# LEVEL

level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
E$from {+24}Mg({+16}O,|a2p|g) 
J$E2 |DJ=2 |g to 3-, 4625 and E1 |DJ=1 |g to 4+, 4689 ({+24}Mg({+16}O,|a2p|g)) 
T$mean lifetime |t in ps, from {+31}P(|a,p|g): 54 {I5} (1972Gr15); from {+35}Cl(t,|a|g): 55 {I7} (1976Co11); from {+24}Mg({+16}O,|a2p|g): 52.9 {I24} (1976Me03). Weighted average: 53.3 {I21} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$from {+34}S(p,p'),(pol p,p'); J=3 from D+Q |DJ=1 gammas to 2+, 3303 and 4+, 4688 ({+31}P(|a,p|g)); |p=- from L=1+3 in {+33}S(d,p) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$M1+E2 |DJ=1 |g to 3+, 4875 and test of spin hypotheses ({+31}P(|a,p|g)) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 600 {I+700-300} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J$D+Q |DJ=1 |g to 2+, 2128 and test of spin hypotheses ({+31}P(|a,p|g)); |p=- from L=1 in {+33}S(d,p) 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_lifetime_unit: FS
level_comment:
E$from {+31}P(|a,p|g) 
J$D |DJ=1 |g to 3-, 5680 ({+31}P(|a,p|g); J=2 excluded by 1977GrZH); |p=(-) from L=(3) in {+33}S(d,p) sustained by argument in {+34}S(|a,|a') 
T$mean lifetime |t in fs from {+31}P(|a,p|g): 60 {I15} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2(+),4(+)
level_comment:
E$from {+31}P(|a,p|g) 
J$D+Q |DJ=0 |g, or Q |DJ=2 |g, to 2+, 2128; |p=(+) from gammas to 2+, 3304 and 4+ 4689 


level_energy_unit: KEV
level_spin_parity: (3,4)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E${+31}P(|a,p|g) 
J$from {+31}P(|a,p|g); |p=+ from {+35}Cl(d,{+3}He) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): <20 (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$test of spin hypotheses of secondary 4892|g with primary 2058|g treated as unobserved ({+31}P(|a,p|g)); |p=- from L=1 in {+33}S(d,p) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$from {+31}P(|a,p|g) 
J$Q, |DJ=2 |g to 0+, g.s. and test of spin hypotheses ({+31}P(|a,p|g)); |p=+ from L=0 in (d,{+3}He) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
WIDTHG0$for J|p=2+ ({+34}S(|g,|g'),(pol |g,|g')) 
J$(1,2+) from {+34}S(|g,|g'),(pol |g,|g'); |g to 4+ 


level_energy_unit: KEV
level_spin_parity: (4)
level_lifetime_unit: FS
level_comment:
J$(2,4) from 1977GrZH in {+31}P(|a,p|g); (4) from D |DJ=1 |g to 5-, 5688 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 20 {I10} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: 5,(4)
level_lifetime_unit: FS
level_comment:
E$from {+31}P(|a,p|g) 
J$5,(4) from {+31}P(|a,p|g) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 230 {I50} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: (-)
level_comment:
E$weighted average of 7649 {I14} ({+34}S(p,p'),(pol p,p')) and 7659 {I11} ({+33}S(d,p)) 
J$L=(3) in {+33}S(d,p) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L=2 in {+32}S(t,p); {+33}S(d,p) gives |p=- from L=1 (not adopted) 
E$weighted average of 7739 {I16} ({+32}S(t,p)) and 7753 {I9} ({+33}S(d,p)) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: FS
level_comment:
E$from {+24}Mg({+16}O,|a2p|g) 
J$M1+E2 |DJ=1 |g to 5-, 5691 and E2 |DJ=2 |g to 4-, 6252 ({+24}Mg({+16}O,|a2p|g) 
T$weighted average of values (in fs), from {+24}Mg({+16}O,|a2p|g): 132 {I35} (2005Ma03), and from {+31}P(|a,p|g): 80 {I24} (from mean lifetime |t 115 {I35} (1977GrZH)) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 7801 {I16} ({+32}S(t,p)) and 7805 {I5} ({+34}S(p,p'),(pol p,p')) 
J$L=2 in {+32}S(t,p) 


level_energy_unit: KEV
level_spin_parity: 5
level_lifetime_unit: FS
level_comment:
E$from {+31}P(|a,p|g) 
J$from {+31}P(|a,p|g) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 64 {I10} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: FS
level_comment:
E$from {+24}Mg({+16}O,|a2p|g) 
J$E2 |DJ=2 |g to 5-, 5691 and D |DJ=1 |g to 6-, 7791; 7- in 2005Ma03 
T$weighted average of values (in fs) from {+24}Mg({+16}O,|a2p|g): 85 {I28} (2005Ma03) and from {+31}P(|a,p|g): 83 {I14} (from mean lifetime |t in fs: 120 {I20} (1977GrZH)) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: FS
level_comment:
E$from {+24}Mg({+16}O,|a2p|g) 
J$D |DJ=1 |g to 5, 5691; |p=+ from band structure 
T$mean lifetime |t in fs from {+31}P(|a,p|g): 40 {I10} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
E$weighted average of 8656 {I5} ({+34}S(p,p'),(pol p,p')) and 8657 {I7} ({+34}S(|g,|g'),(pol |g,|g')) 
J$from {+34}S(|g,|g'),(pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
E$weighted average of 9478 {I4} ({+34}S(|g,|g'),(pol |g,|g')) and 9481 {I5} ({+34}S(p,p'),(pol p,p')) 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
E$weighted average of 9700 {I6} ({+34}S(p,p'),(pol p,p')) and 9711 {I5} ({+34}S(|g,|g'),(pol |g,|g')) 
J$from {+34}S(|g,|g'),(pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
E$weighted average of 9860 {I7} ({+34}S(|g,|g'),(pol |g,|g')) and 9872 {I5} ({+34}S(p,p'),(pol p,p')) 
J$from {+34}S(|g,|g'),(pol |g,|g') 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: S
level_comment:
E$from least-squares fit to E|g data in {+33}S(n,|g) dataset. This value is higher by |?0.10 keV than S(n)=11417.12 {I6} (2011AuZZ). Other: S(n)=11417.11 {I9} (2003Au03), 11417.22 {I5} and 11417.12 {I10} (1983Ra04) using 'mass-doublet standard' and 'gold standard', respectively 
J$ s-wave capture in {+33}S g.s., J|p=3/2+ 
$ Observed deexcitation intensity is 83% {I2}, other 17% intensity of the primary |g rays is unaccounted 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-n} and |G|a from {+33}S(n,|g),(n,n); |G{-|g} from {+30}Si(|a,|g),(|a,n) 
J$E1 |DJ=1 |g to 0+, g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_lifetime_unit: KEV
level_comment:
$All data are from {+33}S(n,|g),(n,n) 
J$E1+M2 |DJ=(1) |g to 2+, 2128 (angular correlation excludes 3-) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
J$E1 |DJ=1 |g to 0+, g.s. 
E$from {+33}S(n,|g),(n,n) 
$|G from {+33}S(n,|g),(n,n) and |G{-|g} from {+30}Si(|a,|g),(|a,n) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 2127.0 {I6} (1970Mo09); 2126.8 {I8} (1970Gr11); 2127 (1971Mu03); 2127 {I1} (1974Gr06); 2126 {I1} (1969Gr03) 
J$E2 |DJ=2 |g to 0+, g.s. 
T$mean lifetime |t in fs: 440 {I50} (1970Gr11); 400 {I32} (1970Ra17); 400 {I40} (1974Gr06); 350 {I60} (1969Gr03); 460 {I95} (1970Br18); 467 {I90} (1970Cu02). Weighted average: 407 {I20} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3303.2 {I4} (1970Mo09); 3303.0 {I9} (1970Gr11); 3303 (1971Mu03); 3304 {I2} (1974Gr06); 3300 {I3} (1969Gr03) 
T$mean lifetime |t in fs: 218 {I30} (1970Gr11); 175 {I25} (1970Ra17); 145 {I20} (1974Gr06); 120 {I30} (1969Gr03); 190 {I40} (1970Br18); 144 {I28} (1970Cu02). Weighted average: 161 {I13} (external uncertainty) 
J$D+Q |DJ=0 |g to 2+, 2127 (1970Mo09); |p=+ from E2 |g to 0+, g.s. (1979Ba54) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
E$weighted average of: 3913.1 {I10} (1970Mo09); 3915.1 {I9} (1970Gr11); 3915 (1971Mu03); 3914 {I2} (1974Gr06) 
J$D,Q |g to 2+, 2127 (1970Mo09); 0+ in Adopted Levels 
T$mean lifetime |t in fs: 1600 {I130} (1970Gr11); 1890 {I500} (1970Ra17, or a more conservative value is >1390); |>400 (1974Gr06). Weighted average: 1618 {I126} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average (external uncertainty) of: 4071.9 {I10} (1970Mo09); 4075 {I2} (1970Gr11); 4075 (1971Mu03); 4078 {I3} (1974Gr06) 
J$D |DJ=1 |g to 0+, g.s. (1970Mo09, 1971Mu03); |p=+ from M1+E2 |g to 2+, 2127 
T$mean lifetime |t in fs: <33 (1970Gr11); <24 (1970Ra17); |<50 (1974Gr06). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average (external uncertainty) of: 4114.2 {I8} (1970Mo09); 4116 {I2} (1970Gr11); 4116 (1971Mu03); 4119 {I3} (1974Gr06) 
J$E2 |DJ=2 |g to 0+, g.s. 
T$mean lifetime |t in fs: 89 {I20} (1970Gr11); 110 {I10} (1970Ra17); 100 {I15} (1974Gr06). Weighted average: 105 {I9} 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$weighted average of: 4622.4 {I7} (1970Mo09); 4623 {I2} (1970Gr11); 4623 (1971Mu03); 4622 {I3} (1974Gr06) 
J$3, D(+Q) |DJ=1 |g to 2+, 2127 and test of spin hyphotheses; |p=- from E2 |g from 5-, 5688 
T$mean lifetime |t in fs: 125 {I20} (1970Gr11); 135 {I17} (1970Ra17); 145 {I50} (1971So01); 115 {I10} (1974Gr06). Weighted average: 121 {I8} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 4687.6 {I7} (1970Mo09); 4688 {I2} (1970Gr11); 4688 (1971Mu03); 4687 {I2} (1974Gr06); 4688 {I1} (1977GrZH) 
J$E2 |DJ=2 |g to 2+, 2127 and test of spin hyphotheses (1971Mu03) 
T$mean lifetime |t in fs: 132 {I15} (1970Gr11); 131 {I13} (1970Ra17); 110 {I20} (1971So01); 125 {I10} (1974Gr06); 130 {I20} (1977GrZH). Weighted average: 127 {I6} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 4875.2 {I7} (1970Mo09); 4874 {I2} (1970Gr11); 4874 (1971Mu03); 4874 {I4} (1974Gr06) 
J$M1+E2 |DJ=1 |g to 2+, 3303 and test of spin hyphotheses (1971Mu03) 
T$mean lifetime |t in fs: <85 (1970Gr11); 57 {I22} (1970Ra17); |<70 (1974Gr06). Weighted average: 55 {I20} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 4890 {I4} (1970Mo09); 4892 {I2} (1970Gr11); 4892 (1971Mu03); 4892 {I4} (1974Gr06) 
J$E2 |DJ=2 |g to 0+ g.s. (1970Mo09, 1971Mu03) 
T$mean lifetime |t in fs: <40 (1970Gr11); 52 {I14} (1970Ra17). Weighted average (external uncertainty): 42 {I15} 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_comment:
E$weighted average of: 5318 {I2} (1970Gr11); 5318 (1971Mu03); 5322 {I4} (1974Gr06) 
J$D+Q |DJ=0 |g to 2+, 2127 
T$mean lifetime |t in fs: 24 {I10} (1970Gr11); |<40 (1974Gr06) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$5380 (1971Mu03); 5382 {I4} (1974Gr06) 
J$D |DJ=1 |g to 0+, g.s. and M1+E2 |DJ=1 |g to 2+, 2127 (1971Mu03) 
T$mean lifetime |t in fs: |<70 (1974Gr06) 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$weighted average of: 5680 (1972Jo10); 5680 {I4} (1974Gr06); 5679 {I1} (1977GrZH) 
J$D+Q |DJ=0 |g to 2, 2127; J=3,(2) (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
E$5689 (1972Jo10); 5688 {I4} (1974Gr06) 
J$|DJ=2 |g to 3, 4622; E1 |DJ=1 |g 4+, 4688 
T$mean lifetime |t in ps: |>0.5 (1974Gr06); 54 {I5} (1972Gr15) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
E$6250 (1972Jo10); 6251 {I2} (1977GrZH) 
J$M1+E2 |DJ=1 |g to 3+, 4875 and test of spin hypotheses; J=4,(3) (1977GrZH) 
T$mean lifetime |t in fs: 600 {I+700-300} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: (3,4)
level_lifetime_unit: FS
level_comment:
E$6640 (1972Jo10); 6639 {I1} (1977GrZH) 
J$presence of non-zero A{-4} coefficients for correlations from this level (A{-4}=+0.19 {I7} for 1176|g, and A{-4}=-0.29 {I13} for 3303, both from 3303, J=2) makes unlikely J=1 but allow J=(2,3,4) (1972Jo10); J=3 from D |DJ=1 |g to 2, 5679; J=4 (1977GrZH) 
T$mean lifetime |t in fs: 60 {I15} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: 5
level_lifetime_unit: FS
level_comment:
E$6864 (1972Jo10); 6864 {I1} (1977GrZH) 
J$5, from Q |DJ=2 |g to 3, 4622 (1977GrZH); (0,2,4) from D+Q |DJ=0 |g, or Q |DJ=2 |g, to 2, 2127 and test of spin hypotheses 
T$mean lifetime |t in fs: 39 {I10} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: (3,4)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$6890 {I1} (1977GrZH); 6898 (1972Jo10 with no other piece of information) 
J$(3,4) from 1977GrZH 
T$mean lifetime |t in fs: <20 (1977GrZH) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2
level_comment:
E$6950 (1972Jo10) 
J$from test of spin hypotheses of secondary 4892|g with primary 2058|g treated as unobserved (see A{-2},A{-4} values at 4892|g from 4892) 


level_energy_unit: KEV
level_spin_parity: (4)
level_lifetime_unit: FS
level_comment:
E$7245 (1972Jo10); 7248 {I2} (1977GrZH) 
J$(2,4) from 1977GrZH; (4) from D |DJ=1 |g to 5-, 5688 
T$mean lifetime |t in fs: 20 {I10} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: 6
level_lifetime_unit: FS
level_comment:
E$7788 {I1} (1977GrZH) 
J$4,6 from D |DJ=1 |g to 5-, 5688; 6 from 1977GrZH (test of spin hypotheses) 
T$mean lifetime |t in fs: 115 {I35} (1977GrZH) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: S
level_comment:
E$ from least-squares fit to E|g data, this value is higher by |?0.10 keV from S(n)=11417.12 {I6} (2011AuZZ). Other: S(n)=11417.11 {I9} (2003Au03), 11417.22 {I5} and 11417.12 {I10} (1983Ra04) using 'mass-doublet standard' and 'gold standard', respectively 
J$ s-wave capture in {+33}S g.s., J|p=3/2+ 
$ Observed deexcitation intensity is 83% {I2}, other 17% intensity of the primary |g rays is unaccounted 


level_energy_unit: KEV
level_comment:
E$weighted average of: 3305 {I2} (1972Cr08); 3302 {I10} (1963Br05) 
L$0+2 (1971Va21) 
S$0.22+1.7 (1971Va21) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 4118 {I4} (1972Cr08); 4120 {I10} (1963Br05) 
L$0+2 (1971Va21) 
S$0.46+2.4 (1971Va21) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 4627 {I5} (1972Cr08); 4629 {I10} (1963Br05) 
L$1+3 (1971Va21) 
S$0.35+1.4 (1971Va21) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 5384 {I6} (1972Cr08); 5384 {I10} (1963Br05) 
L$0+2 (1971Va21) 
S$0.20+0.36 (1971Va21) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$weak, from 1972Cr08; also observed by 1971Va21. Reported with no uncertainty, which was adopted by evaluators (equal to maximum in the dataset) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 6483 {I8} (1972Cr08); 6480 {I14} (1963Br05) 
L$1(+3) (1971Va21) 
S$1.20(+0.89) (1971Va21) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 6644 {I9} (1972Cr08); 6634 {I10} (1963Br05) 
L$(1+)3 (1971Va21) 
S$(0.041),2.2 (1971Va21) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 7388 {I14} (1972Cr08); 7398 {I14} (1963Br05). The 1972Cr08 energy is reported with no uncertainty, which was adopted by evaluators (equal to maximum in the dataset) 


level_energy_unit: KEV
level_comment:
E$weak, from 1972Cr08; reported with no uncertainty, which was adopted by evaluators (equal to maximum in the dataset) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$E2 |DJ=2 |g to 3, 4625 and D |DJ=1 |g to 4+, 4689; 5- in 2005Ma03 
T$mean lifetime |t in ps: 52.9 {I24} (1976Me03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E,J$from Adopted Levels 
T$mean lifetime |t in fs, from DSAM: 465 {I50}; from B(E2)|^ (extracted by evaluators with data shown here): 461 {I30}. Weighted average: 462 {I26} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g}=3 eV 
$(2J+1)|G{-|g}|G{-|a}/|G=9 
$E(|a)(lab)=3250 {I5} 
$Observed by both 1964Va09 and 1965Mc07 
S$from 1964Va08 
$(2J+1)|G{-|g0}|G{-|a}/|G=7.2 eV (1965Mc07) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g}=1.4 eV 
$E(|a)(lab)=3892 {I5} 
$(2J+1)|G{-|g0}|G{-|a}/|G=0.8 eV (1965Mc07) 
J,T$from 1965Mc07 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|G{-|g}=1.5 eV 
$E(|a)(lab)=3908 {I5} 
T$from 1965Mc07 
$(2J+1)|G{-|g0}|G{-|a}/|G=0.1 eV (1965Mc07); (2J+1)|G{-|g1}|G{-|a}/|G=2.0 eV (1967Wi01) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g}=0.6 eV 
$E(|a)(lab)=4042 {I5} 
$(2J+1)|G{-|g0}|G{-|a}/|G=0.9 eV (1965Mc07) 
J,T$from 1965Mc07 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g}=1.0 eV 
$E(|a)(lab)=4104 {I5} 
$(2J+1)|G{-|g0}|G{-|a}/|G=0.9 eV (1965Mc07) 
J,T$from 1965Mc07 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|G{-|g}=2.3 eV 
$E(|a)(lab)=4215 {I5} 
$(2J+1)|G{-|g0}|G{-|a}/|G=4.7 eV (1965Mc07) 
J,T$from 1965Mc07 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t in fs: 1600 {I130} (given by 1975So11 from 1970Gr11, see {+31}P(|a,p|g) dataset) 
$For g.s. decay (1975So11): |G{-|p}/|G(|*\ 10{+-3})=0.38 {I6}, E0 matrix element <M>{-|p}=1.55 {I15} fm{+2}; see also 2005Ki02: q{+2}{-K}(E0/E2)=0.055 {I9}; X(E0/E2)=0.093 {I15}; 10{+3}|*\ |r{+2}(E0)=11 {I3} (E0 refers to 3916.4|g and E2 to 1788.8|g) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
$|G{-|g0}=0.41 eV {I19} 
T$weighted average of 0.4 {I3} (1984Be26) and 0.41 {I25} (1978Be46). According to 1984Be26 this peak could be contaminated with inelastically scattered photons from 10790 level to 2+, 2127 in which case |G{-0}=1.39 eV, and |G{-inelastic}=1.18 eV 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Difference in neutron r.m.s. radii r{-n}({+34}Cl)-r{-n}({+32}Cl): 0.06 {I1} fm (1991Kr06, elastic scattering), 0.062 {I19} fm (1985Gy02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$M{-n}/M{-p}=+1.17 {I9} (1991Kr06); +1.10 {I10} (1987Mo07, from M{-n}=17.1 {I11}, M{-p}=15.5 {I10}); 0.88 {I6} (1984So13) 
$|b{-p}=0.232 {I32}, |b{-n}=0.287 {I32} (1984So13) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|b{-2}(p,p')=0.28 {I1} (1985Al03); 0.24 {I2} (1999Ma63 by reanalysing 1985Al03 data with Becchetti-Greenless optical potential). Other: 1983Iv01 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$2129 {I18} (1968Mo22); 2127 (1991Ke09, 1991Kh06), 
J$from 1991Ke09, 1991Kh06, 1973Go42, 1985SaZS; J=2 from 1985Al03, 1983Iv01, 1975Al28 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$3306 {I14} (1968Mo22); 3303 (1991Ke09, 1991Kh06) 
J$from 1991Ke09, 1991Kh06, 1985SaZS; J=2 from 1985Al03, 1983Iv01 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$4115 {I14} (1968Mo22); 4114 (1991Ke09, 1991Kh06) 
J$from 1991Ke09, 1991Kh06, 1985SaZS; J=2 from 1985Al03 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E,J$from Adopted Levels 
T$mean lifetime |t in fs, from B(E2)|^ (extracted by evaluators with data shown here): 442 {I25} 
$g-factor=+0.50 {I8} (1979Za01) 


level_energy_unit: KEV
level_comment:
E,L$from 1968Mi02 and 1977Pa29 
S$weighted average of 1.06 {I14} and 1.16 {I15} (1977Pa29); others: S{+DW}=1.58, S{+PW}=1.05 (1968Mi02); 1.07 (1967Fa10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E,L$from 1968Mi02 and 1977Pa29 
S$weighted average of 0.34 {I5} and 0.45 {I6} (1977Pa29); others: from 1968Mi02, S{+DW}=0.29 (with no cut-off), S{+DW}=0.36 (with cut-off radius of 4.1 fm), S{+PW}=0.19; 0.358 {I13} (1967Fa10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E,L$from 1968Mi02 
S$from 1968Mi02: S{+DW}=0.87 (adopted), S{+PW}=0.30; others: 0.95 {I3} (1967Fa10) 


level_energy_unit: KEV
level_comment:
S$other: 0.39-0.32,(<0.39) (1968Wi20); none,<0.93 (1962Cu07) 
$Pickup particle: s{-1/2},d{-3/2} (1969Pu03) 


level_energy_unit: KEV
level_comment:
S$other: 1.11-0.99,(<0.78) (1968Wi20, second value for L=(2)) 
$Pickup particle: s{-1/2} (1969Pu03) 


level_energy_unit: KEV
level_comment:
S$other: 0.93-0.86,(<0.42) (1968Wi20, second value for L=(2)) 
$Pickup particle: s{-1/2} (1969Pu03) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
MOMM1$+1.00 {I4} or -1.07 {I4} from 1954Bu05 using Microwave absorption method, negative value is less likely from systematics of odd-A S isotopes 
$ Note that positive sign of 1.07 {I4} value quoted in 2011StZZ seems a misprint 
MOME2$from multiconfigurational Hartree-Fock calculated efg's in 1990Su19, also +0.045 {I10} (1954Bi40) using Microwave absorption method 
J$spin from microwave spectroscopy (1949Co12, 1951We11), parity from L(pol d,p)=2 and L-1/2 from analyzing powers 
T$weighted average of 87.1 d {I12} (1947Hu06), 86.35 d {I17} (1959Co56), 87.16 d {I10} (1958Se49), 88.8 d {I10}(1959Ca12), 89.0 d {I5} (1961Wy01), 87.1 d {I9} (1961Oz01), 87.9 d {I3} (1965Fl02), 87.39 d {I10} (1968Wo06), 87.5 d {I4} (1969La34), 87.38 d {I3} (1999Pa18). Other: 88 d {I3} (1941Ka01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
$A1572.29 3 
$B1574 2.29 PS 35 
$C1572.369 9 
$E1572.92 19 1/2+ 0 0.34 9 
$F1572 1/2+ 0 0.27,0.18 
$G1572.5 41/2+ 1.3 PS GT 
$H1575 10 0+2 
$I1575.1 6 1/2+ 
J$ L(pol d,p)=0 and L+1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
$A1994 
$C1991.28 5 
$E1991.08 16 7/2- 3 0.68 18 
$F1992 7/2- 3 1.16,0.73 
$G1991.7 4 7/2- 1.02 NS 5 
$H1992 10 3+5 
$I1993.1 6 5/2-,7/2- 
J$ L(pol d,p)=3 and L+1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$ L(pol d,p)=1 and L+1/2 from analyzing powers 
T$weighted average of 0.90 ps {I14} in ({+32}S,n|g) and 0.71 ps {I15} in (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
$A3802 
$C3801.949 17 0.08 
$E3801.9 3 1 
$F3802 3/2- 1 0.10,0.08 
$G3802.5 53/2- 25 FS 18 
$I3806.2 8 
J$ L(pol d,p)=1 and L+1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$C4105.6 8 
$E4109 10 
$G4107.5 5 55 FS LT 
$H4114 10 0+2 
$I4110.3 10 
J$ |g's to 3/2+ and L(p,{+3}He)=0+2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$C4189.271 16 0.15 
$E4189.87 26 1 
$F4190 1/2- 1 0.15,0.13 
$G4189.5 4 35 FS LT 
J$ L(pol d,p)=1 and L-1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$C4477.61 7 
$E4481 8 
$F4482 7/2- 3 0.06,0.05 
$G4480.5 4 62 FS LT 
$H4489 10 2 
$I4485.2 6 
J$ |g's to 1/2+ and L(p,{+3}He)=2; J|p=7/2- and L=3 from (pol d,p) presumably erroneous. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$C4903.357 16 0.49 
$E4903.28 16 1/2- 1 0.776 
$F4904 1/2- 1 0.48,0.41 
J$ L(pol d,p)=1 and L-1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$C4963.083 23 0.19 
$E4963.12 16 3/2- 1 0.218 
$F4963 3/2- 1 0.19,0.17 
$H4963 10 (0+2) 
J$ L(pol d,p)=1 and L+1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2-)
level_comment:
E$ level not in 1990En08, but introduced in private communication (S. Raman to P. M. Endt). This level is populated by 1144.6|g from thermal neutron capture state (previously placed from 2717.1 level) and is depopulated by 4268.6|g (previously placed from thermal neutron capture state). 
J$ |g to 1/2+ 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$D8093.0 5 1/2 1 1140.0 5 
$H8103 10 (1+3) 
J$ L(n,n)=1 and R-Matrix analysis of resonances in (n,n) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=162.1 {I1} 
$g|G{-n}=<1 eV; g|G{-n}|G{-|g}/|G=0.42 eV {I1} 
$E{-n}=162.1 {I2} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=313.0 {I8} 
$g|G{-n}=<6 eV; g|G{-n}|G{-|g}/|G=0.31 eV {I3} 
$E{-n}=313.0 {I6} (2006MuZX) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E{-n}(lab)(keV)=396.14 {I4} 
$g|G{-n}=6430 eV {I150}; |G{-|g}=3.08 eV {I20} 
$E{-n}=396.10 {I4} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=463.9 {I4} 
$g|G{-n}=296 eV {I30}; |G{-|g}=0.28 eV {I3} 
$E{-n}=463.9 {I40} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=490.5 {I6} 
$g|G{-n}=50 eV {I10}; g|G{-n}|G{-|g}/|G=0.33 eV {I4} 
$g|G{-n}=50 {I20} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=767.3 {I7} 
$g|G{-n}=<4 eV; g|G{-n}|G{-|g}/|G=0.31 eV {I13} 
$E{-n}=767.3 {I6} (2006MuZX) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-n}(lab)(keV)=798.65 {I6} 
$g|G{-n}=25350 eV {I300}; |G{-|g}=1.52 eV {I50} 
$E{-n}=798.65 eV {I60}; g|G{-n}=2535 eV {I300} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=930.0 {I12} 
$g|G{-n}=<20 {I}; g|G{-n}|G{-|g}/|G=0.57 eV {I25} 
$E{-n}=930.0 {I6} (2006MuZX) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-n}(lab)(keV)=935.78 {I6} 
$g|G{-n}=4100 eV {I160}; |G{-|g}=3.48 eV {I23} 
$|G{-|g}=0.348 eV {I230} (2006MuZX) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-n}(lab)(keV)=997.9 {I1} 
$g|G{-n}=930 eV {I80}; |G{-|g}=3.51 eV {I19} 
$E{-n}=997.90 {I6}; g|G{-n}=4100 eV {I160}(2006MuZX) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-n}(lab)(keV)=1017.7 {I1} 
$g|G{-n}=4020 eV {I180}; |G{-|g}=1.22 eV {I17} 
$E{-n}=1017.70 {I6} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=1449.6 {I3} 
$g|G{-n}=3025 eV {I260} 
$E{-n}=1449.6 {I4}; g|G{-n}=30250 eV {I260} (2006MuZX) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)(keV)=1475.5 {I4} 
$g|G{-n}=3795 eV {I340} 
$E{-n}=1475.5 eV {I13}; g|G{-n}=37950 eV {I340} (2006MuZX) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
E$weighted average from 1970Bu18, 1972Fr11 and 1975VaYG 
T$weighted average from 1970Bu18 and 1972Fr11 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
S$from multi-dimensional fit to the data to account for L=1 transfer to the 3.22 MeV state in {+33}S (2024Ku24) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$ spin measurement by microwave spectroscopy (1949Lo21) 
$ Nuclear rms charge radius=3.2982 fm {I21} (2004An14 evaluation); 3.2985 fm {I24} from 2008 update of 2004An14 
$ Mean radius r{-0}{+2}=1.26 fm{+2} {I10} from measured integrated |s{-R}=2.44 b {I19} at 46.17 MeV/nucleon in Si({+36}S,X) reaction (1999Ai02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$ from DSA in Coul. Ex. (2008Sp01). Other: 76 fs {I21} (1972Sa09), also given in 2001Ra27 evaluation 
J$ E2 |g to 0+ 
MOMM1$ transient field technique in Coulomb excitation in inverse kinematic reaction, g factor=+1.3 {I5} (2008Sp01) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$B(E3)=0.008 {I3} (2002Ki06 evaluation), from |b{-3} in (p,p') (1990Ho19) 
T$ from DSA in Coul. Ex. (2008Sp01). Other: 0.8 ps {I+4-3} (DSA in (t,p|g) (1972Sa09) 
MOMM1$ transient field technique in Coulomb excitation in inverse kinematic reaction, g factor=+0.8 {I5} (2008Sp01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$too short to be measured with the present setup for the lifetime range of 1 ps to 100 ps (2022Gr07) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
T$weighted average of 5.04 min {I2} (1946Bl01), 5.07 min {I1} (1959El41), and 4.99 min {I2} (1974Li09). 
J$ L(d,p)=3, L+1/2 from A{-y}(|q) in (pol d,p) 
$ Mean energy-integrated reaction cross section=2.26 b {I14}, r{+2}{-0}=1.16 fm{+2} {I7} (1999Ai02) in Si({+37}S,X) at 45 MeV/nucleon 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$ L(d,p)=(1,2), L+1/2 for L=1 and L-1/2 for L=2 preferred over L-1/2 and L+1/2, respectively from A{-y}(|q) in (pol d,p) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2+)
level_comment:
J$ L(d,p)=(1,2), L-1/2 for L=1 and L+1/2 for L=2 preferred over L+1/2 and L-1/2, respectively from A{-y}(|q) in (pol d,p) 


level_energy_unit: KEV
level_spin_parity: (5/2-,9/2+)
level_comment:
J$ L(d,p)=(3,4), L-1/2 for L=3 and L+1/2 for L=4 preferred over L+1/2 and L-1/2, respectively from A{-y}(|q) in (pol d,p) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
L$ 3 (1984Th08,1984Pi03) 
$ d|s/d|W=10.35 mb/sr 
$ (2J+1)S=6.2 (1984Th08), S=0.92 for 7/2 (1984Pi03). 
$ Evaluated S=0.88 {I12} (2005Ts03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
L$ 1 (1984Th08,1984Pi03) 
$ (2J+1)S=2.6 (1984Th08), S=0.7 for 3/2 (1984Pi03) 
$ S=1.45 for 1/2 (1984Pi03) 
$ d|s/d|W=7.13 mb/sr 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
L$ 2 (1984Th08,1984Pi03) 
$ (2J+1)S=0.22 (1984Th08), S=0.053 for 3/2 (1984Pi03) 
$ S=0.028 for 5/2 (1984Pi03) 
$ d|s/d|W=0.292 mb/sr 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
L$ 1 (1984Th08,1984Pi03) 
$ (2J+1)S=0.15 (1984Th08), S=0.075 for 3/2 (1984Pi03) 
$ S=0.155 for 1/2 (1984Pi03) 
$ d|s/d|W=0.425 mb/sr 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
L$ (3) (1984Th08,1984Pi03) 
$ (2J+1)S=0.14 (1984Th08), S=0.068 for 5/2 (1984Pi03) 
$ S=0.034 for 7/2 (1984Pi03) 
$ d|s/d|W=0.303 mb/sr 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
L$ 1 (1984Th08,1984Pi03) 
$ (2J+1)S=1.54 (1984Th08), S=0.83 for 1/2 (1984Pi03) 
$ S=0.40 for 3/2 (1984Pi03) 
$ d|s/d|W=3.41 mb/sr 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
L$ 1 (1984Th08,1984Pi03) 
$ (2J+1)S=0.60 (1984Th08), S=0.14 for 3/2 (1984Pi03) 
$ S=0.29 for 1/2 (1984Pi03) 
$ d|s/d|W=1.09 mb/sr 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
L$ >0 (1984Th08), 1 (1984Pi03) 
$ S=0.029 for 3/2, 0.061 for 1/2 for L=1 (1984Pi03) 
$ d|s/d|W=0.280 mb/sr 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
L$ >1 (1984Th08), 3 (1984Pi03) 
$ S=0.061 for 7/2 (1984Pi03) 
$ S=0.118 for 5/2 (1984Pi03) 
$ d|s/d|W=0.432 mb/sr 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
L$ (1) (1984Th08) 1 (1984Pi03) 
$ (2J+1)S=0.28 (1984Th08), S=0.084 for 3/2 (1984Pi03) 
$ S=0.172 for 1/2 (1984Pi03) 
$ d|s/d|W=0.416 mb/sr 


level_energy_unit: KEV
level_comment:
$|s=40.0 mb/sr at 10|' in ({+14}C,{+13}C) 
E$ from ({+18}O,{+17}O|g). Other: 662 {I15} in ({+14}C,{+13}C) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
$f{-5/2} orbital 
E,J,S$from literature, three states centered around 5.6 MeV, all of J|p=5/2- (see Adopted Levels of {+37}S in ENSDF database) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
$Configuration=|n[(1d{-3/2}){+4}(1f{-7/2}){+1}]~# |p[(1d{-5/2}){+6}(2s{-1/2}){+1}(1d{-3/2}){+1}]; 70% amplitude 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
$Configuration=|n[(1d{-3/2}){+4}(1f{-7/2}){+1}]~# |p[(1d{-5/2}){+6}(2s{-1/2}){+1}(1d{-3/2}){+1}]; 76% amplitude. This strongly populated level in this work is also interpreted as |n(1f{-7/2}){+1}~#(first 2+ in {+36}S) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$A previously proposed 1239 transition from 3262 level to 2023 level, with an expected relative intensity of 1.6 was not seen by 2016Ch14 
$Configuration=|n[(1d{-3/2}){+4}(1f{-7/2}){+1}]~# |p[(1d{-5/2}){+6}(2s{-1/2}){+1}(1d{-3/2}){+1}]; 45% amplitude 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)
level_comment:
$Configuration=|n[(1d{-3/2}){+4}(1f{-7/2}){+1}]~# |p[(1d{-5/2}){+6}(2s{-1/2}){+1}(1d{-3/2}){+1}] for J|p=9/2-; 78% amplitude 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
J$(7/2)- is given Fig. 5 of 2016Ch14, but (7/2,9/2) in authors' Table II. In {+37}S Adopted Levels in the ENSDF database, J|p=(7/2)- 
$Configuration=|n[(1d{-3/2}){+4}(1f{-7/2}){+1}]~# |p[(1d{-5/2}){+6}(1d{-3/2}){+2}] for J|p=7/2-; 34% amplitude 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)
level_comment:
J$(1/2-,3/2+) was assigned based on L(d,p)=(1,2) in {+37}S Adopted Levels in the ENSDF database. But in the present work 3605|g to 7/2- g.s. is inconsistent with 1/2- or 3/2+. Either there is a disagreement in J|p assignments or the level in (d,p) is different from the one reported here, although the level energies are in excellent agreement 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$from the observation of only the component corresponding to |g rays after passage of the {+37}Si recoils through the setup for lifetime range of 1 ps to 100 ps (2022Gr07) 


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$from the observation of only the component corresponding to |g rays before passage of the {+37}Si recoils through the setup for lifetime range of 1 ps to 100 ps (2022Gr07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$weighted average of 172 min {I1} (1958Ne10), 169.6 min {I7} (1971En01), and 170.0 min {I8} (1972Vi11). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2 from 0+ 
T$from B(E2)|^=0.0235 {I30} in Coulomb excitation (1996Sc31). Other: >0.31 ps from DSAM in (t,p|g) 
MOMM1$from g=+0.13 {I5} (2006St21,2006Da08: high-velocity transient-field technique in Coulomb excitation). Compilation: 2014StZZ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
J$1513|g to 2+; 0 and 4 less likely from RUL; shell-model predicts 2+ (1994Fo04) in {+160}Gd({+36}S,{+38}S|g) 
T$from DSAM in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: S
level_comment:
J$log| {Ift}=5.06 to 5/2- in {+39}Cl; systematics of g.s. J|p=7/2- for N=23 isotones; probable |pf{-7/2}{+3} configuration (1989Dr03); 7/2- from shell-model calculations (2016Ch33) 
J$ 1990En08 QUOTED (3/2,5/2,7/2)- FROM LOGFT=5.1 TO 5/2- 
T$from 1980Hi01. 


level_energy_unit: KEV
level_comment:
E$compiler considers E=3309 given by 2019Ab06 to be a typo, as both energy sum of 3110|g depopulating this level and feeding the 398 level and scale of energy in the drawing of Figure 12 - suggest the energy is 3509. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
MOMM1$from measured g-factor=-0.01 {I6} using transient field technique in Coulomb excitation (2006Da08) 
J$Coulomb excited from 0+ 
T$deduced by evaluator from measured B(E2) by 1996Sc31 in Coulomb excitation and adopted E|g=903.68 {I9} 
$|b{-2}(p,p')=0.35 {I5} (1999Ma63), |b{-2}(Coul. ex.)=0.284 {I16} (1996Sc31) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$1013.17|g to 2+; probable member of 2-phonon triplet. J|p=0+ is not excluded but similarity with {+42}Ar states suggests 4+ is more likely 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$ (2+) assigned by 2001Wi21 in {+40}P |b{+-} decay based on probable member of 2-phonon triplet, but J=(4+) from |g-ray anisotropy in {+9}Be({+48}Ca,X|g) (2002So14) and from yrast band structure in {+208}Pb({+36}S,X|g) (2010Wa12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_comment:
E$from {+208}Pb({+36}S,X|g) (2010Wa12) 
J$2010Wa12 proposed J|p=(6+) for this level with J|p=(4+) for 2255 level based on band structure. However, 2001Wi21 in {+40}P |b{+-} decay propose J|p=(2+) for the 2255 level. 


level_energy_unit: KEV
level_comment:
J$suggested by 2001Wi21 in {+40}P |b{+-} decay as possible member of 3-phonon triplet since the level decays to members of 2-phonon triplet 


level_energy_unit: KEV
level_comment:
J$suggested by 2001Wi21 as possible member of 3-phonon triplet since the level decays to members of 2-phonon triplet 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$1356|g(|q) allows 0+, 2+ and 4+; but 0+ is ruled out by |g to 0+ in Adopted Gammas; fragmentation reaction used by 2002So14 favors yrast states. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$from E|g (1996Sc31) 
J$Coulomb excited from 0+ 
T$deduced by evaluator from measured B(E2) in 1996Sc31 and adopted E|g=903.68 {I9} in Adopted Gammas. 
$g-factor=-0.01 {I6} (2006Da08) 
MOMM1$from measured g-factor=-0.01 {I6} using transient field technique (2006Da08) 


level_energy_unit: KEV
level_lifetime_unit: S
level_comment:
T$from 1998WiZV. Other: 2.6 s {I14} (1995ReZZ) 
J$(7/2-) predicted by particle-rotor model calculations (1999Ib01), (5/2-) predicted by shell model calculations (2011Wa13). 


level_energy_unit: KEV
level_comment:
J$(5/2-) predicted by particle-rotor model calculations (1999Ib01), (7/2-) predicted by shell model calculations (2011Wa13). 
BE2$assigned as E2 transition by 1999Ib01 based on systematics of transition strengths in this mass region; E1 transition cannot be ruled out. 


level_energy_unit: KEV
level_comment:
J$(9/2-) proposed in 1999Ib01 based on particle-rotor model calculations 
BE2$assigned as E2 transition by 1999Ib01 based on systematics of transition strengths in this mass region; E1 transition cannot be ruled out. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
J$(11/2-) proposed by 2011Wa13 based on population characteristics of multi-nucleon transfer reactions 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
%B-N$<4 (1995So03), but none observed by 1998WiZX 
$Theoretical T{-1/2}=2.5 s, %|b{+-}n=1.5 (2003Mo09) 
$Theoretical T{-1/2}=1.26 s, %|b{+-}n=7.2 (2016Ma12) 
T$weighted average of 1.013 s {I15} from 1998WiZX and 1.03 s {I3} from 2006Wi10. Other: 0.56 s {I6} (1995So03) 
$Mean radius r{+2}{-0}=1.251 fm{+2} {I25} (2006Kh08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=20.6 ps {I15}(stat) using recoil-distance method (2017Pa02). This value can be compared with T{-1/2}=11.9 ps {I20}, deduced from B(E2)=0.0397 {I63} in Coul. ex. (1996Sc31) and E|g=903 keV 
$Measured probability ratio of reactions induced by the target versus by the degrader was 1.30 {I10} (2017Pa02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from |t=21.5 ps {I+11-9} measured by recoil distance method. The quoted uncertainty in 2018Mi07 is probably statistical only, considering that a 17% systematic uncertainty is added for their halflife measurements of excited states in {+43}S in the same experiment. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
$Configuration=|np{-3/2}. This state is found to be part of well deformed K=1/2 decoupled rotational band from shell-model calculations 
J$3/2- proposed from shell-model (2000Sa21,2009Ri11,2009Ga05); 7/2- proposed (1999Ib01) from syst. 
T$weighted average of 282 ms {I27} (2004Gr20) and 260 ms {I15} (1998WiZV), from |b({+43}S) time correlation measurements. Other: 220 ms {I+80-50} (1989Le16) 
$Measured mean-square radius (r{+2}{-0})=1.22 fm{+2} {I6} (2006Kh08) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
T$from 2009Ga05. Other: 0.48 |ms {I5} (2000Sa21) 
J$7/2- proposed from shell-model calculations (2000Sa21); also from agreement of g(Schmidt)=-0.546 for |nf{-7/2} with the experimental value (2009Ga05). 
MOMM1$from g factor=-0.317 {I4} (2009Ga05) by TDPAD method, the uncertainty includes the statistical and that in the magnetic field. 
MOME2$TDPAD method (2012Ch16). This value is significantly larger than predicted by single-particle state which suggests that the isomer is not a spherical state (2012Ch16), only the magnitude is known, not the sign 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$probably a multiplet. B(E2) applies to the sum of unresolved levels. Experimental B(E2) is consistent with calculated B(E2) for a multiplet of states generated near 1 MeV in either the particle-rotation (prolate and oblate) or the particle-vibration calculations, assuming J|p(g.s.)=7/2- 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$3/2- proposed from shell-model calculations (2000Sa21,2009Ga05). 
$Configuration=|np{-3/2}. This state is found to be part of well deformed K=1/2 decoupled rotational band from shell-model calculations (2009Ga05). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: US
level_comment:
J$from agreement of g(Schmidt)=-0.546 for |nf{-7/2} with the experimental value (2009Ga05) 
T$from 2009Ga05, from time interval between an event in plastic scintillator and a signal in one of the Ge detectors. Others: 0.45 |ms {I5} (2000Sa21), 0.20 |ms {I+14-7} (2012Ka36). 
MOMM1$from g factor=-0.317 {I4} (2009Ga05) by TDPAD method, the uncertainty includes the statistical and that in the magnetic field. 2009Ga05 state that their g factor indicated that 320.5, J=7/2- level is built on |nf{-7/2} orbital 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: PS
level_comment:
T$from |t=7.8 ps {I+14-13}(stat) {I+13-16} (syst) in 2018Mi07, with statistical and systematic uncertainties added in quadrature. 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: PS
level_comment:
T$from |t=6.2 {I+14-13}(stat) {I13} (syst) in 2018Mi07, with statistical and systematic uncertainties added in quadrature. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$assignment taken from the literature, also predicted in the shell-model calculations by 2020Mo32 
$Exclusive |s=12 mb {I4} 
$Inclusive |s=91 mb {I4} 
S$for configuration=|n2p{-3/2} 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$Level and J|p proposed based on shell-model predictions (2020Mo32) 
$Exclusive |s=0.4 mb {I1} 
S$for configuration=|n2p{-1/2} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
E$320 in 2020Mo32, with no uncertainty 
$Exclusive |s=43 mb {I3} 
S$for configuration=|n1f{-7/2}{+-1} 
T$measured by 2020Mo32, from decay curve of {+43}S implants. Authors compare this value to 415 ns {I5} in 2009Ga05 (Phys. Rev. Lett. 102, 092501), 0.20 |ms {I+14-7} in 2012Ka36 (Phys. Rev. C 86, 054319), and 0.45 |ms {I5} in 2000Sa21 (Phys. Rev. Lett. 84, 5062) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$Placement in the present work as also in 2009Ri11, whereas it was placed from 1161 level in 2018Mi07, i.e. the ordering of the 977-185 |g cascade is reversed in 2020Mo32 from that in 2018Mi07, based on the measured |g-ray intensities. 
$Exclusive |s=1.2 mb {I6} 


level_energy_unit: KEV
level_comment:
J$possible J|p=5/2- as discussed in text by 2020Mo32 
E$1780 {I5} in 2020Mo32 
$Exclusive |s=0.0 mb {I4} 


level_energy_unit: KEV
level_spin_parity: 3/2+,(5/2+)
level_comment:
J$momentum distribution of this state could only be reproduced by assuming removal of a neutron from the 1d{-3/2} orbital 
$Exclusive |s=8.8 mb {I4} 
S$for configuration=|n1d{-3/2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$unweighted average of 125.5 ms {I25} in (implants)|b-decay curve and 119 ms {I6} in (implants)|b|g-decay curve (2022Tr03); 100 ms {I1} in (implants)|b-decay (2004Gr20,2003Gr22); 123 ms {I10} in (implants)|b-decay (1995So03,1993So06). Other: 200 ms {I+50-30} (1989Le16). 
%B-N$unweighted average of 40 {I5} (2022Tr03, |b and |g decay of {+44}S and its descendants in the decay chain at NSCL-MSU); 18 {I3} (1993So06, also 1995So03); and 30 {I10} (1989Le16). The values from 1993So06 and 1989Le16 are from (implants)|b-n-coin in two different reactions at GANIL. 
$Measured mean square radius (r{+2}{-0})=1.62 fm{+2} {I17} (2006Kh08). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$weighted average of 0.0221 {I28} (2021Lo08) and 0.0314 {I88} (1997Gl02) in Coulomb excitation 
J$level excited from 0+ in Coulomb excitation. 
T$deduced from adopted B(E2). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
J$E0 transition to 0+. 
T$from time distribution of 1362.5 electron peak in {+9}Be({+48}Ca,X|g) (2010Fo04). 


level_energy_unit: KEV
level_comment:
J$2002So14 in ({+48}Ca,X|g) proposed (0+) tentatively, but only one excited 0+ at |?1365 is seen in other studies (2011Sa25,2005Gr30), and predicted by shell-model calculations in this energy region. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$level defined in 2011Sa25 through the tentative placement of 1891-keV |g ray. Existence of this level is based on finding of a 2.6-|ms isomer at 1365 keV (2010Fo04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$|s=0.022 {I4} 
T$recoil-distance method (2017Pa02), only an upper limit estimated from observation of only one peak for 949|g, indicative of a prompt transition, in contrast to the 1140 and 1319 |g rays, both of which show two distinct peaks 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
$|s=0.019 {I4} 
T$measured mean lifetime |t=76 ps {I14}(stat) {I20}(syst) using recoil-distance method (2017Pa02). The two uncertainties have been added in quadrature by evaluators 
$Based on experimental B(E2)(W.u.) value, the 4+ level is interpreted by 2017Pa02 as an isomer with K|p=4+, and not as a member of the ground-state rotational band. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M
level_comment:
$Values of B(E2) from 1329,2+ to 1365 level and |r{+2} for E0 transition are the lowest in this mass region which suggests weak mixing between the g.s. and the 0+ isomer and shape coexistence. Comparison with full {Isd(fp)} shell-model calculations shows consistency with the experimental data. 
T$from time distribution of 1362.5 electron peak (2010Fo04). Other: 2.3 |ms {I3} from ce(t) (2005Gr30) 


level_energy_unit: KEV
level_comment:
J$2002So14 proposed (0+) tentatively, but excited 0+ at 1365 keV is reported by 2005Gr30. Only one excited 0+ is predicted by shell-model calculations in this energy region which most likely corresponds to 1365 level 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
J 2003Au02 suggest 3/2+ based on systematics. 
T from 2004Gr20. Other: 82 ms {I13} (1995So03). 
%B-N From 1995So03. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$Inclusive |s=2.6 mb {I1} for one-proton removal, derived from yield of {+45}S reaction products and number of incoming {+46}Cl projectiles, 5% systematic uncertainty has been added in quadrature 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$ comparison with shell-model calculations, systematics of even-even nuclei 
$ Population=63% {I12} from efficiency-corrected peak areas 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
T$ >200 ns, estimated from time of flight in 1990Le03. Other: 10 ms (2021Ko27, syst) 
$ Theoretical T{-1/2}=13.9 ms (2019Mo01), 21.0 ms (2016Ma12) 
$ Theoretical %|b{+-}n=77, %|b{+-}2n=8 (2019Mo01) 
$ Theoretical %|b{+-}n=32, %|b{+-}2n=3.8, %|b{+-}3n=6.4 (2016Ma12) 


level_energy_unit: KEV
level_comment:
$Only the |b{+-} decay mode is expected, followed by delayed neutron decays, thus 100% |b{+-} decay is assigned by inference. However, S(n)=70 {I300} (syst, 2021Wa16) and 30 keV (theory, 2019Mo01) suggests this nuclide on the margin of being stable towards one-neutron emission. 
$A total of five events were assigned to {+49}S, one event each with tuned setting of the spectrometer for {+53}Cl and {+57}K, and three events for setting on {+54}Ar (2018Ta17). 
$Theoretical T{-1/2}(|b)=4.0 ms, %|b{+-}n=31, %|b{+-}2n=14, %|b{+-}3n=1, %|b{+-}4n=0, %|b{+-}5n=0 (2019Mo01) 
$Theoretical T{-1/2}(|b)=12.4 ms, %|b{+-}n=27.4, 26.8; %|b{+-}2n=22.2, 24.2; %|b{+-}3n=2.1, 2.0; %|b{+-}4n=0.026, 0.023; %|b{+-}5n=0 (2021Mi17); two values for a decay mode refer to different fission barriers. 
$The observed events are assumed to correspond to the ground-state of {+49}S 
T$half-life of the {+49}S activity has not been measured. It is expected to be greater than the time-of-flight through the beam transport system, which may be about 500 ns. From systematics of half-lives of neighboring S isotopes, the half-life is expected to be <25 ms from 50 ms for {+46}S, 68 ms for {+45}S, 117 ms for {+44}S and 265 ms for {+43}S, assuming a decreasing trend of half-life as neutron number increases in neutron-rich nuclei. From systematics, T{-1/2}=4 ms in 2021Ko07. 
J$5/2- (2019Mo01, theory); 1/2- (syst, 2021Ko07) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
$Decays to ground state of {+28}S (2015Mu13) 
E$the ground state is deduced at E(p)=1.8 MeV {I1} (2015Mu13) 
T$<20 ns from 1996PoZZ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_comment:
$Decays to ground state and first 2+ state of {+28}S (2015Mu13) 
E$from E(p)=1.8 MeV and 2.3 MeV peaks in proton spectrum (2015Mu13) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
$Decays to ground state of {+28}S 
E$the ground state is deduced at E(p)=1.8 MeV {I1} from analysis of peak #1 in Figure 3 of 2015Mu13, implying S(p)({+29}Cl)=-1.8 MeV {I1} i.e. ground state is unbound towards 1p emission. Note that in 2012Wa38, S(p)=-2410 {I430} from systematics. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_comment:
$Decays to ground state and first 2+ state of {+28}S 
E$the excited state is deduced from the analysis of peak #1 with E(p)=1.8 MeV and peak #2 with E(p)=2.3 MeV in Figure 3 of 2015Mu13. This energy difference is similar to energy difference calculated by applying a Thomas-Ehrman shift to energy levels in isobaric mirror nuclide, {+29}Mg. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
$Decays by p decay to {+28}S ground state 
$From analysis of proton distribution spectrum from 2p decays of {+30}Ar 
E$the ground state is deduced at E(p)=1.8 MeV {I1} from analysis of peak "A" in Fig. 7 of 2018Xu04 (also peak #1 in authors' Fig. 9), implying S(p)({+29}Cl)=-1.8 MeV {I1} i.e. ground state is unbound towards 1p emission. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$This state decays by p decays to the ground state and first excited 2+ state of {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 0.50 MeV {I14}, deduced from E(p)=2.3 MeV {I1} in {+29}Cl+p in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by p decay to the ground state of {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 1.1 MeV {I+2-3}, deduced from E(p)=2.9 MeV {I+2-3} in {+29}Cl+p in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by p decay to the ground state of {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 1.7 MeV {I+4-3}, deduced from E(p)=3.5 MeV {I+4-3} in {+29}Cl+p in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by p decay to the ground state of {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 2.1 MeV {I+6-5}, deduced from E(p)=3.9 MeV {I+6-5} in {+29}Cl+p in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by p decay to the ground state of {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 3.5 MeV {I+7-4}, deduced from E(p)=5.3 MeV {I+7-4} in {+29}Cl+p in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
T > 100 ns, estimated value in 2018Mu18, based on the Thomas-Ehrman shift, from 3+ {+30}Al g.s. to the 3+ g.s. of {+30}Cl, for E{-r}= 50-150 keV and their experimental setup. 
J$also from systematics 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$from the difference between the measured E{-T}(1p) of this state and that of g.s. 
$E{-T}(1p)=617 {I35}, 1p decay to g.s. of {+29}S 
$Population ratio of 253 level to g.s. is 0.585 {I22}/0.415 {I16} (2022Gi04) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
T T{-1/2} > 100 ns, estimated in 2018Mu18 based on the Thomas-Ehrman shift, from 3+ {+30}Al g.s. to the 3+ g.s. in {+30}Cl, of E{-r}= 50-150 keV and conclude that for such low decay energies, the {+30}Cl g.s. should live a sufficiently long time to survive the flight through the second achromatic stage of the FRS fragment separator (of |?150 ns). 
$E{-r}(c.m.)=480 keV {I20} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
$%|ep is deduced by the evaluators from {+31}Cl to {+31}S decay scheme based on |g and proton data from 2011SaZM. Other: %|ep=0.65 {I5} from 2006Ka11 is in disagreement 
J$log| {Ift}=4.94 to 1249, 3/2+ and log| {Ift}=4.44 to 2235, 5/2+ levels in {+31}S. Some evidence of |b{++} feeding (log| {Ift}=5.5) to 8509, 1/2+ level in {+31}S. Also mirror state of {+31}Si g.s., 3/2+, and evidence of strong |e+|b{++} feeding of 6280, 3/2+ (lowest T=3/2 state) in {+31}S which is identified as the IAS of the {+31}Cl g.s. 
T$from mass-separated {+31}Cl and 17 different runs (2011SaZM). Other: 150 ms {I+25-20} (1982Ay01, yield ratios with different counting windows used) 
$Dominant d-wave component for the valence proton in {+31}Cl deduced from the measured momentum distribution and Glauber analysis in {+12}C({+31}Cl,{+30}S) reaction (2011Fu11) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$weighted average of 726 {I16} (2016Ka15) and 782 {I32} (2014La09). Other: 745 {I16} (2009Wr03, IMME analysis) 
$E(level)=726 {I16} from measured E(p)(lab)=446 keV {I15} (E(p)(c.m.)=461 {I15} (1998Ax02, from {+31}Ar decay) and measured S(p)=264.6 {I34} (2016Ka15). Others: 782 {I32} (measured by 2014La09); 745 {I16} from IMME analysis by 2009Wr03 
$Resonance energy E(p)=472 keV {I14} as average of measured values of E(p)(lab)=446 {I15} or E(p)(c.m.)=461 {I15} (1998Ax02); and E(p)(c.m.)=517 {I32} (from level energy=782 {I32} in 2014La09 and S(p)=264.6 {I34} from 2016Ka15). Evaluators obtain a weighted average of 471 {I22} from the two values. 
$E(level)=782 {I32} (2014La09, from excitation spectrum in Pb({+31}Cl,{+31}Cl'). First excited state of {+31}Cl is expected to be 1/2+ at approximately 750 keV as a mirror state of {+31}Si known at 752.23 keV. In 1998Ax02 a very weak proton group from {+31}Ar decay was proposed at 446 {I15} leading to excited state in {+31}Cl at 740 {I50}, but in their later paper 2000Fy01 this peak was not discussed and the low energy portion of the proton spectrum in 1998Ax02 was ascribed mostly to delayed two proton decay. 
J$from shell-model predictions (2014La09), and mirror analogy to 752.23, 1/2+ level in {+31}Si 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E$from measured E(p)(lab)=1416 keV {I2} or E(p)(c.m.)=1463 {I2} (2000Fy01) and S(p)=264.6 {I34} (2016Ka15). Others: 1793 {I26} (measured by 2014La09); 1746 {I7} from IMME analysis (2009Wr03); 1746 {I5} from |e decay of {+31}Ar, 1749 {I5} (1998Ax02), 1820 (1992Ba01) 
$Resonance energy E(p)=1464 keV {I2}, as average of measured values of E(p)(lab)=1416 {I2} or E(p)(c.m.)=1463 {I2} (2000Fy01) and E(p)(c.m.)= 1528 {I26} (from level energy=1793 {I26} in 2014La09 and S(p)=264.6 {I34} from 2016Ka15). Evaluators obtain a weighted average of 1463 {I5} from the two values. 
J$(5/2+) from shell-model predictions (2014La09) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=3634 {I3} to g.s. in {+30}S, I(p)=6.1 {I8}; E(p)=1504 {I2} to 2211 level, I(p)=6.2 {I2} 
E$others: 4030 9, 4049 10 (1998Ax02), 4060 (1992Ba01) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=3020 {I3} to 2211 level in {+30}S, I(p)=1.08 {I14}; E(p)=1870 {I3} to 3403 level, I(p)=0.8 {I2} 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=5276 {I5} to g.s. in {+30}S, I(p)=17.6 {I3}; E(p)=3153 {I4} to 2211 level, I(p)=0.44 {I10}; E(p)=2008 {I2} to 3403 level, I(p)=10.0 {I2} 
E$ other: 5742 7, 5765 10 (1998Ax02), 5790 (1992Ba01) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=6049 {I9} to g.s. in {+30}S, I(p)=0.51 {I12}; E(p)=3902 {I3} to 2211 level, I(p)=2.22 {I14} 
E$ other: 6550 (1992Ba01) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)+
level_comment:
$E(p)=6145 {I7} to g.s. in {+30}S, I(p)=0.51 {I12}; E(p)=4030 {I3} to 2211 level, I(p)=7.0 {I2}; E(p)=2881 {I3} to 3403 level, I(p)=0.99 {I13}; E(p)=1211 {I4} to 5136 level, I(p)=1.7 {I5}; E(p)=1131 {I5} to 5217 level, I(p)=2.7 {I16} (connected with two-proton decay) 
$Others: 6663 5, 6658 6 (1998Ax02), 6674 9 (1998Ax01) 
E$other: 6674 {I6} (2014Ko17) 
$pp(|q): A{-2}=-0.12 {I14} (2014Ko17) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)
level_comment:
$E(p)=1300 {I13} to 5217 level in {+30}S, I(p)=0.70 {I11} (connected with two-proton decay) 
$ ^I(p)=0.7 11 listed in table 2 of 2000Fy01 seems a misprint, the evaluators have assumed 0.70 instead of 0.7 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=4730 {I5} to 2211 level in {+30}S, I(p)=1.68 {I18}; E(p)=3561 {I11} to 3403 level, I(p)=3.6 {I8}; E(p)=1819 {I3} to 5217 level, I(p)=3.0 {I4} (connected with two-proton decay) 
E$other: 7380 {I6} (2014Ko17) 
$pp(|q): A{-2}=+0.16 {I11} (2014Ko17) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=6950 {I9} to g.s. in {+30}S, I(p)=0.70 {I9}; E(p)=3432 {I3} to 3668 level, I(p)=0.89 {I11}; E(p)=1923 {I3} to 5217 level, I(p)=0.44 {I14} (connected with two-proton decay) 
E$ Other: 7478 13 (1998Ax02) 
E$other: 7512 {I7} (2014Ko17) could be a different level considering the unmatched energy 
$pp(|q): A{-2}=+0.35 {I19} 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$from 2014Ko17 only, based on measured proton decay to 5217 {I3} level in {+30}S; not reported in 2000Fy01 
$pp(|q): A{-2}=+0.48 {I19} (2014Ko17) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E(p)=8860 {I19} to g.s. in {+30}S, I(p)=0.22 {I19}; E(p)=3806 {I4} to 5217 level, I(p)=0.53 {I13} (doubly placed divided I(p) given) 
E$other: 9434 {I9} (2014Ko17) 
$pp(|q): A{-2}=+0.04 {I19} (2014Ko17) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$ Others: 12313 {I14} (1998Ax02), 12340 (1992Ba01) 
E$IAS of {+31}Ar ground state. Other: 12314 {I4} (2014Ko17) 
$E(p)=11654 {I28} to g.s. in {+30}S, I(p)=0.27 {I4}; E(p)=9493 {I20} to 2211 level, I(p)=0.30 {I4}; E(p)=8347 {I15} to 3403 level, I(p)=0.51 {I6}; E(p)=8092 {I14} to 3670 level, I(p)=0.25 {I4}. Branches connected with two-proton decay: E(p)=6540 {I8} to 5217 level in {+30}S, I(p)=0.84 {I11}; E(p)=6386 {I7} to 5389 level, I(p)=0.26 {I5}; E(p)=5952 {I7} to 5842 level, I(p)=0.19 {I6}; E(p)=5632 {I6} to 6202 level, I(p)=0.37 {I9}; E(p)=4389 {I5} to 7485 level, I(p)=0.59 {I11}; E(p)=4289 {I4} to 7598 level, I(p)=0.31 {I8}; E(p)=4200 {I4} to 7693 level, I(p)=1.09 {I18}; E(p)=3806 {I4} to 8077 level (doubly placed). 
$Contribution from delayed two-proton branches to {+29}P (I(p) given as absolute intensity): %I(p)=1.86 {I21} for Q{-2p}=7620 {I5} (to g.s. in {+29}P); %I(p)=1.07 {I13} for Q{-2p}=6246 {I2} (to 1383.55 level in {+29}P); %I(p)=0.75 {I10} for Q{-2p}=5679 {I3} (to 1953.91 level in {+29}P); %I(p)=0.22 {I5} for Q{-2p}=5223 {I5} (to 2422.7 level in {+29}P) 
$pp(|q): A{-2}=+0.03 {I18} (2014Ko17) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MS
level_comment:
J$L({+3}He,t)=2 from 0+; allowed |e feedings to 0+ (E=3379) and 2+ (E=2231) states in {+32}S 
T$from 1968Ar03. Others: 281 ms {I8} (1971Go18), 300 ms (1969St14), 294 ms {I6} (1966An01), 306 ms {I4} (1953Gl32), 320 ms {I10} (1954Br12), 0.28 s (1954Ty33). 
MOMM1$|b-NMR spectroscopy on polarized {+32}Cl nuclei obtained from fragmentation of 100 MeV/nucleon {+36}Ar beam with {+93}Nb target at NSCL facility (2000Ro30). Positive sign is predicted by shell-model calculations. 
$%|ep and %|e|a from 1979Ho27 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$L({+3}He,t)=2 from 0+; allowed |e feeding (log {Ift}=3.9) from 0+ parent; 1+ for 1149-keV level in {+32}P mirror nucleus (1994Vo12) 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E$1331.2 {I5} from ({+3}He,t) 
J$L({+3}He,t)=2 from 0+; 2+ from comparison of |s(|q) data with CDE calculations in ({+3}He,t) (1989Je07); 2+ for 1323-keV level in {+32}P mirror nucleus (1994Vo12). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E$1736.7 {I6} from ({+3}He,t) 
J$L({+3}He,t)=(4) from 0+; 3+ from comparison of |s(|q) data with CDE calculations in ({+3}He,t) (1989Je07); 3+ for 1755-keV level in {+32}P mirror nucleus (1994Vo12). 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
E$2131.1 {I4} from ({+3}He,t) 
J$L({+3}He,t)=4 from 0+; 3+ from comparison of |s(|q) data with CDE calculations in ({+3}He,t) (1989Je07); 3+ for 2177-keV level in {+32}P mirror nucleus (1994Vo12). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E$2209.5 {I5} from ({+3}He,t) 
J$L({+3}He,t)=(2) from 0+; 1+ for 2230-keV level in {+32}P mirror nucleus (1994Vo12). 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E$2283.5 {I5} from ({+3}He,t) 
J$L({+3}He,t)=2 from 0+; 2+ for 2218-keV level in {+32}P mirror nucleus (1994Vo12) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$L({+3}He,t)=(4) from 0+; 3+ from comparison of |s(|q) data with CDE calculations in ({+3}He,t) (1989Je07). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$2+ from mirror symmetry argument by 2011Ma69 in ({+3}He,t). But L({+3}He,t)=3(+2) from 0+ favors negative parity 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 4082 {I4} from {+32}Ar |e decay, 4060 {I30} from (p,n), and 4075 {I4} from ({+3}He,t) 
J$L({+3}He,t)=2 from 0+; allowed |e feeding (log {Ift}=4.0) from 0+ parent 


level_energy_unit: KEV
level_spin_parity: (1)
level_comment:
E$weighted average of 4561 {I13} from {+32}Ar |e decay, 4580 {I30} from (p,n), and 4581 {I6} from ({+3}He,t) 
J$|e feeding from 0+ parent (log {Ift}=6.3) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: EV
level_comment:
$|G and |G{-|g} from 2008Bh08 in {+32}Ar |e decay. 
J$supper-allowed |e feeding from 0+ parent (log {Ift}=3.19); IAS of {+32}Ar g.s. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MS
level_comment:
$|e feeding to g.s. is assumed to be negligible (2021Bl02). 1985Bj01 report that g.s. feeding is limited to <2% by intensity balance to levels in {+32}S from the decay of g.s. of {+32}Cl; 2021Bl02 give a range of 0.007% to 5.6% based on theoretical predictions. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: EV
level_comment:
E$5044 {I3} from E(p) 
$E(p0)=3352.7 {I30}, E(p1)=2145.5 {I50} 
$|G from ISOLDE data (quoted by 2008Bh08 as paper in preparation). 
E$IAR of {+32}Ar g.s. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$others: 1157 {I5} (1989Je07), 1168 (1994Vo12, used as reference); 1168.5 {I2} used as reference in 2010Wr02 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E$others: 1734 {I5} (2011Ma69), 1736 {I2} (1997Le14), 1735 {I3} (1994Vo12), 1719 {I4} (1989Je07). 
$Deduced E{-p}(c.m.)=156 {I5} (2011Ma69), 155.4 {I8} (2010Wr02), 162 {I11} (1994Vo12) for {+31}S(p,|g) 
$|G{-|g}/|G=0.92 {I20} (1997Le14) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E$others: 2128 {I5} (2011Ma69), 2130 {I2} (1997Le14), 2129 {I3} (1994Vo12), 2122 {I5} (1989Je07). 
$Deduced E{-p}(c.m.)=549 {I5} (2011Ma69), 549.8 {I7} (2010Wr02), 556 {I11} (1994Vo12) for {+31}S(p,|g) 
J$proposed by 1994Vo12 and 1997Le14 
L$other: 0 from tp(|q) (2011Ma69) 
$|G{-|g}/|G=0.52 {I28} (1997Le14) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
L$other: 0 from tp(|q) (2011Ma69) 
E$others: 2203 {I5} (2011Ma69), 2213 {I3} (1994Vo12,1997Le14), 2193 {I7} (1989Je07). 
$Deduced E{-p}(c.m.)=625 {I6} (2011Ma69), 628.2 {I8} (2010Wr02), 640 {I11} (1994Vo12) for {+31}S(p,|g) 
J$proposed by 1994Vo12 
$|G{-|g}/|G<0.08 (1997Le14) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$others: 2279 {I5} (2011Ma69), 2281 {I3} (1994Vo12,1997Le14), 2270 {I5} (1989Je07). 
$Deduced E{-p}(c.m.)=701 {I5} (2011Ma69), 702.2 {I7} (2010Wr02), 708 {I11} (1994Vo12) for {+31}S(p,|g) 
J$proposed by 1994Vo12 
L$other: 0 from tp(|q) (2011Ma69) 
$|G{-|g}/|G<0.05 (1997Le14) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E,J$new level reported in 2011Ma69. 
$Deduced E{-p}(c.m.)=1033 {I6} (2011Ma69) 
L$other: 0 from tp(|q) (2011Ma69) 
$%p: fit result is 95 {I32} (2011Ma69) 


level_energy_unit: KEV
level_comment:
E$average of 2665 {I10} (1989Je07), 2677 {I5} (2011Ma69) 
$Deduced E{-p}(c.m.)=1099 {I5} (2011Ma69) 
L$other: 0 from tp(|q) (2011Ma69) 
$%p: fit result is 94 {I16} (2011Ma69) 


level_energy_unit: KEV
level_comment:
E$average of 2858 {I5} (1989Je07), 2859 {I4} (2011Ma69) 
$Deduced E{-p}(c.m.)=1281 {I5} (2011Ma69) 
L$others: 1 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E$average of 2941 {I5} (1989Je07), 2932 {I5} (2011Ma69) 
$Deduced E{-p}(c.m.)=1353 {I5} (2011Ma69) 
L$other: 0 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_comment:
E$average of 3056 {I5} (1989Je07), 3055 {I5} (2011Ma69). 
$Deduced E{-p}(c.m.)=1477 {I5} (2011Ma69) 
L$other: L=2 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_comment:
E$average of 3166 {I5} (1989Je07), 3164 {I4} (2011Ma69) 
$Deduced E{-p}(c.m.)=1586 {I5} (2011Ma69) 
L$other: 2 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_comment:
E$average of 3290 {I10} (1989Je07), 3281 {I5} (2011Ma69) 
$Deduced E{-p}(c.m.)=1703 {I5} (2011Ma69) 
L$other: 2 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$average of 3692 {I7} (1989Je07), 3695 {I4} (2011Ma69) 
$Deduced E{-p}(c.m.)=2117 {I4} (2011Ma69) 
J$based on mirror symmetry argument (2011Ma69) 
L$other: 2 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E$average of 3883 {I5} (1989Je07), 3875 {I4} (2011Ma69) 
$Deduced E{-p}(c.m.)=2297 {I5} (2011Ma69) 
J$based on mirror symmetry argument (2011Ma69) 
L$other: 2 from tp(|q) (2011Ma69) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
J$L(p,t)=0 from 3/2+; L({+3}He,d)=L(d,n)=2 from 0+. 
T$weighted average of 2.5038 s {I22} (2015Gr14), 2.507 s {I8} (1977Az01), 2.513 s {I4} (1973Ta04), 2.52 s {I14} (1972Es02), 2.47 s {I2} (1970Sc16), 2.51 s {I2} (1960Ja12), and 2.53 s {I2} (1958Mu05). Others: 2.8 s (1940Ho01), 2.4 s {I2} (1941Wh02), 2.8 s (1948Sc20), 1.8 {I1} (1951Bo56), 1.7 s (1954Ty33), 2.9 s {I1} (1960Wa04), 1962Va27, 2.5 s {I5} (1970Ba65). 
MOMM1$from |b-NMR method (2004Ma98). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
$|G{-|g}=3.7|*10{+-4} eV {I6} 
J$L({+3}He,d)=L(d,n)=0 from 0+ 
T$from DSAM in {+2}H({+32}S,n|g). Other: >0.17 ps by DSAM in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: PS
level_comment:
$|G=5.0|*10{+-5} eV {I31}; |G{-|g}=1.4|*10{+-5} eV {I6} 
$(2J+1)|G{-|g}|G{-p}/|G=9|*10{+-5} eV {I4} (1976Al01) 
J$L(d,n)=L({+3}He,d)=3 from 0+; 2685.5|g to 3/2-; possible 1874.8|g to 1/2+. But 7/2- from theoretical predictions (1976Al01) cannot be ruled out 
T$deduced by the evaluators from |G=5.0|*10{+-5} eV {I31} determined based on |G{-|g}=1.4|*10{+-5} eV {I6} and |G{-|g}/|G=0.22 {I8} in (p,|g):res (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
$|G{-|g}=0.14 eV {I5} 
$(2J+1)|G{-|g}|G{-p}/|G=0.08 eV {I1} (1976Al01) 
J$from |g(|q) and |g(lin pol) in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
$|G{-|g}=0.07 eV {I2} 
$(2J+1)|G{-|g}|G{-p}/|G=0.21 eV {I3} (1976Al01) 
J$spin from |g(|q) and parity from |g(lin pol) in (p,|g):res; also L(d,n)=L({+3}He,d)=1 from 0+. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
$|G{-|g}=7.7|*10{+-3} eV {I18} 
J$spin from |g(|q) in (p,|g):res and parity from L(p,t)=2 from 3/2+. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$(2J+1)|G{-|g}|G{-p}/|G=0.053 eV {I7} (1976Al01) 
J$spin from |g(|q) in (p,|g):res; parity from 1464.4|g M1+E2 to 3/2+ 
$E=3816.1 {I3} in (p,|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$(2J+1)|G{-|g}|G{-p}/|G=0.03 eV {I2} (1976Al01) 
J$spin from |g(|q) and |g|g(|q) in (p,|g); parity from 3970.9|g M1+E2 to 1/2+ 
T$from 2006Tr10 in (p,|g):res. Others: 0.6 keV (1968Li07), 5 keV {I3} (1976Al01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$spin from |g(|q) in (p,|g):res; parity from 1132.6|g M1+E2 to 3/2- 
$(2J+1)|G{-|g}|G{-p}/|G=0.38 keV {I4} in (p,|g):res (1976Al01) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} in (p,|g):res 
J$2113|g to 5/2+, 3289|g to 1/2+ 
$(2J+1)|G{-|g}|G{-p}/|G=0.019 eV {I8} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
J$spin from |g|g(|q) in (p,|g):res; parity from 3301.4|g M1+E2 to 1/2+ 
T$other: <3 keV from {+33}Ar |e+|b{++} decay 
$(2J+1)|G{-|g}|G{-p}/|G=0.07 eV {I2} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} in (p,|g):res 
J$also supported by L(d,n)=L({+3}He,d)=1 from 0+. 
T$weighted average of 14 keV {I4} (1976Al01) and 10 keV {I3} (1992Il01) in (p,|g):res and 8.5 keV {I15} (1958Ol16) in (p,p):res. 
$(2J+1)|G{-|g}|G{-p}/|G=0.19 eV {I7} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
J$spin=1/2,3/2 from |g(|q) in (p,|g):res; parity from allowed |e+|b{++} feeding (log {Ift}=4.81 {I5}) from 1/2+ parent; 1/2 from (p,p) in a private communication by the evaluator of 1978En02 in 1977 with V. Meyer, one of the authors of the later publications of 1980Wa28 and 1983Wa28. 
T$from {+33}Ar |e+|b{++} decay and (p,|g):res. 
$(2J+1)|G{-|g}|G{-p}/|G=0.30 eV {I4} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$spin from |g(|q) in (p,|g):res: parity from allowed |e+|b{++} feeding (log {Ift}=5.638 {I8}) from 1/2+ parent 
$(2J+1)|G{-|g}|G{-p}/|G=0.14 eV {I2} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} in (p,|g):res 
J$spin=5/2 from |g(|q) in 1970PrZW; M2 for 3936|g to 1/2+ ruled out by RUL and T{-1/2}<2.3 fs 
T$deduced by the evaluators from |G>0.2 eV based on (2J+1)|G{-|g}|G{-p}/|G=1.4 eV {I2} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} in (p,|g):res and (p,p):res 
J$1930|g E2 to 3/2-; L({+3}He,d)=3 from 0+. 7/2- also from R-matrix analysis of |s(|q) data in (p,p):res 
$(2J+1)|G{-|g}|G{-p}/|G=0.093 eV {I19} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+33}Ar |e+|b{++} decay 
J$spin=3/2 from |g(|q) in (p,|g):res; parity from allowed |e+|b{++} feeding (log {Ift}=5.509 {I8}) from 1/2+ parent 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} in (p,p):res. Other: 5002 in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} in (p,p):res. Other: 5090 {I20} from ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+33}Ar |e+|b{++} decay. Other: 5105 {I2} from (p,p):res 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=5.84 {I6}) from 1/2+ parent; 3/2 favored in barrier-penetration calculations (2010Ad03). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
T$others: <2 keV in (p,|g):res, <0.8 keV in {+33}Ar |e+|b{++} decay 
$IAS of 1/2+ g.s. in {+33}Ar. 
$(2J+1)|G{-|g}|G{-p}/|G=0.76 eV {I18} (1972Es02) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 5732 {I3} from {+33}Ar |e+|b{++} decay and 5738 {I5} from (p,p) 
T$weighted average of 30 keV {I10} from {+33}Ar |e+|b{++} decay and 40 keV {I5} from (p,p) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
E$from (p,p):res. Other: 5870 {I20} from ({+3}He,d), 5890 from (d,n) 
T$other: 15 keV for E(level)=5879 {I9} from (p,|g):res, the large width could indicate a composite peak 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 6142 {I9} from (p,|g):res and 6150 {I3} from (p,p) 
T$other: 13 keV from (p,|g):res, the large width could indicate a composite peak 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$6198 {I6} from (p,|g):res could be a doublet of 6192 {I3} and 6203 {I3} in (p,p):res. 
T$other: <10 keV for E(level)=6198 {I6} in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_comment:
E$6253 {I6} from (p,|g):res could be a doublet of 6247 {I5} and 6256 {I5} in (p,p):res. 
T$other: <6 keV for E(level)=6253 {I6} in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$from {+33}Ar |e+|b{++} decay. Other: 6256 {I5} from (p,p) 
J$1/2+,3/2+ from allowed |e+|b{++} feeding (log {Ift}=4.589 {I16}) from 1/2+ parent; (1/2+,7/2+) from R-matrix analysis of |s(|q) data in (p,p):res. 
T$others: 6 keV {I3} from (p,p):res; <6 keV for E(level)=6253 {I6} in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
E$from (p,p):res. Others: 6290 from (d,n), 6250 {I30} from ({+3}He,d) 
J$also supported by L(d,n)=(3) and L({+3}He,d)=3 from 0+ 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_comment:
E$from {+33}Ar |e+|b{++} decay. Other: 6308 {I9} from (p,|g):res 
J$|e+|b{++} feeding (log {Ift}=6.28 {I20}) from 1/2+ parent 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_comment:
E$from {+33}Ar |e+|b{++} decay. Other: 6580 {I30} in ({+3}He,d) 
J$|e+|b{++} feeding (log {Ift}=6.69 {I7}) from 1/2+ parent. But L({+3}He,d)=(3,4) suggests (5/2-,7/2,9/2+) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E$6629 {I9} from (p,|g):res could be a doublet of 6626 {I3} and and 6230 {I5} in (p,p):res. 
T$other: 33 keV for E(level)=6629 {I9} in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: 1/2(+),3/2(+)
level_comment:
E$from {+33}Ar |e+|b{++} decay. Other: 6938 {I9} in (p,|g):res, 6050 {I50} from (p,t) 
J$probable allowed |e+|b{++} feeding (log{Ift}=5.94 {I3}) from 1/2+ parent 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$7280 {I9} from (p,|g):res could be a doublet of 7264 {I6} and and 7275 {I4} in (p,p):res. 
T$other: 29 keV for E(level)=7280 {I9} in (p,|g):res 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: KEV
level_comment:
J$1/2+,3/2+ from allowed |e+|b{++} feeding (log {Ift}=5.59 {I8}) from 1/2+ parent; 3/2 favored from barrier-penetration calculations (2010Ad03). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
E$from (p,p):res. Others: 7343 {I9} from (p,|g):res, 7350 {I50} from (p,t) 
J$other: (9/2+,7/2-) for a group at 7330 in (d,n) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E$7297 {I9} from (p,|g):res could be a doublet of 7392 {I2} and and 7399 {I3} in (p,p):res. 
T$other: <2 keV for E(level)=7297 {I9} in (p,p):res. 
$(2J+1)|G{-|g}|G{-p}/|G=1.50 eV {I37} (1972Es02) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$from {+33}Ar |e+|b{++} decay. Others: 7486 {I6} in (p,|g):res and 7482 {I4} in (p,p):res. 
J$from R-matrix analysis of |s(|q) data in (p,p); allowed |e+|b{++} feeding (log {Ift}=4.35 {I6}) from 1/2+. 
T$others: <8 keV from (p,|g):res, 13.0 keV {I13} from (p,p):res 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: KEV
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=5.32 {I6}) from 1/2+ parent; 1/2 favored from proton decay to 0+ g.s. and 0+ excited state, possible L(p)=0 transition. 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: KEV
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=4.27 {I12}) from 1/2+ parent; 1/2 favored in barrier-penetration calculations (2010Ad03) 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_comment:
J$allowed |e+|b{++} feeding (log| {Ift}=5.74 {I6}) from 1/2+ parent; 1/2 favored from proton decay to 0+ g.s. and 0+ excited state, possible L(p)=0 transition. However, L(d,n)=(3) from 0+ for a group at 8490 suggests (5/2-,7/2-) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=4.57 {I9}) from 1/2+ parent; 3/2 favored in barrier-penetration calculations (2010Ad03). 
$E=8558 {I5} in (|b{++}). 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_comment:
J$allowed |e+|b{++} feeding (log|{Ift}=4.65 {I18}) from 1/2+ parent. But L(d,n)=(3) from 0+ for a group at 8860 suggests (5/2-,7/2-) 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_comment:
J$|e+|b{++} feeding (log {Ift}=6.28 {I13}) from 1/2+ parent. But L(d,n)=(3) from 0+ for a group at 8860 suggests (5/2-,7/2-) 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=4.35 {I11}) from 1/2+ parent; 1/2 favored in barrier-penetration calculations (2010Ad03). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=4.69 {I5}) from 1/2+ parent; 3/2 favored in barrier-penetration calculations (2010Ad03). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$allowed |e+|b{++} feeding (log {Ift}=4.61 {I5}) from 1/2+ parent; 3/2 favored in barrier-penetration calculations (2010Ad03). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
S$average of 0.70 and 0.63 for two sets of optical parameters (1972Ko02). Others: 0.47 {I14} (1966Gr26), 0.90 (1970Mo01), 0.54 (1975In03), 0.86 and 0.69 for two sets of optical parameters in 1994Ve04, 0.73 (2021Lo14) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$weighted average of 806 {I12} (1970Mo01), 810 {I9} (1970Mo08), and 810 {I6} (1972Ko02). Others: 810 (1975In03, 2021Lo14) 
S$average of 0.32 and 0.37 for two sets of optical parameters (1972Ko02). Others: 0.22 {I7} (1966Gr26), 0.29 (1970Mo01), 0.22 (1975In03), 0.37 (1994Ve04), 0.25 (2021Lo14) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 2360 {I20} (1970Mo01), 2351 {I9} (1970Mo08), and 2358 {I25} (1972Ko02). Others: 2358 (1975In03), 2352 (2021Lo14) 
S$other: 0.073 (2021Lo14) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$weighted average of 2690 {I12} (1970Mo01), 2686 {I8} (1970Mo08), and 2686 {I16} (1972Ko02). Others: 2686 (1975In03), 2685 (2021Lo14) 
S$average of 0.50 and 0.41 for two sets of optical parameters (1972Ko02). Others: 1.1 {I3} (1966Gr26), 0.73 (1970Mo01), 0.52 (1975In03), 0.44 (2021Lo14). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$weighted average of 2860 {I12} (1970Mo01), 2848 {I9} (1970Mo08), and 2842 {I15} (1972Ko02). Others: 2860 (1975In03), 2846 (2021Lo14) 
S$average of 0.50 and 0.58 for two sets of optical parameters (1972Ko02). Others: 0.74 {I22} (1966Gr26), 0.55 (1970Mo01), 0.72 (1975In03), 0.28 (2021Lo14). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$weighted average of 4119 {I9} (1970Mo08) and 4120 {I20} (1972Ko02) 
S$average of 0.060 and 0.075 for two sets of optical parameters (1972Ko02) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
S$average of 0.097 and 0.091 for 5/2- and average of 0.054 and 0.050 for 7/2- for two sets of optical parameters (1972Ko02). 


level_energy_unit: KEV
level_comment:
S$0.060 for L=(3), J|p=(5/2-), average of 0.059 and 0.061; 0.034 for L=(3), J|p=(7/2)-; 0.028 for L=(4), J|p=(9/2+), average of 0.032 and 0.024. Two values for each J|p are from two sets of optical parameters (1972Ko02). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
S$average of 0.041 and 0.042 for 5/2- and average of 0.024 and 0.025 for 7/2- for two sets of optical parameters (1972Ko02). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 5301 {I2} from E{-p0}=2932 {I2} and 5292 {I10} from E{-p1}=761 {I10}. Others: E{-p1}=768 {I5} and E{-p0}=2927 {I4} (1996Ho24) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from E{-p0}=3299 {I19} and E{-p1}=1092 {I34} in 1971Ha05. But those proton groups are not observed in later studies and considered questionable by the evaluator 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$from E{-p0}=3350 {I3}. Other: E{-p}=3363 {I29} (1971Ha05); E{-p1}=1225 {I34} from 1971Ha05, but this p1 proton decay is not seen in other studies. 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_lifetime_unit: KEV
level_comment:
E$from E{-p1}=1318 {I3}. Others: E{-p1}=1322 {I29} and a weak peak of E{-p0}=3482 {I34} probably for several groups (1971Ha05); E{-p1}=1322 {I3} and E{-p0}=3485 (1996Ho24) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from E{-p0}=3636 {I34} and E{-p1}=1473 {I34} in 1971Ha05. But those proton groups are not observed in later studies and considered questionable by the evaluators 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from E{-p0}=3741 {I34} and E{-p1}=1539 {I39} in 1971Ha05. But those proton groups are not observed in later studies and considered questionable by the evaluators 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 6253 {I3} from E{-p0}=3855 {I3} and 6256 {I2} from E{-p1}=1696 {I2}. Other: E{-p0}=3852 {I19} (1971Ha05) 


level_energy_unit: KEV
level_spin_parity: 1/2(+),3/2(+)
level_comment:
E$from E{-p1}=2367 {I2}. Other: E{-p}=2364 {I34} p0 decay to a level at 4720 {I35}, but changed to p1 by the evaluators, as assigned in 1993Sc16 and 2010Ad03 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 7286 {I4} from E{-p0}=4856 {I4} and 7300 {I7} from E{-p1}=2708 {I7}. Other: E{-p0}=4832 {I39} and E{-p1}=2605 {I29} from 1971Ha05 give a level at 7219 {I32} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 7476 {I4} from E{-p0}=5040 {I4} and 7483 {I2} from E{-p1}=2885 {I2}. Others: E{-p0}=5030 {I19} and 2884 {I39} (1971Ha05); E{-p0}=5036 {I4} (1996Ho24) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$from E{-p1}=2951 {I2}. Other: E{-p1}=2950 {I5} (1996Ho24); E{-p1}=2955 {I29} and E{-p0}=5179 {I29} from 1971Ha05 give a level at 7588 {I32} 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 7666 {I4} from E{-p0}=5225 {I4} and 7670 {I6} from E{-p1}=3066 {I2}. Other: E{-p}=3068 {I29} p0 proton from a level at 5442 {I30} in 1971Ha05, but changed to p1 decay by the evaluator 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: KEV
level_comment:
E$unweighted average of 7761 {I3} from E{-p0}=5317 {I3} and 7771 {I4} E{-p2}=1664 {I4}. Other: E{-p0}=5318 {I39} (1971Ha05) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 8075 {I3} from E{-p0}=5621 {I3} and 8083 {I6} E{-p1}=3467 {I6}. Others: E{-p0}=5626 {I19}, E{-p1}=3482 {I34} and E{-p2}=1960 {I29} (p2) (1971Ha05), with p2 proton not seen in other studies 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 8180 {I3} from E{-p0}=5723 {I3} and 8190 {I5} from E{-p1}=3570 {I5}. Other: E{-p0}=5722 {I24} (1971Ha05) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_comment:
E$weighted average of 8318 {I6} from E{-p1}=3695 {I6} and 8313 {I9} from E{-p0}=5852 {I9}. Other: E{-p0}=5845 {I29} (1971Ha05) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$weighted average of 8568 {I10} from E{-p0}=6099 {I10} and 8555 {I5} E{-p1}=3924 {I5}. Other: E{-p0}=6117 {I39}, E{-p1}=3981 {I34} (1971Ha05) 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_comment:
E$weighted average of 8955 {I10} from E{-p0}=6474 {I10} and 8970 {I8} from E{-p1}=4327 {I8}. Other: E{-p0}=6484 {I29} (1971Ha05) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$weighted average of 9140 {I9} from E{-p0}=6654 {I9}, 9155 {I6} from E{-p1}=4506 {I6} and 9166 {I10} from E{-p2}=3014 {I10} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
T$weighted average of 2.52 s {I14} (1972Es02), 2.47 s {I2} (1970Sc16), 2.513 s {I4} (1973Ta04), 2.53 s {I2} (1958Mu05) 
$C{+2}S=0.84 {I21} (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$from |t>250 ps by DSAM in 1972Bi19 
$|G{-|g}=3.7|*10{+-4} eV {I6} (1976Al01) 
$C{+2}S=0.28 {I5} (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$1986.5|g M1+E2 to 3/2+, 988.9|g M1+E2 from 7/2+. 
J$other: 5/2,7/2 from |g(|q) in 1970PrZW 
T$from |t=76 fs {I17}, weighted average of 94 fs {I+14-20} (1972Bi19) and 61 fs {I16} (1976Al01) 
$|G{-|g}=0.011 eV {I3} (1976Al01) 
$C{+2}S<0.26 (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
T$from |t=100 fs {I30} (1976Al01) 
$|G{-|g}=0.007 eV {I2} (1976Al01) 
$S{-p|g}=7.0|*10{+-17} eV with E{-p}=77.3 {I8} deduced from level energy in 1992Il01 
$C{+2}S<0.66 (1992Il01) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J$2090|g M1+E2 from 7/2-; 699|g D+Q to 5/2+; 2685.5|g to 3/2+ and probable 1875|g to 1/2+ favor 5/2-. But 7/2- from theoretical predictions (1976Al01) 
S$from 1992Il01. Resonance not observed in 1976Al01; a value of 421.8 {I6} is deduced by the authors from level energy 
$Estimated S{-p|g}=9|*10{+-5} eV {I4} (1976Al01), 7.4|*10{+-5} eV {I16} (1992Il01) 
$|G{-|g}=1.4|*10{+-5} eV {I6} (1976Al01) 
$C{+2}S<3.8 (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in 1958Va22 and |g(lin pol) in 1959Su55 
T$from |t=4.4 fs {I15} (1976Al01) 
S$other: 579.8 {I15} (1958Va22) 
$S{-p|g}=0.027 eV {I10} (1958Va22), 0.022 eV {I6} (1962Lo06), 0.08 eV {I1} (1976Al01). Unweighted average is 0.043 eV {I19} 
$|G{-|g}=0.14 eV {I5} (1976Al01) 
$C{+2}S<0.47 (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
J$from |g(|q) in 1958Va22 and |g(lin pol) in 1959Su55 
T$from |t<1 fs (1976Al01) 
S$weighted average of 587.4 {I15} (1958Va22), 587.9 {I5} (1976Al01) and 589 {I1} 1992Il01. 
$S{-p|g}=0.10 eV {I4} (1958Va22), 0.06 eV {I2} (1962Lo06), 0.14 eV {I2} (1966En04), 0.21 eV {I3}(1976Al01), 0.20 eV {I4} (1975Ke11), 0.26 eV {I6} (1992Il01). Unweighted average is 0.16 eV {I3} 
$|G{-|g}=0.070 eV {I20} (1976Al01) 
$C{+2}S=0.77 {I13} (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$2975.4|g E2(+M3) to 3/2+ 
T$from |t=86 fs {I20} (1976Al01) 
S$resonance not observed in 1976Al01; quoted value is deduced by the authors of 1976Al01 from level energy 
$Estimated S{-p|g}=1.4|*10{+-4} eV {I6} (1976Al01) 
$|G{-|g}=7.7|*10{+-3} eV {I18} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
S$weighted average of 1587.8 {I11} (1976Al01) and 1589 {I1} (1992Il01) 
$S{-p|g}=0.053 eV {I7} (1976Al01), 0.054 eV {I12} (1992Il01) 
$|G{-|g}>8.8|*10{+-3} eV (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
S$weighted average of 1748.4 {I10} (1976Al01) and 1949 {I1} (1992Il01) 
T$from 2006Tr10. Others: 0.6 keV (1968Li07), 5 keV {I3} (1976Al01) 
$S{-p|g}=0.09 eV {I2} (1976Al01), 0.090 eV {I18} (1992Il01) 
$|G{-|g}=0.023 eV {I4} (1976Al01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
T$from 1968Li07 
S$from 1968Li07, giving E(level)=3978.3 {I8} which is in better agreement with E|g data than E{-p}(lab)=1757.2 {I9} from 1976Al01 that gives E(level)=3980.8 {I10} 
$S{-p|g}=0.38 eV {I4} (1976Al01), 0.36 eV {I12}(1968Li07), 0.14 eV {I4} (1962Lo06). Unweighted average is 0.29 eV {I8} 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} and S(p) 
J$2113|g to 5/2+, 3289|g to 1/2+ 
$S{-p|g}=0.019 eV {I8} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
J$spin from |g|g(|q) in 1968Li07 
T$from 1968Li07 
S$weighted average of 1892.8 {I7} (1968Li07) and 1893.8 {I11} (1976Al01) 
$S{-p|g}=0.07 eV {I2} (1976Al01), 0.22 eV {I8} (1962Lo06 and 1968Li07), 0.46 eV {I15} (1975VaYG). Unweighted average is 0.25 eV {I11} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} and S(p) 
T$weighted average of 14 keV {I4} (1976Al01) and 10 keV {I3} (1992Il01) 
S$weighted average of 1898 {I2} (1976Al01) and 1899 {I2} (1992Il01) 
$S{-p|g}=0.19 eV {I7} (1976Al01), 0.18 eV {I8} (1992Il01) 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_lifetime_unit: KEV
level_comment:
J$from |g(|q) in 1970PrZW 
T$from 1976Al01. Other: |G<1 keV (1968Li07) 
S$from 1968Li07. Other: 2229.4 {I13} (1976Al01) 
$S{-p|g}=0.30 eV {I4} (1976Al01), 0.50 eV {I20} (1968Li07) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} and S(p) 
J$from |g(|q) in 1970PrZW 
$S{-p|g}=1.4 eV {I2} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from E{-p} and S(p) 
$Estimated S{-p|g}=0.093 eV {I19} in 1976Al01 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
J,L$from 1972Lo19. J|p=5/2-,7/2- from 1958Ol16 
T$other: 1.0 keV {I5} (1972Lo19) 
S$weighted average of 2578 {I3} (1958Ol16) and 2580 {I3} (1972Lo19) 
$|G{-p0}|?0.25 keV from |G{-p0}/|G|?1 and |G=0.25 keV {I5} (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
S$weighted average of 2810 {I2} (1958Ol16) and 2814 {I3} (1972Lo19) 
T$same value also from 1972Lo19 
$|G{-p'}|?1.5 eV (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
J$from 1972Lo19. Other: 5/2-,7/2- from 1958Ol16 
T$other: |?0.5 (1972Lo19) 
$|G{-p0}/|G|?1, |G{-p'}|?1.0 eV (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
J,T,L,S$same results from 1972Lo19 
$|G{-p0}|?1.5 from |G{-p0}/|G|?1 and |G=1.5 keV {I5}, |G{-p'}|?1.8 eV (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$1972Lo19 consider the resonance at E{-p}=2895 {I30} reported in 1958Ol16 the same one as seen by them at E{-p}=2930 {I15} 
J,L$from both 1958Ol16 and 1972Lo19 
T$weighted average of 360 keV {I60} (1958Ol16) and 283 keV {I30} (1972Lo19) 
S$weighted average of 2895 {I30} (1958Ol16) and 2930 {I15} (1972Lo19). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$|G{-p0}=0.29 keV {I5} and |G{-p'}=0.05 keV {I2} from |G{-p0}/|G=0.85 {I5} and |G=0.34 keV {I6} (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
S$weighted average of 3273 {I4} (1958Ol16) and 3271 {I1} (1970Ab15) 
T$weighted average of 32 keV {I4} (1958Ol16), 30 keV {I2} (1970Ab15), and 30 keV {I4} (1976Ik03). 
$|G{-p0}=30 keV {I1} (1970Ab15), 30 keV {I4} (1976Ik03). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
$The E{-p}=3370 keV (E{-x}=5544 keV) (1970Ab15) in the evaluation of 1998En04 is erroneous and it is replaced by this new value, which is confirmed by E{-p}=3375 keV {I3} (E{-x}=5549 keV {I3})(1974Fi02) and E{-x}=5548.5 keV {I4} in the (p,|g) reaction (2006Tr10). 
J,L$from 1970Ab15, 1974Fi02, 2002Py01 
T$weighted average of 100 eV {I25} (1970Ab15), 150 eV {I50} (1974Fi02), 115 eV {I15} (1976Ik03), 100 eV {I9} (1992Wi13). 
S$from 2002Py01. Others: 3375 {I3} (1974Fi02), 3370 {I1} (1970Ab15), 3379 {I2} (1958Ol16) 
$|G{-p0}=100 eV {I25} (1970Ab15), 98 eV {I9} (1992Wi13), 115 eV {I15} (1976Ik03). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
J,L$from 1958Ol16, 1970Ab15, 1976Ik03, 2002Py01 
T$weighted average of 1.00 keV {I20} (1958Ol16), 0.60 keV {I10} (1970Ab15) and 1.0 keV {I2} (1976Ik03) 
S$from 2002Py01. Others: 3379 {I2} (1958Ol16), 3377 {I1} (1970Ab15), 3379 {I7} (1980Va02) 
$|G{-p0}=0.20 keV {I5} (1970Ab15), 0.4 keV (1976Ik03) 
$|G{-p0}=0.40 keV {I9} and |G{-p'}=0.60 keV {I13} from |G{-p0}/|G=0.40 {I4} and |G=1.00 keV {I20} (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
T$other: 1.5 keV {I5} (1976Ik03) 
S$other: 3718 {I10} (1980Va02) 
$|G{-p0}=0.75 keV (1976Ik03) 
$|G{-p0}=0.84 keV {I21} and |G{-p'}=0.66 {I18} from |G{-p0}/|G=0.56 {I8} and |G=1.50 keV {I30} (1958Ol16) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$|G{-p0}=3.7 keV {I4} (1973Ab05) 
T$other: 5.0 {I10} (1974Fi02) 
J$3/2+ in 1974Fi02 gives a better fit to the data than 5/2+ in 1973Ab05. 
L$also from 1974Fi02 
S$weighted average of 4049 {I3} (1974Fi02) and 4050 {I3} (1973Ab05) 
S$4050 {I3} (1973Ab05) 


level_energy_unit: KEV
level_spin_parity: (1/2+,7/2+)
level_lifetime_unit: KEV
level_comment:
S$weighted average of 4102 {I5} (1973Ab05) and 4106 {I5} (1974Fi02) 
T$from 1974Fi02, but |G=15 keV {I2} from 1973Ab05 is discrepant 
J,L$L=4 and J|p=(7/2+) from 1973Ab05, but L=(0) and J|p=(1/2+) from 1974Fi02 
$|G{-p0}=3.5 keV {I7} (1973Ab05) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
J,L$from 1973Ab05 and 1974Fi02 
T$weighted average of 3.0 keV {I5} (1974Fi02) and 5.0 keV {I5} (1973Ab05) 
S$weighted average from 4140 {I3} (1973Ab05) and 4139 {I3} (1974Fi02) 
$|G{-p0}=4.0 keV {I4} (1973Ab05) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
J,L$from 1973Ab05 and 1974Fi02 
T$weighted average of 60 keV {I20} (1974Fi02) and 70 keV {I7} (1973Ab05) 
S$weighted average of 4245 {I5} (1973Ab05) and 4246 {I10} (1974Fi02) 
$|G{-p0}=62 keV {I6} (1973Ab05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
J,L$other: L=(2), J|p=(3/2+,5/2+) from 1974Fi02 
T$weighted average of 5 keV {I2} (1974Fi02) and 8.0 keV {I8} (1973Ab05) 
S$weighted average of 4485 {I3} (1973Ab05) and 4488 {I5} (1974Fi02) 
$|G{-p0}=4.0 keV {I4} (1973Ab05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
J,L$from 1973Ab05 and 1974Fi02 
T$weighted average of 4.0 keV {I10} (1974Fi02) and 6.0 keV {I6} (1973Ab05) 
S$weighted average 4560 {I3} (1973Ab05) and 4561 {I3} (1974Fi02) 
$|G{-p0}=5.3 keV {I5} (1973Ab05) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_comment:
$|G{-p0}=26.7 keV {I27} (1973Ab05) 
J$5/2+ from 1973Ab05 and 3/2+ from 1974Fi02. 
T$from 1974Fi02. Other: |G=28 keV {I3} (1973Ab05) 
L$from 1973Ab05 and 1974Fi02 
S$weighted average of 4721 {I3} (1973Ab05) and 4726 {I8} (1974Fi02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
J$from 1980Wa28 and 1992Wi13 
T$from 1992Wi13. Other: 50 eV (1980Wa28) 
S$from 1980Wa28. Other: 5273 (1992Wi13) 
$|G{-p0}=96 eV {I2} (1992Wi13), 40 eV (1980Wa28) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$others: 880 {I70} (1960Ma32), 760 {I70} (1953Mi10), 810 (1967Mu12), 820 (1998TeZV) 
L$from 1972El03, 1988Eg03, 1998TeZV 
S$other: 0.17 (1988Eg03,1972El03) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from 1960Ma21. Other: 2110 (1967Mu12) 
L$from 1967Mu12 
$This level is not seen in 1972El03, 1998TeZV and other studies and considered questionable by the evaluators. It may correspond to the 1993 level 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from 1960Ma21. Other: 2500 (1967Mu12). 
$This level is not seen in 1972El03, 1998TeZV and other studies and considered questionable by the evaluators. It may correspond to the 2351 level 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$other: 2690 (1988Eg03,1998TeZV) 
L$from 1988Eg03 and also favored by |g(q) in 1972El03 
S$others: 0.92 (1988Eg03), 0.50 (1972El03). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 2840 {I60} (1953Mi10), 2820 {I60} (1960Ma21), 2850 (1967Mu12), 2860 (1998TeZV) 
S$others: 1.2 (1988Eg03), 0.55 (1972El03) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$IAS of {+34}S g.s. 
J$log| {Ift}=3.5 from 0+ g.s. of {+34}Ar parent (superallowed transition) 
$T{-1/2}: weighted average of: 1.5268 s {I5} (2006Ia05), 1.5277 s {I22} (1983Ko22), 1.5252 s {I11} (1976Wi08), 1.526 s {I2} (1973Ry01); others: 1.530 s 4 (1975Ha24, earlier result: 1.534 s {I3} in 1972Ha28, superseded by 1983Ko22), 1.565 s {I7} (1965Eb01), 1.565 s {I7} (1965Fr06), 1.560 s {I14} (1961Ja22), 1.58 s {I1} (1960Ja12), 1.61 s {I1} (1958Mi85), 1.53 s {I2} (1954Kl36) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
J$L=2+4 ({+32}S({+3}He,p)) 
$T{-1/2}: weighted average of 31.99 min {I5} (1965Eb01), 32.06 min {I8} (1975Va02), 31.93 min {I9} (1980Wi13), and 31.98 min {I5} (1982Gr07). Others: 32.40 min {I4} (1956Gr07), 40 min {I5} (1934Fr01) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$L=0+2 ({+36}Ar(d,|a),(pol d,|a)); |DJ=1 |g to 0+ 
$T{-1/2}: mean lifetime |t in ps, from {+24}Mg({+12}C,pn|g)...: 8.1 {I9} (1971Ba98); from {+32}S({+3}He,p|g): 7.1 {I7}. Adopted weighted average: 7.5 {I6}. Other, from {+32}S({+3}He,p|g): 9 {I4} (1970Br10); also other measured T{-1/2} values: 4.0 {I+16-12} (2010Do03, |DT{-1/2} calculated by evaluators from given statistical and systematic uncertainties; another more unprecise T{-1/2} from another measurements is also given); 5.0 {I+20-15} and 6 {I2} (2007DoZV by two Doppler shift methods; they also list the effective T{-1/2}=7.3 {I6} that includes observed feeding) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$L=0+2 ({+36}Ar(d,|a),(pol d,|a)); |DJ=1 |g to 0+ 
$T{-1/2}: mean lifetime |t in ps, from {+24}Mg({+12}C,pn|g)...: 13.2 {I8} (1978En02); 14.2 {I15} (1971Ba98); from {+32}S({+3}He,p|g): 12.8 {I10} (1971Sn01); adopted weighted average: 13.2 {I6}. Other, from {+32}S({+3}He,p|g): 14 {I+11-6} (1970Br10) also other measured T{-1/2} values: 13 {I5} and 32 {I+10-14} (2007DoZV by two Doppler shift methods; they also list the effective T{-1/2}=13.8 {I15} that includes observed feeding) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$D+Q |DJ=1 gammas to 1+, 461 and 3+, 146 levels; |p=+ from L=0 in {+33}S({+3}He,d) 
$T{-1/2}: mean lifetime |t in ps, from {+32}S({+3}He,p|g): 19.4 {I14} (1971Sn01); from {+24}Mg({+12}C,pn|g)...: 22 {I4} (1971Ba98); adopted weighted average: 19.7 {I13}. Other, from {+32}S({+3}He,p|g): >14 (1970Br10) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$D+Q |DJ=1 gammas to 1+, 461 and 3+, 146 levels; |p=+ from L=0 in {+33}S({+3}He,d) 
$T{-1/2}: mean lifetime |t in fs, from {+32}S({+3}He,p|g): 2400 {I1300} (1973Ca15); 940 {I400} (1970Br11); adopted unweighted 1670 {I730} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$0,2 from D(+Q) |DJ=1 |g to 1+, 461; 2,4 from D+Q |DJ=1 |g to 3+, 146; |p=+ from L=2 in {+33}S({+3}He,d) 
$T{-1/2}: mean lifetime |t in fs, from {+24}Mg({+12}C,pn|g),.: 49 {I5} (1985La16); 47 {I5} (1984Ke01); 46 {I10} (1983Wa27); 36 {I15} (1977Da02); from {+32}S({+3}He,p|g): 100 {I30} (1973Ca15); 46 {I15} (1970Br11); adopted weighted average: 48 {I3} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$L=2+4 ({+36}Ar(d,|a),(pol d,|a)) 
T$mean lifetime |t in fs, from {+32}S({+3}He,p|g): 600 {I150} (1973Ca15); 400 {I100} (1970Br11); from {+33}S(p,|g): 800 {I400} (1985La16); 630 {I190} (1983Wa27); 600 {I350} (1977Da02); adopted weighted average: 504 {I73} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$weighted average of 2375.7 {I2} ({+33}S(p,|g)) and 2376.5 {I4} ({+32}S({+3}He,p|g)) 
J$D+Q |DJ=0 |g from 4-, 4076 ({+33}S(p,|g)); |p=+ from E2 |g to 2+, 1230 
T$mean lifetime |t in fs, from {+32}S({+3}He,p|g): 275 {I70} (1973Ca15); 260 {I75} (1970Br11); from {+33}S(p,|g): 250 {I50} (1985La16); 200 {I50} (1983Wa27) 210 {I80} (1977Da02); 150 {I50} (1973An13); adopted weighted average: 216 {I24} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$L=0+2 in {+36}Ar(d,|a),(pol d,|a) 
T$mean lifetime |t in fs, adopted from {+32}S({+3}He,p|g): 47 {I12} (1973Ca15). Others: from {+33}S(p,|g): <7 (1985La16); <5 (1983Wa27); 3.0 {I25} (1977Da02) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$1,2,3 from D |g to 2+, 2158; 1,2 excluded from D, |DJ=1 |g from J=4, 6641; |p=+ from L=2 in {+35}Cl({+3}He,|a) 
T$mean lifetime |t in fs from {+33}S(p,|g): 340 {I140} (1985La16); 210 {I60} (1983Wa27); adopted weighted average: 230 {I55}. Others, from {+33}S(p,|g): >450 (1977Da02), from {+32}S({+3}He,p|g): 820 {I350} (1973Ca15) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$L=1+3 in {+32}S({+3}He,p) 
T$adopted mean lifetime |t in ps from {+32}S({+3}He,p|g): >2 (1973Ca15); others, from {+33}S(p,|g): >1.5 (1985La16); >0.4 (1977Da02); >1 (1973An13) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=0+2 in {+36}Ar(d,|a),(pol d,|a) 
T$mean lifetime |t in fs from {+33}S(p,|g): <4 (1985La16); <10 (1983Wa27). Other: from {+32}S({+3}He,p|g): 40 {I12} (1973Ca15) 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_lifetime_unit: FS
level_comment:
J$L=2 in {+32}S({+3}He,p) 
T$mean lifetime |t in fs, from {+33}S(p,|g): 53 {I20} (1985La16); from {+32}S({+3}He,p|g): 115 {I35} (1973Ca15); adopted weighted average: 68 {I27} 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: FS
level_comment:
J$L=0+2 in {+35}Cl({+3}He,|a) 
T$mean lifetime |t in fs, from {+33}S(p,|g): 9 {I4} (1985La16): 7.5 {I17} (1984Ke01); adopted weighted average: 7.7 {I16}. Others, from {+33}S(p,|g): <10 (1983Wa27); <3 (1977Da02); from {+32}S({+3}He,p|g): <50 (1973Ca15) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$2-,3-,4- from L=3 in {+32}S({+3}He,p); 3- from D(+Q), |DJ=0 |g to 3+, 146 ({+33}S(p,|g)) 
T$mean lifetime |t in fs, from {+33}S(p,|g): 150 {I30} (1985La16); 140 {I45} (1983Wa27); from {+32}S({+3}He,p|g): 140 {I40} (1973Ca15); adopted weighted average: 145 {I21}. Other, from {+33}S(p,|g): >500 (1973An13) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
T$adopted mean lifetime |t in ps from {+24}Mg({+12}C,pn|g)...: 23 {I5} (1978Ba61). Others, from {+33}S(p,|g): >0.7 (1973An13); from {+32}S({+3}He,p|g): >2 (1973Ca15) 
J$0-,4- from E2 |DJ=2 |g to 2-,2721; 2,4 from D(+Q) |DJ=1 |g to 3+, 146 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$4-,5-,6- from L=5 in {+32}S(|a,d), {+32}S({+3}He,p); 3,5 from D |DJ=1 |g to 4+, 2376 
T$adopted mean lifetime |t in ps from {+24}Mg({+12}C,pn|g)...: 280 {I60} (1978Ba61). Others, from {+33}S(p,|g): >1.1 (1985La16), >0.7 (1977Da02), from {+32}S({+3}He,p|g): >3 (1973Ca15) 


level_energy_unit: KEV
level_spin_parity: (3,4,5+)
level_lifetime_unit: FS
level_comment:
J$1+,2,3,4,5+ from D,E2 |g to 3+, 146; 1,2 less likely from no |g (or weak) to 0+, g.s. 
T$mean lifetime |t in fs: 220 {I90} ({+33}S(p,|g)) 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: FS
level_comment:
J$|p=- from L=1 in {+33}S({+3}He,d); |DJ=(1) E1 |g to 0+, g.s. 
T$mean lifetime |t in fs from {+33}S(p,|g): 110 {I20} (1985La16); 55 {I15} (1983Wa27), and from {+32}S({+3}He,p|g): 115 {I30} (1973Ca15); mean value: 93 {I19} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=0 in {+36}Ar(p,{+3}He) and isobaric analog state of {+34}Ar state from {+36}Ar(p,t) reaction (1969Br21) 
T$from {+33}S(p,|g) 


level_energy_unit: KEV
level_spin_parity: (2,3,4)+
level_lifetime_unit: FS
level_comment:
J$(2,3,4) from gammas to 2+, 2157; 3+, 146; and 4+, 2376; |p=+ from L=2 in {+35}Cl({+3}He,|a) 
T$mean lifetime |t in fs: 90 {I70} (1985La16); 160 {I60} (1977Da02). Adopted weighted average: 130 {I46} 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$weighted average of 3982.1 {I3} ({+35}Cl({+3}He,|a)), 3983.0 {I5} ({+32}S({+3}He,p)), and 3983.5 {I2} ({+33}S(p,|g)) 
J$D(+Q), |DJ=0 |g to 3+, 146 ({+33}S(p,|g)); |p=- from L=3 in {+35}Cl({+3}He,|a) 
T$mean lifetime |t in fs from {+33}S(p,|g): 200 {I40} (1985La16); 165 {I60} (1983Wa27); adopted weighted average: 189 {I33}. Other >100 (1973An13) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$4-,5-,6- from L=5 in {+32}S(|a,d); 2,4 from D(+Q) |DJ=1 |g to 3+, 2181 (1977Da03) 
T$adopted mean lifetime |t in ps, from {+32}S({+3}He,p|g): 1.3 {I+17-6} (1973Ca15). Others, from {+33}S(p,|g) in fs: >500 (1977Da02); >250 (1973An13) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$L=1+3 in {+32}S({+3}He,p); L({+3}He,d)=1+3 from 3/2+ target 
T$mean lifetime |t in fs from {+33}S(p,|g): 150 {I60} (1985La16); 120 {I40} (1983Wa27). Adopted weighted average: 129 {I33} 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: FS
level_comment:
J$L=0+2 ({+35}Cl({+3}He,|a)) 
T$mean lifetime |t in fs {+33}S(p,|g): 7 {I3} (1985La16); 11 {I9} (1977Da02). Adopted weighted average: 7.4 {I28} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$0-,1-,2- from L=1 in {+32}S({+3}He,p); 0- and 2- excluded from D,E2 |g to 2+, 2157, and D,E2 |g to 0+, g.s. 
T$mean lifetime |t in fs, from {+33}S(p,|g): 43 {I8} (1985La16); from {+32}S({+3}He,p|g): 65 {I20} (1973Ca15); adopted weighted average: 46 {I8}. Other, from {+33}S(p,|g): <10 (1983Wa27) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$2-,3-,4- from L=3 in {+32}S({+3}He,p); 3-,4- less likely from gammas to 1+, 665 and 1+, 461 
T$mean lifetime |t in fs from {+33}S(p,|g): 35 {I11} (1985La16) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
J$2-,3-,4- from L=3 in {+32}S({+3}He,p); 3- excluded from D |DJ=1 |g to 3+, 146 ({+33}S(p,|g)); 2- excluded from D |DJ=1 |g from 5(-), 6870 
T$mean lifetime |t in fs from {+33}S(p,|g): 165 {I35} (1985La16); 180 {I60} (1983Wa27); 160 {I60} (1977Da02). Adopted weighted average: 167 {I27} 


level_energy_unit: KEV
level_spin_parity: (2,3,4)-
level_lifetime_unit: FS
level_comment:
J$|p=- from L=1 in {+33}S({+3}He,d) 
T$mean lifetime |t in fs, from {+33}S(p,|g): 370 {I250} (1985La16); from {+32}S({+3}He,p|g): 200 {I60} (1973Ca15) adopted weighted average: 209 {I58} 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$L=1+3 in {+32}S({+3}He,p) 
T$mean lifetime |t in fs from {+33}S(p,|g): 15 {I5} (1985La16); 15 {I7} (1983Wa27); adopted weighted average: 15 {I4} 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_lifetime_unit: PS
level_comment:
J$1,2,3: 1,2,3,4- from D,E2 |g to 2-, 2721; 0+,1,2,3,4+ from D,E2 |g to 2+, 2158. |p=(-) from L=1 in {+33}S({+3}He,d) and {+35}Cl({+3}He,|a) if these can be confirmed to pertain to this level 
T$mean lifetime |t in fs: 350 {I240} ({+33}S(p,|g)) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$L=(3) in {+36}Ar(p,{+3}He) and isobaric analog state of {+34}Ar state from {+36}Ar(p,t) (1969Br21) 


level_energy_unit: KEV
level_spin_parity: 0+,1,2,3,4+
level_lifetime_unit: FS
level_comment:
J$D,E2 |g to 2+, 2158 
T$mean lifetime |t in fs from {+33}S(p,|g): 9 {I4} (1985La16, adopted). Other: <10 (1983Wa27) 


level_energy_unit: KEV
level_spin_parity: 1+,2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$1+,2,3+ from D,E2 |g to 3+, 146 and 1+, 461; 3+ excluded by RUL for I(4717)|g<1% to 0+, g.s. 
T$mean lifetime |t in fs from {+33}S(p,|g): <13 (1985La16) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: PS
level_comment:
J$6 from: 4,6 from D+Q |DJ=1 |g 5-, 3631; 2,6 from Q |DJ=2 |g to 4-, 3600; |p=- from |DJ=3 E3 |g to 3+ 
T$mean lifetime |t in ps from {+24}Mg({+12}C,pn|g)...: 7 {I3} (1978Ba61, adopted); other: >3 (1978Ba39) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
E$weighted average of 4824.10 {I9} ({+24}Mg({+12}C,pn|g)...), 4824.5 {I2} ({+33}S(p,|g)), and 4824.8 {I24} ({+32}S({+3}He,p)) 
J$3 to 7+ from L=4,6 in {+32}S(|a,d); 1,5 from Q |DJ=2 |g to 3+, 146 ({+24}Mg({+12}C,pn|g)...) 
T$mean lifetime |t in fs, from {+24}Mg({+12}C,pn|g)...: 450 {I200} (1982Va02), and from {+33}S(p,|g): 480 {I220} (1983Wa27); adopted weighted average: 464 {I148}. Other, from {+33}S(p,|g): >500 (1985La16) 


level_energy_unit: KEV
level_spin_parity: 0:4+
level_comment:
E$weighted average of 4925 {I4} ({+34}S({+3}He,t)), 4930 {I20} ({+32}S(|a,d)), 4939 {I11} ({+35}Cl({+3}He,|a)) 
J$L=2 in {+35}Cl({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$0 to 4+ from L=2 in {+35}Cl({+3}He,|a); 0,1,2 from D,Q |g to 0+ g.s.; 1+,2,3 from D,E2 |g to 3+, 146 
T$mean lifetime |t in fs from {+33}S(p,|g): <17 (1985La16) 


level_energy_unit: KEV
level_spin_parity: (0)+
level_uncertain: ?
level_comment:
E$reported in {+36}Ar(p,{+3}He) and {+36}Ar(d,|a),(pol d,|a) (both measurements from 1969Br21); because of the high uncertainty it is not clear if this is a stand-alone peak or might be associated with another known peak 
J$L=0 in {+36}Ar(p,{+3}He) (and {+36}Ar(d,|a),(pol d,|a)) and isobaric analog state of {+34}Ar state from {+36}Ar(p,t) reaction (also studied by 1969Br21) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: FS
level_comment:
J$L=0+2 in {+35}Cl({+3}He,|a) 
T$mean lifetime |t in fs from {+33}S(p,|g): 7 {I4} (1985La16, adopted). Other: <5 (1983Wa27) 


level_energy_unit: KEV
level_spin_parity: 4
level_lifetime_unit: FS
level_comment:
J$1+,2,3,4,5+ from D,E2 |g to 3+, 146; 4,6 from D |DJ=1 from 5(-), 6870 
T$mean lifetime |t in fs from {+33}S(p,|g): 90 {I35} (1985La16); 60 {I30} (1977Da02). Adopted weighted average: 73 {I23} 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
J$3+,7+ from E2 |DJ=2 |g to 5+, 4824; 5,7 from D, |DJ=1 |g to 6-, 4743 
T$mean lifetime |t in ps from {+24}Mg({+12}C,pn|g)...: 94 {I12} (1978Ba39) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$3,7 from |DJ=2, Q |g from 5(-), 6870 
T$mean lifetime |t in fs from {+33}S(p,|g): >1000 (1977Da02) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$(2,3,4+) from |g to 3+, 146, |g to 3-, 3545, and |g to 2+, 1230; (2) less likely from no |g (or weak) to 0+, g.s.; |g to (1)- 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: EV
level_comment:
J$D |DJ=0 |g to 3-, 3984 (and to 3-, 3545 and 3+, 146); |p=(-) from no |g (or weak) to 1+, 665 
T$from {+33}S(p,|g) (1977Da03) 


level_energy_unit: KEV
level_spin_parity: (3-,4)
level_comment:
J$(2+,3,4+) from gammas to 4+, 2376 and 2+, 1887; (2,3+) less likely from no |g (or weak) to 1+, 461 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
J$(2,3,4) from gammas to 3+, 146 and 3-, 3545; (2,3,4+) less likely from no |g (or weak) to 2+, 2158 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
J$(1+,2,3,4+) from gammas to 3+, 146 and 2+, 1887; (1,2,3+) less likely from no |g (or weak) to 1+, 665 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_lifetime_unit: EV
level_comment:
J$D |DJ=0 |g to 5-, 3632; |p=(-) from intense transition to 3-, 5540 and no or weak transition to 3+, 146 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: KEV
level_comment:
E$from {+33}S(p,|g) and {+33}S(p,p); uncertainty from {+33}S(p,p) 
$Member of triplet resonance in 1977Da02 ({+33}S(p,|g)) together with 6984.5 and 6990.3 
J$1- from {+33}S(p,p), which differs from (2-,3) from {+33}S(p,|g). However the components of the triplet resonance are insufficiently separated in order to allow the proper assignment of the |g branching (1977Da02) 
J$assignment based on |g branching ({+33}S(p,|g), 1977Da02): (1,2,3) from |g to 2+, 2158 and |g to 2-, 2721; (2-,3) from |g to 4-, 3600 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
E$weighted average of: 6990.7 {I19}, 6992.6 {I10} (both from {+33}S(p,|g)), and 6991.2 {I15} ({+33}S(p,p)) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_comment:
J$3 from D(+Q) |DJ=0 |g to 3+, 146; |p=- from L=1 in {+33}S(p,p) 
T$weighted average |G of 1.0 {I1} ({+33}S(p,p),1989Va15) and 0.787 {I30} ({+33}S(p,|g),1977Da03) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
E$weighted average of 7250.0 {I6} ({+24}Mg({+12}C,pn|g)...) and 7249.8 {I10} ({+33}S(p,|g)) 
T$mean lifetime |t in ps from {+24}Mg({+12}C,pn|g)...: 0.20 {I7} 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E$weighted average of 7673.5 {I15} ({+33}S(p,p)) and 7675.8 {I10} ({+33}S(p,|g)) 
J$(D+Q) |DJ=(0) |g to 2+, 2158; |p=+ from L=2 in {+33}S(p,p) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
E$weighted average of 7802.4 {I11} ({+24}Mg({+12}C,pn|g)...) and 7803.8 {I10} ({+33}S(p,|g)) 
T$mean lifetime |t in ps from {+33}S(p,|g): 0.10 {I7} (1978Ba39) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: PS
level_comment:
J$D |DJ=1 |g to 0+ g.s. 
T$mean lifetime |t in ps: 7.1 {I7} (1971Sn01); 9 {I4} (1970Br10); adopted: 7.1 {I7} 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: PS
level_comment:
J$D |DJ=1 |g to 0+ g.s. 
T$mean lifetime |t in ps: 12.8 {I10} (1971Sn01); 14 {I+11-6} (1970Br10); adopted: 12.8 {I10} 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: PS
level_comment:
J$D+Q |DJ=1 |g to J=1, 461 level 
T$mean lifetime |t in ps: 19.4 {I14} (1971Sn01); >14 (1970Br10); adopted: 19.4 {I14} 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: PS
level_comment:
J$D+Q |DJ=1 |g to J=1, 461 level 
T$mean lifetime |t in fs: 2400 {I1300} (1973Ca15); 940 {I400} (1970Br11); adopted unweighted 1670 {I730} 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$mean lifetime |t in fs: 100 {I30} (1973Ca15); 46 {I15} (1970Br11); adopted unweighted average: 73 {I27} 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$mean lifetime |t in fs: 600 {I150} (1973Ca15); 400 {I100} (1970Br11); adopted weighted average: 462 {I83} (external uncertainty) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$mean lifetime |t in fs: 275 {I70} (1973Ca15); 260 {I75} (1970Br11); adopted weighted average: 268 {I51} 


level_energy_unit: KEV
level_spin_parity: (1)
level_lifetime_unit: FS
level_comment:
J$(D) |DJ=1 |g to 0+ g.s. 
E$from 1983Wa27 ({+33}S(p,|g)). Others: 2.58 MeV (1973Ca15); 2587 (1970Sy01) 
T$mean lifetime |t in fs: 47 {I12} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 2.61 MeV (1973Ca15) 
T$mean lifetime |t in fs: 820 {I350} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.13 MeV (1973Ca15) 
T$mean lifetime |t in fs: 40 {I12} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.33 MeV (1973Ca15) 
T$ mean lifetime |t in FS: 115 35 (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.38 MeV (1973Ca15) 
T$mean lifetime |t in fs: <50 (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.55 MeV (1973Ca15) 
T$mean lifetime |t in fs: 140 {I40} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.60 MeV (1973Ca15) 
T$mean lifetime |t in ps: >2 (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.63 MeV (1973Ca15) 
T$mean lifetime |t in ps: >3 (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 3.77 MeV (1973Ca15) 
T$mean lifetime |t in fs: 115 {I30} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 4.08 MeV (1973Ca15) 
T$mean lifetime |t in ps: 1.3 {I+17-6} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 4.14 MeV (1973Ca15) 
T$mean lifetime |t in fs: 150 {I50} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 4.35 MeV (1973Ca15) 
T$mean lifetime |t in fs: 65 {I20} (1973Ca15) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1983Wa27 ({+33}S(p,|g)). Others: 4.46 MeV (1973Ca15) 
T$ mean lifetime |t in FS: 200 60 (1973Ca15) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from weighted average of 1.526 s {I2} (1973Ry01), 1.5252 s {I11} (1976Wi08), 1.5277 s {I22} (1983Ko22), and 1.5268 s {I5} (2006Ia05); other: 1.534 s {I3} (1972Ha82, superseded by 2006Ia05) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_lifetime_info: ;ISO=M
level_comment:
E$based on E|g; other: 146.52 {I26} (2012Er02) 
T$from weighted average of 31.99 min {I5} (1965Eb01), 32.06 min 8 (1975Va02), 31.93 min {I9} (1980Wi13), and 31.98 min {I5} (1982Gr07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
%EC+%B+$Adopted value 
T$weighted average of: 1.5268 s {I5} (2006Ia05), 1.5277 s {I22} (1983Ko22), 1.5252 s {I11} (1976Wi08), 1.526 s {I2} (1973Ry01); others: 1.534 s {I3} (1972Ha82), 1.565 s {I7} (1965Eb01), 1.560 s 14 (1961Ja22), 1.58 s {I1} (1960Ja12), 1.61 s {I1} (1958Mi85), 1.53 s {I2} (1954Kl36) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: PS
level_comment:
J$D |DJ=1 |g to 0+ g.s. 
T$mean lifetime |t in ps: 13.2 {I8} (1978En02); 14.2 {I15}(1971Ba98); adopted weighted average: 13.4 {I7} 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 49 5 (1985La16); 47 5 (1984Ke01); 46 10 (1983Wa27); 36 15 (1977Da02). Weighted average: 47 3 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 800 400 (1985La16); 630 190 (1983Wa27); 600 350 (1977Da02). Weighted average: 649 154 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 250 50 (1985La16); 200 50 (1983Wa27) 210 80 (1977Da02); 150 50 (1973An13). Weighted average: 201 27 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 340 140 (1985La16); 210 60 (1983Wa27); GT 450 (1977Da02). Weighted average: 230 55 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: LT 4 (1985La16); LT 10 (1983Wa27). Weighted average (of 2 2 AND 5 5): 2.4 19 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 9 4 (1985La16): 7.5 17 (1984Ke01); 10 LT (1983Wa27); LT 3 (1977Da02). Weighted average (of 9 4 and 7.5 17): 7.7 16 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 150 30 (1985La16); 140 45 (1983Wa27); GT 500 (1973An13). Weighted average (of 150 30 and 140 45): 147 25 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 200 40 (1985La16); 165 60 (1983Wa27); GT 100 (1973An13). Weighted average (of 200 40 and 165 60): 189 33 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$ mean lifetime |t in fs: 165 35 (1985La16); 180 60 (1983Wa27); 160 60 (1977Da02). Weighted average: 167 27 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.08 {I4} 
$E(p)(lab)=447 {I1} 
$ E(p)(lab)=446.5 36 (1959Ku79), 445 (2011Fr04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.7 {I2} 
$E(p)(lab)=507.6 {I2} 
$ E(p)(lab)=507 1 (1964Gl04), 507.1 10 (1959Ku79), 507 (2011Fr04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.16 8 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.5 {I2} 
$E(p)(lab)=731.4 {I3} 
$ E(p)(lab)=731 1 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.050 25 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.0 {I3} 
$E(p)(lab)=974.61 {I4} (1994Li20), 974.83 {I16} (1983Ra04), 976 {I2} (1964Gl04) 
E$unweighted average of 6088.84 {I8} (from E(p)(lab)=974.61 {I4} in 1994Li20) and 6088.97 {I8} (from |g cascades in 1994Li20) 
S$from 1983Wa27 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.6 {I2} 
$E(p)(lab)=1023.4 {I11} 
$ E(p)(lab)=1023 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.02 1 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.9 {I5} 
$E(p)(lab)=1029.1 {I11} 
$ E(p)(lab)=1029 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.15 8 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.5 {I7} 
$E(p)(lab)=1057.3 {I11} 
$ E(p)(lab)=1058 (1971Hy02); 1057 (1969Gr29); 1057 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.45 23 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=3.6 {I5} 
$E(p)(lab)=1069.7 {I2} 
$ E(p)(lab)=1071.1 11 (1977Da02); 1071 (1969Gr29); 1071 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.6 3 (1964Gl04); 3.6 5 (1977Da02) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.2 {I10} 
$E(p)(lab)=1096.5 {I12} 
$ E(p)(lab)=1098 (1973An13,1971Hy02); 1096 (1969Gr29); 1096 2 
$ (1964Gl04) (2J+1)|G{-p}|G{-|g}/|G=0.29 15 (1964Gl04) 
T$ mean lifetime |t in fs: LT 2 (1973An13) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.2 {I3} 
$E(p)(lab)=1118.5 {I3} 
$ E(p)(lab)=1119.6 12 (1977Da02); 1121 (1971Hy02); 1119 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.21 11 (1964Gl04); 0.9 3 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.7 {I10} 
$E(p)(lab)=1164.5 {I13} 
$ E(p)(lab)=1165 (1969Gr29); 1165 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.8 4 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.9 {I7} 
$E(p)(lab)=1215.2 {I13} 
$ E(p)(lab)=1214 (1969Gr29); 1214 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.19 10 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.4 {I2} 
$E(p)(lab)=1255.4 {I13} 
$ E(p)(lab)=1255 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.050 25 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.7 {I6} 
$E(p)(lab)=1264.4 {I2} 
$ E(p)(lab)=1266.4 13 (1977Da02); 1266 (1969Gr29); 1266 2 (1964Gl04) 
$ (2J+1)|G{-p}|G{-|g}/|G=2.5 8 (1977Da02); 0.23 12 (1964Gl04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.9 {I3} 
$E(p)(lab)=1347.3 {I2} 
$ E(p)(lab)=1348.9 14 (1977Da02); 1346.5 15 (1973An13) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.1 
$E(p)(lab)=1506.7 {I20} (1973An13) only; adjusted to 1509.9 to match the energy scale of 1977Da02 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=3.8 {I6} 
$E(p)(lab)=1543.49 {I5} (1994Li20); 1543.6 {I2} (1983Wa27); 1545.4 {I15} (1977Da02); 1542 (1975Ke11); 1542.0 20 (1973An13) 
E$unweighted average of 6640.85 {I9} (from E(p)(lab)=1543.49 {I5} in 1994Li20) and 6640.97 {I3} (from |g cascades in 1994Li20) 
$(2J+1)|G{-p}|G{-|g}/|G=3.8 {I6} (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.0 {I4} 
$E(p)(lab)=1629.4 
$ E(p)(lab)=1630.3 16 (1977Da02); 1626.5 20 (1973An13) 
$ (2J+1)|G{-p}|G{-|g}/|G=0.9 4 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.4 {I2} 
$E(p)(lab)=1780.7 {I3} 
$ E(p)(lab)=1782.2 16 (1977Da02) 
$ (2J+1)|G{-p}|G{-|g}/|G=1.6 8 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.9 {I10} 
$E(p)(lab)=1798.1 {I3} 
$ E(p)(lab)=1799.3 16 (1977Da02); 1796.4 20 (1973An13) 
$ (2J+1)|G{-p}|G{-|g}/|G=2.0 6 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.4 {I6} 
$E(p)(lab)=1812.3 {I3} 
$ E(p)(lab)=1813.4 16 (1977Da02); 1809.5 20 (1973An13) 
$ (2J+1)|G{-p}|G{-|g}/|G=2.8 9 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.7 {I3} 
$ E(p)(lab)=1898 {I1} 
$Same as the 1898 {I2} component of the triplet resonance E(p)(lab)=1898 {I1} (1977Da02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.7 {I10} 
$E(p)(lab)=1900 
$Resonance triplet E(p)(lab)=1898 {I2}, 1900 {I2}, 1904 {I2} (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.7 {I3} 
$ E(p)(lab)=1904 {I2} (1977Da02) 
$Component of a triplet resonance in 1977Da02 that might Be same E(p)(lab)=1906 {I1} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=8 {I2} 
$E(p)(lab)=1974.4 {I3} 
$ E(p)(lab)=1974 1 (1992Ka39); 1975.3 18 (1977Da02) 
$ (2J+1)|G{-p}|G{-|g}/|G=8 2 (1992Ka39); 8 2 (1977Da02) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=4.4 {I20} 
$E(p)(lab)=1994.86 {I7} (1994Li20); 1997.2 {I18} (1977Da02) 
E$unweighted average of 7078.83 {I10} (from E(p)(lab)=1994.86 {I7} in 1994Li20) and 7079.00 {I6} (from |g cascades in 1994Li20) 
S$from 1983Wa27 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=128.0 
$E(p)(lab)=1444.8 keV 
$ E(p)(lab)=1445 2 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=0.19 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=25.0 
$E(p)(lab)=1714.7 keV 
$ E(p)(lab)=1713 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=0.6 EV; |G=6 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=42.0 
$E(p)(lab)=1751.5 keV 
$ E(p)(lab)=1748 2 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=17 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=15.0 
$E(p)(lab)=1801.0 keV 
$ E(p)(lab)=1799 2 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=5 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=80.0 
$E(p)(lab)=1846.4 keV 
$ E(p)(lab)=1845 2 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=21 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=8.2 
$E(p)(lab)=1900.0 keV 
$ E(p)(lab)=1902 2 (1964Va12), probable 1900.0+1904.6 
$ (2J+1)|G{-p0}|G{-p1}/|G=1.0 EV; |G=5 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=38.6 
$E(p)(lab)=2041.6 keV 
$ E(p)(lab)=2044 3 (1964Va12), probable 2041.6+2048 
$ (2J+1)|G{-p0}|G{-p1}/|G=11 EV; |G=18 KEV 3 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=13.0 
$E(p)(lab)=2115.7 keV 
$ E(p)(lab)=2114 2 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=10 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=15.9 
$E(p)(lab)=2133.8 keV 
$ E(p)(lab)=2131 2 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=7 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=6.4 
$E(p)(lab)=2439.3 keV 
$ E(p)(lab)=2435 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=3.0 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=170.0 
$E(p)(lab)=2461 keV 
$ E(p)(lab)=2460 3 (1964Va12); could be a mixture of three resonances in this energy range 
$ (2J+1)|G{-p0}|G{-p1}/|G=60 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=0.52 
$E(p)(lab)=2546.0 keV 
$ E(p)(lab)=2541 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=3.1 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=110.0 
$E(p)(lab)=2582 keV 
$ E(p)(lab)=2578 4 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=460 EV; |G=39 KEV 5 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=6.6 
$E(p)(lab)=2607.7 keV 
$ E(p)(lab)=2604 3 (1964Va12); probably 2607.7+2608.5 
$ (2J+1)|G{-p0}|G{-p1}/|G=280 EV; |G=6 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=1.81 
$E(p)(lab)=2625.2 keV 
$ E(p)(lab)=2625 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=60 EV (1964Va12) 
J$possible (2)+ (1989Va15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=18.2 
$E(p)(lab)=2654.8 keV 
$ E(p)(lab)=2652 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=490 EV; |G=7 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=27.0 
$E(p)(lab)=2766.1 keV 
$ E(p)(lab)=2763 4 (1964Va12); probably 2764.1+2766.1 
$ (2J+1)|G{-p0}|G{-p1}/|G=210 EV; |G=8 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=4.0 
$E(p)(lab)=2871.1 keV 
$ E(p)(lab)=2865 4 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=9 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1:4)+
level_comment:
$E(p)(lab)=2886.6 keV 
$ E(p)(lab)=2883 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=3.6 EV, (2J+1)|G{-p0}|G{-p2}/|G=6 EV (1964Va12) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2896 {I3} (1964Va12) 
$(2J+1)|G{-p0}|G{-p1}/|G<3.6 eV, (2J+1)|G{-p0}|G{-p2}/|G=3.5 eV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=3.5 
$E(p)(lab)=2918.5 keV 
$ E(p)(lab)=2915 3 (1964Va12); probable 2910.9+2918.5 
$ (2J+1)|G{-p0}|G{-p2}/|G=10 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=55.0 
$E(p)(lab)=2929.0 keV 
$ E(p)(lab)=2921 4 (1964Va12), energy matching based on widths in 1989Va15 and 1964Va12; may contain 2920.9 and 2918.5 
$ (2J+1)|G{-p0}|G{-p1}/|G=600 EV; |G=24 KEV 4 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=35.0 
$E(p)(lab)=2972.6 keV 
$ E(p)(lab)=2969 4 (1964Va12); may contain 2965.6 
$ (2J+1)|G{-p0}|G{-p1}/|G=450 EV; |G=13 KEV 3 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=12.1 
$E(p)(lab)=2988.6 keV 
$ E(p)(lab)=2984 4 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=270 EV, (2J+1)|G{-p0}|G{-p2}/|G=18 EV; |G=6 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=1.6 
$E(p)(lab)=2993.7 keV 
$ E(p)(lab)=2988 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p2}/|G=10 EV (1964Va12) 
J$possible (1)+ (1989Va15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=30.0 
$E(p)(lab)=3034.3 keV 
$ E(p)(lab)=3029 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G<25 EV; (2J+1)|G{-p0}|G{-p2}/|G=100 EV (1964Va12); |G=4 KEV 2 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2)-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=9.4 
$E(p)(lab)=3053.8 keV 
$ E(p)(lab)=3048 4 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=16 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=7.0 
$E(p)(lab)=3075.4 keV 
$ E(p)(lab)=3070 4 (1964Va12); probable 3066.4+3075.4 
$ (2J+1)|G{-p0}|G{-p1}/|G=7 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=140.8 
$E(p)(lab)=3097.9 keV 
$ E(p)(lab)=3093 4 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p1}/|G=700 EV; |G=18 KEV 3 (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|g{+2}=2.1 
$E(p)(lab)=3104.5 keV 
$ E(p)(lab)=3100 3 (1964Va12) 
$ (2J+1)|G{-p0}|G{-p2}/|G=50 EV (1964Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2)-
level_comment:
$E(p)(lab)=3113.8 keV 
$ E(p)(lab)=3109 3 (1964Va12); probable 3108.0+3113.8 
$ (2J+1)|G{-p0}|G{-p2}/|G=14 EV (1964Va12) 


level_energy_unit: KEV
level_spin_parity: (0:5)
level_comment:
S$for L=1+3: 0.0060 {I5} for L=1, 0.022 {I2} for L=3. For L=2, value is 0.200 {I8} 
$E(p)(res)=195 {I2} 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
$E(p)(res)=292.2 {I14} from adopted value of E{-x}=5435.4 {I14} in Table 2 of 2014Pa44. Resonance strength |w|g=0.082 meV {I+18-21} 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
$E(p)(res)=310.2 {I14} from adopted value of E{-x}=5453.4 {I14} in Table 2 of 2014Pa44. Resonance strength |w|g=0.028 meV {+10-8} 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
$E(p)(res)=434.3 {I7} from adopted value of E{-x}=5577.5 {I7} in Table 2 of 2014Pa44. Resonance strength |w|g=50 meV {I8} 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
S$for L=1+3: 0.0081 {I7} for L=1, 0.054 {I2} for L=3. Value for L=2 is 0.247 {I4} 
$E(p)(res)=492.5 {I2}. Resonance strength |w|g=65 meV {I10} 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_comment:
$E(p)(res)=642.1 {I9} from adopted value of E{-x}=5785.3 {I9} in Table 2 of 2014Pa44. Resonance strength |w|g=50 meV {I25} 


level_energy_unit: KEV
level_spin_parity: (0:5)-
level_comment:
S$0.0028 {I6} for L=1, 0.016 {I1} for L=3 
$E(p)(res)=662.7 {I10}. Resonance strength |w|g=50 meV {I25} 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
S$0.012 {I1} for L=1, 0.039 {I3} for L=3 
$E(p)(res)=709.6 {I3}. Resonance strength |w|g=63 meV {I25} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1$using NMR method (1972Bl07) 
MOME2$using the method atomic beam magnetic resonance (1972St38). Others: -0.076 {I5} (1986El09), -0.817 {I8} (1993Su36), 0.0819 {I11} (2000Ha64), 0.0850 {I11} (2004Al08); also from 2011StZZ. 
J$spin from microwave spectroscopy and atomic beam methods (1948To10,1949Da14), parity from L(pol d,{+3}He)=2 and L-1/2 from analyzing power 
$Evaluated rms charge radius=3.365 fm {I15} (2004An14 evaluation), 3.365 fm {I19} from 2008 update of 2004An14. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,{+3}He)=0 
T$weighted average of 146 fs {I62} from (|a,p|g), 106 fs {I14} from (p,|g), 201 fs {I28} from ({+34}S,n|g), 90 fs {I21} from (|g,|g), 139 fs {I56} from (n,n'|g), 150 fs {I35} from (p,p'|g), 150 fs {I20} from coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$L(d,n)=2; |DJ=1, M1+E2 |g to 3/2+ 
T$weighted average of 0.38 ps {I11} from (|a,p|g), 0.35 ps {I6} from (p,|g), 0.374 ps {I49} from ({+34}S,n|g), 0.43 ps {I20} from (p,p'|g), 0.41 ps {I4} from coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2; |g|g(DCO) in (HI,xn|g) 
T$weighted average of 208 fs {I62} from (|a,p|g), 146 fs {I21} from (p,|g), 187 fs {I62} from (n,n'|g), 165 fs {I35} from (p,p'|g) and 180 fs {I60} from coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L({+3}He,d)=L(d,{+3}He)=2; p'|g(|q) and |g-polarization in (p,p'|g) 
T$weighted average of 49 fs {I21} from (|a,p|g), 14 fs {I2} from (p,|g), 24 fs {I7} from (|g,|g), 43 fs {I6} from (n,n'|g) and 44 fs {I11} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d, {+3}He)=2 and L+1/2 from analyzing power 
T$weighted average of 33 fs {I6} from (|a,p|g), 13 fs {I2} from (p,|g), 17 fs {I7} from (|g,|g), 50 fs {I9} from (n,n'|g), 18 fs {I9} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$L(pol d, {+3}He)=3 and L+1/2 from analyzing power 
T$weighted average of 34 ps {I3} from (|a,p|g), 25.6 ps {I28} from (p,|g), 32 ps {I4} from (p,p'|g) and 30.9 ps {I6} from (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
J$|g(|q) in (|a,p|g) and |g|g(DCO) in (HI,xn|g) 
T$weighted average of 229 fs {I35} in (|a,p|g) and 173 fs {I41} in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$({+3}He,d)=1 and |g(|q) in (p,|g) 
T$weighted average of 21 fs {I9} from (|a,p|g) and 14 fs {I2} from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$L({+3}He,d)=1; |g(|q) and |g-polarization in (p,|g) 
T$weighted average of 47 fs {I17} from (|a,p|g) and 24 fs {I3} from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$p|g(|q) and |g-polarization in (|a,p|g) and |g|g(DCO) in (HI,xn|g) 
T$weighted average of 2.0 ps {I7} in (|a,p|g), 0.229 ps {I42} in (p,|g) and 0.91 ps {I19} in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$p|g(|q) and |g-polarization in (|a,p|g) and |g|g(DCO) (HI,xn|g) 
T$weighted average of 6.4 ps {I6} in (|a,p|g) and 5.3 ps {I10} in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 55 fs {I28} (1971Wi13), 121 fs {I14} (1972Hu11), 104 fs {I29} (1973Fa07), 100 fs {I21} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$3/2+,from 1967Ko20 and 1967Ko23, (5/2,7/2) from 1971Wi13 
T$weighted average of 177 fs {I45} (D), 139 fs {I21} (O) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$(3/2,5/2) from 1971Wi13 
T$weighted average of 15 fs {I2} (1972Hu11), 13 fs {I4} (1973Fa07), 14 fs {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 55 fs {I28} (1971Wi13), 15 fs {I2} (1972Hu11), 10 fs {I3} (1973Fa07), 11 fs {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J$from |g-feeding 
T$weighted average of 73 fs {I23} (1971Wi13), 38 fs {I4} (1972Hu11), 24 fs {I6} (1976Me12) 
$|G=6.5 keV {I22} (1971Wi13) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=754.3 {I7} 
E$weighted average from E,O 
J$from 1976Me12 
$|w|g=0.04 eV (1963Ha32) 
$|w|g=0.5 eV {I3} (1972Hu10) 
$|w|g=0.50 eV {I15} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-p}=831.8 {I8} 
$|w|g=0.4 eV {I2} (1972Hu10) 
$|w|g=0.30 eV {I9} (1976Me12) 
$|w|g=0.14 eV {I2} (2001Vo24) 
$|G{-|g} |> 0.07 eV (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)+
level_comment:
$E{-p}=848.2 {I7} 
J$from 1960An06 
$|w|g=0.17 eV (1963Ha32) 
$|w|g=1.1 eV {I3} (1972Hu10) 
$|w|g=1.2 eV {I4} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$E{-p}=880.1 {I8} 
$|w|g=0.073 eV (1963Ha32) 
$|w|g=0.4 eV {I2} (1972Hu10) 
$|w|g=0.30 eV {I9} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=888.8 {I8} 
$|w|g=0.23 eV (1963Ha32) 
$|w|g=1.3 eV {I4} (1972Hu10) 
$|w|g=1.9 eV {I6} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
$E{-p}=928.6 {I9} 
J$from 1960An06 
$|w|g=0.31 eV (1963Ha32) 
$|w|g=1.4 eV {I4} (1972Hu10) 
$|w|g=2.2 eV {I7} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=1020.6 {I8} 
$|w|g=0.48 eV (1963Ha32) 
$|w|g=3.2 eV {I10} (1972Hu10) 
$|w|g=2.5 eV (1973Fa07) 
$|w|g=3.1 eV {I9} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_comment:
$E{-p}=1055.6 {I10} 
$|w|g=0.67 eV (1963Ha32) 
$|w|g=0.4 eV {I2} (1972Hu10) 
$|w|g=0.4 eV (1973Fa07) 
$|w|g=0.50 eV {I15} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=1112.3 {I6} 
J$from 1972LeYW 
$|w|g=0.3 eV {I2} (1972Hu10) 
$|w|g=0.3 eV (1973Fa07) 
$|w|g=0.40 eV {I12} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_comment:
$E{-p}=1182.0 {I7} 
J$from 1977Ko35 
$|w|g=0.2 eV {I1} (1972Hu10) 
$|w|g=0.3 eV (1973Fa07) 
$|w|g=0.40 eV {I12} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E{-p}=1212.5 {I4} 
J$3/2 from 1976Me12 
$|w|g=2 eV (1963Ha32) 
$|w|g=21 eV {I3} (1966En04) 
$|w|g=2.6 eV {I4} (1967Wa22) 
$|w|g=9.7 eV {I9} (1974Al04) 
$|w|g=9.8 eV {I10} (1975Ke11) 
$|w|g=21 eV {I3} (1976Me12) 
$|w|g=9 eV {I1} (1979Pa16) 
$|w|g=9.7 eV {I7} (1976Sp08) 
$|w|g=9.7 eV {I7} (1996Ka21) 
$|w|g=9.9 eV {I7} (2001Vo24) 
$|w|g=9.5 eV {I12} deduced from |w|g for E{-p}=1891 in 1981Bi05 and relative strength in 1976Sp08 (1981Bi05) 
$|G=5.8 eV {I13}, |G{-p}=3.8 eV {I13}, |G{-|g}=2.0 eV {I13} (1975Ke11) 
$|G{-|g}=1.8 eV {I7} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
$E{-p}=1225.7 {I6} 
$|w|g=1.5 eV {I5} (1972Hu10) 
$|w|g=1.1 eV (1973Fa07) 
$|w|g=1.5 eV {I5} (1976Me12) 
$|w|g=0.7 eV {I2} (2001Vo24) 
$A{-2}=2 (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E{-p}=1266.5 {I8} 
J$3/2 from 1977Ko34 
$|w|g=3.4 eV, |G{-|g}|?0.57 eV (1971Wi13) 
$|w|g=3.2 eV {I10} (1972Hu10) 
$|w|g=2.9 eV (1973Fa07) 
$|w|g=2.8 eV {I9} (1976Me12) 


level_energy_unit: KEV
level_comment:
$E{-p}=1323.9 {I8} 
$|w|g=0.5 eV {I3} (1972Hu10) 
$|w|g=0.5 eV (1973Fa07) 
$|w|g=0.8 eV {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2)
level_comment:
$E{-p}=1339.7 {I8} 
$|w|g=1.5 eV {I5} (1972Hu10) 
$|w|g=1.4 eV (1973Fa07) 
$|w|g=1.3 eV {I4} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-p}=1353.7 {I6} 
$|w|g=2.5 eV {I8} (1972Hu10) 
$|w|g=2.4 eV (1973Fa07) 
$|w|g=2.8 eV {I9} (1976Me12) 
$|G{-p}=445 eV {I11} (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=1375.2 {I8} 
$|w|g=3.7 eV {I11} (1972Hu10) 
$|w|g=3.1 eV (1973Fa07) 
$|w|g=4.4 eV {I13} (1976Me12) 
$|G{-p}=4 eV {I1} (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$E{-p}=1414.8 {I9} 
$|w|g=1.3 eV {I4} (1972Hu10) 
$|w|g=1.2 eV (1973Fa07) 
$|w|g=1.7 eV {I5} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=1448.0 {I9} 
$|w|g=1.5 eV {I5} (1972Hu10) 
$|w|g(1.4) eV (1973Fa07) 
$|w|g=1.5 eV {I5} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$E{-p}=1452.7 {I12} 
$|w|g=0.8 eV {I4} (1972Hu10) 
$|w|g(0.9) eV (1973Fa07) 
$|w|g=0.9 eV {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E{-p}=1468.6 {I9} 
J$from 1988Va06, 3/2 from 1976Me12 
$|w|g=1.5 eV {I5} (1972Hu10) 
$|w|g=1.6 eV (1973Fa07) 
$|w|g=1.4 eV {I4} (1976Me12) 
$The J|p=1/2- invalidates the two large mixing ratios for the transitions of 7.80 to 0 and 7.80 to 1.22 in 1976Me12 (1988Va06) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E{-p}=1510 {I1} 
T$from 1971Wi13 
$|w|g=3.4 eV {I6} (1967Wa22) 
$|w|g |? 7.5 eV, |G{-|g}=1.9 eV (1971Wi13) 
$|w|g=11 eV (1972Hu10) 
$|w|g=1.3 eV (1973Fa07) 
$|w|g=(4.8) eV (1976Me12) 
$|w|g=2.2 eV {I3} (2001Vo24) 
$|G{-|g}=0.55 eV {I6} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
$E{-p}=1542.3 {I10} 
$|w|g=0.5 eV {I3} (1972Hu10) 
$|w|g=(0.5) eV (1973Fa07) 
$|w|g=1.0 eV {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
$E{-p}=1554.8 {I9} 
$|w|g=1.6 eV {I5} (1972Hu10) 
$|w|g=1.3 eV (1973Fa07) 
$|w|g=2.2 eV {I7} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
$E{-p}=1573.7 {I7} 
$|w|g=1.4 eV {I4} (1972Hu10) 
$|w|g=1.0 eV (1973Fa07) 
$|w|g=2.2 eV {I7} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
$E{-p}=1598.6 {I9} 
$|w|g=0.8 eV {I4} (1972Hu10) 
$|w|g=(0.7) eV (1973Fa07) 
$|w|g=1.0 eV {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
$E{-p}=1646.9 {I10} 
$|w|g=1.2 eV {I4} (1972Hu10) 
$|w|g=(1.0) eV (1973Fa07) 
$|w|g=1.9 eV {I6} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=1665 {I1} 
$|w|g=1.5 eV {I5} (1972Hu10) 
$|w|g=(1.3) eV (1973Fa07) 
$|w|g=1.2 eV {I4} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$E{-p}=1673 {I1} 
$|w|g=2.7 eV {I8} (1972Hu10) 
$|w|g=(2.3) eV (1973Fa07) 
$|w|g=2.1 eV {I6} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=1682.1 {I2} 
J$from 1981Bi05 
$|w|g=4.1 eV {I12} (1972Hu10) 
$|w|g=(3.4) eV (1973Fa07) 
$|w|g=4.8 eV {I15} (1976Me12) 
$|w|g=4.5 eV {I14} (1972Hu10) 
$|G{-p}=21 eV {I3} (1981Bi05) 


level_energy_unit: KEV
level_comment:
$E{-p}=1714.1 {I10} 
$|w|g=0.9 eV {I5} (1972Hu10) 
$|w|g(0.9) eV (1973Fa07) 
$|w|g=0.8 eV {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=1717.2 {I11} 
$|w|g=3.5 eV {I11} (1972Hu10) 
$|w|g=3.0 eV (1973Fa07) 
$|w|g=2.9 eV {I9} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2-)
level_comment:
$E{-p}=1755.7 {I11} 
$|w|g=1.6 eV {I5} (1972Hu10) 
$|w|g(1.3) eV (1973Fa07) 
$|w|g=1.6 eV {I5} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2+)
level_comment:
$E{-p}=1776.9 {I11} 
$|w|g=2.5 eV {I8} (1972Hu10) 
$|w|g=2.5 eV (1973Fa07) 
$|w|g=2.4 eV {I7} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=1787.1 {I11} 
$|w|g=4.2 eV {I13} (1972Hu10) 
$|w|g=3.6 eV (1973Fa07) 
$|w|g=3.7 eV {I11} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
$E{-p}=1794.2 {I11} 
$|w|g=1.2 eV {I4} (1972Hu10) 
$|w|g(1.1) eV (1973Fa07) 
$|w|g=1.6 eV {I5} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-p}=1829.1 {I11} 
$|w|g=2.4 eV {I7} (1972Hu10) 
$|w|g=1.5 eV (1973Fa07) 
$|w|g=1.7 eV {I5} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2-)
level_comment:
$E{-p}=1839.0 {I11} 
$|w|g=2.1 eV {I6} (1972Hu10) 
$|w|g=2.1 eV (1973Fa07) 
$|w|g=1.9 eV {I6} (1976Me12) 


level_energy_unit: KEV
level_comment:
$E{-p}=1862.3 {I12} 
$|w|g=0.8 eV {I4} (1972Hu10) 
$|w|g(0.7) eV (1973Fa07) 
$|w|g=0.9 eV {I3} (1976Me12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=1891.7 {I10} 
E$weighted average from 1976Me12 and 2001Vo24 
J$from 1981Bi05, 1996Ka21 and 2001Vo24 
$|w|g=8.0 eV {I24} (1972Hu10) 
$|w|g=6.0 eV (1973Fa07) 
$|w|g=9.0 eV {I27} (1976Me12) 
$|w|g=4.1 eV {I5}, |G{-p}=39 eV {I5} (1981Bi05) 
$|w|g=2.6 eV {I7} (1996Ka21) 
$|w|g=4.2 eV {I8} (2001Vo24), sum of |w|g for the resonances at E{-p}=1891 and 1893, |G{-|g}=0.70 eV {I14} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=1900.3 {I10} 
$|w|g=4.7 eV (1973Fa07) 
$|w|g=6.2 eV {I19} (1972Hu10) 
$|w|g=7.1 eV {I21} (1976Me12) 
$|w|g=1.7 eV {I5} (1996Ka21) 
$|w|g=3.3 eV {I5} (2001Vo24) 
$|G{-|g}=0.55 eV {I8} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$E{-p}=1926.8 {I10} 
$|w|g=1.9 eV {I6} (1972Hu10) 
$|w|g=1.9 eV (1973Fa07) 
$|w|g=2.2 eV {I7} (1976Me12) 
$|w|g=1.0 eV {I3} (2001Vo24) 
$|G{-|g}=0.25 eV {I8} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$E{-p}=1954.5 {I5} 
$|w|g=1.8 eV {I5} (1972Hu10) 
$|w|g=(1.9) eV (1973Fa07) 
$|w|g=2.0 eV {I6} (1976Me12) 
$|w|g=0.6 eV {I3} (1976Sp08) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=1963.0 {I5} 
$|w|g=1.6 eV {I5} (1972Hu10) 
$|w|g=(1.7) eV (1973Fa07) 
$|w|g=1.5 eV {I5} (1976Me12) 
$|w|g=0.7 eV {I4} (1976Sp08) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$E{-p}=1973.5 {I3} 
J$from 1981Bi05, 3/2 from 1976Me12 
$|w|g=2.9 eV {I9} (1972Hu10) 
$|w|g=1.6 eV {I5} (1976Me12) 
$|w|g=0.9 eV {I5} (1976Sp08) 
$|G{-p}=48 eV {I6} (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E{-p}=1984.7 {I5} 
$|w|g=4.0 eV {I12} (1972Hu10) 
$|w|g=3.5 eV {I11} (1976Me12) 
$|w|g=0.9 eV {I5} (1976Sp08) 


level_energy_unit: KEV
level_comment:
$E{-p}=2005.1 {I3} 
$|w|g=4.2 eV {I13} (1972Hu10) 
$|w|g=4.6 eV (1973Fa07) 
$|w|g=4.2 eV {I13} (1976Me12) 
$|w|g=2.7 eV {I5} (1976Sp08) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=2070.7 {I6} 
J$from 2001Vo24 
$|w|g=6.1 eV {I12} (1976Sp08) 
$|w|g=6.1 eV {I6} (2001Vo24) 
$|G{-|g}=1.02eV {I10} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$E{-p}=2176.3 {I5} 
J$from 2001Vo24 
$|w|g=2.1 eV {I4} (1976Sp08) 
$|w|g=2.1 eV {I4} (2001Vo24) 
$|G{-|g}=0.36 eV {I6} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)+
level_comment:
$E{-p}=2597.3 {I5} 
J$from 2001Vo24 
$|w|g=1.2 eV {I2} (1976Sp08) 
$|w|g=1.2 eV {I4} (2001Vo24) 
$|G{-|g}=0.20 eV {I6} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=2611.3 {I5} 
J$from 2001Vo24 
$|w|g=1.5 eV {I3} (1976Sp08) 
$|w|g=1.5 eV {I3} (2001Vo24) 
$|G{-|g}=0.25 eV {I5} (2001Vo24) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}=2791.0 {I4} 
$|w|g=16.0 eV {I32} (1976Sp08) 
$|w|g=16.3 eV {I4} (1996Ka21) 
$|w|g=16.0 eV {I3} (2001Vo24) 
$|G=65 eV {I20}, |G{-p}=62 eV {I20}, |G{-|g}=2.3 eV {I4}, |w|g=13.4 eV {I22} (1976Sp09) 
$|G{-p}=59 eV {I7} (1981Bi05) 
$|G{-|g}=2.7 eV {I5} (2001Vo24) 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 3.2 (1969Gr23), 5.2 (1970Mo01) 
S$0.72 in 1969Gr23, 1.3 in 1970Mo01 and 1.07 in 1994Ve04; for J|p=3/2+ 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 12.0 (1969Gr23), 2.5 (1970Mo01) 
S$0.26 in 1969Gr23, 0.28 in 1970Mo01; for J|p=1/2+ 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 0.32 (1969Gr23), 0.7 (1970Mo01) 
S$0.023 in 1969Gr23, 0.04 in 1970Mo01; for J|p=5/2+ 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 3.3 (1969Gr23), 5.5 (1970Mo01) 
S$0.36 in 1969Gr23, 0.66 in 1970Mo01; for J|p=7/2- 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 1.3 (1969Gr23), 0.6 (1970Mo01) 
S$0.03 in 1969Gr23, 0.06 in 1970Mo01; for J|p=1/2+ 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 6.1 (1969Gr23), 8.0 (1970Mo01) 
S$0.095 in 1969Gr23, 0.15 in 1970Mo01; for J|p=3/2- 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 14.0 (1969Gr23), 15 (1970Mo01) 
S$0.213 in 1969Gr23, (0.28,0.62) in 1970Mo01; for J|p=3/2- 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 0.84 (1969Gr23), 4 (1970Mo01) 
E$Multiplet in 1970Mo01 
L$from 1969Gr23; (2) in 1970Mo01 
S$0.028 in 1969Gr23; for J|p=3/2- 


level_energy_unit: KEV
level_comment:
$(d|s/d|w){-max}(mb/sr): 0.92 (1969Gr23), 1.2 (1970Mo01) 
L$ 1 in 1969Gr23, 0 in 1970Mo01 
S$0.03 in 1969Gr23 for J|p=3/2-, 0.21 in 1970Mo01 for J|p=1/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-|a}=3750 {I5} 
J$5/2 from 1971Mc23 and (5/2+,7/2-) from 1975Sc40 
$(2J+1)|G{-|a}|G{-p}/|G=63 ev 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$E{-|a}=3840 {I5} 
J$(1/2, 3/2) from 1971Mc23 and (3/2+,7/2+) from 1975Sc40 
$(2J+1)|G{-|a}|G{-p}/|G=61 ev 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E{-|a}=3995 {I5} 
J$1/2 from 1971Mc23 and (1/2+,5/2+) from 1975Sc40 
$(2J+1)|G{-|a}|G{-p}/|G=182 ev 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
$E{-|a}=4155 {I5} 
J$3/2 from 1971Mc23 and (3/2+,5/2+) from 1975Sc40 
$(2J+1)|G{-|a}|G{-p}/|G=132 ev 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$E{-|a}=4220 {I5} 
J$3/2 from 1971Mc23 and (3/2+,9/2+) from 1975Sc40 
$(2J+1)|G{-|a}|G{-p}/|G=269 ev 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
$|G{-p}=0.0072 keV {I15} 
$E{-p}(lab)(keV)=1214 
$|G=11.0 eV {I15}, |G{-|g}=3.8 eV {I15} (1974Bi16) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|G{-p}=3.73 keV {I38} 
$E{-p}(lab)(keV)=1510.0 {I5} 
$|G=3.8 keV {I2}, |G{-p}=3.8 keV {I2} (1974Bi16) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|G{-p}=0.011 keV {I5} 
$E{-p}(lab)(keV)=1682.1 {I5} 
$|G{-p}=21 keV{I3} for J|p=5/2+, 24 eV {I3} for J|p=3/2+ (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
$|G{-p}=0.033 keV {I10} 
$E{-p}(lab)(keV)=1893.2 {I5} 
$|G=100 eV {I20}, |G{-p}=120 eV {I20} (1974Bi16) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|G{-p}=0.094 keV {I15} 
$E{-p}(lab)(keV)=1894.4 {I5} 
$|G{-p}=39 eV {I5} for J|p=5/2+, 44 eV {I6} for J|p=3/2+, 120 eV {I11} for J|p=1/2+ (1981Bi05) 
$|G=270 eV {I50}, |G{-p}=270 eV {I50} (1974Bi16) 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_comment:
$|G{-p}=0.04 keV {I1} 
$E{-p}(lab)(keV)=1975.7 {I5} 
$|G{-p}=49 eV {I11} for J|p=3/2-, 48 eV {I6} for J|p=1/2- (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$|G{-p}=0.023 keV {I7} 
$E{-p}(lab)(keV)=2072.2 {I5} 
$|G=30 eV {I7}, |G{-p}=28 eV {I6}, |G{-|g}=2.4 eV (1974Bi16) 
J$5/2+ in 1974Bi16 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
$|G{-p}=0.001 keV {I1} 
$E{-p}(lab)(keV)=2541.7 {I5} 
$|G{-p}=4 eV {I1} for J|p=7/2-, 2 eV {I1} for J|p=5/2- (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
$|G{-p}=0.057 keV {I10} 
$E{-p}(lab)(keV)=2793.2 {I5} 
$|G{-p}=59 eV {I7} for J|p=5/2+, 67 eV {I8} for J|p=3/2+ (1981Bi05) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.19 ps {I10} (1969Du08), 0.146 ps {I35} (1972Br45) and 0.149 ps {I52} (1972Va06) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$unweighted average of 0.80 ps {I38} (1969Du08), 0.34 ps {I6} (1972Br45) and 0.142 ps {I52} (1972Va06) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
T$unweighted average of 240 fs {I60} (1969Du08), 180 fs {I40} (1972Br45) and 128 ps {I35} (1972Va06). 1971Ca40 gives 58 fs {I15}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T$from Adopted Levels of {+35}Cl in ENSDF database 
$Q(transition)=0.31 {I4}, |b{-2}=0.15 (2013Bi10) 


level_energy_unit: KEV
level_spin_parity: (1/2+:7/2+)
level_comment:
E$from 2017Ch22, likely associated with the doublet of 6656+6681 observed via {+32}S(|a,p) by 1973Go16. 
J,L$spin-parity is from L=2 adopted by 2017Ch22 based on the best DWBA fit to measured differential cross section; L=0+2 or L=1+3 are possible but would not alter the conclusion regarding possible spin and parity assignment (2017Ch22). 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
$(2J+1)C{+2}S=0.049 {I2} 
$E(p)(resonance)=56 keV {I2} 
$|w|g(min)=6.5|*10{+-24} eV {I2}, |w|g(max)=2.2|*10{+-22} eV {I1} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
$(2J+1)C{+2}S=0.034 {I1} 
$E(p)(resonance)=97 keV {I2} 
$|w|g(min)=4.2|*10{+-14} eV {I5}, |w|g(max)=4.7|*10{+-14} eV {I5} 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
$(2J+1)C{+2}S=0.072 {I2} 
$Adopted E(level)=6491.5 {I8}, E(p)(resonance)=120.6 keV {I5} 
$|w|g(min)=3.7|*10{+-13} eV {I1}, |w|g(max)=4.1|*10{+-13} eV {I1} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
$(2J+1)C{+2}S=0.004 {I1} for L=0, 0.0028 {I4} for L=1 
$E(p)(resonance)=174 keV {I2} 
$|w|g(min)=7.4|*10{+-10} eV {I13}, |w|g(max)=4.1|*10{+-9} eV {I1} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
$(2J+1)C{+2}S=0.0144 {I8} 
$E(p)(resonance)=272 keV {I2} 
$|w|g(min)=8.5|*10{+-6} eV {I10}, |w|g(max)=8.9|*10{+-6} eV {I10} 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2)
level_comment:
$(2J+1)C{+2}S=0.0020 {I4} for L=1, 0.0048 {I6} for L=2, 0.008 {I1} for L=3. 
$E(p)(resonance)=303 keV {I2} 
$|w|g(min)=2.4|*10{+-8} eV {I2}, |w|g(max)=4.1|*10{+-6} eV {I8} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_comment:
$(2J+1)C{+2}S=0.0056 {I12} for L=0, 0.0032 {I4} for L=1 
$E(p)(resonance)=390 keV {I2} 
$|w|g(min)=2.4|*10{+-4} eV {I3}, |w|g(max)=1.5|*10{+-3} eV {I1} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
$(2J+1)C{+2}S=0.0084 {I8} 
$E(p)(resonance)=407 keV {I2} 
$|w|g(min)=9.4|*10{+-4} eV {I12}, |w|g(max)=1.0|*10{+-3} eV {I1} 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
$(2J+1)C{+2}S=0.006 {I4} 
$E(p)(resonance)=452 keV {I2} 
$|w|g(min)=2.7|*10{+-3} eV {I3}, |w|g(max)=2.7|*10{+-3} eV {I3} 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)
level_comment:
$(2J+1)C{+2}S=0.0216 {I6} for L=2, 0.035 {I2} for L=3 
$E(p)(resonance)=471 keV {I2} 
$|w|g(min)=3.3|*10{+-5} eV {I1}, |w|g(max)=7.0|*10{+-4} eV {I3} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$(2J+1)C{+2}S=0.0160 {I2}(L=0)+0.0660 {I6} (L=2) 
$Adopted E(level)=6866.4 {I6}, E(p)(resonance)=495.5 keV {I6} 
E$6866.7 {I6} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 
$|w|g(min)=3.0|*10{+-2} eV {I3}, |w|g(max)=4.7|*10{+-2} eV {I5} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$(2J+1)C{+2}S=0.0088 {I8} for L=1, 0.012 {I1} for L=2 
$Adopted E(level)=7065.9 {I10}, E(p)(resonance)=695.1 keV {I10} 
E$7066.2 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 
$|w|g(min)=2.2|*10{+-2} eV {I1}, |w|g(max)=2.2|*10{+-2} eV {I1} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$(2J+1)C{+2}S=0.0184 {I12} for L=1, 0.025 {I2} for L=3 
$Adopted E(level)=7103.3 {I10}, E(p)(resonance)=732.5 keV {I10} 
E$7103.3 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 
$|w|g(min)=6.0|*10{+-2} eV {I3}, |w|g(max)=1.30 eV {I7} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$(2J+1)C{+2}S=0.032 {I3} 
$Adopted E(level)=7178.6 {I10}, E(p)(resonance)=807.8 keV {I10} 
E$7178.6 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E(p)(resonance)=814 keV {I1} 
E$likely that the 7185-keV level was not resolved from the observed 7178 and 7194-keV levels. 
E$7185.0 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Adopted E(level)=7194.1 {I10}, E(p)(resonance)=823.3 keV {I10} 
E$7194.5 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$E(p)(resonance)=853.7 keV {I10} 
E$the 7225 keV and 7234 keV levels appear as a single peak in 2017Gi09 at 7227 {I2} with (2J+1)C{+2}S=0.065 {I15} for L=0, 0.044 {I2} for L=1 
E$7225.5 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
$E(p)(resonance)=862.7 keV {I10} 
E$the 7225 keV and 7234 keV levels appear as a single peak in 2017Gi09 at 7227 {I2} with (2J+1)C{+2}S=0.065 {I15} for L=0, 0.044 {I2} for L=1 
E,J$7234.0 {I3}, 5/2+ in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$(2J+1)C{+2}S=0.050 {I12} for L=0, 0.030 {I1} for L=1 
$Adopted E(level)=7272.8 {I10}, E(p)(resonance)=902.0 keV {I10} 
E$7272.6 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 
$|w|g(min)=11 eV {I2}, |w|g(max)=34 eV {I3} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$(2J+1)C{+2}S=0.0040 {I8} 
$Adopted E(level)=7361.9 {I10}, E(p)(resonance)=991.1 keV {I10} 
E$7362.0 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 
$|w|g(min)=0.30 eV {I4}, |w|g(max)=3.0 eV {I6} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$(2J+1)C{+2}S=0.042 {I2} for L=2, 0.0656 {I24} for L=3 
$Adopted E(level)=7397.4 {I16}, E(p)(resonance)=1026.6 keV {I16} 
E$7396.0 {I3} in {+35}Cl Adopted Levels in the ENSDF database (Oct 2011 update) 
$|w|g(min)=0.18 eV {I1}, |w|g(max)=0.19 eV {I1} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: Y
level_comment:
J$ spin from microwave spectroscopy (1949To10,1951Jo21,1952Gi04, 1955Aa23); parity from |s(|q) and vector analyzing power in (pol d,|a) 
MOMM1$measured by magnetic nuclear resonance (1955So10) 
MOME2$measured by microwave absorption in gases (1972St38) 
T$3.071|*10{+5} {I15} y weighted average of partial T{-1/2}'s of |b{+-} decay: 3.08|*10{+5} {I3} y (1955Ba93), 3.10|*10{+5} {I4} y (1966Go07), 3.06E5 2 y (1966Go07), the first two by 4|p|b proportional gas counting method, the third by liquid scintillator method. 
T$ 2010Ja03, 2010St07: analysis of {+32}Si/{+36}Cl half-life ratio data of 1986Al10 for periodic annual variation of half-life or for solar influence on half-life.  


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J$also: 2,3 from 7790|g-778|g angular correlation (1966Va05); 3+ from 778|g linear polarization (1971Ho30) in {+35}Cl(n,|g) 
T$adopted mean lifetime |t in ps: 21.2 {I15}, weighted average of 19.9 {I17} (1977He12), 23 {I2} (1976Co02) in {+2}H({+35}Cl,p|g); others: 32.3 {I25} (1976Me03) in {+27}Al({+14}N,p|a|g), 30 {I2} (1973No03) in {+33}S(|a,p|g), 3.0 {I12} (1973Yo01) in {+35}Cl(d,p|g), >5 (1973Wa10) in {+2}H({+35}Cl,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$also: 1,2 from 7414|g-1165|g angular correlation (1966Va05); 1+ from 778|g linear polarization (1971Ho30) in {+35}Cl(n,|g) 
T$adopted mean lifetime |t in ps: 9.9 {I6}, weighted average of 9.2 {I6} (1977He12), 10.4 {I5} (1976Co02) in {+2}H({+35}Cl,p|g); others: 7.1 {I5} (1973No03) in {+33}S(|a,p|g), 9.2 {I6} (1977He12), 10.4 {I5} (1976Co02) in {+2}H({+35}Cl,p|g), 3.0 {I12} (1973Yo01) in {+35}Cl(d,p|g), 13 {I4} (1976Co11) in {+3}H({+35}Cl,d|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$also: 1,2 from 6978|g-1601|g angular correlation (1966Va05) in {+35}Cl(n,|g); |p=+ from L=0 in {+35}Cl(d,p) 
T$from DSAM. Mean lifetime |t=927 fs {i60} from weighted average of |t=940 fs {i60} (1977He12) in {+2}H({+35}Cl,p|g); 1100 fs {i300} (1991Ul02) in {+35}Cl(n,|g); 800 fs {i150} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$from 6111|g-517|g angular correlation (1966Va05) in {+35}Cl(n,|g); |p=- from L=1+3 in {+35}Cl(d,p) 
T$adopted mean lifetime |t in ps: 2.7 {I3}, weighted average of 2.3 {I2} (1976No03) in {+33}S(|a,p|g) and 2.95 {I14} (1976Co02) in {+2}H({+35}Cl,p|g); others: 1800 {I500} (1991Ul02) in {+35}Cl(n,|g), 1800 {I+1000-500} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$from 6620|g-1959|g angular correlation (1966Va05) in {+35}Cl(n,|g); |p=+ from L=0 in {+35}Cl(d,p) 
T$adopted mean lifetime |t in ps: 62.9 {I20}, weighted average of 63 {I2} (1992Ku17, 1991Ul02) in {+35}Cl(n,|g) and 60 {I15} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$3 from 6111|g-517|g angular correlation (1966Va05); |p=- from 6111|g circular polarization (1969Ko05) in {+35}Cl(n,|g), or L=1 in {+37}Cl(p,d) 
T$adopted mean lifetime |t in ps: 1.40 {I15}, weighted average of 1.20 {I25} (1991Ul02) in {+35}Cl(n,|g) and 1.50 {I18} (1973Wa10) in {+2}H({+35}Cl,p|g); others: 0.470 {I50} (1973Yo01) in {+35}Cl(d,p|g); <1 (1976No03) in {+33}S(|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$|DJ=0 M1+E2 |g from 2+, 8580 (1976Sp06) in {+35}Cl(n,|g) 
T$adopted mean lifetime |t in fs: 57 {I13} weighted average of 48 {I26} (1992Ku17, 1991Ul02) in {+35}Cl(n,|g) and 60 {I15} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J$E3 |g to 2+, g.s. and M2+E3 |g to 3+, 788 
T$adopted mean lifetime |t in ns: 2.33 {I11}, weighted average of 2.30 {I16} (1976Ke02) in {+27}Al({+14}N,p|a|g) and 2.36 {I16} (1973No03) in {+33}S(|a,p|g); others: |?2.4 (1976Co02) in {+2}H({+35}Cl,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+,(2+)
level_lifetime_unit: FS
level_comment:
J$M1+E2 |g to 2+, g.s., as given in {+33}S(|a,p|g) T{-1/2}; mean lifetime |t in fs: 31 {I5} (1992Ku17, 1991Ul02); other <10 (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$E2 |g to 2-, 1951 and M1(+E2) |g to 5-, 2518 
T$adopted mean lifetime |t in ps: 3.4 {I3}, weighted average of 3.3 {I3} (1976No03) in {+33}S(|a,p|g), 4.9 {I10} (1976Co02) in {+2}H({+35}Cl,p|g), 2.7 {I10} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: FS
level_comment:
J$(1,2,3)+ from |DJ=(0,1), M1+E2 |g from 2+, 8580 (1976Sp06); (3)+ |g from (4)-, 3101 
T$mean lifetime |t in fs: 21 {I1} (1992Ku17, 1991Ul02) in {+35}Cl(n,|g); other: <15 (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_lifetime_unit: FS
level_comment:
J$(2-,3) from |g's to 4-, 2811; 2+, 1959; and 2-, 1951, respectively; |p=- from L=1+3 in {+35}Cl(d,p); 
T$mean lifetime |t in fs: 860 {I80} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (1,2,3)-
level_lifetime_unit: FS
level_comment:
J$(1,2,3) from |g's to 2+, g.s., and 2-, 2995; |p=- from L=1 in {+35}Cl(d,p) 
T$mean lifetime |t in fs: 90 {I12} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: FS
level_comment:
J$2-,3-,4- from M1+E2 |g to 3-, 2468; (4)- from no |g to 2+, g.s. 
T$mean lifetime |t in fs: 215 {I+70-40} (1973Yo01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_uncertain: ?
level_comment:
E$estimated in {+38}Ar(p,{+3}He) based on analogy with {+36}Ar 
J$0+, based on L=0 and T=1 analog state ({+38}Ar(p,{+3}He)) 


level_energy_unit: KEV
level_spin_parity: (0:3)-
level_lifetime_unit: FS
level_comment:
J$L=1 in {+35}Cl(d,p) and |g's to 1+, 1165 and 2-, 1951 
T$mean lifetime |t in fs: 140 {I20} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: FS
level_comment:
J$(1,2,3)- from |DJ=(0,1), E1 |g from 2+, 8580 (1976Sp06); (2,3+) from |g's to 3+, 788; 3-, 1959; and 1+, 1601, respectively 
T$mean lifetime |t in fs: 105 {I10} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+,(2)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=0+2 in {+37}Cl(p,d) from 3/2+ target. 369|g to (4)-, 1601 level is presumed to be erroneous placement in (n,|g) (1990En08) 
T$mean lifetime |t in fs: <35 (1973Yo01) 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: FS
level_comment:
J$1-,3- from |DJ=1, E1 |g from 2+, 8580; (3)- |g to 3-, 2468 
T$mean lifetime |t in fs: 59 {I3} (1992Ku17, 1991Ul02) in {+35}Cl(n,|g); other: 60 {I20} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: FS
level_comment:
J$1-,3- from |DJ=1, E1 |g from 2+, 8580; (1)- from |g to 1+, 1165 
T$mean lifetime |t in fs: 30 {I15} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (1-,2)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g's to 2+, g.s.; 2-, 1951; 1+, 1165; (1,2,3)-, 2997 
T$mean lifetime |t in fs: <80 (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$(1,2,)- from |DJ=(0,1), E1 |g from 2+, 8580 (1976Sp06); (1)- less likely from |g from (3)+, 4997.2 
T$mean lifetime |t in fs: <30 (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (1,2,3)-
level_lifetime_unit: FS
level_comment:
J$(0+,1,2,3,4+) from |g to 2+, 1959; |p=- from L=1 in {+35}Cl(d,p) 
T$mean lifetime |t in fs: 30 {I10} (1973Yo01) in {+35}Cl(d,p|g) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
J$(0,1,2) from |g's to 1+, 1601 and (1)-, 3635; (2,3,4) from |g's to 3+, 788 and (3)-, 3599; |p=- from L=1 in {+35}Cl(d,p) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: PS
level_comment:
J$M1+E2 |g to 5-, 2518; E2 |g to 4-, 2810 
T$adopted mean lifetime |t in ps: 5.2 {I48}, from >0.4 (1977No09) in {+33}S(|a,p|g) and <10 (1976Wa11) in {+27}Al({+14}N,p|a|g); other: <20 (1976Ke02) in {+27}Al({+14}N,p|a|g) 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: PS
level_comment:
J$E1+M2 |g to 6-, 4295; M2(+E3) |g to 5-, 2518 
T$mean lifetime |t in ps: 32 {I3} (1976Wa11), 27.2 {I17} (1976Ke02) in {+27}Al({+14}N,p|a|g); weighted average: 28.4 {I21} 


level_energy_unit: KEV
level_spin_parity: (8)
level_uncertain: ?
level_comment:
J$6,8 from D |g 7+, 5314; (8) since spin usually increase with increasing E(level) for this type of reactions 
T$mean lifetime |t in ps: 0.5 to 1000 (1976Wa11) in {+27}Al({+14}N,p|a|g) 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
E$weighted average of 6150 {I8} ({+35}Cl(d,p)) and 6166 {I13} ({+37}Cl({+3}He,|a)) 
J$|p=- from L=1 in {+35}Cl(d,p) 


level_energy_unit: KEV
level_spin_parity: -
level_comment:
E$weighted average of 6440 {I8} ({+35}Cl(d,p)) and 6444 {I20} ({+37}Cl({+3}He,|a)) 
J$|p=- from L=1 in {+35}Cl(d,p) 


level_energy_unit: KEV
level_spin_parity: (2)
level_comment:
J$(1,2,3) from |g's to 2+, 2492 and (2)-, 3332; (2) with extra |g's to (1+,2+,3+), 3941 and (1,2,3)-, 5079 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E$weighted average of 6618 {I5} ({+37}Cl(p,d)) and 6621 {I15} ({+37}Cl({+3}He,|a)) 
J$|p=+ from L=2 in {+37}Cl(p,d) 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E$weighted average of 6893 {I7} ({+37}Cl(p,d)) and 6897 {I13} ({+37}Cl({+3}He,|a)) 
J$|p=+ from L=0+2 in {+37}Cl(p,d) 


level_energy_unit: KEV
level_spin_parity: +
level_comment:
E$weighted average of 7652 {I16} ({+37}Cl({+3}He,|a)) and 7665 {I6} ({+37}Cl(p,d)) 
J$|p=+ from L=0+2 in {+37}Cl(p,d) 


level_energy_unit: KEV
level_spin_parity: 2+
level_uncertain: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 2006De21. Other: 8579.79 {I1} (2011AuZZ) in {+35}Cl(n,|g) 
J$from {+35}Cl(n,|g): 1+,2+ based on selection rules; 1+ ruled out by positive A{-4} angular correlation coefficients for all possible M1+E2 mixings for primary-secondary |g cascades (see A{-4} values at 7790|g for 7790|g-778|g, and at 6111|g for 6111|g-517|g). 2+ also sustained by 1966Va05 and 1956Br99 who show that the capture state is dominated by a single negative-energy resonance close to the n-capture state, which thus has a definite spin. 1976Sp06 argue that a small 0.6% admixture of 1+ is possible 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$2,3 from 7790|g-778|g angular correlation (1966Va05); 3+ from 778|g linear polarization (1971Ho30) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$1,2 from 7414|g-1165|g angular correlation (1966Va05); 1+ from 778|g linear polarization (1971Ho30) 


level_energy_unit: KEV
level_spin_parity: 1,2
level_lifetime_unit: FS
level_comment:
J$1,2 from 6978|g-1601|g angular correlation (1966Va05) 
T$mean lifetime |t in fs: 1100 {I300} (1991Ul02) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_comment:
J$from 6111|g-517|g angular correlation (1966Va05) 
T$mean lifetime |t in fs: 1800 {I500} (1991Ul02) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_comment:
J$from 6620|g-1959|g angular correlation (1966Va05) 
T$mean lifetime |t in fs: 63 {I2} (1992Ku17, 1991Ul02) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$3 from 6111|g-517|g angular correlation (1966Va05); |p=- from 6111|g circular polarization (1969Ko05) 
T$mean lifetime |t in fs: 1200 {I250} (1991Ul02) 


level_energy_unit: KEV
level_spin_parity: (2,3)+
level_lifetime_unit: FS
level_comment:
J$|DJ=(0,1), M1+E2 |g from 2+, 8580 (1976Sp06) 
T$mean lifetime |t in fs: 21 {I1} (1992Ku17, 1991Ul02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_uncertain: S
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 2006De21. Observed deexcitation intensity is 95.6% of g.s. feeding 
J$1+,2+ based on selection rules; 1+ ruled out by positive A{-4} angular correlation coefficients for all possible M1+E2 mixings for primary-secondary |g cascades (see A{-4} values at 7790|g for 7790|g-778|g, and at 6111|g for 6111|g-517|g). 2+ also sustained by 1966Va05 and 1956Br99 who show that the capture state is dominated by a single negative-energy resonance close to the n-capture state, which thus has a definite spin. 1976Sp06 argue that a small 0.6% admixture of 1+ is possible 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t in ps: 19.9 {I17} (1977He12), 23 {I2} (1976Co02); weighted average: 21.2 {I15}. Other: >5 (1973Wa10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: PS
level_comment:
T$mean lifetime |t in ps: 9.2 {I6} (1977He12), 10.4 {I5} (1976Co02), weighted average: 9.9 {I6}. Other: >3 (1973Wa10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_comment:
$E(n)(lab)=1563.1, |G{-|g}=0.384 eV, |G{-n}=621.9 keV 
$ E(n)(lab)=7563.1 in table IV of 2006Sa17 seems a misprint 


level_energy_unit: KEV
level_comment:
E$1160 {I20} (1972Ro10), 1165 {I15} (1968Br10), 1165 {I15} (1976Ve01) 
S$first value is an upper limit 


level_energy_unit: KEV
level_comment:
E$1600 {I20} (1972Ro10), 1608 {I15} (1968Br10), 1600 {I15} (1976Ve01) 
S$uncertainty refers to the first value; second value is an upper limit 


level_energy_unit: KEV
level_comment:
E$1960 {I20} (1972Ro10), 1970 {I15} (1968Br10), 1960 {I15} (1976Ve01) 
S$with |DC{+2}S=0.09 for the first value, and |DC{+2}S=0.08 for the second value 


level_energy_unit: KEV
level_comment:
E$2500 {I20} (1972Ro10), 2497 {I15} (1968Br10), 2489 {I15} (1976Ve01) 
S$uncertainty refers to the first value 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$from 1969Ha19 (energy estimated in this range based on analogy with {+36}Ar) 
J$0+, T=1 analog state 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$RELATIVE=150 
E$from 1970Ha10 (table 2 "Summary of experimental results for high-T states") 
J$0+, T=2 analog state 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=64 fs {I+10-8} from ZBL model using 1131|g. Others: |t=59 fs {I+9-8} from KrC model using 1131|g; |t=68 fs {I+20-14} from ZBL model using 3599|g; |t=63 fs {I+19-13} from KrC model using 3599|g (2020Cr02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOMM1$using NMR method 
MOME2$using the method atomic beam magnetic resonance. Others: -0.068 {I10} (1986El09), -0.0644 {I7} (1993Su36); also from 2005St24. 
J$L(pol d,{+3}He)=2 and L-1/2 from analyzing power 
$ Nuclear rms charge radius=3.384 fm {I17} (2004An14 evaluation); same value in 2008 update of 2004An14 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J$L(pol d,{+3}He)=0 
T$weighted average of 0.13 ps {I4} from (|a,p|g), 0.143 ps {I14} from (n,n'|g), 0.13 ps {I3} from (p,p'|g) and 0.12 ps {I2} from coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in (|a,p|g) and (p,|g); negative parity is excluded by RUL in (|a,p|g) 
T$weighted average of 23 fs {I8} from (p,|g), 69 fs {I20} from (n,n'|g), 46 fs {I10} from (p,p'|g) 
$A3086.33 19 36 FS 8 
$G3086.7 105/2(+) 28 FS LT 
$H3086.12 7 5/2 23 FS 8 
$J3086 69 FS 20 
$K3086.1 4 46 FS 10 
$M3086 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$L(pol d,{+3}He)=3 and L+1/2 from analyzing power 
T$weighted average of 14 ps {I2} from {+3}He({+35}Cl,p|g), 15.2 ps {I28} from {+26}Mg({+14}N,2pn|g), 13.6 ps {I21} from {+27}Al({+12}C,2p|g), 11 ps {I6} from (p,p'|g), 19 ps {I3} from (|a,p|g). Others: 33 ps {I4} from (|a,p|g); 1.5 ps {I4} from (n,n'|g) 
$A3103.510 20 7/2- 
$B3105.2 97/2- 14 PS 2 
$C3103.54 20 7/2- 
$D3103.54 20 7/2- 15.2 PS 28 
$E3103 7/2- 13.6 PS 21 
$F3103.3 5 7/2- 
$G3104.6 67/2- 19 PS 3 
$G3104.6 67/2- 33 PS 4 
$H3103.59 8 7/2- 0.55 PS GT 
$J3103 7/2- 1.5 PS 4 
$K3103.2 2 11 PS 6 
$L3101 8 7/2- 3 0.19 
$M3103 7/2- 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,{+3}He)=2 and L-1/2 from analyzing power 
T$weighted average of 31 fs {I16} from (|a,p|g), 35 fs {I14} from (p,|g) and 28 fs {I14} from (p,p'|g) 
$L3603 40 3/2+ 2 0.03 
$A3627.2 10 
$G3626.3 83/2- 31 FS 16 
$H3626.82 6 3/2(+) 35 FS 14 
$K3626.7 3 3/2- 28 FS 14 
$M3627 3/2(+) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in (|a,p|g) and (p,|g); negative parity is excluded by RUL's in (p,|g) 
T$weighted average of 42 fs {I17} from (|a,p|g), 35 fs {I14} from (p,|g) and 66 fs {I21} from (p,p'|g) 
$A3708 4 
$G3708.1 8(3/2+,5/2-) 42 FS 17 
$H3707.79 9 3/2+ 35 FS 14 
$J3710 203/2+ 
$K3707.7 3 5/2 66 FS 21 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J$from |g(|q) and |g-polarization in (|a,p|g) and allowed |b{+-} decay 
T$weighted average of 22 fs {I17} from (|a,p|g) and 21 fs {I7} from (p,|g) 
$A3741.27 10 5/2- 
$G3740.9 75/2- 22 FS 17 E 
$H3741.05 15 5/2 21 FS 7 
$K3741.2 4 (3/2+,5/2,7/2+) 21 FS LT 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q) and |g-polarization in (|a,p|g); R(ADO) in {+24}Mg({+16}O,3p|g) 
T$weighted average of 24 ps {I3} from {+3}H({+35}Cl,p|g), 23.6 ps {I14} from {+26}Mg({+14}N,2pn|g), 22.7 ps {I14} from {+27}Al({+12}C,2p|g), 21 ps {I2} from (|a,p|g) 
$A4009.84 7 9/2- 
$B4012.2 99/2- 24 PS 3 
$C4009.8 4 9/2- 
$C4009.88 22 9/2- 23.6 PS 14 
$E4011 9/2- 22.7 PS 14 
$F4010.1 5 9/2- 
$G4011.0 69/2- 21 PS 2 
$H4011.3 6 
$K4010.6 4 9/2 1.0 PS +7-4 
$O4009.98 8 9/2- 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$L(pol d,{+3}He)=2 and L-1/2 from analyzing power; |g(|q) in (p,|g) 
T$weighted average of 0.10 ps {I4} from (p,|g) and 0.13 ps {I6} from (p,p'|g). 0.13 ps {I+18-8} from (|a,p|g) 
$A4016.3 8 
$G4016.7 141/2 0.13 PS +18-8 
$H4016.27 9 3/2 0.10 PS 4 
$K4015.9 4 (1/2,3/2-) 0.13 PS 6 
$L4013 14 2 0.13 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$from |q(|q) in (p,|g); positive parity is excluded by |g to 7/2- 
T$from (p,p'|g) 
$A4176.6 11 
$G4179.6 5 (3/2,5/2+) 0.4 PS GT 
$H4176.64 9 3/2(-) 0.21 PS GT 
$K4179.6 5 3/2- 0.8 PS +14-4 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in (p,|g) and (p,p'|g) 
$G4269.7 25(1/2,3/2) 32 FS LT 
$H4268.87 9 1/2 42 FS 14 
$K4270.2 6 1/2 42 FS LT 
$L4262 12 5/2+ 2 0.02 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in (p,|g), RUL's exclude the positive parity; R(ADO) in {+24}Mg({+16}O,3p|g) 
T$from (p,|g). 0.19 ps {I+21-7} from (p,p'|g) 
$A4272.59 10 7/2- 
$G4272.9 6 7/2- 
$H4272.52 17 7/2- 76 FS 28 
$K4272.9 6 7/2- 0.19 PS +21-7 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in (p,|g) 
T$from (p,|g). 0.19 ps {I+12-7} from (|a,p|g) 
$A4396.35 20 5/2 
$G4397.5 7 7/2+ 0.19 PS +12-7 
$H4396.3 7 5/2 13 FS 5 
$K4397.5 7 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$from |g(|q) and RUL's in (p,|g); R(ADO) in {+24}Mg({+16}O,3p|g) 
T$weighted average of 42 fs {I31} from (|a,p|g) and 60 fs {I20} from (p,|g) 
$A4460.4 11 
$G4461 3 7/2+,(9/2+) 42 FS 31 
$H4459.97 15 7/2- 0.06 PS 2 
$K4459.2 2 7/2 
$4460.32 21 7/2- 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q) and |g-polarization in (|a,p|g) 
T$weighted average of 3.3 ps {I8} from {+26}Mg({+14}N,2pn|g) and 1.7 ps {I4} from (|a,p|g) 
$C4545.7 4 11/2- 
$D4545.80 24 11/2- 3.3 PS 8 
$F4545.9 7 11/2- 
$G4546.5 611/2- 1.7 PS 4 
$H4546 
$K4560 20 
$O4545.85 9 11/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol d,{+3}He)=2 and L+1/2 from analyzing power 
$H4801.21 11 5/2+ 7 FS LT 
$L4813 7 5/2+ 2 1.26 


level_energy_unit: KEV
level_spin_parity: 7/2
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$from |g(|q) in (p,|g) and (|a,p|g) 
$G4812.3 9 (5/2-,7/2) 0.35 PS GT 
$H4810.9 3 7/2 40 FS 10 
$K4810 20 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g(|q) in (p,|g) 
T$from (p,|g). 87 fs {I35} from (|a,p|g) 
$G4855.3 10 (5/2-,7/2) 87 FS 35 
$H4853.96 13 3/2 3.5 FS LT 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q) and RUL's in (p,|g); R(ADO) in {+24}Mg({+16}O,3p|g) 
T$from (p,|g) 
$H4903.65 19 7/2+ 24 FS 10 
$O4903.7 23 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$from R(ADO) in {+24}Mg({+16}O,3p|g) and Hauser-Feshbach analysis in (|a,p|g) 
T$from (|a,p|g) 
$G4920.9 17 9/2 55 FS 31 
$K4920 20 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q) and |g-polarization in (|a,p|g) 
T$weighted average of 3 ps {I1} from {+26}Mg({+14}N,2pn|g), 1.9 ps {I3} from (|a,p|g) 
$C5270.1 4 13/2- 
$D5270.2 3 13/2- 3.0 PS 10 
$E5270 
$F5270.3 8 13/2- 
$G5270.8 613/2- 1.9 PS 3 
$K5270 20 
$O5270.73 9 13/2- 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g(|q), |g-decays and |g-feedings in (p,|g) and (|a,p|g) 
$G5706 3(7/2,9/2) 
$H5700.9 5 9/2- 0.2 PS LT 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J$from |g(|q) in {+27}Al({+19}F,2|ap|g) and (|a,p|g); R(ADO) in {+24}Mg({+16}O,3p|g) 
$E7020 2.1 PS 10 
$F7020.3 9 15/2 
$G7020 3 (9/2,11/2,15/2) 1.4 PS GT 
$O7020.29 11 15/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$ 3/2,5/2+ from |g(|q) and RUL's of |g-decays in (p,|g); L(d,p)=2 and L+1/2 from A{-y}(|q) from (pol d,p) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
E$ 9465 {I71} in (d,p) is arbitrarily associated with 9461.96 level. L(d,p)=2 and L+1/2 from analyzing powers gives 5/2+ for this level or any of the other levels in vicinity 


level_energy_unit: KEV
level_spin_parity: 1/2
level_comment:
$T{-1/2}=97 fs {I42} 
J$from |g(|q) in 1970Ha41 
T$from 1973Pi10. 118 fs {I+62-35} from DSAM in 1970Ha41. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$T{-1/2}=40 fs {I10} 
T$weighted average of 35 fs {I14} from 1984No06 and 42 fs {I10} from 1973Pi10 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$E{-p}=1886.9 {I3} 
$T{-1/2}=32 eV {I3} 
$|G=35 eV {I8}, |G{-p}=23 eV {I5}, |G{-|g}=12 eV {I5} (1975Ke01) 
$|G=12.1 eV {I25}, |G{-p}=7.9 eV {I15}, |G{-|g}=4.2 eV {I15} (1975Ke01) 
$|G{-p}=13.3 eV {I26}, |G{-|g}=6.25 {I13} (2002Vo17) 
$|w|g=130 eV {I20} from 1968Hy01, 59 eV {I9} from 1970Ha41, 22 eV {I3} from 1975Ke11, 31 eV {I3} from 2002Vo17 
$Decay corrected for contributions from E(p)=1885.6 


level_energy_unit: KEV
level_comment:
$E{-p}=2038 {I3} 
$T{-1/2}=9.3 eV {I9} 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10). 
$|w|g=40 eV {I2} from 1998Ka52 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
$E{-p}=2083 {I3} 
$T{-1/2}=23.2 eV {I9} 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=20 eV {I2} from 1998Ka52 


level_energy_unit: KEV
level_comment:
$E{-p}=2126 {I3} 
$T{-1/2}=21.7 eV {I9} 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=23 eV {I3} from 1998Ka52 


level_energy_unit: KEV
level_comment:
$E{-p}=2167 {I3} 
$T{-1/2}=14.5 eV {I6} 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=23 eV {I3} from 1998Ka52 


level_energy_unit: KEV
level_comment:
$E{-p}=2230 {I3} 
$T{-1/2}=11.8 eV {I13} 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=22 eV {I2} from 1998Ka52 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E{-p}=2392 
$T{-1/2}=13.6 eV {I8} 
E$from 1998Ka52 and 2008Ka10 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=27 eV {I3} from 1998Ka52 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E{-p}=2428 
$T{-1/2}=18.8 eV {I12} 
E$from 1998Ka52 and 2008Ka10 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=19 keV {I2} from 1998Ka52 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E{-p}=2459 
$T{-1/2}=25.7 eV {I48} 
E$from 1998Ka52 and 2008Ka10 
$|w|g normalized to 32 eV {I3} at E{-p}=1887 (2008Ka10) 
$|w|g=25 eV {I3} from 1998Ka52 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=1.3 {I1} 
$|G{-n}=0.7 eV, assuming |G{-|g}=1 eV 
$g|G{-n}|G{-p}/|G=0.07 eV {I1}, (2J+1)|G{-|g}|G{-p}/|G=1.01 eV {I19} 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=3.5 {I3} 
$|G{-n}=0.14 eV, assuming |G{-|g}=1 eV 
$g|G{-n}|G{-p}/|G=0.08 eV {I3}, (2J+1)|G{-|g}|G{-p}/|G=5.9 eV {I9} 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=8.2 {I9} 
$|G{-n}=4.6 eV, assuming |G{-|g}=1 eV 
$g|G{-n}|G{-p}/|G=1.7 eV {I3}, (2J+1)|G{-|g}|G{-p}/|G=3.7 eV {I6} 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
E$weighted average of 1726.3 {I2} (1986La10), 1726.4 {I3} (1969Du08), 1726.6 {I1} (1972Br45), and 1726.44 {I20} (1972Bo02) 
J$from p|g(|q) in 1969Du08 
T$0.16 ps {I5} from 1969Du08, 12 ps {I+4-2} from 1972Br45 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$weighted average of 3085.7 {I4} (1986La10), 3087.3 {I10} (1969Du08) and 3087 {I1} (1972Br45) 
T$from 1969Du08 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
E$weighted average of 3103.8 {I4} (1986La10), 3104.6 {I10} (1969Du08) and 3103.0 {I2} (1972Br45) 
T$from 1974Hu09 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
L$ 1d{-5/2} or 1f{-7/2} proton transfer in 1993Ma50 and L=3 in 1974Do12 
S$For L=3, 0.12 for L=2 (1993Ma50); 0.31 for L=3 in 1974Do12 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$ 2s{-1/2} or 1d{-5/2} proton transfer in 1993Ma50 and L=2 in 1974Do12 
S$For L=2, 0.07 for L=2 (1993Ma50); 0.17 in 1974Do12 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
L$ 1p{-1/2} or 1d{-5/2} proton transfer in 1993Ma50 and L=2 in 1974Do12 
S$for L=2, 0.17 for L=1 (1993Ma50); 0.19 in 1974Do12 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$weighted average of 7933 {I31} in 1993Ma50 and 7920 {I20} in 1974Do12 
L$ 1p{-1/2} proton transfer (1993Ma50) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
J$L(d,|a)=1 from 0+ and L(d,p)=1+3 from 3/2+; log| {Ift}=4.9 to 3- and 9.2 to 0+; shape of spectrum of |b transition to 0+ ({+38}Ar g.s.) is characteristic of first-forbidden unique |b transitions (1968Va06) 
T$Weighted average of 37.236 min {I9} (1988An03), 37.4 min {I2} (1972Em01), 37.18 min {I7} (1969St23), 37.140 min {I35} (1965KaZY), 37.0 min {I1} (1963Wi11), 37.12 min {I18} (1962Mo21), 37.29 min {I4} (1950Co69). Others: 1955Ma99, 1954Ma95, 38.5 min {I5} (1946Ho02), 1945Sl02, 1940Cu01, 1937Hu01, 37.0 min {I3} (1936Va01) 
MOMM1$polarized nuclei and |b detection of NMR (1972La22). Compilation: 2014StZZ 
$Adopted (1977En02) neutron stripping spectroscopic factor (S)=0.78 {I14} for L=3; 0.02 {I1} for L=1 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
J$L(d,p)=3 from 3/2+; 671.360|g M3 to 2- 
T$from 1972Br53 in {+38}Cl IT decay. 
$Adopted (1977En02) neutron stripping spectroscopic factor (S)=0.72 {I13} for L=3 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1+3 from 3/2+ and L(d,|a)=3 from 0+ give 2-,3-; J|p=2- would require an unreasonably large B(E2) for 553.605|g from 4- 
$Adopted (1977En02) neutron stripping spectroscopic factor (S)=0.56 {I10} for L=3; 0.08 {I2} for L=1 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=3 from 3/2+ and L(d,|a)=5 from 0+; 1308.8|g to 2- and 637.685|g to 5-; RUL 
$Adopted (1977En02) neutron stripping spectroscopic factor (S)=0.67 {I12} for L=3 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$945.89|g to 5-; RUL 
$Adopted (1977En02) neutron stripping spectroscopic factor (S)=0.34 {I6} for L=1 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
T$from 1972Br53. Others: 0.77 s {I5} (1974Gr48), 0.74 s {I3} (1962Ki09), 1.0 s {I2} (1954Sc37) 
T$1972Br53 quote a value of 735 ms {I10} by K. Hubner, ATKE 10, 196 (1965) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.155 eV {I4} 
$E{-n}(lab)=8.303 {I5} 
$ EN(LAB)=8.312 8 (1974Si25), 8.6 (1969Al09) 
$|G{-|g}=0.248 eV {I6}, g|G{-n}=58 eV {I2} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$g|G{-n}|G{-|g}/|G=0.17 eV {I3} 
$E{-n}(lab)=25.580 {I15} 
$ EN(LAB)=25.56 5 (1974Si25), 25.433 (1969Al09) 
$|G{-|g}=0.51 eV {I7}, g|G{-n}=289 eV {I32} 


level_energy_unit: KEV
level_spin_parity: [0-]
level_comment:
$g|G{-n}|G{-|g}/|G=0.039 eV {I2} 
$E{-n}(lab)=27.820 {I15} 
$ EN(LAB)=27.81 3 (1974Si25) 
$(8/5)g|G{-|g}=0.063 eV {I4}. g|G{-n}=2.5 eV {I12} (1974Si25) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.22 eV {I4} 
$E{-n}(lab)=46.650 {I24} 
$ EN(LAB)=46.58 6 (1974Si25), 46.423 (1969Al09) 
$|G{-|g}=0.36 eV {I6}. g|G{-n}=0.27 keV {I4} (1974Si25) 


level_energy_unit: KEV
level_comment:
$g|G{-n}|G{-|g}/|G=0.092 eV {I17} 
$E{-n}(lab)=55.44 {I3} 
$ EN(LAB)=55.36 7 (1974Si25) 
$L=1 for 55.36 (1974Si25); L=0, J=2 for 55.152 (1969Al09) 
$(8/5)g|G{-|g}=0.148 eV {I20}. g|G{-n}=74 eV {I16} for 55.36+55.13 doublet (1974Si25). 1984Ma25 assign 64 eV to 55.36 and 10 eV to 55.13 


level_energy_unit: KEV
level_spin_parity: [1-]
level_comment:
$E{-n}(lab)=66.71 {I3} 
$ EN(LAB)=66.74 10 (1974Si25) 
$(8/5)g|G{-|g}=0.212 eV {I22}. g|G{-n}=33 eV {I8} (1974Si25) 


level_energy_unit: KEV
level_spin_parity: [2+]
level_comment:
$g|G{-n}|G{-|g}/|G=0.17 eV {I5} 
$E{-n}(lab)=93.14 {I5} 
$ EN(LAB)=93.06 16 (1974Si25), 92.700 (1969Al09) 
$(8/5)g|G{-|g}=0.28 eV {I8}. g|G{-n}=0.40 keV {I3} (1974Si25) 


level_energy_unit: KEV
level_spin_parity: [2+]
level_comment:
$g|G{-n}|G{-|g}/|G=0.22 eV {I6} 
$E{-n}(lab)=127.8 {I6} 
$ EN(LAB)=127.5 3 (1974Si25) 
$(8/5)g|G{-|g}=0.36 eV {I9}. g|G{-n}=0.21 eV {I3} (1974Si25) 


level_energy_unit: KEV
level_comment:
E$others: 758 {I5} (1974Fi08), 756 {I8} (1966Ra12) 
S$others: 0.56, 3.80 (1974Fi08); 0.64, 4.12 (1966Ra12) 


level_energy_unit: KEV
level_comment:
E$others: 1788 {I5} (1974Fi08), 1790 {I12} (1966Ra12) 
S$others: 0.94 (1974Fi08), 0.72 for L=2 (1966Ra12) 


level_energy_unit: KEV
level_comment:
E$others: 2452 {I5} (1974Fi08), 2461 {I12} (1966Ra12) 
L$weakly populated group in 1990Pi05, L=0 excluded from authors' measurement near 0|', L=2 not excluded 
S,L$0.08 (1966Ra12) for L=(0) 


level_energy_unit: KEV
level_comment:
E$others: 2954 {I5} (1974Fi08), 2952 {I15} (1966Ra12) 
L$weakly populated group in 1990Pi05, L=0 excluded from authors' measurement near 0|' 
S$other: 0.12 (1966Ra12) 


level_energy_unit: KEV
level_comment:
$T=3, deduced from measured |s(p,t)/|s(p,{+3}He)=0.36 {I4}, compared to the calculated value of 0.35 for T=3 (1970Ha10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|s=79 
E,J$(4-) proposed by 1971Su05; 3- for a level at 1617 and (1,2)- for 1692 in Adopted Levels 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.225 ps {I42} (1974Mc16), 0.201 ps {I37} (1973We01), 0.37 ps {I12} (1972En02) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.35 ps {I6} (1974Mc16), 0.39 ps {I+12-9} (1973We01), 0.69 ps {I+62-28} (1972En02) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$from 1973Wa10. Others: 0.77 ps {I+18-15} (1974Mc16), 1.0 ps {I+7-4} (1973We01), 1.6 ps {I+16-6} (1972En02). Weighted average of all values is 1.18 ps {I21} 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.92 ps {I+22-19} (1974Mc16), 0.83 ps {I+24-19} (1973We01), 1.3 ps {I5} (1972En02) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.44 ps {I+14-10} (1974Mc16), 0.69 ps {I23} (1973We01), 1.5 ps {I+10-5} (1972En02) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.39 ps {I6} (1973Wa10), 0.229 ps {I39} (1974Mc16), 0.18 ps {I6} (1973We01), 0.30 ps {I6} (1972En02). 


level_energy_unit: KEV
level_spin_parity: (4,5,6)
level_comment:
$Possible configuration=|p[(1d{-5/2}{+6}(2s{-1/2}{+-1})(1d{-3/2}{+2})] ~#|n1f{-7/2}{+1}, if J|p=6- for 3809 level (2010Od01) 


level_energy_unit: KEV
level_spin_parity: GE5
level_uncertain: ?
level_comment:
$If J|p=5-, possible configuration=|p[(2s{-1/2}{+1})(1d{-3/2}{+2})] ~#|n1f{-7/2}{+1} with significant admixtures of |p1d{-3/2}{+3} ~#|n1f{-7/2} and |p[((1d{-5/2}){-1})(2s{-1/2}{+1})(1d{-3/2}{+3})] ~#|n1f{-7/2} (2010Od01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
J$L(pol d,{+3}He)=2 from 0+; first forbidden-unique |b{+-} decay to 7/2- in {+39}Ar 
T$from 1972En01 (average of four independent measurements). Others: 55.5 min {I2} (1949Ha53,1950Ha77); 55 min, 58 min (1952Ru23), 1956Pe38. The value given in 1949Ha53 has not been used by the evaluators in averaging, even though it has a much lower uncertainty than that of 1972En01. Based on sharp discrepancies noted in half-life measurements, 1970Al21 pointed out that some of the older measurements had large counting statistics thus giving low uncertainties, but the systematic errors may have been larger than the statistical errors and may not have been included. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$904.8|g to 1/2+; not 1/2 from intensity ratio in (t,p|g); log {Ift}=6.1 from (7/2)- 
T$<2.8 ns from p|g(t) in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$L(pol d,{+3}He)=2+3 for 1698+1722 gives 5/2-,7/2- for one component and 5/2+ for the other; 1326.0|g to 1/2+ and RUL determines this level is the L=2, J|p=5/2+ component while 1698 level is the L=3, J|p=5/2-,7/2- component 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_comment:
J$1745.03|g to 3/2+; not 1/2 from I|g(0|')/I|g(90|') in (t,p|g); 7/2+ from shell-model calculations in {+208}Pb({+40}Ar,X|g) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$log {Ift}=5.83 from (7/2)- in {+39}S |b{+-} decay; 484.64|g to (5/2+); possibly the lowest 7/2- state, as expected from systematics 
T$<2.8 ns from p|g(t) in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(pol d, {+3}He)=2 from 0+ and L+1/2 transfer from analyzing power. 
E$ TWO SEPARATE LEVELS AT 2053 20, 5/2+ AND 2060.5 10, 1/2+ WERE ADOPTED BY 1998En04; WHERE 1/2+ FOR 2060.5 LEVEL ORIGINATED FROM L=0 FOR A 2100 60 GROUP IN (D,3HE) WORK OF 1969Wa03. HOWEVER, BASED ON (POL D,3HE) WORK, THE 2100 GROUP IN 1969Wa03 IS, INSTEAD, ASSOCIATED WITH THE 2233 GROUP IN 1993Ma50 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$637.7|g to (7/2-), 678.8|g to (7/2+), 1122.9|g to (5/2+); 9/2+ from shell-model calculations in ({+37}Cl,{+39}Cl|g) (1994Fo04) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_comment:
J$log {Ift}=5.4 from (7/2)- in {+39}S |b{+-} decay (9/2-) from shell-model predictions in ({+40}Ar,X|g) (2013Sz02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$1984An03 used this group (with energy=2585.8 {I20} from (t,p|g)) to determine Q value=5701.9 {I25} 


level_energy_unit: KEV
level_comment:
E$from 1250 {I+70-250} weak group from 1969Wa03 only. There is some evidence of this group in spectrum (figure 2) of 1993Ma50 


level_energy_unit: KEV
level_spin_parity: 5/2+&(5/2,7/2)-
level_comment:
E$Multiplet of 1696+1722 
J$L=2+3 for 1696+1722 gives 5/2-,7/2- for one component and 5/2+ for the other 
L,S$other: L=3, C{+2}S=0.47 (1969Wa03) 
E$other: 1700 {I20} (1969Wa03) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
J$log| {Ift}=4.9 for |b{+-} decay to 1- level at E=5880 in {+40}Ar, log| {Ift}=5.9 to 3- level at E=4083 in {+40}Ar. 
T$weighted average of 1.32 min {I2} (1972Kl06), 1.44 min {I8} (1970Ke12), 1.38 min {I2} (thesis (masters) by E.L. Robinson, Purdue University,1958). Other: 1.4 min (1956Mo39) 


level_energy_unit: KEV
level_spin_parity: (0-:3+)
level_comment:
J$(3-) from figure 9 in 2013Sz02, based on shell-model prediction; (0-) listed in authors' table II. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
J$From probable allowed |b feeding to 1/2+ levels in {+41}Ar and from 2013Sz02 based on an analogy with {+37}Cl and {+39}Cl where the yrast 5/2+ level decays only to the 3/2+ and not to the 1/2+ level 
T$from 1981HuZT. Other: 34 s {I3} (1974Gu10) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$From 2013Sz02 based on an analogy with {+37}Cl and {+39}Cl where the yrast 5/2+ level decays only to the 3/2+ and not to the 1/2+ level 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
J$From 2013Sz02 based on an analogy with {+39}Cl. Note that the 7/2- alternative would require the 1346 |g to be M2 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$log| {Ift}=5.5 from 0+, however, due to weak |b feeding and incomplete decay scheme, J|p is considered as tentative 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
$Measured mean-square radius (r{+2}{-0})=1.184 fm{+2} {I21} (2006Kh08) 
T$from fit to decay curve (2006Wi10). Earlier result from this group: 3.07 s {I7} (1998WiZX). Others: 3.3 s {I2} (1981Vo04), 3.4 s {I3} (1981HuZT). 
J$3/2+ proposed (2012Au07) from syst 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_uncertain: ?
level_comment:
E$tentative level proposed in ({+48}K,X|g) from 882 {I14} |g not in coin with any other |g-ray (2012St12). E|g=888 {I6} in {+1}H({+46}Ar,X|g) (2006Ga31) and 881 {I5} placed from an 1830 level 
J$possible |g to (1/2+) is dipole 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
E$level proposed in ({+48}K,X|g) from 1338 {I15} |g in coin with 327|g (2012St12). E|g=1342 {I7} in {+1}H({+46}Ar,X|g) (2006Ga31) and 1338 {I6} placed from a 1338 level 


level_energy_unit: KEV
level_comment:
E$ordering of the 256-1338 |g cascade is not established in this work, but in 2006Ga31, intensity of the 256|g is much weaker than that of the 1338|g 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<4560 {I60} from Q(|b{+-})({+43}S)-S(n)({+43}Cl), where Q(|b{+-})=11960 {I60} and S(n)=7400 {I90} from 2021Wa16. This represents a range of unobserved levels that subsequently decay to {+42}Cl via one-neutron emission. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
MOMM1$from g factor=(-)0.2749 {I2} measured using |b-NMR method (2010De11). Sign is from theoretical model calculations. 
$2011MeZZ is a conference report from the same group as 2010De11 
J$L=1 in {+9}Be({+45}Cl,{+44}Cl) implies knockout of a neutron from 1p{-3/2} orbit. Measured g factor (2010De11) and comparisons with shell-model calculations supports 2- assignment with highly mixed configuration containing main components: |pd{-3/2}{+3}~#|nf{-7/2}{+7} and |ps{-1/2}{+1}~#|np{-3/2}{+1}. 
T$unweighted average of 650 ms {I50} (1999WiZX) and 434 ms {I60} (1995So03). 
$Cross sections in Si({+44}Cl,X): 2.92 b {I21} at 51.62 MeV/nucleon, 2.63 b {I7} at 44.98 MeV/nucleon. Strong absorption radius r{-0}{+2}=1.21 fm{+2} {I3} at 44.98 MeV/nucleon (2006Kh08). Other: 1.33 fm{+2} {I13} at 65.47 MeV/nucleon (1999Ai02). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_comment:
J$shell-model calculations predict 4- isomer at 620 keV de-exciting by an E2 transition to a g.s. and M1 transition to a 515 level. 
T$measured by 2009Ri04 from line-shape method in ({+45}Cl,{+44}Cl|g). 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
L$from momentum distributions of the recoiling {+44}Cl particles and eikonal-model calculations. L=1 implies knockout of a neutron from 1p{-3/2} orbit 
$|s=16.6 mb {I14} (2009Ri04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
E,J$ shell-model calculations predict 4- isomer at 620 keV de-exciting by an E2 transition to a g.s. and M1 transition to a 515 level 
T$measured by 2009Ri04 from line-shape method 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: MS
level_comment:
J from shell-model calculations in ({+46}Ar,2p|g) (2006Ga31). Other: 3/2+ (2003Au02; syst) 
T weighted average of 400 ms {I43} (1993So06. Mean value of 400 ms {I45}, 395 ms {I48}, and 405 ms {I35}) and 420 ms {I30} (1998WiZV) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J agreement between ({+46}Ar,2p|g) data and shell-model predictions for the energy splitting of the 1/2+, g.s., and the first excited 3/2+ (2006Ga31). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$ shell-model calculations predict 1/2+ and 3/2+ within 200 keV, former being lower in energy. Disagreement of experimental and predicted B(M1) value suggests 3/2+ for g.s. and 1/2+ for 130-keV level. See detailed discussion in 2012St12 about tensor correction 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_comment:
J$ see comment for g.s. 
T$ from Doppler broadened peak-shape analysis and GEANT4 simulations (2012St12) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
T$Measured by 2023Bh05 from (implants)|b|g-correlated decay curve. Authors compared their result with 400 ms {I43} measured by 1993So06: Phys. Rev. C 47, 2941; and with 420 ms {I30} from 1998WiZV (Proc. Conf. on Exotic Nuclei and Atomic Masses (1998), AIP Conf. Proc. 455 (1998)). The values are within 2|s of the quoted uncertainties. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<9070 {I310} (syst) from Q(|b{+-})({+45}S)-S(n)({+45}Cl), where Q(|b{+-})=14920 {I330} (syst) and S(n)=5850 {I160} from 2021Wa16. This represents a range of unobserved levels that subsequently decay to {+44}Cl via one-neutron emission. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
J$ from shell-model calculations (2012St12,2010Ga15) 
T$ from |b(implant) correlations (2004Gr20,2003Gr22). Other: 223 ms {I37} (1993So06,1995So03, |b-fragment correlations) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
T$|>200 ns estimated from time of flight in 1988Gu03. Other: 30 ms (2021Ko27, syst). 
$Theoretical T{-1/2}=25.6 ms (2019Mo01), 70.9 ms (2016Ma12) 
$Theoretical %|b{+-}n=69, %|b{+-}2n=14 (2019Mo01) 
$Theoretical %|b{+-}n=43, %|b{+-}2n=6 (2016Ma12) 


level_energy_unit: KEV
level_comment:
$|b{+-} is the only possible decay mode, followed by |b-delayed neutron emissions, thus 100% |b{+-} decay is assigned by inference, although, no radiation from the decay of {+50}Cl has yet been observed. 
$Theoretical T{-1/2}=5.5 ms, %|b{+-}n=66, %|b{+-}2n=18 (2019Mo01) 
$Theoretical T{-1/2}=17.2 ms, %|b{+-}n=5.2, %|b{+-}2n=50.6, %|b{+-}3n=2.6 (2016Ma12) 
E$observed activity is assumed to correspond to the ground state of {+50}Cl 
$Measured cross section=0.037 pb {I+43-26}, received in e-mail reply of Nov 11, 2009 from O. Tarasov (first author of 2009Ta05) 
E$fragment observed by 2009Ta05 is assumed to be in the ground state of {+50}Cl. 
J$2-,3- from |W=1/2+ for proton and |W=5/2- for neutron in theoretical calculations by 2019Mo01 
T$half-life of the decay of {+50}Cl has not yet been measured. T{-1/2}>650 ns from time-of-flight of 620-650 ns, given in e-mail reply of Sept 23, 2009 from O. Tarasov. From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+50}Cl g.s. is expected to be <50 ms, based on measured half-lives of 101 ms for {+47}Cl, 232 ms for {+46}Cl, 413 ms for {+45}Cl, and 560 ms for {+44}Cl available in the ENSDF database (as of March 25, 2019). 2017Au03 give 20 ms from systematic trend 


level_energy_unit: KEV
level_comment:
T$lower limit of >200 ns estimated from time of flight in 1990Le03. Actual half-life expected to be much longer as indicated by systematic value of 2 ms from 2017Au03. 
J$(3/2+) from syst. 


level_energy_unit: KEV
level_comment:
$|b{+-} is the only possible decay mode, followed by |b-delayed neutron emissions. 
$A total of two events were assigned to {+52}Cl, one event each with the spectrometer setting tuned for {+57}K and {+54}Ar. 
$Theoretical T{-1/2}=4.2 ms, %|b{+-}n=33, %|b{+-}2n=59, %|b{+-}3n=5, %|b{+-}4n=1, %|b{+-}5n=0, %|b{+-}6n=0, (2019Mo01) 
$Theoretical T{-1/2}=6.5 ms, %|b{+-}n=7.2, %|b{+-}2n=60.3, %|b{+-}3n=1.5, %|b{+-}4n=2.8, %|b{+-}5n=0.4 (2016Ma12) 
E$observed activity is assumed to correspond to the ground state of {+52}Cl 
J$0-, 1- from |W(proton)=1/2+ and |W(neutron)=1/2- in theoretical prediction (2019Mo01) 
T$half-life of the decay of {+52}Cl has not yet been measured. T{-1/2}>600 ns from typical time-of-flight in ion extraction experiments. From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+52}Cl is expected to be <20 ms, based on measured half-lives of 413 ms for {+45}Cl, 232 ms for {+46}Cl, and 101 ms for {+47}Cl, available in literature. Other: 2 ms (2021Ko07, systematics) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Decays to {+28}S ground state 
$From analysis of proton distribution spectrum following 2p decays of {+30}Ar, 2015Mu13 conclude that the process is a combination of the two decay processes: "true" or simultaneous 2p emission, and sequential 1p emissions 
E$the ground state is deduced at E(2p)=2.25 MeV {I+15-10} (2015Mu13) implying S(2p)({+30}Ar)=-2.25 MeV {I+15-10}. 
T$measured by 2015Mu13 from analysis of {+28}S+p+p events. Another estimate from consideration of different decay mechanisms (sequential as well as simultaneous or "true" 2p decay) gives T{-1/2}=0.1-1 fs (2015Mu13). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$from analogy with mirror states in {+30}Mg at 1483.14 keV (2018Xu04). 
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state and first excited 2+ state in {+28}S (2015Mu13, 2018Xu04) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (0+)
level_comment:
J$from analogy with mirror states in {+30}Mg at 1788.21 keV (2018Xu04) 
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state and first excited 2+ state in {+28}S, as shown in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by one branch of sequential 1p emission via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Decays by 2p decay to {+28}S ground state 
$From analysis of proton distribution spectrum from 2p decays of {+30}Ar, 2015Mu13 conclude that the process is a combination of the two decay processes: "true" or simultaneous 2p emission, and sequential 1p emissions; see Fig. 4b and Fig. 7 in 2015Mu13. 
E$the ground state is deduced at E(2p)=2.45 MeV {I+5-10} from analysis of peak "B" in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 (also analyzed as peak #2 in authors' Fig. 9), implying S(2p)({+30}Ar)=-2.45 MeV {I+5-10} i.e. ground state is unbound towards 2p emission. 
E$the ground state is deduced at E(2p)=2.25 MeV {I+15-10} from analysis of peak "B" in {+28}S+p+p spectrum in Figs. 2c and 4b of 2015Mu13, implying S(2p)({+30}Ar)=-2.25 MeV {I+15-10} i.e. ground state is unbound towards 2p emission. Note that in 2012Wa38 S(2p)=-2840 {I530} from systematic trend. 
T$from 2015Mu13 based on analysis of {+28}S+p+p events. Another estimate from consideration of different decay mechanisms (sequential as well as simultaneous or "true" 2p decay) gives T{-1/2}=0.1-1 fs (2015Mu13). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$the excited state is 0.45 MeV {I+30-14}, deduced from analysis of observed peak "C" with E(2p)=2.9 MeV {I+3-1} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 (also analyzed as peaks #3 in authors' Fig. 9). Other: 0.7 |* 10{+3} (2015Mu13) - the excited state is deduced from analysis of observed peak "A" with E(2p)=1.4 MeV, and peak "C" with E(2p)=2.9 MeV in {+28}S+p+p spectrum in Fig. 2c of 2015Mu13, the latter also analyzed as peaks #1 and #2 in authors' Fig. 4c. This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state and first excited 2+ state in {+28}S, as shown in Fig. 5 of 2015Mu13. 
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state and first excited 2+ state in {+28}S, as shown in Fig. 10 of 2018Xu04 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (0+)
level_comment:
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state and first excited 2+ state in {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 1.45 MeV {I+190-20}, deduced from analysis of observed peak "D1" with E(2p)=3.9 MeV {I+19-2} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 1.75 MeV {I+20-14}, deduced from analysis of observed peak "D2" with E(2p)=4.2 MeV {I+2-1} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 3.15 MeV {I+10-14}, deduced from analysis of observed peak "E" with E(2p)=5.6 MeV {I1} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 5.45 MeV {I+80-110}, deduced from analysis of observed peak "F1" with E(2p)=7.9 MeV {I+8-11} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by one branch of sequential 1p emission via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 6.95 MeV {I+170-210}, deduced from analysis of observed peak "F2" with E(2p)=9.4 MeV {I+17-21} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 


level_energy_unit: KEV
level_comment:
$This state decays by two branches of sequential 1p emissions via the lowest states in {+29}Cl, finally to the ground state in {+28}S, as shown in Fig. 10 of 2018Xu04 
E$the excited state is 10.15 MeV {I+100-120}, deduced from analysis of observed peak "G" with E(2p)=12.6 MeV {I+10-12} in {+28}S+p+p spectrum in Fig. 7 of 2018Xu04 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MS
level_comment:
$Other decay modes: %|b{++}|ap<0.38 and %|b{++}|a<0.03 (1998Ax02), 
$%|e+%|b{++} is primarily |b{++} (|e decay mode being negligible). 
$%|b{++}p: from 2015Li20. 
$%|b{++}2p: weighted average of 9.0 {I2} (2015Li20) and 8.5 {I4} (2000Fy01). Others: 7.2 {I11} (1998Ax02), |?12 (2002Fy01) 
$%|b{++}3p: from 2015Li20. Others: |?0.08 (based on 0.039% {I3}p decay in 2014Ko17 from IAS at 12313 keV in {+31}Ar and statement by authors that this decay represents about half the total 3p events); <0.11 (1999Fy01, at 99% confidence limit); the claim of a strong |b3p branch by 1992Ba01 with %|b{++}3p=2.1 {I10} is not supported by other measurements. 1998Ax02 pointed out that a proton peak assigned to |b{++}3p in 1992Ba01 was observed as a single-proton transition in their work 
$Note that the total %|b{++}p+%|b{++}2p+%|b{++}3p=77.27 {I36}, while summed proton branching ratio is 62% {I6}, of all observed and resolved proton branches which are assigned to proton decay of excited states in {+31}Cl from data in 2000Fy01. The missing delayed proton branch of 15% {I9} is attributed by 2000Fy01 to unresolved one or two-proton decays. 
J$spin from |b-recoil energy shift (2002Fy01,1999Th09,1998Ax01); parity from log| {Ift}=4.9 to 3/2+ g.s. of {+31}Cl 
T$weighted average of 15.1 ms {I3} (2014Ko17), 14.1 ms {I7} (2000Fy01), 15.1 ms {I+13-11} (1992Ba01), and 15 ms {I3} (1987Bo36). Others: 16.5 ms {I40} (1969Kl08); 17.7 ms {I10} (1972Kl04) is discrepant 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
E$a continuum region of {+31}Ar excitations above 5 MeV inferred based on observed 1p transitions in a broad range of energy probably feeding the 3.0 MeV {I2} level in {+30}Cl (2018Mu18) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$-6 keV {I34} inferred based on isobaric symmetry assumptions (2018Mu18) 
J$from the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$from the Adopted Levels 
$|s=10.4 mb {I13}, spectroscopic factor=24% {I3} of predicted value from many-body shell-model calculations. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from timing of delayed protons distinguishing |b{++} and |g-rays through pulse shape discrimination (1985Bj01). Others: 2008Bh08 quote 100.5 ms {I3} from unpublished ISOLDE-CERN data (reference 10 in 2008Bh08 and this value was also communicated to one of the previous evaluators by A. Garcia in an e-mail reply of November 21, 2006); 75 ms {I+75-30} (1977Ha29). 
$%|ep: other: 43 {I3} (1985Bj01). 
$Evaluated <r{+2}>{+1/2}=3.3468 fm {I62} (2013An02). 
$Measured <r{+2}>({+38}Ar-{+32}Ar)=-0.38 fm{+2} {I10} (1996Kl04); statistical uncertainty=0.038, systematic uncertainty=0.096. 
$Effective rms radii: matter radius R{+m}=3.08 fm {I9}, neutron radius R{+n}=2.87 fm {I22}, proton radius R{+p}=3.228 fm {I18} (2002Oz03). 
$Major decay branch by superallowed |b transition (0+ to 0+) to {+32}Cl 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$From E|g 
J$level Coulomb excited from 0+ 
T$deduced from B(E2)|^ and adopted E|g=1855 {I16} by the evaluator 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$from Adopted Levels 
T$deduced from B(E2)|^ and E|g=1824 
BE2$from measured cross section and relativistic Coulomb excitation theory. 
$Proton multipole matrix element (M{-|p})=0.163 b {I21}; M{-|n}/M{-|p}=0.65 {I13}, assuming M{-|n} for {+32}Ar=M{-|p} for {+32}Si=0.106 b {I15} (deduced by 2002Co09 from B(E2)|^ in 1998Ib01). This value of M{-|n}/M{-|p} is consistent with hydrodynamical estimate: N/Z=0.78 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
$Nuclear rms charge radius=3.3438 fm {I58} (2013An02 evaluation). 
$Evaluated |d<r{+2}>({+33}Ar-{+38}Ar)=-0.395 fm{+2} {I21} (2013An02) 
J$L({+1}H({+34}Ar,d)) or L(p,d)=0 from 0+; mirror analog of 1/2+ g.s. in {+33}P. 
T$weighted average of 174.1 ms {I11} (1987Bo21), 173.0 ms {I20} (1971Ha05), 171 ms {I15} (1999Tr04), 178 ms {I10} (1966Ha22,1965Ha08), 178 ms {I5} (1966Po12), and 182 ms {I5} (1964Re08). 
MOMM1$Collinear fast-beam laser spectroscopy and |b-NMR (1996Kl04). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
BE2$from Coulomb excitation 
J$mirror analog state at 1431.7, 3/2+ in {+33}P Adopted Levels; positive parity expected from Coulomb excitation from 1/2+ g.s. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
J$mirror analog state at 1847.7, 5/2+ in {+33}P Adopted Levels; positive parity expected from Coulomb excitation 1/2+ g.s. 
T$deduced by evaluators from measured B(E2)(W.u.) for 1799|g (2014We13) and |g branching ratio of 1799|g 
BE2$from Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
L$from |s(|q) in 2010Le03, 2011Le01 
S$from 2011Le01 for CH89 potential parameter. Others: 0.85 {I6} for JLM+HF parameters (2011Le01), 0.38 {I7} (2004Ga15) in {+9}Be({+34}Ar,{+33}Ar|g). Comparison with large-basis shell-model calculations give reduction factors of 0.84 {I8} for CH89 and 0.65 {I7} for JLM+HF potential parameters (2010Le03) 
$|s=4.7 mb {I9} (2004Ga15) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$Corresponding mirror state at 1431.7, 3/2+ in {+33}P Adopted Levels 
S$0.36 {I9} (2004Ga15) in {+9}Be({+34}Ar,{+33}Ar|g) 
$|s=3.2 mb {I8} (2004Ga15) 
E$1360 and 1800 form an unresolved doublet in 2010Le03, 2011Le01 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$Corresponding mirror state at 1847.7, 5/2+ in {+33}P Adopted Levels 
S$0.56 {I8} (2004Ga15) in {+9}Be({+34}Ar,{+33}Ar|g) 
$|s=4.9 mb {I7} (2004Ga15) 
E$1360 and 1800 form an unresolved doublet in 2010Le03, 2011Le01 


level_energy_unit: KEV
level_spin_parity: 3/2+,(5/2+)
level_comment:
J$from level-scheme Fig. 2 in 2004Cl02; 3/2+ listed in authors' Table I. 
$Corresponding mirror state at 3276.2, 3/2+ in {+33}P Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
E$3460 and 3820 form an unresolved doublet in 2010Le03, 2011Le01 
S$2004Cl02 report 0 
$Corresponding mirror state at 3627.9, 7/2+ in {+33}P Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
S$|>0.34 {I7} (2004Ga15) in {+9}Be({+34}Ar,{+33}Ar|g) 
$|s=2.8 mb {I6} (2004Ga15) 
E$3460 and 3820 form an unresolved doublet in 2010Le03, 2011Le01 
$Corresponding mirror state at 4048.3, 5/2+ in {+33}P Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$ <r{+2}>{+1/2}=3.365 fm {I4} (2004An04 evaluation and its 2008 update on webpage: http://cdfe.sinp.msu.ru) 
$ |d<r{+2}>({+38}Ar,{+34}Ar)=-0.251 fm{+2} {I6} {I62}, first is statistical and the second is systematic uncertainty (1996Kl04, 2000Ge20) 
T$ from 2006Ia05, half-life measured and analyzed using parent-daughter ({+34}Ar to {+34}Cl decay) composite decay and a new fitting procedure, gas-ionization chamber used as detection system. Beam of pure {+34}Ar ions was produced in {+1}H({+35}Cl,2n) reaction. Others: 844.5 ms {I34} (1974Ha26, also 1972Ha58), 0.85 s {I10} (1967Ba36), 1.2 s {I3} (1966Mi11) 
T$ Check 1971Mo27 for half-life ?? 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|b{-2}(p,p')=0.27 {I2} (2001Kh17) 
J$L(p,t)=L(p,p')=2 
T$ 2001Ra27 evaluation lists 305 fs {I49} which is close to the value given here from 1985Al18. It seems a somewhat different averaging procedure is used in 2001Ra27 


level_energy_unit: KEV
level_comment:
L$neither L=2 nor L=3 fits |s(|q) data in 1969Br21, (3-) is preferred since first 3- is expected near this energy. 
E$ 4560 40 (1969Br21) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$M{-n}/M{-p}=0.99 {I17}(N/Z) (experimental), 1.35 {I0.28}(N/Z) (2001Kh17) (phenomenological analysis of experimental data) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$340 FS 45 (LINE-SHAPE), 284 FS 55 (CENTROID-SHIFT) (1985Al18) 
T$others: 229 fs {I55} (1974Be18), 139 fs {I42} (1974Gr19), 104 fs {I35} (1972Ca22) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$177 FS 35 (LINE-SHAPE), 267 FS 66 (CENTROID-SHIFT) (1985Al18) 
T$others: 149 fs {I49} (1974Be18), 90 fs {I42} (1974Gr19), 83 fs {I45} (1972Ca22) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$n(840|g)(|q) gives J=1-4, J=2 is preferred by 1974Gr19 based on mirror argument 
T$<215 FS (LINE-SHAPE) (1985Al18) 
T$90 fs {I+118-90} from centroid-shift method (1985Al18). Others: <243 fs (1974Be18), >277 fs (1974Gr19) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$3- is supported by |g(|q) data of 1974Be18, but 1- is not ruled out. 2+ is five times less likely from these data 
T$weighted average of 270 fs 125 (1974Be18), 180 fs 55 (1974Gr19), 208 fs 55 (1972Ca22) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$from |b(t) using two component fit to the decay of {+34}Ar and {+34}Cl (2020Ia01). The T{-1/2} of {+34}Cl was fixed to the world average of 1526.55 ms {I44}. 2020Ia01 give the T{-1/2} of {+34}Ar with only statistical uncertainty as 0.84646 s {I19}; final quote uncertainty includes systematic effects. 


level_energy_unit: KEV
level_spin_parity: (2+,4+)
level_comment:
$E{-c.m.}=4353 keV. Assuming J{+|p}=2{++}, |G{-|a}=20 keV {I+80-17}, |G{-p}=25 keV {I+500-20}. |w|g(|a,p)=100 keV. Assuming J{+|p}=4{++}, |G{-|a}=0.5 keV {I+1.4} {I-0.4}, |G{-p}=0.3 keV {I+3.5} {I-0.3}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|s=52.1 mb {I29} measured from laboratory scattering angles |q=0|' to |q{-max}=55|' mrad at 64.3 MeV/nucleon mid-target energy 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
MOMM1$ |b-NMR (2002Ma41). Others: +0.633 {I2} (1965Ca04), +0.633 {I7} (1996Kl04). Measured using |b-NMR method. Also from 2011StZZ, 1989Ra17 
MOME2$from 1996Kl04 using |b-NMR method. Also from 2011StZZ. 
J$L(p,d)=L({+3}He,|a)=2; log| {Ift}=5.09 to 1/2+ level in {+35}Cl 
T$weighted average of 1.83 s {I3} (1956Ki29), 1.83 s {I2} (1959Al10), 1.79 s {I1} (1960Ja12), 1.84 s {I10} (1960Wa04), 1.76 s {I3} (1963Ne05), 1.770 s {I6} (1969Wi18), 1.787 s {I12} (1971Ge04), 1.774 s {I4} (1977Az01), and 1.7754 s {I11} (2006Ia05). 
$Evaluated rms charge radius=3.3632 fm {I66} (2004An14 evaluation), 3.3629 fm {I42} from 2008 update of 2004An14. 


level_energy_unit: KEV
level_comment:
E$weighted average of 2600 {I20} in 1968Ko11 and 2630 {I20} in 1968Jo04. 
L$ 1 from 1968Jo04, in disagreement with L({+3}He,|a)=2 
S$0.12 from 1968Jo04 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$ from L=2 and d{-3/2} configuration 
S$ extracted neutron spectroscopic factors for g.s., d{-3/2}: 1.60 {I16}, 0.76 {I8}, 2.29 {I23}, 1.09 {I11} using different sets of parameters (2010Le03). 2011Le01 give 2.3 {I2} for CH89 parameters and 1.6 {I1} for JLM+HF parameters 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$ Nuclear rms charge radius: 3.3902 fm {I20} (2004An14,evaluation); 3.3901 fm {I23} from 2008 update of 2004An14 
$ Spin measurement by optical spectroscopy (1937Ko03,1953Me73) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
MOMM1$transient-field method (2006Sp01) 
MOME2$measured by Coulomb excitation reorientation (1971Na06, {+206}Pb({+36}Ar,{+36}Ar'|g)) 
T$weighted average (in fs) of: 310 {I31} ({+9}Be({+40}Ca,{+13}C|g)), 341 {I20} ({+36}Ar(e,e')), 335 {I27} ({+197}Au({+36}Ar,{+36}Ar'|g)), 305 {I49} ({+206}Pb({+36}Ar,{+36}Ar'|g)), 319 {I78} ({+32}S(|a,|g):res), 319 {I28} ({+35}Cl(p,|g):res); other: 450 {I14} ({+12}C({+32}S,{+8}Be)). 2001Ra27 evaluation gives adopted |t=463 fs {i46} or T{-1/2}=321 fs {i32} 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
E$6868.5 {I10} (1972Ho40), 6865.2 {I10} (1974Jo02) 
J$(1,2+) from {+35}Cl(p,|g):res; |p=- from L=(0) in {+35}Cl({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$7710.7 {I18} (1972Ho40), 7711.1 {I15} (1974Jo02) 
J$1+,2+,3+ from log| {Ift}=4.9 ({+36}K |e decay); 1 from {+35}Cl(p,|g) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$from {+36}K |e decay 
J$1+,2+,3+ from log| {Ift}=5.4 from 2+ parent ({+36}K |e decay); 3+ less likely from no |g to 0+, g.s. 


level_energy_unit: KEV
level_spin_parity: (1,2,3-)
level_comment:
E,J$ strong |g to 0+ suggests J|p=1,2,3-. In {+35}Cl(p,p{-0}) data, J|p=(1,2,3)- is proposed, but 2+ is suggested from |g-ray data (as commented in 1978En04 evaluation). This level may be a doublet 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_comment:
$Weighted average of 9147.6 {I14} (E(p)=622.7 {I14} (1996Il02)) and 9149 {I3} (E(|a)=2229 {I3} (1996Il02)) 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$Weighted average of 9709 {I3} (E(|a)=2727 {I3} (1996Il02)) and 9709.2 {I14} (E(p)=1168.5 {I14} (1996Il02)) 


level_energy_unit: KEV
level_comment:
$Weighted average of 10435 {I10} (E(p)=1874 {I10} (1980Es01)) and 10450 {I3} (E(|a)=3385 {I3} (1996Il02)) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$Weighted average of 10556 {I10} (E(p)=1992 {I10} (1980Es01)) and 10564 {I3} (E(|a)=3487 {I3} (1996Il02)) 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_comment:
$Weighted average of 11036 {I10} (E(p)=2458 {I10} (1980Es01)) and 11058 {I3} 11036 {I10}( E(|a)=3926 {I3} (1996Il02)) 


level_energy_unit: KEV
level_spin_parity: 1+,2+,3+
level_comment:
$Weighted average of 11223 {I10} (E(p)=2640 {I10} (1980Es01)) and 11238 {I4} (E(|a)=4086 {I4} (1996Il02)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E,J$ from Adopted Levels 
$ Measured Ep(c.m.)=610 keV. Strength |w|g{-p,|a}=0.018 eV {I2}, using an isotropic distribution and |w|g{-p,|a}=0.012 eV {I2} using the angular distribution estimated by the R-matrix code MULTI for on-resonance beam energy, E{+35}Cl==21.83, 21.85, 21.87 and 21.90 MeV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(|a)(lab)=2552.1 {I10} (weighted average) 
$E(|a)(lab)=2552.0 {I10} (1994Il01, deduced from E(level)=8909.0 {I10}), E(|a)(lab)=2554 {I5} (1964Er04) 
$S(|a,p)=0.03 {I1} (1964Er04) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(|a)(lab)=2787.2 {I14} (weighted average) 
$E(|a)(lab)=2787.4 {I15} (1994Il01, deduced from E(level)=9118.2 {I15}), E(|a)(lab)=2785 {I5} (1964Er04) 
$S(|a,p)=0.3 {I1} (1964Er04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_uncertain: ?
level_comment:
$E(|a)(lab)=4168 {I5} (1971Cl09); according to 1983Ch29 this resonance is probably non-existent 
$S(|a,p)=0.50 {I25} (1971Cl09) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$1970.39 {I5} (1972Ho40), 1970.2 {I3} (1974Jo02) 
T$mean lifetime |t in fs: 400 {I100} (1970Th04); 350 {I120} (1972Ho40); 340 {I110} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$4178.33 {I11} (1972Ho40), 4178.1 {I7} (1974Jo02) 
T$mean lifetime |t in fs: >2000 (1970Th03); >1800 (1972Ho40); >1500 (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$4414.36 {I17} (1972Ho40), 4414.7 {I5} (1974Jo02) 
T$mean lifetime |t in fs: 125 {I20} (1970Th03); 86 {I18} (1972Ho40); 90 {I40} (1974Jo02); 129 {I8} (1975Sa03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$4440.1 {I2} (1972Ho40), 4440.2 {I5} (1974Jo02) 
J$|p from 2699.4, M1+E2 |g from 3+, 7140 
T$mean lifetime |t in fs: 94 {I30} (1970Th03); 100 {I40} (1972Ho40); 100 {I40} (1974Jo02); 153 {I6} (1975Sa03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$4951.9 {I5} (1972Ho40), 4950.9 {I5} (1974Jo02) 
J$|p=+ based on RUL 
T$mean lifetime |t in fs: <70 (1972Ho40); <50 (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
E$4974.05 {I19} (1972Ho40), 4974.1 {I7} (1974Jo02) 
T$mean lifetime |t in fs: >1000 (1970Th03); >1000 (1972Ho40); >1600 (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
E$5171.14 {I16} (1972Ho40), 5170.9 {I7} (1974Jo02) 
T$mean lifetime |t in fs: >1000 (1970Th03); >850 (1972Ho40); >450 (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$5835.9 {I8} (1972Ho40), 5836.0 {I5} (1974Jo02) 
T$mean lifetime |t in fs: 6 {I4} (1970Th03); 8 {I3} (1972Ho40); 14 {I5} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$5856.7 {I2} (1972Ho40), 5856.0 {I7} (1974Jo02) 
T$mean lifetime |t in fs: 840 {I300} (1970Th03); 340 {I170} (1972Ho40); 260 {I110} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$5895.9 {I2} (1972Ho40), 5896.1 {I7} (1974Jo02) 
T$mean lifetime |t in fs: >600 (1970Th03); 800 {I350} (1973Ho33, superseding 400 {I+1400-200} (1972Ho40)) 300+650-140 (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_comment:
E$6217.1 {I3} (1972Ho40), 6217.8 {I5} (1974Jo02) 
T$mean lifetime |t in fs: 280 {I90} (1972Ho40); 230 {I60} (1974Jo02) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$6610.8 {I3} (1972Ho40), 6611.4 {I5} (1974Jo02) 
T$mean lifetime |t in fs: 23 {I19} (1972Ho40); 22 {I10} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$6835.2 {I2} (1972Ho40), 6834.9 {I5} (1974Jo02) 
T$mean lifetime |t in fs: 800 {I250} (1973Ho33, superseding >800 (1972Ho40)); >350 (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$6836.5 {I2} (1972Ho40), 6836.5 {I4} (1974Jo02) 
T$mean lifetime |t in fs: 330 {I140} (1970Th03); 230 {I80} (1972Ho40); 200 {I80} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: FS
level_comment:
E$7136.3 {I18} (1972Ho40), 7136.6 {I10} (1974Jo02) 
T$mean lifetime |t in fs: <27 (1972Ho40); 13 {I5} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: FS
level_comment:
E$7354.0 {I3} (1972Ho40), 7353.6 {I7} (1974Jo02) 
T$mean lifetime |t in fs: 190 {I90} (1972Ho40); 140 {I30} (1974Jo02) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$7432.9 {I9} (1972Ho40), 7431.6 {I10} (1974Jo02) 
T$mean lifetime |t in fs: 50 {I+60-40} (1972Ho40) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$7573.1 {I3} (1972Ho40), 7573.0 {I7} (1974Jo02) 
T$mean lifetime |t in fs: 300 {I100} (1972Ho40); 160 {I80} (1974Jo02) 


level_energy_unit: KEV
level_spin_parity: (2+,3,4-)
level_comment:
$E(p)(lab)=444.3 {I5} 
$444.1 {I5} (1961He19); 445.9 {I15} (1961Ku01); 444.0 {I3} (1965Er06); 442.4 {I8} (1994Il01, deduced from E(level)) 
$S(p,|g)=0.09 


level_energy_unit: KEV
level_spin_parity: (3-,4,5-)
level_comment:
$E(p)(lab)=522.5 {I10} 
$522.2 {I8} (1965Er06); 519.8 {I17} (1994Il01, deduced from E(level)) 
$S(p,|g)=0.012 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
$E(p)(lab)=533.2 {I6} 
$532.9 {I6} (1961He19); 533.8 {I15} (1961Ku01); 533.0 {I8} (1965Er06); 531.9 {I13} (1994Il01 deduced from E(level)) 
J$from 1976Gr05 
$S(p,|g)=0.18 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=575.5 {I6} 
$575.2 {I6} (1961He19); 575.9 {I15} (1961Ku01): 575.4 {I9} (1965Er06); 572.7 {I15} (1994Il01 deduced from E(level)) 
$S(p,|g)=0.17 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=643.5 {I7} 
$643.2 {I7} (1961He19); 644.2 {I15} (1961Ku01); 643.1 {I10} (1965Er06); 643.4 {I14} (1994Il01 deduced from E(level)) 
$S(p,|g)=0.17 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_comment:
$E(p)(lab)=656.3 {I7} 
$656.0 {I7} (1961He19); 656.8 {I15} (1961Ku01); 656.0 {I10} (1965Er06); 653.9 {I15} (1994Il01 deduced from E(level)) 
$S(p,|g)=0.11 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$E(p)(lab)=733.8 {I11} 
$734.6 {I15} (1961Ku01); 733.4 {I11} (1965Er06); 733.8 {I13} (1994Il01 deduced from E(level)) 
$S(p,|g)=0.7 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
$E(p)(lab)=816.0 {I4} 
$818.2 {I15} (1961Ku01); 817.0 {I12} (1965Er06); 816.0 {I4} (1972Ho40) 
$S(p,|g)=0.6 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=859.6 {I4} 
$861.4 {I15} (1961Ku01); 859.7 {I13} (1965Er06); 859.9 {I4} (1972Ho40); 859.2 {I7} (1994Il01 deduced from E(level)) 
$|G=12 eV (1971BrXT) 
$S(p,|g)=4.9 {I7} (1966En04), S(p,|g)=5.5 {I13} (1978Pa03) 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$E(p)(lab)=873.6 {I8} 
$873.3 {I13} (1965Er06); 873.2 {I11} (1968Bo06) 
$S(p,|g)=0.3, S(p,|a{-0})=1.2 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=883.7 {I8} 
$885.7 {I15} (1961Ku01); 883.5 {I13} (1965Er06); 883.4 {I11} (1968Bo06) 
$S(p,|g)=0.7, S(p,|a{-0})=8 


level_energy_unit: KEV
level_spin_parity: 1-,2+,3-
level_comment:
$E(p)(lab)=968.2 {I9} 
$968.0 {I5} (1965Er06); 968.0 {I12} (1968Bo06) 
$S(p,|g)=0.14, S(p,|a{-0})=1.8 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$E(p)(lab)=986.5 {I5} 
$985.9 {I25} (1965Er06); 986.5 {I5} (1974Jo02); 985.5 {I12} (1968Bo06) 
$S(p,|g)=0.6, S(p,|a{-0})=0.5 


level_energy_unit: KEV
level_spin_parity: (2,3)
level_comment:
$E(p)(lab)=1024.5 {I5} 
$1023 {I2} (1965Er06); 1023.1 {I13} (1972Ho40); 1024.5 {I5} (1974Jo02) 
$S(p,|g)=0.3 


level_energy_unit: KEV
level_spin_parity: (0+:4+)
level_comment:
$E(p)(lab)=1073.4 {I5} 
$1073 {I2} (1965Er06); 1073.0 {I3} (1972Ho40); 1073.4 {I5} (1974Jo02) 
$S(p,|g)=0.9 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
$E(p)(lab)=1098.1 {I4} 
$1097 {I2} (1965Er06); 1098.1 {I3} (1972Ho40); 1098.1 {I4} (1974Jo02) 
$S(p,|g)=2.4 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1119.8 {I7} 
$1116 {I2} (1965Er06); 1119.8 {I7} (1974Jo02); 1119.4 {I13} (1968Bo06) 
$S(p,|g)=0.4, S(p,|a{-0})=12 


level_energy_unit: KEV
level_spin_parity: (0,1,2)-
level_comment:
$E(p)(lab)=1131.5 {I5} 
$1129 {I2} (1965Er06); 1128.3 {I17} (1972Ho40); 1131.5 {I3} (1974Jo02) 
$S(p,|g)=0.2 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=1193.5 {I10} 
$1191 {I2} (1965Er06); 1193.5 {I10} (1974Jo02); 1192.6 {I13} (1968Bo06) 
$S(p,|g)=0.3, S(p,|a{-0})=7 


level_energy_unit: KEV
level_spin_parity: 4+,6+
level_comment:
$E(p)(lab)=1208.8 {I5} 
$1207 {I2} (1965Er06); 1208.8 {I5} (1974Jo02) 
J$|DJ=2 E2, or |DJ=0, M1+E2 |g to 4+, 4414 
$S(p,|g)=0.12 


level_energy_unit: KEV
level_spin_parity: 1-,3-,4+
level_comment:
$E(p)(lab)=1262.7 {I5} 
$1264 {I2} (1965Er06); 1262.7 {I5} (1974Jo02); 1264.0 {I14} (1968Bo06) 
$S(p,|a{-0})=3.1 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=1266.0 {I8} 
$1267 {I2} (1965Er06); 1264.0 {I9} (1972Ho40); 1266.0 {I18} (1974Jo02) 
$|G=400 eV (1971BrXT) 
$S(p,|g)=1.9 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$E(p)(lab)=1394.7 {I5} 
$1396 {I2} (1965Er06); 1393.0 {I9} (1972Ho40); 1394.7 {I5} (1974Jo02) 
$S(p,|g)=0.5 


level_energy_unit: KEV
level_spin_parity: (2+,3+,4+)
level_comment:
$E(p)(lab)=1411.1 {I5} 
$1412 {I2} (1965Er06); 1409.1 {I11} (1972Ho40); 1411.1 {I5} (1974Jo02) 
$S(p,|g)=0.2 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1422.1 {I5} 
$1422 {I2} (1965Er06); 1422.1 {I5} (1974Jo02); 1423.4 {I15} (1968Bo06) 
J$1-,2+ (1974Jo02, |g(|q)) and (2-,3-) (|g decay) are contradictory and may indicate a doublet 
$S(p,|g)=0.5, S(p,|a{-0})=14 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$E(p)(lab)=1435.3 {I5} 
$1436 {I2} (1965Er06); 1435.3 {I5} (1974Jo02); 1436.3 {I15} (1968Bo06) 
$S(p,|g)=0.4, S(p,|a{-0})=2.8 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
$E(p)(lab)=1461.3 {I5} 
$1462 {I2} (1965Er06); 1461.3 {I5} (1974Jo02) 
J$from 2002Ro24 based on measured |g multipolarities 
$S(p,|g)=0.3 


level_energy_unit: KEV
level_spin_parity: (2,3-)
level_comment:
$E(p)(lab)=1476.9 {I5} 
$1477 {I2} (1965Er06); 1475.6 {I12} (1972Ho40); 1476.9 {I5} (1974Jo02) 
$S(p,|g)=0.6 


level_energy_unit: KEV
level_spin_parity: 1+,(2+)
level_comment:
$E(p)(lab)=1518.8 {I5} 
$1517 {I2} (1965Er06); 1518.8 {I5} (1974Jo02); 1518.1 {I16} (1968Bo06) 
$S(p,|g)=18 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$E(p)(lab)=1527.7 {I16} 
$1528 {I2} (1965Er06); 1527.7 {I16} (1968Bo06) 
$S(p,|g)=0.5 (sum of strengths of 9991.9 and 9992.9), S(p,|a{-0})=60 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1528.7 {I9} 
$1528 {I2} (1965Er06); 1528.6 {I9} (1972Ho40); 1528.7 {I9} (1974Jo02) 
$S(p,|g)=0.5 (sum of strengths of 9991.9 and 9992.9) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=1581.7 {I12} 
$1578 {I2} (1965Er06); 1581.7 {I12} (1974Jo02); 1581.5 {I20} (1968Bo06) 
T$2.1 {I5} keV (1968Bo06), 900 eV (1971BrXT) 
$|G=1.5 {I3} keV (1965Er06); |G=2.1 {I5} keV (1968Bo06) 
$S(p,|g)=8.4, S(p,|a{-0})=24 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1588.1 {I15} 
$1588.1 {I15} (1974Jo02); 1588.3 {I20} (1968Bo06) 
$|G=0.9 {I5} keV (1968Bo06), |G=400 eV (1968Bo06) 
$S(p,|g)=0.8, S(p,p{-1})=0.03, S(p,|a{-0})=240 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1633.7 {I15} 
$1633 {I2} (1965Er06); 1633.7 {I15} (1974Jo02); 1634.3 {I20} (1968Bo06) 
$S(p,|g)=0.3, S(p,p{-1})<0.01, S(p,|a{-0})=6 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=1638.3 {I6} 
$1637 {I2} (1965Er06); 1638.3 {I6} (1974Jo02); 1637.0 {I18} (1968Bo06) 
$|G=400 eV (1971BrXT) 
$S(p,|g)=1.6, S(p,|a{-0})=180 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=1708.3 {I5} 
$1705 {I3} (1965Er06); 1708.3 {I5} (1974Jo02); 1708.8 {I20} (1968Bo06) 
$S(p,|g)=3.0, S(p,|a{-0})=15 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$E(p)(lab)=1714.4 {I5} 
$1714 {I3} (1965Er06); 1714.4 {I5} (1974Jo02); 1714.9 {I20} (1968Bo06) 
$|G=0.9 {I5} keV (1968Bo06) 
$S(p,|g)=5.0, S(p,|a{-0})=150 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_comment:
$E(p)(lab)=1762.7 {I5} 
$1761 {I3} (1965Er06); 1759.9 {I8} (1972Ho40); 1762.7 {I5} (1974Jo02) 
$S(p,|g)=2.9 
$E(p)(lab)=1761.9 {I9} 


level_energy_unit: KEV
level_spin_parity: (3-,4)
level_comment:
$E(p)(lab)=1799.4 {I10} 
$1797 {I3} (1965Er06); 1799 {I3} (1965Er06); 1799.4 {I10} (1974Jo02) 
$S(p,|g)=0.8 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=1811.0 {I5} 
$1811 {I3} (1965Er06); 1811.0 {I5} (1974Jo02); 1812.6 {I21} (1968Bo06) 
$|G=400 eV (1971BrXT) 
$S(p,|g)=1.2, S(p,|a{-0})=13 


level_energy_unit: KEV
level_spin_parity: (3-,4-,5-)
level_comment:
$E(p)(lab)=1815.6 {I6} 
$1815 {I3} (1965Er06); 1813.3 {I6} (1972Ho40); 1815.6 {I6} (1974Jo02) 
$S(p,|g)=1.8, S(p,p{-1})=0.03 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=1825.2 {I10} 
$1825.2 {I10} (1974Jo02); 1827.4 {I21} (1968Bo06) 
$S(p,|g)=0.3, S(p,p{-1})=0.01, S(p,|a{-0})=2.6 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$E(p)(lab)=1846.2 {I9} 
$1845 {I3} (1965Er06); 1846.2 {I9} (1974Jo02); 1847.3 {I19} (1968Bo06) 
$S(p,|g)=1.9, S(p,p{-1})=0.01, S(p,|a{-0})=13 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1864.7 {I15} (1974Jo02) 
$1864.7 {I15} (1974Jo02); 1867.1 {I19} (1968Bo06) 
$S(p,|g)=0.6, S(p,p{-1})=0.02, S(p,|a{-0})=80 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=1969.0 {I10} 
$1969 {I3} (1965Er06); 1967 {I3} (1972Ho40); 1969.0 {I10} (1974Jo02); 1969.1 {I19} (1974Jo02, (p,p{-1})) 
$|G=7 {I2} keV (1965Er06) 
$S(p,|g)=13, S(p,p{-1})=29 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1983.6 {I14} 
$1984 {I3} (1965Er06); 1983 {I3} (1972Ho40); 1983.6 {I14} (1974Jo02); 1984.2 {I6} (1974Jo02, (p,p{-1})) 
J$(1,2,3)- (1971BrXT, (p,p{-0})) and (2+) from |g decay may indicate a doublet 
$|G=15 {I5} keV (1965Er06) 
$S(p,|g)=6.1, S(p,p{-1})=2.6 


level_energy_unit: KEV
level_spin_parity: (1,2,3)-
level_comment:
$E(p)(lab)=2050.7 {I5} 
$2051.3 {I7} (1974Jo02); 2050.7 {I5} (1974Jo02, (p,p{-1})) 
$|G=2.5 keV (1971BrXT) 
$S(p,|g)=1.3, S(p,p{-1})=33 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=2091.2 {I12} 
$2091 {I3} (1965Er06); 2091.6 {I16} (1974Jo02); 2091.2 {I12} (1974Jo02, (p,p{-1})) 
$S(p,|g)=7.0, S(p,p{-1})=29 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=2114.3 {I9} 
$2113 {I3} (1965Er06); 2114.1 {I10} (1974Jo02); 2114.3 {I9} (1974Jo02, (p,p{-1})) 
$S(p,|g)=2.1, S(p,p{-1})=1.4, S(p,|a{-0})=140 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
$E(p)(lab)=2135.7 {I6} 
$2135 {I3} (1965Er06); 2135.7 {I13} (1972Ho40); 2135.9 {I10} (1974Jo02); 2135.7 {I6} (1974Jo02, (p,p{-1})) 
$S(p,|g)=2.7, S(p,p{-1})=1.1 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
$E(p)(lab)=2169.4 {I7} 
$2168 {I3} (1965Er06); 2166.9 {I5} (1972Ho40); 2169.5 {I10} (1974Jo02); 2169.4 {I7} (1974Jo02, (p,p{-1})); 2168 {I3} (1968Bo06) 
$|G=2.9 {I5} keV (1968Bo06) 
$S(p,|g)=10, S(p,p{-1})=5.9, S(p,|a{-0})=60 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=2190.1 {I5} 
$2191 {I3} (1965Er06); 2190 {I3} (1972Ho40); 2189.4 {I10} (1974Jo02); 2190.1 {I5} (1974Jo02, (p,p{-1})) 
$|G=4.1 keV (1971BrXT), |G=7 {I2} keV (1965Er06) 
$S(p,|g)=5.3, S(p,p{-1})=3.0 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=2205.4 {I11} 
$2205.4 {I11} (1974Jo02, (p,p{-1})); 2207 {I3} (1968Bo06) 
$|G=2.0 {I5} keV (1968Bo06), |G=1.5 keV (1971BrXT) 
$S(p,p{-1})=26, S(p,|a{-0})=1000 


level_energy_unit: KEV
level_spin_parity: 5
level_comment:
$E(p)(lab)=2231.4 {I10} 
$2231 {I3} (1965Er06); 2230.4 {I7} (1972Ho40); 2231.4 {I10} (1974Jo02); 2231.5 {I10} (1974Jo02, (p,p{-1})) 
$S(p,|g)=9.7, S(p,p{-1})=7.0 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=2256.6 {I15} 
$2256 {I3} (1965Er06); 2256.6 {I15} (1974Jo02); 2258.4 {I23} (1968Bo06) 
$|G=300 eV (1971BrXT) 
$S(p,|g)=5.4, S(p,p{-1})=4.7, S(p,|a{-0})=80 


level_energy_unit: KEV
level_spin_parity: (0+,1-,2+)
level_comment:
$E(p)(lab)=2258.0 {I12} 
$2256.7 {I9} (1972Ho40); 2258.0 {I12} (1974Jo02, (p,p{-1})); 2260.1 {I25} (1968Bo06) 
$S(p,|a{-0})=190 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_comment:
$E(p)(lab)=2318.9 {I15} 
$2318.9 {I15} (1974Jo02, (p,p{-1})); 2318.0 {I23} (1968Bo06) 
$S(p,p{-1})=1.5, S(p,|a{-0})=160 


level_energy_unit: KEV
level_spin_parity: (0+,1-,2+)
level_comment:
$E(p)(lab)=2348.9 {I15} 
$2348.9 {I15} (1974Jo02, (p,p{-1})); 2348.0 {I25} (1968Bo06) 
$S(p,p{-1})=1.5, S(p,|a{-0})=13 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2368.3 {I12} 
$2368.3 {I12} (1974Jo02); 2367.5 {I15} (1974Jo02, (p,p{-1})); 2368.2 {I15} (1976Hu01) 
$S(p,|g)=4.0, S(p,p{-1})=1.6 


level_energy_unit: KEV
level_spin_parity: (1-,3-,4+)
level_comment:
$E(p)(lab)=2392.3 {I15} 
$2390.1 {I15} (1974Jo02, (p,p{-1})); 2392.3 {I15} (1976Hu01); 2392.5 {I24} (1968Bo06) 
$S(p,p{-1})=1.3, S(p,|a{-0})=31 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2406.1 {I15} 
$2403.8 {I15} (1974Jo02, (p,p{-1})); 2406.1 {I15} (1976Hu01) 
$S(p,p{-1})=0.7 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=2412.6 {I15} 
$2410.0 {I15} (1974Jo02, (p,p{-1})); 2412.6 {I15} (1976Hu01) 
$S(p,p{-1})=1.4 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=2414.4 {I15} 
$2414.4 {I15} (1976Hu01); 2410 {I4} (1976Ma40); 2413.1 {I24} (1968Bo06) 
$S(p,|g)=0.10 (1976Hu01), S(p,|a{-0})=290 
$|G{-|g}=80 {I5} meV (1976Ma40) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2468.1 {I10} 
$2468.1 {I10} (1974Jo02); 2468.5 {I15} (1974Jo02, (p,p{-1})) 
$S(p,p{-1})=14 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2532.0 {I15} 
$2532.0 {I15} (1974Jo02); 2533.3 {I15} (1974Jo02, (p,p{-1})) 
$S(p,p{-1})=1400 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2593.4 {I15} 
$2595 {I4} (1965Er06); 2593.4 {I15} (1974Jo02); 2594.8 {I15} (1974Jo02, (p,p{-1})); 2595 {I3} (1968Bo06) 
$|G=1.0 {I5} keV (1968Bo06) 
$S(p,p{-1})=23, S(p,|a{-0})=800 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$E(p)(lab)=2609.5 {I15} 
$2609.5 {I15} (1974Jo02, (p,p{-1})); 2610 {I3} (1968Bo06) 
$S(p,p{-1})=190, S(p,|a{-0})=160 


level_energy_unit: KEV
level_spin_parity: 1-,3-
level_comment:
$E(p)(lab)=2626.3 {I15} 
$2626.3 {I15} (1974Jo02, (p,p{-1})); 2630 {I3} (1968Bo06) 
$|G=1.3 {I5} keV (1968Bo06) 
$S(p,p{-1})=4.0, S(p,|a{-0})=410 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2687.1 {I15} 
$2687.1 {I15} (1974Jo02, (p,p{-1})); 2688 {I4} (1968Bo06) 
$|G=5.5 {I15} keV (1968Bo06) 
$S(p,p{-1})=140, S(p,|a{-0})=110 


level_energy_unit: KEV
level_spin_parity: 1-,3-
level_comment:
$E(p)(lab)=2700.0 {I15} (1974Jo02, (p,p{-1})) 
$2700.0 {I15} (1974Jo02, (p,p{-1})); 2704 {I3} (1968Bo06) 
$S(p,p{-1})=10, S(p,|a{-0})=430 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=2725.3 {I15} (1974Jo02, (p,p{-1})) 
$2725.3 {I15} (1974Jo02, (p,p{-1})); 2729 {I3} (1968Bo06) 
$|G=1.1 {I5} keV (1968Bo06) 
$S(p,p{-1})=770, S(p,|a{-0})=420 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2752.4 {I15} (1974Jo02, (p,p{-1})) 
$2751.7 {I15} (1974Jo02); 2752.4 {I15} (1974Jo02, (p,p{-1})) 
$S(p,p{-1})=6.4 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2777.5 {I15} 
$2777.5 {I15} (1974Jo02, (p,p{-1})); 2777 {I3} (1968Bo06) 
$S(p,p{-1})=64, S(p,|a{-0})=13 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=2911 {I2} 
$2911 {I4} (1965Er06); 2909 {I2} (1974Jo02); 2911 {I2} (1974Jo02, (p,p{-1})); 2913 {I3} (1968Bo06) 
$|G=0.8 {I5} keV (1968Bo06) 
$S(p,p{-1})=320, S(p,|a{-0})=90 


level_energy_unit: KEV
level_spin_parity: (0:3)-
level_comment:
E$weighted average of: 8302 {I10} (1970Mo10), 8303.4 {I30} (1994Il01) 
L,S$also 0.34 for L=(1), 0.25+0.46 for L=(0+2) (1994Il01) 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
J$(1+,2+,3-) from 1994Il01 and |p=- from 1970Mo10 
L,S$also 0.41 for L=(1), 0.27+0.62 for L=(0+2) (1994Il01) 


level_energy_unit: KEV
level_spin_parity: (1:5)-
level_comment:
E$weighted average of: 8365 {I10} (1970Mo10), 8365.3 {I30} (1994Il01) 
J$(1,2,3-,4-,5-) based on L=(1+3), or L=(3), or L=(0+2) (1994Il01); |p=- from L=1 or L=1+3 (1970Mo10) selects (1:5)- 
L,S$0R 1+3 (1970Mo10); other: 0.14+1.1 for L=(1+3), 1.5 for L=(3), 0.30+0.84 for L=(0+2) (1994Il01) 


level_energy_unit: KEV
level_spin_parity: (-)
level_comment:
E$weighted average of: 8448 {I10} (1970Mo10), 8448.7 {I30} (1994Il01) 
L,S$other: 0.24+0.43 for L=(1+3) (1994Il01; they also give L=(0+2) or (1) or (2) and (2J+1)C{+2}S=0.16+0.74 or 0.40 or 0.93 respectively) 


level_energy_unit: KEV
level_spin_parity: (+)
level_comment:
E$weighted average of: 8505 {I10} (1970Mo10), 8505.5 {I30} (1994Il01) 
L,S$others: 0.13 for L=(3), 0.017+0.10 for L=(0+2), 0.12 for L=(2), 0.050 for L=(1) (1994Il01) 


level_energy_unit: KEV
level_spin_parity: (-)
level_comment:
E$weighted average of: 8672 {I10} (1970Mo10), 8671.5 {I30} (1994Il01) 
L,S$others: 0.086 for L=(1), 0.19 for L=(2), 0.031+0.15 for L=(0+2), 0.12 for L=(0) (1994Il01) 


level_energy_unit: KEV
level_spin_parity: (1,2,3-,4-,5-)
level_comment:
E$energetically not resolved from transition to weak 9024 in (p,|g) reaction (1994Il01) 
L,S$for L=(3), 0.73+1.3 for L=(0+2) (1994Il01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$observed by 1984Um04, 1980Ya02, 1979Oe02, 1973Ma46, 1972Be29, 1971Gu07 
S$0.13 (1984Um04), 0.50 (1980Ya02), 0.40 (1979Oe02, relative mean value), 0.54 (1973Ma46, relative), 0.09 (1972Be29, relative) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$observed by 1984Um04, 1980Ya02, 1979Oe02, 1973Ma46, 1972Be29 
S$0.18 (1984Um04), 1.08 (1980Ya02), 1 (1979Oe02, relative mean value), 1.15 (1973Ma46, relative), 0.22 (1972Be29, relative) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
E$observed by 1984Um04, 1980Ya02, 1979Oe02, 1973Ma46 
S$0.37 (1984Um04), 1.15 (1980Ya02), 1.7 (1979Oe02, relative mean value), 1.90 (1973Ma46, relative) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$measured mean lifetime |t=490 fs {I50} (2017VaAA) from DSAM and Monte Carlo |g-ray line-shape simulations using several approaches. In the first analysis method, experimental |g-ray line shapes were compared to simulated line shapes generated within the Lindhard formalism with multiple nuclear scattering and stopping modeled under a Monte Carlo technique, and the mean lifetimes obtained were: 557 fs {I58} for minimum of reduced |h{+2} approach, and 532 fs {I58} using ratio R=R(stopped)/R(shifted) as a function of simulated lifetime. In the second analysis method, more comprehensive Monte Carlo GEANT4 simulations were used, where the two corresponding mean lifetimes were: 489 fs {I51} for minimum of reduced |h{+2} approach, and 484 fs {I50} from ratio R=R(stopped)/R(shifted) as a function of simulated lifetime. The latter method was considered by the authors as more robust, thus they adopted the average value of mean lifetime |t=490 fs {I50}, keeping a 2-significant-figure result. This value can be compared with |t=456 fs {I+18-29} in 2016Pr01 (At. Data and Nucl. Data Tables 107, 1) evaluation of model-independent methods. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$<2+ || E2 || 2+> = 0.163 {I42} (2021Or05) 
MOME2$ from measurement of Coulex yields combined with value of <2+ || E2 || 0+> = 0.1735 {I46} from 2016 b(E2) evaluation 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: D
level_comment:
$Nuclear rms charge radius: 3.3901 fm 28 (2004An14 evaluation); 3.3903 fm {i22} from 2008 update of 2004An14 
MOMM1$measured by: nuclear magnetic resonance and optical pumping with radiative detection (1988PiZY); optical spectroscopy (1965Ro13) 
MOME2$measured by collinear fast beam LASER spectroscopy: NMR with |b detection (1996Kl04) 
J$log| {Ift}=3.657 {I3} (1997Ha32, {+37}K |e decay); L=2 and VAP ({+36}Ar(d,p)) 
T$weighted average of following values (with uncertainties at 68% confidence level): 34.95 d {I4} (2001Re07), 35.02 d {I2} (1975Ki10), 35.06 d {I9} (1973Co26), 35.1 d {I1} (1965St09) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J$L=0 and VAP ({+36}Ar(d,p)) 
T$weighted average of: 0.45 ps {I24} ({+35}Cl({+3}He,p|g)), 0.75 ps {I+12-9} ({+34}S(|a,n|g)), and 476 fs {I106} ({+37}Cl(p,n|g)) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
MOMM1$measured by time dependent perturbed angular distribution (1971Ra22) 
J$|DJ=2, M2+E3 |g to 3/2+, g.s. ({+26}Mg({+14}N,p2n|g)..., {+34}S(|a,n|g), {+37}Cl(p,n|g)); L=3 and VAP ({+36}Ar(d,p)); 
T$weighted average of: 4.5 ns {I2} ({+37}Cl(p,n|g)), 4.34 ns {I11} ({+34}S(|a,n|g)) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$|DJ=2, E2 |g to 3/2+, g.s. ({+34}S(|a,n|g)); L=4 and VAP ({+36}Ar(d,p)) 
T$weighted average of: 387 fs {I60} ({+37}Cl(p,n|g)), 274 fs {I15} ({+34}S(|a,n|g)), 0.42 ps {I12} ({+35}Cl({+3}He,p|g)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=0, E1 |g to 3/2+, g.s.; L=1 and VAP ({+36}Ar(d,p)) 
T$weighted average of: 568 fs {I76} ({+37}Cl(p,n|g)), 0.82 ps {I29} ({+34}S(|a,n|g)), 0.28 ps {I9} ({+35}Cl({+3}He,p|g)) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L=2 and VAP ({+36}Ar(d,p)); |DJ=1, M1+E2 |g to 3/2+, g.s. ({+34}S(|a,n|g), with 1/2+ rejected by |h{+2}) 
T$weighted average of: 16 fs {I5} ({+37}Cl(p,n|g)), 10 fs {I8} ({+34}S(|a,n|g)) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$|DJ=1, M1+E2 |g to 3/2+, g.s. ({+34}S(|a,n|g), with 1/2+ rejected by |h{+2}) 
T$weighted average of: 61 fs {I8} ({+37}Cl(p,n|g)), 52 fs {I7} ({+34}S(|a,n|g); other: 21 fs {I10} ({+35}Cl({+3}He,p|g)) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=1, M1+E2 |g to 7/2-, 1611, and |DJ=1, E1 |g from 11/2+, 5214 ({+34}S(|a,n|g)) 
T$weighted average of: 206 fs {I26} ({+37}Cl(p,n|g)), 194 fs {I7} ({+34}S(|a,n|g)), 0.66 ps {I31} ({+35}Cl({+3}He,p|g)) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J$E1 |g to 3/2+, g.s. and M1+E2 |g to 7/2-, 1611 
T$weighted average of: 31 fs {I21} ({+35}Cl({+3}He,p|g)), 33 fs {I7} ({+37}Cl(p,n|g)), 24 fs {I2} ({+34}S(|a,n|g)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$L=1 and VAP ({+36}Ar(d,p)) 
T$mean value of 64 fs {I24} ({+37}Cl(p,n|g)) and 17 fs {I3} ({+34}S(|a,n|g)) with unc. Covering both values 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=1, E1 |g to 5/2+, 2796 and |DJ=0, M1+E2 |g to 7/2-, 1611 
T$weighted average of: 416 fs {I208} ({+37}Cl(p,n|g)), 409 fs {I55} ({+34}S(|a,n|g)) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$1/2+,3/2+,5/2+ from log| {Ift}=4.958 {I24} ({+37}K |e decay - this also rejects |p=- from L=1 in {+36}Ar(d,p)); 3/2+,5/2- based on |g(|q) and polarization measurements ({+34}S(|a,n|g)) 
T$weighted average of: 21 fs {I3} ({+34}S(|a,n|g)), 55 fs {I17} ({+37}Cl(p,n|g)), 35 fs {I10} ({+35}Cl({+3}He,p|g)) 


level_energy_unit: KEV
level_comment:
E$weighted average of: 4188 {I5} ({+35}Cl({+3}He,p)), 4209 {I9} ({+36}Ar(d,p)); other: 4215 {I16} ({+39}K(d,|a), tentative level) 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=1 or 0 E1(+M2) |g to 3/2+, g.s. ({+34}S(|a,n|g); 1/2 excluded by |g(|q)); 5/2 and |p=- also from L=3 in {+36}Ar(d,p) 
T$from {+34}S(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$weighted average of: 4750 {I16} ({+39}K(d,|a)), 4758 {I12} ({+36}Ar(d,p)) 
J$L=1 and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of: 4980 {I20} ({+38}Ar(p,d)), 4991 {I16} ({+39}K(d,|a)), 4993 {I6} ({+39}K(p,{+3}He)), 5005 {I10} ({+36}Ar(d,p)) 
J$L=0 in {+37}Cl(p,n); L(p,d)=2 with some preference for 3/2 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=1 |g's to 3/2+ g.s. and 7/2-, 1611 respectively ({+34}S(|a,n|g)) is not adopted here 
T$from {+34}S(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=1, E1 |g to 9/2-, 3185 and |DJ=2, Q |g to 7/2+, 2218 
T$weighted average of: 4.2 ps {I14} ({+26}Mg({+14}N,p2n|g)...), 2.50 ps {I21} ({+34}S(|a,n|g)) 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$weighted average of: 5221 {I16} ({+39}K(d,|a)), 5235 {I13} ({+36}Ar(d,p)) 
J$L=1 and shell model calculations ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$weighted average of: 5341 {I6} ({+35}Cl({+3}He,p)), 5354 {I16} ({+39}K(d,|a)), 5369 {I15} ({+36}Ar(d,p)), 5390 {I20} ({+38}Ar(p,d)) 
J$from L=1 and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$weighted average of: 5572 {I13} ({+36}Ar(d,p)), 5573 {I6} ({+35}Cl({+3}He,p)) 
J$from L=1 and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of: 5662 {I6} ({+35}Cl({+3}He,p)), 5670 {I20} ({+38}Ar(p,d)), 5692 {I10} ({+36}Ar(d,p)) 
J$from L=2 in {+38}Ar(p,d) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=1, E1 |g from 15/2+, 6473 ({+34}S(|a,n|g), 17/2- rejected based on the |h{+2} fit) 
T$from {+34}S(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
E$weighted average of: 5872 {I9} ({+36}Ar(d,p)), 5880 {I20} ({+38}Ar(p,d)) 
J$L=(1) and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E$weighted average of: 5955 {I6} ({+35}Cl({+3}He,p)), 5975 {I9} ({+36}Ar(d,p)) 
J$L=(3) and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of: 6100 {I10} ({+36}Ar(d,p)), 6112 {I20} ({+38}Ar(p,d)) 
J$L(p,d)=2; L=0 in {+37}Cl(p,n) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to 11/2+, 5213 ({+34}S(|a,n|g); 9/2+ rejected based on the |h{+2} fit) 
T$weighted average of: 3.2 ps {I4} ({+34}S(|a,n|g)), 2.8 ps {I7} ({+26}Mg({+14}N,p2n|g)...) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$weighted average of: 6309 {I10} ({+36}Ar(d,p)), 6320 {I10} ({+35}Cl(|a,d)) 
J$from L=3 and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 7/2:17/2+
level_comment:
E$weighted average of: 6416 {I10} ({+36}Ar(d,p)), 6430 {I10} ({+35}Cl(|a,d)) 
J$L=6 in {+35}Cl(|a,d) 


level_energy_unit: KEV
level_spin_parity: 7/2:13/2+
level_comment:
E$weighted average of: 6452 {I10} ({+36}Ar(d,p)), 6470 {I10} ({+35}Cl(|a,d)) 
J$L=4+6 in {+35}Cl(|a,d) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1(+E2) |g to 13/2+, 6150 ({+34}S(|a,n|g)), 11/2+ rejected based on the |h{+2} fit 
T$weighted average of: 4.4 ps {I4} ({+34}S(|a,n|g)), 5.8 ps {I5} ({+26}Mg({+14}N,p2n|g)...) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_comment:
E$weighted average of: 6650 {I20} ({+38}Ar(p,d)), 6670 {I20} ({+39}K(p,{+3}He)), 6680 {I10} ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 13/2+,17/2+
level_lifetime_unit: FS
level_comment:
J$|DJ=1, M1 |g to 15/2+, 6473 ({+34}S(|a,n|g)), both 13/2+ and 17/2+ are acceptable by the |h{+2} fit) 
T$weighted average of: 381 fs {I83} ({+34}S(|a,n|g)), 0.3 ps {I3} ({+26}Mg({+14}N,p2n|g)) 


level_energy_unit: KEV
level_spin_parity: 3/2:13/2+
level_comment:
E$weighted average of: 7880 {I20} ({+38}Ar(p,d)), 7890 {I10} ({+35}Cl(|a,d)) 
J$from L=4 in {+35}Cl(|a,d) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E$weighted average of: 8080 {I20} ({+38}Ar(p,d)), 8114 {I16} ({+36}Ar(d,p)) 
J$from L=(3) and VAP ({+36}Ar(d,p)) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J$from Adopted Levels, Gammas dataset 
T$From 1971Ra03. Mean lifetime |t in fs: 1750 {I50} (1974Ga12); 1080 +170-130 (1971Ra03) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
J$|DJ=2, M2+E3 |g to 3/2+, g.s. 
T$mean lifetime |t in ns: 6.08 {I28} (1974Ga12), 6.47 {I22} (1973Ve05), 6.02 {I29} (1971Ra05), 7.43 {I101} (1967Go09, from reported T{-1/2}=5.15 {I70} ns); weighted average: 6.27 {I16} 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$|DJ=2, E2 |g to 3/2+, g.s. 
T$mean lifetime |t in fs: 400 {I25} (1974Ga12), 380 {I50} (1971Ra03); weighted average: 396 {I22} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$1/2-,3/2- from L=1 in 1965Ro08 ({+36}Ar(d,p)); 3/2- from |DJ=0, E1(+M2) |g to 3/2+, g.s. 
T$mean lifetime |t in fs: 1620 {I100} (1974Ga12), 775 {I+105-89} (1971Ra03); weighted average: 1185 {I422} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$1/2+,5/2+ from |DJ=1, M1+E2 |g to 3/2+, g.s.; 1/2+ rejected by 1975No01 based on the |h{+2} fit 
T$mean lifetime |t in fs: 14 {I11} (1971Ra03); other: <15 (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$1/2+,5/2+ from |DJ=1, M1+E2 |g to 3/2+, g.s.; 1/2+ rejected by 1975No01 based on the |h{+2} fit 
T$mean lifetime |t in fs: 75 {I10} (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: (9/2)-
level_lifetime_unit: FS
level_comment:
J$5/2-,9/2- from |DJ=1, M1+E2 |g to 7/2-, 1611. {I5}/2- less likely from intense |g from 13/2-, 5793 
T$mean lifetime |t in fs: 280 {I10} (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J$1/2-,5/2- from |DJ=1, E1(+M2) |g to 3/2+, g.s.; 1/2- excluded by M1+E2 |g to 7/2-, 1611 
T$mean lifetime |t in fs: 35 {I3} (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$3/2-,7/2- from |DJ=1, E1(+M2) |g to 5/2+, 2796; 7/2- from |DJ=0, M1+E2 |g to 7/2-, 1611 
T$mean lifetime |t in fs: 590 {I80} (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2-
level_lifetime_unit: FS
level_comment:
J$3/2,5/2 based on |g(|q) and 3/2+,5/2- from polarization measurement (1974Ga12) 
T$mean lifetime |t in fs: 30 {I5} (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
J$3/2-,11/2- from |DJ=2, E2 |g to 7/2-, 1611; 3/2- excluded from |DJ=1, M1 |g to (9/2)-, 3185. {I7}/2- also tested and found inconsistent with pol(|g) by 1974Ga12 
T$mean lifetime |t in fs: 370 {I20} (1974Ga12) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=0 |g to 9/2-, 3185, and M1+E1 |g to 7/2-, 1611 
T$mean lifetime |t in fs: 40 {I15} (1975No01) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=0,1 E1(+M2) |g to 3/2+, g.s.; 1/2 excluded by |g(|q) (1975No01) 
T$mean lifetime |t in fs: <10 (1975No01) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$1/2,5/2 from |DJ=1 D+Q |g to 3/2+, g.s.; 1975No01 reject 1/2 based on |g(|q) and suggest 3/2,5/2+ which are not adopted here 
T$mean lifetime |t in fs: <20 (1975No01) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$1/2,5/2 from |DJ=1 D+Q |g to 3/2+, g.s.; 1/2 excluded by 1975No01 from |g(|q); they also consider J=3/2+ which is not adopted here 
T$mean lifetime |t in fs: <10 (1975No01) 


level_energy_unit: KEV
level_spin_parity: 7/2-,11/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=0,2 E2(+M3) |g to 7/2-, 1611; 1975No01 exclude 3/2- from |g(|q) 
T$mean lifetime |t in fs: 50 {I15} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|DJ=1 |g's to 3/2+ g.s. and 7/2-, 1611 respectively; |p=- in 1975No01 is not adopted here 
T$mean lifetime |t in fs: <30 (1975No01) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_comment:
J$1/2,5/2 from |DJ=1 |g to 3/2+, g.s.. 1975No01 adopts 3/2,5/2 (and |p=+, not adopted here). However 3/2 is not sustained by |g(|q). Adopted here is 5/2 
T$mean lifetime |t in fs: 25 {I10} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$7/2+,11/2+ from |DJ=1, E1 |g to 9/2-, 3185; 7/2 excluded from |DJ=2, Q |g to 7/2+, 2218 
T$mean lifetime |t in ps: 3.6 {I3} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: FS
level_comment:
J$13/2-,17/2- from |DJ=1, E1 |g from 15/2+, 6473; 17/2- rejected by 1975No01 based on the |h{+2} fit 
T$mean lifetime |t in fs: 50 {I15} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
J$9/2+,13/2+ from |DJ=1, M1+E2 |g to 11/2+, 5213; 9/2+ rejected by 1975No01 based on the |h{+2} fit 
T$mean lifetime |t in ps: 4.6 {I6} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J$11/2+,15/2+ from |DJ=1, M1(+E2) |g to 13/2+, 6150; 11/2+ rejected by 1975No01 based on the |h{+2} fit 
T$mean lifetime |t in ps: 6.3 {I6} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 13/2+,17/2+
level_lifetime_unit: FS
level_comment:
J$|DJ=1, M1 |g to 15/2+, 6473 (both 13/2+ and 17/2+ are acceptable by the |h{+2} fit) 
T$mean lifetime |t in fs: 550 {I120} (1975No01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 1409.82 {I10} (1972Lu02), 1409.0 {I6} (1971Ca40) 
T$mean lifetime |t in fs: 620 {I185} (1973Kr04), 1220 {I500} (1972Lu02), 940 {I+170-100} (1972Wo17), 370 {I+190-110} (1971Ca40). Weighted average: 687 {I153} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
E$weighted average of: 1611.26 {I10} (1972Lu02), 1610.7 {I10} (1971Ca40) 
T$from 1971Ra22 (which reported T{-1/2}); other measured mean lifetimes |t in ps: >10 (1972Lu02), >3 (1972Wo17) 
$|m=-1.33 {I5} (1971Ra22) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 2217.1 {I4} (1972Lu02), 2216.4 {I15} (1971Ca40) 
T$mean lifetime |t in fs: 540 {I145} (1973Kr04), 910 {I180} (1972Lu02), 510 {I70} (1972Wo17). Weighted average: 559 {I87} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of: 2490.0 {I4} (1972Lu02), 2489.0 {I10} (1971Ca40) 
T$mean lifetime |t in fs: 755 {I170} (1973Kr04), 1040 {I190} (1972Lu02), 660 {I+250-160} (1972Wo17), 88 {I24} (1971Ca40). Weighted average (excluding 88 {I24}): 820 {I110} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 2795.5 {I6} (1972Lu02), 2795.1 {I13} (1971Ca40) 
T$mean lifetime |t in fs: 23 {I8} (1973Kr04), 22 {I14} (1972Wo17). Weighted average: 23 {I7}. Others: <40 (1972Lu02), <8 (1971Ca40). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3169.7 {I8} (1972Lu02), 3171 {I3} (1971Ca40) 
T$mean lifetime |t in fs: 81 {I15} (1973Kr04), 100 {I20} (1972Lu02). Weighted average: 88 {I12} 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3184.9 {I10} (1972Lu02), 3184 {I3} (1971Ca40) 
T$mean lifetime |t in fs: 310 {I80} (1973Kr04), 300 {I60} (1972Lu02), 285 {I60} (1972Wo17). Weighted average: 296 {I37} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3271.6 {I10} (1972Lu02), 3272 {I3} (1971Ca40) 
T$mean lifetime |t in fs: 38 {I15} (1973Kr04), 60 {I20} (1972Lu02), 50 {I20} (1972Wo17). Weighted average: 47 {I10} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3515.9 {I10} (1972Lu02), 3519 {I6} (1971Ca40) 
T$mean lifetime |t in fs: 93 {I35} (1973Kr04), <50 (1972Lu02) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3525.7 {I20} (1972Lu02), 3535 {I6} (1971Ca40) 
T$mean lifetime |t in fs: >1120 (1973Kr04), 600 {I300} (1972Lu02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of: 3603.0 {I20} (1972Lu02), 3599 {I10} (1971Ca40) 
T$mean lifetime |t in fs: 82 {I25} (1973Kr04), <80 (1972Lu02) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of: 6.1 {I6} ps (1991Ja11); 6.2 {I14} ps (1976Me03, from |t 9 {I2}); 5.2 {I8} (1976Wa11, from |t 7.5 {I12}) 


level_energy_unit: KEV
level_comment:
E$3168 {I20} (1971Se04) 
S$1971ChZI suggest L=1 for 3171, unresolved from 3186 for which they suggest L=2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$3511 {I20} (1971Se04); 3528 {I10} (1966Ho03) 
S$0.33 (1971Me12); 0.45 (1971ChZI); 0.36 (1965Ro08) 


level_energy_unit: KEV
level_comment:
E$5441 {I20} (1971Se04; 5541 in table I is probably a typographic error since it is compared with 5460 and 5467 from other refs); 5467 {I10} (1966Ho03) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
E$6921 {I20} (1971Se04); 6952 {I10} (1966Ho03) 
S$0.065 if J|p=1/2- or 0.033 if J|p=3/2- (1971Me12) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E$7131 {I20} (1971Se04); 7162 {I15} (1966Ho03) 
L$1 (1971Se04); 3 (1971Me12) 
S$0.035 if J|p=5/2- or 0.018 if J|p=7/2- (1971Me12) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$7571 {I20} (1971Se04); 7571 {I15} (1966Ho03) 
S$0.095 if J|p=1/2- or 0.050 if J|p=3/2- (1971Me12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$ R(|q)=1.1 {I3} 
E$ weakly excited peak listed in text and shown in figure 5 of 2012Sh05. Ratio of counts=1.1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
L$ not L=0 since mean value of R(|q) is abnormally large, although, within uncertainty it overlaps value of 1 
$ R(|q)=4.1 {I53} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$no hyperfine structure observed in optical spectroscopy (1953Me73) 
$<r{+2}>{+1/2}=3.4028 fm {I19} (2013An02 evaluation) 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=2.8 {I5} for L=2 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)=1.0 {I2} for L=2 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$2167.60 {I6} from (p,|g):resonances 
J$L(t,p)=L(p,t)=2 from 0+; 2167.4|g E2 to 0+ 
$T{-1/2}: weighted average of 0.492 ps {I21} from ({+34}S,{+8}Be|g), 0.444 ps {I25} from ({+16}O,|ap|g), 0.45 ps {I2} from (|a,p|g), and 0.37 ps {I5} from (p,|a). 
MOMM1$transient magnetic field and DSA in {+12}C({+34}S,{+8}Be) reaction (2006Sp01). See also 2014StZZ compilation. 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=2.6 {I7} for L=2; (0.02) for L=0 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)=4.2 {I5} for L=2; 0.08 {I3} for L=0 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
E$3377.36 {I23} from (p,|g):resonances 
J$L(t,p)=L(p,t)=0 from 0+; E0 transition to 0+ 
$T{-1/2}: from recoil-distance method in (|a,p|g). Other: >0.35 ps in (p,|g):resonances 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=(0.5) for L=0 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)?<0.02 for L=0 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$3810.09 {I11} from (p,|g):resonances 
J$L(p,t)=3 and L(t,p)=3,4 from 0+; L({+3}He,d)=1+3 from 3/2+; 1642.7|g |DJ=1 E1(+M2) to 2+ 
$T{-1/2}: weighted average of 52 fs {I14} in (|a,p|g) and 74 fs {I28} in (p,|g) 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=0.18 {I5} for L=3; 0.01 {I1} for L=1 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)<0.06 for L=3; small for L=1 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$3936.61 {I18} from (p,|g):resonances 
J$L(t,p)=L(p,t)=2 from 0+; L({+3}He,d)=L(d,{+3}He)=0 from 3/2+ 
$T{-1/2}: weighted average of 47 fs {I6} in ({+34}S,{+8}Be|g), 32 fs {I13} in (|a,p|g), 33 fs {I10} in (p,|g) and 54 fs {I15} in (|a,|g):resonances 
MOMM1$transient magnetic field and DSA in {+12}C({+34}S,{+8}Be) reaction (2006Sp01). See also 2014StZZ compilation. 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=0.13 {I4} for L=2; 0.01 {I1} for L=0 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)=0.32 {I10} for L=2; 0.32 {I12} for L=0 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
E$4479.92 {I14} from (p,|g):resonances 
J$L({+3}He,d)=3 from 3/2+; J=4 from |g(|q) in (p,|g):resonances; 669.8|g |DJ=1 M1(+E2) to 3- 
$T{-1/2}: weighted average of 0.93 ps {I20} in ({+16}O,|ap|g) and 1.3 fs {I+8-3} in (|a,p|g). Other: >0.42 ps in (p,|g):resonances 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=0.04 {I1} for L=3 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)<0.06 for L=3 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$4565.5 {I2} from (p,|g):resonances 
J$1+,2+ from L(d,{+3}He)=L({+3}He,d)=0 from 3/2+ ; 1+ is ruled out by 755.3|g to 3- and RUL 
$T{-1/2}: weighted average of 35 fs {I3} in ({+34}S,{+8}Be|g), 51 fs {I14} in (|a,p|g) and 38 fs {I11} in (p,|g):resonances. Other: <62 fs in (|a,|g):resonances 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=(0.01) for L=2; 0.03 {I1} for L=0 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)=0.5 {I2} for L=2; 0.09 {I2} for L=0 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
E$4585.2 {I4} from (p,|g):resonances 
J$L(p,t)=5 from 0+; L({+3}He,d)=3 from 3/2+; 775.7|g E2 to 3- and 105.9|g M1(+E2) to 4- 
$T{-1/2}: weighted average of 136 ps {I7} in ({+16}O,2p|g), 130 ps {I4} in ({+14}N,n2p|g), 135 ps {I4} in ({+16}O,|ap|g), and 128 ps {I6} in (|a,p|g). Other: >0.35 ps in (p,|g):resonances 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=0.33 {I9} for L=3 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
E$4710.3 {I2} from (p,|g):resonances 
J$L(t,p)=L(p,t)=0 from 0+ 
$T{-1/2}: from (|a,p|g). Other: >0.42 ps in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$4876.87 {I14} from (p,|g):resonances 
J$2709.4|g E1+M2 |g to 2+ and 1066.8|g M1(+E2) |g to 3-; L(t,p)=3,4 from 0+; L({+3}He,d)=1+3 from 3/2+; J=3 from |g(|q) in (p,|g):resonances 
$T{-1/2}: weighted average of 53 fs {I14} in (|a,p|g) and 31 fs {I6} in (p,|g) 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=0.31 {I8} for L=3; 0.01 {I1} for L=1 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)<0.14 for L=3; small for L=1 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: FS
level_comment:
E$5084.3 {I5} from (p,|g):resonances 
J$1-,2-,3- from L({+3}He,d)=1+3 from 3/2+; J=2 is proposed in (|a,p|g) and (p,|g):resonances. But 1- and 3- are not completely ruled out 
$T{-1/2}: weighted average of 57 fs {I21} in (|a,p|g) and 35 fs {I10} in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$5157.3 {I2} from (p,|g):resonances 
J$L(t,p)=L(p,t)=2 from 0+; L(d,{+3}He)=L({+3}He,d)=0 from 3/2+ 
$T{-1/2}: weighted average of 28 fs {I13} in (|a,p|g) and 22 fs {I7} in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
E$5349.5 {I2} from (p,|g):resonances 
J$J=4 from p|g(|q) in (|a,p|g); 3182.2|g |DJ=2 E2 to 2+; 1539|g to 3- 
$T{-1/2}: weighted average of 0.14 ps {I4} in (|a,p|g) and 0.15 ps {I5} in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$5513.38 {I16} from (p,|g):resonances 
J$L(t,p)=3,4 from 0+; L({+3}He,d)=1+3 from 3/2+ 
$T{-1/2}: weighted average of 0.19 ps {I6} in (|a,p|g) and 0.19 ps {I7} in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: FS
level_comment:
E$5552.21 {I18} from (p,|g):resonances 
J$L({+3}He,d)=L(d,{+3}He)=0 from 3/2+ 
$T{-1/2}: from (p,|g):resonances. Other: <31 fs in (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$5594.6 {I6} from (p,|g):resonances 
J$L(t,p)=2 from 0+; 2217.6|g and 5594.2|g to 0+. L({+3}He,d)=1+3 from 3/2+ (suggesting 1-,2-,3-) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_comment:
E$5658.1 {I5} from (p,|g):resonances 
J$1072.8|g |DJ=0 M1(+E2) to 5-; L({+3}He,d)=3 from 3/2+ 
$T{-1/2}: weighted average of 64 fs {I28} in (|a,p|g) and 28 fs {I4} in (p,|g):resonances. Other: <0.7 ps in {+27}Al({+14}N,n2p|g) 
$Adopted (1977En02) proton stripping spectroscopic factor (S)=0.48 {I12} for L=3 
$Adopted (1977En02) proton pick-up spectroscopic factor (S)<0.24 for L=3 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$5733.9 {I5} from (p,|g):resonances 
J$1,2+ from 5733|g to 0+ and RUL; 2+ is ruled out by L({+3}He,d)=1 or 1+3 from 3/2+. But L(t,p)=2 for 5740 group (suggesting 2+) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$5824.9 {I2} from (p,|g):resonances 
J$L(t,p)=3,4 from 0+; L({+3}He,d)=1+3 from 3/2+; 3657|g to 2+ and 1345|g to 4-. 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: FS
level_comment:
E$5857.5 {I2} from (p,|g):resonances 
J$L({+3}He,d)=3 from 3/2+ gives 1- to 5-; 981|g to 3- and RUL require |DJ<2, since |DJ=2 would require an unreasonably large B(E2) or B(M2) value; 3690|g to 2+ disfavors 4-; J=2 is favored by 5547|g from the 10631,(2-) level with T=(2), possible IAS of {+38}Cl g.s., J|p=2-. But 3- is not completely ruled out 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: FS
level_comment:
E$6053.1 {I3} from (p,|g):resonances 
J$(3,4+) from 704|g to 4+, 1573|g to 4-, 1488|g and 2116|g to 2+; (4+) is favored by band structure 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$6210.0 {I10} from (p,|g):resonances 
J$1729|g(|q) in (p,|g):resonances gives J=4; L({+3}He,d)=3 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
E$6213.8 {I3} from (p,|g):resonances 
J$6213|g to 0+, 5517.0|g from (4+); primary 4959|g and 5054|g from 3- in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
E$6249.9 {I3} from (p,|g):resonances 
J$901|g to 4+ and 2873|g to 0+; primary 4952|g from 1- in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$6276.1 {I4} from (p,|g):resonances 
J$L(p,t)=4 from 0+; L(t,p)=3,4 from 3/2+; 2340|g and 4108|g to 2+, 927|g to 4+, 1796|g to 4- 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$6353.5 {I4} from (p,|g):resonances 
J$L({+3}He,d)=1+3 from 3/2+ gives 1-,2-,3-; 6353|g to 0+ and RUL rules out 2- and 3- 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$J=6 from |g(|q) in ({+16}O,2p|g) and ({+14}N,n2p|g); 1822|g |DJ=1 E1(+M2) to 5- 
$T{-1/2}: from {+24}Mg({+16}O,2p|g). Other: <1.4 ps from {+27}Al({+14}N,n2p|g) 


level_energy_unit: KEV
level_spin_parity: (1-,2,3-)
level_lifetime_unit: FS
level_comment:
E$6485.4 {I7} from (p,|g):resonances 
J$4318|g to 2+, 2675|g to 3-, 4829|g from 1-. L({+3}He,d)=1 for 6486 {I10} group gives (0,1,2,3)- for any of the three levels near this energy 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$6574.3 {I5} from (p,|g):resonances 
J$L({+3}He,d)=1 or 1+3 from 3/2+; 6574|g to 0+ and RUL. But L(t,p)=3,4 is inconsistent with 1- 


level_energy_unit: KEV
level_spin_parity: (1-,2,3-)
level_lifetime_unit: FS
level_comment:
E$6621.6 {I4} from (p,|g):resonances 
J$2056|g to 2+, 2811|g to 3-, 4930.7|g from (1)-. L({+3}He,d)=(2) from 3/2+ suggests |p=+ 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$6772.7 {I5} from (p,|g):resonances 
J$6772|g to 0+ gives (1,2+); L({+3}He,d)=1 from 3/2+ and RUL rules out 1+ and 2+ 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_lifetime_unit: FS
level_comment:
E$6824.0 {I15} from (p,|g):resonances 
E$unresolved doublet at 6824 keV in (p,|g):resonances 
J$4656|g to 2+, 3014|g to 3-, 4728.3|g from (1)-, 4906.9|g from (4+); L({+3}He,d)=1 suggests (0 to 3)- for 6824.0 and/or 6824.1 


level_energy_unit: KEV
level_spin_parity: (0+:4+)
level_comment:
E$6824.1 {I15} from (p,|g):resonances 
E$unresolved doublet at 6824 keV in (p,|g):resonances 
J$2888|g to 2+. L(t,p)=2 for a 6838 {I15} group suggests 2+ for any of the levels from 6824 to 6852 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
E$weighted average of 7047 {I2} from (|a,p|g) and 7045 {I2} from (p,|g):resonances. 
J$4878|g to 2+, 2566|g to 4-; primary |g 4256 from 5- in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (6)-
level_lifetime_unit: FS
level_comment:
J$2483.9|g M1+E2 to 5- and 437.8|g from 7- favors J|p(7070)=6-. Assignment of J|p=5- from |g(|q) and RUL in (|a,p|g) is inconsistent with J|p=6- from |g(DCO) in ({+28}Si,|a2p|g). It should be noted that 2483.9|g(DCO) in ({+28}Si,|a2p|g) are also marginally consistent with |DJ=0 giving 5- as in (|a,p|g) and also with |DJ=2 giving 7-, the latter ruled out by 2590|g to 4- and RUL. In the opinion of the evaluator, the spin of this level needs reinvestigation. Here the evaluator have adopted J|p=(6)-, but J|p=5- can not be ruled out. 
$T{-1/2}: from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (1-:4+)
level_lifetime_unit: FS
level_comment:
E$7100.8 {I5} from (p,|g):resonances 
J$4933|g to 2+, 4072|g from 3-. L(d,{+3}He)=2 gives 0+,1+,2+,3+ for 7100.8 and/or 7128 


level_energy_unit: KEV
level_spin_parity: (1-:4+)
level_comment:
E$weighted average of 7235 {I2} from (|a,p|g) and 7233.0 {I17} from (p,|g):resonances. 
J$5066|g to 2+, 4189.9|g from (3-) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$weighted average of 7234 {I2} from (|a,p|g) and 7238 {I2} from (p,|g):resonances. 
J$7235|g to 0+; L(t,p)=2 from 0+ for a level at 7249 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: FS
level_comment:
J$1939.4|g |DJ=2 E2 to 4+; 879.9|g to 6+ and 2704|g to 5- 
$T{-1/2}: weighted average of 53 fs {I20} in (|a,p|g) and 21 fs {I10} in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (1-:4+)
level_comment:
E$weighted average of 7335 {I1} from (|a,p|g), 7336 {I15} from (t,p), and 7329 {I2} from (p,|g):resonances. 
J$3524|g to 3- and 5166|g to 2+ 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E$7370 {I2} from (|a,p|g) and (p,|g):resonances 
J$7369|g to 0+; M1 excitation in (e,e') for a level at 7381 


level_energy_unit: KEV
level_spin_parity: (2-,3,4+)
level_lifetime_unit: FS
level_comment:
E$7431.0 {I3} from (p,|g):resonances 
J$5263|g to 2+; primary 3742|g and 4375|g from 3- and weak 4497|g from 4- 


level_energy_unit: KEV
level_spin_parity: (1-:4+)
level_comment:
E$weighted average of 7452 {I2} from (|a,p|g) and 7451 {I2} from (p,|g):resonances. 
J$2575|g to 3- and 5284|g to 2+ 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GE
level_comment:
J$2922.6|g |DJ=2 E2 |g to 5-; 1100|g to 6+ 
$T{-1/2}: from (|a,p|g); <1.4 ps in {+27}Al({+14}N,n2p|g) 


level_energy_unit: KEV
level_spin_parity: (3,4,5)
level_lifetime_unit: FS
level_comment:
E$weighted average of 7539 {I2} from (|a,p|g), 7544 {I15} from (t,p), and 7538 {I2} from (p,|g):resonances. 
J$1486|g to (4+) and 3059|g to 4- 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_lifetime_unit: FS
level_comment:
E$weighted average of 7684 {I2} from (|a,p|g) and 7681 {I2} from (p,|g):resonances. 
J$3203|g to 4- and 5515|g to 2+; L(t,p)=(3,4) from 0+ for a level at 7700 


level_energy_unit: KEV
level_spin_parity: (1-,2,3-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$from (|a,p|g) and (p,|g):resonances 
J$5824|g to 2+; primary 2405|g and 3210|g from 1-, 3358|g from 3- in (p,|g):resonances 
$T{-1/2}: from (|a,|g):resonances (1981BuZY) 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
J$(5,7) is assigned in (|a,p|g) based on an assignment of J|p(7070)=5- 1421|g(|q) to 7070 level which is consistent with |DJ=0 or 2 and 1421|g(DCO) in ({+28}Si,|a2p|g) is consistent |DJ=1, but for large D+Q admixture, it can also be consistent with |DJ=0. The evaluator has adopted |DJ=0 for 1421|g to 7070 level and assigned J|p(8491)=(6-) based on J|p(7070)=(6)- not 5- (see comment there). 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$2161.0|g |DJ=2 E2 to 6+, 1061.4|g to 7- 
J$Note that 493|g |DJ=1 is already used as an argument for J|p(8077) 
$T{-1/2}: from {+24}Mg({+16}O,2p|g) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$4386.2|g |DJ=2 E2 to 5-, 2564.4|g E1+M2 to 6+ 
$T{-1/2}: <28 fs from DSAM for 4386|g in {+35}Cl(|a,p|g) (1976Gl10). Other: 4.2 ps {I14} for 2564|g in {+27}Al({+16}O,|ap|g) (1976Ko10) is discrepant, where the 2564|g was placed from 10174 level. Reversed ordering (proposed by 1976Gl10) of the 1201-2564 cascade defined a level at 8973 instead of 7610. 


level_energy_unit: KEV
level_spin_parity: 8(+)
level_comment:
J$2046|g is already used as argument for J(7491) 
J$967.4|g |DJ=0 d to 8+, 2248|g and 3128|g to 6+; band member 


level_energy_unit: KEV
level_spin_parity: 9-
level_lifetime_unit: PS
level_comment:
J$1201.32|g |DJ=2 E2 to 7-, 1604.67|g |DJ=1 E1+M2 |g to 8+ 
J$835.3|g is already used as argument for J(9339) 
$T{-1/2}: weighted average of 4.6 ps {I14} from ({+14}N,n2p|g) and 2.6 ps {I4} from ({+16}O,2p|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$10183|g D to 0+, |p=natural for resonant states in (|a,|g):resonances 
$T{-1/2}: DSAM in (|a,|g):resonances (1981BuZY) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$10393 {I5} from (|a,|g):resonances 
J$10400|g D to 0+, |p=natural for resonant states in (|a,|g):resonances 
$T{-1/2}: DSAM in (|a,|g) (1981BuZY) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$10429|g D to 0+, |p=natural for resonant states in (|a,|g):resonances 
$T{-1/2}: DSAM in (|a,|g) (1981BuZY) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$10585|g D to 0+, |p=natural in (|a,|g):resonances 
$T{-1/2}: DSAM in (|a,|g):resonances (1981BuZY) 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
J$11011|g D to 0+, |p=natural in (|a,|g):resonances. This level could correspond to 11000.2, 11005.9 and 11014.6 levels in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J$11030|g D to 0+, |p=natural in (|a,|g):resonances. This level could correspond to 11023.2 in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$8877|g D+Q to 2+; |g(|q) in (|a,|g):resonances gives 3- for unresolved 11044.2 and 11045.2 levels 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g(|q,pol) in (p,|g):resonances; 5643|g M1+E2 to 5-; probable IAS of 671, 5- in {+38}Cl from ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$from |g(|q,pol) in (p,|g):resonances; 5648|g M1+E2 to 5-; probable IAS of 671, 5- in {+38}Cl from ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$9182|g E1(+M2) to 2+, 7540|g and 6473|g M1+E2 to 3-, 5074|g and 6001|g to 4+, 4749|g and 5141|g to 4-; |p=natural from {+37}Cl(p,|a):res; possible IAS of 755, 3- in {+38}Cl from ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$possible doublet 
J$from |a(|q) in (p,|g):resonances; possible IAS of 755, 3- in {+38}Cl from ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$from |a(|q) in (p,|g):resonances; possible IAS of 755, 3- in {+38}Cl from ({+3}He,d) 
$ Possible T=2 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$(1-,3-) from |a(|q) in (p,|g):resonances; 5884|g to 2+ and 5820|g to 5- 
$|g transitions from either of the two levels: 11478.4 and/or 11478.9 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$(0+,1-,2+) from |a(|q) in (p,|g):resonances; 8175|g and 11551|g to 0+, 5727|g and 6675|g to 3-; L(p,p)=1 in (p,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$from |a(|q) in (p,|g):resonances; 9429|g to 2+ and 5939|g to 5-; |p=natural from {+37}Cl(p,|a):res 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$probable doublet from (p,|g):resonances (1974Al05) 
J$(4+,5-) from |a(|q) in (p,|g):resonances; 6136|g and 7165|g to 2+, 6072|g and 7145|g to 5- 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 11840.3 {I8} from (p,|g):resonances and 11840.0 {I3} from (n,n),(n,|a):resonances. 
J$from |a(|q) in (p,|g):resonances; also from {+37}Ar(n,n),(n,|a):resonances with L(n)=0 from 3/2+ 
$|G from {+37}Ar(n,n),(n,|a): resonances 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 11841.3 {I8} from (p,|g):resonances and 11841.0 {I3} from (n,n),(n,|a):resonances. 
$|G and J from {+37}Ar(n,n),(n,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$5326|g M1(+E2) and 5718|g M1(+E2) to 4-, 6414|g D(+Q) to 3-, 7341|g D+Q to 5-; possible IAS of 1309, 4- in {+38}Cl from ({+3}He,d) 
$ possible T=2 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.9 eV {I6} 
$E(|a)=2670 {I5} 
J$ 1 from |g(|q) in 1964Er04 
S$weighted average of 2669 {I5} (1979Si10) and 2670 {I5} (1964Er04) 
T$1.71 eV {I34} (1979Si10), 4.0 eV {I12} (1964Er04) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.4 eV {I3} 
$E(|a)=2773 {I5} 
J$ 1 from |g(|q) in 1979Si10 and 1964Er04 
S$weighted average of 2774 {I5} (1979Si10), and 2772 {I5} (1964Er04) 
T$1.3 eV {I3} (1979Si10), 1.5 eV {I5} (1964Er04) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.30 eV {I15} 
$E(|a)=2894 {I5} 
J$ 3 from |g(|q) in 1979Si10 
S$2894 {I5} (1979Si10) 
T$0.30 eV {I15} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.3 eV {I1} 
$E(|a)=2910 {I5} 
J$ 1 from |g(|q) in 1979Si10 and 1964Er04 
S$weighted average of 2909 {I5} (1979Si10), and 2911 {I5} (1964Er04) 
T$0.30 eV {I15} (1979Si10), 0.3 eV {I1} (1964Er04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.6 eV {I3} 
$E(|a)=3002 {I5} 
J$ 2 from |g(|q) in 1979Si10 
S$3002 {I5} (1979Si10) 
T$0.6 eV {I3} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.9 eV {I6} 
$E(|a)=3024 {I5} 
E$level energy listed at 9926 by 1981BuZY from E|g's is too high by >10 keV from that derived from averaged E|a(lab)=3024 
J$ 1 from |g(|q) in 1979Si10 and 1964Er04 
S$weighted average of 3022 {I5} (1979Si10), 3025 {I5} (1964Er04), and 3030 {I10} (1964Ph02) 
T$2.62 eV {I56} (1979Si10), 4.5 eV {I15} (1964Er04) 
$T{-1/2}=12 fs {I10} (DSAM for 9926|g,1981BuZY) from 9926|g 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.2 eV {I1} 
$E(|a)=3066 {I5} 
J$ 2 from |g(|q) in 1979Si10 
S$3066 {I5} (1979Si10) 
T$0.2 eV {I1} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.9 eV {I5} 
$E(|a)=3116 {I5} 
J$ 1 from |g(|q) in 1979Si10 and 1964Er04 
S$weighted average of 3109 {I10} (1979Si10), 3116 {I5} (1964Er04), and 3120 {I10} (1964Ph02) 
T$1.7 eV {I4} (1979Si10), 3.0 eV {I10} (1964Er04) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.3 eV {I8} 
$E(|a)=3159 {I5} 
J$ 1 from |g(|q) in 1964Er04 
S$weighted average of 3155 {I5} (1979Si10), 3161 {I5} (1964Er04), and 3170 {I10} (1964Ph02) 
T$2.0 eV {I5} (1979Si10), 4.5 eV {I15} (1964Er04) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.04 eV {I2} 
$E(|a)=3173 {I5} 
S$3173 {I5} (1979Si10) 
T$0.04 eV {I2} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.6 eV {I3} 
$E(|a)=3196 {I5} 
J$ 3 from |g(|q) in 1979Si10 
S$3196 {I5} (1979Si10) 
T$0.6 eV {I3} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.30 eV {I15} 
$E(|a)=3284 {I10} 
J$ 2 from |g(|q) in 1979Si10. Other: -1 for a resonance at E(|a)=3290 {I10} (1964Ph02) 
S$3284 {I10} (1979Si10). 3290 {I10} with J|p=1- (1964Ph02) 
T$0.30 eV {I15} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.4 eV {I6} 
$E(|a)=3311 {I5} 
J$ 2 or 3 from |g(|q) in 1979Si10, 2 ruled out by RUL 
$3311 {I5} (1979Si10) 
$2.4 eV {I6} (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=5.2 eV {I12} 
$E(|a)=3327 {I5} 
E$level energy listed at 10210 by 1981BuZY from E|g's is too high by >20 keV from that derived from averaged E|a(lab)=3327 
J$ 1 from |g(|q) (1979Si10,1971Cl09) 
S$weighted average of 3323 {I10} (1979Si10), 3324 {I5} (1971Cl09), and 3340 {I10} (1964Ph02) 
T$4.9 eV {I12} (1979Si10), 8 eV {I4} (1971Cl09) 
$T{-1/2}=19 ps {I10} (DSAM for 8027|g and 10210|g,1981BuZY) 
$E|g=5625 {I3}, 5720 {I3}, 6273 {I8} (1981BuZY) shown in the level scheme by 1981BuZY do not fit, thus omitted here, values are too high by about 20 keV. A 10031|g is also reported by 1981BuZY for this resonance 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.04 eV {I2} 
$E(|a)=3364 {I5} 
$3364 {I10} (1979Si10) 
$0.04 eV {I2} (1979Si10) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.04 eV {ILT} 
$E(|a)=3395 {I10} 
$3394 {I10} (1979Si10) 
$<0.04 eV (1979Si10) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.6 eV {I6} 
$E(|a)=3406 {I5} 
J$ 1 from |g(|q) (1979Si10,1971Cl09) 
S$weighted average of 3401 {I10} (1979Si10), 3408 {I5} (1971Cl09), and 3400 {I10} (1964Ph02) 
T$2.6 eV {I6} (1979Si10), 2.7 eV {I14} (1971Cl09) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.7 eV {I4} 
$E(|a)=3496 {I5} 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 3491 {I10} (1979Si10), 3498 {I5} (1971Cl09), and 3490 {I10} (1964Ph02) 
T$1.6 eV {I4} (1979Si10), 2.1 eV {I11} (1971Cl09) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.004 eV {I2} 
$E(|a)=3548 {I5} 
$3548 {I5} (1996Fu07) 
$0.004 eV {I2} (1996Fu07) 
S$other: 3550 {I10} (1964Ph02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=3.0 eV {I10} 
$E(|a)=3563 {I5} 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 3563 {I5} (1971Cl09) and 3563 {I5} (1996Fu07). Other: 3550 {I10} (1964Ph02) 
T$6 eV {I3} (1971Cl09), 2.8 eV {I9} (1996Fu07) 
$T{-1/2}=12 fs {I11} (DSAM for 7017|g and 10400|g,1981BuZY) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=10 eV {I4} 
$E(|a)=3603 {I5} 
E$level energy listed at 10446 by 1981BuZY from E|g's which is too high by |?15 keV from that derived from E|a(lab). All E|g's from 1981BuZY are correspondingly higher by |?15 keV, thus not adopted here 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 3603 {I5} (1971Cl09), 3603 {I5} (1996Fu07), and 3600 {I10} (1964Ph02), 
T$14 eV {I7} (1971Cl09), 8 eV {I4} (1996Fu07) 
$T{-1/2}=26 ps {I12} (DSAM for 10446|g,1981BuZY) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.05 eV {I3} 
$E(|a)=3673 {I5} 
J$ 1 from |g(|q) (1996Fu07) 
$3673 {I5} (1996Fu07) 
$0.05 eV {I3} (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.02 eV {I1} 
$E(|a)=3688 {I5} 
$3688 {I5} (1996Fu07) 
$0.02 eV {I1} (1996Fu07) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.06 eV {I3} 
$E(|a)=3698 {I5} 
$3698 {I5} (1996Fu07) 
$0.06 eV {I3} (1996Fu07) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.25 eV {I8} 
$E(|a)=3732 {I5} 
$3732 {I5} (1996Fu07) 
$0.25 eV {I8} (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=3.3 eV {I9} 
$E(|a)=3777 {I5} 
J$ 1 from |g(|q) (1971Cl09,1972Ch25) 
S$weighted average of 3778 {I5} (1971Cl09), 3773 {I10} (1972Ch25), 3777 {I5} (1996Fu07) and 3776 {I5} (1981BuZY) 
T$6 eV {I3} (1971Cl09), 4.5 eV {I15} (1972Ch25), 2.6 eV {I9} (1996Fu07) 
$T{-1/2}=18 fs {I11} (DSAM for 8415|g and 10590|g,1981BuZY) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.3 eV {I5} 
$E(|a)=3804 {I5} 
$3804 {I5} (1996Fu07) 
$1.3 eV {I5} (1996Fu07) 
E$triplet (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: (1-,2+,3-,4+)
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.5 eV {I5} 
$E(|a)=3866 {I5} 
J$from 1996Fu07 
$3866 {I5} (1996Fu07) 
$1.5 eV {I5} (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.7 eV {I2} 
$E(|a)=3886 {I5} 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 3889 {I5} (1971Cl09), 3876 {I10} (1972Ch25), and 3886 {I5} (1996Fu07) 
T$0.9 eV {I5} (1971Cl09), 0.8 eV {I5} (1972Ch25), 0.7 eV {I2} (1996Fu07) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.3 eV {I4} 
$E(|a)=3932 {I5} 
$3932 {I5} (1996Fu07) 
$1.3 eV {I4} (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.1 eV {I7} 
$E(|a)=3980 {I5} 
$3980 {I5} (1996Fu07) 
$2.1 eV {I7} (1996Fu07) 
J$from |g(|q) (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.7 eV {I6} 
$E(|a)=4019 {I5} 
J$from Adopted Levels. (1,2)+ from 1996Fu07 
$4019 {I5} (1996Fu07) 
$1.7 eV {I6} (1996Fu07) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.9 eV {I6} 
$E(|a)=4079 {I5} 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 4082 {I5} (1971Cl09), and 4068 {I10} (1972Ch25) 
T$2.0 eV {I10} (1971Cl09), 1.8 {I6} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=6.8 eV {I23} 
$E(|a)=4164 {I10} 
$4164 {I10} (1972Ch25) 
$6.8 eV {I23} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=4.3 eV {I27} 
$E(|a)=4253 {I7} 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 4256 {I5} (1971Cl09), and 4239 {I10} (1972Ch25) 
T$3.0 eV {I15} (1971Cl09), 9.6 eV {I30} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=6.0 eV {I23} 
$E(|a)=4275 {I6} 
J$ 1 from |g(|q) (1971Cl09) 
S$weighted average of 4278 {I5} (1971Cl09), and 4264 {I10} (1972Ch25) 
T$4.5 eV {I23} (1971Cl09), 8.6 eV {I30} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=4.1 eV {I14} 
$E(|a)=4289 {I10} 
$4289 {I10} (1972Ch25) 
$4.1 eV {I14} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=7.3 eV {I25} 
$E(|a)=4314 {I10} 
$4314 {I10} (1972Ch25) 
$7.3 eV {I25} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.1 eV {I7} 
$E(|a)=4374 {I10} 
$4374 {I10} (1972Ch25) 
$2.1 eV {I7} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=6.8 eV {I23} 
$E(|a)=4434 {I10} 
J$ 1 from |g(|q) (1972Ch25) 
$4434 {I10} (1972Ch25) 
$6.8 eV {I23} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.6 eV {I6} 
$E(|a)=4518 {I10} 
$4518 {I10} (1972Ch25) 
$1.6 eV {I6} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=5.8 eV {I20} 
$E(|a)=4540 {I10} 
J$ 3 from |g(|q) (1972Ch25) 
$4540 {I10} (1972Ch25) 
$5.8 eV {I20} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=16 eV {I5} 
$E(|a)=4591 {I10} 
$4591 {I10} (1972Ch25) 
$16 eV {I5} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=2.0 eV {I12} 
$E(|a)=4633 {I10} 
$4633 {I10} (1972Ch25) 
$2.0 eV {I12} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=1.1 eV {I5} 
$E(|a)=4657 {I10} 
$4657 {I10} (1972Ch25) 
$1.1 eV {I5} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=5.0 eV {I17} 
$E(|a)=4685 {I10} 
$4685 {I10} (1972Ch25) 
$5.0 eV {I17} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=10 eV {I3} 
$E(|a)=4721 {I10} 
$4721 {I10} (1972Ch25) 
$10 eV {I3} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=10 eV {I3} 
$E(|a)=4733 {I10} 
$4733 {I10} (1972Ch25) 
$10 eV {I3} (1972Ch25) 


level_energy_unit: KEV
level_spin_parity: (4+,5-)
level_comment:
J$the angular correlation function is best fitted in forward angles with L=4, but L=5 cannot be excluded due to the rising pattern in the function at backward angles (2005Fu03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W (at 20|')=150 |mb/sr (1972St27) 
$24% L=0, 20% L=2 and 56% L=4 (1972St27). Proton(|q): A{-1}=+0.137, A{-2}=+0.171, A{-3}=-0.076, A{-4}=-0.085 (1972St27) 


level_energy_unit: KEV
level_comment:
E$this peak is wider by |? 4 keV in the spectrum figure of 1971EnZU, thus most likely it is a doublet. 
J$ both components are possible IAS of 671, 5- state in {+38}Cl 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$other: 2160 {I30} (1983Bh03) 
L$1970Gr02 and 1968Wi14 suggest a small L=0 component with C{+2}S=0.015 {I15} 
S$others: 2.50 (1970Gr02), 2.50 (1968Wi14) 


level_energy_unit: KEV
level_comment:
E$weighted average of 7070 {I30} (1983Bh03) and 7140 {I20} (1970Gr02). It could be a doublet of 7101 and 7128 levels in Adopted Levels 
S$assumed L+1/2 transfer. Others: 0.40 (1970Gr02), 0.44 (1968Wi14) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(0|')=0.28 
S$1984Mi04 give 0.26 mb {I5} for the integrated cross section between 0|' and 50|'. 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
E$the 1201-2564 cascade is reversed in 1976Va24, resulting in a level at 7609 instead which is removed by 1979Aa01. 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
T$4.2 ps {I14} for 2564|g (1976Ko10), but <28 fs (1976Gl10) from DSAM for 4386|g in {+35}Cl(|a,p|g). The latter value is listed in Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from DSAM (2017Da13). Uncertainty from stopping powers, estimated by the authors as |?5%, is added in quadrature to the original value of 444 fs {I10} in 2017Da13. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: PS
level_comment:
E,T$the halflife quoted here is for a 7609 level in 1991Ja11 which is taken from 1976Ko10 in {+27}Al({+14}N,n2p|g) based on their placement of 1201|g. This level is now obsolete since the 1201|g is re-placed from the 10174 level in later studies. So the halflife (presumably 1201|g) is for the 10174 level 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$others: 2163 {I3} (1969Gr03), 2163 {I2} (1968Li04) 
T$weighted average of 0.47 ps {I2} (1976Fo12), 0.53 ps {I17} (1971Ja15) (supersede 0.65 ps {I19} not corrected for delayed feedings in 1971Ja10), 0.33 ps {+11-8} (1970Cu02), 0.31 ps {I8} (1969Gr03), 0.45 ps {I6} (1968Li04), 0.37 ps {I5} (1969En04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$weighted average of 23.9 ps {I11} (1984Bh03), 24 ps {I4} (1972Ba15), and 19 ps {I2} (1972Ke03). Others: >2 ps (1971Ja10), 25 ps {I+8-12} (1970Cu02), 7 ps {I4} (1969En04), 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$other: 3808 {I3} (1968Li04) 
T$weighted average of 76 fs {I42} (1971Ja10), 52 fs {I21} (1969En04), 49 fs {I14} (1968Li04) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
E$other: 4477 {I3} (1968Li04) 
T$weighted average of 1.1 ps {I+8-3} (1972Ba15) and 1.9 ps {I+14-7} (1971Ja10). Others: |<1.04 ps {I23} (1969En04), >0.7 ps (1968Li04) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
T$weighted average of 131 ps {I25} (1973Gr19), 136 ps {I7} (1972Ba15), 157 ps {I15} (1972Li15,RDM), 162 ps {I28} (1972Li15,DSAM), 126 ps {I9} (1970En04) and 119 ps {I6} (1972Ke03). Other: |<243 ps (1968Li04,delayed-coincidence) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$other: 4890 {I3} (1968Li04) 
J$J=(2,3) from p|g(|q) in 1967Ro16 
T$other: 0.10 ps {I6} (1968Li04) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$J=4 from p|g(|q) in 1974Be68. 1967Ro16 give J=(1,2) based on p|g(|q) correlations of 1413|g, 3182|g and 3937|g, but 1974Be68 state that the first two correlations in 1967Ro16 were actually in excellent agreement of J(5350)=4 while the last one did not agree. 1974Be68 also mention that the last correlation was remeasured by G. Schmid at the same laboratory (Freiburg) in 1973 and agreement with J=4 was established but with J=2,3 not excluded. 1971Ja10 also claim that the assignment of J=(1,2) by 1967Ro16 was probably incorrect. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_comment:
J$from 2485|g |DJ=0 M1+E2 |g to 5- based on p|g(|q) in 1976Gl10. However, (6)- is assigned in Adopted Levels based on |g(|q)(DCO) value in {+28}Si(|a,2p|g) and a 437.8|g from 7- which favors |DJ<2. In the opinion of the evaluator, the spin of this level needs reinvestigation. Also see comments for this level in {+28}Si(|a,2p|g) and Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (5,7)
level_comment:
J$from |DJ=0 or 2 1418|g to J|p(7070)=5-, based on p|g(|q) in 1976Gl10. However, J|p(8488)=(6-) and J|p(7070)=(6)- is assigned in Adopted Levels based on |g|g(|q)(DCO) value in {+28}Si(|a,2p|g). See detailed comment there. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
E$1980Ke01 place 2954|g from a level at 10024 and 1900|g from a level at 10029. In Adopted Levels, the two levels in 1980Ke01 are considered as the same level, based on results in ({+28}Si,|a2p|g) (2002Ru01). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$weighted average of 3810.12 {I11} (1974Al05) and 3810.0 {I2} (1968En01) 
J$from |g(|q,pol) in 1966Er07 
$T{-1/2}: weighted average of 76 fs {I59} (1968En01) and 73 fs {I28} (1984La24) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 3936.65 {I18} (1974Al05) and 3936.3 {I5} (1968En01) 
$T{-1/2}: weighted average of 73 fs {I21} (1968En01) and 31 fs {I5} (1984La24) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$weighted average of 4479.98 {I13} (1974Al05) and 4479.6 {I3} (1968En01) 
J$from |g(|q,pol) in 1966Er07 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 4565.4 {I2} (1974Al05) and 4565.9 {I5} (1968En01) 
$T{-1/2}: weighted average of 33 fs {I11} (1968En01) and 47 fs {I14} (1984La24) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$weighted average of 4585.3 {I4} (1974Al05) and 4585.0 {I5} (1968En01) 
J$from |g(|q,pol) in 1966Er07 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$weighted average of 4876.84 {I14} (1974Al05) and 4877.0 {I3} (1968En01) 
J$from |g(|q,pol) in 1968En01 
$T{-1/2}: weighted average of 32 fs {I6} (1984La24), 31 fs {I11} (1974Al06) and 27 fs {I11} (1968En01) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$weighted average of 5513.43 {I16} (1974Al05) and 5512.9 {I5} (1968En01) 
J$from Adopted Levels. J=3 from |g(|q) in 1968En01 
$T{-1/2}: weighted average of 0.18 ps {I7} (1984La24) and 0.22 ps {I11} (1974Al06). Other: >0.21 ps from 1968En01 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 5594.7 {I3} (1974Al05) and 5591 {I2} (1968En01) 
$T{-1/2}: weighted average of 49 fs {I18} (1984La24) and 76 fs {I21} (1974Al06) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_comment:
E$weighted average of 5658.3 {I5} (1974Al05) and 5657.7 {I6} (1968En01) 
J$from |g(|q,pol) in 1966Er07 
$T{-1/2}: weighted average of 27 fs {I4} (1984La24), 28 fs {I8} (1974Al06) and 44 fs {I15} (1968En01) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$weighted average of 5824.9 {I2} (1974Al05) and 5825.3 {I20} (1968En01) 
$T{-1/2}: from 1974Al06. Other: >125 fs (1984La24) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_lifetime_unit: FS
level_comment:
E$weighted average of 5857.5 {I2} (1974Al05) and 5853 {I3} (1968En01) 
$T{-1/2}: other: <11 fs (1974Al06) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$unweighted average of 6211.0 {I2} (1974Al05) and 6209.0 {I7} (1968En01) 
J$from |g(|q)in 1968En01 and RUL 
$T{-1/2}: weighted average of 95 fs {I30} (1984La24) and 62 fs {I23} from 1968En01 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E$weighted average of 6353.5 {I4} (1974Al05) and 6352.5 {I20} (1968En01) 
$T{-1/2}: weighted average of 3.5 fs {I14} (1984La24) and 4.2 fs {I28} (1974Al06) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$weighted average of 6601.17 {I19} (1974Al05) and 6601.2 {I4} (1968En01) 
J$from |g(|q) and RUL (1968En01) 
$T{-1/2}: weighted average of 12.5 fs {I21} (1984La24), 11 fs {I7} (1974Al06), and 17 fs {I7} (1968En01) 


level_energy_unit: KEV
level_spin_parity: (5)-
level_lifetime_unit: FS
level_comment:
E$weighted average of 6673.5 {I6} (1974Al05) and 6673.3 {I15} (1968En01) 
$T{-1/2}: weighted average of 12.5 fs {I35} (1984La24) and 16 fs {I5} (1974Al06) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$from 1974Al05, unresolved doublet at 6824 (1974Al05,1988Wa34) 
$T{-1/2}: other: <14 fs (1974Al06) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=400 {I2} 
$Resonance listed in table 38.17 in 1990En08 (taken from Utrecht annual report of 1978 and a priv comm.; c.f. ref Va78h in 1990En08) 
$THIS RESONANCE APPEARS IN A 1978 UTRECHT ANNUAL REPORT AND IS given IN TABLE 38.17 of 1990En08 WITH REFERENCE ^Va78h AND priv comm FROM ^C. van der ^Leun 


level_energy_unit: KEV
level_spin_parity: (2)
level_comment:
$E(p)(lab)=600.6 {I6} 
$S({-p|g})=0.14 {I5} (1988Wa34) relative to the value 1.00 eV {I13} (1979Pa16) for E(p)=846 
S$weighted average of 600.5 {I6} (1961He19) and 600.7 {I9} (1988Wa34) 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_comment:
$E(p)(lab)=624.4 {I7} 
$S{-p|g}=0.15 {I5} (1988Wa34) relative to the value 1.00 eV {I13} (1979Pa16)for Ep=846 
S$weighted average of 624.2 {I7} (1961He19) and 624.7 {9} (1988Wa34) 


level_energy_unit: KEV
level_spin_parity: (1-,2,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=690.5 {I5} 
S$weighted average of 690.1 {I7} (1961He19) and 690.7 {I5} (1974Al05) 
$S{-p|g}=0.23 eV {I5} (1974Al05); |G=140 eV {I30} (1961He19) 


level_energy_unit: KEV
level_spin_parity: (2-,3,4+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=724.3 {I5} 
$S{-p|g}=0.49 eV {I11} (1974Al05) 
S$weighted average of 724.0 {I15} (1961Ku01) and 724.3 {I5} (1974Al05) 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
$E(p)(lab)=740.7 {I6} 
J$spin from (p,|g(|q)) (1988Wa34) 
S$weighted average of 740.7 {I15} (1961Ku01) and 740.7 {I6} (1974Al06) 
$S{-p|g}=0.70 eV {I14} 


level_energy_unit: KEV
level_spin_parity: (2)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=766.2 {I7} 
J$from Adopted Levels. (2,3) from (p,|g(|q)), (2,3-) with 1967Bo03 combined (1988Wa34) 
S$weighted average of 766.1 {I15} (1961Ku01) and 766.2 {I7} (1974Al05) 
$S{-p|g}=2.4 eV {I5} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=823.8 {I6} 
$S{-p|g}=0.9 eV {I2} 
S$weighted average of 824.1 {I15} (1961Ku01) and 823.5 {I6} (1974Al06) 


level_energy_unit: KEV
level_spin_parity: (1+,2,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=846.3 {I6} 
$S{-p|g}=1.06 eV {I15} (1974Al05), 1.04 eV {I15} (1968En01), 1.00 eV {I13} (1979Pa16) 
S$weighted average of 846.8 {I15} (1961Ku01) and 846.2 {I6} (1974Al06) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=876.4 {I6} 
E$weighted average of 876.0 {I11} (1967Bo03) and 876.5 {I6} (1974Al05) 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}|<0.07 eV {I5} (1974Al05); S{-p|a}=0.8 eV (1967Bo03) 


level_energy_unit: KEV
level_spin_parity: (1-,2+,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=877.9 {I6} 
E$weighted average of 877.5 {I11} (1967Bo03) and 878.0 {I6} (1974Al05) 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=1.3 eV {I3} (1974Al05); S{-p|a}=1.1 eV (1967Bo03) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=880.2 {I6} 
$S{-p|g}=0.27 eV {I8} (1974Al05) 
S$weighted average of 879.6 {I15} (1961Ku018) and 880.3 {I6} (1974Al05) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=894.3 {I6} 
$Probable doublet (1974Al05) 
E$weighted average of 893.8 {I11} (1967Bo03) and 894.4 {I6} (1974Al05) 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=0.09 eV; S{-p|a}=1.5 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=898.4 {I6} 
J$(p,|a(|q)): A{-2}=+0.820 {I8} (1967Bo03) 
$S{-p|g}=0.41 eV; S{-p|a}=4.6 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=904.6 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 904.0 {I11} (1967Bo03) and 904.8 {I6} (1974Al05) 
$S{-p|g}=0.06 eV {I2}; S{-p|a}=0.40 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=926.7 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 926.2 {I11} (1967Bo03) and 926.8 {I6} (1974Al05) 
$S{-p|g}=0.20 eV {I6}; S{-p|a}=2.6 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=928.3 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 927.7 {I11} (1967Bo03) and 928.5 {I6} (1974Al05) 
$S{-p|a}=4.4 eV 


level_energy_unit: KEV
level_spin_parity: (2,3-)
level_comment:
$E(p)(lab)=929.3 {I6} 
E$probable doublet in 1974Al05, not reported in 1988Wa34. 
$S{-p|g}=2.3 eV {I5}, not resolved from E(p)=928.5 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=940.3 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 939.8 {I12} (1967Bo03) and 940.5 {I7} (1974Al05) 
$S{-p|g}<0.05 eV; S{-p|a}=0.6 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=956.1 {I6} 
J$(1,2,3) from |g(|q) in 1988Wa34, 3- from (p,|a(|q)): A{-2}=+0.809 {I5} (1967Bo03) 
S$weighted average of 955.6 {I12} (1967Bo03) and 956.2 {I6} (1974Al05) 
$S{-p|g}=1.5 eV {I3}; S{-p|a}=7 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=965.9 {I6} 
S$weighted average of 965.0 {I12} (1967Bo03) and 966.1 {I6} (1974Al05) 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=0.10 {I4} eV; S{-p|a}=0.8 eV 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=968.2 {I6} 
S$968.0 {I12} (1967Bo03), 968.2 {I6} (1974Al05) 
J$(2,3) from (p,|g(|q)) (1988Wa34) and |p=natural from {+37}Cl(p,|a) 
$S{-p|g}=3.6 eV {I7}; S{-p|a}=0.25 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=972.1 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 971.5 {I12} (1967Bo03) and 972.2 {I6} (1974Al05) 
$S{-p|g}=0.15 eV {I6}; S{-p|a}=0.25 eV 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=985.8 {I6} 
J$from (p,|a(|q)): A{-2}=-0.92 {I4} (1974Al05) 
S$weighted average of 985.5 {I12} (1967Bo03) and 985.9 {I6} (1974Al05) 
$S{-p|g}=2.6 eV {I5}; S{-p|a}=1.6 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=988.2 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 987.9 {I12} (1967Bo03) and 988.3 {I7} (1974Al05) 
$S{-p|g}<0.10 eV; S{-p|a}=4.8 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=998.9 {I6} 
J$from (p,|a(|q)): A{-2}=-0.35 {I3} (1967Bo03) 
S$weighted average of 998.4 {I12} (1967Bo03) and 999.0 {I6} (1974Al05) 
$S{-p|g}=0.50 eV {I11}; S{-p|a}=37 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1000.7 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1000.3 {I12} (1967Bo03) and 1000.8 {I8} (1974Al05) 
$S{-p|g}<0.04 eV; S{-p|a}=2.2 eV 


level_energy_unit: KEV
level_spin_parity: (1,2,3)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1011.9 {I2} 
J$from (p,|g(|q)) (1988Wa34) 
S$used by 1974Al05 as a secondary energy standard 
$S{-p|g}=2.1 eV {I4} 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1018.4 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1018.1 {I20} (1967Bo03) and 1018.4 {I6} (1974Al05); not reported in 1988Wa34 
$S{-p|g}=0.37 eV {I9}; S{-p|a}=0.3 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1045.2 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1044.6 {I12} (1967Bo03) and 1045.3 {I6} (1974Al05) 
$S{-p|g}=0.05 eV {I3}; S{-p|a}=1.9 eV 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1055.7 {I6} 
J$(p,|a(|q)): A{-2}=+0.808 {I6}, 1- less likely (1967Bo03) 
S$weighted average of 1055.0 {I12} (1967Bo03) and 1055.9 {I6} (1974Al05) 
$S{-p|g}=0.3 eV {I2}; S{-p|a}=1.9 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1061.4 {I6} 
S$weighted average of 1060.8 {I12} (1967Bo03) and 1061.5 {I6} (1974Al05) 
J$(p,|a(|q)): A{-2}=-0.56 {I4} (1967Bo03) 
$S{-p|a}=12 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1061.6 {I6} 
E$probable doublet in 1974Al05 
$|G for E(p)=1061.5 
$S{-p|g}=2.4 eV {I5} (with E(p)=1061.5) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1070.0 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1069.5 {I12} (1967Bo03) and 1070.1 {I6} (1974Al05) 
$S{-p|g}=0.19 eV {I7}; S{-p|a}=0.9 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1077.8 {I6} 
J$(p,|a(|q)), A{-2}=+0.17 {I3} (1967Bo03) 
S$weighted average of 1077.2 {I13} (1967Bo03) and 1077.9 {I6} (1974Al05) 
$S{-p|g}<0.08 eV; S{-p|a}=10 eV 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1089.0 {I5} 
J$from |g(|q,pol) in 1966Er07 
S$weighted average of 1089.0 {I13} (1967Bo03), 1088.7 {I5} (1968En01) and 1089.5 {I6} (1974Al06) 
$S{-p|g}=3.4 eV {I7}; S{-p|a}=0.4 eV {I2}; (2J+1)|G{-p}<50 eV (1968Bo07); S{-p|g}=3.5 eV {I5} (1968En01) 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1093.0 {I6} 
J$(p,|a(|q)): A{-2}=-0.19 {I2} (1967Bo03) 
S$weighted average of 1092.6 {I13} (1967Bo03) and 1093.1 {I6} (1974Al05) 
$S{-p|g}=0.10 eV {I7}; S{-p|a}=50 eV; (2J+1)|G{-p}<50 eV (1968Bo07) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1094.3 {I5} 
J$from |g(|q,pol) in 1966Er07 
S$weighted average of 1094.0 {I5} (1968En01) and 1094.8 {I6} (1974Al06) 
$S{-p|g}=7.0 eV {I14} (1974Al05), 7.0 eV {I10} (1968En01) 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1103.7 {I6} 
J$(p,|a(|q)): A{-2}=+0.808 {I7}, 1- less likely (1967Bo03). 
S$weighted average of 1103.3 {I13} (1967Bo03) and 1103.8 {I6} (1974Al05) 
$S{-p|g}=0.67 eV {I14}; S{-p|a}=12 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1113.5 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=0.20 eV {I7}; S{-p|a}|?0.1 eV (1974Al05) 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$E(p)(lab)=1114.6 {I6} 
J$(p,|a(|q)); A{-2}=+0.37 {I5} (1967Bo03). 
S$weighted average of 1114.3 {I13} (1967Bo03) and 1114.6 {I6} (1974Al05). 1114.3 {I13} in 1967Bo03 could be a triplet corresponding to 1113.5+1114.6+1115.6 in 1974Al05 
$S{-p|g}<0.07 eV; S{-p|a}|?1.3 eV (1974Al05), 2.3 (1967Bo03) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1115.6 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=1.3 eV {I3}; S{-p|a}|?1.0 eV (1974Al05) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1117.5 {I6} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1118.2 {I13} (1967Bo03) and 1117.4 {I6} (1974Al05) 
$S{-p|g}<1.9 eV; S{-p|a}=0.6 eV 


level_energy_unit: KEV
level_spin_parity: (2,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1126.2 {I6} 
J$(2,3) from (p,|g(|q)), (2,3-) with 1967Bo03 combined (1988Wa34) 
$S{-p|g}=4.3 eV {I8} B 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1136.8 {I6} 
$S{-p|g}=1.1 eV {I2} (1974Al05), 0.8 eV {I3} (1968En01) 
S$weighted average of 1136.4 {I8} (1968En01) and 1137.0 {I6} (1974Al06) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1138.5 {I6} 
J$(p,|g(|q)) and pol(|g) 1968En01; (p,|a(|q)): A{-2}=+0.805 {I3} (1967Bo03) 
S$weighted average of 1138.3 {I13} (1967Bo03), 1138.5 {I6} (1968En01) and 1138.6 {I6} (1974Al05) 
$|G from (p,|g) (1974Al05); S{-p|g}=6.5 eV {I13} (1974Al05), 7.3 eV {I12} (1968En01); S{-p|a}=160 eV (1967Bo03); |G{-p}=25 eV {I8} (1968Bo07) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1142.6 {I6} 
J$(p,|a(|q)): A{-2}=+0.804 {I5} (1967Bo03) 
S$weighted average of 1142.3 {I13} (1967Bo03), 1142.5 {I7} (1968En01), 1142.8 {I6} (1974Al05) 
$|G from (p,|g) in 1974Al05; S{-p|g}=3.1 eV {I6}; S{-p|a}=80 eV; |G{-p}=12 eV {I3} (1968Bo07) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1155.8 {I7} 
J$(p,|a(|q)): A{-2}=+0.805 {I6} (1967Bo03) 
S$weighted average of 1155.6 {I13} (1967Bo03) and 1155.9 {I7} (1974Al05) 
$S{-p|g}=0.78 eV {I17}; S{-p|a}=60 eV 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1164.2 {I7} 
J$(p,|a(|q)): A{-2}=+1.008 {I16}, A{-4}=+0.52 {I12} (1967Bo03) 
S$weighted average of 1164.5 {I13} (1967Bo03) and 1164.1 {I7} (1974Al05) 
$S{-p|g}<0.16 eV; S{-p|a}=2.9 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1167.8 {I7} 
J$(p,|a(|q)): A{-2}=+0.45 {I3} (1967Bo03) 
S$weighted average of 1168.1 {I13} (1967Bo03) and 1167.7 {I7} (1974Al05). Probable doublet in 1974Al05 
$S{-p|g}=1.4 eV {I3}; S{-p|a}=6 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1172.2 {I7} 
J$(p,|a(|q)): A{-2}=-0.20 {I3} (1967Bo03) 
S$weighted average of 1172.6 {I13} (1967Bo03) and 1172.1 {I7} (1974Al05) 
$|G for E(p)=1171.9 
$S{-p|g}=3.3 eV {I7} (with E(p)=1171.9); S{-p|a}=17 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=1173.8 {I7} 
J$(p,|a(|q)): A{-2}=+0.804 {I11} (1967Bo03) 
S$weighted average of 1174.0 {I13} (1967Bo03) and 1173.8 {I7} (1974Al05) 
$S{-p|g}=1.2 eV {I5}; S{-p|a}=50 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1182.2 {I7} 
J$(p,|a(|q)): A{-2}=+0.822 {I7}, A{-4}=+0.027 {I12}, A{-6}=-0.28 {I5} (1967Bo03) 
S$weighted average of 1182.5 {I13} (1967Bo03) and 1182.1 {I7} (1974Al05) 
$S{-p|g}=0.93 eV {I19}; S{-p|a}=18 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1212.6 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}<0.3 eV; S{-p|a}=2.2 eV (from 1974Al05) 


level_energy_unit: KEV
level_spin_parity: (2+,3-,4+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1213.8 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1214.3 {I13} (1967Bo03) and 1213.7 {I7} (1974Al05). 1214.3 in 1967Bo03 could be a doublet corresponding to 1212.6+1213.7 in 1974Al05 
$S{-p|g}=5.0 eV {I10}; S{-p|a}=2.2 eV (1974Al05), 4.4 eV (1967Bo03) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1233.3 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$seen in (p,|g) and (p,|a) in 1974Al05. Other: 1235.5 {I14} from (p,|a) in 1967Bo03 
$S{-p|g}<0.15 eV; S{-p|a}=0.4 eV 


level_energy_unit: KEV
level_spin_parity: (1,2,3)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1234.1 {I7} 
J$from (p,|g(|q)) 
S$from (p,|g) in 1974Al05, not seen in (p,|a) in 1974Al05 
$S{-p|g}=1.5 eV {I3} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1243.4 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$from 1974Al05. Other: 1244.9 {I14} (1967Bo03) 
$S{-p|g}=1.6 eV {I3}; S{-p|a}=3.8 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1246.3 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$from 1974Al05. Other: 1247.8 {I14} (1967Bo03) 
$S{-p|g}<0.3 eV; S{-p|a}=2.3 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1257.3 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1258.4 {I14} (1967Bo03) and 1257.0 {I8} (1974Al05) 
$S{-p|g}<0.6 {I3} eV; S{-p|a}=6 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1262.4 {I7} 
J$(p,|a(|q)): A{-2}=-0.39 {I6} (1967Bo03); (1,2) from (p,|g(|q)) (1988Wa34) 
S$weighted average of 1263.5 {I14} (1967Bo03), 1262.4 {I15} (1968En01) and 1262.1 {I7} (1974Al06) 
$S{-p|g}=2.6 eV {I5} (1974Al05), 3.8 eV {I15} (1968En01); S{-p|a}=19 eV 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1270.3 {I7} 
J$(p,|a(|q)): A{-2}=+0.800 {I3}, 1- less likely (1967Bo03) 
S$weighted average of 1271.3 {I14} (1967Bo03) and 1270.0 {I7} (1974Al05); probable doublet in 1974Al05 
$S{-p|a}=33 eV 
$|g rays could be from 1269.8 resonance also 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1273.9 {I7} 
S$weighted average of 1274.7 {I14} (1967Bo03) and 1273.7 {I7} (1974Al05) 
$S{-p|g}=0.33 eV {I19}; S{-p|a}=14 eV 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1278.8 {I7} 
J$(p,|a(|q)): A{-2}=+0.798 {I14}, 1- less likely (1967Bo03) 
S$weighted average of 1279.6 {I14} (1967Bo03) and 1278.6 {I7} (1974Al05) 
$S{-p|g}=0.03 eV {I2}; S{-p|a}=12 eV 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1285.4 {I8} 
J$from (p,|a(|q)): A{-2}=-0.18 {I4}, A{-4}=-0.35 {I6} (1967Bo03) 
S$weighted average of 1286.0 {I14} (1967Bo03) and 1285.2 {I8} (1974Al05) 
$S{-p|g}<0.10 eV; S{-p|a}=12 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1293.3 {I7} 
J$(p,|a(|q)): A{-2}=-0.336 {I15} (1967Bo03); (1,2) from (p,|g(|q)) in 1988Wa34 
S$weighted average of 1293.8 {I14} (1967Bo03) and 1293.2 {I7} (1974Al05) 
$S{-p|g}=1.3 eV {I3}; S{-p|a}=48 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1300.4 {I7} 
J$(p,|a(|q)): A{-2}=+0.18 {I4} (1967Bo03) 
S$weighted average of 1300.8 {I14} (1967Bo03) and 1300.3 {I7} (1974Al05) 
$S{-p|g}=0.08 eV {I5}; S{-p|a}=15 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1304.0 {I7} 
S$probable doublet in 1974Al05 
$S{-p|g}=2.1 eV {I7} 
$|g's from 1303.4 resonance also 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1306.9 {I7} 
J$(p,|a(|q)): A{-2}=-0.632 {I12} 
S$weighted average of 1307.5 {I14} (1967Bo03) and 1306.7 {I7} (1974Al05) 
$S{-p|g}=2.2 eV {I5}; S{-p|a}=32 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1311.1 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1311.6 {I14} (1967Bo03) and 1311.0 {I7} (1974Al05). 1311.6 in 1967Bo03 could be a doublet corresponding to 1311.0+1312.2 in 1974Al05 
$S{-p|g}=0.11 eV {I7}; S{-p|a}=4.5 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1312.2 {I3} 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=1.8 eV {I4}; S{-p|a}|?1.0 eV (from 1974Al05) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1320.3 {I7} 
$S{-p|g}=1.9 eV {I4} (1974Al05), 4.0 eV {I15} (1968En01) 
S$weighted average of 1320.3 {I15} (1968En01) and 1320.3 {I7} (1974Al06); 1968En01 observed on resonance at this energy, probable triplet with 1318.5, 1322.8 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1323.0 {I7} 
J$(p,|a(|q)): A{-2}=-0.01 {I2} (1974Al06) gives 0+,1-,2+, |g to g.s. excludes 0+ 
S$weighted average of 1323.6 {I14} (1967Bo03) and 1322.8 {I7} (1974Al05) 
$S{-p|g}=1.9 eV {I4}; S{-p|a}=20 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1324.8 {I7} 
J$(p,|a(|q)): A{-2}=+0.74 {I3} (1974Al06) 
S$weighted average of 1325.4 {I14} (1967Bo03) and 1324.7 {I7} (1974Al05) 
$S{-p|g}=1.6 eV {I5}; S{-p|a}=60 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1327.1 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=0.18 eV {I8}; S{-p|a}=24 eV 
S$weighted average of 1327.7 {I14} (1967Bo03) and 1326.9 {I7} (1974Al05) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1333.3 {I7} 
J$(p,|a(|q)): A{-2}=-0.732 {I9} (1967Bo03) 
S$weighted average of 1334.2 {I14} (1967Bo03) and 1333.1 {I7} (1974Al05) 
$S{-p|g}=0.29 eV {I11}; S{-p|a}=230 eV 
$|G=0.33 eV {I11} from (p,|g) in 1974Al05, (2J+1)|G{-p}=0.27 keV {I11}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1337.7 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1338.4 {I14} (1967Bo03) and 1337.5 {I7} (1974Al05) 
$S{-p|g}=0.45 eV {I16}; S{-p|a}=24 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1346.0 {I7} 
J$(0+,1-,2+) from (p,|a(|q)): A{-2}=+0.06 {I2}, A{-4}=-0.06 {I3} (1974Al06); |g to g.s. excludes 0+ 
S$weighted average of 1346.6 {I14} (1967Bo03) and 1345.9 {I7} (1974Al05). Other: 1342 (1966Ka18) 
$|G from (p,|g) in 1974Al05; S{-p|g}=2.5 eV {I5}; S{-p|a}=180 eV; (2J+1)|G{-p}=0.18 keV {I7}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1351.7 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1352.6 {I14} (1967Bo03) and 1351.5 {I7} (1974Al05). Other: 1356 (1966Ka18) 
$S{-p|g}<0.3 eV; S{-p|a}=19 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$E(p)(lab)=1372.2 {I8} 
J$(p,|a(|q)): A{-2}=-0.46 {I7} (1967Bo03) 
S$weighted average of 1373.1 {I15} (1967Bo03) and 1372.0 {I8} (1974Al05) 
$S{-p|g}<0.3 eV; S{-p|a}=6 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1373.6 {I7} 
J$(p,|a(|q)): A{-2}=+0.418 {I13} (1967Bo03) 
S$weighted average of 1374.3 {I15} (1967Bo03) and 1373.5 {I7} (1974Al05) 
$S{-p|g}=1.4 eV {I5}; S{-p|a}=14 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1387.4 {I7} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)): A{-2}=+0.92 {I3}, A{-4}=+0.23 {I4} (1967Bo03) 
S$weighted average of 1388.4 {I15} (1967Bo03) and 1387.2 {I7} (1974Al05) 
$S{-p|g}=1.8 eV {I5}; S{-p|a}=11 eV 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1392.6 {I7} 
J$(p,|a(|q)): A{-2}=+1.032 {I9}, A{-4}=+0.59 {I2}, A{-6}=+0.06 {I3} (1967Bo03) 
S$weighted average of 1393.6 {I15} (1967Bo03) and 1392.4 {I7} (1974Al05) 
$S{-p|g}=0.75 eV {I16}; S{-p|a}=5 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$E(p)(lab)=1403.2 {I8} 
J$(p,|a(|q)): A{-2}=-0.33 {I5} (1967Bo03) 
S$weighted average of 1403.5 {I15} (1967Bo03) and 1403.1 {I8} (1974Al05) 
$S{-p|a}|?4 eV (1974Al05), 6 eV from 1967Bo03 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1408.3 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1409.0 {I15} (1967Bo03) and 1408.2 {I7} (1974Al05) 
$S{-p|a}=50 eV 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1410.9 {I7} 
J$(p,|a(|q)): A{-2}=-0.887 {I10} (1967Bo03) 
S$weighted average of 1411.7 {I15} (1967Bo03) and 1410.7 {I7} (1974Al05) 
$|G from (p,|g) in 1974Al05; S{-p|g}=0.8 eV {I4}; S{-p|a}=150 eV; (2J+1)|G{-p}=0.24 keV {I11}, l{-p}=1 (1974Al05) |G=0.7 eV {I6} from 1967Bo03 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1420.2 {I7} 
J$(p,|a(|q)): A{-2}=-0.29 {I4} (1967Bo03) 
S$weighted average of 1421.4 {I15} (1967Bo03) and 1419.9 {I7} (1974Al05). Other: 1422 (1966Ka18) 
$S{-p|g}=0.5 eV {I2}; S{-p|a}=15 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1439.2 {I7} 
J$(p,|a(|q)): A{-2}=+0.13 {I3} (1967Bo03) 
S$from 1974Al05. Other: 1440.4 {I15} (1967Bo03) could be a doublet corresponding to 1439.2+1439.3 in 1974Al05 
$S{-p|a}=60 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1447.5 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1448.3 {I15} (1967Bo03) and 1447.3 {I7} (1974Al05) 
$S{-p|g}=0.2 eV {I1}; S{-p|a}=3.3 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1450.1 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1451.0 {I15} (1967Bo03) and 1449.8 {I7} (1974Al05) 
$S{-p|g}<0.4 eV; S{-p|a}=26 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1452.9 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1453.6 {I15} (1967Bo03) and 1452.7 {I7} (1974Al05) 
$S{-p|g}=0.10 eV {I7}; S{-p|a}=11 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1456.4 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1457.4 {I15} (1967Bo03) and 1456.2 {I7} (1974Al05) 
$S{-p|g}=3.7 eV {I8}; S{-p|a}=29 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1467.3 {I7} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)): A{-2}=+0.47 {I3} (1967Bo03) 
S$weighted average of 1468.4 {I15} (1967Bo03) and 1467.1 {I7} (1974Al05) 
$S{-p|g}=0.5 eV {I2}; S{-p|a}=60 eV 


level_energy_unit: KEV
level_spin_parity: (4+,5-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1479.7 {I7} 
J$(p,|a(|q)): A{-2}=+1.038 {I16}, A{-4}=+0.61 {I4}, A{-6}=+0.10 {I5} and odd terms (1967Bo03); (p,|g(|q)) (1974Al06) 
S$weighted average of 1481.1 {I15} (1967Bo03) and 1479.4 {I7} (1974Al05). Other: 1476 (1966Ka18) 
$S{-p|g}=1.1 eV {I2}; S{-p|a}=2.1 eV 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1483.1 {I7} 
J$(p,|a(|q)): A{-2}=+0.05 {I4}, A{-4}=-0.57 {I4} (1967Bo03) 
S$weighted average of 1483.9 {I15} (1967Bo03) and 1482.9 {I7} (1974Al05) 
$S{-p|g}<0.5 eV; S{-p|a}=20 eV; 
$|G from (p,|g) in 1974Al05; (2J+1)|G{-p}=0.9 keV {I3}, l{-p}=1, (p,p) resonance could be double(1974Al05) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1499.3 {I7} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1500.1 {I16} (1967Bo03) and 1499.1 {I7} (1974Al05) 
$S{-p|g}=0.09 eV {I5}; S{-p|a}=18 eV 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1510.1 {I8} 
J$(p,|a(|q)): A{-2}=+1.051 {I8}, A{-4}=+0.64 {I3}, A{-6}=+0.13 {I4} (1967Bo03) 
S$weighted average of 1510.8 {I16} (1967Bo03) and 1509.9 {I8} (1974Al05) 
$S{-p|g}=0.45 eV {I17}; S{-p|a}=15 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1514.5 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1515.5 {I16} (1967Bo03) and 1514.3 {I8} (1974Al05); probable doublet 1974Al05 
$S{-p|g}=1.9 eV {I4}; S{-p|a}=9 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1521.5 {I8} 
$|G from (p,|g) in 1974Al05; S{-p|g}=2.9 eV {I11}; (2J+1)|G{-p}=0.9 keV {I3}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1526.0 {I8} 
J$(p,|a(|q)): A{-2}=+0.414 {I11}, A{-4}=-0.25 {I5} (1967Bo03) 
S$from 1974Al05. Other: 1527.3 {I16} (1967Bo03) 
$S{-p|g}<0.3 eV; S{-p|a}=50 eV 


level_energy_unit: KEV
level_spin_parity: (4+,5-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1529.5 {I8} 
$Probable doublet (1974Al05) 
J$(p,|a(|q)): A{-2}=+1.43 {I15}, A{-4}=+0.58 {I17} (1974Al06) 
S$weighted average of 1530.6 {I16} (1967Bo03) and 1529.2 {I8} (1974Al05) 
$S{-p|g}=4.9 eV {I10}; S{-p|a}=8 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1534.9 {I8} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)): A{-2}=+1.01 {I3}, no odd terms (1967Bo03) 
S$from 1974Al05. Other: 1537.5 {I16} (1967Bo03) 
$S{-p|g}<0.2 eV; S{-p|a}=28 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1537.8 {I8} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)) 
S$weighted average of 1538.8 {I16} (1967Bo03) and 1537.5 {I8} (1974Al05) 
$S{-p|a}=160 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1541.5 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|g}=1.5 eV {I4}; S{-p|a}|?20 eV (1974Al05) 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1542.4 {I8} 
J$(p,|a(|q)): A{-2}=+0.17 {I2} (1967Bo03) 
S$weighted average of 1543.3 {I16} (1967Bo03) and 1542.2 {I8} (1974Al05) 
$S{-p|g}<0.3 eV; S{-p|a}=370 eV; (2J+1)|G{-p}=0.35 keV {I14}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1554.6 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1555.6 {I16} (1967Bo03) and 1554.3 {I8} (1974Al05). Other: 1550 (1966Ka18) 
$(p,|a(|q)): A{-2}=+1.06 {I3}, A{-4}=+0.09 {I4} , A{-6}=-0.11 {I4} (1974Al06) no solution 
$S{-p|g}=1.2 eV {I2}; S{-p|a}=160 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1557.7 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1558.7 {I16} (1967Bo03) and 1557.4 {I8} (1974Al05) 
$S{-p|g}=0.30 eV {I18}; S{-p|a}=340 eV; (2J+1)|G{-p}=0.36 keV {I18}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1565.7 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$from 1974Al05. Other: 1566.8 {I16} (1967Bo03) could be a doublet corresponding to 1565.1+1565.7 in 1974Al05; 1566 (1966Ka18) 
$S{-p|g}=0.5 eV {I2}; S{-p|a}=18 eV (with 1565.1) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1569.2 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1570.3 {I17} (1967Bo03) and 1569.0 {I8} (1974Al05) 
$S{-p|g}=0.41 eV {I16}; S{-p|a}=12 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1572.3 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1573.2 {I17} (1967Bo03) and 1572.1 {I8} (1974Al05) 
$S{-p|g}<0.07 eV; S{-p|a}=28 eV 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1574.5 {I8} 
$(p,|a(|q)): A{-2}=+0.94 {I13}, A{-4}=+0.83 {I20}, A{-6}=-0.26 {I18} (1974Al06) 
S$weighted average of 1575.8 {I17} (1967Bo03) and 1574.2 {I8} (1974Al05) 
$S{-p|g}=1.3 eV {I3}; S{-p|a}=13 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1580.3 {I8} 
$|G from (p,|g) in 1974Al05; S{-p|g}=2.8 eV {I6}; (2J+1)|G{-p}=0.6 keV {I2}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1583.8 {I8} 
J$(p,|a(|q)): A{-2}=+0.806 {I15} (1967Bo03) 
S$from 1974Al05. Other: 1584.8 {I17} (1967Bo03) could be a doublet corresponding to 1583.8+1583.9 in 1974Al05 
$S{-p|a}=4.4 eV 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1587.9 {I8} 
J$(p,|a(|q)): A{-2}=-0.619 {I16} (1967Bo03) 
S$weighted average of 1589.6 {I17} (1967Bo03) and 1587.5 {I8} (1974Al05) 
$S{-p|g}<0.2 eV; S{-p|a}=3.3 eV 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1590.9 {I8} 
J$(p,|a(|q)): A{-2}=-0.969 {I11} (1967Bo03) 
S$weighted average of 1591.8 {I17} (1967Bo03) and 1590.7 {I8} (1974Al05) 
$S{-p|a}=20 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1594.5 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1595.0 {I17} (1967Bo03) and 1594.4 {I8} (1974Al05) 
$S{-p|g}=3.0 eV {I6}; S{-p|a}=1.6 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1606.2 {I8} 
J$(1-,3-) from (p,|a(|q)): A{-2}=+0.83 {I5} (1967Bo03); (2,3) from (p,|g(|q)) (1988Wa34) 
S$weighted average of 1607.3 {I17} (1967Bo03) and 1606.0 {I8} (1974Al05) 
$S{-p|g}=3.1 eV {I6}; S{-p|a}=31 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1611.0 {I8} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)): A{-2}=-0.6 {I4}, A{-4}=-0.37 {I16} and odd terms (1967Bo03) 
S$weighted average of 1611.9 {I17} (1967Bo03) and 1610.8 {I8} (1974Al05) 
$S{-p|g}=0.11 eV {I7}; S{-p|a}=140 eV 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1615.5 {I8} 
J$(p,|a(|q)): A{-2}=+0.885 {I11} (1967Bo03) 
S$weighted average of 1616.2 {I17} (1967Bo03) and 1615.3 {I8} (1974Al05) 
$S{-p|g}=0.61 eV {I12}; S{-p|a}=220 eV |G from (p,|g) in 1974Al05 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1619.8 {I8} 
J$|p=natural (p,|a(|q)): A{-2}=-1.09 {I5} and odd terms (1967Bo03) 
S$weighted average of 1620.6 {I17} (1967Bo03) and 1619.6 {I8} (1974Al05). Other: 1624 (1966Ka18) 
$S{-p|g}=0.35 eV {I8}; S{-p|a}=120 eV 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1633.0 {I8} 
J$(p,|a(|q)): A{-2}=+0.739 {I18}, A{-4}=-0.16 {I4} (1967Bo03) 
S$weighted average of 1634.0 {I17} (1967Bo03) and 1632.8 {I8} (1974Al05) 
$S{-p|g}=4.0 eV {I8}; S{-p|a}=60 eV (1974Al05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=1641.6 {I8} 
J$(p,|a(|q)): A{-2}=+0.083 {I20}, A{-4}=-0.378 {I14} (1967Bo03) 
S$weighted average of 1642.5 {I18} (1967Bo03) and 1641.4 {I8} (1974Al05) 
$S{-p|g}=2.3 eV {I8}; S{-pn}=9 eV {I3}; S{-p|a}=500 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1647.2 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1648.0 {I18} (1967Bo03) and 1647.0 {I8} (1974Al05). Other: 1648 (1966Ka18) 
$S{-p|g}=0.8 eV {I4}; S{-pn}<0.2 eV; S{-p|a}=100 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$E(p)(lab)=1663.0 {I8} 
J$(p,|a(|q)): A{-2}=+0.354 {I20} (1967Bo03) 
S$weighted average of 1663.4 {I18} (1967Bo03) and 1662.9 {I8} (1974Al05) 
$S{-p|a}=4.6 eV, S{-pn}=4.7 eV {I13} 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1666.6 {I8} 
J$(p,|a(|q)): A{-2}=+0.784 {I1}, 1- less likely (1967Bo03) 
S$weighted average of 1667.4 {I18} (1967Bo03) and 1666.4 {I8} (1974Al05) 
$|G from (p,|g) in 1974Al05, |G=1.0 eV {I6} from 1967Bo03 
$S{-p|g}=3.9 eV {I8}; S{-pn}<0.2 eV; S{-p|a}=130 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1680.0 {I8} 
$|G from (p,n) in 1974Al05; S{-p|g}=4.0 eV {I10}; S{-pn}=29 eV {I8}; (2J+1)|G{-p}=1.8 keV {I5}, l{-p}=1 (1974Al05) 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1683.3 {I8} 
J$(p,|a(|q)): A{-2}=+0.820 {I7}, 1- less likely (1967Bo03) 
S$weighted average of 1684.9 {I18} (1967Bo03) and 1683.0 {I8} (1974Al05) 
$|G from (p,n) in 1974Al05, |G=1.1 eV {I6} from 1967Bo03 
$S{-p|g}=4.1 eV {I15}; S{-pn}=70 eV {I30}; S{-p|a}=70 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1690.4 {I8} 
$|G from (p,n) in 1974Al05; S{-p|g}=16 eV {I4}; S{-pn}=180 eV {I50}; (2J+1)|G{-p}=1.1 keV {I3}, l{-p}=1 (1974Al05) 
$|G=1.5 keV from 1952Sc09 for E(p)=1690.8 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1692.8 {I10} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1693.9 {I18} (1967Bo03) and 1692.5 {I10} (1974Al05). Other: 1692 (1961Ma28) 
$S{-p|a}=15 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1697.5 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1698.2 {I18} (1967Bo03) and 1697.4 {I8} (1974Al05) 
$S{-p|g}=0.7 eV {I4}; S{-pn}=15 eV {I4}; S{-p|a}=13 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1700.8 {I8} 
S$other: 1702.7 (1952Sc09) 
$|G from (p,n) in 1974Al05; S{-p|g}=4.2 eV {I14}; S{-pn}=64 eV {I14} 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1704.5 {I10} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1705.6 {I18} (1967Bo03) and 1704.2 {I10} (1974Al05) 
$S{-p|g}<0.2 eV; S{-pn}<4 eV; S{-p|a}=100 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1707.6 {I10} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1708.7 {I18} (1967Bo03) and 1707.3 {I10} (1974Al05) 
$S{-p|a}=1.10 keV (1967Bo03), |G=3.9 eV {I6} (1967Bo03) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1719.6 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1720.9 {I18} (1967Bo03) and 1719.3 {I8} (1974Al05). Other: 1716 (1966Ka18) 
$S{-p|g}=3.1 eV {I12}; S{-pn}<10 eV; S{-p|a}=170 eV 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1731.6 {I8} 
J$spin from (p,|g(|q)), parity from polarization (1968En01) 
S$from 1974Al05. Other: 1732.3 {I10} probable doublet in 1968En01 
$|G from (p,|g) in 1974Al05; S{-p|g}=35 eV {I7}; S{-pn}<10 eV; S{-pp}|?22 eV (1968Bo07) 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1732.1 {I8} 
J$(p,|a(|q)): 1967Bo03: E(p)=1732.3 {I18}; 1-,2+; A{-2}=+0.30 {I3} (1967Bo03) 
S$weighted average of 1732.3 {I18} (1967Bo03), 1732.3 {I10} (1968En01) and 1732.0 {I8} (1974Al06). 1968En01 observe one resonance with J=4, |g decays at this energy, probable doublet with Ep=1731.6. Others: 1733.2 (1952Sc09), 1735 (1961Ma28) 
$S{-pn}=100 eV {I20}; S{-p|a}=140 eV; S{-p|g}=47 eV {I7} (1968En01) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1738.8 {I8} 
J$(p,|a(|q)) A{-2}=1.002 {I14}, A{-4}=+0.50 {I4}, A{-6}=-0.08 {I6} (1967Bo03) 
S$weighted average of 1738.7 {I18} (1967Bo03) and 1738.8 {I8} (1974Al05). Others: 1739.8 (1952Sc09), 1738 (1966Ka18), 1741 (1961Ma28) 
$S{-p|g}=3.0 eV {I8}; S{-pn}=26 eV {I6}; S{-p|a}=19 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1744.2 {I8} 
S$other: 1745.3 (1952Sc09) 
$|G from (p,n) in 1974Al05; S{-p|g}=13 eV {I4}; S{-pn}=31 eV {I8} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1750.0 {I8} 
S$other: 1950.1 (1952Sc09) 
$|G from (p,n) in 1974Al05; S{-p|g}=1.3 eV {I10}; S{-pn}=70 eV {I30} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1753.2 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1753.7 {I18} (1967Bo03) and 1753.1 {I8} (1974Al05). Other: 1954.5 (1952Sc09), 1753 (1961Ma28) 
$|G from (p,n) in 1974Al05; S{-p|g}=6.3 eV {I19}; S{-pn}=170 eV {I40}; S{-p|a}=240 eV, |G=1.3 eV {I6} in 1967Bo03 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1761.9 {I8} 
S$others: 1963.0 (1952Sc09), 1758 (1961Ma28) 
$S{-p|g}=6.7 eV {I19}; S{-pn}=170 eV {I40} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1771.0 {I8} 
J$|p=natural from {+37}Cl(p,|a) 
S$weighted average of 1771.5 {I18} (1967Bo03) and 1770.9 {I8} (1974Al05). Other: 1767 (1961Ma28) 
$S{-p|g}=15 eV {I4}; S{-pn}=70 eV {I60}; S{-p|a}=20 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1772.5 {I8} 
S$others: 1772.4 (1952Sc09), 1774 (1961Ma28) 
$S{-p|g}=1.3 eV {I9}; S{-pn}<30 eV 
$|G=1.6 keV from 1952Sc09 for E(p)=1772.4 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1777.8 {I8} 
J$(p,|a(|q)): A{-2}=+0.811 {I12}, 1- less likely (1967Bo03) 
S$weighted average of 1778.3 {I18} (1967Bo03) and 1777.7 {I8} (1974Al05). Other: 1777.6 (1952Sc09) 
$S{-p|g}=1.5 eV {I6}; S{-pn}=9 eV {I6}; S{-p|a}=100 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1782.8 {I8} 
S$others: 1783.8 (1952Sc09), 1781 (1961Ma28) 
$S{-p|g}=1.7 eV {I6}; S{-pn}=57 eV {I13} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1787.2 {I19} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)); A{-2}=+1.36 {I20}, A{-4}=+0.31 {I9} and odd terms (1967Bo03) 
S$others: 1788.0 (1952Sc09), 1786 (1961Ma28) 
$S{-p|a}=80 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1804.3 {I19} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)); A{-2}=+0.74 {I4}, A{-4}=+0.53 {I6} (1967Bo03) 
S$others: 1803 (1966Ka18), 1803.7 (1952Sc09) 
$S{-p|a}=34 eV 
$|G<1.0 keV from 1952Sc09 for E(p)=1803.7 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1811.7 {I19} 
J$(p,|a(|q)): A{-2}=+0.807 {I14} (1967Bo03) 
S$others: 1810 (1966Ka18), 1812.9 (1952Sc09) 
$S{-p|a}=80 eV 
$|G=1.6 keV from 1952Sc09 for E(p)=1812.9 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1823.2 {I19} 
J$|p=natural from {+37}Cl(p,|a) 
S$others: 1824 (1961Ma28) 
$S{-p|a}=4.9 eV 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1830.4 {I19} 
S$others: 1834 (1966Ka18), 1831.8 (1952Sc09), 1828 (1961Ma28) 
J$(p,|a(|q)): A{-2}=+0.06 {I3}, A{-4}=-0.11 {I3} (1967Bo03) 
$S{-p|a}=310 eV 
$|G=1.3 keV from 1952Sc09 for E(p)=1831.8, 3.5 keV from 1966Ka18 for E(p)=1834 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=1845.3 {I19} 
J$(p,|a(|q)): A{-2}=-0.53 {I3} (1967Bo03) 
S$other: 1844.8 (1952Sc09) 
$S{-p|a}=70 eV 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1848.8 {I19} 
S$others: 1852 (1966Ka18), 1846.4 (1952Sc09) 
J$(p,|a(|q)): A{-2}=+0.14 {I3} (1967Bo03) 
$S{-p|a}=410 eV 
$|G=2.2 keV from 1952Sc09 for E(p)=1846.4, 8 keV from 1966Ka18 for E(p)=1852 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=1860.6 {I19} 
J$(p,|a(|q)): A{-2}=+0.70 {I1}, A{-4}=-1.64 {I4} (1967Bo03) 
S$other: 1857 (1961Ma28) 
$S{-p|a}=90 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1870.7 {I19} 
J$|p=natural from {+37}Cl(p,|a) 
S$others: 1872 (1961Ma28), 1872.3 (1952Sc09) 
$S{-p|a}=50 eV 
$|G<1 keV from 1952Sc09 for E(p)=1872.3 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1874.9 {I19} 
S$other: 1875.0 (1952Sc09) 
J$|p=natural from {+37}Cl(p,|a) 
$S{-p|a}=80 eV 
$|G<1 keV from 1952Sc09 for E(p)=1875.0 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1878.6 {I19} 
J$|p=natural from {+37}Cl(p,|a) 
S$others: 1880 (1961Ma28), 1880.0 (1952Sc09) 
$S{-p|a}=200 eV 
$|G<1 keV from 1952Sc09 for E(p)=1880.0 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1889.3 {I19} 
S$other: 1890.9 (1952Sc09) 
J$|p=natural from {+37}Cl(p,|a) 
S$other: 1889 (1961Ma28), 1890.9 (1952Sc09) 
$S{-p|a}=17 eV 
$|G=2.3 keV from 1952Sc09 for E(p)=1890.9 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1893.5 {I19} 
J$(p,|a(|q)): A{-2}=+0.954 {I15} (1967Bo03) 
S$others: 1896 (1966Ka18), 1894.7 (1952Sc09) 
$S{-p|a}=42 eV 
$|G=5.6 keV from 1966Ka18 for E(p)=1896 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1905.8 {I19} 
J$(p,|a(|q)): A{-2}=0.00 {I3}, A{-4}=-0.22 {I4} (1967Bo03) 
$S{-p|a}=160 eV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1919.2 {I19} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)); A{-2}=-1.24 {I11}, odd terms (1967Bo03) 
S$other: 1918.3+1920.3 in 1952Sc09 
$S{-p|a}=80 eV 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1926.1 {I19} 
J$(p,|a(|q)): A{-2}=+1.00 {I5} (1967Bo03) 
S$other: 1924 (1961Ma28), 1927.3 (1952Sc09) 
$S{-p|a}=160 eV 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_comment:
$E(p)(lab)=1931.6 {I20} 
J$(p,|a(|q)): A{-2}=+0.81 {I3} (1967Bo03) 
$S{-p|a}=140 eV 
$|G=1.5 keV from 1952Sc09 for E(p)=1933.1 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1936.6 {I20} 
J$(p,|a(|q)): A{-2}=-0.32 {I5} (1967Bo03) 
S$others: 1935 (1961Ma28), 1933.1 (1952Sc09) 
$S{-p|a}=260 eV 
$|G=1.5 keV from 1952Sc09 for E(p)=1933.1 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1945.4 {I20} 
J$(p,|a(|q)): A{-2}=-0.64 {I2} (1967Bo03) 
S$others: 1946 (1961Ma28), 1946.1 (1952Sc09) 
$S{-p|a}=160 eV 
$|G=2.3 keV from 1952Sc09 for E(p)=1946.1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1952.6 {I20} 
J$|p=natural from {+37}Cl(p,|a) 
S$other: 1953.3 (1952Sc09) 
$S{-p|a}=460 eV 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1962.9 {I20} 
J$|p=natural from {+37}Cl(p,|a); (p,|a(|q)); odd terms in p(|q) 
S$other: 1964.2 (1952Sc09) 
$S{-p|a}=90 eV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=1986.1 
S$others: 1987 (1961Ma28), 1983 (1966Ka18) 
$|G=7.8 keV from 1966Ka18 for E(p)=1983 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(lab)=2010.1 
S$others: 2008 (1961Ma28), 2010 (1966Ka18) 
$|G=16 keV from 1966Ka18 for E(p)=2010 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$E(p)(lab)=2088.7 
S$others: 2089 (1961Ma28), 2086 (1966Ka18) 
$|G=3.3 keV from 1966Ka18 for E(p)=2086 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$E(p)(lab)=2104.1 
S$others: 2104 (1961Ma28), 2102 (1966Ka18) 
$|G=3.3 keV from 1966Ka18 for E(p)=2102 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(lab)=2211 
S$from 1974Al05. Others: 2208.6 (1952Sc09), 2210 (1966Ka18), 2207 (1961Ma28) 
$|G=11 keV from 1966Ka18 for E(p)=2210 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(lab)=2302.8 
S$others: 2300 (1961Ma28), 2298 (1966Ka18) 
$|G=3.2 keV from 1966Ka18 for E(p)=2298 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=2393.4 
S$others: 2392 (1961Ma28), 2396 (1966Ka18) 
$|G=16 keV from 1966Ka18 for E(p)=2396 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=2414.8 
S$others: 2412 (1961Ma28), 2414 (1966Ka18) 
$|G=7.8 keV from 1966Ka18 for E(p)=2414 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(lab)=2423.4 
S$others: 2423 (1961Ma28), 2426 (1966Ka18) 
$|G=3.3 keV from 1966Ka18 for E(p)=2426 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_uncertain: ?
level_comment:
$E(p)(lab)=2448.7 
S$others: 2450 (1961Ma28), 2446 (1966Ka18) 
$|G=8 keV from 1966Ka18 for E(p)=2446 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: Y
level_comment:
J$spin from optical hyperfine structure (1967Tr12); parity from L(d,p)=L(p,d)=L(d,t)=L({+3}He,|a)=3 
T$from re-evaluation of T{-1/2}=269 d {I3} relative to T{-1/2}=35.1 d {I1} for {+37}Ar measured in 1965St09, using Adopted T{-1/2}=35.011 d {I19}. Note that currently quoted uncertainty=8 is deduced based on the statement in 1965St09 that the systematic uncertainty is 3%. The same value is also from the re-evaluation by 1990Ho28 using T{-1/2}=35.02 d {I2} for {+37}Ar from 1975Ki10. Other: 265 y {I30} (1952Ze01) 
MOMM1,MOME2$from collinear laser spectroscopy (1996Kl04). Other: |m=-1.3 {I3} (1967Tr12, optical method). Compilations: 2014StZZ, 2016St14 
$Experimental nuclear charge radius <r{+2}>{+1/2}=3.409 fm {I3} (2013An02, evaluation) 
$|D<r{+2}>({+38}Ar,{+39}Ar)=0.04 fm{+-2} {i7} (1996Kl04) 
$ ADOPTED (1977En02) NEUTRON PICK-UP SPECTROSCOPIC FACTOR (^S)=1.2 2 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR (^S)=0.64 12 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$from L(pol d,t)=L(d,p)=L(p,d)=1 and L+1/2 transfer from analyzing powers in (pol d,t) 
T$from |g|g(t) in {+39}Cl |b{+-} decay (1956Pe38) 
$ ADOPTED (1977En02) NEUTRON PICK-UP SPECTROSCOPIC FACTOR (^S)=0.10 2 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR (^S)=0.57 9 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
J$L(pol d,t)=L(d,p)=L(p,d)=L({+3}He,|a)=2 and L-1/2 transfer from analyzing powers in (pol d,t); also L({+3}He,p)=0 from 3/2+ 
T$from |g|g(t) {+39}Cl |b{+-} decay (1956Pe38) 
$ ADOPTED (1977En02) NEUTRON PICK-UP SPECTROSCOPIC FACTOR (^S)=2.0 3 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR (^S)=0.06 3 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$L(d,t)=L(d,p)=L(p,d)=L({+3}He,|a)=0 
$ ADOPTED (1977En02) NEUTRON PICK-UP SPECTROSCOPIC FACTOR (^S)=1.0 4 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR (^S)=0.03 1 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1 ,2433.49|g to 7/2- and RUL. J=1/2 assigned by 1972Se04 in (d,p) based on J-dependence (Lee-Schiffer effect) is inconsistent. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: PS
level_comment:
J$2503.28|g to 7/2-, 1236.19|g to 3/2- and 985.861|g to 3/2+ give (3/2-,5/2); negative parity would lead to unacceptably large M2 strengths for 985.861|g 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=1; J=3/2 from |g(|q) in (|a,n|g). J|p=1/2 proposed in (d,p) based on J-dependence (Lee-Schiffer effect) is inconsistent with anisotropy of 1998.3|g in (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 3379 {I6} from (|a,d), 3379 {I8} from (p,d), 3385 {I10} from ({+3}He,|a) and 3382 {I8} from (d,|a) 
J$L(p,d)=2 


level_energy_unit: KEV
level_spin_parity: (11/2:17/2)+
level_comment:
E$weighted average of 3450 {I6} from (|a,d), 3450 {I8} from (d,|a) and 3440 {I10} from ({+3}He,|a) 
J$L(|a,d)=6 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$weighted average of 3619 {I8} from (d,|a), 3627 {I8} from (p,d) and 3633 {I10} from ({+3}He,|a) 
J$L(p,d)=1 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E$weighted average of 3885 {I8} from (d,|a), 3892 {I8} from (p,d), 3895 {I10} from ({+3}He,|a) and 3887 {I20} from (d,p) 
J$L(p,d)=2; L(d,p)=1,(2); L(pol d,t)=(2,3) and L+1/2 transfer from analyzing powers give 5/2+ or 7/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$weighted average of 4175 {I8} from (d,|a), 4177 {I8} from (p,d), 4178 {I10} from ({+3}He,|a), 4184 {I10} from (|a,d), and 4180 {I20} from (d,p) 
J$L(d,p)=1. {I3}/2- assigned by 1972Se04 in (d,p) based on L=1 and observed J-dependence (Lee-Schiffer effect). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$weighted average of 4252 {I8} from (d,|a), 4257 {I8} from (p,d), 4260 {I10} from ({+3}He,|a), 4250 {I20} from (|a,d), and 4250 {I20} from (d,p) 
J$L(pol d,t)=L(d,p)=L(p,d)=3 and L+1/2 transfer from analyzing powers in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 4466 {I8} from (d,|a), 4476 {I8} from (p,d), 4481 {I10} from ({+3}He,|a). Other: 4475 {I20} from (|a,d) 
J$L(p,d)=2; L(d,t)=(2); (5/2+) preferred from analyzing power in (pol d,t) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$weighted average of 4813 {I8} from (d,|a), 4815 {I8} from (p,d), 4822 {I10} from ({+3}He,|a), 4816 {I10} from (|a,d) 
J$L({+3}He,p)=0 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2+)
level_comment:
E$weighted average of 4904 {I8} from (d,|a), 4914 {I8} from (p,d), 4925 {I15} from ({+3}He,|a), 4916 {I20} from (d,p). Possibly a doublet 
J$possibily a doublet with 1/2-,3/2- for one component and 3/2+,5/2+ for the other. L(d,p)=1 for 4916 {I20}; L(p,d)=2 for 4914 {I8} 


level_energy_unit: KEV
level_spin_parity: (11/2:17/2)+
level_comment:
E$weighted average of 4998 {I10} from (|a,d) and 4987 {I8} from (d,|a); possibly a doublet 
J$L(|a,d)=6 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$weighted average of 4990 {I20} from (d,p), 5006 {I8} from (p,d) and 5008 {I10} from ({+3}He,|a) 
J$L(d,p)=1 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$weighted average of 5169 {I8} from (p,d), 5147 {I10} from (|a,d), and 5149 {I20} from (d,p). 
J$L(d,p)=L(p,d)=3 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$weighted average of 5526 {I10} from ({+3}He,|a), 5527 {I8} from (p,d) and 5508 {I20} from (d,p) 
J$L(d,p)=3 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$1968Fi05 and 1972Se04 assign J=1/2 based on Lee-Schiffer effect, while on the basis of energy matching, this level is considered equivalent to the 3265.6 level in (|a,n|g) where J=3/2 is assigned from |g(|q). 
S$ for J=1/2. Others: 0.95 (1968Fi05), 1.0 (1967Ho02) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$(11/2-) in 1976Wa03 
T$from |t=1.0 ps {I3}, weighted average of 1.1 ps {I3} and 0.9 ps {I3}. Other: <2.8 ps (1976Wa03) 


level_energy_unit: KEV
level_spin_parity: (13/2)+
level_lifetime_unit: PS
level_comment:
J$(13/2+) in 1976Wa03 
T$from |t=1.1 ps {I3}, weighted average of 0.8 ps {I3}, 1.1 ps {I3}, and 1.7 ps {I5}. Other: <2.8 ps (1976Wa03). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$Optical spectroscopy measurements: 1937Ko03, 1953Me73; no hyperfine structure seen 
$Evaluated rms charge radius=3.4274 fm {I26} (2013An02) 
$|D<r{+2}>({+38}Ar-{+40}Ar)=0.169 fm{+2} 33 (1996Kl04), 0.17 fm{+2} (1986Mu06) 
$charge radius <r{+2}>{-1/2}=3.415 fm {I5} (1976Pf01), 3.429 fm {I6} (1971Bb11) from Muonic x-ray data; 3.393 fm {I15}(stat) (1976Fi12), 3.41 fm {I4}, (1971Sc09), 3.47 fm {I5} (1971Gr27,1975GrYY), 3.48 fm {I4} (1974We02) from {+40}Ar(e,e') data. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(t,p)=L(pol d,d')=L(pol p,p')=L(d,{+3}He)=2 
T$weighted average of 1.09 ps {I28} from {+37}Cl(|a,p|g), 1.11 ps {I4} from {+40}Ar(e,e'), 1.35 ps {I10} from {+40}Ar(p,p'|g) and 1.25 ps {I14} from {+12}C({+36}S,2|a|g). 
MOMM1$using transient-field technique (2008Sp04). Others: -2 {I2} (1992Cu04), -0.03 {I8} (2005St22). 
MOME2$from reorientation in Coulomb Excitation (1970Na05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(pol d,d')=L(pol p,p')=2 
T$weighted average of 0.24 ps {I4} from (|a,p|g), 0.194 ps {I35} from (e,e') and 0.34 ps {I6} from (p,p'|g). Others: 0.50 ps {I8} from {+36}S(|a,|g):resonances, 0.47 ps {I7} from {+12}C({+36}S,2|a|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(pol d,d')=L(pol p,p')=4 
T$weighted average of 2.9 ps {I14} from {+26}Mg({+16}O,2p|g), 2.3 ps {I6} from (|a,p|g), 1.80 ps {I28} from {+12}C({+36}S,2|a|g), and 3.0 ps {I+18-9} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(t,p)=L(pol p,p')=2 
T$weighted average of 28 fs {I14} from (|a,p|g) and 35 fs {I7} from (e,e'). Others: 62 fs {I12} from (|a,|g):resonances, <24 fs from (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,d')=L(d,{+3}He)=2 
T$weighted average of 62 fs {I12} from (|a,|g):resonances, 49 fs {I14} from (|a,p|g) and 83 fs {I31} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$3918.6|g E2 to 0+, L(t,p)=L(pol p,p')=2 
T$weighted average of 0.28 ps {I3} from (|a,p|g) and 0.30 ps {I4} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$based on |g(|q,pol) in (|a,p|g) and p|g(|q) in (p,p'|g), log| {Ift}=5.9 from 2- in {+40}Cl |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: FS
level_comment:
J$log| {Ift}=5.1 from 2- in {+40}Cl |b{+-} decay; possible natural parity in (|a,|a'); L(p,p')=(2,3) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(d,{+3}He)=0, L(t,p)=2 
T$weighted average of 15 fs {I6} from {+36}S(|a,|g):resonances and 18 fs {I7} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_comment:
J$2959|g, 1896|g and 1212|g to 2+ gives (0+:4+); natural parity in (|a,|a') for 4420 and/or 4427 levels gives 1-,2+,3-,4+; L(pol d,d')=(2) gives (2+); L(pol p,p')=3 gives 3- 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
J$from |g(|q) in (|a,|g):resoances, (|g,|g') and (|a,p|g) 
T$from (2J+1)|G{-0}{+2}/|G=0.21 eV {I4} with |G{-0}/|G=1 in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: FS
level_comment:
J$2+,3 is given by 1983Bi08 in (|a,p|g) based on |g(|q), but J|p=2+ should be ruled out since it results in |DJ=2 for the 1685|g to 4+, which expects positive A{-2} value while the measured A{-2} by 1983Bi08 is negative. Natural parity in (|a,|a') gives |p=- for J=3 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
J$2078|g and 3141|g to 2+; possible natural parity in (|a,|a') 
T$unweighted average of 73 fs {I12} from (|a,|g):resonances and 33 fs {I14} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
J$based on |g(|q,pol) in (pol |g,|g') and |g(|q) in (|a,p|g); possible |p=natural in (|a,|a') 
T$from (2J+1)|G{-0}{+2}/|G=2.46 eV {I17} with |G{-0}/|G=1 in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_lifetime_unit: PS
level_comment:
J$based on |g(|q,pol) of 765|g in (|a,p|g), which implies a parity conserving transition to 4(-). But the parity is inconsistent with possible natural parity in (|a,|a'), which is |p=+ for J=4. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
J$1650|g to 4+ and 3704.6|g to 2+; natural parity in (|a,|a') favors (2,4)+; L(d,{+3}He)=0 from 3/2+ for a level at 5200 gives 1+,2+; (1,2+) from possible 5165.5|g to 0+ 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_comment:
J$1186.7|g and 1589.0|g to 3- and 2063.0|g to 2+; possible natural parity in (|a,|a'); log| {Ift}=5.9 from 2- in {+40}Cl |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$possible natural parity from (|a,|a'); 1228|g and 1629|g to 3-; L=2 for a level at 5298 {I15} in (t,p) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
J$spin from |g(|q) in (|g,|g'); natural parity in (|a,|a'). L(p,p')=(5) for a level at 5410 is inconsistent and it might imply that it is a different level. 
T$from (2J+1)|G{-0}{+2}/|G=0.09 eV {I2} in (|g,|g') assuming |G{-0}/|G=1 


level_energy_unit: KEV
level_spin_parity: (1,2,3)
level_comment:
J$4147.8|g to 2+; log| {Ift}=6.3 from 2- in {+40}Cl |b{+-} decay; possible natural parity in (|a,|a') for a group near 5608 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
J$log| {Ift}=4.9 from 2- in {+40}Cl |b{+-} decay; spin=1 from |g(|q) in (|g,|g') 
T$from (2J+1)|G{-0}{+2}/|G=0.35 eV {I4} in (|g,|g') assuming |G{-0}/|G=1 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$3784.9|g to 0+; log| {Ift}=5.8 from 2- in {+40}Cl |b{+-} decay; possible natural parity in (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: EV
level_comment:
E$a level at the same energy is also observed in (|a,p|g) but with completely different decay mode and it is considered by evaluator as a separate level. 
T$from (2J+1)|G{-0}{+2}/|G=0.15 eV {I5} in (|g,|g') assuming |G{-0}/|G=1 


level_energy_unit: KEV
level_spin_parity: (7-)
level_comment:
J$from (|a,p|g) based on analog in {+42}Ca, and from |g(DCO) and band assignment in {+26}Mg({+18}O,2p2n|g) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: EV
level_comment:
J$spin from |g(|q) in (|g,|g'); log| {Ift}=5.9 from 2- in {+40}Cl |b{+-} decay. 
T$from (2J+1)|G{-0}{+2}/|G=1.24 eV {I19} in (|g,|g') assuming |G{-0}/|G=1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
E$as quoted in 1976Se09 in (pol d,d'). A level at the same energy is also observed in {+40}Cl |b{+-} decay and (|g,|g') but with J|p=1(-). Therefore it is considered as a separate level. 
J$L(pol d,d')=4 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J$based on |g|g(|q) in (|g,|g') and 6100|g to 0+ 
$|G{-0}=0.22 eV {I6} for J(6100)=1 and 0.13 eV {I4} f0r J(6100)=2 from (2J+1)|G{-0}{+2}/|G=0.17 eV {I5} in (|g,|g') with |G{-0}/|G=0.26 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
J$spin from |g|g(|q) in (|g,|g'); log| {Ift}=5.6 from 2- in {+40}Cl |b{+-} decay 
T$from (2J+1)|G{-0}{+2}/|G=0.87 eV {I10} in (|g,|g') with |G{-0}/|G=1 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
J$spin from |g|g(|q) in (|g,|g'); log| {Ift}=5.6 from 2- in {+40}Cl |b{+-} decay. L(t,p)=(2) is inconsistent 
T$from (2J+1)|G{-0}{+2}/|G=1.29 eV {I16} in (|g,|g') with |G{-0}/|G=1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+)
level_comment:
E$from (|a,p|g). Other: 6801 from {+26}Mg({+18}O,2p2n|g) 
J$from |g(DCO) and band assignment in {+26}Mg({+18}O,2p2n|g); possible analog state of {+42}Ca (1983Bi08) from (|a,p|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8-)
level_comment:
J$from |g(DCO) and band assignment in {+26}Mg({+18}O,2p2n|g); possible analog state of {+42}Ca (1983Bi08) from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$doublet: 9408+9417 in (|a,|g) with same J|p for both; the second component seems to correspond to 9416 in (|g,|g') 
T$from (|g,|g'). 4.0 eV {I20} from {+36}S(|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$doublet:9581+9586 in (|a,|g), 9580+9585 in (|g,|g'); the second component has J|p=(1-,2+) in (|a,|g) 
T$from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$weighted average of 9954 {I3} from (|a,|g), 9950 {I3} from (|g,|g') 
T$from (|g,|g'). |>9.6 eV from {+36}S(|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_uncertain: ?
level_comment:
E$this level is constructed by 1972Kl06 only based on a 1333-keV transition to a level at 4943 which is considered as improbable by 1983Bi08 in (|a,p|g). Therefore, the evaluator has considered this level as questionable as well. 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.10 {I5} 
$E|a(Lab)=2353 
$|G{-|a}/|G{-|g}|<0.11, |G{-|g}|>0.33 eV (1988Cs02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.18 {I3} 
$E|a(Lab)=2584 
$|G{-|a}/|G{-|g}=0.10 {I2}, |G{-|a}=0.07 eV {I2}, |G{-|g}=0.65 eV {I16}, |G{-|g0}=0.65 eV {I17} (1988Cs02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=0.8 {I1} 
$E|a(Lab)=2838 
$|G{-|a}/|G{-|g}=0.63 {I17}, |G{-|a}=0.43 eV {I21}, |G{-|g}=0.69 eV {I23}, |G{-|g0}=0.60 eV {I21} (1988Cs02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$for unresolved 9408+9417 doublet, with E|a=2897 {I4} and 2907 {I4}, and (2J+1)|G{-|a}|G{-|g}/|G=0.5 eV {I1} and 0.8 eV {I1}, respectively. 
$|G{-|a}/|G{-|g}=0.07 {I3}, |G{-|a}=0.10 eV {I5}, |G{-|g}=3.9 eV {I20}, |G{-|g0}=1.4 eV {I7} (1988Cs02). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=3.3 {I4} 
$E|a(Lab)=3004.4 
$|G{-|a}/|G{-|g}=0.19 {I4}, |G{-|a}=1.3 eV {I5}, |G{-|g}=6.9 eV {I17}, |G{-|g0}=6.2 eV {I16} (1988Cs02) 


level_energy_unit: KEV
level_comment:
E$for unresolved 9581+9586 doublet, with E|a=3089 {I3} and 3095 {I7}, and (2J+1)|G{-|a}|G{-|g}/|G=4.6 eV {I7} and 0.9 eV {I4}, respectively. 
J$1- for E|a=3089 component and (1-,2+) for E|a=3095 component 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
E$for unresolved 9687+9694 doublet, with E|a=3207 {I3} and 3215 {I5}, and (2J+1)|G{-|a}|G{-|g}/|G=2.4 eV {I7} and 1.5 eV {I8}, respectively. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$for unresolved 9849+9852 doublet, with E|a=3387 {I3} and 3391 {I5}, and (2J+1)|G{-|a}|G{-|g}/|G=1.9 eV {I2} and 0.7 eV {I3}, respectively. 
$|G{-|a}/|G{-|g}=0.03 {I1}, |G{-|a}=0.65 eV {I29}, |G{-|g}=22 eV {I6}, |G{-|g0}=10 eV {I3} (1988Cs02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=GE
level_comment:
$(2J+1)|G{-|a}|G{-|g}/|G=5.5 {I7} 
$E|a(Lab)=3503 
$|G{-|a}/|G{-|g}=2.9 {I10}, |G{-|a}|>7.1 eV, |G{-|g}|>2.5 eV, |G{-|g0}|>1.7 eV (1988Cs02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.39 ps {I28} (1983Bi08) and 0.83 ps {I26} (1971Ja15). Other: 1.7 ps {I+125-9} (1970Cu02) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.2 ps {I6} (1983Bi08) and 2.9 ps {I14} (1975Wa23). Other: 2.8 ps {I+56-14} (1971Ja15) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
T$weighted average of 0.693 ns {I21} from direct timing p|g(t) (1975Po13) and 0.645 ns {I35} from recoil-distance method (1975Wa23). Others: >2.8 ps (1983Bi08) 


level_energy_unit: KEV
level_spin_parity: 3
level_lifetime_unit: FS
level_comment:
J$2+,3 is given in 1983Bi08, but J|p=2+ results in |DJ=2 for the 1685|g to 4+, which expects positive A{-2} value while the measured A{-2} by 1983Bi08 is negative. 


level_energy_unit: KEV
level_comment:
$|b{-2}=0.242 {I5} or 0.220 {I4} (1985De03), 0.24 {I2} or 0.26 {I2} (1971Ru04), 0.21 (1968Jo14) 
$B(E2)(from g.s.)=0.046 {I8}, 0.0459 {I19}, 0.0448 {I20}, 0.0430 {I10}, 0.0441 {I10}, 0.0447 {I10} (1985De03) 


level_energy_unit: KEV
level_comment:
L$from 1985De03. Other: |<2 (1965Gr11), 1 (1968Jo14) 
$|b{-1}=0.05 for L=1 (1968Jo14) 
$|b{-0}=0.032 {I8} or -0.029 {I8} (1985De03) 
$BE0(from g.s.)=0.000016 110, 0.0045 10, 0.0012 9 (1985De03) 
$B(E2)(from 1460,2+)=0.0046 {I17}, 0.00078 {I14}, 0.00014 {I4} (1985De03) 


level_energy_unit: KEV
level_comment:
L$other: (0),1 (1965Gr11) 
$|b{-2}=0.33 {I3} (1985De03), 0.05 (1968Jo14) 
$B(E2)(from g.s.)=0.0039 {I7}, 0.00350 {I2}, 0.0024 {I2} (1985De03) 
$BE0(from 1460,2+)=0.00029 6, 0.00235 27 (1985De03) 
$B(E2)(from 1460,2+)=0.0011 {I2}, 0.00013 {I11}, 0.00006 {I14} (1985De03) 
$B(E4)(from 1460,2+)=0.0000048 {I12}, 0.000079 {I8}, 0.000047 {I41} (1985De03) 
$B(E2)(from 2120,0+)=0.097 {I9}, 0.23 {I4} (1985De03) 


level_energy_unit: KEV
level_comment:
$|b{-4}=0.107 {I12} or 0.078 {I7} (1985De03), 0.11 (1968Jo14) 
$B(E4)(from g.s.)=0.00113 {I6}, 0.00077 {I11}, 0.00080 {I5} (1985De03) 
$B(E2)(from 1460,2+)=0.024 {I4}, 0.0040 {I1}, 0.0054 {I22}, 0.014 {I4} (1985De03) 
$B(E4)(from 1460,2+)=0.000294 {I13}, 0, 0.00063 {I37}, 0.00005 {I9} (1985De03) 


level_energy_unit: KEV
level_comment:
$|b{-2}=0.07 (1968Jo14) 
$B(E2)(from g.s.)=0.0010 {I3} (1985De03) 
$B(E2)(from 1460,2+)=0.0014 {I5} (1985De03) 
$B(E4)(from 1460,2+)=0.00040 {I34} (1985De03) 


level_energy_unit: KEV
level_comment:
$|b{-3}=0.07 for L=3 (1968Jo14) 
E,L,S$complex structure (1988Bl04), known levels at 3512, 4+ and 3464, 6+ may be included in the peak at 3510. The angular distribution (in 1988Bl04) for 3510 does not agree with that expected for L=2 


level_energy_unit: KEV
level_comment:
$|b{-3}=0.26 {I3} (1985De03,1968Jo14), 0.29 {I2} or 0.31 {I2} (1971Ru04) 
$B(E3)(from g.s.)=0.0150 {I5} (DWBA), 0.0165 {I3} (CC) (1985De03) 
$B(E2)(from 1460,2+)=0.0038 {I10} (1985De03) 
$B(E5)(from 1460,2+)=0.000035 {I17} (1985De03) 


level_energy_unit: KEV
level_comment:
$|b{-2}=0.07 (1968Jo14) 
$B(E2)(from g.s.)=0.0024 {I2} (1985De03) 
$B(E2)(from 1460,2+)=0.0065 {I29} (1985De03) 
$B(E4)(from 1460,2+)=0.00105 {I17} (1985De03) 


level_energy_unit: KEV
level_comment:
E$Two separate levels near this energy in Adopted Levels: one deexcited by 545 and 1333 |g rays, and the other by 1705 and 2768 |g rays. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|b{-2}(CCBA)=+0.182 (1976Se09) 
$|b{-2}=0.22-0.25 (1968Hi09) 
$|b{-2}=+0.17 or -0.20; |b{-4}=+0.10 (1987Nu01) 
$Coupling parameter |b{-02}=0.17 (1987Nu01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$as quoted in 1976Se09. A level at the same energy is observed in {+40}Cl |b{+-} decay and (|g,|g') but with J|p=1(-). Therefore the evaluator have considered them as two separate levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$rounded value from Adopted Levels. 1465 {I24} from 1998Ib01. 
$B(E2)=0.037 {I7} (1998Ib01), 0.032 {I5} (1970Na05), 0.049 {I10} (1965Gu10) 
$g=-0.015 {I42} (2005St22), -0.1 {I1} (1992Cu04) 
MOME2$using the reorientation effect (1970Na05) 
J$from Adopted Levels 


level_energy_unit: KEV
level_comment:
$Integrated=0.58 {I12} 
$spectroscopic factor=0.24 {I9} from PWIA analysis, 0.53 {I9} from DWIA analysis (1976Sh02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$<r{+2}>{+1/2}=3.393 fm {I15}(stat) (1976Fi12), 3.41 fm {I4} (1971Sc09), 3.47 fm {I5} (1971Gr27,1975GrYY), 3.48 fm {I4} (1974We02). Others from Muonic x-ray data: 3.423 {I6} (1971Bb11,1974Da05), 3.415 fm {I5} (1976Pf01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$other: 0.23 ps {I4} from |b{-2} in 1956He83 
$|b{-2}=0.025 {I5} (1956He83) 
$|G{-|g to g.s.}=1.04 eV {I19} (1977Fi09) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E,J$could correspond to the level at 6053.6, J|p=1(-) or the level at 6054 J|p=4+ in Adopted Levels 


level_energy_unit: KEV
level_comment:
E$isoscalar giant quadrupole resonance with FWHM=6900 {I600} from 1979Di03. Other: 17600 {I300} with FWHM=4700 {I300} (1976Yo02) 
L$from 1979Di03 and 1976Yo02. Small admixtures of L=4 and L=0 are not excluded (1979Di03) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$I{-0-i-0}=11.9 {I26} 
$B'(E1)|^(from 1461,2+)<12.0, or B'(M1)|^(from 1461,2+)<1.1 
$B'(E1)|^(from g.s.,0+)=0.50 {I+10-14}, or B'(M1)|^(from g.s.,0+)=0.046 {I+9-12} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MIN
level_comment:
T$Weighted average of 109.64 min {I4} (1990Ab06), 109.32 min {I12} (1986Ru09), 109 min {I2} (1971Ju04), 109.8 min {I12} (1964Pa03), 110 min {I1} (1952Ka44), 109.6 min {I4} (1951Ha78), 109.4 min {I10} (1946Bl28), 110 min {I1} (1936Sn01). Others: 109.31 min (2014Bh09), 103.5 min {I24} (1969Bo11), 111 min {I1} (1956Sc91), 107 min {I3} (1950Br29) 
MOMM1,MOME2$From collinear fast beam laser spectroscopy-accelerated beam. See compilation in 2014StZZ and recommended Q in 2013StZZ 
J$L(pol d,p)=3 and |g from (9/2-) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L(pol d,p)=3 and |g from 1/2- 
T$From advanced time delayed |b|g|g(t) method in {+41}Cl |b- decay (2007Wh01). Others: 410 ps {I30} (1966Fo12), >3.5 ps (1977Sc11) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: NS
level_comment:
T$From advanced time delayed |b|g|g(t) method in {+41}Cl |b- decay (2007Wh01). Others: 340 ps {I20} (1966Fo12), >2.8 ps (1977Sc11). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$from 4.5 ps {I+277-26} from |t=6.5 {I+400-37} (1978Ra13). Other: >2.8 ps (1977Sc11). 
J$L(pol d,p)=2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$From weighted average of 0.44 ps {I6} from |t=0.64 ps {I+9-8} (1977Sc11) and 0.32 ps {I8} from |t=0.46 ps {I12} (1978Ra13). Other: <100 ps (1966Fo12). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E,J$Level seen in (d,p) was only weakly excited and the angular distribution data was only qualitatively reproduced by the DWBA calculations (1975Se13). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
E$Tentative 3279 level in (n,|g) decaying by a 3111|g may correspond to this level. There is also a tentative 3293 level in {+41}Cl |b{+-} 


level_energy_unit: KEV
level_uncertain: S
level_comment:
E$S(n)+E(n)(c.m.). S(n)=6098.9 {I3} (2012Wa38). E(n)(c.m.) is deduced from E(n)(lab) where E(n)(lab)=58 keV {I4}. The 58-keV resonance is probably at 59.309 reported by 1991Wi02 in {+40}Ar(n,n) 
J$(5/2+) suggested by 1974Ke18, but a 59.309 resonance (1991Wi02) is assigned as 1/2- 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J$7/2- proposed by 1975Se13 from vector analyzing power data, which was L=2 or 3 but was considered not well reproduced by the DWBA calculations as the state was only weakly populated. Evaluators assign (5/2-) since |g from 1/2- is seen in {+40}Ar(n,|g) 
S$From 1975Se13 for 5/2. Other: 0.12 (1988EcZY) for 5/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
S$From 1975Se13 for L=1. 
J$Level seen in 1975Se13 was only weakly excited and the angular distribution data was only qualitatively reproduced by the DWBA calculations 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
S$Others: 0.34 {I6} (1975Se13), 0.21 for L=1, J=1/2 (1968Fi05), 0.72 (1971Co15) 
J$1/2- proposed by 1971Co15 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$1/2- (1988EcZY), 3/2- (1975Se13) 
S$For J=1/2 (1988EcZY). Other: 0.32 {I6} for J=3/2, 0.160 {I28} for J=1/2 (1975Se13) 


level_energy_unit: KEV
level_spin_parity: 3/2-,7/2-
level_comment:
L$1 (1961Ka18,1975Se13), 3 (1988EcZY) 
J$3/2 (1975Se13), 7/2 (1988EcZY) 
S$For L=3, J=7/2 (1988EcZY). Other: 0.32 {I6} for J=3/2 (L=1) (1975Se13) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
L,J$L=3, J=5/2 (1975Se13); L=(3,4), J|p=(7/2-,9/2+) (1988EcZY) 
S$For J=5/2 (1975Se13). Others: 0.73 {I14} for J=7/2 (1975Se13), 0.04 for J=7/2 and 0.06 for J=9/2 (1988EcZY) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
J$L(t,p)=0 
$The rms charge radius (<r{+2}>){+1/2}=3.4354 fm {I39} (2013An02 evaluation. 
$d<r{+2}>({+38}Ar,{+42}Ar)=+0.2623 fm{+2} {I12}(stat) {I62}(syst) (2008Bl01, also 2005Bl33, laser spectroscopy). 
T$from 1965St09 (|b-counting). Others: 1964Ho31, 1952Ka44. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=2 
$In a review article by 2008BeZH, Fig. 4 seems to give g factor for the first 2+ states in {+38,40,42}Ar, but from Fig. 3 in 2006Sp01 (reference 18 in 2008BeZH), the isotopes should be {+36,38,40}Ar, instead. It would seem that the x-axis in 2008BeZH is erroneously marked in neutron number. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$L(t,p)=3,4; |g from (6+) supports 4+ 
$ Measured upper limit of branching is <10 for transition to g.s. 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=2, E2(+M3) |g to 2+; L(t,p)=3,4 
$ Measured upper limit of branching is <5 for transition to g.s. (1973Pr10) 


level_energy_unit: KEV
level_spin_parity: (6+)
level_comment:
J$proposed by 2011Sz02 as the members of the 2+, 4+ and 6+ yrast sequence and from comparison with shell model calculations as well. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J,E$L=2 for 4012 level in (t,p) which is considered as associated with 4005.3 level in (t,p|g). It is possible part of this level may also correspond to 4013.6 level populated in |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
J$L(t,p)=(3,4). 
E$possible 4902|g to g.s. from a tentative 4902 level in {+42}Cl |b{+-} may correspond to this level, but |g to 0+ is inconsistent with J|p=(3-,4+) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
T$from |g(t) followed over 13 years (2024Sc06). Value is a lower limit as outgassing of Ar from the sample could not be excluded. Value is weighted average of 5 measurements using {+22}Na, {+60}Co, {+44}Ti lines as a reference. 


level_energy_unit: KEV
level_spin_parity: 5/2(-)
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius=3.4414 fm {I41} (2013An02) 
MOMM1,MOME2$fast beam collinear laser spectroscopy using highly sensitive ion detection of optical resonance. Statistical uncertainty=0.002 and systematic uncertainty of 10% in Q due to electric field gradient and Sternheimer shielding correction are combined in quadrature. 
$ Isotope shift ({+38}Ar,{+43}Ar)=556.7 MHz {I23} (2008Bl01); statistical uncertainty=1.4, systematic uncertainty=1.8 
$Measured mean-square radius (r{+2}{-0})=1.23 fm{+2} {I8} (beam energy=50 MeV/nucleon, 1999Ai02), 1.31 fm{+2} {I7} (beam energy=90 MeV/nucleon, 1999Ai02), 1.23 fm{+2} {I3} (beam energy=70 MeV/nucleon, 1997Li15). The rms charge radius (<r{+2}>){+1/2}=3.4415 fm {I23} from |d<r{+2}>({+38}Ar,{+43}Ar)=+0.221 fm{+2} {I14}(stat) {I66}(syst) (2008Bl01, laser spectroscopy). 
J$from laser spectroscopy in 2008Bl01. Hyperfine structure intervals and relative amplitudes of the resonances firmly establish 5/2. log| {Ift}=6.6 (log| {If{+1u}t}<8.5) to 3/2- and log| {Ift}=6.2 to 5/2+ give 3/2 or 5/2. log| {Ift}=7.8 to 7/2- and log| {Ift}=7.9 to 7/2+ make 3/2 less likely. Model arguments as discussed by 1999Ma89 propose 5/2- or 7/2- from systematics of N=23 and 25 nuclides. Possible configuration= |pd{-3/2}{+-2}|nf{-7/2}{+-3} (1999Ma89). 
T$from 1970Hu11 (|b and |g activity measurements). Other: 5.35 min {I15} (|b decay, 1969Ha03), 6.5 min {I18} (1969La16). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_uncertain: ?
level_comment:
E$this level was proposed only in 2009Mo09 but not confirmed in other measurements. It is probably the same level as the 0+x level. 
J$from theoretical predictions in {+9}Be({+36}S,2p|g) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (11/2-)
level_comment:
J$assignment based on conclusion from 1999Ma89 that this is a negative parity state which is dominated by a configuration with the valence neutrons in the {Ifp} shell and new results from 2006Wi10. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_comment:
J$assignment based on strong 2{++}~#f{-7/2} component of the wave function for the state, similar to that in {+41}Ar 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
L$from |s(|q) and comparison with DWBA calculations 
J$suggested by syst (1999Ma89). 
|b{-2}=0.25 {I3}, assuming E2 excitation. For analysis of (p,p') data, J|p(g.s.)=5/2- was assumed by 1999Ma89 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_uncertain: ?
level_comment:
E$this level is uncertain since it has not been observed and confirmed in other experiments. 
J$from theoretical predictions 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (7/2-)
level_comment:
E$x |? 100 keV predicted. Previous assignment of a 200-keV |g-ray from this level (2009Mo09) was not confirmed in the present work 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (9/2-)
level_comment:
J$assignment based on strong 2{++}({+42}Ar)~#|nf{-7/2} component of the wave function for the state, similar to that in {+41}Ar 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius (<r{+2}>){+1/2}=3.4454 fm {I46} (2013An02) 
$Evaluated change in charge radius |d<r{+2}>({+44}Ar-{+38}Ar)=+0.289 fm{+2} {I9} (2013An02) 
T$from 1970Hu11. Other: 14.0 min {I15} (1969La16). 
$Measured rms charge radius (<r{+2}>){+1/2}=3.4454 fm {I22} from |d<r{+2}>({+44}Ar-{+38}Ar)=+0.289 fm{+2} {I9}(stat) {I81}(syst) (2008Bl01, laser spectroscopy). 


level_energy_unit: KEV
level_spin_parity: (0+)
level_uncertain: ?
level_comment:
E$Shell-model calculations predict a 0+ level at 830 (1976Cr03). But this level is considered as uncertain (by the evaluators) since recent |g-ray studies (1999WiZX,1999Wa21) show the first excited state at 1158 with J|p=2+. If this state exists, a weak 408 keV |g-ray could have missed since it would have an intensity |<10% of the 1158 keV |g-ray. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2,MOME2$from Coulomb Excitation (2009Zi01). Value of quadrupole moment not listed in 2021StZZ, 2016St14 and 2014StZZ evaluations 
J$strong Coulomb excitation from 0+ g.s. 
T$weighted average of 4.1 ps {I14} from RDDS in ({+48}Ca,X|g) and 3.77 ps {I+49-33} deduced from B(E2)|^ measured in Coulomb excitation 
BE2$weighted average of 0.0345 {I41} (1996Sc31) and 0.0378 {I+34-55} (2009Zi01) from Coulomb excitation 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
BE2$from Coulomb Excitation (2009Zi01). 
J$level Coulomb excited from 0+ g.s. 
T$deduced by evaluators from adopted B(E2) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J$strong |g branch to 0+ suggests J=1,2. If the 2610 {I160} level from ({+46}K,pn|g) decaying by a 1500 {I80} |g is the same as the 2746 level in {+44}Cl |b{+-} decay, then J|p=4+ as proposed by 1999Wa21 is less likely by a strong |g to 0+. It is possible that either there are two different levels near this energy or that the 2747|g is incorrectly placed in the decay study. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$E2 matrix element (from g.s.)=+0.194 {I+9-15} (2009Zi01) 
$Diagonal E2 matrix element=-0.11 {I4} (2009Zi01) 
BE2$weighted average of 0.0345 {I41} (1996Sc31) and 0.0378 {I+34-55} (2009Zi01) 
MOME2$deduced from measured B(E2)|^ in 2009Zi01 
J$level Coulomb excited (1996Sc31) 
T$deduced by the evaluators from B(E2) and adopted E|g from the Adopted Gammas 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from B(E2)|^ and adopted E|g and branching ratios from the Adopted Gammas. 
$B(E2)(from 1158,2+ level)=0.068 {I+15-9} (2009Zi01) 
$E2 matrix element (from g.s.)=+0.048 {I4} (2009Zi01) 
$E2 matrix element (from 1158,2+)=+0.58 {I+6-4} (2009Zi01) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$this level is uncertain since the 1780 {I80} |g may be the same as the 1817.7|g from a 2976 level seen in {+44}Cl |b{+-} decay. 
J$(2+) proposed from shell-model calculations 


level_energy_unit: KEV
level_comment:
J$(4+) proposed from shell-model calculations. But a similar level fed in {+44}Cl |b{+-} decay de-excites to 0+ which rules out 4+. See the Adopted Levels, Gammas dataset 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: PS
level_comment:
J$|g to 0+ makes (4+) less likely. It is possible that either the level populated here is different from the one populated in the in-beam |g-ray studies or that the 2747|g should be placed elsewhere 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$unshifted 693|g was observed for all target-to-degrader distances. Taking into account the time range of the plunger setup and the low statistics of the peak a lower limit was extracted 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: S
level_comment:
J J|p=7/2- from shell-model syst, syst of other odd-A Ar, and from comparison of branching ratios and log| {Ift}'s for the decay of {+43}Ar and {+45}Ar discrepant with J|p=1/2,3/2,5/2- from log| {Ift}=7.6 {I2} (log| {If{+1u}t}=9.6 {I2}) to 1/2+ 
T from 1980Hu01. Others: 20.8 s {I5} (1978Pe04) and 21 s {I1} (1974TiZW). See {+45}Ar |b{+-} decay for details. 


