# LEVEL

level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=L(d,d')=4 from 0+ 
T$from DSAM in (p,p'|g). Other: <0.7 ps from RDM in ({+12}C,2p|g) 
$B(E4)=0.000192 (1983Li02) in (e,e') 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
J$dipole 3628.7|g to 0+; |s(|q) in (p,p') (1989Wi13); expected 1+ from shell-model predictions (see 1989Wi13) 
T$from |G{-0}=0.205 eV {I9} in (|g,|g'). Other: 5 fs {I3} in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2; M1+E2 2914.8|g to 2+. L(|a,|a')=L(p,p')=L({+3}He,{+3}He')=4 for a 3698 {I20} level inconsistent, if it is the same level as seen in other reactions 
T$from DSAM in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: PS
level_comment:
J$J|p=5+ from p|g(|q) in (p,p'|g); L(p,p')=4; and absence of this level in (|a,|a'). However (4-) cannot be ruled out as proposed by 1998Br34 from |g(|q) in ({+28}Si,|a2p|g) 
T$from RDM in ({+16}O,|a2p|g). Other: >73 fs from DSAM in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$logft=5.0 from 5+; angular distribution of the 661.76 keV |g corresponds to |DI=0 dipole or stretched quadrupole transition 
T$inconsistent with 3.5 ps {I+35-14} (1973De09) from RDM in ({+12}C,2p|g). Other: <1.4 ps from RDDS in 1974Br04 in ({+16}O,|a2p|g) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=0. L(|a,|a')=L(d,d')=L({+3}He,{+3}He')=4 for 3898 {I20} is inconsistent if it is the same level as in other reactions 
T$from DSAM in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(d,d')=L(p,p')=L({+3}He,{+3}He')=3 from 0+ 
T$from DSAM in (p,p'|g). 
$B(E3)(from g.s.)=0.0033 {I13} (2002Ki06 evaluation) deduced from |b{-3} in (|a,|a') (1990Ba23) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 6+; spin=2 from |g(|q) in ({+16}O,|a2p|g) 
MOMM1$g=+0.54 {I9} from TF in ({+40}Ca,2p|g) (1994Pa34) 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$784.6|g to (6-), 1630.9|g to 5-; band assignment 
T$effective half-life=0.28 ps {I7} from DSAM in ({+28}Si,|a2p|g) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J$from 1998Br34 based on |g(|q), similarity to unnatural parity states in neighboring nuclides of {+48}Cr and {+46}Ti, and from theory, although angular distribution is also consistent with 5+. 1998Ca26 quote 4+ probably from a previous measurement (1968Mo07). 5+ in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$from 2002Br41, belongs to 4- band. 
T$0.28 ps {I7} is effective value, not corrected for side feeding 


level_energy_unit: KEV
level_comment:
$d|s/d|W=620 {I50} 
$L=0, d|s/d|W(0|')=1.23 mb/sr {I5}; d|s/d|s(DW)=2.12 (1975Al05) 
$L=0, d|s/d|W(0|')=1.4 mb/sr (1974Ev02) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=160 {I20} 
$E=4.00 MeV {I5}, L=0, d|s/d|W(0|')=0.26 mb/sr {I5}; S=0.30 (1975Al05) 
$E=3.95 MeV {I6}, L=0+2, d|s/d|W(0|')=0.13 mb/sr (1974Ev02) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=530 {I40} 
$E=5.84 MeV {I5}, L=0, d|s/d|W(0|')=0.71 mb/sr {I6}; S=0.71 (1975Al05) 
$E=5.76 MeV {I3}, L=0, d|s/d|W(0|')=0.35 mb/sr (1974Ev02) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E,L$level from 1974Ev02 only, but not confirmed by 1975Bo14 at E({+3}He)=13 MeV. This level is not included in the Adopted Levels. 
$d|s/d|W(20|')=0.17 mb/sr (1974Ev02) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=400 {I50} 
$E=11.5 and 11.9 MeV, L=0, d|s/d|W(0|')=0.7 mb/sr {I2}; S=0.6 (1975Al05) 
$E=11.57 MeV {I3}, L=0, d|s/d|W(0|')=0.27 mb/sr (1974Ev02) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=440 {I70} 
$IAS({+50}V 3.43 MeV). 
$E=11.95 MeV {I3}, L=0, d|s/d|W(0|')=0.35 mb/sr (1974Ev02) 


level_energy_unit: KEV
level_comment:
L$(|a,|a') |s(|q) does not agree with DWBA for L=4. State probably excited by double excitation (1974Pe01). (|a,|a') |s(|q) reproduced by harmonic vibrator model (HVM) and rotor model (RM) coupled-channel calculations (1990Ba23). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$from excitation cross section in Coul. ex., weighted average of 0.102 {I5} (1975To06); 0.115 {I10} (1972Ra14); 0.092 {I10} (1971DaZM); 0.115 {I12} (1966Mc18,1961Mc18); 0.15 {I3} (1960An09, uncertainty estimated in 2001Ra27 evaluation) 
$2001Ra27 erroneously gave 1960An07, instead of 1960An09 
T$other: 6.9 ps {I14} (1972Ra14) 
G$transient-magnetic field method (2000Er06). Others: +0.59 {I10} based on T{-1/2}=9.22 ps {i35} (1977Fa07,IMPAC; E({+16}O)=36 MeV; recoil into Fe); +0.45 {i15} (1987Pa28,E({+16}O)=36 MeV; |g(|q,H); based on T{-1/2}=9.00 ps) 


level_energy_unit: KEV
level_comment:
$(2L+1)|s(EXP)/|s(DWUCK)=1140 {IAP} 
$Also L=0 from 2016Le10 
$Measured d|s/d|W=6.50 mb/sr {I30} at |q{-c.m.}=10|' (2016Le10), compared to d|s/d|W=1.15 mb/sr from shell model prediction 


level_energy_unit: KEV
level_comment:
E,L$From 2016Le10, energy uncertainty is estimated by evaluators. Other: 3694 {I8}, L=0 and possible doublet in 1972Ra14. 2016Le10 neither confirmed L=0 state at 3694 keV, nor a doublet near this energy 


level_energy_unit: KEV
level_comment:
E$from 1972Ra14, possible doublet. Other: 3860 {I30} in 1971Ba46 is identified with 3895 level. Level also seen in 2016Le10 


level_energy_unit: KEV
level_comment:
E,L$from 2016Le10. Others: 3898 {I7}, possible doublet in 1972Ra14; 3860 {I30}, L=0+|>2 in 1971Ba46 
$Measured d|s/d|W=72 |mb/sr {I3} at |q{-c.m.}=10|', compared with 64 |mb/sr from shell model prediction (2016Le10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$from Adopted Levels. Doublet near 4069 keV resolved by 2016Le10, the second component being the L=0, 4068.8 keV. See also comment for 4068.8 level for population in study by 1971Ba46 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E,L$from 2016Le10. Other: 4050 {I30}, possible doublet with L=0+|>2 in 1971Ba46. Doublet is resolved in 2016Le10, the second component assigned to a 4052, 3- level from Adopted Levels 
$Measured d|s/d|W=106 |mb/sr {I6} at |q{-c.m.}=10|', compared with 5 |mb/sr from shell model prediction (2016Le10) 


level_energy_unit: KEV
level_comment:
E,L$from 2016Le10. Other: 4350 {I30}, L=0 in 1971Ba46. 2016Le10 did not confirm L=0 for a 4350-keV level 
S$|?74 for L=0 in 1971Ba46 


level_energy_unit: KEV
level_comment:
$(2L+1)|s(EXP)/|s(DWUCK)=74 {IAP} 
E$from 2016Le10. Other: 4750 {I30} (1971Ba46) 
L$from 1971Ba46. 2016Le10 stated that L-value could not be deduced from their |s(|q) data 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 9.2 ps {I4} (M.M. Giles et al., Phys. Rev. C, accepted April 9, 2019), 8.7 ps {I15} (1974Br04), and 8.4 ps {I8} (1973De09). Method: recoil-distance Doppler shift (RDDS) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$others: 3.4 ps {I5} (M.M. Giles et al., Phys. Rev. C, accepted April 9, 2019, RDDS); <2.8 ps (1974Br04, RDDS) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$other: <1.6 ps (1974Br04) 
$g-factor adjusted for T{-1/2}=0.69 ps {I14} (1998Br34) from original g=+0.54 {I16} (1994Pa34) which used T{-1/2}=1.25 ps {I28} (1973De09) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
J$4- assignment in 2019-Giles paper seems to have been taken from 1998Br34 that was based on systematics and model considerations, but evaluators assign 5+ in the Adopted Levels based on arguments from experimental evidence in different reactions 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$|G{-0}{+red}=4.29 meV/MeV{+3} {I19} 
$Level also reported by 1998En05 
E$theoretical analysis indicates the 1+ state has an isovector orbital character with a minor spin admixture which supports trends for the scissors-like mode in the {Ifp}-shell region (2016Pa04) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$Level also reported by 1970Mo26, 1973MoYZ with spin=1 from |g(|q) 
$|G{-0}{+red}=0.76 meV/MeV{+3} {I7}. 
$Other |G{-|g}=0.75 eV {I20} (1970Mo26,1973MoYZ) from temperature variation and self-absorption is consistent with that from 2016Pa04 


level_energy_unit: KEV
level_comment:
$(|b{-L}R){+2}=1.14 
E$from 1964Bj01. Others: 786 {I7} (1966Ma42), 783 {I20} (1974Pe01), 778 {I10} (1968Ro09) 


level_energy_unit: KEV
level_comment:
$(|b{-L}R){+2}=0.643 
E$other: 4050 {I20} (1972Pe28) 
J$0+ from |s(|q) for a level at 4040 in 1989Wi13; but 3- from |g(|q) in (1972Pe28) 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_lifetime_unit: FS
level_comment:
J$2+ in Adopted Levels; possible 3698|g to 0+ does not allow 3+ 
T$other: 15 fs {I+7-6} from centroid shift (1972As01) 


level_energy_unit: KEV
level_comment:
E$other: 1888 {I20} (1974Pe01) 
L$|s(|q) does not agree with DWBA for L=4. State probably excited by double excitation (1974Pe01). 
$d|s/d|W(maximum)=0.15 mb/sr (1968Ha31) 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J$compiler's note: it is not clear from |s(|q) distribution shown in authors' Fig. 5e, how 5- is definitely assigned, as the observed |s(|q) distribution seems to deviate significantly from the DWBA calculation between |q(c.m.) of 30|' and 40|' 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: D
level_comment:
J J from atomic beam (1976Fu06), L=3 in {+50}V({+3}He,d), {+52}Cr({+3}He,|a) and {+50}Cr(d,p). 
T from weighted average of 27.70 d {I3} (2014Un01), 27.710 d {I30} (1976WaZH,1982DeYX,1983Wa26), 27.71 d {I1} (1982ChZF), 27.690 d {I5} (1980Ho17), 27.720 d {I27} (1975La16), 27.703 d {I8} (1974Ts01), 27.750 d {I9} (1973Vi13), 27.76 d {I15} (1972Em01), 27.704 d {I3} (1969MeZV, 1970MeZQ, 1980RuZY), 27.80 d {I51} (1968Bo25), 27.701 d {I6} (1964Ma56), 27.82 d {I20} (1963Ho17), 27.75 d {I30} (1957Wr37), 27.8 d {I1} (1956Sc87), 27.75 d {I30} (1952Ly17). Others: 27.6999 d {I13} (2012Fi12, superseded by 2014Un01), 27.7010 d {I12} (2002Un02, superseded by 2014Un01), 27.7010 d {I12} (1992Un01, superseded by 2014Un01), 27.73 d {I1} (1982HoZJ, superseded by 2014Un01), 28.1 d {I17} (omitted as outlier, 1973ArZI), 27.679 d {I17} (1976WaZH, superseded by 1983Wa26), 27.7 d {I2} (1967LaZZ, superseded by 1975La16), 27.5 (1965Sa09), 28.04 d {I16}, 27.85 d {I2} (omitted as outlier, 1957Ka65), 27.9 d {I2} (omitted as outlier, 1956Ka33), 27 (1948Mi12), 26 (1948Ho04), 26.0 d {I10}, 26.5 d {I10} (omitted as outlier, 1940Wa023), 27.7009 d {I20} (2004Wo02,evaluation). 
|m=(-)0.934 {I5} (1970Ad07,1989Ra17,2014StZZ) 
MOMM1${+53}Cr standard, Atomic Beam Magnetic Resonance (AB)(1970Ad07) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J E2 |g to 7/2-, L=1 in {+52}Cr({+3}He,|a), {+50}Cr(d,p). 
T From {+51}V(p,n|g). Others: 7.25 ns {I25} in {+48}Ti(|a,n|g), 7.6 ns {I3} in {+51}Mn |e decay, 8.3 ns {I19} in {+52}Cr(n,2n|g). 
MOMM1 From |g(|q,H,t) in {+48}Ti(|a,n|g), Time Dependent Perturbed Angular Distribution (TDPAD) (1974Ko10) 
IAS of 5133 in {+51}Mn 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
J L=1 in (d,p) gives 1/2- and 3/2-. J|p=1/2- from J dependence of |s(|q) in (d,p). For J|p=3/2-, the unobserved |g to g.s. would have B(E2)(W.u.)<0.00015; an unreasonably small value 
T From {+51}V(p,n|g). 
IAS of 5077 in {+51}Mn 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J M1+E2 |g to 7/2-, M1 |g from 11/2-; also from measured angular distribution with non-pickup character and coupled-reaction channel (CRC) analysis in ({+3}He,|a). 
T From weighted av. of 76 fs {I7} in {+48}Ti(|a,n|g) and 63 fs {I12} in {+51}V(p,n|g). Others: |<0.7 ns in {+51}Mn |e decay, and 77 fs in (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J M1+E2 |g to 3/2-, M1(+E2) |g to 7/2-, L=3 in {+52}Cr({+3}He,|a), {+50}Cr(d,p). 
T other: >0.59 ps in {+51}V(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J Stretched E2 |g to 7/2-, |g from 13/2-, L=3 in {+50}V( {+3}He,d). 
T others: 0.49 ps {I+28-13} in {+51}V(p,n|g), and 0.56 ps in (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J E2 |g to 3/2-, L=3 and vector and tensor analyzing power in {+50}Cr(pol d,p), L=3 in {+52}Cr({+3}He,|a). 
T other: >0.485 ps in {+51}V(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J L=1 and vector and tensor analyzing power in {+50}Cr(pol d,p). 
T other: 0.27 ps {I+10-5} in {+51}V(p,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J M1+E2 |g to 7/2-, L=3 in {+50}V({+3}He,d), also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
T from average of 19 fs {I4} (1971Iy03) and 15.2 fs {I42} in (p,n|g). Other: 24 fs {I10} in {+48}Ti(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J E2 |g to 11/2-, L=3 in {+50}V({+3}He,d), |g(|q) in {+48}Ti(|a,n|g). 
T other: 46 ps in (HI,xn|g), >69 fs in {+51}V(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J (M1) |g to 9/2-, L=3 in {+50}Cr(d,p) and {+52}Cr({+3}He,|a), also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
T other: <21 fs in {+48}Ti(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J M1 |g to 7/2-, M1+E2 |g to 11/2-, also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
T from weighted av of 0.37 ps +{I14}-{I9} (1971Iy03), 0.15 ps {I12} (1985Av04) in (p,n|g), 0.42 ps {I+14-10} in (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: FS
level_comment:
J M1+E2 |g to 11/2-, L=3 in {+50}V({+3}He,d), also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
T From weighted av. of 59 fs {I12} in {+51}V(p,n|g) and 56 fs {I+14-12} in {+48}Ti(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
J E2 |g to 7/2-, also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g); J=11/2 from shell-model calculation. 
T others: 39 fs {I+30-20} in (p,n|g) (1971Iy03), >416 fs in (|a,n|g) (1980Ka10), 234 fs {I+24-21} in (|a,n|g) (1973Sz01). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J 1287.2 |g M1+E2 to 11/2-, L=3 in {+50}V({+3}He,d), also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
T from unweighted av of 49 fs {I+14-12} in {+48}Ti(|a,n|g) and 33 fs {I10} in {+51}V(p,n|g). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: FS
level_comment:
J L=1 in ({+3}He,|a), log| {Ift}=6.0 from 5/2-, also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
IAR of 7274 in {+51}Mn 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J 5/2+ for IAR at 7459 in {+51}Mn. This is consistent with L=(2) for the possible 3004.4 + 3016 peak in {+51}Cr(d,p). 
E 3012 {I10} level in {+52}Cr({+3}He,|a) probably corresponds to either the 3004.4 {I3} or the 3016 {I8} levels. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
T from 1973Sz01. other:<28 fs (1980Ka10) 
J 3020.3 |g to 7/2-, 633 |g to 13/2-, RUL rules out 9/2-; also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J L=1, vector and tensor analyzing power in {+50}Cr(pol d,p), L=1 in ({+3}He,|a), also |g(|q), |g(pol) and RUL in {+48}Ti(|a,n|g). 
Corresponding IAR in {+51}Mn (7560 level) is 3/2-,5/2- 


level_energy_unit: KEV
level_spin_parity: (17/2)-
level_comment:
T an effective half-life of 0.42 ps is reported in (HI,xn|g) 
J L=3 in {+50}V({+3}He,d), f7/2 band member 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_lifetime_unit: FS
level_comment:
J E(d,p)=3204 {I8}, with L=3, could correspond to either or both the 3204.1 and 3207.22 levels. Also, presumably either or both of these levels could be the parent of the (5/2,7/2)IAR at 7669 in {+51}Mn. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J 5495|g-CP measurement in {+50}Cr(pol n,|g), |g from 1/2+ capture state is E1. J|p=(3/2-) for possible IAR at 8199 in {+51}Mn 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J L=2 in {+50}Cr(d,p) and RUL for |g to 7/2- rules out mult=M2 
5/2+ for possible IAR at 8352, 8358 in {+51}Mn 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2-)
level_lifetime_unit: FS
level_comment:
J |g's to 3/2- and 7/2-. L=1+3 for E=4020 {I15} in ({+3}He,d). If the L=3 component corresponds to this level, then J|p=(5/2,7/2)-. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J L=1 in {+50}Cr(d,p) and 5222|g-CP measurement from 1/2+ thermal neutron capture state in {+50}Cr(pol n,|g). 
IAR of 8403 in {+51}Mn 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J L(d,p)=0; primary |g from 1/2+ in {+50}Cr(n,|g), |g to 1/2- suggests J|p|=5/2+. J|p=1/2+ for IAR at 8749 in {+51}Mn. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T from 1974Ko10 
MOMM1 From |g(|q,H,t) relative to 197 level in {+19}F (1974Ko10). Value is an average of -0.78 {I13} from this reaction and -0.95 {I10} from (d,p|g). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
T from 1980Ka10. Other: 234 fs {I+24-21} (1973Sz01) is wrong because the 1148|g used by 1973Sz01 is a triplet. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E,J,S 1968Ro09 report L=3 for 3002 level and do not give L for the 3016 level. 1977Ch12 report L=(2) with C{+2}S'=0.08 (1d3/2), 0.023 (2d5/2) for the doublet. In adopted levels, there is a 3001.7 level with J|p=5/2- and a 3004.3 level with J|p=3/2+. The 3016 level is resolved only in this reaction. 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J from 1977Ch12. 5/2- favored by 1972Ma39 on the basis of the decrease in |s between E(d)=7.5 and E(d)=10 MeV. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E possible doublet (1977Ba14). Authors note that the small magnitude of the vector-analyzing power can be accounted for by the assumption that the peak consists of two states with 1/2- and 3/2- configurations. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
C{+2}S': from 1972Ma39. L from 1972Ma39,1968Ro09. Spectrum of 1977Ch12 is contaminated at forward angles. 


level_energy_unit: KEV
level_comment:
L,S from 1972Ma39, 1968Ro09 report L=(1), with C{+2}S'=0.04, 1972Ma39 report L=2 with C{+2}S'=0.10, and 1977Ch12 report L=(1,2) with C{+2}S'=0.03,0.05. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T From 1970Ha01. Other: 3.3 ns {I4} from |g(t) measurement and values are not corrected for feeding from the 777 level (1980Sa07). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
T other: 39 fs {I+30-20} (1971Iy03). This value is in error since the 2705|g used by the authors is a doublet (see 1978Ka32 in (|a,n|g)). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E,J IAS of 7/2- g.s. in {+51}V; |DE(Coulomb)=8145 {I5}. Value deduced from Q({+3}He,t) relative to Q(g.s.) from (p,n). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: D
level_comment:
T$from 320|g(t) in 2022Ba21. Other: 30.97 d {I390} and 31.25 d {I289} from the inner and outer Ga targets, respectively. Extracted from the fit to the saturation in production rate data due to {+71}Ge and {+51}Cr activities in 2022Ba21. 
E,J$From the Adopted Levels of {+51}Cr in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
rms charge radius=3.6424 fm {I21} (2004An14). others: rms charge radius=3.61 fm {I8}, muonic x-ray (1962Jo05), rms charge radius=3.674 fm {I15} (1976Li19) (e,e'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+. 
T$From Coulomb Ecitation. Other: 0.69 ps {I+31-17} ({+3}He,d|g) and >0.49 ps (n,n|g). 
MOMM1$Others: +3.0 {I5} (1987St07) and +3.2 {I22} (1987Pa28) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L(|a,|a')=4. 
BE4 from weighted average of 0.00067 {I12} in (e,e') and 0.00066 {I10} in (|p{++},|p{++}),(|p{++},|p{++}'). 
T$From DSAM (Coulomb Ecitation). Others: 9.4 ps {I+24-16}, DSAM (HI,xn|g), 1.04 ps {I+35-17} ({+3}He,d|g) DSAM. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L(|a,|a')=4. 
T DSAM, from weighted average of values 1.4 ps {I+5-3} ({+3}He,d|g) and 2.5 ps {I6} (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+. 
T from (p,p'|g). Others: 0.47 ps {I+22-13}, DSAM ({+3}He,d|g), 0.42 ps {I21} (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J L(p,p')=4. 
T from weighted average of values 0.22 ps {I+8-5} ({+3}He,d|g) and 0.33 ps {I9} (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J 1968Mo19 propose the existence of two levels in this vicinity separated by 3.0 keV, one decaying by 703|g and having a spin of 3, 5 (from p,p'|g(|q)), and another with spin 2 decaying by 2038|g. Subsequent work (1977Ya08, 1974Br04) shows that a single level at 3472.2 emits two |g's (704.6 (78%) and 2038.0 (22%)) and suggests that the two-level hypothesis was a result of an error in the energy assigned to the 704|g by 1968Mo19. Furthermore, the p,p'|g(|q) data on the 2038|g (1968Mo19) were found to be consistent with 3. T{-1/2}, together with L in transfer, suggest |p=+. One further complication is the assignment of L=4 to the level by 1970Pr08 in (p,p'). L(p,p')=2+3. Thus existence of a J|p=4+ level at 3472 is tentatively ruled out. 
T RDM. Other: >1.9 ps ({+3}He,d|g), DSAM, > 0.49 ps (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
J log| {Ift}=6.15 from 6+, |g(|q) in (HI,xn|g); |p from L({+3}He,d)=1. 
T from 1.4 ps<T{-1/2}<3.8 ps, lower limit, DSAM; upper, RDM. Other: >0.76 ps in ({+3}He,d|g), and 0.10 ps 7 (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J L(|a,|a')=2, L({+3}He,d)=1. 
$B(E2)|^=0.0071 {I8} (2007En02) 
T from weighted average of values 9 fs {I3} (n,n'|g) and 9 fs {I4} (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
J log| {Ift}=6.6 from 6+, |p from L({+3}He,d)=1. 
T from weighted average of values 0.58 ps {I+32-19} ({+3}He,d|g) and 0.7 ps {I5} (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J L(|a,|a')=L(e,e')=3. 
T other: 0.27 ps {I+12-6} ({+3}He,d|g). 
B(E3) from weighted average of values 0.0065 {I4} in (e,e') and 0.0068 {I5} in (|p{++},|p{++}),(|p{++},|p{++}'). 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J L(|a,{+2}He)=5,7, L({+3}He,d)=1 from 7/2-. 
E From average of values in ({+3}He,d) and (|a,{+2}He). 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
IAS ({+52}V g.s.). Some authors identify 11256.5 state as g.s. IAS. However, from a comparison of relative M1 transition rates from 11264.9 state with Gamow-Teller |b decay matrix elements for {+52}V g.s. 1973Fa12 concluded that most of the IAS strength lies in the 11265 state. The 11256 state might still be a fragment of the g.s. IAS. 


level_energy_unit: KEV
level_comment:
$|s=86 {I7} 
S |q at 35|'. 
E: Identified as unresolved triplet of IAS of the three states in {+52}V at 0.0, 17 and 23 keV with spins 2+, 3+ and 4+. Angular distribution can be well fit by L=2+4 (can also be fit with L=3, but existence of an additional state with J|p=3- seems unlikely). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_comment:
J compared integrated cross sections with Hauser-Feshbach integrated cross sections in the same angular interval (90|' to 140|'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from |G{-|g0}=673|*10{+-6} eV {I13}. Others: resonance fluorescence: 0.55 ps {I14} (1959Of14), 0.76 ps {I21} (1964Bo22). 
$ I{-i,0}<64 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+,1-,2+
level_comment:
$B(M1)|^=0.009 {I2}; B(E1)|^=0.0000010 {I2}; B(E2)|^=0.00105 {I20} (1998En05) 
J|p=1+, 1-, 2+ for B(M1), B(E1), B(E2), respectively. 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$B(M1)|^=0.089 {I21}, B(E1)|^=0.98|*10{+-5} {I23} 
$B(M1)|^=0.075 {I24}, B(E1)|^=0.84|*10{+-5} {I26} (2000Is11) 
$B(M1)|^=0.085 {I13}; B(E1)|^=0.0000094 {I14}; B(E2)|^=0.0071 {I12} (1998En05) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$B(M1)|^=0.171 {I11}, B(E1)|^=1.88|*10{+-5} {I12} 
$B(M1)|^=0.164 {I21} (2000Is11). 
$B(M1)|^=0.19 {I4}; B(E1)|^=0.000021 {I4} (1998En05) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$B(M1)|^=0.071 {I7}, B(E1)|^=0.78|*10{+-5} {I8} 
$B(M1)|^=0.044 {I25}; B(E1)|^=0.0000049 {I28}; B(E2)|^=0.0029 {I16} (1998En05) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$B(M1)=0.124 {I9}, B(E1)=1.37|*10{+-5} {I10} 
$B(E2)|^=0.0687 {I13} (1981Ah02) B(E2)|^=0.0061 {I36} (1998En05) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$B(M1)|^=0.90 {I5} 
|G{+2}{-|g0}/|G=2.68 eV {I16} (1983Sm02). |G{+2}{-|g0}/|G=2.9 eV {I5} (1979Ku14). 


level_energy_unit: KEV
level_comment:
Ground-state rms charge radius from elastic scattering: 3.674 fm {I15} (1976Li19), 3.655 fm (1971Pe11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
BE2$from weighted average of 0.0634 {I39} (1976Li19), 0.080 {I8} (1978Po04), 0.071 {I9} (1971Pe11), 0.0761 {I30} (1975DeXW), and 0.052 {I4} (1964Be32). Other: 0.0632 (1983Li02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
|b{-2}=0.18 {I4} (1979Fu01) with B(E2) taken as 0.063 (insensitive to actual value within 20%). |b{-2}=0.25 (ion-ion nuclear potential) (1979Po16) with B(E2)=0.061 {I5}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 From weighted average of 0.066 {I3} (1975To06), 0.069 {I7} (1972WaYZ), 0.072 {I9} (1966Mc18), 0.061 {I5} (1979Po16), 0.059 {I5}, 0.054 {I5} (1979Po08), 0.060 {I15} (1960Ad01), 0.062 {I12} (1960Le07), 0.062 {I22} (1960An09), 0.048 {I2} (1965Si02), and 0.043 {I9} (1967Af03). Others: 0.061 (1976Le12), 0.0588, 0.0933 (1978Ro12). 
T Other: 0.60 ps {I9} DSAM (1972WaYZ). 


level_energy_unit: KEV
level_comment:
Broad peak interpreted by 1969Da02 as analog of state in {+52}V. 
E from weighted average of values from 1978Fo34 and 1969Da02. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_uncertain: ?
level_comment:
From the forward rise in |s(|q) typical of a J=2 state, the authors conclude that this peak probably contains the 3160 level; known to have J=2+. The evaluators note that 2964 level, also with J|p=2+, could also be contributing to this peak. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from RDM, 1974Br04. Inconsistent with T{-1/2}=2.7 ps {I+8-7} (DSAM) from 1977Be22. 1974Br04 explicitly take feeding into account, 1977Be22 make no correction. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$RDM. Others: 45 ps {I6} (1987Ba72) RDM, 2.5 ps {I6} (1977Be22) DSAM. The DSAM result appears to be incorrect. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T From 1974Po15. Others: 0.10 ps {I+8-6} (1987Ba72), 0.44 ps {I10} (1977Be22). Value of 1977Be22 not corrected for cascade feedings. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T from 1974Br04 (RDM). Other: 1.9 ps {I+7-5} (1977Be22). Value of 1977Be22 not corrected for cascade feedings. 
J from 2007Ku19. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T other: 0.7 to 4.2 ps, lower limit from DSAM, upper limit from RDM, see 1974Po15. 0.30 ps {I+17-12} (1987Ba72). 


level_energy_unit: KEV
level_comment:
E$level from literature as there was no beam setting between 8.1-8.75 MeV in the present experiment for 1+ states. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOME2 From AB/LF (atomic beam magnetic resonance/ LASER-fluorescence technique) (1982Er09). Other: see 2005St24. 
J from 1976Fu06 (ESR), L(d,p)=1 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J J=1/2 from isotropic |g to 3/2-; |p=- from L(d,p)=1 
T weighted average of values of (|a,n|g) and Coul. ex. Other: |>0.35 ps (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J |g to 3/2- is D+E2, |g from 7/2- is |DJ=1, M1(+E2), L(d,p)=3. 
T from Coul. ex. Others: <1.7 ps (|a,n|g), >0.7 ps (p,p'),(p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J |g to 3/2- is |DJ=2, E2; |g to 5/2- is |DJ=1, M1(+E2) L(d,p)=(3). 
|m=+2.8 {I49} (1989Ra17) 
T from Coul. ex. Other: <2.1 ps (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J |g to 5/2- is |DJ=1, M1(+E2), |g to 3/2- is |DJ=2, E2, L(d,p)=(3). 
T other: 0.80 ps {I9} in Coul. ex. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J |g to 3/2- is M1+E2. CP(|g) in (n,|g) E=thermal L(d,p)=1. 
T from Coul. ex. Other: 7.6 fs {I35} (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T RDM. Others: >0.55 ps, DSAM (1972Ca11); 4.6 ps {I21}, DSAM (1974En04); 4.8 ps {I+55-21}, DSAM (1979Ra05). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0100 {I8} (1977Pa22). Others: 0.011 {I2} (1969Ga25), 0.0094 (1967Af03), 0.0115 {I10} (1966Mc18), 0.0118 {I8} (1961Mc18). 
T from 1973ErZZ, DSAM. Other: 50 ps {I4} from B(E2) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0116 {I9} (1977Pa22). Others: 0.020 {I6} (1969Ga25), 0.0102 (1967Af03), 0.0072 {I12} (1966Mc18), 0.011 (1973ErZZ). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0253 {I16} (1977Pa22). Others: 0.024 {I6} (1969Ga25), 0.0216 (1967Af03), 0.030 {I12} (1966Mc18), 0.027 (1973ErZZ). 
T other: 0.90 ps {I20} (1973ErZZ). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
B(E2)=0.0018 {I2} (1977Pa22). Other: 0.0022 {I9} (1969Ga25). This value corresponds to B(E2)=6.9|*10{+-5}. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J from L(t,p)=(6), |g(|q) in ({+9}Be,3n|g), 1398|g E2 to 4+. 
T other: 0.40 ps {I+8-7} (|a,p),(|a,p|g). 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J fed in |b{+-} decay by a log| {Ift}=5.69 branch from J|p=3+ and 594|g to 6+. 
T from {+51}V(|a,p),(|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: FS
level_comment:
J 820|g to 6+, cascade of the yrast levels; 2221|g to 4+. 
T other: T{-1/2}<0.12 ps from ({+9}Be,3n|g). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J from L(t,p)=3 and (pol n,|g). But L(d,p)=3 from 1964Le03 and log| {Ift}=5.69 from JPi=3+ give |p=+. 


level_energy_unit: KEV
level_spin_parity: (1-,4+)
level_comment:
E from weighted average of 4864 {I7} (p,p'),(p,p'|g) and 4866 {I5} (t,p). Unresolved doublet in (t,p) based on fit to |s(|q). 
J from L(t,p)=(1+4). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
T account has been taken of the measured target composition for those states which decay almost entirely in the target material. Other: T{-1/2}<7 fs. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E this level reported by 1979SmZQ, not confirmed by 1980St04, probably belongs to {+55}Cr (1966Ma42). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
T account has been taken of the measured target composition for those states which decay almost entirely in the target material. Other: T{-1/2}=0.30 ps. 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
E this level reported by 1979SmZQ only, not confirmed by 1980St04, probably belongs to {+55}Cr (1966Ma42). 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
J L=6 fits well in region 30|' to 90|' but the |s(|q) fit for forward angles is not good and in fact suggests presence of L=1 component. There is no evidence to indicate a possible doublet. 


level_energy_unit: KEV
level_comment:
J expected and thought to have unnatural parity requiring a multi-step process to explain its excitation. 


level_energy_unit: KEV
level_comment:
J the shape of |s(|q) can be explained by several combinations of L=1,2,4,5 and might have unnatural parity. 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
The quadrupole deformation parameter |b{-2}=0.20 from 1980Fa07. Other: |b{-2}=0.46 from |s(|q) 1971An17. 
J from |g(|q), see 1967Ab01. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$The |g factor of the first state of {+54}Cr was measured by 2001Wa36 employing the combined technique of projectile Coulomb excitation in inverse kinematics and transient magnetic fields. 
T from B(E2). 
BE2 Others: 0.079 {I20} (1959Al95), 0.057 {I11}(1960An07), 0.106 {I7} (1961Mc18), 0.100 {I10} (1966Mc18), 0.0760 {I19} (1973ToXV), 0.085 {I3} (1975To06). 
G Others: 0.56 {I10} (1977Fa07), 0.53 {I12} (1987Pa28). 
MOME2 Determined from reorientation effect (1975To06). 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
If the state is interpreted to be the result of double E2 excitation of a 4+ state, the value obtained for the ratio B(E2)(1828 keV to 835 keV)/B(E2)(835 keV to 0)=2.16 {I35} for 54Cr (1966Mc18). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MIN
level_comment:
T from 1977Co19. Others: 3.52 min {I3} (1952Fl21), 3.67 min {I25} (1954Ba57), 3.5 min {I1} (1961Ch04), and 3.59 min {I4} (1965Ko09). 
J L(t,p)=0, J|p({+53}Cr)=3/2-. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J based on |g intensities and |g(|q) feeding to and deexciting from this level in ({+11}B,p3n|g); L(t,p)=4 from 3/2- (see 1978Na06). 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J based on direct feeding intensities, consistency of 1317|g(|q) with that expected for J+2 to J transition, and 365|g is at least partially dipole in ({+11}B,p3n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_uncertain: ?
level_comment:
1972Ma66 indicate that some difficulty was experienced in resolving the 2710 level from the nearby states and as a result the data are considered accurate to only 20%. Evaluator regards this level as tentative. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J the authors assumed E1 transitions from 2031 (J|p: 5/2+) and 2098 (J|p: 9/2+) levels to 1135 level. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 |g to 0+; L(t,p)=2 
T$Weighted average of 3.81 ps {I10} (2011Se09, recoil-distance method in ({+11}B,2np|g)) and 5.0 ps {I+26-13} (2005Bu29, B(E2)(W.u.) in Coulomb excitation). Other: |>1.4 ps from DSAM in (t,p|g) (1976Ba45) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$log| {Ift}=4.6 from 1+ parent; shell-model prediction (see Fig. 13 in 2006Zh42 for a predicted 0+ state at 1991 keV). However, note that no 0+ state was found in (t,p) work of 1968Ch20 or in (t,p|g) work of 1976Ba45 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 2+; J not 0 from |g(|q) distribution 
T$from recoil-distance method in ({+11}B,2np|g) (2011Se09) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$|DJ=1, dipole |g to 2+; possible member of |g band. J=1 is less likely due to yrast-pattern of level population in ({+48}Ca,X|g) 


level_energy_unit: KEV
level_comment:
E$energy is close to that of 4448.9, (7-) level, however, it seems unlikely that L=7 is populated in (t,p) reaction 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=3.15 ps {I11} (2011Se09). Other: mean lifetime |t|<3.4 ps {I6} or <4 ps (T{-1/2}<2.8 ps) (1977Na12), without applying feeding correction from higher level(s) 


level_energy_unit: KEV
level_spin_parity: (6)
level_comment:
E$due to reversed ordering of the 587.6|g - 607.8|g cascade in the Adopted dataset, this level corresponds to 3841.2 level in the Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7-
level_comment:
L$L=7 is assigned as tentative in 1990Fi07, as experimental |s(|q) distribution of this most intense peak in the spectrum is hampered by contribution from impurities: {+14}C g.s. peak from {+12}C(|a,{+2}He) and {+18}O g.s. peak from {+16}O(|a,{+2}He){+18}O 
$Proposed configuration=|nf{-5/2}~#|ng{-9/2} (1990Fi07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+,8+
level_comment:
L$tentative assignment (1990Fi07) 
$Proposed configuration=|ng{-9/2}{+2} for 8+, |ng{-9/2}~#|nd{-5/2} for 6+ (1990Fi07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$from the Adopted Levels 
BE2,T$ deduced by evaluator from measured B(E2)(W.u.)=8.7 {I30} (2005Bu29). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: S
level_comment:
J$ log| {Ift}=5.45 {I9} to 5/2- g.s. in {+57}Mn. 3/2- in isotones (N=33) {+59}Fe, {+61}Ni and {+63}Zn 
T$ from timing of 205.8|g (1978Da04) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
E$a 1581 level is reported in {+14}C({+48}Ca,|an|g) deexciting by 639.1 {I2} and 1313.8 {I4} |g rays, I|g(1313.8|g)/I|g(639.1|g)=28 {I8}/100 {I6}. In {+57}V |b{+-} decay, a 1582 level is reported deexciting by 892.5 {I6} and 1314.3 {I5} |g rays, I|g(1314.3|g)/I|g(892.5|g)=100 {I50}/50 {I25}. Moreover 892.5|g fits poorly if placed from the same level as 639.1|g 1313.8|g, thus two levels are defined by the evaluator, although, it remains unclear why 639.1|g was missed in |b{+-} decay experiment 


level_energy_unit: KEV
level_comment:
E$it should be noted that 1314.3 {I5}+267.8 {I3}=1582.1 {I6} and 892.5 {I6}+692.4 {I4}=1584.9 {I7} differ by 2.8 {I9} keV. This suggest two separate levels near this energy. See comment in 'adopted levels', where 892.5|g and 1314.3|g are placed from two separate levels based on above discrepancy in energy sum and on results from {+14}C({+48}Ca,ang) reaction. In the latter reaction, a strong 639.1|g is also seen from a 1581 level. It is not obvious why this |g ray was missed in |b{+-} study 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_comment:
E$ |g decays from this level to predicted 5/2+ band member, |?360 keV below the 9/2+ member is not observed in 2005De34. For E|g=360 keV, detectable limit of intensity is <4%. The 1/2+ bandhead is predicted at |?120 keV below the 9/2+ member, E4 transition is unlikely. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ B(E2) deduced from |s=185 mb {I19} (2012Ba31) 
$ Other B(E2)=0.099 {I28} (2005Bu29) 
T$ deduced by compiler from B(E2) using E|g=880.7 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$other: 1.87 ps {I14} from RDDS with decay-curve analysis 
$Q{-0}=0.88 {I+7-6}, |b{-2}=0.22 (2015Br10) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_comment:
T$From 1.0 s {I4} (1985Bo49 - coin |b-1238|g(t)), 0.6 s {I3} (1988Bo06 - coin |b-112|g(t)), 0.46 s {I5} (1996Do23 - |b(t) and |b|g(t)), and 1.05 s {I9} (2005Li53 - 1238|g(t)) - using the limitation of statistical weight method (1985ZiZY). Discrepant dataset. Weighted average is 0.74 s {I6}. Values reported in 1985Bo49, 1988Bo06, and 1996Do23 are from the same research group. 1996Do23 note new value is better compared to earlier ones due to better accuracy of isotope-separation over mass-separation (1985Bo49, 1988Bo06). However, 2005Li53 verify consistency of their {+59}Cr and {+59}V half-life values. The evaluator recommends a value from these discrepant datasets. 
$Possible (|n 1/2[321]) oblate configuration (see J|p footnote). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: US
level_comment:
T from {+59}Cr IT decay (1998Gr14). 
$Possible (|n 9/2[404]) intruder oblate configuration (see J|p footnote). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$208 {i1} in Adopted Levels, based on reversed cascade of 207.1|g-102.7|g from other studies with better statistics. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$(13/2+) in table I of 2004Fr17 is a misprint (as per e-mail reply of June 7, 2004 from S.J. Freeman) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_uncertain: ?
level_comment:
E,J$1093.8, (7/2)- in table I of 2004Fr17 are misprint (as per e-mail reply of June 7, 2004 from S.J. Freeman). Level marked as questionable by evaluator based on uncertain 256|g placement. 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$(9/2)- in table I of 2004Fr17 is a misprint (as per e-mail reply of June 7, 2004 from S.J. Freeman) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from 2006Li15. T{-1/2}=0.57 s {i6} from 1988Bo06, 4|p|b time spectrum, {+60}Mn (1.77 s) activity subtracted. T{-1/2}=0.51 s {i15} if {+60}Mn g.s. is fed in |b{+-} decay, or 0.47 s {i15} if 3+, {+60}Mn (1.77 s) isomer is fed in 100% of |b{+-} decays (1996Do23), 0.4 s {i1} (1997AmZZ), 0.38 s {i3} (1995AmZX) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$ Measured excitation cross section=25 mb {I7} (2009Ao01) 
$Deformation parameter=0.23 {I3} (2009Ao01) 
$Deformation length=1.12 fm {I16} (2009Ao01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ B(E2) deduced from |s=237 mb {I17} (2012Ba31) 
T$ deduced by evaluator from B(E2) using E|g=643 keV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$other: 19.1 ps {I10} from RDDS with decay-curve analysis 
$Q{-0}=1.18 {I+8-7}, |b{-2}=0.29 (2015Br10) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$other: 3.5 ps {I3} from RDDS with decay-curve analysis 
$Q{-0}=1.23 {I+12-9}, |b{-2}=0.31 (2015Br10) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T$effective half-life, not corrected for side feeding 
$Q{-0}=1.23 {I+44-22}, |b{-2}=0.31 (2015Br10) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=703 ms, %|b{+-}n=0.69 (2003Mo09) 
$Theoretical T{-1/2}=365 ms, %|b{+-}n=0.2 (2016Ma12) 
J$possible configuration=|n5/2[303] of f{-5/2} orbital or |n1/2[301] of p{-1/2} orbital. From likelihood of |b feeding to the ground state, |n5/2[303] configuration is favored by 2005Ga01. 3/2+ in theoretical calculations (1997Mo25) 
T$weighted average of 233 ms {I11} (2009Cr02); 251 ms {I22} (1999So20,1999Le67,2001So07, also 250 ms {I110} in 2002MaZN thesis). Other: 0.27 s {I2} (1998Am04) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$Possible configuration=|n5/2[303] of f{-5/2} orbital or |n1/2[301] of p{-1/2} orbital. From likelihood of |b feeding to the ground state, the former configuration is favored by 2005Ga01. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
J$proposed by 2020On01 as |n3/2[321] state 
T$from Adopted Levels of {+61}Cr in the ENSDF database (March 2019 update) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(n)({+61}Cr)+x, where S(n)=3880 {I220} (2017Wa10: AME2016); x<8437 {I38} from Q(|b{+-})-S(n), Q(|b{+-})=12317 {I310} 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_comment:
E$y corresponds to quasicontinuum from 2.26 to 12.0 MeV, with pseudo-levels in 50 keV bins up to 3.2 MeV, and in 100 keV bins up to 3.95 MeV, and in 200 keV bins up to 12.0 MeV. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 209 ms {I12} (2005Ga01) and 190 ms {I30} (1998Am04). 2005Ga01 state that fit to their decay curve could be achieved only when attributing a short half-life of 92 ms {i13}, not a longer one of 671 ms for {+62}Mn. Other: 187 ms {I15} (1999So20, from the same group as 2005Ga01) 
$Calculated %|b{+-}n=1 (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$Measured excitation cross section=38 mb {I6} 
$Deformation parameter=0.27 {I3} 
$Deformation length=1.36 fm {I14} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$other: 91 ps {I4} from RDDS with decay-curve analysis 
$Q{-0}=1.36 {I+8-6}, |b{-2}=0.33 (2015Br10) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$other: 4.8 ps {I5} from RDDS with decay-curve analysis 
$Q{-0}=1.44 {I+9-8}, |b{-2}=0.35 (2015Br10) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E$1399, first excited 0+ predicted from shell-model calculations (2021Ga02). The second 2+ state is predicted at 1899 keV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ B(E2) deduced from |s=377 mb {I30} (2012Ba31) 
T$ from peak-shape analysis (2012Ba31) 
$ B(E2)=0.1605 {+302-246} deduced from half-life 
$ B(E2)=0.1625 {I220} gives T{-1/2}=99 ps {I+15-12} 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_comment:
J$from systematic trends in neighboring nuclides 
T$from 2005Ga01 (also 2003So21). Others: 128 ms {I8} (2011Da08,2002MaZN), 113 ms {I16} (1999So20,1999Le67), 110 ms {I70} (1998Am04); 161 ms {I+104-91} (2004NiZY, preliminary) 
T$115 ms {I16} in 1999Le67 is likely a misprint. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Only the |b{+-} decay mode has been observed, thus 100% |b{+-} decay is assigned by inference 
$Theoretical T{-1/2}=90.6 ms, %|b{+-}n=3.0 (2019Mo01) 
$Theoretical T{-1/2}=40.7 ms, %|b{+-}n=0.6 (2016Ma12) 
T$weighted average of 44 ms {I3} (2011Li50,from decay curves for |g rays); 42 ms {I2} (2011Da08,2002MaZN) and 43 ms {I1} (2005Ga01, 2003So21), and 44 ms {I12} (1999So20, implant-|b correlated decay curve). In 2011Da08 and 2005Ga01, values are from time correlation between implantation and |b-ray events in the DSSSD, the fitting procedure included five parameters: |b-detection efficiency, background rate, mother, daughter and granddaughter half-lives. Other: 61 ms {I+60-19} (2004NiZY,2005NiZZ) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced from B(E2)|^=0.156 {I40} (2013Cr02), determined in intermediate-energy Coulomb excitation 
J$Coulomb excited state 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$2156, first 6+ predicted from shell-model calculations (2021Ga02), where the second 2+ state is predicted at 1827 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$Angle-integrated Coulomb excitation |s=333 mb {I83} 
T$deduced from B(E2)|^=0.156 {I40}, using adopted E|g=429 {I3} 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E$2156, first 6+ predicted from shell-model calculations (2021Ga02), where the second 2+ state is predicted at 1827 keV 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_comment:
$2005Ga01: no significant |b{+-}n, %|b{+-}n=5.45, %|b{+-}2n=0.32 (Theory). 
T$From 2005Ga01, 2003So21 
J$From systematics 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$ based on time correlation between implantation and |b-ray events in the DSSSD. Fitting procedure included five parameters: |b-detection efficiency, background rate, mother, daughter and granddaughter half-lives (2011Da08) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 23 ms {I4} (2011Da08, implant-|b(t)) and 24 ms {I2} (2011Li50, implant-|b(t)). Others: 10 ms {I6} (2005Ga01,2003So21, implant-|b(t)) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E$assuming that observed events correspond to the g.s. 
T$limiting value from ~360 ns time of flight through the separator as in 2005St29 (similar experimental setup as 2009Ta05). Actual half life is expected to be much longer as suggested by the calculated value of 26 ms (1997Mo25). 
$This level is expected to undergo |b-delayed neutron emission with a calculated value of %|b{+-}n=15 (1997Mo25). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Theoretical values: %|b{+-}n=21, %|b{+-}2n=6.5 (1997Mo25) 
$ 5/2+ from theoretical prediction (1997Mo25) 
$ Measured production cross section=0.025 pb {I+13-14} using {+9}Be target, and 0.42 pb {I+74-31} using W target (e-mail reply of May 22, 2013 from O. Tarasov, first author of 2013Ta14). 
T$ time-of-flight=620-650 ns (considered by the evaluator to be about the same as in 2009Ta24, which was communicated to the evaluator in e-mail reply of Sept 23, 2009 from O. Tarasov). Actual half-life is expected to be much longer as suggested by the theoretical value of 19 ms for |b{+-} decay mode (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_uncertain: ?
level_comment:
$Only one event was found to be consistent with {+70}Cr 
T$lower limit estimated from time-of-flight of |?620 ns as in 2009Ta24 (same lab as 2013Ta14). Actual half-life is expected to be much longer as suggested by the value of 14 ms from theoretical calculations (2003Mo09) 
E$assuming observed event corresponds to the ground state of {+70}Cr. 
$Theoretical calculations give %|b{+-}n=35, %|b{+-}2n=2.5 (2003Mo09). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
T$upper limit estimated from expected production rates (1992Bo37). 
J$1- or 4- from |W{-p}=5/2- and |W{-n}=3/2+ (theory, 2019Mo01); 2- from systematics (2021Ko07) 
$Theoretical T{-1/2}(|b)=9 ms (2019Mo01) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: MS
level_comment:
$%|ep: from 2007Do17. Others: 58 {I9} (2001Gi01, earlier value from the same group as 2007Do17); 22 {I2} (1992Bo37) 
J$ T=2 quadruplet in {+46}Sc (g.s.,4+), {+46}Ti (9168,4+,tentatively identified as IAS of {+46}Sc g.s.), {+46}Cr (9152 state) and {+46}Mn (g.s.). Superallowed type |b{++} decay (log {Ift}|?3.4) to the 9152 level of {+46}Cr is consistent with this interpretation 
T$ from 2007Do17. Others: 34.0 ms {+45-35} (2001Gi01, earlier value from the same group as 2007Do17); 41 ms {I+7-6} (1992Bo37) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ This state is expected to decay by proton emission. The 2p decay mode is energetically possible but predicted rate is small. From measurements in 2007Do17, only 7.9% {I32} proton branch is known, with no evidence for 2p decay mode 
E$ IAS of {+46}Fe g.s. For energy, see detailed comment in {+46}Fe |e decay 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$ from 2007Do17. From IMME analysis using mass excesses of -43135 {I2} for {+46}Ca IAS, -37636 {I5} for {+46}Sc IAS, and -29970 {I6} for {+46}Ti IAS, 2007Do17 obtain mass excess of -7473 {I61} for IAS in {+46}Mn and +759 {I96} for g.s. in {+46}Fe. Further using mass excess=-12490 {I30} for {+46}Mn g.s., excitation energy of 5017 {I71} is obtained for IAS in {+46}Mn (2007Do17). 
$ This state is expected to decay by proton emission. The 2p decay mode is energetically possible but predicted rate is small. From measurements in 2007Do17, only 7.9% {I32} proton branch is known, with no evidence for 2p decay mode (2007Do17,2001Gi01) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J$from 2003Au02 (systematics) 
T$from 1996Fa09 (from the whole spectrum including |b{++} particles and protons) 
%ECP$from 1996Fa09. E(p)=651 keV {I20} 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
E,T$from the Adopted Levels 
J$from the adopted levels. Assumed to be mirror state of the {+47}Ti g.s. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E$mean value from E(p)=5975 {I25} and E(p)=4880 {I20} and the mass excesses of {+46}Cr and {+47}Mn. Uncertainty is the sum in quadrature of 35 keV from |D(Ep) and 160 keV from the {+47}Mn mass excess uncertainty. Others: 6867 keV {I+30-160} from E(p)=5975 keV {I25} and 6868 keV {I+25-160} from E(p)=4880 lev 20. 
J$IAS of {+47}Ti 7/2-, 3226 assuming {+47}Mn g.s. is the mirror state of the {+47}Ti g.s. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MS
level_comment:
J,ISPIN$from log {Ift}=3.5 to 5792, 4+ level with T=1. 
T$from 752|g(t) in {+48}Mn |e decay, weighted average of 158.1 {I22} (1991Sz03) and 150 ms {I10} (1987Se07). 
%B+P$from comparison of Ip to I|g(752|g) measured simultaneously (1991Sz03). Other: 0.27 {I12} (1987Se07) 
%B+A$only one |b{++}-delayed |a emission observed (1987Se07). 


level_energy_unit: KEV
level_spin_parity: 1+
level_uncertain: ?
level_comment:
E$from 2281-keV proton peak, which gives a 4299-keV level in {+48}Mn, while it can also be explained as entirely feeding the 98-keV level in {+47}Cr, thus giving a level at 4399 keV in {+48}Mn (2016Or03). 


level_energy_unit: KEV
level_spin_parity: 1+
level_uncertain: ?
level_comment:
E$2281-keV proton peak, which gives a 4299-keV level in {+48}Mn, may also be explained as entirely feeding the 98-keV level in {+47}Cr, thus giving a level at 4399 keV in {+48}Mn 
$E{-p}(c.m)=2281 {I10}, %I{-p}=1.2 {I3} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
J,ISPIN from super-allowed decay to {+49}Cr g.s. 
T weighted av of 381.7 ms {I74} (1988HaZB. |b{++}'s; |DE/E scin telescope, tape transport, ms) and 384 ms {I17} (1980Ha12. g+(t); on-line isotope separator; tape-transport system. Measured for 5 to 6 T{-1/2}'s. High background). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J,ISPIN from proton decay to {+48}Cr 2+ state and systematics of T{-z}=-3/2 |b{++}-delayed proton emitters. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E from S(p)=2085 keV {I25}, E(p)=1521 keV {I46} (unweighted av. Of 1083 keV {I16} (1996Fa09) and 1161 keV {I17} (2007Do17)), and E({+48}Cr level)=752 (evaluator). 


level_energy_unit: KEV
level_spin_parity: (7/2-,5/2-)
level_comment:
E from S(p)=2085 {I25}, E(p)=1544 keV {I17} (weighted av. (int.) of 1538 keV {I24} (1996Fa09) and 1550 keV {I23} (2007Do17)), and E({+48}Cr level)=752 (evaluator). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
IAS in {+49}Mn (2007Do17) 
E from S(p)=2085 {I25}, E(p)=1977 keV {I14} (weighted av. (int.) of 1978 keV {I29} (1996Fa09) and 1977 keV {I16} (2007Do17), and E({+48}Cr level)=752 (evaluator). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E from difference in tabulated mass excesses for this state and g.s. (evaluator). |DE estimated by the evaluator. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
$T{-z}=-1/2 
$J|p from {+49}Mn Adopted Levels in ENSDF database (July 2008 update). 
T$measured by 2017Ku12 from ({+49}Mn implants)|b correlated decay curve. Others: 381.7 ms {I74} in H. Hama et al., (AIP Conf. Proc. 164, 650 (1987)) or 1988HaZB or 1988HaZD; 384 ms {I17} in 1980Ha12 (Phys. Lett. B91, 207). Value of 382 ms {I7} is listed in {+49}Mn Adopted Levels in the ENSDF database 
$Total number of {+49}Mn implanted ions=9.25|*10{+4} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
J$spin from hyperfine structure using laser-spectroscopy (2010Ch15 and e-mail replies from F. Charlwood on June 18 and June 30, 2010); super-allowed |b{++} decay to 0+. 
T$from timing of positron spectra. The adopted value is the weighted average of 283.10 {I14} (2006Ba33), 283.29 {I8} (1997Ko65; their earlier value was 284.0 {I4} (1974Ha59)), 282.72 {I26} (1976Wi08; their earlier value was 285.1 {I9} (1973Al02)) and 282.8 {I3} (1975Fr02; their earlier value was 285.7 {I6} (1965Fr08)). Others: 288 {I7} (2013Su07, decay-time spectra fitted with exponential curves), 304 {I5} (1962Su10), 295 {I1} (1958Mi84), 270 (1954Ty33), 280 {I20} (1952Ma55). All values are quoted in ms. 
ISPIN$ IAS({+50}Cr g.s.). 
$|d<r{+2}>({+55}Mn,{+50}Mn)=+0.168 fm{+2} {I4}(stat) {I53}(syst) (2016He14, hyperfine spectra using collinear laser spectroscopy on ionic transitions) 
$|d<r{+2}>({+55}Mn,{+50}Mn)=+0.046 fm{+2} {I3}(stat) (2010Ch15, laser spectroscopy at Jyvaskyla accelerator laboratory). The systematic uncertainty is |?15% 
$Isotope shift measurement: |d|n({+55}Mn,{+50}Mn)=-1573 Hz {I2} (2010Ch15, laser spectroscopy) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Penning-trap mass measurement (2008Er04). 2017Au03 (NUBASE) give 225.31 keV {I7} from mass difference 
J$spin from hyperfine structure using laser-spectroscopy (2010Ch15 and e-mail replies from F. Charlwood on June 18 and June 30, 2010); log| {Ift}=5.0 {i1} to 4+ and 6.0 {i2} to 6+ 
T$weighted average of 1.74 min {I10} (2013Su07, decay curve for |g-spectrum gated by |b rays and |DE-tof); 1.76 min {i3} (1972Ra14, decay curves for 783|g and 1098|g, 1 h counting period); 1.72 min {i4} (1962Su10, |b{++} decay curve) 
MOMM1,MOME2$ hyperfine structure using laser-spectroscopy (2010Ch15). See also 2014StZZ and 2016St14 compilations. 
%EC+%B+,%IT$%IT<7.4 from I|g(IT)/I|g(783|g)<0.02 (1972Ra14), assuming E|g(IT)|<229, and |a(229|g; M5 theory (1976Ba63))|?3. 
$|d<r{+2}>({+55}Mn,{+50m}Mn)=+0.051 fm{+2} {I16}(stat) {I53}(syst) (2016He14, hyperfine spectra using collinear laser spectroscopy on ionic transitions) 
$|d<r{+2}>({+55}Mn,{+55m}Mn)=-0.057 fm{+2} {I13}(stat) (2010Ch15, laser spectroscopy at Jyvaskyla accelerator laboratory). The systematic uncertainty is |?15% 
$Isotope shift measurement: |d|n({+55}Mn,{+50}Mn)=-1514 Hz {I8} (2010Ch15, laser spectroscopy) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$E2 799.9|g to 0+. 
T$from RDDS in {+40}Ca({+12}C,pn|g) (M.M. Giles et al., Phys. Rev. C, accepted April 9, 2019). Other: >0.7 ps (2002Pi04, DSAM in ({+12}C,pn|g)) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$3- proposed in {+50}Cr(p,n|g) from |DJ=1, D+Q |g to 2+ and |g to 1-. 4+ proposed in ({+32}S,|apn|g) based on cascade of |DJ=2 quadrupole transitions feeding this level. 612.5|g to 1- favors 3- 


level_energy_unit: KEV
level_spin_parity: (9+)
level_lifetime_unit: PS
level_comment:
J$|DJ=2, (E2) 1503.7|g to (7+); band member 
T$from DSAM (1999Br40) in ({+28}Si,|apn|g). Other: <0.77 ps in ({+12}C,pn|g) (2002Pi04) 


level_energy_unit: KEV
level_spin_parity: (15+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$1340 |g to (13+), band member 
T$fully stopped peak shape in ({+28}Si,|apn|g) for 1340|g implies that lifetime is longer than the recoil-stopping time of |?2 ps. 


level_energy_unit: KEV
level_spin_parity: 15+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$fully stopped peak shape for 1340|g implies that lifetime is longer than the recoil-stopping time of |?2 ps. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from mean lifetime |t=6.4 ps {I2} (M.M. Giles et al., Phys. Rev. C, accepted April 9, 2019) using recoil-distance Doppler-shift (RDDS) and differential decay curve method (DDCM). Other: >0.7 ps (2002Pi04, DSAM) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E$from measured mass difference between g.s. and isomer of {+50}Mn from Penning-trap mass measurement (2008Er04). Other: 230 {I20} (1973Mc11) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$ 4-3-2 spin sequence established for 1931-1143-800 levels from the measurement of (788|g)(343|g)(|q) (2000Sc35). The |g|g(|q) data are inconsistent with J(1931)=1,2,3. Parity is from |DJ=2, quadrupole transition to 2+ and RUL 


level_energy_unit: KEV
level_spin_parity: (2+,1+)
level_comment:
J$2+ in Adopted Levels 
E$possible IAS of T=1 {I583} level in {+50}Cr. 
$|b{-2}=0.31 {I5} assuming J=2, (DWBA, 1972Fa01). 


level_energy_unit: KEV
level_spin_parity: (3+,4+)
level_comment:
J$(3+) in Adopted Levels 
E$IAS of T=1 {I1881} level in {+50}Cr. 
$|b{-4}=0.44 {I8} assuming J=4 (DWBA, 1972Fa01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from analysis of differential decay curve method applied to the unresolved Doppler-shifted components of the 149|g. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5+
level_comment:
J$listed as 4+ in 2020Ba02, however, in authors paper 2019Gi07 and in the Adopted Levels of {+50}Mn in the ENSDF database, this level has J|p=5+ 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
$|D<r{+2}>({+55}Mn,{+51}Mn)=-0.023 fm{+2} {I45} (stat) (2010Ch15). The syst uncertainty is approximately 15 % 
J$J=5/2 from atomic beam (1976Fu06) and analysis of hyperfine structure spectrum (2015Ba49); L=3 in {+50}Cr({+3}He,d). 
T$from |g(t) measurement in {+51}Mn |e decay (1970Er01, and quoted by 1973Fe12). Other: 46.5 min {I2} (1966Gl02). 
$|m=3.5683 {I13} ({+55}Mn standard,Atomic Beam Magnetic Resonance (AB), 1971Jo10,1989Ra17,2014StZZ) Other: |m=+3.577 {I4} (COLLAPS, {+55}Mn standard,2015Ba49) 
$Q=0.42 {I7} ({+55}Mn standard, AB, 1971Jo10,1989Ra17, 2014StZZ) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$L=3 in {+50}Cr({+3}He,d); J=7/2 from |g(|q) in {+50}Cr(p,|g) and {+54}Fe(p,|a|g) 
T$other: >0.7 ps in {+54}Fe(p,|a|g) (1977No01) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$Stretched E2 |g to 7/2- and |g(|q) in {+50}Cr(p,|g) rule out all J except 7/2, 11/2. Population in (HI,xn|g) both directly and by cascade |g's from higher states suggests J>7/2 (1977No01). 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$J=3/2 from |g(|q) of primary |g's in (p,|g) from states with known J|p. (M1) |g to 5/2-, (E2) |g to 7/2-, |g from 1/2+ and 1/2-. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$M1 |g to 5/2-,g.s., E2 |g to 7/2-,237. 
T$others: 40 fs {I+10-7} in {+50}Cr({+3}He,d|g), 35 fs {I+13-10} in {+54}Fe(p,|a|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$L=1 in {+50}Cr({+3}He,d), J=1/2 from |g(|q) to 5/2- and D(Q) 4349 |g from 3/2- S(p)+1059 
T$unweighted average of 0.49 fs {I+12-8} in {+50}Cr({+3}He,d|g) and 0.26 fs {I+10-7} in {+54}Fe(p,|a|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$M1+E2 |g to 5/2-, L=1 in {+50}Cr({+3}He,d) 
T$others: 39 fs {I+17-15} in {+54}Fe(p,|a|g) and 36 fs {I+9-6} in {+50}Cr({+3}He,d|g). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: FS
level_comment:
J$|g's to 9/2- and 5/2- are (M1), L=3 in {+50}Cr({+3}He,d),({+7}Li,{+6}He) 
T$other: 28 fs {I+15-13} in (p,|a|g) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E$may be a doublet in ({+3}He,d) with L=(1),(3) for 3048.6+3058.1 
J$from L=(1),(3) in {+50}Cr({+3}He,d); |g's to 7/2- and 1/2+ gives 3/2-,5/2+. 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
E$see notes of 3048.6 level. 
J$|g(|q) of primary |g's from resonance states to this level in (p,|g), L=(1),(3) in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (1/2-:7/2-)
level_comment:
E$may be a doublet: one with J|p=(1/2-,3/2-) and the other with J|p=(5/2-,7/2-). It is not known which of two members of the doublet is fed by the primary |g's in {+50}Cr(p,|g). log| {Ift}=4.98 {I13} from 5/2-, but it is not clear which level is fed 
J$L=(1),(3) in {+50}Cr({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 17/2-
level_lifetime_unit: NS
level_comment:
T$From 2005Ma81 in {+40}Ca({+14}N,2pn|g). Others: 1.52 ns {I21} in (HI,xn|g), 1.43 ns {I+6-5} from 2000Ek02 in ({+32}S,2|ap|g). 
J$E2 |g to (13/2-) and band member 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2-
level_uncertain: ?
level_comment:
J$1791|g(|q) is non-isotropic to 3/2- 2140, so J|=1/2; 2377|g(|q) from 3/2- (S(p)+1059)-keV res state gives |d=-0.05 {I3} and +4.9 {I10} or |d=-0.47 {I10} for a J=3/2 or J=5/2 level, respectively; mult (2377|g)=E1+M2 is not ruled out, since |d=-0.05 {I3} is almost consistent with zero, although mult=E1+M2 with |d=-0.47 {I10} is not allowed from RUL and |G{-|g}(2377|g). 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
J$J=(3/2,5/2) from |g(|q) of primary |g's from resonance states, |p=(-) from (M1) |g from 3/2- (S(p)+1059.1)-keV res state to this level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2- : 7/2-
level_comment:
E$may be a doublet: one with J|p=1/2-,3/2- and the other with J|p=5/2-,7/2-. 
J$L=1,3 in {+50}Cr({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
T$from 2004Du25 in ({+32}S,|ap|g). Others: 90.1 ps {I17} in (HI,xn|g) 
J$(E2) |g to (23/2-) and band member 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$From |g(|q) to lower states with known J|p (1986Di01). 
$D |g's to 1/2 and 5/2-. Possible IAS of 2970 in {+51}Cr 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$From |g(|q) to lower states with known J|p (1986Di01). 
$D |g's to 3/2- and 7/2-. |p=+ for probable IAS of 3016 in {+51}Cr 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$From |g(|q) to lower states with known J|p (1986Di01). 
$D+Q |g to 5/2-,g.s. IAS of 3263 in {+51}Cr 


level_energy_unit: KEV
level_spin_parity: (35/2)-
level_comment:
$Possible configuration=[|p(1f{-7/2}){+-3}~#|n(1f{-7/2}){+-3}]{-15+} ~#|n(1f{-5/2}). This configuration is favored by 2004Ek02 for this state, as it accounts for 80% of the yrast 35/2- wave function. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
T$from 2004Du25. The uncertainty was deduced by adding the systematic (2.1 ps) and statistical (0.8 ps) uncertainties in quadrature. The half-life was obtained by applying the recoil distance Doppler shift (RDDS) method to the 831.8|g (from 6471 level) transition in spectra taken in coincidence with low-lying |g-rays. The analysis of 704|g was hampered due to the presence of closely spaced doppler-shifted components of 723|g and 717|g from lower levels and a 701 keV background peak. 


level_energy_unit: KEV
level_spin_parity: (17/2,19/2)
level_comment:
J$Based on yrast arguments, 2004Ek02 considers the 17/2 spin assignment for this level more likely. 


level_energy_unit: KEV
level_spin_parity: 31/2,33/2-
level_comment:
J$ E2+M1 |g to 31/2-,13170. (33/2)- listed in table I of 2004Ek02 for the 3876 transition, 31/2 in 2004Ek02 for |DJ=0,2217 transition. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J from ({+3}He,d) L(p)=1, J|p=1/2- or 3/2-; for |g(|q) of S(p)+1059 to 2841-keV level there exists no solution for 3/2, but isotropic transitions of 2841 to 1825 and to 1959-keV levels are in good agreement with J|p=1/2- (1974Sc17). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MIN
level_comment:
$|D<r{+2}>({+55}Mn,{+51}Mn)=-0.023 fm{+2} {I45} (stat) (2010Ch15). The syst uncertainty is approximately 15 % 


level_energy_unit: KEV
level_comment:
L L=(0)(1967Ra14) and L=(1) (1979Pa01). |s(|q) of 1967Ra14 nearly consistent with L=1, but |s(|q) of 1979Pa01 is not consistent with L=0. 
C{+2}S': 0.02 (1967Ra14), 0.04 (1979Pa01) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T from 1959Ju40. Others: 21.3 min (1940He01), 20.1 min {I8} (1956Ru45); 22.1 min {I3} (1965Ka12). 
T stripped atom T{-1/2}({+52}Mn{+25+})=22.7 min {I30} (1995Ir01). 
J atomic beams (1976Fu06) and E4 |g to 6+. 


level_energy_unit: KEV
level_spin_parity: (5+,6+,7+)
level_comment:
J from L({+3}He,p)=6, but L=(1) reported for level at 2968 keV in (p,{+3}He). Perhaps two distinct states are involved. 


level_energy_unit: KEV
level_comment:
J L(d,|a)=3, L(p,{+3}He)=4, L({+3}He,p)=2 for contradictory assignments. Could be more than one level. 


level_energy_unit: KEV
level_spin_parity: 11+
level_lifetime_unit: PS
level_comment:
T RDM, weighted average of values 15.0 ps {I14} in {+51}V(|a,3n|g) (1987Ba72) and 15.2 ps {I14} in (HI,xn|g) (1976Av06). 


level_energy_unit: KEV
level_comment:
J L({+3}He,p)=0+2, L(d,|a)=3 for contradictory J assignments. (2)+ in ({+3}He,t) from |s(|q) compared with |s(|q) for states for known J. 


level_energy_unit: KEV
level_comment:
$|D<r{+2}>({+55}Mn,{+52}Mn)=-0.259 fm{+2} 13 (stat) (2010Ch15). The syst uncertainty is approximately 15 % 


level_energy_unit: KEV
level_comment:
$|D<r{+2}>({+55}Mn,{+52m}Mn)=-0.195 fm{+2} 5 (stat) (2010Ch15). The syst uncertainty is approximately 15 % 


level_energy_unit: KEV
level_comment:
$d|s/d|W=22 
L 1973De03 assigned L=0+2 or L=1. 1973Ga07 assigned L=3. 1971Gu03 assigned L=0, 1972Ke04 assigned L=1+3. 


level_energy_unit: KEV
level_comment:
S 1973De03 reported d|s/d|W=10 (|mb/sr) for unresolved pair and L=(4). 
L 1973Ga07 assigned L=0+2 to level at 3984 {I10}. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: Y
level_comment:
|m=5.024 {I7} (2005St24) 
J L({+3}He,d)=L(d,n)=L(d,{+3}He)=3. 
T from 1971Ho24. Others: 2.9|*10{+6} y {I12} (1971Ma18), 10.8|*10{+6} y {I45} (1969Ho35), 1.9|*10{+6} y {I5} (1965Ka10). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
MOMM1 Other: |m=2.9 {I4} (1974Ke11) 
J L(p,t)=0, L({+3}He,d)=L(d,{+3}He)=(3). 
T from (p,n|g) (1966Go19). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T from (|a,p|g) (1974Ge07). Other: >0.13 ps (p,n). 
J L({+3}He,d)=L(d,n)=L(d,{+3}He)=1, J dependence of |s(|q) in (|a,p) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T from (|a,p|g) (1974Ge07). Others: 0.14 ps {I+21-7} (p,n), 0.7 ps {I2} (1978Li21) (HI,xn|g). 
J |g to 7/2- is |DJ=2, E2 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T from 1974Ge07 (|a,p|g). Other: 0.21 ps {I+70-14} (1973Ch25) (p,n|g). 
J |g to 7/2- is M1+E2, |g to 5/2- is |DJ=2, E2 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T from 1974Ge07 (|a,p|g). Others: 0.22 ps {I+34-11} (1973Ch25) (p,n|g), >70 fs (p,|g). 
J L=0+2 component in (p,t) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T from 1979Fi08 (|a,p|g). Others: |?0.084 ps (1975Sc08) (p,|g), 0.08 ps {I+10-4} (1973Ch25) (p,n|g). 
J |g to 7/2- is |DJ=2, E2; L({+3}He,d)=L(d,n)=L(d,{+3}He)=1 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
T from 1974Br04 (HI,xn|g). Other: 14 ps {I+6-4} (1974En04) (|a,p|g). 
J |g to 11/2- is |DJ=1, M1+(E2), L(p,t)=2 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T from 1979Fi08 (|a,p|g). Others: 0.029 ps {I+42-25} (1973Ch25) (p,n|g), |?0.042 ps (1970Ma25) (p,|g). 
J |g to 7/2- is |DJ=0, D+Q. L(p,t)=2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
T from (1970Ma25) (p,|g). Other: 0.07 ps {I+9-5} (p,n|g). 
J L({+3}He,d)=L(d,n)=1, J dependence of |s(|q) in (|a,p) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T from (HI,xn|g). Other: 0.04 fs {I3} (|a,p|g). 
J |g to 11/2- is |DJ=2, E2; |g to 13/2- is |DJ=1, M1+E2. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T from 1975Sc08 (p,|g). Others: 0.11 ps {I2} (1974Ge07) (|a,p|g), 0.046 ps {I+63-30} (1973Ch25) (p,n|g). 
J L({+7}Li,{+6}He)=L({+3}He,d)=1, |g to 7/2- 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_lifetime_unit: PS
level_comment:
T from 1974Ge07 (|a,p|g) 
J log| {Ift}=5.1 via 7/2- parent, |g to 7/2- |DJ=1, D+Q, yield in (p,n|g). L(p,t)=2+4 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
T from 1974Ge07 (|a,p|g). 
J log| {Ift}=4.5 via 7/2- parent, J dependence of |s(|q) in (|a,p). L({+3}He,d)=3, L(d,{+3}He)=(3). L(p,t)=4 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T from (HI,xn|g). Other: 0.09 ps {I+4-3} (|a,p|g), 0.06 ps {I3} (|a,2n|g). 
J |g to 15/2- is |DJ=0, M1+E2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
T contradictory values from (p,|g): 27 fs {I+21-10} (1975Sc08), <4 fs (1970Ma25). 
J L({+3}He,d)=L(d,n)=1, J dependence of |s(|q) in (|a,p) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
T from (|a,2n|g). Other: <49 fs (HI,xn|g). 
J |g to 17/2(-) is |DJ=1, M1+E2, |g to 15/2- is |DJ=2, E2. 


level_energy_unit: KEV
level_spin_parity: (23/2-)
level_lifetime_unit: PS
level_comment:
T from (|a,2n|g). Other: 1.29 ps {I18} (HI,xn|g). 
J |g to 21/2- is |DJ=1, M1+E2 and linear polarization of 471|g in (HI,xn|g) (1979Gu10). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E IAS of 1/2- 564 level in {+53}Cr (see 1976Ga20) ({+3}He,d) 
J L({+3}He,d)=1, IAS of 1/2- 564 level in {+53}Cr. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J L({+3}He,d)=4 for E=9194 {I8} and |g(|q) in p,|g). (p,|g) excit by L=4 is more likely than by L=5 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$from comparison of the single-particle proton strength ({+3}He,d) of the low-lying levels in {+53}Mn with the corresponding |g strength from the deexcitation of the resonance (1983Kl03), and |g(|q) in (p,|g). 
IAS of 3/2- 2321 level in {+53}Cr, see 1991Di07. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$from comparison of the single-particle proton strength ({+3}He,d) of the low-lying levels in {+53}Mn with the corresponding |g strength from the deexcitation of the resonance (1983Kl03) 
IAS of 3/2- 2321 level in {+53}Cr, see 1991Di07. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
J$from inelastic proton angular distribution in (p,p),(p,p'),(p,p'|g). 
E$IAS of {+53}Cr 3180, (3/2-) (see 1985Oz01) (p,p),(p,p'),(p,p'|g) Res 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E IAS of {+53}Cr 3706, 9/2+ (1979Fo19) (p,|g). |g(|q) consistent with J=9/2 
J$from |g(|q) (1979Fo19) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T others: 0.43 ps {I10} (1979Fi08), <0.54 ps (1973Sa10), 0.6 ps {I2} (1972Go10), 0.8 ps {I3} (1972Br14), <2.1 ps (1974En04). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T others: 0.36 ps {I+11-8} (1979Fi08), <0.29 ps (1973Sa10), 0.46 {I+17-11} (1972Go10), 0.39 {I11}(1972Br14) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: Y
level_comment:
$|D<r{+2}>({+55}Mn,{+53}Mn)=-0.292 fm{+2} 4 (stat) (2010Ch15). The syst uncertainty is approximately 15 % 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$others: 0.55 ps {I4} (1974Ge07), 0.41 ps {I+14-10} (1979Fi08), 0.60 ps {I14} (1972Br14), 0.6 ps {I2} (1972Go10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T$others: 0.60 ps {I8} (1974Ge07), 0.43 ps {I10} (1979Fi08), 0.6 ps {I2} (1972Go10), 0.8 ps {I3} (1972Br14), 0.14 ps {I+21-7} (1973Ch25), 0.7 ps {I2} (1978Li21) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T$others: 0.48 ps {I6} (1974Ge07), 0.36 ps {I+11-8} (1979Fi08), 0.46 {I+17-11} (1972Go10), 0.39 {I11}(1972Br14), 0.21 ps {I+70-14} (1973Ch25) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$others: 0.25 ps {I5} (1974Ge07), 0.21 ps {I6} (1979Fi08), 0.33 ps {I+11-7} (1972Go10), 0.22 ps {I+34-11} (1973Ch25) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
T$From the weighted average of 134 ps {I10} and 111 ps {I8} deduced from the simulated lineshape analysis to the experimental data determined by using a reduced |h{+2} at both 37{+|o} and 90{+|o} of SeGA rings, respectively. The uncertainty includes the statistical error and an overall systematic error due to the ambiguities in the geometry of the setup, |g-ray anisotropy effects and an additional systematic error of |DT{-1/2}=11 ps (half the difference between the two independent half-life results) to account for the uncertainty in the target position. The lifetimes of the observed feeding states are < 1 ps and therefore not included to the T{-1/2} analysis. 
$|s{-exp}|?12%. Shell Model predicts a very small cross section. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$|s{-exp}|?12%. Shell Model predicts a very small cross section. The authors stated that the cross section data indicated that the depopulating 1117.5|g is a doublet transition. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: Y
level_comment:
$|d<r{+2}>({+55}Mn,{+53}Mn)=-0.270 fm{+2} {I12(stat)20(syst)} (atomic), and -0.285 fm{+2} {I7(stat)20(syst)} (ionic) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: D
level_comment:
%B- others: %|b{+-}=0.9|*10{+-4} (1997Za07). %|b{+-}<3.9|*10{+-5} (1997Ki37), %|b{+-}<2.9|*10{+-4} From log| {Ift}>14.1 expected for a 3+ to 0+ transition (1993Da20), %|b{+-}<4.4|*10{+-6} from log| {Ift}>13.3 expected for a 3+ to 0+ transition. Partial T{-1/2}(|b{+-})>4|*10{+4} y (1989Su08). Partial T{-1/2}(|b{+-})>2.95|*10{+5} y (1993Da20), Partial T{-1/2}(|b{+-}): between 1|*10{+6} y and 2|*10{+6} y (1996Du15). Partial T{-1/2}(|b{+-})>2.2|*10{+4} y (1997Ki37). Partial T{-1/2}(|b{+-})=9.3|*10{+5} y (1997Za07). Partial T{-1/2}(|b{+-})=6.3|*10{+5} y {I13} (1998Wu01), Partial T{-1/2}(|b{+-})=9.2|*10{+5} y (1999Za19). 
%EC+%B+ %|b{++}=1.20|*10{+-7} {I26}(1998Wu01), %|b{++}=1.8|*10{+-7} {I8} (1997Za07,1999Za19), %|b{++}<5.7|*10{+-7} (1993Da20), %|b{++}<8|*10{+-5} (1968Be01). Partial T{-1/2}(|b{++})=7.1|*10{+8} y {I15} (1998Wu01), Partial T{-1/2}(|b{++})=4.7|*10{+8} y (1997Za07). Partial T{-1/2}(|b{++})=4.7|*10{+8} y {I21} (1999Za19). Partial T{-1/2}(|b{++})>1.5|*10{+8} y (1993Da20). 
MOMM1,MOME2$Compiled by 2011StZZ. 
T from limitation of relative statistical weighted average of 312.32 d {I9} (2010Va13), 312.1 d {I9} (2006Da20), 312.028 d {I34} (2002Un02), see also 1992Un01, 1991UnZZ), 312.6 d {I5} (2000Hu20), 312.11 d {I5} (1997Ma75), 312.02 d {I4} (1982HoZJ), 312.15 d {I12} (1982RyZX), 312.21 d {I5} (1979MeZY), 312.6 d {I8} (1974Cr05), 312.2 d {I3} (1968La10), 312 d {I5} (1968Ha47), and 312.40 d {I10} (1966Va26). Others: 311.12 d {I82} (2008AdZX), 315.40 d {I3} (1973Vi13), 312.99 d {I10} (1968Zi01). See also 1974MeZY, 1965An07, and 1965Ta10. 
J J=3 from electron paramagnetic resonance and dynamic nuclear orientation (1976Fu06); |p from L({+3}He,d)=L(d,n)=3. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
|m=3.4 {I+28-16} 
J 54|g to 3+ is M1, J=2, 4, from |g(|q) in (p,n|g). Observed yield and calculated excitation functions rule out J=4; however, very poor agreement is observed between the CCBA curve for J=2 or 3 and the experimental curve in (t,{+3}He) from 1985Aj03. 
MOMM1 From gT{-1/2}=83 ps {I28} (1974Ke11) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T unweighted average from RDM: 209 ps {I17} (|a,n|g), 157 ps {I44} ({+11}B,5n|g), 193 ps {I+28-83} ({+7}Li,3np|g). 
MOMM1 gT{-1/2}=236 ps {I42} from 156.2|g (|q,H) in (p,n|g) (1974Ke11). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
MOMM1 gT{-1/2}=52 ps {I28} from 211|g (|q,H) in (p,n|g) by 1974Ke11. 
T Weighted average values from 6.3 ps {I13} in (|a,n|g), (p,n|g) and 7.2 ps {I11} in ({+7}Li,3np|g). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
|m=2.8 {I15} 
|m: from gT{-1/2}=104 ps {I55} (1974Ke11) 
T Weighted average values from 221 ps {I8} in (|a,n|g), (p,n|g) and 202 ps {I35} in ({+7}Li,3np|g). 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: FS
level_comment:
E existence of a doublet at 1374 keV, see (p,n|g) (1976Be14). 
J L(d,|a)=L({+3}He,p)=2, M1+E2 |g to 2+. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E from (pol d,t), (d,t). 
J from angular distribution, spectroscopic factor in (pol d,t) and a rapidly decreasing cross section at forward angles in (pol d,|a). 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
T weighted average from 0.84 ps {I+94-31} (|a,pn|g) and 0.69 ps {I+55-28} (|a,n|g), (p,n|g). Other: 0.7 ps>({+11}B,5n|g). 
J$Based on |g(|q), linear polarization and ch**2 analysis in (|a,pn|g), J|p=5+ or 7+ was yielded, |g from 2867-keV 8+ state excludes 5+. So 1979To05 assigned J|p=7+ for the level. L((pol d,t),(d.t))=3. But from coincidence angular anisotropy and coincidence linear polarization measurement in {+51}V({+20}Ne,X|g), 2008Ki14 indicated J|p=7(-) for the level. Negative-parity level at such a low-excitation energy has not been observed in the neighbouring odd-odd nuclei. J|p=7- is tentatively assigned. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: FS
level_comment:
J L({+3}He,d)=1, |g deexcited to 3+, 5+, analyzing power fitted by some f7/2 strength, CCBA fit of angular distribution in (t,{+3}He) shows J=4+. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J L({+3}He,d)=0, unnatural parity from T20 in (pol d,|a). L(p,{+3}He)=1+3 confirms J|p=2-, L(d,|a)=2, in disagreement with these results. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J from |g(|q), linear polarization, DCO ratios and |g decay in (|a,pn|g) and yield function in (|a,n|g). 
T other: <6.93 ps (|a,pn|g). 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_comment:
J L(t,{+3}He)=4+6 for a composite peak. |g's to 2+, 3+, 4+. The |g to 2+ suggests possibility that the (p,|g) reaction is also populating the 2881 level; otherwise, this decay mode is not consistent with J|p=5+. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
J from f7/2 transfer in (pol d,t), L(t,{+3}He)=4+6, |g(3213) to 3+, |g(3158) to 2+, and |g(3056) to 4+. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E unweighted average of values in (d,t), (t,{+3}He), (d,n), and (pol d,|a), (d,|a), (p,{+3}He). 
J L(p,{+3}He)=(0+2). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E unweighted average of values in ({+3}He,p), and (pol d,|a), (d,|a), (p,{+3}He). 
J L(p,{+3}He)=(0+2). 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3+)
level_comment:
E unweighted average of values in ({+3}He,p) and (pol d,|a), (d,|a), (p,{+3}He). 
J L(p,{+3}He)=(2). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
gT{-1/2}=83 ps {I28} from 54.4|g(|q,H) (1974Ke11). 
T from theoretical g factor and gT{-1/2} (1974Ke11). 
J J=2,4 from |g(|q). Excit rules out J=4. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: D
level_comment:
$|D<r{+2}>({+55}Mn,{+54}Mn)=-0.165 fm{+2} 7 (stat) (2010Ch15). The syst uncertainty is approximately 15 % 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: D
level_comment:
$|d<r{+2}>({+55}Mn,{+54}Mn)=-0.177 fm{+2} {I12(stat)10(syst)} (atomic), and -0.166 fm{+2} {I8(stat)10(syst)} (ionic) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J J=5/2 from atomic beam method (1989Ra17 and 1979De19); |p=- from L(n,d)=L(d,{+3}He)=L({+3}He,d)=3. 
MOMM1 Measured values uncorrected: 3.4438 {I20} (1967Mi04), +3.437 {I5} (1967Es04), 3.4420 {I15} (1967Dy02), 3.4460 {I11} (1971Sa16), +3.4614462 {I22} (1974Lu08). 
MOME2 Other measurements: +0.40 {I2} (1969Ha22) and +0.35 {I5} (1962Wa30). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J from |g(|q) and M1+E2 |g to 7/2-. 
T from Coul. ex.; others: 0.28 ps {I12} (p,p'|g), 0.33 ps {I+16-11} (n,n'|g), 0.31 ps {I+10-6} (|a,p|g), 0.69 ps {I7} (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_comment:
J (|a,|a') suggests 11/2+ in the state at 1289 level; it appears to be populated by a L=3 transition (1969Ga15). (p,{+3}He) and (d,|a) give L=0+4+6, and 4, respectively. Evaluator notes that L=4+6 and L=4 assignments are based on the assumption that J=11/2; evaluator cannot determine if other L values also fit the data. L=0 component in (p,{+3}He) but not in (d,|a) suggests a second level with J|p=1/2-. A level is also suggested by L=1 in (d,n). 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: PS
level_comment:
E 1293 level in (|p{++},X|g) may correspond to 1292.18 level. 
J |p=- from E2 |g to 7/2-; J=11/2 from |s(E) Hauser-Feshbach analysis in (n,n'). Evaluator notes that J|p assignment of 1292 level is not unique; see 1972Sa38. 
T others: 1.1 ps {I8} (p,p'|g), 0.64 ps {I+49-21} (n,n'|g), 2.3 ps {I+29-10} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E evaluator assumes that 1293 level is distinct from 1292.18 level. 
J L(p,{+3}He)=0 and |s(|q) in (d,|a) yield 1/2-. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J L({+3}He,d)=L(d,{+3}He)=1; M1+E2 |g to 5/2- g.s. 
T others: 90 fs {I20} (n,n'|g), 49 fs {I+9-11} (|a,p|g), and 120 fs {I42} (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: FS
level_comment:
J L(d,{+3}He)=L({+3}He,d)=3, M1+E2 |g from (9/2)-. 
T weighted average of 9 fs {I2} (n,n'|g), 19 fs {I3} (p,|g), and 11 fs {I8} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=AP
level_comment:
E observed only in Coul. ex. 
J M1+E2 |g to 9/2- and 5/2-. 
T calculated from B(E2), branching, and |d values. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J M1+E2 |g to 9/2- and 5/2-. 
T weighted average of 16 fs {I4} (n,n'|g) and 24 fs {I3} (p,|g); others: 17 fs {I+9-12} (|a,p|g), 19 fs {I10} (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J L(d,n)=L({+3}He,d)=1; M1 |g to 5/2-. 
T weighted average of 25 fs {I2} (n,n'|g) and 18 fs {I3} (p,|g); others: 15 fs {I6} (|a,p|g), 67 fs {I28} (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: FS
level_comment:
J |p=- from M1+E2 |g to 3/2- and 5/2-; J=5/2 from |s(|q) DWBA analysis in (d,{+3}He). 
T others: 140 fs {I40} (n,n'|g), 148 fs {I+57-21} (|a,p|g), 28 fs {I14} (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (1/2)
level_comment:
E from (p,p'). 
J value from 2285 level in 1975An12 based on the Hauser-Feshbach analysis. 
T 20 fs {I4} if g.s. branching=100% and B(E2)=0.0154 {I30}. 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J |g(|q) in (|a,p|g), M1+E2 |g to (11/2)-. 
T others: 0.110 ps {I+18-6} (p,p'|g), 67 fs {I+28-24} (|a,p|g), and 60 fs {I+9-5} (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J |p=- based on E2 |g to 5/2-; J=5/2 based on |g(|q) in (n,n'|g). 
T weighted average of 24 fs {I3} (n,n'|g), 33 fs {I11} (|a,p|g), and 21 fs {I3} (p,|g). Other: <7 fs (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: LE 9/2-
level_lifetime_unit: FS
level_comment:
J L(p,p')=2. 
T weighted average of 18 fs {I4} (n,n'|g) and 15 fs {I5} (|a,p|g). Other: 114 fs {I+80-40} (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J L({+3}He,d)=L(d,{+3}He)=L(|a,p)=1; M1+E2 |g to g.s. 5/2-. 
T weighted average of 7 fs {I2} (n,n'|g), 8 fs {I2} (p,|g), and 12 fs {I6} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J J from |g(|q) to g.s. |h{+2} fit and long T{-1/2} of 2727 level in (|a,p|g); |p from 1435|g(E2) to (11/2)- and RUL. 
T weighted average of 1.25 ps {I14} (|a,p|g) and 0.71 ps {I14} (n,n'|g). Other: >693 fs (p,|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-,9/2-
level_lifetime_unit: FS
level_comment:
J L(d,|a)=2+4 from 1/2-; but 7/2 was ruled out by 868.6 |g(|q) to 5/2-, 7/2- 1884 in (|a,p|g). 
T weighted average of 22 fs {I3} (p,|g) and 33 fs {I5} (n,n'|g); other: 14 fs {I+28-14} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
J from |g(|q) in (n,n'|g). Comparison of |G (2873.2|g) to RUL excludes |D|p=yes. 
T other: 110 fs {I+40-20} (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J from |g(|q) in (n,n'|g), E2 |g to 5/2-. 
T weighted average of 14 fs {I2} (n,n'|g) and 12 fs {I2} (p,|g); other: 37 fs {I+6-8} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: FS
level_comment:
J L(d,{+3}He)=3; |s(|q) in (d,{+3}He) suggests J=7/2 
T weighted average of 20 fs {I4} (n,n'|g) and 10 fs {I2} (p,|g). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: FS
level_comment:
J from L(p,p')=(1) and |s(E|g,|q) in (n,n'|g). 
T others: 15 fs {I8} (|a,p|g) and 21 fs {I7} (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: FS
level_comment:
E evaluator notes that in (p,|g), there are two lifetimes (17 fs {I3} and 83 fs {I21}) for 3036.3 level which correspond to two |g transitions, 2910.4 and 769.9, respectively. Evaluator therefore assumes that 3036.3 level in (p,|g) involves two levels which may correspond to 3035.92 and 3037.9 levels, respectively. 
J from |g(|q) in (n,n'|g) and |G (2909.7|g). 
T weighted average of 52 fs {I4} (n,n'|g) and 40 fs {I8} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: PS
level_comment:
J L(|a,|a')=3. Comparison of |G's (1522.5|g,2925|g) to recommended upper limits allows only 3/2+, 5/2+. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J 1/2, 3/2, and 5/2 are allowed from |g(|q) and T{-1/2} in (|a,p|g). 
T other: 3 fs {I+12-3} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: (13/2)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=?
level_comment:
J comparison of |G (2049.8|g) to recommended upper limits excludes |D|p=yes. 
T no uncertainty given. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
E from ({+3}He,d). 
J L({+3}He,d)=3; in both ({+3}He,d) and (|a,p), the authors made DWBA analyses, but gave different J values: (5/2) and (3/2). Evaluator adopts (5/2) based on analyses. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E probably doublet. 
J 1/2-,3/2- and 3/2+,5/2+ based on |s(|q) DWBA analysis for L=1 and 2; the fit for L=1 looks better. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
Configuration=(|p f{-7/2}){+-3} (1969Ra02) 
E from (p,p') (1957Ma22). 1969Ra02 observed for weak transitions. With small cross sections to the state. 


level_energy_unit: KEV
level_comment:
L assignment applies to 4997+5026+5058+5085 levels; strengths are about 0.05, 0.06, 0.07, and 0.12 for each level. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
T from unweighted average values of 0.21 ps {I3} (1981Ka46) and 0.062 ps {I18} (1989Ge09). 
J adopted value is 5/2-. 


level_energy_unit: KEV
level_comment:
$B=0.078 
L evaluator assumes that the assignment applies to strongest member of 3037+3045+3050 triplet. 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
$ Integrated cross section (eV*b)=45.0 eVb {I37}. This cross section data were normalized by 2008Be31 to that of the 2211-keV transition in {+27}Al and its known strength. 
$ 2008Be31 point out that their measured cross section is in better agreement with results from 1968Al13: Nucl Phys A 116, 281 (1968) and using adopted branching ratios from ENSDF database than with the widely discrepant lifetime data as listed in ENSDF database. 
$ The measured cross section for 1884-keV state was used to normalize NRF data for {+235}U 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: H
level_comment:
MOMM1 Other: +3.218 (1969Fu11) 
T from |g(t) measurement (1992An13). Others: 2.585 h {I1} (1968Sh07), 2.576 h {I2} (1953Ba12), 2.581 h {I3} (1953Ba48), 2.574 h {I3} (1953Lo09), 2.587 h {I6} (1972Em01), 2.573 h {I4} (1968Re04), 2.586 h {I5} (1950Bi20), 2.578 h {I8} (1968Go22), 2.578 h {I9} (1968La10), 2.591 h {I8} (1965Li11), 2.5764 h {I8} (1969MeZW), 2.8 h (1983Va33), 2.5785 h {I2} (1973La12), 2.54 h {I3} (1986Ku20), 2.581 h {I3} (1988No03), and 2.73 h (1989Ah03). See also 1994Ya02. 
J J=3 from atomic beam (1976Fu06) and |p=+ from L({+3}He,p)=2 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J J=4 from |g(|q) of 212|g to 3+ g.s. in {+48}Ca({+11}B,3n|g) and |p=+ from L(d,p)=1. 
T other: |<0.5 ns in {+55}Mn(n,|g). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: NS
level_comment:
Configuration=(|f7/2 p{-3/2})5+ 
J J=5 from |g(|q)'s of deexciting |g's in {+48}Ca({+11}B,3n|g) and |p=+ from L(d,|a)=4. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: PS
level_comment:
J |p=+ from L(d,p)=1. |g(|q) of 476|g to (4)+ 716 gives J=(4,5) in {+48}Ca({+11}B,3n|g); L(d,p)=1 rules out J=(5). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: H
level_comment:
$|d<r{+2}>({+55}Mn,{+56}Mn)=+0.081 fm{+2} {I15(stat)10(syst)} (atomic), and +0.053 fm{+2} {I12(stat)10(syst)} (ionic) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$Total intensity=17% {I3} per decay, for total cascade energy=7270 to this level; only 70% {I5} of it is observed and resolved (2019Kn02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Total intensity=13% {I3} per decay, for total cascade energy=7243 to this level; only 70% {I7} of it is observed and resolved (2019Kn02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$Total intensity=5.0% {I10} per decay, for total cascade energy=7160 to this level; only 51% {I9} of it is observed and resolved (2019Kn02) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$Total intensity=16.0% {I20} per decay, for total cascade energy=7058 to this level; only 49% {I5} of it is observed and resolved (2019Kn02) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$Total intensity=6.0% {I10} per decay, for total cascade energy=6929 to this level; only 40% {I6} of it is observed and resolved (2019Kn02) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
J predominantly L=0 transfer in (t,p) 
T from 1978Wy02; unweighted average of T{-1/2}(122|g)=87.2 s {i9} and T{-1/2}(136|g)=83.7 s {i18} (Ge(Li), |?6 T{-1/2}'s). Others: 92.4 s {i30} from 1969Wa12 (|b|g(t)(122|g,136|g),scin,Ge(Li); 122|g,136|g,692|g(t), Ge(Li)). See also 1977Au04 


level_energy_unit: KEV
level_energy_info: ;ERR=GE;ERR=?
level_uncertain: ?
level_comment:
E energy of state could not be determined. From |g|g data in ({+13}C,3np|g) and ({+15}n,2n|a|g), a state with E|>1228 should be fed 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
Note that L=2,4 in (t,p) suggesting the possibility of two distinct states. However, this was the weakest group observed in (t,p) and, therefore, assumption of relative s-state for transferred neutrons may not be valid 


level_energy_unit: KEV
level_energy_info: ;ERR=GE;ERR=?
level_uncertain: ?
level_comment:
E energy of state could not be determined. From |g|g data in ({+13}C,3np|g) and ({+15}n,2n|a|g), a state with E|>3287 should be fed 


level_energy_unit: KEV
level_energy_info: ;ERR=GE;ERR=?
level_uncertain: ?
level_comment:
Energy of state could not be determined. From |g|g data in ({+13}C,3np|g) and ({+15}n,2n|a|g), a state with E|>3287 should be fed 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-,5/2-
level_comment:
J (1/2-) from a fit to a peak at 1064 representing this and the next level (1978An10); J=1/2 to 5/2 from p|g(|q) (1976Ma03) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
$|d<r{+2}>({+55}Mn,{+57}Mn)=+0.185 fm{+2} {I15(stat)19(syst)} (atomic), and +0.202 fm{+2} {I11(stat)19(syst)} (ionic) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
T$from DSAM analysis of 988|g (2023Kl03). Lifetime is corrected for feeding from the long lived second excited 11/2- level. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
E$the group in (t,{+3}He) is a broad group with a spacing of 35 keV {I15}, implying that there may be another level near 35 keV 
J$strong |b feeding (log| {Ift}|?4.9) to 0+. Shell-model calculations in the full {Ifp} space (2006Li15) predict 4+ g.s. and 1+ as the first excited state. First 0+ in this calculation is predicted above 1.5 MeV. The {+60}Mn nuclide also has 1+ g.s. and 4+ isomer (2006Li15). J|p=2+,3+ assigned from |s(|q) in (t,{+3}He) is inconsistent, which may be due to the complex structure of the lowest energy group in (t,{+3}He) that is assigned (1985Aj02) to the g.s. 
T$from timing of |b decay curve (1969Wa10). Other: 2.4 s {I9} (1988Bo06) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%IT$ B(M3)(W.u.) values in ENSDF database for A=45-90 mass region. The highest value of B(M3)(W.u.)=4.8 {I10} in this mass region gives %IT<20, but B(M3)(W.u.)=0.159 {I12} for a similar M3 transition in {+60}Mn gives %IT=0.5. 
T$from timing of |b, |g and ce; weighted average of 66 s 6 (1961Ch04), 65 s {I1} (1969Wa10), 65.3 s {I7} (1971Dy01,1972Dy01), 65.1 s {I11} (1978Wy02) and 69 s {I2} (1993ScZS,timing of 72-keV |g and corresponding ce(K) line). 
J$M3 |g to 1+; See also comment for g.s. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
J$|g's to (3+) and (5+); |s(|q) and coupled-channels analysis in {+58}Fe(t,{+3}He). 
E$679 {I10} level in (t,{+3}He) is associated with 661.1 level from ({+48}Ca,p2n|g), based on J|p analogy, although, the energy matching is somewhat poor 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
J$0+ for g.s. and 3+ for isomeric state were proposed by 1993ScZS 
T$weighted average of 66 s 6 (1961Ch04), 65 s {I1} (1969Wa10), 65.3 s {I7} (1971Dy01), 65.1 s {I11} (1978Wy02) and 69 s {I2} (1993ScZS) 


level_energy_unit: KEV
level_spin_parity: 2+,3+
level_comment:
E,L$broad group, possibly two unresolved levels with a spacing of 35 keV {I15} (1985Aj02) or 30 keV {I10} (1977Fl03)) 
J$2+,3+ is inconsistent with (1+) in 'adopted levels'. This inconsistency may be due to unresolved structure of the lowest group in (t,{+3}He) 
$d|s/d|W=3.7 |mb/sr (1977Fl03) 


level_energy_unit: KEV
level_comment:
E$unresolved states with possible spacing of |?30 keV. Possibly corresponds to the 65.4-s isomer, J|p=(4+) 
E$ 77 8 (1977Fl03) 
$d|s/d|W=2.8 |mb/sr (1977Fl03) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$|s(0|'-53|')/|s(DW)=1.5 {I3} (1984Aj03), d|s/d|W=6.4 |mb/sr for 665 level (1977Fl03) that corresponds to 651+679 (1985Aj02) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
$|d<r{+2}>({+55}Mn,{+59}Mn)=+0.316 fm{+2} {I10(stat) 37(syst)} (atomic), and +0.297 fm{+2} {I21(stat) 37(syst)} (ionic) (2016He14) 
J 5/2 from analysis of hyperfine structure (2015Ba49). Allowed |b{+-} decay to 3/2- and 5/2- levels in {+59}Fe. 
T From |b(t) (2001Oi02). Other: 4.6 s {I1} from composite decay curve for 287|g, 473|g, 571|g, 591|g, and 726|g in {+59}Mn |b{+-} decay (1977Pa18). 
MOMM1,MOME2$from 2016Ba44 (collinear laser spectroscopy). Other: |m=+3.493 {I2} (2015Ba49 - same research group of 2016Ba44) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$252.1|g M1 to 9/2-, 1188.7|g E2 to 7/2- 
T$from measured mean lifetime |t=2.63 ps {i40} using RDDS method (2017Kl01). 


level_energy_unit: KEV
level_spin_parity: (13/2)
level_uncertain: ?
level_comment:
E$ ordering of the 181-297 |g cascade is not established. Reversed ordering will give a level at 2922 keV, different from the 2922, 15/2- level. 
J$297.4|g D to (11/2) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
Double giant dipole resonance (double GDR); not a discrete level. 
E from {+59}Co(|p{+-},|p{++}). 
$|G from (|p{+-},|p{++}). 


level_energy_unit: KEV
level_spin_parity: (13/2)
level_uncertain: ?
level_comment:
E$ ordering of the 181-297 |g cascade is not established. Reversed ordering will give a level at 2922 keV, different from the 2922, 15/2- level 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
J$from log| {Ift}=4.5 to 0+ (2006Li15) is consistent with G-T decay. Systematics show that |b{+-} log| {Ift} values in the 3.6 to 6.4 range are inconsistent with 0+ to 0+ decays (1973Ra10). J|p is consistent with M3 |g-ray from 271-keV level. 
T$from 2006Li15. T=51 s {I6} (1988Bo06, was not confirmed in 1993ScZS, since T{-1/2} was very similar to that of Indium isomers detected in the spectra) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
%B-,%IT From %IT/%|b{+-}=0.13 {I1} (from 1985Ru05, 1988Bo06; details not given) 
J$271-keV M3 |g ray to J|p=1+ g.s., J|p=4+ from shell-model calculations (2006Li15) 
T$from 1988Bo06. Other: 1.79 s {I10} (1978No03) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
T$from 2006Li15. Other: 51 s {I6} (1988Bo06); however, 1993ScZS were not able to confirm the value of 1988Bo06 since T{-1/2} was very similar to that of Indium isomers detected in the spectra 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_uncertain: ?
level_comment:
E$ placement of 114|g and isomer energy are uncertain. Level has not been included in Adopted Levels, Gammas. 
J$ from shell-model predictions 
T$ Measured in 2009Fo05 from time correlations between implanted {+60}Mn nuclei and |g-ray events. 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_lifetime_unit: S
level_comment:
$Other %|b{+-}n=0.6 {I1} from 2000HaZL is not adopted, as values for other Mn isotopes in this work are in disagreement with published data. 
$Theoretical T{-1/2}=224 ms, %|b{+-}n=0.02 (2003Mo09) 
$Theoretical T{-1/2}=5.7 s, %|b{+-}n=0.4 (2016Ma12) 
J$spin from analysis of hyperfine structure spectrum in 2015Ba49, using collinear laser spectroscopy. Spin of 7/2 gave unrealistically large and negative static quadrupole moment of -5.6 {I8}. Parity from probable allowed |b feeding of (3/2-) g.s. in {+61}Fe from {+61}Mn decay. Large-scale shell-model calculations, and systematics of ground states of odd-A Mn nuclei suggest 5/2-. 
MOMM1,MOME2$from collinear laser spectroscopy technique at ISOLDE-CERN (2016Ba44) The moments were measured with reference to |m=+3.46871790 {I9} (1974Lu08) and Q=+0.33 {I1} (1979De19) for {+55}Mn. Earlier value: |m=+3.534 {I1} (2015Ba49 and 2015He10, from the same group as 2016Ba44). See also 2017Ne04 review article from the same group. 
$|d<r{+2}>({+55}Mn,{+61}Mn)=+0.504 fm{+2} {I15}(stat) {I53}(syst) for atomic transitions; +0.504 fm{+2} {I5}(stat) {I54}(syst) for ionic transitions (2016He14, from hyperfine structures using collinear laser spectroscopy at ISOLDE-CERN) 
$Isotope shift: |d<|n>({+55}Mn,{+61}Mn)=1843 MHz {I7}(stat) {I25}(syst) for atomic transitions; 1215 MHz {I2}(stat) {I27}(syst) for ionic transitions (2016He14, from hyperfine structures using collinear laser spectroscopy at ISOLDE-CERN) 
J$large-scale shell-model predictions and systematics of ground states of odd-A Mn nuclei. Probable allowed |b feeding of (3/2-) g.s. in {+61}Fe from {+61}Mn decay supports this assignment, and also suggests the same parity for the ground states of {+61}Mn and {+61}Fe 
T$weighted average of 0.708 s {I8} (2013Ra17, decay curves for several |g rays) and 0.71 s {I1} (1985Ru05, from |g timing). Other: 623 ms {I10} (1999Ha05, method not given, possibly |b-fragment correlations). Low and discrepant value from 1999Ha05 is probably due to mixture of some impurities. Values obtained from |g-ray measurements, being more specific, are preferred here. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)
level_comment:
J$2009Cr02 suggested (3/2-,5/2-) based on apparent log| {Ift} value, competing (assumed M1) transitions to (5/2-), g.s. and (1/2-,3/2-), 1142 level 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1+)
level_lifetime_unit: MS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$ systematics of even-A Mn nuclei (2010Ch51) support (1+) as the ground state and (4+) as the isomer, however, there is no experimental evidence as yet for the placement of the 92-ms and 671-ms states. 
$ Calculated (1997Mo25) %|b{+-}n=0.03 
T$from 1999So20. Others: 84 ms {I10} (M. Hannawald, thesis, Mainz, 1998), 2005Ga01 deduced half-life of g.s. of {+62}Cr, their decay curve could be fitted only by attributing a shorter half-life of 92 ms {I13} for {+62}Mn, not a longer one of 671 ms 
J,E$from syst of neighboring even Mn nuclides (2010Ch51). Possible |b feeding of (0+) state in {+62}Fe. Possible configuration= K=1/2- proton state coupled to K=1/2- neutron state (2011Li50). Large-scale shell-model calculations by 2010Sr03 predict 2+ ground state for GXPF1A and KB3G interactions. 2005Ga01, in their shell-model calculations, predict 2+ using KB3G interaction with 4+ at 453 keV, but 1+ using KB3 interaction with 4+ at 360 keV. 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (4+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J,E$ from systematics of neighboring even Mn nuclides (2010Ch51). (3+) is less likely but not completely ruled out. 2005Ga01, in their shell-model calculations, predict 4+ at 360 keV using KB3 interaction, which also predicts a 1+ ground state. Possible configuration=|pf{-7/2}~#|np{-1/2} (2011Li50) 
T$from 1999Ha05. Other: 0.88 s {I15} (1983Ru06, |b|g(t), |?5 half-lives). Weighted average of the two values is 671 ms {I7} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_uncertain: ?
level_comment:
E$2005Ga01 propose the existence of this level and its de-exciting 1215 |g ray based upon the difference in intensities of the 355 and 285 transitions, which indicates an additional |b-decay branch to the 285 level. The observed 1215|g transition accounts for the missing intensity. 


level_energy_unit: KEV
level_spin_parity: (2+,3+)
level_comment:
E$72 keV {I+8-3} above the 671-ms, (4+) isomer in 2015Ga38 from GOSIA calculations comparing the observed yields to a range of different B(E2) transition strengths as a function of excitation energy. 
J$From the GOISA calculations and the comparison of the similar levels in neighboring isotopes and isotones in 2015Ga38. 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_lifetime_unit: S
level_comment:
J$spin from analysis of hyperfine-structure spectrum in 2015Ba49; parity from systematic trends in Mn isotopes. 
T$weighted average of 0.275 s {I4} (1999Ha05), 0.322 s {I23} (1999Le67,1999So20), 0.24 s {I3} (1997AmZZ), and 0.25 s {I4} (1985Bo49). Other: 0.29 s {I2} (1995AmZX, statistical uncertainty only) 
MOMM1$from collinear laser spectroscopy, with |m({+55}Mn)=+3.46871790 {I9} from 1974Lu08 as reference (2016Ba44). Quoted value is the evaluated value from the 2019StZV evaluation, based on the original value of +3.441 {I3} in 2016Ba44 and the evaluated |m({+55}Mn)=+3.4669 {I6} in 2019StZV. Other: +3.435 {I4} (2015Ba49, previous measurement of 2016Ba44). 
MOME2$from collinear laser spectroscopy, with Q({+55}Mn)=+0.33 {I1} from 1979De19 as reference (2016Ba44). See also 2021StZZ compilation 
$|d<r{+2}>({+55}Mn,{+63}Mn)=+0.706 fm{+2} {I13(stat)69(syst)} (atomic), and +0.704 fm{+2} {I10(stat)69(syst)} (ionic) (2016He14). 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: MS
level_comment:
$|d<r{+2}>({+55}Mn,{+64}Mn)=+0.873 fm{+2} {I14}(stat) {I76}(syst); isotopic shift |d|n({+55}Mn,{+64}Mn)=+2566 MHz {I6}(stat) {I35}(syst) (2016He14, also 2015He10 and 2017Ne04; hyperfine spectra for atomic transitions using collinear laser spectroscopy) 
$%|b{+-}n=2.7 {I6} in 2012Pa39, determined from the absolute intensity of the 995-keV |g ray (from {+63}Fe |b{+-} decay) as 43% {I8} and the total number of {+64}Mn decays. Other: 33% {I2} (2000HaZL, from |b and n measurements) 
J$spin from hyperfine structure, collinear laser spectroscopy (2015He28), parity from possible allowed |b feeding from 0+ parent 
T$weighted average of 90 ms {I9} (2011Da08, also 2002MaZN, fitting of the implant-|b correlated decay curve, including background rate, and half-lives of mother, daughter and grand-daughter activities, at GANIL); 91 ms {I4} (2005GaZR, |b-fragment correlation, at GANIL); 89 ms {I4} (1999Ha05, |b-fragment correlation at ISOLDE-CERN, also 2000HaZL). Others: 85 ms {I5} (1999So20, |b-fragment correlations, also 1999Le67, earlier conference reports from GANIL); 140 ms {I30} (1998Am04, |b-implant correlated decay curve at GSI, earlier value was 170 ms {I20} in 1995AmZY). The value from 1998Am04 agrees within 1.5|s, but is much less precise, and it does not affect the adopted half-life. 
MOMM1,MOME2$from hyperfine structure using collinear laser spectroscopy technique (2015He28, see also 2015He10 and 2017Ne04) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J$(M2)-(E1) cascade to 1(+) 
T$weighted average of 400 |ms {I40} (2011Li50, decay curves for |g rays); 0.50 ms {I5} (2005GaZR, |g(t)). Other: >100 |ms (1998Gr14) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$weighted average of 400 |ms {I40} (2011Li50, decay curves for |g rays); 0.50 ms {I5} (2005GaZR, |g(t)). Other: >100 |ms (1998Gr14) 
E$in the ce spectrum a line corresponding to E|g=175 {i10} seen and interpreted as sum line of 135+40 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MS
level_comment:
%B-N$2024Vo03 take precise value from NERO detector measurements. Other: 1.37 {I14} deduced from TAGS spectrum above 7.5 MeV, with an assumption by 2024Vo03 that all the events above S(n)({+64}Fe)=7405 {I7} keV emanate from the |b{+-}-delayed neutron activity in {+64}Mn. 
$Compiler's note: there may be some competition with |g activity from higher-energy levels. 
T$measured by 2024Vo03 from (implants)|b-correlated decay curve. Authors compared their measurement with T{-1/2}=90 ms {I4} in {+64}Mn Adopted Levels in the ENSDF database (Nov 2021 update). 
J$2024Vo03 quote measurement by 2015He28 (Phys. Rev. C 92, 044311). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J$From syst (2003Au02). 
T$From 2003So21. Others: 100 ms {i8} (1999So20, erratum), 88 ms {i4} (1999Ha05), 110 ms {i20} (1998Am04) 
%B- No significant |b{+-} delayed neutron emission (2005Ga01). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J$From syst (2003Au02). 
T$From 2003So21. Others: 100 ms {I8} (1999So20,1999Le67), 88 ms {I4} (1999Ha05), 110 ms {I20} (1998Am04) 
$Observation of 364 |g ray from |b- decay of {+65}Mn in |?50% of the cases, is very similar to feeding of 54% {I2} deduced for this line from the direct |b-decay of {+65}Mn. 2005Ga01 concluded that |b-delayed neutron emission scarcely occurs for this nuclide. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T Weighted average of 64 ms {I2} (2003So21), 66 ms {I4} (1999Ha05), 62 ms {I14} (1999Le67,1999So20), 90 ms {I20} (1998Am04). 
Measured production cross section=3.1|*10{+-6} mb 25 (1992We04) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: MS
level_comment:
T$from 574|g(t) (2018St18) 
%B-N$deduced from 364|g intensity and ground state feeding intensity of {+66}Mn to {+65}Fe (2018St18) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
T$from 2003So21. T{-1/2}=42 ms {I4} (1999Ha05) measured delayed n. Other: 1995CzZZ 
J$from systematics expected configuration=(n,f5/2) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E$Population of this level in one-proton removal from {+68}Fe is difficult to be explained. Possible contributions from non-sudden dissipative process of {+68}Fe(p,p){+68}Fe{+2+}(p,2p){+67}Mn multi-step reaction are also possible. 


level_energy_unit: KEV
level_spin_parity: >3
level_lifetime_unit: MS
level_comment:
E$assuming that observed events correspond to the g.s. 
T$weighted average of 29 ms {I4} (2011Da08), 28 ms {I8} (2003So21), and 28 ms {I4} (1999Ha05). 
%B-N$from existence of |b-delayed neutrons (1999Ha05). This level is expected to undergo |b-delayed neutron emission with a calculated value of %|b{+-}n=13 (1997Mo25). 
J$suggested by non observation of |b feeding to the (2+) state in {+68}Fe (2011Da08). 


level_energy_unit: KEV
level_spin_parity: (0-,2+)
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) gated on 521|g, 865|g, 1250|g, and 1514|g (2015Be32). Other: 38.3 ms {I36} from implant-|b(t) (2015Be32). |DT includes both statistical and systematic uncertainty. 
%B-N$deduced as free parameters in the fit to implant-|b(t) curves (2015Be32). 
J$as proposed by 2015Be32 based on shell model calculations and observed |b-feeding pattern to states in {+68}Fe. 2015Be32 note that the decay scheme is most likely incomplete and the assignment is tentative. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J$from systematics 
T$from weighted average of 18 ms {I4} (2011Da08) and 14 ms {I4} (1999Ha05) 
%B-N$23.62 estimated from theory (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) gated on 135|g, 325|g, 355|g, 521|g, and 1207|g (2015Be32). Other: 24.1 ms {I26} from implant-|b(t) (2015Be32). |DT includes both statistical and systematic uncertainty. 
%B-N$deduced as free parameter in the fit to implant-|b(t) curves (2015Be32). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) in 2015Be32; |DT{-1/2} includes both statistical and systematic uncertainty. 
%B-N$deduced as free parameters in the fit to implant-|b(t) curves (2015Be32). 


level_energy_unit: KEV
level_comment:
$%|b{+-}=100; %|b{+-}n=? ; %|b{+-}2n=? ; %|b{+-}3n=? 
$ Decay mode has not been experimentally detected. As |b{+-} decay, followed by delayed-neutron emission, is the only possible decay, 100% |b{+-} decay is assigned by inference. 
$ Theoretical T{-1/2}=7.4 ms, %|b{+-}n=43, %|b{+-}2n=2, %|b{+-}3n=0 (2019Mo01) 
$ Theoretical T{-1/2}=18.5 ms, %|b{+-}n=85.5, 87.1; %|b{+-}2n=1.26, 2.1; %|b{+-}3n=0.008, 0.046 (2021Mi17) 
$ Based on A/Q spectrum and Z versus A/Q plot, three counts were assigned to {+71}Mn isotope. (Q=charge state). As stated by 2010Oh02, misidentification of {+71}Mn isotope is not possible since no events were observed for hydrogen-like peaks. 
$ Measured |s=4 pb (2010Oh02), systematic uncertainty |?50% 
E$ it is assumed that the observed activity is associated with the ground state of {+71}Mn 
T$ half-life of {+71}Mn decay has not been measured. It is expected to be >637 ns from time-of-flight in 2010Oh02, as communicated to one of the evaluators by T. Kubo in an e-mail reply of July 14, 2010. From a trend of decreasing half-lives with increasing neutron number in neutron-rich nuclei, half-life is expected to be <20 ms, based on measured half-lives of 19.9 ms for {+70}Mn, 22.1 ms for {+69}Mn and 33.7 ms for {+68}Mn. 
J$ 5/2- from systematics (2021Ko07); |W{-p}=5/2- orbital (2019Mo01, theory). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$ Theoretical values: %|b{+-}n=48.7, %|b{+-}2n=14.9 (1997Mo25) 
$ 5/2- for valence proton orbital and 7/2+ for valence neutron orbital from theoretical prediction (1997Mo25) 
$ Measured production cross section=0.0056 pb {I+64-42} using {+9}Be target (e-mail reply of May 22, 2013 from O. Tarasov, first author of 2013Ta14). 
T$ time-of-flight=620-650 ns (considered by the evaluator to be about the same as in 2009Ta24, which was communicated to the evaluator in e-mail reply of Sept 23, 2009 from O. Tarasov). Actual half-life is expected to be much longer as suggested by the theoretical value of 7.3 ms (1997Mo25) 


level_energy_unit: KEV
level_comment:
$Theoretical T{-1/2}=5.9 ms, %|b{+-}n=66, %|b{+-}2n=5 (2019Mo01). %|b{+-}3n=3.0 (2003Mo09). 
$Theoretical T{-1/2}=11.6 ms, %|b{+-}n=85, %|b{+-}2n=3.0, %|b{+-}3n=0.8 (2016Ma12). 
$Only the |b{+-} decay mode is expected, accompanied by delayed neutron decays 
J$|W{-proton}=5/2 (theory,2019Mo01) 
T$half-life of the {+73}Mn activity has not been measured. It is expected to be greater than the time-of-flight of few hundred ns through the beam transport system. From systematics of half-lives of neighboring Mn isotopes, the half-life is expected to be <20 ms (19.9 ms for {+70}Mn, 16 ms for {+69}Mn and 28 ms for {+68}Mn), assuming a decreasing trend of half-life as neutron number increases in neutron-rich nuclei. 
$Three counts assigned to {+73}Mn by 2017Su15, which are assumed here to correspond to the g.s. activity of {+73}Mn 
$Measured production |s=1.4|*10{+-11} mb {I+14-8} (2017Su15) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
J from systematics (2003Au02) 
T$weighted average (internal) of 4.7 ms {I+34-14} (2002Gi09), 3.2 ms {I+26-10} (2002Pf02), 1.6 ms {I+5-3} (2005Do20), and 3.5 ms {I+16-8} (2007GiZZ). 6.0 ms {I+17-3} (2001Gi02) seems discrepant. 
%2P$others: 70|<%2p|<80 (2002Gi09) and |?80 (2002Pf02) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Relative branches of delayed proton decay: %|ep=63 {I8}, |e2p=26 {I7}, %EC3P=11 {I5} (2007Mi36). The %|e+%|b{++} branch=30 {I4} assumes that all |e+|b{++} decay events are followed by delayed proton decays. 
T$ time distribution of 2p- and |b-decay events using maximum likelihood method (2007Mi36,2007Mi40,2009MiAA) 
T$partial half-life for |e+|b{++} decay=8.7 ms {i13} (2007Mi36,2009MiAA) 
T$partial half-life for 2p decay mode=3.7 ms {I4} and |G{-2p}=1.23|*10{+-19} MeV {I+15-12} (2007Mi40,2009MiAA) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
$%2p branching is in agreement with previous measurements of 65% {I5} (2008Bl03: Rev. Prog. Phys. 71, 046301) and 70% {I4} (2009Mi29: Eur. Phys. J. A42, 431). 2012Au08 recommend an average value of 68% {I3} from the three above measurements 
$From proton spsctrum, measured total decay energy=1.21 MeV {I5}. The protons share equally the decay energy and are emitted simultaneously. This value is in agreement with previous measurement of 1.151 MeV {I15} (2008Bl03) 
J$from systematics (2012Au07: NUBASE-2012) 
T$determined by 2012Au08 from the time difference between implantation events and subsequent decay events with maximum-likelihood analysis. This value agrees well with previous measurement with values of 2.5 ms {I2} (2008Bl03) and 2.6 ms {I2} (2009Mi29). 2012Au08 recommend an average T{-1/2}=2.56 ms {I14}. Partial half-life for 2p decay mode=3.76 ms {I26} determined from total T{-1/2} and branching ratio 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
%ECP$other: 36 {I20} (2001Gi01, earlier value from the same group as 2007Do17) 
T$ from 2007Do17, time correlation of implantation events due to {+46}Fe and subsequent emission of protons and/or |g rays. Others: 12.0 ms {+42-32} (2001Gi01,2001Gi02, earlier results from the same group as 2007Do17, note that half-life of 9.7 ms {I+35-43} is also listed in 2001Gi01 in their figure 13 and table 6); 20 ms {I+20-8} (1992Bo37) 
$No delayed 2p decay seen (2001Gi01), in agreement with predicted %|e2p/%|ep=0.10 (1991De26) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from 2014Po05, time correlation of implantation events due to {+46}Fe and subsequent emission of protons, and using the maximum likelihood method. Other measurement: 13.0 ms {I17} (2007Do17). 2014Po05 give an average value of 14.0 ms {+14-13} from their measurement and that from 2007Do17: Nucl. Phys. A 792, 18 (2007) 
$%|ep from 2014Po05 using T{-1/2}=14.0 ms {I+14-13} for {+46}Fe. Other %|ep=79 {I4} (2007Do17) 
$%|e2p=0.4 {I6} given by 2014Po05 is listed here as 0.5 {I5} to avoid non-physical negative branching ratio 
$Production |s=25 pb {I12} (2014Po05) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
J$systematics (2003Au02) 
T$from 2001Gi01. Other: 27 ms {I+32-10} (1992Bo37; 13 protons detected; maximum-likelihood method) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 51 ms {I3} (2016Or03), 45.3 ms {I6} (2007Do17), 44 ms {I7} (1996Fa09). 
$%|ep: weighted average of 14.4 {I7} (2016Or03) and 15.9 {I6} (2007Do17). Other: >3.6 {I11} for E(p)=959 keV {I33} (1996Fa09). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$proposed by 2007Do17 based on comparisons with the mirror nucleus {+48}Ti and the neighboring {+50}Fe isotope. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
J,ISPIN from systematics of T{-z}=3/2- |b{++}-delayed proton emitters (1996Fa09) 
T From 2007Do17. Others: 75 ms {I10} (1970Ce02), 70 ms {I3} (1996Fa09) 
%B+P From 2007Do17. Other: |>52 {I10} (1996Fa09. Sum of Ip(1083)=4 {I1}, Ip(1538)=5 {I1}, and Ip(1978)=42 {I10}) 


level_energy_unit: KEV
level_energy_info: ;OFF=X+825;ERR=?
level_spin_parity: (3/2+)
level_comment:
E$ the energy of this state could not be determined since subsequent decays from the 5/2- state were not observed. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$T{-z}=-1 
T$weighted average of 152.1 ms {I6} (measured by 2015Mo01 at RCNP-Osaka from {+50}Fe implants and |b correlated events); and 150.1 ms {I29} (measured by 2015Mo01 from |g-decay curves). Other values: 145 ms {I13} (measured by 2017Ku12 at GANIL from ({+50}Fe implants)|b correlated decays); and 155 ms {I11} (measured by 1997Ko46 at Chalk River from decay curve for 651|g). Values from 2017Ku12 and 1997Ko46 are in agreement with values from 2015Mo01 but much less precise, and do not affect the weighted averaged value. 
$2017RuZX conference report gives half-lives of g.s., same results as in 2015Mo01 and 2017Ku12. 
%ECP,%ECA$Q(|ep)=3568 keV {I9} for {+50}Fe suggests that this nuclide may be a possible delayed proton emitter, but such branches would be weak compared with the superallowed |b transition. Low value of Q(|e|a)=180 keV {I60} would also not allow competition with the superallowed |b transition. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$angular distribution pattern in Pb({+50}Fe,{+50}Fe') is consistent with |DJ=2, quadrupole excitation. 
T$from B(E2)|^=0.140 {I30} in Pb({+50}Fe,{+50}Fe'|g). Note that in the 2010 update (2011El01, the value of 1.5 ps {I3} was erroneous, as it was missing a multiplicative factor of (2J+1), where J=2. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(p)({+50}Fe)+x, where x<12750 {I75} from Q(|e)({+50}Co)-S(p)({+50}Fe), S(p)({+50}Fe)=4145 {I9} (2017Wa10) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E$from E(p)(c.m.)=2772 {I12}, S(p)({+50}Fe)=4145 {I9} (2017Wa10) and E({+49}Mn, 11/2-)=1541.31 {I25} (from Adopted Levels for {+49}Mn in ENSDF database). E(p)(c.m.)=2772 {I12} is the weighted average of E(p)=2790 {I41} (1996Fa09), E(p)=2770 {I12} (2007Do17). 
E$identified as IAS of (6+) g.s. of {+50}Co based on strong |e decay to this level with log| {Ift}=3.32. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from B(E2). Note that in the 2010 update of {+50}Fe (2011El01), the value of 1.5 ps {I3} was erroneous, as it was missing a multiplicative factor of (2J+1), where J=2. 
J$angular distribution pattern is consistent with E2 excitation. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
J log| {Ift}=4.86 to 7/2- and log| {Ift}=5.5 to 3/2-. 
T from av of 308 ms {I5} (|b (t), 2015Sh16), 301 ms {I4} (|b (t), 2013Su07), 305 ms {I5} (1988HaZD), 310 ms {I5} (1984Ay01), 298 ms {I14} (237|g(t), 1989Ho13), Others: 360 ms {I100} (1825|g(t), 1989Ho13), 245 ms {I7} (1977Ho25). 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: NS
level_comment:
T$from 2000Ek02. 15% systematic uncertainty not added. 
J$ |DJ=1 d |g to (15/2-),3276 and |DJ=2 Q |g to (13/2-),2953. 


level_energy_unit: KEV
level_spin_parity: (27/2-)
level_lifetime_unit: PS
level_comment:
J$ |DJ=2 Q |g to (23/2-),6492. 
T$from 2004Du25. The uncertainty was deduced by adding the systematic and statistical uncertainties in quadrature (by evaluators). The half-life was obtained by applying the recoil distance Doppler shift (RDDS) method to the 777 and 704 transitions in spectra taken in coincidence with low-lying |g-rays. 


level_energy_unit: KEV
level_spin_parity: 27/2-
level_lifetime_unit: PS
level_comment:
T$from 2004Du25. The uncertainty was deduced by adding the systematic (2.1 ps) and statistical (1.1 ps) uncertainties in quadrature (by evaluators). The half-life was obtained by applying the recoil distance Doppler shift (RDDS) method to the 777 transitions in spectra taken in coincidence with low-lying |g-rays. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: MS
level_comment:
T$ from decay-time spectra fitted with exponential curves (2013Su07). Combining present and previous results, 2013Su07 recommend 303 ms {I3} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: H
level_comment:
T from 1974Ro18. Others: 8.23 h {I4} (1967Pa22). 
T stripped atom T{-1/2}({+52}Fe{+26+})=12.5 h {I+15-12} (1995Ir01). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2) (Coulomb excitation). Other: >0.7 ps DSAM {+50}Cr({+3}He,n|g). 
J from L({+3}He,n)=L(p,t)=2. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$1998Ur05 determined the lifetime of this level from the best fit of the experimental spectrum with that obtained after summing the calculated line shape of the 2035 |g-ray and the experimental line shape of the 2045 contaminant line from {+49}Cr. 
J from E2 |g to 6+. 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
E$from 2005Ga20; others: 6957.3 keV {I5} (2003Ax01,2004Ur02) and 6820 keV {I130} (1998Ur05). 
T from 1979Ge02. 
$Hindered E4 decay of the 12+ isomer in 28SI(28SI,2P2NG). 
J from E4 |g to 8+. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
A doublet with energy splitting of 4 keV in (p,t). 
IAS ({+52}Cr g.s., {+52}Mn 2926 keV) in {+54}Fe(p,t) and {+50}Cr({+3}He,n). 
J from L({+3}He,n)=L(p,t)=0. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T 1998Ur05 determined the lifetime of this level from the best fit of the experimental spectrum with that obtained after summing the calculated line shape of the 2035 |g-ray and the experimental line shape of the 2045 contaminant line from {+49}Cr. 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: S
level_comment:
%IT=0.009 {I3} (2005Ga20) 
E from 2005Ga20; Others: 6957.3 keV {I5} (2003Ax01,2004Ur02) and 6820 keV {I130} (1998Ur05). 
T from adopted levels. 
$Hindered E4 decay of the 12+ isomer (1998Ur05). 


level_energy_unit: KEV
level_comment:
$(|s/2|p)(|mb)=4.7 
This level appears to correspond to 6390 keV {I20} level of 1977Su01 and 6380 keV {I30} level of 1971Vi03. 1977Su01 and 1978De18 assigned L=4. 1971Vi03 assigned L=5. 


level_energy_unit: KEV
level_comment:
$(|s/2|p)(|mb)=7.3 
Identified as IAS ({+52}Cr g.s., {+52}Mn 2926 level). See 1978De18, 1971Vi03, 1978Ko27. 


level_energy_unit: KEV
level_comment:
$(|s/2|p)(|mb)=1.4 
Identified as IAS ({+52}Cr 1434 keV, {+52}Mn 4390 keV), see 1978De18 and 1971Vi03. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured isotope shift: |d|n({+56}Fe,{+52}Fe)=-1.839 GHz {I3}(stat) {I6}(syst) (2016Mi27) 
$Measured differential charge radius: |d<r{+2}>({+56}Fe,{+52}Fe)=-0.034 fm{+2} {I13} {I110}; |d<r{+2}>({+54}Fe,{+52}Fe)=+0.282 fm{+2} {I14} {I73} (2016Mi27); in each case, the first uncertainty is the quadratic sum of the statistical and systematic uncertainties for isotope shifts, and the second uncertainty is from atomic factors 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured |t=7.00 ps {I24}(stat) {I28}(syst) (from text in 2017Ar09; rounded to 7.0 ps {I4} in authors' Table 2); narrow gate was set on the shifted part of the 1535|g (first 4+ to first 2+ transition), and the lifetime was determined using the upstream detector ring, since a contaminant in the range of the shifted part of the 849|g (first 2+ to g.s. transition) did not permit the lifetime analysis in the forward detector ring. Measured value in the present work is compared to the previously measured mean lifetime |t=11.3 ps {I14} (2004Yu07: Phys. Rev. C70, 034301). The analysis using only the one detector-ring combination was checked for consistency with an independent analysis of the lifetime of the first 2+ state in {+50}Cr. 
$B(E2|_: 4+ to 2+)/B(E2|_: 2+ to 0+)=1.14 {I+32-21} (2017Ar09), where authors used B(E2: 4+ to 2+) from {+52}Fe Adopted dataset in the ENSDF database. Compiler obtains 1.14 {I+41-26} using the limiting values. The value from 2017Ar09 is compared to the previous B(E2) ratio of 1.83 {I+57-38} (compiler obtains 1.85 {I+88-51} using limiting values). 


level_energy_unit: KEV
level_spin_parity: 6+
level_comment:
E$IAS of {+52}Co g.s. with J|p=6+ 
$A possible 516|g to 5141 level would be masked by annihilation radiation at 511 keV 


level_energy_unit: KEV
level_spin_parity: 12+
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E$from measured mass excess=-48330.67 keV {I60} for g.s. of {+52}Fe and -41370.01 keV {I65} for the 45.9-s, 12+ isomer (2017Ne05). Value is 6958.0 keV {I4} in {+52}Fe Adopted Levels in the ENSDF database, based on |g-ray data 
J$from {+52}Fe Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
T from weighted average of 8.51 min {I2} 1965Eb01, 8.51 min {I25} (1976Bo19), 8.45 min{I12} (1968De27), 8.80 min {I24} (1961Ra06), 8.5 min {I3} (bare)(1995Ir01); see also 1959Ju40, 1954Nu22. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J$ From angular distributions and correlations of both populating and depopulating transitions of level. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M1
level_comment:
T from weighted average of 2.58 min {I3} (1967Es06), 2.51 min {I2} (1968De27), 2.65 min {I6} (1974FiZI). 2.48 min {I5} (bare) (1995Ir01). 
J from analysis of B(EL)(W.u.), B(M+L)(W.u.) and I|g to 7/2-, 9/2-, 11/2- levels. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
J L=3 in (p,d), ({+3}He,|a) 
E from weighted average of 3774 {I5} (p,d) and 3785 {I12} ({+3}He,|a). 


level_energy_unit: KEV
level_spin_parity: 21/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T RDDS method (2005Du19), decay curve of 3325 transition was least-squares fitted with two lifetime components, one of which was fixed to a value corresponding to lower limit of the lifetime of th 25/2- state. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J From angular distributions and correlations of both populating and depopulating transitions of level. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: MIN
level_comment:
E Transitions depopulating isomer impossible to observe in prompt coin with feeding |g rays due to long half-life of level. 
T From adopted levels. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Measured isotope shift: |d|n({+56}Fe,{+53}Fe)=-1.252 GHz {I4}(stat) {I5}(syst) (2016Mi27). 
$Measured differential charge radius: |d<r{+2}>({+56}Fe,{+53}Fe)=-0.218 fm{+2} {I13} {I91}; |d<r{+2}>({+54}Fe,{+53}Fe)=+0.097 fm{+2} {I14} {I35} (2016Mi27); in each case, the first uncertainty is the quadratic sum of the statistical and systematic uncertainties for isotope shifts, and the second uncertainty is from atomic factors. 
J$from {+53}Fe Adopted Levels in the ENSDF database (March 2007 update) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
MOMM1$deduced by 2017Mi19 from measured hyperfine coupling constant A{+HF}({+53}Fe) and known values of A{+HF}({+57}Fe) from 1966Ch16: Phys Rev 148, 74 (1966), and |m({+57}Fe) from 1974Sa25: Z Naturforsch 29a, 1763 (1974). 
MOME2$deduced by 2017Mi19 from measured hyperfine coupling constant B{+HF} and calculated electric field gradients using the multiconfiguration Dirac-Fock (MCDF) method. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_comment:
$Isomeric ratio=0.050 {I2}, determined by collecting the low-energy Fe beam on a foil and detecting characteristic |g rays from the isomeric and ground states (2017Mi19). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
$Decay mode for fully-ionized {+53}Fe{+26+} 
J$from {+53}Fe Adopted Levels in the ENSDF database (March 2007 update) 
T$measured half-life of the bare (fully-ionized) {+53}Fe{+26+} (2018Tu03), using Schottky frequency spectrum for stable {+54}Fe as a reference. This value can be compared with T{-1/2}=8.51 min {I2} for neutral {+53}Fe atom, where %|b{++} decay mode is 97.1% {I3} (from {+53}Fe |e decay dataset in the ENSDF database), based on which expected half-life of bare {+53}Fe ion is 8.76 min {I3}, in reasonable agreement with the measured value of 8.47 min {I19} (2018Tu03). In a previous study of half-life of bare {+53}Fe ion at GSI, measured value was 8.5 min {I3} (1995Ir01: Phys. Rev. Lett. 75, 4182). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$Compiler's note: there is |g-transition intensity imbalance at the 1328 level, with feeding I(|g+ce)=80.45 {I30} (for 1011.1|g and 1712.6|g) versus outgoing I(|g+ce)=83.1. A query sent by e-mail on March 31, 2023 to the corresponding author of 2023Pa08 was not responded as of April 23, 2023. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$Compiler's note: there is small |g-transition intensity imbalance at the 2339 level, with feeding I(|g+ce)=100.0 for the 701.1|g versus outgoing I(|g+ce)=101.7 {I4} for 1011.2|g and 2338.3|g. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
The double |b decay of {+54}Fe was investigated, upper limit on the half-time>4.4|*10{+20} y, see 1998Bi13. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1,MOME2$Compiled by 2011StZZ. 
J from L=2 in ({+3}He,n), ({+6}Li,d). 
T$from Coulomb excitation (2000Sp08). Others: 0.76 ps {I+35-22} in (p,p'|g); 2.3 ps {I+25-16} from DSAM in (|a,|a'|g). 
MOMM1 Weighted average values from 1977Br23 and 1977Fa07. 
BE2 Others: 0.0676 {I38} for {+54}Fe+{+16}O and {+54}Fe+{+40}Ca (1981Le02), 0.064 {I7} for {+54}Fe+{+16}O (1979Po08), 0.060 {I5} for {+54}Fe+{+18}O (1979Po08), 0.064 {I4} for {+54}Fe+{+12}C and {+54}Fe+{+13}C (1979Po16), 0.061 {I12} for {+54}Fe+{+12}C (1967Af03); 0.045 (1976Le12), 0.0595 (1971DaZM), 0.051 {I2} (1965Si02). 
G g=1.05 {I6} (2000Sp08), g=1.05 {I17} (1992Sp02), g=1.08 {I19} (1977Fa07), g=1.68 {I38} (1977Br23), g=+0.95 {I11} (2009Ea02). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J from L=4 in (e,e'), (|a,|a'). 
T from {+40}Ca({+16}O,2p|g), RDM. other: |>2.1 ps, DSAM in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J from |g(|q), linear polarization and DCO triple angular correlation ratios in (|a,2n|g) (1979St13). 
T weighted average from 1.22 ns {I2} (p,p|g),(1971He21), 1.19 ns {I3} in |e decay (1.48 min) (1970Co32) and 1.24 ns {I4} in |e decay (1.48 min) (1971Sa07); other: |>0.55 ps from DSAM (1972Mo21). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J from L=2 in ({+6}Li,d), (p,t). 
T weighted average of 0.052 ps {I8} (p,p'|g) and 0.052 ps {I7} (n,n'|g). Other: 1.6 ps {I+21-7}, DSAM in (|a,|a'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T weighted average of 0.16 ps {I+4-3} (p,p'|g) and 0.14 ps {I+4-3} (n,n'|g). 
J from L=2 in (p,t), (|a,|a'). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T weighted average of 0.063 ps {I14} from (p,p'|g) and 0.061 ps {I+15-11} from (n,n'|g). 
J from L=4 in (p,t), (|a,|a'). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J from L({+3}He,n)=0 and strong pair-line spectrum with no corresponding |g in (p,p'|g) (1980PaZM). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+,4+
level_comment:
J from 4074|g to 2+ and 1435|g to 4+, so 2+, 3+, 3-, and 4+ are likely, 2944|g (M1+E2) to 4+, J|p=3+, 4+. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: FS
level_comment:
J 3432|g with E2 to 6+. 146|g with E2 from 10+. 
T from DSAM in ({+6}Li,pn|g) (1979Gu07); <1.4 ns from RDM in ({+16}O,2p|g) (1978Da09). 


level_energy_unit: KEV
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
MOME2 From weighted average values from 1984Ha07 and 1983Ra03. 
J from 146|g (E2) to 8+ and 3577|g (E4) to 6+. 
T from {+40}Ca({+16}O,2p|g). Other: 358 ns {I31} from {+52}Cr(|a,2n|g). 


level_energy_unit: KEV
level_spin_parity: 8-
level_comment:
J from fit of squared inelastic form factor for 8- to experimental data. Purely transverse and most probably magnetic transition, T=1. 


level_energy_unit: KEV
level_spin_parity: 8-
level_comment:
J from fit of squared inelastic form factor for 8- to experimental data. Purely transverse and most probably magnetic transition, T=2. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_comment:
{+54m}Fe(10+) level is a very important nuclear probe for investigations of magnetic structure of solids with the recoil implantation technique. 


level_energy_unit: KEV
level_spin_parity: 8+
level_comment:
J probably high spin states belonging to configuration=((|p 1f{-7/2}){++5}(|p 2p{-3/2})) or configuration=((|p 1f{-7/2}){++6}(|n 1f{-7/2}){+-1}(|n 2p{-3/2})). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=170 {I30} 
E isobaric analog of 1460 level of {+54}Mn based partly on the assumption of J|p=0+ for the parent analog state from 1975Bo14. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=480 {I30} 
E isobaric analog of 2110 level of {+54}Mn based partly on the assumption of J|p=0+ for the parent analog state from 1975Bo14. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W=280 {I30} 
E isobaric analog of 6150 level of {+54}Mn based partly on the assumption of J|p=0+ for the parent analog state from 1975Bo14. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
|b{-L}=0.094 {I12} (|p{++},|p{++}') at 180 MeV, |b{-L}=0.10 {I2} (|p{+-},|p{+-}') at 180 MeV, see 1991Ra22. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
J strong pair-line in spectrum with no corresponding |g (1980PaZM). R(|w)=0.253 {I13} agree with the expected 0.26 for E0 transitions. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
deformation parameter for the charge distribution (Coulomb): |b{-2}(Coulomb)=0.22 for {+54}Fe+{+12}C (1979Po16) and for {+54}Fe+{+16}O (1979Po08), |b{-2}(Coulomb)=0.21 for {+54}Fe+{+18}O (1979Po08). Deformation parameter for the ion-ion nuclear potential: |b{-2}(nuclear)=0.17 for {+54}Fe+{+12}C (1979Po16), |b{-2}(nuclear)=0.16 for {+54}Fe+{+16}O, |b{-2}(nuclear)=0.12 for {+54}Fe+{+18}O (1979Po08). 
BE2 Others: 0.0676 {I38} for {+54}Fe+{+16}O and {+54}Fe+{+40}Ca (1981Le02), 0.064 {I7} for {+54}Fe+{+16}O (1979Po08), 0.060 {I5} for {+54}Fe+{+18}O (1979Po08), 0.064 {I4} for {+54}Fe+{+12}C and {+54}Fe+{+13}C (1979Po16), 0.061 {I12} for {+54}Fe+{+12}C (1967Af03); 0.045 (1976Le12), 0.0595 (1971DaZM), 0.051 {I2} (1965Si02). 
G Others: g=1.08 {I19} (1977Fa07), g=1.68 {I38} (1977Br23), g=0.95 {I11} (2009Ea02), g=1.43 {I28} (1972Hu08, 1974Hu01). 
$ g(1408,2+ in {+54}Fe)/g(847, 2+ in {+56}Fe)=1.67 {I17} (2009Ea02). Using 1.90 {I8} (2000Sp08,2000Er06) and 1.67 {I17}, 2009Ea02 gave average relative ratio=1.87 {I7}. g=+0.95 {I11} (2009Ea02) is from average relative ratio and g=+0.509 {i105} for {+56}Fe) (2009Ea01). 
T From 2000Sp08. 


level_energy_unit: KEV
level_comment:
$|s=150 |mb 30. See 1985Mi06 for absolute cross section measured at L=0, c.m. angle=20.7|', E(p)=51.9 MeV. 


level_energy_unit: KEV
level_comment:
$|s(|q) of the 6330+6410+6510 levels contains no L=0 contribution but is well reproduced by a superposition of L=2 and L=4. |s(|q) integrated from 6|' to 52.5 ' is 28 {I6}. 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
S$for E2 strength (ISGQR). 
$Centroid=17.31 MeV {I13}, with %EWSR=60 and width=6.7 MeV {I4} from a a single Gaussian fit to the E2 distribution 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: Y
level_comment:
J L(d,p)=1 and L(p,t)=2 from 1/2-. 
T Limitation of relative statistical weight (LWM): 2.752 y {I4} (2006Va13), 2.748 y {I6} (2000Sc20), 2.724 y {I8} (1998Ka30), 2.729 y {I16} (1994Mo36), 2.763 y {I5} (1982HoZZ), 2.677 y {I19} (1982La25), 2.739 y {I4} (1980Ho17), and 2.685 y {I10} (1968An01). Others: 2.84 y {I3} (1950Br76), 2.60 y {I2} (1956Sc87), and 2.41 y {I12} (1965EvZX). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J L(d,p)=3, E2 |g to 1/2-. 
T from (d,p|g), DSAM. Others: <8.3 ps (HI,xn|g), 9.3 ps {I28} (|a,n|g), RDM. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J L(d,p)=3 and L(p,t)=4 from 1/2-. 
T RDM. Others: 0.63 ps {I+63-21} (p,n|g), DSAM; 1.4 ps {I+14-4} (|a,n|g), DSAM; 10 ps {I2} (d,p|g), DSAM. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J L(d,p)=3 and L(p,t)=4 from 1/2-. 
T RDM. Others: 48 ps {I5} (|a,n|g), RDM; 28 ps {I+28-14} (d,p|g), DSAM; 34 ps {I7} (p,n|g), direct-timing method. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J J=9/2,11/2 from 1223|g(|q) in (p,n|g); |p=- from E2 |g to 7/2-. 
T RDM. Other: >0.40 ps (p,n|g), DSAM. 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: PS
level_comment:
J in (HI,xn|g), 1974Po14 compared the energies of the yrast levels they observed with those of the higher spin states calculated by 1971Ho33. The experimental results indicated J(5099 level)>17/2; the 1681|g would then correspond to a weak E2 transition to 3419 level (J|p: 15/2-). 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J in (HI,xn|g), 1974Po14 compared the energies of the yrast levels they observed with those of higher spin states calculated by 1971Ho33. Combining T{-1/2} and |s(|q) information, 1974Po14 made this tentative J assignment. M1+E2 |g to (19/2-). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
E from (p,t). 
J L(p,t)=2+4 from 1/2-; L({+3}He,|a)=3, probable isobaric analog of 7/2- 126 in {+55}Mn. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E the correspondence with adopted levels is not clear. 
S S=0.67 for J|p=9/2+, S=0.88 for J|p=1/2-. 


level_energy_unit: KEV
level_comment:
E E(p)=1543 (1978Vi03). 
S from fig. 5 in 1978Vi03, radius parameter=1.25 fm, diffuseness parameter=0.65 fm. 
|DE(Coul.)=8641 keV {I20} in {+55}Mn-{+55}Fe pair (1967Co13). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J E2 |g to 0+ g.s. 
T from Coul. ex. Others: 5.5 ps {I9} from RDM (HI,xn|g), 6.8 ps {I14} (|g,|g') and 6.9 ps {I4} (e,e'). 
MOME2 Other: -0.23 {I3} (1989Ra17). 
MOMM1 IMPAC measurement in Coulomb excitation. Others: +1.3 {I4} in {+56}Fe(|g,|g'), +1.1 {I5} in {+56}Co |e decay. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T from midpoint of overlap region of 0.7 ps {I+4-2} in (p,p'|g), 0.59 ps {I+17-14} (n,n'|g), 0.66 ps {I+24-14} (HI,xn|g); |DT{-1/2} from difference between the midpoint and maximum value of overlap region. 
J J=4 from |g(|q) of 1238|g to 2+ 846 in {+54}Fe(|a,2p|g) and |p=+ from L(t,p)=4. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T other: 0.15 ps {I+8-6} (p,p'|g). 
J J=0 from |g|g(|q) of 2094|g (to 2+) and 846|g (to 0+) in {+56}Fe(p,p'|g) and |p=+ from L(t,p)=0. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T from RDM in (HI,xn|g). Others: >1.4 ps (|a,2p|g), >0.55 ps (n,n'|g). 
J |g(|q) of E2 1303|g to 4+ 2085 in (HI,xn|g). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
T other: <28 fs (p,p'|g). 
J J=3 from |g(|q) of 2598|g to 2+ 847 in {+56}Fe(n,n'|g) and |p=+ from L(d,t)=1(+3). L(t,p)=2 is not consistent with J|p=3+. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T other: <13 fs (p,p'|g). 1.5 fs {I4} from |G{+2}{-|g0}/|G=0.077 eV {I12} (|g,|g') with adopted branching. 3.7 fs {I6} with |G(0)/|G=0.79 {I2} from (|g,|g'). 
J |g to 0+ and 2+. |g(0) in (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E 3605 level from {+56}Fe(p,p'|g) and 3601 level from {+56}Fe(n,n'|g) are the same levels because of the same |g transitions and J|p. 
T others: 0.12 ps {I+7-5} (p,p'|g), 17 fs {I6} from |G{+2}{-|g0}/|G=0.011 eV {I2} (|g,|g') and 0.18 ps {I8} from B(E2) in {+56}Fe(e,e'). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J |g(|q) of E2 1670|g to 4+ 2085 in (HI,xn|g). 
T from DSA in {+54}Fe(|a,2p|g). Others: 0.14 ps {I3} (HI,xn|g) and 0.13 ps {I5} (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
T from DSA in {+54}Fe(|a,2p|g). Other: 0.09 ps {I3} (HI,xn|g). 
J |g(|q) of M1+E2 1312|g to 6+ 3388 in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J from L=2 in {+56}Fe(e,e'). 
T from (e,e'). 
E the 4729.9 {I10} level in {+56}Fe(n,n'|g) probably corresponds to one of 4728 and 4730 levels. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J |g(|q) of E2 1868|g to 6+ in {+54}Fe(|a,2p|g) and (HI,xn|g). 
T from DSA in {+54}Fe(|a,2p|g). Other: 0.31 ps {I+12-6} in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: GE 1
level_lifetime_unit: FS
level_comment:
T from |G{+2}{-|g0}/|G=0.027 eV {I6} in {+56}Fe(|g,|g'). 
J J>0 on the basis of an observed transition to 0+. 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J |g(|q) of E2 1871|g to 6+ 3756 in {+54}Fe(|a,2p|g), |g(|q) of M1+E2 926|g to 7+ 4701 in {+54}Fe(|a,2p|g). 
T from (|a,2p|g). 


level_energy_unit: KEV
level_spin_parity: (7-)
level_comment:
J based on |s(|q) DWBA calculation and excited two neutron configuration=((|n f{-5/2})(|n g{-9/2})) in {+54}Fe(|a,2p). 


level_energy_unit: KEV
level_spin_parity: (8+)
level_comment:
E From {+54}Fe(|a,2p). 
J based on |s(|q) DWBA calculation and excited two neutron configuration=((|n g{-9/2})(|n g{-9/2})) in {+54}Fe(|a,2p). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E From {+54}Fe(|a,2p). 
J based on |s(|q) DWBA calculation and excited two neutron configuration=((|n g{-9/2})(|n 2d{-5/2}))6+ in {+54}Fe(|a,2p). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G From |g(|q,H) for T{-1/2}=6.07 ps, the adopted value. The authors' value is 0.57 {I18} calculated with T{-1/2}=6.8 ps. 
T weighted average of 6 ps {I2} (1961Ke06), 7.4 ps {I11} (1961Me11), 6.7 ps {I13} (1963Be29), and 5.6 ps {I28} (1964Bo22). 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$I(90|')/I(127|')=0.86 {I7} 
T from |G=0.118 eV {I10} (1998Is05). 
|G{+2}{-|g0}/|G=0.077 eV {I12} (1984Ch14). g|G{+2}{-|g0}/|G=0.251 eV (1994IsZZ). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
|G{+2}{-|g0}/|G=0.011 eV {I2} (1984Ch14). The authors point out that their |G is probably an upper limit since a comparison of yields at 10.3 and 7.6 MeV indicate very strong feeding of this level from above, an observation that could account for the difference in T{-1/2} values. 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$I(90|')/I(127|')=0.98 {I18} 
|G{+2}{-|g0}/|G=0.037 eV {I6} (1984Ch14). g|G{+2}{-|g0}/|G=0.176 eV (1994IsZZ). 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
$I(90|')/I(127|')=2.22 {I31} 
|G{+2}{-|g0}/|G=0.023 eV {I4} (1984Ch14). g|G{+2}{-|g0}/|G=0.073 eV (1994IsZZ). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$I(90|')/I(127|')=1.21 {I29} 
|G{+2}{-|g0}/|G=0.027 eV {I6} (1984Ch14). g|G{+2}{-|g0}/|G=0.054 eV (1994IsZZ). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$I(90|')/I(127|')=1.56 {I31} 
|G{+2}{-|g0}/|G=0.024 eV {I6} (1984Ch14). g|G{+2}{-|g0}/|G=0.059 eV (1994IsZZ). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$I(90|')/I(127|')=1.35 {I33} 
|G{+2}{-|g0}/|G=0.028 eV {I5} (1984Ch14). g|G{+2}{-|g0}/|G=0.081 eV (1994IsZZ). 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$I(90|')/I(127|')=0.85 {I25} 
|G{+2}{-|g0}/|G=0.056 eV {I13} (1984Ch14). g|G{+2}{-|g0}/|G=0.212 eV (1994IsZZ). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$I(90|')/I(127|')=0.75 {I7} 
|G{+2}{-|g0}/|G=0.70 eV {I11} (1984Ch14); |G{+2}{-|g0}/|G=1.10 eV {I29} (1979Ku14). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$I(90|')/I(127|')=0.86 {I12} 
|G{+2}{-|g0}/|G=0.50 eV {I8} (1984Ch14); |G{+2}{-|g0}/|G=0.77 eV {I22} (1979Ku14). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$I(90|')/I(127|')=1.30 {I27} 
|G{+2}{-|g0}/|G=1.94 eV {I30} (1984Ch14); |G{+2}{-|g0}/|G=3.55 eV {I74} (1979Ku14). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$I(90|')/I(127|')=1.37 {I19} 
|G{+2}{-|g0}/|G=2.63 eV {I42} (1984Ch14); |G{+2}{-|g0}/|G=5.75 eV {I92} (1979Ku14). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$I(90|')/I(127|')=1.35 {I27} 
|G{+2}{-|g0}/|G=2.04 eV {I31} (1984Ch14); |G{+2}{-|g0}/|G=4.92 eV {I95} (1979Ku14). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J from (nuclear resonance fluorescence) results for dipole transitions (1994Go36) 
|G{+2}{-|g0}/|G=0.86 eV {I18} (1984Ch14). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$I(90|')/I(127|')=1.00 {I4} 
|G{+2}{-|g0}/|G=0.57 eV {I12} (1984Ch14); |G{+2}{-|g0}/|G=1.28 eV {I17} (1983Sm02). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J from NRF (nuclear resonance fluorescence) results for dipole transitions (1994Go36) 
|G{+2}{-|g0}/|G=0.95 eV {I31} (1984Ch14). 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_comment:
J from NRF (nuclear resonance fluorescence) results for dipole transitions (1994Go36) 
|G{+2}{-|g0}/|G=0.75 eV {I17} (1984Ch14). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: PS
level_comment:
BE2 Others: 0.094 {I5} (1971He08), the B(E2) values are somewhat model dependent in the sense that the Coulomb excitation B(E2) to the 2+ state is used as a constraint on the possible charge density model 0.125 {I27} (1970Pe15), 0.068 {I5} (1972Li28), 0.072 {I4} (1962Be18). 


level_energy_unit: KEV
level_spin_parity: 0+,2+
level_comment:
The fraction of the sum rules with T=0 exhausted by the 16.1 MeV resonance state become about 80% and 140% for E2 and E0 assignments, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
|b{-2}=0.252 {I18} for E(n)=11 MeV, |b{-2}=0.292 {I20} for 26 MeV (1986Me01), |b{-2}=0.24 {I1}, |b{-2}R=1.07 fm {I4} (1982De45), |b{-2}=0.23 {I1} (1975Hy01). 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
Broad peak at |?8300, assumed by the authors to include the 8130, 8243, and 8538 levels, with J=1, and seen in (|g,|g'). |s(|q) consistent with J|p=1+, not with 1-. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from B(E2). Others: 7.8 ps {I+28-17} (1965Es01), DSA 7.1 ps {I14} (1969Sp05), DSA. 
BE2 From weighted average of values 0.109 {I15} (1969Sp05), 0.111 {I6} (1972Ca05), and 0.102 {I6} (1981Le02). Others: 1964El03 report the ratio B(E2)|^(847)=(9.30 {I9})|*B(E2) (668 level in {+63}Cu). For B(E2)({+63}Cu)=0.0113 {I8} (1980Ku08), one gets B(E2)(847)=0.105 {I8}. 0.097 (1964El03,1967No04) 
MOME2 From weighted average of -0.19 {I8} (1981Le02), -0.23 {I3} (1971Th14), and -0.25 {I6} (1972Le09), based on reorientation effect. Others: -0.34 {I6} (1970Sc15), -0.12 {I16} or +0.02 {I16} (1972Ca05). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E may be composed of 2942 and 2960 
S other: 0.12 if J=1/2 or 0.33 if J=3/2 for L=1 neutron transfer (1981Bi04). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T from RDM (1981Ke05). Others: >0.69 ps in RDM and DSA (1974Po15), 2.7 ps {I+28-12} in DSA (1977Be27). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$g=+0.504 {I63} (2009Ea01) at low field, g=+0.40 {I15} at high field. Using the two literature values from radioactivity measurements, 2009Ea01 recommend an adopted value of +0.509 {I53}, the same value is listed in authors' companion paper 2009Ea02. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J J=1/2 from paramagnetic resonance (1976Fu06) and L(d,p)=1 
Small spectroscopic factor in (d,p) implies that {+57}Fe g.s. is deformed (1973De23) 
MOME2=2.00 IF THE EFFECTIVE CHARGE=0.8 (1975Sa07; THEORY) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
J M1+E2 to 1/2- 
T From |e decay. The internal conversion decay of this level in different ionic charge states was determined by 1989Ph01; The T{-1/2} for two-electron ion was 100 ns {i5} and for the total spin f=1 state of the one-electron ion was 79 ns {i6}. 
MOME2 see review/evaluation by 1992Ru07 who estimate it to be 0.13-0.15 from an analysis of Mossbauer spectroscopy data 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
J L(d,p)=3; E2 to 1/2- 
T weighted av of 8.6 ns {i3} from Coulomb excitation and 9.0 ns {i7} from {+57}Co |e decay 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J M1+E2 to 1/2- 
T weighted av of 11 ps {i2} from RDM in ({+13}C,4n|g) and 10 ps {i2} from Coulomb excitation. Other: |<4 ns from |e decay 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J 7/2 from |g(|q) in (|a,n|g); |p=- from M1+E2 to 5/2- 
T >1.0 ps in (n,n'|g) is inconsistent with adopted value 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J L(n)=3 in (d,p); J|=5/2 from |g(|q) in (|a,n|g). Based on the excitation function of the 650|g, J|p=3/2- was assigned in (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
T weighted average of 53 fs {i11} from centroid shift of |g-rays in (d,p|g), 62 fs {i14} from DSAM in (n,n'|g), and 56 fs {i20} from |g-ray induced Doppler broadening in (n,|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
T weighted average of 25 fs {i8} from DSAM in (n,n'|g), 33 fs {i6} from centroid shift in (d,p|g), and 35 fs {i9} from |g-ray induced Doppler broadening in (n,|g) 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: PS
level_comment:
J from |g(|q) and linear pol in (|a,n|g) 
T other: |?0.42 ps from DSAM in (|a,n|g), <0.14 ps from DSAM in ({+13}C,4n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
T unweighted average of 60 fs {i10} from DSAM in (n,n'|g), and 95 fs {i19} from centroid shift in (d,p|g) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2-)
level_lifetime_unit: FS
level_comment:
T unweighted average of 22 fs {i8} from DSAM in (n,n'|g) and 15 fs {i3} from centroid shift in (d,p|g) 
J from |g's to 1/2-, 3/2-; J=1/2 from Hauser-Feshbach analysis in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_comment:
J J|p=3/2,5/2 from CP in (pol n,|g) E=thermal; J|p=1/2- from Hauser-Feshbach analysis in (n,n'|g), although 3/2- does not seem to be definitely ruled out. 


level_energy_unit: KEV
level_spin_parity: (13/2)-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J (13/2) from |g(|q) in ({+13}C,4n|g); |p from E2 to 9/2- 
T other: |<0.46 ps from DSAM in (|a,n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+,9/2+
level_comment:
J L(d,p)=4 
E the 3340.33 level seen in (n,|g) is most likely different from this level with L(n)=4 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
L(n)=4 in (d,p) inconsistent with 1811|g to 3/2- state. Therefore, state observed in (n,|g) is probably different 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
J L(d,p)=4 
E the 3608.51 level seen in (n,|g) is most likely different from this level with L(n)=4. 


level_energy_unit: KEV
level_spin_parity: 7/2+,9/2+
level_comment:
J L(d,p)=2+4, E=3784 {i10}. |g's from 3792 {i1}/2- and 5/2- levels suggest J=1/2,3/2,5/2 making this a likely candidate for the L=2 component in (d,p). The 3784 {i10} level is thus assigned as the L=4 component. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J stretched-quadrupole radiation pattern in ({+13}C,4n|g) 
T unweighted av from 0.19 ps {i6} from (|a,pn|g) and 0.38 ps {i14} ({+13}C,4n|g) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J|p=(1/2+) and (3/2+) from analyzing power(|q) and |s(|q) in (pol d,p) based on empirical curves. Data clearly show this level to be a doublet. 


level_energy_unit: KEV
level_spin_parity: (1/2+)&(7/2-)
level_comment:
J from analyzing power(|q) and |s(|q) in (pol d,p). Data clearly show this to be a doublet. Assignment based on empirical curves 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J p-wave resonance from transmission and scattering (Cf. 1981MuZQ). J=1/2 from |g(|q) and strong transition to g.s. (1970Ch10) 
|g|G{-n}|G{-|g}/|G=68.7 meV {i15}; |s{-0}|G{-|g}=161 b|*eV 4 from 1983Ma13; not consistent with 1981MuZQ. 


level_energy_unit: KEV
level_spin_parity: (25/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J stretched-quadrupole radiation pattern in ({+13}C,4n|g) 
T same results from DSAM in (|a,pn|g) and ({+13}C,4n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T unweighted av of |g|g(t), 97.9 ns {i2} (1961Cl11,NaI), 98 ns {i1} (1965Ki03,NaI), 97.7 ns {i2} (1966Ec05,NaI), 97.8 ns {i14} (1978AlZX,scin), 99.2 ns {i4} (1995Ah04,Ge(Li)), and |g|g(|q,H,t), 99.3 ns {i5} (1969Ho28,NaI). Other: 97 ns {i4} (1978AlZX,X|g(t),scin). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
MOMM1 DPAD. E(p)=4.4 MeV; 122|g+136|g doublet detected with NaI. Assumed |g(|q) from 1969Sp05 and T{-1/2}=8.8 ns {i3}. See also 1978LeZA 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_comment:
$1.0 ps<T{-1/2}<3.5 ps 
T lower limit from DSAM; upper limit from RDM 
J (13/2+) from stretched-quadrupole radiation pattern 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J 3/2 or 7/2 from |g(|q). J=3/2 was preferred by 1972Sa38 on the basis of excitation function measurements. However, J=5/2 or 7/2 is required by (d,p) measurements. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J CP consistent with 3/2, not 1/2. 
T unweighted average of 36 fs {i3} (1992Ku17) and 76 fs {I+7-6} which is a reanalyzed value of 1989Ul01 quoted by 1992Ku17 and published in a thesis of s.ulbig (Gottingen Univ. 1991) not available to the evaluator 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J CP consistent with 3/2, not 1/2. 
T unweighted average of 26 fs {i2} (1992Ku17) and 43 fs {i4} which is a reanalyzed value of 1989Ul01 quoted by 1992Ku17 and published in a thesis of S.Ulbeg (Gottingen Univ. 1991) not available to the evaluator 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L no L=0 strength observed in |s; however, if data had been taken at more forward angles, such strength may have been observed 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J,L no L could be determined. If L=1 is assumed, the data are not consistent with either J|p=1/2- or 3/2-. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
G {+57}Co source, {+57}Fe scatterer. Measured 6.4 K| x ray and observed partially resolved 136-keV hfs. The sign of the g-factor is discrepant with the adopted for |m and with g=+0.366 {i18} from inelastic scattering 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
T 100 ns 5 for a two-electron ion; 79 ns 6 for a total spin f=1 state of one-electron ion (1989Ph01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
$g,|m from |w|t=-0.230 {i6} if T{-1/2}=8.8 ns. 
BE2 weighted av of 0.040 {i6} (1969Sp05), 0.043 {i5} (1960Fe06), 0.038 {i6} (1962Ri09). Other: 0.026 {i3} (1969Ga25) 
T weighted av of pulsed beam measurements (NaI): 8.5 ns {i4} (1969Ja18; E({+16}O)=22.5 MeV), 8.8 ns {i4} (1961Ho05; E|a=4 MeV), and 8.6 ns {i8} (1960Fe06; E|a=2 MeV). Other: 9.0 ns {i13} from B(E2)|^ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
G 1969Sp05 conclude that either the absolute value is <0.4 or that the effective field acting on the state is not constant during its lifetime 
BE2 weighted av of 0.040 {i7} (1969Sp05), and 0.040 {i6} (1962Ri09). B(E2)|^(367)/B(E2)|^(136)=1.00 {i6} (1969Sp05) agrees with this value. Other: 0.022 {i5} (1969Ga25) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
BE2 weighted av of 0.013 {i2} (1969Sp05), 0.011 {i3} (1969Ga25), and 0.0127 {i17} derived from B(E2)|^(707)/B(E2)|^(136)=0.31 {i3} (1969Sp05) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_uncertain: S
level_comment:
E$the deduced level energy can be compared with S(n)=7646.08 {I4} from 2012Wa38: AME-2012 
J$s-wave capture in {+56}Fe g.s. 
T$<|G{-|g0}> value 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$g factor=+0.468 {I56} from measured g(811,2+,{+58}Ni)/g(847,2+,{+56}Fe)= 0.920 {I55} (2009Ea02) and measured g factor=+0.509 {I53} (2009Ea01) for the 847, 2+ state in {+56}Fe. Using earlier measured ratio of 0.75 {I24} (1977Br23), 2009Ea02 recommend averaged ratio of 0.912 {I54} and g factor of +0.464 {I56}. Further, 2009Ea02 recommend averaged g factor=+0.473 {I51} by considering earlier measured (1969Si13, IPAC method) g factor=+0.514 {I118}. 1989Ra17 give +0.92 {I26} from 1977Br23 (transient- field integral PAC). See also 2005St24 compilation with quoted values from 1977Br23 and 1969Si13 
MOME2$reorientation in Coulomb excitation (1981Le02). See also 2005St24 compilation 
J$E2 |g to 0+ 
T$from B(E2)=0.1234 {I36} (1981Le02, Coul. ex.). 2001Ra27 evaluation gives 6.73 ps 22 based on adopted B(E2)=0.120 {I4} from Coulomb excitation and DSA methods. Values of 2.4 ps {I7} from DSAM in (|a,p|g) and 8.6 ps {I7} from B(E2) in (e,e') are discrepant. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 2+ 
T$weighted average of 0.24 ps 4 in (n,n'|g), 0.24 ps 7 and 0.37 ps +6-5 in (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T from (|a,p|g) 
J$|DJ=1, M1+E2 |g to 2+, |DJ=1, dipole |g from 4+. Significant excitation in (p,p'), ({+6}Li,d), and (t,p) suggests important role of indirect two-step processes, L=4 in ({+6}Li,d) from 1977Fu03 contradicts J=3+ 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 2+; M1+E2 |g to 4+ 
T$unweighted average of 0.37 ps +12-7 and 0.73 ps 14 in (|a,p|g) Other: >0.28 ps in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
E population in ({+6}Li,d) is questionable 
T$weighted average of 0.18 ps +3-2 in (|a,p|g) and 0.20 ps +9-5 in (n,n'|g). Other: 0.062 ps 17 in (n,|g) is in disagreement 
J 1+,2+ from M1+E2 to 2+ and primary |g D from 0-,1- neutron resonance; |g(|q) in neutron capture excludes J=2 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.094 ps 14 in (|a,p|g) and 0.097 ps +21-14 in (n,n'|g). Other: 0.030 ps +17-8 in (n,|g) is in disagreement 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.025 ps +6-4 in (|a,p|g), 0.033 ps +12-8 in (n,n'|g) and 0.047 ps {I9} in (n,|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T$weighted average of 6 fs 3 in (|a,p|g) and 10 fs 3 in (n,n'|g) 
J$L=1, L+1/2 in (pol d,p), |g|g(|q) in (n,|g); |g(circ pol) in (n,|g) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 4+; band assignment 
T$unweighted average of 0.34 ps 4 and 0.15 ps +3-2 in (|a,p|g); 0.11 ps +8-4 in (n,n'|g). Other: <3 ps in ({+13}C,3n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$|s(|q) in (p,p') inconsistent with L=2 which may imply a separate level near this energy. 
T$unweighted average of 6 fs 2 in (|a,p|g), 15 fs 3 in (n,n'|g) and 2.6 fs +29-11 in (n,|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
T from (|a,p|g); other: 0.7 fs {I7} (n,|g) 
J 0+,1+ from CP of |g's in polarized thermal (n,|g) and L(d,p)=1; |g to 0+ excludes 0+ 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 4+; |DJ=0 |g to 6+; L=3 in (d,{+3}He) 
T weighted average of 0.49 ps {I+15-7} (1977Ca28) and 0.47 ps +17-11 (1978Bo35) from (|a,p|g). Other: 11.8 ps {I14} in ({+13}C,3n|g) is in severe disagreement 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T from (n,|g); other: <0.7 fs in (|a,p|g) 
J 0+,1+ from CP of polarized thermal (n,|g) and L(d,p)=1; |g to 0+ excludes 0+ 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: PS
level_comment:
J$|DJ=1 |g to 4+. Positive parity is tentatively proposed in (|a,p|g) and ({+13}C,3n|g) and from shell-model predictions (1978Na06,2000ApZW). The 1997 evaluation (1997Bh02) assigned negative parity, primarily based on L(p,p')=5+3 for a 4230 {I30} group, but this L value gives J|p=4- in contradiction to J=5 from angular distribution data in (|a,p|g) and ({+13}C,3n|g) reactions. The L(t,p)=(6) and L(d,p)=(3) suggest positive parity but implied spins are in disagreement with 5+. For (p,p'), a separate level is now proposed. 
T$from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T from (n,|g) 
J 0+,1+ from CP of |g's in polarized thermal neutron capture; L=1, L-1/2 in (pol d,p); |g to 0+ excludes 0+ 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: PS
level_comment:
E unresolved doublet in (|a,{+2}He) at 4650 {I50} with (7- and 5-) from DWBA analysis. L(t,p)=2+8 for E=4670 
J |DJ=2 |g, E2 |g to (5+); |DJ=1 |g to 6+ 
T from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J 0+,1+ from CP of |g's in polarized thermal (n,|g); L=1, L-1/2 in (pol d,p); |g to 0+ excludes 0+ 
T from (n,|g) 


level_energy_unit: KEV
level_spin_parity: 1,2
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T from (n,n'|g); other: <2.4 fs in (n,|g) 
J dipole |g from 0-,1- (n,|g) resonance; |g to 0+ excludes J=0 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
J L=2 in (d,{+3}He), with J|p=1- to 6-. This peak could include the 5370 {I10} level if J|p=5-, and/or the 5414 level if J|p=2-. 


level_energy_unit: KEV
level_spin_parity: (1+,2,3-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J |g's to 2+ and 3+; primary |g from 0-,1- 
E 5418.1 keV obtained from the 4626.5 {I5} primary neutron capture |g ray populating this level is discrepant with the level energy from a least-squares fit. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L incompatible with adopted J|p=3+. In view of the poor resolution of this measurement, the observed peak could be due to the 2077 J|p=4+ level. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T other: 0.34 ps {I4} (1977Ca28) is in disagreement 
J J=3,4,6 from DCO; 1520|g(|q) stretched Q to 4+ gives J=6 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J=4 or 6 from |g(|q); J=4 can be rejected from the excitation functions of 289|g and 1752|g. 
T other: 0.49 ps {I+15-7} (1977Ca28) 


level_energy_unit: KEV
level_spin_parity: (7+)
level_lifetime_unit: PS
level_comment:
J=5,6 or 7 from |g(|q); J=5 or 6 ruled out from the large |d required for these J assignments and RUL. 


level_energy_unit: KEV
level_comment:
J$7- and 5- doublet, L=7 preferred for the dominant level at 4610 
E unresolved doublet of 4610 and 4840 levels 
S$for (f{-5/2},g{-7/2}){-7-}+(p{-1/2},g{-9/2}){-5-} doublet 


level_energy_unit: KEV
level_spin_parity: 1-
level_uncertain: S
level_comment:
E$n capture state. Energy agrees well with s(n)=10044.60 {I18} (2009AuZZ) 
J for s-wave capture on {+57}Fe(J|p=1/2-). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=2.7 {I5} 
$2g|G{-n}=5.2 keV {I6} ,|G{-|g}=3.5 eV {I7} ,|G{-n}=513 
$E(n)(lab)=29.05 {I6} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=0.85 {I11} 
$2g|G{-n}=0.68 keV {I15} ,|G{-|g}=1.14 eV {I15}, E(n)(lab)=47.05 {I5} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=0.95 {I20} 
$2g|G{-n}=2.9 keV {I3} ,|G{-|g}=1.27 eV {I27}, E(n)(lab)=76.90 {I15} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=0.35 {I15} 
$2g|G{-n}=0.30 keV {I8} ,|G{-|g}=0.47 eV {I20}, E(n)(lab)=93.70 {I9} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=2.3 {I11} 
$2g|G{-n}=6.3 keV {I11}, |G{-|g}=3.0 eV {I15}, E(n)(lab)=129.50 {I13} 


level_energy_unit: KEV
level_spin_parity: 0-
level_comment:
$g|G{-n}|G{-|g}/|G=0.95 {I25} 
$2g|G{-n}=1.65 keV {I25} ,|G{-|g}=3.8 eV {I10}, E(n)(lab)=134.5 {I3} 


level_energy_unit: KEV
level_comment:
E$1660 {I30} (1964Bo08), 1682 (1963Fu04) 
L$1 (1964Bo08,1963Fu04) 
J$1+,2+ from L+1/2 for L=1 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_comment:
J$2+,3+ from L-1/2 transfer in Ay(|q) (1975Ko19); but L+1/2 transfer cannot be definitely ruled out, thus 4+ is also possible 
E$2090 {I30} (1964Bo08), 2143 (1963Fu04) 
L$1 (1964Bo08), 3 (1963Fu04) 


level_energy_unit: KEV
level_comment:
E$2780 {I30} (1964Bo08), 2787 (1963Fu04) 
L$1 (1964Bo08,1963Fu04) J; 1+,2+ from L+1/2 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_comment:
E$3090 {I30} (1964Bo08), 3098 (1963Fu04) 
L$1 (1964Bo08,1963Fu04) 
J$1+,2+ from L+1/2 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_comment:
E$3610 {I30} (1964Bo08), 3652 (1963Fu04) 
L$1 (1964Bo08,1963Fu04) 
J$1+,2+ from L+1/2 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_comment:
E$4190 {I30} (1964Bo08), 4175 (1963Fu04) 
L$1 (1964Bo08,1963Fu04) 
J$0+,1+ from L-1/2 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_comment:
L,S$from 1975Ko19. 1972Ra17 obtain L=1+3 and J|p=2+ which is discrepant in view of |s(|q) and analyzing power data of 1975Ko19 which gives 2-,3- from L+1/2 transfer 
E$ 4454 (1963Fu04) 


level_energy_unit: KEV
level_comment:
E$4540 {I30} (1964Bo08), 4552 (1963Fu04) 
L$1 (1964Bo08) 
J$0+,1+ from L-1/2 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_comment:
E$4990 {I30} (1964Bo08), 5008 (1963Fu04) 
L$(1) (1964Bo08), 1 (1963Fu04) 
J$0+,1+ from L-1/2 transfer in Ay(|q) (1975Ko19) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$from measured ratio=0.920 {I55} (2009Ea02) of g factor of 811, 2+ state in {+58}Fe to that of 847, 2+ state in {+56}Fe, and measured g factor=+0.509 {I53} (2009Ea01) for the 847, 2+ state in {+56}Fe. Using earlier measured (1977Br23) ratio of 0.75 {I24}, 2009Ea02 recommend averaged ratio of 0.912 {I54} and g factor of +0.464 {I56}. Further, 2009Ea02 recommend averaged g factor=+0.473 {I51} by considering earlier measured (1969Si13, IPAC method) g factor=+0.514 {I118} 
MOME2$from reorientation effect) (1981Le02). Other: +29 (1974ToZJ), sign is probably wrong 
BE2$Others: 0.20 {I5} (1959Al95), 0.11 {I2} (1960An07), 0.086 {I5} (1974ToZJ) 
J$From 'adopted levels' 
T$deduced from B(E2)=0.1234 {I36} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: D
level_comment:
MOMM1 from |b-NMR on oriented nuclei (1996Oh02). Other: 0.29 {I3} from low-temperature nuclear orientation (1976Kr10, 2014StZZ). 
J 3/2 from atomic beam (1965Do11); L(d,p)=1. 
T Weighted average of 44.472 d {I8} (1997Ma75), 44.508 d {I16} (Updated NIST value in 2014Un01 - earlier value 44.507 d {I7} in 2002Un02 and 1992Un01 superseding 1982HoZJ), 44.530 d {I21} (1983Wa26) and 44.496 d {I7} (1980Ho17). Others: 1960Su10 (46.5 d {I10}), 1959Pi43 (45.60 d {I8}), 1958Ke26 (44.56 d {I3}), 1960Fu03, 1957Wr37, 1956Ru45, 1953To17, 1951Sc56. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E,J$Proposed by 2017FiZZ on the basis of population by a primary |g-ray from the 1/2+ capture state consistent with J=1/2,3/2 and inconsistent with (5/2)- assigned to the 570.85-keV level. L-1,3 in (d,p) for doublet. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
J L(d,p)=3; L(t,p)=2. Inconsistent with primary |g from 1/2+ in (n,|g) E=thermal, but primary E|g is 2 keV lower, so |g may be misplaced. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2-)
level_comment:
E must differ from (7/2)- level excited in (d,p); otherwise, mult(1137|g) to 1/2- would be M3 and transition could not compete with the [E2] 2349|g observed in |b{+-} decay. 
J |g to 1/2-. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$1426.4|g Q to (13/2+). Band member. (15/2) in ({+15}N,3np|g), ({+18}O,3n|a|g). 
T$2008Ho05 also noted lifetime for this level is markedly shorter than the stopping time of {+59}Fe in {+238}U. 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_uncertain: ?
level_comment:
E 3559.6 {I6} or 4985.2 {I9} depending on whether 1247|g feeds 3737 or 2312 level. Placement of 1247|g is confirmed in 2007De56. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E,J$This new level proposed in 2017FiZZ on the basis of population by a primary |g-ray from the 1/2+ capture state consistent with J=1/2,3/2 and inconsistent with (5/2)- assigned to the 570.85-keV level. The adopted spin resolves the assignment of L=1,3 in (d,p). 


level_energy_unit: KEV
level_comment:
E 230 eV p-wave resonance; E from S(n)=6581.01 {I11} (2017Wa10) and E(res). E=6581.6 {I13} from least squares adjustment of E|g. 


level_energy_unit: KEV
level_comment:
E 359 eV p-wave resonance; E from S(n)=6581.01 {I11} (2017Wa10) and E(res). E=6581.1 {I10} from least squares adjustment of E|g. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T From 2009Ru08. Specific activity measurement. Measured activity of {+60}Fe in the source, its isotopic composition, and the number of iron atoms in the source. 
T Other values: 1.49|*10{+6} y {I27}, specific activity measurement and radioisotope concentration (1984Ku28). 3|*10{+5} y (1957Ro54). 
T a larger sample material and a more accurate determination of the number of atoms suggests the result in 2009Ru08 is the most accurate 
T The half-life of {+60}Fe plays a prominent role in various astrophysical matters.  


level_energy_unit: KEV
level_comment:
J|p=2+ from 1476|g M1 to 2+, and 2300|g E2 to 0+. However, log| {Ift}=5.0 to 2300-keV level is not consistent with |b{+-} decay from {+60}Mn(4+) to {+60}Fe(2+). 


level_energy_unit: KEV
level_comment:
J|p=2+ from 1476|g M1 to 2+, and 2300|g E2 to 0+. However, log| {Ift}=6.0 to 2300-keV level is not consistent with |b{+-} decay from {+60}Mn(4+) to {+60}Fe(2+). 


level_energy_unit: KEV
level_comment:
S N=60 {I30} for L=4; N=40 {I20} for L=5. 
J$|s(|q) shows a large deviation at large angles in comparison to DWBA computations for both L=4 and L=5. The 4+ configuration results in a more reasonable normalization constant. 
Configuration ((p3/2)(f5/2))4+, ((p1/2)(g9/2))5- 


level_energy_unit: KEV
level_comment:
S N=60 {I20} for L=5; N=30 {I15} for L=7. 
J |s(|q) shows a large deviation at large angles in comparison to DWBA computations for both L=5 and L=7. The 5- configuration results in a reasonable normalization constant. Also from comparison to the spectrum of the {+60}Ni(|a,{+2}He) reaction. 
Configuration ((f5/2)(d5/2))5-, ((f5/2)(g9/2))7- 


level_energy_unit: KEV
level_comment:
$S=70 {I20} 
Unresolved doublet, can be fitted with a pure L=6 configuration. 
N=70 {I20} for configuration (g9/2){+2}8+ + ((g9/2)(d5/2))6+ 
N=120 {I30} for configuration ((g9/2)(d5/2))6+ 
N=200 {I120} for configuration (g9/2){+2}8+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$from 2017Os02. Deduced from the measured activity of {+60m}Co daughter (t{-1/2}=10.467 min) through 58.6-keV isomeric transition and 1.131 |* 10{+15} {I59} {+60}Fe atoms in the sample measured by Accelerator Mass Spectroscopy (AMS) at Notre Dame University (2017Os02). Considering 1.15 |*10{+15} {I5} {+60}Fe atoms in the sample (measured by 2015Wa06), 2017Os02 deduce the half-life as 2.72 |* 10{+6} y {I16}. A preliminary half-life value of 2.53 |* 10{+6} y {I24} was reported in 2015Os02 using 1.15 |*10{+15} {I5} {+60}Fe atoms in the sample as measured by 2015Wa06. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$extracted from ingrowth of the {+60g}Co activity by measuring the 1173-keV and/or the 1332-keV |g-ray transition in its daughter nucleus {+60}Ni (2015Wa06). Authors compare their value with two values in literature: 1.49 |*10{+6} y {I27} (1984Ku28: Nucl. Instr. & Meth. |b{-5}, 430) and 2.62 |*10{+6} y {I4} (2009Ru08: Phys. Rev. Lett. 103, 072502). 2015Wa06 give weighted averaged value of 2.60 |*10{+6} y {I5} from their work and that of 2009Ru08 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=1.20 ps {I30} using RDDS method (2017Kl01). This value was compared with the same value obtained by 1977Wa10 (Phys. Rev. C16, 1027). Authors state that 21% of the intensity of the 4+ state is fed from the 6+ and 5- states with an effective mean lifetime of 15 ps {I15}, 24% through undetected transitions of >9 ps lifetime. 2017Kl01 used their measured mean lifetime |t=1.537 ps {I76}(stat) {I150}(syst) for the first 2+ state in {+64}Ni to constrain the offset parameter for the distance. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MIN
level_comment:
J$shell-model predictions (2008Ho05). (9/2+) -->(5/2-) --->(3/2-) sequence supported for 654.8 -->206.9 cascade in g factor measurement of 861.7 level (2004Ma80). Allowed |b transition with log| {Ift}=4.7 from {+61}Mn decay to {+61}Fe g.s. gives same parity for ground states of {+61}Fe and {+61}Mn 
T$From |g(t) in {+61}Mn |b{+-} decay (1975Br04). Others: 6.0 min {I1} (1966Le19,1968Ka22), 5.95 min {I20} (1967Eh02), 6.15 min {I6} (1967Gr15), 5.76 min {I15} (1964Cr07), 6.0 min {I5} (1957Ri10) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$|g to (3/2-) gives 1/2 to 7/2-; analogy with 287, 1/2- level in {+59}Fe supports 1/2-. Shell-model calculations (2013Ra17) predict 1/2- ground state 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$log| {Ift}=4.76 from (5/2-); |g to (1/2-); analogy with a 726, 3/2- level in {+59}Fe; shell-model calculations (2013Ra17) predict a 3/2- at 696 keV 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
MOMM1$from g factor=-0.229 {I2} by time-dependent perturbed angular distribution TDPAD method (2004Ma80). 
MOME2$ from TDPAD method (2007Ve05); value of 0.41 {I6} in 2007Ve05 re-evaluated by 2013StZZ. In 2007Ve05 value is determined from Q(9/2+ isomer in {+61}Fe)/Q(3/2- isomer in {+57}Fe)=2.75 {I13}, and Q(98-ns, 3/2- in {+57}Fe)=+0.15 {I2}. The sign of Q is undetermined. 
J$|DJ=2, (M2) |g to (5/2-); |ng{-9/2} orbital 
T$weighted average of 239 ns {I5} from |g|g(t) (2004Ma80,2002MaZN); and 237 ns {I6} from ({+61}Fe)|g(t) (2015Wi02). Other: 250 ns {I10} (1998Gr14). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$|DJ=1, dipole |g to (5/2-); analogy with a 1023, 7/2- level in {+59}Fe; shell-model calculations (2013Ra17) predict a 7/2- at 1007 keV 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$|g rays to (3/2-) and (5/2-) give 1/2- to 7/2-; analogy with a 1211, 1/2- level in {+59}Fe; shell-model calculations (2013Ra17) predict a 1/2- at 1349 keV 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J$log| {Ift}=5.68 from (5/2-); J|p assignments of 1161 and 1253 levels in analogy with ordering of 5/2- and 3/2- levels in {+59}Fe 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$log| {Ift}=5.64 from (5/2-); |g to (1/2-); J|p assignments of 1161 and 1253 levels in analogy with ordering of 5/2- and 3/2- levels in {+59}Fe 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$|g rays to (5/2-) and (7/2-); lack of |b feeding from (5/2-) and absence of transition to (3/2-) suggest J>7/2 


level_energy_unit: KEV
level_spin_parity: (1/2-,9/2-)
level_comment:
J$|g to (5/2-); lack of |b feeding from (5/2-) and absence of transition to (3/2-) suggest J>7/2 or 1/2 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_comment:
J$log| {Ift}=6.04 from (5/2-); |g to (1/2-); shell-model calculations (2013Ra17) predict a 5/2- at 1881 keV 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_comment:
J$log| {Ift}=6.04 from (5/2-); |g to (1/2-); shell-model calculations (2013Ra17) predict a 3/2- at 1901 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
$|m=-1.03 {i2} from measured g factor=-0.229 {I2} (2004Ma80). 
$Q=0.41 {I6} (2007Ve05), derived relative to the quadrupole moment of the {+57}Fe (3/2-,98 ns) isomer, Q(9/2+ isomer in {+61}Fe)/Q(3/2- isomer in {+57}Fe)=2.75 {i13} and Q(98-ns, 3/2- in {+57}Fe)=+0.15 {i2}. With this value, obtain Q({+61}Fe,9/2+)=0.41 {i6}. The sign of Q is not determined. 
T$weighted average of 239 ns {I5} from |g|g(t) (2004Ma80,2002MaZN); and 237 ns {I6} from ({+61}Fe)|g(t) (2015Wi02). Other: 250 ns {I10} (1998Gr14). 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_comment:
J$yrast population favors the 13/2+, spin-parity assignments indicating configuration=|ng{-9/2}~#(2+ in {+60}Fe). 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$Given Q{-0}=+1.15 estimate the mean lifetime of the 1342 keV, 17/2+ to 13/2+ transition to be |t=0.4 ps. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2+)
level_comment:
E$number of |g coincidences with broad proton peak around 1 MeV is much smaller than with rest of proton spectrum, indicating strong contribution for the 862-keV isomeric level. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 0+ 
T$ average of 5.1 ps {I6} (2010Lj01, RDDS and differential decay-curve analysis in {+64}Ni({+238}U,X|g)) and 5.5 ps {I7} (2011Ro02, RDDS and line-shape analysis in {+197}Au({+62}Fe,{+62}Fe'|g)) 


level_energy_unit: KEV
level_comment:
E$this level reported in ({+14}C,{+16}O) is probably different from the 4902 (9-) level from {+238}U({+64}Ni,X|g) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$reported in 1976Hi14 only from ({+18}O,{+20}Ne), with a possible weak group in 1977Co08 from ({+11}B,{+13}N). This level is not reported in any of the |g-ray studies, is judged to be suspect by the evaluators, and therefore is not included in the Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$From E|g. 
MOME2$from comparison of 877|g to GOSIA calculations, constrained by the T{-1/2} measurements in 2011Ro02 (Phys. Rev. Lett. 106, 022502) and 2010Lj01 (Phys. Rev. C 81, 061301) 
T$deduced by compilers from B(E2)|^=0.095 {I29} (quoted as B(E2)|_=13 W.u. {I+4-3} in 2015Ga38 and based on the assumption of Q=0). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=0.86 ps {I25} using RDDS method (2017Kl01). Authors state that 27% of the intensity of the 4+ state is fed from the 6+ state with an effective mean lifetime of 9.5 ps {I24}, 25% via 5- state with an effective mean lifetime of 58 ps {I50}, and 14% through undetected transitions with an effective mean lifetime of 75 ps {I75}. 2017Kl01 used their measured mean lifetime |t=1.537 ps {I76}(stat) {I150}(syst) for the first 2+ state in {+64}Ni to constrain the offset parameter for the distance. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: S
level_comment:
J$allowed |b{+-} feeding to 7/2- g.s.; strong and possibly allowed |b{+-} feeding to 3/2-, 995 level in {+63}Co. 5/2- also from systematics of neighboring isotones. Other: 1/2- proposed by 2009Ma22 in {+63}Mn |b{+-} decay based on comparisons of theoretical calculations with their preliminary level scheme. 
T$from |g(t) in 1985Ru05. Other: 4.9 s {I5} from an earlier measurement (1983Ru06) by the authors of 1985Ru05 and superseded by the remeasurement in 1985Ru05. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from |b{+-} decay curve in 1985Ru05, weighted average of 2.5 s {I6} and 1.8 s {I4} (which gives 2.0 s {I4}, whereas 2.0 s {I2} in 1985Ru05). Other: |?3.5 s (1985Ru05) from decay curve for |b-gated 310.8|g in {+64}Co from the decay of {+64}Fe. 
T$theoretical estimates: 2019Mo01, 1988Be23, 1984Kl06, 1973Ta30 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to 0+. 
T$weighted average of 7.1 ps {I7} (2011Ro02, RDDS and line-shape analysis); and 5.1 ps {I18} (2010Lj01, RDDS and differential decay-curve analysis); both measurements in {+64}Ni({+238}U,X|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$measured effective mean lifetime |t<1.8 ps using RDDS method (2017Kl01) in ({+238}U,X|g). Authors state that mean lifetime is 0.19 ps {I98} if the feeding from the 5- state and unobserved feeding are included, and that 57% of the feeding was observed with an effective mean lifetime of 32 ps {I29}. 
J$|DJ=2, E2 |g to 2+; 0+ not allowed from |g|g(|q) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
E$this level may be populated in this decay as stated by 2006Ho20 that a 1017|g has been tentatively identified (by 2006Ho20) in a |g-ray spectrum from {+64}Mn decay measured at ISOLDE (reference 17 in 2006Ho20: priv comm from K.L. Kratz and ISOLDE collaboration (2005)). The evaluator also obtained a copy of this spectrum and the peak at 1017 keV is clearly visible with an intensity of about 25% of 1105|g. This level is confirmed in the study of {+65}Mn |b{+-}n decay by 2013Ol06 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 7.1 ps {I7} (2011Ro02, RDDS and line-shape analysis); and 5.1 ps {I18} (2010Lj01, RDDS and differential decay-curve analysis) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$measured effective mean lifetime |t<1.8 ps using RDDS method (2017Kl01). Authors state that mean lifetime is 0.19 ps {I98} if the feeding from the 5- state and unobserved feeding are included, and that 57% of the feeding was observed with an effective mean lifetime of 32 ps {I29}. 


level_energy_unit: KEV
level_comment:
$Compiler's note: this level may correspond to the 4226.9 discrete level in {+64}Mn decay dataset in the ENSDF database (Nov 2021 update), although, 2024Vo03 stated that fits with this level did not reproduce the TAS data well. 


level_energy_unit: KEV
level_energy_info: ;ERR=GE;ERR=?
level_comment:
E$7500+x, where x<4576 {I9} from Q(|b{+-})({+64}Mn)=11981 {I6} - S(n)({+64}Fe)=7405 {I7} (2021Wa16:AME2020) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_comment:
T From 2009Pa16. Other value: 0.45 s {I15} (1994Cz02). 
Measured mass-excess=-51221.3 keV 33 (2008Bl05). 
From 1994Cz02. 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E E=402 keV, deduced from measurements of mass-excess for the ground state and for this level (mass-excess=-50819.4 keV 38, 2008Bl05). 
T From 2009Pa16. Other values: >150 ms, time-of-flight measurement (2008Bl05); 1.12 s {I25} (1994Cz02); 1.3 s {I3} (1999Le67, 1999So20). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: MS
level_comment:
E,J,T$ from 2008Bl05. The energy of the isomer is deduced from mass measurements of g.s. and isomer. The half-life is from 2009Pa16. Tentative J|p assignment is from systematics (2008Bl05). 
$ Measured mass excess=-50819.4 keV {I38} (2008Bl05) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$ No direct |b feeding is expected from (5/2-) parent state. Indirect feeding through 215.8|g from 609.5 level is 1.56% {I11} 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_lifetime_unit: PS
level_comment:
T$ from Table IV and text of 2013Ol06, uncertainty is listed as 50 ps in authors' level-scheme figure 7 and table II 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_lifetime_unit: PS
level_comment:
T$ from Table IV and text of 2013Ol06, uncertainty is listed as 10 ps in authors' level-scheme figure 7 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$ x corresponds to composite of levels above S(n)({+65}Fe)=4323 {I8} decaying by delayed neutrons; Q(|b{+-}n)({+65}Mn)=5931 {I6} (2012Wa38) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E$feeding to the 364-keV level is sum of the 364 and 398 level feedings as the 34-keV transition depopulating the 398-keV level was below the measurable energy range of the experiment (2018St18) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_comment:
T$from |g(t) (2019Ol02). Authors show a fit to 882.8|g, however, state that final result is weighted average of different |g transitions (not specified). 
J$from the Adopted Levels of {+65}Fe in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$Measured mass excess=-51218.7 keV {I84} (2020Po02) 
J$from the Adopted Levels of {+65}Fe in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
E$deduced from mass measurements of g.s. and isomer. 
J$from the Adopted Levels of {+65}Fe in the ENSDF database 
$Measured mass excess=-50821.4 keV {I77} (2020Po02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ First B(E2) value from 245.2 mg/cm{+2} target, second from 492 mg/cm{+2} target of {+209}Bi 
$ Angle-integrated Coulomb excitation |s=318 mb {I22} for 245.2 mg/cm{+2} target, and 331 mb {I30} for 492 mg/cm{+2} target of {+209}Bi 
T$ deduced from B(E2)=0.145 {I12}, average of above two measured values 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$assuming T{-1/2}|?0 ps for the 1414, 0+ level, as the 834.1- and 840.6-keV |g rays are not resolved in LaBr{-3}Ce detectors 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$assuming T{-1/2}|?0 ps for the 1408, (4+) level, as the 834.1- and 840.6-keV |g rays are not resolved in LaBr{-3}Ce detectors 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T$from 2004NiZY. Others: T{-1/2}=0.5 s {I1} (1999So20,1999Le67), 0.47 s 5 (1998Am04). Others: 1997AmZZ, 1995AmZX 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 187 ms {I6} (2003So21), 180 ms {I19} (2011Da08) and 189 ms {I6} (2012Li02). Others: 155 ms {I+34-18} (2005NiZZ), 155 ms {I50} (1999So20), 100 ms {I60} (1991Be33). 1999So20,2012Li02 observe that the |b(t) curve indicates feeding of the longer-lived isomer in {+68}Co 
%B-N$from the existence of |b-delayed neutrons (1999Ha05). This level is expected to undergo |b-delayed neutron emission with %|b-n=1.8 (1997Mo25). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+,2+)
level_comment:
J$2015Be32 interpreted this state as a low J state based on similar feeding intensity as the first excited 2+ level. No direct |g to 0+ observed from this state. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
J$possible (1/2-) from J{+|p} suggested by 2008Bl05 (and Erratum) for {+65}Fe and {+67}Fe. 
T$from weighted average of 110 ms {I6} (2011Da08) and 109 ms {I9} (2003So21). Other: 0.17 s {I3} (1998Am04) 
%B-N$6.94 estimated from theory (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from |b|g(implants) correlated decay curves (2015Li33), using three most intense |g rays of 250, 291 and 446 keV. 2015Li33 state that if |g coincidence requirement is removed, half-life is close to the literature value. (Note: T{-1/2}=102 ms {I10} in a previous work from NSCL-MSU: 2013Ma10: Phys. Rev. C 88, 064320) 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_comment:
E$deduced from mass measurements of g.s. and isomer. 
J$as proposed by 2022Po02 
$Measured mass excess=-39281.7 keV {I91} (2020Po02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 61 ms {I5} (2013Ma87), 71 ms {I10} (2011Da08) and 94 ms {I17} (2003So21), all from implant-|b(t). 
$Theoretical calculations give %|b{+-}n=11 (2003Mo09). 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$The |b{+-} decay mode has been detected, and it is the only decay possible, thus 100% |b{+-} is assigned. 
$Theoretical T{-1/2}=69.8 ms, %|b{+-}n=16, %|b{+-}2n=0 (2019Mo01) 
$Theoretical T{-1/2}=48.6 ms, %|b{+-}n=4.2, 4.6; %|b{+-}2n=0.16, 0.23 (2021Mi17) 
T$from weighted average of 34.7 ms {I36} (2014XuZZ, time distribution of |b(215.5|g)-coin events); 36.6 ms {I20} (2014XuZZ, time distribution of |b({+71}Fe implants), where fitting involved half-lives of |b and |b{+-}n daughters, and respective grand daughters, together with theoretically estimated %|b{+-}n values; from Fig. 3.7 in this work it appears that a larger number of {+71}Fe nuclei were detected); 42 ms {I6} (2013Ma87, time distribution of |b({+71}Fe implants)-correlated events, with 184 implants); and 28 ms {I5} (2011Da08, 2002MaZN, (implants)|b-correlated events, fitting procedure included five parameters: |b-detection efficiency, background rate, mother, daughter and grand-daughter half-lives). 
J$7/2+ from systematics (2021Ko07); |W{-n}=5/2+ orbital (2019Mo01, theory) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GE
level_comment:
T$assumed to be approximately equal to or larger than the flight time through the fragment separator. 
$%|b{+-}n calculated using the Kratz-Herrmann formula (2002Pf04) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$ measured by 2013Ma87 from time distribution of |b({+72}Fe) correlated events 
$ Number of implanted ions=76 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only the |b{+-} decay mode observed by 2014XuZZ 
$The observed 12.9-ms activity is assumed to correspond to the ground state of {+73}Fe. 
$Theoretical T{-1/2}=44.9 ms, %|b{+-}n=29, %|b{+-}2n=1 (2019Mo01). 
$Theoretical T{-1/2}=27.9 ms, %|b{+-}n=3.3, %|b{+-}2n=0.7 (2016Ma12). 
J$7/2+ from systematic trend (2017Au03). Also |W{-neutron}=7/2+ in theoretical calculations (2019Mo01) 
T$preliminary value from (implant)|b correlated decay curve (2014XuZZ) 
$Since no events were observed for neighboring hydrogen-like peaks, the misidentification of {+73}Fe is not possible, according to 2010Oh02 
$Measured |s=6 pb (2010Oh02), systematic uncertainty|?50% 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=47 ms, %|b{+-}n=44.0, %|b{+-}2n=0.79 (2003Mo09). 
$Theoretical T{-1/2}=21 ms, %|b{+-}n=4.5, %|b{+-}2n=0.5 (2016Ma12). 
$Measured |s=1 pb (2010Oh02), systematic uncertainty|?50% 
T$preliminary value from 2014XuZZ, based on implant-|b correlations and detailed analysis of decay curve which included half-lives of daughters and grand-daughters, as well as P{-n} values for delayed neutron emitters (see Fig. A.118 and Table A.68 on p251 in 2014XuZZ) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_uncertain: ?
level_comment:
$ Only one observed event is consistent with the identification of {+75}Fe nuclide. Measured cross section=0.0032 pb {I+57-24} using {+9}Be target (|s from e-mail reply of May 22, 2013 from O. Tarasov, first author of 2013Ta14). 
$ Theoretical values: %|b{+-}n=82, %|b{+-}2n=17.5 (1997Mo25) 
J$ 9/2+ from theoretical predictions (1997Mo25) 
T$ time-of-flight=620-650 ns (considered by the evaluator to be about the same as in 2009Ta24, which was communicated to the evaluator in e-mail reply of Sept 23, 2009 from O. Tarasov). Actual half-life is expected to be much longer as suggested by the theoretical value of 49.8 ms (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|b{+-} decay is the only decay mode possible, followed by delayed neutron decays through one- and two-neutron emissions, thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=21.3 ms, %|b{+-}n=73, %|b{+-}2n=2, %|b{+-}3n=0 (2019Mo01). 
$Theoretical T{-1/2}=12.6 ms, %|b{+-}n=57.1, 70.0; %|b{+-}2n=1.86, 2.83; %|b{+-}3n=0.016, 0.068 (2021Mi17), the two values are for different fission barriers. 
$Only one event assigned to {+76}Fe by 2017Su15, which is assumed by the evaluators to correspond to the g.s. activity of {+76}Fe 
$Measured production |s=4 fb {I+10-3} (2017Su15) 
T$half-life is not measured, but expected to be greater than few hundred ns from the flight time of fragments through the separator. Based on decreasing trend of half-lives as the neutron number increases in n-rich nuclei, evaluators estimate T{-1/2}<10 ms from literature half-lives of 8.2 ms for {+74}Fe, 12.9 ms for {+73}Fe, 17 ms for {+72}Fe, 34 ms for {+71}Fe, 61 ms for {+70}Fe and 162 ms for {+69}Fe. Other: 3 ms from systematics (2021Ko07) 


level_energy_unit: KEV
level_uncertain: S
level_comment:
J$2021Ko27 suggest J|p(g.s.)=6+ from systematics and possible proton decay. 
$Theoretical T{-1/2}=9.6 ms (2019Mo01) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MS
level_comment:
T$from 2007Do17, measured by time correlation of implantation events due to {+50}Co and subsequent emission of protons. Other: 44 ms {I4} (1996Fa09). Weighted average of two values of half-lives is 39.8 ms {I21} with a |h{+2}=1.4, whereas unweighted average is 41.4 ms {I26} 
J,ISPIN$isobaric multiplet systematics. The isobaric analog state of this level is identified in {+50}Fe at 8460 keV the J|p assignment of which is based on its mirror nucleus {+50}Cr. 
$%|ep=70.5 {I7} is most likely total delayed proton decay, including possible |e2p decay, deduced from time spectrum of events with energy >900 keV in the charged-particle spectrum. Possible small contributions from delayed-|a and delayed-2p decays are ignored. Other: 54 {I13} (1996Fa09). Only two proton peaks detected. 


level_energy_unit: KEV
level_spin_parity: (0)+
level_comment:
J$log| {Ift}=3.42 from 0+; identified as an isobaric analog state of {+50}Ni ground state based on strong |b decay of {+50}Ni to this state. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$S(p)({+50}Co)+x, where x<13280 {I400} from Q(|e)({+50}Ni)-S(p)({+50}Co), S(p)({+50}Co)=170 {I400} (syst, 2017Wa10) 


level_energy_unit: KEV
level_spin_parity: (0)+
level_comment:
E$decays by delayed two-proton mode to {+48}Mn. Level energy is determined from the measured proton energy of 1972 {I13} (2007Do17) and mass excesses of -29300 {I18} (2007Do17, from IAS energy and |g cascade in {+48}Mn and -17585 {I41} (2007Do17, from isobaric multiplet mass equation,IMME) for {+48}Mn and {+50}Co ground states, respectively. Using S(2p)({+50}Co)=2910 {I400} (syst, 2017Wa10) and the measured proton energy 1972 {I13} (2007Do17), IAS energy=4882 {I400}. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MS
level_comment:
%ECP$No delayed protons were detected. The total proton branching ratio is from time spectrum of events with energy >900 keV in the charged-particle spectrum. Thus {+51}Co decays mostly by |b{++}+|e decay to {+51}Fe (2007Do17). 
T$By time correlation of implantation events due to {+51}Co and subsequent emission of protons and |g rays (2007Do17). Other: >200 ns (tof, 1987Po04) 
J$from analysis of cross section data and parallel momentum distribution (2012Mc01) 
$|S{+inc}{-exp}({+12}C)=0.53 mb {I13}, |S{+inc}{-exp}({+9}Be)=0.57 mb {I8} (2012Mc01) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$ 7/2- supported in the present work from analysis of cross section data and parallel momentum distribution 
$|S{+inc}{-exp}({+12}C)=0.53 mb {I13}, |S{+inc}{-exp}({+9}Be)=0.57 mb {I8} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MS
level_comment:
T$By time correlation of implantation events due to {+51}Co and subsequent emission of protons and |g rays (2007Do17). Other: >200 ns (tof, 1987Po04) 
%ECP$No delayed protons were detected. The total proton branching ratio is from time spectrum of events with energy >900 keV in the charged-particle spectrum. Thus {+51}Co decays mostly by |b{++}+|e decay to {+51}Fe (2007Do17). 
J$From Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MS
level_comment:
J$From adopted levels. 
T$from weighted average values of 115 ms {I23} (1997Ha04) and 103 ms {I7} (2013Su07). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E from measured G cascade (E|g=2418.3 I3 and E|g=142.3 I1) and excitation energy of the first state(370 I30). 
J$Based on |g to 1+ and |b{++} (from 0+) decay to the state. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MS
level_comment:
T$from weighted average of 115 ms {I23} (1997Ha04) and 103 ms {I7} (2013Su07). 
J based on apparently allowed |e to 6+ state in {+52}Fe and analogy to {+44}V (4 particles in f7/2 shell, 4 holes in f7/2 shell for {+52}Co) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E,J$comparison to mirror 2+ state in {+52}Mn at 377.749 keV {I5} with T{-1/2}=21.1 min, 2016Or03 predict that the 378-keV level would also be an isomeric state decaying mainly by |e+|b{++} emission. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$T{-z}=-1 
$%I|g=75 {I23} (2016Or04) from the 2622, 0+ IAS 
E,J$isobaric analogue state (IAS) of {+52}Ni ground state. This level could contain a contribution from an unresolved 1+ state, based on results from charge exchange {+52}Cr({+3}He,t){+52}Mn reaction in the mirror nucleus {+52}Mn where levels were reported at 2875, 1+ and 2938, 0+ (2015Fu03: Acta. Phys. Pol. B46, 57, Fig. 5; also Fujita et al., Prog. Part. Nucl. Phys. 66, 549 (2011)). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MS
level_comment:
$T{-z}=-1 
$J|p from {+52}Co Adopted Levels in ENSDF database (July 2015 update) 
T$measured by 2017Ku12 from ({+52}Co implants)|b correlated decay curve. This half-life may correspond to a mixture of the (6+) g.s., and (2+) 387-keV isomeric activities. Others: 112 ms {I3} in 2016Or08 (Phys. Rev. C93, 044336) for the g.s., (6+) activity; 112 ms {I4} in 2015Sh16 (Phys. Rev. C91, 047304); 103 ms {I7} in 2013Su07 (Phys. Rev. C87, 024312); 115 ms {I23} in 1997Ha04 (Nucl. Phys. A613, 183). Some of the above values may correspond to mixture of the g.s. and isomeric activities. Value is 114 ms {I7} in {+52}Co Adopted Levels in the ENSDF database; based on 2013Su07 and 1997Ha04 data 
$Total number of {+52}Co implanted ions=8.24|*10{+4} 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: MS
level_comment:
$Measured mass excess=-34361 keV {I8} (2016Xu10) 
T$from 2016Or08 (Phys. Rev. C 94, 044315). 2016Xu10 quote 115 ms {I23} without a citation, however the value is given in measurement by 1997Ha04: Nucl. Phys. A613, 183. Others: 103 ms {I7} (2013Su07: Phys. Rev. C 87, 024312), 112 ms {I4} (2015Sh16: Phys. Rev. C 91, 047304) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$Measured mass excess=-33974 keV {I10} (2016Xu10) 
E$deduced by 2016Xu10 from measured mass excess of ground state and isomer. 
T$from 2016Or08. 2016Xu10 quote 104 ms {I11} without a citation, however the value appears in 1997Ha04 from the decay of an 849|g from {+52}Co decay 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$New level proposed by 2016Xu10, based on the assignment of 1352 keV {I10} proton peak with I(p)=13.7% {I2} (2016Or03) to a 2800, 1+ level. In 2016Or03 (also 2016Or08), this proton branch was assigned to the decay of 2935, IAS. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Deduced mass excess=-31426 keV {I10} (2016Xu10) 
E$derived by 2016Xu10 from isomer excitation energy and cascade of 141|g-2407|g deexciting the IAS. 
E,J$isobaric analogue state (IAS) of {+52}Ni ground state. 2016Xu10 propose that this level decays only by |g transition 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: MS
level_comment:
$Measured mass excess=-34361 keV {I8} (2018Zh29,2016Xu10) 
T$from 2016Or08 (Phys. Rev. C 94, 044315). 2016Xu10 quote 115 ms {I23} without a citation, however the value is given in measurement by 1997Ha04: Nucl. Phys. A613, 183. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$Measured mass excess=-33974 keV {I10} (2018Zh29,2016Xu10) 
E$deduced by 2018Zh29 and 2016Xu10 from measured mass excesses of ground state and isomer. This value is in agreement with 378 keV {I1} for the 2+ isomer in mirror nucleus {+52}Mn. Value is 370 keV {I30} in {+52}Co Adopted Levels in the ENSDF database (July 2015 update). 
T$from 2016Or08. 2016Xu10 quote 104 ms {I11} without a citation, however the value appears in 1997Ha04 from the decay of an 849|g from {+52}Co decay 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: MS
level_comment:
T$measured by 2016Or08, from correlation-time spectrum from summed spectra of 1329-, 1535- and 1942-keV |g rays from the decay of {+52}Co to {+52}Fe. 2016Xu10 quote 115 ms {I23} without a citation, however the value is given in the measurement by 1997Ha04: Nucl. Phys. A613, 183. Others: 103 ms {I7} (2013Su07: Phys. Rev. C 87, 024312), 112 ms {I4} (2015Sh16: Phys. Rev. C 91, 047304) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$from 2016Or08, from analog of 377.749-keV, 2+ isomer in {+52}Mn and uncertainty of 50 keV for mirror-energy differences. Other: 387 keV {I13} from mass measurement by 2016Xu10 (Phys. Rev. Lett. 117, 182503) 
T$measured by 2016Or08, from correlation-time spectrum gated on 849|g from the decay of {+52m}Co to {+52}Fe. 2016Xu10 quote a value of 104 ms {I11} without citation, however the value appears in 1997Ha04 from the decay of an 849|g from {+52}Co decay 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: MS
level_comment:
$T{-z}=-1 
$J|p from {+52}Co Adopted Levels in ENSDF database (July 2015 update) 
T$from 2016Or08: Phys. Rev. C 94, 044315 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$from measured mass excess=-34331.6 keV {I66} for g.s. of {+52}Co and -33958 keV {I11} for the 102-ms isomer (2017Ne05). Other: 387 keV {I13} from mass measurement in 2016Xu10: Phys. Rev. Lett. 117, 182503 
J,T$from 2016Or08 


level_energy_unit: KEV
level_comment:
E$deduced by 2017Ne05 and assigned as a proton-decaying state by a 1352 keV {I10} (value from 2016Or03) proton transition to {+51}Fe g.s. Energy was deduced as 2800 keV {I16} in 2016Xu10 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$deduced by 2017Ne05 for T=2, IAS, based on modification of level-scheme given in 2016Or03: Phys. Rev. C 93, 044336. Energy of this level was 2926 keV {I50} in 2016Or03, and incorrectly assigned as a proton-decaying level. This level decays by a 2407 keV {I1} |g ray (2016Or03). Energy of this level was deduced as 2935 keV {I13} in 2016Xu10 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
J syst for Z=27 nuclei, shell model 
T from 2002Lo13. Others: 240 ms {I20} (1989Ho13, see also 1985EsZZ,1986EsZX), 262 ms {I25} (1973Ko10) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T from 1972Ce01. Others: 242 ms {I15} (1970Ce04), 260 ms {I20} (1976Vi02) 
E From 2003Au02. Possible IAS of {+53}Fe(19/2-,3041 keV). 
J log| {Ift}|?3.6 for |b{++} to 19/2- IAS in {+53}Fe. 
Proton decay to {+52}Fe(g.s.) with E(p)=1570 keV {I30} (1970Ce04), 1590 keV {I30} (1976Vi02). Proton branching estimated to be |?1.5% from comparison of measured and calculated |s for {+54}Fe(p,2n) (1972Ce01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2-)
level_comment:
E,J IAS of {+53}Fe(7/2-,4250 keV). Proton decay observed. E(p)(c.m)=1940 {I50}, I(p)|?0.45 per decay 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$ from decay-time spectra fitted with exponential curves (2013Su07). Combining present and previous results, 2013Su07 recommend 238 ms {I8} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$assigned as IAS of 7/2- g.s. of {+53}Ni from superallowed type of log| {Ift}=3.36 value. 2016Su10 note that in the previous work by 2007Do17, 4385 level was erroneously assigned as the IAS. 
$This level does not seem to decay by delayed protons, only a very weak proton branch of 1861 keV with I(p)<0.9% {I3} to the first 2+ state of {+52}Fe may be present. Proton branch to g.s. of {+52}Fe, expected at 2710 keV, was searched by 2016Su10, but no visible peak was seen at this energy 
$Mixing of this IAS with 7/2-, T=1/2 in the range of |+500 keV is theoretically calculated by 2016Su10 using two-level mixing approach. 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-,9/2-)
level_comment:
$This state decays by proton emission, E(p)(c.m.)=1921 {I8} (2016Su10) 
%P$only proton decay has been observed in 2016Su10 and 2007Do17 
E$from E(p)+E(first excited state in {+52}Fe + S(p)({+53}Co) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$T{-z}=-1/2 
$J|p from {+53}Co Adopted Levels in ENSDF database (March 2007 update). 
T$measured by 2017Ku12 from ({+53}Co implants)|b correlated decay curve. The half-life may be due to a mixture of the g.s. and isomeric activity. Others: 230 ms {I17} in 2013Su07 (Phys. Rev. C87, 024312); 240 ms {I9} in 2002Lo13 (Phys. Rev. C66, 025803; from GANIL); 240 ms {I20} in 1989Ho13 (Nucl. Phys. A496, 462); 267 ms {I25} in H. Hama et al., (AIP conf. proc. 164, 650); 262 ms {I25} in 1973Ko10 (Nucl. Phys. A204, 185). Some of the above values may correspond to a mixture of the g.s. and isomeric activities. Value of 240 ms {I9} from 2002Lo13 is listed in {+53}Co Adopted Levels in the ENSDF database 
$Total number of {+53}Co implanted ions=1.71|*10{+6} 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$J|p and %p from {+53}Co Adopted Levels in ENSDF database 
T$from 1972Ce01 (Nucl. Phys. A188, 666); also listed in {+53}Co Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$J|p and decay mode from {+53}Co Adopted Levels in the ENSDF database (March 2007 update). 
T$measured by 2017Ku12 (Eur. Phys. Jour. A53, 134) 
$S(p)({+53}Co g.s.)=1615.6 keV {I16}, deduced by 2017Ne05 from mass excess=-48330.67 keV {I60} for {+52}Fe g.s. in the present work, and mass excess=-42657.3 keV {I15} for {+53}Co g.s. measured by 2010Ka26. Other: S(p)=1618 keV {I5} (2017Wa10: AME-2017) 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$from measured mass excesses of -42657.3 keV {I15} for {+53}Co g.s. and -39482.9 keV {I16} for the (19/2-) isomer (2010Ka26). Others: 3174.2 keV {I9} (2017Au03: NUBASE-2016, from mass differences); 3197 keV {I29} in {+53}Co Adopted Levels in the ENSDF database. 
$E(p)(c.m.)=1558.8 keV {I17}, deduced by 2017Ne05 from mass excess=-39482.9 keV {I16} for {+53}Co isomer, measured by 2010Ka26, and S(p)({+53}Co g.s.)=1615.6 keV {I16} deduced above. This value can be compared with E(p)(lab)=1590 keV {I30} given in {+53}Co p decay (247 ms) dataset in the ENSDF database (July 2015 update) 
$J|p, half-life and decay modes from {+53}Co Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T from 1997Ko65. Others: 193.7 ms {I10} (1964Fr01), 193.4 ms {I4} (1974Ha59), 193.0 ms {I3} (1974Ho21), 193.28 ms {I18} (1977Al11), 172 ms {I23} (2002Lo13). 
J$from log ft=3.485 to 0+ {+54}Fe g.s., T=0 isobaric analog of 0+ g.s. of {+54}Fe 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E identified as spin-isospin transition for L=0 transfer. 
J L=0 G-T transition from |g(|q) in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E isobaric analog of the first 1408 level of {+54}Fe from ({+3}He,t). 
J from angular distribution for T=1 in ({+3}He,t), natural parity. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J from identically shaped angular distribution and the same cross sections as the state at 1822 keV (see 1978Zi03). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J from experimental angular distribution pattern which is identical with those of 6+ spin known in ({+3}He,t) (see 1969Br04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
Corresponding IAS transition and carrying all the Fermi strength: B(F)=2 (1983Ra30). Measured Q(|e)=8244.54 {i10} from Penning-trap mass measurement (2008Er04). 
J T=1 isobaric analog of 0+ ground state of {+54}Fe. For data analysis see also 1968Ba29, 1973Ri15 and 1975Ca18. Ratios of cross sections integrated between 3|' and 40|': I(E(p)=40 MeV):I(E(p)=35 MeV):I(E(p)=32 MeV)=1:1.08:1.07. 
L L=0 transfer are identified as spin-isospin transitions (excitation of Gamow-Teller states) or as isospin transitions (excitation of isobaric analog states). See 1983Ra30. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E strong 1+ state represents part of Gamow-Teller strength: B(G-T)=0.73 (1983Ra30). T=0 from 1981Or02. 
J J from |g(|q) by 1971Sa05. |p from systematics of odd N=Z nuclei up to {+54}Co. 


level_energy_unit: KEV
level_comment:
E T=1 from 1981Or02. Excited state analog of 2+ 1408 keV. The direct process seems to dominate at E=35 MeV (1983Ma37). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
T=0 component of the Gamow-Teller giant resonance. 
J from the energy dependence of cross sections and angular distribution. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
T=1 component of the Gamow-Teller giant resonance. 
J from the energy dependence of cross sections and angular distribution. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
Isobaric analog of 0+ ground state of {+54}Fe from 1969Br04. See also: 1969Ro18, 1970Za07, 1971Fa03, 1972Fa06, 1972Fa12, 1966Ya08, 1967Co13, 1971Be29. 
$Measured yield=4946 {I254} (2012Ad03). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E a doublet broader peak at forward than at backward angles and angular distribution shows two maximal of almost equal cross section. 
J from experimental angular distribution pattern which is identical with those of 6+ spin known in ({+3}He,t) (1969Br04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7+
level_lifetime_unit: MIN
level_comment:
E,T,J$from the Adopted Levels of {+54}Co in the ENSDF database. Decay from this level not observed in 2019Sp06 because of experimental constraints. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: H
level_comment:
T weighted average of 17.54 h {I4} (1974Ro18) and 17.52 h {I3} (1982Gr10). See also 1952Ru23, 1977Mi21, and 1979La19. 
MOMM1 Value from 1973Ca06 (nuclear resonance on oriented nuclei). Other: 4.3 {I3} (1961Ch12). See also 1960Ba20. 


level_energy_unit: KEV
level_spin_parity: 9/2-,(7/2)
level_lifetime_unit: FS
level_comment:
J from |g(|q) to 7/2- g.s. in (p,|g); if J=7/2, multipolarity will be uncertain; if J=9/2, observed transition strengths of a M1/E2 transition are quite typical; whereas the M2 transition strength of a E1/M2 transition will be above the recommended upper limit. So for J=9/2, the negative parity is suggested. Analyzing power in (p,|a) suggests J|p=(9/2-). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_uncertain: ?
level_comment:
E this level is not fed from any resonance levels, but is populated only as a cascade transition via 4548(5/2-) level (observed only by 1980Ul01). 
J from |g(|q) in (p,|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_uncertain: ?
level_comment:
J from ({+3}He,d|g). 1972Sh04 show that the 3/2- state (4721 level) is observed to decay to the 3933 level with a significant strength and is associated with a |DT=1, |DJ=0 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E identified as analog state of g.s. (3/2-) in {+55}Fe in ({+3}He,d) and (p,|g) reactions; |DE(Coul.)=8954 keV {I3} in (p,|g), 8986 keV in ({+3}He,d). 
T other: <23 fs ({+3}He,d|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
Identified as analog state of g.s. (3/2-) in {+55}Fe in (p,|g) and ({+3}He,d). |DE(Coul.)=8980 keV {I3} in (p,|g), 8986 keV {I16} in ({+3}He,d). 
T other: 26 fs {I+23-19} ({+3}He,d|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
Identified as analog state of 411 (1/2-) keV in {+55}Fe in (p,|g), ({+3}He,d) and ({+3}He,d|g). 
T other: <28 fs ({+3}He,d|g). 


level_energy_unit: KEV
level_comment:
E evaluator regards this level as a possible doublet. One member decays to ground state and has J|>3/2; the other decays to 2166(3/2-) level and has J|p=3/2-. 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
E identified as analog of 1919 state in {+55}Fe; |DE(Coul.)=9038 keV {I15} in ({+3}He,d). 
J |g(|q) to 3/2- 2166, 1/2+ 2922, 1/2-,(3/2)- 2939, 1/2- 3323, 3/2- 3643, 1/2-,3/2- 3943, and 5461 levels are isotropic, which suggests J=1/2; L=1 in ({+3}He,d): |p=-. 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
J |g(|q) to 7/2- g.s. and 3/2- 2166 lead to J=3/2 or 5/2; when J=3/2, the recommended upper limits will be exceeded for E2/M3 and M2/E3 transitions to 7/2- g.s.; also, one cannot assign parity from strengths of primary transitions to 7/2- g.s. and 3/2- 2166; so J=5/2 is proposed. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E identified as analog state of 3/2- 2052 state in {+55}Fe; |DE(Coul.)=9026 keV {I18} in ({+3}He,d). 
J |g(|q) and M1+E2 |g to 3/2- 2166, 3/2- 2566, 5/2- 3725, 3/2- 4164, and 3/2- 4721. 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_uncertain: ?
level_comment:
J |g(|q) of |g to 7/2- g.s. allows J=5/2 or 9/2 (1972Ma26). The resonance strength 0.37 eV {I5} determined by 1972Ma26 ruled out J=9/2. |p=(-) from L=(3) in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
E identified as analog state of 2144 (5/2-) state in {+55}Fe in ({+3}He,d). |DE(Coul.)=9014 keV {I17} in ({+3}He,d). 
J |s(|q) and L=3 in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E identified as analog state of 2144(5/2-) state in {+55}Fe. |DE(Coul.)=9014 keV {I17} in ({+3}He,d). 
J L({+3}He,d)=3. M1+E2 |g to 4721, 3/2- gives J|p=5/2-. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E identified as analog state of 2471(3/2-) state in {+55}Fe; |DE(Coul.)=8993 keV {I3} in {+55}Fe-{+55}Co pair. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E identified as analog state of 2471(3/2-) state in {+55}Fe; |DE(Coul.)=9052 keV {I16} in ({+3}He,d), 9031 keV {I3} in (p,|g). 
J J=3/2 from |g(|q) to 3/2- 2166, 5/2- 2659, 5/2- 3303, 5/2- 3725, and 3/2- 4721; |p=- from corresponding M1+E2 multipolarities in (p,|g). 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_comment:
E identified by 1989Di08 as analog state of 2573-keV (5/2-) state in {+55}Fe. |DE(Coul.)=8991 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E identified by 1989Di08 as analog state of 2872-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=8997 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
E identified by 1989Di08 as analog state of 2872-keV and 2939-keV (5/2-,7/2-) states in {+55}Fe. |DE(Coul.)=9014 keV and 8947 keV, respectively, in {+55}Fe-{+55}Co pair (1989Di08). 
J |s(|q) and L=3 in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_comment:
E identified by 1989Di08 as analog state of 2939-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=8977 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
E identified by 1989Di08 as analog state of 2939-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=9001 keV in {+55}Fe-{+55}Co pair (1989Di08). 
J |s(|q) and L=3 in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_comment:
E identified by 1989Di08 as analog state of 2939-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=9044 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_comment:
E identified by 1989Di08 as analog state of 3109-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=8996 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E identified by 1989Di08 as analog state of 3109-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=9003 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (7/2)
level_comment:
E identified by 1989Di08 as analog state of 3109-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=9012 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E identified by 1989Di08 as analog state of 3552-keV (3/2-) state in {+55}Fe. |DE(Coul.)=8978 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E identified by 1989Di08 as analog state of 3552-keV (3/2-) state in {+55}Fe. |DE(Coul.)=8983 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
E identified by 1989Di08 as analog state of 3801-keV (3/2-) state in {+55}Fe. |DE(Coul.)=8891 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E identified by 1989Di08 as analog state of 3814-keV (7/2+,9/2+) state in {+55}Fe. |DE(Coul.)=8885 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E identified by 1989Di08 as IAR of 3814(7/2+,9/2+) state in {+55}Fe; |DE(Coul.)=8885 keV in {+55}Fe-{+55}Co pair from (p,|g). 
J from analyzing power in (pol {+3}He,d). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E identified by 1989Di08 as IAR of 3814(7/2+,9/2+) in {+55}Fe; |DE(Coul.)=8889 keV in (p,|g). 
J |g(|q) and E1 transitions to 7/2- g.s., M1 to 9/2+. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
E identified by 1989Di08 as IAR of 3814(9/2+) in {+55}Fe; |DE(Coul.)=8898 keV in {+55}Fe-{+55}Co. 
J |g(|q) and E1 transitions to 7/2- g.s. and 7/2- 2918. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E identified as analog state of 3907-keV (1/2-,3/2-) state in {+55}Fe by 1989Di08. |DE(Coul.)=8957 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_comment:
E identified by 1989Di08 as analog state of 4057-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=8969 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E identified by 1989Di08 as analog state of 4057-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=8982 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J |s(|q) and L=3 in ({+3}He,d). 
E identified by 1989Di08 as analog state of 4057-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=9004 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E identified by 1989Di08 as analog state of 4057-keV (5/2-,7/2-) state in {+55}Fe. |DE(Coul.)=9013 keV in {+55}Fe-{+55}Co pair (1989Di08). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
Identified as IAR of 4463(5/2+) state in {+55}Fe. |DE(Coul.)=8910 keV {I16} in {+55}Fe-{+55}Co pair from ({+3}He,d). 
J |s(|q) and L=2 in ({+3}He,d). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=AP
level_comment:
J based on |g(|q) and lifetime measurements by 1977Er02. See also 1980Ha37. 
T 49 fs {I+180-31} from 1977Er02. 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_comment:
E observed by 1980Ul01 where the level is not fed from any of the resonance levels, but is populated only as cascade transition via 4548-keV (5/2-) level at E(p)=1653 keV. 
J from 1980Ul01. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E identified by 1989Di08 as analog state of g.s. in {+55}Fe. |DE(Coul.)=8958 keV in {+55}Fe-{+55}Co pair (1989Di08). 
J based on polarization measurement of 1972Ma26. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E identified by 1989Di08 as analog state of g.s. in {+55}Fe. |DE(Coul.)=8985 keV in {+55}Fe-{+55}Co pair (1989Di08). 
J it is difficult to assign J|p of this level because of the complexity of feeding and decay, so other arguments are used for it. Analogy analysis. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
E identified by 1977Er02, 1980Ha36, and 1980Ha37 as analog state of 411-keV (1/2-) state in {+55}Fe. |DE(Coul.)=8994 keV {I3} in {+55}Fe-{+55}Co pair (1977Er02). 
J from analogy analysis (1977Er02). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_comment:
E IAS of {+55}Fe(3553 level); |DE(Coul.)=9075 keV {I19} in {+55}Fe-{+55}Co pair. 
L L=1 for J|p=3/2-; L=3 for J|p=5/2-. 
S C{+2}S'=0.11 for J|p=3/2-; C{+2}S'=0.10 for J|p=5/2-. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2
level_lifetime_unit: FS
level_comment:
J J=(3/2-) in 1972Sh04. 
T from 1975Ca36. Others: 21 ps {I+10-7} (1976Ne01), 35 fs {I+7-3} (1976Ne04). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
E identified as analog state of 1/2- 411 state in {+55}Fe. 
T from 1976Ne01. Other: <28 fs (1976Ne04). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: D
level_comment:
J J=4 from atomic beam (1976Fu06) and |p=+ from L=4 in {+54}Fe(|a,d). 
T from evaluation of T{-1/2} by 2004WoZZ. Others: 77.12 d {I7} (1978La21), 77.12 d {I10} (1977An13), 78.4 d {I5} (1974Cr05), 77.2 d {I8} (1954Bu58), 77.30 d {I9} (1989Al24), 78.76 d {I12} (1972Em01), 77.3 d {I3} (1957Wr37), 77.08 d {I8} (1989Le17), 77.28 d {I4} (1989Sc17), and 77.29 d {I3} (1990Al29), 77.210 d {I28} and 77.290 d {I40} (1992Fu02). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
T others: 0.33 ps {I+22-10} (p,n|g), 0.33 ps {I+22-11} ({+3}He,p|g). 
J configuration=((|p 1f{-7/2})(|n 1p{-3/2}))5+. See also J=5 from |g|g(|q) ({+12}C,np|a|g) and |p=+ from L(|a,d)=4 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T others: >0.76 ps (p,n|g), >1.4 ps (d,|a|g). 
J J=4 from |g(|q) of 671|g to 3+ 158 in {+54}Fe(|a,np|g) and |p=+ from L(p,{+3}He)=4. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T others: 0.076 ps {I+21-14} (p,n|g), <0.1 ns in {+56}Ni |e decay, and 0.139 ps {I+31-24} (d,|a|g). 
J J=2 from p|g(|q) of 812|g to 3+ 158 in {+54}Fe({+3}He,p|g) and |p=+ from L({+3}He,p)=2. 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
T others: 0.44 ps {I+25-12} in {+56}Fe(p,n|g), 0.27 ps {I+18-9} in {+54}Fe({+3}He,p|g). 
J from analyzing power in {+58}Ni(pol d,|a) and L(d,|a)=4. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T others: 0.24 ps {I+4-2} ({+3}He,p|g), 0.139 ps {I+28-24} (d,|a|g). 
J J=3 from {+56}Fe(p,n), (p,n|g). M1+E2 |g to 4+. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
E anti-analog state of 0+ g.s. in {+56}Fe in {+56}Fe(p,n), (p,n|g). 
T others: >2.0 ps ({+3}He,p|g), >0.4 ps (p,n|g). 
J J=0 from |g|g(|q) in {+56}Ni |e decay, |p=+ from L(p,{+3}He)=0. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
T others: 0.47 ps {I+40-16} ({+3}He,p|g), 0.31 ps {I+38-13} (d,|a|g). 
J from analyzing power in {+58}Ni(pol d,|a) and L(d,|a)=0. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J |p=+ from L=2 in {+54}Fe(|a,d); p|g(|q)'s in {+54}Fe({+3}He,p|g) gives J=2,(3); 670|g from 1+ 2730 is mult=D based on comparison with RUL, D from 1+ 2730 rules out J=(3). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T other: 15 fs {I+19-11} in {+54}Fe({+3}He,p|g). 
J from analyzing power in {+58}Ni(pol d,|a) and L(p,{+3}He)=2. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T is from {+56}Fe(p,n), {+58}Ni(p,{+3}He). 
T other: 67 fs {I+33-19} ({+3}He,p|g). 
J from analyzing power and L(d,|a)=0. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J from analyzing power and partially resolved doublet for 2926 and 2969 levels in {+58}Ni(pol d,|a), and L({+3}He,p)=2. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E,J IAS of 0+ g.s. in {+56}Fe in {+56}Fe({+3}He,t). 
T=2 
T is from {+56}Fe(p,n), {+58}Ni(p,{+3}He). 


level_energy_unit: KEV
level_spin_parity: 8-
level_comment:
J |p=- from L=7 and J=8 from DWBA, configuration=((|p 1f{-7/2})(|n 1g{-9/2}))8- (1994Fi01) in {+54}Fe(|a,d). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E 961 and 1001 unresolved 
L L=2+4 may be for 961+1001 doublet, adopted J|p(961)=2+ would require L=2 only. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E$576.50 in ENSDF database 
S$for L=4 at E(p)=80 and 118 MeV; 0.1 for E(p)=100 MeV. For L=6, value is <0.01 at all energies 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$970.23 in ENSDF database 
S$for L=2 for 970 known level at E(p)=80 MeV; <0.001 for E(p)=100, 118 MeV 


level_energy_unit: KEV
level_spin_parity: 5+&3+
level_comment:
E$doublet. 1009.13,5+ and 1114.51,3+ in ENSDF database 
S$for L=4 for 1009 known level at E(p)=100 MeV; <0.001 for E(p)=80 MeV and <0.01 for E(p)=118 MeV. For L=6, value is <0.001 for E(p)=80 and 118 MeV and <0.01 for E(p)=100 MeV. 
S$<0.001 for L=2 and 4 components of known 1115 level at all energies, except <0.1 for L=2 at 100 MeV 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: D
level_comment:
T weighted average of 271.68 d {i9} (1997Ma75) and 271.79 d {i9}, the recommended value from 1990Ni03. Others: 271.65 d {i13} (1965An07), 271.23 d {i21} (1972La14), 271.77 d {i5} (1980Ho17), 271.90 d {i9} (1981Va11), and 271.84 d {i4} (1983Wa26) 
J 7/2 from paramagnetic resonance (1976Fu06); |p=- from L(d,{+3}He)=3 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J 9/2 from |g(|q) in (|a,p|g); |p=- from M1 to 7/2- 
T weighted av of 54 fs {i6} in (|a,p|g), 54 fs {i8} in (p,|g), 52 fs {i24} in (|a,2n|g), and 59 fs {i21} in ({+12}C,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J 11/2 from |g(|q) in (|a,p|g); |p=- from E2 to 7/2- 
T weighted av of 0.24 ps {i2} in (|a,p|g), 0.22 ps {i8} in (|a,2n|g), and 0.22 ps {i7} in ({+12}C,p2n|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J 7/2 from |g(|q) in (|a,p|g); |p=- from L(d,{+3}He)=3 
T from DSAM in (|a,p|g). DSAM in (p,|g) gives 59 fs {i9} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J 7/2 from |g(|q) in (|a,p|g); |p=- from M1 to 9/2- 
T weighted av of DSAM in (|a,p|g) and (|a,2n|g). DSAM in (p,|g) gives 0.14 ps {i3} 


level_energy_unit: KEV
level_spin_parity: (13/2)-
level_lifetime_unit: PS
level_comment:
J 9/2 to 13/2 from |g(|q) and DCO in ({+12}C,p2n|g). |d(11/2)=-0.63 {i10} and RUL probably exclude J=11/2. J|p|=9/2 from |g deexcitation and stronger excitation in ({+12}C,2np|g) than in (|a,p|g). |p=- from M1 to 11/2-. 
T from DSAM in (|a,p|g). Others: 0.08 ps {i3} from {+55}Mn(|a,2n|g) and 0.11 ps {i4} from {+48}Ti({+12}C,p2n|g) 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2,11/2-)
level_lifetime_unit: PS
level_comment:
J from d, E2 transitions to 7/2-,11/2- 
T weighted av of 0.51 ps {i10} from (|a,p|g), 0.36 ps {i15} from (|a,2n|g), and 0.35 ps {i21} from (p,|g). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J from J-dependence of small angle cross-section in {+56}Fe({+7}Li,{+6}He); data fit both 5/2-,7/2-; however, rise in cross section at forward angles tends to favor 7/2- 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
J 5/2 assigned to the 3993 level from |g(|q) of primary capture |g rays from E(p)=1408, J=5/2 resonance in (p,|g). However, J|p=7/2- assumed to extract spectroscopic factors in ({+7}Li,{+6}He) gives a better fit than J|p=5/2-. 


level_energy_unit: KEV
level_spin_parity: (15/2)
level_lifetime_unit: PS
level_comment:
J 11/2 to 15/2 from |g(|q) and DCO. J|=13/2 from |d and RUL. J=15/2 favored from unique decay to (13/2) state and very weak excitation in (|a,p|g). 
T from DSAM in (|a,2n|g). Other: 0.07 ps {i5} from ({+12}C,p2n|g). 


level_energy_unit: KEV
level_comment:
J=(3/2-) from J-dependance of small angle cross section in {+56}Fe({+7}Li,{+6}He) at 4295; L({+3}He,d)=1, at 4295 {i15} 


level_energy_unit: KEV
level_spin_parity: 9/2(+)
level_comment:
J 9/2 from |g(|q) of primary capture |g rays in (p,|g); |p=(+) from comparison of |d for primary transition from the E(p)=3720 J|p=9/2+ resonance with single particle estimates. 


level_energy_unit: KEV
level_spin_parity: (17/2)
level_lifetime_unit: PS
level_comment:
J 17/2 favored from possible J=11/2-17/2 from stretched quadrupole type of |g(|q) of 2294|g 
T from RDM in ({+12}C,p2n|g) 


level_energy_unit: KEV
level_spin_parity: (19/2)
level_lifetime_unit: PS
level_comment:
J 15/2,19/2 from |g(|q) and DCO. 19/2 from unique decay to (17/2) state. 
T weighted av of DSAM in (|a,2n|g) and ({+12}C,p2n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (13/2)-
level_lifetime_unit: PS
level_comment:
J (13/2); J=9/2 to 13/2 from |g(|q) and DCO. |d=-0.63 {i10} for J=11/2 and T{-1/2} give extremely enhanced Q transition which excludes J=11/2. |g-deexcitation and stronger excitation of this level in ({+12}C,2np|g) than in (|a,p|g) make J=9/2 very improbable. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (15/2)
level_lifetime_unit: PS
level_comment:
J (15/2); J=11/2 to 15/2 from |g(|q) and DCO. From T{-1/2} and quadrupole transition probabilities, J=11/2 and 15/2 remain the most probable. J=15/2 favored from unique decay to (13/2-) state and very weak excitation in (|a,p|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (17/2)
level_lifetime_unit: PS
level_comment:
T$from 1981Ke05 (E({+12}C)=39 MeV; RDM). Other: 1.0 ps {I+28-3} (1977Be16) 
J 17/2 most likely from strong excitation in ({+12}C,p2n|g) compared to (|a,p|g) and stretched-quadrupole radiation. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J 9/2 from |g(|q) (1969Da05); |p=- from M1 to 7/2- 
T weighted av of 52 fs {i8} (1971Da22), and 58 fs {i12} (1971Bu04). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J 11/2 from |g(|q) (1971Da22); |p=- from E2 to 7/2- 
T from 1971Da22. Other: 0.18 ps {i8} (1971Bu04). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J 3/2 from |g(|q) (1970Co16); |p=- from E2 to 7/2- 
T weighted av of 0.31 ps {i4} (1971Da22) and 0.25 ps {i5} (1971Bu04) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J 7/2 from |g(|q) (1971Da22); |p=- from M1 to 9/2- 
T weighted av of 0.19 ps {i5} (1971Da22) and 0.22 ps {i6} (1971Bu04) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J 3/2 from |g(|q) (1971Da22); |p=- from E2 to 7/2- 
T unweighted average of 97 fs {i42} (1971Da22) and 35 fs {i14} (1971Bu04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J=7/2 from |g(|q); |p=- from RUL for the primary |g transition from the E(p)=3720 J|p=9/2+ resonance (1985El09) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2(+)
level_comment:
J=9/2 from |g(|q); |p=(+) from a comparison of the |d for the primary |g transition from the E(p)=3720 J|p=9/2+ resonance with single particle estimates (1985El09). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_comment:
J 9/2(+) from |g(|q) and comparison of the |d for the primary |g transition from the E(p)=3727 J|p=9/2+ resonance with single particle estimates (1979Ra13) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
J 5/2(+) from |g(|q) and comparison of the |d for the primary |g transition from the E(p)=3774 and 3794 J|p=5/2+ resonances with single particle estimates (1986El06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2-)
level_comment:
$C{+2}S=0.018 
J fits to the experimental data for J|p=7/2- or 5/2- are not significantly different, although the rise in cross section at forward angles would tend to favor J|p=7/2-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
$C{+2}S=0.026 
J 7/2- gives a better fit with a |h{+2} less than by a factor of 3 compared to the fit with J|p=5/2-. However, J|p=5/2- from adopted levels with a C{+2}S=0.035. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_comment:
$C{+2}S=0.060 
J 3/2+ preferred by comparison with ({+3}He,d) and (d,n) data of 1967Ro04 and 1976Ad05, respectively; 3/2- cannot be ruled out. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: D
level_comment:
J$ 1,2 from paramagnetic resonance (1957Do38); L(d,n)=3 from 1/2- does not allow J=1. Also L(d,|a)=L({+3}He,p)=L(t,{+3}He)=2; L({+3}He,d)=1, L(d,t)=1+3 
MOMM1,MOME2$NMR on oriented nuclei (1972Ni01). Others: |m=+4.040 {I14} (1957Do38,EPR method), 3.5 {I3} (1952Da19, nuclear orientation). 
T$weighted average of 70.77 d {I12} (measured value of 70.75 d {I7} in 1982HoZJ reanalyzed by 2002Un02, 2012Fi12 and 2014Un01); 70.916 d {I15} (1980Ho17), 70.81 d {I3} (1976Va30), 70.78 d {I4} (1975La16), 71.1 d {I2} (1972We17), 70.8 d {I9} (1972Cr02), 70.4 d {I10} (1972Cr02), 71.5 d {I8} (1968De08), 71.3 d {I2} (1956Sc87). Other measurements: 72 d {I6} (1973ArZI), 71.0 d (1955Co31), 75 d {I3} (1952Ru23), 72 d {I4} (1952Ho58), 72 d (1941Li01). In the Limitation of Relative Statistical Weight (LRSW) method the uncertainty of 1980Ho17 was increased from 0.015 to 0.022 to reduce its relative weight to 50%. The LRSW method increased the final uncertainty to 0.06 to include the most precise value of 70.916 d. This result agrees with the evaluation of 1991BaZS, except for a small reduction in the uncertainty. In November 2013 DDEP evaluation (www.nucleide.org), T{-1/2}=70.85 d {I3}, and in 2013Be43 compilation it is listed as 70.83 d {I10} 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 9.15 h {I10} (1967St23) and 8.94 h {I17} (1970Ca19). Others: 9.0 h {I2} (1960Pr05,1952Av17), 9.2 h {I2} (1952Ho58, 1950Ch62) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
MOMM1$stroboscopic observation of perturbed angular distribution (1970Be33). 
T$weighted average of 10.4 |ms {I3} in (p,n|g), 11.4 |ms {I6} in (|a,n|g) and 10.2 |ms {I6} in (|g,n) (1964Br27) 
J$L({+3}He,d)=3; E2+M1 |g to 5+; |g to 2+ 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: NS
level_comment:
MOMM1$integral PAD (1972Ha61) for T{-1/2}=0.18 ns 
T$weighted average of 0.18 ns {I3} in (p,n|g) and 0.12 ns {I2} in (|a,n|g) 
J dipole |gs to 2+ and 4+; L({+3}He,d)=3 


level_energy_unit: KEV
level_comment:
J (3+,4+,5+) if the L(d,|a)=(4) corresponds to this level; or (1+,2+) from L({+3}He,d)=1 and |g to 3+; 


level_energy_unit: KEV
level_spin_parity: (3,4)+
level_comment:
J (3+,4+) if the L(d,|a)=(4) corresponds to this level and |g to 2+; (2+) from L({+3}He,d)=1 and |g to 4+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$L-values in several particle transfer reactions strongly suggest 1+ assignment for a level near 1867 keV. However, in (p,|g) experiment, 1975Er07 suggest 2+ based on 1814.9|g placed from this level to 53, 4+ level. Note that the 1814.9|g was not reported in {+56}Fe({+3}He,p|g) reaction where the 1867 level was populated 


level_energy_unit: KEV
level_comment:
E most probably a triplet according to 1972Sc13: with levels at 3090 {I9}, L=(1,2) (d,|a); 3096 {I9}, L=1 ({+3}He,d); 3100 {I10}, L=2 ({+3}He,p); 3100 {I15}, J|p=2+,3+ (t,{+3}He) 


level_energy_unit: KEV
level_comment:
J 1+ from L({+3}He,p)=0+2 is not consistent with J|p=(2-,3-,4-) from L(d,|a)=(3); |gs to 1+ disfavor J|p=3-,4- 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J L({+3}He,p)=0+2 
E weighted average of 3668 {I11} ({+3}He,d), 3668 {I20} (t,{+3}He), 3670 {I10} ({+3}He,p) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 9.15 h {I10} (1967St23) and 8.94 h {I17} (1970Ca19). Others: 9.0 h {I2} (1960Pr05,1952Av17), 9.2 h {I2} (1952Ho58,1950Ch62). Same value in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 7+
level_comment:
E$ based on the ordering of the 802-1600 cascade from the 5097 level as shown in figure 1 of 2006Si37. In authors' table I, the ordering is given as reversed which gives energy of the intermediate level at 3498 keV 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.2 ps +7-4 (1975Br05) and 1.0 ps {I+8-4} (1972Ge14) 
J J=3 from |g(|q) and RUL (1975Br05) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.5 ps +9-5 (1975Br05) and 0.62 ps {I+51-24} (1972Ge14) 
J J=3 or 5 from RUL and |g(|q) (1975Br05) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.87 ps +31-26 (1975Br05) and 0.8 ps {I+6-3} (1972Ge14) 
J J=5 is ruled out by |g(|q) of 1975Br05 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.019 
E,S includes the 25 level (1973Ca07), but the contribution from this level is expected to be small (1973Ha27) 
L$from 1973Ha27 


level_energy_unit: KEV
level_comment:
$d|s/d|W (max)=0.034 mb/sr (1973Ha27) 
From the relative strength of excitation of 3423 and 3555 in 1973Ha27, this level should have been seen by 1973Ca07. 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.965 
E,S probably a doublet (1973Ha27). Two 0+ levels at about this energy are deduced from ({+3}He,p|g) data 


level_energy_unit: KEV
level_spin_parity: 6-&8-
level_comment:
E from 1980Ok03 
J$a doublet with (f{-7/2},g{-9/2}){-8-}+(p{-3/2},g{-9/2}){-6-} configuration according to the analysis of 1994Fi01 for a level at 3720 who observe an enlarged line width. A single level with a (f{-7/2},g{-9/2}){-8-} configuration is deduced by 1993Yu07 who determine L=7 giving 6-,7-,or 8-, but assign J|p=8- based on an expectation that the maximum coupling should dominate. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$1994Fi01 assign a (g{-9/2},p{-3/2}){-6-} configuration to this level; and 1993Yu07 assign (f{-5/2},f{-5/2}){-5-}. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E$ 365 with 0.2 uncertainty (1975Er07) is assumed to be a typographical error since they also report an EG=365.6 1 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1191 {I2} 
$ EP=1171 QUOTE BY 1970Er03 SEEMS IN C.M. SYSTEM, ENERGY OF THIS PEAK IS HIGHER THAN 1171 IN SPECTRAL FIGURE SHOWN IN 1970Er03 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1193 {I2} 
$ EP=1173 QUOTE BY 1970Er03 SEEMS IN C.M. SYSTEM, ENERGY OF THIS PEAK IS HIGHER THAN 1173 IN SPECTRAL FIGURE SHOWN IN 1970Er03 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1204 {I2} 
$ EP=1184 QUOTE BY 1970Er03 SEEMS IN C.M. SYSTEM, ENERGY OF THIS PEAK IS HIGHER THAN 1184 IN SPECTRAL FIGURE SHOWN IN 1970Er03 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1210 {I2} 
$ EP=1190 QUOTE BY 1970Er03 SEEMS IN C.M. SYSTEM, ENERGY OF THIS PEAK IS HIGHER THAN 1190 IN SPECTRAL FIGURE SHOWN IN 1970Er03 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1467 {I2} 
$Unassigned |g rays in 1970Er03: 1974.5 {I10} (4.0% {I5}), 1477.7 {I10} (4.0% {I5}), 911.1 {I5}; not reported in 1975Er03 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1583 {I2} 
$An 8395 {I3} |g with I|g=0.5 {I2} and a 6769 {I4} |g with I|g=2.0 {I5} from 1970Er03 are omitted since 1975Er07 did not confirm a 116 level in {+58}Co and the 6769|g proposed in 1970Er03 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1626 {I2} 
$An 8439 {I4} |g with I|g=1.0 {I5} from 1970Er03 is omitted since 1975Er07 did not confirm a 116 level in {+58}Co proposed in 1970Er03 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.140 {I9} 
$B(>)=0.15 {i1} 
$d|s/d|W=0.159 mb/sr {I9} (2004Ha01) 
E$probable parent of isobaric analog of 9835 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.055 {I5} 
$B(>)=0.06 {i1} 
$d|s/d|W=0.057 mb/sr {I5} (2004Ha01) 
E$probable parent of isobaric analog of 11423 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.143 {I9} 
$B(>)=0.17 {i1} 
$d|s/d|W=0.145 mb/sr {I9} (2004Ha01) 
E$probable parent of isobaric analog of 11661+11683 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.125 {I8} 
$B(>)=0.15 {i1} 
$d|s/d|W=0.126 mb/sr {I8} (2004Ha01) 
E$probable parent of isobaric analog of 11883 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.062 {I7} 
$B(>)=0.07 {i1} 
$d|s/d|W=0.065 mb/sr {I7} (2004Ha01) 
E$probable parent of isobaric analog of 12197 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.076 {I9} 
$B(>)=0.09 {i1} 
$d|s/d|W=0.080 mb/sr {I9} (2004Ha01) 
E$probable parent of isobaric analog of 12293 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.058 {I7} 
$B(>)=0.07 {i1} 
$d|s/d|W=0.067 mb/sr {I7} (2004Ha01) 
E$probable parent of isobaric analog of 12386 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.060 {I6} 
$B(>)=0.07 {i1} 
$d|s/d|W=0.062 mb/sr {I6} (2004Ha01) 
E$probable parent of isobaric analog of 12636 in {+58}Ni 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: H
level_lifetime_info: ;ISO=M
level_comment:
T$measured by 2019Mo11; weighted average of 8.847 h {I23} from decay curve of 24.9|g shown in Fig. 3 of 2019Mo11, and 8.942 h {I70} from the growth and decay function, as shown in Fig. 4 of 2019Mo11, and by keeping the half-life of the ground state of {+58}Co fixed at 70.86 d. Authors compared their value with previous measurements of 8.94 h {I17} (1970Ca19: Nucl. Phys. A152, 631); 9.5 h {I5} (1968Wi10: Z. Physik 213, 56); 9.3 h {I3} (1968Rh01: Phys. Rev. 167, 1049); 9.15 h {I10} (1967St23: Z. Physik 207, 119); 9.0 h {I2} (1960Pr05: Nucl. Phys. 15, 326); 9.2 h {I2} (1952Ho58: J. Phys. Chem. 56, 1097); 9.0 h {I2} (1952Av17: Phys. Rev. 87, 216|a); 9.2 h {I2} (1950Ch62: Phys. Rev. 80, 1110); 8.8 h (1950St22: Phys. Rev. 79, 487). Authors also compare their measured value with evaluations such as 8.94 h {I17} in 1973Ba67: At. Energy Rev. 11, 524; and 9.10 h {I9} in 2010Ne01: Nucl. Data Sheets 111, 897. 
$Compiler's note: 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J 7/2 from electron paramagnetic resonance (1951Bl38) and optical spectroscopy (see 1976Fu06); L=3 in ({+3}He,d), (t,|a), (d,{+3}He), (|a,t). 
MOMM1 From NMR (1967Wa16/1951Pr02, 2014StZZ). 
MOME2 From 2008Py02, 2016St14, Atomic beam magnetic resonance. Others: +0.41 {I1} (1993De41 - reevaluation of hfs parameters), 2014StZZ quote +0.40 {I4} (1961Eh01, atomic beam, uncorrected for polarization) and 0.42 {I3} (1969Mu11, optical spectroscopy, Sternheimer correction included); 0.35 {I3} (1990Gu28, optical spectroscopy, no Sternheimer correction); +0.42 {I3} (2008Py02/1960Eh03, 2014StZZ - reevaluation - atomic beam). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L=1 in ({+3}He,d), (t,|a), (d,{+3}He), (|a,t); L(p,p')=2. Analyzing power analysis in (pol p,|a). 
T weighted average of 3.0 ps {I6} (Coulomb excitation) and 2.7 ps {I6} (|g,|g). Other: >2.4 ps (p,p'|g), <14 ps ({+59}Fe |b{+-} decay). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
E: 1190.6 3 (A), 1191.4 9 (B), 1190.7 1 (C), 1189.5 1 (D), 1189.6 5 (I) 
J L=2 in (p,p'), (|a,|a'); 9/2- from (pol p,|a). 
T weighted average of 53.7 fs {I25} (|g,|g), 55 fs {I7} (Coulomb excitation). Others: 33 fs {I6} (p,p'|g); 75 fs {I17} (n,n'|g); <111 fs (p,|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J L=1 in ({+3}He,d), (t,|a), (d,{+3}He), (|a,t); 3/2,5/2 from p-|g(|q) in (|a,p|g). 
T from {+59}Fe |b{+-} decay. Other: >0.76 ps from (p,p'|g). 
MOMM1$From integral perturbed angular correlation (IPAC) (1974Ba08, 2014StZZ). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J L=1 in ({+3}He,d); not 3/2 from |g|g(|q) in {+59}Fe |b{+-} decay. 
T from |b{+-} decay (delayed coin). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J 11/2- from (pol p,|a); 11/2,7/2 from p-|g(|q) in (|a,p|g). 
T weighted average of 1.14 ps {I14} (Coulomb excitation), 0.94 ps {I13} (|g,|g'). Uncertainty lowest input value. Others: 2 ps {I+11-1} (p,p'|g), 0.7 ps {I+7-3} (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J L=2 in (p,p'); 5/2 from p-|g(|q) in (|a,p|g). 
T weighted average of 190 fs {I20} (|g,|g), 139 fs {I+35-28} (p,p'|g) and 180 fs {I+100-60} in (n,n'|g). Others: |<173 fs in (p,|g), |<14 ps in {+59}Fe |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
E: 1745.0 10 (B), 1744.7 4 (C), 1745.1 3 (D), 1743.63 8 (G) 1745 1 (I) 
J from (pol p,|a); 7/2,9/2 from p-|g(|q) in (|a,p|g); L(t,|a)=3. 
T weighted average of 0.28 ps {I12} (Coulomb excitation) and 0.36 ps {I11} (|g,|g). Others: 0.52 ps {I+55-21} (p,p'|g); 0.42 ps {I+21-17} (n,n'|g); |<0.17 ps (p,|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
E: 2061.6 10 (B), 2061.7 1 (C), 2062.8 4 (D), 2060.73 10 (G) 
J L(t,|a)=3; 7/2 from p-|g(|q) in (|a,p|g). Analyzing power analysis in (pol p,|a). 
T Weighted average of 0.10 ps {I+6-4} from {+59}Co(p,p'|g) and 0.19 ps {I+9-5} from {+59}Co(n,n'|g), DSAM. Other: |<0.097 ps (p,|g). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: FS
level_comment:
E: 2087.0 11 (B), 2087.0 2 (C), 2088.3 5 (D), 2086.18 10 (G) 
J 5/2,3/2 from p-|g(|q) in (|a,p|g); 5/2- from statistical analysis in (n,n'|g); M1(+E2) |g to 3/2- and 7/2-. 
T From (n,n'|g), DSAM. Others: 0.2 ps {I+12-1} (p,p'|g), |<173 fs (p,|g). 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
E: 2153.5 3 (A), 2153.6 10 (B), 2153.8 3 (C), 2153.4 6 (D) 
J Conflicting spin assignments. 9/2,13/2 in p-|g(|q) in (|a,p|g); 9/2+ from Analyzing power analysis in (pol p,|a). (13/2) from systematics in ({+15}N,4n|g); statistical analyses yield 15/2 in (p,p'|g), (7/2-) in (n,n'|g); |g from (7/2-) favors 9/2, however, |g from (15/2) yields |DJ=3. 
T from (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: FS
level_comment:
E: 2183.4 3 (A), 2183.5 10 (B), 2183.2 3 (C), 2185.4 6 (D) 
J From analyzing power analysis in (pol p,|a). D(+Q) |g to 9/2-; (11/2) from reaction systematics and |g(|q) in ({+15}N,4n|g); statistical analysis gives 11/2 in (p,p'|g). Other: 7/2- in (n,n'|g). 
T Using the Limitation of Relative Statistical Weight (lwm) method (1985ZiZY) of 33 fs {I+8-6} from (p,p'|g) and 66 fs {I12} from (n,n'|g) (DSAM) (discrepant data). 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
E: 2205.1 10 (B), 2204.8 2 (C), 2204.5 6 (D),2203.77 9 (G). 
J 5/2 from p-|g(|q) in (|a,p|g) and from statistical analysis in (n,n'|g); |g to 1/2- and 9/2-. 
T from (n,n'|g). Other: |>0.14 ps in (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (9/2)
level_lifetime_unit: PS
level_comment:
E: 2394.5 9 (B), 2394.6 2 (C), 2397.1 6 (D), 2397 6 (E) 
J 7/2,9/2 from p-|g(|q) in (|a,p|g); 9/2 from Hauser-Feshbach analyses in (p,p'|g) and (n,n'|g). 
T from (n,n'|g), DSAM. Other: 0.07 ps {I+14-6} from (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: FS
level_comment:
E: 2478.4 10 (B), 2478.5 5 (C), 2479.0 7 (D), 2479 1 (I). 
J statistical analyses give 5/2 in (p,p'|g) and 5/2- in (n,n'|g); M1+E2 |g to 7/2-. 
T weighted average of 31 fs {I3} from (n,n'|g), 23 fs {I3} from (|g,|g) and 26 fs {I+13-8} (d,d'|g). Other: |<13 fs, (p,|g). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
E: 2542.7 10 (B), 2540.3 2 (C), 2541.0 9 (D). 
J 5/2,7/2,9/2 from p-|g(|q) in (|a,p|g); statistical analysis yields 5/2(-) in (n,n'|g), 9/2 in (p,p'|g). |g rays to 7/2- and 9/2-. |g ray from (1/2-). 
T from (n,n'|g) - DSAM. Other: 0.2 ps {I+18-1} in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
E: 2584.9 10 (B), 2586.4 9 (C), 2585.9 7 (D) 
J from (pol p,|a). Statistical analyses yield 7/2 in (p,p'|g), but 9/2- in (n,n'|g). L(t,|a)=3. 
T weighted average of 62 fs {I+28-14} from (p,p'|g) and 69 fs {I14} from (n,n'|g), DSAM. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: FS
level_comment:
E: 2780.1 12 (B), 2782.3 9 (C), 2781.0 9 (D), 2783 1 (I). 2782.0 3 (G). 
J 5/2(-) from statistical analysis in (n,n'|g); |g to 3/2- and 7/2-. 
T from (n,n'|g). Other: <58 fs from {+59}Co(p,p'|g), DSAM. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: FS
level_comment:
J 3/2- from statistical analysis in (n,n'|g). 
T from DSAM in (n,n'|g); possibly low by a factor of |?3. 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
$E: 2965.1 12 (B), 2966.2 8 (C), 2966 1 (I) 
J$(3/2-) from statistical analysis in (n,n'|g) conflicts 782.4|g feeding to (11/2) state at 2183.5, see spin-parity comment there. 
T from (|g,|g); uncertainty in 2966|g branching not included. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
E: 3015.9 12 (B), 3014.9 8 (C) 
T from {+59}Co(n,n'|g), DSAM. 
J from statistical analysis in (n,n'|g). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
E: 3081.4 3 (A), 3082.3 12 (B), 3081.7 2 (C) 
J from excitation, |g(|q) in ({+15}N,4n|g); conflicts with 5/2- from statistical analysis in (n,n'|g). (9/2-) from (pol p,|a) for this and/or 3091 level. 
T from (n,n'|g), DSAM. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_comment:
E: 3090.6 12 (B), 3090.4 6 (C), 3086.5 6 (G) 
T from {+59}Co(n,n'|g), DSAM. 
J from statistical analysis in (n,n'|g). (9/2-) for 3081 and/or 3091 level from (pol p,|a). 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)
level_comment:
E: 3142.3 12 (B), 3140.5 14 (C), 3141.03 18 (G) 
J from statistical analysis in (n,n'|g). J|p=(7/2-) from (pol p,|a) for E=3142.3 {I12} level(s). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
Differs from 3140.5 level in (n,n'|g) because |g branching differs. 
J |g to 11/2-; |g from (3/2-). J|p=(7/2-) from (pol p,|a) for E=3142.3 {I12} level(s). 


level_energy_unit: KEV
level_comment:
3222.6 11 (B), 3218.6 6 (C) 
J 3/2- from statistical analysis in (n,n'|g). 824.7|g to (9/2) in the same dataset yields |DJ=3. 


level_energy_unit: KEV
level_comment:
3322.1 11 (B), 3324.3 10 (C), 3326 5 (E) 
J 7/2(-) from statistical analysis in (n,n'|g), yields |DJ=3 for 1889.1|g transition. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: FS
level_comment:
3382.3 11 (B), 3381.9 5 (C), 3383 6 (E) 
J from statistical analysis in (n,n'|g). 
T from {+59}Co(n,n'|g), DSAM. 


level_energy_unit: KEV
level_comment:
3416.0 12 (B), 3413.1 11 (C), 3416 5 (E) 
J$9/2- assignment from statistical analysis in (n,n'|g) yields |DJ=3 for 2315.2|g transition. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E approximate centroid of {+59}Fe(287 level) analogue fragments. See {+58}Fe(p,p') for E and |G{-p0} of 10 fragments, E=9751 {I3} to 9890 {I3}. 
J from {+58}Fe(p,p'). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: NS
level_comment:
J 3/2 excluded by 142|g-1292|g(|q), 142|g-192|g(|q) and 192|g-1099|g(|q). 
T from 1971Ar07. Delayed coin. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$The energy of this level exceeds the decay Q(|b{+-})value. From re-analysis of |g spectrum coincident with cobalt K x-rays observed in the decay of {+59}Ni in 1991Ja02, 2015Pf02 propose the population through virtual or 'detour' transitions. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=AP
level_comment:
E 9542.0 from E(p)(lab)=2216 keV (1975Br29) and S(p)=7363.6 {I4} (2017Wa10). 
J if fragment of {+59}Fe(g.s.) analogue. 
|G{-|g}=0.81 eV (1975Br29), if |G|?|G{-p0}; 1.0 eV (1972Pe23). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=AP
level_comment:
E 9549.9 from E(p)(lab)=2224 keV (1975Br29) and S(p)=7363.6 {I4} (2017Wa10). 
J if fragment of {+59}Fe(g.s.) analogue. 
|G{-|g}=0.62 eV (1975Br29), if |G|?|G{-p0}; 0.92 eV (1972Pe23). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=AP
level_comment:
E 9552.85 from E(p)(lab)=2227 keV (1975Br29) and S(p)=7363.6 {I4} (2017Wa10). 
J if fragment of {+59}Fe(g.s.) analogue. 
|G=1.06 eV (1975Br29), if |G|?|G{-p0}; 1.40 eV (1972Pe23); 1.25 eV {I20} (1977Ri14), if |G=|G{-p0}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-)
level_comment:
E from E(p)(lab)=3900 keV (1993Ti06) and S(p)=7363.6 {I4} (2017Wa10). 
J analogue of 5/2- {+59}Fe(1570 level) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2-)
level_comment:
E from E(p)(lab)=3850, the average of 3900 keV (1993Ti06) and 3800 (1975Br05) assuming S(p)=7363.6 {I4} (2017Wa10). 
J analogue of 5/2- {+59}Fe(1570 level) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (3/2-)
level_comment:
$E(p)(LAB)=2980 |? 
J analogue of 3/2- {+59}Fe(726 level); identified but not analyzed in detail by 1971Li14. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$|G{-|g0}{+2}/|G=0.146 {I26} 
T$From |t=3.96 ps {I83}, unweighted average of 4.79 ps {I55} (1981Ca10) and 3.13 ps {I60} (from |G{-0}=0.21 meV 4 in 1971Sw06 and |G{-0}/|G=1). 
|G{-|g0}{+2}/|G: 0.11 {I2} (1971Sw06), 0.138 {I16} (1981Ca10). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
T from |G{-|g0}=8.5|*10{+-3} eV {I4}, weighted average of 8.2|*10{+-3} eV {I9} (1971Sw06) and 9.0|*10{+-3} eV {I4} (1981Ca10). Uncertainty lowest input value. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
$|G{-|g0}{+2}/|G=0.40 {I6} 
T$From |t=1.35 ps {I19}, weighted average of 1.19 ps {I14} (from 1.17 ps {I14} - 1981Ca10) and 1.57 ps {I16} (from |G{-0}=0.39 meV 4 in 1971Sw06 using |G{-0}/|G=0.929). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G=1.49 {I16} 
T$From |t=0.27 ps {I3}, unweighted average of 0.242 ps {I30} (from 0.254 ps 31 - 1981Ca10) and 0.299 ps {I30} (from |G{-0}=1.68 meV 17 in 1971Sw06 using |G{-0}/|G=0.763). 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G=15.2 {I8} 
T From |G{-|g0}{+2}/|G (from 1971Sw06 assuming J=5/2 and W(|q)=1.010 {I9}) and |G{-0}/|G=0.87 {I10}. 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
$|G{-|g0}{+2}/|G=5.4 {I16} 
T$From |G{-|g0}{+2}/|G (from 1971Sw06 assuming J=3/2 and W(|q)=1.00 and |G{-0}/|G=0.65). Uncertainty does not include that for branching (2966|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
B(E2): weighted average of 0.0089 {I18} (1964Al27), 0.005 {I2} (1967No04), 0.005 {I1} (1969Ga25). Other: 1961An07. 
T from B(E2). 10 ps {I11} (1977Do16) and >2.9 ps (1967No04) from DSAM. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
B(E2): weighted average of 0.017 {I3} (1964Al27), 0.022 {I2} (1967No04), 0.023 {I4} (1969Ga25). Others: 1961An07, 1960Ad01. 
T from DSAM (1967No04). Others: 54 fs {I17} (from B(E2), branching and adopted |d=0.20 {I3}), 71 fs {I11} (DSAM, 1977Do16), 50 ps {I20} (DSAM, 1967St11). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
B(E2)=0.0007 {I3} (1969Ga25), 0.012 {I2} (1964Al27); B(E2)|?0.000013 is implied by adopted T{-1/2}(1292 level), so both measured B(E2) values are presumed to be erroneous. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2)-
level_lifetime_unit: PS
level_comment:
B(E2): weighted average of 0.007 {I2} (1969Ga25), 0.012 {I2} (1967No04), 0.010 {I3} (1964Al27), 0.013 {I3} (1961An07), 0.015 {I5} (1960Ad01). Uncertainty lowest input value. 
T weighted average of 1.15 ps {I14} (from B(E2) and I|g) and 1.11 ps {I28} (DSAM, 1967No04). Uncertainty lowest input value. 


level_energy_unit: KEV
level_comment:
C{+2}S: after allowance for small L=1 contribution from the tail of the 3/2- 1099 level. Other C{+2}S: 5.15 (1961Co08). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: D
level_comment:
MOMM1$From nuclear magnetic resonance (NMR) on oriented nuclei (1972Ni01,1989Ra17,2011StZZ). 
MOME2$From nuclear magnetic resonance (NMR) on oriented nuclei; no pol correction included (1972Ni01,1989Ra17,2011StZZ). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: H
level_comment:
J$L(t,p)=0; L(t,|a)=L(p,|a)=3 
T$weighted average of 1.650 h {I5} (1951Sm64), 1.66 h {I1} (1956Nu02), 1.645 h {I7} (1956Ru45), 1.70 h {I3} (1962Va23), 1.58 h {I3} (1966St11), 1.63 h {I3} (1967Gr15,1968Ka21), 1.66 h {I7} (1982Ma41). Reduced |h{+2}=1.7. Others: 1.75 h (1948Ku01), 1.75 h {I5} (1949Pa01), 1.70 h {I5} (1960Pr05), 1969Ki09. 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2; |g to 7/2-; 9/2- from (p,|a); first 9/2- predicted at 1405 keV in shell-model calculations (2011Sr04) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$298(|q) probably isotropic in ({+48}Ca,p2n|g); log| {Ift}=5.90 from (3/2-); 1/2- favored in (p,|a) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
J$L(d,{+3}He)=3; 7/2- is suggested from |s(|q) in (p,|a), but possible |b feeding (log| {Ift}=7.5) from (3/2-) supports 5/2- 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=15 
$L=2 or (1+3) or (2+4),better fitted with L=1+3 (1985Fo02). 
$L=2,for 2765 {i25} group, |s{-max}=14 |mb/sr (1971Hu01). 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=24 
$L=2,for 3017 {i25} group, |s{-max}=29 |mb/sr (1971Hu01). 
L$2 for a 3017 {I25} group (1971Hu01). 


level_energy_unit: KEV
level_comment:
$d|s/d|W(max)=38 
$L=0+2,for 3515 {i25} group, |s{-max}=110 |mb/sr (1971Hu01). 
$L=2+3 or 2+4, or 1+3+6 (1985Fo02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+,11/2+
level_uncertain: ?
level_comment:
$Fictitious level corresponding to a negative value of resonance energy 
$E(n)(lab)=-0.100 keV, |G{-|g}=(1.2) eV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$measured effective mean lifetime |t<2 ps using RDDS method (2017Kl01). Feeding from 13/2- state was included in the fitting, but statistics were insufficient to deduce a precise lifetime. Authors compared this value to previous measurement of |t=10 ps {I+10-3} by 1996Re18 (Phys. Rev. C54, 1084) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (J GE 23/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$x |? 8.5 MeV from level-scheme figure 3 in 2015Ay02 


level_energy_unit: KEV
level_spin_parity: (2)+
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=5.71 and 5.57 to 2+ states; L(d,|a)=(2,0+2); shell model predictions (1999Ca29). Lack of |b feedings to 0+ and 4+ states is consistent with J=2 
T$ weighted average of 1.4 min {I2} (1970Jo12, from decay curve of 1129|g followed for more than five half-lives, also 1971JoZN thesis - half-life plots given for several gamma rays); 1.50 min {I4} (1969Wa16, from |g|g coin and high energy |b(E>3 MeV) - only lists half-life, no decay curves shown - uncertainty increased to 0.2 by the evaluators); 1.5 min {I1} (1962Va23, from |b-decay curve followed over about four half-lives - no discussion of contaminants - uncertainty increased to 0.2 by the evaluators); 1.9 min {I3} (1960Pr05, from |b decay curve - only lists half-life, no decay curves shown); 1.6 min {I2} (1949Pa01, from |b decay curves followed over six half-lives) 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$ may be a doublet according to (t,{+3}He) results with second component being 2+. 
J$log| {Ift}=5.4 to 4+; L(d,|a)=4; |s(|q) and A{-y}(|q) patterns consistent with J|p=5+. Shell model predictions (1999Ca29) suggest a 5+ level at |?250 keV 
T$ from weighted average of 13.5 min {I3} (1970Jo12, from decay curves of 1163|g and 1173|g followed for more than two half-lives, also 1971JoZN thesis - half-life plots shown); 13.8 min {I5} (1969Mo04, from decay curves of 1163, 1172, 1717, 2003, and 2103 |g rays followed over about six half-lives - half-life plots shown); 14.00 min {I24} (1969Wa16, from |b(E>1.5 MeV) and |g(E>1.4 MeV decay curves - only lists half-life, no decay curves shown); 13.9 min {I2} (1962Va23, from |b-decay curve shown and followed over about two half-lives - no discussion of contaminants); 13.8 min {I2} (1960Pr05, from |b decay curve - only lists half-life, no decay curves shown); 13.91 min {I5} (1957Ga15, from |g decay measured in a well-type scintillation detector, minor {+64}Cu and {+65}Ni impurities detected - only lists half-life, no decay curves shown; uncertainty inflated to 0.2 by the evaluators); 13.9 min {I2} (1949Pa01, from |b decay curves followed over six half-lives) 
$ Searches for a 22-keV isomeric transition as photons or Co x rays following possible heavily-converted IT decay have proved negative (1969Es03,1970Jo12). Implies almost 100% |b{+-} decay of the isomer 


level_energy_unit: KEV
level_comment:
E$ 246 {I10} doublet in (d,|a) probably corresponds to 230+244 seen in (t,{+3}He) 
J$(3+,4+) proposed in (t,{+3}He). L(d,|a)=(2) for a 246-keV doublet suggests (1+,2+,3+) for one of the components 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J$L(d,|a)=4; |s(|q) pattern in (pol d,|a) consistent with J=5, also analogy with |s(|q) pattern for 5+ g.s. in {+60}Co. (5+,6+) suggested in (t,{+3}He) 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_comment:
J$L(d,|a)=2; comparison of |s(|q) pattern with known cases in neighboring nuclei favors L=2, J=3 in preference to J=2. (2+) proposed in (t,{+3}He) 


level_energy_unit: KEV
level_spin_parity: (7)
level_lifetime_unit: PS
level_comment:
J$|DJ=1, dipole |g to (6). (5+,6+) proposed in {+62}Ni(t,{+3}He) 
T$from DSAM in {+48}Ca({+18}O,p3n|g) 


level_energy_unit: KEV
level_comment:
E$doublet in (t,{+3}He). E=2149 {i10} in (d,|a) probably corresponds 2135+2165 groups in (t,{+3}He) 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3+)
level_comment:
J$L(d,|a)=(2); comparison of |s(|q) pattern with known cases in neighboring nuclei favors L=2, J=3 in preference to J=2 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E,J$1976Aj03 state (2+ and 5+) for a doublet. Not clear whether 22-keV group is a doublet with J|p=2+ and 5+, or whether 22-keV group and g.s. form a doublet. The evaluators consider the latter possibility as more likely 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_comment:
J$L(pol d,{+3}He)=L(t,|a)=3 from 0+; L+1/2 transfer from analyzing powers 
T$weighted average of 26 s {I1} (1969Wa15), 27.5 s {I3} (1972Jo08), 27.4 s {I5} (1995ItZY). Other: 52 s {I5} from 1960Mo01 is discrepant 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(pol d,{+3}He)=L(t,|a)=1 from 0+; L+1/2 transfer from analyzing powers 
T$from RDDS in ({+238}U,X|g). Other: >10 ps from (d,{+3}He|g) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
J$1382.8|g (D), |DJ=(1) to 7/2-; 290.3|g (D), |DJ=(1) from 11/2-; also band assignment. But L(d,{+3}He)=(3) from 0+ gives (5/2-,7/2-) 
T$from RDDS in ({+238}U,X|g). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$L(t,|a)=(1) from 0+; 1495|g to 7/2-. Other: L(d,{+3}He)=(3) from 0+ is inconsistent; see comments in (d,{+3}He) dataset 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$1673.5|g E2, |DJ=2 to 7/2- gives 3/2- or 11/2-; although L(d,{+3}He)=(5) favoring 11/2- is tentative, but L=1 favoring 3/2- is ruled out from analysis of measured |s(|q) in 1991Se09 and 1979Ha03. 
T$weighted average of 0.38 ps {I13} from ({+238}U,X|g) and 0.7 ps {I2} from ({+64}Ni,X|g), both using RDDS 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$1333.5|g to to 11/2-; 1623.9|g to (9/2-); (13/2-) proposed in ({+48}Ca,p2n|g), assuming J increases as excitation energy increases 


level_energy_unit: KEV
level_spin_parity: (17/2-)
level_lifetime_unit: PS
level_comment:
J$407.1|g (D), |DJ=(1) to (15/2-); (17/2-) proposed in ({+48}Ca,p2n|g) assuming J increases in excitation energy increases 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: FS
level_comment:
J$(3/2,5/2)+ in 1992Se03. See comments for L-transfer of 3413 level in (d,{+3}He) where L=3 from 1979Ha03 is adopted instead of L=(2) from 1991Se09 
T$original value=41 fs {I+41-20} 


level_energy_unit: KEV
level_comment:
E$other: 1430 {I30} (1979Ha03) 
L$from 1979Ha03. Other: L=(1) from 1991Se09. As claimed in 1991Se09 L=3, 1 and 3 are assigned to the weak levels of 1382, 1423, and 1491, respectively, but no |s(|q) data are shown in 1991Se09, while L=(3) for a 1430 level in 1979Ha03 seems to be a good fit to their measured |s(|q) data and L=(1) is assigned to the 1492 level by 1966Bl15 in (t,|a). The evaluator has adopted L(1423)=(3) and L(1491)=(1) 
S$from 1979Ha03 for J=7/2. Other: 0.01 for J|p=1/2- and 3/2- in 1991Se09 


level_energy_unit: KEV
level_comment:
L$see comments for 1423 level. Other: L=(3) with C{+2}S=0.08 or 0.04 from 1991Se09, but not adopted by the evaluator. 


level_energy_unit: KEV
level_comment:
S$40.54 for J=11/2 in 1991Se09 is very likely a misprint 
E$other: 1660 {I20} (1979Ha03) 
S$other: 0.2 for J=11/2 (1979Ha03) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$other: 2160 {I10}, doublet of 2129+2191 (1979Ha03) 
S$other: 1.4 for J=7/2 from 1966Bl15 in (t,|a) assumed in analysis (1979Ha03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$rounded value from (d,{+3}He|g) data in 1992Se03; not reported in 1992Se03 but a weak peak can been seen at around this energy in the {+3}He spectrum in 1992Se03. See also comments for 2473 level 


level_energy_unit: KEV
level_comment:
E$a peak at this energy is clearly seen in the {+3}He spectrum (FWHM=20 keV) in Fig.5 of 1991Se09, but not seen in the {+3}He spectrum in 1992Se03 (FWHM=170 keV) and 1979Ha03 (FWHM|?100 keV) probably because it is not resolved from the 2330 level due to poor resolution. However, a level at 2374.8 is reported by 1992Se03 based on |g data of (d,{+3}He|g) but it is not reported in 1991Se09. A weak peak in Fig.5 of 1991Se09 between 2330 and 2473 peaks and on the tail of 2330 peak may correspond to this level in 1992Se03. 


level_energy_unit: KEV
level_comment:
J$3/2+ is favored from analyzing powers, but 5/2+ can not be ruled out compeltely (1991Se09) 
E$other: 2680 {I20} (1979Ha03) 
S$other: 1.8 for J=3/2 (1979Ha03) 


level_energy_unit: KEV
level_comment:
E$other: 3400 {I20} (1979Ha03) 
L$from 1979Ha03. Other: (3,2) from 1991Se09; L=(2) from 1992Se03. Note that 1992Se03 assigned L=2 based on their measured |g(|q), which however looks structureless. This makes their L=2 assignment questionable. The L=3 assignment from 1979Ha03 looks to be a good fit to their |g(|q). 
S$other: 0.6 for J=7/2 (1979Ha03); 0.11 for J|p=3/2+ and 0.07 for 5/2+ with L=(2) (1991Se09) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T$from |t=0.55 ps {I19} using RDDS method with 1672|g (2017Kl01). Unobserved feeding is 62% with effective mean lifetime of 7 ps. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
T$from 1974Ra31. Other: 0.40 s {I5} (1969Wa15) 
J$log| {Ift}=4.3 to 0+ (see {+64}Co |b{+-} decay); L(d,{+2}He)=0 from 0+ 


level_energy_unit: KEV
level_lifetime_unit: MS
level_lifetime_info: ;ERR=GT;ISO=M
level_uncertain: ?
level_comment:
E$from mass excess of -59792 keV {I20} for {+64}Co g.s. in 2021Wa16 and measured mass excess of -59685.7 keV {I41} using LEBIT at NSCL-MSU, 2010Fe01, tentatively, propose an isomer at 107 keV {I20}. 
J$(5+) assigned by 2010Fe01 in analogy with low-lying (5+) isomers in {+62}Co and {+66}Co, but note that J|p=(3+), instead of (5+) is assigned for the 175-keV isomer in {+66}Co by 2012Li02 
T$estimated by 2010Fe01 from the time interval spent by the ions in the mass measurement apparatus. 2021Ko07 give 300 ms from systematics 


level_energy_unit: KEV
level_comment:
E$level listed in the text, not in table I of 2007Po06 
L$probable L=0 transition from strong intensity at low angles. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E$assumed as the g.s. by 2000As05 based on level spacings of the 867, 804, 703, 463 and 0 levels in (t,{+3}He) (1972Fl17) being similar to the 64-97-232-441 cascading |g-ray energies from the 6.4-ns isomer, and non-observation of a 33 keV group in (t,{+3}He). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: S
level_comment:
T Weighted average of 1.00 s {I15} (2009Pa16), 1.12 s {I25} (1994Cz02), 1.14 s {I3} (1988Bo06), and 1.25 s {I5} (1985Ru05). 
J From log| {Ift}=4.4 to {+65}Ni ground state. Systematics of J|p=7/2- in {+61}Co and {+63}Co. Shell model. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: S
level_comment:
J 3+ or 1+ from shell model; 3+ seems to be likely since no |b{+-} transition was observed to the ground state of {+66}Ni (1988Bo06); however, J|p=1+ is not ruled out 
T weighted average of 0.24 s 3 (1994Cz02), 0.23 s 2 (1985Bo49), 0.23 s 2 (1999So20), and 0.18 s 1 (2000Mu10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8-)
level_lifetime_unit: US
level_lifetime_info: ;ERR=GT
level_comment:
J$Expected |pf7/2|ng9/2 quasiparticle configuration (1998Gr14). 
T From |g|g coin, |g-particle coin (1998Gr14). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: S
level_comment:
T From 1999We07. Others: 0.42 s {I7}(1985Bo49), 0.44 s {I8} (1999So20), 0.31 s {I2}(1995AmZX), 0.436 s {I77}(1999Le67). 
J from shell model systematics 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$ from correlation technique as quoted by 2008Pa33 from their companion publication: Pauwels et al, Nucl Instr & Methods B 266, 4600 (2008). 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$ from correlation technique (2008Pa33), see details in a companion publication by Pauwels et al, Nucl Instr & Methods B 266, 4600 (2008). This half-life is the weighted average of 503 ms {I42} and 483 ms {I56} determined by two different methods 
$ Probable configuration=|p1/2[321], intruder state %|b{+-}<20 (2008Pa33)$ %IT>80 
$ Upper limit of |b decay from this isomer is deduced by 2008Pa33 from correlation techniques 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
$From the |b-decay curve, the {+68}Fe decay populates the long-lived isomer of {+68}Co. 
J$log {Ift}=4.9 from {+68}Fe |b{+-} decay (J|p=0+) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
J$from systematics 
T$ weighted average of 229 ms {I24} (2011Da08), 232 ms {I17} (2005GaZR), 0.22 s {I2} (1999Mu17), 190 ms {I40} (1999So20), 0.27 s {I5}(1991Be33) 
%B-N$0.88 estimated from theory (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$Only the |b{+-} decay has been observed 
J$assignment from 2015Li33 based on possible |pf{-7/2}{+-1} configuration 
T$from |b(594|g)(implants) correlated decay curves (2015Li33). Authors state that if |g coincidence requirement is removed, half-life is 206 ms {I20}. Other: 150 ms {I20} from growth and decay curve for 594|g populated in {+69}Fe decay (2015Li33). In Figure 3d, authors state that it was not possible to fit the decay curves with a single half-life and a constant background. They postulate another isomer of longer half-life of 750 ms {I250} 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1/2-)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M
level_comment:
$Only the |b{+-} decay has been observed 
J$from comparison with similar isomers in {+65}Co and {+67}Co, and from possible proton-intruder state as in {+65}Co and {+67}Co (2015Li33) 
T$from 2015Li33, using a composite decay curve for {+69}Fe and {+69}Co activities. See also comment for half-life of ground state 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
J$2020Ca08 give J|p from systematics 
$mass excess, |D=-50207 keV {I36} (2020Ca08) 
E$from difference in mass excess values (2020Ca08). 


level_energy_unit: KEV
level_spin_parity: (6-,7-)
level_lifetime_unit: MS
level_comment:
T$weighted average of 100 ms {I10} (2015Pr10), 108 ms {I7} (2011Da08), 121 ms {I8} (2003So21), 110 ms {I9} (2003Sa40), 120 ms {I30} (2000Mu10), 150 ms {I20} (1998Am04). Others: 135 ms {I+11-9} (2005NiZZ, preliminary result), 92 ms {I25} (1999Le67,1999So20 both same group as 2003So21). 
J$from systematics of neighboring Co nuclides (2000Mu10,2003GrZZ) and direct |b{+-} feeding of J|p=(5,6,7) and (6+) levels in {+70}Ni. Suggested configuration of |pf{-7/2}{+-1}|ng{-9/2}{++3} 
%B-N$theoretical calculations give %|b{+-}n=2.0 (2003Mo09). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (3+)
level_lifetime_unit: S
level_lifetime_info: ;ISO=M1
level_comment:
T$weighted average of 0.47 s {I5} (2015Pr10) and 0.50 s {I18} ( 2000Mu10). Also observed as delayed state by 2003Sa40 
J$from systematics of neighboring Co nuclides (2000Mu10). Suggested configuration of |pf{-7/2}{+-1}|np{-1/2}{+-1}|ng{-9/2}{++4} 


level_energy_unit: KEV
level_energy_info: ;OFF=Y;ERR=?
level_lifetime_unit: NS
level_comment:
T$from implant-|g(t) in Ni({+86}Kr,X|g) 
J$proposed as (4-) in Ni({+86}Kr,X|g). However, observation of a single 274|g following {+70}Fe |b{+-} decay (J|p=0+) suggests a low-spin assignment. 
E$based on nearly equal transition intensities of a 273|g and a 164|g, it is assumed that these transitions are emitted in cascade. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
T$from implant-|g(t) (2010Da06,1999DaZQ). 
E$based on the nearly equal transition intensities of the 273|g and 164|g, 1999DaZQ assume these are emitted in cascade. 
J$as proposed by 2010Da06,1999DaZQ. J|p assignment is not adopted, as there is a discrepancy with the results of {+70}Fe |b{+-} decay. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (1+,2+)
level_lifetime_unit: MS
level_comment:
J$as proposed in 2017Mo02 based on observed |b feedings to {+70}Ni 
T$from |b(t) (2017Mo02) 
E$from the Adopted Levels of {+70}Co in the ENSDF database (July 2016 update). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (6-,7-)
level_lifetime_unit: MS
level_comment:
T$measured by 2024Si12 from decay curve of |b-decay activity gated on 448.5|g. 
%B-N$measured by 2024Si12 from summing the |b feeding of pseudolevels levels that emit delayed neutrons 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (1+,2+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from 2017Mo02. Other: 650 ms {i150} measured by 2024Si12 from decay curve of |b-decay activity with a fixed high-spin half-life of 113 ms. 
%B-N$measured by 2024Si12 from summing the |b feeding of pseudolevels levels that emit delayed neutrons 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n |? 16 {I2} (2020MoZS). This communication also states %|b{+-}2n=1.4 {I3}, but Q(|b{+-}2n) is -533 {I470}, which forbids this decay mode. Other: <2.7 {I9} from estimate of intensity of 1259|g in {+70}Ni (2012Ra10). The observation of 1259|g ray in {+71}Co decay confirms existence of the delayed-neutron decay mode. Note that 2005Ma95 stated %|b{+-}n|>3 {I1}, which probably should have read |<3 {I1} 
$Theoretical T{-1/2}=33.3 ms, %|b{+-}n=4 (2019Mo01) 
$Theoretical T{-1/2}=179 ms, %|b{+-}n=7.0, 8.5 (2021Mi17) 
J$possible |pf{-7/2}{+-1} configuration based on systematics (2009St07, 2012Ra10) 
T$weighted average of 86 ms {I10} (2019Ly02, (implants)|g-correlated decay curve); 80 ms {I3} (2012Ra10, time distribution of |b-gated |g events); and 79 ms {I5} (2011Da08,2004Sa59,2002MaZN, time distribution of (implants)|b correlated events, where fitting procedure included five parameters: |b-detection efficiency, background rate, mother, daughter and granddaughter half-lives). Others: 97 ms {I2} (2003So21,2005GaZR); 210 ms {I40} (1998Am04,1997AmZZ). As discussed by 2004Sa59, the half-lives measured by 1998Am04 are systematically higher by a factor of two or three. The difference in measured half-lives (79 ms and 97 ms) in the two GANIL measurements may suggest existence of two activities populated in two different reactions. Even-A Co isotopes generally show isomerism, but no isomerism has yet been found in odd-A Co isotopes. In the absence of confirming evidence for the existence of an isomer in {+71}Co, evaluators adopt only one half-life. In an e-mail reply of March 7, 2007, author (L. Gaudefroy) of 2005GaZR mentioned that it was less likely that a mistake was made in their work since there was an overall consistency in the measured half-lives of other isotopes 


level_energy_unit: KEV
level_spin_parity: [6-,7-]
level_lifetime_unit: MS
level_comment:
T$weighted average of 59 ms {I2} (|b(t), 2005Ma59) and 62 ms {I3} (|g(t), 2003Sa40). Other: 90 ms {I20} (|b(t), 1998Am04). 
J$from shell model calculations (2003Sa40) 
$Preliminary value of %|b{+-}n|>6 {I2} (2005Ma95) 


level_energy_unit: KEV
level_spin_parity: [6-,7-]
level_lifetime_unit: MS
level_comment:
T$from |b|g-coin decay curve (2014Xu07). Other: 59.9 ms {I17} in {+72}Co Adopted Levels in ENSDF database 
J$from {+72}Co Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (6-,7-)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n|>6 {i2} from 2005Ma95 (Eur. Phys. J. A25, Supplement 1, 93); |b{+-}2n>0 from observation of |g rays in {+70}Ni from {+72}Co decay (2016Mo07). Both values are combined for the two activities 
T$measured by 2016Mo07 from decay curve of |b-decay activity gated on 454|g. This value can be compared with 52.8 ms {I16} (2014Xu07: Phys. Rev. Lett. 113, 032505) and 55 ms {I4} in 2014Ra20 (J. Phys. G41, 115104), where only the one activity in {+72}Co was reported 


level_energy_unit: KEV
level_energy_info: ;OFF=Y
level_spin_parity: (0+,1+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
$%|b{+-}n|>6 {i2} from 2005Ma95 (Eur. Phys. J. A25, Supplement 1, 93); |b{+-}2n>0 from observation of |g rays in {+70}Ni from {+72}Co decay (2016Mo07). Both values are combined for the two activities 
T$measured by 2016Mo07 from decay curve of |b-decay activity gated on 1680|g, 1689|g, 1732|g, 2023|g, 2538|g, 2650|g, 2885|g, 3040|g and 3383|g 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$%|b{+-}n: measured value is <22 {I8} (2012Ra10) based on absolute intensity of 1095|g in {+72}Ni from the beta-delayed neutron decay of {+73}Co; earlier value from this group was >9 {I4} (2005Ma95). Other measurement: %|b{+-}n<7.9 (2010Ho12). In a recent study carried out at RIBF-RIKEN by 2016Mo07, eight |g rays from the |b{+-}n decay of {+73}Co to {+72}Ni were detected in coincidence mode (see Fig. 4 in the paper) 
$Theoretical T{-1/2}=19.0 ms, %|b{+-}n=9, %|b{+-}2n=0 (2019Mo01). 
$Theoretical T{-1/2}=97.5 ms, %|b{+-}n=5.8, %|b{+-}2n=0.1 (2016Ma12). 
$The observed 40.7-ms activity is assumed to correspond to the ground state of {+73}Co. 
J$7/2- from systematic trend (2017Au03). Also |W{-proton}=7/2- in theoretical calculations (2019Mo01) 
T$weighted average of 40.4 ms {I13} (2014Xu07), 42 ms {I3} (2012Ra10), 41 ms {I4} (2011Da08,2004Sa59), and 41 ms {I6} (2010Ho12) 
$2014Xu07 (also 2014XuZZ) T{-1/2} measurement: |b|g-coin decay curve from time difference between implantation and correlated |b decays. 
$2012Ra10 T{-1/2} measurement: time distribution of all |b-gated |g events. Other values: 40 ms {I9} and 54 ms {I9} from |g decay curves for 239.2|g and 774.7|g, respectively 
$2011Da08, 2004Sa59 T{-1/2} measurement: time correlation between implantation and |b-ray events in the DSSSD. Fitting procedure included five parameters: |b-detection efficiency, background rate, mother, daughter and granddaughter half-lives 
$2010Ho12 T{-1/2} measurement: time sequence of decay type events correlated with the implanted nuclei of {+73}Co in Si detectors. The authors used method of maximum likelihood analysis which required, as input parameters, values of |b-detection efficiency, background, half-lives of daughter and granddaughter nuclei and experimental or theoretical values of %|b{+-}n of all nuclei involved 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
T$from |g(t) (2020Go10); weighted mean of several |g(t) measurements 
%B-N$estimated from intensity of 1095|g in {+72}Ni. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=23 ms, %|b{+-}n=6.4, %|b{+-}2n=1.5 (2003Mo09). 
$Theoretical T{-1/2}=71 ms, %|b{+-}n=4.4, %|b{+-}2n=1.3 (2016Ma12). 
T$weighted average of 30 ms {I3} (2005Ma59, 2005Ma95, |b and |b|g correlated with {+74}Co ions) and 31.6 ms {I15} (2014Xu07, |b-implants correlated decay curves). Other less precise measurements using |b-implant correlated decay curves: 34 ms {I+6-9} (2010Ho12) and 19 ms {I7} (2011Da08,2002MaZN). Weighted average of all the four values is 30.9 ms {I15} 
$|b{+-}n decay to {+73}Ni is indicated by the presence of a 240|g (belonging to {+73}Ni) in |b|g coin spectrum (2005Ma59). From the detailed analysis of |b(implant) decay curve, 2010Ho12 deduce %|b{+-}n=18 {I15}. Others: |>26 {I9} (2005Ma59, from |b|g data and decay scheme analysis), %|b{+-}n=14 {I11} (2014XuZZ, preliminary value) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$ from measurement of time sequence of decay type events correlated with the implanted nuclei (of {+75}Co) in Si detectors (2010Ho12). The authors used method of maximum likelihood analysis which required, as input parameters, values of |b-detection efficiency, background, half-lives of daughter and granddaughter nuclei and experimental or theoretical values of %|b{+-}n of all nuclei involved. 
J$7/2- proposed from systematics (2012Au07) and theory (1997Mo25) 
$Theoretical values: %|b{+-}n=6.9 (1997Mo25), 7.4, 8.0 (2002Pf04); %|b{+-}2n=0.5 (1997Mo25). Systematic %|b{+-}n=37.9 (2002Pf04) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from |b|g-coin decay curve (2014Xu07). Other: 30 ms {I11} in {+75}Co Adopted Levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=12.7 ms, %|b{+-}n=18, %|b{+-}2n=2 (2019Mo01). 
$Theoretical T{-1/2}=37.6 ms, %|b{+-}n=50.0, 70.1; %|b{+-}2n=1.6, 3.0 (2021Mi17). 
E,J$ground state with (1-) proposed by 2015So23 with possible configuration=|pf{-7/2}{+-1}~#|ng{-9/2}{+-1}. Note that in 2021Ko07 (1-) is proposed as an isomer at 100 keV {I100} and (8-) as the g.s. 1- or 8- from |W{-p}=7/2- and |W{-n}=9/2+ from theory (2019Mo01) 
T$from |b|g(t) (2015So23), in the inset of the upper panel of Fig. 3 in 2015So23, T{-1/2}=16 ms is shown from |b-decay time distribution gated on prompt 990|g. Other: 17.4 ms {I30} (preliminary value in 2014XuZZ) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (8-)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
E$Note that in 2021Ko07, (1-) is proposed as an isomer at 100 keV {I100} and (8-) as the g.s. 
J$from 2015So23, based on shell-model predictions, with possible configuration=|pf{-7/2}{+-1}~#|ng{-9/2}{+-1} 
T$from 2014Xu07, from |b|g-coin decay curve. Other: in the inset of the middle panel of Fig. 3 in 2015So23, T{-1/2}=22 ms is shown from |b-decay time distribution gated on delayed 355|g 
$Measured |s=8 pb (2010Oh02), systematic uncertainty|?50% 
$Since no events were observed for neighboring hydrogen-like peaks, the misidentification of {+76}Co is not likely (2010Oh02) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from 192|g(t) (2015So23) 
E,J$from 2015So23, based on shell-model predictions, with possible configuration=|pf{-7/2}{+-1}~#|np{-1/2}{+-1}. Other: 740 keV {I100} in 2021Ko07, based on (8-) as the g.s. and (1-) as the g.s. 
$This isomer decays to g.s. by 446.4|g-192.02|g cascade with a level sequence of (3+) -> (2-) -> (1-) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
E,J$from 2015So23, based on shell-model predictions, with possible configuration=|pf{-7/2}{+-1}~#|np{-1/2}{+-1} 
T$from |g(t) (2015So23) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Only the |b{+-} decay mode has been observed in 2014Xu07, thus 100% |b{+-} decay is assigned by inference. Beta-delayed neutron decays are expected 
$Theoretical T{-1/2}=10.8 ms, %|b{+-}n=55, %|b{+-}2n=2, %|b{+-}3n=0.0 (2019Mo01). 
$Theoretical T{-1/2}=26.9 ms, %|b{+-}n=76.9, %|b{+-}2n=5.3, %|b{+-}3n=0.2 (2016Ma12). 
E$the observed activity is assumed to be correspond to the ground state 
J$7/2- from systematic trend (2017Au03) and from |W{-p}=7/2- (theory, 2019Mo01) 
T$from 2014Xu07; measured from decay curve of time difference between implantations and correlated |b decays using maximum likelihood (MLH) method and including half-lives of parent, daughter, and grand-daughter nuclei together with |b-delayed neutron emission channels. 


level_energy_unit: KEV
level_comment:
$|b{+-} decay is the only decay mode possible, followed by delayed neutron decays through one- and two-neutron emissions, thus 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=5.9 ms, %|b{+-}n=68, %|b{+-}2n=14, %|b{+-}3n=0, %|b{+-}4n=0 (2019Mo01). 
$Theoretical T{-1/2}=20.6 ms, %|b{+-}n=63.4, 63.3; %|b{+-}2n=6.0, 8.1; %|b{+-}3n=0.024, 0.126, %|b{+-}4n=0 (2021Mi17), the two values are for different fission barriers. 
$Five events were assigned to {+78}Co by 2017Su15, which are assumed by the evaluators to correspond to the g.s. activity of {+78}Co 
$Probability of misidentification of {+78}Co<0.01% (2017Su15). 
$Measured production |s=2.5 fb {I+17-11} (2017Su15) 
J$3-,4- from |W{-p}=7/2-, |W{-n}=1/2+ (theory, 2019Mo01). 
T$half-life is not measured, but expected to be greater than few hundred ns from the flight time of fragments through the separator. Based on decreasing trend of half-lives as the neutron number increases in n-rich nuclei, evaluators estimate T{-1/2}<15 ms from literature half-lives of 13.0 ms for {+77}Co, 21.7 ms for {+76}Co, 30 ms for {+75}Co, and 31.6 ms for {+74}Co. Other: 11 ms from systematics (2021Ko07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2011Po09 from maximum-likelihood analysis for six events for which decay time could be measured. Two identified {+48}Ni nuclei were not observed to decay, a possible explanation is that their decay occurred within 70 |ms of implantation before the chamber reached full sensitivity. Based on the branching ratios deduced in this study partial half-life for the |b{++}p channel is 7.0 ms {I+66-51}, and for 2p channel is 3.0 ms {I+22-12} (2011Po09). Same half-life reported in 2014Po05. Others: 2.1 ms {I+21-7} from 2005Do20; >0.5 |ms (2000Bl01, estimated from tof). See 2006Ro09 for calculations of the partial T{-1/2} ({+48}Ni g.s.,0+ |) {+46}Fe g.s.,0+)'s for diproton and sequential 2p decay. 
$Decay modes from observation of two events decaying by |b{++}p decay and four by proton decay (2011Po09). 2005Do20 report one event with decay energy of 1.35 MeV {I2} with no |b coincident consistent with model predictions for 2p decay, which happens after 1.66 ms and is followed by charged-particle emission with an energy release of 4748 keV {I20} after 1.03 ms. 
$One-proton emission energetically forbidden (1997Or04, 1996Co14, 1991Br06). 
$Production |s=100 fb {I30} (2011Po09), 150 fb {I50} (2014Po05); 50 fb {I20} (2000Bl01) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
J$(7/2-) from systematics (2003Au02) 
T$from 2007Do17. Other: 12 ms {I+5-3} (2001Gi01. Assuming a possible contamination of 0 to 10% from {+48}Fe |b{++}p decay.) 
%B+P$assuming 969.5 {I5} |g is due to the 2+|)0+ decay in {+48}Fe. Other: >0 (2001Gi01. 3.7 MeV charged particle line observed.) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from 2007Do17, measured by time correlation of implantation events due to {+50}Ni and subsequent emission of protons. Other: 12 ms {I+3-2} (2003Ma34). Weighted average of two values of half-lives is 17.3 ms {I25} with a |h{+2}=5.5, whereas unweighted average is 15.3 ms {I32} 
$%|ep=86.7 {I39} is total delayed proton branch in 2007Do17 from time spectrum of events with energy >900 keV in the charged-particle spectrum, out of which 14% {I5} seems associated with |e2p branch, from the observed intensity of 1972 proton group in 2007Do17. Possible small contribution from delayed-|a is ignored. Other %|ep=70 {I20} (2003Ma34). 
$Production |s=0.061 nb {I+33-30} (1994Bl10) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
%ECP$Total proton branching ratio is from time spectrum of events with energy >900 keV in the charged-particle spectrum. Possible small contributions from delayed-|a and delayed-2p decays are ignored. 
%EC2P$With the total |b{++}p=87.2% {I8} measured by 2007Do17, the |b{++}2p/|b{++}1p ratio is less than 5% in agreement with calculation by 1991De26. 
T$By time correlation of implantation events due to {+51}Ni and subsequent emission of protons and |g rays (2007Do17). Other: >200 ns (tof, 1987Po04) 
J$7/2- from systematics in 2017Au03. Theoretical calculations in 1997Mo25 suggest 3/2-. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Other %|ep=31.4 {I15} (2007Do17: Nucl. Phys. A792, 18, GANIL work) 
T$from time correlations between each proton decay and all the {+52}Ni implants (2016Or03). Other: 40.8 ms {I2} (2007Do17, GANIL work; value also listed in {+52}Ni Adopted Levels dataset in the ENSDF database (July 2015 update)) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: MS
level_comment:
J$ IAS of 4390, (7/2-) in {+53}Co; mirror analog of g.s. 7/2- in {+53}Mn 
T$ from proton decay curve over 20 half-lives (2007Do17). Others: 56 ms {I8} (2013Su07,from proton decay curve over about 9 half-lives); <85 ms (1993Xu04), 45 ms {I15} (1976Vi02,1979ViZY, from proton decay curve for about four half-lives); 
%ECP$ from 2007Do17. Other: |?45% (1976Vi02) 
$ 2013Su07 report proton peaks at 1929 and 2399 keV. 2007Do17 report six proton groups at 1077, 1251, 1639, 1939, 2111, and 2399 keV. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
T$From simulated lineshape analysis to the experimental data determined by using a reduced |h{+2} at both 37{+|o} and 90{+|o} of SeGA rings. The uncertainty includes the statistical error (198 ps {I8}) and an overall systematic error of 4.6% from uncertainties due to ambiguities in the geometry of the setup (3%), |g-ray anisotropy effects (1.5%), assumptions in the background (3%) and effects due to the feeding of the 5/2- state from short-lived states (1%). 
$|s{-exp}|?12%. Shell Model predicts a very small cross section. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$From |b=0.416 {I6} determined by aligning 1718|g in both 37{+|o} and 90{+|o} SeGA rings (using Doppler-correction analysis). Authors stated that time for beam to traverse the target thickness was |?8 ps therefore the measured |b indicated the average point of decay was inside the target volume. 
$|s{-exp}|?5%. |s{-theory}=10% using Shell Model. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MS
level_comment:
T$from decay-time spectra fitted with exponential curves (2016Su10), same procedure as in authors' previous paper 2013Su07. This value can be compared with 56 ms {I8} in 2013Su07 and 55.2 ms {I7} in {+53}Ni Adopted Levels in the ENSDF database (June 2013 update), a value taken from 2007Do17 (Nucl. Phys. A792, 18). 2016Su10 quote 55.2 ms in decay-scheme Fig. 5. Compiler obtains weighted average of the three values as 55.3 ms {I7}, almost the same as that in 2007Do17 
J$From the Adopted Levels of {+53}Ni in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T From 2012MoZW. Others: 113 ms {I9} (2013Su07), 114 ms {I5} (2008Fu04), 103 ms {I9} (2002Lo13, 2002Bl17), 106 ms {I12} (1997Wo06, 1999Re06), and 143 ms {I23} (1995ReZY). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$T{-z}=-1 
T$measured by 2017Ku12 from ({+54}Ni implants)|b correlated decay curve. Others: 114.2 ms {I3} in 2015Mo01 (Phys. Rev. C91, 014301); 113 ms {I9} in 2013Su07 (Phys. Rev. C87, 024312); 114 ms {I5} in 2008Fu04 (Jour. Phys. G35, 014041); 103 ms {I9} in 2002Lo13 (Phys. Rev. C 66, 025803); 106 ms {I12} in 1999Re06 (Phys. Rev. C59, 2416). Value of 114.2 ms {I3} from 2012MoZW (AIP Conf. Proc. 1423, 23, same group as 2015Mo01) is listed in {+54}Ni Adopted Levels in the ENSDF database (June 2014 update) 
$Total number of {+54}Ni implanted ions=2.41|*10{+5} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$R=3.738 fm {I4} with {+58}Ni as reference isotope, R=3.737 fm {I3} with {+60}Ni as a reference isotope (2021Pi10) 
$|d<r{+2}>{+54,58}=-0.235 fm{+2} {I29}, |d<r{+2}>{+54,60}=3.737 fm{+2} {I3} (2021Pi10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_lifetime_unit: NS
level_comment:
T$from 158.6 ns {I29} from implant-p1(t) and 155.9 ns {I45} from implant-p2(t) (2021Gi18) 
%P$deduced from measured proton branches by 2021Gi18 combined with prior measurement of gamma-rays and Ep=1.20 MeV proton branch. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured differential rms charge radius |d<r{+2}>({+54}Ni,{+60}Ni)=-0.522 fm{+2} {I9} {I19} (2022So14), first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 
$Measured isotope shift |d|n({+54}Ni,{+60}Ni)=-1919.7 MHz {I79} (2022So14), uncertainty is combined: statistical and systematic. 
$Measured absolute rms charge radius=3.7366 fm {I13} {I31} (2022So14); first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MS
level_comment:
T$weighted average by Rajeval technique (RT) of 203 ms {I2} (2017Ku12, from ({+55}Ni implants)|b correlated decay curve, with total implants of 2.70|*10{+6} using LISE3 at GANIL); 196 ms {I5} (2002Lo13,2002Bl17, implants)|b correlated decay curve at GANIL); 204 ms {I3} (1999Re06,1997Wo06, |b decay curve using LISOL facility at Louvain-la-Neuve); 212.1 ms {I38} (1988HaZD,1988HaZB)); 208 ms {I5} (1984Ay01, IGISOL at the University of Jyvaskyla cyclotron facility); 189 ms {I5} (1977Ho25, |b{++} decay curve, at Aarhus University); 219 ms {I6} (1976EdZX). In this method, uncertainties for the following values were adjusted upwards: 5.6 ms in 1988HaZD, 9.4 ms in 1977Ho25, and 9.7 ms in 1976EdZX. Weighted average (and LWM weighted average) is 203.9 ms {I26}, but reduced |h{+2} is 3.9 as compared to critical |h{+2} of 2.1 at 95% confidence level. Weighted average by NRM is 204.3 ms {I24} with reduced |h{+2}=3.1. Unweighted average is 204.4 ms {I38}. Others: 155 ms {I10} (1994Ve09, at Louvain-la-Neuve, value is discrepant); <5 s (1973Di11). 
$2017RuZX superseded by 2017Ku12 
J$log| {Ift}=3.625 {I5} for decay of {+55}Ni g.s. to 7/2- g.s. in {+55}Co, deduced in the present evaluation; L(n)=3 in {+{+1}H}({+56}Ni,d); measured magnetic moment is in agreement with shell-model calculations for configuration=|nf{-7/2{+-1}; mirror analogy to 7/2-, g.s. of {+55}Co. 
MOMM1$|b-NMR method, negative sign is from theoretical considerations for g.s. configuration=|nf{-7/2{+-1} (2009Be22). 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_comment:
J$level is Coulomb excited from 7/2- g.s. 
$B(E2)|^=0.0251 {I69} for J|p(2879)=11/2- from Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$3186 and 3183 seem to be different levels from two different J|p values. 
J$L(n)=0 in {+{+1}H}({+56}Ni,d) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$interpreted by 2013Tr09 as split IAS of (3/2-) g.s. of {+55}Cu, the other at 4599 keV, and also interpreted as mirror state of 4721, 3/2- state in {+55}Co 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$interpreted by 2013Tr09 as split IAS of (3/2-) g.s. of {+55}Cu, the other at 4579 keV, and also interpreted as mirror state of 4748, 3/2- state in {+55}Co 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$1997Ru07 point out that a tentative ground state transition (2796 keV) in the yrast decay reported by 1996Ca48 does not correspond to the 2882 transition observed in their work. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Coulomb displacement energy=9477 {I10} (1977Mu03) 
$Measured d|s/d|W=1.20 |mb/sr {I12} at 8|' (1975Mu09); 1.81 |mb/sr {I20} at 9|' (1972KaYT) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$3/2- in 2013Tr09 
E,J$proton-bound IAS of 3/2-. {+55}Cu g.s., and mirror state of 4721, 3/2- state in {+55}Co 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$3/2- in 2013Tr09 
E,J$proton-bound IAS of 3/2-. {+55}Cu g.s., and mirror state of 4748, 3/2- state in {+55}Co 


level_energy_unit: KEV
level_energy_info: ;ERR=LT;ERR=?
level_comment:
$Measured Gamow-Teller strength=5.3 {I5}(stat) {I+25-15}(syst) for 0-15 MeV excitation energy range in {+55}Ni (2012Sa37). This value is compared by authors to 6.8 and 6.2 from shell-model calculations using GXPF1J and KB3G interactions, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$Configuration=2p{-3/2}. 
$2014Sa46 state that small spectroscopic factor for this state, reproduced by the theoretical calculations, indicates 3-qp configuration of |n1f7/2){+-2}~#|n2p{-3/2}, and implies non-negligible 2p{-3/2} components in the {+56}Ni ground state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_uncertain: ?
level_comment:
E,J$from the Adopted Levels 
E$for |q<9|', excess strength is observed at E>3.5 MeV which the authors assign to a previously observed (3/2+), 3.75-MeV level. 


level_energy_unit: KEV
level_spin_parity: (9/2-&11/2-)
level_comment:
$Measured parallel momentum distribution is displayed in Fig. 4 of 2019Sp02, but no L-transfer or J|p is deduced. 
$Possible doublet of multiplet with configuration of 1f{-7/2}{+-1}~#(first 2+ state in {+56}Ni) 
$Measured partial |s=1.42 mb {I10} (3.7% {I3}) (2019Sp02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$Measured partial |s=1.49 mb {I7} (read from Fig. 3 in 2019Sp02) 
L$from comparison of experimental momentum distribution with predictions of the eikonal theory 
J$proposed by 2019Sp02 based on measured momentum distribution. 


level_energy_unit: KEV
level_spin_parity: (9/2-,11/2-)
level_comment:
$Proposed configuration=|nf{-7/2}{+-1}~#first 2+ state of {+56}Ni 
$Measured integrated Coulomb excitation cross section=57 mb {I16} 
$B(E2)|^=0.0251 {I69} for J|p(2879)=11/2-, and 0.0257 {I+95-73} for J|p(2879)=9/2- obtained by comparing the measured cross section section with the Alder-Winther theory of relativistic Coulomb excitation, assuming 92% of the excitation cross section is of type E2 if J|p(2879)=9/2-, as <4.9 mb excitation cross section for pure M1 was calculated using the recommended upper limits on M1 transition rates (2004Yu11). For deexcitation of the level, a maximum contribution of 29% from E2 deexcitation transitions was calculated by the authors for J|p(2879)=9/2- 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$from {+55}Ni Adopted Levels in the ENSDF database (April 2022 update) 
MOMM1$from measured hyperfine structure parameters, based on |m({+61}Ni g.s.)=-0.74965 {I5} taken from 2014StZZ compilation in INDC(Nuclear Data Sheets)-0658 (2014); same |m value in 2019StZV evaluation in INDC(Nuclear Data Sheets)-0794 (2019). 
$Measured differential rms charge radius |d<r{+2}>({+55}Ni,{+60}Ni)=-0.607 fm{+2} {I23} {I9} (2022So14), first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 
$Measured isotope shift |d|n({+55}Ni,{+60}Ni)=-1426.9 MHz {I191} (2022So14), uncertainty is combined: statistical and systematic. 
$Measured absolute rms charge radius=3.7252 fm {I32} {I21} (2022So14); first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: D
level_comment:
T from 1992Da15. Others: 6.10 d {I2} (1963We06), 6.4 d {I1} (1952Sh30), 6.0 d {I5} (1952Wo15), 5.9 d {I1} (1990Su13), and 5.8 d {I6} (1961Mo10). 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$J|p=(3+) and T=0,1 quoted in 2001Bo54 have been revised by the authors. The revised note further suggests that J|p=(4+) and T=0 are favored by shell-model calculations. L(p,t)=4. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
$J|p=(3,4,5)(+) and T=0,1 quoted in 2001Bo54 have been revised by the authors. The revised assignment is based on a comparison of energy differences of isobaric analog states in {+56}Ni and {+56}Cu. 


level_energy_unit: KEV
level_spin_parity: 7
level_comment:
$ This level decays by protons to 7/2-, g.s. in {+55}Co. E(p)(lab)=2540 {I30}, observed in (proton)(summed |g) coin spectrum 


level_energy_unit: KEV
level_spin_parity: (3+,4+,5+)
level_comment:
$J|p=(3+) and T=0,1 quoted in 2001Bo54 have been revised by the authors. The revised note further suggests that J|p=(4+) and T=0 are favored by shell-model calculations. 


level_energy_unit: KEV
level_spin_parity: (2+,3+,4+,5+)
level_comment:
J$ 6+ assignment is not expected to be populated in one-neutron knockout reaction due to angular momentum considerations. 


level_energy_unit: KEV
level_comment:
E$exotic state consisting of many |a particles. Energy extrapolated from observed 7|a emission channel and method of distributed m|a ensembles. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured differential rms charge radius |d<r{+2}>({+56}Ni,{+60}Ni)=-0.626 fm{+2} {I2} {I16} (2022So14), first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 
$Measured isotope shift |d|n({+56}Ni,{+60}Ni)=-1002.7 MHz {I38} (2022So14), uncertainty is combined: statistical and systematic. 
$Measured absolute rms charge radius=3.7226 fm {I3} {I27} (2022So14); first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: H
level_comment:
J J=3/2 from |b|g(CP) (1968At03); |p=- from L(n)=1 in pickup. 
T weighted average of 35.54 h {i5} (1986Di02) and 35.65 h {i5} (1982Gr10). Other: 36.16 h {i11} (1974Ro18; NaI well, chem; >7 T{-1/2}'s). See also 1978LeZA. See 1987De19 for measurement of difference in |e decay rate of {+57}Ni in different chemical compounds. 
MOMM1 from nuclear magnetic resonance on oriented nuclei 
MOME2=-2.32 IF EFFECTIVE CHARGE=0.8 (1975Sa07,THEORY) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
6000 {i20}, 3/2, state in ({+3}He,|a|g) may correspond to this or the 6029 state. However, the evaluator has assigned the two gammas seen in ({+3}He,|a|g) to this level 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J from CRC analysis in ({+3}He,|a). Good agreement between d|s/d|W and calculations. From E(level) and J|p, this state may be the analog of the IAS({+57}Co,1224,9/2-) but there are problems. See ({+3}He,|a) for discussion. 


level_energy_unit: KEV
level_comment:
The 12.1-, 13.1-, and 13.3 MeV states may be the T=1/2 states of 12.4 MeV, 3/2-; 13.16 MeV, 5/2-; and 13.48 MeV, 1/2-, suggested as the principal states fed by the {+58}Ni 16.4 MeV, T(<)=1, GDR (1973RoYN). See (|g,n), (e,e'n) res 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J 7/2 from |g(|q) and excitation function (1989Sa47); |p=- from E2 to 3/2- 
T weighted av of 54 fs {i9} (1971Be33) and 42 fs {i7} (1970Go18). Other: 90 fs {i50} (1989Sa47) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J 3/2,5/2 from |g(|q) (1971Be33); (5/2,7/2) from |g(|q) and excitation function (1989Sa47) 
T unweighted av of 15 fs {i8} (1971Be33) and 8 fs {i4} (1972Go02). Other: 110 fs {i30} (1989Sa47) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)-
level_comment:
The 3.71- and 3.85-MeV states are the most strongly populated in ({+6}Li,t); see 1978Wo01 for a discussion of these levels. No J|p assignment to this level by 1978Wo01. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
J (3/2,5/2) proposed on the basis of the strong population of this level in ({+6}Li,t) and the weak population in neutron pickup (1978Wo01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T from 1989Sa47; a comparison of these authors' T{-1/2}(3007) with the adopted value suggests that a side-feeding lifetime larger than that assumed by the authors is required. 
J 11/2 from |g(|q) and excitation function (1989Sa47); |p=- from E2 to 7/2- 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
T from 1989Sa47; see the comment on the 3864 level. 
J 15/2 from |g(|q) and excitation function (1989Sa47); |p=- from E2 to 11/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
Definite J dependence observed in |s(|q) (1973Ed01); but very little J dependence seen by 1974Oh02 at their higher bombarding energy. 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_comment:
J CRC analysis. Non-pickup |s(|q). ({+3}He,{+3}He,|a') path not possible for (({+58}Ni 2-)(|n 1f7/2){+-1}) or (({+58}Ni 3-)(|n 1f7/2){+-1}); therefore, the influence of other hole configurations is expected to be larger than for higher-lying states. 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J 7/2- from analyzing power data (1980FuZV); J|p=7/2- assumed by 1979Fo09 to extract the spectroscopic factors. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J CRC analysis. Non-pickup |s(|q) reproduced well by assuming two-step excitation of the members of the (({+58}Ni 3-)(|n 2p3/2){+-1})9/2+ or (({+58}Ni 3-)(|n 1f7/2){+-1})9/2+ multiplet. Also compared L=4 and L=5 DWBA; L=5 gave a reasonable fit but was considered unlikely since 1h11/2 and 1h9/2 are expected to be very weakly populated in {+58}Ni g.s. 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
J CRC analysis. Non-pickup |s(|q) reproduced well assuming two-step excitation of (({+58}Ni 2+)(|n 1f7/2-){+-1}); equally well reproduced by assuming direct L=5 pickup. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
J CRC analysis. Non-pickup |s(|q) 
Good agreement between |s(|q) and CRC. From E(level) and J{+|p}, this state may be tentatively assigned as IAS({+57}Co,1224,9/2-); however, from the weak coupling model the {+57}Co 1218 state should be (({+58}Ni 2+)(|p 1f7/2){+-1}). |s(|q), here, implies (({+58}Ni 2+)(|n 1f5/2){+-1}). 1979Fo09 cannot explain this. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J 7/2 from J-dependence of d|s/d|W; however, the effect of excitation energy on this dependence could not be determined (1973Ed01). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
E the value 8225 in table1 of 1979Fo09 is assumed by the evaluator to be a misprint (see authors' spectrum) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E,L from 1974Oh02. Assumed by evaluator to be the L(n)=0 member of the 8530 L=0(+3) multiplet observed by 1979Fo09. FWHM|?70 keV compared with 20 keV for 1979Fo09, but the higher bombarding energy of 1974Oh02 apparently enhances the L=0 component. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E this level corresponds to peak 88 in 1979Fo09 with an energy of 8745; the evaluator feels this is a misprint and using Fig.1 has estimated the energy of this peak to be about 8800 and changed the energy to 8795 {i10}. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J J=7/2 from |a|g(|q). L(n)=3 from pickup work 
Clear evidence of the effect of the deuteron d-state on polarization of this state in d|g(|q) (1981Oh02; E=30 MeV. Si, d; NaI, |g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J (7/2) from |a|g(|q); assignment based partially on isobaric analog arguments. However, existence of branch to 780 level would violate the argument. 


level_energy_unit: KEV
level_spin_parity: (+)
level_comment:
J |<1/2,3/2 from |a|g(|q)(5560|g). J|=5/2 from |a|g(|q)(4450|g). This level may correspond to either 5546 {i6} or 5561 {i6} levels, both with J|p=(+). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J 3/2 from |a|g(|q)(4890|g,6000|g). This level may correspond to either J|p(5980 {i8})=(3/2)+ or J|p(6027 {i10})=3/2+,5/2+ in adopted levels 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
T$>7.0|*10{+20} y for decay by double |e|b{++} channel to the 0+ g.s. of {+58}Fe, and >4.0|*10{+20} y for decay by the same mode to the 2+, 811-keV level of {+58}Fe (1993Va19). Others: 1984No09, 1982Be20 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$ <r{+2}>{+1/2}=3.7748 fm {I14} (2004An14 evaluation) 
J$E2 |g to 0+ 
T$ different averaging methods were employed to 20 independent values given in header comments above but minimum uncertainty was assigned as 5%, which required increasing the uncertainty by a factor of |?2 to values in 1970Le17 and 1971ChZF. Average values of |t in ps obtained are: 0.95 {I3} by weighted average, normalized |h{+2}=2.0; 0.95 {I9} by limitation of statistical weights method (the uncertainties is increased to overlap the most precise value of 0.86 {I4}); 0.931 {I21} by normalized residuals method (NRM), normalized |h{+2}=1.2; 0.926 {I21} by Rajeval's technique, normalized |h{+2}=1.0. The evaluators adopt 0.94 {I3} as in 2008Or02; this value overlaps all the averaging methods used. 2001Ra27 evaluation (which did not include 2008Or02, 2004Yu10 and 2001Ke08) lists |t=0.904 ps {I26}. 
MOMM1$transient field integral perturbed angular correlation (2001Ke02). Other: -0.12 {I24} (1978Ha13,1989Ra17) 
MOME2$reorientation in Coulomb excitation (1974Le13,1970Le17). See also 2005St24 compilation 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from DSA in (p,p'|g). T{-1/2}=57 fs {I+25-13} from B(E2) in (e,e') is in disagreement 
J$L(|a,|a')=2 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$from |g|g(t) in {+58}Cu decay (1970Ra34). Other: 2.01 ns 7 in (p,p'|g) (1971St02) is in disagreement. Value from decay work is preferred due to cleaner |g-ray spectra such studies than in reaction data 
J$E0 transition to g.s. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=2 
T$unweighted average of 75 fs {I7} (2001Ke08, Coulomb excitation), 40 fs {I6} from (p,p'|g), 47 fs {I+13-9} from (|g,|g'), 66 fs {I6} from (e,e'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=2 
T$unweighted average of 53 fs {I8} (2001Ke08, Coulomb excitation), 30 fs {I4} from (|g,|g'), 25 fs {I4} from (p,p'|g), 44 fs {I21} from (n,n'|g), 33 fs {I3} from (e,e') 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=2 
T$unweighted average of 13 fs {I+10-5} from (|g,|g'), 34 fs {I+8-6} from (e,e'), and 23 fs {I3} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,p')=2 
T$unweighted average of 65 fs {I10} from (p,p'|g), 0.14 ps {I+9-4} from (e,e'), 0.10 ps {I+16-4} from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$ broad peak, from energy matching it could correspond to 4295 level, but J|p's are different 
J L({+3}He,n)=2 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
T$weighted average of 19 fs {I8} from (p,p'|g), and 24 fs {I8} from (n,n'|g) 
$B(E3)(|^)=0.0176 {I16} (2002Ki06 evaluation, adopted from (e,e')) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J L(|a,|a')=4 
E weighted average of 4750 {I5} (e,e'), 4750 {I7} (p,t), 4750 {I8} (|a,|a'), 4755 {I5} (p,p') 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$in (e,e'), level is at 5909 {I8} with J=2 in one study and 5903 {I15} in another with J=1, with assumed natural-parity states. It is possible that it is doublet in (e,e') representing 1+ and 2+ levels 


level_energy_unit: KEV
level_spin_parity: 1(+)
level_lifetime_unit: FS
level_comment:
J from analysis of |s(|q) in (p,p'), J=1 from (|g,|g') 
$ Configuration=|n(p{-3/2}p{-1/2}) ((p,p'),1986Ho15) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$ 1+,(2-) suggested in (e,e') and (1+) in (p,p') are in disagreement, if the levels in these two reactions are the same as in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$possible IAS of 1050,1+ in {+58}Co 
T$from (|g,|g') for J=1 
$ Configuration=|n(p{-3/2}p{-1/2}) ((p,p'),1986Ho15) 


level_energy_unit: KEV
level_spin_parity: (12+)
level_comment:
$ E(p)(c.m.)=1.83 MeV {I5} (2009Jo03) 
$Prompt p decay populates 2524, 13/2- level in {+57}Co which deexcites through 834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: (13-)
level_comment:
$ E(p)(c.m.)=2.15 MeV {I5} (2009Jo03) 
$Prompt p decay populates 4814, 17/2- level in {+57}Co which deexcites through 2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (13-)
level_comment:
$ E(p)(c.m.)|?2.35 MeV (2009Jo03). 
$Prompt p decay populates 4814, 17/2- level in {+57}Co which deexcites through 2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: (14-)
level_comment:
J$ from 2005Ru06, decays by protons to 5918, 19/2- level in {+57}Co; the decay mode not shown in 2009Jo03 


level_energy_unit: KEV
level_spin_parity: (14-)
level_comment:
$ E(p)(c.m.)=2.56 MeV {I5} (2009Jo03) 
$Prompt p decay populates 5918, 19/2- level in {+57}Co which deexcites through 1104-2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: (14-)
level_comment:
$ E(p)(c.m.)=2.61 MeV {I12} (2009Jo03) 
$Prompt p decay populates 5918, 19/2- level in {+57}Co which deexcites through 1104-2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: (14-)
level_comment:
$ E(p)(c.m.)=2.59 MeV {I8} (2009Jo03) 
$Prompt p decay populates 5918, 19/2- level in {+57}Co which deexcites through 1104-2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: (15-)
level_lifetime_unit: PS
level_comment:
T$from estimated T{-1/2}=7-28 ps (2001Ru03) from average Q(transition) in the band=2.4 {I3}, assuming that 1364|g and 1385|g are part of the continuation of the band and that Q(transition) does not change at lower spins. 
$ E(p)(c.m.)=1.62 MeV {I6}, E(|a)(c.m.)=6.90 MeV {I6} (2009Jo03) 
$Prompt p decay populates 6976, 21/2- level in {+57}Co which deexcites through 1058-1104-2290-834-466-1224 cascade to {+57}Co g.s. 
$Prompt |a decay populates 2949, 6+ level in {+54}Fe which deexcites through 411(6+ to 4+)-1130(4+ to 2+)-1408(2+ to g.s.) cascade 


level_energy_unit: KEV
level_spin_parity: (15-)
level_comment:
$ E(p)(c.m.)=2.35 MeV {I6} (2009Jo03) 
$Prompt p decay populates 6976, 21/2- level in {+57}Co which deexcites through 1058-1104-2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: (15-)
level_comment:
$ E(p)(c.m.)=2.43 MeV {I4}, E(|a)(c.m.)=7.71 MeV {I8} (2009Jo03). 
$Prompt p decay populates 6976, 21/2- level in {+57}Co which deexcites through 1058-1104-2290-834-466-1224 cascade to {+57}Co g.s. 
$Prompt |a decay populates 2949, 6+ level in {+54}Fe which deexcites through 411(6+ to 4+)-1130(4+ to 2+)-1408(2+ to g.s.) cascade 


level_energy_unit: KEV
level_spin_parity: (15-)
level_comment:
$ E(p)(c.m.)=2.47 MeV {I7} (2009Jo03) 
$Prompt p decay populates 6976, 21/2- level in {+57}Co which deexcites through 1058-1104-2290-834-466-1224 cascade to {+57}Co g.s. 


level_energy_unit: KEV
level_spin_parity: 15-
level_lifetime_unit: PS
level_comment:
T$from estimated T{-1/2}=7-28 ps (2001Ru03) from average Q(transition) in the band=2.4 {I3}, assuming that 1364|g and 1385|g are part of the continuation of the band and that Q(transition) does not change at lower spins. 
$ E(p)(c.m.)=1.62 MeV {I6}, E(|a)(c.m.)=6.90 MeV {I6} (2009Jo03) 
$Prompt p decay populates 6976, 21/2- level in {+57}Co which deexcites through 1058-1104-2290-834-466-1224 cascade to {+57}Co g.s. 
$Prompt |a decay populates 2949, 6+ level in {+54}Fe which deexcites through 411(6+ to 4+)-1130(4+ to 2+)-1408(2+ to g.s.) cascade 
$A 1432|g proposed in 2005Ru06 is not confirmed in 2009Jo03 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
E$level populated by E(p)=1916- and 1949-keV proton branches from 7792,17/2+ and 7825,17/2+ levels in {+59}Cu, respectively 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_comment:
E$level populated by E(p)=1897- and 2019-keV proton branches from 11917,25/2+ and 12039,25/2+ levels in {+59}Cu, respectively 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$this level is questionable and omitted in adopted levels due to the reassignment of 627|g from 9346, 10- level in high-spin study of 2009Jo03 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7
level_uncertain: ?
level_comment:
E$this level is questionable and omitted in adopted levels due to the reassignment of 537|g from 6604,8+ level in recent high-spin studies 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.70 ps 4 from weighted averaged |G=0.00065 eV {I4} from the following measurements: 0.00074 eV {I10} (1981Ca10), 0.000613 eV {I43} (1972ArZD), 0.00067 {I6} (1970Me18), 0.00106 {I35} (1964Bo22) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: EV
level_comment:
T$from 1970Me18. Other: |G{-0}=0.0015 eV {I4} (2000Ba63), from which |G{-0}{+2}/|G=0.00060 eV {I16} using adopted |G{-0}/|G=0.402 {I14}, which is in disagreement with value from 1970Me18. It appears that in this case value listed as |G{-0} in 2000Ba63 actually corresponds to |G{-0}{+2}/|G 
$T{-1/2}=47 fs {I+13-9} from average |G{-0}{+2}/|G=0.00156 eV {I34} and |G{-0}/|G=0.402 {I14} from adopted gammas. 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.0056 eV {I7} deduced from |G{-0}=0.012 eV {I3} and |G{-0}/|G=0.47 {I10} in 2000Ba63 compared with |G{-0}{+2}/|G=0.0053 eV {I8} from 1970Me18, average value=0.0055 eV {I7}. Note that Uncertainty of 0.10 for |G{-0}/|G is from table III of 2000Ba63, 0.01 in authors; table IV seems a misprint; the former seems more realistic in view of weak population of this level. Also uncertainty for |G{-0} is from table III, it is 0.002 in table IV. 
$T{-1/2}=30 fs {I4} from |G{-0}{+2}/|G=0.0055 eV {I7} and adopted |G{-0}/|G=0.598 {I11}. 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
E$ this level is assumed to be the same as a nearby level populated in {+58}Cu decay, (n,n'|g) and (p,p'g). The measured branching |G{-0}/|G=0.24 {I3} in 2000Ba63 is in severe disagreement with 0.63 {I3} in adopted gammas. It seems that the branching in 2000Ba63 is in error, it would be in better agreement if 0.24 refers to branching for |g ray to the excited state. 
T$from |G{-0}{+2}/|G=0.0046 eV {I8} (1970Me18) and adopted |G{-0}/|G=0.63 {I3}. Other: 0.033 eV {I8} (2000Ba63) 
$T{-1/2}=39 fs {I7} from |G{-0}{+2}/|G=0.0046 eV {I8} and adopted |G{-0}/|G=0.63 {I3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$from 1970Me18, not reported by 2000Ba63 
$T{-1/2}=13 fs {I+10-5} for |G{-0}/|G=0.24 {I2}, |G{-0}{+2}/|G=0.0021 eV {i9} (1970Me18) 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
T$from |G{-0}{+2}/|G=0.0010 eV {i6} (1970Me18) and adopted |G{-0}/|G=0.465 {I22}. Other: 0.027 eV {I2} (2000Ba63) with feeding effects 
$T{-1/2}=0.10 ps {I+16-4} for J=2, from |G{-0}{+2}/|G=0.0010 eV {i6} (1970Me18) and adopted |G{-0}/|G=0.465 {I22} 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.352 eV {I11} deduced from |G{-0}=0.435 eV {I22} and |G{-0}/|G=0.81 {I3} in 2000Ba63 
T$uncertainty of 0.012 in 2000Ba63 increased to 0.022 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.85 fs {I5} from |G{-0} and |G{-0}/|G=0.81 {I3} of 2000Ba63; ; 1.4 fs {I+8-4} for |G{-0}=0.33 eV {i12}, |G{-0}/|G=1 (1981Ac02) 
$Note that |G{-0}{+2}/|G=0.173 eV {i20} (1998Is13) is in disagreement with values from 1981Ac02 and 2000Ba63 by a factor of |?2 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.83 fs {I3} from |G{-0} of 2000Ba63; 0.67 fs {I+41-18} for |G{-0}=0.69 eV {i26}, |G{-0}/|G=1 (1981Ac02) 
$B(E1)(|^)=4.55|*10{+-5} {I14} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.72 fs {I3} for |G{-0} from 2000Ba63; 0.94 fs {I+65-27} for |G{-0}=0.49 eV {i20} (1981Ac02) 
$B(M1)(|^)=0.358 {I13} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.24 eV {I7} deduced from |G{-0}=0.34 eV {I16} and |G{-0}/|G=0.69 {I25} in 2000Ba63 
T$uncertainty of 0.07 in 2000Ba63 increased to 0.16 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.9 fs {I5} 
$|G{-0}/|G=0.69 {i25} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.127 fs {I2} for |G{-0} from 2000Ba63; 0.15 fs {I+3-2} for |G{-0}=3.0 eV {i5} 
$B(E1)(|^)=18.5|*10{+-5} {I3} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.62 eV {I8} deduced from |G{-0}=0.84 eV {I16} and |G{-0}/|G=0.74 {I11} in 2000Ba63 
T$uncertainty of 0.08 in 2000Ba63 increased to 0.16 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.40 fs {I8} 
$ |G{-0}/|G=0.74 {I11}, B(E1)(|^)=4.1|*10{+-5} {I4} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.223 fs {I11} for |G{-0} from 2000Ba63; T{-1/2}=0.40 fs {I+21-11} for |G{-0}=1.2 eV {i4} (1981Ac02). 
$B(M1)(|^)=0.82 {I4} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.58 fs {I6} for |G{-0} from 2000Ba63; T{-1/2}=0.46 fs {I+30-13} for |G{-0}=1.0 eV {i4} (1981Ac02) 
$B(E1)(|^)=2.9|*10{+-5} {I3} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.71 eV {I5} deduced from |G{-0}=0.98 eV {I11} and |G{-0}/|G=0.72 {I7} in 2000Ba63 
T$uncertainty of 0.06 in 2000Ba63 increased to 0.11 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.33 fs {I5} 
$|G{-0}/|G=0.72 {i7} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.37 fs {I4} for |G{-0} from 2000Ba63; T{-1/2}=0.36 fs {I+22-10} for |G{-0}=1.3 eV {i5} (1981Ac02) 
$B(E1)(|^)=4.3|*10{+-5} {I4} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=1.31 eV {I8} deduced from |G{-0}=2.25 eV {I24} and |G{-0}/|G=0.58 {I5} in 2000Ba63 
T$uncertainty of 0.15 in 2000Ba63 increased to 0.024 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.118 fs {I13} 
$|G{-0}/|G=0.58 {i5}, B(E1)(|^)=7.5|*10{+-5} {I5} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$T{-1/2}=0.335 fs {I20} for |G{-0} from 2000Ba63; 0.30 fs {I+20-8} for |G{-0}=1.5 eV {i6} (1981Ac02) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.45 eV {I5} deduced from |G{-0}=1.19 eV {I23} and |G{-0}/|G=0.38 {I6} in 2000Ba63 
T$uncertainty of 0.12 in 2000Ba63 increased to 0.23 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.15 fs {I3} 
$|G{-0}/|G=0.38 {i6} (2000Ba63), 7595.9|g not included 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.54 eV {I10} deduced from |G{-0}=0.81 eV {I26} and |G{-0}/|G=0.67 {I18} in 2000Ba63 
T$uncertainty of 0.17 in 2000Ba63 increased to 0.26 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.38 fs {I13} for |G{-0} and |G{-0}/|G from 2000Ba63; 0.24 fs {I+13-6} for |G{-0}=1.9 eV {i7}, |G{-0}/|G=1 (1981Ac02) 
$|G{-0}/|G=0.67 {i18} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: EV
level_comment:
$|G{-0}{+2}/|G=0.74 eV {I7} deduced from |G{-0}=1.76 eV {I26} and |G{-0}/|G=0.42 {I5} in 2000Ba63 
T$uncertainty of 0.13 in 2000Ba63 increased to 0.26 using uncertainties in |G{-0}/|G and in cross section as in 2000Ba63 
$T{-1/2}=0.109 fs {I16} 
$B(E1)(|^)=5.5|*10{+-5} {I4} (2000Ba63) 


level_energy_unit: KEV
level_spin_parity: 1,2
level_comment:
E$from 1981Ac02. This level is not reported by 2000Ba63, too high an energy to be detected near the end-point energy 
$T{-1/2}=0.26 fs {I+27-10} for J=1 and |G{-0}=1.8 eV {I9}, 0.49 fs +0.53-17 for J=2 and |G{-0}=0.9 eV {I4}; in both cases |G{-0}/|G=1 assumed (1981Ac02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$B(E2): average of 0.059 {I4} (1983Kl09), 0.055 {I3} (1969Af01), 0.0657 {I11} (1967Du07); all uncertainties are statistical. 1967Du07 state a systematic uncertainty of 15%. Other: 0.098 {I13} (1961Cr01) 
$ d|s/d|W=59 nb/sr {I15} (1976Li23) 


level_energy_unit: KEV
level_spin_parity: 2,1
level_comment:
E$ 5903 (1983Kl09) and 5909 (1987Me16) are considered as the same level. It is possible that the level in (e,e') is a doublet corresponding to a 1+ level in (|g,|g') and 2+ in (p,p') 
J$ 2 from 1987Me16, tentative 1(-) from E1 assignment in 1983Kl09 with B(E1)=0.0068 {I4} 
$ d|s/d|W=5.4 nb/sr {I6} (1976Li23) for 5909+5934 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$a 6420 {I15} level in 1983Kl09 assigned 3(-) with B(E3)(|^)=0.00129 {I18} is possibly the same as 6417 {I8} in 1987Me16 
$ d|s/d|W=4.5 nb/sr {I6} (1976Li23) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$1983Kl09 suggest 4(+) for a 7100 level 
$ d|s/d|W=9.3 nb/sr {I8} (1976Li23) for 7109+7200+7209+7255 
B(E4)=0.00097 {I9} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$a 7200 {I15} level in 1983Kl09 assigned 4+ with B(E4)(|^)=0.00423 {I25} is possibly the same as 7209 {I8} in 1987Me16 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$ possible IAS of 1729,1+ in {+58}Co 
$ d|s/d|W=8.3 nb/sr {I10} (1976Li23) for 10514+10550+10582+10633+10670 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
E$from 1978Li25, uncertainty assumed to be the same as in 1978Li02 
J$tentative assignment of E6 excitation (1978Li25) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
|b{-2}=0.148 {I11} (1992Ke07) from a reanalysis of data by 1964St15 
T$from DSAM: 0.65 ps {I8} (1969Be48), 0.64 ps {I12} (1973BeYD) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E,J priv comm from L.R.Kouw quoted by 1984Bl19 mentions a J|p=0+ level at 4020 observed in high resolution (p,p') experiment. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_comment:
J priv comm from L.R.Kouw quoted by 1984Bl19 mentions a J|p=0+ level at 4540 observed in high resolution (p,p') experiment. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E weighted average of 5165 {I10} (1967Te02) and 5166 {I10} (1983Fu14) 
$ Configuration=|n(p{-3/2}p{-1/2}) (1986Ho15) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E 5467 {I5} in 1988Fu03 with L=4 
E weighted average of 5472 {I5} (1967Te02) and 5467 {I5} (1988Fu03) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E unweighted average of 6304 {I5} (1969Be18) and 6312 {I5} (1988Fu03). Other: 6306 {I10} (1967Te02) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$ Other: 8433 10 (1982BeZO) 
$ d|s/d|W=0.17 mb/sr {I8} (2007Fu04) 
$ Configuration=|n(f{-7/2}{+-1}f{-5/2}) (1986Ho15) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$ from comparison of isobar analog states in {+58}Cu, 2007Fu04 propose 1+ for this state, but assume E1 transition in their analysis following assignment in (|g,|g') 
$ d|s/d|W=0.37 mb/sr {I4} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$ Other: 9850 20 (1986Ho15) 
$ d|s/d|W=0.33 mb/sr {I4} (2007Fu04) 
$ Configuration=|n(p{-3/2}p{-1/2}) (1986Ho15) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$in e-mail reply of April 10, 2008 from the first author of 2007Fu04, 10211, 1+ is a different level from 10209, L=3 from 1988Fu03, since L>0 transitions are expected to be strongly suppressed in the 0|' spectrum of 2007Fu04 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$ Other:10662 10 (1982BeZO) 
$ d|s/d|W=1.59 mb/sr {I5} (2007Fu04) 
$ Configuration=|n(f{-7/2}{+-1}f{-5/2}) (1986Ho15) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$in e-mail reply of April 10, 2008 from the first author of 2007Fu04, 11165, 1+ is a different level from 11063, L=3 from 1988Fu03, since L>0 transitions are expected to be strongly suppressed in the 0|' spectrum of 2007Fu04 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$Relative=600 
|b{-2}=0.175 {I20} (1971Du09) others: 0.12 (1968Tj01), 0.19 (1968Hi09), 0.232 (1969Jo01), 0.147 (1992Ra31) 
L from 1971Du09 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S |b{-2}=0.15 (1967Fl02), |b{-2}=0.15 (1967Gi05), |b{-2}=0.163 (1968Bi04) 
|b{-2}R=0.873 (1988Bu21) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L,E$neither L=2 nor L=4 gives a good fit; but L=4 is the better of the two (1967Gi05), probable doublet (3600+3620) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$ a weakly excited state in 1967Ja08 to which they assign a doublet of levels 2900 and 2940, known from (p,p') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2+)
level_comment:
E 3558 as given by 1967Ja08 in table 4 is an error; both 1967Ja08 and 1966Sw03 give EL=3588 in other figures and text. 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$ Isoscalar giant-quadrupole resonance 
$ %EWSR=76 {I10} (2006Lu01), 58 {I12} (1992Yo01), 52 {I8} (1991Yo03), 38 {I8} (1988Du17), 55 {I15} (1976Yo02) 
E$from 2006Lu01. Others: 16.3|*10{+3} {I+8-9} (2006Na17), 16.5|*10{+3} {I3} (1992Yo01), 16.1|*10{+3} {I2} (1991Yo03), 16.4E3 2 (1988Du17), 16.4E3 3 (1976Yo02) 
$|G from 2006Lu01. Others: 5.4 MeV {I3} (1992Yo01), 4.7 MeV {I2} (1991Yo03), 4.3 MeV {I2} (1988Du17), 4.9 MeV {I2} (1976Yo02) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$ %EWSR=4% {I2} (2006Lu01), 19 {I10} (1991Yo03), 23 {I5} (1988Du17) 
E$from 2006Lu01. OTHERs: 17.0|*10{+3} {I3} (1991Yo03), 17.3|*10{+3} {I2} (1988Du17) 
$|G from 2006Lu01. Others: 4.0 MeV {I3} (1991Yo03), 3.1 MeV {I2} (1988Du17) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$ Isoscalar giant-monopole resonance 
$ %EWSR=2.9 {I+21-29} for L=0, 6.9 {I20} for L=2 (1991Yo03) 
E$from 2006Lu01. OTHERs: 20.4|*10{+3} {I3} (1991Yo03), 20.2E3 2 (1988Du17) 
$|G from 2006Lu01. Other: 4.4 MeV {I2} (1991Yo03), 3.8 MeV {I8} (1988Du17) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.071 {I15} (2004Yu10,2005Ga15), 0.0740 {I18} from B(E2)/B(E2)({+60}Ni)=0.783 {I14} (1970Le17) and B(E2)({+60}Ni)=0.0945 {I15} (1993Ki10); 0.066 {I4} (1973Ch13), 0.068 {I2} (1971ChZF), 0.072 {I7} (1962St02). Others: 0.063 {I7} (1960Go08), 0.080 {I16} (1960An07), 0.12 {I3}, 0.10 {I3} (1959Al95), 
T$618 fs {I13} from B(E2). Value from DSAM (2001Ke08) is much higher. Adopted T{-1/2}=0.652 ps {I21} which includes all measurements related to lifetime determination (see adopted levels, gammas dataset) 
$Q=+0.076 {I18} (2001Ke02), -0.10 {I6} (1974Le13), -0.14 {I10} (1971ChZF) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from mean lifetime of |t=16 ps {I+2-3}, uncertainty includes statistical (1 ps) and systematic (1 ps from reactions on degrader and +1-2.5 ps from feeding from 3620-keV level) added in quadrature. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+60}Ni,{+58}Ni)=-0.275 fm{+2} {I7}; deduced total charge radius R{-c}({+58}Ni)=3.770 fm {I2} (2020Ka22) 
$Measured isotope shift |d|n({+60}Ni,{+58}Ni)=-509.1 MHz {I25}(stat) {I42}(syst) (2020Ka22) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured differential rms charge radius |d<r{+2}>({+58}Ni,{+60}Ni)=-0.276 fm{+2} {I1} {I6} (2022So14), first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 
$Measured isotope shift |d|n({+58}Ni,{+60}Ni)=-506.3 MHz {I25} (2022So14), uncertainty is combined: statistical and systematic. 
$Measured absolute rms charge radius=3.7695 fm {I2} {I19} (2022So14); first uncertainty is combined: statistical and systematic; second uncertainty is correlated through the uncertainty in King-plot parameters. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_lifetime_info: ;ERR=GE
level_comment:
T$for 0|n2|e decay mode. No visible line at 1918.3 keV {I7} was observed corresponding to the expected Bremsstrahlung energy (2016Le08). The lower T{-1/2} limit was determined from Monte Carlo simulations including uncertainties on the background counts, the detection efficiency, the energy resolution and the peak position. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J From (pol d,p); L(d,p)=3. 
T Wt. ave. of 64 ps {I7} (p,n|g) and 83 ps {I14} (|a,n|g). 
MOMM1$From integral perturbed angular distribution (1974We05,2014StZZ). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J From (pol d,p); L(d,p)=1. 
T$From (|a,n|g). Others: 0.49 ps {I17} (p,n|g) and 0.43 ps {I+62-24} (n,|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$From (pol p,d), L(p,d)=3; log| {Ift}=7.0 from 3/2- in {+59}Cu |e decay. 
T Wt. ave. of 0.28 ps {I6} (|a,n|g), 0.26 ps {I6} (p,n|g) and 0.14 ps +6-4 (n,|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J From (pol d,p); L(d,p)=1. 
T Wt. ave. of 0.25 ps {I5} (|a,n|g), 0.097 ps {I24} (p,n|g) and 0.14 ps +6-4 (n,|g). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J 1428.02|g E2 to 5/2-; 429.58|g M1+E2 to 7/2-; Band member. 
T Wt. ave. of 0.56 ps {I14} (|a,n|g) and 0.83 ps {I32} (p,n|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J From (pol d,p); L(d,p)=3. Possible f{-5/2} band member as from ({+3}He,2p|g) only. 
T Wt. ave. of 0.135 ps {I27} (|a,n|g) and 0.10 ps {I3} (p,n|g). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
J log| {If{+1u}t}<8.5 from 3/2- in {+59}Cu |e decay. L(d,p)=3, J=5/2 from (pol d,p) for probable doublet dominated by this level. 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: FS
level_comment:
J Spin from (pol n,|g), parity suggested by 2013Sc06,2013ScZZ based on cross section ratio in (d,p) and (|a,{+3}He). 
T From (n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: (3/2-,1/2-)
level_lifetime_unit: FS
level_comment:
J,T$from (n,|g) E=thermal. Fed by primary |g; |g to 1/2-, 5/2-, 7/2-. Weaker 1513.0|g to 7/2- favors 3/2-. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E,J Energy: wt. ave. of 4286 {I10} ({+3}He,|a) and 4293 {I10} (d,p), (pol d,p). J|p from (pol p,d), L=3 (p,d). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J L(p,d)=3; probable {+59}Co(g.s.) analogue fragment. 
E from (d,p). 36.2 keV {I2} below strongest analogue fragment in (p,d). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J L(p,d)=3; probable {+59}Co(g.s.) analogue fragment. 
E from (d,p). 17.7 keV {I3} above strongest analogue fragment in (p,d). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (21/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$This level is likely the same as 8129.5, i.e. X=0. There is a small possibility that unobserved weak and multipath connecting transitions from this level to the normal bands may exist, noted in 2002Yu01. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_spin_parity: (21/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$This level is likely the same as 8129.5. However, 2002Yu01 note that there is a small possibility that unobserved weak and multipath connecting transitions from this level to the normal bands may exist 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
L,S from 1994Iw01; however, 2692 level probably not resolved from 2683 level, so evaluator adopts J|p=(5/2-). 


level_energy_unit: KEV
level_comment:
L=(3), 2, (2) and (2J{-f}+1)C{+2}S=0.398, 0.064, 0.010 respectively in 1966Co11, 1964Fu04, 1973Ch11. 


level_energy_unit: KEV
level_comment:
L L=(1 and 4), J|p=(1/2- and 9/2+), (2J{-f}+1)C{+2}S=0.218 and 0.250 at E=4295 reported in 1994Iw01; possibly for 4264+4293+4328 multiplet. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J 5/2 for 6206 level in 1994Iw01, but 6206 and 6225 levels may not have been resolved ((2J{-f}+1)C{+2}S=0.138). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
Probable fragment of {+59}Co g.s. IAS; 36.2 keV {I2} below strongest component of IAS, relative intensity 11.0% {I7} (1978Ik02). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J,S from 1995Ma06. Analogue of 7/2- {+59}Co g.s. (1995Ma06,1978Ik02,1965Sh06). 
Other E: 7280 {I50} (1965Sh06), 7304 (1995Ma06). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
Probable fragment of {+59}Co g.s. IAS; 17.7 keV {I3} above strongest component of IAS, relative intensity 12.2% {I5} (1978Ik02). 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
E$No nearby energy levels from (d,p) or other reactions is comparable considering the fact of centroid energy shift (see footnote). Earlier evaluation (1993Ba85 and 2002Ba42) listed in Adopted Level with a 7342 {I10} level from (d,p) - but this the level is absent in (d,p) data set. Not listed in Adopted Levels. 
Probable fragment of {+59}Co g.s. IAS; 40.1 keV {I3} above strongest component of IAS, relative intensity 14.0% {I9} (1978Ik02). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E 4181 in 1990Se07. Apparent doublet exists near 4200 {I50} in 1966Fo01 (based on shape for 4200-keV peak) 


level_energy_unit: KEV
level_comment:
E reported only by 1965Br29; peak (in spectrum of fig. 2) is too broad to be attributed to a single level. 


level_energy_unit: KEV
level_comment:
$|d<r{+2}>({+60}Ni,{+59}Ni)=-0.180 fm{+2} {I9}. Total charge radius R{-c}=3.782 fm {I2} (2022Ma04) 
$isotope shift |d|n({+60}Ni,{+59}Ni)=-204.3 MHz {I27}(stat) {I22}(syst) (2022Ma04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
Configuration=(|n p{-3/2}){+2} 
T$From 2008Or02, recommended value based on all known measurements. T{-1/2}=0.77 {I4} Wt. av.: 0.90 ps {I+21-14} in (n,n'|g), 0.91 ps {i2} from DSA in Coul. ex. (2001Ke08), 0.715 ps {I16} in {+60}Ni(|g,|g') (1970Me08), 0.9 ps {I3} |g|g(t) (1976Kl04), 0.77 ps {I6} from B(E2)=0.087 {I7} (1974Si01), 0.73 ps {I2} from B(E2)=0.0928 {I20} (1974Li13), 0.69 ps {I5} DSA (1973Fi15) 
MOMM1$other: 0.18 {I24} from transient field integral PAC (1978Ha13) 
MOME2 from Coulomb excitation reorientation (1989Ra17,2011StZZ). Other value: -0.104 {I18} from electron scattering (1972Li12). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from Coul. ex. (2001Ke08). Others: 1.1 ps {I3} from B(E4)=0.00165 {I30} (from (e,e'), average of 0.0015 {I3} (1969To08), 0.0018 {I3}(1961Cr01)) and I|g(2506|g)=2.0|*10{+-6} {I4} (1978Fu05)). Others (from DSA): 0.9 ps {I+12-4} (1979Mo06), 3.3 ps {I5} (1975Iv04), 0.5 ps {I+19-3} (1973Ro20), |<4 ps (1980Ke06), 0.4 ps {I+4-2} (1989Ko54) 
J$configuration=((|n p{-3/2})(|n f{-5/2})) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=AP
level_comment:
T$from |<0.7 ps in {+56}Fe({+7}Li,2np|g) and >0.5 ps in {+60}Ni(p,p'|g), DSA. Other: 0.6 ps {I+5-3} (1989Ko54) in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: PS
level_comment:
T$others: 1.6 ps {I7} from {+56}Fe({+7}Li,2np|g), DSA, 0.12 ps {I+5-2} (1989Ko54) in (n,n'|g) 
J$J|p=3+ in {+28}Si({+35}Cl,3p|g), (p,|g) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
T from {+56}Fe({+7}Li,2np|g), DSA. 1.4 ps {I+14-6} from {+58}Ni(|a,2p|g), DSA, 0.09 ps {I+9-3} (1989Ko54) in (n,n'|g), DSA 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
The |b{+-} feeding of this level is a unique 4{+th} forbidden transition. From the systematics (1998Si17), the log{Ift} of this transition will be >23 and the corresponding intensity will be <1.0x10{+-10}%. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
T 187 ps {I35} reported by 1975Iv04, see 1979Mo06 for comment. 
J positive parity from linear pol of the 1757 keV |g (1979Mo06). 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J 6+, 8+ from |g(|q) and linear polarization data of the decay |g; |g yield function suggests J|<6. 


level_energy_unit: KEV
level_spin_parity: 5,7
level_comment:
J |g(|q) and linear polarization data of the decay |g is D+Q. J=7 favored from high excitation energy and absence of decays to low spin states. Positive parity favored from large |d. 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
J$from excitation function, the absence of decays to low spin states, and population systematics in HI induced reactions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E known J|p=3+ level. |s(|q) and analyzing power reproduced reasonably well by sequential transfer reaction calculation (1977Bo11). 


level_energy_unit: KEV
level_comment:
$S=130 {I25} 
Unresolved doublet at 5.00 MeV (5-) and 5.31 MeV (7-) 
Configuration ((f5/2)(g9/2))7- + ((p1/2)(g9/2))5 
N=190 {I40} for pure L=7; N=440 {I80} for pure L=5 


level_energy_unit: KEV
level_comment:
S N=125 {I40} for L=8; N=60 {I15} for L=6. 
Configuration (g9/2){+2}8+, or ((g9/2),(d5/2))6+ 
J J=8 preferred from magnitude of normalization constant and resemblance to the {+56}Fe(|a,{+2}He){+58}Fe spectrum. 


level_energy_unit: KEV
level_comment:
S N=90 {I20} for L=6; N=190 {I50} for L=8. 
Configuration ((g9/2)(d5/2))6+, or (g9/2){+2}8+ 
J J=6 from reasonable normalization constant. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T |G=0.638|*10{+-3} eV {I14} from |G(0){+2}/|G=0.638|*10{+-3} eV {I14} (1970Me08). 
BE2 0.0938 {I20} (1970Me08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$J=2 from ratio of resonantly scattered |g rays at 98|' and 127|'. 
T |G=22|*10{+-3} eV {I7} from |G(0){+2}/|G=3.2|*10{+-3} eV {I5} (1970Me18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$J=1 from ratio of resonantly scattered |g rays at 98|' and 127|'. 
T |G=37|*10{+-3} eV {I9} from |G(0){+2}/|G=11.1|*10{+-3} eV {I15} (1970Me18). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from DSAM (2008Or02). The authors give 0.735 ps {i21} as the averaged recommended value from all the measurements, including the current value. 


level_energy_unit: KEV
level_comment:
L there is no adopted 3- level in this energy region. In particular, L(|a,|a')=2 for a level at 3110 keV which implies J|p=2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2 measurement of 1969Cl05 corrected by 1974Le13. 
T$from 2001Ke08. Other: 0.69 ps {I5} from DSA measurement of 1973Fi15 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
$|G{-0} (eV)=0.024|*10{+-3} {I8} 
T$>3.1 fs {I12} 
$B(M1)|^<0.190 {I67} 
E$level not observed in the 6.0-MeV data 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.017 {I1} 
E$ 3908.1 {I3} in table IV of 2013Sc20 seems a misprint 
$B(E1)|^=0.82|*10{+-5} {I15} or B(M1)|^=0.074 {I14} 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.036 {I21} 
E,J$level seen only in 8.0-MeV data; spin assignment is tentative 
$B(E1)|^=0.34|*10{+-5} {I20} or B(M1)|^=0.031 {I18} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.214 {I36} 
$B(M1)|^=0.133 {I23}. 
$ Value of 1.47E-5 25 corresponds to B(E1)(|^), which should be discarded, according to e-mail reply of Nov 13, 2013 from author 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.590 {I86} 
E$ uncertainty of 0.2 keV in table III of 2013Sc20 seems a misprint 
$B(M1)|^=0.304 {I44} 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.436 {I68} 
T,S$ for J|p=1-. For J|p=1+, values are: T{-1/2}=1.66 fs {I35}, |G{-0}=0.273 eV {I51} 
$B(E1)|^=2.27|*10{+-5} {I36} or B(M1)|^=0.129 {I24} 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.203 {I45} 
T,S$ for J|p=1-. For J|p=1+, values are: T{-1/2}=4.6 fs {I16}, |G{-0}=0.100 eV {I35} 
$B(E1)|^=0.96|*10{+-5} {I22} or B(M1)|^=0.043 {I15} 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.17 {I13} 
T,S$ for J|p=1-. For J|p=1+, values are: T{-1/2}=1.2 fs {I6}, |G{-0}=0.38 eV {I17} 
$B(E1)|^=0.63|*10{+-5} {I45} or B(M1)|^=0.124 {I55} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G{-0} (eV)=0.15 {I13} 
E$ from E|g. E(level)=9640.0 {I21} listed in table II of 2013Sc20 
$B(E1)|^=0.48|*10{+-5} {I40} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+60}Ni,{+58}Ni)=+0.2731 fm{+2} {I48} (2021Ko18) 
$Measured isotope shift |d|n({+60}Ni,{+58}Ni)=+506.4 MHz {I19}, (2021Ko18) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured absolute rms charge radius=3.8059 fm {I17} (2022So14); uncertainty correlated through the uncertainty in King-plot parameters. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius=3.8225 fm {I19} (2013An02) 
$Evaluated |d<r{+2}>({+61}Ni,{+60}Ni)=+0.082 fm{+2} {I7} (2013An02) 
MOMM1$NMR (1964Dr02), recalculated in 
MOME2$Atomic beam, includes polarization correction (1968Ch10). See also 2008Py02 evaluation 
J$spin from electron paramagnetic resonance (1958Wo52). L(d,p)=L(p,d)=1; L+1/2 from A{-y} in (pol d,p) and (pol p,d) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
MOMM1,MOME2$Mossbauer effect (1971Go31). Other: Q=-0.08 {I7} (1976Ob01) 
J$L(d,p)=L(p,d)=L(d,t)=3; L-1/2 from A{-y}(|q) in (pol d,p), (pol p,d) 
T$from |b{++}|g(t) in {+61}Cu |e decay. Other: 5.1 ns {I3} (Coulomb excitation) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(p,d)=L(d,t)=1; L-1/2 from A{-y}(|q) in (pol d,p), (pol p,d) 
T$weighted average of 22 ps {I4} (|b{++}|g(t) in {+61}Cu |e decay) and 24 ps {I4} ({+58}Fe(|a,n|g)). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(d,t)=1; L-1/2 from A{-y}(|q) in (pol d,t), (pol p,d). See 2012PeZX who question assignment of 1/2- for 656 level based on branching ratio measurements and theory in {+61}Cu decay 
T$other: <21 ps from |b{++}|g(t) in {+61}Cu |e decay 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$|g(|q) and |g(lin pol) in (|a,n|g); L(p,d)=(3); L+1/2 from (pol p,d); L(t,p)=2 from 3/2- target 
T$from {+48}Ca({+18}O,5n|g) (1978Wa09). Others: 6 ps {I2} in {+58}Fe(|a,n|g), {+53}Cr({+11}B,{+12}C), >1.7 ps in Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1; L+1/2 from A{-y}(|q) in (pol d,t); L(t,p)=0+2 from 3/2- target 
T$from {+61}Ni(n,n'|g). Others: 0.25 ps {I+47-11} in {+58}Fe(|a,n|g), {+53}Cr({+11}B,p2n|g) and 0.18 ps {I8} in {+60}Ni(n,|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(p,d)=3; (L-1/2) from (pol p,d); |g(|q) and |g(lin pol) in (|a,n|g). 
T$unweighted average of 0.29 ps {I5} ({+58}Fe(|a,n|g)) and 0.35 ps {I4} (Coul. ex.). Other: 0.14 ps {I4} in {+61}Ni(n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(p,d)=L(d,t)=1, L+1/2 from A{-y}(|q) in (pol d,p), (pol p,d), (pol d,t) 
T$from Coul. ex. Others: 0.14 ps {I+8-4} in {+61}Ni(n,n'|g), 0.145 ps {I35} in {+61}Ni(|g,|g'), 0.104 ps {I17} in {+58}Fe(|a,n|g), {+53}Cr({+11}B,p2n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=L(d,t)=1; L+1/2 from (pol p,d); L(t,p)=0+2 from 3/2- target 
T$other: 0.062 ps {I14} in {+61}Ni(n,n'|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(d,t)=3; L(p,t)=2 from 3/2- target; |g(|q) and |g(lin pol) in (|a,n|g). 
T$from {+61}Ni(n,n'|g). Other: 0.042 ps {I11} in {+58}Fe(|a,n|g), {+53}Cr({+11}B,p2n|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_comment:
J$9/2+ from |g(|q) and |g(lin pol) in (|a,n|g); L=4 component of a doublet with L(d,p)=L(pol d,p)=1+4 and L(d,t)=(1+4). See 2123-keV level; L+1/2 for L=4 component from (pol d,p); L(t,p)=3+5 from 3/2- target 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$L=1 component of 2130-keV doublet with L(d,p)=L(pol d,p)=L(d,t)=1+4; L-1/2 from (pol d,p); log| {Ift}=5.0 from 3/2- parent 
T$other: 0.045 ps {I19} in {+61}Ni(n,n'|g) and 0.051 ps {I10} in {+60}Ni(n,|g). 


level_energy_unit: KEV
level_comment:
J$ L(d,p)=2 for a composite of 4360+4374+4386+4403 suggests 3/2+,5/2+ for one or more of these levels, but not for 4376 which is assigned 7/2- here 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
J$ |g to 5/2-; primary |g from 1/2+. L(d,p)=(0) for a composite of 5366+5395+5405 levels suggests (1/2+) for one or more of these levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$1.7-MeV peak in 1961Sa09 may correspond to the strongly populated 2122 level 
S$for J|p=9/2+ 
$d|s/d|W(7|')=3.53 mb/sr 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$2.7-MeV peak in 1961Sa09 may correspond to the strongly populated 2122 level 
$d|s/d|W(7|')=0.32 mb/sr 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$from g[|G{+2}{-0}/|G]|w(|q)=0.0019 eV {I5} with |G{-0}/|G=0.77 {I8} and |d(1185|g)=0.14 taken from Adopted Gammas. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$|g to the g.s. as seen in other reaction was masked by 1458|g from {+58}Ni, as 1977Pa06 used a natural target 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S$for J|p=5/2- 
$1968Ru02 report 1150 group with L(1+3), S=0.59 for L=3, 5/2- 
$E(level)=1150 40 (1968Ru02) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: NS
level_comment:
T$from |b{++}|g(t), average of values from 1971AzZZ and 1975Ro25. Other: 4.1 ns {I3} (1971VoZX) from (1150|b)(67|g)(t) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from |b{++}|g(t) (1967Be12) 
J$2015Cv01 suggest 3/2- based on branching ratios, low log| {Ift} value and systematics of levels in neighboring nuclides. 
$Measured branching ratios (1977Wa03): I|g(373):I|g(589):I|g(656)=15 {I1}:9 {I1}:76 {I1} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$Measured branching ratios (1977Wa03): I|g(529):I|g(902):I|g(1118):I|g(1185)=9 {I1}:2 {I1}:1 {I1}:88 {I1} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$Measured branching ratios (1977Wa03): I|g(1073):I|g(1446):I|g(1662):I|g(1729)=19 {I6}:30 {I5}:30 {I5}:21 {I4} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$from recoil-distance method (1978Wa09). Other: 6 ps {I2} from 1977Wa15 
J$7/2- (1977Wa03), 7/2- (1975Wi28) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_uncertain: ?
level_comment:
E$fictitious level from negative value of resonance energy 
$E(n)(Lab)=-2.438 keV, |G{-|g}=[1.16] eV 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.038 {I3} 
$E(n)(Lab)=5.5341 keV {I10}, g|G{-n}=0.041 eV {I3}, |G{-|g}=[0.5] eV 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=2.29 {I17} 
$E(n)(Lab)=12.423 keV {I1}, g|G{-n}=2.349 keV {I60}, |G{-|g}=2.29 eV {I17} 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
$g|G{-n}|G{-|g}/|G=0.23 {I2} 
$E(n)(Lab)=23.802 keV {I1}, g|G{-n}=4.7 eV {I2}, |G{-|g}=0.24 eV {I2} 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
$g|G{-n}|G{-|g}/|G=0.29 {I1} 
J$2018MuZY list (1/2) which seems inconsistent with L=(2) 
$E(n)(Lab)=56.331 {I1}, g|G{-n}=0.60 eV {I5}, |G{-|g}=0.56 eV {I3} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.57 {I30} 
$E(n)(Lab)=161.84 {I1}, g|G{-n}=1.330 keV {I27}, |G{-|g}=0.57 eV {I3} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.50 {I18} 
$E(n)(Lab)=186.01 {I1}, g|G{-n}=5.38 keV {I14}, |G{-|g}=0.50 eV {I18} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.69 {I14} 
$E(n)(Lab)=198.97 {I1}, g|G{-n}=3.025 keV {I75}, |G{-|g}=0.83 eV {I14} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$g|G{-n}|G{-|g}/|G=2.27 {I46} 
$E(n)(Lab)=230.39 {I2}, g|G{-n}=107.4 eV {I20}, |G{-|g}=0.77 eV {I16} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.95 {I9} 
$E(n)(Lab)=252.10 {I1}, g|G{-n}=0.566 keV {I30}, |G{-|g}=0.95 eV {I9} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.59 {I9} 
$E(n)(Lab)=257.90 {I1}, g|G{-n}=1.840 keV {I45}, |G{-|g}=0.59 eV {I9} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=1.15 {I42} 
$E(n)(Lab)=317.20 {I1}, g|G{-n}=2.866 keV {I75}, |G{-|g}=1.15 eV {I42} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=2.86 {I60} 
$E(n)(Lab)=325.30 {I1}, g|G{-n}=7.27 keV {I19}, |G{-|g}=2.86 eV {I60} 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
$g|G{-n}|G{-|g}/|G=0.66 {I8} 
$E(n)(Lab)=329.31 {I5}, g|G{-n}=40 eV {I4}, |G{-|g}=0.67 eV {I8}. Uncertainty of 0.5 keV listed for E(n) in 2018MuZY seems too large. Evaluator assigns 0.05 keV 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=1.75 {I42} 
$E(n)(Lab)=338.60 {I1}, g|G{-n}=3.560 keV {I90}, |G{-|g}=2.5 eV {I6} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=1.17 {I20} 
$E(n)(Lab)=357.76 {I1}, g|G{-n}=1.562 keV {I60}, |G{-|g}=1.17 eV {I20} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.95 {I18} 
$E(n)(Lab)=359.59 {I10}, g|G{-n}=1.256 keV {I7}, |G{-|g}=0.47 eV {I90} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=2.03 {I87} 
$E(n)(Lab)=376.90 {I1}, g|G{-n}=3.815 keV {I50}, |G{-|g}=2.03 eV {I87} 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.27 {I5} 
$Uncertainty of 0.50 in resonance strength in 2018MuZY seems a misprint 
$E(n)(Lab)=407.43 {I10}, g|G{-n}=30 eV {I6}, |G{-|g}=0.27 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.63 {I20} 
$E(n)(Lab)=422.80 {I1}, g|G{-n}=1.806 eV {I55}, |G{-|g}=0.63 eV {I2} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.87 {I20} 
$E(n)(Lab)=438.07 {I1}, g|G{-n}=1.164 keV {I55}, |G{-|g}=0.87 eV {I20} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$g|G{-n}|G{-|g}/|G=2.51 {I12} 
$E(n)(Lab)=444.58 {I20}, g|G{-n}=163 eV {I14}, |G{-|g}=0.26 eV {I12} 


level_energy_unit: KEV
level_comment:
L$(1) in 1967Co27 is not confirmed in (|a,{+3}He) measurement by 2013Sc06, where L=3 is obtained. Thus (2J+1)C{+2}S=0.014 in 1967Co27 is not adopted 
$(d|s/d|W){-max}=0.062 mb/sr 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)-
level_comment:
$L=1+3 and J=1/2-,3/2-,5/2- for a doublet 1101+1132 keV from (1976Ko06). 
S$for L=3, 5/2-. Others: 0.11 for L=1, 3/2- component (2013Sc06,2013ScZZ); 0.11 for L=1, 0.18 for L=3 (1976Ko06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_comment:
$L=4+1 and J=(1/2-,9/2+) for a 2120 group quoted in 1976Ko06. 
S$for L=4, 9/2+. Others: 0.04 for L=1, 1/2- component (2013Sc06, 2013ScZZ); 0.25, 0.021 (1976Ko06) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$ (<r{+2}>){+1/2}=3.8406 fm {I21} (2004An14 evaluation, and 2008 update available on http://cdfe.sinp.msu.ru) 
$ 2012Sc01 deduced valence orbit neutron occupancy as follows from summed experimental spectroscopic factors in their study of {+62}Ni(p,d) reaction: 2.31 each for 1p{-3/2} and 0f{-5/2}, 0.93 for 1p{-1/2}, 0.34 for 0g{-9/2} with a total of 5.89 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$transient-field integral PAC (2001Ke02). Others: |m=+0.68 {I14} (1988Sp04), +0.64 {I22} (1978Ha13). 
MOME2$reorientation in Coul. ex. (1974Le13,1989Ra17). 
J$from E2 Coul. ex. from 0+ g.s.; L(p,t)=L(t,p)=2 
BE2$from adopted lifetime 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J$from (n,n'|g). g.s. transition from this level as seen in (n,|g) is disputed. A{-2},A{-4} measurements indicate |DJ=1 for all three |g (2011Ch05). L(p,t)=2 is discrepant. 


level_energy_unit: KEV
level_spin_parity: (2,4)+
level_comment:
J from L({+6}Li,d)=2+4, L(t,p)=(2+4) for unresolved doublet. Also, L(d,p)=1+3 
E may include 3270 level 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$other: 0.42 ps {I+7-6} in (n,n'|g) 
J L(p,t)=4 for a level at 3271 {I5}; L(|a,|a')=4 for a level at 3270; |g decay to 2+ state is Q 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
T$other: 0.35 ps {I+8-6} in (n,n'|g) 
J$earlier suggested as 1+,2+. |g|g(|q) measurement suggest 3369|g to be stretched dipole (2011Ch05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$J=2,4 from |g|g(|q) in {+61}Ni(n,|g); |g decays to 0+ levels; L(t,p)=2; L(p,t)=0+2. L=0 component is most likely for 3524 level 
T$other: 0.62 ps {I+12-10} in (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: PS
level_comment:
J$J=1,2 from |g transitions to 0+ states, |p=+ from log| {Ift}=5.6 from 1+; L(d,p)=1; L(p,t)=2 for a doublet 


level_energy_unit: KEV
level_spin_parity: (6)+
level_lifetime_unit: PS
level_comment:
T$from DSA and RDM in ({+18}O,4n|g). Other: 0.076 ps {I+62-28} in (|a,p|g) 
J E2 |g to 4+ and intense feeding in ({+18}O,4n|g) 


level_energy_unit: KEV
level_spin_parity: 5-,6-
level_lifetime_unit: PS
level_comment:
J$L=4, dominant J-transfer of 9/2+ in (pol d,p) gives 3- to 6-. Lifetime and strong feeding in ({+18}O,4n|g) exclude 3 and 4 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$from weighted average of |t=0.235 ps 45 (1978Ke11), 0.12 ps +12-7 (1978Oh04). Lifetimes measured for both gamma rays from this level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-&7-
level_comment:
$Normalization=70 {I15} 
$Configuration=|nf{-5/2}~#|nd{-5/2} for 5- and |nf{-5/2}~#|ng{-9/2} for 7- 
S$ for 5-, 60 {I15} for 7- 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+&6+
level_comment:
$Normalization=130 {I25} 
$Configuration=|ng{-9/2}~#|ng{-9/2} for 8+ and |ng{-9/2}~#|nd{-5/2} for 6+ 
S$ for 8+, 65 {I15} for 6+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+,8+
level_comment:
$Normalization=55 {I25} 
$Configuration=|ng{-9/2}~#|ng{-9/2} for 8+ and |ng{-9/2}~#|nd{-5/2} for 6+ 
S$ for 6+, 100 {I40} for 8+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ 2007ChZX list a 2891.00 {I25} |g from this level without I|g. This |g is not possible for 0+ assignment 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$ 2007ChZX list only a 3756.5 {I5} |g from this level without I|g. This |g is less likely for 3- assignment 


level_energy_unit: KEV
level_spin_parity: 3-,4-,5-
level_comment:
$ 2007ChZX list only a 4201.0 {I3} |g from this level without I|g. This |g is not likely for 3-,4-,5- assignment 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ 2007ChZX list a 4231.7 {I15} |g from this level without I|g. This |g is not possible for 0+ assignment 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T from ((2J+1) |G{+2}{-|g0}/|G)*W(|q)=0.88 {I17} (meV) (1981Ca10). Other: 2.1 ps {I5} (1977Ca14, same authors as 1981Ca10) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E differs by 14.35 eV {I15} from recoil-corrected E|g of Fe capture |g ray (1974Mo15) 
J J=1 from |g(|q) (1970Mo26); parity from polarization measurement (1972Mo03) 
|G{-|g}=0.48 eV {I5} (1970Mo26) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J$from |g(|q) data. J|p=2+ is inconsistent with |g(|q) for 722|g and 757|g. The g.s. transition was not observed in 2011Ch05, with an detection limit of <2% branching ratio 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_lifetime_unit: PS
level_comment:
$ When feeding from the 1221 doublet transition is considered, measured branching ratios are 4.8 {I2} for 968|g, 38.9 {I10} for 1221|g, 44.7 {I13} for 2097|g and 11.6 {I14} for 3270|g 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: PS
level_comment:
$ Without including the intensity of the weak 265|g and considering feeding from the 1221 doublet transition, the measured branching ratios are 4.6 {I3} for 463|g, 24.8 {I6} for 1186|g and 70.7 {I16} for 1221|g 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
E,J$level population from 1985KoZM 
$According to 1985KoZM, there is another |g deexciting the 3757 level, but no E|g is listed 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
2048.4 keV E0 transition with B(E0 to g.s.)/B(E2 to 1173)=0.028 {I5} from ce(K)(2048|g)/ce(K)(876|g)=0.084 {I11} (1981Pa10) 
Monopole strength reported by 1981Pa10, but adopted T{-1/2} corresponds to 2301 and not 2048 level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
G$ from transient magnetic field method following Coulomb excitation. Other: g=+0.32 {I11} (1978Ha13, in Coul. ex. with {+32}S beam at 73.8 MeV, 73.8 MeV, recoil nuclei in magnetized Fe) 
T$ from 2001Ke08 (also 2001Ke02). Method: DSA following Coulomb excitation in {+12}C({+62}Ni,{+62}Ni'|g) reaction. Uncertainty of 0.05 ps quoted by 2001Ke08 is statistical only. Systematic uncertainty from stopping powers is estimated to be 5% (as per email reply from one of the authors of 2001Ke08), which has been added in quadrature by the evaluator. Other values: 1.58 ps {I13} (1965Es01, DSA method following Coulomb excitation); 1.45 ps {I5} from adopted B(E2)=0.088 {I3} 
$Adopted B(E2)(|^)=0.088 {I3} from weighted average of 0.088 {I3} (1971ChZT), 0.090 {I3} (1970Le17), 0.084 {I5} (1969Ha31), 0.083 {I8} (1962St02), 0.085 {I17} (1960An07). Other: 0.140 {I35} (1959Al95, same group as 1960An07; evaluator assumes that value from 1959Al95 is superseded by that in 1960An07). 1970Le17 measured B(E2)({+62}Ni,first 2+)/B(E2)({+60}Ni,first 2+)= 0.964 {I26}. 
$Deformation length=0.99 fm (1977We05), |b{-2}=0.208 (1975Re17) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-0}|G{-|g}/|G=0.21 {I3} 
$E(n)(lab)=1.35450 keV {I6}, g|G{-n}=0.127 eV {I1}, |G{-|g}=0.95 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$g|G{-0}|G{-|g}/|G=0.085 {I20} 
$E(n)(lab)=3.14400 keV {I21}, g|G{-n}=0.087 eV {I4}, |G{-|g}=1.0 eV 


level_energy_unit: KEV
level_comment:
$C{+2}S=0.79 
$C{+2}S: for {+10}B in the 3+ g.s., the authors obtain for C{+2}S=0.39; for {+10}B in the 1+ first excited state, C{+2}S=0.48 (1985Wi18). See 1985Wi18 for details of the optical-model parameters and for C{+2}S values deduced for other parameter sets 


level_energy_unit: KEV
level_spin_parity: 8(+)
level_comment:
J$8+ or 8- from |g(|q). Comparison with cranked Nilsson-Strutinsky calculations suggests tentative 8(+). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$2019Ev01 take weighted average of 1.8 ps {I+19-6} (2011Ch05) and 0.76 ps {I+76-28} (in {+62}Ni Adopted dataset in the ENSDF database). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+60}Ni,{+62}Ni)=+0.223 fm{+2} {I5}; deduced total charge radius R{-c}({+62}Ni)=3.835 fm {I2} (2020Ka22) 
$Measured isotope shift |d|n({+60}Ni,{+62}Ni)=+503.9 MHz {I25}(stat) {I39}(syst) (2020Ka22) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Measured |d<r{+2}>({+62}Ni,{+58}Ni)=+0.5000 fm{+2} {I48}; |d<r{+2}>({+62}Ni,{+60}Ni)=+0.2266 fm{+2} {I48}; |d<r{+2}>({+64}Ni,{+62}Ni)=+0.1365 fm{+2} {I48} (2021Ko18) 
$Measured isotope shift |d|n({+62}Ni,{+58}Ni)=+1010.6 MHz {I24}, |d|n({+62}Ni,{+60}Ni)=+504.4 MHz {I27}, |d|n({+64}Ni,{+62}Ni)=+524.7 MHz {I26} (2021Ko18) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: Y
level_comment:
J$L(pol d,p)=L(pol d,t)=1 from 0+; L-1/2 transfer from analyzing powers 
T$weighted average of 101.2 y {I15} (2008Co01) and 100.1 y {I20} (1971Ba89). Others: 125 y {I6} (1956Mc95) and 91.6 y {I31} (1962Ho05) seems discrepant; 101.1 y {I14} (1996Co25; superseded by 101.2 y {I15} in 2008Co01 from the same lab, as stated in 2008Co01) 
MOMM1$from laser resonant photoionization spectroscopy, using |m({+61}Ni)=-0.74868 {I4} as a reference (2017Dy01). See also 2019StZV evaluation. 
$|d<r{+2}>({+60}Ni,{+63}Ni)=0.277 fm{+2} {I8}. Total charge radius R{-c}=3.842 fm {I2} (2022Ma04). 
$isotope shift |d|n({+60}Ni,{+63}Ni)=784.9 MHz {I26}(stat) {I27}(syst) (2022Ma04). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$L(pol d,p)=L(pol d,t)=3 from 0+; L-1/2 transfer from analyzing powers 
T$weighted average of 1.61 |ms {I7} from 1975Ro25 in {+63}Co |b{+-} decay, and 1.71 |ms {I3} from {+62}Ni(d,p|g) 
MOMM1$from 1970Bl06 by TDPAD. See also 2020StZV evaluation 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$L(pol d,p)=L(pol d,t)=1 from 0+; L-1/2 transfer from analyzing powers 
T$from 1991Ul01 in (n,|g):E=th based on |g-ray induced Doppler broadening method (GRID) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: NS
level_comment:
J$L(d,p)=L(d,t)=4 from 0+ 
T$other: 10 ns {I2} (1997Is13) from |g(t) using {+198}Pt({+}Ge,X|g) reaction 
MOMM1$from 1989Mu27 by TDPAD. See also 2020StZV evaluation. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$weighted average of 1787 {I10} from (d,p) and 1790 {I15} from (d,|a) 
J$L(d,t)=3 from 0+ for a level at 1770. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$weighted average of 1899 {I10} from (d,p) and 1910 {I15} from (d,|a) 
J$L(d,t)=3 from 0+ for a level at 1910. However, L(d,p)=(1) for level at 1899 {I10} giving (1/2-,3/2-). 


level_energy_unit: KEV
level_spin_parity: 11/2(+)
level_lifetime_unit: PS
level_comment:
J$891.56|g D+Q to 9/2+; 630.5|g D+Q from 2815, 13/2+; parity=(+) from band assignment. See comments for J|p(2815) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$1522.48|g E2, |DJ=2 to 9/2+ gives 5/2+ or 13/2+; 5/2+ assignment would require J(2183)=7/2 (based on 630.5|g D+Q from 2815 to 2183 level and 891.7|g D+Q from 2183 to 1292, 9/2+ level), which is inconsistent with J(2183)=(11/2,13/2) from |g(|q) in ({+18}O,3n|g). This argument here also determines J(2183)=11/2. 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$weighted average of 4358 {I10} from (d,p) and 4370 {I40} from ({+3}He,|a) 
J$L({+3}He,|a)=3 for a level at 4370 {I40}. 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_comment:
J$tentative assignment in ({+48}Ca,2|a3n|g) from the comparison with cranked Nilsson-Strutinsky model calculations. 


level_energy_unit: KEV
level_spin_parity: (21/2-)
level_comment:
J$proposed in ({+48}Ca,2|a3n|g), with no explicit argument given for the negative parity; 759.3|g D, |DJ=1 to (19/2+) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$IAS ({+63}Co g.s.), assigned in {+64}Ni(p,d); also supported by coupled-channel analysis of measured |s(|q) data in (p,d) IAS. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (25/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$x|?12.7 MeV and J|p|?25/2- from comparison of energies and spins of observed bands (Fig. 6 in 2013Al19) in ({+48}Ca,2|a3n|g) 


level_energy_unit: KEV
level_spin_parity: (11/2+,13/2+)
level_lifetime_unit: PS
level_comment:
T$from |t=5.2 ps {I8} in 1978Wa09 
J$from |g(|q) and also from comparisons of the level spacings between even-parity states in odd-A nuclides with the spacing and Q(2+) value of the |DJ=2 g.s. transitions of the coresponding A-1 nuclides (see FIG.9 of 1978Wa09). 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
J$(13/2+) suggested from comparison of level diagrams of similar odd nuclides (1978Wa09) 
T$from |t=0.7 ps {I3} in 1978Wa09, which is from |t(631|g)<1 ps by RDM and |t(1523|g)>0.4 ps by DSAM 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
T$from |t=2.46 |ms {I4}, weighted average of 2.48 |ms {I4} using 87.2|g(t) by 1970Bl06 and 2.43 |ms {I5} by 1978Ho06. 
$g-factor is measured using the pulsed-beam time-differential spin precession method (1970Bl06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
S$others: 3.23 for an unresolved group around E|?100 (1968Ru02); 6.0 for a triplet of g.s.+90+160 (1969Ar20) 
L$3 for an unresolved group (1968Ru02) 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_comment:
J$967|g(|q) gives (17/2,19/2,21/2); tentative assignment of 17/2+ is from the comparison with cranked Nilsson-Strutinsky model calculations by authors. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: J AP (25/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$x|?12.7 MeV and J|p|?25/2- estimated from comparison of energies and spins of observed bands in Fig. 6 in 2013Al19. 


level_energy_unit: KEV
level_comment:
S$57.024 in 2018MuZY is a misprint and it should be 70.893 adopted from 2014Le04 
$g|G{-n}=0.3 eV, |G{-|g}~0.46 eV. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
J$spin=1/2 also from |g|g(|q) in 1964Co13. 
T$from |t=0.60 ps {I+44-23} in 1991Ul01 based on |g-ray induced Doppler broadening method (GRID), with a correction for 30% reduction claimed by 1992Ku17 based on re-analysis of some data in 1991Ul01 using a more realistic description of slowing down of low velocity recoil nuclei compared to that in 1991Ul01. Note that the main authors of 1991Ul01 including the first author are also among the authors of 1992Ku17 


level_energy_unit: KEV
level_comment:
J$(3/2) proposed in 1977Is01 from |g decays with approximately equal branching to lowest 1/2-, 3/2-, 5/2- levels, but no other supporting evidence is available. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
L$also from 1977St07, 1970Li03, 1963Fu04, 1970Tu02 
S$others: 0.83 (2013Sc06), 0.747 (1963Fu04), 0.414 (1977St07), 0.85 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$other: 88 (1963Fu04,1970Tu02,1977St07) 
S$others: 3.55 (2013Sc06), 2.39 (1963Fu04), 2.32 (1977St07), 3.40 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 158 (1970Li03,1963Fu04), 155 (1970Tu02,1977St07) 
S$others: 1.11 (2013Sc06), 1.07 (1963Fu04), 0.567 (1977St07), 1.15 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 518 (1970Li03,1970Tu02,1977St07), 526 (1963Fu04) 
S$others: 0.34 (2013Sc06), 0.306 (1963Fu04), 0.276 (1977St07), 0.32 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$others: 1000 (1970Li03,1970Tu02), 1008 (1963Fu04) 
S$others: 0.68 (2013Sc06), 0.663 (1963Fu04), 0.82 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
E$others: 1292 (1970Li03,1970Tu02,1977St07), 1306 (1963Fu04) 
S$others: 3.21 (2013Sc06), |?6.1 (1963Fu04), 3.376 (1977St07), 6.72 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 2291 (1970Li03,1970Tu02,1977St07), 2302 (1963Fu04) 
S$others: 1.66 (1963Fu04), 1.99 (1970Tu02), 1.245 (1977St07) 


level_energy_unit: KEV
level_spin_parity: (9/2)+
level_comment:
E$others: 2529 (1963Fu04), 2514 (1977St07,1970Tu02) 
S$others: 1.75 (2013Sc06), 2.70 (1963Fu04), 1.606 (1977St07), 2.58 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$others: 2701 (1963Fu04), 2692 (1977St07,1970Tu02) 
S$others: 0.07 (2013Sc06), 0.10 (1970Tu02), for L=1; |?0.16 for L=2 and |?0.7 for L=3 (1963Fu04); 0.08 for L=2 (1977St07) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$others: 2941 (1970Li03,1970Tu02,1977St07), 2960 (1963Fu04) 
S$others: 0.375 (1963Fu04), 0.275 (1977St07), 0.23 (1970Tu02) 


level_energy_unit: KEV
level_comment:
E$others: 3100 (1963Fu04), 3092 (1970Tu02) 
L$other: 1 from 1963Fu04 and 1970Tu02 
S$other: 0.061 (1963Fu04), 0.04 (1970Tu02), for L=1 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 3283 (1970Li03,1970Tu02,1977St07), 3291 (1963Fu04) 
S$others: 3.96 (1963Fu04), 0.213 (1977St07), 0.43 (1970Tu02) 


level_energy_unit: KEV
level_comment:
E$others: 3731 (1970Li03), 3726 (1963Fu04), 3709 (1977St07) 
S$others: 0.213 (1963Fu04), 0.096 (1977St07) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$others: 3964 (1970Li03,1970Tu02), 3959 (1963Fu04), 3939 (1977St07) 
S$other: 0.739 (1963Fu04), 0.302 (1977St07), 0.81 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$others: 4083 (1963Fu04), 4052 (1977St07) 
L,S$for the 4063 and 4074 states together (1970An25); however, L=2, (2J+1)C{+2}S=0.418 reported by 1977St07; L=2, (2J+1)C{+2}S=0.258 in 1963Fu04 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$others: 4279 (1970Li03,1970Tu02,1963Fu04), 4258 (1977St07) 
S$others: 0.18 (1963Fu04), 0.137 (1977St07), 0.10 (1970Tu02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$other: 4415 (1963Fu04), 4376 (1977St07,1970Tu02) 
S$other: 0.309 (1963Fu04), 0.194 (1977St07), 0.40 (1970Tu02) 


level_energy_unit: KEV
level_comment:
E,L$other: L=2 for a doublet of 4415+4473 in 1970Li03; 4473 with L=2 (1963Fu04) 
S$other: 0.087 (1963Fu04) 


level_energy_unit: KEV
level_comment:
E$other: 5200 with L=0 (1963Fu04) 
L$from 1963Fu04. Other: L=(0) from 1970An25 
S$other: |?0.1 (1963Fu04) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
E$from 1979Ik04. Assigned as IAS ({+63}Co g.s.) from systematics. Other: 11850 {I80} (1970De18) 
J,L,S$from coupled-channel analysis of |s(|q) (1970De18) 


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}=3.8572 fm {I23} (2013An02) 
$Evaluated |d<r{+2}>({+60}Ni,{+64}Ni)=+0.338 fm{+2} {I10} (2013An02) 
$Measured |d<r{+2}>({+60}Ni,{+64}Ni)=+0.368 fm{+2} {I9}; deduced total charge radius R{-c}({+64}Ni)=3.854 fm {I2} (2020Ka22). 
$Measured isotope shift |d|n({+60}Ni,{+64}Ni)=+1027.2 MHz {I25}(stat) {I77}(syst) (2020Ka22). 
$Measured |d<r{+2}>({+64}Ni,{+58}Ni)=+0.6362 fm{+2} {I48}; |d<r{+2}>({+64}Ni,{+60}Ni)=+0.3631 fm{+2} {I48} (2021Ko18) 
$Measured isotope shift |d|n({+64}Ni,{+58}Ni)=+1534.3 MHz {I26}, |d|n({+64}Ni,{+60}Ni)=+1028.2 MHz {I26} (2021Ko18) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(|a,|a')=L(d,d')=L(p,p')=2 from 0+ 
T$weighted average of 1.065 ps {I116} from RDDS in {+238}U({+64}Ni,{+64}Ni'|g) (2017Kl01) and 1.088 ps {I35} from DSAM in Coul. Ex. (2001Ke08,2001Ke02). Others: 0.017 ps {I8} from DSAM in (n,n'|g) (1983El03, 1989Ge09); 0.28 ps {I10} from DSAM in (|a,|a'|g) (1974Iv01); 0.91 ps {I4} from adopted B(E2)|^=0.0705 {I29}. 
MOMM1$from transient-fields in Coul. ex. (2001Ke02,2001Ke08). Other: +0.92 {I26} (1978Ha13,1979BrZP) from Coul. ex. 
MOME2$from Coul. ex. (1971ChZT). 2021StZZ and 2016St14 list rounded value of 0.4 {I2} 
BE2$weighted average of 0.070 {I10} from ({+18}O,{+16}O|g) (2020Ma37), 0.071 {I3} from (e,e'); 0.0718 {I29} (2014Al20), 0.065 {I4} (1971ChZT), 0.087 {I17} and 0.077 {I15} (1960An07), 0.090 {I18} (1959Al95) from Coul. ex. Others: 0.069 {I5} from inelastic scattering (1996Ch03); see also (|a,|a') dataset for deformation parameter. 
B2$from (pool p,p'). In (|a,|a') (1971Go36), negative sign is indicated from relative phase of |s(|q) for (|a,|a) and (|a,|a'). Others: 0.13 to 0.22 (see (|p,|p'), (p,p'); (d,d'); ({+3}He,{+3}He'); (|a,|a'); inelastic scattering). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E,J$spin=2 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); parity from L(d,{+3}He)=L(t,|a)=1 from 3/2-. Other: L(p,p')=(0) proposed (1963Di11) for a weak group at 2275 and J|p=0+ assumed by 1987Ba78 in the analysis of |s(|q) for a 2280 group in (|a,|a') suggest an additional (0+) level near 2275 
$B(E2)|^<0.0002 (e,e') (1988Br10). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from DSA in Coul. Ex. (2001Ke08). Other: >0.31 ps from DSA in (n,n'|g) (1989Ko54). 
J$1264.3|g E2 to 2+; L(t,p)=L(e,e')=L(p,p')=4 from 0+ 
$B(E4)|^=0.0018 {I4} (e,e') (1988Br10). 
$|b{-4}=0.09 (1969Be20), 0.07 (1974Ba74). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=0 from 0+; spin=0 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g) Other: L(p,p')=(2) from 0+ and L(d,{+3}He)=1+3 from 3/2- could indicate a separate level. 
T$from B(E2) in Coulomb excitation (2020Ma37); also 1.4 ps {I6} from RDDS in {+62}Ni({+18}O,{+16}O|g) (2020Ma37). Value of 0.04 ps {I2} from DSAM in (n,n'|g) (1989Ko54) seems discrepant. 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_lifetime_unit: PS
level_comment:
E$probable doublet in (t,p) and (p,p'). 
J$2972.0|g to 0+. J|p=(2+) from L(t,p)=(2) for one member of the doublet. 2+ proposed by 2020Ma37 in ({+18}O,{+16}O|g) but no arguments given 
T$from DSAM in (n,n'|g) (1989Ko54). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$spin=0 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); 1680.1|g E2 to 2+ 
T$from RDDS in {+62}Ni({+18}O,{+16}O|g) (2020Ma37). Other: 4.1 ps {I+5-4} from B(E2) in Coulomb excitation (2020Ma37) and adopted branching ratio of 1680|g 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L(|a,|a')=2 from 0+. Other: 1+ reported by 2020Ma37 in {+62}Ni({+18}O,{+16}O|g), but no arguments given 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$spin=4 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); parity from L(e,e')=L(p,p')=4 from 0+. 
T$from DSAM in (n,n'|g) (1989Ko54). 
$B(E4)|^=0.00058 {I14} (e,e') (1988Br10). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(|a,|a')=2 from 0+ 
T$from B(E2)|^=0.0025 {I1} from (e,e') (1988Br10) and adopted branching of 3275.9|g. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$spin=0 from |g|g(|q) in (n,|g) E=th (2020Ma37); 2117.86|g to 2+; primary |g from 1- expected to be E1. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$spin=3 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); L(t,p)=L(|a,|a')=L(p,p')=L(e,e')=3 from 0+. 
BE3$from (e,e'), average (by 2002Ki06) of two values: 0.031 and 0.026 listed by 1988Br10 using two different models. Others: 0.022 or 0.024 ((|a,|a'), 1985Al24) and (|p,|p') (1993Pe09). 
B3$from (pol p,p'). Others: 0.11-0.17 (see (p,p'); (d,d'); ({+3}He,{+3}He'); (|a,|a')). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$3578.3|g to 0+; 2012Pa39 in {+64}Co |b{+-} decay proposed (1+) based on non-observation in (t,p) and 278.6|g most likely M1 from 3856 level with parity=(+) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$spin=2 from |g|g(|q) in (n,|g) E=th (2020Ma37); 2403.25|g M1+E2 to 2+ 
T$from line-shape analysis for 2403|g observed in {+65}Cu({+11}B,{+12}C|g) (2020Ma37). See {+62}Ni({+18}O,{+16}O|g) dataset 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_comment:
J$spin=4 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); 189|g to 3- and 99.9|g from 5- are most likely M1. But L(|a,|a')=(4) for a group at 3745 suggests (4+) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from ({+18}O,{+16}O|g) (2020Ma37). Other: 3797 {I5} from (p,p'). 
J$probable 2451|g to 2+; 2020Ma37 in (n,|g) E=th state that J|p=2+ is firmly established, but no further details are given. 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
J$L(e,e')=L(|a,|a')=5 from 0+ and L(t,|a)=4 from 3/2-. 
$Possible dominant configuration=|ng{-9/2}|np{-1/2} (1994Pa20). 
$B(E5)|^=0.00055 {I3} (e,e') (1988Br10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$2020Ma37 in (n,|g) E=th note that 0+ is established based on a 702|g-3154|g correlation cascade from a (n,|g) E=th experiment at ILL, which has not been published. 


level_energy_unit: KEV
level_spin_parity: (0+:4+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 3958 {I10} from (t,p) and 3965 {I7} from (p,p') 
J$probable 2671|g to 2+ 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$from (e,e'). L(|a,|a')=(4,5) suggests a doublet with J|p=4+ and 5- 
J$L(e,e')=4 from 0+ and L(t,|a)=3 from 3/2-. 
$B(E4)|^=0.00030 {I7} (e,e') (1988Br10). 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_comment:
J$spin=5 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); 236.2|g to 5- is most likely M1; L(|a,|a')=(4,5) suggests a doublet with J|p=4+ and 5- 


level_energy_unit: KEV
level_spin_parity: 6(-)
level_comment:
J$spin=6 from |g|g(|q) in {+238}U({+64}Ni,{+64}Ni'|g); 323.4|g to 5- and 359.4|g from 7- are most likely M1 
$Possible configuration=|ng{-9/2}|np{-3/2}+|ng{-9/2}|nf{-5/2}{+-1} (1994Pa20). 


