopes with configuration=[(|ph{-11/2}{+2}){-10+}~#(|nf{-7/2}) (|nh{-9/2})(|ni{-13/2})]{-49/2+} 
T$weighted average of 12.6~ns~{I5} (1981Ha17) and 10.9~s~{I6} (1979Li14). Others: 15~ns~{I3} (1979Pi07), 18~ns~{I4} (1979Ha29), 12~ns~{I1} (1980Bo07) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (43/2)
level_comment:
J$1993Ra07 suggest 43/2, 47/2. J=(51/2) (1988Ra19) from deexcitation out of band. An intensity plot given by 1994Tw01 (figure 11~b) suggests that 577|g is 51/2 to 47/2 transition 
Percent population=1.3 (1988Ra19), 1.0 (1995Ni06). Other: 2.3 8 (1992Mu10) in 122SN(34S,5NG) E=170 MEV 
T$estimated (1988Ra19) as<43~fs for deexcitation between top 9 transitions 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E$from intensity balance this level has a considerable negative feeding. This suggests that some of the |g rays feeding this level are perhaps placed incorrectly, since the level is known from (HI,xn|g) to decay with a single |g transition. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
$This level was introduced by 1979Pi07 on the basis of the 46.9-keV transition seen in ce data 
T$from centroid-shift method (1979Pi07) 


level_energy_unit: KEV
level_spin_parity: (49/2+)
level_lifetime_unit: NS
level_comment:
$ Possible configuration=(|ph{-11/2}{+2}){-10+}~#(|nf{-7/2}) (|nh{-9/2})(|ni{-13/2}) (1985Ho17) 
T$weighted average of 12.6~ns~{I5} (1981Ha17) and 10.9~s~{I6} (1979Li14). Others: 15~ns~{I3} (1979Pi07), 18~ns~{I4} (1979Ha29), 12~ns~{I1} (1980Bo07) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (43/2)
level_comment:
J$1993Ra07 suggest 43/2, 47/2. J=(51/2) (1988Ra19) from deexcitation out of band. An intensity plot given by 1994Tw01 (fig. 11~b) suggests that 577|g is 51/2 to 47/2 transition 
A REPORT OF AN SD BAND BY 1993Ma20 FROM 122CL(35CL,X) REACTION IS NOT INCLUDED HERE DUE TO QUESTIONABLE NATURE OF RESULTS GIVEN IN THAT PAPER 
T$estimated (1988Ra19) as<43~fs for deexcitation between top nine transitions 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T$weighted average of 2.41 h {I5} (1962Si14) and 2.37 h {I2} (1965Ma51). Others: 2.55 h {I17} (1972Fl09), 1960Ba31, 1958To27, 1957Su23, 1953Ra02 
%A from 1974To07 
$<r{+2}>{+1/2}=5.10 fm 22 (2004An14) 


level_energy_unit: KEV
level_spin_parity: 17+
level_lifetime_unit: NS
level_comment:
J$E2 |g to 15+. No transition to J<15. If J{+|p} were 16+, for example, one would have B(E2)(W.u.)=0.0016xBRANCHING, where branching is the branching ratio for the unobserved 658|g to the 14+ 4430 level 


level_energy_unit: KEV
level_spin_parity: (24+)
level_comment:
Q(intrinsic)=17.5 {I+4-2} (1997Ni01), 17.5 {I2} (1996Sa15), 18 {I3} (1991Be12) 
J$J{+|p}=24+ proposed by 1994Da20. Theoretical analysis suggests J=24 or 26 (1993Ra07) 


level_energy_unit: KEV
level_spin_parity: (24+)
level_comment:
J$from 2002La02. The same J|p was proposed by 1994Da20. Theoretical analysis suggests J=24 or 26 (1993Ra07). Others: J=25 (1991Ze01), (22+) (1991Be12) 
Feeding out of band: see 2002La02. Others: fraction of decay out of band: 0.21 (1989AlZS); 19% {I4} to the 25- level; 6% {I5} to the 23- level; 56% {I14} to the 21- level; 19% {I4} to the 19- level (1986Tw01); 75% of the deexcitation of the band is via the 60-ns isomer (1986Tw01); 35% {I15} of the |g flow from the SD states bypasses the 17+ 60 ns isomer (1987De17) 


level_energy_unit: KEV
level_spin_parity: (10)-
level_lifetime_unit: NS
level_comment:
J$From 2000Sm03. This assignment leads to J{+|p}=12- for the 3969 level. Earlier works assign 11- and 13-, respectively to these two levels. The 11- assignment was based on mult=E2 for the 254|g to the 2907~{I9}- level. 2000Sm03 argue that the 11- assignment makes the 3160 state far more yrast than their experimental observations suggest, and they reassign mult(254|g) as M1. The lead author of 1983St03 is one of the authors of 2000Sm03. IT should be noted that the 10- assignment requires mult=M2 for the 660|g from the 12+ 3820 level, and also for the 461|g from the 14+ 4430 level feeding the 3969 level 
T$1980Na04 report T{-1/2}=4.3~ns~{I9} from |g|g(t); however, in later works by the same authors, namely 1983St03, 1987St15, and 1988StZW, the level schemes show the value 3.9~ns. No uncertainty and no source are given. The evaluator assumes that the later value is a revision of that given in 1980Na04 and that the same uncertainty can be assigned 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
E$The relative order of the 622-633 cascade feeding the 3395 level, as proposed by 1991Be12, and giving a level at 4029.9 has been reversed by 2000Sm03, giving the level at 4016.9. the corrected sequence is given here 


level_energy_unit: KEV
level_spin_parity: (12-)
level_comment:
J$Proposed as 12- by 2000Sm03 on the basis of excitation energy arguments. |g(|q)(526|g) suggests stretched Q, however, the data are also consistent with a non-stretched dipole transition 


level_energy_unit: KEV
level_spin_parity: 17+
level_lifetime_unit: NS
level_comment:
T$Weighted average (ns) of 60~{I10} (1979Ja14), 49.5~{I14} (1979Me01, and 60~{I4} (1981Ha17), all from |g|g(t) 


level_energy_unit: KEV
level_spin_parity: 16+
level_comment:
E$The 565.8-546.5 cascade connecting the 5762 and 4650 levels, as given by 1991Be12, defines a level at 5195.8. The relative order of the cascade has been reversed by 2000Sm03 giving E(level)=5215.6. This reversed order is given here 


level_energy_unit: KEV
level_spin_parity: 21-
level_lifetime_unit: NS
level_comment:
T$Weighted average (ns) of 9.9~{I6} (1979Me01) and 9.5~{I7} (1981Ha17) from |g|g(t). Other 13~{I2} (1979Ja14) 


level_energy_unit: KEV
level_comment:
E$The 131|g-901|g cascade connecting the 11575 and 10541 levels and defining a level at 11443 in 2000Sm03, is reversed in 1986Ny02 (and in other earlier works), giving the intermediate level at 10673. The order in 2000Sm03 is adopted here 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: H
level_comment:
$<r{+2}>{+1/2}=5.10 fm 25 (2013An02,evaluation) 
J From 1970Ro21 atomic-beam magnetic resonance. |p=- suggested by analogy with N=87 isotones {+151}Gd and {+149}Sm. Probable configuration=(|n 2f{-7/2}). 
T Weighted average of 6.4 h {I2} (1964Ma19), 6.75 h {I15} (1965Ma51), 5.8 h {I9} (1967Go32), 6.29 h {I10} (1970Ch09). Other measurements: 1958An39, 1958Do61, 1958Go86, 1958To27, 1960Ba31, 1961Dz04, 1962Ry03, 1970Ro21. 
MOMM1$From 2014StZZ compilation based on a private communication from Neugart (by collinear fast beam laser spectroscopy - accelerated beam); other: -0.715 {I6} from reevaluation of data of 1972Ro36. 
MOME2$From 2016St14 compilation based on a private communication from Neugart (by collinear fast beam laser spectroscopy - accelerated beam); other: -0.15 {I9} from a reevaluation of data of 1972Ro36. 
%A From average of 0.0113% {I17} and 0.0083% {I13} (1974To07); others: 0.0033% {I2} (1960Ma47) and |? 0.004% (1960To05) which are much lower. 1991Ry01 evaluation recommends 0.009% {I4}. 
|D<r{+2}> can be read from a graph of 1985Ne09; these values are (152-153) |? 0.08 fm{+2}, (153-154) |? 0.24 fm{+2}, (151-153) |? 0.23 fm{+2}, and (153-155) |? 0.45 fm{+2}. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_comment:
J From E2 |g to 7/2(-) level and strong |e feeding from 1/2+ {+153}Ho (9.3 min). 
T From delayed coincidence in {+153}Ho |e decay (1978An25). 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J From M1 |g to (3/2-) level and E2 to 7/2(-). This value conflicts with the 1.8% |e+|b{++} branch (with log {Ift}=6.3) to this level from 11/2- {+153}Ho (2.01 min), however, this intensity may be incorrect due to incompleteness of the scheme. 
T From delayed coincidence in {+153}Ho |e decay (1978An25). 


level_energy_unit: KEV
level_spin_parity: (-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J From M1 |g to (3/2-,5/2-) level. Current {+153}Ho (9.3 min) decay scheme requires |e feeding from 1/2+ parent which would further limit J to 1/2 or 3/2; however, this scheme is very incomplete. 
T From delayed coincidence in {+153}Ho |e decay (1978An25). 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J From M1 |g to (3/2-) level and E2 to 7/2(-). Current {+153}Ho (9.3 min) decay scheme requires |e feeding from 1/2+ parent which would further limit J to 1/2 or 3/2; however, this scheme is very incomplete. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
E Original |e decay scheme has one level at 830 keV, but due to the |g decays from it, the evaluator proposes two levels. 
J The |g's to (13/2+) and 11/2(-) levels and possible |e feeding (with log {Ift}=6.0) from 11/2- parent. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E Original |e decay scheme has one level at 830 keV, but due to the |g decays from it, the evaluator proposes two levels. 
J From |g's to (3/2-) and (5/2-,7/2-) levels 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J From E2 |g to 13/2+ level and band assignment. 
T$From recoil-distance, plunger method (1977Ba77, (|a,xn|g)). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$9/2-,11/2-,13/2- from |e feeding (with log {Ift}=5.7) from 11/2- parent. 11/2-,13/2- less likely from |g to (5/2-,7/2-) level 


level_energy_unit: KEV
level_spin_parity: (9/2+,11/2-)
level_comment:
J From |g's to (5/2-,7/2-) and (13/2+) levels and |e feeding (with log {Ift}=5.7) from 11/2- parent. 


level_energy_unit: KEV
level_spin_parity: (21/2+)
level_lifetime_unit: PS
level_comment:
J From E2 |g to (17/2+) level and band assignment. 
T$From recoil-distance, plunger method (1977Ba77, (|a,xn|g)). 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_comment:
J From E2 |g to (21/2+) level and band assignment. 
T$From recoil-distance, plunger method (1977Ba77, (|a,xn|g)). 


level_energy_unit: KEV
level_spin_parity: (47/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J$From E2 |g to (43/2-) level. 
T From |g(t) in ({+34}S,5n|g) (1983Ko45). 
Probable oblate aligned-particle yrast isomer, analogous to those known in {+151}Dy and {+152}Dy. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$ J{-1} |? 59/2 (1995Ce03); others: 55/2 (1993Ra07,1992Wu05) 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: J2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$ J{-2} |? 61/2 (1995Ce03); others: 57/2 (1993Ra07,1992Wu05) 


level_energy_unit: KEV
level_comment:
E In the Adopted Levels, levels are placed at 829.93, with depopulating |g's of 117 and 192 keV, and 830.4, with depopulating |g's of 141, 253, and 721 keV. 
J The Adopted Levels are at 829.93 with J|p=(13/2+) and 830.47 with J|p=(7/2-). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 49/2
level_comment:
E 1991Zh35 has the 169.3 and 957.3 |g's in the opposite order, so "this" level is at 6549.1 keV; 1988CuZY has "this" level at 5761. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
|D<r{+2}>({+152}Dy-{+154}Dy)=0.285 {I25} fm{+2} and |D<r{+2}>({+154}Dy-{+156}Dy)=0.37 {I3} (1987Au06). Other: 0.297 {I94} and 0.39 {I14}, respectively, experimental values from compilation of 1995Ne12. See also 1996La03. 
$From an evaluation of data on nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.12~fm~{I26}. 
$E|a=2870 {I5} (recommended by 1991Ry01) 
T From evaluation of 1985HoZN and based on 1.5|*10{+6} y {I9} (revision of value from 1961Ma18) and 4|*10{+6} y (revision of value from 1971Go08). Others: 2.9|*10{+6} y {I15} (1965Ma51) and 10|*10{+6} y {I4} (1967Go32). Calculated T{-1/2}=1.2|*10{+6} y (1991Bu05). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$The |g branching is from the {+154}Ho |e decay. IT is very different from that observed in the heavy-ion study. 
J From E0 component in |g to 2+ level. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$The |g branching is from the {+154}Ho |e decay. IT is very different from that observed in the heavy-ion study. 
J From E0 component in |g to 4+ level. 


level_energy_unit: KEV
level_spin_parity: 1,2,3
level_comment:
E$See the comment in the {+154}Ho |e decay (11.76~min) data set regarding problems with this level. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J$E0 component in |g to 7+; M1 |g's to 6+ and 8+. Allowed-unhindered (log| {Ift}=4.9) |e transition from 3.10-min, 8+, isomer in {+154}Ho establishes configurations for both levels. 


level_energy_unit: KEV
level_spin_parity: 48+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Band-terminating state. Configuration: |p[(d{-5/2}/g{-7/2}){-6}{+-2}(h{-11/2}){-16}{+4}]{-22+}~# |n[(i{-13/2}){-12}{+2}(f{-7/2}){-6}{+2}(h{-9/2}){-8}{+2}]{-26+} (2009Pa17) 


level_energy_unit: KEV
level_spin_parity: 1,2,3
level_comment:
E$As reported by 1980Zo02. These authors report a 2318.43, 7+, level in the decay of the 3.10-m isomer. The |g-decay modes of these two states are quite different. Also, a 7+ level at this energy cannot be appreciably populated in the decay of the 11.76-m state in {+154}Ho. The evaluator concludes that this 2183.9 level is not the same as the 7+ level seen in the decay of the 3.01-m isomer and questions its existence, but has chosen to include it here anyway. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
E$Note that this is not the same as the 2183.9 level proposed to be populated in the decay of 11.76-m {+154}Ho. See the comment in that data set. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
S Relative to 100 for the ground state, the (p,t) "strength" (measured cross section divided by the DWBA cross section) for this state is 74 (1992Ta22). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
S Relative to 100 for the ground state, the (p,t) "strength" (measured cross section divided by the DWBA cross section) for this state is 16 (1992Ta22). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J atomic beam (1970Ro21). |p=- from L=1 in (d,t) (1976St06). 
T weighted average of: 9.59 h {I10} (1970Ch09); 10.3 h {I3} (1967Ha12); 10.0 h {I5} (1964Ma10); 10.2 h {I1} (1964Pe13). Others: 11 h {I2} (1958Dz02); 9 h {I2} (1958Do61). 
MOMM1 From 2014StZZ. 2014StZZ also list |m=-0.385 {I4} 
MOME2 From 2016St14. 
In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.1457 fm {I2751}. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J M1+E2 to g.s. Enhanced B(E2) to the g.s. indicates that this is a member of the g.s. band. The small (d,t) cross section to this level is expected for the 5/2- member of the 3/2[521] band. 
T from {+155}Ho |e decay 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J L=3 in (d,t) requires J|p=5/2- or 7/2-. The enhanced B(E2) of the transition to the g.s. and the (d,t) cross section indicate that this is the 7/2- member of the 3/2[521] band. 
T from {+155}Ho |e decay 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J E1 to 7/2-. Angular distribution in (d,t) is consistent with L=4, and transition from 13/2+ requires J|p=9/2+. 
T from 1982Ka36, |g(t) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
J L=6 in (d,t) requires 11/2+ or 13/2+. Large ({+3}He,|a) cross section indicates 13/2+ because of i13/2 character of the neutron orbitals involved. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T from {+155}Ho |e decay 
J M1 transitions to 5/2- and 7/2- require J|p=5/2- or 7/2-. If J|p were 5/2-, the 92.2|g would be M2 and would have B(M2)(W.u.)|>220, which violates RUL. Hence, J|p=7/2-. Note, however, that with this J|p value the 22.15|g must be pure E2, which is in disagreement with the reported mult. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T from {+155}Ho |e decay 
J L=2 in (d,t) indicates J|p=3/2+ or 5/2+. The large (d,t) cross section indicates that this is the 3/2[402] Nilsson state. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T from {+155}Ho |e decay 
J E1 transition to 3/2- and E2 to 9/2+. Coriolis-mixing calculations of 1976St06 indicate that this is the 5/2+ member of the "1/2[660]" band. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J L=0 in (d,t). The large (d,t) cross section to this level establishes it as the 1/2[400] Nilsson state. 


level_energy_unit: KEV
level_spin_parity: 5/2-,(3/2)-
level_comment:
J M1 transitions to 3/2- and 5/2- states. The existence of an M1 component in the 238.5|g to 7/2- would rule out 3/2-. Assigned as the 5/2- member of the 3/2[532] band by 1976St06. 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
J E2 to 13/2+. The population pattern in the in-beam studies establishes this as the 17/2+ member of the indicated band. 


level_energy_unit: KEV
level_spin_parity: 3/2-,(1/2)-
level_comment:
J L=1 in (d,t). Strong population in (d,t) suggests that this is the 3/2- member of the 1/2[530] band. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J L=3 in (d,t). The multipolarities of the two |g's tentatively placed from this level are not consistent with the proposed J|p value. See the comment regarding these |g's in the {+155}Ho |e Decay data set. 
E$Level population is uncertain in {+155}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J L=1 in (d,t). From Coriolis-mixing calculations, 1976St06 assign this as the 1/2- member of 1/2[530]. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J E1 transitions to 5/2+ and 5/2+,7/2+ states suggest J|p=3/2-,5/2-,7/2-. L=2,3 in (d,t) rules out 3/2-. 1976St06 propose 5/2-. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J L=(5) in (d,t). The strong population of this level in ({+3}He,|a), together with the observation of transitions with similar characteristics in several odd-A Gd isotopes, suggests that this is the 11/2- member of 9/2-[514]. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J from Cranked Relativistic Mean-Field Theory calculations, 1998Af02 suggest J=75/2-. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T$adopted value 
T from 1990AbZW,1990AbZS, |gce(t). Others: 3.4 ns {I1} (1979Al31), 5.5 ns {I3} (1972Ki21), |gce(t). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
Coriolis-mixing calculations of 1976St06 indicate that this may be the 5/2+ member of the "1/2[660]" band. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+&5/2-,(3/2)-
level_comment:
S this large value indicates that the bandhead of 1/2[400] is present in this peak 
L the strong contribution from L=0 obscures that from the other component. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+&1/2-,3/2-
level_comment:
L the expected contribution from the L=2 component is not large enough to affect the angular distribution (1976St06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 17/2+&3/2-,(1/2)-
level_comment:
Note that the 17/2+ level cannot be directly populated in single-nucleon transfer. 1976St06 suggest that it is populated by competing two-step processes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_comment:
The strong population of this level in ({+3}He,|a), together with the observation of transitions with similar characteristics in several odd-A Gd isotopes, suggests that this is the 11/2- member of 9/2-[514] 
S value at |q=40|' 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T$2011Be18 report an experimental lower limit for the half-life of the |a transition to the first 2+ state in {+152}Gd of 3.8|*10{+16} y. The model calculation of 1988Al13 gives T{-1/2}(|a)=4.3|*10{+24} y. Authors quote a measured limit of >1.0|*10{+15} y. From systematics of |a decay using a radius parameter extrapolated from {+150,152,154}Dy, one deduces T{-1/2}(|a)=2.2|*10{+24} y. 2011Be18 report measured lower limits for the half-lives of |e|e and |e|b{++} transitions, both 0|n and 2|n, to a number of levels in {+156}Gd. These range from |?1.8|*10{+14} y to |?7.1|*10{+16} y. 2002Hi09 calculate 2|n double |e decay for several deformed nuclei. For {+156}Dy, they compute T{-1/2}=2.74|*10{+22} y, 8.31|*10{+24} y, and 1.08|*10{+25} y, respectively, for 2|n |e decay to the g.s., the first excited 0+ state, and the second excited 0+ state of {+156}Gd. These values are also given in 1999Ce12, which involves some of the same authors. More recent calculations of various aspects of the "double-beta-decay" process are given by 2009Ra26, 2010Ra06, 2011Kr07 and 2011El05. These are discussed in the {+156}Gd data set. 2002Hi09 calculate 2|n |e decay for several deformed nuclei. For {+156}Dy, they report calculated upper limits for T{-1/2} values for the 2|n |e decay to the g.s., the first and second excited 0+ levels in {+156}Gd. 
The change in the mean square charge radius has been determined from optical isotope shift data. From 1987NeZW |D<r{+2}>(156-154)|?0.38 fm{+2} and |D<r{+2}>(158-156)|?0.20 fm{+2} (values read from plot by evaluator). From 1990Wa25, |D<r{+2}>(158-156)=0.199 fm{+2} {I10}. For the nuclear parameter, |l (which |? |D<r{+2}>), 1982Cl04 report |l(158-156)=0.215 fm{+2} {I12}. The compilation of 1987Au06 quotes values of |l(156-154)=0.37 fm{+2} {I3} and |l(158-156)=0.194 fm{+2} {I17}. 
$From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.16~fm {I25}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J E2 |g to 0+ gs; L=2 in (p,t). 
T$Computed from B(E2)|^=3.72 {I3} (1977Ro27) in Coul. ex. Others: 0.82~ns {I5} (1966Ab02) and 0.90~ns {I8} (1970Mo39), from {+156}Ho |e decay; and 0.74~ns {I4} (2006Mo22), from (HI,xn|g). 
MOMM1$From the evaluation by 1989Ra17. See also the compilation by 2005St24. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$The |g decay of this level is quite different from what is expected (and observed) for |g vibrations in other nuclides. This, together with an apparent E0 component in the transition to the 2+ member of the g.s. band, suggests that this state may be more than simply a |g vibration. 
J E2 |g to 0+, L=2 in (p,t). 
T$Computed from B(E2)|^=0.180~{I11} (1982Ro07) in Coul. ex. and the adopted |g branching. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
$2003KaZP report this level but give no other information about it. 2008VaZU, with many of the same authors, also list it but also provide no information other than what is given here. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$|g's to 0+, 2+, and 3+ levels. Presumed M1 |g to 2+ gives J{+|p}=2+. Evaluator associates this level with the 1385 level in (p,t), which was assigned J{+|p}=(3-) based on L=(3). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$|g's to 0+ and 4+ levels; L=2 in (p,t). Assigned as a "|b-|g" vibrational bandhead by 1977Ko04 from (p,t). 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$E1 |g to 4+ indicates J=3,4,5 and |p=-. Population in (d,d') indicates natural parity. Assignment requires |g to g.s. to be E3. In (p,t), L=(0) which implies J{+|p}=(0+). 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J$E2 |g's to 3+ and 4+ levels indicates |p=+. L=(4) in (p,t). Proposed in (p,4n|g) as a member of the "Super" band. However, 1977Ko04, (p,t), suggest that it is the bandhead of a K{+|p}=4+ band. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J$M1 |g to 3+ level indicates J{+|p}=2+,3+,4+. M1+E2 |g to 4+ rules out 2+. Probable excitation in (p,t) indicates natural parity. Note that L=(5) in (p,t). 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$E2 to 2+, possible M1 to 2+ and |g's to 4+ indicate |p=+ and J=2,3,4. L=(2) in (p,t) suggests J=2. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J$Feeding by stretched quadrupole (i.e. E2) transition from negative-parity level indicates |p=-. J=6 from proposed band assignment. Assigned as (6,7)+ in (p,4n|g). 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
J$E2 to 3+ indicates |p=+. Thus, this is not likely to be the (3-) level at 1927 in (d,d') and at 1934 in (p,t). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$L=(3) in (p,t). If J{+|p} is indeed 3-, then this level is not the same as the 2058 level in {+156}Ho |e decay, since this latter level has a decay |g to a 5+ level. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$|g's to 3+ and 5+ levels indicate J{+|p}=3+,4,5+. If the 2103 level in (p,t) is the same as the 2103 level in |e decay, then the implied natural parity gives 4+. 


level_energy_unit: KEV
level_spin_parity: 8-
level_comment:
J$Feeding by stretched quadrupole (i.e., E2) transition from negative-parity level indicates |p=-. J=8 from proposed band assignment. Assigned as 8+ in (p,4n|g). 


level_energy_unit: KEV
level_spin_parity: 10-
level_comment:
J From E2 |g to 8- level and expected band structure. Negative parity for this level and its associated band members is proposed by 1988Ri09, in (HI,xn|g), based on cranked shell-model and signature-splitting considerations. (Level assigned as 10+ in (p,xn|g) (1977De28).) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_comment:
$From log| {Ift}|?4.5 in {+156}Ho |e decay (7.6~min), conf = |n5/2[523]+|n11/2[505]. 
J$|g's to 6+ and 10+ levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-,6+
level_comment:
J$1968Gr08 report J{+|p}=(5-). If this peak corresponds to the 1526.1 level, then J{+|p}=5-. However, it may also contain a contribution from the 1525.2, 6+, level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3-)
level_comment:
L$Angular distribution in (p,t) is well described by L=3. If this is the same as the 2169 level in {+156}Ho |e decay (56~min), then band-structure arguments indicate J{+|p}=3+. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Assigned as a "|b-|g" bandhead by 1977Ko04, based largely on the relatively large (p,t) cross section. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
$Assigned as a K{+|p}=4+ bandhead by 1977Ko04. For another proposed configuration, see the Adopted Levels data set. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
L$Angular distribution is well described by L=3. If this is the same as the 2169 level in {+156}Ho |e decay (56~min), and the band-structure arguments there are correct, then J{+|p} would be 3+. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
$1977De28 assign this as a member of the S, or "Super" band. However, 2002Ca49, in {+156}Ho |e decay, do not confirm this level. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J$1976El13 report J{+|p}=3+,4+,5+. 1977De28 report J{+|p}=(4,5)+. Both assign this as a member of the S, or "Super", band. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J$1976El13 report 6+. 1977De28 report J{+|p}=(6,7)+. Both assign this as a member of the "Super" band. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 6.27~ps {I10} (2006Mo22); 7.8~ps {I6} (1979Wa12); and 9.1~ps {I+6-8} (1984Em02). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 2.29~ps {I7} (2006Mo22); 2.2~ps {I1} (1979Wa12); and 2.2~ps {I3} (1984Em02). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 1.17~ps {I8} (2006Mo22); 0.89~ps {I6} (1979Wa12); and 0.90~ps {I+28-14} (1984Em02). 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 0.72~ps {I5} (2006Mo22); 0.54~ps {I3} (1979Wa12); and 0.46~ps {I+10-8} (1984Em02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 0.49~ps {I10} (2006Mo22); 0.68~ps {I8} (1979Wa12); and 0.51~ps {I7} (1984Em02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 20+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.25~ps {I7} (2003Pe22) and 0.23~ps {I10} (1984Em02). Other: 0.19~ps (1979Wa12). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 24+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 0.180~ps {I19} (2003Pe22) and 0.15~ps {I6} (1989Em01). Other: 0.39 {I6} (1984Em02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 26+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.132~ps {I24} (2003Pe22) and 0.11~ps {I3} (1989Em01). Other: 0.21~ps {I+7-6} (1984Em02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 28+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.085~ps {I17} (2003Pe22) and 0.11~ps {I3} (1989Em01). Other: 0.16~ps {I+7-6} (1984Em02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 30+
level_lifetime_unit: PS
level_comment:
T$Weighted average of: 0.060~ps {I15} (2003Pe22) and 0.080~ps {I10} (1989Em01). Other: 0.12~ps {I+6-4} (1984Em02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$weighted average of results from 5 different target-to-degrader and degrader-to-stopper measurements with TPEN operated in differential mode (2019Gi19). Other: 34.7 ps {I42} with TPEN operated as standard two-foil plunger (2019Gi19). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J J measured by atomic-beam magnetic resonance (1970Ro21) and |p from assignment as 3/2[521] state. 
T Weighted average of 8.2 h {I1} (1953Ha81), 8.06 h {I8} (1963Pe20), 8.2 h {I2} (1963Ra15), 8.2 h {I1} (1964Ma10), 8.3 h {I3} (1967Ha12), and 8.1 h {I1} and 8.1 h {I2} (1970Ro21). Others: 8.5 h {I5} (1958Do61) and |? 8 h (1957Go72). 
MOMM1 From 1989Ra17 evaluation and 2011StZZ compilation and based on priv. comm. (Neugart 1987) and 1972Ro36. Other: 0.32 {I2} (1961Na04,1962Na15). 
MOME2 From 1989Ra17 evaluation and 2011StZZ compilation and based on priv. comm. (Neugart 1987) and 1972Ro36. 
$RMS charge radius <r{+2}>{+1/2}=5.1709~fm~{I2936} (2013An02) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J From M1 |g to 3/2- level and band structure. 
T From {+157}Ho |e decay as quoted in 1980Al07; others: 90 ps {I30} (preliminary value of 1979AbZZ) and |<0.8 ns (1972Ki21). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J From M1 |g to 5/2- level and band structure. 
T From {+157}Ho |e decay as quoted in 1980Al07; other: |<50 ps (preliminary value of 1979AbZZ). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_comment:
J from E1 |g to 7/2- level and interpretation of charged-particle reaction data. 
T from Gd(|a,xn|g) by |g|g(t) (1974An11). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J From E1 |g to 3/2- level and E2 |g to 9/2+. 
T From Gd(|a,xn|g) by |g|g(t) (1974An11); other: 1.1 ns from {+157}Ho |e decay as quoted in 1980Al07. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J from (E1) |g to 9/2+ level, (E2) |g to 7/2-, interpretation of the charged-particle reaction data, and expected presence of 11/2-,11/2[505] state. 
T from IT decay (21.6 ms) by |g(t) and beam pulse-|g(t). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J From E1 |g's to 3/2+ and 7/2+ levels. The log {Ift}=4.86 {+157}Ho |e decay gives Nilsson orbital assignment uniquely. 
T From {+157}Ho |e decay as quoted in 1980Al07. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J From |g's to 7/2- and 9/2- levels, band structure, and interpretation of charged-particle reaction data. 


level_energy_unit: KEV
level_comment:
J Assigned as (5/2+) from interpretation of charged-particle data; however, configuration is not adopted. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J from M1 |g to 5/2- level and log {Ift}=6.6 from 7/2- level. If 379 |g has E0 component, J|p=(7/2)-. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J From interpretation of charged-particle reaction data, but same data used to support 3/2- assignment. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J From E1 |g to 7/2+, M1 |g to 5/2- level, strong |g to 9/2+, and interpretation of charged-particle reaction data. 


level_energy_unit: KEV
level_spin_parity: (57/2-)
level_comment:
E$THIS IS 7047 4 LEVEL THAT GETS MIXED UP WITH THE 7047 3 LEVEL IN THE BAND DRAWING OF THE FORMER, REASON FOR WHICH I ARTIFICAILLY MADE IT 7047.1 40 
J From |g to 53/2- level and band structure. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_comment:
T The measured values of 19.2 ms {I5} (1973Kl03), 24 ms {I1} (1971KiZQ), and 21 ms {I3} (1970Bo02) are inconsistent; their weighted average is 20.2, with an internal uncertainty of 0.4, a reduced-|h{+2} of 9.2, and an external uncertainty of 1.4. The evaluator has adopted the mean of the weighted average of 21.2 {I13} from the Normalized Residual Method (1992Ja06) and 21.9 {I19} from the Rajeval Method (1992Ra08); both of these methods increase the uncertainties of the more discrepant input values. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
T From 1980Al07 (and 1979AlZO). Others: 90 ps {I30} from ce|g coincidences (preliminary value of 1979AbZZ) and |< 0.8 ns from ce-ce coincidences (1972Ki21). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
T From 1980Al07 (and 1979AlZO). Others: |< 50 ps from ce|g coincidences (preliminary value of 1979AbZZ). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J Calculated mixing (1975Gr38) for 3/2[651], 5/2[642], and 1/2[660] is 54%, 24% and 19%, respectively. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J Calculated mixing (1975Gr38) for 3/2[651], 5/2[642], and 1/2[660] is 66%, 20% and 10%, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2+
level_comment:
J Calculated mixing (1975Gr38) for 3/2[651], 5/2[642], and 1/2[660] is 48%, 22% and 27%, respectively. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J Calculated configuration (1974Ny01) is 98% {I3}/2[532]. Original assignment 13/2+ (1970Gr46) and 1975Gr38 suggest that observed peak may include 5/2+,3/2[402]. 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
J Calculated configuration (1974Ny01) is 91% {I3}/2[521]. Originally assigned as 3/2,3/2[532] (1970Gr46), but in 1974Ny01 this assignment is made to the 350 level. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J Calculated mixing (1974Ny01) for 3/2[532] and 5/2[523] is 60% and 30%, respectively. Also, 1975Gr38 suggest that observed peak may include 7/2+,3/2[402]. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J Calculated configuration (1975Gr38) is 80% {I3}/2[402]. 
J No assignment is given in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J Calculated mixing (1974Ny01) for 1/2[521] and 1/2[530] is 50% and 48%, respectively, for this portion of doublet. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
E In 1975Gr37 the energy of the 9/2- level is given as 538. 
J Calculated mixing (1974Ny01) for 5/2[523] and 3/2[532] is 45% and 41%, respectively, for this portion of doublet. 


level_energy_unit: KEV
level_comment:
J Original assignment (1970Gr46) 7/2-,3/2[532], which is now assigned to 554 level. Also, 1975Gr38 suggest that observed peak may include a 9/2+ contribution with mixture for 5/2[642], 1/2[660], and 7/2[633] of 50%, 29%, and 10%, respectively. 
J Assignment in Adopted Levels is 5/2-,7/2-. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J Calculated mixing (1974Ny01) for 3/2[532] and 5/2[523] is 57% and 38%, respectively. Original assignment was doublet of 5/2-,1/2[521] and 3/2-,1/2[530] (1970Gr46). 


level_energy_unit: KEV
level_comment:
J 1975Gr38 suggest that observed peak may include 13/2+ contribution with mixture for 5/2[642], 1/2[660], and 7/2[633] of 50%, 29%, and 17%, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_comment:
T From {+157}Dy IT decay and based on values of 19.2 ms {I5} (1973Kl03), 24 ms {I1} (1971KiZQ), and 21 ms {I3} (1970Bo02). 


level_energy_unit: KEV
level_spin_parity: 37/2+
level_comment:
E,J$From {+157}Dy Adopted Levels in the ENSDF database - listed by compiler for 676.4|g placement from 3521.2 keV level. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated RMS charge radius: <r{+2}>{+1/2}=5.1815~fm~{I3023} (2013An02) |d<r{+2}>(156-158)=0.215 fm{+2} {I12} and |d<r{+2}>(158-160)=0.150 fm{+2} {I12} (1982Cl04); others: 1970Va21 and 1978Ho09. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J From E2 |g to 0+ level. 
T$Weighted average of 1.63 ns {I8} (1970Mo39) from {+158}Ho |e decay; 1.76 ns {I10} (1968Sc04) and 1.64 ns {I8} (1966Fu03) from {+158}Tb |b- decay; and 1.66 ns {I4} calculated from B(E2)|^=4.67 {I4} (1977Ro27). Other: 1.7 ns {I1} (1966Ab02) from {+158}Ho |e decay. 
MOMM1$Measured by Integral Perturbed Angular Correlation (1993Al09, and adopted by 2014StZZ compilation) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J From E2 |g to 2+ level and expected band structure. 
T Weighted average of 75 ps {I8} microwave (1968Be29) and 71 ps {I5} recoil-distance (1981Em01). 
MOMM1$From g-factor=+0.340 {I20} measured by Perturbed Angular Correlation (1993Al09); others (also quoted in 2014StZZ compilation): +1.33 {I10} (from g-factor +0.333 {I25} (1997Al04 by same authors as 1993Al09); +1.4 {I2} (from g-factors +0.35 {I6} (1983Se09) and +0.36 {I6} (1973Ka25)) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J From E2 |g to 4+ level and expected band structure. 
MOMM1$From g-factor=+0.236 {I22} measured by Perturbed Angular Correlation (1997Al04); others: +1.2 {I2} (from g-factor +0.21 {I4} (1993Al09 by same authors as 1997Al04)) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
MOMM1$Measured by Perturbed Angular Correlation (1997Al04); g-factors: +0.31 {I9} (1997Al04), +0.21 {I11} (1993Al09 by same authors as 1997Al04), +0.41 {I13} (1983Se09), 0.36 {I6} (1973Ka25) 
J From E2 |g to 6+ level and expected band structure. 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J From |g's to 6+ and 8+ levels and expected band structure. Assigned to both the K|p=0+ |b-vibrational band and K|p=2+ |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J$Based on DCO ratios of in-band 334|g and inter-band 1053|g in ({+12}C,4n|g) (2003Ha45; values not given) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J From M1 |g's to 2+ and 4+ levels and |g|g(|q). 
J Assigned on the basis of |g|g(|q) as 4+ by 1993Al09 with configuration ((|n,5/2[523])+(|n,3/2[521])) and ((|n,11/2[505])-(|n,3/2[521])). 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J$Based on DCO ratios of inter-band 469|g and 1188|g in ({+12}C,4n|g) (2003Ha45; values not given); band |p=(-) given at 2476 band level 


level_energy_unit: KEV
level_spin_parity: (10-)
level_comment:
J$Based on band assignment and DCO ratio measurements in ({+12}C,4n|g) (2003Ha45; values not given) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
J From |g's to 8+ and 10+ levels, J is 8, 9, or 10. From model calculations of decay |g's, 1997Ka49 assign this level as the 8+ level of the K|p = 4+ band. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$There is a serious intensity imbalance at this level with a feeding of |> 55 and depopulation of 31 to 37. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$In {+158}Dy Adopted Levels, J|p=(6+) based on the 2920 |g to the 4+ level at 317 keV, but this is inconsistent with |e feeding from 9+ parent. So, there is a problem with this scheme or the Adopted J|p. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(|mb/sr)=13 {ILE} 
J In Adopted Levels, 2096 level has no J|p assignment and 2107 level has 4+ assignment. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(|mb/sr)=13 
J In Adopted Levels 2096 level has no J|p assignment and 2107 level is assigned 4+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$From 1977Ro27, 1982Ro07; other: 4.7 {I4} (1963Bj04). 1977Ro27 list in Table II the following values (not retrieved by evaluator): 4.67~{I40} (1968Se02), 4.73~{I23} (1974Sh12), 4.41~{I25} (1966Ab01), 4.76~{I24} (1968Sc04), 4.56~{I27} (F.K. McGowan, and P.H. Stelson, Nuclear Spectroscopy and Reactions, edited by J. Cerny (Academic, New York, 1974), Part C, p. 3). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: D
level_comment:
J$J, from atomic-beam magnetic resonance (1965Al16). |p=-, from M1 |g from 5/2- level at 309~keV. |m value also supports |p and the Nilsson-orbital assignment (1989Be04). 
T$From 1959Ke28. Others: 134~d (1951Bu24), 139~d {I10} (1960Gr15), 130~d {I20} (1961Bj02), 151~d {I2} (1963Ho15), 138 d {I5} (1963Ra15), and 138~d {I7} (1964Ma10). The uncertainty of 0.2~d (1959Ke28) may not include all contributions. If one increases this uncertainty to 2~d, the weighted average of the six values with uncertainties is 146~d {I2}. 
MOMM1$From the 1989Ra17 evaluation and the compilation by 2005St24. 
MOME2$From the 1989Ra17 evaluation and the compilation by 2005St24. 
$From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.18~fm {I27}. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$From M1 |g to 3/2- g.s. and expected band structure. 
T$From 1978AlZC and 1975VaYX from {+159}Ho |e decay; other: 0.2~ns (1975Gr44). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
J$From E1 |g's to 3/2- and 7/2- levels. 
T$Weighted average of 9.0~ns {I5} (1974An11), from (|a,2n|g), 10.4~ns {I10} (1975VaYX), from {+159}Ho |e decay. Other: 9~ns (1975Gr44). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J$From E1 |g's to 5/2- and 7/2- levels and expected band structure. 
T$From {+159}Ho |e decay (1987AlZC). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$From M1 |g's to 3/2- and 7/2- levels and log {Ift}=4.8, from {+159}Ho decay. This {Iau} transition establishes the confs for both this level and the {+159}Ho g.s., as well as the |p of the {+159}Dy g.s. 
T$From 1978AlZC, {+159}Ho |e decay; others: 1.3~ns {I2} (1975VaYX, by same authors) and 3~ns (1975Gr44). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$From E1 |g to 9/2+ level, expected isomer based on the |n11/2[505] Nilsson state. 
T$From isomeric decay (1967Co26); other: 115 |ms {I10} (1965Bo22). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
J$From identification of (d,p) and (d,t) cross-section ratio as the |n3/2[402] Nilsson state, with an admixture of |n3/2[651]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_comment:
J$From the (d,p) cross-section data, assigned as the bandhead of the band built on the |n1/2[521] Nilsson orbital. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_uncertain: ?
level_comment:
J$From (d,t) cross-section data, identified as the bandhead of the |n3/2[651] Nilsson orbital, with an admixture of |n3/2[402]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
J$From (d,p) cross-section data, assigned as a member of the band built on the |n1/2[521] Nilsson orbital. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
J$From (d,t) cross-section data, assigned as the head of the band built on the |n3/2[532] Nilsson orbital. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
J$From (d,t) cross-section data, assigned as a member of the band built on the |n3/2[532] Nilsson orbital. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J$From (d,p) cross-section data, assigned as the 7/2- member of the |n1/2[521] band, but the peak is part of a doublet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
J$From (d,t) cross-section data, assigned as the 3/2- member of the |n1/2[530] band, but the peak is part of a doublet. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J$From M1 |g's to 3/2- and 7/2- levels; also E0 component in |g to 5/2- level. Since this E0 transition is between levels with K differing by 1, some K mixing in one, or both, levels is implied. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$From E1 |g's to 5/2+ and 9/2+ levels and M1 |g's to 5/2- and 9/2-. E0 component in |g to 7/2- level. Since this E0 transition is between levels with K differing by 1, some K mixing in one,or both, levels is implied. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2-)
level_comment:
J$From (d,p) cross-section data, assigned as the 9/2- member of the |n5/2[512] band. Note that this 9/2,5/2[512] state is assigned to the 1213 level by 1974Ny01. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$From 1967Co20; others: 115 |ms {I10} (1965Bo22) and 121 |ms (1968Io01) all from |g(t) following p or |a beam pulse. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$other: 10.4~ns {I10} (1975VaYX by same authors as 1978AlZC). 1972Ki21 report a half-life of 9~ns for a level at or above 177~keV and below 309~keV. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$1975VaYX report 1.3~ns {I2} for level at 309~keV. Since the same authors report this value for the 209-keV level in 1978AlZC, either the level energy is a typographical error or there was an error in the earlier measurement. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
E$Lowest energy peak reported in ({+3}He,|a) and assigned energy of 137~keV. 
S$d|s/d|W=45 |mb/sr at |q=40|' in ({+3}He,|a). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
E$Peak reported in ({+3}He,|a) at 242, could include both 239 levels. 
S$d|s/d|W=26 |mb/sr at |q=40|' in ({+3}He,|a) for the composite peak. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
E$Peak reported in ({+3}He,|a) at 359, could include 352 and two 365 levels. 
S$d|s/d|W=241 |mb/sr at |q=40|' in ({+3}He,|a) for the 359 peak. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S$No value listed at |q=90|' by 1970Gr46. Values of 5 |mb/sr and 13 |mb/sr at |q=60|' and 125|', respectively, are listed by these authors. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
E$Peak reported in ({+3}He,|a) at 515, could include 534 level. 
S$d|s/d|W=14 |mb/sr at |q=40|' in ({+3}He,|a). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$Peak reported in ({+3}He,|a) at 799, could include 774 and 828 levels. 
J$Assigned as 9/2,1/2[521] by 1974Ny01. 
S$d|s/d|W=43 |mb/sr at |q=40|' in ({+3}He,|a). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$From ({+3}He,|a). May correspond to a peak reported at 983 in (d,p). This peak is not reported in (d,t). 
S$d|s/d|W=47 |mb/sr at |q=40|' in ({+3}He,|a). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$From ({+3}He,|a). May correspond to a peak reported at 1891 in (d,p). 
S$d|s/d|W=43 |mb/sr at |q=40|' in ({+3}He,|a). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Possible |a decay: T{-1/2}|>8.5|*10{+15} y (2011Be18) 
From optical isotope-shift measurements, 1990Wa25 report the values (in fm{+2}) for the nuclear parameter, |l(|?|D<r{+2}>): |l({+160}Dy-{+158}Dy)=0.127 {I7}; |l({+162}Dy-{+160}Dy)=0.129 {I8}; and |l({+161}Dy-{+160}Dy)=0.0345 {I21}. In a recent compilation of such data, 1987Au06 give the following values, respectively, for these quantities: 0.132 {I12}; 0.134 {I12}; and 0.036 {I4}. From combined x-ray and optical-shift information, 1974Bo60 give (in fm{+2}) |l({+160}Dy-{+158}Dy)=0.126 {I11} and |l({+162}Dy-{+160}Dy)=0.134 {I11}. In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.20 fm {I31}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
MOMM1$weighted average of the values +0.74 {I2} (1973Ka25) and +0.70 {I3} (1984Si07) from 2014StZZ compilation (both measured by time-dependent perturbed angular correlation (TDPAC)) 
MOME2$from 2016St14 compilation (TDPAC) 
J E2 transition to g.s. 
T from {+160}Tb |b{+-} decay. This is essentially the same as that given by 2001Ra27. Other: 2.26 ns {I16}, from B(E2) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1 Computed by the evaluator from g=+0.353 {I19}, a weighted average of: g=+0.350 {I20}, from 1996Al02, as discussed in the {+160}Tb |b{+-} Decay data set; and +0.359 {I30}, from 1997Al04 (|a,2n|g) (both references by integral perturbed angular correlation (IPAC)). 2014StZZ list |m=+1.40 {I8} (1996Al02) and +1.60 {I12} (1997Al04) 
J E2 transition to 2+ state. Member of g.s. rotational band. 
T weighted average of: 103 ps {I5}, from {+160}Tb |b{+-} decay; and 110 ps {I11}, from B(E2)(2+|)4+), in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J E2 transition to 4+ level. Member of g.s. rotational band. 
MOMM1 Computed from g=+0.352 {I17}, 1999Br43 (Coul. ex., TF). Other: +1.13 {I12}, from g=+0.188 {I20} (1997Al04, IPAC in (|a,2n|g)) (after correction of their reported value, +0.242 {I20}, for the different T{-1/2} value used here). 2014StZZ list |m=+2.11 {I10} (1999Br43) and +1.45 {I12} (1997Al04, without correction) 
T from B(E2)(4+|)6+) in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
E$ level reported in 2009Ad04 (|e decay) from the observation of a K-shell electron line corresponding to transition energy of 681.3 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
E$from 2010BoZZ (|e decay) based on their observance of 703.0 transition, presumably E0; by their assignment of 1594.5 transition (previously unplaced) at existing 2297.5, 2+ level; and by postulating 616.2 transition from this level to the 86.8, 2+ level (with existing 616.18 |g from 2701.0, 1- level, this would be a doublet with) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 transition to g.s. 
MOMM1 From g=0.401 {I27} from 1999Br43 (Coul. ex., TF). |m=+0.65 {I5}, from g=+0.324 {I25}, computed by the evaluator from g=+0.317 {I13} as reported by 1995Al22 (IPAC, after correction for the different T{-1/2} value adopted here). See "{+160}Dy Levels from {+160}Tb |b{+-} Decay" for a discussion. 2014StZZ also report +0.80 {I5} (1999Br43), together with +0.63 {I2} (1995Al22) and +0.34 {I9} (1969Si01, 1975Kh03) for |m. 
T from B(E2) and adopted branching. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J E2 transition to 6+ level. Coulomb-excited; member of g.s. band. 
MOMM1 From g=+0.310 {I22}, 1999Br43, (Coul. ex., TF), computed by the evaluator from their reported value, g=0.343 {I22}, after correction for the different T{-1/2} value used here. Other |m values (also listed by 2014StZZ): 2.4 {I8}, from g=+0.301 {I95} (1997Al04, IPAC from (|a,2n|g)); +2.7 {I2} (1999Br43) 
T from Doppler-broadened line shape and B(E2)(6+|)8+), both in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J E2 and E2+M1 transitions to the 2+ and 4+ members, respectively, of the g.s. band. Energy considerations suggest this is a member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
J E1 transitions to 2+ and 3+ levels, but not to 4+. |g|g(|q) results consistent with J=2. 
T from 1972Ab09, |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J E1 transitions to 2+ and 4+ levels 
T from Doppler-broadened line shape in Coul. ex. (1981Mc06) 
BE3 from Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J E2 transitions to the 4+ and 6+ members of the g.s. band and the 3+ member of the |g-vibrational band. Energy considerations and this decay pattern suggest this is the 5+ member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J E1 |g to 2+ and 3+ levels indicate J|p=2-,3-. E1 |g from 1+ rules out 3-. 
T from |b{+-} decay (1972Ab09). Note that the B(E1)(W.u.) values from this T{-1/2} value are considerably smaller than one might expect from the decay of a state with this proposed J|p and configuration assignment. 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J E1 components in transitions to 3+ and 4+ levels. Energy agrees well with expected position of 4- member of K|p=2- octupole band. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J decays only via E2 to 8+ member of the g.s. band. Coulomb excited. Member of g.s. band. 
T Doppler-broadened line shape in Coulomb excitation (1977Ke06). Other: 1.20 ps {I12}, from B(E2). 
MOMM1 From g=+0.306 {I31}, 1999Br43 (Coul. ex., by TF); same |m value is also listed by 2014StZZ compilation 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J E2 |g's to 4+ members of the g.s. and |g-vibrational bands and an E2+M1 |g to the 6+ member of the g.s. band. Energy consistent with expected position of the 6+ member of the |g-vibrational band. Population in Coul. ex. indicates collective character. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J transitions to g.s. and first 2+ level require J=1 or J|p=2+. log| {Ift}=11.66 from 3- rules out 1-. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J E2 |g to 4+, |g's to 2+ and 5+ members of the |g band. Value based on comparison of shape of the angular distribution in ({+3}He,|a) with that of transitions to known levels. Band assignment is that proposed in ({+3}He,|a) and {+160}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
J E1 transition to the 6+ member of the g.s. band. Energy consistent with the expected 7- member of the K|p=2- band. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J Coulomb excited via an E3 transition (1981Mc06). Possibly the 3- member of a K|p=0- (octupole) band. 
BE3 from Coul ex. 


level_energy_unit: KEV
level_spin_parity: 4+,5,6+
level_comment:
J |g's to 4+ and 6+ levels. Possible excitation in (d,d') may indicate natural parity. 1981Ji01 assign this level as the J|p=5- member of the K|p=1- octupole band, while 1987Gr37 assign this state as the bandhead of a K|p=5- band with configuration=(|n 5/2[642] + |n 5/2[523]). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J E2 transitions to 2+ and 5+ levels establish |p=+ and J=3 or 4. The allowed-unhindered (au) |e transition (log| {Ift}=4.69, see 1996Re22) from the {+160}Ho g.s. (J|p=5+) uniquely establishes the assigned two-quasineutron configuration (and, hence, J|p=4+) for this state. 
T from {+160}Ho |e decay 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J L=6 in ({+3}He,|a). The strength of this peak, together with the relative cross sections to other {+160}Dy levels, suggests that this is the 6+ member of the S band. 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J E1 to 4+ level indicates |p=-. (d,t) population pattern for the proposed band members is consistent with the indicated K|p=4- configuration. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
E this level was proposed to deexcite via 252.2 and 498.6 |g's by 1987Ri08, (|a,2n|g). No 192.6 and 233 |g's were reported by 1987Ri08. |g data are from {+160}Ho |e decay. 
J E1 transition from 5+ level indicates |p=-. E2 |g to 4- and expected band structure. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J E2 transitions to the 6+ members of the g.s. and |g-vibrational bands and E2(+M1) transition to the 8+ member of the g.s. band. Level energy is that expected for the 8+ member of the |g band. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J M1 component in transitions to 4+ and from 6+ levels requires J|p=5+. Level energy suggests that it is the 5+ member of the K|p=4+ band. 


level_energy_unit: KEV
level_spin_parity: 9-
level_comment:
J (E1) transition to 8+ member of the g.s. band. Level energy consistent with that expected for the 9- member of the K|p=2- band. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J E2 transition to 4+ state indicates |p=+. Level-energy considerations, together with the occurrence of transitions to the 4+ and 5+ members of the 4+ band at 1694, indicate that this is the 6+ member of this band. 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J decays only via an E2 transition to the 10+ member of the g.s. band. Coulomb excited. Member of the g.s. band. 
T from Doppler-broadened line shape in Coulomb excitation (1977Ke06). Other: 0.54 ps {I24}, from B(E2). 
MOMM1 From g=+0.302 {I60}, 1999Br43 (Coul. ex., by TF); same value is also listed by 2014StZZ complilation 


level_energy_unit: KEV
level_spin_parity: (6)-
level_comment:
J |p=-, from L=5 in ({+3}He,|a). Transition to the 5+ member of the |g band. From considerations of rotational-band structure, this level is assigned as the 6- member of the indicated K|p=4- band. 


level_energy_unit: KEV
level_spin_parity: (8)+
level_comment:
J E2 transition to 6+ member of g.s. band indicates |p=+. The strength of this L=6 transition and the relative cross sections of the ({+3}He,|a) transitions to other {+160}Dy levels suggest that this is the 8+ member of the S band. 


level_energy_unit: KEV
level_spin_parity: 9+
level_comment:
J E2 transitions to 7+ member of the |g band and 8+ member of the g.s. band. These decay modes and the level energy are consistent with the assignment of this level as the 9+ member of the |g band. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7-)
level_uncertain: ?
level_comment:
J$from (|a,2n|g), (1987Ri08) based on the interpretation of an otherwise unplaced |g as a crossover transition to the 5- member of this band. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J |g's to 5+ and 8- levels and expected band structure. 1981Ji01, in ({+3}He,|a), report L=5 transfer to this level and interpret it as the bandhead of a K|p=3- band. 


level_energy_unit: KEV
level_spin_parity: (3)
level_comment:
J |g's to 2+ and 4+ levels. Level fed by |g's from 2- and 5- levels. Mult(1091.1|g)=(E1) and mult(1856.38|g)=(E2,M1), proposed by 2002Ad34 in |e decay give opposite parities for this state. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J |g to 2+ is sole mode of decay. Level is fed via an E1 from a positive-parity state, indicating |p=-. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J |g to 8+ and possible |g to 10+ members, respectively, of the g.s. band. Together with rotational-band considerations, this suggests that this level is the 10+ member of the indicated band. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J E1 transitions to 2+ levels indicate J|p=1-,2-,3-. Absence of transitions to 3+ and 1+ suggests J|p is probably not 1- or 3-. 


level_energy_unit: KEV
level_spin_parity: 8-
level_comment:
J E1 transition to 7+ and |g's to 8+ levels indicate |p=- and J=7 or 8. Strong L=5 transition in ({+3}He,|a) consistent with assigned configuration, indicating J=8. 


level_energy_unit: KEV
level_spin_parity: 11+
level_comment:
J E2 transition to 9+ member of the |g band and E2+M1 to 10+ member of the g.s. band. Together with rotational-band spacings, these support the assignment of this level as the 11+ member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
J E2 transition to 12+ member of the g.s. band. Population in Coulomb excitation indicates that this is the 14+ member of the g.s. band. 
T from Doppler-broadened line shape following Coulomb excitation (1977Ke06). 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
The large (d,t) strength to the 2524 level indicates the presence of the |n 1/2+[400] Nilsson orbital. Hence this level contains a significant component of the two-quasineutron state having configuration=(|n 5/2+[642] + |n 1/2+[400]). 
J gammas to the 2+ and 4+ members of the g.s. band. The indicated configuration has K|p=3+. Hence this level should have J|p=3+. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J E1 to 2- indicates |p=+. Excitation in (|g,|g') then indicates J|p=1+ as does mult=(M1) for the 3061 |g. 1775 |g to 3- may disfavor 1+. 2002Ad34, |e decay, suggest J|p=(1,2+). 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J E2 |g's to 7+, 8+ levels require |p=+. |g's to 4+ and 8+ levels indicate J=6. In their table 1, 2002Ad34 show J|p=7- for this level, but elsewhere J|p=6+ is shown. 7- is probably a misprint. 


level_energy_unit: KEV
level_comment:
E from energy sum based on placement of 596.5 |g. 1987Ri08 give E(level)=3113 and do not show it in their level scheme. 


level_energy_unit: KEV
level_spin_parity: 18+
level_comment:
J E2 transition to 16+ member of the g.s. band. This, and energy-spacing considerations, indicates that this is the 18+ member of the g.s. band. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T weighted average of: 2.03 ns {I2} (1972Lo01) |g|g(t); 1.97 ns {I4} (1971Ab05) |b|g(t), (ce)(ce)(t), |gce(t); 2.02 ns {I10} (1969Fo08) |g|g(t); 2.01 ns {I5} (1968Ku03) |gce(t); 2.02 ns {I9} (1966Fu03) |gce(t); 2.00 ns {I4} (the mean of three values reported by 1965Me08) |b|g(t),|gce(t); 1.99 ns {I4} (1965Gu02) |g|g(t); 1.99 ns {I5} (1963Li04) |bce(t); 1.92 ns {I5} (1963Fo02) |bce(t); 2.059 ns {I16} (1963De21) |gce(t). Other: 1981Is14, 1970Mo39, 1964Do06, 1962Ri07, 1960El07, 1952Mc03 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
G From 1996Al02, IPAC. This value is based on T{-1/2}=104.8 ps {I25}, used by these authors in their analysis. This value is quite close to that (104 ps {I4}) adopted in this evaluation. 
T weighted average of 101 ps {I9} (1971Ab05 |gce(t), |bce(t), (ce)(ce)(t)), 95 ps {I10} (1970Mo39 |g|g(t)), 112 ps {I11} (1966Ay01 |g|g(t)), 107 ps {I15} (1963Li04 |gce(t), |bce(t)). Other: 1961Bu15 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
G from 1995Al22, IPAC. The value, g=+0.317 {I12}, reported by these authors has been adjusted by the evaluator to be consistent with the somewhat different T{-1/2} value adopted here, namely T{-1/2}=1.31 ps {I9}. (in their work, 1995Al22 use T{-1/2}=1.340 ps {I25}.) Others: 0.28 {I4} (1969Si01, IPAC) and 0.27 {I10} (1975Kh03, IPAC). In these latter two studies, the g factors were reported to be 0.18 {I6} and 0.16 {I7}, respectively, based on the value T{-1/2}=2.1 ps {I6} for this level. The listed values were computed by the evaluator using the adopted T{-1/2} value. 
T in their studies, 1975Kh03 and 1969Si01 use T{-1/2}=2.1 ps {I6}, taken from B(E2)=0.069 {I20}, reported by 1965Yo04 in Coul. ex. This is quite different from the value adopted in the present evaluation (see {+160}Dy Adopted Levels). 1972Ab09 report T{-1/2}|<14 ps. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
E$ level reported in 2009Ad04 from the observation of a K-shell electron line corresponding to transition energy of 681.3 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
$from 2010BoZZ based on their observance of 703.0 transition, presumably E0; by their assignment of 1594.5 transition (previously unplaced) at existing 2297.5, 2+ level; and by postulating 616.2 transition from this level to the 86.8, 2+ level (with existing 616.18 |g from 2701.0, 1- level, this would be a doublet with) 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J possible member of the |g-vibrational band. The level energy agrees with, but the |g decay pattern differs from, that reported by 2002Ju08. The evaluator has adopted the latter values. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J E1 |g to 2- indicates |p=+. Excitation in (|g,|g') indicates J|p=1+, as does (M1) for the 3061 |g. However, 1775 |g to 3- may disfavor 1+. 2002Ad34 report J|p=(1,2+). 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
$According to 2009KaZY there is no coin in between 1036.2|g and 404.7|g, and 1036.2|g and 1481.9|g, by which they question the existence of 3099 level, decayed by 1481.9|g. While 1481.9|g is the most intense one decaying the level no comments are done about the other six transitions that are decaying the level 
J in their table 1, 2002Ad34 show J|p=7- for this level, but elsewhere J|p=6+ is shown. 7- is probably a misprint. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
g-factor as reported by 1997Al04 is +0.359 {I30}, computed assuming T{-1/2}=105 ps {I5} for the 4+ level. This value is sufficiently close to that used in this evaluation (104 ps {I4}) that no correction of the authors' value was made. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
g-factor as reported by 1997Al04 is +0.242 {I20}, computed assuming T{-1/2}=14.4 ps {I4} for the 6+ level. The listed value has been corrected to take into account the different T{-1/2} value (18.6 ps {I10}) used in this evaluation. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
g-factor reported by 1997Al04 is +0.301 {I95}, calculated assuming T{-1/2}=3.86 ps {I11} for the 8+ level. Since this is essentially the same as that used in this evaluation (3.8 ps {I3}), no correction was applied to the authors' value. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7+)
level_comment:
J from 1987Ri08, who assign this level as the 7+ member of the K|p=4+ band whose bandhead is at 1694. However, 1981Ji01 report that this level is populated by L=5 transfer in ({+3}He,|a), indicating that |p=-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (12+)
level_comment:
$NOTE:** 1987Ri08 IN TABLE 1 SAY THE 432.8 G COMES FROM A 2698.3 LEVEL AND THAT THE 469 AND 746.6 G'S COME FROM THE 12+ MEMBER OF THE GAMMA BAND (WHICH THEY PLACE AT 2698.3!?). I ASSUME THESE ARE THE SAME LEVEL. 
J 2002Ju08, from ({+7}Li,p4n|g), place the 12+ member of the |g-vibrational band at 2707 and assign J|p=13- to a level at 2696.7. 


level_energy_unit: KEV
level_spin_parity: 4-
level_uncertain: ?
level_comment:
E 1987Ri08, (|a,2n|g), place this 4- band member at 1536. From {+160}Ho |e decay, 2002Ad34 place the 4- member of this band at 1535 and do not report a level at this energy. Since this 1554 level is supported by only one feeding |g, about which there is some question, the evaluator has shown it as uncertain. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
E this level was proposed to deexcite via 252.2 and 498.6 |g's by 1987Ri08, (|a,2n|g). No 192.6 and 233 |g's were reported by 1987Ri08. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
$d|s/d|W(|mb/sr)=21 
when corrected for the Q value dependence of the (t,p) cross section, this value is reduced from 21 to 19 |mb/sr (1988Bu08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G{+2}\{-|g0}/|G (meV)=9.4 {I15} 
T calculated by the evaluator from the |G{-|g0} value for this level and the listed |g branching. 
S computed by the evaluator from the |G{-|g0} value of 1991Zi01 and the listed relative I|g values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
$|G{+2}\{-|g0}/|G (meV)=59 {I7} 
The |e decay data of 2002Ad34 do not indicate any |g decay from this level to levels above the first excited state. 
T calculated by the evaluator from the |G{-|g0} value for this level and the listed |g branching. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$|G{+2}\{-|g0}/|G (meV)=61 {I7} 
The |e decay data of 2002Ad34 indicate that the intensities of the 2777 and 2864 |g's represent only about 17% of the decays of this level. Thus, the |G{-|g0} and BM1|^ values deduced for this level by 1988We10 are most likely incorrect. The evaluator has not deduced |t or B(M1)-related information for this level and its deexciting |g's. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
$|G{+2}\{-|g0}/|G (meV)=8.4 {I17} 
The |e decay data of 2002Ad34 indicate that the intensities of the 2790 and 2877 |g's represent only about 12% of the decays of this level. Thus, the |G{-|g0} and BE1|^ values deduced for this level by 1988We10 are most likely incorrect. The evaluator has not deduced |t or B(E1)-related information for this level and its deexciting |g's. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$|G{+2}\{-|g0}/|G (meV)=19 {I3} 
The |e decay data of 2002Ad34 indicate that the intensities of the 2974 and 3061 |g's represent only about 5% of the decays of this level. Further their decay data give a quite different ratio for the intensities of the two |g's to the g.s. band. Thus, the |G{-|g0} and BM1|^ values deduced for this level by 1988We10 are most likely incorrect. The evaluator has not attempted to deduce |t or B(M1)-related information for this level and its deexciting |g's. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$d|s/d|W(|mb/sr)=6120 
BE2 deduced by 1968Gr08 from the measured cross section assuming d|s/d|W(|q=90|')=1290|*B(E2). 
R=2.34 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$d|s/d|W(|mb/sr)=130 
BE2 deduced by 1968Gr08 from the measured cross section at 90|' assuming d|s/d|W=880|*B(E2). 
R=2.88 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$d|s/d|W(|mb/sr)=163 
BE3 deduced by 1968Gr08 from measured cross section at 90|' assuming d|s/d|W=1400|*B(E3). 
R=1.35 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_comment:
R<1. d|s/d|W(|q=125|')=13 |mb/sr, but level not observed in (d,d') spectrum at 90|'. 
J 1968Gr08 report J|p=(5-) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T from B(E2)(4{++}|)6{++}) and |a=0.0664 {I8} 
B(E2)(4{++}|)6{++})=1.78 {I9} (1974Sa03) 
G From 1999Br43. These authors do not list the '+' sign, but the lower-spin members of the g.s. band have positive g-factors. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 weighted average of 0.122 {I6} (1981Mc06) and 0.105 {I8} (1974Oe01). Other: 0.069 {I20} (1965Yo04). 
T from B(E2) and adopted branching. Other: 1.35 ps {I17} (Doppler-broadened line shape (1975In02)). 
G From 1999Br43, who report g=0.401 {I27}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T weighted average of: 3.43 ps {I25}, from 1977Ke06, Doppler-broadened line shape; and 4.11 ps {I26}, from 1974Sa03, B(E2)(6{++}|)8{++}). 
B(E2)(6{++}|)8{++})=2.05 {I13} (1974Sa03) 
G Computed by the evaluator from g=0.343 {I22}, as reported by 1999Br43, after correction for the different value of T{-1/2} (3.43 ps {I25}) used by them. The '+' sign is given, since the lower-spin members of the g.s. band have positive signs. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T from Doppler-broadened line shape (1981Mc06) 
reported B(E3) measurements include 0.119 (1974Oe01) and 0.171 {I10} (1981Mc06) 
J assignment by 1981Mc06 based upon |g(|q) measurement for transition to 2+ member of g.s. band. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J assignment based upon |g(|q) measurements for transitions to 0+ and 4+ members of g.s. band. Substantial E0 component in transition to 2+ member indicates K=0 assignment. 
T from B(E2) and adopted branching 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T from 1977Ke06. Listed B(E2) value implies T{-1/2}=1.20 ps {I12}. 
B(E2)(8{++}|)10{++})=2.73 {I27} (1974Sa03). g from 1999Br43, who report g=0.306 {I31}. These authors do not show the positive sign for g, but the lower-spin members of the g.s. band have positive g-factors. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T from 1977Ke06. Listed B(E2) value implies T{-1/2}=0.53 ps {I23}. 
B(E2)(10{++}|)12{++})=3.2 {I14} (1974Sa03) 
G From 1999Br43, who report g=0.302 {I60}. The positive sign is included, since the g-factors for the lower-spin members of the g.s. band are positive. 


level_energy_unit: KEV
level_comment:
J 1981Ji01 report J|p=(5-) and assign it as the 5- member of the K|p=1- octupole band. However, subsequent studies place this state lower in the level scheme, at 1586. Also, this peak may correspond to two {+160}Dy levels, having J|p=4-,5- and 4+,5,6+, respectively. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J tentatively assigned as the 7+ member of the K|p=4+ band at 1694 by 1987Ri08 in (|a,2n|g). However, population of this level via L=5 transfer here indicates |p=-. 1981Ji01 assign this level as the head of a K|p=3- band. Its |g deexcitation suggests J=7. 


level_energy_unit: KEV
level_comment:
J peak may correspond to two {+160}Dy levels, one of which has J|p=4+,5+,6+. 1981Ji01 report J|p=(5-). 


level_energy_unit: KEV
level_comment:
$d|s/d|W(mb/sr)=0.02 
from systematics of strongly populated excited 0+ states in other strongly deformed nuclides, this level is most likely the 2+ member of the 0+ band at 1275 keV 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J J from 1956Co21 and 1958Pa11 by paramagnetic resonance and 1962Sp03 by atomic-beam, magnetic resonance. From the agreement of the calculated |m (1989Be04) with that for 5/2[642] but not with that of other possible K=5/2 states, it is concluded that this is the correct Nilsson-orbital assignment. Hence, |p=+. 
From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.197 fm 6. 
MOMM1 from the evaluation by 1989Ra17. In the compilation by 2005St24, values of -0.480 {i3} and -0.481 {i5} are listed. 
MOME2 from the evaluation by 1989Ra17. In the compilation by 2005St24, values of +2.51 {i2} and +2.47 {3} are listed. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J J from Mossbauer studies summarized in 1976St23. |p from E1 |g to 5/2+ ground state. 
T weighted average of: 27.8 ns 15 (1969Ve05), 29.0 ns 14 (1975VaYX), and 28.6 ns 5 (1978AlZC), from {+161}Ho |e decay; and 27 ns 2 (1957Ve17,1960Ve03), 28 ns 2 (1958Ha13), 29 ns 3 (1959Fa06), 29.4 ns 10 (1965Me08), 28.4 ns 12 (1969Be54), and 30.0 ns 5 (1977Pe20), from {+161}Tb |b{+-} decay. The 0.2 ns uncertainty shown by 1978AlZC has been increased to reduce the normalized weight of this value in the average from 78% to 36%, so that this (unpublished) value will not dominate the average to this extent. 
MOMM1 from the evaluation by 1989Ra17. This value is also listed in the compilation by 2005St24. 
MOME2 from the evaluation by 1989Ra17. In the compilation by 2005St24, +2.51 {i2} (the same value as for the g.s.) is listed. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J M1 component in |g to 5/2+, Coulomb excited, and expected band structure. 
T weighted average of 0.78 ns 6 (1967As03), from Coul. ex., and 0.99 ns 13 (1975VaYX) and 1.0 ns 2 (1978AlZC), from {+161}Ho |e decay. From B(E2), one computes T{-1/2}=0.78 ns 7. It should be noted that the values of 1975VaYX and 1978AlZC might be related and that the value of 1967As03 contributes 77% of the normalized weight. Other: 0.76 ns (1981GrZV), from {+161}Ho |e decay. 
MOMM1 from the evaluation by 1989Ra17. The same value is listed in the compilation by 2005St24. 
MOME2 from the evaluation by 1989Ra17. The same value is listed in the compilation by 2005St24. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J resonance-averaged n capture gives J|p=1/2-,3/2-. E1 |g to 5/2+ rules out 1/2-. 
T weighted average of: 2.3 ns 7 (1957Ve17,1960Ve03), 3.0 ns 3 (1958Ha13), 3.1 ns 6 (1959Fa06), 2.95 ns 15 (1965Ay02), 3.36 ns 10 (1965Me08), 3.34 ns 18 (1969Be49), 3.08 ns 5 (1969Be54), and 3.16 ns 5 (1977Pe20), from {+161}Tb |b{+-} decay. (in the average, the 0.05 ns uncertainty of 1965Me08 was increased, because the value is inconsistent with several other values as well as the average.) 
MOMM1 from the evaluation by 1989Ra17. The same value is listed in the compilation by 2005St24. 
MOME2 from the evaluation by 1989Ra17. The compilation by 2005St24 lists this value, but with a positive sign. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J from (E2) |g to 5/2+, M1 |g to 7/2+, Coulomb excited, and expected band structure. 
T computed by the evaluator from B(E2)|^=0.79 {I4} (from Coul. ex.) and the adopted properties of the deexciting |g's. Other: 0.1 ns (1981GrZV), from {+161}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J E1 |g's to 5/2+ and 7/2+ levels and expected band structure. 
T weighted average of 0.55 ns 3 (1975VaYX) and 0.64 ns 3 (1978AlZC), from {+161}Ho |e decay. Other: 0.61 ns (1981GrZV) from {+161}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J (E1) |g to 7/2+ level and M1 |g to 3/2-. 
T from (1969Be49), {+161}Tb |b{+-} decay. Others: |<3 ns (1958Ha13), |<0.3 ns (1965Me08), |<0.3 ns (1989Be04) from {+161}Tb |b{+-} decay and 0.13 ns (1981GrZV), from {+161}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J E1 |g to 7/2+, (E1) |g to 9/2+, and expected band structure. 
T from 1981GrZV, {+161}Ho |e decay. Other: |<0.3 ns (1975VaYX,1978AlZC), {+161}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
J from expected band structure, |g's to 7/2- and 9/2- levels, and L=(5) in (d,t). 
T from 1981GrZV, {+161}Ho |e decay. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J from L=1 in (d,t) and resonance-averaged n capture, J|p=1/2-,3/2-. E2 |g to 5/2- and expected band structure makes 3/2- unlikely. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J from resonance-averaged n capture, J|p=1/2+,3/2+. M1 component in |g to 5/2+ eliminates 1/2+. 
T the B(E2) value is available from Coul. ex., but |d for the g.s. transition is not known, so the level half-life cannot be computed. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J L=0 in (d,t). Population in ({+3}He,{+3}He') indicates the presence of an admixture of the K-2 |g vibration built on the {+161}Dy g.s. (1987Ra16). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J resonance-averaged n capture indicates J|p=1/2+,3/2+. E1 |g to 5/2- eliminates 1/2+. Its strong population in ({+3}He,{+3}He'|g) indicates that this state has a component of the K-2 |g vibration built on the {+161}Dy g.s. 1987Ra16 assign this level as the J|p=1/2+ member of this vibrational band. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J M1,E2 |g to 7/2+ indicates |p=+. |g's to 3/2- and 7/2- require J=5/2. From its population in ({+3}He,{+3}He'), 1987Ra16 assign this as the 5/2+ member of the K-2 |g vibration built on the 5/2[642] g.s. This level probably contains admixtures of all the proposed configurations. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J from |g's to 5/2+,7/2+,and 5/2- levels, J|p=3/2+,5/2,7/2. From ({+3}He,{+3}He'|g), 1987Ra16 assign this as the 3/2+ member of the K-2 |g-vibrational band built on the 5/2[642] g.s. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J resonance-averaged n capture indicates J|p=1/2-,3/2-. M1 component in the |g to 5/2- eliminates 1/2-. 


level_energy_unit: KEV
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
J from (M1+E2) |g to 19/2+ and expected band structure (Coulomb excited). 
T from 1988Os01, Coul. ex. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J from E1 |g to 7/2- level, |g's to 5/2- and 5/2+, and interpretation of (d,p) and (d,t) reaction data. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J from E2 |g's to 7/2- and 9/2- levels, |g's to 3/2- and 5/2-, and interpretation of (d,p) reaction data. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J |g's to 5/2+ and 9/2+ indicate J|p=5/2+,7/2,9/2+. From its strong population in ({+3}He,{+3}He'), 1987Ra16 assign this as the K+2 |g vibration built on the 5/2[642] g.s. Hence, J|p=9/2+. 


level_energy_unit: KEV
level_spin_parity: 5/2,7/2-
level_comment:
J from |g's to 3/2-, 5/2-, 7/2+, and 7/2- levels. Probable feeding from n-capture state suggests J|p=5/2+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+,7/2+
level_comment:
J excitation in (|g,|g') via dipole transition from 5/2+ g.s. Gammas to 9/2+ and 3/2- eliminate J=3/2, 5/2- and 7/2. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T weighted average of: 27 ns 2 (1957Ve17); 28 ns 2 (1958Ha13); 29 ns 3 (1959Fa06); 29.4 ns 10 (1965Me08); 28.4 ns 12 (1969Be54); and 30.0 ns 5 (1977Pe20). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T weighted average of: 2.3 ns 7 (1957Ve17 or 1960Ve03); 3.0 ns 3 (1985Ha13); 3.1 ns 6 (1959Fa06); 2.95 ns 15 (1965Ay02); 3.36 ns 10 (from 1965Me08 but with uncertainty increased from 0.05 because value is inconsistent with other values); 3.34 ns 18 (1969Be49); 3.08 ns 5 (1969Be54), and 3.16 ns 5 (1977Pe20). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T weighted average of: 27.8 ns 15 (1969Ve05); 28.6 ns 5 (1978AlZC); and 29.0 ns 14 (1975VaYX). The 0.2 ns uncertainty from 1978AlZC was increased to 0.5 ns (see the comment on this point in the Adopted Levels data set). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=?
level_comment:
T from 1981GrZV 
If this level has no G feeding, the LOGFT to it is 9.1. This is much too small for a 2nd-forbidden transition. 


level_energy_unit: KEV
level_spin_parity: 5/2+,7/2,9/2+
level_comment:
There is also a level reported at 772.7 keV, with J|p=1/2+ (see the Adopted Levels). 
J possible bandhead of 7/2[633]. If this is correct, then J|p=7/2+. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: S
level_comment:
E S(n) value from 1986Sc16; neutron-capture "state". 
J from predominantly s-wave n-capture by a 0+ target. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$RELATIVE=195 {I12} 
E energy given as 550 {I13} in 1986Sc16, but evaluator assumes that this is a misprint and that the uncertainty should actually be 1.3 keV. 


level_energy_unit: KEV
level_comment:
$RELATIVE=44 {I6} 
J assigned as 5/2-,7/2+ by 1977Be03 from L=(1). L=2,3 from 1975Ho21, and L=4 from 1976Pe02 (d,t). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$RELATIVE=29 {I7} 
In 1977Be03, this level is assigned as 5/2-,3/2[532], and the 1/2+ state is placed at 777 keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2-)
level_comment:
E this level is assumed (1970Gr46) to constitute the main part of an unresolved peak at this energy. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$RELATIVE {+3}He' INTENSITIES=85 {IAP} 
Population of this level in ({+3}He,{+3}He') indicates the presence of an admixture of the K-2 |g vibration built on the {+161}Dy g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$RELATIVE {+3}He' INTENSITIES=110 {IAP} 
J 1987Ra16 assign this as J|p=1/2+ and consider it to be the bandhead of the K-2 |g vibration built on the {+161}Dy g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$RELATIVE {+3}He' INTENSITIES=170 {IAP} 
J because of its strong population in ({+3}He,{+3}He'), 1987Ra16 propose that it contains a significant component of the K-2 |g vibration built on the {+161}Dy g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$RELATIVE {+3}He' INTENSITIES=75 {IAP} 
J population in ({+3}He,{+3}He') indicates the presence of an admixture of the K-2 |g vibration built on the {+161}Dy g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$RELATIVE {+3}He' INTENSITIES=270 {IAP} 
J assigned by 1987Ra16 as the 3/2+ member of the K-2 |g vibration built on the {+161}Dy g.s. (5/2[642]). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
BE2 from 1978Br20. Other: 0.59 {I14} (1960Be16). 
T computed by the evaluator from the listed B(E2) and the properties of the deexciting |g's as taken from the Adopted Gammas. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_comment:
BE2 from 1965Er08. 
T half-life could be deduced from B(E2) value, but conflicting values have been given for |d of the 550 |g. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E this is presumably the same as the 772.1 level (J|p=7/2+), seen in the {+161}Ho |e decay. 
BE2 from 1965Er08. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$RELATIVE=1650 {I20} 
E energy given as 550 {I13} in 1986Sc16, but evaluator assumes that this is a misprint and that the uncertainty should actually be 1.3 keV. The value in 1970Gr46 is 551. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$RELATIVE=385 {I18} 
J others: Assigned (9/2+) by 1975Ho21 and (7/2-) by 1977Be03. 
L others: L=4 from 1975Ho21 and (4) from 1977Be03. 


level_energy_unit: KEV
level_comment:
$RELATIVE=120 {I7} 
J assignment of 1977Be03 is 3/2-,3/2[532], based on L=(1). 
L others: L=2,3 from 1975Ho21 and (1) from 1977Be03. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$RELATIVE=416 {I30} 
E doublet level (1986Sc16). 
J assigned as 5/2-,3/2[532] by 1975Ho21. 
L others: L=3 from 1975Ho21 and 1 from 1977Be03. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$RELATIVE=66 {I7} 
J assignment of 1977Be03 is 5/2-,5/2[512] and that of 1970Gr46 is 5/2-,1/2[530]. 
L from 1975Ho21. 


level_energy_unit: KEV
level_comment:
$RELATIVE=110 {I24} 
J assignment of 1977Be03 is 5/2-, 7/2- and of 1975Ho21 is 9/2-,3/2[532]. 
L other: L=3 from 1977Be03. 


level_energy_unit: KEV
level_comment:
$RELATIVE=71 {I5} 
J assignment of 1975Ho21 is 11/2-,3/2[532] and 11/2-,1/2[530]. 
L from 1975Ho21. 


level_energy_unit: KEV
level_comment:
$RELATIVE=33 {I5} 
J 1977Be03 assign this as 1/2-,1/2[510]. 
L other: L=(1), from 1977Be03, which would appear to agree with the J|p=1/2- assignment for the 1268.9 level. However, interpreted as the bandhead of 1/2[510], the 1268.9 level is not expected to be observed in this single-nucleon transfer reaction. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$RELATIVE=13.4 {I20} 
E assigned as the 3/2- member of the 1/2[510] band. The other band members are not observed in (d,t) because their smaller relative cross sections imply that they will not be appreciably populated in this reaction (1/2[510] is a high-lying particle state in {+161}Dy). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
T$also 29.04 ns {I4} measured by 2013Lo07 under other conditions. These values are consistent with 29.1 ns {I3} from Adopted Levels of {+161}Dy in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
T$this value differs significantly from 3.14 ns {I4} from Adopted Levels of {+161}Dy in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
|D<r{+2}> data are available: for {+160}Dy-{+162}Dy, |D<r{+2}>|?0.13 fm{+2} (1985Ne09, read from plot by evaluator) and |l=0.129 {I8} fm{+2} (1990Wa25) where |D<r{+2}>|?|l. For {+162}Dy-{+164}Dy, |D<r{+2}> |?0.12 fm{+2} (1985Ne09) and |l=0.119 fm{+2}. See also 1970Va21 and 1978Ho09. Other isotope shift data: 1968De36, 1973Le16, and 1982Cl04. 
In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.2074 fm {I172}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J from E2 |g to 0+ level. 
T weighted average of: 2.25 ns {I7} (1963Li04), from {+162}Ho |e decay (67 min); and 2.19 ns {I3} (1967Ku07) and 2.17 ns {I4}, both from Coul. ex. Others: 3.05 ns {I20} (1973Ch28) from {+162}Ho (67 min) decay and 2.22 ns (1959Bi10) and 2.0 ns {I2} (1967As03) both from Coul. ex. For comparison, the evaluation of 1987Ra01 gives 2.19 ns {I3}, which is based on the B(E2) as well as the direct half-life measurements. 
MOMM1 from the compilation of 2014StZZ and based on g=0.343 {I14} (1970Be36). Others: g=0.362 {I24} (1967Ku07) and 0.37 {I4} (1967He15). The compilation by 2005St24 lists |m=+0.69 {I3}. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
J from E2 |g to 2+ level and expected gs band structure. 
T weighted average of 0.132 ns {I8} (1963Li04) from {+162}Ho (67 min) decay and 0.132 ns {I6} (1978Hu03) from Coul. ex. 
T$from B(E2)(2{++}|)4{++})=2.68 {I13} (Coul. ex.), the computed half-life is 0.134 ns {I7}. 
MOMM1 computed by the evaluator from g=+0.285 {I31}, from IPAC in (|a,2n|g) (1997Al04). This value is also listed in the compilation by 2014StZZ. 
BE4 From Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J from E2 |g to 4+ level and expected gs band structure. 
T from Coul. ex. (1978Hu03). 
T$from B(E2)(4{++}|)6{++})=2.10 {I15} (Coul. ex.), the computed half-life is 19.9 ps {I15}. 
MOMM1 computed by the evaluator from g=+0.364 {I18} in Coul. ex. (1999Br43). Other: +1.68 {I18}, from g=+0.28 {I3}, from IPAC in (|a,2n|g) (1997Al04). The compilation by 2014StZZ lists |m=+2.18 {I11}, together with +1.8 {I2}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J from E2 |g to 0+ level. Excited in Coul. ex. 
T computed from B(E2)|^=0.122 {I5} (Coul. ex.) and the adopted |g branching. Other: 0.74 ps<T{-1/2}<3.24 ps (2017Ap01, (n,|g) E=th) 
MOMM1 computed by the evaluator from g=0.46 {I3}, from 1999Br43 (Coul. ex.). This value is also given in the compilation by 2014StZZ. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J from population in Coul. ex., |g to 6+ level, and expected gs band structure. 
T weighted average of 4.1 ps {I3} (1977Ke06), 4.6 ps {I3} (1978Hu03), and 4.1 ps {I2} (1979Gu15) all from Coul. ex. 
T from B(E2)(6+|)8+)=1.96 {I16} (Coul. ex.), the computed half-life is 5.1 ps {I4}. 
MOMM1 computed by the evaluator from g=+0.381 {I20} in Coul. ex. (1999Br43). Other: +3.4 {I10}, from g=+0.45 {I12}, from IPAC in (|a,2n|g) (1997Al04). The compilation by 2014StZZ lists |m=+3.05 {I16} as well as +3.4 {I10}. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J from |g to K|p=2+ bandhead, |g to 4+ level, and expected band structure. 
T$0.25 ps<T{-1/2}<2.83 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J from |g's to 2+ and 6+ levels, M1 component in the |g to 4+ level. 
T$0.491 ps<T{-1/2}<2.20 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J E1 |g's to 2+ and 3+ levels indicate 2- or 3-. log| {Ift}=4.95 from the 1- gs of {+162}Tb rules out 3-. This allowed-unhindered |b{+-} transition involves the (|n 5/2[523]) and (|p 7/2[523]) orbitals. It thus establishes the two-quasiparticle state with configuration=(|p 7/2[523])-(|p 3/2[411]) as at least a large part of the configuration of this 2- band. This supports the interpretation of this level as being the bandhead of a K|p=2- octupole vibration, since this two-quasiparticle state is expected to be the dominant component of the 2- octupole vibration in {+162}Dy (1996So19). 
T from {+162}Tb |b{+-} decay (1968Se02). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J from E1 |g's to 0+ and 2+ levels. 
T from (|g,|g'). See the comment there about the reliability of this value. Other: <0.15 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J from |g's to 4+ and 6+ levels, authors' interpretation of (d,d') angular distribution data, and expected band structure. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J from population in Coul. ex., |g to 8+ level, and expected gs band structure. 
T$from Coul. ex. (1977Ke06). Other: 1.5 ps {I1} (1979Gu15) from Coul. ex. 
T$from B(E2)(8{++}|)10{++})=2.65 {I21} (Coul. ex.), the computed half-life is 1.34 ps {I11}. 
MOMM1 From 1999Br43 (Coul. ex.). This value is also listed in the compilation by 2014StZZ. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J E1 |g's to 4+ and 6+ levels. log| {Ift}=4.77 from 6- in {+162}Ho (67.0 min) |e decay establishes configuration assignments for both states. 
T weighted average of 1.91 ns {I19} (1969Ho17) and 1.93 ns {I13} (1973Ch28), from {+162}Ho (67.0 min) |e decay. Other: <2.02 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J from M1 component in |g to 3+ level, |g's to 2+ and 6+ levels, and expected band structure. 
T$0.10 ps<T{-1/2}<3.6 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J from resonance-averaged n-capture and |g's to 2+ and 6+ levels. In (d,d'), level is assigned 3-. 
T$0.75 ps<T{-1/2}<2.1 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J log| {Ift}=5.82 from 6- in {+162}Ho (67.0 min) |e decay indicates |p=- and J=5, 6, 7. |g to 4- rules out J=7. Expected band structure. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J from resonance-averaged n-capture and |g to 1- level. Other: (d,d') data give J|p not 2+, so level might be a doublet. 
T$0.17 ps<T{-1/2}<0.7 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
Listed |g branching is from (n,n'|g), except where noted otherwise. 
J from |g's to 0+ and 4+ levels and expected band structure. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
Member of a possible doublet. 1995Be02 assign a number of |g's deexciting this level. 2006Ap01, however, state that this level is not populated in the (n,|g) reaction with thermal neutrons. The listed |g branching is from (n,n'|g). 
J from resonance-averaged n-capture. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
The listed |g branching is from 2002Go15, in (n,n'|g). For a discussion of the problems associated with this |g branching, see the comments on this level in the {+161}Dy(n,|g) E=th data set. 
J from resonance-averaged n-capture and E2 |g to 2+ level. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
|g-decay properties are from (|a,2n|g). 
J M1 component in |g to 6+, E2 |g to 5+, and expected band structure. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
Listed |g branching is from (n,n'|g). 
J from resonance-averaged n-capture and |g's to 1- and 4+ levels. 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
J from E2 |g to 10+ level and expected gs band structure. 
T weighted average of 0.93 ps {I6} (1977Ke06) and 0.76 ps {I4} (1979Gu15) from Coul. ex. 
T from B(E2)(10+|)12+)=2.1 {I3} (Coul. ex.), the computed half-life is 0.75 ps {I11}. 


level_energy_unit: KEV
level_comment:
Assigned as the 4+ member of the K|p=1+ band at 1745 keV by 1995Be02 from (n,|g). However, the fact that this level is populated differently in (d,p) and (d,t) from the lower-spin members of this band suggests that it is not a member. In a subsequent (n,|g) study, 2006Ap01 do not confirm the population in (n,|g) of a level at this energy. They propose that the J|p=4+ band member is at 1954 keV. 
E value from 1995Be02 ((d,p) and (d,t)). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J from E1 |g's to 2+ and 4+ levels and resonance-averaged n-capture. 
T$0.17 ps<T{-1/2}<0.21 ps (2017Ap01, (n,|g) E=th) 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
E 1995Be02 (in (n,|g)) report |g's depopulating this level to levels with J|p ranging from 0+ and 1- to 4+ and 6-, which suggests more than one level here. Resonance-averaged n capture also suggests the presence of a doublet of levels at this energy. The |g branching from the level listed here is that reported by 2006Ap01, which is adopted, differs from that given by 1995Be02. 
J E1 |g to 4- and M1 |g to 3+. Level assigned as the 4+ member of the K|p=1+ band by 2006Ap01. However, 1995Be02 place that 4+ state at 1904.13 keV, an assignment that is not adopted here. 


level_energy_unit: KEV
level_comment:
J assigned by 1995Be02, in (n,|g), as the 5+ member of the K|p=1+ band at 1745 keV. This seems to Be based, in part, on the identification by 1995Be02 of the 1904 level as the 4+ band member. However, this assignment is not adopted. |g to a 3- level suggests J|p=5+ is incorrect. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
|g-decay properties are from (|a,2n|g). 
J M1 component in |g to 7+, E2 |g to 8+, and expected band structure. 


level_energy_unit: KEV
level_spin_parity: (4)
level_comment:
J from 1995Be02, (n,|g). |g's to 2+ and 6+ levels imply J|p=4+. Note, however, that this level is not populated in resonance-averaged n capture, where all the J=4 levels should Be populated via primary |g transitions. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_comment:
T$ from |g|g(t) (2011Sw02) 
$Proposed configuration=|n11/2[505]~#|n5/2[523], K|p=8+, in 2011Sw02 ({+160}Gd({+9}Be,|a3n|g)) 
J$(7-,8+) from |g's to 6+ and 9- respectively; (8+) from proposed configuration 


level_energy_unit: KEV
level_spin_parity: 9+
level_comment:
|g branching and properties are from (|a,2n|g). 
J M1 components in |g's to 8+ and 9+ levels, E2 |g to 7+, and expected band structure. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E the evaluator has chosen not to identify this level with those listed at 2291.4 and/or 2292, since the other members of this proposed K|p=4+ band are not observed in either of the reactions in which these levels are reported. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$|g's to (8+) and (9+) and band assignment 
$ Magnitude of g{-K}-g{-R}=0.24 {I4} (2011Sw02, {+160}Gd({+9}Be,|a3n|g)) 


level_energy_unit: KEV
level_spin_parity: (11+)
level_comment:
J$|g's to (9+) and (10+) and band assignment 
$ Magnitude of g{-K}-g{-R}=0.27 {I+8-6} (2011Sw02, {+160}Gd({+9}Be,|a3n|g)) 


level_energy_unit: KEV
level_spin_parity: 1-,2,3
level_uncertain: ?
level_comment:
E$this level which is bound in 1977Ka08 (Q(|b{+-})=2530 {I80}) is getting unbound for the actual adopted value (Q(|b{+-})=2301.6 {I22} (2021Wa16)) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E Level is populated by |g from 1453 level, deexcitation |g's are not reported by 1975Ed02 or 1973Ba21, but are given in {+162}Dy Adopted |g radiations. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$adopted value. 2.25 ns {I7} from 1963Li04 from electron-|g coincidences with two plastic scintillators. Other: 3.05 ns {I20} (1973Ch28). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
T$adopted value. 0.132 ns {I8} from 1963Li04 from electron-|g coincidences with two plastic scintillators. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
T Weighted average of 1.91 ns {I19} (1969Ho17) and 1.93 ns {I13} (1973Ch28 from x-|g coincidences with plastic scintillators). 
T The value in 1969Ho17 is given as 1.91 NS 19 in the text and 1.94 NS 19 in the abstract. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
G$g factor as reported by 1997Al04 is +0.301 {I31}, computed assuming T{-1/2}=17.4 ps {I5} (quoted by 1997Al04). The listed value has been corrected to take into account the different T{-1/2} value (18.4 ps {I10}, from Adopted Levels, Gammas) used in this evaluation. Note, however, that this |m value has not been adopted. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
G$g factor as reported by 1997Al04 is +0.43 {I12}, computed assuming T{-1/2}=4.39 ps {I12} (quoted by 1997Al04). The listed value has been corrected to take into account the different T{-1/2} value (4.2 ps {I2}, from Adopted Levels, Gammas) used in this evaluation. Note, however, that this |m value has not been adopted. 


level_energy_unit: KEV
level_spin_parity: (9-)
level_comment:
E consistent with that proposed as the 9- member of a K|p=6- band. But the existence of this band at the previously proposed location has not been confirmed. The two decaying |g's are relocated by 2011Sw02 ({+160}Gd({+9}Be,|a3n|g)) at (9-), 2188 isomeric level 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
Band assignment is that of 2001Wu05 ({+162}Dy,{+162}Dy'|g) and 2002Ju08 ({+7}Li,p4n|g). 2006Ap01 assign it as a member of the |g-vibrational band. See, also, the comment on the 2623 level. 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
Band assignment is that of 2001Wu05 ({+162}Dy,{+162}Dy'|g) and 2002Ju08 ({+7}Li,p4n|g). 2006Ap01 assign it as a member of the S band. See, also, the comment on the 2535 level. 
J 2006Ap01 show this value in parentheses. 


level_energy_unit: KEV
level_spin_parity: 14+
level_comment:
J assignment is that of the evaluator and is based on data from ({+7}Li,p4n|g). 2006Ap01 assign this tentatively as the 13- member of the K|p=0- octupole band, but in ({+7}Li,p4n|g) this band member is placed at 2693.7 keV. 


level_energy_unit: KEV
level_spin_parity: 13-
level_comment:
J J|p and band assignment is that of the evaluator and is based on data from ({+7}Li,p4n|g). 2006Ap01 report this level but show its J|p value as questionable. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (20+)
level_uncertain: ?
level_comment:
2001Wu05 and 2002Ju08 report this level as being deexcited by a 746.4 |g and a 747 |g, respectively. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$Level observed via primary |g (1967Ba34) but with contradictory deexcitation pattern. 1995Be02 found secondary deexciting |g's, which were not confirmed by 2006Ap01. This level was also observed in (n,n'|g), however its |g branching is quite different from that reported by 1995Be02. The evaluator decided not to list deexciting |g's for this level. The adopted |g branching is from 2002Go15, in (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
From resonance-averaged n capture, there may be more than one level at this energy. 
J assigned as the 4+ member of the K|p=1+ band by 2006Ap01. However, 1995Be02 place that 4+ state at 1904.13 keV. This latter assignment is not adopted by the evaluator. Note that, with the 4+ level at 1951 keV, the implied band parameters seem unreasonable. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$2006Ap01 reported a 1999.085 level with J|p=(3+,4+) but with a somewhat different |g branching. These authors, however, show it with a question mark. The evaluator has adopted the data from 1995Be02 for this level. 


level_energy_unit: KEV
level_comment:
J assigned by 1995Be02 as the 5+ member of the K|p=1+ band at 1745 keV. However, this assignment is not adopted. See the comment in the Adopted Levels data set. 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_comment:
Thermal-neutron-capture state. 
E$S(n) as measured by 1967Ba34, which differs from S(n)=8196.99 {I6} given in the mass evaluation of 2021Wa16. This latter value, together with the primary |g energies of 1967Ba34, leads to final-state level energies that differ systematically (although within the quoted uncertainties) from those known from other studies, indicating possible energy calibration problems of 1967Ba34. This dataset needs a new measurement. 
J from s-wave n capture into the {+161}Dy g.s. (J|p=5/2+). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+,3+
level_comment:
E This level represented the 2-keV neutron capture state (1967Ba34); it is primarily populated by s-wave capture. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E This level represented the 24-keV neutron capture state (1967Ba34) and is populated by both s- and p-wave capture. 


level_energy_unit: KEV
level_comment:
Possible doublet, consisting of the 7- member of the 2- octupole band and the bandhead of the 1- octupole band. 


level_energy_unit: KEV
level_comment:
J assigned as the 4+ member of the K|p=1+ band at 1745 keV by 1995Be02. However, the lower-spin band members are not observably populated in (d,p), which casts doubt on such a band assignment. It is not adopted in this evaluation. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
The listed B(E1) value is from 1991Zi01. 
T computed by the evaluator from the B(E1) value and the relative intensities of the two deexciting |g's given by 1991Zi01. Note, however, that this |g branching differs markedly from the adopted |g branching, suggesting that the deduced T{-1/2} value may be in error. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T from |G{+2}{-|g0}/|G (meV)=18.7 {I21} and |G{-2}/|G{-0}=0.54 {I6} (1988We10), the evaluator computes T{-1/2}=10.3 fs {I13}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
T from |G{+2}{-|g0}/|G (meV)=14.2 {I17} and |G{-2}/|G{-0}=1.13 {I11} (1988We10), the evaluator computes T{-1/2}=7.1 fs {I10}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T from |G{+2}{-|g0}/|G (meV)=103 {I11} and |G{-2}/|G{-0}=0.47 {I3} (1988We10), the evaluator computes T{-1/2}=2.07 fs {I24}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T from |G{+2}{-|g0}/|G (meV)=67 {I8} and |G{-2}/|G{-0}=0.29 {I7} (1988We10), the evaluator computes T{-1/2}=4.1 fs {I6}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$resulting from the decay of 2961 level by the 2840.2|g transition but unobserved in other datasets, therefore tentatively adopted here 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E {+162}Ho (67.0 min) |e decay no longer supports the existence of this level. It is not included in the Adopted Levels. 


level_energy_unit: KEV
level_comment:
It is tempting to associate this level with the 2525.6 level in (|g,|g'), but the pattern of deexciting |g's from these two is different. 


level_energy_unit: KEV
level_comment:
E Reported only by 1973St07. Level is not reported in other studies and is not included in the {+162}Dy Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J J|p(2100)=6+, J|p(2101)=(9-), J|p(2104)=2+,3+,(4+) in Adopted Levels. (d,d') may be exciting a separate level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T weighted average of: 2.19 ns 3, from 1967Ku07, pulsed-beam techniques; and 2.17 ns 4, from the listed B(E2)|^ and the theoretical |a=6.14 (2005KiZW). An estimated uncertainty of 1.4% in this |a value has been included the computation. Others: 2.22 ns (1959Bi10); and 2.0 ns {I2} (1967As03). 
BE2 Weighted average of 5.11 {I15} (1960El07) and 5.38 {I5} (from matrix element of 1972Er04). Others: 5.1 {I4} (1961Go09), 4.68 {I35} and 4.80 {I35} from ce data (1963Gr04), and 5.2 {I3} (1974ThZG). For comparison, the evaluation of 1987Ra01 gives 5.28 {I15} which is based on half-life as well as B(E2) measurements. 
G$From 1999Br43 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
T From 1978Hu03. 
BE2 B(E2)(2+ to 4+) weighted average of 2.64 {I24} (1974Sa03) and 2.70 {I16} (1974ThZG) and B(E4) from 1972Er04. Others: 2.75 {I13} [1978Hu03 scaled by evaluator to B(E2)(0+ to 2+)=5.35] and 2.93 {I20} (from matrix element of 3.83 {I12} from 1974Le09). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T From 1978Hu03. 
BE2$B(E2)(4+ to 6+) weighted average of 2.00 {I9} (1974Sa03) and 2.31 {I13} [1978Hu03 scaled by evaluator to B(E2)(0+ to 2+)=5.35]. 
G From 1999Br43. The '+' sign not listed by these authors, but is included by the evaluator, based on the expected similarity with the adjacent even Dy isotopes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 Weighted average of 0.130 {I5} (1974Ba81), 0.105 {I8} (1974Oe01), 0.129 {I10} (1975VeZW), and 0.118 {I6} (1981Mc06). Others: 0.094 {I18} (1965Yo04), 0.124 (1968Gr08), 0.153 {I11} (1972Do01), and 0.125 {I30} (1974ThZG). 
T computed by the evaluator from B(E2)|^ and the adopted |g branching. 
G From 1999Br43 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T Weighted average of 4.1 ps {I3} (1977Ke06), 4.6 ps {I3} (1978Hu03), and 4.1 ps {I2} (1979Gu15). 
BE2$B(E2)(6+ to 8+) weighted average of 1.85 {I10} (1974Sa03) and 2.19 {I14} [1978Hu03 scaled by evaluator to B(E2)(0+ to 2+)=5.35]. 
G From 1999Br43. Plus sign not listed by these authors, but is included by the evaluator, based on the expected similarity with the adjacent even Dy isotopes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
BE3 From 1981Mc06. Others: 0.81 and 0.103 (1974Oe01) and 0.108 {I27} (1974ThZG); and 0.094 deduced from (d,d') inelastic scattering (1968Gr08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
BE3 From 1974ThZG. Others: 0.051 (1974Oe01) and <0.015 (1981Mc06); and 0.027 deduced from (d,d') inelastic scattering (1968Gr08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T From 1977Ke06. Other: 1.46 ps {I7} (1979Gu15). 
BE2$B(E2)(8+ to 10+) weighted average of 2.53 {I34} (1974Sa03) and 2.68 {I27} [1978Hu03 scaled by evaluator to B(E2)(0+ to 2+)=5.35]. 
G From 1999Br43, who report g=0.364 {I35}. Plus sign not listed by these authors, but is included by the evaluator, based on the expected similarity with the adjacent even Dy isotopes. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T Weighted average of 0.93 ps {I6} (1977Ke06) and 0.76 ps {I4} (1979Gu15). 
BE2$B(E2)(10+ to 12+) weighted average of 3.6 {I14} (1974Sa03) and 2.11 {I26} [1978Hu03 scaled by evaluator to B(E2)(0+ to 2+)=5.35]. 


level_energy_unit: KEV
level_comment:
Assigned by 1995Be02 as the 4+ member of the K|p=1+ band at 1745 keV. However, population of this level in (d,p) is not consistent with such an assignment. 


level_energy_unit: KEV
level_comment:
Level not reported in any of the other studies of {+162}Dy. The evaluator has chosen not to include it in the Adopted Levels data set. It is assumed that it is not the same as the 2584.0 {I4} level. 


level_energy_unit: KEV
level_comment:
Level not reported in any of the other studies of {+162}Dy. It is not included in the Adopted Levels data set. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
T$2018Be25 estimate lower limits of partial half-lives at the level of |?10{+15}-10{+18} years with 90% confidence level for different decay modes and branches, see the table above. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: US
level_comment:
T$ from |g|g(t) (2011Sw02) 
$Proposed configuration=|n11/2[505]~#|n5/2[523], K|p=8+, based on various considerations in 2011Sw02 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$T{-1/2}({+163}Dy{+66+} ion)=48 d {I3} (1997Kl06,1992Ju01) 
$%|b-({+163}Dy{+66+} ion)=100 
J$spin from electron paramagnetic resonance (1958Pa11) and atomic beam. (1962Sp03). Parity: L(d,t)=3 from 0+ target; measured |m is consistent with |n5/2[523]. 
$Q{-4}|?+0.67 (1972DaYT, atomic beam magnetic resonance) 
MOMM1$atomic beam magnetic resonance (1974Fe05,1972FeZY). Others: 0.66 {I4} (1973Mu06, hyperfine structure in optical spectroscopy), +0.65 {I6} (1970Ch31, atomic beam), +0.66 {I13} (1967Eb01, atomic beam), +0.635 {I14} (1963Bl25, electron paramagnetic resonance), 0.51 {I6} (1958Pa11, electron paramagnetic resonance). Recalculations: 1962Li06, 1972Ro36). 
MOME2$quadrupole hyperfine splitting of muonic M x rays (1984Ta04). Sign from |m=+2.57 {I17} (AB, Sternheimer correction included, 1970Ch31). Others: 2.318 {I6} (1974Fe05,1972FeZY, atomic beam), +2.46 {I21} (1973Mu06, hyperfine structure in optical spectroscopy), +2.5 {I3} (1970Ch31, atomic beam), +2.46 {I4} (1967Eb01, atomic beam), +1.6 {I4} (1963Bl25, electron paramagnetic resonance), 1.3 {I4} (1958Pa11, electron paramagnetic resonance). 1966Ko14 measured ratio Q({+163}Dy)/Q({+161}Dy) in NMR method. 
$|D<r{+2}>({+162}Dy-{+163}Dy)=0.041 fm{+2} {I2} (1990Wa25) 
From an evaluation of nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.2091 fm 25. 
$Hexadecapole moment: 1972FeZY (also 1972DaYT) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J$L(d,t)=3. M1+E2 |g from 9/2- rules out 5/2-. 
T$from recoil-distance method in Coul. ex. Other: 1.34 ns {I7} from B(E2) in Coul. Ex 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=(2) (E2) |g to 9/2-, |DJ=1 |g to 11/2-. Coulomb excited. Band member. 
T$from DSAM in Coul. ex. (1987Mi04) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=1 |g to 13/2- and |DJ=2, (E2) |g to 11/2-. Coulomb excited. Band member. 
T$from DSAM in Coul. ex. (1987Mi04) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 13/2-, |g to 15/2-. Coulomb excited. Band member. 
T$from DSAM in Coul. ex. (1987Mi04) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$E1 |g's to (5/2)- and (1/2)- 
E$from L(d,t)=(2+5), another 11/2- level (possibly due to 3/2[521]) may be present near this energy 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$(M1,E2) |g to 5/2-; |g to 9/2-; band member. In ({+3}He,|a), 11/2[505] is assigned, based on large cross section and analogy with {+161}Dy, but here this orbital is assigned to a level at 851.5. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J Large cross section in ({+3}He,|a) indicates a large L transfer. Relative cross section for population in (d,p) and (d,t) indicates level is a hole state. Most plausibly assigned as the 11/2[505] state. Assignment is also consistent with systematics. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J L(d,t)=0. Probable bandhead of the K|p=2- octupole vibration built on the 5/2[523] g.s. orbital. The low log| {Ift} value indicates that it is populated via a |n5/2[523]|)|p7/2[523], {Iau}, |b{+-} transition, implying that the dominant configuration is |n5/2[523]-|p7/2[523]+|p3/2[411]. This situation is presumably similar to that in {+162}Dy, where the K|p=2- octupole vibration occurs relatively low in the level scheme (1148.2 keV) and has these two proton orbitals as the dominant configuration, which is what is expected for the K|p=2- octupole phonon in this mass region. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=(2) |g to 15/2-, |DJ=1 |g to 17/2-. Coulomb excited. Band member. 
T$from DSAM in Coul. ex. (1987Mi04) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=(2) |g to 17/2-, |g to 19/2-. Coulomb excited. Band member. 
T$from DSAM in Coul. ex. (1987Mi04) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$M1 |g to 1/2+; |g to 7/2+. L(d,t)=0 for a 1145 {I2} group (1976Ma33) is inconsistent with J=3/2. The level in (d,t) may be different 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$M1 |g's to (1/2)- and (5/2)-; band member. L(d,t)=(0) for a 1191 group (1976Ma33) is inconsistent with J|p=(3/2)-. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$(E1) |g to (1/2)-; (M1,E2) |g to (3/2+); resonance-averaged n capture. L(d,t)=(0) is inconsistent with (3/2+) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
J$(M1,E2) |g's to (1/2)- and 3/2-. Resonance-averaged n capture results (1989Sc31) suggest positive parity 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$d|s/d|W=2 
L$from figure 4 and consultation (in 1998) with one of the authors of 1985Lo19. L=(2) is less likely 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$possibly a doublet which is predominantly the 3/2+ member of the K-2 |g-vibrational band built on 5/2[642], but may also contain a 11/2-, 3/2[521] component (1989Sc31). 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
E$918 (1967Sc05), 918 (1970Gr46), 915 (1974Ho24). On the basis of a model-dependent assignment, 1989Sc31 suggest that a 915.2 group is populated in (d,p) and a 916.1 in (d,t) 


level_energy_unit: KEV
level_comment:
J if this is the same level as the 1734 level in (d,p), then J|p=3/2+,5/2+ and the 1730 |g is E1, not M1 as assumed by 2003No02. 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
J from (t,p), J|p=5/2+. This implies that the deexciting |g's are E1, not M1 as assumed by 2003No02. 


level_energy_unit: KEV
level_comment:
J if this is the same as the 1986 level in (d,t), then J|p=3/2+,5/2+ and the deexciting |g is E1, not M1 as assumed by 2003No02. 


level_energy_unit: KEV
level_spin_parity: 5/2,7/2
level_comment:
J from L=4 in (t,p), |p=+, suggesting that the deexciting |g's are E1, not M1 as suggested by 2003No02. 


level_energy_unit: KEV
level_comment:
T value computed not taking into account the 2213 |g. Including this |g, 2003No02 compute 20.8 meV 26. 
BM1 Value computed not taking into account the 2213 |g. Including this |g, 2003No02 compute 0.151 {I19}. 


level_energy_unit: KEV
level_comment:
J if this is the same as the 2387 level in (d,t), J|p=3/2+,5/2+, which would imply that the deexciting |g's are E1, not M1 as assumed by 2003No02. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
T value computed using the listed |g-decay modes. Neglecting the 2514 |g, 2003No02 compute 25.4 meV 22. 
BM1 Neglecting the 2514 |g, 2003No02 compute B(M1)=0.127 {I11}. 


level_energy_unit: KEV
level_comment:
T value computed not taking into account the 2844 |g. Including this |g, 2003No02 compute 11.3 meV 9. 
BM1 Value computed not taking into account the 2844 |g. Including this |g, 2003No02 compute 0.039 {I3}. 


level_energy_unit: KEV
level_spin_parity: 5/2,7/2
level_comment:
T value computed not taking into account the 2946 |g. Including this |g, 2003No02 compute 6.2 meV 5. 
BM1 Value computed not taking into account the 2946 |g. Including this |g, 2003No02 compute 0.020 {I2}. 


level_energy_unit: KEV
level_spin_parity: 5/2,7/2
level_comment:
T value computed not taking into account the 3212 |g. Including this |g, 2003No02 compute 1.6 meV 6. 
BM1 Value computed not taking into account the 3212 |g. Including this |g, 2003No02 compute 0.004 {I1}. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
T value computed using the listed |g-decay modes. Neglecting the 3506 |g, 2003No02 compute 2.4 meV 8. 
BM1 Neglecting the 3506 |g, 2003No02 compute B(M1)=0.005. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
T value computed not taking into account the 3565 |g. Including this |g, 2003No02 compute 6.0 meV 8. If this level decays through the 3471 |g and 3638 |g only, 3.8 meV 7 is computed. If it decays through the 3638 |g only, 1.6 meV 4 is computed. 
BM1 Value computed not taking into account the 3565 |g. Including this |g, 2003No02 compute B(M1)=0.011 {I2}. If this level decays through the 3471 |g and 3638 |g only, 0.007 {I1} is computed. If it decays by the 3638 |g only, 0.003 {I1} is computed. 


level_energy_unit: KEV
level_comment:
T value computed not taking into account the 3506 |g. Including this |g, 2003No02 compute 5.9 meV 16. 
BM1 Value computed not taking into account the 3506 |g. Including this |g, 2003No02 compute 0.010 {I3}. 


level_energy_unit: KEV
level_spin_parity: 5/2,7/2
level_comment:
T value computed using the listed |g-decay modes. Neglecting the 3617 |g, 2003No02 compute 10.5 meV 11. 
BM1 Neglecting the 3617 |g, 2003No02 compute B(M1)=0.018 {I2}. 


level_energy_unit: KEV
level_comment:
T value computed not taking into account the 3565 |g. Including this |g, 2003No02 compute 5.5 meV 8. 
BM1 Value computed not taking into account the 3565 |g. Including this |g, 2003No02 compute 0.009 {I1}. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
T value computed using the listed |g-decay modes. Neglecting the 3604 |g, 2003No02 compute 4.3 meV 7. 
BM1 Neglecting the 3604 |g, 2003No02 compute B(M1)=0.007 {I1}. 


level_energy_unit: KEV
level_comment:
T value computed not taking into account the 3776 |g. Including this |g, 2003No02 compute 10.6 meV 17. 
BM1 Value computed not taking into account the 3776 |g. Including this |g, 2003No02 compute 0.015 {I2}. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
T$from nuclear recoil (1966As03). Other: 1.34 ns {I7} from B(E2) 
BE2$others: 2.44 {I14} (from E2 matrix element=3.83 {I10} in 1978Wo02), 2.56 {I15} (1963El06), 1960Be16, 1959De29, 1957He26 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_comment:
T$from B(E2) and adopted |g properties 
BE2$others: 0.89 {I2} (from E2 matrix element=2.31 {I2} in 1978Wo02), 0.68 {I10} (1963El06), 1960Be16, 1959De29, 1957He26 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)-
level_lifetime_unit: NS
level_comment:
T$from |eB(E2)|^(428|g) and adopted |g properties. Other: 0.29 ns {I12} from |eB(E2)|^(354|g) and adopted |g properties 
$B(E2)(7/2- to 5/2-)=0.0088 {I24} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)-
level_lifetime_unit: NS
level_comment:
T$from |eB(E2)|^(402|g) and adopted |g properties. Other: |<0.78 ns from |eB(E2)|^(475|g) and adopted |g properties 
$B(E2)(7/2- to 5/2-)=0.006 {I4} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$could correspond to 587.5 in (d,p) (1989Sc31) 
S$0.20 for L=5 expected for 9/2- assignment (1970Gr46) 


level_energy_unit: KEV
level_spin_parity: (3/2)+&(11/2-)
level_comment:
E,J$consistent with the possibility that this is a doublet which is predominantly the 3/2+ member of K|p=1/2+ band (from 5/2[642]-Q{-22}), but may also contain a 11/2-, 3/2[521] component (1989Sc31). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
L,J$inconsistent with adopted J|p=3/2+. It is possible that this group corresponds to 5/2-, 1258 level 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$d|s/d|W=112 
J$probable 11/2[505] state, based on large |s and by analogy with {+161}Dy. Note that 1980St31 tentatively suggest that the bandhead is at 514 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$The rms charge radius (<r{+2}>){+1/2}: 5.222 fm {I11} (2013An02 evaluation). See also 2009An12 for trends in nuclear radii 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$Mossbauer effect (1968Mu01). Others: |m=+0.73 {I3} (1970Be36), 1967Ku07. 
J$E2 |g to 0+. 
T$from 2016Pr01 evaluation, based on B(E2) measurements in Coulomb excitation: B(E2)=5.66 {I6} (1974Wo01), 5.59 {I12} (1974Sh12, earlier value of 5.55 {I9} in 1973Gr05), 5.57 {I5} (1972Er04), 5.64 {I25} (1960El07), 6.1 {I15} (1956Hu49, not included in the evaluation); measured mean lifetimes |t=3.460 ns {I110} (1969Av01, (particle)|g(t) in Coulomb excitation); |t=3.444 ns {I54} (1967Ku07) and |t=3.490 ns {I90} (1959Bi10) from (p|g(t) in (p,p'|g). Other: B(E2)=5.48 {I10} from muonic x-rays (1970Hi03). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$IPAC (1997Al25). Other: +1.48 {I48} (1989Do12, transient-field technique) 
J$E2 |g to 2+; M1+E2 673.743|g from 4+ 
T$from B(E2) and recoil-distance Doppler-shift in Coulomb excitation 
|b{-4}=-0.023 {I7} (1971Su01), from cross section of first 4+ state in {+162}Dy populated in {+164}Dy(p,t) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field technique. Others:+1.62 {I30} (1997Al25), +1.68 {I48} (1983Se09) 
J$E2 |g to 4+; no |g to 0+ and 2+ 
T$from B(E2) and recoil-distance Doppler-shift in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field technique. Other:+0.62 {I20} (1989Do12) 
J$E2 |g to 0+. 
T$from B(E2) in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 6+; band structure 
T$from B(E2), recoil-distance Doppler-shift (RDDS), and Doppler-broadened line shapes in Coulomb excitation 
MOMM1$transient-field technique. Other: +2.2 {I7} (1989Do12) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$E1 277.488|g to 2+ gives 1-,2-,3-; 1- and 2- ruled out by 123.32|g to 4+ since it would require an unreasonably large B(M2) 
BE3$from Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 8+; band structure 
T$from Doppler-broadened line shape in Coulomb excitation 
MOMM1$transient-field technique. Other:+3.5 {I13} (1989Do12) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$the existence of this level is questioned by 2017Go07 in (n,n'|g) 
J$possible |b feeding from (5+); |g to 2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$(2,3)+ from ARC in (n,|g); 1716.25|g E2 to 0+ 
T$from Doppler broadening of second order of reflection in a curved-crystal spectrometer in (n,|g) (1998Le03). Statistical assumptions of initial recoil velocity was used in the analysis. T{-1/2}=0.35-5.7 ps if extreme conditions were used for the initial recoil velocity 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
E,J$from ARC in (n,|g). This level is probably different from 1933.62 level due to very different spins implied from population mechanisms 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$(2)+ for one component in (n,|g) E=res from J|p=(2,3,4)+ from ARC; and |g to 0+. Other component is 2+,3+ from ARC in (n,|g) 


level_energy_unit: KEV
level_spin_parity: (5)-
level_comment:
J$intensity pattern in (t,|a). 
E$this level seems different from 1998.2 level populated in |b{+-} decay due to different J|p values implied from (t,|a) and from decay modes in |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: PS
level_comment:
E$2017Go07 in (n,n'|g) suggests that there could be two different levels of close energy excited in {+164}Tb |b{+-} decay and in (n,|g) E=thermal and (n,n'|g) based on their observed deexcitations not in agreement with those in {+164}Tb |b{+-} decay 
J$gammas to 2+ and 4+; E2 |g to 3+; evidence of |b feeding from (5+). Implied [M2] |g to 2- is inconsistent 
T$from Doppler broadening of second order of reflection in a curved-crystal spectrometer in (n,|g) (1997Co18). Statistical assumptions of initial recoil velocity was used in the analysis. T{-1/2}=0.076-0.53 ps if extreme conditions were used for the initial recoil velocity 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$gammas to 2+ and 4+; evidence of |b feeding from (5+). J|p=(5+) assigned in (d,p) for a 2190 group 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
BM1$from (p,p'). Other: 0.43 {I10} (1995Jo20) in (n,n'|g) 
T$from DSAM in (n,n'|g) (1995Jo20). Other: |G=0.035 eV {i6} (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
BM1$from (e,e'). Other: 0.43 {I20} (1995Jo20) in (n,n'|g) 
T$from DSAM in (n,n'|g) (1995Jo20). Other: |G=0.179 eV {i22} (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$4+,(1+,2+,3+) (ARC). Population from a 3- resonance (1972Da28) rules out 1+. R(2 keV/{I24} keV)=1.12 {I13} 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_comment:
J$2+,3+ (ARC). 4+ is ruled out by population from 2-, 1.71 eV resonance. R(2 keV/{I24} keV)=1.48 {I16} 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$2+,3+ (ARC). 4+ is ruled out by population from 2-, 1.71 eV resonance. R(2 keV/{I24} keV)=1.3 {I3} 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
J$2+,3+ (ARC). 4+ is ruled out by population from 2-, 1.71 eV resonance. R(2 keV/{I24} keV)=1.06 {I15} 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
J$2+,3+ (ARC). 4+ is ruled out by population from 2-, 1.71 eV resonance. R(2 keV/{I24} keV)=1.21 {I19} 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E,J$reduced |g-intensities indicate an unresolved doublet of J|p=2+,3+ and 2+,3+,4+ (ARC). R(2 keV/{I24} keV)=0.87 {I8} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$Placements of 549.1|g, tentative 911.0|g and 1431.0|g from this level are given by 1984De31 but not observed in 2017Go07 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_uncertain: ?
level_comment:
E$the existence of this level is not confirmed by 2017Go07 and the |g transitions from this level are placed differently in 2017Go07. 
J$excitation function suggests J=(2) (1984De31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$Other B(M1): <0.31 (1985Dj02) for the unresolved group of three states of J|p=1+ at 3111, 3160 and 3170 
$[B(M1)(orbital)/B(M1)(spin)]{+1/2}=1.8 to 2.3 or 3.4 to 4.3 (1985Dj02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
B(E2)=5.59 {I3} from weighted average of 5.64 {I25} (1960El07); 5.48 {I10} (1970Hi03, muonic x rays); 5.57 {I5} (1972Er04); 5.55 {I9} (1973Gr05); 5.59 {I10} (1974Sh12); 5.66 {I6} (1974Wo01). 
T$from B(E2). Other: from p|g(t), T{-1/2}=2.40 ns {I8} (1969Av01). In Adopted Levels, Gammas dataset, value is 2.393 ns 29 (from 2016Pr01 evaluation) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from weighted average of mean lifetime |t=265 ps {I29} (from B(E2)(2+ to 4+)=2.83 {I31}, 1974Sa03); 294 ps {I9} (Doppler-shift recoil-distance, 1977Si15); 286 ps {I15} (Doppler-shift recoil distance, 1978Sa03). 
g-factor=0.25 {I3} (1997Al25), 0.37 {I12} (1989Do12) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
g-factor=0.325 {I17} (1999Br43), 0.27 {I5} (1997Al25), +0.28 {I8} (1983Se09,1989Do12) 
T$from weighted average of mean lifetime |t=44.4 ps {I24} (from B(E2)(4+ to 6+)=2.06 {I11}, 1974Sa03); 37.7 ps {I14} (Doppler-shift recoil-distance, 1977Si15); 39.0 ps {I19} (Doppler-shift recoil distance, 1978Sa03). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J multiple Coulomb-excitation yield shows J|p=2+, K=2 (1974Oe01). 
T from B(E2)=0.114 {I6} (1981Mc06). Others B(E2) measurements: 0.122 {I5} (1977Wo03); 0.101 {I9} (1974Oe01); 0.121 {I5} (1974Ba81); 0.13 {I2} (1965Yo04). 
g-factor=0.38 {I3} (1999Br43), 0.31 {I10} (1989Do12) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
g-factor=0.310 {I20} (1999Br43), 0.27 {I9} (1989Do12). 
T$from weighted average of mean lifetime |t=11.7 ps {I7} (from B(E2)(6+ to 8+)=1.86 {I11}, 1974Sa03); 8.9 ps {I11} (Doppler-broadened line shape, 1977Ke06); 9.8 ps {I7} (Doppler-shift recoil distance, 1977Si15); 10.4 ps {I7} (Doppler-shift recoil distance, 1978Sa03). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
g-factor=0.31 {I4} (1999Br43), 0.35 {I13} (1989Do12) 
T$from weighted average of mean lifetime |t=3.37 ps {I21} (in single measurements) and 3.23 ps {I20} (in particle-|g coin) (Doppler-broadened line shape (1977Ke06)). Others: |t=3.2 ps {I4} (from B(E2)(8+ to 10+)=2.44 {I32}, (1974Sa03)), 3.7 ps {I8} (recoil distance Doppler-shift (1978Sa03)). 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$from weighted average of mean lifetime |t=1.64 ps {I10} in single measurements and 1.77 ps {I11} in particle-|g coin (Doppler-broadened line shape, 1977Ke06)). Others: |t=1.3 ps {I7} (from B(E2)(10+ to 12+)=2.7 {I14}, 1974Sa03); 1.6 ps {I8} (recoil-distance Doppler-shift, 1978Sa03). 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T from weighted average of mean life=0.95 ps {I6} (in singles measurements) and 1.1 ps {I2} (in particle-|g coin) (Doppler-broadened line shape (1977Ke06)). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$this value can be compared with 2.393 ns {I29} in the ENSDF database 
$|b{-2}=0.332 {I4}, Q{-transition}=7.58 {I9} (2020Ca03) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: NS
level_comment:
T$this value can be compared with 0.201 ns {I8} in the ENSDF database 
$Q{-transition}=7.35 {I14} (2020Ca03) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
T$this value can be compared with 0.0272 ns {I8} in the ENSDF database 
$Q{-transition}=8.0 {I11} (2020Ca03) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$I{-s,g.s.}=6 eVb {I+3-4} 
$Compiler's note: in earlier (|g,|g') studies, a large branching to the first 2+ state was reported 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: H
level_comment:
T$weighted average of 2.29 h {I6} (2014Le22, decay curves for 94.7|g and 361.7|g); 2.334 h {I1} (1989Ab05, decay curve for 94.7|g, three measurements, uncertainty increased to 0.004 h to decrease its weight to |?50%, and to account for possible systematic uncertainties); 2.334 h {I6} (1973Ha20, integral activity using a scintillation detector, average of five measurements); 2.317 h {I8} (1963Pe11). Others: 2.4 h (1962Ma24); 2.373 h {I8} (1960Ha34); 2.33 h {I8} (1960Wi10); 2.355 h {I2} (1959Cr80); 2.369 h {I10} (1958Gu09); 2.38 h {I4} (1954Ma62); 2.3195 h {I23} (1952Sh42); 2.42 h {I5} (1947Sl14); 2.33 h (1947Se33); 2.5 h (1947In08); 2.333 h {I25} (1946Bo25); 2.5 h (1938Po05); 2.5 h (1935He03); 2.5 h {I1} (1935Ma03). Weighted average of all the values listed with uncertainties, but with a minimum uncertainty of 0.010 h in pre-1960 measurements, is 2.338 h {I5} with normalized |h{+2}=3.6 as compared to critical |h{+2}=2.1. Unweighted average is 2.358 h {I15}. 
J$spin from atomic beam (1961Ca07); parity from allowed |b{+-} to |p=+ level at E=995. 
MOMM1,MOME2$atomic beam method, deduced hyperfine structure constants a=|+89.8 MHz {I7} and b=|-1521 MHz {I30}, |m=-0.50, Q=2.8, |m/Q<0 (1968Ra03). Experimentally, only the relative signs of |m and Q were determined in 1968Ra03, however, authors mentioned that sign of Q was chosen positive (probably based on agreement of measured and predicted Q=+3.2 for |n7/2[633] configuration), thereby fixing the negative sign of |m. In 1989Ra17 compilation, |m=-0.520 {I5} and Q=-3.49 {I7} were deduced with reference to {+163}Dy, using hyperfine constants a and b from 1968Ra03 for {+165}Dy, and hyperfine constants A=+162.754272 MHz {I20}, B=+1152.8635 MHz {I12} for {+163}Dy from 1974Fe05. Note that relative signs of |m and Q in 1989Ra17 were inconsistent with those deduced in 1968Ra03. In 2019StZV evaluation, sign of Q is assigned positive, and the value of |m in 2019StZV evaluation is slightly different from that in 1989Ra17. In evaluator's opinion, while the signs of |m and Q are not known experimentally, systematics of neighboring odd-A Dy nuclei ({+155},{+157},{+159},{+161},{+163}Dy), N=99 isotones (7/2[633] g.s. in {+167}Er, {+169}Yb and {+171}Hf), and experimental |b{-2} parameters in Fig. 12 of 1984Ta04 for several rare-earth nuclei strongly suggest positive sign for Q, thus negative sign for |m, from experimental |m/Q<0 in 1968Ra03. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
J$108.159 |g E3 to 7/2+, 425.335|g M1,E2 from 5/2- 
T$from time scaling of |g rays from {+165}Dy isomer decay (1964Ha19). Others: 1.263 min {I16} (1960Ho16), 1.3 min {I2} (1960Wi10) 
T$other: 1959Cr80. 
$%IT: from %IT+%|b{+-}=%I(|g+ce)(108.6|g)({+165}Dy)+|SI(|g+ce to g.s.)({+165}Ho)=100, using measured I|g in 1972Ma06. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: NS
level_comment:
J$72.768 |g E2 to 1/2-; band assignment 
T$from (n,|g) (1978An22). Other from (n,|g): 10.7 ns {I35} (1968Na21). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$139.096|g E2 to (3/2)-, 116.76|g E2 (from ce data) to (5/2)-; band assignment 
T$this upper limit deduced in 1968Na21 results in larger B(E2)(W.u.) of 116.760|g and 139.096|g than allowed by RUL, which may indicate a T{-1/2} greater than this upper limit. 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
J$565.578|g E2 to (9/2)+, 648.962|g M1+E2 to 7/2+; 110.328|g to 3/2+; 462.883|g to (11/2+); band assignment 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-,9/2-)
level_comment:
E$probably a doublet with J|p=(5/2 to 11/2)- and (7/2,9/2)+ (1990Ka21) in (n,|g) E=thermal 
J$441.12|g to 7/2-, 365.724|g to 9/2-; L(t,p)=(2) from 5/2- 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$primary |g from 1/2+, 1074.75|g to (9/2)+, 420.4|g and 452.208|g to (7/2)-, 509.139|g to (7/2)+. But (1/2,3/2) from ARC in (n,|g) E=2, 24 keV is inconsistent 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$weighted average of 1195 {I2} from (t,p) and 1197.1 {I5} from (d,p) 
J$L(t,p)=0 from 5/2- target. 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$(1/2,3/2,5/2+) from ARC in (n,|g) E=2, 24 keV; 846.058|g to (1/2)-, 258.217|g to (5/2+), possible 882.833|g to 5/2- 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2-
level_uncertain: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$S(n)=5715.96 {I5} (2021Wa16), E(n)=2 keV 
J$s- or p-wave capture in 0+ g.s. of {+164}Dy 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2-
level_uncertain: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$S(n)=5715.96 {I5} (2021Wa16), E(n)=24 keV 
J$s- or p-wave capture in 0+ g.s. of {+164}Dy 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E$from the Adopted Levels 
T$from the Adopted levels, where value is from time scaling of |g rays in 1964Ha19. Others: 1.263 min {I16} (1960Ho16), 1960Wi10, 1959Cr80. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_comment:
$d|s/d|W (|mb/sr)=27 
J$(13/2+) in the Adopted Levels 
$I(p)(14 MeV)=6.3 {I8}, I(p)(22 MeV)=49.4 {I18} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$d|s/d|W (|mb/sr)=7 
L$(1) suggested by intensity ratio, 3 expected from band assignment 
$I(p)(14 MeV)=2.1 {I4}, I(p)(22 MeV)=1.8 {I4} 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$d|s/d|W (|mb/sr)=156 
J$none in the Adopted Levels 
$I(p)(14 MeV)=3.9 {I12}, I(p)(22 MeV)=9.0 {I18} 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$d|s/d|W (|mb/sr)=108 
J$(3/2+) in the Adopted Levels 
$I(p)(14 MeV)=46 {I4}, I(p)(22 MeV)=39 {I5} 
L$(1) suggested by intensity ratio, 3 expected from band assignment 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
J g.s. of even-even nucleus; L(t,p)=0. 
T weighted average from 81.8 h {I2} (1962Gu03) and 81.46 h {I20} (1963Ho15). Others: 80.2 h {I5} (1960He09), 82 h (1950Bu30), 81 h (1949Ke22). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$From |g|g|g(t) (2020Ca03), fast timing triple coincidences events from HPGe - LaBr{-3} - LaBr{-3} detector system 
$|b{-2}=0.344 {I17} (2020Ca03) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MIN
level_comment:
T$from decay curves for 133, 250, 259, 310 and 570 |g rays (1977Tu01). Others: |?6 min (1974Ka21), |?4.5 min (1963Ka10), 4.4 min {I4} (1960Wi10) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_uncertain: ?
level_comment:
J$possible |n5/2[512] bandhead, expected at |?100 keV, based on energy systematics for this bandhead in nearby N=101 isotones, which should deexcite to the 3/2 member of the 1/2[521] band (1999As03). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_uncertain: ?
level_comment:
J$possible |n5/2[512] bandhead, expected at |?100 keV, based on energy systematics for this bandhead in nearby N=101 isotones, which should deexcite to the 3/2 member of the 1/2[521] band (1999As03). Same J|p assignments in the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
J g.s. of even-even nucleus. 
T weighted average of 8.5 min {I5} (1982Ge04) and 8.8 min {I3} (1990Ch37). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from |g(t) in {+9}Be({+236}U,F|g) by 2019Zh49. The presence of this isomer is affirmed independently here using |g-|g-|g coincidence with Gammashpere (2019Zh49) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: S
level_comment:
J$log| {Ift}|?5.4 to 7/2- 7/2[523] g.s. of {+169}Ho; 5/2[512] assignment for 103rd neutron orbital is well established in this mass region. 
T$from 1990Ch34. Other: 78 s {I37} (2017Wu04) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: US
level_comment:
J$from systematics of (1/2-) isomers in heavier N=103 isotones. 
T$from 166.1|g(t) in {+9}Be({+238}U,f|g) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$From systematics of known quasiparticle states in neighboring nuclei and the proposed configuration (by the compiler). The assignment is tentative. 
T$From a fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. The data analysis included contributions from the parent, daughter and grand-daughter decays, as well as a constant background. 
CONF$|n5/2[512] Nilsson orbital, based on systematics of known structures in neighboring, well-deformed nuclei (by the compiler). The assignment is tentative. 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$7/2- from systematics of known quasiparticle states in neighboring nuclei 
T$from 2017Wu04, using a fit to the implanted ion-|b{+-}(t) spectrum applying the least-squares and maximum-likelihood methods; data analysis included contributions from the parent, daughter and ground-daughter decays, as well as a constant background. Value is reported as 4.07 s {I40} in 2017Wu04 
$Production |s(at 1 GeV/nucleon)=441 nb {I18} (2012Ku26) 


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 
E$ the observed {+172}Dy fragments assumed to correspond to the g.s. 
T$ limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by 3 s from systematics (2012Au07), and 7.7 s from theoretical calculations (1997Mo25) 
$ Production |s=121 nb {I7} (2012Ku26) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$From 2017Wu04, where 0.674 s {I66} is reported. Other: 710 ms {I50} (2016Wa19) 
E,J,%IT$From 2016Wa19 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E,J$Interpreted as (2+) member of |g-vibrational band. Extrapolated value of 671 keV from the (5+), (6+) and (7+) members in Fig. 2. Population of this level is likely from a potential 3+ isomeric state, also present in fission of {+238}U. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$K|p=8- isomer with configuration=|n7/2[514]~#|n9/2[624] (2016Wa19) 
T$from decay curve for summed |g rays from the 1278-keV isomer (2016Wa19) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$From systematics of known quasiparticle states in neighboring nuclei and the proposed configuration (by the evaluator). The assignment is tentative. 
T$From 2017Wu04, using a fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. The data analysis included contributions from the parent, daughter and ground-daughter decays, as well as a constant background. 
CONF$|n9/2[624] Nilsson orbital, based on systematics of known structures in neighboring, well-deformed nuclei (by the evaluator). The assignment is tentative. 
$ Production |s(at 1 GeV/nucleon)=18 nb {I2} (2012Ku26) 


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. Predicted %|b{+-}n=0 (1997Mo25) 
E$ the observed {+174}Dy fragments assumed to correspond to the g.s. 
T$ limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by 1.8 s from theoretical calculations (1997Mo25) 
$ Production |s=1.9 nb {I6} (2012Ku26) 


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}=1.026 s, %|b{+-}n=0 (2019Mo01) 
$Theoretical T{-1/2}=2.16 s, %|b{+-}n=0.3 (2016Ma12) 
$A total of six counts were assigned to {+175}Dy for spectrometer setting on Pr, and 22 counts for setting on Gd. 
$Production |s=57 pb {I12} for Gd setting, with 50% systematic uncertainty on |s values (2018Fu08) 
E$it is assumed that the observed events correspond to ground-state activity. 
J$1/2- from |W{-|n}=1/2- orbital proposed in 2019Mo01 
T$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 1.026 s (2019Mo01) and 2.16 s (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+175}Dy is expected to be <2 s, based on measured half-lives of 4.1 s for {+171}Dy, 3.9 s for {+172}Dy, and 1.43 s for {+173}Dy, available in literature. 


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}=867.2 ms, %|b{+-}n=0 (2019Mo01) 
$Theoretical T{-1/2}=1.35 s, %|b{+-}n=0.3 (2016Ma12) 
$A total of three counts were assigned to {+176}Dy for spectrometer setting on Gd. 
$Production |s=7.5 pb {I+73-41} for Gd setting, with 50% systematic uncertainty on |s value (2018Fu08) 
T$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 867 ms (2019Mo01) and 1.35 s (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+176}Dy is expected to be <2 s, based on measured half-lives of 4.1 s for {+171}Dy, 3.9 s for {+172}Dy, and 1.43 s for {+173}Dy, available in literature. 


level_energy_unit: KEV
level_spin_parity: (6-,0-,8+)
level_lifetime_unit: MS
level_comment:
$Since measured T{-1/2} is far shorter than expected for other decay modes, we adopt %p=100 
E$assuming that the proton connects the ground state of {+140}Ho and {+139}Dy 
T$from 1999Ry04 
J$from 2001Fe05, from coupling between a proton at [523]7/2- orbital and a neutron at [402]5/2+, [404]7/2+ and [514]9/2- orbitals; 8+ based on syst (2017Au03) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
%P$decay modes other than p were not observed and their calculated T{-1/2} are far larger than the experimental T{-1/2}; as a consequence we adopt %p=100 
$Configuration=|p([523]7/2-) (1998Da03) 
J$from Nilsson model analysis of lifetime. T{-1/2}(calc) for [523] state=19.1 ms (2000Bb02). 
T$weighted average of 4.2 ms {I4} (1998Da03), 3.9 ms {I5} (1999Ry04), and 4.1 ms {I1} (2008Ka16) 
$Proton decay of J|p(p)=7/2-, T{-1/2}(p)=4.1 ms {I1} g.s.: 
$1) to 0+ g.s. in {+140}Dy: E(p)(0+ g.s.)=1169 keV {I8}, Q(p)=1190 keV {I8} (1998Da03), B(p)=0.991 {I2} 
$2) fine structure - proton decay to first 2+ state in {+140}Dy: E(p)(2+)=968 keV {I10} (2008Ka16, 201 keV {I6} smaller than E(p)(0+ g.s.)), B(p)=0.009 {I2} (2008Ka16) 
$|s|?250 nb at 76 MeV at and 88 MeV of excitation energy (1998Da03); |s|?130 nb at 95 MeV of excitation energy (1999Ry04); 1.4 |mb at 300 MeV of excitation energy (2008Ka16) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
%P$decay modes other than p were not observed and their calculated T{-1/2} are far larger than the experimental T{-1/2}; as a consequence we adopt %p=100 
$Configuration=|p([411]1/2+) (1999Ry04) 
E$from energy difference in Q(p)'s to g.s. 
J$from Nilsson model analysis of lifetime. T{-1/2}(calc) for [411] state=14.6 |ms (2000Bb02) 
T$weighted average of 8 |ms {I3} (1999Ry04), 6.5 |ms {I+9-7} (2001Se03), and 7.4 |ms {I3} (2008Ka16) 
$Proton decay of J|p(p)=1/2+, T{-1/2}(p)=7.3 |ms {I3} isomer: 
$1) to 0+ g.s. in {+140}Dy: E(p)(0+ g.s.)=1234 keV {I8} (weighted average of 1230 keV {I20} (1999Ry04) and 1235 keV {I9} (2001Se03)), Q(p)=1256 keV {I8}, B(p)=0.983 {I5} 
$2) fine structure - proton decay to first 2+ state in {+140}Dy: E(p)(2+)=1030 keV {I14} (2008Ka16, 204 keV {I11} smaller than E(p)(0+ g.s.)), B(p)=0.017 {I5} (2008Ka16) 
$|s|?30 nb at 95 MeV of excitation energy (1999Ry04); 240 nb at 290 MeV of excitation energy (2008Ka16) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (3/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x |?20 keV from particle-rotor calculations (2001Se03) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$Configuration=|p([523]7/2-) (1998Da03) 
T$weighted average of 4.2 ms {I4} (1998Da03), 3.9 ms {I5} (1999Ry04), and 4.1 ms {I1} (2008Ka16) 
$Proton decay of J|p(p)=7/2-, T{-1/2}(p)=4.1 ms {I1} g.s. 
$1) to 0+ g.s. in {+140}Dy: E(p)(0+ g.s.)=1169 keV {I8}, Q(p)=1190 keV {I8} (1998Da03), B(p)=0.991 {I2} 
$2) fine structure - proton decay to first 2+ state in {+140}Dy: E(p)(2+)=968 keV {I10} (2008Ka16, 201 keV {I6} smaller than E(p)(0+ g.s.)), B(p)=0.009 {I2} (2008Ka16) 
$|s|?250 nb at 76 MeV and 88 MeV of excitation energy (1998Da03); |s|?130 nb at 95 MeV of excitation energy (1999Ry04); 1.4 |mb at 300 MeV of excitation energy (2008Ka16) 
$In the high-statistics work of 2001Se03, fine structure - proton decay to 2+ state in {+140}Dy was not observed and a limit of 1% was set for the 2+ branching ratio. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: US
level_comment:
$Configuration=|p([411]1/2+) (1999Ry04) 
E$from energy difference in Q(p)'s to g.s. 
T$weighted average of 8 |ms {I3} (1999Ry04), 6.5 |ms {I+9-7} (2001Se03), and 7.4 |ms {I3} (2008Ka16) 
$Proton decay of J|p(p)=1/2+, T{-1/2}(p)=7.3 |ms {I3} isomer: 
$1) to 0+ g.s. in {+140}Dy: E(p)(0+ g.s.)=1234 keV {I8} (weighted average of 1230 keV {I20} (1999Ry04) and 1235 keV {I9} (2001Se03)), Q(p)=1256 keV {I8}, B(p)=0.983 {I5} 
$2) fine structure - proton decay to first 2+ state in {+140}Dy: E(p)(2+)=1030 keV {I14} (2008Ka16, 204 keV {I11} smaller than E(p)(0+ g.s.)), B(p)=0.017 {I5} (2008Ka16) 
$|s|?30 nb at 95 MeV of excitation energy (1999Ry04); 240 nb at 290 MeV of excitation energy (2008Ka16) 


level_energy_unit: KEV
level_spin_parity: (7-,8+)
level_lifetime_unit: S
level_comment:
J$From 2001Xu01 the strongest observed |g line in {+141}Tb is the 307 keV (15/2-) to (11/2-). Based on relative branching ratios to other final states in {+141}Tb, it is suggested that the ground state J assignment could be 6, 7, or 8. Based on the same experimental data, this suggestion was later modified to 5,6, or 7. It is further mentioned that the energy spectrum of |b-delayed protons is fit by 7{+-} and 8{++} with potential energy surface calculations favoring 7{+-}. Conf=(|ph{-7/2-}[523]~#|nh{-11/2-}[404]) is suggested (2002Xu11). However, branching ratios are also consistent (2002Xu11) with 8{++}, conf=(|ph{-7/2-}[525]~#|nh{-9/2-}[514]) suggested in 1995Mo29 
$Direct proton radioactivity from {+142}Ho was searched for but not found (1993Li40), which is explained because of the small value of the proton separation energy. As a consequence, we adopt %p|?0 
T$from 307 |g(t)({+141}Tb) (2001Xu02) 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: S
level_comment:
T$ from timing of delayed protons (1986Wi15) 
$Configuration=[|ph{-11/2}~#|ns{-1/2}]+[|ph{-11/2}~#|nd{-3/2}] 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
J$ E1 |g to (7-); probable configuration=|ph{-11/2}~#|nh{-11/2} 
T$from |g(t): weighted average of 564 ns {I60} (2006Ta08) and 500 ns {I20} (2001Sc09) 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: NS
level_comment:
$Configuration=|ph{-11/2}~#|nh{-11/2} 
T$from |g(t): weighted average of 564 ns {I60} (2006Ta08) and 500 ns {I20} (2001Sc09). Other: 455 ns {I77} (2005Ta31) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (6-)
level_lifetime_unit: S
level_comment:
E$shell-model analysis shows that this state may be not g.s. but an isomeric state 
J$ Spin assignment of {+146}Ho state is ambiguous: {Ii}) J|p=(6-) (|ph{-11/2}|nd{+-1}{-3/2}) multiplet member was assumed by 2010Ma37 on the basis of relative proton branching ratio (equal to 0.9) to the 13/2- and 15/2- levels in {+145}Tb and that the |b-delayed protons de-excite the states populated by allowed >-transitions of the precursor (see also 1988WiZN); {Iii}) J|p=(9+,10+,11+) (but J=7- can not be excluded) from strong |e decay to J|p=10+ isomer in {+146}Dy (1982Gu07). The evaluators suggest the first version 
T$weighted average of 3.1 s {I5} (1986Wi15), 3.5 s {I3} (1981NoZY), 3.9 s {I8} (1982Gu07), 2.8 s {I5} (2010Ma37) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_comment:
J$based on shell model (three valence protons in (3s{-1/2}, 1h{-11/2}, 2d{-3/2}) subshells) and log| {Ift}=5.0 to {+147}Dy (11/2-), 750 keV (1982No08) 
T$from 1982No08 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
CONF$|ph{-11/2}~#|n{+-2}(2+) 3qp state analogous to 13+,4532 keV in {+148}Er (2001Ro15 in ({+58}Ni,3p|g)) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
CONF$|ph{-11/2}~#|n{+-2}(4+) state analogous to 14+, 4704 keV in {+148}Er (2001Ro15 in ({+58}Ni,3p|g)) 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
E$from 32 keV gap in |g energy loops (2001Ro15 in ({+58}Ni,3p|g)) 
T$from 1982No07 
CONF$|ph{-11/2}{+3} state analogous to 27/2-, 2687 keV in {+149}Ho (2001Ro15 in ({+58}Ni,3p|g)) 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
E$1982No07 place this level above 2655 keV level from absence of K x rays in coin with transitions from 2655-keV level. 2001Ro15 find an energy gap of 32 keV in the |g energy loops 
T$from 1982No07; same value (with no uncertainty) in 2001Ro15 
CONF$|ph{-11/2}{+3} state analogous to 27/2-, 2687 keV in {+149}Ho (2001Ro15) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
T$ from 1982No08 
J$ probable allowed |b transitions to 0+ g.s. in {+148}Dy and from 0+ g.s. in {+148}Er 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5)-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$ 250 {I100} from systematics (2011AuZY) 
T from 1989Ta11, 1988To03; others: 9.7 s {I3} (1988To03), 10 s {I2} (1981GaZS), 9 s {I1} (1979To01) 
J$ shell-model prediction (2010Ko12) with configuration= |ph{-11/2}~#|ns{-1/2}{+-1}. Parity from log| {Ift}|?5.3 to negative parity level at 2348 in {+148}Dy 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (10)+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M2
level_comment:
T$ from |g(t). Weighted average of 2.62 ms {I18} (2010Ko12) and 2.35 ms {I4} (1989Br22,1984Br07) 
J$ E3 |g to (7)-; shell-model prediction with configuration= |ph{-11/2}~#|nh{-11/2}{+-1}; also (10+) isomer in N=81 nuclides of {+142}Pm, {+146}Tb and {+150}Tm 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_comment:
J 1988To03 estimate that the sum of the total transition intensities of 142|g, 244|g, and 315|g (if they are M1+E2 ) represent |?25% of the total |b{+-} decay strength. Hence, they estimate |?75% of the |b{+-} decay strength populating the g.s. with log| {Ift}|?4.7 and assign (1+) to the g.s. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 5-
level_lifetime_unit: S
level_comment:
J$ 2010Ko12 state that 6-, as suggested in |e decay of this isomer to {+148}Dy, is not ruled out 
T$ from Adopted Levels 
$ Configuration=|ph{-11/2}~#|ns{-1/2}{+-1} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 10+
level_lifetime_unit: MS
level_comment:
$ Configuration=|ph{-11/2}~#|nh{-11/2}{+-1} 
T$ from weighted average of 2.97 ms {I49} from 108|g(t), 2.68 ms {I19} from 180|g(t), 2.58 ms {I21} from 321|g(t), and 2.60 ms {I15} from 373|g(t) (2010Ko12) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11)
level_comment:
$ If 11-, configuration=|ph{-11/2}{+3}(27/2)~#|nd{-5/2}{+-1}. 2010Ko12 list (11+) in table III, but comparison with shell-model predictions seems to suggest 11- with above configuration. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (12)
level_comment:
$ In table V, configuration=|ph{-11/2}{+3}{-27/2}~#|nd{-3/2}{+-1}, but in text on page 10, it seems that neutron hole is in d{-5/2}; possibly a misprint in table V 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_comment:
T$weighted average of 21.1 s {I2} (1993Al03), 20.5 s {I5} (1994Me13), 23 s {I4} (1982Ba75), and 21 s {I2} (1979To01) 
$Configuration=|ph{-11/2} 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$from 1994Me13. Others: 58 s {I3} (1989Me13, superseded by 1994Me13), 54 s {I5} (1988ToZW) 
$Configuration=s{-1/2} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$probable allowed |e decay from (1/2+) in {+149}Er; configuration=|ps{-1/2}~#(2+ in {+148}Dy) (1989Fi01) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_uncertain: ?
level_comment:
$1980Bo07 propose the following |g rays deexciting this isomer: 337, 436, 636, 648, 671, 777, 896. But no level scheme is proposed 
T$from |g(t) in ({+50}Ti,xn|g) (1980Bo07) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T$from |g(t) (1980Bo07). 1980Wi11 mention a nanosecond isomer above the 59-ns isomer but no data are given 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: S
level_comment:
J$E1 |g from 1+ 
T$from 1982No08. Others: 88~s {I15} (1980Li18), 90~s {I10} (1982Mo19), 78~s {I2} (1993Al03). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9)+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$X=0~{I50} from 2012Au06. 
J$log| {Ift}=4.7 to 8+ and association of this high spin isomer with the two-quasiparticle configuration=((|p h{-11/2})(|n f{-7/2}))9+ (1986Mc14). 
T$from average of 23.3~s {I3} (1990Sa32), 24.0~s {I6} (1993Al03), 26~s {I2} (1982Mo19), 24~s {I1} (1980Li18) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_comment:
$ <r{+2}>{+1/2}=5.05 fm {I3} (2004An14 evaluation) 
%|a from weighted average of 28 {I7} (1991To08), 22 {I3} (1990Po13), 22 {I3} (1982Ba75), 18 {I5} (1974Sc19), 20 {I5} (1963Ma17) 
T$|a(t) (1982Bo04). Other: 34.0 s {I5} (1993Al03) 
J$shell-model consideration and analogy to {+153}Ho. Spin=11/2 from hyperfine structure using collinear laser spectroscopy (1988NeZZ), but no details are available 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$deduced from {+151}Er |e decay (23.5 s) (1991To08) 
%A$from 1991To08. Others: 47 {I8} (1990Po13), >40 (1982Ba75), 19 {I4} (1974Sc19), 28 {I+28-14} (1963Ma17) 
T$|a(t): weighted average of 47.9 s {I13} (1982Bo04) 42 s {I4} (1963Ma17) and 47 s {I2} (1970To16) 
J$|a decay properties (1987Li09) and shell model consideration. Probable s{-1/2} proton state. Spin=1/2 from hyperfine structure using collinear laser spectroscopy (1988NeZZ), but no details are available 


level_energy_unit: KEV
level_comment:
E$the adopted level energy is the average of two values obtained from the (poorly fitted) 694.4|g and 898.0|g 


level_energy_unit: KEV
level_spin_parity: (43/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=AP
level_comment:
$Configuration=(|ph{-11/2}{+3})~#(|nf{-7/2})(|nh{-9/2}), seniority=3 
T$from |g(t) in {+127}I({+29}Si,5n|g) (1994Zh08) 


level_energy_unit: KEV
level_spin_parity: (GE 57/2)
level_lifetime_unit: NS
level_comment:
T$|g(t) in {+127}I({+29}Si,5n|g) (1994Zh08). Other: 14 ns {I3} (1981Gi12) 
J$from multiplicity=17|+2 and assumption (by 1994Zh08) that an average yrast transition removes 1.65|+0.16 units of angular momentum. J(isomer)=J(g.s.)+1.65(multiplicity)=(67/2)|+5. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$the |a group is thought to feed the low-spin {+151}Ho isomer on the basis that the 4.60-MeV |a line from the decay of the low-spin {+151}Ho isomer showed an appreciably longer half-life than 47~s due to the feeding from a parent which has approximately the same half-life. 


level_energy_unit: KEV
level_spin_parity: (GE 57/2)
level_lifetime_unit: NS
level_comment:
T$from |g(t) (1994Zh08). Other: 14~ns~{I3} (1981Gi12) 
J$from multiplicity=17+-2 and assuming that an average yrast transition removes 1.65+-0.16 units of angular momentum. J(isomer)=J(g.s.)+1.65*MULTIPLICITY=(67/2)+-5. 


level_energy_unit: KEV
level_spin_parity: (GE 57/2)
level_lifetime_unit: NS
level_comment:
J$from multiplicity=17+-2 and assuming that an average yrast transition removes 1.65+-0.16 units of angular momentum. J(isomer)=J(g.s.)+1.65(multiplicity)=(67/2)+-5. 
T$ |g(t) (1981Gi12) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: S
level_comment:
J HF(|a)=2.6 for |a decay to 2- {+148}Tb, |g from 1+ is E1 
T from 1982Bo04. Others: 135 s {I9} (1993Al03), 143 s {I13} (1989Ga11), 154 s {I5} (1982Ba75), 141 s {I7} (1963Ma17) 
%A$%|a=12~{I3} (1977Ha48) 
$AVRSQ**1/2=5.07~fm~{I4} (2004An14) 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E from 1987StZU based upon |a decay of the 9+ and 2- isomers. 
J log| {Ift}=4.6 to 8+ and 5.9 to 10+ in {+152}Dy 
T$Weighted average of 49.5~s~{I3} (1990Sa32), 50.3~s~{I3} (1989Ga11), 49.5~s~{I3} (1982Ba75,1981Ga36), 49.7~{I4} (1982Bo04), 50.0~s~{I8} (1993Al03). other: 52.3~s~{I5} (1963Ma17). The units of minutes quoted by 1993Al03 is assumed by the evaluator to be a misprint. The value of 1963Ma17 is excluded by chauvenet's criterion 
%A$weighted average of 11 {I2} (1981Ga36) and 10.5 {I30} (1979To09); others: 6.4 {I13} (1974Sc19), 19 {I5} (1963Ma17) 


level_energy_unit: KEV
level_spin_parity: 28-
level_lifetime_unit: NS
level_comment:
Proton configuration=(|p,h{-11/2}){++3}{-27/2} 
J E2 |g to 26- level 
T from 1980Ja16. Other: 49 ns {I7} (1988Pi10) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
T$On the basis of the observation that the 253|g feeding this level is stronger than the deexciting 837|g,1997Ri02 suggest that the 837+x level May be an isomer with a lifetime of roughly a few nanoseconds 


level_energy_unit: KEV
level_spin_parity: 28-
level_lifetime_unit: NS
level_comment:
Proton configuration=(|p,h{-11/2}){++3}{-27/2} 
T from 1980Ja16. Other: 49 ns {I7} (1988Pi10, assigned to a J=19, 2977 level) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E$Transitions from E=x and higher levels with E="+X" are in prompt coincidence with the 1973|g and thus feed levels above E=7072 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
T$On the basis of the observation that the 253|g feeding this level is stronger than the deexciting 837|g, 1997Ri02 suggest that the 837+x level May be an isomer with a lifetime of roughly a few nanoseconds 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MIN
level_comment:
$<r{+2}>{+1/2}=5.076 fm {I34} (2013An02,evaluation) 
%A |a branching deduced by 1974Sc19 from measured I{-Kx}, corrected for direct feeding of excited states in {+153}Dy. Value may be incorrect since I|g in 1974Sc19 do not agree with subsequent measurements. 
J From collinear spectroscopy measurements (1988NeZZ and 1989Al27); parity deduced from HF |? 0.5 for |a decay to 11/2- level. 
J Possible h{-11/2} proton state. 
T Weighted average of 2.0 m {I1} (1971To01), 2.00 m {I5} (1984Al31), 2.02 m {I3} (1993Al03) 
MOMM1$From 2014StZZ compilation and based on data of 1989Al27 (by laser resonance ionization mass spectroscopy) 
MOME2$From 2016St14 and based on data of 1989Al27 (by laser resonance ionization mass spectroscopy) 
|D<r{+2}> values (1989Al27) are: (153-165)=1.252 fm{+2} {I5}, (153-154)=0.085 {I6}, (153-155)=0.303 {I6}, and (152-153)=0.154 {I7}. The uncertainties are the statistical contributions only. Other: see plot in 1988NeZZ. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J From collinear laser spectroscopy measurements (1988NeZZ); parity deduced from HF |? 3 to 1/2+ level. Possible s{-1/2} proton state. 
%A |a branching deduced by 1974Sc19 from measured I{-Kx}, corrected for direct feeding of excited states in {+153}Dy. Value may be incorrect since I|g in 1974Sc19 do not agree subsequent measurements. Other %|a: 0.12 {I7} (1967Ha34, some of same authors as 1974Sc19), 0.3 {I2} (1963Ma17), and 0.08 {I5} (quoted in 1974Sc19 from Golovkov, 1969). 
E From |g energies in {+153}Er |e decay; other: 68 {I7} from the measured |a-decay energies for the 2.0-min and 9.3-min states and E(h{-11/2} in {+149}Tb)=36.0 {I3}. 
T From 1967Ha34; other: 9 m {I2} (1963Ma17). 
MOMM1$From 2014StZZ compilation and based on data of 1989Al27 (by laser resonance ionization mass spectroscopy) with sign from 1989Ra17 evaluation. 
|D<r{+2}> value (1989Al27) is: (153m-165)=1.271 fm{+2} {I7} compared to 1.252 {I5} for the {+153}Ho ground state. 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_comment:
J$(5/2-,7/2-,9/2-) from log| {Ift}=5.0 from (7/2-) g.s. of |e decay parent; (7/2-,9/2-) from |g to 11/2- ground state. 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_comment:
J$(5/2-,7/2-,9/2-) from log| {Ift}=5.2 from (7/2-) g.s. of |e decay parent; (7/2-,9/2-) from |g to 11/2- ground state. 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_comment:
J$(5/2-,7/2-,9/2-) from log| {Ift}=4.8 from (7/2-) g.s. of |e decay parent; (7/2-,9/2-) from |g to 11/2- ground state. Possible configuration=(|p h{-11/2})(|n h{-9/2})1+(|n f{-7/2})5/2- 


level_energy_unit: KEV
level_spin_parity: 31/2+
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M2
level_comment:
J From E2 |g to 27/2+ level and expected J progression. 
T$other value 251 ns {I+54-38} (Rf-|g(t) spectra, from 2016Pr06 in {+139}La({+20}Ne,6n|g)). 


level_energy_unit: KEV
level_spin_parity: 43/2+
level_lifetime_unit: NS
level_comment:
J From E2 |g to 39/2+ level and band assignment. 
T$unit is ps in (HI,xn|g) but subsequebtly corrected to ns by 2016Pr06 in {+139}La({+20}Ne,6n|g) 


level_energy_unit: KEV
level_spin_parity: 53/2+
level_comment:
$Level depopulated by 761|g observed only in {+139}La({+20}Ne,6n|g) and by 1042|g observed only in (HI,xn|g) 
J From E2 |g to 49/2+ level and band assignment. 


level_energy_unit: KEV
level_spin_parity: 67/2-
level_lifetime_unit: NS
level_comment:
J$From unambiguous E3 |g to 61/2+ level and and band assignment. 
T$other value: |?50 ns (2016Pr06, {+139}La({+20}Ne,6n|g)) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
|D<r{+2}>({+154}Ho-{+156}Ho)=0.334 fm{+2} {I4} (1989Al27). Others: 0.26 fm{+2} (1989OtZZ); 0.4 fm{+2} (read from graph of 1988NeZZ). 
$From an evaluation of data on nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.086~fm~{I33}. 
J From hyperfine structure (1988NeZZ and 1989Al27); |p from E1 |g from 1+ level. This value conflicts with J=1 reported from atomic-beam magnetic resonance data (1969Ek01). 
T Weighted average of 11.75 m {I20} (1993Al03) and 11.8 m {I5} (1968Wa12) from {+154}Ho |e decay. Others: 11.8 m {I10} (1967Ha34) and 12.5 m {I5} (1974PeZS) from |a decay. 
%A From 1974Sc19, who give 0.017 {I3} and 0.028 {I9}. Other: 0.042 {I24} (1968Go13). 
$E|a=3937 {I5} (from 1974Sc19 evaluation) 
MOMM1$From 2019StZV based on the measurement by 1989Al27 by Laser Resonance Ionisation Mass Spectroscopy. 
MOME2$From 2019StZV based on the measurement by 1989Al27 by Laser Resonance Ionisation Spectroscopy 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$log| {Ift} |? 4.0 from {154}Er 2- |e decay parent and E1 |g to g.s. 
J$Fed by an |e transition having a small log| {Ift} value (|? 4.0, if all the |e strength proceeds to this level), suggesting that it is a spin-flip ((|p h{-11/2})|)(|n h{-9/2})) transition. Since J{+|p}=0+ for the {+154}Er g.s., J{+|p}=1+ is indicated for this final state. 


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 LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
|D<r{+2}>(ground state-isomer)=0.015 fm{+2} (1989Al27, 1989OtZZ). 
E$x=243 {I28} (2021Ko07). 
E$x=239 {I28} calculated by evaluator from E|a({+154}Ho(8+)->{+150}Tb(9+))=3721 {I5} (1974Sc19), E|a({+154}Ho(2-)->{+150}Tb(2-))=3937 {I5} (1974Sc19), and E({+150}Tb(9+))=461 {I27} (2021Ko07). One gets fisrt the Q|s values from the corresponding E|a's, then x=Q|a(8+)+461-Q|a(2-)= 3820+461-4042=239 {I28}. 2021Ko07 got x=243 {I28} from same data except E|a({+154}Ho(2-)->{+150}Tb(2-))=3933 {I5} (1974Sc19, but not updated). Since the difference is small and relatively difficult to explain, I (N. Nica) prefer to simply quote 2021Ko07 
J$J=8 measured by 1989Al27 (using resonance ionization spectroscopy). |p=+ from allowed-unhindered (log{Ift}=4.9) |e transition to a 7+ state in {+154}Dy and no, or little, |e decay to 6+ states. 1990So04 suggest the configuration (|p 5/2[532])+(|n 11/2[505]) for this level, but F. Kondev rejected this in his review of this mass chain 
T Weighted average of 3.25 m {I10} (1968Wa12) and 2.80 m {I15} (1993Al03) from {+154}Ho |e decay and 3.0 m {I3} (1971To01) from |a decay. 
%A From {+154}Ho |a decay (3.10 m) (1974Sc19). 
$E|a=3721 {I5} (from evaluations by 1974Sc19 and 2013Ba31) 
%IT IT decay is unobserved. 
MOMM1$From 2019StZV based on the measurement by 1989Al27 by Laser Resonance Ionisation Mass Spectroscopy. 
MOME2$From 2019StZV based on the measurement by 1989Al27 by Laser Resonance Ionisation Spectroscopy 
$Configuration: |p(h{-11/2}[532]){-5/2}~#|n(h{-11/2}[505]){-11/2} (1998Ja07), rejected by F. Kondev 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (21+)
level_comment:
J$(21) from D(+Q) |g to (20+); |p=(+) from expected four quasiparticle configuration assigned by 2013Mo35 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (22+)
level_comment:
J$(22) from D(+Q) |g to (21+); |p=(+) from expected four quasiparticle configuration assigned by 2013Mo35 
T$according to 2013Mo35 based on unbalanced intensity between populating / depopulating transitions an isomer with half-life of a few hundreds of ns is expected for (22+) level 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MIN
level_comment:
J atomic beam (1969Ek01). M1 transition from 7/2+ state indicates that |p=+. Probable configuration=(|p 5/2[402]). 
T weighted average of: 48 min {I2} (1972To07), 48 min {I2} (1967Av03), 46 min {I3} (1960Da14). Other measurements: 1966La11, 1959Ka08. 
MOMM1$From the compilation 2014StZZ 
MOME2$From the compilation 2016St14 
From the measured hyperfine structure using resonance-ionization spectroscopy, 1989Al27 report |D<r{+2}>({+155}Ho-{+165}Ho)=-0.949 fm{+2} {I2}. In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.1076 fm {I326} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J M2 from 11/2- level indicates J|p=7/2+ through 15/2+. M1 to g.s. requires J|p=7/2+. 
T from 1990AbZS, 1990AbZW, {+155}Er |e decay. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J M2-M1 cascade to J=5/2, together with the T{-1/2} value of this state, indicate that J=11/2. Bandhead of h11/2-based band. The similarity of this low-energy level structure to that of the isotone {+153}Tb supports the assertion that this is in fact the 11/2- bandhead. 
T from 1979Fo11, (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J sole mode of population in in-beam studies is via an E2 transition from 13/2-; decays via an M1 transition to an 11/2- state 


level_energy_unit: KEV
level_spin_parity: 29/2(+)
level_comment:
J$D(+Q) inter band to 27/2+, bandhead of |a=+1/2, |p=(+) inferred from |p=+ of |a=-1/2 partner band 


level_energy_unit: KEV
level_spin_parity: (87/2)
level_comment:
J$(D+Q) to (81/2) 
$Non-collective oblate state with configuration= |p[(d{-5/2}((g{-7/2}){+-1}){-3/2})((h{-11/2}){+4}(16))]{-35/2+}~# |n[((i{-13/2}){+2}(12))(f{-7/2}(h{-9/2}){+4}(14)]{-26+} 


level_energy_unit: KEV
level_spin_parity: (89/2)
level_comment:
J$(M1+E2) inter band to (87/2) and in band |g to (85/2) 
$Non-collective oblate state with configuration= |p[(d{-5/2}(g{-7/2}){+-1}(5/2))((h{-11/2}){+4}(16))]{-37/2+}~# |n[((i{-13/2}){+2}(12))(f{-7/2}(h{-9/2}){+4}(14)]{-26+} 


level_energy_unit: KEV
level_spin_parity: (87/2-)
level_comment:
J$E2 to (83/2-) 
$Non-collective oblate state with configuration= |p[(d{-5/2}(g{-7/2}){+-1}(5/2))((h{-11/2}){+3}(27/2))((d{-3/2}){-3/2})] {-35/2-}~#|n[((i{-13/2}){+2}(12))(f{-7/2}(h{-9/2}){+4}(14)]{-26+} 


level_energy_unit: KEV
level_spin_parity: 39/2-
level_comment:
$B(M1)/B(E2)=0.88 {I9}. 2015Re03 list values for 37/2- band member, but the gamma-ray energies listed correspond to those from 39/2- level 


level_energy_unit: KEV
level_spin_parity: 65/2-
level_comment:
$Non-collective oblate state with configuration=|ph{-11/2}{+3}{-27/2-} ~#|n[(i{-13/2}{+2}{-12})(f{-7/2}/h{-9/2}{+4}{-7}]{-19+} 


level_energy_unit: KEV
level_spin_parity: 79/2-
level_comment:
$Non-collective oblate state with configuration=|ph{-11/2}{+3}{-27/2-} ~#|n[(i{-13/2}{+2}{-12})(f{-7/2}/h{-9/2}{+4}{-14}]{-26+} 


level_energy_unit: KEV
level_spin_parity: (87/2)
level_comment:
$Non-collective oblate state with configuration= |p[(d{-5/2}/g{-7/2}{+-1}{-3/2})(h{-11/2}{+4}{-16})]{-35/2+}~# |n[(i{-13/2}{+2}{-12})(f{-7/2}/h{-9/2}{+4}{-14}]{-26+} 


level_energy_unit: KEV
level_spin_parity: (89/2+)
level_comment:
$Non-collective oblate state with configuration= |p[(d{-5/2}/g{-7/2}{+-1}{-5/2})(h{-11/2}{+4}{-16})]{-37/2+}~# |n[(i{-13/2}{+2}{-12})(f{-7/2}/h{-9/2}{+4}{-14}]{-26+} 


level_energy_unit: KEV
level_spin_parity: 87/2-
level_comment:
$Non-collective oblate state with configuration= |p[(d{-5/2}/g{-7/2}{+-1}{-5/2})(h{-11/2}{+3}{-27/2})(d{-3/2}{-3/2})] {-35/2-}~#|n[(i{-13/2}{+2}{-12})(f{-7/2}/h{-9/2}{+4}{-14}]{-26+} 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: MIN
level_comment:
$Assuming additivity of the |m values (given by, e.g., 1989Be04) of the two quasiparticles assumed to make up this state, one finds good agreement with the measured |m value. 
J$From collinear fast beam laser spectroscopy (1988NeZZ), J=4. M3 transition from 1- gives |p=-. 
T Average of 57 min {I3} (1960Gr24), 55 min {I5} (1961Ba32), 56 min {I2} (1964Ab03), 57 min {I2} (1965Zh02), 55 min {I1} (1966La11), and 56 min {I1} (1967Av03). 
The change in charge radius, |D<r{+2}>, has been determined from isotope shifts to be |D<r{+2}>(158-156)=0.40 (1988NeZZ) and 0.39 (1989Al27) and |D<r{+2}>(156-154)=0.40 (1988NeZZ) and 0.33 (1989Al27); the values of 1988NeZZ were obtained from graphs by evaluator. Other: 1987AlZU, by the same authors as 1989Al27. 
$From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.115~fm~{I32}. 
MOMM1$From 1989Al27. The evaluation of 1989Ra17 quotes 2.99 {I3} from a private communication from the same author. The compilation by 2005St24 lists |m=2.99~{I3}. 
MOME2$From 1989Al27. The evaluation of 1989Ra17 quotes the same value from a private communication from the same author. The compilation by 2005St24 lists Q=2.3~{I2}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
%IT$Presumed to be 100%, since |e decay has not been reported. See the discussion in the {+156}Ho IT decay (9.5~s) data set. 
$The relatively large B(M3)(W.u.) value indicates that at least one, and possibly both, of the quasiparticle orbitals making up this state is the same as those in the g.s. 
J$M1 |g from 1-, M3 |g to 4-. 
T$From ce(L)(52|g,t) in {+156}Er |e decay (1995KaZS). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
J$M1+E2 |g to 1-. If a possible E2 |g deexcites this level, then J{+|p}=2- uniquely. 
T Weighted average of 1.46 ns {I15} (1975Al26) and 1.25 ns {I20} (1978Sc10) from {+156}Er |e decay studies. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
J$E1 |g to negative-parity state indicates |p=+. Feeding in |e+|b{++} decay from 0+ level gives J=1. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J$Allowed-unhindered ({Iau}) |e+|b{++} transition (log| {Ift} probably |?4.6, (see the comment in the {+156}Er |e decay data set)) from 0+, indicating the occurrence of a |p7/2[523]|)|n5/2[523] transition. 
T From Kx-35|g coincidences in {+156}Er |e decay. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 9+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M2
level_comment:
$%|e+%|b{++} is from 1999KaZV, from a study of the decay of this isomer. These authors do not list an uncertainty for this value. 
$Bandhead of a K{+|p}=9+ band. Conf=|p7/2[523]+|n11/2[505]. The evaluator has assumed that this level is associated with the YA{-p} band seen in the {+148}Nd({+14}N,6n) reaction. If so, then the parity of the levels in this band is positive. 
E$170~{I70} (2012Au07) from mass measurement 
E$From comparison with {+158}Ho, E(level) is expected to be |?0.2~MeV. From consideration of the expected log| {Ift} values for the {Iau} |b transitions in this region, 1999KaZV estimate E(level)|?350~keV. 
J$From an {Iau} |b transition to the 2787, 8+ level in {+156}Dy. This also establishes the listed conf for this state. 
T$From {+156}Ho |e Decay (7.6~min). 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (12)
level_comment:
E$From the possible decay of this level to the 185.5+y, (10-) level, z>185.5+y. The energy of this transition is not reported. Also, if the 7.6-min, 9+ level is the head of this band, then y>x. 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: (11)
level_comment:
E$From the possible decay of this level to the 185.5+y, (10-) and 171.5+y, (10-) levels, u>185.5+y. The energies of these transitions are not reported. 


level_energy_unit: KEV
level_energy_info: ;OFF=V
level_spin_parity: (22)
level_comment:
E$From the possible decay of this level to the 3496.3+y, (22-) and 3133.6+y, (21-) levels, v>3496.3+y. The energies of these transitions are not reported. 


level_energy_unit: KEV
level_energy_info: ;OFF=W
level_spin_parity: (24)
level_comment:
E$From the possible decay of this level to the 4297.2+y, (24-) and 3930.5+y, (23-) levels, w>4297.2+y. The energies of these transitions are not reported. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Probable conf=|p5/2[402]-|n3/2[521], the |S=0 coupling of two orbitals. The g.s. represents the |S=1 coupling of these two. 
T$From 1995KaZS, (ce(L)(52|g),t). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$See the discussion in the Adopted Levels, Gammas data set regarding the configuration of this level. 
T$From 1995KaZS, (ce(L)(52|g),t). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: NS
level_comment:
T Weighted average of 1.46 ns {I15} (1975Al26) and 1.25 ns {I20} (1978Sc10) from (|g+x)-30 coincidences. 1999KaZV report 1.25 ns. 
$1999KaZV report J{+|p}=2-. If the 82.18 |g is correctly placed, then the possible J{+|p} values, 0- or 1- are ruled out. In this case, little |e+|b{++} feeding of this level is expected (and observed). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
T$From Kx-35|g coincidences (2005KaZY). From Kx-35|g coincidences, 1978Sc10 report T{-1/2} = 58~ns~{I4}. 1999KaZV report 58~ns. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (12)
level_comment:
E$ y>185.5+x from possible decay of this level to 185.5+x, (10-). The energy of this transition is not reported. 


level_energy_unit: KEV
level_energy_info: ;OFF=Z
level_spin_parity: (11)
level_comment:
E$ z>185.5+x from possible decay of this level to 185.5+x, (10-) and 171.5+x, (10-). The energies of these transitions are not reported. 


level_energy_unit: KEV
level_energy_info: ;OFF=U
level_spin_parity: (22)
level_comment:
E$ u>3496.3+x from possible decay of this level to 3496.3+x, (22-) and 3133.6+x, (21-). The energies of these transitions are not reported. 


level_energy_unit: KEV
level_energy_info: ;OFF=V
level_spin_parity: (24)
level_comment:
E$ v>4297.2+x from possible decay of this level to 4297.2+x, (24-) and 3930.5+x, (23-). The energies of these transitions are not reported. 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: MIN
level_comment:
$No features of the IT decay branch are presently known. However, since such a branch exists, it is expected that the g.s. is in fact populated in the decay of the 7.6-min isomer. 
T$From the adopted values. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: 9+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
$From an allowed-unhindered ({Iau}) |b{++} transition to the 2787, 8+ level in {+156}Dy, conf=|p7/2[523]+|n11/2[505]. 
E$From consideration of the expected log| {Ift} values for the {Iau} |b transitions in this region, 1999KaZV estimate E(level)|?350~keV. 
T$Weighted average of: 7.25~min {I35} 2003KaZP; and 7.8~min {I3} 2002KaZO. Others: 7.4~min (1976IwZZ); |?6~min (1999KaZV). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
J J from atomic-beam magnetic resonance (1969Ek01) and laser spectroscopy (1988NeZZ) and |p from 7/2[523] Nilsson state assignment. The log {Ift}=4.87 gives unique Nilsson orbitals for both initial and final states. 
T From 1972To05. Others: 18 m {I+2-4} (1965Zh02) and 14 m {I1} (1966La11). 
MOMM1 Value from 1989Al27 and sign from 1989Ra17 evaluation and 2011StZZ compilation; uncertainty is the statistical contribution only. Calculated |m=3.94 for 7/2[523] state (1989Al27). 
MOME2 Value from 1989Al27 and 1989Ra17 evaluation and sign from 1989Ra17 and 2011StZZ compilation; uncertainty is statistical contribution only. 
From 1989Al27, |D<r{+2}>(157-165)=0.490 fm{+2} {I2}, and by subtraction of values therein |D<r{+2}>(157-158)=0.036 fm{+2} {I4}, |D<r{+2}>(156-157)=0.343 fm{+2} {I4}. Others: 1987AlZU, 1987AlZB and 1988NeZZ (data given in graphs). Related calculations: 1989Ba43. 
$RMS charge radius <r{+2}>{+1/2}=5.1535~fm~{I316} (2013An02) 


level_energy_unit: KEV
level_comment:
E Reported in {+157}Er |e decay, but no depopulating transitions were reported. However, several |g's reported feeding this level. 
J 3/2+,3/2[411] assigned in {+157}Er |e decay and in the review by 1990Ja11. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
E In the {+157}Er |e decay, a |g of 83 keV is placed from the 174 level, but this placement is not adopted here. 
J From (M1) |g to 5/2+ level and band structure. L=2 in ({+3}He,d) agrees, but this could include 177 level. 
T From {+157}Er |e decay. 


level_energy_unit: KEV
level_comment:
E Reported in {+157}Er |e decay, but no depopulating transitions were reported. 
J 3/2+,1/2[411] assigned in {+157}Er |e decay. 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J 5/2+,1/2[411] assigned in {+157}Er |e decay and L=2 in ({+3}He,d) suggests 3/2+ or 5/2+ and authors give (3/2)+. 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2
level_comment:
J From log{Ift}=6.6 from |e decay from 3/2- level and |g to 7/2- level; band assignment assumes 5/2+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J L=4 reported in ({+3}He,d) which implies 7/2+ or 9/2+, but assigned there as 7/2-,1/2[541] which requires L=3. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
E Level added by evaluator based on (HI,xn|g) data and {+157}Er |e decay schemes of 1979Al33, 1979DzZZ, and 1987AlZP. 
T from 1979Al33. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
T Weighted average of values measured for 121-keV |g, 0.54 ns {I5} (1979Al33) and 0.75 ns {I10} (1975Gr44). 


level_energy_unit: KEV
level_comment:
E Transitions depopulating this level have not been observed. 
J Assigned 3/2,1/2[411] with bandhead at 174 keV by 1978BrYV in {+157}Er |e decay. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: MIN
level_comment:
J J measured by atomic-beam magnetic resonance (1969Ek01) and laser spectroscopy (1988NeZZ). |p from E3 |g from 2-; |p,7/2[523] is assigned to all odd-A Ho ground states (A=157 to 169) and |n,3/2[521] to the ground states of the N=91 nuclides {+155}Gd, {+157}Dy, {+159}Er, and {+161}Yb (1990Ja11). The 2+ state resulting from the other coupling of these two states is reported at 74 keV. 
T Weighted average of 11.5 m {I5} (1962Sc10) and 10.9 m {I6} (1965St08). 
MOMM1,MOME2$Both from 1989Al27, and 2014StZZ compilation (|m), and 2016St14 evaluation (Q); measured by laser resonance ionization spectroscopy (data published in 1989Al27 as |m=3.76 {I3} and Q=4.1 {I4}) 
$Evaluated RMS charge radius: <r{+2}>{+1/2}=5.1571~fm~{I316} (2013An02) 
|D<r{+2}>({+158}Ho-{+165}Ho)=0.454 fm{+2} {I4} from table in 1989Al27, and by subtraction of entries |D<r{+2}>({+156}Ho-{+158}Ho)=0.389 fm{+2} {I5}, |D<r{+2}>({+157}Ho-{+158}Ho)=0.036 fm{+2} {I5}, and |D<r{+2}>({+158}Ho-{+160}Ho)=0.091 fm{+2} {I5}. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
%EC+%B+ From I{-|g+ce}(feeding 67 level)-I{-|g+ce}(67), assuming I{-|g}(67) was measured at equilibrium in {+158}Er |e decay. 
J J measured by atomic-beam magnetic resonance (1969Ek01) and laser spectrometry (1988NeZZ). |p from E1 |g from 2+ level. Probable configuration ((|p,7/2[404])(|n,3/2[521])) (1986So02). 
T Average of 27 m {I2} (1960Dn01) and 29 m {I2} (1962Sc10); others: |? 30 m (1961Ba32), 30 m {I5} (1961Bo24), and 27 m (1965St08). 
MOMM1,MOME2$Both from 1989Al27, and 2014StZZ compilation (|m), and 2016St14 evaluation (Q); measured by laser resonance ionization spectroscopy (data published in 1989Al27 as |m=2.43 {I3} and Q=1.62 {I17}) 
|D<r{+2}>({+158}Ho(2-)-{+158}Ho(5+))=+0.158 fm{+2} {I5} from subtraction of entries in 1989Al27. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J From M1 |g from 1+ level and missing population in |e decay from 0+ parent 
T$From {+150}Ho |e decay, 2005KaZY, with uncertainty adjusted by V.G. Kalinnikov, priv. comm., 2010 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J From log {Ift} = 4.8 for |e decay from 0+ {+158}Er used to eliminate 2+ or 3+ possibilities. 
T From {+158}Er |e+|b+ decay (1978Sc10,1977AnZG); other: 1.7 ns {I2} (1973BuZT). 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: NS
level_comment:
J From |g to 5+ level and expected presence of other pairing of Nilsson states involved in 2- level at 67 keV. Probable configuration is ((|p,7/2[404])(|n,3/2[521])) (1986So02). Other possibility is 6- discussed in in-beam study (1976Ri09). 
T From in-beam study (1976Ri09). 


level_energy_unit: KEV
level_energy_info: ;ERR=CA;ERR=?
level_spin_parity: (9+)
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M2
level_comment:
E From calculation of 1986So02. 
J From log {Ift}=4.5 for |e+|b+ decay to (8+) level in {+158}Dy (although the log {Ift} value is not very reliable its low value is compatible with this assignment) and expected presence of configuration of ((|p,7/2[523])(|n,11/2[505])). 
T From IT decay (1974Al30); others: 19.5 m (1970ScZO) and 21 m {I2} (1975Al13). 
%IT The single-particle estimate of half-life for an E4 |g to 5+ ground state is 325 min, which corresponds to 7% IT decay, so the unobserved IT decay should be less than this value. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J From |g to (5-) level and assumed band structure in {+159}Tb(|a,5n) and {+160}Dy(p,3n) (1976Ri09). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$|g's from, and to, 1+ levels respectively, and no |e feeding from 0+ {+158}Er parent; no |g feeding from upper 0+ levels makes 2+ less likely 


level_energy_unit: KEV
level_spin_parity: 0,1
level_comment:
J Conflict on parity since have E1 |g to 1+ level and M1,E2 |g to 0+, 1+, 2+ level. Spin determined from log {Ift}=5.7 from 0+ {+158}Er. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
%EC+%B+ From I{-|g+ce}(feeding 67 level)-I{-|g+ce}(67), assuming I{-|g}(67) was measured at equilibrium in {+158}Er |e decay. 
T From {+158}Ho Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
E level proposed by 1996Go06. 
T$From 2005KaZY, with uncertainty adjusted by V.G. Kalinnikov, priv. comm., 2010; same value as in {+158}Ho Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
T$From X{-K}-ce delayed coincidence (1978Sc10, 1977AnZG), same value as in {+158}Ho Adopted Levels; other: 1.7 {I2} (1973BuZT). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-)
level_lifetime_unit: NS
level_comment:
J Authors' assignment, but they note that in some other even-mass Ho isotopes the isomeric state is 6-. 
T from {+158}Ho Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=CA;ERR=?
level_spin_parity: 9+
level_lifetime_unit: MIN
level_comment:
E From calculations of 1986So02 for |e decay of this level; however, 1999Lu03 did not observe |g's linking this band to other levels. 
T from {+158}Ho Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: NS
level_comment:
J Authors' assignment, but they note that in some other even-mass Ho isotopes the isomer is 6-. 
T The observed half-life could be associated with this level or one slightly above it which decays via an unobserved low-energy transition. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
J$J measured by atomic-beam magnetic resonance (1969Ek01) and laser spectroscopy (1970LiZY,1988NeZZ,1989Al27). |p=- from the {Iau} |e+|b{++} decay (log {Ift}=4.8) to the 5/2- level at 309~keV in {+159}Dy. This {Iau} |e transition establishes the J{+|p} values and configurations of both levels involved. The conf assignment of this level is also supported by the |m value: the alternate Nilsson-assignment, |p7/2[404], would give |m of about +2.0. 
T$From 1982Vy02; others: 33~min {I3} (1958To32), 35~min {I5} (1964Ma10), and 33~min {I1} (1966La11). All values are from the {+159}Ho |e decay. 1958To32 measured activity with Geiger counter and others measured |g(t) with NaI(Tl), Si, or Ge detector. 
MOMM1$From 1989Ra17 evaluation, and based on an earlier report by the authors of 1989Al27 (where value is 4.27 {I3}). See, also, the compilation by 2005St24. 
MOME2$From 1989Ra17 evaluation, and based on an earlier report by the authors of 1989Al27 (where the same value is given). See, also, the compilation by 2005St24. 
E$|D<r{+2}> results are given by 1987AlZU and 1988NeZZ only in plots. From a table of 1989Al27, |d<r{+2}>({+159}Ho-{+165}Ho)=0.350~fm{+2} {I2}. Deduced by evaluator from table of 1989Al27, |d<r{+2}>({+157}Ho-{+159}Ho)=0.140 {I3}, |d<r{+2}>({+158}Ho-{+159}Ho)=0.104 {I5}, |d<r{+2}>({+159}Ho-{+160}Ho)=0.013 {I3}, and |d<r{+2}>({+159}Ho-{+161}Ho)=0.110 {I3}, all in fm{+2}. 
$From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.168~fm {I31}. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
J$From E1 |g to 7/2- level, L=4 in ({+3}He,d), and expected occurrence of the |p7/2[404] Nilsson orbital in this region. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$From E3 |g to 7/2- level, and expected occurrence of the |p1/2[411] Nilsson state in this region. 
T$From 1971Ge01, other: 6.9~s {I3} (1966Bo02); both from {+159}Ho IT decay. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$From assignment as the 3/2+ member of the |p1/2[411] band, with the bandhead at 205~keV. L=(2) in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$From E1 |g to 7/2- level and L=2 in ({+3}He,d) and (p,|a). 
J$Calculated configuration (1973Ga29) gives 56% |p5/2[402] and 28% |p5/2[413]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2+)
level_comment:
J$From cross-section patterns in (p,|a), where it is assigned as the 7/2,|p5/2[402] state. However, here this conf is assigned to the 381.7 level. 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$From |g to 5/2+ level and band assignment. In the (p,|a) study, the 7/2,5/2[402] state is assigned to the 364 level. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$From E1 |g to 3/2+ level, |g to 1/2+, L=1 in ({+3}He,d), and intensity pattern for those levels assigned to the |p1/2[541] band in ({+3}He,d). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+,9/2+
level_comment:
J$From L=4 in (p,|a) (1982Ha17). Other: L=2,3 in ({+3}He,d) and in (|a,t) (1977Pa23). Band assignment, from (p,|a), implies 7/2+. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$From E1 |g to 1/2+ level, L=1 in ({+3}He,d), and intensity pattern for those levels assigned to the |p1/2[541] band in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
E$From {+152}Sm({+11}B,4n|g). Other: 595.4, from (|a,4n|g),({+3}He,3n|g) 
J$From |g to 7/2+ level and proposed band structure. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2-)
level_comment:
J$Assigned (3/2+,5/2+) from L=2 in ({+3}He,d) and (5/2-,7/2-) from L=(3) in (p,|a). Band assignment, from (p,|a), requires 7/2-. 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_comment:
J$From |g's to 11/2+ and 13/2- levels. The 775 level has also been proposed as the 15/2,|p7/2[404] level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
J$From L=5 in ({+3}He,d), J{+|p}=9/2-,11/2-. Population in the single-nucleon-transfer experiments indicates 11/2-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-,3/2)
level_comment:
J$From L=1 in ({+3}He,d), J{+|p}=1/2-,3/2-. Tentatively assigned (1982Ha17) as the 3/2+ member of the |p1/2[420] band. Level may be a doublet. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$From M1 |g to 7/2+ level, possible |g to (3/2-), and log {Ift}=7.2 from the {+159}Er g.s. (J{+|p}=3/2-). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$See the comment on this level in the (|a,4n|g),({+3}He,3n|g) data set. 
J$|g to 17/2-. Proposed as (17/2+) in (|a,4n|g),({+3}He,3n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_comment:
J$From M1(+E2) |g to 5/2- level and log {Ift}=6.6 from the {+159}Er g.s. (J{+|p}=3/2-). 
J$Assigned as the |p3/2[541] bandhead by 1990Na14. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$From M1 |g to 7/2+ level, log {Ift}=6.6 from the {+159}Er g.s. (J{+|p}=3/2-), and L|<2 in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$Level proposed by 1977Bo26 as 3/2+ member of the |p1/2[411] band, with the bandhead at 205~keV. Level populated by several |g's, but no depopulating |g's are observed. 1977HaYT place the 3/2+ level at 211.4~keV, with a 211.4 |g to the g.s. This requires the 211.4 |g to be E3, but the data of 1977Bo26 and 1979Ad08 imply a |g of this energy is E1 and this |g is placed from the 424 level. 


level_energy_unit: KEV
level_comment:
J$1977Bo26 suggest this is the 9/2+ member of the |p7/2[404] band. This is supported by the data from the heavy-ion study of 2000Ma06. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_uncertain: ?
level_comment:
E$1977Bo26 report this level, but have no |g's depopulating it. From the (|a,t) and ({+3}He,d) studies, 1977Pa23 report 5/2- at 464~keV. From data of 1977Bo26, it is not clear whether level is populated in this decay. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
L$The angular-distribution graphs (fig. 6) of 1977Pa23 indicate a level at 539~keV, which evaluator assumes is actually this level (589~keV). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+,5/2+
level_comment:
J$Assigned as (5/2-,7/2-) from L=(3) in (p,|a). (7/2-) is adopted, based on band and conf assignment. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
J$L=5 indicates 9/2-,11/2-. Band assignment and population in this reaction give preference to 11/2-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
S$Value is larger than expected for 5/2[402] Nilsson state. This may reflect contributions from the L=2 members of the |p3/2[411] and/or 1/2[411] bands. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
L$The angular-distribution graphs (fig. 6) of 1977Pa23 indicate a level at 539~keV, which evaluator assumes is actually this level (590~keV). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_comment:
J$L=5 indicates 9/2-,11/2-. Band assignment and population in this reaction gives preference to 11/2-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2+)
level_comment:
E,J$This level not given in the {+152}Sm({+11}B,4n|g) study of 2000Ma06; and the 15/2+ member of this band is assigned in that study to a level at 819~keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2+)
level_comment:
E,J$This level is not given in the {+152}Sm({+11}B,4n|g) study of 2000Ma06 and would be the only signature=+1/2 member of the |p1/2[411] band thus far reported in this nucleus in the high-spin studies. The evaluator regards it, or at least its assignment, as questionable. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Nuclear-structure factor=0.04. 
L$Measured angular distributions do not agree with DWBA calculations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
$Nuclear-structure factor=0.10. 
L$Measured angular distributions do not agree with DWBA calculations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+,9/2+
level_comment:
$Nuclear-structure factor=0.67. Value deduced for 7/2+. 9/2+ band member is assigned to level at 630~keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-,7/2-)
level_comment:
$Nuclear-structure factor=0.19. Value deduced for 7/2. 
L$Measured angular distributions do not agree with DWBA calculations. 
J$Assigned (3/2+,5/2+), from L=2 in ({+3}He,d). Assigned as the 7/2- band member in (p,|a). (7/2-) is given in the adopted values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$Nuclear-structure factor=(0.27). Value assumes band and spin assignments are correct. 
J$Tentative band assignment. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+,5/2+)
level_comment:
$Nuclear-structure factor=(0.23). Value assumes band and 5/2 spin assignments are correct. 
J$Tentative band assignment. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: MIN
level_comment:
J atomic beam (1969Ek01,1970LiZL) and collinear fast-beam LASER spectroscopy (1988NeZZ). |p=+, from log| {Ift}=4.69 for the |e+|b{++} transition to the 4+, 1694 level in {+160}Dy. This small log| {Ift} value indicates that this transition is allowed unhindered and, hence, that the odd proton in {+160}Ho occupies the 7/2[523] Nilsson state. The odd neutron is assigned the configuration=3/2[521], since the N=93 nuclides {+155}Sm, {+157}Gd, {+159}Dy and {+161}Er all have this configuration in their ground states (1971Bu16). The K=5 coupling of these two orbitals is expected to lie below that with K=2. 
T from |g(t) (1965St08). Other measurements: 22.5 min {I5} (1950Wi13), 22 min (1954Ha19), 28 min {I3} (1958To32), 25 min {I1} (1966La11), 26 min (1969Ek01). 
MOMM1$from 2014StZZ compilation (originally from 1989Al27, using laser resonance ionization mass spectroscopy, relative to {+165}Ho) 
MOME2$from 2016St14 compilation (originally from 1989Al27, using laser resonance ionization mass spectroscopy, relative to {+165}Ho) 
|D<r{+2}>({+160}Ho-{+165}Ho)=-0.363 fm{+2} {I2}, from measured hyperfine structure and isotope shift using resonance ionization spectroscopy (1989Al27). In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.17 fm {I3}. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
%EC+%B+,%IT$weighted average of %IT values (measured by almost the same group of authors by varied methods): 73.6 {I52} (2002Ad34), 73.3 {I30} (2003KaZR), 77.9 {I20} (2006KaZX) (the smallest measured unc was adopted); other: 65 {I3} (1974Al28). 
J collinear fast-beam LASER spectroscopy (1988NeZZ), atomic beam (1969Ek01), E3 transition to g.s. 
T from |g(t) (1965St08). Other measurements: 5.0 h (1969Ek01), 4.6 h {I3} (1966La11), 5.0 h {I2} (1963Ra15), 4.76 h {I10} (1960Gr15), 5.3 h {I2} (1957Dz60), 5.6 h {I7} (1957Dz58), 5.0 h (1955Ne03). 
MOMM1$from 2014StZZ compilation (originally from 1989Al27, using laser resonance ionization mass spectroscopy, relative to {+165}Ho) 
MOME2$from 2016St14 compilation (originally from 1989Al27, using laser resonance ionization mass spectroscopy, relative to {+165}Ho) 
from the hyperfine structure and isotope shifts measured using resonance ionization spectroscopy, 1989Al27 report that the difference between the mean square charge radii of this state and the {+165}Ho g.s. is -0.446 fm{+2} {I5}. 1995Ga38 report -0.083 fm{+2} {I7} for the difference between the mean-square charge radii of this state and the {+160}Ho g.s. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
J log| {Ift}=4.73 of the |e transition from the {+160}Er g.s. (J|p=0+) requires J|p=1+ and also establishes the two-nucleon configuration (|p 7/2[523] - |n 5/2[523]) as being at least a major component of this level. 
T$from 2006KaZX ({+160}Er |e decay) by measuring the retarded KX(Ho)-|g coincidences with respect to the time decrease in the 7.1|g intensity. Other: 30 ns {I8} (2005KaZY, obtained by the same group) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: NS
level_comment:
J E1 transitions to 5+ (g.s.) and 6+ states establish |p=- and J=5 or 6. Calculations (1996Dr03) of bandhead energies of the low-lying two-nucleon configurations indicate that the lowest such negative-parity bands expected are those from the K|p=6- and 1- couplings of the orbitals |p 7/2[523] and |n 5/2[642], with 6- lying below 1-. The lowest expected K|p=5- band is expected higher in the level scheme. The hindrance factor of the E1 transition to the g.s. is consistent with that observed for E1 transitions between the same two (neutron) orbitals in several neighboring odd-A nuclides (1996Dr03), supporting the proposed configuration assignment and, hence, the J|p value. 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
J M1 to 6- level indicates |p=-. Energy consistent with that expected for the 7- member of the proposed band. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (9+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
E x<55, from absence of K| x ray associated with the deexciting |g. 2004Es01 report the level energy as 176 keV, but give no basis for it. 
J 1988Bh05 give J>7, based on absence of direct |g to 118 level. Of the bandheads having K(=J) larger than 7, only two (having K|p=9- and 9+) are expected at low energies. The configuration having 9+ agrees better with the information on this band than does that having 9-, as discussed by 1996Dr03. 
T$measured by 2005KaZX ({+160}Ho IT decay (3.2 s)) by the decrease of the 118|g 


level_energy_unit: KEV
level_spin_parity: (1-)
level_uncertain: ?
level_comment:
E,J$level introduced by 2010VaZZ ({+160}Er |e decay) based on |g assumed to decay to 67, 1+ level with J|p value postulated by authors; because of the lack of evidence this level is questionable 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J M1+E2 |g to 6+ level indicates |p=+. Energy consistent with that expected for the 7+ member of the proposed band. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
%EC+%B+,%IT$weighted average of %IT values (measured by almost the same group of authors by varied methods): 73.6 {I52} (2002Ad34), 73.3 {I30} (2003KaZR), 77.9 {I20} (2006KaZX) (the smallest measured unc was adopted); other: 65 {I3} (1974Al28). 
T,J from the adopted values 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
%EC+%B+,%IT$weighted average of %IT values (measured by almost the same group of authors by varied methods): 73.6 {I52} (2002Ad34), 73.3 {I30} (2003KaZR), 77.9 {I20} (2006KaZX) (the smallest measured unc was adopted); other: 65 {I3} (1974Al28). 
$Since this level has %|e+%|b{++}=23.8 {I20}, there is an imbalance in the listed intensities into and out of it. Further, this level has T{-1/2}=5.02 h, with the result that the intensity of the radiations deexciting it will exhibit a time dependence relative to that of the feeding transition. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
T$from 2006KaZX by measuring the retarded KX(Ho)-|g coincidences with respect to the time decrease in the 7.1|g intensity. Other: 30 ns {I8} (2005KaZY, obtained by the same group) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_uncertain: ?
level_comment:
E,J$level introduced by 2010VaZZ based on |g assumed to decay to 67, 1+ level with J|p value postulated by authors; because of the lack of evidence this level is questionable 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (9+)
level_lifetime_unit: S
level_lifetime_info: ;ERR=AP;ISO=M2
level_comment:
E,T$2004Es01 report the energy of this level as 176 keV, but give no basis for it. Also the T{-1/2} value is given with no detail 


level_energy_unit: KEV
level_spin_parity: 10+
level_comment:
E value rounded off, and uncertainty increased, to reflect the poor energy fit (several standard deviations) of the two |g's deexciting this level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (22+)
level_uncertain: ?
level_comment:
E value based on this placement (from 2004Es01) of the 601 |g. These authors point out that the order of the 601 and 609 |g's may be interchanged, in which case the energy of this level will be 8 keV higher. 2003LuZY place a 696.5 |g from the (22+) member of this band. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (24+)
level_comment:
2004Es01 state that the ordering of the 601 and 609 |g's may may be interchanged. This will not affect the energy of this level, but it will affect the energy of the |g transition deexciting it. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (28-)
level_uncertain: ?
level_comment:
From 2004Es01. Previous studies do not report this level. Note: if the E|g value deexciting the 26- level is that of 2004Es01 rather than that of 2003LuZY (which is adopted here), then the energy of this level will have to be increased accordingly. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (6-)
level_comment:
1996Dr03 state that a 112.06 |g involving no parity change deexcites this level. But, other than having negative parity, which of the established levels is the final state is not known. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (17-)
level_comment:
E from the evaluator's placement of the listed deexciting |g's. 2004Es01 show only a 660 |g from a (17-) level. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (18-)
level_comment:
E from the evaluator's placement of the listed deexciting |g. 2004Es01 do not report levels in this band above a (17-) level. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (20-)
level_comment:
E from the evaluator's placement of the listed deexciting |g's. 2004Es01 do not report levels in this band above a (17-) level. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_spin_parity: (22-)
level_comment:
E from the evaluator's placement of the listed deexciting |g's. 2004Es01 do not report levels in this band above the (17-) level. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (9+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M2
level_comment:
E x<55, from absence of K| x ray associated with deexciting |g 
T$measured by 2005KaZX by the decrease of the 118|g 
J adopted value. 1988Bh05 give J>7, based on the absence of a direct |g to the 118 level. However, this lower limit seems overly conservative in view of the quite small transition probabilities that would be implied for the isomeric transition if its mult were E2 or less. Based on this observation, J|p would be expected to be 9+ (but not 9-) or larger. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: H
level_comment:
J J measured by atomic-beam magnetic resonance (1964Bu09 and 1969Ek01) and laser spectroscopy (1987AlZO,1988NeZZ). Log{Ift}=4.88 to 5/2- level indicates an allowed-unhindered |e transition, which in this mass region is |p7/2[523]|)|n5/2[523]. This thus establishes 7/2[523] as the configuration of the {+161}Ho g.s. 
T weighted average of 2.48 h {I5} (1965Ab04), 2.5 h {I2} (1963Ra15), 1.9 h {I5} (1961Bj02), and 3.0 h {I5} (1961Ba32). Others: 4.6 h {I1} (1950Wi13) and 2.5 h (1954Ha01). 
MOMM1 from the compilation of 2005St24 and based on a measurement of 1989Al27. 
MOME2 from the compilation of 2005St24 and based on a measurement of 1989Al27. 
|d<r{+2}>(161-162)=0.033 fm{+2} 7 and |d<r{+2}>(160-161)=0.123 fm{+2} 3, from 1989Al27; values computed by evaluator by subtraction of table entries. Uncertainties are computed by error propagation and may be overestimates. Other: plot in 1987AlZU by same authors. 
From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.179 fm 31. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J from E3 |g to 7/2- and expected occurrence of this Nilsson orbital in this energy region. 
T weighted average of 6.80 s {I10} (1965St08) and 6.73 s {I10} (1971Ge01). Others: 6.1 s {I3} (1966Bo02) and 6.78 s {I15} (1967Ge09 by the same authors as 1971Ge01) (all from {+161}Ho IT decay) . 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J from L=4 in ({+3}He,d), analysis of (pol t,|a) data, and E1 |g's to 7/2- and 9/2-. 
T from |g|g(t) in (p,n|g) study (1976Sc19). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J from E1 |g to 1/2+ level, L=1 in ({+3}He,d) and band structure. 
J from model calcuations of 1992Bo45, this state is 30% 1/2[541], 18% {I1}/2[550], 25% quadrupole vibration, and 14% octupole vibration. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J from L=(2) in ({+3}He,d), E1 |g to 7/2- level, and band structure. 
J from model calcuations of 1992Bo45, this state is 82% 5/2[402], 5% quadrupole vibration, and 5% octupole vibration. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J from L=(5) in ({+3}He,d), analysis of (pol t,|a) data, and D |g to 7/2+ level. 
T From (p,n|g) study (1976Sc19). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J from E2 |g to 7/2- level and E1 |g to 3/2+. 
J from model calcuations of 1992Bo45, this state is 36% 3/2[541], 49% quadrupole vibration, and 9% octupole vibration. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
J from E2,M1 |g to 3/2+ level, |g's to 1/2+ and 5/2-. The placement of the 1352|g to 1/2- is only by 1972Wo08; if this is correct, J|p is not 5/2+. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$no assignment in 1972Ka37. Note that the |g multipolarities (1979DzZZ) suggest inconsistent parities (i.e., M1 to 3/2- and M1 to 3/2+). 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_comment:
E 2004Es01, in {+160}Gd({+7}Li,6n|g), report a different |g decay pattern from that given here and place the 25/2+ band member elsewhere in the level scheme. 


level_energy_unit: KEV
level_spin_parity: 29/2-
level_comment:
E 2004Es01, in {+160}Gd({+7}Li,6n|g), report a different |g decay pattern from that given here and place the 29/2- band member elsewhere in the level scheme. 


level_energy_unit: KEV
level_spin_parity: (27/2+)
level_comment:
E 2004Es01, in {+160}Gd({+7}Li,6n|g), report a different |g decay pattern from that given here and place the 27/2+ band member elsewhere in the level scheme. 


level_energy_unit: KEV
level_spin_parity: 31/2-
level_comment:
E 2004Es01, in {+160}Gd({+7}Li,6n|g), report a |g-decay pattern different from that given here. The data for this level and for the higher-spin levels in this band that are included in the adopted values are those from the study of 2004Es01. 


level_energy_unit: KEV
level_comment:
$d|s/d|W(|mb/sr)=90 
J this level and the 211 levels are assigned as the 11/2-,7/2[523], 1/2+,1/2[411], and 3/2+,1/2[411] states. 
L value applies to 212 and 222 levels. 
Cross-section value includes 211, 221, and 222 levels. 


level_energy_unit: KEV
level_comment:
$d|s/d|W(|mb/sr)=44 
S=0.41 
J assigned as a doublet, 5/2-,1/2[541] and 7/2+,3/2[411]. 
S value is for the 459,463 doublet. 


level_energy_unit: KEV
level_comment:
$d|s/d|W=230 
J assigned as triplet composed of: 11/2-,7/2[523]; 1/2+,1/2[411]; and 3/2+,1/2[411]. 
S value includes 211, 221, and 222 levels. 
From analysis of cross-section and analyzing-power data, 1981Bu03 deduce S=1.40 {I10} and S=0.15 {I5}, respectively, for the 11/2- and 3/2+ levels. 


level_energy_unit: KEV
level_comment:
$d|s/d|W=47 
J assigned as doublet composed of 5/2+,5/2[402] and 7/2+,3/2[411]. 
If all the cross section is due to the 7/2+ level, S=0.36. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$d|s/d|W=20 
J assigned as doublet composed of 9/2+,5/2[413] and 9/2-,5/2[532]. 
If all the cross section is due to the 9/2+ level, S|?0.13. If it is due to 9/2-, S|?0.19 (1981Bu03). 


level_energy_unit: KEV
level_comment:
$d|s/d|W=94 
J assigned as doublet composed of 3/2+,1/2[420] and 5/2+,1/2[420]. 46 
If all the cross section is due to the 5/2+ level, S=0.32. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$d|s/d|W=22 
J The observed peak also contains contributions from the 1/2+ and 3/2+ levels of the 1/2[411] band, which are at 211 and 222 keV in the Adopted Levels. 
Cross-section includes 211, 221, and 222 levels. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J J from atomic-beam magnetic resonance measurement (1969Ek01,1988NeZZ) and |p from allowed |e decay (log| {Ift}=5.0 and 4.9, respectively) to the 0+ g.s. and the first 2+ level in {+162}Dy. Configuration=(|p 7/2[523])-(|n 5/2[523]) from expected Nilsson states for the odd particles and supported by calculated (1988Ra41) |m=2.60 and Q=0.65. 
T average of 15.0 min {I10} (1965St08) and 15 min {I1} (1973Ba21). Others: 11.8 min {I10} (1961Jo10), 12 min {I2} (1969Ak01), and 15 min (1969Ek01). 
MOMM1 from 1988NeZW as quoted in 1988Ra41. 
MOME2 from 1988NeZW as quoted in 1988Ra41. 
For {+162}Ho-{+160}Ho, |D<r{+2}>|?0.20 fm{+2} (taken from plot of 1989Al27 by evaluator). 
In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.182 fm {I31}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
J from M1 |g to 1+ level and expected structure of 1+ band. 
T from 1978Sc10 by |g-ce coincidences following {+162}Ho IT decay (67 min): also 1977AnZG by same authors. 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E from {+162}Ho IT decay 
J J from atomic-beam magnetic resonance measurement (1969Ek01) and |p from allowed |e decay (log| {Ift}=4.77) to 5- level in {+162}Dy. Configuration=(|p 7/2[523])+(|n 5/2[642]) with an admixture of configuration=(|p 7/2[523])+(|n 3/2[651]) from expected Nilsson states for the odd particles and supported by calculated |m=3.3 (1988Ra41). 
T weighted average of 68 min {I2} (1964Ma10), 65 min {I5} (1965GrZZ), 67 min {I2} (1969Ak01), 66 min {I3} (1969Ho17), 63.5 min {I19} (1971Wo09), and 68 min {I1} (1973Ba21). Others: 1957Mi67, 68 min (1961Jo10), 65 min {I5} (1965GrZZ), 68 min (1969Ek01), and 72 min (1973St22). 
%EC+%B+,%IT$from evaluator's analysis based on Ice(L)(38.34)/Ice(K)(184.99) ratio measured by 1961Jo10, with 38.34|g in {+162}Ho IT decay (67 min) scheme and 184.99|g in {+162}Ho |e decay (67.0 min) scheme, giving %IT=63 and %|e=37. See {+162}Ho IT decay (67.0 min) dataset for details 
MOMM1 from the compilation by 2014StZZ and based on the measurement of 1989Al27, where the value is 3.59 {I4}: other: 3.60 {I9} from 1988NeZW, 1988Ra41. 
MOME2 from the compilation by 2016St14 and based on the measurement of 1989Al27; others: 1988NeZW, 1988Ra41. 
For the 6- isomer (67 min), 1989Al27 give for {+162}Ho-{+160}Ho, |D<r{+2}>=0.156 fm{+2} {I7} and for {+165}Ho-{+162}Ho, |D<r{+2}>=0.207 fm{+2} {I7}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: NS
level_comment:
E the 179 |g has been placed from a level at 179 keV as suggested by 1978Sc10, rather than from a level at 286 keV with J|p=5+ as given by 1972WaYO and others. 
J J|p and configuration proposed by 1978Sc10; this would be the other coupling of the two orbitals in the 6-, 106 state. 
T from |g|g(t) in {+162}Dy(p,n|g) (1978Sc10). Other: 9 ns (1973GoYV). 
T the same datum, 8.7 NS 2, is given by 1973AnYZ and 1973ScXL. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_lifetime_unit: NS
level_comment:
E level energy is based on placement of the 179.9|g to the g.s., as proposed by 1978Sc10, rather than from a 5+ level at 286 keV to the 106 level as proposed by 1972WaYO, 1973AnYZ, and 1973ScXL. 
T from 1978Sc10, |g|g coin.; other: 9 ns (1973GoYV). 
T the same datum, 8.7 NS 2, is given in 1973AnYZ and 1973ScXL. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: Y
level_comment:
T${+163}Ho{+66+} ion is stable (1997Kl06,1992Ju01) 
$|D<r{+2}>({+163}Ho-{+165}Ho)=-0.117 fm{+2} {I6} (1989Al27) 
From an evaluation of nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.19 fm 3. 
E$population is uncertain in ({+3}He,d) 
J,MOMM1,MOME2$resonance ionization spectroscopy (1989Al27). Spin also from hyperfine collinear laser spectroscopy (1988NeZZ). Parity: L(p,t)=0 from 7/2- target 
T$from 1983Ba32 (uncertainty=50 y at 95% confidence level; isotope-dilution mass spectrometry; four points; 0.35-0.6 y). Others: 4569 y {I30} (1988Ka20, isotope-dilution mass spectrometry); 7000 y {I200} (1982An19, based on a partial T{-1/2}=4.0|*10{+4} y {I12} for M-capture Auger electrons and M x ray) and Q(|e)=2.3 {I10} (from {+163}Dy(d,t), {+162}Dy({+3}He,d)); 33 y {I23} (1968Ho17); >1000 y (1960Na10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T see the comment in the heavy-ion data set. 
J value deduced from the configuration assignment by 2004Ho19 (in {+160}Gd({+11}B,|a4n|g)), assuming that this situation is similar to that in the isotone, {+165}Tm. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
From comparison with the neighboring Ho isotopes, possible member of the K-2 |g vibrational-band built on the g.s. (|p7/2[523]). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|p5/2[413] bandhead(?). This level deexcites to |p7/2[404] and |p1/2[411] in a manner similar to that of the |p5/2[413] bandhead in {+165}Ho. 


level_energy_unit: KEV
level_spin_parity: (7/2+&5/2+)
level_comment:
E$triplet of levels: dominant component is expected to be the |p7/2[404] bandhead. Other components are: 7/2,1/2[411] and 5/2,3/2[411] 


level_energy_unit: KEV
level_comment:
E$strong 1371 (L=3) reported in 1974Le27 is probably a different group from 1371 in 1977Pa23 due to an energy discrepancy of |?25 keV (higher value in 1974Le27) between the two studies near this excitation energy (see comments for 1328 and 1435 levels) 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_comment:
E$1465 (1974Le27) 
S$0.98 (1974Le27) 
L$from |s(|q) (1974Le27) and |s({+3}He,d)/|s(|a,t) (1977Pa23) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$Predicted S=0.05. Large discrepancy between experimental and predicted value is unexplained (1981Bu03) 


level_energy_unit: KEV
level_spin_parity: 7/2+&5/2+
level_comment:
$7/2+,1/2[411] may be obscured by this doublet 
S$from simultaneous analysis of |s(|q) and A(|q) at each angle. |DS(7/2+)=0.05, |DS(5/2+)=0.10 estimated from the scatter in values at each angle 
$Predicted S=0.29 for 7/2+, 0.38 for 5/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 7/2+(&15/2-)
level_comment:
J$Ay(|q) small when compared to DWBA; consistent with results for Ay(|q) of 7/2+,3/2[411] for (pol t,|a) in neighboring nuclides 
$Predicted S=0.22 for 7/2+ 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J,L$|s(|q) not consistent with DWBA but similar behavior has been observed in other cases for the |p1/2[420] band. Ay(|q) is small, as predicted and observed in other cases 
$Predicted S=0.16 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M1
level_comment:
T$ from 974|g(t) (2012Sw01), |g observed in 156-ns pulse width 
$ Possible configuration=|p7/2[523]~#|n5/2[523]~#|n5/2[642] if J|p(1506 level)=17/2+. Less likely configurations=|p7/2[404]~#|n5/2[523]~#|n5/2[642] and |p7/2[523]~#|p7/2[404]~#|p3/2[411] J|p(1506 level)=17/2+ 
$ Magnitude of experimental g{-K}-g{-R}=0.22 {I+4-3} from rotational model formula using Q{-0}=6.4 eb. Theoretical values are 0.41 {I5} for first configuration for 17/2+, 0.13 {I5} and 0.84 {I5} for the second and third configurations for 17/2-. 


level_energy_unit: KEV
level_spin_parity: (23/2+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$ from 974|g(t) (2012Sw01) 
$ Possible configuration=|p7/2[523]~#|n5/2[642]~#|n11/2[505] if J|p(2109 level)=23/2+. Less likely configuration=|p7/2[523]~#|n5/2[523]~#|n11/2[505] if J|p(2109 level)=23/2- 
$ Magnitude of experimental g{-K}-g{-R} |< 0.037 from rotational model formula using Q{-0}=6.4 eb. Theoretical values are 0.02 {I5} for first configuration for 23/2+, 0.11 {I5} for the second configuration for 23/2-. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J$spin from atomic beam (1969Ek01,1970LiZY); parity from log| {Ift}=4.6 to 0+; 1+ also supported in (d,t) 
T$from weighted average of 28.1 min {I10} (1972Dr04), 29.0 min {I5} (1972Ka19), and 29 min {I2} (1966Jo07). Others: 23.9 min {I5} (1966Se07), 46 min (1964Bo41), 33.6 min {I10} (1961We02), 38.5 min (1961Kh06), 36.7 min {I5} (1954Br96), 41 min (1954Ha19), 41.5 min (1950Wa12, earlier value of 38.6 min in 1948Wa13), 34.0 {I5} (1950Wi13), 47 min (1938Po05). In the studies prior to 1966, the g.s. and isomeric activities were not isolated. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$(45.79|g)E3 - (56.64|g)M1+E2 - (37.34|g)M1+E2 |g cascade from J=6 level at 139.78 to J=1+ g.s. establishes negative parity for 139.78 level, 3+ for 93.99 level, and 2+ for 27.34 level. 2+ also supported in (d,t) 
T$|g|g(t) (1965Hu02). 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$spin from atomic beam (1969Ek01,1970LiZY), parity from E3 |g to 3+. See J|p comment for 37.34 level. 6- also supported in (d,t) 
T$weighted average of 36.4 min {I3} (2008Ha21), 36.7 min {I10} (1972Dr04), and 37.3 min {I5} (1972Ka19). Others: 41 min {I1} (1971Pa02), 42.4 min {I3} (1968Bo25), 37.5 min {I+15-5} (1966Jo07), 39.0 min {I5} (1966Se07). Possibility of an isomeric activity was first proposed by 1954Br96, but separate half-lives of the ground state and the isomer were first measured by 1966Jo07 and 1966Se07 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E,J$note that in (d,t), a 367 keV {I4} level was tentatively assigned as (9-) member of K|p=6- band. Based simply on the energy agreement, the 367 level in (d,t) is considered the same as 370 level in ({+11}B,|a3n|g) 


level_energy_unit: KEV
level_comment:
$1970Jo11 suggest possible J=3 from K|p=3+, |p7/2[523]|^-|n1/2[521]|_, but the authors note that a state with a similar configuration is proposed at 188.6 in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (9-)
level_comment:
$d|s/d|W=13 
J$assignment by 1970Jo11 is tentative as the peak at 367 keV is weak and unresolved from a stronger peak at 343 keV. Note that 9- member of the K|p=6- band is assigned to a 407-keV level in the heavy-ion |g-ray work by 2004Ho19 


level_energy_unit: KEV
level_comment:
$d|s/d|W=51 
$Possible J=3 from K|p=3+, |p7/2[523]|^-|n1/2[521]|_, but a state with a similar configuration is proposed at 188.6 in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$ The 73.4 and 91.4 keV |g rays are seen by 2008Ha21 from the decay of {+164}Ho g.s. through |e and |b{+-} modes. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$<r{+2}>{+1/2}=5.202 fm {I31} (2013An02 evaluation) 
$Intrinsic hexadecapole moment=0.50 {I23} (1976Po05); 0.50 {I10} (1975Po03). Other: 1972DaYT 
MOMM1$+4.177 {I5} from re-evaluation (by 1998Gu22) of measured result of +4.094 {I45} (1972Ha45,atomic beam method). Other measurement: +4.1267 {I11} (1997Be64, hyperfine structure by electron-beam method; systematic uncertainty, which may be few times the quoted value, is not included). Compilation by 1989Ra17 gives +4.17 {I3} based on the original measurement of 1972Ha45 and subsequent re-evaluation by 1974Da11 and 1982Bu13 (who quote thesis by G. Nachtsheim (Bonn,1980)). Others: 1989Al27, 1987ArZT, 1968Su04, 1964Go09, 1963Bl25, 1962Wy04, 1962Li06, 1962Go20, 1962Fr14, 1958Hu17, 1958Ba35, 1958Be85 
MOME2$pionic x rays (1983Ol03). Others: +3.49 {I3} (muonic x rays, 1976Po05), 3.49 {I3} (atomic beam,1974Da11,1972Ha45), 3.69 {I3} (1977Ga08), 3.53 {I8} (pionic x rays,1974Eb03,1978Eb01), 3.57 {I4} (1978Ch37), 3.60 {I2} (pionic x rays,1981Ba07), 3.41 {I8} (kaonic x rays,1981Ba07). Note large discrepancy with other measurements: +2.716 {I9} (atomic beam,1982Bu13), +2.73 {I6} (atomic beam,1974Da10). Others: 1964Go09, 1963Bl25, 1962Wy04, 1958Ba35. 
T$>6|*10{+16} y (1956Po16), from detection limit of |a particles in the energy region of 1500-2500 keV 
J$spin from optical spectroscopy (1935Sc02,1957Be39) and paramagnetic resonance (1958Ba35,1955Ba04,1958Hu17). Parity from L(t,|a)=3 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
MOMM1$from |m(94.7)/|m(g.s.)=0.99 {I4} (Mossbauer effect,1972Ge21) and |m(g.s.)=+4.177 {I5}. 
MOME2$muonic x rays (1976Po05). 
T$weighted average of 23.6 ps {I18} (from B(E2) in Coulomb excitation), 22.0 ps {I4} (in (|g,|g):Mossbauer (1970BlZT)); and 28.4 ps {I24} (microwave method in (|a,|a'|g) (1970Ar02)). Other: 25 ps {I10} (|g|g(t) in {+165}Dy |b{+-} decay, 1967Ba27) 
J$M1+E2 |g to 7/2-; L(t,|a)=5 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$7/2+ and 15/2- assigned to a doublet of 491+499 from |s(|q) and cross-section ratio data in (|a,t) and analyzing powers in (pol t,|a); the 491-keV component is assigned with J|p=7/2+; member of a rotational band 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
E$in (t,|a), two levels are reported at 596 keV {I2}, a doublet with J|p=7/2+ and 9/2+, and another one at 604 keV {I1} with J|p=9/2+ 
J$L({+3}He,d)=4; |gs to 3/2+ 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E$in (t,|a), two levels are reported at 596 keV {I2}, a doublet with J|p=7/2+ and 9/2+, and another one at 604 keV {I1} with J|p=9/2+ 
J$|gs to 5/2+ and 7/2+; rotational band member 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J$M1+E2 |g to 9/2-; |gs to 5/2- and 11/2-; band assignment 
T$B(E2) values and branching ratios are not known well to determine half-life 


level_energy_unit: KEV
level_comment:
J$L({+3}He,d)=2 gives 3/2+,5/2+; but |gs to 7/2- and 9/2- suggest 5/2-,7/2,9/2,11/2-. There may be two different levels near this energy 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$(|g,|g') excitation from 7/2-; (M1) excitation in (e,e') from 7/2-; L({+3}He,d)=L(|a,t)=(5) from 0+ for a group around 1470 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$|g to 7/2-; possible |p9/2[514] bandhead; L({+3}He,d)=L(|a,t)=(5) from 0+ for a group around 1470 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2+)
level_comment:
J$7/2- from L(pol t,|a)=(3); (L+(1/2)) from Ay(|q), but L=2 and 4 are not excluded, thus (3/2+,5/2+) and (7/2+,9/2+) are also possible. L=(4) from |s({+3}He,d)/|s(|a,t) suggests 7/2+,9/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$d|s/d|W(|mb/sr)=2.1 
$NSF=0.037 
L$|s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) suggests 0,1,2; inconsistent with Adopted J|p=7/2- 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$d|s/d|W(|mb/sr)=1.0 {IAP} 
L$5 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); but L=3,4 not ruled out 
$NSF|?0.087 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$d|s/d|W(|mb/sr)=3.5 
L$3 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) is inconsistent 
$NSF=0.21 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$d|s/d|W(|mb/sr)=14.2 
L$0 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) is inconsistent 
$NSF=0.104 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_uncertain: ?
level_comment:
E$only a weak peak may have been seen by 1975Wa12 
L$L=1 from |s(|q) in 1974Le27, disagrees with L=4,5 from their |s({+3}He,d)/|s(|a,t) ratio 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$d|s/d|W(|mb/sr)=8.1 
$L=4 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) in disagrement with 7/2- assignment in their band assignment 
$NSF=0.10 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$d|s/d|W(|mb/sr)=3.2 
L$from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) 
$NSF=0.042, 5/2[413] assignment 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$d|s/d|W(|mb/sr)=15.7 
$NSF=0.80 
L$from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) 
E,L$other: L=6 from |s(|q) and 5 or 6 from |s({+3}He,d)/|s(|a,t) ratio (1974Le27) for a 1561 group which is identified with 1594 group in 1975Wa12 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$d|s/d|W(|mb/sr)=24.4 
L$0 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=1 is not ruled out 
E$1586 {I10} in 1974Le27 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$d|s/d|W(|mb/sr)=7.7 
L$1,0,2 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) 
E$1620 {I10} in 1974Le27 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$d|s/d|W(|mb/sr)=11.6 
L$from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=2,4 are not ruled out 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$NSF=0.023 
L$1,0,2 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) are inconsistent with J|p=7/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$d|s/d|W (|mb/sr)=69 {ILT} 
L$2,3,4 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=2 consistent with J|p=5/2+ 
$NSF|?0.52 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$d|s/d|W (|mb/sr)=76 
L$2,3 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=2 consistent with J|p=3/2+ 
$NSF|?0.73 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$d|s/d|W (|mb/sr)=7.0 
L$3 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) inconsistent with J|p=7/2+ 
$NSF|?0.13 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$d|s/d|W (|mb/sr)=3.6 {IAP} 
L$0 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) inconsistent with J|p=1/2- 
$NSF=0.046 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$d|s/d|W (|mb/sr)=82 
L$4,5 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=4 consistent with J|p=7/2+ 
$NSF=1.67 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 3/2-
level_comment:
$d|s/d|W (|mb/sr)=8.2 {IAP} 
L$0,1 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=1 consistent with J|p=3/2- 
$NSF=0.080 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 9/2+
level_comment:
$d|s/d|W (|mb/sr)=4.2 {ILE} 
L$4,5 from |s({+3}He,d)/|s(|a,t) (1974Le27); L=4 consistent with J|p=9/2+ 
$NSF|<0.04 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$d|s/d|W (|mb/sr)=18.8 
L$4 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12) is inconsistent with J|p=7/2- 
$NSF=0.13 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (9/2-)
level_comment:
$d|s/d|W (|mb/sr)=2.6 
L$5 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=4 is not ruled out 
$Possible |p9/2[514] 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (7/2-)
level_comment:
$d|s/d|W (|mb/sr)=1.1 
$Possible |p5/2[532] 
L$3 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=1,2 are not ruled out 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr)=3.5 
L$0 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=1 is not ruled out 
$Possible J|p=1/2+, |p1/2[400] 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$d|s/d|W (|mb/sr)=1.7 {ILE} 
L$1,0,2 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=4 is not ruled out 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr)=4.2 
L$3 from |s({+3}He,d)(60|')/|s(|a,t)(45|') (1975Wa12); L=2,4 is not ruled out 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 22 ps {I1} (1972Ge21), 20 ps {I3} (1972HaVV), 22.0 ps {I4} (1970BlZT). Other: |>22 ps (1966Ro10) 
$|m(94.7)/|m(g.s.)=0.99 {I4} (1972Ge21) 


level_energy_unit: KEV
level_spin_parity: 7/2,9/2
level_lifetime_unit: EV
level_comment:
T$24.9|*10{+-3} eV {I25} if decays also through 2991|g 
BM1$0.073 {I7} if decays also through 2991|g 


level_energy_unit: KEV
level_spin_parity: (9/2)
level_lifetime_unit: EV
level_comment:
T$16.8|*10{+-3} eV {I13} if decays also through 2973|g 
BM1$0.045 {I4} if decays also through 2973|g 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)=2.42 {I11} (2003Iw01). Other: 28.1 ps {I24} (microwave method in (|a,|a'|g) (1970Ar02)). 
BE2$others: 2.30 {I46} (1985Si06), 2.41 {I7} (1960Ol02) 
$E2 matrix element (from 7/2-,g.s.)=+4.4 {I1} (2003Iw01) 
$M1 matrix element (from 7/2-,g.s.)=+2.22 {I4} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
BE2$others: 0.62 {I8} (1985Si06), 0.63 {I4} (1960Ol02) 
$B(E2) (from 9/2-,95)=2.6 {I+2-7} (2003Iw01) 
T$from B(E2)=0.64 {I4} and adopted branching ratio 
$E2 matrix element (from 7/2-,g.s.)=+2.26 {I6} (2003Iw01) 
$E2 matrix element (from 9/2-,95)=+5.1 {I+2-7} (2003Iw01) 
$M1 matrix element (from 9/2-,95)=+2.82 {I+8-7} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)=1.16 {I+4-7} from 95 and branching from the Adopted Gammas 
$B(E2) (from 9/2-,95)=1.16 {I+4-7}, B(E2)(from 11/2-,210)=2.0 {I3} (2003Iw01) 
$E2 matrix element (from 9/2-,95)=+3.41 {I+6-11} (2003Iw01) 
$E2 matrix element (from 11/2-,210)=+4.9 {I3} (2003Iw01) 
$M1 matrix element (from 11/2-,210)=+4.00 {I+7-11} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T$from B(E2)=1.84 {I8} and branching from the Adopted Gammas 
$B(E2) (from 11/2-,210)=1.84 {I8}, B(E2) (from 13/2-,345)=2.2 {I+4-5} (2003Iw01) 
$E2 matrix element (from 11/2-,210)=+4.7 {I1} (2003Iw01) 
$E2 matrix element (from 13/2-,345)=+5.5 {I+5-6} (2003Iw01) 
$M1 matrix element (from 13/2-,345)=+5.1 {I+3-2} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
BE2$others: 0.0289 {I35} (1963Di09), B(E2)=0.044 {I5} (1967Se09), 0.030 {I3} (1985Si06) 
T$from B(E2)=0.061 {I6} and branching from the Adopted Gammas 
$E2 matrix element (from 7/2-,g.s.)=+0.70 {I3} (2003Iw01) 
$Diagonal E2 matrix element=+2.0 {I+3-8} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
BE2$others: 0.014 {I2} (1963Di09) and 0.021 {I2} (1967Se09), 0.013 {I2} in 1985Si06 
$B(E2)(from 9/2-,95)=0.018 {I+5-3}; B(E2)(from 3/2-,516)=3.2 {I+12-14} (2003Iw01) 
T$from B(E2)=0.018 {I+5-3} and branching from the Adopted Gammas 
$E2 matrix element (from 7/2-,g.s.)=-0.25 {I+4-3} (2003Iw01) 
$E2 matrix element (from 9/2-,95)=+0.43 {I+5-3} (2003Iw01) 
$E2 matrix element (from 3/2-,516)=+3.6 {I+6-9} (2003Iw01) 
$M1 matrix element (from 7/2-,g.s.)=+0.12 {I+2-2} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$B(E2) (from 9/2-,95)=0.016 {I+20-12} (2003Iw01) 
T$B(E2) values and |g branchings are not known well to deduce half-life 
$E2 matrix element (from 7/2-,g.s.)=-0.35 {I+8-4} (2003Iw01) 
$E2 matrix element (from 9/2-,95)=+0.4 {I2} (2003Iw01) 
$M1 matrix element (from 7/2-,g.s.)=-2.0 {I+2-5} (2003Iw01) 
$M1 matrix element (from 9/2-,95)=+1.2 {I+2-3} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: PS
level_comment:
$B(E2)(from 13/2-,345)=1.79 {I+21-15}; B(E2)(from 15/2-,499)=1.6 {I+14-6} (2003Iw01) 
T$from B(E2)=1.79 {I+21-15} and branching from the Adopted Gammas 
$E2 matrix element (from 13/2-,345)=+5.0 {I+3-2} (2003Iw01) 
$E2 matrix element (from 15/2-,499)=+5.0 {I+19-9} (2003Iw01) 
$M1 matrix element (from 15/2-,499)=+4.4 {I+4-2} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
$B(E2)=0.040 {I4} (1985Si06), 0.042 {I5} (1963Di09) and B(E2)=0.073 {I7} (1967Se09) 
T$from B(E2)=0.092 {I+5-7} and branching from the Adopted Gammas 
$B(E2) (from 9/2-,95)=0.038 {I+4-3}; B(E2)(from 15/2-,499)=0.05 {I4} (2003Iw01) 
$E2 matrix element (from 7/2-,g.s.)=+0.86 {I+2-3} (2003Iw01) 
$E2 matrix element (from 9/2-,95)=-0.62 {I+3-2} (2003Iw01) 
$E2 matrix element (from 15/2-,499)=-0.9 {I+3-4} (2003Iw01) 
$M1 matrix element (from 11/2-,210)=-0.16 {I+2-2} (2003Iw01) 
$Diagonal E2 matrix element=+4.1 {I+4-8} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$B(E2)(from 5/2-,567)=2.5 {I+45-7} (2003Iw01) 
$E2 matrix element (from 5/2-,567)=+3.9 {I+26-6} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
$B(E2)(from 9/2-,95)=0.23 {I3}; B(E2)(from 11/2-,699)=0.9 {I+9-5} (2003Iw01) 
$E2 matrix element (from 9/2-,95)=+1.50 {I+8-9} (2003Iw01) 
$E2 matrix element (from 11/2-,689)=+3.2 {I+13-10} (2003Iw01) 
$M1 matrix element (from 11/2-,210)=+2.8 {I+6-5} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_comment:
$B(E2)(from 15/2-,499)=3.3 {I+7-3} (2003Iw01) 
$E2 matrix element (from 15/2-,499)=+7.3 {I+7-3} (2003Iw01) 
$M1 matrix element (from 17/2-,673)=+4.1 {I+8-3} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_comment:
$B(E2)(from 17/2-,673)=2.0 {I+4-5} (2003Iw01) 
$E2 matrix element (from 17/2-,673)=+6.0 {I+6-7} (2003Iw01) 
$M1 matrix element (from 19/2-,863)=+5.6 {I+8-14} (2003Iw01) 


level_energy_unit: KEV
level_spin_parity: (7/2)+&(15/2-)
level_comment:
$d|s/d|W (|mb/sr)=23 
E,J$unresolved doublet of 491+499 levels seen in |g-ray studies, with the two components belonging to |p3/2[411] and |p7/2[523] band, respectively. 
$Ay(|q)(30|')=+0.09 {I9} 


level_energy_unit: KEV
level_spin_parity: 7/2+&9/2+
level_comment:
$d|s/d|W (|mb/sr)=15 
E$correspond to 590+604 in 1975Wa12. 
$NSF|?0.24(1978Lo08), 0.074 for 7/2+ at 590, 0.12 for 9/2+ at 604 (1975Wa12) 
$Ay(|q)(30|')=0.00 {I9} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: US
level_lifetime_info: ;ERR=LT
level_comment:
T$|g(t) (1958Ka10) 
J$|g(|q) from oriented {+165}Dy |b decay for 620|g and 715|g agree only with J|p=5/2+, not with 7/2+; however, 620|g to 9/2- disfavors 5/2+; L=4 and analyzing powers in (pol t,|a) strongly favor 7/2+ 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: H
level_comment:
T weighted average of 26.74 h {I5} (1966Da04), 26.79 h {I3} (1968Ne02), 26.83 h {I3} (1974Ry01), 27.00 h {I4} (1976Ra32), 26.827 h {I5} (1989Ab05), 26.794 h {I23} (2002Un02; supersedes 26.7663 {I44} (1994Co02 and 1992Un01)). Others: 1946Bo25, 1949Co15, 1949Gr01, 1950An12, 1958Co76, 1963Fu17, 1963Ho15. 
J J measured by atomic beam (if J>0 |m|<10|*10{+-4}) (1976Fu06); 1773|b{+-} to 2+ level in {+166}Er has 2-yes shape; E1 426|g from 1+ 426. 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: Y
level_lifetime_info: ;ISO=M
level_comment:
J cross section fingerprint at 3 angles for 3 band members in (d,p) and (d,{+3}He). 
E calculated by 1978Ba78. 
T from 1965Fa01. Other: 1952Bu18. 
|m, Q: from static nuclear orientation. Other |m: 3.60 {I16} (1981Kr12), 3.65 {I13} (1981Ma43) from static nuclear orientation. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: US
level_comment:
J E1 137|g to 2- 54; E1 20|g to 3- 171; (d,p) cross section fingerprint. 
T from 1965Bj03. Others: 214 |ms {I10} (1960Al27); 158 |ms {I14} (1964KaZZ); 207 |ms (1965Mc03); see also 1961Kr01, 1962En04. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J (d,p) cross section fingerprint; J=3,4 from 5761|g(|q) in (pol n,|g) E=thermal. 
T from (n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J J=3 from |g(|q) for primary |g feeding level in (pol n,|g); 389|g to 1+ 426; M1(+E2) 257|g to 4+ 559. 


level_energy_unit: KEV
level_spin_parity: 2,4
level_comment:
J 2,4 from primary |g(|q) (1979Bo08). However, deexciting gammas proposed in (n,|g) E=thermal: |g|g coin feed 5+ and 4- and 1- levels, so some must have been misplaced. 
E from (n,|g) E=thermal: |g|g coin 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J 837|g to (5)+ 264; band assignment. However, 624|g to (3)- 476; this suggests that 624|g is misplaced or that 1097 level is a doublet. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: US
level_comment:
T from 1965Bj03. Others: 214 |ms {I10} (1960Al27); 158 |ms {I14} (1964KaZZ); 207 |ms (1965Mc03); see also 1961Kr01, 1962En04. 


level_energy_unit: KEV
level_comment:
Possibly a doublet including the adopted 788.6 and 792.8 levels, but |g deexcitation pattern agrees with neither. 


level_energy_unit: KEV
level_comment:
Probable multiplet; levels adopted at 806.6 and 807.0 could not have been resolved in this experiment and the presence of an additional level cannot be ruled out. A 434|g and 546|g are known to deexcite the adopted 806.6 level but they should be accompanied by much stronger 336|g and 325|g, neither of which is seen here. 


level_energy_unit: KEV
level_comment:
Adopted J=2,4 for this level but the proposed deexciting gammas feed levels with J|p including 5+ and 4- and 1-, so some placements are presumably incorrect. 


level_energy_unit: KEV
level_comment:
Possible doublet; E|g values for deexciting transitions consistent with levels at ~1164 and ~1167 keV. 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_uncertain: S
level_comment:
E deduced from E|g=6188.3 assuming E=54.2 for the first excited state of {+166}Ho. This differs from S(n)=6243.64 {I2} (2003Au03); all primary |g energies from 1970Bo29 appear to be approximately 1 keV low. 
J assuming s-wave capture by J|p=7/2- target; p-wave capture is expected to be relatively small (1970Bo29). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$I(P)=12 {I1} 
E reported energy (1687 {I4}) appears to be a misprint since it is listed out of numerical order. 1697 seems a reasonable possibility. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$broad bump centered at 3 MeV in the |g strength function. Interpreted by 2023Po02 as corresponding to the M1 scissors resonance. 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: D
level_comment:
T$from weighted average of 26.806 h {I12} from IC measurement over 11 half-lives, 26.793 h {27} from IC measurement over 2.5 half-lives, 26.818 h {i16} from NaI measurement over 8 half-lives, 26.828 h {I28} and 26.800 h {i26} from HPGe measurements (2019Bo14) 
J$from adopted levels of {+166}Ho in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: H
level_comment:
J$angular distribution and analyzing power in {+168}Er(pol t,|a). 
T$from 2002Ka45, decay curves for 321|g and 347|g. 2002Ka45 give weighted average of 3.003 h {I18} from the following eight measurements, four for each of the two |g rays: 2.952 h {I5}, 2.961 h {I32}, 3.035 h {I3}, 2.948 h {I11}, 2.947 h {I3}, 2.932 h {I15}, 3.0253 h {I20}, and 3.002 h {I23}, uncertainties being statistical only. However, evaluators find that the dataset of T{-1/2} values in 2002Ka45 is highly discrepant, with reduced |h{+2}=106 as compared to critical |h{+2}=2.0. Evaluators adopt unweighted average of 2.98 h {I3}, where the uncertainty has been doubled to account for systematic uncertainties. Others: 3.1 h {I1} (1960Wi10, |b counting), 3.0 h (1955Ha45, from |g decay). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$M2 |g to 7/2-; angular distribution and analyzing power in {+168}Er(pol t,|a). 
T$|b|g(t) in {+167}Dy |b{+-} decay (1977Tu01). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$|g to 3/2+ and position of level relative to 3/2+ 1/2[411] state consistent with 1/2[411] bandhead assignment. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$doublet from a wider peak than normal, although |s(|q) and A{-y}(|q) distributions consistent with 5/2+ for most of the peak (1979Lo02) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Implicit L=3 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in poor agreement with L=3 
$d|s/d|W (30|')=19 |mb/sr, A{-y} (30|')=+0.50 {I10} 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$Implicit L=5 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in reasonable agreement with L=5 
$d|s/d|W (30|')=14 |mb/sr, A{-y} (30|')=-0.73 {I10} 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$Implicit L=5 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in good agreement with L=5 
$d|s/d|W (30|')=221 |mb/sr, A{-y} (30|')=+0.52 {I3} 
$Large spectroscopic factor consistent with origin of |p7/2[523] orbital in the |ph{-11/2} shell-model state. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$Implicit L=2 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in approximate agreement with L=2 
$d|s/d|W (30|')=29 |mb/sr, A{-y} (30|')=-0.76 {I7} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$Implicit L=2 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in approximate agreement with L=2 
$d|s/d|W (30|')=288 |mb/sr, A{-y} (30|')=+0.43 {I3} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$Implicit L=2 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in reasonable agreement with L=2 
$d|s/d|W (30|')=97 |mb/sr, A{-y} (30|')=-0.51 {I4} 
E$includes possible component from 7/2+, |p3/2[411] state. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
$Implicit L=(4) from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in reasonable agreement with L=4 
$d|s/d|W (30|')=44 |mb/sr, A{-y} (30|')=+0.10 {I7} 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
$Implicit L=(4) from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is not in good agreement with L=4 
$d|s/d|W (30|')=22 |mb/sr, A{-y} (30|')=-0.40 {I10} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$Implicit L=4 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in approximate agreement with L=4 
$d|s/d|W (30|')=42 |mb/sr, A{-y} (30|')=-0.65 {I6} 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
$Implicit L=(5) from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3a of 1979Lo02 is in poor agreement with L=5 
$d|s/d|W (30|')=9 |mb/sr, A{-y} (30|')=-0.37 {I15} 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
$Implicit L=(4) from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in good agreement with L=4, but poor agreement of A{-y}(|q) for L-1/2 
$d|s/d|W (30|')=69 |mb/sr, A{-y} (30|')=-0.21 {I6} 
J$possible 7/2 member of a |g-vibration band built on the 1/2+, |p1/2[411] state. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$Implicit L=4 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in good agreement with L=4 
$d|s/d|W (30|')=67 |mb/sr, A{-y} (30|')=-0.73 {I5} 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
$Implicit L=(4) from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in reasonable agreement with L=4 
$d|s/d|W (30|')=23 |mb/sr, A{-y} (30|')=+0.31 {I10} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$L=2 assigned by 1979Lo02 from |s(|q) distribution 
J$agreement with L+1/2 for A{-y}(|q) is poor in Fig. 3b 
$d|s/d|W (30|')=22 |mb/sr, A{-y} (30|')=+0.08 {I10} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Implicit L=3 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in approximate agreement with L=3 
$d|s/d|W (30|')=52|mb/sr, A{-y} (30|')=+0.45 {I6} 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$Implicit L=5 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in good agreement with L=5 
$d|s/d|W (30|')=108 |mb/sr, A{-y} (30|')=+0.36 {I4} 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
$Implicit L=0 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in good agreement with L=0 
$d|s/d|W (30|')=70 |mb/sr, A{-y} (30|')=-0.15 {I6} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$Implicit L=2 from J|p assignment based on A{-y}(|q) distributions. The |s(|q) distribution in Fig. 3b of 1979Lo02 is in poor agreement with L=2 
$d|s/d|W (30|')=131 |mb/sr, A{-y} (30|')=+0.19 {I4} 
E$doublet from a wider peak than normal, although |s(|q) and A{-y}(|q) distributions consistent with 5/2+ for most of the peak (1979Lo02) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_comment:
J log| {Ift}=5.45 to 2+ 821, log| {Ift}=6.9 to 4+ 995 in {+168}Ho |b{+-} decay. Suggested configuration: (|p 7/2[523])-(|n 1/2[521]) (1973Ti02), based on systematics. 
T weighted average of 3.3 min {I5} (1960Wi10), 3.0 min {I1} (1963Ka10), and 2.98 min {I9} (1973Ka07). 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (6+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%|b{+-}: limit consistent with apparent absence of |b{+-} decay to low-lying 4+ and 6+ states in {+168}Er (1990Ch37). 
J possible (M3) |g to 3+ g.s.; no |b{+-} branch from 0+. Suggested configuration: (|p 7/2[523])+(|n 5/2[512]) (1990Ch37). 
T from 1990Ch37. 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
J M2 144|g to 3+ g.s.; |g from 1+. 
T estimate from intensity ratios in singles and coincidence spectra in {+168}Dy |b{+-} decay (1990Ch37). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J log| {Ift}=4.5 from 0+ {+168}Dy; |g to 3+ g.s.. Allowed unhindered |b{+-} decay to level suggests presence of (|p 5/2[532]) or (|p 7/2[523]) in its configuration. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
J log| {Ift}=4.9 to 853 level in {+169}Er indicates allowed unhindered |b{+-} decay which, in this mass region, establishes configurations of (|p 7/2[523]) for this level and (|n 5/2[523]) for the {+169}Er state fed. This is also consistent with known structure in lighter odd-mass Ho nuclei. 
T weighted average of 4.8 min {I1} (1963Mi17), 4.4 min {I2} (1966Fu09), 4.7 min {I2} (1978Ka16). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)-
level_comment:
J log| {Ift}|?4.9 from (5/2)- {+169}Dy. 1990Ch34 suggest that this may Be a three quasiparticle state with configuration (|p 7/2[523])~#(|n 5/2[512])~#(|n 5/2[523]){+-1}, but decline to actually make this assignment. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J from (pol t,|a). L=(3) in (d,{+3}He) but angular distribution does not enable definitive fit; possibly different states are excited by these two reactions. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
Bandhead was placed at centroid of unresolved multiplet; the nature of an additional nearby transition is unknown (possibly from a contaminant). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J strong population favors 7/2+ 5/2[413] assignment over 7/2+ 1/2[411]; overlap with expected 9/2+ 3/2[411] state increases uncertainty of assignment. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
S value is much smaller than expected (level is dominant band member) because Coriolis coupling to the 7/2+ 7/2[404] state moves strength to that level. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
S$value is smaller than predicted value (1/2[420] orbital has its origin in the 2d{-5/2} shell-model state) suggesting high-energy fragmentation of single-particle strength. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_lifetime_unit: US
level_comment:
J$ 19/2+ preferred over other possible choices of 19/2- and 21/2- 
$ Proposed configuration=|p7/2[523]~#|n5/2[512]~#|n7/2[633] 
T$ from time dependence of the intensity of selected transitions following the decay of the isomer (2010Dr05), mean lifetime (|t)=170 |ms {I8} 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MIN
level_comment:
J from systematics; neighboring Z=67 and N=103 odd nuclei have g.s. configurations of (|p 7/2[523]) and (|n 5/2[512]), respectively, so configuration (|p 7/2[523])+(|n 5/2[512])6+ is expected for {+170}Ho g.s. (assuming Gallagher-Moszkowski rule). 
T from |g(t) (1978Ka16). Others: 2.8 min {I2} (1974Ka21), 2.9 min (1969Sc01). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%B- no isomeric transition observed in 1974Ka21. 
E from difference in endpoint energies in {+170}Ho |b{+-} decay (43 s) and {+170}Ho |b{+-} decay (2.76 min) (1978Tu04). 
J log| {If{+1u}t}<8.5 to 0+ g.s. and/or (0+) 891 level of {+170}Er, independent of assumptions about magnitude of |b{+-} branch to g.s. in {+170}Ho |b{+-} decay (43 s), so J=0,1 is probable; nonzero |b{+-} feeding of 2+ 79-keV level (though imprecisely determined) rules out 0+ and probably 0- (log| {If{+1u}t}<8.5 if |b{+-} branch to 2+ is |>7%); J|p systematics in neighboring nuclei favor J|p=1+, with configuration=((|p 7/2[523])-(|n 5/2[512]))1+ (1978Tu04). 
T from |g(t) (1974Ka21). Others: 40 s {I10} (1960Wi10), 45 s {I5} (1961Ta08), 44 s {I5} (1963Ka10), 42 s {I3} (1969Sc01). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
J g.s. configuration probably 7/2[523], as established for lighter odd-mass Ho nuclei ({+157}Ho to {+169}Ho); slight changes in deformations from {+164}Er to {+170}Er support assignment. 
T weighted average of 56 s {I4} (1990Ch34, |b(t)), 54 s {I3} (1990Ch34, |g(t)), and 47 s {I5} (1989Ry04). Data from 1990Ch34 are presumed to supersede preliminary data from X(t) in 1989Ch05 (49 s {I5}). 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
J$Low energy level spectrum has been calculated by 1991Be04 using a macroscopic-microscopic model. Below 260 keV, six excitations are proposed from coupling of following proton and neutron states: proton states: 7/2[523], 1/2[411]. Neutron states: 9/2[624], 7/2[514], 5/2[512]. These give J|p=(1-,8-) for g.s.; (0+,7+) for 8 keV; (3-,4-) for 70 keV; (4+,5+) for 72 keV; (1+,6+) 180 keV; and (2-,3-) for 258 keV. Possible |b feeding of (4+) and (1,2+) levels in {+172}Er would support J|p({+172}Ho g.s.)=3,4-. 
E,J$2000GrZV reconstructed the decay scheme of {+172}Ho to {+172}Er using data |g and |g|g-coin data from 1991Be04 and levels data from 1980Sh14, and postulated two activities in {+172}Ho, each of about 25 s half-life, one with J|p=1-, configuration=|p7/2[523]-|n9/2[624], and the other with J|p=7+, configuration=|p7/2[523]+|n7/2[514], the latter populating an 8+ -> 7+ -> 6+ -> 5+ -> 4+ sequence, starting from a 2548.9-keV, 8+ level decaying through a 757.2-153.7-137.8-103.7 |g cascade. However, in the high-spin study by 2010Dr02, no 8+ state at 2548.9 keV in {+172}Er was reported, which casts doubt on the reconstructed decay scheme of {+172}Ho to {+172}Er in 2000GrZV. In the opinion of the evaluator, further improved experiments are needed to investigate possible isomerism in {+172}Ho and establish the decay scheme of {+172}Ho, which seems incomplete at present, and also experimentally investigate the possibility of isomerism in {+172}Ho 
T$from |b(t) and |g(t) (1991Be04) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$From systematics of known quasiparticle states in neighboring nuclei and the proposed configuration (by the compiler). The assignment is tentative. 
T$From a fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. The data analysis included contributions from the parent, daughter and grand-daughter decays, as well as a constant background. The assignment to the ground state is ambiguous, given the possible existence of an isomeric state. 
CONF$From systematics of well-deformed nuclei in this mass region, the |p7/2[523] and |n7/2[514] Nilsson orbitals are expected near the proton and neutron Fermi surfaces, respectively. Thus, using the Gallagher-Moszkowski rule, one may expect the K|p=0+, |p7/2[523]~#|n7/2[514] configuration for the ground state. The existence of a high-spin, K|p=7+ isomer, arising from the same configuration, is also possible. The assignment is made by the compiler. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$From systematics of known quasiparticle states in neighboring nuclei and the proposed configuration (by the evaluator). The assignment is tentative. 
T$From 2017Wu04, using a fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. The data analysis included contributions from the parent, daughter and ground-daughter decays, as well as a constant background. A value of 6.90 s {I48} is quoted in 2017Wu04 
CONF$|p7/2[523] Nilsson orbital, based on systematics of known structures in neighboring, well-deformed nuclei (by the evaluator). The assignmnet is tentative. 
$ Production |s(at 1 GeV/nucleon)=341 nb {I15} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
%B-$only |b{+-} decay mode is expected. 
J$from proposed configuration of |p7/2-[523] 
T$from a fit to the implanted ion-|b(t) spectrum (2020Li28). Fit includes contribution from daughter, granddaughter, and great-granddaughter, as well as background. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_lifetime_unit: US
level_comment:
T$from a fit to the implanted ion-|b(405|g)(t) spectrum (2020Li28). 
J$from proposed configuration of |p3/2+[411] 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$From systematics of known quasiparticle states in neighboring nuclei and the proposed configuration (by the evaluator). The assignment is tentative. 
T$From 2017Wu04, using a fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. The data analysis included contributions from the parent, daughter and ground-daughter decays, as well as a constant background. The assignment to the ground state is ambiguous, given the possible existence of an isomeric state. 
CONF$From systematics of well-deformed nuclei in this mass region, the |p7/2[523] and |n9/2[624] Nilsson orbitals are expected near the proton and neutron Fermi surfaces, respectively. Thus, using the Gallagher-Moszkowski rule, one may expect the K|p=8-, |p7/2[523]~#|n9/2[624] configuration for the ground state. The existence of a low-spin, K|p=1- isomer, arising from the same configuration, is also possible. The assignment is made by the evaluator. 
$ Production |s(at 1 GeV/nucleon)=98 nb {I6} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_lifetime_unit: S
level_comment:
%B-$only |b{+-} decay mode is expected. 
J$from proposed configuration of |n9/2+[624]|~#|p7/2-[523] 
T$from a fit to the implanted ion-|b(t) spectrum (2020Li28). Fit includes contribution from daughter, granddaughter, and great-granddaughter, as well as background (2020Li28). Other: 3.9 s {I11} from 199|g(t) (2020Li28). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
%B-$Only |b{+-} decay mode is expected. 
J$From systematics of known quasiparticle states in neighboring nuclei and the proposed configuration (by the evaluator). The assignment is tentative. 
T$From 2017Wu04, using a fit to the implanted ion-|b{+-}-t spectrum using the least-squares and maximum-likelihood methods. The data analysis included contributions from the parent, daughter and ground-daughter decays, as well as a constant background. A value of 1.88 s {I55} is quoted in 2017Wu04 
CONF$|p7/2[523] Nilsson orbital, based on systematics of known structures in neighboring, well-deformed nuclei (by the evaluator). The assignmnet is tentative. 
$ Production |s(at 1 GeV/nucleon)=22 nb {I2} (2012Ku26) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Mainly |b{+-} decay mode is expected. Predicted %|b{+-}n=0.12 (1997Mo25) 
E$ the observed {+176}Ho fragments assumed to correspond to the g.s. 
J$ 7/2- for valence proton and 1/2- for valence neutron predicted (1997Mo25) 
T$ limiting value from time-of-flight of 160 ns in 2012Ku26. Actual |b-decay half-life is expected to be much longer as suggested by 0.54 s from theoretical calculations (1997Mo25) 
$ Production |s=2.2 nb {I6} (2012Ku26) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
%B-$Only |b{+-} decay mode is expected for such a neutron-rich nucleus 
J$Systematic of known single-particle structures in deformed, odd-Z Ho isotopes; expected ground-state configuration 
T$>550 ns; lower limit from time-of-flight in 2018Fu08. Actual half-life is expected to be much longer. 
CONF$Most likely the |p7/2[523] Nilsson orbital 
$Production |s=0.10 nb {I2}, with 50% systematic uncertainty (2018Fu08) 


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}=314.5 ms, %|b{+-}n=3 (2019Mo01) 
$Theoretical T{-1/2}=2.19 s, %|b{+-}n=1.0 (2016Ma12) 
$A total of five counts were assigned to {+178}Ho for spectrometer setting on Gd. 
$Production |s=15 pb {I+10-6} for Gd setting, with 50% systematic uncertainty on |s values (2018Fu08) 
E$it is assumed that the observed events correspond to ground-state activity. 
J$2+ or 5+ from |W{-|p}=7/2- and |W{-|n}=3/2- orbitals proposed in 2019Mo01 
T$lower limit from time-of-flight of 550 ns given in 2018Fu08. Actual half-life is expected to be much longer as suggested by the theoretical values of 314.5 ms (2019Mo01) and 2.19 s (2016Ma12). From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+178}Ho is expected to be <2.5 s, based on measured half-lives of 6.9 s for {+173}Ho, 3.2 s {I11} for {+174}Ho, and 1.9 s {I6} for {+175}Ho, available in literature. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T$from (2000So11), T{-1/2} has to be of the same order or larger than the flight time through the spectrograph, which for this experiment was 200 ns 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T from 1989Vi02. 0.7 s (2006Ta08) 
$Observed delayed protons in coin with Ho K| x ray and known 2+ to 0+ and 4+ to 2+ |g's in {+144}Dy (1989Vi02). No |g's associated with |e decay were observed (1989Vi06) level previously assigned as the g.s.. Other: 1988WiZN 
J$configuration=(|n h{-11/2}), L=0 p transition from {+146}Tm 5-, g.s. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$|g(K| X ray)(delayed proton) coincidences were observed in the {+146}Er |e decay of 1.7 s activity; no detailed |g spectra were available (1993To05) 
T$from observation of (Ho K| X rays)(|b{++})(t) (1993To05) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
T$estimated by 2010Ma27 from the |b-delayed proton spectrum from the |ns1/2 g.s. of {+147}Er. They obtained this spectrum by subtracting the component in coincidence with the 4+ to 2+, 926-keV transition in {+146}Dy from the proton spectrum gated with the 2+ to 0+, 683-keV transition in {+146}Dy. This is based on the assumption that the |b-delayed proton decay of {+147}Er g.s. contributes mostly to the direct population of the 2+, 683-keV state in {+146}Dy granddaughter (due to the high difference in between the angular momenta of |nh11/2 isomer and |ns1/2 g.s. of {+147}Er parent). Other: |? 2.5 s (mentioned by 1987ToZU quoting 1984ScZT, see comment on the 11/2- isomer) 
CONF$|ns1/2 (1993To02) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$x=100 keV {I50} (2021Ko07, syst); x<118 keV (1993To02) 
T$measured by 2010Ma27 from the time distribution of the proton spectrum gated by the 4+ to 2+, 926-keV transition in {+146}Dy assuming that the 4+ state in {+146}Dy was mainly produced by the |b-delayed proton of the |nh11/2 isomer in {+147}Er parent. According to 2010Ma27 the delayed proton spectrum gated by the 683-keV transition in {+146}Dy decaying with an apparent T{-1/2}=2.5 s {I2} corresponds to the composed decay of both |nh11/2 isomer and |ns1/2 g.s. of {+147}Er. The previous measurements of 1984ScZT and 1988WiZN also determined 2.5 s {I2} previously adopted by 1992De38 and 2009Ni02 for this isomeric state, as well as |? 2.5 s for the g.s. 
%EC+%B+,%B+P$also reported by 1984ScZT (|b{++}p), 1984ScZT (|e+|b{++}) 
CONF$|nh11/2 (1993To02) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$x=100 keV {I50} (2021Ko07, syst); x<118 keV (1993To02) 
%EC+%B+,%B+P$from the Adopted Levels 
CONF$|nh{-11/2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$ Delayed proton emission probability |?0.15% (if I(141|g+244|g+315|g)|?25%) (1988To03) 
T$ average of 4.8 s {I2} (1989Ta11), 4.4 s {I2} (1988To03), 4.5 s {I4} (1982No08) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
T$unweighted average of 8.9 s {I2} from 1989Fi01 in IT decay, 10.8 s {I6} (1984ScZT) and 9 s {I1} (1984To07) from {+149m}Er |e decay 
J$probable h{-11/2} neutron state and systematics 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E,J,T$from the Adopted Levels. Other: E(level)=741.5 {I2} from 630.5|g+111.0|g 
T$value from this study: 8.9 s {I2} from 1989Fi01. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: US
level_comment:
J$from systematics and model calculations for (|p,h11/2,n)10+ isomers in neighboring proton-rich nuclei (1981La26). 
J,T$from (HI,xn|g): 2.55 |ms delayed. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$from level energy systematics, based on the 3- level in {+146}Gd, and compatibility of B(E3)(W.u.) assignments to the assumed E3 and determined E1 transitions with measured branching (1982No07,1984Ch11). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
T$weighted average of 23~s~{I2} (1970To16), 21~s~{I4} (1982Ba75) and 24.6~s~{I20} (1988Ba02) 
J$probable configuration=|nf{-7/2} (1997Co24) from systematics 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$from analogy to the decay of {+147}Tb and {+149}Ho. It is supported also by log| {Ift}|?4.6 from (11/2-) parent. 
$Configuration=|nh{-9/2} (1997Co24) 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: NS
level_comment:
J$(E3) |g to (7/2-) 
T$from pulsed beam |g(t) in (1980Ja16) 
$Configuration=(|nf{-7/2}~#3-)+|ni{-13/2} (1997Co24) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$|g to (7/2-); possible configuration=|nf{-7/2}~#2+ (1997Co24). But possible |g to (13/2+) disfavors this assignment 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J$(M1) |g to (13/2+); |g from (17/2+). But possible |g's to (9/2-) and (7/2-) are inconsistent with 15/2+ assignment. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%EC+%B+$From I(|g+ce)(1140|g+338|g) and average I(|g+ce) of 789|g, 597|g and 297|g. Same value was given by 1988Ba02. 
J$E3 |g to (21/2+); configuration=|ph{-11/2}{+2}~#|nf{-7/2} (1997Co24) 
T$weighted average of 0.57~s~{I1} (1988Ba02) and 0.62~s~{I2} (1980Ja16). 
T$Half-life of fully-ionized atom ({+151}Er{+68+})=19~s~{I3} (2003Li42). The ions of {+151}Er were produced in the fragmentation of {+209}Bi beam at 900~MeV/nucleon followed by mass separation using fragment-recoil separator and storing the fragments in cooler ring (ESR) at GSI facility. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
$Configuration=|nf{-7/2}~#2+ 
$354.2|g and 692.8|g placed from this level by 1990Ak01 in {+151}Tm |e decay (4.17~s) study are not reported by 1997Co24 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$Configuration=|nf{-7/2}~#2+ 
$408.3|g placed from this level by 1990Ak01 in {+151}Tm |e decay (4.17~s) study is not reported by 1997Co24 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
$718.0|g and 1411.0|g placed from this level by 1990Ak01 in {+151}Tm |e decay (4.17~s) study are not reported by 1997Co24 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$1980Ja16 measured delayed |g multiplicity: 3.4~{I5}. 
$Configuration=|ph{-11/2}{+2}~#|nf{-7/2} 
T$from 'adopted levels'. Half-life of fully-ionized (bare) atom ({+151}Er{+68+})=19~s~{I3} (2003Li42), where {+151}Er was produced in the fragmentation of {+209}Bi beam at 900~MeV/nucleon followed by mass separation using fragment-recoil separator and storing the fragments in cooler ring (ESR) at GSI facility. 


level_energy_unit: KEV
level_spin_parity: (67/2-)
level_lifetime_unit: US
level_comment:
T$recoil-shadow method with a pulsed ({+40}Ca) beam (1990An25) 
$Possible configuration=|p[h{-11/2}{+4}d{-3/2}{+1}d{-5/2}{+-1}]{-20+} ~#|n[f{-7/2}h{-9/2}h{-11/2}{+-1}]{-27/2-} (2000Fo15) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$T{-1/2} from 1982Bo04. Others: 10 s {I1} (1982To14), 9.8 s {I3} (1981HoZM,1970To16), 10.1 s {I2} (1977Ha48) 
%A From 1987To02 
$<r{+2}>{+1/2}=5.07 fm 3 (2004An14) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$E2 |g to 0+ 
$Predicted B(E2)|^=0.59 {I10} (1989Ra16, best fit global syst). this corresponds to T{-1/2}=1.39~ps~{I+29-20} 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (1-,2-,3-)
level_uncertain: ?
level_comment:
E from E(|b{++})|?4.0 MeV in (808|g)(|b{++}) coin (1987To02) and Q(|e) 
J probable low log| {Ift} suggests allowed decay to this level 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: NS
level_comment:
Configuration=(|n,f{-7/2})(|n,h{-9/2}) 
T from 1984AdZZ. Others: |?2 ns (1981Ba33); 1.2 ns {I3} (1980Ba33) 
g-factor: from |g(|q,H) with paramagnetic correction 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: NS
level_comment:
T from 1984AdZZ. Others: |?1.5 ns (1992Ku13,1981Ba33), 0.8 ns 3 (1980Ba33) 
g-factor: from |g(|q,H) with paramagnetic correction 


level_energy_unit: KEV
level_spin_parity: 28+
level_lifetime_unit: NS
level_comment:
T from 1992Ku13. Other: possibly the 32 ns {I3} isomer at E(exc.)=8.5 {I4} MeV seen by 1980Bo07 
Configuration=((|p,h{-11/2}){++4}{-16+}(|n, i{-13/2}){++2}{-12+})28+ 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
T From 1982Bo04; others: 35.1 s {I20} and 36.3 s {I20} (1980Da09), 36 s (1978De34), 40 s {I2} (1977Ha48), 36 s {I1} (1970To16), and 36 s {I2} (1963Ma18). 
J Tentative assignment based on J|p of nearby isotones {+151}Dy and {+149}Gd and shell-model predictions 
%A From 1977Ha48 and 1979Ho10; others: 38 {I+19-7} (1974To07) and 1963Ma18. Evaluation of 1991Ry01 recommends 53%. 
MOMM1 From 2014StZZ 
MOME2 From 2016St14 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
T$From 1982Ca09 (({+14}N,p4n|g),({+12}C,3n|g)); others: 380 ns 30 (1981Ho05), 0.40 |ms 20 (1980Ja16), 0.30 |ms 10 (1980Bo07), and 0.5 |ms 3 (1979Ha29). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (41/2-)
level_lifetime_unit: NS
level_comment:
T Weighted average of 270 ns {I20} (1981Ho05) and 200 ns {I30} (1980Ja16) with internal uncertainty of 17 and reduced-|h{+2} of 3.8; others: 1.0 |ms 5 (1980Bo07) and > 0.2 |ms (1979Ha29). (all references are from ({+14}N,p4n|g),({+12}C,3n|g) dataset) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
From log{Ift} systematics (1998Si17), for |DJ=2, no feeding log{Ift} > 10.6, so I(|e+|b{++}) < 6x10{+-5}%. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (27/2-)
level_lifetime_unit: NS
level_comment:
T From 1982Ca09; others: 380 ns {I30} (1981Ho05), 0.40 |ms {I20} (1980Ja16), 0.30 |ms {I10} (1980Bo07), and 0.5 |ms {I3} (1979Ha29). This T{-1/2} was assigned to 2751 level by 1982Ca09, but to this level, which had an energy of 2751+x, by 1981Ho05 and 1982Fo06. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (41/2-)
level_lifetime_unit: NS
level_comment:
T Weighted average of 270 ns {I20} (1981Ho05) and 200 ns {I30} (1980Ja16) with internal uncertainty of 17 and reduced-|h{+2} of 3.8; others: 1.0 |ms {I5} (1980Bo07) and > 0.2 |ms (1979Ha29). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$From an evaluation of data on nuclear rms charge radii, 2014An02 report <r{+2}>{+1/2}=5.113~fm~{I27}. 
T Weighted average of 3.6 m {I3} (1982Ba75) and 240 s {I20} (1982To14) from |e decay and 3.75 m {I12} (1974PeZS) and 3.6 m {I2} (1982Bo04) from |a decay. Others: 3.75 m {I50} (1974To07) and 4.5 m {I10} (1963Ma18) from |a decay. 
%A From 1974To07. Other: 0.17 {I10} (1968Go13). 
$E|a=4168 {I3} (from 2013Ba31 evaluation recommended by 1991Ry01) 
|D<r{+2}>({+152}Er-{+154}Er)=0.25 fm{+2} {I6} and |D<r{+2}>({+154}Er-{+156}Er)=0.26 fm{+2} {I9}, experimental values from the compilation of 1995Ne12; the values were computed by subtraction of two entries. 


level_energy_unit: KEV
level_spin_parity: 11(-)
level_lifetime_unit: NS
level_comment:
J$from agreement of measured g-factor (1983Ng02 and 1984Ra11) with that calculated for the configuration ((|n i{-13/2})(|n h{-9/2})). This configuration is expected to lie lower than that with J|p=10-. 
T weighted average of 35 ns {i3} (1978Ag01), 40 ns {i3} (1979Ba03), and 50 ns {i5} (1980Bo07) from (HI,xn|g) studies. 
MOMM1$from 2020StZV based on g-factor=+0.0154 {i12} (1984Ra11). Other: g-factor= +0.017 {i3} (1983Ng02). 
%A from a search for |a decay of high-spin isomers (1980Vr01). 


level_energy_unit: KEV
level_spin_parity: 21(-)
level_uncertain: ?
level_comment:
E$See the comment on this level energy in the heavy-ion data set. 
J$E2 |g from 23(-) level and E2 |g to 19(-) level 


level_energy_unit: KEV
level_spin_parity: 35(+)
level_uncertain: ?
level_comment:
E$See the comment on this level energy in the heavy-ion data set. 
J$J=35 from D |g to 34 level and |p=(+) from M1+E2 |g from 36(+) 


level_energy_unit: KEV
level_spin_parity: 36(+)
level_comment:
J$J=36 from |DJ=1, 393.6|g to 35(+), 11506 level (its M1+E2 character was used to define parity for 11506 level); |p=(+) from |g to 34(+) level 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$2001La17, from (HI,xn|g):SD,TSD suggest J{-1}|?(24+). 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$2001La17, from (HI,xn|g):SD,HD suggest J{-2}|?(26+). 


level_energy_unit: KEV
level_spin_parity: 11-
level_lifetime_unit: NS
level_comment:
E deduced from energies of |g's feeding this level. 
T weighted average of 35 ns {I3} (1978Ag01), 40 ns {I3} (1979Ba03), and 50 ns {I5} (1980Bo07). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J1
level_comment:
J 2001La17 suggest J{-1}|?(24+), which is the value shown in the compilation of 2002Si26. This band appears to feed into the normal-deformed levels of J|p=19- to 25- (2001La17). Other: (26+) (1995Be36), from considerations of |g intensity within the SD and yrast bands. This latter value appears in the compilation of 1999Ha56. 
E 1995Be36 infer that the likely entry region of the SD band into the states of normal deformation in {+154}Er is near an excitation energy of 7.4 MeV. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: J2
level_comment:
J 2001La17 suggest J{-2}|?(26+). This band appears to have a feeding pattern similar to that of the SD-1 band, although it may feed levels somewhat higher up in the spectrum of states of normal deformation. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
J favored |a transition to J=7/2(-) g.s. of {+151}Dy. |g from 531.7, 11/2- level indicates |p=-. Assignment consistent with systematics of nearby N=87 isotones {+151}Gd and {+153}Dy. |n f{-7/2} spherical shell-model state. 
T from measured I|a(t) (1969To06) 
%A From I(K|a{-1}| x ray)/I|a (1974To07) 
MOMM1 From 2014StZZ 
MOME2 From 2016St14 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J M1 to 7/2- indicates J|p=5/2-, 7/2-, 9/2-. Probable Gamow-Teller transition (1991To08, from {+155}Tm |e decay (21.6 s), state log| {Ift}=4.7) from 11/2- indicates J|p=9/2- and establishes configuration=(|n h{-9/2}) for this state. 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: NS
level_comment:
MOMM1$from 2014StZZ compilation (measured g-factor in (HI,xn|g) (1984Ra11)) 
J E1 |g to 11/2-. Head of a 13/2+ signature=+1/2 sequence of levels. The measured g-factor supports the 13/2+ assignment, as does the systematics of the odd-A Er isotopes from {+157}Er to {+165}Er. 
T from 1987Ra20, |g(t) in (HI,xn|g). 1977Ag02 report T{-1/2}=30 ns {I3}, from |g|g(t) in (HI,xn|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 41/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
"maximally aligned" structure involving two f{-7/2} neutrons, two h{-9/2} neutrons and an i{-13/2} neutron (2001Ni13). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 77/2-
level_comment:
"double maximum alignment" structure, involving the alignment of the spins of both neutron and proton pairs outside the {+146}Gd core, with those of the four h{-11/2} valence protons being coupled to 16+ (2001Ni13). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 79/2-
level_comment:
"double maximum alignment" structure, involving the alignment of the spins of both neutron and proton pairs outside the {+146}Gd core, with those of the four h{-11/2} valence protons being coupled to 16+ (2001Ni13). 
According to the calculations presented by 2001Ni13, the configurations of all the negative-parity yrast states above this one involve broken proton pairs in the {+146}Gd core. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 81/2+
level_comment:
According to the calculations presented by 2001Ni13, the configurations of all the positive-parity yrast states above this one involve broken proton-pairs in the {+146}Gd core. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J probable Gamow-Teller transition from 11/2- in {+155}Tm establishes configuration=(|n h{-9/2}) for this state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2+
level_lifetime_unit: NS
level_comment:
1987Ra20 report Q({+154}Er,11-)/Q({+155}Er,13/2+)=1.18 {I3} 
T from 1987Ra20, |g(t). 1977Ag02 report T{-1/2}=30 ns {I3}, from |g|g(t). 
G$NOTE THAT THE PAPER IN WHICH THIS G-FACTOR IS REPORTED ASSUMES THAT T=30 NS 3 (FROM 1977Ag02). YET 1987Ra20 REPORT A DIFFERENT T! ON THE OTHER HAND, THIS SAME G-FACTOR IS GIVEN BY THESE AUTHORS IN THE SAME TABLE AS THE NEW T VALUE. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T From 1975Al26, |g(t). Others: <15 min (1965Gr34), <12 min (1965Zh02) and <4 min (1966La11). These upper limits (see, e.g., 1965Zh02) come from an inability to observe a clear ingrowth of |b{++} activity from {+156}Ho in the decay of samples containing both Er and Ho. 
%A$From the sum of %|a=12|*10{+-6}~{I3} for a 3450 |a transition (1996ByZY) and %|a=5|*10{+-6}~{I2} for a 3.30-MeV |a transition (1992KaZP,1995KaZS). 2002KaZR report I{-|a}=1.0|*10{+-6} per decay for the 3450 |a. 
|D<r{+2}>(156-154)=0.26 and |D<r{+2}>(158-156)=0.29 fm{+2} (1987NeZW, obtained from graph by evaluator). 
$From an evaluation of data on nuclear rms charge radii, 2004An14 report <r{+2}>{+1/2}=5.134~fm~{I32}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+ g.s. 
MOMM1$From perturbed |g|g(|q) for recoiling nuclei in hyperfine magnetic fields (1970No01, in (HI,xn|g)). This is the value given in the evaluation by 1989Ra17. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$E2 |g to 2+, |g to 4+, and expected band structure. 
J 1975Ag02 and 2011Re06 assign 3+, while 1980Zo02 assign 4+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$Assigned as 5- by 1985AzZY (HI,xn|g), but this assignment is not adopted by the evaluator. (See the comment in the (HI,xn|g) data set.) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E$Assigned by the evaluator as a member of this band based on the systematics of octupole-related states in the adjacent N=88 nuclides (see, e.g., 1980Zo02, {+156}Tm |e decay). 
J$|g's to 0+ and 2+ levels and assumed band structure. 


level_energy_unit: KEV
level_comment:
J$Previously tentatively assigned as the 5+ member of the |g-vibrational band, but a subsequent high-spin study (2011Re06) places this band member elsewhere in the level scheme. See the comment in the {+156}Tm |e Decay data set. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$Stretched E2 to 6+ and expected band structure. |g(|q) establishes the spin sequence 9|)8 for the 531.2 |g populating this level from the 2491.4, 9- level. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J$Stretched E2 to 8+ and expected band structure. In (HI,xn|g), |g(|q) establishes the spin sequence 11|)10 for the 290.7 |g populating this level from the 2925.4, 11- level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 30+
level_comment:
E$Level not reported by 2009Pa17. These authors do not report levels in this band above 28+. 
J$|g to 28+ level and expected band structure. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (38+)
level_comment:
E$From the energy of the 36+ level and the listed E|g value. E(level)=12676.1 is listed in (HI,xn|g). 
J |g to (36+) level. 


level_energy_unit: KEV
level_spin_parity: 42+
level_comment:
J E2 |g to 40+ level and proposed band structure. 
$Band termination point. Above this level, the states are presumed (2009Pa17) to include excitations of the {+146}Gd core. 
J$State represents the full alignment of the ten valence nucleons outside the {+146}Gd core. Configuration is ((|p h{-11/2}){+4}(16+))~#[((i{-13/2}){+2}(12+))(|n f{-7/2},h{-9/2}){+4}(14+))]{-26+}. 


level_energy_unit: KEV
level_comment:
J$Assigned as the 3+ member of the |g-vibrational band by 1980Zo02, but this band member is placed elsewhere (at 1350~keV) in the level scheme in the high-spin study of 2011Re06. |g's to 2+ levels indicate J{+|p} values from 0+ to 4+. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$From the high-spin study of 2011Re06. Assigned as the 2+ member of an even-spin positive-parity band by 1980Zo02. 


level_energy_unit: KEV
level_comment:
J$Assigned as the 5+ member of the |g-vibrational band by 1980Zo02, but this band member is placed elsewhere (at 1834~keV) in the level scheme in the high-spin study of 2011Re06. |g to 4+ level indicates J{+|p} values from 2+ to 6+. 


level_energy_unit: KEV
level_comment:
J$|g to 2+ indicates J{+|p} from 0+ through 4+. ce data suggest an E0 component in this transition (1975Ag02). 


level_energy_unit: KEV
level_spin_parity: 2+,3,4+
level_comment:
J$Assigned as the 3- member of some octupole-related states by 1980Zo02, but that 3- level is placed at 1303 in the high-spin study of 2009Pa17. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T Weighted average of 33.2 ps {I17} (1969Di02), 34.7 ps {I13} (1979Bo29), and 33.5 ps {I16} (1985AzZY). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$1985AzZY assign this level as 5-. However, from the systematics of the negative-parity octupole-related states in the neighboring N=88 nuclei (see, e.g, 1980Zo02, {+156}Tm |e Decay), this energy is not consistent with that expected for the 5- state. Rather, the 1611, 5- level seen in the {+156}Tm |e decay appears to be the relevant 5- level. 


level_energy_unit: KEV
level_spin_parity: 42+
level_comment:
$Band termination point. Above this level, the states are presumed (2009Pa17) to include excitations of the {+146}Gd core. 
J$State represents the full alignment of the ten valence nucleons outside the {+146}Gd core. Configuration is (|p h{-11/2}{+4}{-16+})~#[(i{-13/2}{+2}{-12+})(|n f{-7/2},h{-9/2}){+4}{-14+})]{-26+}. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
J J measured by atomic-beam, magnetic-resonance method (1969Ek01). |p from assignment of 3/2[521] Nilsson orbital, although 3/2[651] has also been suggested. 
T From {+157}Er |e decay (1984GrZL). Others: 24 m {I+2-4} (1965Zh02), |?25 m (1966La11), and 22 m {I2} (1975AlYW). 
%EC+%B+ From extrapolation of T{-1/2}(|a) vs E{-|a} from {+153}Er, using slopes from adjacent nuclides, one gets a conservative limit of %|a < 0.02. 
MOMM1 From 1989Ra17 evaluation and 2011StZZ compilation. 
MOME2 From 1989Ra17 evaluation and 2011StZZ compilation. 


level_energy_unit: KEV
level_spin_parity: -
level_lifetime_unit: NS
level_comment:
J |p from M1 |g from 110-keV negative-parity level. 
T From {+157}Tm |e decay (1983Be17) by ce-|g(t) measurements. Other: 7 ns {I1} (1979Al33). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_uncertain: ?
level_comment:
E This value assumes that the observed 155.4-keV |g populates the ground state rather than the 10- or 35-keV level. 
J If placement of 155 |g is correct, E3 |g to 3/2- level suggests J|p=9/2+. 
T From (HI,xn|g) study (1971LeYU). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
T Weighted average of 49.0 ps {I25} (1974Na08) and 57 ps {I2} (1986Os02) ((HI,xn|g) dataset) 
MOMM1 Deduced from g-factor=0.05 {I5} (1974Na08). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (87/2-)
level_comment:
$Interpreted by 2004Ev01 as terminating state with configuration= |p(h{-11/2}{+4}){-16+}~#|n[(i{-13/2}{+2}) (h{-9/2} and/or f{-7/2}){+5}]{-55/2-} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (89/2-)
level_comment:
$Interpreted by 2004Ev01 as terminating state with configuration= |p(h{-11/2}{+4}){-16+}~#|n[(i{-13/2}{+2}) (h{-9/2} and/or f{-7/2}){+5}]{-57/2-} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (93/2+)
level_comment:
$Interpreted by 2004Ev01 as terminating state with configuration= |p(h{-11/2}{+4}){-16+}~#|n[(i{-13/2}{+3}) (h{-9/2} and/or f{-7/2}){+4}]{-61/2+} 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_uncertain: ?
level_comment:
E Value assumes that the 155-keV |g populates the ground state rather than the level at 10 or 35 keV. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 5/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$2006Ev02 incorrectly assign this state as the g.s. in their discussion in section 3 for bands 5 and 6 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
$Evaluated RMS charge radius: <r{+2}>{+1/2}=5.1761~fm~{I312} (2013An02); other: <r{+2}>=26.78 fm{+2} {I24} (1993Ba55 and 1991Ho27, both from references cited therein). 
T Weighted average of 150 min {I10} (1961Bo24), 2.25 h {I10} (1965St08), 2.4 h {I2} (1968Ab14), 2.27 h {I18} (1975Ru02,1974RuZX), 2.24 h {I10} (1982Vy06, also given as 2.24 h {I12} by 1977KaYG); other: 2.4 h (1960Dn01). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J From E2 |g to 0+ level. 
MOMM1 From 2014StZZ compilation and based on data of 1970No01; also given as |? 0.72 in 1989Ra17 evaluation based on the same data. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J From E2 |g to 8+ level and expected band structure. 
MOMM1 From g-factor=0.58 {I33} estimated by evaluator from 2001St09. 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
J From E2 |g to 12+ level and expected band structure. 
MOMM1 From g-factor=0.02 {I20} estimated by evaluator from plot of 2001St09. 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_comment:
J From E2 |g to 14+ level and expected band structure. 
MOMM1 From g-factor=0.10 {I10} estimated by evaluator from 2001St09. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (46+)
level_comment:
E 1994Si10 suggests that this yrast band terminates at this point and is fed by several weak |g's, including those of 1380, 1454, 1539, 1602, and 1657 keV. 
J From expected band structure and |g to (44+). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (23)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$|?65 for the highest level (2007Pa03), whence J |? 23 for this level based on the number of |DJ=2 transitions in this band 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T Weighted average of 236 ps {I7} (2002Sh09), 257 ps {I14} (1986Os02), and 300 ps {I15} (1969Di02) with uncertainty in 2002Sh09 value increased to 10 ps in averaging process. Values are inconsistent since the final reduced-|h{+2} is still 6.2. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T Weighted average of 13.1 ps {I3} (2002Sh09), 14.1 ps {I5} (1986Os02), and 14.4 ps {I7} (1969Di02) with reduced-|h{+2} of 2.4. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T Weighted average of 0.94 ps {I6} (2002Sh09), 0.83 ps {I16} (1986Os02), 1.1 ps {I3} (1973Wa06), and 1.2 ps {I5} (1969Di02). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T Weighted average of 0.75 ps {I8} (2002Sh09), 0.47 ps {I13} (1986Os02), and 0.8 ps {I4} (1973Wa06). 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T Weighted average of 0.51 ps {I6} (2002Sh09) and 0.4 ps {I3} (1986Os02); others: |< 0.7 ps (1973Wa06), < 0.46 ps (1988Be43). 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T Weighted average of 3.4 ps {I3} (2002Sh09), 3.0 ps {I10} (1988Be43), 2.6 ps {I3} (1986Os02), and 2.1 ps {I5} (1973Wa06) with reduced-|h{+2} of 2.1. 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_comment:
T Weighted average of 2.3 ps {I2} (2002Sh09), 1.7 ps {I5} (1988Be43), 2.5 ps {I2} (1986Os02), and 1.7 ps {I6} (1973Wa06). 


level_energy_unit: KEV
level_spin_parity: 18+
level_lifetime_unit: PS
level_comment:
T Weighted average of 0.89 ps {I14} (2002Sh09), 0.90 ps {I21} (1988Be43), and 1.1 ps {I2} (1986Os02); other: < 1.5 ps (1973Wa06). 


level_energy_unit: KEV
level_spin_parity: 20+
level_lifetime_unit: PS
level_comment:
T Weighted average of 0.46 ps {I10} (2002Sh09), 0.54 ps {I8}, (1988Be43), and 0.78 ps {I+15-13} (1986Os02). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
J$J from atomic-beam magnetic-resonance (1969Ek01); |p from |m value for |n3/2[521] Nilsson orbital (1989Be04). 
T$From 1966La11. Others:|?1 h (1961Ab06); 1.0 h {I3} (1965St08); 50~min {I15} (quoted in 1968Ab16). 
MOMM1$From the evaluation of 1989Ra17 and the compilation of 2005St24. 
MOME2$From the evaluation of 1989Ra17 and the compilation of 2005St24. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$From M1 |g to 3/2- level and expected band structure. 
T$From {+159}Tm |e decay (1983Be17). Other:|<0.20~ns (1975VaYW). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_comment:
J$From E1 |g to 7/2- level and similar low-energy 9/2+ isomers in {+161}Er, {+159}Dy, and {+151}Sm. 
CONF$Model calculations of 1979Ka16 suggest contributions from |n3/2[651] (51%), |n1/2[660] (33%), and |n5/2[642] (13%). 
T$From {+159}Tm |e decay (1975Bu10). Others: 0.31 |ms {I3} (1975St07), from {+159}Tm |e decay, and 0.32 |ms {I3}, from (HI,xn|g) (1971LeYU). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J$From M1 |g to 3/2- level, (M1) |g to 7/2- level, and expected band structure. 
T$From {+159}Tm |e decay (1983Be17). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$From (E1) |g to 5/2- level, M1 |g to 9/2+, and expected band structure. 
T$From {+159}Tm |e decay (1983Be17). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
J$From M1 |g to 9/2- level and (E2) |g to 7/2-. The small B(E2)(W.u.) to the 7/2- member of the 3/2- g.s. band indicates that this state is not a member of that band. Assigned as the |n11/2[505] bandhead (1971LeYU in HI,xn|g). 
T$Weighted average of 0.55 |ms {I15} from {+159}Tm |e decay (1975St07) and 0.60 |ms {I6} from (HI,xn|g) (1971LeYU). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J$From E2 |g to 13/2+ level and expected band structure. 
T$Weighted average of 95~ps {I5} (1974Na08) and 103~ps {I+3-4} from (HI,xn|g) (1986Os02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
J$From E2 |g to 17/2+ level and expected band structure. 
T$Weighted average of 8.2~ps {I9} (1974Na08) and 9.8~ps {I+7-8} (1986Os02) from (HI,xn|g). 
MOMM1$From the evaluation by 1989Ra17, based on data of 1980Sp03. See also the compilation by 2005St24. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: US
level_comment:
E$From 1971LeYU 
J$From 1971LeYU, based on analogy with the {+157}Er level scheme. 
T$From 1971LeYU, from ce(t) between beam pulses. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: US
level_comment:
J$Shown in 1987De18 as part of the |n3/2[521] g.s. band, but the B(E2)(W.u.) value for the transition to the 7/2- member of the g.s. band does not support this. Most reasonably assigned as the bandhead of |n11/2[505], as assigned in 1971LeYU. 
T$From 1971LeYU, from ce(t) between beam pulses. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 21/2+
level_lifetime_unit: PS
level_comment:
$g-factor|<0.07, from 1980Sp03. 
T$Weighted average of 8.2~ps~{I9} (1974Na08) and 9.8~ps~{I+7-8} (1986Os02). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
|D<r{+2}>({+160}Er-{+150}Er)=1.30 fm{+2}, estimated by the evaluator from the figure given in 1985Ne09. This same information, in graphical format, is given in a number of publications by this group. In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.2045 fm {I336}. 
T deduced from |g(t) measurements of 197|g from {+160}Ho(5.02-h) daughter in equilibrium with parent (1970Ka23). Other measurements: 1954Mi16, 1955Ne03, 1957Dz60, 1957Go72, 1958Pa16, 1961Bj02, 1963Ra15, 1966La11. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 transition to g.s. 
T other: 850 ps {I150}, from {+160}Tm |e decay (1978Ad03). These authors also mention the value T{-1/2}=919 ps {I46}, given in a 1972 monograph from another group. 
MOMM1$From the compilation of 2014StZZ by perturbed angular correlation method (measured by 2005Wo06) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J collective E2 transition to 2+ first excited state. Member of g.s. band 
MOMM1$From the compilation of 2014StZZ by recoil into gas or vacuum method (measured by 1970No01; see discussion of the experimental considerations underlying these data). g-factors for the g.s. band members are approximately constant up through the 8+ state 1989Ra17. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J collective E2 transition to 4+ member of g.s. band. Energy spacings indicate that this is the 6+ member of the g.s. band. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$E0 |g to 0+ g.s. This, together with the relatively low excitation energy, strongly suggests that this is the bandhead of the first excited K|p=0+ band. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
J |g's only to 2+ and 4+ members of g.s. band require J|p=2+, 3, or 4+. Relative I|g values, location of state in the level scheme and E2 character of transition to 2+ member of g.s. band strongly suggest that this is the 3+ member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J 1983Si20 suggest this state may be the 4+ member of the |g-vibrational band. M1+E2 |g to 4+ and log| {Ift}=6.6 from J=5 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J collective E2 transition to 6+ member of the g.s. band and energy spacing indicate that this is the 8+ member of the g.s. band. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$E0+M1+E2 |g to 4+. 1983Si20 suggest that this may be the 4+ member of the first excited K|p=0+ band. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$M1+E2 transition to 4+ state indicates J|p=3+, 4+, or 5+; 2006Du02 in (HI,xn|g) dataset assign 5+ as for member in the |g-vibrational band 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_comment:
J$|DJ=1, D |g's from this and 2151 second level of this band to 6+ of g.s. determine J=5 for this level (band head) and J=7 for 2151. |p=(-) based on assigned configurations. 


level_energy_unit: KEV
level_spin_parity: 7(-)
level_comment:
J$|DJ=1, D |g's from 1756 band head and from this level to 6+ of g.s. band determine J=5 for 1756 and J=7 for this level. |p=(-) based on assigned configurations. 


level_energy_unit: KEV
level_spin_parity: (10+)
level_comment:
J$|g's to 9(-),10(-) and |p=(+) (based on assigned configurations) select the most likely J|p values equal to (9+),(10+); (10+) from |DJ=(1) interband transition from (11+) 


level_energy_unit: KEV
level_spin_parity: (11+)
level_comment:
J$|g's to 10(-),11(-) and |p=(+) (based on assigned configurations) select the most likely J|p values equal to (10+),(11+); (11+) is postulated by 2011Ol02 ((HI,xn|g) dataset) 


level_energy_unit: KEV
level_spin_parity: (13+)
level_comment:
$J=(13) compatible with |g to 12+, assigned in (HI,xn|g) (2011Ol02) based on the fact that if J>13 this band would become yrast at higher spins, which is contrary to the observed intensities. |p=(+) based on assigned configurations. 


level_energy_unit: KEV
level_spin_parity: (14+)
level_comment:
$J=(14) compatible with |g to (13+), assigned in (HI,xn|g) (2011Ol02) based on the fact that if J>14 this band would become yrast at higher spins, which is contrary to the observed intensities. |p=(+) based on assigned configurations. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$adopted value; possible bandhead of the first excited K|p=0+ band. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J J from atomic-beam magnetic resonance (1969Ek01) and |p from agreement of the measured |m with the value calculated for the assigned Nilsson orbital (1974Ba18, see also 1989Be04). 
T from {+161}Er |e decay, weighted average of 3.24 h {I4} (1972Wo08), 3.1 h {I1} (1963Ra15), 3.1 h {I1} (1961Gr25), 3.2 h {I1} (1961Bj02), 3.4 h {I2} (1960Da23), and 3.17 h {I17} (1960Dn02). Others: 3.5 (1954Mi01) and 3.05 (1955Ne01). 
MOMM1 from 1989Ra17 evaluation and based on data from 1985 Proc. Symp. on Quantum Electronics, Bombay, India; other: -0.369 {I3} from 1989Ra17 evaluation and based on data of 1972Ek03. The compilation by 2005St24 lists both values. 
MOME2 from 1989Ra17 evaluation and based on data of 1972Ek03; other: +1.35 {I2} 1989Ra17 evaluation and based on data from 1985 Proc. Symp. on Quantum Electronics, Bombay, India. The compilation by 2005St24 lists both values. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J from M1 component in |g to 3/2- level and expected band structure. 
T from {+161}Tm |e decay (1983Be17,1981AbZU); other: |<0.17 ns from {+161}Tm |e decay (1975VaYW,1979AlZU). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J from E2 |g to 3/2- level and expected band structure. 
T from {+161}Tm |e decay (1983Be17,1981AbZU,1980FrZQ); other: |<0.2 ns from {+161}Tm |e decay (1979AlZU). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J from M1 components in |g's to 3/2- and 7/2- levels 
T from {+161}Tm |e decay, combination of 0.25 ns {I4} (1983Be17,1981AbZU) and 0.45 ns {I5} (1979AlZU). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J from E1 |g to 7/2- level and agreement of experimental and calculated (d,t) cross sections. 
T from {+161}Tm |e decay, combination of 93 ns {I4} (1975Bu10) and 74 ns {I3} (1979AlZU). Others: 70 ns {I20} from (|a,xn|g) (1970Hj02) and 70 ns (1972AnZL). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: NS
level_comment:
J from E1 |g's to 5/2- and 7/2- levels and M1 component in |g to 9/2+. 
T from {+161}Tm |e decay (1983Be17,1981AbZU). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J from E2 |g to 3/2- level, M1 to 7/2-, and expected band structure. 
T from {+161}Tm |e decay (1983Be17,1981AbZU); other: |<0.30 ns from {+161}Tm |e decay (1979AlZU). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: NS
level_comment:
J from E2 |g to 9/2+ level and expected band structure. 
T from {+161}Tm |e decay, average of 1.9 ns {I2} (1983Be17,1981AbZU) and 2.2 ns {I2} (1979AlZU). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J E1 |g to 3/2- level and M1 to 5/2+ indicate J{+|p}=3/2+,5/2+. Large (d,t) cross section indicates presence of 3/2+,3/2[402]. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J from E2 |g to 7/2- level and E1 to 13/2+. 
T from {+161}Er IT decay (1970Bo02). Other: 8 |ms (1972AnZL) and, from in-beam study, 8.0 |ms (1969BoZL). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J E1 |g to 3/2- level and M1 to 5/2+ indicates J|p=3/2+,5/2+. Large value of this (d,t) cross section indicates presence of 3/2+,3/2[402]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_uncertain: ?
level_comment:
E level proposed (1970Bo02) to allow decay of 267- and 297-keV levels; existence of level is established in |e decay of {+161}Tm. 
J from Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2+
level_comment:
E level proposed (1970Bo02) to allow decay of 397-keV level by an observed |g; existence of level is established in |e decay of {+161}Tm and in-beam studies. 
J from Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2+
level_comment:
E level proposed (1970Bo02) to allow decay of 397-keV level by an observed |g; existence of level is established in |e decay of {+161}Tm. 
J from Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J Possible K|p=9/2+ bandhead. Probable conf is |p7/2[404]+|p7/2[523]-|n5/2[523], from population via an allowed-unhindered |e transition from |p7/2[404]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$(d|s/d|W),=5 
J levels at 212 and 217 are assigned as 5/2+ and 7/2+ members of the mixed positive-parity band in Adopted Levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$(d|s/d|W),=50 
J assigned as 7/2,5/2[523] plus the 13/2 member of the positive-parity band by 1969Tj01 and in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J$From {+161}Er Adopted Levels in the ENSDF database (June 2011 update) 
T$Measured by 2016Ba65 from decay curve for 314.71-keV |g ray, counted for |?20 half-lives. Value is 3.21 h {I3} in {+161}Er Adopted Levels in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T from a cluster-model calculation, 2004Xu02 estimate T{-1/2}(|a)=2.8|*10{+29} y. See, also, 1988Al13 and 1956Po16 for discussions of the |a-decay half-life. 
T using the pseudo SU(3) model, 1999Ce12 compute a value of 2.85|*10{+22} y for the half-life of the 2|e2|n decay to the g.s. of {+162}Er. Subsequently, this same value is given in 2002Hi09, a work by some of the same authors. 2004Su27 discuss the neutrinoless 2|e decay of {+162}Er. 
In an evaluation of nuclear rms charge radii, 2013An02 report <r{+2}>{+1/2}=5.225 fm {I4}. 
|D<r{+2}> results (in fm{+2}) are: for {+160}Er-{+162}Er, |D<r{+2}>|? 0.15 (1985Ne09) and for {+162}Er-{+164}Er, |D<r{+2}>|?0.144 (1985Be34), |? 0.10 (1985Ne09), 0.143 (1987Ah03), and 0.15 (1987Ok03). Values of 1985Ne09 and 1987Ok03 were taken from plots by the evaluator. For calculations of these values see 1988SuZW. For other isotope shift data, see 1965Ha11, 1965Vo02, 1967Ca21, and 1986Ch07. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J from E2 |g to 0+ level. 
T$from weighted average lifetime, |t=2004 ps {I30}, of the following measured |t values: 2040 ps {I30} (2020Kn03, from time distribution curve, see {+154}Sm({+12}C,4n|g) dataset); 2200 ps {I400} (from |b|g(t) in 2003Ca03); 1985 ps {I25} (from B(E2)|^=5.01 {I3} in 1977Ro27); 1690 ps {I150} (from ce-|g(t) in 1970Mo39); 2036 ps {I104} (from B(E2)|^=4.89 {I25} in 1963Bj04). 
MOME2$from the compilation of 2016St14 and based on data of 1981Hu02. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
BE4 computed from the E4 matrix element of 0.16 {I+16-26} in Coul. ex. (1977Ro27). 
J E2 |g to 2+. Level energy consistent with that expected for the 4+ member of the g.s. band. 
T$mean lifetime |t=87 ps {I6} (2020Kn03) in {+154}Sm({+12}C,4n|g) dataset 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J |g to 4+ level and population in Coul. ex. Energy is consistent with that expected for the 6+ member of the g.s. band. 
T$mean lifetime |t=9 ps {I6} (2020Kn03) in {+154}Sm({+12}C,4n|g) dataset 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J from |g to 0+ level and direct population in Coul. ex. 
T computed from B(E2)|^=0.164 {I8} (Coul. ex.) and the adopted |g branching. 
MOME2$from the compilation of 2016St14 and based on Coulomb excitation reorientation data (1983Hu01). 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J from E2 |g to 2+ level, |g to 4+. Energy consistent with that of the 3+ member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J |g to 6+ member of the g.s. band. Energy is consistent with that expected for the 8+ member of the g.s. band. Also, from |g(|q) in {+165}Ho(p,4n|g) (1977Ja06). 
T$mean lifetime |t<5 ps (2020Kn03) in {+154}Sm({+12}C,4n|g) dataset 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J |g's to 0+ and 4+ levels. E0 component in the |g transition to a 2+ level. 
T computed from B(E2)|^=0.042 {I7} (Coul. ex.) and the adopted |g branching. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (4+)
level_comment:
J energy consistent with that expected for the 4+ member of the proposed first-excited K|p=0+ band. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J |g's to 2+ and 3+ levels suggest J|p=1+,2-. 2002Ca35, in {+162}Tm |e decay, suggest J|p=2-, based on the occurrence of K|p=2- octupole bands in several neighboring nuclei. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E0 component in |g transition to 2+. 
T computed from B(E2)|^=0.018 {I8} (Coul. ex.) and the adopted |g branching. 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J M1 component in |g to 6+, |g's to 4+ and |g(|q). Energy consistent with that expected for the 6+ member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J |g to 4+ and |g(|q). Energy consistent with that expected for the 5- member of the associated band. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J from |g's to 0+ and 3+ levels. Possible population in Coul. ex. makes 0+ unlikely. 
T from B(E2)|^<0.022 (Coul. ex.) and the adopted |g branching, one computes T{-1/2}>0.32 ps, but the B(E2) may be influenced by multistep processes. 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J |g's to 0+ and 2+ levels. This argument also allows 1+ and 2+ assignments, but assignment as the K|p=1- bandhead supports 1-. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J |g deexcitation and |g(|q) in {+165}Ho(p,4n|g) agree with the listed J value, but other values are allowed. This assignment is that proposed by 1977Ja06 in {+165}Ho(p,4n|g) from consideration of the expected octupole-band structure. 


level_energy_unit: KEV
level_spin_parity: 10+
level_comment:
J |g to 8+ level and |g(|q). Energy consistent with that expected for the 10+ member of the g.s. band. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
BE3 from 1982Ro07, Coul. ex. 
J from (d,d') cross-section ratios and |g's to 0+, 2+, and 4+ levels. The |g to 0+ may suggest the presence of two levels. 
T from B(E3)<0.072 in Coul. ex. and the adopted |g branching. 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
J M1 component in transition to 6+, |g's to 5+ and 8+, and |g(|q). Energy consistent with that expected for that of the 7+ member of the |g-vibrational band. 


level_energy_unit: KEV
level_spin_parity: 7(-)
level_comment:
J |g(|q) and |g to 6+. Energy consistent with that expected for the 7- member of the associated band. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$from |g's to 2+, 3+, and 4+ levels and log| {Ift} |? 4.6 for the |e transition from 24 s {+162}Tm (J|p=5+). This fast |e transition establishes the presence of the 5/2[523] neutron orbital as a component in this state. The dominant configuration is most likely (|n 5/2[523])+(|n 3/2[521]). 1994Bu16 assign this state as a hexadecapole vibration. 


level_energy_unit: KEV
level_spin_parity: 7(-)
level_lifetime_unit: NS
level_comment:
J$|g's to 6+ and 8+ levels, |g(|q). Level energy and decay path are similar to that of a 7(-) 1985-keV isomer in {+164}Er ({+9}Be) (2012Sw01) 
T$half-life |t=76.7 ns {I39}, weighted average of 76 ns {I4} (2020Kn03, {+12}C) and 88 ns {I16} (2012Sw01, {+9}Be) 
$configuration=|p7/2[523]~#|p7/2[404] (BCS calculations ({+9}Be), 2012Sw01) 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J |g to 8+ and stretched E2 to (6-). Energy consistent with that of the 8- member of this level sequence. 


level_energy_unit: KEV
level_spin_parity: 9+
level_comment:
J |g's to 7+, 8+, and 10+ levels. Energy consistent with that expected for the 9+ member of the indicated 2+ band. 


level_energy_unit: KEV
level_spin_parity: 12+
level_comment:
J E2 |g to the 10+ member of the g.s. (yrast) band. Energy consistent with that expected for the 12+ member of this band. 


level_energy_unit: KEV
level_spin_parity: (10-)
level_comment:
J |g to 10+ and stretched E2 to (8-). Level energy consistent with that of the 10- member of this level sequence. 


level_energy_unit: KEV
level_spin_parity: 14+
level_comment:
J |g to 12+, |g(|q). Energy consistent with that expected for the 14+ member of the g.s. (yrast) band. 


level_energy_unit: KEV
level_spin_parity: 13-
level_comment:
J E1 |g to 12+ and |g to 11-. Energy consistent with that expected for the 13- member of the associated band. 


level_energy_unit: KEV
level_spin_parity: (12-)
level_comment:
J stretched E2 to (10-). Level energy consistent with that of the 12- member of this level sequence. 


level_energy_unit: KEV
level_comment:
J |g's to 1-, 3-, 2+, 3+, and (0+) levels suggest J|p=2+, but if the (0+) assignment to the 2114 level is not correct, J|p could also be 2- or 3-. 


level_energy_unit: KEV
level_spin_parity: 16+
level_comment:
J |g to 14+, |g(|q). Energy consistent with that expected for the 16+ member of the g.s. (yrast) band. 


level_energy_unit: KEV
level_spin_parity: 18+
level_comment:
J |g to 16+, |g(|q). Energy consistent with that expected for the 18+ member of the g.s. (yrast) band. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 20+
level_comment:
J |g to 18+, |g(|q). Energy consistent with that expected for the 20+ member of the g.s. (yrast) band. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$adopted value. Measured in this dataset: 1.17 ns {I10}, ce|g(t) coin (1970Mo39); and 1.5 ns {I3}, |b|g coin (2003Ca03). For a summary of the T{-1/2} measurements, see the Adopted Levels data set. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
Bandhead of a K|p=4+ band. log| {Ift} |? 4.6 for the |e transition from the 5+ level in {+162}Tm establishes the presence of the neutron orbital 5/2[523] in this state. The dominant configuration is (|n 5/2[523]+|n 3/2[521]). 1994Bu16 propose that this state is a hexadecapole vibration. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
BE2 from 1977Ro27. Other: 4.89 {I25} (1963Bj04). 
BE2 The value 4.89 25 is also given by 1963El06. 
T computed by the evaluator from the listed B(E2) value and |a=2.73. In the calculation, an uncertainty of 1.4% in the |a value was assumed. For other values of T{-1/2}, see the Adopted Levels data set 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$from 1982Ro07 (for 900.7|g) 
T computed by the evaluator from the listed B(E2) value and the adopted |g branching. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$from 1982Ro07. 
T computed by the evaluator from the listed B(E2) value and the adopted |g branching. The possible contribution of multistep processes to the measured B(E2) value has been considered by 2002Ca35, in {+162}Tm |e decay (21.70 min), and been estimated to be small (<10%). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 from 1982Ro07. 
T computed by the evaluator from the listed B(E2) value and the adopted |g branching. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=2040 ps {I30} (2020Kn03), from time distribution curve for LaBr{-3}(Ce) gates on the 227, 4{++}|)2{++} and 102 2{++}|)0{++} transitions. B. Singh analysis: weighted this value can be compared with literature values of mean lifetime |t=2.2 ns {I4} (from |b|g(t) in 2003Ca03); 1985 ps {I25} (from B(E2)|^=5.01 {I3} in 1977Ro27); 1.69 ns {I15} (from ce-|g(t) in 1970Mo39); 2036 ps {I104} (from B(E2)|^=4.89 {I25} in 1963Bj04). Weighted average of the literature results is 1981 ps {I29}. Weighted average of the first three literature values is 1978 ps {I35}. It appears that T{-1/2}=1.29 ps {I6} (or |t=1861 ps {I87} in ref. 38 of 2020Kn03 - 2007Re16 evalution) quoted as the weighted average of the first three literature values, is erroneous. (NN): Indeed, the correct weighted average is T{-1/2}=1.37 ps {I6} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=87 ps {I6} (2020Kn03) obtained from data for the 6{++}|)4{++}|)2{++} cascade, with additional HPGe gate on the 8{++}|)6{++} transition in two arrangements: LaBr gate on 4{++}|)2{++}, HPGe gate on 8{++}|)6{++}; and LaBr gate on 6{++}|)4{++}, HPGe gate on 8{++}|)6{++}. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t=9 ps {I6} (2020Kn03) obtained from data for the 8{++}|)6{++}|)4{++} cascade, with additional HPGe gate on the 4{++}|)2{++} transition in two arrangements: LaBr gate on 6{++}|)4{++}, HPGe gate on 4{++}|)2{++}; and LaBr gate on 8{++}|)6{++}, HPGe gate on 4{++}|)2{++}. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$mean lifetime |t<5 ps, estimated based on the uncertainty of the Prompt Response Difference (PRD) curve, where PRD is the difference between the centroids of the Prompt-Response-Function (PRF) for the delayed and anti-delayed time distribution. 


level_energy_unit: KEV
level_spin_parity: 7(-)
level_lifetime_unit: NS
level_comment:
T$half-life of 76 ns {I4} measured by 2020Kn03 from 1359|g(t). B. Singh: It can be compared with 88 ns {I16} from 2012Sw01 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
MOMM1,MOME2$ atomic beam; Q includes Sternheimer correction. 
J$ spin from atomic beam (1969St05,1969Ek01). Parity: log {Ift}=5.33 {I2} to 1801.56 level from 1/2+ parent; the 1801.56 level decays by E1-E2 cascade to the g.s.; "finger-print" method of measured and predicted cross sections in (d,t) and (d,p); measured |m consistent with calculated |m=+0.66 for |n5/2[523], |b{-2}=0.2. 
T$weighted average of 75.1 min {I4} (1963Pe16) and 73 min {I2} (1965St08). Others: 1963Gr14, 1961Bj02, 1960Bu27, 1953Ha43, 1951Bu25 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: US
level_comment:
J$|DJ=1 |g to 9/2-, |g's to 11/2+ and 11/2- and |s(|q) in (d,t). Systematics of odd-A Gd nuclides and N=95, 11/2-,|n11/2[505] states support this assignment. 
T$|g|g(t) in (|a,2n|g) (1974An04) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$E1 |g to 3/2-, (E2) |g to 7/2+ and log| {Ift}=7.2 from 1/2+. Agreement of |s(exp)/|s(predicted) in (d,t) and weak population in (d,p) is characteristic of a hole state. Dominant configuration is 3/2[402]. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$E2 |g to 5/2+, log| {Ift}=6.9 from 1/2+. Agreement of |s(exp)/|s(predicted) in (d,t) and weak population in (d,p) is characteristic of a hole state. Configuration=|n1/2[400]. 


level_energy_unit: KEV
level_spin_parity: (15/2-)
level_comment:
J$Based on a comparison of experimental and calculated (K-allowed and K-hindered) reduced transition (E2) probabilities and K|p=19/2- for the 1845 bandhead, 1994Br09 deduce K|p=15/2- for the 1297 bandhead. 1994Br09 state that coupling between the available orbitals does not produce J|p=15/2-. However, a K+2 |g vibration built on |n11/2[505] would have 15/2- in its ground state 
T$1 ns to 75 ns |g|g(t) (1994Br09) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$E1 |g to 5/2-, log| {Ift}=5.5 from 1/2+ 
$Probable configuration=(|n5/2[523])(|p7/2[523])(|p1/2[411]) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
T$1 ns to 75 ns from |g|g(t) (1994Br09) 
J$Based on decay modes, Routhian calculations and calculated transition rates (B(M1)/B(E2)) using a tilted-axis cranking model, the best predicted configuration (1994Br09) is |n5/2[642] coupled to the 7- proton state formed by (|p7/2[523])+(|p7/2[404]) in {+164}Er (1994Br09). No signature splitting is observed. 


level_energy_unit: KEV
level_spin_parity: (19/2+)
level_comment:
T$1 ns to 75 ns from |g|g(t) (1994Br09) 
J$Based on decay modes, Routhian calculations and calculated transition rates (B(M1)/B(E2)) using a tilted-axis cranking model, the best predicted configuration (1994Br09) is |n5/2[523] coupled to the 7- proton state (|p7/2[523])+(|p7/2[404]) in {+164}Er. But, the configuration (|n11/2[505])(|n5/2[523])(|n3/2[521]), giving K|p=19/2-, is not ruled out (1994Br09). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
E$from E|g. Level held fixed in least-squares analysis 
T$weighted average of 8.8 ns {I5} (1969Ve05,|g|g(t)) and 7.7 ns {I6} (1974An04,|gce(t)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T$ce|g(t) (1974An04) 
$1970BaYN, 1972Af03, 1976AlZW and 1994MoZY probably refer to the same measurement as in 1974An04 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 5/2+
level_comment:
$d|s/d|W=1 {IAP} 
J$from adopted levels. 1969Tj01 tentatively propose this as 7/2+ member, but 7/2+ is inconsistent with |g-ray data 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
$d|s/d|W=25 
J$|s(|q) consistent with 9/2+,|n5/2[642], although the experimental cross section is somewhat larger than predicted 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$d|s/d|W=1 {IAP} 
$The 5/2- member of the |n3/2[521] band is not predicted to be populated with an observable intensity. The observed weak group may be due to Coriolis coupling between the |n3/2[521] and |n5/2[523] orbitals 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$d|s/d|W=103 
J$this level may be mixed with the K-2 |g-vibrations built on the levels with the following configurations: |n3/2[521] and |n5/2[523] (1971Bu16,1969Tj01). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$d|s/d|W=33 
J$ weaker population in (d,p) than in (d,t) implies a hole state, thus supporting |n3/2[402] 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$d|s/d|W=35 
J$ weaker population in (d,p) than in (d,t) implies a hole state, thus supporting |n1/2[400]. Expected to be mixed with |n1/2[660] by a |DN=2 interaction 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$d|s/d|W=156 
$|s(|q) pattern is consistent with L=3, possibly 7/2-, but measured cross section is only 44% of the predicted value 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$d|s/d|W=21 
J$|s(|q) indicates low L-transfer and cross section is consistent with that predicted for 3/2-,|n1/2[530] 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 5/2+
level_comment:
$d|s/d|W=4 {IAP} 
J$from adopted levels. 1969Tj01 tentatively propose this as 7/2+ member, but 7/2+ is inconsistent with |g-ray data 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
$d|s/d|W=53 
J$|s(|q) consistent with 9/2+,|n5/2[642], although the experimental cross section is somewhat larger than predicted 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$d|s/d|W=198 
$Experimental cross section is much higher than predicted, probably due to Coriolis coupling of low-lying negative parity bands. The band assignment, however, seems firm 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$d|s/d|W=47 
J$this level may be mixed with the K-2 |g-vibrations built on the levels with the following configurations: |n3/2[521] and |n5/2[523] (1971Bu16,1969Tj01). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$d|s/d|W=39 
J$comparison of coupled-channel predictions (1984Pe03) agrees with |s(|q) data (of 1969Tj01 at three angles) consistent with the |n11/2[505] assignment to this level. Predicted/experimental d|s/d|W (90|')=82/95. The latter includes contribution from the 5/2 member of the |n1/2[521] band 
$Occupation number(V{+2})=0.68 {I14}, emptiness number(U{+2})<0.14 (1984Pe03, CCBA) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$d|s/d|W=172 
J$ weaker population in (d,p) than in (d,t) implies a hole state, thus supporting |n3/2[402]. Predicted/experimental d|s/d|W (90|')=612/450. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$d|s/d|W=207 
J$ weaker population in (d,p) than in (d,t) implies a hole state, thus supporting |n1/2[400]. Predicted/experimental d|s/d|W (90|')=780/602. Expected to be mixed with |n1/2[660] by a |DN=2 interaction. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$d|s/d|W=63 
J$|s(|q) indicates low L-transfer and cross section is consistent with that predicted for 3/2-,|n1/2[530] 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$The rms charge radius (<r{+2}>){+1/2}: 5.2389 fm {I35} (2013An02 evaluation). See also 2009An12 for trends in nuclear radii 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
MOMM1$Mossbauer effect (1968Mu01). Other: 0.686 {I16} (transient-field integral PAC method,1996Br09) 
MOME2$reorientation method (1981Hu02) 
J$E2 |g to 0+ 
T$from 2016Pr01 evaluation, based on |g|g(t) and |b|g(t) in {+164}Ho decay, (ce)|g(t) in {+164}Tm decay, and B(E2) in Coulomb excitation. Measured values are: B(E2)=5.48 {I4} (1977Ro27), 5.04 {I35} (1960El07); mean lifetimes |t=2.140 ns {I120} (1970Mo39), 2.190 ns {I90} (1968Se02), 2.060 ns {I70} (1963Fo02), 2.499 ns {I46} (1963De21), 2.020 ns {I720} (1954Br96). 
MOMM1$Mossbauer effect. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
MOMM1$IPAC method (1997Al25). Other: +1.36 {I8} from transient-field method (1996Br09) 
J$stretched E2 |g to 2+ 
T$from microwave beam pulsing method (1968Be29). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field integral PAC method 
MOME2$reorientation method in Coulomb excitation (1983Hu01) 
J$E2 |g to 0+ 
T$from B(E2) (1982Ro07) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field integral PAC method 
J$stretched E2 |g to 6+ 
T$Doppler-broadened line shape in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field integral PAC method 
T$from Doppler-broadened line shape and Coul. ex. (1977Ke06,1980Ya03). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$|g|g(t) (1973Ch28) in {+164}Tm |e decay (5.1 min). 
J$E1 |g to 6+; |g to 4+. Configuration=|n5/2[523]~#|n5/2[642], K|p=5- 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
J$M1 |g to 6-; E2+M1 |g to 7-; 6- rejected by |g to 8+ and RUL; also log| {Ift}=5.0 from 6- parent. Configuration=|p7/2[523]~#|p7/2[404] 
T$weighted average of 22.7 ns {I17}, 23.3 ns {I16} in {+164}Tm |e decay (5.1 min) and 21.6 ns {I15} in (|a,2n|g) 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from B(E2)|_(620|g)=2.3 {I3} in Coul. ex. (1980Ya03), assuming 100% branch for 620|g 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from B(E2)|_(549|g)=1.5 {I7} in Coul. ex. (1980Ya03), assuming 100% branch for 549|g 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=2, E2 |g to 14+ 
T$deduced by evaluators from B(E2)|_(561|g)<2.8 in Coul. ex. (1980Ya03) and using the |g-branching ratios for 388|g and 561|g 


level_energy_unit: KEV
level_spin_parity: 14+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from B(E2)|_(534|g)=1.9 {I9} in Coul. ex. (1980Ya03), assuming 100% branch for 534|g 


level_energy_unit: KEV
level_spin_parity: (12+)
level_lifetime_unit: NS
level_comment:
$4-qp state with configuration=|n(5/2[523],5/2[642])~#|p(7/2[523],7/2[404]) 
T$555|g(t) (2012Sw02). Other: |>170 ns (1997Ba63) 


level_energy_unit: KEV
level_spin_parity: 16+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from B(E2)|_(709|g)=1.5 {I3} in Coul. ex. (1980Ya03), assuming 100% branch for 709|g 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: NS
level_comment:
T$average of 22.7 ns {I17} (1971De22) and 23.3 ns {I16} (1973Ch28) 
$Configuration=|p7/2[404]~#|p7/2[523] 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$From relative |g-branching ratios, a 967.8|g should have been seen in (|a,2ng) with expected intensity of 4.4 units 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$(3+), and assigned as member of |g band in 1982Bo39, is incorrect as there is |g to 0+ g.s. J|p=1- in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
From measured |g-ray yields for heavy and light projectiles, 1981Hu02 propose the intrinsic shape as prolate 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOME2$reorientation effect (1983Hu01) 
T$from B(E2) (1982Ro07) and branching ratio from 1983Hu01 
BE2$other: 0.18 {I5} (1965Yo04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$Doppler-broadened line shape. Weighted average of 2.63 ps {I20} (1977Ke06) and 2.56 ps {I12} (1980Ya03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
T$from Coul. ex. Weighted average of 0.98 ps {I5} (1977Ke06, Doppler broadening); 1.01 ps {I6} (1980Ya03, Doppler broadening); and 1.11 ps {i10} (1980Ya03, from B(E2)|_(493.4|g)=1.70 {I16}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 12+
level_lifetime_unit: PS
level_comment:
T$from Coul. ex. Unweighted average of 0.82 ps {I8} (1977Ke06, Doppler broadening); 0.55 ps {I4} (1980Ya03, Doppler broadening); and 0.52 ps {i5} (1980Ya03, from B(E2)|_(564.7|g)=1.89 {I19}) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T$|b|g(t). Weighted average of 1.4 ns {I5} (1954Br96), 1.43 ns {I5} (1963Fo02), 1.52 ns {I6} (1968Se02). Other: 1963De21. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: H
level_comment:
J$spin from atomic beam (1964Bu09); parity from log| {Ift}=4.7 to 7/2- 
T$weighted average of 10.39 h {I7} (1963Zy01), 10.34 h {I5} (1963Ry01), 10.4 h {I1} (1963Ra15), 10.3 h {I2} (1965St08). Others: 1963Sc18, 1961Bj02, 1960Wi10, 1960Bu27, 1958Gr03, 1957Go78, 1952Ku15, 1950Wi16, 1950Bu85 
MOMM1,MOME2$collinear fast beam LASER spectroscopy (1987OtZW). Other: |m=0.65 {I3}, Q=2.2 {I1} (atomic beam,1965Al10). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: NS
level_comment:
T$others from {+165}Tm |e decay: 3.25 ns {I20} (1964Ja09), 4.4 ns {I7} (1970Ba71) 
J$E1 |g to 5/2-; E1 |gs from 7/2- and 3/2- 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J$E2 |g to 7/2-; L(d,t)=1 
MOMM1$from 1978EgZY, probably perturbed angular correlation method. No value is listed in 2020StZV 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
T$other: |<1.0 ns (1970BaYN) 
J$297|g E2 (from ce data) to 5/2-, 54.4|g M1(+E2) to 3/2-; L(d,t)=1 from 0+; 1/2- from measured intensity pattern, |s(|q) in (d,p); 54.4|g|g(|q) in {+165}Tm |e decay is consistent with J=1/2 (1988Ul02) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LE
level_comment:
J$589.9|g E2 (from ce data) to 5/2-; 346.9|g M1(+E2) to 3/2-; |g|g(|q) in {+165}Tm |e decay is consistent with spin=1/2 (1988Ul02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$531.2|g E2 (from ce data) to 7/2-; 365.6|g M1+E2 to 3/2-; only spin=3/2 with a small |d from 312|g|g(|q) in {+165}Tm |e decay (1988Ul02) is consistent with Mult=M1 for 312|g from measured ce data. 


level_energy_unit: KEV
level_spin_parity: (19/2,21/2)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from 799.8|g(t) (2012Sw01) in {+160}Gd({+9}Be,4n|g):E=57 MeV 
J$Possible configurations=|n5/2[523]~#|p7/2[523]~#|p7/2[404] for J|p(1823 level)=19/2+; |n5/2[642]~#|p7/2[523]~#|p7/2[404] for J|p(1823 level)=19/2-; |n7/2[633]~#|p7/2[523]~#|p7/2[404] or |n11/2[505]~#|n5/2[523]~#|n5/2[512] for J|p(1823 level)=21/2-, proposed in {+160}Gd({+9}Be,4n|g):E=57 MeV (2012Sw01) 


level_energy_unit: KEV
level_spin_parity: 29/2+
level_uncertain: ?
level_comment:
E$this level is not included in the Adopted Levels, Gammas dataset, as 29/2+ member of this band is identified at 1610.7 level in {+160}Gd({+9}Be,4n|g),E=42,45 MeV (2011Wa19) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$J=5/2, |n5/2[523] (1969Tj01) 
$L=3 in 1979Ja23 
$d|s/d|W (|mb/sr): 30 (60|'), 34 (90|'), 17 (125|') (1969Tj01) 
$d|s/d|W (30|')=50 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 1 (20|'), 3 (25|'), 5 (30|'), 6 (35|'), 10 (40|'), 12 (45|'), 20 (50|'), 30 (60|'), 32 (75|'), 34 (90|'), 27 (105|'), 17 (125|'), 9 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$J=5/2, |n5/2[642] for a 48 level (1969Tj01) 
$d|s/d|W (|mb/sr): 8 (60|'), 3 (90|'), 2 (125|') (1969Tj01) 
$d|s/d|W( 30|')=33 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$J=7/2, |n5/2[523] for a 76 level (1969Tj01) 
$d|s/d|W (|mb/sr): 11 (60|'), 16 (90|'), 9 (125|') (1969Tj01) 
$d|s/d|W (30|')=32 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 1 (25|'), 3 (30|'), 13 (35|'), 17 (40|'), 29 (45|'), 37 (50|'), 53 (60|'), 70 (75|'), 71 (90|'), 62 (105|'), 37 (125|'), 25 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$J=9/2, |n5/2[642] for a 98 level (1969Tj01) 
$L=4 in 1979Ja23 for 98 level 
$d|s/d|W (|mb/sr): 53 (60|'), 71 (90|'), 37 (125|') (1969Tj01) 
$d|s/d|W (30|')=110 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$J=9/2, |n5/2[523] for a 176 level (1969Tj01) 
$L=5 in 1979Ja23 for 176 level 
$d|s/d|W (|mb/sr): 15 (60|'), 33 (90|'), 27 (125|') (1969Tj01) 
$d|s/d|W (30|')=35 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 1 (30|'), 1 (35|'), 3 (40|'), 6 (45|'), 10 (50|'), 15 (60|'), 27 (75|'), 33 (90|'), 35 (105|'), 27 (125|'), 21 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$J=3/2, |n3/2[521] for a 242 level (1969Tj01) 
$L=1 in 1979Ja23 for 242 level 
$d|s/d|W (|mb/sr): 159 (60|'), 233 (90|'), 124 (125|') (1969Tj01) 
$d|s/d|W (30|')=360 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 6 (10|'), 9 (15|'), 14 (20|'), 21 (25|'), 31 (30|'), 46 (35|'), 68 (40|'), 81 (45|'), 102 (50|'), 159 (60|'), 164 (75|'), 233 (90|'), 136 (105|'), 124 (125|'), 70 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$J=1/2, |n1/2[521] for a 297 level (1969Tj01) 
$L=1 in 1979Ja23 for 297 level 
$d|s/d|W (|mb/sr): 92 (60|'), 92 (90|'), 39 (125|') (1969Tj01) 
$d|s/d|W (30|')=240 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 5 (10|'), 10 (15|'), 11 (20|'), 11 (25|'), 21 (30|'), 31 (35|'), 41 (40|'), 59 (45|'), 72 (50|'), 92 (60|'), 88 (75|'), 92 (90|'), 70 (105|'), 39 (125|'), 25 (150|') (1979Ja23). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$J=3/2, |n1/2[521] for a 355 level (1969Tj01) 
$L=1 in 1979Ja23 for 355 level 
$d|s/d|W (|mb/sr): 12 (60|'), 9 (90|'), 5 (125|') (1969Tj01) 
$d|s/d|W (30|')=40 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 1 (20|'), 1 (25|'), 2 (30|'), 3 (35|'), 5 (40|'), 7 (45|'), 6 (50|'), 12 (60|'), 11 (75|'), 9 (90|'), 7 (105|'), 5 (125|'), 1 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$J=7/2, |n3/2[521] for a 372 level (1969Tj01) 
$L=3 in 1979Ja23 for 372 level 
$d|s/d|W (|mb/sr): 164 (60|'), 217 (90|'), 136 (125|') (1969Tj01) 
$d|s/d|W (30|')=280 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 4 (20|'), 13 (25|'), 25 (30|'), 59 (40|'), 69 (45|'), 98 (50|'), 164 (60|'), 182 (75|'), 217 (90|'), 165 (105|'), 102 (125|'), 68 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$J=5/2, |n1/2[521] for |?384 level (1969Tj01) 
$d|s/d|W (|mb/sr): |?13 (60|'), |?21 (90|'), |?13 (125|') (1969Tj01) 
$d|s/d|W (30|')=45 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$J=9/2, |n3/2[521] for a 469 level (1969Tj01) 
$d|s/d|W (|mb/sr): 2 (60|'), |?5 (90|'), 5 (125|') (1969Tj01) 
$d|s/d|W (30|')=15 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$J=1/2, |n1/2[660] for a 507 level (1969Tj01) 
$L=0 in 1979Ja23 for 507 level 
$d|s/d|W (|mb/sr): 114 (60|'), |?168 (90|'), 102 (125|') (1969Tj01) 
$d|s/d|W(30|')=400 |mb/sr 
$d|s/d|W (|mb/sr): 46 (10|'), 5 (15|'), 4 (20|'), 6 (25|'), 19 (30|'), 40 (35|'), 65 (40|'), 79 (45|'), 89 (50|'), 114 (60|'), 140 (75|'), 168 (90|'), 106 (105|'), 102 (125|'), 68 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$J=3/2, |n3/2[402] for a 534 level (1969Tj01) 
$L=2 in 1979Ja23 for 534 level 
$d|s/d|W (|mb/sr): 169 (60|'), |?305 (90|') (1969Tj01) 
$d|s/d|W (30|')=390 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 10 (10|'), 14 (15|'), 14 (20|'), 18 (25|'), 24 (30|'), 29 (35|'), 43 (40|'), 66 (45|'), 102 (50|'), 169 (60|'), 198 (75|'), 305 (90|'), 230 (105|'), 140 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$L=5 in 1979Ja23 for 547 level 
$d|s/d|W (|mb/sr): |?17 (60|'), |?57 (90|'), |?36 (125|') (1969Tj01) 
$d|s/d|W (30|')=63 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 3 (10|'), 5 (15|'), 2 (20|'), 4 (25|'), 4 (30|'), 3 (35|'), 6 (40|'), 6 (45|'), 10 (50|'), 17 (60|'), 35 (75|'), 57 (90|'), 14 (105|'), 36 (125|'), 35 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$J=7/2, |n5/2[512] for a 575 level (1969Tj01) 
$d|s/d|W (|mb/sr): |?10 (60|'), |?18 (90|'), 13 (125|') (1969Tj01) 
$d|s/d|W (30|')=40 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_comment:
$J=11/2, |n5/2[505] for a 591 level (1969Tj01) 
$d|s/d|W (|mb/sr): |?18 (60|'), |?33 (90|'), |?27 (125|') (1969Tj01) 
$d|s/d|W (30|')=70 |mb/sr (1976Ma33) 
E$doublet with J|p=3/2+ and (1/2,3/2)-. A 591 group assigned by 1969Tj01 as 11/2[505], but 11/2[505] is located at 547 keV by 1970Hj02 in (|a,3n|g). This group may correspond to doublet at 589 in 'adopted levels', one component of which is assigned as 3/2+ member of configuration= |n1/2[660]+(K-2 |g vibration built on |n5/2[642]) 
L$(1) in 1976Ma33 is inconsistent with 3/2+ and (1/2-,3/2-) doublet from other studies 
S$0.03 for L=1, 0.02 for L=2 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): |?10 (60|'), |?23 (90|'), |?9 (125|') (1969Tj01) 
$d|s/d|W (30|')=35 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 3 (90|'), 6 (125|') for a 652 level (1969Tj01) 
$d|s/d|W (30|')=15 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 5 (60|'), 5 (125|') for a 724 level (1969Tj01) 
$d|s/d|W (30|')=15 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$J=1/2, |n1/2[400] for a 742 level (1969Tj01) 
$L=0 in 1979Ja23 for 746 level 
$d|s/d|W (|mb/sr): 114 (60|'), 190 (90|'), 139 (125|') (1969Tj01) 
$d|s/d|W (30|')=420 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 8 (10|'), 4 (15|'), 1 (20|'), 3 (25|'), 11 (30|'), 28 (35|'), 53 (40|'), 62 (45|'), 72 (50|'), 114 (60|'), 150 (75|'), 190 (90|'), 140 (105|'), 139 (125|'), 85 (150|') (1979Ja23) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 15 (60|'), 40 (90|'), 24 (125|') (1969Tj01) 
$d|s/d|W (30|')=82 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 3 (30|'), 4 (35|'), 4 (40|'), 6 (45|'), 11 (50|'), 15 (60|'), 18 (75|'), 40 (90|'), 23 (105|'), 24 (125|'), 18 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$J=11/2, |n5/2[512] for an 817 level (1969Tj01) 
$d|s/d|W (|mb/sr): 30 (60|'), 58 (90|'), 32 (125|') (1969Tj01) 
$d|s/d|W (30|')=150 |mb/sr (1976Ma33) 
L$3 from 1976Ma33 is inconsistent with adopted J|p=11/2- 
S$for L=5; 0.34 for L=3 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 14 (60|'), 17 (90|'), 6 (125|') (1969Tj01) 
$d|s/d|W (30|')=36 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 9 (60|'), 14 (90|'), 13 (125|') (1969Tj01) 
$d|s/d|W (30|')=10 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$J=3/2, |n1/2[530] for a 1039 level (1969Tj01) 
$L=1 in 1979Ja23 for 1039 level 
$d|s/d|W (|mb/sr): 65 (60|'), 96 (90|'), 56 (125|') (1969Tj01) 
$d|s/d|W (30|')=300 |mb/sr (1976Ma33) 
$d|s/d|W (|mb/sr): 6 (20|'), 6 (25|'), 10 (30|'), 16 (35|'), 23 (40|'), 31 (45|'), 65 (60|'), 75 (75|'), 96 (90|'), 70 (105|'), 56 (125|'), 40 (150|') (1979Ja23) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$J=5/2, |n1/2[530] for a 1063 level (1969Tj01) 
$d|s/d|W (|mb/sr): 4 (60|'), 8 (90|'), 5 (125|') (1969Tj01) 
$d|s/d|W (30|')=35 |mb/sr (1976Ma33) 
L$(1) from 1976Ma33 is inconsistent with adopted J|p=5/2- 
S$for L=3; 0.026 for L=1 
$Band assignment is tentative 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$J=7/2, |n1/2[530] for an 1172 level (1969Tj01) 
$d|s/d|W (|mb/sr): 6 (60|'), 17 (90|'), 14 (125|') (1969Tj01) 
$d|s/d|W (30|')=35 |mb/sr (1976Ma33) 
L$5 or 6 from reevaluation of 1969Tj01 by 1975Gr37. The data of 1976Ma33 do not fit any L value but best agreement is obtained for L=3 
$Band assignment is tentative 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 18 (60|'), 28 (90|'), 24 (125|') (1969Tj01) 
$d|s/d|W (30|')=80 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_comment:
$d|s/d|W (|mb/sr): 10 (60|'), 13 (90|'), 12 (125|') for a 1383 level (1969Tj01) 
$d|s/d|W (30|')=36 |mb/sr (1976Ma33) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(q=60|') (|mb/sr)=26 
J$tentative assignment: (13/2+) (1972Lo20) 
$d|s/d|W=47 |mb/sr (40|') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
$d|s/d|W(q=25|') (|mb/sr)=61 
J$from L(p,t)=0 from 7/2+ target (1975St08) 
$d|s/d|W=12 |mb/sr at 42.5|' 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
$d|s/d|W(q=25|') (|mb/sr)=184 
J$from L(p,t)=0 from 7/2+ target (1975St08) 
$d|s/d|W=37 |mb/sr at 42.5|' 


level_energy_unit: KEV
level_spin_parity: (19/2)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from 799.8|g(t) (2012Sw01) 
$Possible configurations=|n5/2[523]~#|p7/2[523]~#|p7/2[404] for J|p(1823 level)=19/2+; |n5/2[642]~#|p7/2[523]~#|p7/2[404] for J|p(1823 level)=19/2-; |n7/2[633]~#|p7/2[523]~#|p7/2[404] or |n11/2[505]~#|n5/2[523]~#|n5/2[512] for J|p(1823 level)=21/2-. 
$I|g(317.0):I|g(1050.6):I|g(1144.6)=100 {I8}:5 {I1}:17 {I2} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
MOMM1 Mean of +0.649 {I10} (1981Ho31) and +0.632 {I10} (1968Mu01); Mossbauer effect. 
MOME2 From Mossbauer effect; Sternheimer correction applied. Others: -2.7 {I9} (1970McZQ), -2.9 {I10} (1970Ka45); from Coulomb excitation reorientation. 
<r{+2}>{+1/2}(charge)=5.251 {I3} (2004An14). 
T weighted average of 1.76 ns {I5} (1963De21), 1.80 ns {I5} (1963Fo02) in |b{+-} decay (26.824 h); 1.83 ns {I6} (1963Li04), 1.83 ns {I5} (1968Ku03) in |b{+-} decay (1.20 E3 y); 1.86 ns {I5} from B(E2) in Coulomb excitation and adopted |g properties. Others: 1.98 ns {I21} (1961Bo05) in |b decay(26.824 h), 1961Ge14, 1967Ku07. 
J E2 91|g to 0+ g.s. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from |g|g(t) ({+166}Ho |b{+-} decay (1200 y)). Other: 120 ps {I7} from measured B(E2) and adopted |g properties. 
MOMM1 Unweighted average of +1.26 {I6} (1985Al22, IPAC), and +1.14 {I8} (1996Br09) and 1.18 {I5} (1986Do13), transient field IPAC. 
MOME2 From Coulomb excitation reorientation. 
J E2 184|g to 2+ 81. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T from RDM in Coulomb excitation. Other value: 17.7 ps {I+10-14} from measured B(E2) and adopted |g properties. 
MOMM1 Weighted average of +1.55 {I7} (1985Al22, IPAC), +1.51 {I16} (1986Do13, transient field IPAC) and +1.72 {I9} (1996Br09, transient field IPAC). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1 Weighted average of +0.54 {I9} (1986Do13, transient field IPAC) and +0.74 {I5} (1996Br09, transient field IPAC). 
MOME2 Weighted average of 2.2 {I2} (1983Hu01), 2.1 {I4} (1977Mc11) and 2.0 {I3} (1970McZQ); from Coulomb excitation reorientation. 
T from B(E2)|^=0.140 {I4} in Coulomb excitation and adopted |g properties. 
J E2 786|g to 0+ g.s. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J M1 73|g to 2+ 786, E2+M1 594|g to 4+ 265. 
T from B(E2)(594|g) in Coulomb excitation and adopted |g properties. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T from Coulomb excitation. 
MOMM1 Weighted average of +2.1 {I4} (1985Al22, IPAC), +1.8 {I3} (1986Do13, transient field IPAC) and +2.2 {I2} (1996Br09, transient field IPAC). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
J |g's to 4+ and 6+ are E2+M1. 
T from measured B(E2) in Coulomb excitation and adopted transition properties. Other datum: |<60 ps from |g|g(t) ({+166}Ho |b{+-} decay (1200 y)). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J M1+E2 671|g to 6+, E2 951|g to 4+ 265. |g|g(|q) data of 1965Re02 consistent with J=6. 
MOMM1 From 1985Al22 (IPAC). 
T from Coulomb excitation (RDM). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: PS
level_comment:
J continuation of established g.s. band. 
T from Coulomb excitation; weighted average of 1.59 ps {I8} (RDM) and 1.72 ps {I14} (B(E2) and adopted |g properties). 
MOMM1 Weighted average of +1.9 {I7} (1986Do13) and +2.8 {I4} (1996Br09); from transient field IPAC. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
J |g's to 6+ and 8+ are E2+M1. 
T from B(E2)(301|g) in Coulomb excitation and adopted transition properties. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J |g to 0+ is E2. 
T from B(E2)|^=0.018 {I2} in Coulomb excitation and adopted transition properties assuming negligible 572.2 branch. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J E1 |g to 0+. 
T from |G{-|g0}{+2}/|G=13.9 {I16} in (|g,|g') and adopted |G{-|g0}/|G=0.397 {I7}. 
K=(0) (1996Ma18) from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
BE3 From Coulomb excitation; B(E3)(W.u.)|^=20 {I3}. 
J E1(+M2) 1641|g to 2+ 81, D(+Q) 1457|g to 4+ 265. 


level_energy_unit: KEV
level_spin_parity: 9+
level_lifetime_unit: PS
level_comment:
J |g to 8+ is (E2+M1); band assignment. 
T from B(E2)(375|g) in Coulomb excitation and adopted transition properties. 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: FS
level_comment:
J D, |D|p=(no) |g to 0+. 
T from |G{-|g0}{+2}/|G in (|g,|g') and adopted branching. 
K=1 (1996Ma18) from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J M1+E2 154.5|g from 3+ level; (|a,t) |s fingerprint for assigned band. Decay pattern to |g band states consistent with that for a state carrying a portion of the K|p=4+ |g|g vibration strength expected at roughly this energy (1998Fa15). 
T from B(E2)(1193|g) in Coulomb excitation and adopted transition properties assuming 521-keV branch is negligible. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J |g to 2+ and 3+ levels; decay pattern to |g band states consistent with that for a state carrying a portion of the K|p=4+ |g|g vibration strength expected at roughly this energy (1998Fa15). 


level_energy_unit: KEV
level_spin_parity: (7)-
level_comment:
J E1 1082|g to 8+ 911; band assignment. Suggested as possible J=7 member of K|p=4- band (1989Ad12), but E is too high for that. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J D+Q 1169|g to 3+ 859; Q 1243|g to 2+ 786, |g to (4)- 1572; possible |g|g band assignment. 
T from DSAM in (n,n'|g) (1997Ga11). Other value: 0.33 ps {I12} from B(E2)(1243|g) and adopted transition properties, assuming negligible 1070 branch. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+
level_comment:
J from (|a,t) |s fingerprint for assigned band. 
The 1089|g in (n,n'|g) may Be a doublet which deexcites this level as well as the 2047 level. 


level_energy_unit: KEV
level_spin_parity: (7,8,9)-
level_comment:
J E1 1181|g to 8+ 911; band assignment. Suggested as possible J=7 member of K|p=2- octupole band (1989Ad12), but E is too high for that assignment. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J transitions to J=2,3 and possibly 4 members of |g band; candidate for K|p=4+ |g|g vibration state (1994OsZZ). 
T from B(E2)(1316|g) in Coulomb excitation and adopted transition properties assuming negligible 1145|g branch. 


level_energy_unit: KEV
level_spin_parity: (2,3,4)
level_comment:
J |g's to 2+ and 4+. If the 1630|g in (n,n'|g) is correctly placed from this level, its D+Q multipolarity would rule out J=4. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J M1 |g to 0+. 
T from |G{-|g0}{+2}/|G=5.1 {I5} in (|g,|g') and adopted |G{-|g1}/|G{-|g0}=0.44 {I7}. 
K=1 (1996Ma18) from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J M1 |g to 0+. 
T 12 fs {I3} from (|g,|g'), if I(1142|g) is negligible. 
K=1 from (|g,|g') (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
K=1 (1996Ma18) from (|g,|g'). 
J D |g to 0+ g.s. 
E from (|g,|g'). Other E: 3193 in (|g,|g') (1973Me17). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
T from Adopted Levels. Measured values from |b-|g(t) are: 1.76 ns {I5} (1963De21), 1.80 ns {I5} (1963Fo02), 1.98 ns {I21} (1961Bo05). Others: 1950Mc79, 1956Be54, 1959Bi10, 1960Be28, 1960Ma38. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J (1379.4|g)(80.574|g)(|q) is consistent only with J=0 for 0-2-0 cascade (1960Ma19,1960Ma38,1961Ku03). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J (1581.89|g)(80.574|g)(|q) is consistent with 1(D+Q)2(Q)0 cascade and 3(D+Q)2(Q)0 cascade. J=3 ruled out because of log| {Ift}=6.94 for the |b- branch to 1662.45 level (1968Fo11). 1969He02 measured the linear polarization and demonstrate that it is consistent with E1(+M2) for the 1581.89|g only if J=1 for 1662.45 level. 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_comment:
J (1120.3|g)(280.45|g)(|q) A{-2}=-0.103 {I32}, A{-4}=-0.008 {I42} is consistent only with 5(D)6(Q)4 spin sequence (1981La27). 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_comment:
J (1146.8|g)(280.45|g) A{-2}=-0.098 {I45}, A{-4}=-0.06 {I7}; and (1427.25|g)(184.41|g)(|q) A{-2}=-0.089 {I45}, A{-4}=0.00 {I3}. The two sets A{-2}, A{-4} are consistent only with 5(D+Q)6(Q)4 spin sequence with |d(1146.8|g)=-0.02 {I+7-6} or +9 {I+9-6} and 5(D+Q)4(Q)2 spin sequence with |d(1427.25|g)=-0.025 {I25} (1981La27). 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
J (711.68|g)(280.45|g)(|q) A{-2}=-0.05 {I1}, A{-4}=-0.02 {I2} and (1241.48|g)(280.45|g)(|q) A{-2}=+0.129 {I13}, A{-4}=0.000 {I23} are consistent only with J=6 (1981La27). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$d|s/d|W(60=6.1 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 2.2 at 45|', 1.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$d|s/d|W(60=24 
Other E: 258 in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 6.4 at 45|', 5.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
$d|s/d|W(60=10.7 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 2.8 at 45|', 2.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$d|s/d|W(60=1.0 {ILT} 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): <1.0 at 45|' and 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$d|s/d|W(60=1.0 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): <1.0 at 45|' and 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
E absent in (|a,t) (1979Pa15) and in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): <1.0 at 45|' and 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4-)
level_comment:
$d|s/d|W(60=29 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 27 at 45|', 17.7 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4-
level_comment:
$d|s/d|W(60=3.0 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 1.9 at 45|', 1.7 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-)
level_comment:
$d|s/d|W(60=13.5 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 9.8 at 45|', 7.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=1.0 {IAP} 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 3.0 at 45|', ~2.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-)
level_comment:
$d|s/d|W(60=12.8 {IAP} 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 8.2 at 45|', ~5.0 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.6 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 1.2 at 45|', 1.4 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.2 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): <1.0 at 45|' and 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6-)
level_comment:
$d|s/d|W(60=2.5 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 1.9 at 45|', 1.7 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E absent in (|a,t) (1979Pa15) and in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): <1.0 at 45|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6-)
level_comment:
$d|s/d|W(60=5.7 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 6.4 at 45|', 4.9 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=4.5 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 4.4 at 45|', 3.5 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3-)
level_comment:
$d|s/d|W(60=13.8 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 18.0 at 45|', 11.9 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=4.5 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 1.4 at 45|', 2.0 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$d|s/d|W(60=11.2 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 13.2 at 45|', 9.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7-)
level_comment:
$d|s/d|W(60=35 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 19.4 at 45|', 16.9 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4-)
level_comment:
$d|s/d|W(60=12.7 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 14.9 at 45|', 10.3 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=10.4 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 11.7 at 45|', 7.3 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+
level_comment:
$d|s/d|W(60=19.0 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 14.9 at 45|', 15.8 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_comment:
$d|s/d|W(60=17.2 
E doublet; J=1, K|p=1- and J=2, K|p=2-. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 33 at 45|', 19.1 at 60|' for presumed doublet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2-)
level_comment:
$d|s/d|W(60=3.5 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 2.0 at 45|', 2.9 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_comment:
$d|s/d|W(60=2.2 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 2.2 at 45|', 1.9 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_comment:
$d|s/d|W(60=38 
E triplet; J=3, K|p=3+ and J=6, K|p=4+ and J=3, K|p=2-. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 36 at 45|', 26 at 60|' for presumed triplet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2-)
level_comment:
$d|s/d|W(60=8 {IAP} 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): ~13.0 at 45|', 11.3 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2-)
level_comment:
$d|s/d|W(60=2.0 
E absent in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): ~3.5 at 45|', 1.8 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=11.6 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 5.0 at 45|', ~6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=8.0 
E absent in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 8.7 at 45|', 6.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3-)
level_comment:
$d|s/d|W(60=5 {IAP} 
E doublet. J=3, K|p=1- and J=4, K|p=2-. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 11.7 at 45|', 9.8 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$d|s/d|W(60=12.9 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 11.2 at 45|', ~8.5 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7+
level_comment:
$d|s/d|W(60=3.6 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 4.3 at 45|', 3.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E absent in (|a,t) (1979Pa15). 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 3.1 at 45|', 1.0 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.0 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 4.2 at 45|', 2.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=5.1 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 8.4 at 45|', 6.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+
level_comment:
$d|s/d|W(60=3.4 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 4.1 at 45|', 3.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2 {IAP} 
Absent in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): ~4 at 45|', 4.5 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=6 {IAP} 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): ~6 at 45|', 6.3 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=1.8 
E 1993Li12 report E=2430; possibly this a doublet consisting of the 2418 and 2438 levels reported by 1975Pa15. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): ~3 at 45|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.5 
E see comment on 2418 level. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 3.4 at 45|', ~2.3 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=6.1 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 9.3 at 45|', 7.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=6.2 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 7.0 at 45|', 7.1 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=5.7 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 5.9 at 45|', 7.2 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=3.4 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 3.0 at 45|', 5.7 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E absent in (|a,t) (1979Pa15). 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 7.7 at 45|', 7.0 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6-)
level_comment:
$d|s/d|W(60=34 
Possible configuration: |p{+2}(7/2[523]+5/2[402]) (1993Li12). 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 74 at 45|', 56 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=9.8 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 11.9 at 45|', 9.5 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=8.3 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 14.2 at 45|', 10.3 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.1 
Absent in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 5.2 at 45|', 3.6 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=1.3 
Other E: 2920 in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 4.5 at 45|', 3.8 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.1 
Other E: 2959 in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 10.9 at 45|', 10.0 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=1.9 
Absent in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 10.8 at 45|', 8.7 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_comment:
$d|s/d|W(60=6.9 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 6.7 at 45|', ~4 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2.8 
Other E: 3096 in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 5.0 at 45|', 7.5 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=1.2 
Other E: 3168 in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 10.5 at 45|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9+)
level_comment:
$d|s/d|W(60=13.7 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 11.2 at 45|', 6.1 at 60|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E absent in (|a,t) (1979Pa15). Other E: 3482 in 1993Li12. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 15.1 at 45|'. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(60=2 {ILT} 
E absent in (|a,t) (1979Pa15). 
L based on d|s/d|W({+3}He,d)/d|s/d|W(|a,t) at 60|'. 
d|s/d|W(|mb/sr) in ({+3}He,d) at E({+3}He)=24 MeV (1979Pa15): 25.0 at 45|', 22 at 60|'. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=13.9 {I16} 
E from 1991Zi01. 
K=(0) (1996Ma18). 
|G{-|g0}{+2}/|G: weighted average of 15.2 {I17} (1996Ma18) and 17.1 {I11} (1991Zi01, from reported |G{-|g1}/|G{-|g0}=1.50 {I4} and |G{-|g0}=42.8 meV 28) and 12.0 {I8} (1976Me04). 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=5.5 {I10} 
E from 1973Me17. 
T value becomes 39 fs {I7} based on adopted branching. 
|G{-|g0}{+2}/|G: weighted average of 7.0 {I9} (1996Ma18) and 4.8 {I6} (1976Me04). 
K=1 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
E from 1973Me17; not reported in 1996Ma18. 
T |G{-|g0}|G{-|g1}/|G=1.8 {I3} meV (1973Me17); deduced by evaluator from authors' calculated |G{-|g0} and assumed |G{-|g1}/|G. Assuming adopted I(1749|g):I(1830|g)=100.0 {I21}:29.9 {I5} and J=1, this gives |G=10.1 {I17} meV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1(+)
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=5.8 {I6} 
|G{-|g0}{+2}/|G: weighted average of 6.1 {I9} (1996Ma16) and 5.4 {I9} (1976Me04). 
K=0 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=5.1 {I5} 
K=1 (1996Ma18). 
T from |G{-|g0}{+2}/|G=5.1 {I5} and adopted |G{-|g0}/|G{-|g1}=0.44 {I7}. 
|G{-|g0}{+2}/|G: weighted average of 5.3 {I3} (1996Ma16) and 3.9 {I8} (1976Me04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=8.7 {I10} 
|G{-|g0}{+2}/|G: weighted average of 9.0 {I13} (1996Ma16) and 8.3 {I17} (1976Me04). 
K=1 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=16 {I3} 
|G{-|g0}{+2}/|G: weighted average of 23 {I4} (1996Ma16) and 15.4 {I16} (1976Me04). 
K=1 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=9.8 {I9} 
|G{-|g0}{+2}/|G: weighted average of 10.0 {I10} (1996Ma16) and 9.1 {I19} (1976Me04). 
K=1 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=5.2 {I5} 
|G{-|g0}{+2}/|G: weighted average of 5.1 {I5} (1996Ma16) and 5.8 {I11} (1976Me04). 
K=0 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=2.6 {I5} 
|G{-|g0}{+2}/|G: weighted average of 3.2 {I6} (1996Ma16) and 2.2 {I5} (1976Me04). 
T from |G{-|g0}{+2}/|G=2.6 {I5} and adopted |G{-|g0}/|G=0.53 {I6}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=18.9 {I13} 
K=0 (1996Ma18). 
|G{-|g0}{+2}/|G: weighted average of 19.1 {I16} (1996Ma16) and 18.6 {I23} (1976Me04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=39 {I3} 
E 3141 in 1973Me17. 
|G{-|g0}{+2}/|G: weighted average of 42 {I3} (1996Ma16) and 35 {I4} (1976Me04). 
K=1 (1996Ma18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G (meV)=27.0 {I25} 
|G{-|g0}{+2}/|G: weighted average of 29.0 {I21} (1996Ma16) and 23.8 {I27} (1976Me04). 
K=1 (1996Ma18). 
E 3193 in 1973Me17. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
Level shown as tentative and omitted from Adopted Levels because its existence relies entirely on placement of one multiply-placed transition. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
Potential deformation: |b{-2}=+0.230 from (|a,|a') (1968He24); |b{-2}(real)=+0.276 {I6} (1983Ro11), +0.294 (1992Ka07) from (p,p'). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
Potential deformation: |b{-4}=0 from (|a,|a') (1968He24). |b{-4}(real)=+0.009 {I5} (1983Ro11), +0.019 (1992Ka07) from (p,p'). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
Potential deformation: |b{-6}=-0.015 from (|a,|a') (1968He24). |b{-6}(real)=-0.007 {I2} (1983Ro11), -0.020 (1992Ka07) from (p,p'). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: NS
level_comment:
Q=-1.77 {I+14-9} based on diagonal matrix element. 
T from B(E2)|^ and adopted transition properties. 
BE2 From an unweighted average of 5.69 {I16} (1970Ka45); 5.76 {I10} (1972Er04); 5.65 {I5} (1973Be40); 5.85 {I4} (1974Wo01); 5.91 {I3} (1977Fi01). Other: 5.2 {I5} (1992Fa01). 
Static matrix element: <2+ M(E2) 2+> =-2.33 {I+19-12} (1992Fa01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
Q=-1.60 {I+26-12} based on diagonal matrix element. 
g-factor from transient field IPAC: +0.297 {I13} (1986Do13), 0.285 {I20} (1996Br09). 
Static matrix element: <4+ M(E2) 4+> =-2.12 {I+34-16} (1992Fa01). 
E4 matrix element=0.06 {I+12-18} (1972Er04); 0.32 {I16} (1973Be40); 0.22 {I+11-16}(1974Wo01); 0.31 {I+9-10} (1974Sh12); 0.24 {I7} (1977Fi01). 
T from B(E2) and adopted transition properties. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
Q=-2.81 {I+17-14} based on diagonal matrix element. 
g-factor: method, transient field. Other: 0.259 {I30} (1986Do13) from g-factor/g-factor(265)=0.85 {I9}, g-factor(265)=+0.305 {I15}. 
Static matrix element: <6+ M(E2) 6+> =-4.03 {I+25-20} (1992Fa01). 
T from RDM (1992Th04); 17.7 ps {I+10-14} from B(E2) and adopted transition properties. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
Other Q: +2.25 {I+13-11} based on diagonal matrix element. 
g-factor: method, transient field. Other: 0.271 {I44} (1986Do13) from g-factor/g-factor(265)=0.89 {I14}, g-factor(265)=+0.305 {I15} 
Static matrix element: <2+ M(E2) 2+> =+2.97 {I+17-15} (1992Fa01). 
T from B(E2)|^=0.140 {I4} and adopted transition properties. Other value: 4.0 ps {I4} from RDM (1992Th04). 
B(E2)(785.9|g)/B(E2)(705.3|g)=0.544 {I15} (1983Hu01). 
BE2 Weighted average of 0.140 {I8} (1978Mc02), 0.134 {I9} (1972Do01), 0.142 {I5} (1973Be40), and 0.140 {I15} (1992Fa01) from <2+{-|g} M(E2) 0+{-g}> =+0.372 {I19}. Others: 0.176 {I8} (1977Wo03), 0.19 {I4} (1963Yo09). 


