# LEVEL

level_energy_unit: KEV
level_comment:
E$weighted average of 6461 {1} (2000Pi01) and 6461.8 {I10} (1985PuZY). Others: 6450 {I14} (1974Ho28), 6462 {I10} (1983Wa25), 
S$from 1983Wa25 
$ d|s/d|W(max)=1.20 mb/sr {I1} 


level_energy_unit: KEV
level_comment:
E$weighted average of 6583 {I1} (2000Pi01) and 6584.9 {I9} (1985PuZY). Others: 6580 {I14} (1974Ho28), 6587 {I10} (1983Wa25) 
L$other: (2) (1983Wa25) 
$ d|s/d|W(max)=1.80 mb/sr {I2} 


level_energy_unit: KEV
level_comment:
E$others: 6814.4 {I9} (1985PuZY), 6810 {I14} (1974Ho28), 6817 {I10} (1983Wa25) 
L$other: (1) (1983Wa25) 
S$other: 0.20 (1974Ho28) 
$ d|s/d|W(max)=1.420 mb/sr {I14} 


level_energy_unit: KEV
level_comment:
E$from 1985PuZY. Others: 6870 {I14} (1974Ho28), 6886 {I10} (1983Wa25) 
$ d|s/d|W(max)=0.112 mb/sr {I17} 


level_energy_unit: KEV
level_comment:
E$weighted average of 6915.2 {I5} (2000Pi01) and 6916.6 {I9} (1985PuZY). Others: 6900 {I14} (1974Ho28), 6915 {I10} (1983Wa25) 
S$other: 0.09 (1974Ho28) 
$ d|s/d|W(max)=1.35 mb/sr {I14} 


level_energy_unit: KEV
level_comment:
E$from 1985PuZY. Others: 6940 {I14} (1974Ho28), 6949 {I10} (1983Wa25) 
$ d|s/d|W(max)=0.71 mb/sr {I7} 


level_energy_unit: KEV
level_comment:
E$weighted average of 7209 {I2} (2000Pi01), 7205 {I10} (1983Wa25). 
E$7214.9 {I16} (1985PuZY) 
$ d|s/d|W(max)=0.55 mb/sr {I5} 


level_energy_unit: KEV
level_comment:
E$weighted average of 7311 {I2} (2000Pi01), 7310.7 {I14} (1985PuZY), 7290 {I14} (1974Ho28), and 7305 {I10} (1983Wa25) 
$ d|s/d|W(max)=0.39 mb/sr {I4} 


level_energy_unit: KEV
level_comment:
E$weighted average of 7368 {I2} (2000Pi01), 7362 {I2} (1985PuZY), and 7356 {I10} (1983Wa25) 
$ d|s/d|W(max)=0.037 mb/sr {I5} 


level_energy_unit: KEV
level_comment:
E$others: 7439.2 {I12} (1985PuZY), 7420 {I14} (1974Ho28), 7432 {I10} (1983Wa25) 
L$3 from 2000Pi01, while L=2 from 1974Ho28, and (2) from 1983Wa25. In (n,|g),(n,n):resonances, L=2 from R-matrix analysis is reported for a level at E=7438.5 {I8}, which is assumed to the same level as the 7438.3 level here. It is likely there is probably a doublet around this energy. 
S$0.61 for L=3 (2000Pi01), 0.1 for L=2 (1974Ho28) 
$ d|s/d|W(max)=5.00 mb/sr {I25} 


level_energy_unit: KEV
level_comment:
E$weighted average of 7630 {I14} (1974Ho28) and 7648 {I10} (1983Wa25) 
$ d|s/d|W(max)=0.26 mb/sr {I3} 


level_energy_unit: KEV
level_comment:
E$others: 7905.8 {I17} (1985PuZY), 7880 {I14} (1974Ho28), 7899 {I10} (1983Wa25) 
L$other: (1) (1983Wa25) 
S$other: 0.02 (1974Ho28) 
$ d|s/d|W(max)=3.21 mb/sr {I16} 


level_energy_unit: KEV
level_spin_parity: (1/2)
level_lifetime_unit: PS
level_comment:
J$from |g(|q) in 1968Gi04; no unique spin from |g(|q) in 1968We07 
T$from |t=0.76 ps {I17}, weighted average of 0.79 ps {I17} (1970Gr15) and 0.72 ps {I+26-18} (1970Wo03) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$other: (5/2,7/2) from 1968Gi04. Parity from M1+E2 |g to g.s., 3/2+ 
T$from |t=0.82 ps {I21}, weighted average of 0.89 ps {I21} (1970Gr15) and 0.74 ps {I23} (1970Wo03) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$other: (1/2,3/2,5/2) from 1968Gi04. Parity from M1+E2 |g to g.s., 3/2+ 
T$other: <0.21 ps (1970Wo03) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_lifetime_unit: PS
level_comment:
J$other: (3/2,7/2) from 1968Gi04 
T$from |t=0.54 ps {I12}, weighted average of 0.55 ps {I12} (1970Gr15) and 0.50 ps {I+22-26} (1970Wo03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$authors clearly state the 5 MeV peak they see is several unresolved states. 
$B(>)=0.88 {I13} 
$d{+2}|s/d|WdE=2.06 mb/sr MeV for 5 MeV excitation energy 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
$r{-0}{+2}=1.15 fm{+2} {I7} (1999Ai02 in Si({+32}Si,X) at 44.78 MeV/nucleon). Also cross section measured in this work. 
$|d<r{+2}>{+32,28}=0.195 fm {I76} (2024Ko07) 
$R{-ch}=3.153 fm {I12} (2024Ko07) 
T$weighted average (NRM) of 159.4 y {I56} (2015HeZY); 178 y {I10} (1998Ni19); 132 y {I13} (1993Ch10, average of 128 y {I20} and 134 y {I16}); 162 y {I12} (1991Th06); 133 y {I9} (1990Ho27, average of 135 y {I10}, 132 y {I9} and 136 {I13}, uncertainty increased to 9.9 y in NRM); 172 y {I4} (1986Al10, uncertainty increased to 7.5 y in NRM); 108 y {I18} (1980El01, uncertainty increased to 20 y in NRM); and 101 y {I18} (1980Ku11, uncertainty increased to 22 y in NRM). Normalized |h{+2}=4.4, as compared to critical |h{+2}=2.0. Unweighted average is 143 y {I10}, while regular weighted average is 161 y {I7}, with normalized |h{+2}=6.4. The T{-1/2} values from indirect methods, described below, were not used in the averaging procedure because the accumulation rates of {+32}Si in ice cores and sediments are not known well, and the cross sections in reactions are poorly known for determining yields that were used to determine the half-life in the pre-1970 measurements. 
$Direct, specific activity methods for half-life measurement: 1993Ch10: source from implantation of separated projectile ({+40}Ar beam) fragments into an inert collector, decay equilibrium technique, two independent samples. 1991Th06: source produced in {+18}O({+16}O,2p) reaction. {+32}Si/{+31}Si abundance ratio using AMS (accelerator mass spectrometry), and |b scintillation spectrometry. 1990Ho27: source produced in {+37}Cl(p,X) and {+31}P(n,p) reactions. {+32}Si/Si abundance ratio by AMS, and |b spectrometry; three independent samples. 1980Ku11: source from {+30}Si(t,p), AMS technique and |b-scintillation spectrometry. 1980El01: source from Cl(p,X), AMS technique and |b-scintillation spectrometry. 
$Direct decay rate methods for half-life measurement: 2015HeZY: used the same detector system and source as in 1986Al10. Counting for 6000 hours between June 2013 and June 2015. 1986Al10: source from {+30}Si(t,p), |b decay rate measured over four years. 
$Indirect methods (accumulation rates of the naturally occurring {+32}Si in different environments) for T{-1/2}: 178 y {I10} (1998Ni19, measurement of the decrease of activity with depth in an accurately dated varved sediment core from the Kassjon lake, North Sweden, note that this value is close to the values from direct measurements, thus included in averaging); 276 y {I32} (1980De46, natural source from varved core of Gulf of California, later corrected to 217 y {I29} by J.B. Cumming, Radiochem. Radioanaly. Lett. 58, 297 (1983)); 330 y {I40} (1973Cl15, natural source from Greenland ice cores, later corrected to 250 y in 1980De46). 
$Indirect methods (reaction yields, mainly in successive neutron captures in {+30}Si) for T{-1/2}: |?280 y (Jantsch, Kernenergie 10, 89 (1967)); |?500 y (1964Ho31); |? 650 y (1962Ge16); |? 42 y (1957Ro59, 600 y/barn for {+31}Si(n,|g) reaction, and |s=0.07 for E=thermal); |?60 y (1954Tu02); |?710 y (1953Li21). 
$See 1991Ku26 for a review of {+32}Si half-life measurements, 2009Se07 for discussion of possible oscillations in exponential decay of {+32}Si in the measurement by 1986Al10; and 2010Ja03 and 2010St07 for power-spectrum analyses and discussion of variation of decay constant from solar influence. Using the BNL counting system and the {+32}Si and {+36}Cl sources (as used by 1986Al10), 2018Fi04 investigated correlation between the two decays in a 5-hour time interval immediately following the GW170817 binary neutron star inspiral on August 17, 2017; claiming observation of a correlation of the two decay rated on August 17, 2017, with an upward fluctuation peaking at 93 min following the arrival of the gravity wave detected by the LIGO apparatus (2017Ab06). See also 2021Ve11 for separation and purification of non-carrier-added source of {+32}S in preparation for a precise re-determination of {+32}Si half-life. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$1941.4|g E2 to 0+; L(t,p)=2. 
T$unweighted average of 0.33 ps {I5} (1974Gu11), 0.64 ps {I22} (1972Pr18) from DSAM in (t,p|g), 0.54 ps {I8} from ({+22}Ne,2p|g), and 0.76 ps {I+13-10} from adopted B(E2)|^=0.0135 {I20} from Coulomb excitation 
BE2$weighted average of 0.0113 {I33} (1998Ib01) and 0.0143 {I20} (2024He01) in Coulomb excitation 
MOME2$from Coulomb excitation (2024He01) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$proposed by 1982Fo02 in (t,p) based on shell-model prediction and possible unnatural-parity state 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$spin=3 from p|g(|q) in (t,p|g); L(t,p)=3 from 0+ 
T$weighted average of 180 fs {I62} from ({+22}Ne,2p|g) and 128 fs {I28} from (t,p|g), both by DSAM 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$see comment for 5427 level. 
J$spin 1 from p|g(|q) and natural parity suggested from relative excitation in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$this level from (t,p) is considered different from the 5412 level in (t,p|g), as the spin assignments in (t,p) and (t,p|g) are different. 
J$L(t,p)=2 from 0+. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J$3563.8|g E3, |DJ=3 to 2+ 
J$5- or 4+ from L(t,p)=5,4 with some preference for L=5, as in (t,p), 1982Fo02 support 5- on the basis that observed cross section is three times as large as predicted for a 4+ state from theoretical calculations. 
T$from 3563|g(t) in ({+22}Ne,2p|g) (2023Wi06). Other: 33.4 ns {I5} (2002AsZY) 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: NS
level_uncertain: ?
level_comment:
E$level proposed by 1997Fo01 (also 1998Fo07) in {+208}Pb({+37}Cl,X). But 2002AsZY using {+198}Pt({+37}Cl,X) at 9 MeV/nucleon did not confirm this level since they did not observe a 79-keV |g ray. It is not confirmed in ({+22}Ne,2p|g) by 2023Wi06 
J$assigned in 1997Fo01, from systematics of (5-) to (4+) transitions in N=18 isotones, e.g., {+34}S and {+36}Ar 
T$from |g(t) in {+208}Pb({+37}Cl,X) (1997Fo01). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: FS
level_comment:
J$3831|g D+Q to 2+; (3-) from shell-model predictions in ({+22}Ne,2p|g) 
T$from DSAM in ({+22}Ne,2p|g). Other: <139 fs from DSAM in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: (0,1,2)+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GE
level_comment:
J$allowed |b feeding (log| {Ift}=4.8) from 1+ parent. One component of a doublet at 5786 {I6} with L(t,p)=(0) could correspond this level and the other component could correspond to 5773 level. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E$possible doublet in (p,t) (1982Fo02). 
J$tentatively proposed by 1980Fo02 in (t,p) based on theoretical predictions 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$this level in (p,t) is considered different from the 5954 in (t,p|g), as the spins from the two studies are different. 
J$L(t,p)=3 from 0+. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
E,J$6208 {I9} with L=1+2 in (t,p) is a doublet, with L=1 component corresponding to the 6196, J=1 level in (t,p|g) and L=2 component possibly corresponding to the 6170 level in (t,p|g). Spin=1 from p|g(|q) in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: S
level_comment:
E$this value is in disagreement with S(n)=9200.0 {I3} in 2021Wa16. 
J$s-wave capture in 3/2+ g.s. of {+31}S. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$weighted average of 1941.4 {I3} (1974Gu11) and 1942.5 {I20} (1972Pr18) 
T$weighted average of 0.64 ps {I22} (1972Pr18) and 0.33 ps {I5} (1974Gu11) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$weighted average of 4230 {I4} (1974Gu11) and 4234 {I4} (1972Pr18) 
J$2 in 1974Gu11 and 1972Pr18 based on p|g(|q); parity from 2289|g M1+E2 to 2+ level 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LE
level_comment:
E$weighted average of 4982 {I4} (1974Gu11) and 4985 {I4} (1972Pr18) 
J$other: (0,1,2) in 1972Pr18. 0+ in Adopted Levels 
$I|g<4 relative to 100 for 3041 for E|g=4982 in 1974Gu11, consistent with expected nonobservation of E0 transition as a |g ray. 


level_energy_unit: KEV
level_spin_parity: (1:4)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 5220 {I3} (1974Gu11) and 5222 {I7} (1972Pr18) 
J$other: >1 in 1972Pr18. (1+) in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 3(-)
level_lifetime_unit: FS
level_comment:
E$weighted average of 5288.8 {I8} (1974Gu11) and 5290 {I3} (1972Pr18) 
J$other: 3 in 1972Pr18. 3- in Adopted Levels 
T$weighted average of 118 fs {I28} (1974Gu11) and 187 fs {I69} (1972Pr18) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 5412.4 {I9} (1974Gu11) and 5413 {I3} (1972Pr18) 
J$other: 1 in 1972Pr18 
T$<49 fs (1974Gu11), |<51 fs (1972Pr18) 


level_energy_unit: KEV
level_spin_parity: (1,2,3)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 5774 {I4} (1974Gu11) and 5772 {I3} (1972Pr18) 
T$<139 fs (1974Gu11 and 1972Pr18) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
E$weighted average of 5953 {I3} (1974Gu11) and 5956 {I3} (1972Pr18) 
J$2+ in Adopted Levels 
T$other: <69 fs (1974Gu11) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 6391 {I5} (1974Gu11) and 6385 {I5} (1972Pr18) 
J$2+ in Adopted Levels 
T$other: |<50 fs (1972Pr18) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Cross section=22 mb {I6} (1998Ib01) 
$<0+||E2||2+>=0.120 eb {I8} (2024He01) 
$<2+||E2||2+>=0.14 eb {I13} (2024He01) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<3778 {I7} from Q(|b{+-})({+32}Al)-S(n)({+32}Si), where Q(|b{+-})=12978 {I7} and S(n)=9200.0 {I3} from 2021Wa16. This represents a range of unobserved levels that subsequently decay to {+31}Al via one-neutron emission. 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: NS
level_comment:
J$3562.8|g E3, |DJ=3 to 2+ 
T$from 3562.84|g(t) of TIGRESS-CsI timing distribution (2023Wi06). Other: 30.5 ns {I28} from |g|g(t) using 842.1|g and 3562.84|g. The authors of 2023Wi06 stated that the large uncertainty in |g|g(t) is due to the lower statistics. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: S
level_comment:
E$this value is in disagreement with S(n)=9200.0 {I3} in 2021Wa16 
J$s-wave capture in 3/2+ g.s. of {+31}S 


level_energy_unit: KEV
level_comment:
J$(4+) assigned by 1997Fo01, but 2002AsZY assign (5-) 
T$2002AsZY assign isomer of T{-1/2}=33.4 ns {I5} to this state. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
E$level proposed by 1997Fo01 (also 1998Fo07). But 2002AsZY using {+198}Pt({+37}Cl,X) at 9 MeV/nucleon did not confirm this level since they did not observe 79-keV |g ray 
J$(5-) assigned by 1997Fo01, based on systematics of (5-) to (4+) transitions in N=18 isotones ({+34}S and {+36}Ar), but 2002AsZY assign 5- to 5502 level 
T$from |g(t) in 1997Fo01. 2002AsZY report an isomer with T{-1/2}=33.1 ns {I5} but assign this isomer to 5502 state (33.4 ns {I5} from Fig.1 of 2002AsZY) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: S
level_comment:
J$L(d,p)=L({+9}Be({+34}Si,{+33}Si))=2 from 0+ 
T$from |g-multi-scaling (1973Go33). Other: 6.3 s {I3} (1972Go09, same group as 1973Go33). 
MOMM1$from g-factor=0.803 {I21} (preliminary value from NMR of nuclei polarized by optical pumping with |b-asymmetry detection) (1992Sh31, 1992Ma52; also 1992MaZS, 1992Sh23, 1992ShZL). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$1724|g to 7/2-; 9/2- from shell-model predictions (2010Wa20,2020Jo06). Other: L(d,p)=(3) giving (5/2-,7/2-) for a group at 3190 {I20} is in disagreement, which may indicate a separate level. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$L(d,p)=1 from 0+. 2024Ch33 state that the sum-rule analysis strongly supports 1/2- since it almost exhausts the full 1p{-1/2} orbital single-particle strength 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$L({+9}Be({+34}Si,{+33}Si))=(2) from 0+ (2020Jo06) 
$B(E2)|^=0.0069 {I13} for a level at 4300 in Coulomb excitation (2000Pr09) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$L({+9}Be({+34}Si,{+33}Si))=(2) from 0+ (2020Jo06). Other: L(d,p)=(3) in {+2}H({+32}Si,p) giving (5/2-,7/2-) for a group at 5430 {I40} (2024Ch33) is in disagreement, which may indicate a separate level 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$From 2020Jo06 
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$b{-f}=9.0% {I54}, |s{-exp}=10.4 mb {I62} 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$b{-f}=1.7% {I3}, |s{-exp}=2.0 mb {I3} 
$|s=4.9 mb {I7}, C{+2}S=1.3 {I4} for a level at E=4290 {I140}, L=2 (2002En02) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$This state is probably populated by |g rays from higher levels, since |b feeding involving |DJ=2, |D|p=no is expected to be negligible. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$x<7509 {I7} from Q(|b{+-})({+33}Al)-S(n)({+33}Si), where Q(|b{+-})=12017 {I7} and S(n)=4508.0 {I8} from 2021Wa16. This represents a range of unobserved levels that subsequently decay to {+32}Si via one-neutron emission 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$the authors state that the sum-rule analysis strongly supports 1/2- since it almost exhausts the full 1p{-1/2} orbital single-particle strength 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$Measured r{+2}{-0}=1.23 fm{+2} {I4} (2006Kh08) in Si({+34}Si,X) reaction at 51.5 MeV/nucleon and 58.9 MeV/nucleon. Integral cross sections were also measured. 
$r{-0}{+2} (strong absorption)=1.20 fm{+2} {I8} (1999Ai02) 
T$from 1977Na05. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$level excited in Coulomb excitation, inelastic scattering, systematics, and shell-model predictions 
T$from B(E2)=0.0085 {I33} in Coul. ex. (1998Ib01) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$level excited in inelastic scattering, possible allowed |b decay from (4-), systematics, and shell-model predictions 
T$estimated from |b|g(t) (1989Ba50) in {+34}Al |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Measured angular distribution compared with theoretical predictions for |DL=0 transition ({+7}Li({+34}P,{+7}Be|g)) 
$Deduced B(>)=0.74 {I18}(stat) +00-14(syst) ({+7}Li({+34}P,{+7}Be|g)) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$2001Nu01 proposed that 1193.3|g possibly populates excited 0+ state at 2133 keV. 2002En02 in {+9}Be({+35}Si,{+34}SiX|g) reaction reported an 1193|g from 3327 level with a branching of about 13%, but 2002Mi44 set an upper limit of 1% for such a transition in their Si({+34}Si,{+34}Si'|g) reaction study. 2003Iw02 observed 1193|g in coin with 3326|g, thus negating the placement of 1193 transition in parallel with 3326 transition as well as the existence of an excited 0+ level at 2133 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Measured angular distribution compared with theoretical predictions for |DL=0 transition 
$Deduced B(>)=0.74 {I18}(stat) +00-14(syst) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$An upper limit of 1% was set for an hypothetical transition from 3330, 2+ to a first excited 0+ at 2133 keV proposed in 2002En02 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
T$ from time difference between |b ray in one of the Si{-tel} and a pair detected in another. (2012Ro25) $ |b=0.29 {I4} 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: S
level_comment:
MOMM1$ using |b-NMR on a polarized fragment beam (2007Ne14). 
J$(d,p)=3 in {+2}H({+34}Si,p|g), 7/2- from shell-model predictions, and systematic trends in Si isotopes. 
T$from |b-decay measurement (1988DuZT). In an earlier paper by the same group (1986Du07) value given is 0.87 s {I17}. The evaluators adopt the more recent value 
$Mean square absorption radius=1.261 fm{+2} {I35} from 2006Kh08 in Si({+35}Mg,X) reaction at E=33.79 and 38.79 MeV/nucleon, also measured energy-integrated cross sections, |s{-R}=2.53 b {I8}. Other: r{+2}{-0}=1.26 fm{+2} {I9}, |s{-R}=2.46 b {I18} at E=68.81 MeV/nucleon (1999Ai02) 
$Configuration=|nf{-7/2} 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1 in {+2}H({+34}Si,p|g), 3/2- from shell-model predictions, and systematic trends in Si isotopes. 
T$from analysis of broadened lineshape in {+9}Be({+36}Si,{+35}Si|g) (2014St18) 
$Configuration=|np{-3/2} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_uncertain: ?
level_comment:
E,J$corresponding to a possible IAR in {+35}P with L(p)=0 from R-Matrix analysis in {+1}H({+34}Si,p):From IAR (2012Im01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$corresponding to an IAR in {+35}P with L(p)=2 and J=5/2+ from R-Matrix analysis in {+1}H({+34}Si,p):From IAR (2012Im01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-,3/2-)
level_uncertain: ?
level_comment:
E,J$corresponding to a possible IAR in {+35}P with L(p)=1 from R-Matrix analysis in {+1}H({+34}Si,p):From IAR (2012Im01) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$IAR resonance energy in {+35}P: E{-R}(c.m.)=3006 {I2}, corresponding to IAR state in {+35}P at 15196 {I14} (2012Im01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
E$984 {I36} from IAR resonance energy in {+35}P: E{-R}(c.m.)=3990 {I36}, corresponding to IAR state in {+35}P at 16180 {I39} (2012Im01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
E$803 {I18} from IAR resonance energy in {+35}P: E{-R}(c.m.)=3809 {I18}, corresponding to IAR state in {+35}P at 15999 {I23} (2012Im01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_uncertain: ?
level_comment:
E$rounded value of 1444 {I44} from IAR resonance energy in {+35}P: E{-R}(c.m.)=4450 {I44}, corresponding to possible IAR state in {+35}P at 16640 {I46} (2012Im01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
E$2093 {I12} from IAR resonance energy in {+35}P: E{-R}(c.m.)=5099 {I12}, corresponding to IAR state in {+35}P at 17289 {I18} (2012Im01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-,3/2-)
level_uncertain: ?
level_comment:
E$rounded value of 2194 {I15} from IAR resonance energy in {+35}P: E{-R}(c.m.)=5200 {I15}, corresponding to possible IAR state in {+35}P at 17390 {I21} (2012Im01) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$from 1033|g+910|g. 2060 {I50} from proton spectrum (2014Bu01) 
J$large spectroscopic factor discards 3/2- component 
$Configuration=p{-1/2} orbital 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 5/2-
level_comment:
$S$from text on p4 in 2014Bu01; uncertainty is listed as 0.02 in text on 3 and 0.04 in authors' Fig. 2 
$Configuration=f{-5/2} orbital 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$Total knockout |s=81 mb {I2}. 
$Partial knockout |s=52 mb {I4}. 
$One-neutron knockout |s=23 mb {I6} (2015St06) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: PS
level_comment:
T$from analysis of broadened lineshape (2014St18) 
$Partial knockout |s=8 mb {I3} (2014St18,2015St06) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
%|b{+-}n: from 1988Mu08. Calculated %|b{+-}n=80.6 (1997Mo25). Other: 1995ReZZ 
T$from 1986Du07 (and private communication to P.M. Endt). 
$ Mean radius r{-0}{+2}=1.216 fm{+2} {I22} from measured integrated |s{-R}=2.59 b {I8} at 52.56 MeV/nucleon and 2.44 b {I6} at 45.87 MeV/nucleon in Si({+36}Si,X) reaction (2006Kh08) 
$ Mean radius r{-0}{+2}=1.25 fm{+2} {I11} from measured integrated |s{-R}=2.48 b {I21} at 65.88 MeV/nucleon in Si({+36}Si,X) reaction (1999Ai02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$ Feeding-corrected excitation cross-section=7.3 mb {I25} 
$ |b{-2}(p,p')=0.24 {I4} (Vibrational), 0.23 {I+3-4} (prolate), 0.28 {I+4-5} (oblate). Sign of |b{-2} is not given 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
$Theoretical %|b{+-}n=18.8, %|b{+-}2n=0.24 (1997Mo25) 
T$from 1995ReZZ. Other: 1999YoZW 
J$7/2- proposed from syst by 2012Au07, 3/2- proposed in calculations of 1997Mo25 
$|s{-R}=2.44 b {I7} at 49.75 MeV/nucleon, 2.52 b {I7} at 43.40 MeV/nucleon (2006Kh08). 
$Average r{-0}{+2}=1.192 fm{+2} {I25} (2006Kh08) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E$from {+37}Al |b{+-} decay (2013StZY), level energy not resolved in {+9}Be({+38}Si,{+37}Si|g) (2014St18) 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: PS
level_comment:
T$deduced by evaluators from measured B(E2) in Coulomb excitation (1999Ib01) and |g-ray branching ratios 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: NS
level_comment:
T$from analysis of broadened lineshape (2014St18) 
$Partial knockout |s=9 mb {I7} (2014St18,2015St06) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from fit to measured decay curve (2017Tr02). Others: |?100 ms (1999YoZW,tentative result) 
$Calculated T{-1/2}: 90 ms (syst,2017Au03), 168 ms (2003Mo09), 49 ms (calc,2012Ch48), 266 ms (2016Ma12) 
$%|b{+-}n: from 100-(summed |b feeding to the bound levels in {+38}P) (2017Tr02). Other: %|b{+-}n=38 {I7} (1999YoZW, tentative result) 
$Calculated %|b{+-}n=36 (2003Mo09), %|b{+-}n=9.8 (2016Ma12) 
$Authors of 1999YoZW advised by e-mail that their results are preliminary and should not be adopted 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$Coulomb excited from 0+, syst of even-even nuclides 
T$deduced from B(E2)|^ by the evaluator. 
$B(E2)|^ from Coulomb excitation (1998Ib01) 
$|b{-2} from {+1}H({+38}Si,{+38}Si'|g) (2007Ca35), deduced for vibrational model. Others: 0.34 {I+2-3} (prolate rotational model), 0.38 {I3} (oblate rotational model). Sign of |b{-2} is not given in 2007Ca35. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$from Adopted Levels based on Coulomb excitation from 0+; (2+) from from shell-model predictions (2015St14) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
J$from Adopted Levels. 
$Feeding-corrected excitation cross-section=15.4 mb {I23} 
$|b{-2}(p,p')=0.35 {I+2-3} (vibrational), 0.34 {I+2-3} (prolate), 0.38 {I3} (oblate). Sign of |b{-2} is not given in 2007Ca35. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
J$this level is tentatively assigned by 2012Ta20 based on |g|g-coin as the first 4+ state predicted by shell-model calculations. The resulting energy ratio between the first 4+ and 2+ states is R{-4/2}=2.09 {I5} (2012Ta20). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J$from shell-model prediction (1997Mo25,2014St18) and systematics of neighboring nuclei (2017Au03) 
T$from 2004Gr20, obtained in a beam-on mode where the implanted ions are registered continuously with the decaying betas. Others: 33.0 ms {I10} (2003Gr22), 40 ms (1999YoZW), >1 |ms from 1990AuZZ. 
$%|b{+-}n=60 {I13} (tentative result, 1999YoZW) 
$Theoretical %|b{+-}n=27.1, %|b{+-}2n=2.4 (2003Mo09) 
$|s{-R}=2.23 b {I12} at 44.75 MeV/nucleon, 2.62 b {I18} at 38.99 MeV/nucleon (2006Kh08). 
$Average r{-0}{+2}=1.109 fm{+2} {I48} (2006Kh08) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
T$from maximum likelihood fit to the decaying 172-keV |g ray (2015St06), uncertainty is statistical only. Other: 0.90 ns {I14} from broadened lineshape (2014St18) in ({+40}Si,{+39}Si|g) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
T$from maximum likelihood fit to the decaying 172-keV |g ray (2015St06), uncertainty is statistical only. Other: 0.90 ns {I14} from broadened lineshape (2014St18) 
$Partial knockout |s=49 mb {I7} (2014St18,2015St06) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_uncertain: ?
level_comment:
E$tentatively proposed by 2014St18 based on comparison with shell-model predictions 
$Partial knockout |s=14 mb {I2} (2015St06) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: MS
level_comment:
J$From shell-model calculations 
T$From implant-|b(t) (2019Ab06). Other: 39.2 ms {I31} from 355|g(t) (2019Ab06). 
%B-N$from measurement of |b decay of {+38}P to {+38}Si and using known absolute branching ratios of |g rays in {+38}P decay. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n=53 {I12} (preliminary value from 1999YoZW) 
$Theoretical %|b{+-}n=48.7, %|b{+-}2n=0.04 (2003Mo09) 
T$from 2004Gr20 (also 2003Gr22,2004Gr28). Calculated T{-1/2}(|b{+-} decay)=30.6 ms (2003Mo09) 


level_energy_unit: KEV
level_spin_parity: (0+,2+,4+)
level_uncertain: ?
level_comment:
E$1614 {I14} from 2012Ta20 in C({+44}S,{+40}Si|a|g) 
J$predicted by shell-model calculations (2012Ta20) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
E$this level is tentatively assigned by 2012Ta20 in C({+44}S,{+40}Si|a|g) based on |g|g-coin as the first 4+ state predicted by shell-model calculations. The resulting energy ratio between the first 4+ and 2+ states is R{-4/2}=2.56 {I5}. Another possible candidate for the first 4+ state is 1614 keV from the 629|g -> 985|g cascade (2012Ta20) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$feeding-corrected excitation cross-section=20.2 mb {I+21-47} (2007Ca35) 
$|b{-2}(p,p')=0.37 {I+2-5} (Vibrational), 0.35 {I+2-4} (prolate), 0.39 {I+2-5} (oblate). Sign of |b{-2} is not given (2007Ca35) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
E$this level is tentatively assigned by authors based on |g|g-coin as the first 4+ state predicted by shell-model calculations. Resulting energy ratio between the first 4+ and 2+ states is R{-4/2}=2.56 {I5}. Another possible candidate for the first 4+ state is 1614 keV from the 629|g -> 985|g cascade (2012Ta20) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$measured by 2017Tr02, from decay curve of |b-implant correlations in coincidence with strongest |g transitions. The decay curve was fitted using Bateman equations by including the decay of the initial implants, decays of the daughter and the |b{+-}n daughter, together with exponential background. Without the |g-coincidence requirement, half-life=27 ms {I1}. This value can be compared with 33.0 ms {I10} from 2004Gr20: Phys. Lett. B594, 252. 
$%|b{+-}n: from 100-(summed |b feeding to the bound levels in {+40}P) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from implant-|b(t) (2004Gr20). Other: 15 ms {I5} (preliminary value from implant-|b(t) in 1999YoZW, read off graph in Figure 1 by evaluators). 
J$7/2- proposed from systematics (2012Au07), 3/2- from shell model calculations (2011Ka03). 
%B-N$preliminary result of 103 {I43} is given in 1999YoZW; a value greater than 100% indicates multiple neutron emission events were observed. As authors state their %|b-n values are tentatively deduced, the value is not adopted here. Theoretical calculations give %|b{+-}n=45 (2003Mo09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|b{+-}n=103 {I48} (1999YoZW, preliminary result). 
$Theoretical T{-1/2}=43.4 ms, %|b{+-}n=40.4, %|b{+-}2n=4.4 (2003Mo09) 
$Theoretical T{-1/2}=29.5 ms, %|b{+-}n=31.5, %|b{+-}2n=11.5 (2016Ma12) 
T$from |b({+42}Si) time correlations followed over 400 ms (2004Gr20). Other: 20 ms {I10} (1999YoZW, preliminary result) 
$See also comment for (2+) state 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$Low energy of 2+ state and comparison of measured half-life with QRPA calculations (2004Gr20) suggest that {+42}Si is deformed and that there is collapse of N=28 closed shell at Z=14. But the small production cross section of {+42}Si in both studies (2006Fr13 and 2006GrZZ) suggest closed shell nature of {+42}Si. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ Low energy of 2+ state and comparison of measured half-life with QRPA calculations (2004Gr20) suggest that {+42}Si is deformed and that there is collapse of N=28 closed shell at Z=14. But the small production cross section of {+42}Si in both studies (2006Fr13 and 2007Ba47) suggest closed shell nature of {+42}Si. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
E$this level is tentatively assigned by 2012Ta20 based on |g|g-coin as the first 4+ state predicted by shell-model calculations. The resulting energy ratio between the first 4+ and 2+ states (R{-4/2})=2.93 {I5} is close to the rigid-rotor limit, which contradicts the possibility of a doubly closed structure suggested by the two magic numbers Z=14 and N=28 but supports enhanced quadrupole collectivity. Furthermore, large R{-4/2} value indicates a significant static ground state deformation of {+42}Si (2012Ta20) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from fit to decay curve with function that included decay of parent, exponential growth and decay of daughters (including |bn and |b2n branches) and a constant background (2022Cr03). Reported as 15.5 ms {I4} (stat) {I16} (syst). 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$Four events were assigned to {+43}Si by 2002No11. Production |s=5 pb {I2} (2007Ta15) 
E$the observed {+43}Si fragments are assumed to correspond to the g.s. 
T$limiting value from time-of-flight in 2002No11. Actual half-life is expected to be much longer as suggested by systematics value of 15 ms (2012Au07) and calculated value of 13.5 ms (1997Mo25) 
J$systematics: 3/2- (2012Au07,1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from fit to decay curve with function that included decay of parent, exponential growth and decay of daughters (including |bn and |b2n branches) and a constant background (2022Cr03). Reported as 13 ms {I4} (stat) {I2} (syst). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ Allowed decay mode is |b{+-} followed by delayed-neutron emission, thus 100% |b{+-} decay mode is assigned by inference. 
$ Theoretical T{-1/2}=10.6 ms, %|b{+-}n=79, %|b{+-}2n=13, %|b{+-}3n=1, %|b{+-}4n=0 (2019Mo01) 
$ Theoretical T{-1/2}=12.6 ms, %|b{+-}n=30.1; %|b{+-}2n=9.16, 9.35; %|b{+-}3n=1.53, 1.33; %|b{+-}4n=0.002; %|b{+-}5n=0 (2021Mi17); two values for different fission barriers. 
$Production cross section=7|*10{+-10} mb {I5} (2007Ta15) 
T$ half-life of {+44}Si has not been measured, but expected to be >360 ns from estimated from time-of-flight of 363 ns, as stated by 2005St29 (Ref. 13 in 2007Ta15) at NSCL facility. Actual half-life is expected to be much longer. From trend of decreasing half-life with increasing neutron number in neutron-rich nuclei, expected half-life is <12 ms from known half-lives of 12.5 ms for {+42}Si, 20 ms for {+41}Si, 31 ms for {+40}Si and 41 ms for {+39}Si. Other: 4 ms (syst, 2021Ko07) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
T$ estimated from flight time of 314-322 ns, Poisson statistics of the observed distribution (2011Fo08) of one to four events. At 98% confidence level, T{-1/2}<50 ns. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: MS
level_comment:
J$log| {Ift}=4.9 to 2+; |e to (3+) and (4+) levels in {+26}Si; isobaric analogue of T=2, 13015, (3+) state in {+26}Si 
T$from 2004Th09, time correlations of {+26}P ions and |b or |b-2p decay events). Other: 20 ms {I+35-15} (1984Ca29, 1983Ca06, 1983Ho23, 1984CaZV thesis) 
$Total branch for the proton-unbound levels is measured as 39% {I2}; and %|e2p is measured as 2.16 {I24} (2004Th09); from which %|ep=36.8 {I20}. Other measurement: %|ep branch to T=2 analogue state |?1.9% (1984Ca29, 1983Ca06, 1984CaZV thesis); who also estimated 2p/1p ratio for the decay of IAS as |?1 to within 50% (2p/1p|?1.5 within a factor of two in 1983Ho23). Corresponding |ep branch in 2004Th09 is 5.3% {I4}, and 2p/1p=0.69 {I9}. 
$Delayed |e|a decay branch is energetically possible and was searched in experiments by 1984Ca29 and 2004Th09, but no evidence was found. 
$ Theoretical calculation of |ep and |e2p probabilities: 1991De26 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: MS
level_comment:
$%|e+%|b+=100; %|ep=33.5 {I20}; %|e2p=1.5 {I4}; %|ep+%|e2p=35 {I2} 
J$From {+26}P Adopted Levels in the ENSDF database. 
T$Measured by 2017Ja05 from 477 {+26}P implant-p(t) analysis by maximum likelihood method. 
$%|e2p and %|ep+%|e2p values from 2017Ja05. %|ep by compiler - subtracted value of %|e2p from %|ep+%|e2p. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_comment:
E$From E|g, assuming g.s. feeding by the compiler. 
T$Deduced by fitting 164|g(t) using maximum likelihood method (2017Pe04). 
$An isomeric ratio R, probability of {+26}P production in an isomeric state, 14% {I10} (2017Pe09). This value is much lower than 97% {I+3-10} measured by 2014NiZZ. This difference may be due to different production mechanism of {+26}P, noted in 2017Pe09. 
$|G{-|g}=4.39 neV {I59}, 2017Pe09 deduce from measured half-life to estimate proton separation energy. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E$transition from this level not observed as decay occurred far beyond the target position. 
J$proposed by 2019Lo06 based on shell model calculations and comparison to mirror nuclei. 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: MS
level_comment:
J$From {+26}P Adopted Levels in the ENSDF database. 
T$from {+26}P implant-|b-p(t) events fitted with an exponential and a constant background (2020Li06). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
<r{+2}> =4.6(4) fm (measured rms radius in 2006Gu01) 
%|b{++}p from 1996Og01; other: 0.05 (1985Ay02) 


level_energy_unit: KEV
level_comment:
E$Weighted average of 1615 keV 21 ({+7}Li,{+8}He) and 1660 keV 40 ({+3}He,{+8}Li). In 2001Ca37 an average value of 1631 keV 19 is reported. 


level_energy_unit: KEV
level_comment:
E$Isobaric analog state (IAS) of {+27}P deduced in 2001Ca60 from the average of measured two-proton emission energies to the g.s. of {+25}Al. Measured two-proton group energy: 6270(50) keV (2001Ca60), 6410(45) keV (1991Bo32); average: 6340(35) keV. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
|s=31(3) mb 
Total cross section for g.s. + excited state=38(3) mb 
Shell Model Configuration=s{-1/2} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E From |g-ray energy and reported feeding to g.s. 
|s=6.8(11) mb. Shell Model Configuration=d{-3/2} 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$based on S(2p)=6384 keV {I26} (2012Wa38), where x can have values up to |?17 MeV according to figure 2b in 2013Xu13. 2p emission was observed from excited levels of {+27}P from 6.5 to 24 MeV with an energy resolution of 400 keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$value is in good agreement with previous measurements of beta-delayed 2p emission from {+27}P, which yielded values of 12.823 MeV (1991Bo32: Nucl. Phys. A531, 353) and 12.752 MeV (2001Ca60: Eur. Phys. J. A 12, 377). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$24 {I3} <%p < 28 {I2} 
E$From {+27}P Adopted Levels in the ENSDF database. 
$ |G{-|g}/|G{-p}=1.3 {I2} to 1.5 {I2}, deduced by 2017Ja05 assuming only the first excited 3/2+ state has a non-negligible |g decay branch. See I|b footnote. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$ For |G{-|g}/|G{-p}, 2017Ja05 note |J7% proton branch from this state suggest that widths of proton and |g branch are of the same order. This is in contrary to theoretical predictions, where |G{-p} is expected four to five orders of magnitude larger than |G{-|g}. 2017Ja05 attribute this discrepancy to the Pandemonium effect in the {+27}Na decay - used to estimate the %I|b feeding in this work. See I|b footnote. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$E{-p}(res)=318 {I8} 
$B(>)=0.1384 {I256} 
$|G{-|g}= 3.43 meV {I170}, |G{-|p}=2.55 meV {I74} 
$Resonance strength of (p,|g): |w|g =2.92 meV {I191} (2019Su14) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E{-p}(res)=762 {I8} 
$B(>)=0.0264 {I31} 
$Resonance strength of (p,|g): |w|g = 0.65 meV {I+34-30} (2019Su14) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MS
level_comment:
MOMM1$From 2010MaZJ and 2011StZZ 
J$From allowed {+28}P |b{++} decay to 2+ and 4+ states in {+28}Si at 1779 keV and 4618 keV, respectively. 
T$from 1968Ar03 
%ECP,%ECA$from 1996Og01 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$J|p=1+ is assigned in 1997Fu02 from a comparison of ({+3}He,t) spectrum at 0|' with B(M1) strength in {+28}Si(e,e') experiment. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E,J$4610 keV {i50} in 1997Fu02. J|p=1+ is assigned in 1997Fu02 from a comparison of ({+3}He,t) spectrum at 0|' with B(M1) strength in {+28}Si(e,e') experiment. 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
E$From Adopted Levels 
J$From angular distribution and analyzing power studies in (p,n) and (pol p,n) reactions (1985Fa06). 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
T$from line-shape analysis (2019Lo06). Value includes statistical and systematic uncertainty. Other: 91 ps {I24} from simultaneous fit to line-shapes of 106|g and 773|g. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J$L=0 in ({+3}He,d) and from {+29}P(|b{++}|e) decay 
MOMM1$From 2009Zh53 - |b-NMR - diamagnetic correction. Other: 1.2349 {I3} (|b-NMR - 1971SuZI) also in 2005St24, 2011StZZ and 1989Ra17. 
T$weighted av: 4.19 s {I2} (1960Ja12), 4.15 s {I3} (1970Sc16), 4.149 s {I5} (1973Ta04), 4.083 s {I12} (1975Az01), 4.084 s {I22} (1980Wi13) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_comment:
J$From (pol p,p') (1992Wi13) and also in 1980AdZM, 1980AdZN. 
T$From (pol p,p'). Others: 0.36 keV 5 (1976Ik03), 0.17 keV 5 (1969Te02) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$From mean lifetime 218 fs {I18}, weighted average of mean lifetimes 244 fs {I32} (1990Ti07), 240 fs {I70}, 205 fs {I40} (1974By01), 190 fs {I40} (1973Ba35), 240 fs {I80} (1970Wi10), and 200 fs {I60} (1970Mo29) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$From mean lifetime 386 fs {I31}, weighted average of mean lifetimes 450 fs {I90}, 465 fs {I60} (1974By01), 340 fs {I90} (1973Ba35), 390 fs {I140} (1970Wi10), 370 fs {I80} (1970Mo29), 590 fs {I+132-90} (1990Ti07), and 280 fs {I60} (1975Al24). 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$From mean lifetime 28 fs {I4} (1990Ti07). Others: 25 fs {I12} and 33 fs {I11} (1974By01), 70 fs {I35} (1973Ba35) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
$E{-p}=370.7 {I8} 
T$From mean lifetime 33 fs {I15} (1974By01) 
(2J+1)|G{-p}|G{-|g}/|G=2.7 meV 6 (1974By01) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$From mean lifetime 16 fs {I2}, weighted average of mean lifetimes 15 fs {I4} (1974By01), 13 fs {I5} (1973Ba35), 13 fs {I5} (1970Wi10), 15 fs {I4} (1970Mo29), and 24 fs {I5} (1990Ti07). 
$(2J+1)|G{-p}|G{-|g}/|G=63 meV 13 (1974By01) and 28 meV 6 (1971Zu02) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Estimated |G{-p}=51 meV {I31} (2014Ko17) 
$From estimated proton widths, 2014Ko17 suggest that 3p decay proceeds likely from 3447.6-keV level 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
J$from non-nuclear measurement (atomic and molecular beam) -1968Ph02, parity=U in (pol d,|a) (1975Bo46). 
T$weighted average of 2.498 min {I4} (1980Wi13 - {+30}S |e+|b{++} decay), 2.497 min {I5} (1963Mc02), 2.501 min {I2} (2018Ia01). Others: 2.9 m (1937Me02), 3.25 m (1934Cu01,1934Cu02). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$L=2 in ({+3}He,t), parity=U in (pol d,|a) (1975Bo46), L=0 in (|a,d). 
T$weighted average of 33 ps {I2} ({+16}O,pn|g) and 37 ps {I3} ((p,|g),(|a,4n|g)) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
J$L=2 in ({+3}He,|a) and ({+3}He,d), parity=U in (pol d,|a) (1975Bo46), stretched |DJ=2 E2 |g to 1+. 
T$unweighted average of 1.46 ps {I13} from ({+16}O,pn|g) and 2.17 ps {I24} from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L=2 in ({+3}He,t), parity=(N) in (pol d,|a) (1975Bo46). 
T$Other: 62.4 fs {I83} (1979AlZY - |t=90 fs {I12} - the lifetime is not reported lated in 1982Al22) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$L=2 in ({+3}He,t), parity=U in (pol d,|a) (1975Bo46), Log {Ift}=3.6 from (J|p=0+) in {+30}S |e+|b{++} decay. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J (3+) proposed in 2014Mc08,2014McZZ ({+3}He,p|g) - |g to 1+. In 1976Dy01 ({+3}He,d), (1+) was proposed based on |s(|q) and fittings. |g from (5)+ at 6178.4. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$L=2 in ({+3}He,t), parity=U in (pol d,|a) (1975Bo46), L=0+2 in (d,n) and ({+3}He,|a). Tentative L=(1) in (|a,d) is inconsistent with J|p=1+. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L=2 in ({+3}He,t), parity=N in (pol d,|a) (1975Bo46), M1+E2 |g to 1+. L=(1) in (|a,d),({+3}He,p) is inconsistent for parity. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$L=4 in ({+3}He,t), parity=U in (pol d,|a) (1975Bo46), |g to 2+. L=1 in ({+3}He,d) is inconsistent with J|p=3+. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$L=4 in ({+3}He,t) and L=2 in (|a,d), parity=U in (pol d,|a) (1975Bo46). L=(3) in (|a,d),({+3}He,p) is inconsistent for parity. 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: FS
level_comment:
J$1- in (p,|g) 2000Gr19, based on angular distributions of feeding transition, no arguments were provided for the negative parity assignment. L=2 in ({+3}He,d) and parity=U in (pol d,|a) (1975Bo46) for doublet - assumed by the evaluators for the 5508.80 keV level. |g to 0+; 1+; and 2+. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: FS
level_comment:
J$L=2 in ({+3}He,d) and parity=U in (pol d,|a) (1975Bo46) for doublet, D and D(+Q) |g to 3+ and 2+, respectively. |g(|q) data of 4054.3|g D(+Q) indicate a |DJ=1 transition: A{-2}=-0.24 {I4}, A{-4}=+0.09 {I5} (2020Lo11 - ({+3}He,p|g)). 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
J$L=2+6 in ({+3}He,t) for doublet 5701 and 5716 keV levels, parity=U in (pol d,|a) (1975Bo46). Spin parity of (5+) in 2014McZZ was proposed based on 3742.1|g to 3+, assuming the same level at 5719 in ({+3}He,t). 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E$weighted average of 5719 {I5} ({+3}He,t) and 5711 {I5} ({+3}He,d) 
J$in ({+3}He,p|g) (2020Lo11), based on 5039.4|g placement to 0+. 


level_energy_unit: KEV
level_comment:
J$1+,2+,3+ from L=2 in ({+3}He,t). |g to 0+ favors (1,2)+ (2022Do04 (p,|g)), 2020Lo11 ({+3}He,p|g) |g to 0+ not reported and based on |g to (4), 3+ has been proposed. Additional experimental data are needed. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$2996.6|g Q, |DJ=2, to 2+. In 2014McZZ, suggested J{+|p} is (3+) based on 1590|g as Q transition to 5+. The evaluators adopt the proposed assignment in 2020Lo11 based on |g(|q) and DCO measurements. 


level_energy_unit: KEV
level_spin_parity: (5)+
level_comment:
E$weighted average of 6177 keV {I5} ({+3}He,t) and 6179 keV {I5} ({+3}He,d) 
J$L=6 in ({+3}He,p|g), (D) |g to 4- and (Q) |g to (3+). 


level_energy_unit: KEV
level_spin_parity: (1+,2)
level_comment:
J$|gs to 1+; 2+; and 3+. L=2 in ({+3}He,p|g). Unnatural parity in (pol d,|a). In 1969Ha50 (p,|g), J{+|p}=2{+-} based on polarization measurement of 4295.7|g as E1+M2 to 3+. The level expected to be a analog state of {+30}Si at 5614.05, J{+|p}=2{++}, is inconsistent with the assignment in 1969Ha50. Spectroscopic factor in 1976Dy01 ({+3}He,d) suggest L=1. 


level_energy_unit: KEV
level_spin_parity: 4-,5-,6-
level_comment:
E$unweighted average of 6354 {I5} from ({+3}He,t) E=30 MeV and 6372 {I6} from (d,|a) 
J$L=5 in ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: (2-,3)
level_comment:
J$L=(3,4) in (|a,d), |g to (1+). Other: L=6,(7) in ({+3}He,t) would yield (5+,6-) does not support |g to (1+). 


level_energy_unit: KEV
level_spin_parity: (2-,3+)
level_comment:
J$L=4 in ({+3}He,t) for doublet (6654 and 6670), parity=U in (pol d,|a), D+Q |g to 2+, D |g to 2-, |g to 1+ 


level_energy_unit: KEV
level_spin_parity: (3+,4+)
level_comment:
J$from |g-ray feeding 2+, and 3+, and 5+ states. L=6 in ({+3}He,t) presumably associated with this level - for which |g to 2+ would be a less likely placement for the lowest possible J{+|p}=5+. 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$L=1 in ({+3}He,d), |g-rays to 1+, and 0+, and 2- states. L=2 in ({+3}He,t) implies positive parity. 


level_energy_unit: KEV
level_spin_parity: (6+,7+)
level_lifetime_unit: PS
level_comment:
E,J$from ({+16}O,pn|g); if |g to 5+ is M1 - would favor 6+ 
T$from ({+16}O,pn|g). 7+ in (|a,d) (1982De29). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
J$L=1 in (p,|g),(p,p|g) resonances - 1992Fr10, |g to 3+ and 1+. Other: L=2 in ({+3}He,t) is inconsistent for parity. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LT
level_comment:
J$|g to 1+, 4-, 4+, 5+, 2- states. L=6 in ({+3}He,t) is inconsistent with this assignment, probably corresponds to a different level. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$L=2 in (p,|g),(p,p|g) resonances (1992Fr10), D+Q |g to 1+. Additional D+Q |g to 4+ is inconsistent for this assignment. A tentative J|p assginment is made by the evaluators. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$L=0 in (p,|g),(p,p|g) resonances (1992Fr10) and L=2 in ({+3}He,t) probably for a doublet (8096 and 8107). 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$L=3 in (p,|g),(p,p|g) resonances (1992Fr10). Other J{+|p}: 3+,(4,5,6)- in ({+3}He,t). Evaluators list as tentative. 


level_energy_unit: KEV
level_spin_parity: (7+,6+)
level_lifetime_unit: PS
level_comment:
J$2+ is proposed by 2007Ra20 (see figure 2 of 2007Ra20). Private communications via e-mails between XUNDL compilers (S. Geraedts and B. Singh) and the corresponding author of 2007Ra20 (M. Saha Sarkar) made during Sept 25-Oct 6,2007 bring out the conclusion that J|p is probably 7+ or 6+. This assignment corroborates with the previous suggested assignment of 1978Ba76. Preliminary value of Pol(2858|g) suggests M1 favoring 6+ assignment. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: FS
level_comment:
T$weighted average of 90 fs {I10} (1985Re02), 90 fs {I14} (1987Ti03), 107 fs {I21} (1967Ke09), and 111 fs {I31} (1971Sh11). Others: 118 fs {I+152-55} (1972Lu04). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
T$weighted average of 38 ps {I5} (1970Ha52), 37 ps {I7} (1972Sn01), and 37 ps {I4} (1973An01). Others: |>3 ps (1967Ke09), |>0.8 ps (1970La15). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$unweighted average of 4.16 ps {I16} (1977Ra01 - |t=6.01 ps {I23}) and 6.4 ps {I3} (1971He02). Others: |>1 ps (1985Re02), |>166 ps (1969Ha50), |>0.45 ps (1972Lu04). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T$from 1977Ra01 (|t=3.13 ps {I35}). Others: 4.7 ps {I3} (1971He02), >1 ps (1985Re02), |>166 ps (1969Ha50), |>0.5 ps (1971Bi09), 0.3 ps {I+30-2} (1970La15). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
T$weighted average of 139 fs {I21} (1987Ti03) and 156 fs {I14} (1971Sh11). Others: 64 fs {I15} (1969Ha50), 55 fs {I17} (1972Lu04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 111 fs {I10} (1985Re02), 121 fs {I24} (1971Sh11), and 102 fs {I15} (1971Bi09). Other: 67 fs {I10} (1969Ha50) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
T$weighted average of 499 fs {I139} (1985Re02), 423 fs {I125} (1987Ti03), and 832 fs {I139} (1971Sh11). Other: |>159 fs (from 1972Lu04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 45 fs {I3} (1985Re02), 60 fs {I9} (1987Ti03), 66 fs {I10} (1971Sh11), 55 fs {I10} (1969Bi11), and 49 fs {I7}(1971Bi09). Others: 26 fs {I3} (1969Ha50), 33 fs {I5} (1972Lu04), 69 fs {I+29-21} (1970La15). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T$Others: <7 fs (1985Re02), <21 fs (1971Sh11), <8 fs (1972Lu04), <20 fs (1971Bi09), < 10 fs (1970La15) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
T$weighted average of 26 fs {I3} (1985Re02), 38 fs {I6} (1987Ti03), 40 fs {I10} (1969Ha50), 22 fs {I2} (1972Lu04), 17 fs {I6} (1971Bi09), and 28 fs {I4} (1970La15) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 2.4 fs {I8} (1987Ti03) and 2.1 fs {I6} (1980An07). Others: 7 fs {I2} (1985Re02), <14 fs (1971Bi09), <10 fs (1970La15) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
E$1972No02 reported doublet for this energy levels as 4229.9 keV {I13} and 4234.5 keV {I18} with half lives 513 fs {I62} and 28 fs {I21}, respectively. In the absence of firm evidence, the evaluators considered it to be a single energy level. 
T$others: 1.4 ps {I+21-6} (1970La15), >0.7 ps (1985Re02), |>0.8 ps (1969Ha50), >1.5 ps (1972Lu04), >0.9 ps (1971Bi09) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 26 fs {I3} (1985Re02), 38 fs {I6} (1987Ti03), 44 fs {I6} (1969Ha50), and 28 fs {I5} (1971Bi09). Other: 13.2 fs {I55} (1972Lu04), 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T$weighted average of 4.4 fs {I15} (1987Ti03) and 3.5 fs {I21} (1972Lu04). Others: <7 fs (1985Re02), <33 fs (1970La15) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
T$weighted average of 236 fs {I28} (1985Re02), 180 fs {I31} (1987Ti03), 180 fs {I42} (1969Ha50), 152 fs {I14} (1972No02), 166 fs {I28} (1972Lu04), and 194 fs {I42} (1971Bi09). Other: 159 fs {I+74-43} (1970La15) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$(5)- in 1969Ha50 
E$weighted average of 4926.4(2) (1985Re02) and 4925.5(2) (2000Gr19) 
J$|g decay to 2+ level rules out the possibility for 5- assignment as mentioned in 2000Gr19 based on experimental observation 
E Other: 4921 in 1972Lu04 
T$from |t=375 ps {I50} (1978Ba76 (RDM),1990En08). Others: >0.8 ps (1972Lu04), >0.6 ps (1971Bi09), |>0.6 ps (1969Ha50). 
T=0 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$weighted average of 4941.0(3) (1985Re02) and 4941.4(3) (2000Gr19) 
T$Others: <7 fs (1985Re02), 33 fs {I14} (1969Ha50) 
T=0 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
E$from 2022Do04 
$E{-r}(c.m.)=303.4 keV {I10}, |w|g=8.8|*10{+-5} eV {I15} (2022Do04) 
$Resonance energy E{-r}(c.m.) is deduced from E(level)-Q(p,|g) in 2022Do04, with Q(p,|g)=5593.34 {I7} deduced by the authors of 2022Do04 using nuclear masses. S(p)({+30}P)=5594.75 {I7} from 2021Wa16 (AME2020) 
$Resonance strength |w|g given is extracted from the measured |g-ray yields (2022Do04) 
J$from 2022Do04 


level_energy_unit: KEV
level_spin_parity: (1,2,3+)
level_comment:
E$from 2022Do04 
J$from 2022Do04. Other: 2000Gr19 adopted 2- assignment 
$E{-r}(c.m.)=314.2 keV {I6}, |w|g=0.0207 eV {I27} (2022Do04) 
$Resonance energy E{-r}(c.m.) is deduced from E(level)-Q(p,|g) in 2022Do04, with Q(p,|g)=5593.34 {I7} deduced by in 2022Do04 using nuclear masses. S(p)({+30}P)=5594.75 {I7} from 2021Wa16 (AME2020) 
$Resonance strength |w|g given is extracted from the measured |g-ray yields (2022Do04) 
J$from 2022Do04 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
J$from 2022Do04 
$E{-r}(c.m.)=402.9 keV {I6} (2022Do04) 
$Resonance energy E{-r}(c.m.) is deduced from E(level)-Q(p,|g) by 2022Do04, with Q(p,|g)=5593.34 {I7} deduced by the authors of 2022Do04 using nuclear masses. S(p)({+30}P)=5594.75 {I7} from 2021Wa16 (AME2020) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J,L$J|p=3- and l{-p}=1 (1992Fr10). 
$E{-p}=3154 keV {I3}; |G{-p1}=0.50 keV, |G{-p2}=0.20 keV, |G{-|g}=0.73 eV 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
E authors refer this level to 5916 in the literature - which is 5908 keV level in the adopted dataset. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
L other: (0+2) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=383 |mb and |s{-int}(28 MeV)=201 |mb (1974Ha38); |s(20|')=32 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
L other: (0+2) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=668 |mb and |s{-int}(28 MeV)=539 |mb (1974Ha38); |s(20|')=14 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
L other: (2) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=117 |mb and |s{-int}(28 MeV)=85 |mb (1974Ha38); |s(20|')=13 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
L other: (2+4) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=306 |mb and |s{-int}(28 MeV)=294 |mb (1974Ha38); |s(20|')=60 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
L other: (2+4) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=204 |mb and |s{-int}(28 MeV)=232 |mb (1974Ha38); |s(20|')=35 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
L other: (0+2,2+4) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=143 |mb and |s{-int}(28 MeV)=137 |mb (1974Ha38); |s(20|')=30 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|s{-int}(16 MeV)=303 |mb and |s{-int}(18 MeV)=298 |mb (1974Ha38); |s(20|')?200 ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$|s{-int}(16 MeV)=84 |mb and |s{-int}(28 MeV)=43 |mb (1974Ha38) 
S$(0+2) from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|s{-int}(16 MeV)=92 |mb and |s{-int}(28 MeV)=62 |mb (1974Ha38) 
S$(1+3) from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
L other: (3) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=533 |mb and |s{-int}(28 MeV)=610 |mb (1974Ha38); |s(20|')=100 |mb/sr ((|a,d) work of 1976De24) 
S$(1+3) from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$|s{-int}(16 MeV)=129 |mb and |s{-int}(28 MeV)=136 |mb (1974Ha38) 
S$(2+4) from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
L other: (2+4) ({+3}He,p) (1974Ha38) 
$|s{-int}(16 MeV)=202 |mb and |s{-int}(18 MeV)=114 |mb (1974Ha38); |s(20|')=15 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|s{-int}(16 MeV)=527 |mb and |s{-int}(28 MeV)=191 |mb (1974Ha38) 
S$(3) from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$|s{-int}(16 MeV)=107 |mb and |s{-int}(28 MeV)=104 |mb (1974Ha38) 
S$(1+3) from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$4921 keV J=1,2 in 1968Ve04 
$|s(20|')=50 |mb/sr ((|a,d) work of 1976De24) for doublet (4926 and 4937) 


level_energy_unit: KEV
level_comment:
S$from the ({+3}He,p) work of 1974Ha38 carried out at 28 MeV 
$|s{-int}(16 MeV)=167 |mb and |s{-int}(28 MeV)=116 |mb (1974Ha38) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7+
level_comment:
E,J from 1982De29. Spin and parity are proposed based on comparison of d|s/d|W and the microscopic FPSDI calculations. Other: 7231 {I50} and L=(6) in 1976De24. 
$|s(20|')=250 |mb/sr ((|a,d) work of 1976De24) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$1968Ve04 reports two additional |g decay branches from the level. These are 3220 keV and 3252 keV (extracted by the evaluators based on the level energy difference). The reported summed up branchings from the two transitions are 10 {I6} (1968Ve04). The placement of 3252 keV |g decay branch looks to be suspicious based on the assigned J|p value of the level. 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
E$1968Ve04 placed two additional 2778 and 4231 keV |g transitions from the level; the placements of these transitions are suspicious based on the assigned J|p values of the decaying and feeding levels 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$1968Ve04 placed an additional 3917 keV (extracted by the evaluators based on level energy difference) |g transition from the level; the placement of the transition is suspicious based on the assigned J|p values of the decaying and feeding levels 


level_energy_unit: KEV
level_spin_parity: (3-,5-)
level_comment:
E$1968Ve04 placed three additional decay branches from the level. The extracted energies of the corresponding transitions by the evaluators are 1988, 4217 and 4249 keV (based on the level energy differences). The placement of these transitions are suspicious based on the assigned J|p value of the level. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$spin parity of (5+) in 2014McZZ was proposed based on |g to 3+, assuming the same level at 5719 in ({+3}He,t). 


level_energy_unit: KEV
level_comment:
J$2+ assignment in 2020Lo11; this assignment is suspicious due to the presence of |g decay branch to 5+ level 


level_energy_unit: KEV
level_comment:
J$1- assignment in 2020Lo11, appears that the authors assume to be the same level as 5993 with L=1 in ({+3}He,d) as mentioned in the adopted dataset. 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
J$evaluators' note: 5+ is not completely ruled out by |g(|q) and DCO data; the J|p assignment of (6+) by 2014Mc08 appears to be suspicious due to the placements of the two decay branches 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$2014McZZ made a 2+ assignment; but the confirmed assignment can not be made following the results presented in 2014McZZ (Evaluators' note) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W = 250 |mb/sr {I6}; parity=U (1975Bo46) 
$|s=0.42 (relative to 1 for 1972 keV level) summed value for |q=25|' to 90|' (not repeated in the following listing) (1982Ta04). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W = 203 |mb/sr {I6}; parity=U (1975Bo46) 
$|s=0.29 (relative to 1 for 1972 keV level) (1982Ta04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$d|s/d|W = 133 |mb/sr {I4}; parity=N (1975Bo46) 
$|s=0.13 (relative to 1 for 1972 keV level) (1982Ta04). 


level_energy_unit: KEV
level_spin_parity: 1-,(2-)
level_comment:
E$weighted average of 4296 {I10} (1958En51) and 4298 {I4} (1975Bo46). 
$d|s/d|W = 91 |mb/sr {I9} (1975Bo46) 


level_energy_unit: KEV
level_spin_parity: (0-,1+,3+)
level_comment:
E$weighted average of 4734 {I10} (1958En51) and 4735 {I4} (1975Bo46). 
$d|s/d|W = 103 |mb/sr {I6}; parity=U (1975Bo46) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5024 {I10} (1958En51) and 5030 {I5} (1975Bo46). 
$d|s/d|W = 46 |mb/sr {I7}; parity=(N) (1975Bo46) 


level_energy_unit: KEV
level_spin_parity: (1,3)+
level_comment:
E$weighted average of 5200 {I10} (1958En51) and 5208 {I5} (1975Bo46). 
$d|s/d|W = 288 |mb/sr {I11}; parity=U (1975Bo46) 


level_energy_unit: KEV
level_spin_parity: (0-)
level_comment:
E$weighted average of 5412 {I10} (1958En51) and 5418 {I4} (1975Bo46). 
$d|s/d|W = 249 |mb/sr {I12}; parity=U (1975Bo46) 


level_energy_unit: KEV
level_spin_parity: 1+,(3+,1)
level_comment:
E$weighted average of 5504 {I10} (1958En51) and 5511 {I4} (1975Bo46). 
$d|s/d|W = 190 |mb/sr {I13}; parity=U (1975Bo46) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 5598 {I10} (1958En51) and 5594 {I4} (1975Bo46). The quoted uncertainty is 110 keV in 1958En51; probably it is a typo 
$d|s/d|W = 100 |mb/sr {I10}; parity=N (1975Bo46) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$weighted average of 5700 {I10} (1958En51) and 5713 {I4} (1975Bo46). 
$d|s/d|W = 389 |mb/sr {I12}; parity=U (1975Bo46) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$6880 {I5} in 1975Bo46 from literature. 
$d|s/d|W = 100 |mb/sr {I20} (for unresolved doublet in 1975Bo46) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$spin from optical spectroscopy (1933As01,1949Cr31), paramagnetic resonance (1954Fl41) and microwave spectroscopy (1949Gi28); L(pol d,{+3}He)=L({+3}He,d)=L(d,n)=0 from 0+ target. 
MOMM1$from gas phase NMR with new estimate for the absolute shielding constants (2011La24). Other: +1.130903 {I17} from gas phase NMR, with accurate shielding effects (2005An15), +1.13160 {I3} (1954Wa37,NMR), 1.133 {I1} (1969Se11,paramagnetic resonance), 1.13176 {I6} (1963Ba23,NMR), 1.13177 {I12} (1955Fa45,NMR), 1.13159 {I6} (1952Ka06,NMR), 1.13183 {I8} (1951Sh33,NMR), 1.13161 {I12} (1949Bi07,NMR), +1.5 {I5} (1949Cr31,optical spectroscopy), 1.1321 {I2} (1948Po09,NMR). See also 2019StZV compilation 
$RMS charge radius: (<r{+2}>){+1/2}=3.1889 fm {I19} (2013An02 evaluation) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.75 {I8} 
$Adopted (1977En02) proton pickup spectroscopic factor=2.0 {I2} 
$g{-J}=-2.00165 {I39} (1964Pe11), atomic beam magnetic resonance 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(pol {+3}He,d)=2 from 0+ and L-1/2 transfer from analyzing power 
T$weighted average of 510 fs {I24} (2021To09) by DSAM in ({+20}Ne,p|g), 527 fs {I33} (1979Po01), 555 fs {I152} (1974Tw01), 451 fs {I153} (1970Va12), 555 fs {I56} (1969Cu01), 485 fs {I49} (1979Fo02) by DSAM in (|a,p|g), 270 fs {I118} (1975De31), 534 fs {I169} (p,|g), 513 fs {I69} (1966Sk01), 665 fs {I+347-146} (1964Bo22), 319 fs {I160} (1960Bo23) by nuclear resonance fluorescence in (|g,|g'), and 520 fs {I42} by DSAM in Coulomb excitation (1977Sc36). Others: 315 fs {I+83-71} from adopted B(E2)|^=0.0070 {I8} and adopted |d(E2/M1)(1266.1|g)=+0.26 {I3}; 496 fs {I+82-61} from |G=0.00092 eV {I13} in (|g,|g'). 
$B(E2)|^: weighted average of 0.0073 {I8} (1965Ko03) and 0.0069 {I11} (1975Kl03) in (e,e'), 0.0097 {I20} (1966Li02) in (p,p'), 0.0060 {I10} (1977Sc36) in Coulomb excitation 
MOMM1$from transient fields using IMPAC method (1982Ho06). See also 2020StZV compilation. 
$Adopted (1977En02) proton stripping spectroscopic factor=0.97 {I14}. 
$Adopted (1977En02) proton pickup spectroscopic factor=1.5 {I2}. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol {+3}He,d)=2 from 0+ and L+1/2 transfer from analyzing power 
T$weighted average of 236 fs {I21} (1974Tw01), 208 fs {I79} (1970Va12), 263 fs {I21} (1969Cu01), 252 fs {I17} (1979Fo02), and 271 fs {I18} (1979Po01) in (|a,p|g), 236 fs {I87} (1975De31) and 295 fs {I76} (1968Wo01) in (p,|g), 256 fs {I55} (1977Sc36) in Coulomb excitation. Other: 252 fs {I17} from adopted B(E2)|^=0.0118 {I7} and branching ratio of 2233.6|g; 310 fs {I+35-29} from |G=0.00147 eV {I15} in (|g,|g'). 
MOMM1$from IMPAC method (1982Ho06). See also 2020StZV compilation 
$B(E2)|^: weighted average of 0.0097 {I11} (1965Ko03) and 0.0120 {I5} (1975Kl03) in (e,e'), 0.0165 {I40} (1966Li02) in (p,p'), 0.0149 {I22} (1977Sc36) in Coulomb excitation 
$Adopted (1977En02) proton stripping spectroscopic factor=0.10 {I2}. 
$Adopted (1977En02) proton pickup spectroscopic factor=4.2 {I4}. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 3133.7 {I7} from (|a,p|g) 
J$L({+3}He,d)=L(d,n)=L(d,{+3}He)=0 from 0+. Other: (3/2+) suggested from analysis of differential cross section in (p,p') is inconsistent 
T$from |G=0.0645 eV {I39} in (|g,|g'). Others: 9.7 fs {I42} (1975De31), and 5.5 fs {I31} (1968Wo01) from (p,|g), 6 fs {I5} from (n,n'|g), all by DSAM. 
$Adopted (1977En02) proton stripping spectroscopic factor=0.04 {I2}. 
$Adopted (1977En02) proton pickup spectroscopic factor=0.25 {I4}. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$parity from L({+3}He,d)=L(d,{+3}He)=2 from 0+ 
T$weighted average of 54 fs {I24} (1975De31) and 94 fs {I26} (1968Wo01) in (p,|g), 90 fs {I35} from (|a,|g):resonances, 81 fs {I25} from (|a,p|g), 97 fs {I17} from (n,n'|g), all by DSAM. 
$Adopted (1977En02) proton stripping spectroscopic factor<0.01. 
$Adopted (1977En02) proton pickup spectroscopic factor=1.2 {I2}. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$2148.4|g E2, |DJ=2 to 3/2+, 1181.0|g M1+E2 to 5/2+ 
T$weighted average of 308 fs {I125} (1975De31), 208 fs {I62} (1968Wo01), and 159 fs {I69} (1968En03) from (p,|g), 208 fs {I56} from (|a,|g):resonances, 222 fs {I59} from (|a,p|g), and 280 fs {I150} from (n,n'|g). 
$B(E2)|^=0.0039 {I8} for 3415+3506 doublet in (e,e') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 3505.4 {I7} from (|a,p|g) 
J$from |g(|g,pol) and |g|g(|q) in (p,|g) 
T$from |G=0.052 eV {I8}. Others: 8.3 fs {I42} (1975De31) and 9.0 fs {I56} (1968Wo01) from (p,|g), 12 fs {I8} from (n,n'|g), all by DSAM 
$Adopted (1977En02) proton stripping spectroscopic factor <0.01. 
$Adopted (1977En02) proton pickup spectroscopic factor is small. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$parity from 2924.7|g M1+E2 to 3/2+ 
T$from (p,|g). Others: |<10 fs from (|a,p|g), |<28 fs from (|a,|g):resonances; 62 fs {I10} from (n,n'|g) is discrepant 
$Adopted (1977En02) proton stripping spectroscopic factor=0.03 {I2}. 
$Adopted (1977En02) proton pickup spectroscopic factor=1.2 {I2}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 4261 {I1} from (|a,p|g) 
J$L({+3}He,d)=2 from 0+; 4260.1|g M1+E2 to 1/2+ 
$Adopted (1977En02) proton stripping spectroscopic factor=0.06 {I2}. 
T$from (p,|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$L(pol {+3}He,d)=L(d,n)=3 from 0+ and L+1/2 transfer from analyzing power. 4451 in {+31}S and 4431 in {+31}P are probable mirror states (2008Pa27). 
T$weighted average of 0.28 ps {I10} (1975De31) and 0.83 ps {I41} (1968Wo01) from (p,|g), 0.413 ps {I31} (2021To09), 0.50 ps {I6} and 0.46 ps {I10} (2008Pa27) from ({+20}Ne,p|g), and 0.41 ps {I11} from (|a,p|g), all by DSAM. 
$Adopted (1977En02) proton stripping spectroscopic factor=0.45 {I7}. 
$Adopted (1977En02) proton pickup spectroscopic factor=0.08. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 4594.2 {I7} from (|a,p|g) 
J$parity from L({+3}He,d)=2 from 0+ 
T$weighted average of 11.1 fs {I42} (1975De31), 30 fs {I15} (1968Wo01) from (p,|g), and 16 fs {I10} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$1218.8|g M1+E2, |DJ=0 to 7/2+ 
T$weighted average of 101 fs {I28} (1975De31), 69 fs {I27} (1968Wo01) from (p,|g), 62 fs {I14} from (|a,|g):resonances, 69 fs {I20} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$4783.0 {I6} from (|a,p|g), 4783.4 {I11} from (p,|g) 
J$4783.0|g E2, |DJ=2 to 1/2+ 
T$from (p,|g). Others: |<10 fs from (|a,p|g); 62 fs {I35} from (|a,|g):resonances is discrepant 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$5014.5|g D(+Q) to 1/2+, 1719.8|g to 5/2+ and probable 1600.3|g to 7/2+; |s in (d,|a) supports 1/2, which is not entirely ruled out. 
T$weighted average of 31 fs {I12} (1975De31), 46 fs {I14} (1968Wo01) from (p,|g), and 49 fs {I16} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(pol {+3}He,d)=L(d,n)=1 from 0+ and L+1/2 transfer from analyzing power 
T$from DSAM in (p,|g). Other: |<7 fs from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). Other: 5116.0 {I15} from (p,|g) 
J$1701.3|g M1+E2 to 7/2+, 3849.6|g M1+E2 to 3/2+ 
T$from DSAM in (|a,p|g). Other: <42 fs from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(d,{+3}He)=L(d,n)=L({+3}He,d)=0 from 0+ 
T$from (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
J$3110.2|g E2, |DJ=2 to 5/2+, 1928.0|g D(+Q) to 7/2+ 
T$weighted average of 33 fs {I11} from (|a,p|g) and 58 fs {I21} from (p,|g). Other: |<21 fs from (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 5529 {I1} from (|a,p|g) 
J$3296.0|g M1+E2 to 5/2+, 2115.3|g M1+E2 to 7/2+; |s in (d,|a) supports 5/2; possible 5529.5|g to 1/2+ also favors 5/2. Other: 7/2+,(5/2+) from |g(|q) in (|a,p|g) (1974Tw01) seems inconsistent 
T$from DSAM in (n,n'|g). Other: <7 ps from (p,|g); |<10 fs from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$parity from L({+3}He,d)=2 from 0+. |s in (d,|a) also favors 3/2. Other: (7/2)- from (p,p') for a group at 5600 is inconsistent 
T$from (p,|g). 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$also supported by |s in (d,|a). 
T$from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$L(|a,p)=4 from 0+; |s in (d,|a) favors J=7/2; 9/2+ ruled out by 4507.0|g to 3/2+ and RUL 
T$from (p,|g). Other: |<10 fs from (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
J$3658.2|g E2, |DJ=2 to 5/2+, 2477.3|g M1+E2 to 7/2+. But L(d,{+3}He)=2 from 0+ for a group at 5892 {I5} is inconsistent, which could indicate a different level 
T$weighted average of 25 fs {I8} (1975De31) and 55 fs {I44} (1968En03) from (p,|g), 21 fs {I8} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$the 5988 level with de-exciting 4722|g in (|a,p|g) is probably a different level 
J$L({+3}He,d)=2 from 0+; |s in (d,|a) favors 3/2 but with inconsistent negative parity 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 6048 {I1} from (|a,p|g) 
J$spin from p|g(|q) in (|a,p|g); 3812.3|g M1+E2 to 5/2+ 
T$from DSAM in (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
J$3844.6|g E2 (|DJ=2) to 5/2+, 1444.4|g M1+E2 to 7/2+ 
T$from (|a,p|g). Other: |<42 fs from (|a,|g):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2,3/2,5/2)
level_comment:
E$energy is adopted from (d,|a) (1974Te02) since level energies in this region are in very good agreement with the Adopted values, estimated uncertainty is |?5-10 keV (evaluators). Population of this level at 6180 {I23} in {+30}Si(d,n) is considered as uncertain by the evaluators since it is reported as a fairly strong line in 1965Cu03 but not in 1976Uz01. 
J$from analysis of |s in (d,|a). 


level_energy_unit: KEV
level_spin_parity: (7/2)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(|a,p)=4 from 0+; probably the mirror state of 6138, (7/2+) level in {+31}S (2012Do07). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=L(d,n)=2 from 0+; L(p,{+3}He)=0 from 3/2+; |s from (d,|a) supports 3/2 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin from primary |g(|q) from J=7/2 resonance and 1968|g(|q) in (p,|g); |s in (d,|a) also supports 7/2; 1967.7|g (M1(+E2)) to 7/2- 
T$weighted average of 22 fs {I12} from (|a,p|g) and 49 fs {I24} from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: FS
level_comment:
J$3039.3|g E2 (|DJ=2) to 7/2+, 1110.2|g M1+E2 to 9/2+ 
T$weighted average of 24 fs {I12} (|a,|g):res and 22 fs {I12} (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=2 from 0+; L({+3}He,p)=2+4 from 1/2+. But L(d,{+3}He)=0 from 0+ for a group at 6460 {I5}, giving 1/2+, is inconsistent. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$spin from p|g(|q) in (|a,p|g); 2070.6|g M1+E2 to 7/2- 
T$from DSAM in (|a,p|g). Other: |<76fs from (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=1 from 0+; 2419.3|g to 5/2+ disfavors 1/2-; |s in (d,|a) also supports 3/2. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$2364.8|g M1+E2, |DJ=1 to 7/2-; 5/2- ruled out by a strong 1063.4|g from J=11/2 level 
T$from (|a,p|g). Other: 152 fs {I62} from (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from (|a,|g):resonances 
J$|g rays to 5/2+, 7/2-, 7/2+; 5375|g from 11/2- 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=3 from 0+; |s in (d,|a) favors 5/2. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=L(d,n)=1 from 0+; |s in (d,|a) favors 3/2. 


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 
J$spin from p|g(|q) in (|a,p|g); 4697.2|g M1+E2 to 5/2+ 
T$from (|a,p|g) and (p,|g) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)+
level_comment:
E$from ({+3}He,p) 
J$L({+3}He,p)=0(+1) from 1/2+. L=1 component may belong to 7068 and/or 7079.9 levels. 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$2648.6|g to 7/2-; primary 2320.7|g from 1/2+ proton resonance; L({+3}He,d)=1 from 0+ 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$3669.1|g to 7/2+, possible 3939.4|g to 1/2+ 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):resonances. Other: 7117.9 {I27} from (p,|g) 
J$spin from p|g(|q) in (|a,p|g); 3703|g M1+E2 to 7/2+ 
T$from (|a,p|g). Other: |<69 fs from (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$from ({+3}He,d). Other: 7158 {I5} from (d,{+3}He) 
J$L(d,{+3}He)=2 from 0+. L({+3}He,d)=(1,3) from poor fits is inconsistent 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$from ({+3}He,d). Others: 7349 {I6} from ({+3}He,p), 7344 {I5} from (d,{+3}He) 
J$L({+3}He,p)=1+3 from 1/2+ target; L({+3}He,d)=1 or 2 from 0+ 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: FS
level_comment:
J$4027.5|g E2, |DJ=2 to 7/2+; 988.1|g |DJ=0 to 11/2+. 
T$from DSAM in (|a,|g):resonances using 4027.5|g. Other: |<10 fs from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). Other: 7470.4 {I22} from ({+3}He,d) 
J$L({+3}He,p)=3(+5) from 1/2+; L({+3}He,d)=(3) from 0+; |g rays to 9/2-, 7/2- and 7/2+ 
T$from (|a,|g):resonances 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$could be the same level as 7690.9 in ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_comment:
J$3428.6|g, |DJ=2 to 7/2-; 2516.8|g |DJ=1 to 9/2+. L({+3}He,d)=(3) is inconsistent if the same levels are being populated 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: EV
level_comment:
J$L({+3}He,d)=L(d,n)=1 from 0+; spin=1/2 from isotropic |g(|q) in (p,|g) 
T$weighted average of 54 eV {I14} from (p,|g) and 68 eV {I9} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$from ({+3}He,d) 
J$L({+3}He,d)=2 from 0+. L(p,|a)=1 from 0+ for a level at 7979 {I30} suggests (1/2,3/2)- 


level_energy_unit: KEV
level_spin_parity: (5/2)-
level_comment:
J$L({+3}He,p)=1 from 1/2+; L({+3}He,d)=(2,3) from 0+. L(p,|a)=1 from 0+ for a level at 7979 {I30} suggests (1/2,3/2)- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from L(|a,p)=2 from 0+. But L(d,{+3}He)=(1) for a group at 8033 {I5} is inconsistent 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_comment:
J$3645.6|g |DJ=2 to 7/2-; 1253.4|g |DJ=0 to 11/2-. L({+3}He,d)=(1) is inconsistent, but L=(1) is from a poor fit. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$most likely the L=3 component in L({+3}He,d)=1+3 for a level at 8242 {I6} considering L(d,n)=1 for a level at 8251 {I4}. L({+3}He,p)=1+3 probably also corresponds to the 8243+8248 doublet 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(d,n)=1 from 0+ gives 1/2-,3/2-; |g rays to 5/2+ favor 3/2- . See also comments for 8242.7 level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$reported only by 1958Br98 in (p,|g); not seen in other studies 
J$from |g(|q) in (p,|g) 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_lifetime_unit: FS
level_comment:
E$the evaluators consider the level at E=8345.5 {I15} from (|a,|g):resonances is the same level here seen in ({+16}O,2|a,p|g), considering the most intense |g is near 4930 from each level. 
J$4928.5|g |DJ=2 to 7/2+ is likely E2. 
T$from DSAM in (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):resonances. This level may possibly be the same as 8343.5, (11/2+) since the most intense |g is near 4930 from each level, but the transitions to 5/2+ are inconsistent with J|p=(11/2+) based on RUL 
J$|g rays to 5/2+ and 7/2+; 3858|g from 11/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |g(|q), |g|g(|q) and |g(lin pol) in (p,|g); L({+3}He,d)=2 from 0+ 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$from (p,p):resonances. Other: 0.7 keV {I4} from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |g(|q), |g|g(|q) and |g(lin pol) in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$2509.9|g to 9/2+ favors positive parity. Other: 1/2- from R-Matrix analysis in (p,p):resonances is inconsistent 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$strong 2709.6|g to 9/2+; 8599.7|g to 1/2+. But 7/2- may not be completely ruled out 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from R-Matrix analysis in (p,p):resonances and L({+3}He,d)=2 for a level at 8646 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from L({+3}He,d)=2 from 0+ and L({+3}He,p)=0+2 from 1/2+ for a group at E=8731 {I6} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$from (p,p):resonances. Other: 1.5 keV {I4} from (p,|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$spin=7/2 from |g(|q) in (p,|g), (5/2,7/2)- from R-Matrix analysis in (p,p):resonances, and L(|a,p)=3 from 0+ for a level at 8840 would give a firm 7/2-, while L({+3}He,d)=2 for a level at 8840 {I4} gives 3/2+,5/2+, which would imply a separate level with close energy 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$weighted average of 110 eV {I50} from (p,|g) and 90 eV {I15} from (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(3/2,5/2)+ from R-Matrix analysis in (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from L({+3}He,p)=0 from 1/2+; (3/2,5/2)+ from R-Matrix analysis in (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$also supported by L({+3}He,d)=2 from 0+ 
T$weighted average of 100 eV {I5} from (p,|g) and 65 eV {I20} from (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$also supported by L({+3}He,d)=1 from 0+ 
T$weighted average of 9.0 keV {I10} from (p,|g) and 9.3 keV {I9} from (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,p)=2(+4) from 1/2+; 2671.8|g to 3/2+, 2143.0|g to (3/2)-, 2653.6|g to 7/2(-) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(3/2,5/2)+ from R-Matrix analysis in (p,p):resonances 
T$halflife<26 fs from DSAM in (p,|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(5/2,7/2)- from R-Matrix analysis in (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(5/2)+ from R-Matrix analysis in (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,p)=0+3 from 1/2+ for a group at 9155 {I6} gives 1/2+,3/2+ for one component and 3/2 to 9/2 with negative parity for the other. This level could be the negative-parity component in ({+3}He,p) 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,p)=0+3 from 1/2+ for a group at 9155 {I6} gives 1/2+,3/2+ for one component and 3/2 to 9/2 with negative parity for the other. This level could be the positive-parity component in ({+3}He,p) 


level_energy_unit: KEV
level_spin_parity: (13/2)-
level_lifetime_unit: FS
level_comment:
J$2722.3|g |DJ=1 to 11/2+; 1041.7|g M1+E2 from |p=-. 13/2- proposed in ({+16}O,2|ap|g) but 13/2+ in ({+20}Ne,p|g). 
T$from DSAM in ({+16}O,2|ap|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$weighted average of 120 eV {I50} from (p,|g) and 80 eV {I15} from (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$weighted average of 3.1 keV {I4} from (p,|g) and 4.0 keV {I4} from (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(5/2,7/2)- from R-Matrix analysis in (p,p):resonances; 5/2- disfavored by 3361.7|g to 9/2+. 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$3364.7|g to 9/2+, 2760.5|g to 3/2-. Weak 9254.4|g E3 to 1/2+ is allowed by RUL and measured resonance strength 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
$parity from L({+3}He,d)=1 from 0+ 
T$weighted average of 10.1 keV {I8} from (p,|g) and 9.8 keV {I10} from (p,p):resonances 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$2241.1|g to 9/2+ and 2857.1|g to 9/2- gives (7/2,9/2,11/2), which is however excluded by strong 6223.1|g to 1/2+ based on measured proton resonance strength and RUL. These conflicting results are presumably due to a possible broad resonance coinciding with this resonance, as claimed by 1975De31 in (p,|g). This conclusion also applies to the proton resonance at the 9360.8 level 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$2429.3|g to 5/2+, 2766.5|g to 5/2-, 2858.9|g to 9/2- and 3281.8|g to /2+ give J=7/2, which is however excluded by 9359.3|g and 6225.8|g to 1/2+ based on measured proton resonance strength and RUL. These conflicting results are presumably due to a possible broad resonance coinciding with this resonance, as claimed by 1975De31 in (p,|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$9362 in {+30}Si(p,p) could be the same as 9360.8 from {+30}Si(p,|g), but 3/2- from (p,p) is not in agreement with |g decays of 9360.8 level. 
J$also supported by L({+3}He,d)=1 from 0+ for a level at E=9353 {I6} 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from R-Matrix analysis in (p,p):resonances, but with inconsistent J=(5/2) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from L({+3}He,d)=2 from 0+; (5/2)+ from R-Matrix analysis in (p,p):resonances 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$2545.4|g to 5/2+, 2974.9|g to 9/2-, 3584.8|g to 9/2+ gives (7/2,9/2+); strong 9475.3|g to 1/2+ and proton resonance disfavors 9/2+ and 7/2+ 


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,J$spin=3/2 from |g(|q) and |g|g(|q) of 5333.2|g and 9523.0|g in (p,|g) and parity from 5333.2|g M1+E2 to 5/2+, however, 5092.9|g to 7/2- and 6109.4|g to 7/2+ excludes J=3/2 based on measured proton resonance strength and RUL. 3/2- from R-Matrix analysis in (p,p):resonances is also inconsistent. 1975De31 in (p,|g) state that this ambiguity presumably arises because this resonance coincides with a broad resonance. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$unresolved doublet in (p,|g) 
J$spin=5/2 from 7301.7|g(|q) in (p,|g); parity from R-Matrix analysis in (p,p):resonances. However, 2721.1|g to 11/2- and 3081.5|g to 11/2+ disfavors J|<7/2. It is likely that those two transitions belong to a different level with the similar energy. 1975De31 in (p,|g) claim that this level is an unresolved doublet 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$(5/2-,7/2+) from DWBA analysis in (|a,p) for a group at 9570 is inconsistent, which could indicate a different level with similar energy 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=7/2 from |g(|q) and |g|g(|q) in (p,|g); 2967.2|g to 3/2-. But (3/2,5/2)+ from R-Matrix analysis is inconsistent. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2-)
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$1/2+ from R-Matrix analysis in (p,p):resonances, while J=3/2 from |g(|q) and |g|g(|q) in (p,|g). L({+3}He,d)=1 from 0+ for a level at E=9577 {I4}. The evaluators consider either 1/2+ or 3/2- could be possible and it is likely there is a doublet around this energy 
T$weighted average of 3.1 keV {I9} from (p,|g) and 3.8 keV {I4} from (p,p):resonances 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$1975De31 in (p,|g) claim this resonance must be a doublet due to |g(|q) data of 9610.3|g and 8344.6|g (excluding J|<5/2) inconsistent with 3230.9|g to 3/2+ (excluding J|>7/2) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_lifetime_unit: EV
level_comment:
J$from R-Matrix analysis in (p,p):resonances. other: L({+3}He,d)=1+3 from 0+ for a group at 9720 {I4} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$spin=1/2 from |g(|q) in (p,|g), which is however inconsistent with 2602.5|g to 9/2+, 3218.5|g go 9/2-, 3265.6|g to 11/2+; J|p=3/2- from R-Matrix analysis in (p,p):resonances. The contradicting results imply that there could be a multiple around this energy. 1975De31 in (p,|g) claim this proton resonance level is an unresolved doublet 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3/2 from |g|g(|q) of 8576.2|g and 9841.9|g in (p,|g), while 3951.4|g to 9/2+ excludes 1/2 to 5/2- based on measured proton resonance strength and RUL. The contradicting results could indicate a doublet, also considering (3/2,5/2)+ from R-Matrix analysis in (p,p):resonances 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$Doublet with E=9908.5 resolved by a difference of 0.3 {I1} in energy from (p,|g), however the intensity of |g-rays from the levels was not separated. 
J$9/2 for E=9907.5 from 6492|g-2148|g(|q) and 3/2 for 9908.5 from 9905.8|g(|q) in (p,|g) imply this resonance is a doublet (1968Bo13). 3/2- from R-Matrix analysis in (p,p):resonances for E=9907 {I3} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$from (p,p):resonances. Other: 9999.4 {I21} from (p,|g) 
T$weighted average of 5.3 keV {I16} from (p,|g) and 8.0 keV {I8} from (p,p):resonances 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$|g rays to (5/2)+ and 3/2+; (1/2,3/2+) from DWBA analysis of |s in (|a,p) for a group at E=10080 


level_energy_unit: KEV
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$(3/2)+ from (p,p):resonances, which however is excluded by 4197.2|g to 9/2+ based on measured proton resonance strength and RUL. This could imply a doublet 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$3/2- from (p,p):resonances, which however is excluded by 4206.9|g to 9/2+ based on measured proton resonance strength and RUL. This could imply a doublet 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$6729.1|g to 7/2+, 10142.7|g to 1/2+. 
J$10142.7|g to 1/2+ excludes J=7/2 (M3 or E3) based on measured proton resonance strength and RUL 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$parity from 6777.6|g to 7/2+, however, J=3/2 is excluded by 4300.8|g to 9/2+ based on measured proton resonance strength and RUL. This contradicting results could indicate this level is a doublet 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$7/2 from 7977|g(|q) in (p,|g), which is however disfavored by the strong 10210|g to 1/2+. 


level_energy_unit: KEV
level_spin_parity: (15/2)-
level_lifetime_unit: FS
level_comment:
J$3392.8|g E2, |DJ=2 to 11/2-, 1041.7|g M1+E2 to J=(13/2). Other: 13/2- proposed in ({+20}Ne,p|g) is inconsistent. 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$4695|g to 3/2+ favors 7/2+, which however is disfavored by 10223|g to 1/2+. 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$10233|g to 1/2+; D |g to 3/2+; |g to 5/2+. 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_lifetime_unit: PS
level_comment:
J$1815.2|g |DJ=1 to (13/2-); 3078.1|g to 11/2+. 15/2+ proposed in ({+16}O,2|ap|g) but 15/2(-) in ({+20}Ne,p|g) is inconsistent. 
T$from DSAM in ({+16}O,2|ap|g). 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J$776.8|g M1+E2, |DJ=1 to (15/2+); 17/2+ proposed in ({+16}O,2|ap|g) but 17/2- in ({+20}Ne,p|g) is inconsistent 
T$from DSAM in ({+16}O,2|ap|g). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):resonances. Other: 11871 {I4} from (|a,p):resonances 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 12039 {I4} from (|a,p):resonances and 12043 {I2} from (p,|a):resonances 
T$from (|a,p):resonances. Other: <5 keV from (p,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
E$weighted average of 12050 {I4} from (|a,p):resonances and 12053 {I2} from (p,|a):resonances 
T$from (p,|a):resonances. Other: <5 keV from (|a,p):resonances 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$from (p,|a):resonances. Other: 12072 {I4} from (|a,p):resonances 
T$weighted average of 10 keV {I4} (|a,p):res, 3 keV {I2} (p,|a):res. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,|a):res. Others: 12077 {I2} from (|a,|g):res, 12078 {I4} from (|a,p):res. 
T$from (p,|a):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Other: 12151 {I4} from (|a,p):res 
T$from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$weighted average of 12187 {I4} from (|a,p):res and 12180 {I2} from (p,|a):res 
T$from (|a,p):res. Other: <10 keV from (p,|a):res 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g). Others: 12202 {I4} from (|a,p):res, 12200 {I2} from (p,|a):res 
T$from (p,|a):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Other: 12219 {I2} from (p,|a):res 
T$from (p,|g):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$weighted average of 12250 {I4} from (|a,p):res and 12256 {I2} from (p,|a):res 
T$weighted average of 7 keV {I4} from (|a,p):res and 8 keV {I4} from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$from (p,|a):res. Other: 12266 {I4} from (|a,p):res 
T$from (|a,p):res. Other: 12266 {I4} from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Others: 12310 {I4} from (|a,p), 12308 {I2} from (p,|a) 
T$from (p,|a):res. Other: <8 keV from (|a,p):res 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Others: 12333 {I4} from (|a,p), 12331 {I2} from (p,|a) 
T$from (p,|a):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_spin_parity: (5/2:11/2)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Other: 12376 {I4} from (|a,p):res 
T$from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g). Others: 12386 {I4} from (|a,p):res, 12385 {I2} from (p,|a):res 
T$from (p,|a):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$from (p,|a):res. Other: 12394 {I4} from (|a,p):res 
T$from (p,|a):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Others: 12418 {I4} from (|a,p):res, 12418 {I2} from (p,|a):res 
T$from (|a,p):res and (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$from (p,|a):res. Other: 12430 {I4} from (|a,p):res 
T$from (|a,p):res. Other: <5 keV from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$from (p,|a):res. Other: 12434 {I4} from (|a,p):res 
T$from (p,|a):res. Other: <7 keV from (|a,p):res 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res and (p,|a):res. Other: 12447 {I4} from (|a,p):res 
T$from (p,|a):res. Other: <5 keV from (|a,p):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res and (p,|a):res. Other: 12459 {I4} from (|a,p):res 
T$from (|a,p):res. Other: <10 keV from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Others: 10482 {I2} from (p,|a):res, 12459 {I4} from (|a,p):res 
T$from (|a,p):res. Other: <8 keV from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 12496 {I2} from (|a,|g):res, 12495 {I2} from (p,|a):res, and 12494 {I4} from (|a,p):res 
T$weighted average of 15 keV {I4} from (|a,p):res and 12 keV {I2} from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$from (p,|a):res. Other: 12511 {I4} from (|a,p):res 
T$from (|a,p):res. Other: <12 keV from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$from (p,|a):res. Other: 12530 {I4} from (|a,p):res 
T$from (|a,p):res. Other: <8 keV from (p,|a):res 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Other: 12550 {I4} from (|a,p):res 
T$from (|a,p):res. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$spin from |g|g(|q) in 1958Br98, 1963Ha25; parity from 1266|g M1+E2 to 1/2+ 
T$average |t=514 fs {I178} from 390 fs {I170} (1975De31), 770 fs {I244} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$spin from |g|g(|q) in 1958Br98, 1963Ha25; parity from 2233.8|g E2 to 1/2+ 
T$average |t=388 fs {I110} from 340 fs {I125} (1975De31), 425 fs {I110} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q,pol) of 4649|g from 7782,3/2- resonance level in 1964Va09; 1/2 from |g|g(|q) in 1963Ha25 and 1966Va08. Other: 3/2 from |g|g(|q) in 1958Br98 is inconsistent 
T$average |t=10.2 fs {I45} from 14 fs {I6} (1975De31), 8.0 fs {I45} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$polarization measurements show even parity (1967Wi10); J=5/2 from |g|g(|q) in 1958Br98, 1963Ha25, 1966Ha20, 1966Va08 
T$average |t=105 fs {I35} from 78 fs {I35} (1975De31), 135 fs {I37} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$polarization measurements show even parity (1967Wi10); spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11, 1966Va08 
T$average |t=290 fs {I90} from 445 fs {I180} (1975De31), 300 fs {I90} (1968Wo01), 230 fs {I100} (1968En03) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$polarization measurements show even parity (1967Wi10); spin from |g|g(|q) in 1958Br98, 1963Ha25, 1966Ha20, 1966Va08 
T$from |t=12 fs {I6} (1975De31). Other: |t=13 fs {I8} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$spin from |g(|q) and |g|g(|q) in 1958Br98, 1963Ha25; parity from 2924.6|g M1+E2 to 3/2+ 
T$from |t=7 fs {I3} (1975De31). Other: |t<23 fs (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$spin from |g|g(|q) in 1963Ha25; |p=+ from |g(|q,pol) in 1967Wa10 
T$from |t=15.0 fs {I6} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$from primary 4482|g(lin pol) in 1964Ha27 
T$average of |t=453 fs {I179} from 410 fs {I140} (1975De31), 1200 fs {I583} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: FS
level_comment:
J$from |g|g(|q) in 1966Ha20. See comment for 4634 level 
T$average |t=18 fs {I7} from 16 fs {I6} (1975De31), 44 fs {I22} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_lifetime_unit: FS
level_comment:
J$from |g(|q) and |g|g(|q) in 1969Wo01. 3/2 from |g|g(|q) data of 1966Ha20 is most likely for 4592 level probably due to misidentification of |g rays because of poor resolution in |g-ray spectrum. 
T$average |t=122 fs {I39} from 145 fs {I40} (1975De31), 100 fs {I39} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$spin from |g|g(|q) in 1967Wi10; parity from 4783.4|g E2 to 1/2+ 
T$average |t=10 fs {I4} from 10 fs {I4} (1975De31), 14 fs {I12} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_lifetime_unit: FS
level_comment:
J$(1/2,3/2,5/2) from |g|g(|q) in 1963Ha25, 5/2 excluded by strong primary transitions from 1/2- resonance and 5015|g(|q) (1969Wo01) 
T$average |t=54 fs {I17} from 45 fs {I17} (1975De31), 67 fs {I20} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_lifetime_unit: FS
level_comment:
J$|>5/2 excluded by strong primary transitions from 1/2- resonance and 5015|g(|q) (1969Wo01) 
T$average |t=10.9 fs {I74} from 12 fs {I8} (1975De31), 10.0 fs {I74} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$other: 5557 {I2} (1968Wo01) 
J$3/2,5/2,7/2 from primary |g(|q) from J=5/2 resonance at 8910, 5/2 and 7/2 ruled out based on primary |g's from 1/2+ resonances in (p,|g) (1969Wo01) 
T$from |t<25 fs (1969Wo01) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_comment:
E$from 1968Wo01. Other: 5672.1 {I20} (1975De31) 
J$from primary |g(|q) from J=5/2 resonance at 8910, 4405|g(|q) and 3438|g(|q) (1969Wo01) 
T$average |t=36 fs {I8} from 35 fs {I8} (1975De31), 45 fs {I20} (1969Wo01) 


level_energy_unit: KEV
level_spin_parity: +
level_lifetime_unit: FS
level_comment:
E$other: 5892 {I2} (1968Wo01) 
T$average |t=38 fs {I12} from 36 fs {I12} (1975De31), 80 fs {I63} (1968En03) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_lifetime_unit: FS
level_comment:
E$from 1968Wo01. Other: 6399.3 {I20} (1975De31) 
J$from primary |g(|q) from J=7/2 resonance at 8224, 1968|g(|q) and and |g's to 5/2+ and 7/2- level (1969Wo01) 
T$from |t=70 fs {I35} (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$other: 6932 {I3} (1968Wo01) 
J$from 4697.2|g(|q) and |g to 7/2- (1969Wo01) 
T$from |t<40 fs (1968Wo01) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_comment:
$S{-p|g}(eV)=2.28|*10{+-4} {I25} 
E$from 2020De26 based on E|g data, corresponding to E(p)(lab)=434.6 {I3} 
J$proposed in 2020De26 based on |g-decay patterns 
S$from 2020De26 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$S{-p|g}(eV)=0.376 {I28} 
E$from 2020De26 based on E|g data, corresponding to E(p)(lab)=501.1 {I2} 
J$|p=- from |g(pol) in 1966Va08; 3/2 from |g(|q) (1958Br98,1966Va08). 
$E(p)(lab)=498.3 {I10} (1959Ku79) 
S$from 2020De26. Others: 0.33 eV {I5} (1979Ri01), 0.18 eV (1966Va08) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: EV
level_comment:
$S{-p|g}(eV)=3.44 {I24} 
E$from 2020De26 based on E|g data, corresponding to E(p)(lab)=621.7 {I3} 
J$from isotropic |g(|q) (1958Br98) 
$E(p)(lab)=619.6 {I12} (1959Ku79) 
S$weighted average of 3.10 {I26} (1958Sm95), 3.22 eV {I24} (1963Ha25), 3.4 {I8} (1968Ho06), 3.93 {I40} (1969Ly03), 3.88 {I27} (1979Pa16). Other: 5.0 {I3} (1979Ri01) is discrepant 
$|G=54 eV {I14}, unweighted average of 68 eV {I9} (1968Ho06), 40 eV {I7} (1958Sm95) 
$|G{-|g0}=1.54 eV {I12}, weighted average of 1.6 eV {I2} (1968Ho06), 1.52 eV {I12} (1958Sm95) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=0.20 
$|G{-|g}|>0.033 eV (2005Vo24) 
J$from |g(|q) in 1958Br98 
S$from 2005Vo24 
$E(p)(lab)=759.3 {I9} (1959Ku79) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.2 {I2} 
J$from |g(|q) in 1958Br98 
$|G{-|g}|>0.25 eV (2005Vo24) 
S$from 1979Ri01. Other: 1.0 eV (2005Vo24) 
$E(p)(lab)=776.4 {I10} (1959Ku79) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=0.31 {I9} 
J$from |g(|q) in 1958Br98 
$|G{-|g}|>0.073 eV (2005Vo24) 
S$from 1969Wo01. Other: 0.44 eV (2005Vo24) 
$E(p)(lab)=834.2 {I13} (1959Ku79) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: EV
level_comment:
$S{-p|g}(eV)=1.4 {I4} 
$|G=2.6 eV {I2} (1968Ho06), |G{-|g0}=1.4 eV {I1} (1968Ho06) 
J$from |g(|q) in 1958Br98 
$E(p)(lab)=942 {I1} (1968Wo01). Other: 955 (1958Br98) 
S$from 1969Wo01. Other: 2.0 {I3} (1979Ri01) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$S{-p|g}(eV)=0.36 {I6} 
J$from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11 
$E(p)(lab)=1175.6 {I7} (1964Va11). Other: 1177 {I20} (1961Ba03) 
S$weighted average of 0.38 eV {I6} (1963Ha25), 0.29 eV {I10} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$S{-p|g}(eV)=1.24 {I12} 
J$polarization measurements establish even parity (1967Wi10); spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11, 1961Va15 
$E(p)(lab)=1203.6 {I7} (1964Va11). Other: 1204 {I20} (1961Ba03) 
S$weighted average of 1.26 eV {I12} (1963Ha25), 1.1 eV {I3} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=0.9 {I3} 
$1/2+ spin assignment in 1964Va11 to this level is perhaps in error 
$|G=0.7 keV {I4} (1964Va11) 
$E(p)(lab)=1297.9 {I8} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$S{-p|g}(eV)=2.00 {I18} 
$E(p)(lab)=1322.1 {I8} (1964Va11). Other: 1322 {I20} (1961Ba03) 
J$spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11, 1961Va15; parity from |g(|q,pol) in 1967Wi10 
S$weighted average of 2.04 eV {I18} (1963Ha25), 1.6 eV {I6} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=3.04 {I30} 
$E(p)(lab)=1389.9 {I8} (1964Va11). Other: 1393 {I20} (1961Ba03) 
J$spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va111, 1961Va15 
S$weighted average of 3.12 eV {I30} (1963Ha25), 2.5 eV {I8} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=2.48 {I24} 
$E(p)(lab)=1398.4 {I8} (1964Va11) 
J$spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11, 1961Va15 
S$weighted average of 2.44 eV {I24} (1963Ha25), 3.1 eV {I10} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=3.9 {I5} 
$E(p)(lab)=1480.7 {I9} (1964Va11) 
J$spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11 
S$weighted average of 4.0 eV {I5} (1963Ha25), 3.4 eV {I11} (1964Va11) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=2.8 {I5} 
$E(p)(lab)=1482.2 {I9} (1964Va11). Other: 1483 {I20} (1961Ba03) 
J$spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11, 1961Va15 
S$weighted average of 4.8 eV {I9} (2009Ka37), 2.52 eV {I36} (1963Ha25), 2.3 eV {I8} (1964Va11). Other: 8.0 eV for E(p)=1480+1482 doublet (2005Vo24) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.92 {I20} 
J$spin from |g(|q) and |g|g(|q) in 1963Ha25, 1964Va11 
$|G{-|g}=0.5 eV {I2} (2005Vo24) 
$E(p)(lab)=1489.9 {I9} (1964Va11) 
S$weighted average of 2.0 eV {I2} (2009Ka37), 1.92 eV {I20} (1963Ha25), 2.0 eV {I6} (2005Vo24), 1.4 eV {I5} (1964Va11) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.050 {I15} 
$E(p)(lab)=1507 {I1} (2005Vo24). Other: 1506.7 {I9} (1964Va11), very weak 
S$other: 0.07 eV(2005Vo24) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$S{-p|g}(eV)=3.25 {I30} 
$|G{-|g}=0.72 eV (2005Vo24) 
J$even parity from |g(lin pol) (1967Wi10); spin from |g(|q) and |g|g(|q) in 1963Ha25 
$E(p)(lab)=1509.9 {I9} (1964Va11). Other: 1507 {I20} (1961Ba03) 
S$weighted average of 3.36 eV {I30} (1963Ha25), 2.5 eV {I8} (1964Va11). Other: 3.5 eV (2005Vo24) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=0.60 {I18} 
J$from |g(|q) in 1961Va15 
T$from 1964Va11 
$|G from 1964Va11 
$|G{-|g}=0.4 eV (2005Vo24) 
$E(p)(lab)=1516.1 {I9} (1964Va11) 
S$other: 0.8 eV (2005Vo24) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=0.6 {I2} 
$E(p)(lab)=1660.4 {I10} (1966Va07). Other: 1662 {I20} (1961Ba03) 
$|G from 1966Va07 
S$from 1966Va07 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.7 {I5} 
$E(p)(lab)=1694.4 {I10} (1966Va07). Other: 1693 {I20} (1961Ba03) 
S$from 1966Va07 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=0.3 {I1} 
$E(p)(lab)=1746.1 {I10} (1966Va07) 
$|g only seen by 1968Wo01 and they state 40% of the |g branching is unknown 
S$from 1966Va07 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=2.6 {I2} 
$|G{-|g}=0.47 eV {I14} (2004Vo22) 
$E(p)(lab)=1770.1 {I10} (1966Va07). Other: 1768 {I20} (1961Ba03) 
$|G from 1966Va07 
S$weighted average of 2.6 eV {I2} (2009Ka37), 2.8 eV {I8} (2004Vo22), 2.0 eV {I6} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=3.5 {I9} 
$|G{-|g}=1.10 eV {I11} (2004Vo22) 
$E(p)(lab)=1808.4 {I11} (1966Va07). Other: 1811 {I20} (1961Ba03) 
$|G from 1966Va07 
S$weighted average of 4.4 eV {I13} (2004Vo22), 3.1 eV {I9} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
$S{-p|g}(eV)=0.7 {I2} 
J$from Adopted Levels. J=9/2 proposed by 1966Va07 based on Mult(6868|g)=Q, |DJ=2 deduced from 6818|g-2234|g(|q) which, however, could be also consistent with |DJ=0. J=9/2 assignment is inconsistent with observed transitions to 3/2+ levels 
$E(p)(lab)=1815.2 {I11} (1966Va07) 
S$from 1966Va07. Other: 1.0 eV (2004Vo22) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$S{-p|g}(eV)=2.8 {I5} 
$|G{-|g}=0.57 eV {I18} (2004Vo22) 
$E(p)(lab)=1830.1 {I11} (1966Va07). Other: 1828 {I20} (1961Ba03) 
T$from |t<37 fs (1969Wo01) 
S$weighted average of 2.9 eV {I5} (2009Ka37),3.4 eV {I10} (2004Vo22), 2.4 eV {I7} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$S{-p|g}(eV)=0.74 {I19} 
$|G{-|g}=0.12 eV {I12} (2004Vo22) 
$E(p)(lab)=1877.9 {I6} (1975De31). Others: 1876.0 {I15} (1967Bo12), 1875.6 {I11} (1966Va07), 1874 {I20} (1961Ba03) . 
S$weighted average of 0.63 eV {I19} (1975De31), 1.2 eV {I6} (1967Bo12), and 0.9 eV {I3} (1966Va07). Other: 0.88 eV (2004Vo22) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=4.5 {I6} 
$|G{-|g}=0.83 eV {I26} (2004Vo22) 
$E(p)(lab)=1880.1 {I6} (1975De31). Others: 1878.0 {I15} (1967Bo12), 1878.3 {I11} (1966Va07) 
S$weighted average of 5.4 eV {I6} (2009Ka37), 3.4 eV {I11} (1975De31), 4.8 eV {I14} (2004Vo22), 4.0 eV {I20} (1967Bo12), 3.1 eV {I9} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=0.54 {I13} 
$|G{-|g}=0.10 eV {I7} (2004Vo22) 
$E(p)(lab)=1893.5 {I6} (1975De31). Others: 1893.0 {I15} (1967Bo12), 1891.6 {I12} (1966Va07), 1890 {I20} (1961Ba03) 
S$weighted average of 0.42 eV {I13} (1975De31), 0.59 eV {I17} (2004Vo22), 0.70 eV {I35} (1967Bo12), 0.7 eV {I2} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=1.1 {I3} 
$|G{-|g}=0.23 eV {I12} (2004Vo22) 
$E(p)(lab)=1896.0 {I6} (1975De31). Others: 1895.0 {I15} (1967Bo12), 1895.2 {I12} (1966Va07) 
S$weighted average of 1.0 eV {I3} (1975De31), 1.4 eV {I4} (2004Vo22), 1.1 eV {I6} (1967Bo12), and 1.1 eV {I3} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$S{-p|g}(eV)=0.59 {I15} 
$E(p)(lab)=1920.1 {I6} (1975De31). Others: 1918.0 {I15} (1967Bo12), 1918.2 {I12} (1966Va07), 1917 {I20} (1961Ba03) 
S$weighted average of 0.51 eV {I15} (1975De31), 0.70 eV {I35} (1967Bo12), 0.7 eV {I2} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.5 {I4} 
$E(p)(lab)=1922.2 {I6} (1975De31). Others: 1921.0 {I15} (1967Bo12), 1920.4 {I12} (1966Va07) 
S$weighted average of 1.2 eV {I4} (1975De31), 3.0 eV {I15}, and 1.9 eV {I6} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=1.06 {I28} 
$E(p)(lab)=1942.6 {I6} (1975De31). Others: 1939.0 {I16} (1967Bo12), 1941.6 {I12} (1966Va07), 1939 {I20} (1961Ba03) 
$|G from 1966Va07 
S$weighted average of 0.94 eV {I28} (1975De31), 1.3 eV {I4} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$S{-p|g}(eV)=0.48 {I4} 
$E(p)(lab)=1973.7 {I6} (1975De31). Others: 1972.0 {I16} (1967Bo12), 1971.7 {I12} (1966Va07), 1970 {I20} (1961Ba03) 
S$weighted average of 0.48 eV {I4} (1975De31), 0.70 eV {I35} (1967Bo12), and 0.50 eV {I15} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=0.72 {I20} 
$E(p)(lab)=1994.6 {I6} (1975De31). Others: 1994.0 {I16} (1967Bo12), 1992.0 {I12} (1966Va07), 1990 {I20} (1961Ba03) 
$|G from 1966Va07 
S$weighted average of 0.66 eV {I20} (1975De31), 0.70 eV {I35} (1967Bo12), and 0.80 eV {I24} (1966Va07) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.5 {I4} 
$E(p)(lab)=2009.5 {I7} (1975De31). Others: 2007.0 {I16} (1967Bo12), 2004 {I20} (1961Ba03) 
S$weighted average of 1.4 eV {I4} (1975De31), 3.0 eV {I15} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.77 {I25} 
$E(p)(lab)=2022.1 {I7} (1975De31). Others: 2021.0 {I16} (1967Bo12), 2019 {I20} (1961Ba03) 
S$weighted average of 0.73 eV {I25} (1975De31), 0.90 eV {I45} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.73 {I23} 
$E(p)(lab)=2025.2 {I7} (1975De31), 2024.0 {I16} (1967Bo12) 
S$weighted average of 0.70 eV {I23} (1975De31), 0.8 eV {I4} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=1.1 {I3} 
$|G from 1988Va06. Other: 4.5 keV {I14} (1967Bo12) 
J$from |g(|q) (1975De31) 
$E(p)(lab)=2061.3 {I7} (1975De31). Others: 2060.0 {I16} (1967Bo12), 2057 {I20} (1961Ba03) 
S$weighted average of 1.1 eV {I3} (1975De31), 1.0 eV {I5} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=0.55 {I16} 
$E(p)(lab)=2091.0 {I8} (1975De31). Others: 2090.0 {I17} (1967Bo12), 2087 {I20} (1961Ba03) 
S$weighted average of 0.52 eV {I16} (1975De31), 0.70 eV {I35} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.25 {I15} 
$E(p)(lab)=2130.9 {I8} (1975De31). Others: 2130.0 {I17} (1967Bo12), 2129 {I20} (1961Ba03) 
S$unweighted average of 0.39 eV {I13} (1975De31), 0.10 eV {I5} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.93 {I30} 
$E(p)(lab)=2133.7 {I8} (1975De31), 2133.0 {I17} (1967Bo12) 
S$weighted average of 1.1 eV {I3} (1975De31), 0.70 eV {I35} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.37 {I11} 
$E(p)(lab)=2173.9 {I8} (1975De31), 2173.0 {I17} (1967Bo12) 
S$weighted average of 0.35 eV {I11} (1975De31), 0.50 eV {I25} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$S{-p|g}(eV)=10.2 {I16} 
$|G{-|g}=1.63 eV {I25}, |G{-p}=500 eV {I80} (2002Vo17) 
$B(M1)=98 {I15} (2005Vo24) 
J$from 4982|g(lin pol) in 1964Ha27 
$E(p)(lab)=2187.0 {I8} (1975De31). Others: 2086.0 {I17} (1967Bo12), 2183 {I20} (1961Ba03) 
S$weighted average of 8.7 eV {I16} (2009Ka37), 9.4 eV {I31} (1975De31), 13.0 eV {I20} (2002Vo17), 6 eV (1964Ha03), 11 eV {I3} (1969Wo01), 8.5 eV {I43} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.7 {I3} 
$E(p)(lab)=2216.3 {I9} (1975De31). Others: 2215.0 {I18} (1967Bo12), 2215 {I20} (1961Ba03) 
S$weighted average of 1.9 eV {I2} (2009Ka37), 1.1 eV {I3} (1975De31), 2.3 eV {I12} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=2.1 {I6} 
$E(p)(lab)=2224.7 {I9} (1975De31), 2223.0 {I18} (1967Bo12) 
S$weighted average of 2.0 eV {I6} (1975De31), 2.8 eV {I14} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.27 {I8} 
$E(p)(lab)=2253.7 {I9} (1975De31), 2254.0 {I18} (1967Bo12) 
S$weighted average of 0.25 eV {I8} (1975De31), 0.4 eV {I2} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$S{-p|g}(eV)=1.3 {I6} 
J$parity from 5333.2|g M1+E2 to 5/2+ 
$E(p)(lab)=2303.0 {I9} (1975De31). Others: 2302.0 {I18} (1967Bo12), 2300 {I20} (1961Ba03) 
S$weighted average of 1.2 eV {I4} (1975De31), 4.3 eV {I22} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_comment:
$S{-p|g}(eV)=1.2 {I3} 
E$unresolved doublet (1975De31) 
$E(p)(lab)=2315.2 {I10} (1975De31). Others: 2315.0 {I19} (1967Bo12), 2311 {I20} (1961Ba03) 
S$weighted average of 1.1 eV {I3} (1975De31), 1.6 eV {I8} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=3.0 {I7} 
$E(p)(lab)=2350.4 {I10} (1975De31), 2352.0 {I19} (1967Bo12) 
S$weighted average of 3.9 eV {I8} (2009Ka37), 2.2 eV {I7} (1975De31), 6.3 eV {I32} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$S{-p|g}(eV)=1.1 {I3} 
$E(p)(lab)=2357.9 {I10} (1975De31), 2358.0 {I19} (1967Bo12) 
S$weighted average of 1.0 eV {I3} (1975De31), 1.4 eV {I7} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=2.6 {I2} 
$|G from 1967Bo12 
J$spin from |g(|q) (1975De31) 
$E(p)(lab)=2365.4 {I10} (1975De31), 2364.0 {I19} (1967Bo12) 
S$weighted average of 2.6 eV {I2} (2009Ka37), 2.9 eV {I9} (1975De31), 2.9 eV {I15} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.2 {I3} 
$E(p)(lab)=2374.5 {I10} (1975De31), 2375.0 {I19} (1967Bo12) 
S$weighted average of 1.1 eV {I3} (1975De31), 1.7 eV {I9} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=0.20 {I6} 
J$from |g(|q) (1975De31) 
$E(p)(lab)=2379.3 {I10} (1975De31), 2379.0 {I19} (1967Bo12) 
S$weighted average of 0.18 eV {I6} (1975De31), 0.4 eV {I2} (1967Bo12) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=0.43 {I21} 
E$1975De31 claim this resonance must be a doublet due to |g(|q) data of 9610.3|g and 8344.6|g (excluding J|<5/2) inconsistent with 3230.9|g to 3/2+ (excluding J|>7/2) 
$E(p)(lab)=2393.2 {I10} (1975De31), 2392.0 {I19} (1967Bo12) 
S$weighted average of 0.75 eV {I23} (1975De31), 0.30 eV {I15} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 1/2
level_comment:
$S{-p|g}(eV)=7.3 {I5} 
E$unresolved doublet (1975De31) 
S$weighted average of 7.4 eV {I3} (2009Ka37), 4.4 eV {I17} (1975De31), 4.3 eV {I22} (1967Bo12) 
$E(p)(lab)=2505.4 {I10} (1975De31). Others: 2504.0 {I20} (1967Bo12), 2510 {I20} (1961Ba03) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
$S{-p|g}(eV)=10 {I5} 
E$Doublet with E=9908.5 resolved by a difference of 0.3 {I1} in energy in 1968Bo13, however the intensity of |g-rays from the levels was not separated. 
J$9/2 for E=9907.5 from 6492|g-2148|g(|q) and 3/2 for 9908.5 from 9905.8|g(|q) imply this resonance is a doublet (1968Bo13). 
$E(p)(lab)=2698.0 {I22} and 2699.0 {I22} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=1.4 {I7} 
$This level is exceptional in that it decays with equal intensity to all levels with excitation energy less than 5 MeV, except for the level at 4.64 MeV (1968Bo13). 
$E(p)(lab)=2717.0 {I22} (1967Bo12). Other: 2716 {I20} (1961Ba03) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=1.2 {I6} 
$|G from 1967Bo12 
$E(p)(lab)=2756.0 {I22} (1967Bo12). Other: 2753 {I20} (1961Ba03) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=1.1 {I6} 
$|G from 1967Bo12 
$E(p)(lab)=2914.0 {I23} (1967Bo12). Other: 2910 {I20} (1961Ba03) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$S{-p|g}(eV)=0.8 {I4} 
$|G from 1967Bo12 
$E(p)(lab)=2952.0 {I24} (1967Bo12). Other: 2952 {I20} (1961Ba03) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=6.3 {I32} 
J$also from |g(|q) in 1969Wi02 
$E(p)(lab)=2993.0 {I24} (1967Bo12), 2995 {I3} (1969Wi02) 


level_energy_unit: KEV
level_comment:
$S{-p|g}(eV)=4 {I2} 
$E(p)(lab)=3008.0 {I24} (1967Bo12). Other: 3006 {I20} (1961Ba03) 
$Resonance Strength|?4 eV {I2} (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$S{-p|g}(eV)=5.9 {I30} 
$E(p)(lab)=3011.0 {I24} (1967Bo12). Other: 3011 {I3} (1969Wi02) 
$Resonance Strength|?5.9 eV 30 (1967Bo12) 


level_energy_unit: KEV
level_spin_parity: 7/2
level_comment:
$S{-p|g}(eV)=2.9 {I15} 
$E(p)(lab)=3027.0 {I24} (1968Bo13), 3027 {I3} (1969Wi02) for probable doublet. Other: 3022 {I20} (1961Ba03) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.413 ps {I31} from 2021To09, 0.50 ps {I6} (gating on 2029 |g 1266 |g below level and corrected for side feeding) and 0.46 ps {I10} (gating on 2394|g above level) from 2008Pa27. 


level_energy_unit: KEV
level_spin_parity: (3/2,7/2-,9/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=0.34 
$E|a(lab)=1893 {I4} 
$A{-2}=+0.70 {I4}, A{-4}=-0.02 {I6}, A{-6}=0.000 {I1} 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=0.77,0.22 
$E|a(lab)=2223 {I4} 
$A{-2}=+0.44 {I10} 
$|G|a=0.25 eV {I5}, |G{-p0}=8 keV {I4}, |G{-p1}=2.2 keV {I11} 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=1.3,0.61 
$E|a(lab)=2280 {I4} 
$A{-2}=+0.89 {I2}, A{-4}=+0.33 {I4}, A{-6}=+0.09 {I3} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=1.2,9.5 
$E|a(lab)=2476 {I4} 
$A{-2}=+0.14 {I4}, A{-4}=-0.25 {I5} for complex resonance 


level_energy_unit: KEV
level_spin_parity: (3/2,7/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=1.1,14 
$E|a(lab)=2679 {I4} 
$A{-2}=+0.70 {I3}, A{-4}=-0.03 {I5}, A{-6}=0.000 {I1} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=18,18 
$E|a(lab)=2722 {I4} 
$A{-2}=+0.21 {I3}, A{-4}=-0.68 {I4}, A{-6}=+0.13 {I5} for complex resonance 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=28,4.4 
$E|a(lab)=2783.2 {I10} 
$A{-2}=+0.54 {I2}, A{-4}=-0.31 {I3}, A{-6}=+0.044 {I7} 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=10,48 
$E|a(lab)=2822 {I4} 
$A{-2}=+0.94 {I3}, A{-4}=+0.41 {I7}, A{-6}=-0.02 {I7}, A{-8}=+0.002 {I9} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=24,11 
$E|a(lab)=2861 {I4} 
$A{-2}=-0.35 {I3}, A{-4}=+0.13 {I4} for complex resonance 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=28,18 
$E|a(lab)=2870 {I4} 
$A{-2}=+0.32 {I5}, A{-4}=-0.73 {I6}, A{-6}=+0.26 {I7} for complex resonance 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=10,<7 
$E|a(lab)=2909 {I4} 
$A{-2}=+1.054 {I9}, A{-4}=+0.68 {I2}, A{-6}=+0.26 {I3}, A{-8}=+0.006 {I5}, A{-10}=+0.05 {I4} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=56,60 
$E|a(lab)=2931.9 {I10} 
$A{-2}=+0.14 {I4}, A{-4}=+0.14 {I4} for complex resonance 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=330,140 
$E|a(lab)=3120 {I4} 
$A{-2}=-1.09 {I1}, A{-4}=+0.29 {I2} for complex resonance 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=69,130 
$E|a(lab)=3130 {I4} 
$A{-2}=+0.74 {I6}, A{-4}=-0.37 {I7} for complex resonance 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=53,240 
$E|a(lab)=3157 {I4} 
$A{-2}=-0.12 {I3}, A{-4}=-0.41 {I4} for complex resonance 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=72,85 
$E|a(lab)=3171 {I4} 
$A{-2}=+0.13 {I2}, A{-4}=+0.08 {I3} for complex resonance 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=120,42 
$E|a(lab)=3190 {I4} 
$A{-2}=+0.43 {I2}, A{-4}=-0.49 {I3}, A{-6}=+0.116 {I11} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=163,<10 
$E|a(lab)=3244 {I4} 
$A{-2}=+0.36 {I3}, A{-4}=+0.06 {I3} for complex resonance 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-|a}|G{-p}/|G=7.7,29 
$E|a(lab)=3286 {I4} 
$A{-2}=-0.04 {I4}, A{-4}=+0.16 {I6} for complex resonance 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 527 fs {I33} (1979Po01), 555 fs {I152} (1974Tw01), 451 fs {I153} (1970Va12), 555 fs {I56} (1969Cu01), and 485 fs {I49} (1979Fo02), all by DSAM 
$g-factor=+0.20 {I5}, from precession angle (1982Ho06) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 236 fs {I21} (1974Tw01), 208 fs {I79} (1970Va12), 263 fs {I21} (1969Cu01), 252 fs {I17} (1979Fo02), and 271 fs {I18} (1979Po01), all by DSAM 
$g factor=+1.13 {I18}, from precession angles (1982Ho06) 


level_energy_unit: KEV
level_spin_parity: 7/2+,(5/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
J$proposed by 1974Tw01 from |g(|q), with 5/2 being rejected only at the 1% confidence limit; however, 7/2+ is in disagreement with adopted (5/2)+ 


level_energy_unit: KEV
level_comment:
L$also from 1975Na09 
$|s{-exp}/|s{-DWBA}=0.61 (1982Al28), 0.91 (1975Na09), 0.85 or 0.92 (1978Al17) 
$|s{-max}=938 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$other: 2(+0) (1975Na09) 
$|s{-exp}/|s{-DWBA}=1.24 (1982Al28), 1.27 (1975Na09), 0.79 (1978Al17) 
$|s{-max}=111 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$other: 2 (1975Na09) 
$|s{-exp}/|s{-DWBA}=3.3 (1982Al28), 3.54 (1975Na09), 0.07 (1978Al17) 
$|s{-max}=61 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$from other: 0+2 (1975Na09) 
$|s{-exp}/|s{-DWBA}=3.75 (1982Al28), 2.09 (1975Na09,tentative), 5.40 or 2.19 (1978Al17) 
$|s{-max}=325 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$other: 2 (1975Na09) 
$|s{-exp}/|s{-DWBA}=0.41 (1982Al28), 0.45 (1975Na09), 0.17 (1978Al17) 
$|s{-max}=227 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3415 {I9} (1969Mo03), 3418 {I5} (1978Al17) 
L$also from 1975Na09 
$|s{-exp}/|s{-DWBA}=0.96 (1982Al28), 3.64 (1975Na09,tentative), 0.14 (1978Al17) 
$|s{-max}=14 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3507 {I9} (1969Mo03), 3509 {I5} (1978Al17) 
L$from 1975Na09. Other: 0(+2) from 1978Al17 
$|s{-exp}/|s{-DWBA}=0.74 (1982Al28), 0.91 (1975Na09,tentative), 0.23 or 0.16 (1978Al17) 
$|s{-max}=148 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4191 {I9} (1969Mo03), 4189 {I5} (1978Al17) 
L$also from 1975Na09 
$|s{-exp}/|s{-DWBA}=2.32 (1975Na09), 0.18 (1978Al17) 
$|s{-max}=38 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4260 {I9} (1969Mo03), 4259 {I5} (1978Al17) 
L$other: 2(+0) (1975Na09) 
$|s{-exp}/|s{-DWBA}=8.65 (1975Na09,tentative), 0.32 (1978Al17) 
$|s{-max}=64 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4435 {I9} (1969Mo03), 4428 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.36 (1978Al17) 
$|s{-max}=98 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$weighted average of 4595 {I9} (1969Mo03), 4594 {I5} (1978Al17) 
L$other: (0) from 1975Na09 perhaps unresolved from 4630 
$|s{-max}=23 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4646 {I9} (1969Mo03), 4640 {I5} (1978Al17) 
L$other: (4) (1975Na09) 
$|s{-exp}/|s{-DWBA}=0.32 (1978Al17) 
$|s{-max}=12 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$from 1975Na09. Other: (2+4) from 1978Al17 
E$weighted average of 4783 {I9} (1969Mo03), 4779 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.78 (1975Na09) 
$|s{-max}=7 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E,L$doublet from L=1(+0) (1978Al17) or 1+3 (1975Na09) for 5010+5020 doublet 
E$weighted average of 5016 {I9} (1969Mo03), 5010 {I5} (1978Al17) 
$|s{-max}=660 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$other: 4(+2) (1975Na09) 
E$weighted average of 5115 {I9} (1969Mo03), 5116 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.11 (1978Al17) 
$|s{-max}=40 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$also from 1975Na09 
E$weighted average of 5255 {I9} (1969Mo03), 5257 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=1.10 (1975Na09,tentative) 
$|s{-max}=222 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$from 1975Na09. Other: (4) from 1978Al17 
E$weighted average of 5340 {I9} (1969Mo03), 5340 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.48 (1975Na09) 
$|s{-max}=13 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$other: (4) (1975Na09). Perhaps 5530+5560 doublet with L=0+4 
E$weighted average of 5532 {I12} (1969Mo03), 5529 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.03 (1978Al17) 
$|s{-max}=34 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
L$other: (0) (1975Na09) 
E$weighted average of 5560 {I12} (1969Mo03), 5554 {I5} (1978Al17) 
$|s{-max}=97 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5772 {I11} (1969Mo03), 5765 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.09 (1978Al17) 
$|s{-max}=14 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5889 {I9} (1969Mo03), 5890 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.18 (1978Al17) 
$|s{-max}=31 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 6383 {I9} (1969Mo03), 6378 {I5} (1978Al17) 
$|s{-exp}/|s{-DWBA}=0.87 (1978Al17) 
$|s{-max}=196 |mb/sr (1978Al17) 


level_energy_unit: KEV
level_comment:
E$weighted average of 7145 {I9} (1969Mo03), 7135 {I6} (1980Al16) 
$|s{-exp}/|s{-DWBA}=0.64 (1978Al17) 
$|s{-max}=500 |mb/sr (1980Al16) 


level_energy_unit: KEV
level_comment:
E$weighted average of 7847 {I9} (1969Mo03) and 7856 {I6} (1980Al16) 
$|s{-max}=125 |mb/sr (1980Al16) 


level_energy_unit: KEV
level_comment:
E$weighted average of 7900 {I9} (1969Mo03) and 7895 {I6} (1980Al16) 
$|s{-max}=325 |mb/sr (1980Al16) 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$S{-|a|g}[eV]=66 
$E(p)(lab)=5324 {I2} 
$A{-2}=+0.48 {I3}, A{-4}=-0.25 {I4}, A{-6}=+0.67 {I2} 
$|G{-|a0}|>8.3 eV 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-,7/2)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$S{-|a|g}[eV]=61 
$E(p)(lab)=5512 {I2} 
$A{-2}=+0.65 {I2}, A{-4}=+0.01 {I3}, A{-6}=+0.53 {I2} 
$|G{-|a0}|>7.6 eV 


level_energy_unit: KEV
level_spin_parity: (3/2+,7/2-)
level_lifetime_unit: KEV
level_comment:
$S{-|a|g}[eV]=424 
$E(p)(lab)=5695 {I2} 
$A{-2}=+0.69 {I1}, A{-4}=-0.04 {I2}, A{-6}=+0.001 {I1} 
$|G{-|a0}|>53 eV 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$possible doublet indicated in 1965Cu03. Evaluator considers this level as uncertain since there seems no peak in this region in spectral Fig. 1 of 1976Uz01 


level_energy_unit: KEV
level_comment:
E$mixed with a level in {+29}P. 2p{-3/2} orbital (1976Uz01). Probably corresponds to 6460 {I10} in 1965Cu03 with L=1 in 1965Da08 


level_energy_unit: KEV
level_comment:
E$doublet, 6590+6610 in Fig. 1 of 1976Uz01. Other: 6610 {I10} (1965Cu03) with L=1 in 1965Da08 
S$1f{-5/2} orbital for L=3; 2p{-3/2} for L=1 (1976Uz01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
L$0 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1970Me19,1966Be26) 
S$others: 0.34 (1984Mc12), 0.49 (1970Lu07), 0.44 (1970Mo01), 0.47 (1970Wo01), 0.45 {I5} (1966Be26) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$weighted average of 1268 {I4} (1990Ve04), 1270 {I7} (1970Mo01), 1267 {I12} (1969Mo03), and 1270 {I15} (1966Be26) 
L$2 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1970Me19,1966Be26) 
S$others: 0.36 (1984Mc12), 0.65 (1970Lu07), 0.8 (1970Mo01), 0.48 (1970Wo01), 0.45 {I5} (1966Be26) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 2227 {I4} (1990Ve04), 2230 {I7} (1970Mo01), 2234 {I10} (1969Mo03), and 2230 {I15} (1966Be26) 
L$2 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1970Me19,1966Be26) 
S$others: 0.05 (1984Mc12), 0.08 (1970Lu07), 0.08 (1970Mo01), 0.046 (1970Wo01), 0.043 {I4} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3134 {I4} (1990Ve04), 3140 {I7} (1970Mo01), 3135 {I12} (1969Mo03), and 3140 {I15} (1966Be26) 
L$0 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1966Be26) 
S$others: 0.03 (1970Lu07), 0.029 (1970Mo01), 0.022 (1970Wo01), 0.0130 {I13} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3297 {I4} (1990Ve04), 3290 {I7} (1970Mo01), 3301 {I10} (1969Mo03), and 3300 {I15} (1966Be26) 
L$from 1970Lu07. (2) from 1990Ve04 
L$(2) (1990Ve04,1970Mo01,1966Be26), 2 (1970Lu07) 
S$for J=5/2. Others: |?0.0013 (1970Mo01), |?0.0025 (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3501 {I4} (1990Ve04), 3510 {I7} (1970Mo01), 3509 {I13} (1969Mo03), and 3520 {I15} (1966Be26) 
L$(2) (1990Ve04,1970Mo01,1966Be26) 
S$others: |?0.005 (1970Mo01), 0.0025 (1966Be26) 


level_energy_unit: KEV
level_comment:
E$others: 4190 {I7} (1970Mo01), 4191 {I10} (1969Mo03); 4100 {I15} (1966Be26) is discrepant 
L$2 (1990Ve04,1970Wo01,1970Mo01) 
S$for J=5/2. Others: 0.022 (1970Mo01), 0.021 (1970Wo01) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4258 {I4} (1990Ve04), 4265 {I10} (1969Mo03), and 4230 {I15} (1966Be26) 
L$2 (1990Ve04,1970Lu07,1970Wo01,1966Be26) 
S$others: 0.06 (1970Lu07), 0.005 (1970Wo01), 0.025 {I3} (1966Be26) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$weighted average of 4429 {I4} (1990Ve04), 4430 {I7} (1970Mo01), 4432 {I10} (1969Mo03), and 4450 {I15} (1966Be26) 
L$3 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1966Be26) 
S$others: 0.24 (1984Mc12), 0.36 (1970Lu07), 0.29 (1970Mo01), 0.26 (1970Wo01), 0.34 {I4} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4590 {I4} (1990Ve04), 4590 {I7} (1970Mo01), and 4600 {I15} (1966Be26) 
L$2 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1966Be26) 
S$others: 0.06 (1970Lu07), 0.034 (1970Mo01), 0.018 (1970Wo01), 0.007 for J=5/2 (1966Be26) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 5010 {I7} (1970Mo01), 5015 {I10} (1969Mo03), 5030 {I15} (1966Be26) 
L$1 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1966Be26) for unresolved doublet 
S$others: 0.16 (1984Mc12), 0.24 (1970Lu07), 0.21 (1970Mo01), 0.17 (1970Wo01), 0.16 {I2} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5255 {I4} (1990Ve04), 5250 {I7} (1970Mo01), 5257 {I10} (1969Mo03), and 5290 {I15} (1966Be26) 
L$0 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1966Be26) 
S$others: 0.05 (1970Lu07), 0.07 (1970Mo01), 0.03 (1970Wo01), 0.032 {I3} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5560 {I4} (1990Ve04), 5561 {I17} (1969Mo03), and 5590 {I15} (1966Be26) 
L$2 (1990Ve04,1970Wo01,1966Be26) 
S$other: 0.017 (1970Wo01) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5892 {I4} (1990Ve04) and 5907 {I18} (1969Mo03) 
L$from 1970Wo01 
S$from 1970Wo01 for J=7/2; 0.010 for J=9/2 


level_energy_unit: KEV
level_comment:
E$weighted average of 6381 {I4} (1990Ve04), 6400 {I7} (1970Mo01), 6382 {I10} (1969Mo03), and 6410 {I15} (1966Be26) 
L$2 (1990Ve04,1970Lu07,1970Wo01,1970Mo01,1966Be26) 
S$others: 0.25 (1970Lu07), 0.25 (1970Mo01), 0.18 (1970Wo01), 0.079 {I8} (1966Be26) 


level_energy_unit: KEV
level_comment:
L$2 (1990Ve04,1970Wo01) 
S$others: 0.027 (1970Wo01); 0.33 for J=3/2, 0.17 for J=5/2 for a level at 6500 (1984Mc12), which could correspond to the 6381 level 


level_energy_unit: KEV
level_comment:
E$weighted average of 6496 {I4} (1990Ve04), 6494 {I12} (1969Mo03), 6520 {I35} (1970Lu07), 6510 {I7} (1970Mo01), and 6520 {I15} (1966Be26) 
J$the Ay(|q) for the E=6520 {I35} in 1984Mc12 cannot be reproduced with either a 3/2+ or a 5/2+, likely due to many nearby states 
L$1 (1990Ve04,1970Wo01),1966Be26, (1) (1970Lu07), 
S$others: 0.14 (1970Mo01), 0.07 for J=3/2 (1970Lu07), 0.10 (1970Wo01), 0.088 {I9} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$weighted average of 6610 {I4} (1990Ve04), 6630 {I7} (1970Mo01), 6607 {I10} (1969Mo03), and 6640 {I15} (1966Be26) 
L$1 (1990Ve04,1970Lu07,1970Wo01,1966Be26), (1) (1970Mo01) 
S$others: 0.038 for J=3/2 (1970Lu07), 0.013 (1970Mo01), 0.015 for J=3/2 (1970Wo01), 0.037 {I4} (1966Be26) 


level_energy_unit: KEV
level_comment:
E$other: 6843 {I4} (1990Ve04) 
L$3 (1990Ve04,2022Ha03,1970Wo01) 
S$for J=7/2 (1990Ve04). Others: 0.0057 (2022Ha03) and 0.011 (1970Wo01) for J=5/2 


level_energy_unit: KEV
level_comment:
E$others: 6910 {I4} (1990Ve04), 6910 {I20} (1970Mo01) 
L$1 (1990Ve04,2022Ha03,1970Wo01), (1) (1970Mo01) 
S$others: 0.013 (2022Ha03), 0.07 (1970Mo01), 0.022 for J=3/2 (1970Wo01) 


level_energy_unit: KEV
level_comment:
E$other: 6932 {I4} (1990Ve04) 
L$2 (1990Ve04,1970Wo01), 2 or 3 (2022Ha03) 
S$for J=5/2. Other: 0.010 (1970Wo01) and 0.014 (2022Ha03) 


level_energy_unit: KEV
level_comment:
E$others: 7139 {I4} from 1990Ve0, 7150 {I7} (1970Mo01), and 7150 {I15} (1966Be26) 
L$0 (1990Ve04,1970Lu07,1970Wo01),1966Be26, (0) (1970Mo01) 
S$others: 0.34 (1970Lu07), |?0.08 (1970Mo01), 0.08 (1970Wo01), 0.150 {I15} (1966Be26), 0.05 (2022Ha03) 


level_energy_unit: KEV
level_comment:
E$others: 7214 {I4} (1990Ve04), 7206 {I6} (1970Wo01), and 7220 {I15} (1966Be26) 
L$1 (1990Ve04,2022Ha03,1970Wo01,1966Be26) 
S$other: 0.020 (1970Wo01), 0.010 {I1} (1966Be26), 0.005 (2022Ha03) 


level_energy_unit: KEV
level_comment:
$E{-r}=19.6 {I9}, calculated |G{-p}=2.94|*10{+-39} eV and |w|g=1.18|*10{+-38} eV (2022Ha03) 
E$other: 7314 {I4} (1990Ve04) 
L$poor fit with L=3 in 1990Ve04, with C{+2}S=0.002 for J=7/2 


level_energy_unit: KEV
level_comment:
$E{-r}=50.5 {I12}, calculated |G{-p}=5.20|*10{+-21} eV and |w|g=1.04|*10{+-20} eV (2022Ha03) 
$(2J+1)C{+2}S=0.007 for L=1 or 0.0012 for L=2 (2022Ha03) 


level_energy_unit: KEV
level_comment:
$E{-r}=149.2 {I29}, calculated |G{-p}=1.16|*10{+-11} eV and |w|g=2.33|*10{+-11} eV (2022Ha03) 
$(2J+1)C{+2}S=0.0007 for L=2 or 0.0006 for L=3 (2022Ha03) 


level_energy_unit: KEV
level_comment:
$E{-r}=423.0 {I8}, calculated |G{-p}=2.48|*10{+-5} eV and |w|g=7.42|*10{+-5} eV (2022Ha03) 
E$other: 7718 {I4} (1990Ve04) 
L$other: 2 from 1966Be26 for a group at 7720 {I15} is inconsistent 


level_energy_unit: KEV
level_comment:
$E{-r}=440.8 {I7}, calculated |G{-p}=9.79|*10{+-5} eV and |w|g=3.92|*10{+-04} eV (2022Ha03) 
E$other: 7736 {I4} (1990Ve04) 
S$other: 0.014 (2022Ha03) 


level_energy_unit: KEV
level_comment:
$E{-r}=484.6 {I8}, calculated |G{-p}=0.061 eV and |w|g=0.123 eV (2022Ha03) 
E$other: 7780 {I4} (1990Ve04) 
S$other: 0.0038 (2022Ha03) 


level_energy_unit: KEV
level_comment:
$E{-r}=554.9 {I8}, calculated |G{-p}=0.244 eV and |w|g=0.181 eV (2022Ha03) 
E$other: 7855 {I4} (1990Ve04) 
$(2J+1)C{+2}S=0.009 for L=1 or 0.0114 for L=2 (2022Ha03) 


level_energy_unit: KEV
level_comment:
$E{-r}=601.3 {I7}, calculated |G{-p}=6.49 eV (2022Ha03) 
E$others: 7900 {I4} (1990Ve04), 7900 {I15} (1966Be26) 
L$ 1 (1990Ve04,2020Ha03,1966Be26) 
S$for J=1/2. Other: 0.058 (2022Ha03) 


level_energy_unit: KEV
level_comment:
E,L$8190, L=2 in 1970Lu07 probably corresponds to 8209+8227+8242. No L value is adopted here due to the complex nature of this group 


level_energy_unit: KEV
level_comment:
S$Doublet of 8552+8556. 1990Ve04 derives 2 values of C{+2}S=(0.02,0.01) 
L$(0) (1990Ve04) perhaps in error; L=0+1 for the doublet from the best fit to |s(|q) in FIG.3 of 1990Ve04 


level_energy_unit: KEV
level_comment:
J$7/2- from 1984Mc12 is inconsistent with L=1 from 1990Ve04 
S$for J=1/2. Other: 0.2 for J=7/2 (1984Mc12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
T$from 1963Le16. Others: 0.0009 eV {I2} (1966Ho02); mean lifetime |t=0.74 ps {I10} (1966Sk01), 0.96 ps {I+50-21} (1964Bo22), 0.46 ps {I23} (1960Bo23), 0.22 ps {I8} (1962Bo17), from nuclear resonance fluorescence 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
J$|g(|q) in 1963Le16 consistent with 5/2 assignment; 
T$weighted average of 0.00157 eV {I40} (1963Le16) and 0.00145 eV {I15} (1972ArZD). Other: mean lifetime |t=0.45 ps {I16} (1962Bo17) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
$(2J+1)|G{-|g0}[eV]=0.06 {I4} 
T$weighted average of 0.0696 eV {I39} (1972ArZD), 0.061 eV {I4} (1969Ra20), 0.066 eV {I7} (1968Ro14), and 0.049 eV {I10} (1968Cr01). Other: mean lifetime |t=0.020 ps {I7} (1962Bo17) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LE
level_uncertain: ?
level_comment:
E$no evidence of excitation of this T=3/2 level (1970Sh08), only an upper limit of intensity and level width is obtained. 
T$from 1970Sh08 assuming |G{-|g0}/|G=0.18 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$(2J+1)|G{-|g0}[eV]=3.2 {I4} 
S$deduced by 1972Sh07 from their measured branching and |G{-|g0}=1.36 16 from 1965Hi09; used for normalization (1972Sh07) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: EV
level_comment:
$(2J+1)|G{-|g0}[eV]=3.2 {I7} 
S$estimated from resonance strength in (p,|g) (1972Sh07). |G from 1968Ho06 
$resonance strength=1.7 eV {I4} (1968Ho06) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
$(2J+1)|G{-|g0}[eV]=3.7 {I8} 
S$estimated from resonance strength in (p,|g) (1972Sh07). |G from 1968Ho06 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$B(E2)|^: weighted average of 0.0073 {I8} (1965Ko03) and 0.0069 {I11} from B(E2)(W.u.)=6.0 {I9} (1975Kl03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$B(E2)|^: weighted average of 0.0097 {I11} (1965Ko03) and 0.0120 {I5} from B(E2)(W.u.)=6.3 {I3} (1975Kl03) 


level_energy_unit: KEV
level_spin_parity: 3/2+&7/2+
level_comment:
E$doublet of 3415, 7/2+ and 3506, 3/2+ levels in Adopted Levels. Other: 3510 (1975Kl03) 
$B(E2)|^: unweighted average of 0.0047 {I6} (1965Ko03) and 0.0031 {I4} from B(E2)(W.u.)=2.7 {I3} (1975Kl03) 


level_energy_unit: KEV
level_comment:
E$multiplet of three known levels in 5015-5116 region, E4 excitation is only possible if 5342, 9/2+ is also present in this multiplet. Other: 5020 (1975Kl03) 
$ UNITS OF FM**4 IN BE4(UP) SEEMS A MISPRINT, IT SHOULD BE FM**8 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$d|s/d|W(max)=3.4 {I3} 
E$other: 1270 {I30} (1971Ka58) 
$|b{-2}=0.31 (1980Fa07), 0.20 (1968An27 for 1265+2232 group) 
$d|s/d|W{-max}(c.m.)=2.3 {I2} mb/sr (1971Ka58) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$d|s/d|W(max)=5.8 {I6} 
E$other: 2220 {I30} (1971Ka58) 
$d|s/d|W{-max}(c.m.)=4.4 {I2} mb/sr (1971Ka58) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2+)
level_comment:
E$other: 3440 {I40} (1971Ka58) for 3410+3510 
$d|s/d|W{-max}(c.m.)=0.39 {I6} (E4) or 1.20 {I8} (E2) mb/sr (1971Ka58) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$d|s/d|W(max)=3.0 {I3} 
E,J$no 5/2- level between 4500 and 4700 is reported in other studies. This broad group and B(E3) are not included in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$d|s/d|W(max)=3.0 {I3} 
E,J$no 7/2- level between 5500 and 5700 is reported in other studies. This broad group and B(E3) are not included in Adopted Levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
T$0.200 ps {I+36-27} from B(E2) and adopted transition properties 
T$ |t=0.37 ps {I8} from DSAM; 0.30 ps {i5} (1977Sc36) from B(E2) 


level_energy_unit: KEV
level_comment:
E$other: 6010 (1974Ma34) 
S$from 1974Ma34 
L$other: 1 from 1969Ka22 for a level at E=5990 is inconsistent 


level_energy_unit: KEV
level_comment:
L$from 1969Ka22 for a level at E=6410 {I60}, which could correspond to 6397+6460 in 1999Ve09 
S$from 1969Ka22 


level_energy_unit: KEV
level_comment:
L$from 1974Ma34 for a level at E=7980, which could correspond to 7945+8033 in 1999Ve09. L=(1) also from 1969Ka22 for a level at E=8000 {I70} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: D
level_comment:
J,MOMM1$spin and magnetic moment from electron-nuclear double resonance method (1957Fe32); parity from L(pol d,p)=0+2 from 1/2+ target. 
T$average by Normalized Residuals Method (NRM) of 14.263 d {I3} (2002Un02), 14.26 d {I1} (1994Co02), 14.28 d {I4} (1979Pr14), 14.35 d {I5} (1977Mu07), 14.268 d {I42} (1969La34), 14.32 d {I1} (1969Pe04, |DT increased to 0.02 d in NRM), 14.290 d {I14} (1966Go16), 14.282 d {I10} (1961Ma46), 14.2 d {I3} (1958Da10), 14.223 d {I15} (1957An03), 14.30 d {I9} (1950Ba94), 14.35 d {I5} (1948Kl28), 14.07 d {I3} (1940Mu01); |DT increased to 0.072 in NRM, 14.5 d {I3} (1938Ca02), 14.30 d {I3} (1938Ca01), with a reduced |h{+2}=2.6, using the V.AveLib tool. The weighted average gives 14.267 d {I7} with a reduced |h{+2}=6.8 and the unweighted average is 14.284 d {I24}. Others (most are consistently higher than the set of values above): 12 d {I2} (1977Be59), 14.55 d {I6} (1959Ro51), 14.50 d {I4} (1953Lo09), 14.60 d {I5} (1951Si25), 14.5 d {I3} (1937Ne02), 15.0 d {I1} (1936Si01), 15.0 d {I15} (Compt Rend 201, 722 (1935)), 17.5 d {I11} (1934Am01). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 278 ps {I9} from DSAM in (|a,p|g), 253 ps {I25} from |g|g(t) in (n,|g) E=thermal, and 360 ps {I+62-35} from delayed-coincidence in (d,p|g). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$other: 1997Ka15 in {+2}He({+31}P,p|g) and 1990En08 evaluation quote a |t=2.64 ps {I8} from an unpublished work. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$spin=2 from p|g(|q) in (|a,p|g); parity from L(d,p)=2 from 1/2+ 
T$weighted average of 358 fs {I24} from ({+31}P,p|g), 330 fs {I+26-16} from ({+16}O,pn|g), and 267 fs {I49} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
T$weighted average of 426 fs {I28} from ({+31}P,p|g), 427 fs {I+45-32} from ({+16}O,pn|g), and 341 fs {I49} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$spin=3 from p|g(|q) in (|a,p|g); parity from L(d,|a)=4 from 0+ 
T$weighted average of 59 fs {I10} from ({+31}P,p|g) and 41 fs {I9} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$spin=1 from p|g(|q) in (|a,p|g); L(d,p)=2 from 1/2+ 
T$weighted average of 14 fs {I5} from ({+31}P,p|g) and 49 fs {I28} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g) 
J$spin=3 from p|g(|q) in (|a,p|g); L(d,|a)=2 from 0+ 
T$unweighted average of 73 fs {I11} from ({+31}P,p|g), 60 fs {I15} (1973Ca18) and 28 fs {I9} (1973Va14) from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$spin=2 from p|g(|q) in (|a,p|g); L(d,p)=1 from 1/2+ 
T$weighted average of 115 fs {I15} from ({+31}P,p|g), 90 fs {I21} from (|a,p|g), and 146 fs {I+70-42} from (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$L(d,p)=3 from 1/2+ gives 2-,3-,4-; |p=natural from analyzing power in (pol d,|a). Other: (2,4)- from (pol d,p) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
T$weighted average of 264 fs {I31} from ({+31}P,p|g) and 263 fs {I56} from (|a,p|g). Other: <683 fs from ({+16}O,pn|g) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_lifetime_unit: FS
level_comment:
J$L(d,p)=0+2 from 1/2+ for a group at 3795, which is possibly a doublet of 3792+3797, with L=0 component for 3792 and L=2 for 3797 See also comment for 3797 level 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). 
J$spin=3 from p|g(|q) in (|a,p|g); 3719|g M1+E2 to 2+. 3+ also from L(d,|a)=2 from 0+ and analyzing power for a group at 3793, which could be a doublet of 3792+3797 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). 
T$other: <14 fs from DSAM in ({+31}P,p|g) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). 
J$L(d,p)=2(+0) from 1/2+, 1989Ec03 in (d,p) point out 3+ gives a better agreement with theoretical spectroscopic factor 
T$other: <10 fs from DSAM in ({+31}P,p|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$3522.7|g E1 to 0+ 
T$weighted average of 1.5 fs {I6} from ({+31}P,p|g) and 3.5 fs {I21} from (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g) 
J$spin=3 from p|g(|q) in (|a,p|g); L(d,p)=3 from 1/2+. But 4- proposed in (d,p) from analyzing power is inconsistent 
T$weighted average of 19 fs {I7} from ({+31}P,p|g) and 39 fs {I17} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (d,p). Others: 4205.3 {I10} from (n,|g) E=thermal, 4203 {I3} from (|a,p|g) 
T$from DSAM in ({+31}P,p|g) 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g) E=thermal. Other: 4409.8 {I12} from (d,p) 
J$L(d,p)=1 from 1/2+ and analyzing power; |p=unnatural from analyzing power in (pol d,|a); 
T$from DSAM in ({+31}P,p|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). Other: 4554.7 {I6} from (d,p). 4554 from (pol d,|a) is not the same level as the 2+ level here since |p=unnatural is from analyzing power in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$L(d,p)=1 from 1/2+; |p=unnatural from analyzing power in (pol d,|a); 0- is unlikely since it would require Mult(3338|g)=M2 which is ruled out by RUL 
T$from DSAM in ({+31}P,p|g). Other: 0.02 ps {I+17-2} from (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: (5)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=4+(2) from 1/2+ target; 5+ is proposed in in-beam |g-ray data of 2010Gh02, which is possible if L(d,p)=4; 2115.8|g from (6-) favors 5+ over 3+ 
T$from ({+16}O,pn|g) 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). 
J$L(pol d,|a)=4 from 0+ and analyzing power 


level_energy_unit: KEV
level_spin_parity: (3+,4-,5+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). Other: 4847.5 {I11} from (d,p) 
J$|p=unnatural from analyzing power in (pol d,|a); 1701|g to 4+, 2673|g to 3+ 


level_energy_unit: KEV
level_comment:
E$from (d,p). Other: 5010 from (pol d,|a) 
J$|p=unnatural and J not 0 from analyzing power in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$spin=0 from p|g(|q) in ({+3}He,p|g); L({+3}He,p)=0 from 0+. L(|a,d)=(1) from 0+ for a group at 5077 is inconsistent 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,p|g). Other: 5080.5 {I13} from (pol d,p). 
J$L(d,p)=3(+5) from 1/2+ and |p=unnatural from analyzing power (1977Ba68) in (pol d,|a). But (2+) proposed by 1982Ma25 based on analyzing power and L(d,|a)=(2) for a group at 5070 is inconsistent 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$spin=2 from |g|g(|q) in (n,|g) E=thermal; L(d,p)=1 from 1/2+ 
T$from ({+31}P,p|g). Other: 11 fs {I+35-11} from (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: FS
level_comment:
J$(0,1)- from L(d,p)=1 from 1/2+ and analyzing power; possible 5431|g to 2+ 
T$from DSAM in ({+31}P,p|g) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
J$L(d,p)=2 from 1/2+; 1+ from analysis of |s(|q) in (d,{+2}He) for a group at 5670, which could be a doublet of 5663+5674 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$|s(|q) in (d,{+2}He) indicates presence of higher multipoles: (1,2)- and (2,3)+ from neighboring unresolved states, unable to assign a distinct spin. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$spurious level according to calculations in 1997Ka15, as well as experimental (n,|g) data from a priv comm (reference 10 in 1997Ka15) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$spin=2 from |g|g(|q) in 1965Va07 
T$reanalyzed (1997Ka15) from original value of 125 fs {I49} (DSAM,1990Ko43) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$spin=1 from |g|g(|q) in 1965Va07 
T$reanalyzed (1997Ka15) from original value of 2.8 fs {I17} (DSAM,1990Ko43) 


level_energy_unit: KEV
level_spin_parity: 1+
level_uncertain: S
level_comment:
E$7935.65 {I4} from 2021Wa16. Observed deexcitation intensity is 94% of g.s. feeding. 
J$s-wave capture in {+31}P g.s. with J|p=1/2+; |g to 0+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from |t=476 fs {I+38-23} weighted average of 485 fs {I+57-32} for 1323|g and 472 fs {I+38-23} for 1245|g. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
T$see figure 7 in 2014Bh14 where lifetime is measured as a function of the areal density of the target; the mean lifetime (|t) varies from 620 fs for target density of 5.76 mg/cm{+2} to 440 fs for target density of 8.2 mg/cm{+2}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$(0,1,2) from p|g(|q) in 1970Mo09 
T$from 1970Va12. Other: >1.4 fs (1973Va14) 
T$|t>2000 fs (1973Va14), 3.00 ps {I85} (1970Va12) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$other: 1149.8 {I5} (1973Ca18) 
J$(0,1,2,3) from p|g(|q) in 1970Mo09 
T$weighted average from 146 fs {I48} (1973Ca18), 152 fs {I42} (1973Va14), and 187 fs {I45} (1970Va12) 
T$|t=210 fs {I69} (1973Ca18), 220 fs {I60} (1973Va14), 270 fs {I65} (1970Va12) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$other: 1323.1 {I4} (1973Ca18) 
J$spin=1 or 2 from p-1323|g(|q) (1973Va14); spin=2 from p-431|g(|q) from 1754 level (1973Va14); 1323|g M1+E2 to 1+ 
T$weighted average of 243 fs {I49} (1973Va14), 402 fs {I108} (1973Ca18), and 263 fs {I56} 
T$|t=350 fs {I70} (1973Va14), 580 fs {I155} (1973Ca18), 380 fs {I80} (1970Va12) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E$other: 1754.6 {I5} (1973Ca18) 
J$spin=3 from p-1677|g(|q) (1970Mo09,1973Va14); 431|g M1+E2 to 2+ 
T$weighted average of 427 fs {I114} (1973Ca18), 319 fs {I49} (1973Va14), 354 fs {I76} (1970Va12) 
T$|t=616 fs {I164} (1973Ca18), 460 fs {I70} (1973Va14), 510 fs {I110} (1970Va12) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E$others: 2178.2 {I5} (1973Ca18), 2175.3 {I10} (1970Va12) 
J$spin=1,2,3 from p-2100|g(|q) and spin=3 from p-972|g(|q) from 3149 level (1973Va14); 2100|g M1+E2 to 2+ 
T$weighted average of 63 fs {I19} (1973Ca18), 36 fs {I9} (1973Va14), and 42 fs {I18} (1970Va12) 
T$|t=91 fs {I27} (1973Ca18), 52 fs {I12} (1973Va14), 60 fs {I25} (1970Va12) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$others: 2219.0 {I7} (1973Ca18), 2216.5 {I10} (1970Va12) 
J$spin=2,(1) from p-2219|g(|q) (1973Va14); spin=1 excluded by 1931|g from 4149,3- level; 2219|g M1+E2 to 1+ 
T$weighted average of 199 fs {I53} (1973Ca18), 111 fs {I35} (1973Va14), and 146 fs {I35} (1970Va12) 
T$|t=287 fs {I76} (1973Ca18), 160 fs {I50} (1973Va14), 210 fs {I50} (1970Va12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$from 1973Ca18, 1973Va14, 1970Va12 
J$1+ also quoted in 1973Va14, but no p|g(|q) data for this assignment 
T$from 1970Va12. Other: <35 fs (1973Va14) 
T$|t<50 fs (1973Va14), 36 fs {I20} (1970Va12) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$other: 2657 {I2} (1973Va14) 
J$spin=1,2 from p-2658|g(|q) (1973Va14) and spin=1 excluded by 1490|g from 4149,3- level; 
T$from 1973Va14. Other: <28 fs (1973Ca18) 
T$|t<40 fs(1973Ca18), <10 fs(1973Va14) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
E$from 1973Va14. Other: 2746.0 {I7} (1973Ca18) is discrepant, which is probably based on a contaminated 1596|g 
J$from p-2230|g(|q) (1973Va14), but p|g(|q) data not listed by the authors. Other: spin=1,2 from p-2230|g(|q) in 1971St33 
T$from 1973Va14, probably using the strongest 2230|g. Other: 4.9 ps {I+24-18} from 1973Ca18 using a 1596|g is discrepant. This 1596|g in 1973Ca18 could be contaminated by a similar transition in {+29}Si as indicated by authors and this transition is reported as a weak transition in 1973Va14 and is not seen in 1971St33 which report only 2230|g from this level. So the evaluator considers this T{-1/2} from 1973Ca18 questionable. 
T$|t=7.0 ps {I+35-25} (1973Ca18), 70 fs {I40} (1973Va14) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E$weighted average of 3005.4 {I5} (1973Ca18) and 3004.3 {I5} (1973Va14) 
J$spin=3,(2) from p-2927|g(|q) and p-828|g(|q), spin=2 ruled out by p-1682|g(|q) (1973Va14,1976Va09); 1682|g M1+E2 to 2+ 
T$weighted average of 60 fs {I15} (1973Ca18) and 28 fs {I9} (1973Va14) 
T$|t=87 fs {I22} (1973Ca18), 41 fs {I12} (1973Va14) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$others: 3149.7 {I5} (1973Ca18), 3149.0 {I10} (1973Va14) 
J$spin=4 from p-1827|g(|q) (1973Va14); 972|g M1+E2 to 3+ 
T$weighted average of 354 fs {I92} (1973Ca18) and 367 fs {I56} (1973Va14) 
T$|t=510 fs {I133} (1973Ca18), 530 fs {I80} (1973Va14) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$weighted average of 3322.6 {I8} (1973Ca18) and 3321.5 {I9} (1973Va14) 
J$spin=4 ruled out by p-3245|g(|q) (1973Va14) 
T$weighted average of 250 fs {I62} (1973Ca18) and 146 fs {I28} (1973Va14) 
T$|t=360 fs {I91} (1973Ca18), 210 fs {I40} (1973Va14) 


level_energy_unit: KEV
level_spin_parity: (0,1,2)
level_lifetime_unit: FS
level_comment:
E$weighted average of 3445.2 {I4} (1973Ca18) and 3444.0 {I9} (1973Va14) 
J$from p-3444|g(|q) in 1973Va14 
T$from 1973Ca18 
T$|t=35 fs {I17} (1973Ca18) 


level_energy_unit: KEV
level_spin_parity: 3
level_lifetime_unit: FS
level_comment:
E$other: 3795.9 {I6} (1973Ca18) 
J$spin=3 from p-2477|g(|q) (1976Va09) 
T$from 1973Ca18, other: <66 fs (1976Va09) 
T$|t=71 fs {I42} (1973Ca18), <95 fs (1976Va09) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$other: 3992.5 {I10} (1973Ca18) is discrepant 
T$other: <7 fs (1973Ca18) 
T$|t<10 fs (1973Ca18), 18 fs {I8} (1976Va09) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$other: 4150.6 {I6} (1973Ca18) 
J$spin=3 from p-4070|g(|q) (1976Va09); |p=- from Adopted Levels 
T$weighted average of 36 fs {I17} (1973Ca18) and 49 fs {I35} (1976Va09) 
T$|t=52 fs {I24} (1973Ca18), 70 fs {I50} (1976Va09) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
L$also from 1962Ho09 and 1973Va13; (0)+2 from 1978Co21 
$(2J+1)S: <0.07 for s{-1/2} and 3.0 for d{-3/2} (1973Va13); 3.17 and 2.07 for d{-3/2} for 0+78 doublet (1978Co21) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$others: 77 {I3} (1960Pi05), 77 (1962Ho09) 
T$from delayed-coincidence in 1968Me05 
L$also from 1962Ho09 and 1978Co21 
$(2J+1)S: 4.7 for d{-3/2} (1973Va13); 3.17 and 2.07 for 0+78 doublet (1978Co21) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$others: 516 {I3} (1960Pi05), 516 (1962Ho09) 
L$also from 1962Ho09, 1973Va13, 1978Co21 
$(2J+1)S: 0.32 for s{-1/2} (1973Va13); 0.34 and 0.22 (1978Co21) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$others: 1149 {I3} (1960Pi05), 1149 (1962Ho09) 
L$from 1978Co21, 1973Va13, 1962Ho09. Other: 0+2 (1989Ec03) 
$(2J+1)S: 0.53 for s{-1/2} (1973Va13); 1.16 and 0.76 (1978Co21) 


level_energy_unit: KEV
level_comment:
E$others: 1322 {I4} (1960Pi05), 1322 (1962Ho09) 
L$from 1978Co21 
$(2J+1)S: 0.51 and 0.33 for d{-3/2} (1978Co21) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E$others: 1755 {I4} (1960Pi05), 1755 (1962Ho09) 
L$from 1978Co21. Others: 2+4 (1989Ec03), (2) (1973Va13) 
$(2J+1)S: (0.07) for d{-5/2} (1973Va13); 1.21 and 0.79 (1978Co21) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
E$others: 2177 {I4} (1960Pi05), 2177 (1962Ho09) 
$(2J+1)S: 0.45 and 0.30 for s{-1/2}, 0.33 and 0.22 for d{-3/2} for unresolved triplet 2180+2220+2230 in 1978Co21 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$others: 2223 {I4} (1960Pi05), 2223 (1962Ho09) 
L$others: 0+2 (1962Ho09), 2 (1973Va13), 2 (1978Co21) 
$(2J+1)S: 0.13 for s{-1/2} and 0.40 for d{-3/2} (1973Va13); see comments for 2176 level 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$others: 2657 {I5} (1960Pi05), 2657 (1962Ho09) 
L$others: (2,3) (1962Ho09), (1,2,3) (1973Va13), 2 (1978Co21) 
$(2J+1)S: (0.22) for d{-3/2}, (0.01) for p{-1/2}, (0.40) for f{-5/2} (1973Va13); 0.02 and 0.01 for s{-1/2} (1978Co21) 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
E$others: 2743 {I5} (1960Pi05), 2743 (1962Ho09) 
L$others: 2 (1962Ho09), 0+2 (1973Va13 and 1978Co21) 
$(2J+1)S: 0.003 for s{-1/2} and 0.04 for d{-3/2} (1973Va13); 0.15 and 0.10 for d{-3/2} (1978Co21) 


level_energy_unit: KEV
level_spin_parity: (3)+
level_comment:
E$others: 3007 {I5} (1960Pi05), 3007 (1962Ho09) 
L$others: (2,3) (1962Ho09), (2) (1973Va13) 
$(2J+1)S: (0.22) for d{-3/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_comment:
E$others: 3265 {I5} (1960Pi05), 3265 (1962Ho09) 
L$also from 1962Ho09 and 1973Va13 
$(2J+1)S: 1.1 for p{-1/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: (2,4)-
level_comment:
E$others: 3324 {I5} (1960Pi05), 3324 (1962Ho09) 
L$others: 3,(2) (1962Ho09), 3 (1973Va13) 
$(2J+1)S: 3.1 for f{-7/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
E$others: 3447 {I5} (1960Pi05), 3447 (1962Ho09) 
L$from 1973Va13. Others: 3,(2) (1962Ho09), 3(+5) (1989Ec03) 
$(2J+1)S: 7.0 for f{-7/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
E$others: 3798 {I6} (1960Pi05), 3798 (1962Ho09) 
L$other: L=3 from 1973Va13 is in disagreement 
$(2J+1)S: 0.13 for f{-7/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$others: 3879.6 {I6} (1986So01), 3890 {I6} (1960Pi05), 3890 (1962Ho09) 
L$also from 1973Va13 
$(2J+1)S: 0.28 for d{-3/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: (1,3)+
level_comment:
J$1989Ec03 point out that 3+ gives a better agreement with theoretical spectroscopic factors 
E$others: 3994 {I6} (1960Pi05), 3994 (1962Ho09) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
E$others: 4010 {I6} (1960Pi05), 4010 (1962Ho09) 
L$from 1962Ho09. Other: 1+3 (1989Ec03 and 1973Va13) 
$(2J+1)S: 0.33 for p{-1/2} and 0.63 for f{-5/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_comment:
E$others: 4040 {I6} (1960Pi05), 4040 (1962Ho09) 
L$others: 1,(2) (1962Ho09), 1 (1973Va13) 
$(2J+1)S: 1.3 for p{-1/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
E$others: 4158 {I6} (1960Pi05), 4158 (1962Ho09) 
L$from 1973Va13. Other: 3(+5) (1989Ec03) 
$(2J+1)S: 0.18 for f{-7/2} (1973Va13) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$others: 4204.9 {I7} (1986So01), 4209 {I6} (1960Pi05), 4209 (1962Ho09) 
L$from 1962Ho09. Other: 0+2 (1989Ec03) 


level_energy_unit: KEV
level_spin_parity: (0,1)-
level_comment:
E$others: 6195.2 {I14} (1986So01), 6196 {I8} (1960Pi05), 6196 (1962Ho09) 
L$other: 1,(2) (1962Ho09) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$g.s. and 80 are unresolved 
S$from calculations; systematic uncertainty could not be estimated. Transition is L-forbidden 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$This state is weakly excited in the current reaction and is obscured by the peaks at 4200-4550 keV 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_comment:
J$|s(|q) indicated presence of higher multipoles: (1,2)- and (2,3)+ from neighboring unresolved states, unable to assign a distinct spin 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E,J$from 1969Ha19; analog state of 7005 level in {+32}S (1969Ha19) 
$Measured d|s/d|W(p,t)/d|s/d|W(p,{+3}He)=1.20 {I30}, compared to predicted value of 1.8 for T=1 (1969Ha19) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$analog to g.s. of {+32}Si and 12034 {I40} level of {+32}S (1970Ha10) 
J,L$observed |s(|q) consistent with L=0 (1970Ha10) 
$Measured d|s/d|W(p,t)/d|s/d|W(p,{+3}He)=0.66 {I6}, compared to predicted value of 0.60 for T=2 (1970Ha10) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: D
level_comment:
J$L(d,{+3}He)=L(t,p)=0 from 0+. 
T$weighted average of 25.2 d {I5} (1960Fi05), 25.30 d {I5} (1968Re04), 25.56 d {I7} (1972La14), 24.8 d {I5} (1952Je12), 25 d {I2} (1952We29), and 25 d {I2} (1951Sh92), with a reduced |h{+2}=2.1. Other: 24.4 d {I2} (1954Ni06) is discrepant. Weighted average of all is 25.34 d {I10} with a reduced |h{+2}=5.6; unweighted average of all is 25.04 d {I14}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$(pol d,{+3}He)=2 and L-1/2 transfer from analyzing power 
T$weighted average of 0.41 ps {I9} from (|a,p|g) and 0.44 ps {I7} from (t,p|g), both by DSAM. Other: <1.4 ps from RDM in ({+36}S,X|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$L(pol d,{+3}He)=2 and L+1/2 transfer from analyzing power. 
T$from |t=1.12 ps {I15}, 1.20 ps {I30} (1973Ca20), 1.36 ps {I17} (1969Cu01) and 1.20 ps {I20} (1975Ni01) in (|a,p|g), 1.40 ps {I30} (1973Po03) and 0.80 ps {I15} (1973Wa14) in (t,p|g), all by DSAM except RDM in 1975Ni01. Other: <1.4 ps from RDM in ({+36}S,X|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$spin=3/2 from p|g(|q) in (t,p|g); L(d,{+3}He)=2 from 0+ and L(t,p)=2 from 1/2+ 
T$from DSAM in (t,p|g). Other: <7 fs from DSAM in (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,{+3}He)=2 and L+1/2 transfer from analyzing power. 
T$from |t=91 fs {I20}, weighted average of 43 fs {I33} (1973Ca20) from (|a,p|g), 90 fs {I20} (1973Po03) and 110 fs {I20} (1973Wa14) from (t,p|g), all by DSAM. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$spin=7/2 from p|g(|q) in (t,p|g) and (|a,p|g); L(d,{+3}He)=4 from 0+ 
T$|t=218 fs {I40}, weighted average of 160 fs {I56} (1973Ca20) from (|a,p|g), 260 fs {I40} (1973Po03) and 170 fs {I80} (1973Wa14) from (t,p|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$from (pol d,{+3}He). Possible doublet around this energy. See comments at 5053 level 
J$L(pol d,{+3}He)=2 and L+1/2 from analyzing power. See also comments at 5053 level 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$p|g(|q) of 5048|g in (t,p|g) gives J=3/2 with 5/2 clearly excluded, but it contradicts 5/2+ from L(pol d,{+3}He)=2 which well fits measured |s(|q) with L+1/2 from measured analyzing power. This contradiction may imply a doublet around this energy, with 5/2+ and 3/2+ components 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$spin=3/2,5/2 from p|g|g(|q) of 3758|g in (t,p|g); possible 966|g to 7/2- and possible 1563|g to 7/2+; possible 5190|g to 1/2+. Other: (13/2,15/2-) from a very poor DWBA fit in (|a,p) for a group at 5190, which is unlikely to be a different level due to non-observation in other studies. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$from p|g(|q) and |g|g(lin pol) in (|a,p|g), |g|g(|q)(DCO) in ({+18}O,p2n|g). 
T$from RDM in (|a,p|g). Other: >1.3 ps from DSAM in (t,p|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (t,p|g) 
J$from p|g(|q) of 5730|g in (t,p|g) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$1973Po03 in (t,p|g) show two levels near this energy: 5930 and 5990; the first one with a possible transition to the g.s., the second with a transition to 1850 level and a possible transition to g.s. Based on the data from 1973Po02, the evaluators adopt only one level, but it is possible that there are two levels near this energy. 
J$5972|g to 1/2+. 


level_energy_unit: KEV
level_spin_parity: (13/2,15/2-)
level_comment:
J$from 880.3|g to 11/2- and tendency of fusion-evaporation reactions suggesting spin increasing as energy 


level_energy_unit: KEV
level_spin_parity: (9/2)
level_comment:
J$(7/2-,9/2,11/2-) from 1169.2|g to 11/2- and 2582.1|g to 7/2; 9/2 proposed in ({+18}O,p2n|g) based on theoretical predications 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$(9/2,13/2) from |g|g(|q) in ({+13}C,|apn|g) and |g(|q) in ({+18}O,p2n|g); tendency of fusion evaporation reactions to populate higher-lying high-spin states suggests J=13/2; 1484.2|g to 9/2- 


level_energy_unit: KEV
level_comment:
E$from (pol d,{+3}He). Other: 7.62E3 {I15} from (|a,p) 
J$(1/2,3/2+) for a complex group at 7620 {I150} in (|a,p). 


level_energy_unit: KEV
level_spin_parity: (13/2)
level_comment:
J$2448|g to 11/2-, 2632|g to 9/2-; (13/2) proposed by 2018Lu08 in ({+18}O,p2n|g) based on theoretical predictions; (9/2,11/2) from DWBA analysis for a group at 8080 {I150} in (|a,p) 


level_energy_unit: KEV
level_spin_parity: (11/2)
level_comment:
J$(7/2,11/2,15/2) from |g|g(|q) in ({+13}C,|apn|g); 2090.6|g D(+Q) to (7/2-,9/2,11/2-); 3440|g to 11/2-; 2141.6|g to (13/2) 


level_energy_unit: KEV
level_spin_parity: (9/2-,13/2)
level_comment:
J$(5/2,9/2,13/2,17/2) from |g|g(|q) in ({+13}C,|apn|g); 1027.6|g, |DJ=1 to (11/2); 3169.7|g to (13/2-) 


level_energy_unit: KEV
level_spin_parity: (7/2)
level_comment:
J$|g(|q) for 3559 depopulating transition is consistent with |DJ=1 or 0, but not |DJ=2. Tendency of fusion-evaporation reactions to populate higher-lying high-spin states suggests J=7/2 (2018Lu08). 


level_energy_unit: KEV
level_spin_parity: (13/2)
level_comment:
J$1298|g(|q) in 2018Lu08 is consistent with |DJ=1 and excludes |DJ=2. Tendency of fusion-evaporation reactions to populate higher-lying high-spin states suggests J=13/2 (2018Lu08), but DCO ratio of 1298|g-1028|g from 2009Ch43 supports |DJ=2, giving J=15/2. Note that |DJ=1 is also supported by |g|g(|q) in ({+12}C,|apn|g) (2016Fu09). 
T$expected to be in ps region as 1298|g shows a full Doppler shift (2009Ch43). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$from 1969Ha40. Others: 2540 {I5} (1970Be01), 2540 {I8} (1968Be13); 2420 {I30} from 1967Cu01 is discrepant 


level_energy_unit: KEV
level_comment:
E$5443 in Table 1 of 1970Be01 is a typo. It is for peak 16 in between E=5557 for peak 15 and 5731 for peak 17. The position of peak 16 in the proton spectra in Fig. 1 agrees with E=5663 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$3/2 from 1432|g(|q) in 1968Mo16 and 1969Ha40 
T$from |t=596 fs {I133}, weighted average of 525 fs {I133} (1973Ca20) and 790 fs {I220} (1969Cu01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$5/2 from 1850|g(|q) in 1968Mo16 
T$from |t=1278 fs {I170}, weighted average of 1200 fs {I300} (1973Ca20) and 1360 fs {I170} (1969Cu01) by DSAM, and 1200 fs {I200} (1975Ni01) by RDM 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_lifetime_unit: FS
level_comment:
E$other: 3489 {I2} from 1973Ca20 
J$from p-2061|g(|q) in 1969Ha40 
T$from |t=43 fs {I33} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1973Ca20 
J$from p|g(|q) of 1780|g and 2196|g in 1969Ha40; parity from the Adopted Levels 
T$from |t=160 fs {I56} (1973Ca20) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3272 {I15} (1969Da07) and 3280 {I12} (1970Ha48). Other: 3280 (1973Po02,1973Wa14) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3488 {I15} (1969Da07) and 3492 {I10} (1970Ha48). Other: 3490 (1973Po02,1973Wa14) 


level_energy_unit: KEV
level_comment:
E$weighted average of 3623 {I15} (1969Da07) and 3636 {I13} (1970Ha48). Other: 3630 (1973Po02,1973Wa14) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4044 {I15} (1969Da07) and 4050 {I10} (1970Ha48). Other: 4050 (1973Po03,1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$3/2 from p|g(|q) and p|g|g(|q) of 1431|g in 1970Ha48 and 1973Po03; 1431.5|g M1+E2 to 1/2+ 
T$from |t=0.63 ps {I10}, weighted average of 0.70 ps {I15} (1973Po03) and 0.60 ps {I10} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$5/2 from p|g(|q) of 1848|g in 1970Ha48 and 1973Po03; 1847|g E2 to 1/2+ 
T$from |t=0.92 ps {I24}, weighted average of 1.40 ps {I30} (1973Po03) and 0.80 ps {I15} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: FS
level_comment:
J$3/2 from p|g(|q) of 2537|g in 1970Ha48 
T$from |t=50 fs {I20}, unweighted average of 30 fs {I10} (1973Po03) and 70 fs {I12} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_lifetime_unit: PS
level_comment:
J$3/2,5/2 from p|g(|q) of 3275|g in 1970Ha48 
T$from |t=0.20 ps {I4}, weighted average of 0.19 ps {I4} (1973Po03) and 0.21 ps {I4} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$3/2,5/2 from p|g(|q) of 2059|g in 1970Ha48 and 1973Po03; 5/2 from p|g(|q) of 3490|g in 1973Po03; 3490.4|g E2(+M3) to 1/2+ 
$There is a typographic error in the abstract of 1970Ha48 where the J is given as (3/2,1/2). 
T$from |t=0.10 ps {I2}, weighted average of 0.09 ps {I2} (1973Po03) and 0.11 ps {I2} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$7/2 from p|g(|q) of 1779|g and 2196|g in 1970Ha48; 2195.8|g E2(+M3) to 3/2+ 
T$from |t=0.24 ps {I4}, weighted average of 0.26 ps {I4} (1973Po03) and 0.17 ps {I8} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_lifetime_unit: FS
level_comment:
J$3/2,5/2 from p|g(|q) of 2617|g in 1970Ha48 
T$from |t=85 fs {I30}, weighted average of 80 fs {I40} (1973Po03) and 85 fs {I30} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$|<=5/2 in 1973Po02 and 5/2,7/2 in 1970Ha48 from p|g(|q) of 4194|g; 4193.5|g E2(+M3) to 1/2+ 
T$from |t=0.15 ps {I5} in 1973Wa14. Other: <28 fs from |t<0.04 ps in 1973Po02. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$7/2 from p|g(|q) of 2377|g in 1970Ha48; parity from the Adopted Levels. 
T$from |t=0.46 fs {I10}, weighted average of 0.52 ps {I10} (1973Po03) and 0.39 fs {I10} (1973Wa14) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$3/2,5/2 from p|g(|q) of 4855|g and p|g|g(|q) of 3008|g in 1973Po03, with 3/2 favored 
T$from |t<0.11 ps in 1973Po02 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$1973Po03 show two levels near this energy: 5930 and 5990; the first one with a possible transition to the g.s., the second with a transition to 1850 level and a possible transition to g.s. Based on the data from 1973Po02, the evaluators adopt only one level 
T$from |t<0.08 ps in 1973Po02 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$note that this level is reported only in 1973Po02 not in authors' companion paper 1973Po03 
T$from |t=0.08 ps {I6} in 1973Po02 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$from 1973Po02; 6170 level in 1973Po03 is probably the same as 6180 in 1973Po02 
T$from |t<0.09 ps in 1973Po02 


level_energy_unit: KEV
level_comment:
J$5/2+ given by 1988Kh04 as from this work but no angular distribution or analyzing power plot shown by the authors to support this assignment 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: S
level_comment:
$ r{-0}{+2} (strong absorption)=1.14 fm{+2} {I8} (1999Ai02) 
J$ allowed |b transition from 0+ in {+34}Si decay; unnatural parity state in (pol |a,d) 
T$weighted average of 12.40 s {I12} (1946Bl01) and 12.45 s {I10} (1973Go33). Other: 12.5 s (1958Sc31) 


level_energy_unit: KEV
level_spin_parity: 2(-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=1, D(+Q) |g to 1+, 1608; |p=(-) more likely based on qualitative decay-strength arguments in {+18}O({+18}O,pn|g) E=20-44 MeV. Assignment consistent with unnatural parity in {+36}S(pol d,|a|g), but not consistent with the observed population in the Coulomb excitation (hence a different level is not excluded) 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_lifetime_unit: NS
level_comment:
J$|DJ=2, (M2(+E3)) |g to 2+, 429; unnatural parity state from (pol d,|a) 
T$ from 2011MaZP (|g-ray coincidence fast-timing technique) other: 0.3 to 2.5 ns from |g|g(t) (2002AsZY) in {+198}Pt({+37}Cl,x|g) 
$ 2011MaZP: Mason et al., preprint received Sept 2011 


level_energy_unit: KEV
level_spin_parity: (1+,2-,3+)
level_comment:
J$ gammas to 1+ and 2+; unnatural parity state from (pol d,|a). 1+ is less likely if 370|g to 4(-) exists 


level_energy_unit: KEV
level_spin_parity: 5(-)
level_lifetime_unit: PS
level_comment:
J$|DJ=1, D(+Q) |g to 4(-), 2305; |p=(-) more likely in {+18}O({+18}O,pn|g) E=20-44 MeV based on theory 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_lifetime_unit: PS
level_comment:
J$D(+Q) |g to 3(-), 2321 and D,E2 |g to 2(-), 2229; |p=(-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_lifetime_unit: PS
level_comment:
J$D,E2 |g to 3(-), 2321; |p=(-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$D,E2 |g to 3(-), 2321; (4-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$D,E2 |g to 3(-), 2321; (2-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$D,E2 |g to 3(-), 2321; (3-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: PS
level_comment:
J$|DJ=1, D(+Q) |g to 5(-), 3352; |p=(-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$D,E2 |g to 5(-), 3352; (6-) in {+18}O({+18}O,pn|g) E=20-44 MeV based on qualitative decay-strength and theory arguments 


level_energy_unit: KEV
level_comment:
J$(7+) based on shell-model arguments is suggested but not adopted in {+18}O({+18}O,pn|g) E=20-44 MeV (2012Be11); possible 2 particle-hole |pf{-7/2}~#|nf{-7/2} intruder state 


level_energy_unit: KEV
level_spin_parity: 7(+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$|DJ=1, D(+Q) |g to 6(-), 4630; |DJ=2, M2(+E3) |g to 5(-), 3352. |p=(+) is assigned in both {+18}O({+18}O,pn|g) datasets based on level scheme and shell-model arguments; possible 2 particle-hole |pf{-7/2}~#|nf{-7/2} intruder state 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$ B(E2)=0.0020 {I10} if directly excited, but 2000Pr09 propose that this state is being indirectly populated via 2225 state. B(E2) assigned to 2235 will account completely for the population of 429 state 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4-
level_lifetime_unit: NS
level_comment:
J$ 3- or 4- proposed by 1994Fo04 from configuration=|ps{-1/2}|nf{-7/2} 
T$ 0.3 to 2.5 ns from |g|g(t) (2002AsZY) 


level_energy_unit: KEV
level_spin_parity: (6)
level_comment:
J$|g(|q) for 1357 depopulating transition is consistent with |DJ=1 or 0, but not |DJ=2. Tendency of fusion evaporation reactions to populate higher lying high-spin states suggests J=6 (2018Lu08). 


level_energy_unit: KEV
level_spin_parity: (6)
level_comment:
J$|g(|q) for 3571 depopulating transition is consistent with |DJ=1 or 0, but not |DJ=2. Tendency of fusion evaporation reactions to populate higher lying high-spin states suggests J=6 (2018Lu08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=1.5 ps {I5} (2019Gr08), with correction for feeding from higher levels. Authors compared their value with T{-1/2}=1.3 ps {I+6-3} in {+34}P Adopted Levels in the ENSDF database (May 2012 update), where the value was taken from 2012Be11. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J$ L(pol d,{+3}He)=0 
T$weighted average from 45 s {I2} (1971Gr53), 47.4 s {I8} (1972Ap01), and 48.1 s {I14} (1972Go31). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=2783 {I24}. E{-ex}(pp)=-223 keV {I24} in {+35}Si 
$ |G{-p}=4.6 keV {28}, |G{-tot}/|G{-p}=1.0 {I16} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ IAR of g.s., (7/2-) of {+35}Si 
$E(resonance)=3006 {I2}. E{-ex}(pp)=0.0 in {+35}Si 
$ |G{-p}=1.6 keV {I4}, |G{-tot}/|G{-p}=1.0 {I17} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=3151 {I24}. E{-ex}(pp)=145 keV {I24} in {+35}Si 
$ |G{-p}=3.3 keV {I27}, |G{-tot}/|G{-p}=3.2 {I56} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ IAR of 974, (3/2+) of {+35}Si 
$E(resonance)=3809 {I18}. E{-ex}(pp)=803 keV {I18} in {+35}Si 
$ |G{-p}=27 keV {I7}, |G{-tot}/|G{-p}=3.1 {I5} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ IAR of 910, (3/2-) of {+35}Si 
$E(resonance)=3990 {I36}. E{-ex}(pp)=984 keV {I36} in {+35}Si 
$ |G{-p}=185 keV {I43}, |G{-tot}/|G{-p}=1.9 {I1} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ possible IAR of (1/2+) state at |?1440 keV in {+35}Si 
$E(resonance)=4450 {I44}. E{-ex}(pp)=1444 keV {I44} in {+35}Si 
$ |G{-p}=58 keV {I37}, |G{-tot}/|G{-p}=3.7 {I11} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ IAR of 2168, (5/2+) of {+35}Si 
$E(resonance)=5099 {I12}. E{-ex}(pp)=2093 keV {I12} in {+35}Si 
$ |G{-p}=3.8 keV {I9}, |G{-tot}/|G{-p}=1.0 {I20} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ possible IAR of (1/2-,3/2-) state at |?2190 keV in {+35}Si 
$E(resonance)=5200 {I15}. E{-ex}(pp)=2194 keV {I15} in {+35}Si 
$ |G{-p}=21 keV {I12}, |G{-tot}/|G{-p}=1.5 {I6} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s{-f} = 16.0 {I36}. 
L$from the comparison of the experimental parallel momentum distribution with the calculated distribution for {Il}=0 proton removal from the {+36}S ground state which corresponds to J|p=1/2+. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$|s{-f} = 1.5 {I2} 
L$from the experimental parallel momentum distribution with the calculated one computed for {Il}=3 proton removal from the {+36}S ground state. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$|s{-f} = 0.73 {I53} 
J${Il}=1 proton removal from the {+36}S ground state, most likely corresponds to deep-hole configurations involving the 1p{-1/2} orbital. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_comment:
$|s{-f} = 0.63 {I15} 
J${Il}=1 proton removal from the {+36}S ground state, most likely corresponds to deep-hole configurations involving the 1p{-1/2} orbital. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$estimated mean lifetime |t<1 ps. 2019Gr08 stated that lifetime of this level was too short to make a definitive measurement. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$estimated mean lifetime |t>100 ps, from observation of the 4101 gamma line after the degrader, as displayed in Fig. 18 of 2019Gr08. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=3.3 ps {I7} (2019Gr08). Feeding correction seems to have been partially applied. 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: S
level_comment:
J$log| {Ift}=5.72 to 4-, 6.1 to 3-, and 6.39 to 5- 
T$weighted average of 5.9 s {I4} (1982Hi05), 5.2 s {I12} (1986Al11), and 5.3 s {I5} (1986Du07). 
$ Mean-square radius r{-0}{+2}=1.15 fm{+2} {I9} from measured integrated |s{-R}=2.35 b {I18} at 52.60 MeV/nucleon in Si({+36}P,X) reaction (2006Kh08) 
$ Mean radius r{-0}{+2}=1.24 fm{+2} {I7} from measured integrated |s{-R}=2.45 b {I14} at 73.56 MeV/nucleon, and 1.19 fm{+2} {I8} from |s=2.31 b {I15} at 41.89 MeV/nucleon in Si({+36}P,X) reaction (1999Ai02) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$log| {Ift}=5.1 from 0+. (2-) is proposed for a 420 group in charge-exchange reactions (1993Fi03) from comparison of measured |s with calculations. |g to 4- is inconsistent with 1+ 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
$ d|s/d|W=0.26 mb/sr in ({+7}Li,{+7}Be), 0.13 mb/sr in ({+11}B,{+11}C), 0.09 mb/sr in ({+13}C,{+13}N), and 0.50 mb/sr in ({+18}O,{+18}F). 
$ d|s/d|W=0.40 mb/sr in ({+14}C,{+14}N) (1984Ma49) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$ d|s/d|W=0.25 mb/sr in ({+7}Li,{+7}Be), 0.12 mb/sr in ({+11}B,{+11}C), 0.14 mb/sr in ({+13}C,{+13}N), and 0.13 mb/sr in ({+18}O,{+18}F). 
$ d|s/d|W<0.03 mb/sr in ({+14}C,{+14}N) (1984Ma49) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
$ d|s/d|W<0.08 mb/sr in ({+7}Li,{+7}Be), 0.01 mb/sr in ({+11}B,{+11}C), 0.04 mb/sr in ({+13}C,{+13}N), and 0.10 mb/sr in ({+18}O,{+18}F). 
$ d|s/d|W=0.07 mb/sr in ({+14}C,{+14}N) (1984Ma49) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$ In the spectrum figure 2 of 2005Ol04, there is no evidence of a 424.9|g as given in {+36}Si decay dataset 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$(1+) from Adopted Levels of {+36}P in ENSDF database. 2015Ch56 argue that J|p =(1+) would result in E3 and M2 depopulating transitions and a level lifetime long enough that the de-excitation |g-rays would not have been observed at the target position. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$estimated mean lifetime |t<1 ps. Correction due to feeding from (4-) and (7+) levels could not be applied due to poor statistics (2019Gr08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7+)
level_lifetime_unit: PS
level_comment:
T$measured mean lifetime |t=2.7 ps {I6} (2019Gr08). There is no observed feeding from higher levels. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
$Calculated %|b{+-}n=0.02 (1997Mo25) 
T$from 1986Du07 
$ |s{-R}=2.9 b {I10} at 57.02 MeV/nucleon, 2.54 b {I7} at 49.78 MeV/nucleon (2006Kh08); 2.55 b {I20} at 39.71 MeV (1999Ai02) 
$ Average r{-0}{+2}=1.23 fm{+2} {I3} (2006Kh08), 1.31 fm{+2} {I10} (1999Ai02) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
E$assumed that the 0.64 s activity corresponds to the g.s. (1986Du07) 
J$from 2015Ch56 in {+208}Pb({+36}S,X|g) and 2017Tr02 in {+38}Si |b{+-} decay based on shell-model predictions; (0- to 4-) from possible |b feeding of 2+, 1292 state in {+38}S (1986Du07). 
T$from 1986Du07. 
%B-N$other: <10 (1988Mu08) 
$Calculated T{-1/2}: 0.28 s (2003Mo09), 12.6 s (2016Ma12) 
$Calculated %|b{+-}n: 1.6 (2003Mo09), 57.3 (2016Ma12) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: S
level_comment:
J$from shell-model prediction (1997Mo25) and systematics of neighboring nuclei (2017Au03) 
T$weighted average of 0.25 s {I8} (2004Gr20), 0.32 s {I3} (1998WiZV), and 0.19 s {I5} (quoted by 2017Au03 from Reeder et al., P-Arles conference, p587 (1995) and priv. comm. from authors of this conference report ). Other: 0.16 s {I+30-10} (1988Mu08) 
%B-N$from 2015Bi05 evaluation (adopts value from Reeder et al., P-Arles conference, p587 (1995) and priv. comm. from authors of this conference report). Other: 41 {I+32-16} (1988Mu08) 
$Calculated %|b{+-}n=6.4 (2003Mo09) 


level_energy_unit: KEV
level_spin_parity: (2-,3-)
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=210 ms, %|b{+-}n=10.8, %|b{+-}2n=0.26 (2003Mo09) 
J$probable feeding (log| {Ift}=6.1) of 2+ state. Possible coupling of |p1/2[211] and |n5/2[312] (see discussion in 2001Wi21) 
T$weighted average of 153 ms {I8} (2001Wi21) and 125 ms {I25} (2003Gr22). Other: 260 ms {I+100-60} (1989Le16) 
$%|b{+-}n from 2001Wi21. Other: 30 {I10} (1989Le16) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=?
level_comment:
T$the 289|g transition is best fit with a mean lifetime of 15 ps from the Doppler line-shape analysis (2021Hi09) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$weighted average of 100 ms {I5} from implant-|b(t) (2004Gr20) and 120 ms {I20} from |b(t) (1989Le16). Others: 150 ms {I15} (1998WiZV), 1999YoZW. 
%B-N$from 1989Le16. Other: 71 {I21} (1999YoZW, preliminary value) 
J$1/2+ proposed from both systematics (2012Au07) and shell model calculations (2007Ba47), 3/2+ from relativistic mean field model (2014Wa34). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: PS
level_comment:
T$extracted from the best fit of GEANT4 simulated 173|g peak region to the measured spectrum (2019Ri03). 
$|s=6 mb {I2} 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Theoretical T{-1/2}=42.1 ms, %|b{+-}n=36.3, %|b{+-}2n=12.8 (2003Mo09) 
$Theoretical T{-1/2}=219 ms, %|b{+-}n=20.6, %|b{+-}2n=16.3 (2016Ma12) 
T$From 2004Gr20 (|b-decay). Others: 110 ms {I+40-20} (1989Le16, |b-decay) 
$Mean radius r{+2}{-0}=1.25 fm{+2} {I10} (2006Kh08). 
$A new isomeric state was observed in 2008DaZY 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
$Measured mean-square radius (r{+2}{-0})=1.77 fm{+2} {I28} (2006Kh08) 
$|p2s{-1/2} orbital (2006Fr13,2008Ri04) 
T$from |b({+43}P) timing correlations followed up to 400 ms (2004Gr20, measurement at GANIL). Others: 33 ms {I3} (1995So03, earlier measurement at GANIL), 1999YoZW. Weighted average of the two values (from 2004Gr20 and 1995So03) is 35.8 ms {I15} 
%B-N$from 1995So03. Other: 1999YoZW 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$extracted from the best fit of GEANT4 simulated 188|g peak region to the measured spectrum (2019Ri03). 
$|s=4 mb {I2} 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from time correlations between |b rays and fragment implants in all the three studies; the adopted T{-1/2} is weighted average of 18.8 ms {I17} (2022Cr03, statistical uncertainty of 0.8 ms and systematic uncertainty of 1.5 ms added in quadrature); 18 ms {I1} (2022Tr03); 18.5 ms {I25} (2004Gr20,2003Gr22) 
$%|b{+-}n from |b, |g data (2022Tr03), by following the decay chain of {+44}P through |b{+-} and |b{+-}n decay daughters, 
$Theoretical T{-1/2}=14 ms, %|b{+-}n=55, %|b{+-}2n=21, %|b{+-}3n=0 (2019Mo01) 
$Theoretical T{-1/2}=53 ms, %|b{+-}n=17.3, 17.7; %|b{+-}2n=18.6, 23.5; %|b{+-}3n=0.047, 0.11; %|b{+-}4n=0 (2021Mi17); two values for different fission barriers. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_uncertain: ?
level_comment:
J 2003Au02 suggest 1/2+ based on systematics. 
T from time of flight. 2003Au02 suggest 8 ms based on systematics. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from fit to decay curve with function that included decay of parent, exponential growth and decay of daughters (including |bn and |b2n branches) and a constant background (2022Cr03). Reported as 24 ms {I7} (stat) {I9} (syst). 


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. 
$A total of 12 event were assigned to {+47}P, three events each with tuned setting of spectrometer for {+50}S and {+54}Ar, and six events for setting on {+53}Cl, according to data in Table I and text in 2018Ta17 
$Theoretical T{-1/2}(|b)=5.5 ms, %|b{+-}n=45, %|b{+-}2n=35, %|b{+-}3n=19, %|b{+-}4n=0, %|b{+-}5n=0 (2019Mo01) 
$Theoretical T{-1/2}(|b)=11.8 ms, %|b{+-}n=61.9, 60.7; %|b{+-}2n=17.7, 19.5; %|b{+-}3n=7.6, 7.0; %|b{+-}4n=0.11; %|b{+-}5n=0.001 (2021Mi17); two values for a decay mode refer to different fission barriers. 
$The observed events are assumed to correspond to the {+47}P g.s. 
T$half-life of the {+47}P 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 P isotopes, the half-life is expected to be <20 ms from 24 ms for {+45}P, 18.2 ms for {+44}P, 36.5 ms for {+43}P, 48.5 ms for {+42}P and 101 ms for {+41}P, 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$3/2+ (2019Mo01, theory); 1/2+ (syst, 2021Ko07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
T$ Estimated from flight time of 314-322 ns, Poisson statistics of the observed distribution (2011Fo08) of one to four events. At 98% confidence level, T{-1/2}<157 ns. 
$ Based on experimental half-life limit, 2011Fo08 deduce Q(2p)>640 keV in absence of one-proton decay branch, and >230 keV if one-proton decay branch is allowed (2011Fo08). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
T$From 2001Ca60, time vs. particle emission. Other: 21(4) ms (1991Bo32) 
J$from 1991Bo32 
$%|b+2p and %|b{++}p from 2001Ca60. Other: %|b+2p=2.0(10) (1991Bo32) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
$%|e+%|b+=100; %|ep=61 {I3}; %|e2p=3.0 {I6}; %|ep+%|e2p=64 {I3}; %|e3p<0.1 
J$From {+27}S Adopted Levels in the ENSDF database. 
T$Measured by 2017Ja05 from 709 {+27}S implant-p(t) analysis by maximum likelihood method. 
$%|e2p and %|ep+%|e2p values from 2017Ja05. %|ep deduced by compiler subtracting values of %|e2p from %|ep+%|e2p. 2017Ja05 report no observation of |b3p decay of {+27}S, however, taking one event as a limiting value - the upper limit is determined. 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from 6372p(t) (2021Sh23). Other: 17 ms {I4} from p-p(t) events summing between 6200 and 6500 keV. 
$two proton emission from the IAS state of {+27}P to the ground state of {+25}Al was observed at 6372 keV {I15} (2021Sh23). Main mechanism for |b2p decay was found to be sequential in nature (2021Sh23) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T Deduced by the evaluator from B(E2) and Adopted |g-ray properties. 
Integrated (up to 8|') |s=99 mb {i16} (2012To06). 
[M{-n}/M{-p}]/(N/Z)[double ratio]=1.9 {i2} (2012To06) 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$based on S(2p)=3360 keV {I160} (2012Wa38), where x can have values up to |?16 MeV according to figure 2a in 2013Xu13. 2p emission was observed from excited levels of {+28}S from 4 to 20 MeV with an energy resolution of 400 keV. Resonant peaks are visible at |?6.5, 9 and 17 MeV in spectral figure 2 of 2013Xu13. These may originate from several unresolved excited states 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
J$Expected as a mirror of {+29}Al (J|p=5/2+), with 13 odd nucleons (1964Ha45). 
T$weighted av: 195 ms {I8} (1964Ha45), 180 ms {I10} (1967Fi10), and 187 ms {I6} (1979Vi01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
J$L=0 in (p,t) 
T$weighted average of 1.1783 s {I48} (1980Wi13 - method not mentioned), 1.22 s {I3} (1971Mo27 - 678|g(t)), 1.18 s {I4} (1967Ba36 - |b(t)), 1.181 s {I13} (1974ScZL - method not mentioned), 1.1759 s {I17} (2011So11 - |b(t) using a 4|p plastic scintillator), 1.17992 s {I34} (2018Ia01 - |b(t) using a 4|p proportional gas counter), 1.35 s {I10} (1961Ro30 - 511|g(t)), 1.5 s {I1} (1960Jo10), 1.4 s {I1} (1963Fr10 - |b(t)). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L=2 in (p,t) 
T$unweighted average of 70 fs {I35} (1973Ku15), 121 fs {I35} (1970Bi08) 215 fs 52 (1972Ca22) and 176 fs {I15} (1982Al22 - |t=254 fs {I23}), 246 fs {I26} (2017Pe14 - |t=355 fs {I37} - DSAM), all from ({+3}He,n|g) - DSAM, and 153 fs {I13} (Coul. Ex.). Weighted average is 167 fs {I16} |h{+2}=3.4 > |h{+2}{crit}=2.2. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$ from isotropic |g(|q) (2012Lo14 - ({+3}He,n|g)). J|p=(2+),(0+) in 1972Gr39 ({+3}He,n) and proposed configuration: |n(d{-3/2}){++2}. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: FS
level_comment:
J$angular distribution consistent with 1+, does not agree with 0+ in (p,t). 1 from n|g(|q) (1973Ku15 - ({+3}He,n|g)). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$ from triton(|q) measurements and mirror analogue of {+30}Si (2013Se08 - (p,t)). 1 or 3 from |g(|q) and 3+ from mirror analogue of {+30}Si (2012Lo14- ({+3}He,n|g)). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$from triton(|q) and mirror analogue of {+30}Si (2013Se08 - (p,t)) and from comparison of the location of 2{++}{-3} state with the prediction by isobaric multiple mass equation (IMME) (2010Se07 - (p,t)). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: FS
level_comment:
J$from triton(|q) (2013Se08 - (p,t)). Other: 3- based on analogue state to 5487.49 in {+30}Si (1988Kr11). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$weighted average of 5389 {I2} from {+31}Ar |ep decay and 5396 {I4} from (p,t). Other: 5400 {I43} from ({+3}He,n) 
J$from prediction and L=3,(2) in (p,t) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$L=2,3,4 are also possible, J|p=(1,2+,4+) in 2013Se08 ((p,t) and ({+3}He,n|g)) and 4+ in 2012Al23 ((p,t) and ({+3}He,n)). Other: (1-) in 2007Ba69 (p,t) from their L=1 - from measurements of triton(|q) (|?20|' to |'60|'). 


level_energy_unit: KEV
level_spin_parity: 4,5
level_comment:
E$weighted average of 5945 {I3} from {+31}Ar |ep decay, 5950 {I10} from (pol p,|p{+-}), and 5947 {I2} from (p,t) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E$weighted average of 6064 {I3} from {+31}Ar |ep decay and 6071 {I11} from (p,t) 
J L=1 in ({+3}He,n) 


level_energy_unit: KEV
level_comment:
E 6512.1 in (p,t) appears to be a different level. In Table II (2012Al23) (J|p=(1-)), authors list with that of the {+31}Ar |ep decay. Without any details - evaluators list as the same level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from stronger population in ({+12}C,{+10}Be) (1988Kr11). Analogue state of {+30}Si at 7043.17 (J|p=5-). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 6762 {I4} from {+31}Ar |ep decay and 6768 {I3} from (p,t). Other: 6730 {I44} from ({+3}He,n) 
J$L=2 in (p,t) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
E$unweighted average of 7237 {I5} from {+31}Ar |ep decay, 7180 {I41} from ({+3}He,n), and 7194.9 {I18} from (p,t) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from stronger population in ({+12}C,{+10}Be) (1988Kr11). Analogue state of {+30}Si at 8930 (J|p=(6+)). 
$Configuration: |n((f{-7/2}){++2}){-6+} (1988Kr11 - quoted from literature). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_comment:
E,J from ({+12}C,{+10}Be) (1988Kr11). Spin and parity from |s(|q) and DWBA analysis. Analogue state of {+30}Si at 10670 (J|p=6+). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E others: 3681 {I3} (2013Se08), 3707 {I25} (1972Pa02), 3680 {I4} (2010Se07), 3677.3 {I70} (2012Al23). 
J$angular distribution consistent with 1+ and does not agree with 0+. Extremely tentative L=(0) in 1972Pa02, appears to be not acceptable. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E 4682.5 {I57} (2012Al23). 
J$ from triton angular distributions and mirror analogue of {+30}Si (2013Se08) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E,J$energy and angular distribution consistent with 3+ assignment; less likely possibility for 2+. Others: 4693 keV {I5} (2010Se07 - other value 4692.7 {I45} in 2010Se08, 2010Se22). Mirror state of {+30}Si at 4831 (J|p=3+) (2010Se07). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E others: 4812 {I2} (2013Se08), 4813.8 {I34} (2010Se08 - other value in 2010Se07, 2010Se22). 
J$From comparison of the 2{++}{-3} state location with the prediction by isobaric multiple mass equation (IMME) (2010Se07). Mirror to the {+30}Si state at 4810 (J|p=2+) (2010Se07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_comment:
E$used as energy calibration point in 2010Se07, 2013Se08. Other: 5130.0 {I18} (2012Al23). 
J$(4+) in 2013Se08 and 4+ in 2012Al23. Earlier from comparison of the location of the 3{++}{-2} state with the prediction by IMME (2010Se07). 
E$ probable mirror state of 5231, 3+ in {+30}Si 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$probably an unresolved doublet (2007Ba69). 2010Se07 did not observe this peak, in the absence of further experiment, 2010Se07 assumes this is one level and the other one at 5226 keV {I3}. 
$probable mirror state of 5280, 4+ in {+30}Si 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E Others: 5225 {I2} (2013Se08), 5207 {I22} (1972Pa02), 5217.8 {I28} (2012Al23). 
J$assuming this to be a doublet of 5168(6), tentatively assigned by 2010Se07, consistent with mirror pair of 5372 keV level of {+30}Si. Also the same assignment in 2013Se08. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E others: 5315 {I2} (2013Se08), 5306 {I25} (1972Pa02), 5312.1 {I20} (2012Al23). 
J$from prediction of the 3- state location and considering this as the same 5288 keV (J|p=3-) level reported by 1982Yo02 from {+28}Si({+3}He,n){+30}S(p) experiment (2010Se07). Probable mirror state of 5487, 3- in {+30}Si (2010Se07). J|p=(3-,2+) in 2013Se08. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E others: 5393 {I2} (2013Se08), 5426 {I25} (1972Pa02), 5382.0 {I7} (2012Al23). 
E,J$from prediction of the 2+ state location (2010Se07). Other: 5383(8) (2007Ba69), J|p=(3-,2+) (2007Ba69). Probable mirror state of 5614, 2+ in {+30}Si (2010Se07). J|p=3+ in 2013Se08. 


level_energy_unit: KEV
level_comment:
E others: 5849 {I2} (2013Se08), 5835.5 {I13} (2012Al23). 
J$L=2,3,4 are also possible, J|p=(1,2+,4+) in 2013Se08 and 4+ in 2012Al23. (1-) in 2007Ba69 from their L=1 from triton(|q) (|?20|' to 60|'). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E from 2013Se08. Other: 5897 {I27} (1972Pa02) 
J (4+) in 2013Se08 list as adopted - no arguments are available 


level_energy_unit: KEV
level_spin_parity: (2,3)
level_comment:
E others: 6536 {I3} (2013Se08), 6766 {I10} (2007Ba69) 
J (1-) (2012Al23), (2,3) in 2013Se08 from triton angular distributions and mirror analog of {+30}Si 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E other: 5227 {I3} in 2013Ko13. 1814.4 and 3008.5 gammas reported in 2012Lo14 ({+3}He,n|g) from a 5218.8,0+ level were not seen by 2013Ko13. J|p=3+ in 2014Ko17 suggests that 5227 level is different from the 5218.8 level. The assignment of 0+ (2010Se07 - (p,t)) is in disagreement. 
J$from pp(|q) data (2014Ko17); first proton from excited state in {+31}Cl to 5227 level in {+30}S, followed by a second proton to 1/2+ g.s. in {+29}P from the 5227 level in {+30}S. Analysis assumed 0+,1+, 2+,3+,4+ for the 5227 state in {+30}S, and concluded 3+ as the most probable assignment. 
$|G{-|g}/|G{-p}<0.5 at 95% confidence limit (2013Ko13) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E from 2000Fy01. Other: 5847 {I4} (2013Ko13) - No clear evidence of a 3637.7-keV |g reported earlier from this level. 
$|G{-|g}/|G{-p}<9 at 95% confidence limit (2013Ko13); in disagreement with 15.7 (2012Al23) for a 5835.5,4+ level. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T from the Adopted Levels. 
$d|s(n{-0})=2.0 mb/sr {I4} at 5|', for E=5.6 MeV (1967Mc03), d|s(n{-0})=3.7 mb/sr {I11} at 0|' for E=11.60 MeV (1967Mi02). 
$Relative population magnitude, R{-exp}=1.00 (1972Gr39) 
$Configuration: |n(s{-1/2}){++2} (1972Gr39) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 2210 {I30} (1967Mc03 - previous value 2113 {I15} in 1965Mc06), 2190 {I40} (1967Mi02), and 2220 {I25} (1972Gr39). Other: 2200 {I210} (2012Al23). 
$d|s(n{-0})=1.0 mb/sr {I2} at 5|' for E=5.6 MeV (1967Mc03), d|s(n{-0})=0.7 mb/sr {I3} at 0|' for E=11.60 MeV (1967Mi02 from ratio of 0.19 {I5} with g.s. cross section). 
$relative population magnitude, R{-exp}=0.50-0.90 (1972Gr39) 
$Configuration: |n((s{-1/2}){++1} (d{-3/2}){++1}) (1972Gr39); |n(s{-1/2}){++2} (1974Ab03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 3430 {I30} (1967Mc03 - previous value 3291 {I15} 1965Mc06), 3410 {I30} (1972Gr39 - J{+|p}=(0+),(2+)). Other: 3600 {I260} - doublet (2012Al23). 
$Relative population magnitude, R{-exp}=0.15-0.30 (1972Gr39) 
$Configuration: |n(d{-3/2}){++2} (1972Gr39) 
$d|s(n{-0})=0.5 mb/sr {I2} at 5|' (1967Mc03) 


level_energy_unit: KEV
level_comment:
E weighted average of 3690 {I30} (1972Gr39) and 3710 {I30} (1967Mc03). 
$J|p=(2+),(0+) in 1972Gr39. Configuration: |n(d{-3/2}){++2} (1972Gr39) 
$Relative population magnitude, R{-exp}=0.20-0.35 (1972Gr39) 
$d|s(n{-0})=1.00 mb/sr {I+5-3} at 5|' (1967Mc03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
E other: 5210 {I50} (1972Gr39). The level was also populated, not strongly, in ({+12}C,{+10}Be) (1988Kr11) - consistent with a natural parity configuration. 
J J|p=3-, based on analogue state of {+30}Si at 5487 keV (1988Kr11). 
L from 1982Yo02. 
$Relative population magnitude, R{-exp}=1.2-1.9 (1972Gr39) 
$Configuration: |n((f{-7/2}){++1} (s{-1/2}){++1}) (1972Gr39 - J{+|p}=(3-)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E$other: 6110 {I50} with a proposed J|p=(5-) in 1972Gr39 appears to be a different level considering the proposed J|p. Additional experimental support is needed. The evaluators consider it as the same level; 6000 {I41} (2012Al23). 
L From 1982Yo02. 
$ %p(to g.s. of {+29}P)=100 {I2} (2012Al23) 
$Relative population magnitude, R{-exp}=0.30-0.60 (1972Gr39) 
$Proposed configuration: |n((f{-7/2}){++1} (s{-3/2}){++1}) (1972Gr39 - J{+|p}=(5-)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from ({+12}C,{+10}Be) (1988Kr11) strongly populated. Analogue state of {+30}Si at 7043.17 (J|p=5-). 
$Configuration: |n((d{-3/2}){++1} (f{-7/2}){++1}){-5-} (1988Kr11 - quoted from literature). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$ %p(to g.s. of {+29}P)=28 {I5}, %p(to 1383 level in {+29}P)=64 {I7}, %p(to 1954 level in {+29}P)=8 {I2} (2012Al23). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E,J other: 7338 and J=(1,2) in 1982Yo02 
$ %p(to g.s. of {+29}P)=63 {I5}, %p(to 1954 level in {+29}P)=37 {I9} 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E other: 7475 in 1982Yo02 
$ %p(to g.s. of {+29}P)=37 {I8}, %p(to 1383 level in {+29}P)=43 {I6}, %p(to 1954 level in {+29}P)=20 {I4} (2012Al23). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=58 {I10}, %p(to 1954 level in {+29}P)=38 {I25}, %p(to 2423 level in {+29}P)=4 {I2} (2012Al23). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=48 {I5}, %p(to 1383 level in {+29}P)=17 {I7}, %p(to 1954 level in {+29}P)=25 {I10}, %p(to 2423 level in {+29}P)=10 {I8} (2012Al23). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E from ({+12}C,{+10}Be) (1988Kr11) strongly populated. Analogue state of {+30}Si at 8930 (J|p=(6+)) - noted as 8.95 MeV in 1988Kr11. 
$Configuration: |n((f{-7/2}){++2}){-6+} (1988Kr11 - quoted from literature). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=10 {I2}, %p(to 1383 level in {+29}P)=25 {I8}, %p(to 1954 level in {+29}P)=24 {I8}, %p(to 2423 level in {+29}P)=3 {I1}, %p(to 3448 level in {+29}P)=38 {I10} (2012Al23). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=10 {I3}, %p(to 1383 level in {+29}P)=19 {I6}, %p(to 1954 level in {+29}P)=23 {I5}, %p(to 2423 level in {+29}P)=6 {I2}, %p(to 3448 level in {+29}P)=42 {I8} (2012Al23). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=13 {I3}, %p(to 1383 level in {+29}P)=17 {I6}, %p(to 1954 level in {+29}P)=23 {I6}, %p(to 2423 level in {+29}P)=20 {I7}, %p(to 3448 level in {+29}P)=27 {I5} (2012Al23). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (6+)
level_comment:
E,J from ({+12}C,{+10}Be) (1988Kr11) strongly populated, |s(|q) and DWBA analysis. Analogue state of {+30}Si at 10670 (J|p=6+). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=11 {I5}, %p(to 1383 level in {+29}P)=12 {I6}, %p(to 1954 level in {+29}P)=11 {I6}, %p(to 2423 level in {+29}P)=10 {I7}, %p(to 3448 level in {+29}P)=56 {I10} (2012Al23). 


level_energy_unit: KEV
level_comment:
$ %p(to g.s. of {+29}P)=4 {I1}, %p(to 1383 level in {+29}P)=26 {I8}, %p(to 1954 level in {+29}P)=30 {I9}, %p(to 3106 level in {+29}P)=8 {I3}, %p(to 3448 level in {+29}P)=19 {I6}, %p(to 4343 level in {+29}P)= 13 {I4} (2012Al23). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T Weighted average of 1.35 s {I10} (1961Ro30 - 511|g(t)) and 1.5 s {I1} (1960Jo10), 1.4 s {I1} (1963Fr10 - |b(t)). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$unweighted average of 100 fs {I35} (1973Ku15), 121 fs {I35} (1970Bi08), 215 fs 52 (1972Ca22) and 176 fs {I15} (1982Al22 - |t=254 fs {I23}), 246 fs {I26} from mean lifetime |t=355 fs {I37} (2017Pe14). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 80 fs {I28} (1973Ku15), 111 fs {I31} (1972Ca22) and 117 fs 15 (1982Al22 - |t=169 fs {I21}), 166 fs {I24} (2017Pe14 - |t=239 fs {I35}). All by DSAM. 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: FS
level_comment:
J$ 1 or 3 from |g(|q) and DCO; 1+ from mirror analogue of {+30}Si (2012Lo14). 1 from n|g(|q) (1973Ku15). 
T$from 1973Ku15 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J$L(pol p,d)=L(d,t)=L({+3}He,|a)=0 from 0+ 
T$from 2012Ba54, |b detection of a pure source separated using Penning-trap. Others: 2.60 s 3 (1991Mi18), 2.562 s {I7} (1980Wi13), 2.543 s {I8} (1977Az01), 2.605 s {I12} (1974Al03), 2.56 s {I10} (1963Ne05), 2.61 s {I5} (1960Li05), 2.58 s {I6} (1960Wa04), 2.57 s {I1} (1960Ja12), 2.75 s {I25} (1963Va37), 2.72 s {I2} (1958Mi85), 2.40 s {I7} (1954Hu30,conference abstract), 2.66 s {I3} (1952Ha30), 3.2 s {I3} (1951Bo56), 2.6 s {I2} (1949Mc17), 3.18 s {I4} (1941El03), 3.2 s {I2} (1941Wh02). Weighted average (NRM method) of 2012Ba54, 1991Mi18, 1980Wi13, 1977Az01, 1974Al03, 1963Ne05, 1960Li05, 1960Wa04 values is 2.5540 s 23. Evaluators prefer to adopt value from 2012Ba54 due to super-pure source by Penning-trap method 
MOMM1$|b{+-} NMR method (1976Mi16, also 1980HuZX thesis). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$|DJ=1, M1+E2 |g to 1/2+; L(p,t)=0(+2) 
T$DSAM in {+32}S({+3}He,|a|g) (1971En02). Other: 0.8 ps {I5} (stat) {I+9-6} (syst), and 2.2 ps {I33} (stat) {I36} (syst) (2010Do03) from lineshape analysis in ({+37}Ca,X|g); first from cluster HPGe detectors, second from Miniball HPGe detectors, both of RISING |g spectrometer 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$L({+3}He,n)=L({+3}He,|a)=L(d,t)=2; L(p,t)=2+4; |DJ=1 |g to 3/2+; 5/2 also favored by possible mirror state of 4190, 5/2+ in {+31}P 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$L(p,t)=2; |DJ=(0), dipole |g to 3/2+; |g to 1/2+; 3/2 favored by possible mirror state of 4260, 3/2+ in {+31}P 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$existence of this tentative level reported only in ({+3}He,|a) in one study is doubtful as it is not confirmed in any other reaction. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
J$log| {Ift}=5.1 from 3/2+ parent; L({+3}He,|a)=2 from 0+; 5/2 favored by possible mirror state of 4780, 5/2+ in {+31}P. 


level_energy_unit: KEV
level_spin_parity: (1/2)+
level_comment:
J$log| {Ift}=5.0 from 3/2+ parent. L({+3}He,|a)=(1) is in disagreement with positive parity; shell model calculations (2018Be12) support 1/2+ 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_comment:
E$there may be two different levels near this energy, one populated in |e decay and decaying by 4970.2|g, the other in (|a,n|g) and decaying by 3722.5|g 
J$L({+3}He,|a)=1 from 0+; 3/2 favored by possible mirror state of 5015, 3/2- in {+31}P 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$|g to 1/2+; possible |e feeding from 3/2+ parent; shell-model calculations (2018Be12) support 3/2+ 


level_energy_unit: KEV
level_comment:
E$weighted average of 5824 {I3} from ({+3}He,t) E=20 MeV, 5829 {I4} from (p,d), and 5826 {I13} from ({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$see comment for 5891.5 level 
J$L({+3}He,|a)=2 from 0+; shell-model calculations (2018Be12) support 3/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_comment:
E$from energy agreement, this level may be the same as 5890.1, but 4642.6|g is the only |g seen in (|a,n|g) 
J$|DJ=0 |g to 3/2+ 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$possible |e feeding from 3/2+ parent; |g transitions to 7/2+ and 1/2+; shell-model calculations (2018Be12) support 5/2+ 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$|DJ=0 or |DJ=2 |g to 3/2+ from |g(|q) in (|a,n|g) (2014Do04); 9/2 assigned from |s(|q) distribution in ({+3}He,t) (2011Pa14), but 7/2 cannot be ruled out. However, 3/2+ is clearly in disagreement with |s(|q) in ({+3}He,t) 
$Possible mirror state of 6233 level in {+31}P (2014Do04) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_comment:
J$5/2 from |DJ=1 |g to 7/2- from ({+20}Ne,n|g); 7/2 from |DJ=0 |g to 7/2- in (|a,n|g) (2014Do04). But the |s(|q) distribution in ({+3}He,t) (2011Pa14) supports 5/2 
$2014Do04 associated this level with 6399, 7/2+ in {+31}P, but 6399 level is assigned 7/2(-) in {+31}P Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$L(p,d)=L({+3}He,|a)=0 from 0+; |s(|q) in ({+3}He,t) (2011Pa14) 
$Possible mirror state of 6337, 1/2+ in {+31}P (2012Do07) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$L(p,t)=0 from 0+; log| {Ift}=3.4 from 3/2+ parent; IAS of {+31}Cl g.s. 
E$lowest T=3/2 state (1979Na07) 
$Possible mirror state of 6381, 3/2+ in {+31}P (2012Do07) 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$3/2 from |DJ=0 |g to 3/2+ from |g(|q) in (|a,n|g) (2014Do04). 1/2+ from |s(|q) distribution in ({+3}He,t) (2011Pa14) is in disagreement with anisotropic pattern of 5077.7|g in (|a,n|g) data. 3/2+ may not by completely ruled out by |s(|q) data in ({+3}He,t) as well as |g(|q) data in (|a,n|g). Possible mirror state of 6496, 3/2- in {+31}P (2014Do04) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E,J$5/2 from |DJ=1 |g to 3/2+ in (|a,n|g) (2014Do04). The |s(|q) distribution in ({+3}He,t) gives 3/2+ (2011Pa14), which is inconsistent with |g(|q) data for 5108|g in (|a,n|g). Possible mirror state of 6594, 5/2- in {+31}p (2014Do04) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$L(p,d)=5 from 0+; |DJ=1 |g to 7/2+ 
T$effective half-life from DSAM in ({+20}Ne,n|g) (2008Pa27) 
$Possible mirror state of 6501, 9/2- in {+31}P (2014Do04) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E,J$unambiguous J|p assignment made by 2016Be05 from identification of this level as isospin mixed with the IAR at 6279, 3/2+; also log {Ift}=4.1 from 3/2+ parent 
%P$deduced by 2022Bu14 based on measured |b-delayed |g emissions I(|b|g)=0.0338 {I18} from this level by 2018Be12 and |b-delayed proton emission I(|bp)=8.3|*10{+-6} {I+12-9} from this level by 2022Bu14. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$|DJ=1 |g to 3/2+ in (|a,n|g) (2014Do04). An L=2, 6361 {I25} group in ({+3}He,n) may correspond to any of the 6357, 6377 or 6392 levels, but L value is consistent only with that for 6390 and/or 6392 levels 
$Possible mirror state of 6461, 5/2+ in {+31}P (2014Do04) 


level_energy_unit: KEV
level_spin_parity: 11/2(+)
level_comment:
J$|DJ=2 |g to 7/2+; |DJ=1 |g to 9/2+; possible mirror state of 6453, 11/2+ in {+31}P (2014Do04) from (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_comment:
J$|DJ=0 |g to 3/2+ from |g(|q) (2014Do04). (7/2,9/2) from |s(|q) in ({+3}He,t) (2011Pa14) is in disagreement with |g(|q) data in (|a,n|g); possible mirror state of 6610, 3/2- in {+31}P (2014Do04) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
J$assignment in (|a,n|g) by 2014Do04 based on mirror analogy with (5/2,7/2)- level at 6842 in {+31}P, which is now assigned (5/2)- in {+31}P Adopted Levels. 7/2- assigned from |s(|q) in ({+3}He,t) (2011Pa14) 


level_energy_unit: KEV
level_spin_parity: 9/2(-)
level_comment:
J$|DJ=1 |g to 7/2+ in (|a,n|g) (2014Do04); 9/2 from |s(|q) in ({+3}He,t) (2011Pa14); possible mirror state of 6796, 9/2- in {+31}P (2014Do04) 


level_energy_unit: KEV
level_spin_parity: 11/2(-)
level_lifetime_unit: FS
level_comment:
J$|DJ=2 |g to 7/2-; |DJ=1 |g to 9/2+ in ({+20}Ne,n|g); 11/2 from |s(|q) in ({+3}He,t) (2011Pa14); L(p,d)=(5,4), with better fit for L=5 
T$effective half-life from DSAM in ({+20}Ne,n|g) (2008Pa27) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
J$L=0+2 in (p,d) from 0+. 11/2 from |s(|q) distribution in ({+3}He,t) (2011Pa14) is in disagreement. There could be two different levels near this energy 


level_energy_unit: KEV
level_comment:
E$from (p,t) 
J$L({+3}He,n)=0 from 1/2+ gives 1/2+,3/2+ for a group at 7006 {I25} which could be a composite peak of 7010+7037 levels 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
J$log| {Ift}=4.5 from 3/2+ parent 
E$weighted average of 7701 {I3} from {+31}Cl |e decay and 7698 {I3} from ({+3}He,t) E=20 MeV 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
E$weighted average of 7723 {I3} from ({+3}He,t) E=20 MeV and 7728 {I4} from (p,d) 
J$this level is a multiplet in ({+3}He,|a) with L=1+2 favored over L=1+3; also L(p,d)=0+2 from 0+ for the multiplet. Assignments are all possible values from L({+3}He,|a)=1,2 and L(p,d)=0,2. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+,5/2+)
level_comment:
E$from ({+3}He,t) E=20 MeV. Other: 7778 {I17} from {+31}Cl |e decay; 7768 {I25} from ({+3}He,n) 
J$log| {Ift}=5.7 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
E$from (p,d). Others: 7894 {I3} from {+31}Cl |e decay and ({+3}He,t) E=20 MeV, 7888 {I25} from ({+3}He,n) 
J$log| {Ift}=4.9 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$weighted average of 7905 {I3} from ({+3}He,t) E=20 MeV and 7912 {I5} from (p,d) 
J$L(p,d)=0 from 0+ 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
E$weighted average of 8429 {I3} from {+31}Cl |e decay, 8418 {I5} from ({+3}He,t) E=20 MeV, and 8422 {I2} from (p,d) 
J$log| {Ift}=5.0 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
L$from 1968Ko11, 1971Ma58, 1973Go42, 1975Ka10 
S$other: 0.8 (1971Ma58) 
J$from L-transfer and Ay(|q) (1968Ko11,1971Ma58,1973Go42) 
$d|s/d|W(max)=0.62 mb/sr 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$from 1240 {I20} (1968K011), 1240 {I10} (1975Ka10) 
L$from 1968Ko11, 1971Ma58, 1973Go42, 1975Ka10 
S$other: 0.66 (1971Ma58) 
J$from L-transfer and Ay(|q) (1971Ma58,1977Pl03) 
$d|s/d|W(max)=1.20 mb/sr 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$from 2230 {I20} (1968Ko11), 2240 {I10} (1975Ka10) 
E$from 1968Ko11 
L$from 1968Ko11, 1971Ma58, 1973Go42, 1975Ka10 
S$other: 2 (1971Ma58) 
J$from L-transfer and Ay(|q) (1971Ma58,1977Pl03) 
$d|s/d|W(max)=2.30 mb/sr 


level_energy_unit: KEV
level_comment:
E$from 3290 {I20} (1968Ko11) and 3280 {I20} (1975Ka10). Energy of 3284.7 from literature used for calibration in 2020Se16 
E,L$from 1968Ko11; L=2 is favored 
S$from 1975Ka10 
$d|s/d|W(max)=0.78 mb/sr 


level_energy_unit: KEV
level_comment:
E${+31}P mirror state=4190 
E$weighted average of 4083 {I3} (2020Se16) and 4085 {I2} (2007Ma48). Others: 4090 {I20} (1968Ko11), 4080 {I20} (1975Ka10) 
L$from 1968Ko11, 1975Ka10 
S$0.97 (1975Ka10) 
$d|s/d|W(max)=1.00 mb/sr 


level_energy_unit: KEV
level_comment:
${+31}P mirror state=4431 
E$weighted average of 4450 {I3} (2020Se16) and 4446 {I6} (2007Ma48). Others: 4450 {I20} (1968Ko11), 4440 {I40} (1975Ka10) 
L$from 1975Ka10 
S$other: 0.97 (1975Ka10) 
$d|s/d|W(max)=0.34 mb/sr 


level_energy_unit: KEV
level_comment:
${+31}P mirror state=4783 
E$weighted average of 4712 {I2} (2020Se16) and 4707 {I3} (2007Ma48). Others: 4720 {I20} (1968Ko11), 4710 {I30} (1975Ka10) 
L$from 1975Ka10 and 2007Ma48. Other: (0) (1968Ko11) 
S$from 2007Ma48. Other: 0.46 1975Ka10, 0.07 (1968Ko11) if L=0 
$d|s/d|W(max)=0.44 mb/sr 


level_energy_unit: KEV
level_comment:
${+31}P mirror state=5015 
E$weighted average of 4975 {I4} (2020Se16) and 4988 {I8} (2007Ma48). Other: 4990 {I70} (1975Ka10) 
$d|s/d|W(max)=0.1 mb/sr 


level_energy_unit: KEV
level_comment:
${+31}P mirror state=5256 
L$from 2007Ma48. Implied L=0 in 2020Se16 from J|p=1/2+ assignment 
E$energy of 5156.3 keV from literature used for calibration (2020Se16) 
S$other: <0.07 (1975Ka10) 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Other: 5331 {I5} (2007Ma48), 5290 {I70} (1975Ka10) 
$d|s/d|W(max)=0.055 mb/sr 
L$implied from 7/2+,9/2+ assignment in 2020Se16 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Other: 5420 {I20} (1968Ko11) 
J$5/2(-) is assigned in 2020Se16 implying L=(3), but the authors point out that angular distribution in 2020Se16 is featureless 


level_energy_unit: KEV
level_comment:
E$weighted average of 5517 {I2} (2020Se16) and 5497 {I10} (2007Ma48). 
${+31}P mirror state=5559 
L$from 2007Ma48. L=2 also implied from 3/2+,5/2+ assignment in 2020Se16 


level_energy_unit: KEV
level_comment:
E$weighted average of 5775 {I2} (2020Se16) and 5781 {I3} (2007Ma48). 
${+31}P mirror state=5892 
L$from 2007Ma48 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Others: 5959 {I10} (doublet in 2007Ma48), 5880 {I60} (1975Ka10) 
L,S$from 1975Ka10 
$d|s/d|W(max)=0.33 mb/sr 


level_energy_unit: KEV
level_comment:
${+31}P mirror state=6337 
E$from 2022Bu13. Others: 6267 {I5} (2007Ma48), 6320 {I50} (1975Ka10). In 2020Se16, 6255.6 from literature was used for calibration 
L$from 2007Ma48 
S$other: <0.2 (1975Ka10) 
$d|s/d|W(max)=0.21 mb/sr 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Other: 6546 {I15} (2007Ma48) 
${+31}P mirror state=6594 
J$tentative (7/2+,9/2-,11/2+) in 2020S16, implying L=(4,5,6). Authors point out that angular distribution is featureless 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Other: 6848 {I9} (doublet in 2007Ma48) 
J$9/2-,11/2-,7/2+ assigned in 2020Se16, implying L=5,4, with a better fit for L=5 
${+31}P mirror state=7080 or 6825 


level_energy_unit: KEV
level_comment:
E,J$level reported by 2022Bu13, with J|p=(1/2,3/2,5/2)+ from L(d,t) 
L$from 2022Bu13, with estimated mixing ratio of 50% for each L-value. Also 3/2+,5/2+ in 2020Se16, implying L=2 
$Measured |G{-p0}/|G=0.53 {I+5-17} (2022Bu13) 
$E(p)(res)=741 keV {I6} (2022Bu13) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
${+31}P mirror state=7158 
E$weighted average of 7036 {I7} (2022Bu13) and 7044 {I6} (2007Ma48). Others: 7050 {I20} (1968Ko11), 7020 {I40} (1975Ka10). Energy of 7035.4 from literature used for calibration in 2020Se16 
L$from 2022Bu13, 1968Ko11 and 1975Ka10 
S$other: 0.54 (1975Ka10), 1.00 (1968Ko11) 
J$from L-transfer and other arguments, 5/2+ assigned by 2022Bu13. Other: 3/2 (1968Ko11) 
$d|s/d|W(max)=0.85 mb/sr 
$Measured |G{-p0}/|G=0.93 {I+14-10} (2022Bu13) 
$E(p)(res)=905 keV {I7} (2022Bu13) 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Other: 7171 {I8} (2022Bu13) 
L$from 2022Bu13, and implied from 3/2+,5/2+ assignment in 2020Se16 
$Measured |G{-p0}/|G=0.30 {I+9-6} (2022Bu13) 
$E(p)(res)=1040 keV {I8} (2022Bu13) 


level_energy_unit: KEV
level_comment:
E$from 2007Ma48. Others: 7710 {I40} (1975Ka10); energy of 7724 keV from literature used for calibration in 2020Se16 
L$from 2007Ma48. Other: (1) (1975Ka10) 
S$3.0 from 1975Ka10 if L=1 
$d|s/d|W(max)=0.47 mb/sr 


level_energy_unit: KEV
level_comment:
E$from 2020Se16. Other: 7744 {I5} (2022Bu13). 
$Measured |G{-p0}/|G=0.88 {I+8-4} (2022Bu13) 
$E(p)(res)=1613 keV {I5} (2022Bu13) 


level_energy_unit: KEV
level_comment:
E$from 2007Ma48. Others: 7912 {I9} (2022Bu13), 7970 {I70} (1975Ka10); energy of 7907 keV from literature used for calibration in 2020Se16 
$d|s/d|W(max)=0.21 mb/sr 
L$from 2007Ma48 
$Measured |G{-p0}/|G=0.20 {I3} (2022Bu13) 
$E(p)(res)=1781 keV {I9} (2022Bu13) 


level_energy_unit: KEV
level_comment:
E$level from 2022Bu13 
$Measured |G{-p0}/|G=0.42 {I+8-6} (2022Bu13) 
$E(p)(res)=1940 keV {I11} (2022Bu13) 


level_energy_unit: KEV
level_comment:
E,L$from 2007Ma48. Other: 8510 {I80} (1975Ka10); energy of 8498 from literature used for calibration in 2020Se16 
$d|s/d|W(max)=0.14 mb/sr 


level_energy_unit: KEV
level_comment:
E$9432 {I7} (2007Ma48), 9423 {I7} (1975Ka10). Tentative 9415 {I5} level in 2020Se16 
$d|s/d|W(max)=0.60 mb/sr 
L$from 2007Ma48 


level_energy_unit: KEV
level_spin_parity: 7/2(-)
level_comment:
E$ mirror state of 6399, 7/2(-) in {+31}P 
$Evidence for this level at 6403 {I3} deduced also by 2022Ka18 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E,J$new level proposed by 2016Be05, unambiguous J|p assignment made from identification of this level as isospin mixed with the IAR at 6279.0, 3/2+ 
$E(p)(resonance)=260.3 keV {I8}; L=0 resonance in proton capture on {+30}P (g.s. J|p=1+), relevant to {+30}P(p,|g){+31}S reaction rates of astrophysical significance. Other: 273 {I10} (2022Bu14). 
%P$deduced by 2022Bu14 based on measured |b-delayed |g emissions I(|b|g)=0.0338 {I18} from this level by 2018Be12 and |b-delayed proton emission I(|bp)=8.3|*10{+-6} {I+12-9} from this level by 2022Bu14. 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=780 {I2} (2011SaZM), 762 {I14} (2006Ka11) 
$Relative I(p)=20.4 {I2} (2011SaZM), 9.1 {I22} (2006Ka11) 
$I(p)/I|g(2234|g)=0.43 {I1} (2011SaZM), 0.10 {I3} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E$E(p)=877 {I2} (2011SaZM), 853 {I18} (2006Ka11) 
$Relative I(p)=12.4 {I2} (2011SaZM), 1.2 {I12} (2006Ka11) 
$I(p)/I|g(2234|g)=0.26 {I1} (2011SaZM), 0.013 {I13} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
$E(p)=993 {I2} (2011SaZM), 978 {I15} (2006Ka11), also seen in 1996Og01 
$Relative I(p)=100 {I4} (2011SaZM), 100 {I4} (2006Ka11) 
$I(p)/I|g(2234|g)=2.12 {I3} (2011SaZM), 1.08 {I14} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=1185 {I3} (2011SaZM), 1175 {I19} (2006Ka11) 
$Relative I(p)=2.7 {I1} (2011SaZM), 1.7 {I6} (2006Ka11) 
$I(p)/I|g(2234|g)=0.057 {I3} (2011SaZM), 0.018 {I7} (2006Ka11) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$E(p)=1345 {I17} (2011SaZM) 
$Relative I(p)=1.3 {I12} (2011SaZM) 
$I(p)/I|g(2234|g)=0.028 {I26} (2011SaZM) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=1520 {I3} (2011SaZM), 1521 {I20} (2006Ka11), also seen in 1996Og01. 
$Relative I(p)=21.0 {I4} (2011SaZM), 13.6 {I14} (2006Ka11) 
$I(p)/I|g(2234|g)=0.44 {I1} (2011SaZM), 0.15 {I3} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+,5/2+)
level_comment:
$E(p)=1594 {I17} (2011SaZM) 
$Relative I(p)=1.4 {I2} (2011SaZM) 
$I(p)/I|g(2234|g)=0.030 {I4} (2011SaZM) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=1706 {I3} (2011SaZM), 1688 {I22} (2006Ka11). 
$Relative I(p)=6.4 {I2} (2011SaZM), 3.9 {I7} (2006Ka11) 
$I(p)/I|g(2234|g)=0.136 {I5} (2011SaZM), 0.043 {I9} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=1830 {I3} (2011SaZM), 1825 {I23} (2006Ka11) 
$Relative I(p)=10.9 {I2} (2011SaZM), 8.8 {I11} (2006Ka11) 
$I(p)/I|g(2234|g)=0.231 {I5} (2011SaZM), 0.096 {I16} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=1927 {I17} (2011SaZM) 
$Relative I(p)=1.4 {I1} (2011SaZM) 
$I(p)/I|g(2234|g)=0.031 {I2} (2011SaZM) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=2070 {I17} (2011SaZM), 2075 {I30} (2006Ka11) 
$Relative I(p)=1.3 {I1} (2011SaZM), 1.3 {I5} (2006Ka11) 
$I(p)/I|g(2234|g)=0.028 {I2} (2011SaZM), 0.014 {I5} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=2224 {I3} (2011SaZM), 2217 {I30} (2006Ka11) 
$Relative I(p)=2.3 {I1} (2011SaZM), 4.1 {I8} (2006Ka11) 
$I(p)/I|g(2234|g)=0.048 {I2} (2011SaZM), 0.044 {I10} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$ assuming this level corresponds to L=0, 8517 {I13} level in (p,d) 
$E(p)=2286 {I17} (2011SaZM), 2299 {I30} (2006Ka11) 
$Relative I(p)=0.9 {I7} (2011SaZM), 1.5 {I5} (2006Ka11) 
$I(p)/I|g(2234|g)=0.018 {I2} (2011SaZM), 0.016 {I6} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=2489 {I17} (2011SaZM), 2454 {I40} (2006Ka11) 
$Relative I(p)=0.91 {I6} (2011SaZM), 1.0 {I4} (2006Ka11) 
$I(p)/I|g(2234|g)=0.019 {I2} (2011SaZM), 0.010 {I4} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+,5/2+)
level_comment:
$E(p)=2641 {I17} (2011SaZM), 2601 {I40} (2006Ka11) 
$Relative I(p)=0.19 {I4} (2011SaZM), 0.4 {I3} (2006Ka11) 
$I(p)/I|g(2234|g)=0.004 {I1} (2011SaZM), 0.004 {I3} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
$E(p)=2807 {I17} (2011SaZM), 2751 {I40} (2006Ka11) 
$Relative I(p)=0.3 {I1} (2011SaZM), 0.6 {I3} (2006Ka11) 
$I(p)/I|g(2234|g)=0.006 {I2} (2011SaZM), 0.007 {I4} (2006Ka11) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$C{+2}S=0.85 {I21} 
$|s |<12 mb {I3}, 11 mb {I3} from momentum distribution 
$Inclusive |s=36 mb {I4} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
T$ from 2010Do03, deduced from the lineshape analysis using cluster HPGe detectors. The uncertainty is statistical; systematic uncertainty=+0.9-0.6 ps. Other: 2.2 ps {I33} (stat) {I36} (syst) using the lineshape analysis and MINIBALL HPGe detectors (2010Do03). In both cases reaction was {+9}Be({+37}Ca,X|g) at 195.7 MeV/nucleon 


level_energy_unit: KEV
level_comment:
$|e=0.79 
E,J$ 3300 in 1982Al28 corresponds to 3286 and/or 3351 levels. Angular distribution pattern in 1982Al28 is consistent with L=2, 5/2+ 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$d|s/d|W=1434 |mb/sr 
L$from 1999Ve09, 1970Mo08, 1966Gr26, 1966Fo10, 1975In03 
S$others: 0.9 (1966Fo10), 0.96 (1975In03). C{+2}S=0.63-0.78 (1981Ba27) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$d|s/d|W=1687 |mb/sr 
E$weighted average of 1246 {I10} (1970Mo08), 1250 {I10} (1999Ve09), 1245 {I8} (1972Bh01), 1243 {I10} (1966Gr26), 1242 {I20} (1966Aj01) 
L$from 1999Ve09, 1966Gr26, 1966Fo10, 1975In03 
S$others: 1 (1966Gr26), 1.1 (1966Fo10), 0.7 (1975In03). C{+2}S=0.5-0.8 (1981Ba27) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$d|s/d|W=6184 |mb/sr 
E$weighted average of 2234 {I10} (1970Mo08), 2235 {I10} (1999Ve09), 2230 {I11} (1972Bh01), 2221 {I10} (1966Gr26), 2232 {I15} (1966Aj01) 
L$from 1999Ve09, 1966Gr26, 1966Fo10, 1975In03 
S$others: 1.6 (1966Gr26), 2.9 (1966Fo10), 2.12 (1975In03) C{+2}S=1.3-2.2 (1981Ba27) 


level_energy_unit: KEV
level_comment:
$d|s/d|W<120 |mb/sr 
E$weighted average of 3075 {I10} (1970Mo08), 3081 {I10} (1999Ve09), 3075 {I13} (1972Bh01) 
L$from 1970Mo08 and 1999Ve09 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
$d|s/d|W=1170 |mb/sr 
E$weighted average of 3286 {I10} (1970Mo08), 3286 {I10} (1999Ve09), 3281 {I14} (1972Bh01), 3274 {I10} (1966Gr26), 3287 {I15} (1966Aj01) 
L$from 1970Mo08, 1999Ve09, 1966Gr26, 1966Fo10 
S$others: 0.7 (1966Gr26), 0.8 (1966Fo10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=54 |mb/sr 
E$weighted average of 3347 {I10} (1970Mo08), 3352 {I10} (1999Ve09) 3341 {I14} (1972Bh01), 3359 {I15} (1966Aj01), 


level_energy_unit: KEV
level_comment:
$d|s/d|W=180 |mb/sr 
S$for d{-3/2} orbital 
E$weighted average of 3437 {I10} (1970Mo08), 3440 {I10} (1999Ve09), 3434 {I14} (1972Bh01), 3435 {I15} (1966Aj01), 
L$(2) (1970Mo08) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4083 {I12} (1970Mo08), 4087 {I10} (1999Ve09), 4076 {I16} (1972Bh01), 4085 {I20} (1966Aj01), 
L$from 1999Ve09, 1970Mo08, 1966Fo10 
S$other: 1.1 (1966Fo10) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=500 |mb/sr 
L$L=2 (1966Fo10) disagrees with L=3 from 1970Mo08 and L=(3) 1999Ve09 
E$weighted average of 4452 {I9} (1970Mo08), 4451 {I10} (1999Ve09), 4449 {I17} (1972Bh01), 4451 {I15} (1966Aj01), 


level_energy_unit: KEV
level_comment:
E$not observed by 1999Ve09, from 1970Mo08 
E$weighted average of 4522 {I12} (1970Mo08), 4526 {I15} (1966Aj01) 
L$from 1970Mo08 
S$for g{-7/2} orbital 


level_energy_unit: KEV
level_comment:
$d|s/d|W=80 |mb/sr 
E$weighted average of 4581 {I9} (1970Mo08), 4579 {I10} (1999Ve09), 4572 {I18} (1972Bh01), 4582 {I15} (1966Aj01) 
S$0.19 (1999Ve09) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from 1972Bh01 only, not resolved from 4572 level. This level is shown as tentative in authors' Table I 
$d|s/d|W=35 |mb/sr 


level_energy_unit: KEV
level_comment:
$d|s/d|W=780 |mb/sr 
E$weighted average of 4717 {I9} (1970Mo08), 4720 {I10} (1999Ve09), 4722 {I18} (1972Bh01), 4718 {I15} (1966Aj01), 
L$2,(3) (1970Mo08), 2 (1999Ve09,1972Bh01) 
S$0.75 (1999Ve09), 0.45 (1972Bh01) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$not observed in 1999Ve09 
$d|s/d|W=60 |mb/sr 
E$weighted average of 4870 {I19} (1972Bh01), 4866 {I9} (1970Mo08), 4850 {I30} (1966Aj01) 
L$from 1970Mo08. Poor DWBA fit to |s(|q) for s{-1/2} or d{-5/2} orbitals (1999Ve09) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=175 |mb/sr 
E$weighted average of 4968 {I10} (1970Mo08), 4975 {I10} (1999Ve09), 4965 {I19} (1972Bh01), 4976 {I15} (1966Aj01), 
L$from 1999Ve09, 1972Bh01, 1970Mo08 
S$0.077 (1999Ve09), 0.06 


level_energy_unit: KEV
level_comment:
$d|s/d|W=142 |mb/sr 
E$weighted average of 5026 {I16} (1970Mo08), 5028 {I10} (1999Ve09), 5017 {I19} (1972Bh01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$d|s/d|W=443 |mb/sr 
E$weighted average of 5154 {I12} (1970Mo08), 5161 {I10} (1999Ve09), 5154 {I19} (1972Bh01), 5170 {I30} (1966Aj01) 
L$from 1999Ve09, 1972Bh01, 1970Mo08 
S$0.19 (1999Ve09), 0.32 (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=80 |mb/sr 
E$weighted average of 5517 {I15} (1970Mo08), 5519 {I10} (1999Ve09), 5509 {I21} (1972Bh01), 5520 {I30} (1966Aj01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=394 |mb/sr 
E$weighted average of 5777 {I11} (1970Mo08), 5777 {I10} (1999Ve09), 5774 {I21} (1972Bh01), 5792 {I15} (1966Aj01) 
S$0.33 (1999Ve09), 0.27 (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=50 |mb/sr 
E$weighted average of 5824 {I13} (1970Mo08), 5840 {I30} (1966Aj01) 5823 {I21} (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=378 |mb/sr 
E$weighted average of 5893 {I10} (1970Mo08), 5889 {I10} (1999Ve09), 5889 {I22} (1972Bh01), 5910 {I30} (1966Aj01), 
S$ 1.67 (1999Ve09), 0.20 (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=100 |mb/sr 
E$weighted average of 5983 {I13} (1970Mo08), 5975 {I10} (1999Ve09), 5978 {I22} (1972Bh01), 5994 {I20} (1966Aj01) 
S$1.67 (1999Ve09) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=105 {I50} |mb/sr, partially obscured by |a from {+12}C({+3}He,|a){+11}C in 1972Bh01 
E$weighted average of 6154 {I12} (1970Mo08), 6165 {I25} (1966Aj01), 6150 {I22} (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=700 |mb/sr 
E$weighted average of 6268 {I13} (1970Mo08), 6257 {I10} (1999Ve09), 6258 {I23} (1972Bh01), 6273 {I20} (1966Aj01) 
S$0.33 (1999Ve09), 0.22 {I6} (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=60 |mb/sr 
E$weighted average of 6743 {I13} (1970Mo08), 6763 {I20} (1966Aj01), 6746 {I24} (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=1000 |mb/sr 
E$weighted average of 6966 {I20} (1999Ve09), 6990 {I30} (1966Aj01), 6990 {I25} (1972Bh01) 
S$from 1972Bh01. Other: 0.03 (1999Ve09) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=2784 |mb/sr 
E$weighted average of 7036 {I11} (1970Mo08), 7033 {I10} (1999Ve09), 7039 {I25} (1972Bh01), 7048 {I20} (1966Aj01) 
S$other: 1.85 (1972Bh01) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=255 |mb/sr 
E$weighted average of 7161 {I11} (1970Mo08), 7156 {I10} (1999Ve09), 7163 {I25} (1972Bh01), 7181 {I20} (1966Aj01) 
S$other: 0.21 (1972Bh01) 


level_energy_unit: KEV
level_comment:
E$L value implies a multiplet 
E$weighted average of 7726 {I15} (1970Mo08), 7725 {I10} (1999Ve09), 7738 {I20} (1966Aj01) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$C{+2}S=0.02 {ICA} 
$E{-p}(cm)=27.2 keV {I17} 
$|G{-p}=5.19|*10{+-34} keV, 4|*10{+-34} keV {I+53-4}. |G{-|g}=1.5|*10{+-5} keV {i5} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$C{+2}S=0.003 {ICA} 
S$ for L=0. C{+2}S=0.015 if L=2 
$E{-p}(cm)=126.9 keV {I23} 
$|G{-p}=9.47|*10{+-14} keV, 7.1|*10{+-14} keV {I+89-66} for L=0, 3.79|*10{+-15} keV, 2.5|*10{+-15} keV {I+31-15} for L=2. |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$C{+2}S=0.00025 {ICA} 
$E{-p}(cm)=148.2 {I21} 
$|G{-p}=2.08|*10{+-13} keV; |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$C{+2}S=0.044 {ICA} 
$E{-p}(cm)=223.8 {I25} 
$|G{-p}=3.79|*10{+-10} keV, 1.9|*10{+-10} keV {I+22-11}. |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$C{+2}S=0.02 {ICA} 
$E{-p}(cm)=243.9 {I16} 
$|G{-p}=1.34|*10{+-11} keV, 7.2|*10{+-12} keV {I+8-7}. |G{-|g}=1.2|*10{+-4} keV {i4} 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_comment:
$C{+2}S=0.10 {ICA} 
$E{-p}(cm)=260.3 {I16} 
$|G{-p}=5.62|*10{+-12} keV, 1.24|*10{+-13} keV {I+13-12}. |G{-|g}=2.0|*10{+-5} keV {i8} 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_comment:
$C{+2}S=0.02 {ICA} 
$E{-p}(cm)=410.1 {I25} 
$|G{-p}=1.66|*10{+-5} keV, 1.02|*10{+-5} keV {I+36-26}. |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)-
level_comment:
$C{+2}S=0.02 {ICA} 
$E{-p}(cm)=452.1 {I25} 
$|G{-p}=4.78|*10{+-5} keV, 3.6|*10{+-5} keV {I+15-11}. |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$C{+2}S=0.02 {ICA} 
$E{-p}(cm)=503.8 {I20} 
$|G{-p}=1.70|*10{+-7} keV, 8.92|*10{+-8} keV {I44}. |G{-|g}=3.3|*10{+-6} keV {i7} 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$E{-p}(cm)=586.8 {I25} 
$|G{-p}/|G=0.25 {I+7-20}. |G{-p}=3.76|*10{+-4} keV {I64}. |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$E{-p}(cm)=616.0 {I25} 
$|G{-p}/|G=0.57 {I+7-32}. |G{-p}=6.62|*10{+-4} keV {I10}. |G{-|g}=1.5|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$C{+2}S=0.10 {ICA} 
$E{-p}(cm)=663 {I25} 
$|G{-p}=4.38|*10{+-4} keV, 1.31|*10{+-3} keV {I+50-38}. |G{-|g}=2.0|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_comment:
$C{+2}S=0.02 {ICA} 
$E{-p}(cm)=700.4 {I15} 
$|G{-p}=2.88|*10{+-9} keV, |?10|*10{+-11} keV. |G{-|g}=5.4|*10{+-6} keV {i22} 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
$E{-p}(cm)=739.0 {I25} 
$|G{-p}/|G=0.37 {I+9-13}. |G{-p}=3.20|*10{+-4} keV {I46}. |G{-|g}=3.0|*10{+-4} keV 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$I{-|bp}=8.3|*10{+-6} {I+12-9} (2022Bu14). Combined with a previous measurement of I{-|b|g}=0.0338 {I18} gives |G{-p}/|G= 2.5|*10{+-4} {I+4-3} 
$E(p)(resonance)=273 keV {I10} (2022Bu14); uncertainty is 8.5 keV from extrapolating a linear calibration function added in quadrature with a 5-keV systematic error from pulse height defect. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$measurements by optical spectroscopy (1936Ol01,1931Na01). 
$The rms charge radius <r{+2}>{+1/2}=3.2611 fm {I18} (2013An02 evaluation) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$2230.47|g E2 to 0+. 
T$weighted average of 0.205 ps {I16} from (|a,n|g), 0.142 ps {I21} from (p,|g) E=res, 0.163 ps {I24} from measured width in (|g,|g'), 0.24 ps {I4} from (p,p'|g), 0.164 ps {I11} from (|a,|a'|g), and 0.166 ps {I19} from Coulomb excitation, all by DSAM except noted. Other: 0.21 ps {I6} from (|a,|g) E=res; 0.173 ps {I8} from adopted B(E2)|^=0.0297 {I13}. 
MOMM1$average of +0.94 {I18} measured using IMPAC method (1979Za01) and +0.88 {I20} measured using transient-field method (2006Sp01). See also 2020StZV compilation. 
MOME2$from reorientation in Coulomb excitation in 1982Ve09. See also 2021StZZ evaluation. Others: -0.18 {I4} or -0.15 {I4} (1981Da08), -0.12 {I5} (1980Ba40), -0.175 {I5} (1971Ha47), -0.20 {I6} (1970Na05), in Coulomb excitation. 
BE2$from Coulomb excitation. Other: 0.0200 {I22} from (e,e') is discrepant 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$from L(p,t)=0 from 0+; 1548.8|g(|q) is isotropic in (p,|g) E=res. 
T$weighted average of 0.89 ps {I9} from ({+6}Li,pn|g), 0.88 ps {I7} from (|a,n|g), 0.59 ps {I+14-12} from (p,|g) E=res, 0.69 ps {I+21-14} from (p,p'|g), and 0.73 ps {I21} from (|a,|a'|g), all by DSAM 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$4281.6|g E2 to 0+ 
T$weighted average of 41 fs {I6} from ({+31}P,n|g), 40 fs {I5} from ({+6}Li,pn|g), 29.8 fs {I35} from (p,|g) E=res, 32 fs {I5} from width in (|g,|g'), 28 fs {I10} from (n,n'|g), 52 fs {I4} from (p,p'|g), and 33 fs {I9} from (|a,|a'|g), all by DSAM except noted. Other: 71 fs {I27} from (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$spin=4 from |g|g(|q) in (p,p'|g); L(p,t)=4 from 0+ 
T$weighted average of 140 fs {I60} from (p,|g) E=res, 88 fs {I21} from (n,n'|g), 150 fs {I40} from (p,p'|g), and 137 fs {I20} from (|a,|a'|g) 
MOMM1$measured using transient-field (1988Si14). See also 2020StZV compilation. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$spin=1 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=2 from 1/2+ 
T$unweighted average of 286 fs {I74} from (|a,n|g), 367 fs {I35} (1969Pi10), 119 fs {I70} (1969Th03), 277 fs {I28} (1998Ka31), 170 fs {I35} (1974Ch09), and 159 fs {I38} (1972Co13) from (p,|g), 280 fs {I70} (1971In02) and 340 fs {I60} (1970Ol01) from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in (p,|g) E=res 
T$from (p,p'|g) by DSAM. Others: 0.55 ps {I14} from (|a,n|g), 0.56 ps {I14} from (p,|g) E=res, and 0.49 ps {I11} from (n,n'|g) 
BE3$from Coulomb excitation. Other: 0.0050 {I5} from (e,e') 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; L(d,n)=2 from 1/2+ 
T$weighted average of 132 fs {I14} from (p,p'|g), 167 fs {I24} from ({+6}Li,pn|g), 139 fs {I39} from (|a,n|g), and 102 fs {I23} from (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2 from 0+ 
T$weighted average of 58 fs {I10} from ({+31}P,n|g), 45 fs {I6} from (|a,n|g), 56 fs {I8} from (p,|g) E=res, and 83 fs {I21} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$spin=1 from n|g(|q) in (|a,n|g); L(d,n)=L({+3}He,d)=1 from 1/2+ 
T$weighted average of 6.5 fs {I21} from ({+31}P,n|g), 9.7 fs {I49} from (|a,n|g), 5.5 fs {I35} from (p,|g) E=res, and 5.6 fs {I9} from measured width in (|g,|g'), all by DSAM except noted. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,|g) E=res 
J$spin=2 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=1 from 1/2+ 
T$weighted average of 75 fs {I9} from ({+31}P,n|g), 69 fs {I18} from (|a,n|g), 48 fs {I6} from (p,|g) E=res, and 55 fs {I14} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 6412 {I2} from (|a,n|g) and 6410 {I2} from (p,|g) E=res. Other: 6440 {I20} in (p,p'|g) 
J$L(p,t)=4 from 0+ 
T$from DSAM in ({+6}Li,pn|g). Other: 24 fs {I8} from (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 6580 {I5} in ({+3}He,d), 6581 {I10} in (|a,|a'), and 6584 {I5} in (p,t). Other: 6580 from (p,p'|g) 
J$L(|a,|a')=0 from 0+. Other: (2+,3-) from (p,p') is discrepant 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |g(|q,pol) in (p,|g) E=res 
T$from (p,|g) E=res. Other: 1.05 ps {I30} from (|a,n|g) is discrepant 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$from {+31}P(p,|g) |g|q, {+34}S(p,t) angular distributions and L=2 in {+31}P({+3}He,d). 
T$weighted average of 42 fs {I10} from (p,|g) E=res and 49 fs {I21} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=5 from n|g(|q) in (|a,n|g); |p=natural from (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=4 from |g(|q) in (p,|g) E=res; L(|a,|a')=4 from 0+ 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$spin=1 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=2 from 1/2+. Isobaric analog state of g.s. 1+ in {+32}P and {+32}Cl. 
T$weighted average of 1.8 fs {I9} from ({+31}P,n|g) and 1.4 fs {I5} from (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$spin=2 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=2 from 1/2+ 
T$weighted average of 2.9 fs {I13} from ({+31}P,n|g) and 1.59 fs {I35} from (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$L(d,n)=L({+3}He,d)=0 from 1/2+; strong |g to 0+ g.s. 
T$weighted average of 8.3 fs {I21} from ({+31}P,n|g) and 4.9 fs {I17} from (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; 2654|g to 1+ 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(d,n)=L({+3}He,d)=1 from 1/2+; M2 for 7433|g to 0+ ruled out by RUL; 
T$from ({+31}P,n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$spin=2 from |g(|q) in (p,|g) E=res; 7483|g E2 to 0+ 
T$weighted average of 5.0 fs {I12} from DSAM in ({+31}P,n|g), 5.5 fs {I8} from DSAM in (p,|g) E=res, and 9.4 fs {I16} from measured width in (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(p,p')=0 from 0+; L(|a,|a')=0 from 0+ for a group at 7650 {I50}. 0+ also from shell-model prediction (2012Me03). Other: 1+ proposed by 1989Cr02 in (p,p') with L(p,p')=0 and T=1 is considered unrealistic by 1997Br07 based on the facts of no analog state in {+32}P and no expected |g transition to ground state. Similar for J(7921) level 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; L({+3}He,d)=3 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: 4(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=4 from |g(|q) in (p,|g) E=res; 2335|g to 2+ 


level_energy_unit: KEV
level_spin_parity: 0-,1-,2-
level_comment:
E$weighted average of 7887 {I4} from (d,n) and 7883 {I5} from ({+3}He,d). This level is considered different from 7882.9 level in (p,|g) E=res due to different spin assignments. 
J$L(d,n)=L({+3}He,d)=1 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$L(p,p')=0 from 0+; L(|a,|a')=0 from 0+ for a group at 7950 {I50}. Other: 1+ proposed by 1989Cr02 in (p,p') is discrepant. See comment for J(7637) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=4 from |g(|q) in (p,|g) E=res; L({+3}He,d)=3 from 1/2+ 
T$other: 0.15 ps {I+15-10} from (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$from (p,t) 
J$L(p,t)=4 from 0+. Note that |s(|q) in (p,t) is fitted well with L=4, which is inconsistent with L(d,n)=3 from 1/2+ for a group at 7962 {I2} and L({+3}He,d)=3 from 1/2+ for a group at 7973 {I5}, indicating two different levels with similar energies. Other: L({+3}He,|a)=(2) from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=3 from 1/2+; L(|a,|a')=3 from 0+ for a group at 8000 {I50} 


level_energy_unit: KEV
level_spin_parity: 4(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin from |g(|q) in (p,|g) E=res; 2643|g to 2+ 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from (|a,n|g) 
J$spin=3,5 from n|g(|q) in (|a,n|g) and |p=- from Mult with RUL; M2 for 2304|g from 5+ proton resonance ruled out by RUL 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from (p,|g) E=res; L(d,n)=L({+3}He,d)=3 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$this level from (p,|g) E=res is considered different from 8499 level because of no observation of a strong g.s. transition from 8504 level, as seen from 8499 level 
J$L(p,t)=(0) from 0+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g) E=res 
J$spin=2 from |g(|q) in (|a,|g) E=res, with |p=natural for this |a resonance 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; M2 for 2940|g from the 5+ proton resonance is ruled out by RUL. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$allowed |e feeding from 1+ parent, log {Ift}=5.1 {I1}; |p=natural for |a resonance in (|a,|g) E=res; 8860|g to 0+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g) E=res. 
J$L(d,n)=L({+3}He,d)=3 from 1/2+; |p=natural for |a resonance in (|a,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 4-,6-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,n|g). 
J$spin=4,6 from |g(|q) in (p,|g) E=res: 2262|g M1+E2 to 5- 
T$from DSAM in (|a,n|g) 
$%|a: deduced by the evaluator based on |G{-|a}/|G=0.37 {I13} and |G{-|g}/|G=0.75 {I19} measured by 1995Ro22 in (p,|a),(p,p):res. 1995Ro22 don't explain why the sum of |a and |g decay branches is greater 100%. 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(d,n)=L({+3}He,d)=1 from 1/2+; 6828|g to 2+. Other: L(|a,|a')=3 from 0+ for a group at 9060 {I50} (2013It04; measured at |q=4.8|') is inconsistent 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from (|a,|g) E=res 
J$spin=4 from |g(|q) in (|a,|g) E=res; |p=natural for |a resonance in (|a,|g) E=res. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,n|g). Also from (p,|g) E=res 
J$proposes by 1978Ka18 in ({+3}He,d) as analog state of 2178, 3+ level in {+32}P. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$spin=1 from |g(|q) in (p,|g) E=res; allowed |e feeding from 1+ parent, log {Ift}=4.9 {I1}; L(d,n)=0+2 from 1/2+ 
T$from measured width in (|g,|g') 
$This level is considered to decay mostly by |g emission. From 1995Ro22 in (p,|a),(p,p):res, %|a<5 


level_energy_unit: KEV
level_spin_parity: (2+,3,4,5+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$3822|g to 3+, 4776|g to 4+ 
T$from DSAM in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g) E=res 
J$L({+3}He,d)=1 from 1/2+; |p=natural for |a resonance in (|a,|g) E=res 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=2 from 1/2+; proposed by 1997Br07 in (p,|g) E=res as analog state of 2218, 2+ level in {+32}P 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=1 from |g(|q) in (p,|g) E=res; L(d,n)=0+2 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=2 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=1 from 1/2+ 
$This level decays mostly by proton emission, base on measured |G{-|a}/|G|<0.02 and |G{-|g}/|G<0.05 by 1995Ro22 in (p,|a),(p,p):res 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,|g) E=res. Other: 9466.0 {I15} from (|a,|g) E=res 
J$spin=2 from analysis of |s(|q) in (p,|a),(p,p):resonance; |p=natural for |a resonance in (|a,|g) E=res 
$This level decays by both |a and |g emissions with comparable widths based on |G=3.1 eV in (|a,|g) E=res and (2J+1)|G{-|a}|G{-|g}/|G=0.68 eV in (p,|a),(p,p'):res, but the branching of each channel cannot be uniquely determined based on available data. The proton emission branching ratio is negligible compared to the other two channels, according to measured S{-p|g}=a few eV in (p,|g) E=res. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=1 from |g(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=1 from 1/2+ 
$This level decays by |a, p and |g emissions, with %|a|?75.5, %p|?19.6, and %|g|?4.9 based on |G=8.2 eV {I25} in (|a,|g) E=res, (2J+1)|G{-|a}|G{-|g}/|G=0.885 eV {I78} in (p,|a),(p,p'):res, and (2J+1)|G{-|a}|G{-|g}/|G=0.23 eV {I2} in (p,|g) E=res, assuming particle decays are dominant. 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: FS
level_comment:
J$spin=4,6 from n|g(|q) in (|a,n|g); 3015|g M1+E2 or E2 to 4-; 6- from analysis of |s(|q) in (|p{++},|p{++}') for a group at 9650 {I30} 
T$from DSAM in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(p,p')=0 from 0+; 9657|g to 0+; 1+ also from |g(|q,pol) in (|g,|g') 
$This level decays by |a, p and |g emissions, with %p=4.0 {I14}, %|g=23 {I10}, %|a=100-%p-%|g=73 {I10}, based on (2J+1)|G{-p}|G{-|g}/|G=0.22 eV {I4} in (p,|g) E=res, |G=8.2 eV {I25} from (p,|a),(p,p):res and |G{-|g0}=1.5 eV {I4} from (|g,|g'). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=2 from |g(|q) in (|a,|g) E=res; |p=natural 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=2,3,4 from |g(|q) in (p,|g) E=res; 2962|g to 5-, 3501|g to 2- 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(d,n)=1 from 1/2+; 9829|g to 0+, 1781|g to 4- 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=6 from n|g(|q) in (|a,n|g); 5324|g E2 to 4+ 
T$from DSAM in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+31}P(p,|g). 
J$L({+3}He,d)=3 from 1/2+; L(|a,|a')=3 from 0+ for a group at 9860 {I50}; 9815|g to 0+ 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=1 from analysis of |s(|q) in (p,|a),(p,p):resonance; ({+3}He,d)=1 from 1/2+. Other: 9880 {I50} from (|a,|a')=1 from 0+ is most likely the same level, based in J|p assignment 
$This level decays mainly by proton emission. 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=2 from 1/2+; allowed |e feeding from 1+ parent, log {Ift}=4.9 {I1}; 5427|g to 4+. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L(p,t)=2 from 0+; 2382|g to 0+. Other: 3+ proposed in 1997Br07 in (p,|g) E=res is inconsistent 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+31}P(p,|g). 
J$spin=1 from |g(|q) in (p,|g) E=res; L({+3}He,d)=1 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=4 from |g(|q) in (p,|g) E=res; L({+3}He,d)=3 from 1/2+ for a group at 9985 {I10}, which could be an unresolved doublet 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; 2977|g Q(+O) to 1+ 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=2 from |g(|q) in (p,|g) E=res. 2- proposed by 1997Br07 but 2+ cannot be ruled out 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (p,|a),(p,p):resonance. Other: 9986 in (|a,|g):resonances 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=2 from |s(|q) in (p,|g) E=res; L(d,n)=L({+3}He,d)=1 from 1/2+ 
$|g-emission branching ratio is %|g=0.054 {I11}, deduced from |G=1.60 keV {I24} from (p,|a),(p,p):res and |G{-|g}=0.86 eV {I11} from (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=4 from |g(|q) in (p,|g) E=res; |p=natural for |a resonance in (|a,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LE
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; L(p,p)=2 from 1/2+ g.s. of {+31}P 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; L(p,p)=3 from 1/2+ g.s. of {+31}P 
$|G{-p}=16 eV {I2} and |G{-|a}=49 eV {I17} from (p,|a),(p,p):res 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$weighted average of 10224.8 {I15} from (p,|g) E=res and 10225.0 {I16} from (p,|a),(p,p):resonance 
J$from analysis of |s(|q) in (p,p):resonance, with L(p,p)=1 from 1/2+ of {+31}P g.s. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |g(|q) and |g(|q,pol) in (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 10256.0 {I15} from (p,p):resonances 
J$spin=4 from |g(|q) in (p,|g) E=res; L({+3}He,d)=3 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 10286.7 {I15} from (p,|a),(p,p):resonances 
J$spin=3 from |g|g(|q) in (p,|g) E=res; L(p,p)=1+3 from 1/2+ of {+31}P g.s.; |p=natural for |a resonance in (|a,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$also from (p,|a),(p,p):resonances 
J$spin=2 from |g(|q) in (|p,|g):E=res; L(p,p)=1 from 1/2+ of {+31}P g.s. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$other: 10292.0 {I15} from (p,|a),(p,p):resonances, 10291 {I5} from {+32}Cl |e decay 
J$from |s(|q) in (p,p):resonances, with L(p,p)=2 from 1/2+; |p=natural for |a resonance in (|a,|g):resonances; allowed |e feeding from 1+ parent, log {Ift}=5.11 {I5} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,|a),(p,p):resonances. Other: 10330.9 {I15} from (p,|g) E=res 
J$spin=1 from |s(|q) in (p,p):resonances, with L(p,p)=1 from 1/2+; also L(d,n)=L({+3}He,d)=1 from 1/2+; |p=natural from (|a,|g) E=res 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J,T$from R-matrix analysis of |s(|q) in (|a,|a):resonances. Other: J|p=0+ and |G=40 keV from R-matrix analysis for a group at 10380 in {+4}He({+28}Si,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,|a),(p,p):resonances. Other: 10370.3 {I4} from (p,|g) E=res. 
J$spin=2 from |g(|q) in (p,|g) E=res and also from |s(|q) in (p,p):resonances; L(p,t)=2 from 0+ 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: EV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$other: 10396.7 {I6} from (p,|a),(p,p):resonances. 
J$spin=4 from |g(|q) in (p,|g) E=res; L(p,p)=3 from 1/2+ of {+31}P g.s. 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (p,p'):resonances, L(p,p)=1 from 1/2+ of {+31}P. Other: 10399.2 {I15} from (p,|g) E=res 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L({+3}He,d)=2,3 from 1/2+; |p=natural for |a resonance in (|a,|g) E=res. 3- proposed by 1997Br07 based on |g-decay modes in (|a,|g) E=res, but 2+ cannot be ruled out 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 10459 {I5} in {+32}Cl |e decay and 10456 {I6} from (p,|a),(p,p):resonances. 
J$spin=0,1 from |s(|q) in (p,|a),(p,p):resonances; |p=natural for |a resonance; L=0 for resonance in {+4}He({+28}Si,|a):resonances; L(|a,|a')=0 from 0+ for a group at 10490 {I50} 
T$other: 1.7 keV from (|a,|a):resonances, 30 keV from {+4}He({+28}Si,|a):resonances 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$10507|g to 0+. Other: 2+ proposed in 1997Br07, but 1 and 2- cannot be ruled out 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 10531 {I5} from {+32}Cl |e decay and 10525 {I6} from (p,|a) 
J$spin=2 from |s(|q) in (p,|a),(p,p):resonances; allowed |e feeding from 1+ parent; 


level_energy_unit: KEV
level_spin_parity: 2-,3-,4-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from ({+3}He,d). Other: 10539 from (p,p'):resonances. 
J$L({+3}He,d)=3 from 1/2+. Other: L(|a)=1 in {+4}He({+28}Si,|a) suggests 1- 
T$other: 20 keV {+4}He({+28}Si,|a) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=5 from |g(|q) in (p,|g) E=res; parity from rejecting L=5 as a result of strong centrifugal barrier (1997Br07). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$2+,3- from |s(|q) in (p,|a),(p,p):resonances; 10602|g to 0+. Other: 1- in 1997Br07 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from (p,|a),(p,p):resonances. Other: 10624 {I10} from ({+3}He,d) 
J$spin=3 from |s(|q) in (p,|a),(p,p):resonances; L({+3}He,d)=3 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: (3-,4+,5-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
T$3874|g to 5-, 2935|g to 3-; |p=natural for |a resonance in (|a,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$from {+31}P(p,|g). 
J$from |s(|q) of (p,|a):resonances; L(d,n)=L({+3}He,d)=1 from 1/2+. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$L=5 from 0+ in {+4}He({+28}Si,|a):resonances; also 3943|g to 5-, 3004|g to 3- in (p,|g) E=res 
T$from {+4}He({+28}Si,|a):resonances 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from (d,n). Other: 10771 from (p,|a),(p,p):resonances 
J$1-,2+ from |s(|q) of (p,|a):resonances; L({+3}He,d)=1 from 1/2+ for group at 10777 {I10}, which could be a doublet or triplet 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$the 10778 {I10} resonance from (p,|a),(p,p):resonances is likely an unresolved triplet of 10778+10783+10784 that are divided in (p,|g) E=res. |G=4.4 keV for the 10788 {I10} resonance 
J$10776|g to 0+, 3428|g to 3(+), 1755|g to 3- 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$see comment for 10788 level 
J$allowed |e feeding from 1+ parent, log {Ift}=4.5 {I1}; L(p,t)=2 from 0+ 


level_energy_unit: KEV
level_spin_parity: (0,1,2,3+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,T$see comment for 10788 level 
J$3782|g to 1+ 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |s(|q) of (p,|a):resonances and |s(|q) of (|a,|g):resonance. Other: 2+ proposed in 1988Fa01 in (p,|a),(p,p):resonance is in disagreement, which might indicate a different level with similar energy 


level_energy_unit: KEV
level_spin_parity: (2)+
level_comment:
E$from {+32}Cl |e decay 
J$allowed |e feeding from 1+ parent, log {Ift}=5.0 {I1}; |p=natural based on observed subsequent |a decay of this level. 1988Fa01 in (p,|a),(p,p):resonance propose 2+ for a resonance at similar energy, might be the same level as this one. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (|a,|g):resonance, with spin from |g(|q) and |p=natural 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E,J$from (p,|a),(p,p):resonance, with J|p from |s(|q) of (p,|a); L=1 from 1/2+ for a group at 10819 {I6} in (d,n) and at 10826 {I10} in ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (p,|a),(p,p):resonance, with J|p from |s(|q) of (p,|a). Also see comment for 10822 level 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=1 from |g(|q) in (|a,|g):resonance, with |p=natural. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,|a),(p,p):resonances 
J$spin=2 from |g(|q) in (|a,|g) E=res; |p=natural 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g) E=res 
J$spin=1 from |g(|q) in (|a,|g) E=res; |p=natural 


level_energy_unit: KEV
level_spin_parity: 1+,(2-)
level_comment:
E,J$from (e,e'), with J|p from (e,e') strength. Others: L=0 for a {+4}He({+28}Si,|a) suggests 0+ for a group at 10880; 3- from (|a,|a') for a group at 10890 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$others: 10907 {I10} from (p,|a):resonances, 10920 {I50} from (|a,|a') 
J$from |s(|q) of (p,|a):resonances; L(|a,|a')=1 from 0+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (|a,|g) E=res, with J|p from |g(|q) and |p=natural 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$from (|a,|a):resonances. Other: 2+ for a resonance at 10950 in {+4}He({+28}Si,|a):resonances is inconsistent 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin from |g(|q) in (p,|g) E=res; |p=natural from (|a,|g) E=res 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3-,4+,5-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (|a,|g) E=res, with J|p from |g(|q) and |p=natural. Other: 0+ from L=0 for a 11050 resonance in {+4}He({+28}Si,|a) is inconsistent, but it is more likely the same level as 11052 in (|a,|g) E=res because of the same reaction mechanissm, other than as 11063 level in {+32}Cl |e decay. 


level_energy_unit: KEV
level_spin_parity: 0+,2+
level_comment:
E$from {+32}Cl |e decay. 
J$allowed |e feeding from 1+ parent, log {Ift}=5.4; |p=natural from observed |a decay 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (|a,|g) E=res, with J|p from |g(|q) and |p=natural. 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$11113|g to 0+, 4490|g to 4-; |p=natural from (|a,|g) E=res 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$primary 11120|g to 0+. Other: 1+ proposed in 1997Br07 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |s(|q) of (p,p'):resonances, with L(p,p')=0; 11129|g to 0+ 


level_energy_unit: KEV
level_spin_parity: (1,2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$primary 11137|g to 0+. Other: 1+ proposed in 1997Br07 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res. Other: 3+ proposed in 1997Br07, but 3- cannot be ruled out 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; |p=natural in (|a,|a):resonances 
T$from (|a,|a):resonances. Other: 20 keV from {+4}He({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$from (|a,|a):resonances. Other: 2+ for a 11410 resonance in {+4}He({+28}Si,|a) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; 2745|g (M1+E2) to 3+ 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$7707|g to 0+. Other: 2+ proposed in 1997Br07 


level_energy_unit: KEV
level_spin_parity: (0+,1-)
level_lifetime_unit: KEV
level_comment:
E$weighted average of 11556 {I10} from (p,|a) and 11551 {I10} from ({+3}He,d) 
J$from |s(|q) of (p,|a):resonances. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |s(|q) of (p,|g):resonances; L(d,n)=1 from 1/2+ 


level_energy_unit: KEV
level_spin_parity: (1,2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$4066|g to 0+, 6595|g to 3-. Other: 2+ proposed in 1997Br07 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$from ({+3}He,d) 
J$from |s(|q) of (p,p'), with L(p,p')=0. Other: 0+ for a 11620 level in (|a,|a') is inconsistent 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$from (|a,|a):resonances; J|p=3- also from R-matrix analysis of |s(|q) in {+4}He({+28}Si,|a):resonances 
T$other: 10 keV from {+4}He({+28}Si,|a) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=5 from |g(|q) in (p,|g) E=res; |p=- is ruled out since it would require L=5 capture which is effectively suppressed by the centrifugal barrier (1997Br07). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=5 from |g(|q) in (p,|g) E=res; |p=- is ruled out since it would require L=5 capture which is effectively suppressed by the centrifugal barrier (1997Br07). Other: (4+) from ({+20}Ne,|a) for a 11700 level, (2+) from (p,|a):resonances for a 11695 resonance, and 1- from (|a,|a') for a 11710 resonance are inconsistent 
T$other: 55 keV {I24} from {+16}O({+20}Ne,|a) may belong to this level but many levels overlap within uncertainties. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |g(|q) in (|a,|g) E=res and |p=natural. Other: 2+ for a 11730 {I50} resonance from (|a,|a') is inconsistent 


level_energy_unit: KEV
level_spin_parity: (3-,4,5-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$3462|g to 3-, 4996|g to 5-. Other: 2+ for a 11730 {I5} resonance from (|a,|a') is inconsistent 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-,2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E,J$from (|a,|g) E=res, with J|p from |g(|q) and |p=natural. Other: (3-) for a 11800 resonance in {+4}He({+28}Si,|a) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
E$weighted average of 11876 {I10} from ({+3}He,d) and 11880 {I10} from (e,e'). 
J$from |s(|q) in (e,e') 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=3 from |g(|q) in (p,|g) E=res; L({+3}He,d)=3 from 1/2+. Other: 3-,2+ from (p,|a):resonances; (2+) for 11940 resonance in {+4}He({+28}Ca,|g) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 6-
level_lifetime_unit: KEV
level_comment:
E,T$from ({+20}Ne,|a). 
J$from (e,e') and (|p{++},|p{++}). Other: 5- from ({+20}Ne,|a) is inconsistent 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$from |g(|q) in (|a,|g) E=res and |p=natural 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
J$spin=2,3,4 from |g(|q) in (p,|g) E=res; 4- from analysis of |s(|q) in (p,p):resonances with L(p,p)=3; L(d,n)=L({+3}He,d)=3 from 1/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g) E=res 
J$from |g(|q) in (|a,|g) E=res and |p=natural; 3- also from |s(|q) in (|a,|a):resonances 
T$from (|a,|a):resonances 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 12151 {I10} from (p,|a):resonances and 12160 {I10} from ({+3}He,d) 
J$(3-,2+) from |s(|q) in (p,|a),(p,p):resonances; L({+3}He,d)=(2) from 1/2+ 
T$other: 40 keV from {+4}He({+28}Si,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J$levels from all five different reactions have the exact same energies, but completely different spin parities. Adopted J|p=0+ here is from (p,|a),(p,p):resonances, and others are 0-,1-,2- from L(d,n), 1+ from (e,e'), and 4+ from L(|a,|a')=4. No J|p is assigned to 12190 level in (|p{++},|p{++}'). If all the different spin-parity assignments are considered correct, there would be at least four levels with the same energy. 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 12297 {I10} from (p,|a):resonances and 12308 {I10} from ({+3}He,d) 
J$from |s(|q) in (p,|a):resonances 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 12389 {I10} from (p,|a):resonances and 12393 {I10} from ({+3}He,d) 
J$3-,(2+) from |s(|q) in (p,|a):resonances; L({+3}He,d)=1 from 1/2+ suggests 0-,1-,2-, probably indicating a different level 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 12422 {I10} from (p,|a) and 12426 {I10} from ({+3}He,d) 
J$from |s(|q) of (p,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 3-,2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 12457 {I10} from (p,|a) and 12465 {I10} from ({+3}He,d) 
J$from |s(|q) of (p,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$from |s(|q) of (p,|a):resonances. 
T$other: 30 keV from {+4}He({+28}Si,|a):resonances, with J|p=3- assumed 


level_energy_unit: KEV
level_spin_parity: 6-
level_comment:
E,J$from (|p{++},|p{++}'). But 4+ from (|a,|a') for a group at 12630 {I50} is inconsistent, probably indicating a different level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-,3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$(5-) from (|a,|a):resonances and (3-) from {+4}He({+28}Si,|a):resonances 
$|G: other: 30 keV from ({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-,4+)
level_lifetime_unit: KEV
level_comment:
E,T$from (|a,|a):resonances. Other: 50 keV from ({+28}Si,|a):resonances 
J$(5-) from L(|a,|a)=(5), (4+) from L=(4) in ({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5-,6+)
level_lifetime_unit: KEV
level_comment:
E,T$from (|a,|a):resonances. Other: 16690 with |G=50 keV in ({+28}Si,|a):resonances 
J$(5-) from L(|a,|a)=(5) and (6+) from L=(6) in ({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+,7-)
level_lifetime_unit: KEV
level_comment:
E,T$from (|a,|a):resonances. Other: 18980 with |G=60 keV from ({+28}Si,|a):resonances 
J$(8+) from L(|a,|a')=(8), (7-) from L=(7) in ({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+,7-)
level_lifetime_unit: KEV
level_comment:
E,T$from (|a,|a):resonances. Other: 19120 with |G=70 keV from ({+28}Si,|a):resonances 
J$(8+) from L(|a,|a')=(8), (7-) from L=(7) in ({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (8+,7-)
level_lifetime_unit: KEV
level_comment:
E,T$from (|a,|a):resonances. Other: 19800 with |G=90 keV from ({+28}Si,|a):resonances 
J$(8+) from L(|a,|a')=(8), (7-) from L=(7) in ({+28}Si,|a):resonances 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$rounded value from Adopted Levels 
J$2012Me03 also propose 0+ based on shell-model calculation 


level_energy_unit: KEV
level_comment:
E$other: 2237 {I10} (1968Gr17) 
S$others: 5.7 (1994Ve04), 5.64 (1973Ka26), 6.5 (1970Mo01), 6.0 (1968Gr17) 


level_energy_unit: KEV
level_comment:
E$other: 3780 {I10} (1968Gr17) 
S$others: 0.72 (1994Ve04), 0.64 (1973Ka26), 0.66 (1970Mo01), 0.40 (1968Gr17) 
$E0 decay strength to g.s=2.22 fm{+2} 27 (1975Ad03) 
$|G(E0,pair)/|G=0.00035 {I6} (1975Ad03) 


level_energy_unit: KEV
level_comment:
E$others: 5006 {I10} (1968Gr17), 5012 {I8} (1960Hi13) 
S$others: 4.08 (1973Ka26), 3.5 (1970Mo01), 2.24 (1968Gr17) 


level_energy_unit: KEV
level_comment:
E$others: 5548 {I10} (1968Gr17), 5553 {I8} (1960Hi13) 
S$others: 0.70 (1973Ka26), 1.0 (1970Mo01), 0.64 (1968Gr17) 


level_energy_unit: KEV
level_comment:
E$others: 5790 {I10} (1968Gr17), 5799 {I8} (1960Hi13) 
S$others: 0.66 (1973Ka26), 0.78 (1970Mo01), 0.56 (1968Gr17) 


level_energy_unit: KEV
level_comment:
E$others: 6221 {I10} (1968Gr17), 6226 {I8} (1960Hi13) 
S$others: 0.67 (1973Ka26), 0.95 (1970Mo01), 0.60 (1968Gr17) 


level_energy_unit: KEV
level_comment:
E$others: 6666 {I10} (1968Gr17), 6671 {I8} (1960Hi13) 
L$L=2 (1978Ka18) disagrees with L=3 (1970Mo01) but in the latter, contributions from impurities are present. L=(3) in 1968Gr17 
S$other: (0.72) (1968Gr17) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$others: 8110 (1984Bu06), 8130 {I70} (1971Fa15) 
BM1$weighted average of 0.87 {I9} (2002Ho02), 1.14 {I18} (1984Bu06), 1.4 {I7} (1971Fa15) 
$|G{-0}(M1)=2.35 eV {I37} (1984Bu06), 2.8 eV {I+18-14} (1971Fa15) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$other: 9660 {I30} (2002Ho02) 
BM1$weighted average of 0.37 {I6} (2002Ho02), 0.55 {I24} (1994Pe08), and 0.69 {I18} (1984Bu06) 
$|G{-0}(M1)=2.41 eV {I63} (1984Bu06) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$others: 11140 {I70} (1971Fa15), 11140 {I30} (2002Ho02) 
BM1$weighted average of 2.21 {I15} (2002Ho02), 2.40 {I22} (1984Bu06), and 3.6 {I13} (1971Fa15). Other: 1.24 {I13} (1994Pe08) is discrepant 
$|G{-0}(M1)=11.6 eV {I12} (1984Bu06), 18.9 eV {I+74-63} (1971Fa15) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$others: 11620 {I70} (1971Fa15), 11640 {I30} (2002Ho02) 
BM1$weighted average of 1.04 {I9} (2002Ho02), 0.77 {I14} (1994Pe08), 1.26 {I20} (1984Bu06), 1.6 {I9} (1971Fa15) 
$|G{-0}(M1)=7.7 eV {I12} (1984Bu06), 9.7 eV {I+61-48} (1971Fa15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$other: 2220 {I30} (1971Ka58) 
L$from 1967Cr07 
$|b{-2}=0.30 {I2} (2001Kh17), 0.37 (1967Cr07) 
J$ also confirmed by 1968Wi05 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$other: 6450 {I50} (2013It04) 
J,L$for a group at 6450 (2013It04). Other: |p=natural from 1973Ga30 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$other: 6590 {I50} (2013It04) 
J,L$for a group at 6590 (2013It04). Other: |p=natural from 1973Ga30 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$other: 6800 {I50} (2013It04), probably corresponding to 6762+6854 
J,L$for a group at 6800 (2013It04). Other: |p=natural from 1973Ga30 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$isoscalar giant quadrupole resonance. Uncertainty=+0.65-0.83 MeV. E2 EWSR=143% {I+9-12} (2013It04) 
T$rms width (2013It04) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$isoscalar giant monopole resonance. Uncertainty=+0.60-0.66 MeV. E0 EWSR=108% {I+7-8} (2013It04) 
T$rms width (2013It04) 


level_energy_unit: KEV
level_comment:
E$this peak contaminated by contribution from a state in {+31}S (1979Cr02) 
L,S$0.19 for 1d{-5/2} orbit and 0.06 for 2s{-1/2} for unresolved 7640+7700 including contribution from a {+31}S level, with L=2 component from the latter and L=0 for one of 7640 and 7700 levels in {+32}S; limited |s(|q) data (1979Cr02) 


level_energy_unit: KEV
level_comment:
E$other: 7005 (1969Ha19), 7010 (1970Mc04). Analog to 78-keV level of {+32}P 
$Measured d|s/d|W(p,t)/d|s/d|W(p,{+3}He)=1.20 {I30}, compared to predicted value of 1.8 for T=1 (1969Ha19) 


level_energy_unit: KEV
level_comment:
L$|s(|q) fitted well with L=4, which is however inconsistent with L({+3}He,d)=3, which might indicate a different level 


level_energy_unit: KEV
level_comment:
E$from 1970Ha10, also seen by 1979Fr04. Analog to g.s. of {+32}Si and 5071 {I40} level of {+32}P (1970Ha10). Other: 11980 (1970Mc04) 
L$observed |s(|q) consistent with L=0 (1970Ha10) 
$Measured d|s/d|W(p,t)/d|s/d|W(p,{+3}He)=0.66 {I6}, compared to predicted value of 0.60 for T=2 (1970Ha10) 
$Others: %p=86 {I17}, %|a=18 {I7} to g.s. and 11 {I5} to 1st excited state in {+28}Si (1970Mc04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=9.4 fs {I30}, weighted average of 6.9 fs {I30} at E=24 MeV and 11.8 fs {I30} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=108 fs {I13}, weighted average of 99 fs {I20} at E=24 MeV and 112 fs {I13} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=2.6 fs {I12}, weighted average of 2.3 fs {I12} at E=24 MeV and 2.8 fs {I12} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=4.2 fs {I18}, weighted average of 7 fs {I4} at E=24 MeV and 3.6 fs {I18} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=12 fs {I3}, weighted average of 11 fs {I4} at E=24 MeV and 12 fs {I3} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=11.1 fs {I14}, weighted average of 10.0 fs {I18} at E=24 MeV and 11.7 fs {I14} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=7.2 fs {I17}, weighted average of 6.8 fs {I20} at E=24 MeV and 7.4 fs {I17} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$from |t=4.8 fs {I15}, unweighted average of 6.3 fs {I11} at E=24 MeV and 3.3 fs {I10} at E=29 MeV (1998Ka31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 10+
level_comment:
E$from E{-cm}=15.10 MeV (1986Ga24). Others: E{-cm}=15.20 in 1985Li04 and 1984Po15 
J,L$also from 1985Li04 and 1984Po15 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 12+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from E{-cm}=15.95 MeV (1985Ti05). Other: E{-cm}=15.93 MeV (1985Ga05) 
J$other: (8) from 1985Ga05 is discrepant 
$|G{-0}|G{-|a}/|G{+2}=0.000225 (1985Ga05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from E{-cm}=16.10 MeV (1985Ga05). Other: E{-cm}=16.05 MeV (1985Ti05) 
J,L$also from 1985Ti05 
$|G{-0}|G{-|a}/|G{+2}=0.0001 (1985Ga05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 8+
level_comment:
E$from E{-cm}=16.30 MeV (1985Ti05) 
$|G=153 keV for E{-cm}=16.32 MeV in 1983Ti01, probably a doublet of 16.30+16.35 resonances as stated in 1985Ti05 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 12+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from E{-cm}=17.30 MeV (1986Ga24). Other: E{-cm}=17.40 MeV (1985Ti05) 
J,L$also from 1985Ti05 
T$from 1983Ti01 for E{-cm}=17.31 MeV 
$|G{-|a0}=4.9 keV (1985Ti05), 3 keV (1983Ti01) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: PS
level_comment:
E$from 1969Gr03 
T$from |t=0.31 ps {I8}, weighted average of 0.30 ps {I8} (line-shape) and 0.33 ps {I12} (centroid-shift) in 1969Gr03 using DSAM. 
$Deformation parameter |b{-2}=0.25 {I2} (1969Gr03) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E|a=1766 {I2} (1985Ma32), 1767 {I2} (1977Ro07). Others: 1770 (2002Ba81), 1776 {I5} (1971To06) 
$|w|g=16 meV {I3} (1977Ro07), 25 meV {I7} (1971To06), 19.7 meV {I20} (2002Ba81) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E|a=1990 {I3} (1977Ro07), 1995 {I5} (1971To06) 
$|w|g=12 meV {3} (1977Ro07), 20 meV {I6} (1971To06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E|a=2187 {I3} (1977Ro07), 2187 {I7} (1971To06) 
$|w|g=16 meV {I3} (1977Ro07), 41 meV {I14} (1971To06) 


level_energy_unit: KEV
level_comment:
$E|a=2370 (2002Ba81), 2371 {I3} (1977Ro07), 2370 {I4} (1971To06) 
$|w|g=52 meV {I10} (1977Ro07), 93 meV {I23} (1971To06), 58 meV {I6} (2002Ba81) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$spin=4 from |g(|q) in 1985Ma32; |p=natural 
T$from DSAM in 1985Ma32 
$E|a=2420 (2002Ba81), 2419 {I2} (1977Ro07), 2415 {I5} (1971To06) 
$|w|g=64 meV {I13} (1977Ro07), 134 meV {I34} (1971To06), 49 meV {I11} (2002Ba81) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E|a=2610 (2002Ba81), 2614 {I2} (1977Ro07), 2618 {I4} (1971To06), 2618 {I4} (1964Sm03) 
$|w|g=540 meV {I100} (1977Ro07), 610 meV {I150} (1971To06), 505 meV {I34} (2002Ba81), 300 meV (1964Sm03) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E|a=2880 (2002Ba81), 2877.5 {I16} (1977Ro07), 2878 {I4} (1964Sm03) 
$|w|g=720 meV {I150} (1977Ro07), 667 meV {I85} (2002Ba81), 400 meV (1964Sm03). Average of the first two is 680 meV {I85} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E|a=2900 (2002Ba81), 2901 {I2} (1977Ro07), 2904 {I4} (1964Sm03) 
$|w|g=830 meV {I170} (1977Ro07), 897 meV {I78} (2002Ba81), 700 meV (1964Sm03). Average of the first two is 885 meV {I78} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E|a=3159 {I2} (1977Ro07), 3162 {I4} (1964Sm03) 
$|w|g=630 meV {I130} (1977Ro07), 300 meV (1964Sm03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E|a=3474 (1997Br07) 
J$identified by 1997Br07 as the 0+ level seen in (p,p):resonances 
$|w|g|?20 meV (1997Br07) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$3814 {I2} (1977Ro07) and 3816 {I2} (1985Ma32), 3820 (1969Ve01), 
$|w|g=2.3 eV {I4} (1977Ro07), 3.0 eV {I12} (1969Ve01) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$from E|a=3983.4 {I17} (1997Br07). Other: 3992 {I8} (1967Ve05) 
J$from 1997Br07 based on |g-decay modes. 
$|w|g=0.5 eV {I2} (1967Ve07) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 2230.0 {I3} (1974Vi02), 2230.5 {I3} (1972Co13), 2231.1 {I10} (1973Ve08) 
J$spin from |g(|q) in 1973Ve08; 2051|g E2(+M1) from 2+ 
T$weighted average of 175 fs {I28} (1998Ka31), 135 fs {I49} (1974Ch09), 128 fs {I52} (1972Co13), 180 fs {I55} (1969Th03), 121 fs {I21} (1971Re15). 
T$from |t=205 fs {I30}, weighted average of 252 fs {I40} (1998Ka31), 195 fs {I70} (1974Ch09), 185 fs {I75} (1972Co13), 260 fs {I80} (1969Th03), 175 fs {I30} (1971Re15). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
E$weighted average of 3776.0 {I12} (1974Vi02), 3778.2 {I18} (1972Co13), 3778.1 {I14} (1973Ve08). 
J$1549|g(|q) is isotropic (1971In02); M2 for 1547|g to 2+ is ruled out by RUL 
T$weighted average of 0.9 ps {I3} (1998Ka31), 0.36 ps {I+21-7} (1969Pi10), 0.70 ps {I14} (1974Ch09), 0.83 ps {I38} (1972Co13). 
T$from |t=0.85 ps {I+20-17}, weighted average of 1.3 ps {I4} (1998Ka31), 0.52 ps {I+30-10} (1969Pi10), 1.00 ps {I20} (1974Ch09), 1.20 ps {I55} (1972Co13). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 4281.2 {I10} (1974Vi02), 4282.2 {I10} (1972Co13), 4280.8 {I10} (1973Ve08). 
J$4281|g E2, |DJ=2 to 0+ 
T$unweighted average of 40.0 fs {I14} (1998Ka31), 20.1 fs {I14} (1969Pi10), 35 fs {I9} (1969Th03), 25 fs {I6} (1972Co13), 29.0 fs {I27} (2000Ya23). 
T$from |t=43 fs {I5}, unweighted average of 57.7 fs {I20} (1998Ka31), 29 fs {I2} (1969Pi10), 50 fs {I13} (1969Th03), 36 fs {I8} (1972Co13), 41.8 fs {I39} (2000Ya23). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
E$weighted average of 4458.4 {I8} (1974Vi02), 4458.9 {I10} (1972Co13) 
J$2229|g E2, |DJ=2 to 2+ 
T$from 1974Ch09 
T$|t=0.20 ps {I9} (1974Ch09) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: PS
level_comment:
E$4695.6 {I5} (1974Vi02), 4695.3 {I4} (1972Co13), 4696.0 {I10} (1973Ve08) 
J$spin from |g(|q) 1973Ve08 
T$unweighted average of 0.367 ps {I35} (1969Pi10), 0.119 ps {I70} (1969Th03), 0.277 ps {I28} (1998Ka31), 0.170 ps {I35} (1974Ch09), 0.159 ps {I38} (1972Co13). 
T$from |t=0.315 ps {I66}, unweighted average of 0.53 ps {I5} (1969Pi10), 0.17 ps {I10} (1969Th03), 0.40 ps {I4} (1998Ka31), 0.245 ps {I50} (1974Ch09), 0.230 ps {I55} (1972Co13). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$weighted average of 5006.2 {I3} (1976Ve03), 5006.5 {I10} (1972Co13), 5005.4 {I8} (1974Vi02), 5007.8 {I14} (1973Ve08). 
J$from |g(|q,pol) in 1968Do14; spin also from |g(|q) (1973Ve08) 
T$unweighted average of 1.04 ps {I+180-49} (1969Pi10), 0.173 ps {I35} (1969Th03), 0.263 ps {I49} (1998Ka31), 1.07 ps {I26} (1974Ch09), 0.69 ps {I28} (1971Re15), 0.243 ps {I56} (1972Co13), 0.42 ps {I10} (1976Ve03). 
T$from |t=0.80 ps {I21}, unweighted average of |t=1.5 ps {I+26-7} (1969Pi10), 0.25 ps {I5} (1969Th03), 0.38 ps {I7} (1998Ka31), 1.55 ps {I38} (1974Ch09), 1.0 ps {I4} (1971Re15), 0.35 ps {I8} (1972Co13), 0.60 ps {I14} (1976Ve03). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
E$weighted average of 5412.6 {I10} (1972Co13), 5410.4 {I15} (1974Vi02), 5413.8 {I14} (1973Ve08). 
J$spin from |g(|q) 1972Co13; 3182|g M1+E2 to 2+ 
T$weighted average of 67.2 fs {I35} (1969Pi10), 67 fs {I18} (1972Co13), 111 fs {I28} (1976Ve03), 164 fs {I28} (1998Ka31). 
T$contaminating transition in lineshape leads to often quoted 150 fs lifetime (1998Ka31), proper value of |t=237 fs {I40} (1998Ka31) or T{-1/2}{-1/2}=164 fs {I28} 
T$from |t=147 fs {I34}, unweighted average of 97 fs {I5} (1969Pi10), 95 fs {I25} (1972Co13), 160 fs {I40} (1976Ve03), 237 fs {I40} (1998Ka31). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 5546.2 {I12} (1974Vi02), 5548.5 {I14} (1972Co13), 5550.3 {I17} (1973Ve08). 
J$spin from |g(|q) in 1997Br07; 3319|g E2+M1 to 2+ 
T$weighted average of 0.030 ps {I24} (1969Pi10), 0.047 ps {I8} (1969Th03), 0.066 ps {I8} (1998Ka31), 0.07 ps {I2} (1972Co13). 
T$from |t=81 fs {I12}, weighted average of 43 fs {I35} (1969Pi10) , 68 fs {I12} (1969Th03), 95 fs {I12} (1998Ka31), 100 fs {I30} (1972Co13). 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$weighted average of 5797.2 {I19} (1974Vi02), 5797.6 {I10} (1972Co13). 
T$from 1972Co13 
T$|t=8 fs {I5} (1972Co13) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_comment:
E$6224.3 {I9} (1976Ve03), 6224.2 {I10} (1972Co13), 6222.9 {I8} (1974Vi02). 
J$spin from |g(|q) 1973Ve08 
T$weighted average of 76 fs {I35} (1969Pi10), 42 fs {I10} (1969Th03), 52.8 ps {I65} (2000Ya23), 90 ps {I28} (1971Re15), 38 fs {I7} (1972Co13), 52 fs {I10} (1976Ve03) 
T$weighted average of |t=110 fs {I+50-30} (1969Pi10), 61 fs {I15} (1969Th03), 76.3 fs {I94} (2000Ya23), 130 fs {I40} (1971Re15), 55 fs {I10} (1972Co13), 75 fs {I15} (1976Ve03) 


level_energy_unit: KEV
level_spin_parity: (4)
level_comment:
E$from 1974Vi02 
J$4599|g D(+Q) from J=4 and 5259|g D+Q from 5+ based on |g(|q) in 1997Br07; (1,2,3,4) from |g(|q) in 1976Ve03 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
E$6621.7 {I3} (1976Ve03), 6621.0 {I10} (1972Co13), 6620.6 {I8} (1974Vi02). 
J$from |g(|q,pol) in 1968Do14; spin also from |g(|q) 1973Ve08 and 1974Gr15 
T$weighted average of 0.26 ps {I6} (1969Pi10), 0.55 ps {I8} (1998Ka31), 0.39 ps {I8} (1974Ch09), 0.29 ps {I7} (1972Co13), and 0.68 ps {I17} (1976Ve03). Other: >0.7 ps (1969Th03) 
T$from |t=0.52 ps {I8}, weighted average of 0.37 ps {I8} (1969Pi10), 0.80 ps {I12} (1998Ka31), 0.56 ps {I11} (1974Ch09), 0.81 ps {I+35-25} (1974Gr15), 0.42 ps {I10} (1972Co13), 0.98 ps {I25} (1976Ve03). Other: >1 ps (1969Th03). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 6666.1 {I10} (1972Co13), 6664 {I2} (1972Le29) 
J$2888|g E2 to 0+ 
T$unweighted average of 37 fs {I9} (1969Pi10), 61 fs {I6} (1998Ka31), 54.1 fs {I58} (2000Ya23), 15 fs {I5} (1972Co13). 
T$from |t=61 fs {I15}, unweighted average of 54 fs {I+13-9} (1969Pi10), 88 fs {I8} (1998Ka31), 78.1 fs {I84} (2000Ya23), 22 fs {I7} (1972Co13). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_comment:
E$from 1972Co13 
J$from Adopted Levels. (3,4,5) from |g(|q) in 1976Ve03 and 1974Gr15. 
T$from 1998Ka31. Other: >210 fs (1974Gr15) 
T$|t=0.375 ps {I50} (1998Ka31), >300 fs (1974Gr15) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
E$weighted average of 6853.5 {I16} (1972Co13), 6851.5 {I15} (1974Vi02) 
T$from 1972Co13 
T$|t=95 fs {I25} (1972Co13) 
J$spin from |g(|q) (1981He09); 2571|g E2 to 2+ 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
E$weighted average of 7001.44 {I36} (2006Tr03), 7003.7 {I10} (1972Co13), 7004.4 {I16} (1974Vi02), 7000.8 {I14} (1973Ve08). 
J$from |g(|q) in 1973Ve08 
T$from 1998Ka31. Other: <3.5 fs (1972Co13) 
T$2.0 fs {I7} (1998Ka31), <5 fs (1972Co13) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 7116.5 {I10} (1972Co13), 7114 {I2} (1972Le29), 7115.7 {I10} (1974Vi02), 7112.8 {I14} (1973Ve08). 
J$spin from |g(|q) in 1974Vi02; 4884|g M1+E2 to 2+ 
T$from 1998Ka31. Other: <3.5 fs (1972Co13) 
T$2.3 fs {I5} (1998Ka31), <5 fs (1972Co13) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$7189.0 {I15} (1972Co13), 7189 {I5} (1972Le29), 7192.4 {I20} (1974Vi02). 
T$from 2000Ya23 
T$7.1 fs {I25} (2000Ya23) ? 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 7484.8 {I10} (1972Co13), 7485 {I3} (1972Le29), 7482.6 {I12} (1974Vi02). 
J$spin from |g(|q) 1981He09; 7482|g E2 to 0+ 
T$weighted average of 4.8 fs {I12} (1998Ka31) and 5.8 fs {I8} (2000Ya23) 
T$from |t=7.9 fs {I12}, weighted average of 6.9 fs {I17} (1998Ka31), 8.4 fs {I12} (2000Ya23) 


level_energy_unit: KEV
level_comment:
E$weighted average of 7535.5 {I10} (1972Co13), 7535 {I5} (1972Le29), 7535.7 {I10} (1974Vi02), 7536.0 {I14} (1973Ve08). 


level_energy_unit: KEV
level_spin_parity: 3
level_lifetime_unit: FS
level_comment:
E$weighted average of 7701.44 {I36} (2006Tr03), 7702.4 {I10} (1972Co13), 7701.8 {I5} (1997Br07), 7701 {I2} (1974Vi02). 
J$from |g(|q) in 1997Br07 
T$from 2000Ya23 
T$96 fs {I28} (2000Ya23) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$weighted average of 7950.0 {I4} (1976Ve03), 7950.8 {I10} (1972Co13), 7950.1 {I14} (1997Br07), 7950 {I3} (1972Le29). 
J$spin from |g(|q) 1976Ve03; 2944|g E2+M1 to 3- 
T$weighted average of 146 fs {I35} (1998Ka31), 90 fs {I18} (1976Ve03), and 76 fs {I+42-28} (1974Gr15) 
T$|t=0.140 ps {I25}, weighted average of 0.21 ps {I5} (1998Ka31), 0.130 ps {I25} (1976Ve03), 0.11 ps {I+6-4} (1974Gr15). 


level_energy_unit: KEV
level_comment:
E$weighted average of 8125.32 {I24} (2006Tr03), 8126.2 {I10} (1972Co13), 8125 {I5} (1972Le29), 8128.0 {I15} (1974Vi02). 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$from 1997Br07. Other: 8294 {I3} (1974Vi02) 
J$from |g(|q) in 1997Br07 
$19% of the intensity unaccounted for by 1997Br07 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$spin from |g(|q) 1997Br07; negative parity rejected because it would required an unrealistically large B(M2) for 2940|g from the 5+ resonance 
E$from 1997Br07 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$from 2006Tr03. E(p)=355 {I6} (1962Be39), 355 {I1} (1974Vi02), 355 {I1} (1991Il01), 355 (1993Il01) 
J$spin from |g(|q) in 1963Te01 and 1962Ne10. |p=+ is proposed by 1962Ne10 based on the argument of observed isotropic |s(|q) consistent with s-wave proton capture 
$S{-p|g}=4.2 meV {I7} (1991Il01), 17 meV {I2} (1975Ob02), 1.3 meV {I5} (1972Co13; renormalized from 3 meV {I1}) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$E(p)=439 {I1} (1991Il01), 439 {I1} (1974Vi02), 440 {I6} (1962Be39) 
J$from |g(|q) (1963Te01) and |g|g(|q) (1962Ne10). |p=+ is proposed by 1962Ne10 based on the argument of observed isotropic |s(|q) consistent with s-wave proton capture 
$S{-p|g}=25 meV {I4} (1991Il01), 130 meV {I20} (1975Ob02), 111 meV {I33} (1972Co13; renormalized from 250 meV {I75}) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$E(p)=541 {I1} (1974Vi02), 541 {I1} (1991Il01), 540 {I6} (1962Be39) 
J$spin from |g(|q) (1963Ch04). 
T$from 1971Re15 
$S{-p|g}=0.12 eV {I2} (1991Il01), 0.51 eV {I6} (1975Ob02), 0.44 eV eV {I13} (1972Co13; renormalized from 1.0 eV {I3}) 


level_energy_unit: KEV
level_comment:
E$E(p)=618.9 {I10} (1964Sm03), 619 {I1} (1991Il01) 
$S{-p|g}=1.1 meV {I2} (1991Il01), 6 meV 4 (1975Ob02), 2.7 meV {I9} (1972Co13; renormalized from 6 meV {I2}), 3 meV (1964Sm03) 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
E$E(p)=642.1 {I10} (1964Sm03), 642 {I1} (1974Vi02) 
J$from |g(|q) (1964Sm03,1963Sp03) 
$S{-p|g}=0.25 eV {I3} (1975Ob02), 0.23 eV {I5} (1964Sm03), 0.36 eV {I18} (1963Sp03), 0.22 eV {I2} (1979Pa16); 0.52 eV {I8} (1966En04). Note that value from 1966En04 has been used as normalization reference in some later studies (1973Ve08 and 1972Co13) while a different normalization reference is used in other studies. The average of other four values in agreement is 0.23 eV {I2}. See the comment about normalization of S{-p|g} at the top of this table. 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$E(p)=811.8 {I5} (1961An01), 811 {I1} (1974Vi02) 
J$from |g(|q) and |g|g(|q) (1963Sp03) 
$S{-p|g}=1.9 eV {I4} (1963Sp03), 0.93 eV {I12} (1979Pa16), 0.95 eV {I20} (1978Pa03), 1.06 eV {I11} (1975Ob02), 1.0 eV 3 (1972Co13; renormalized from 2.2 eV {I7}). 1979Pa16 report a value of 1.00 eV {I8} from average of their value and that of 1975Ob02 and this value has been used as a normalization reference in some later studies. See the comment about different normalization references of S{-p|g} at the top of this table. 


level_energy_unit: KEV
level_comment:
E$E(p)=821 {I1} (1974Vi02) 
$S{-p|g}=0.23 eV {I4} (1975Ob02), 0.19 eV {I7} (1972Co13; renormalized from 0.43 eV {I15}). Average of the two is 0.22 eV {I4} 


level_energy_unit: KEV
level_comment:
E$E(p)=875.5 {I14} (1964Sm03) 
$S{-p|g}=0.060 eV {I20} (1975Ob02), 0.13 eV {I5} (1972Co13; renormalized from 0.29 eV {I10}), 0.03 eV (1964Sm03) 


level_energy_unit: KEV
level_spin_parity: 2,3,4
level_comment:
E$E(p)=888 {I1} (1974Vi02) 
J$from |g(|q) 1972Co13 
$S{-p|g}=0.034 eV {I17} (1975Ob02), 0.08 eV {I3} (1972Co13; renormalized from 0.18 eV {I6}) 


level_energy_unit: KEV
level_comment:
E$E(p)=895 {I1} (1974Vi02) 
$S{-p|g}=0.31 eV {I7} (1975Ob02), 0.3 eV {I1} (1972Co13; renormlaized from 0.7 eV {I2}) 


level_energy_unit: KEV
level_comment:
E$E(p)=983.8 {I10} (1972Co13), 983 {I1} (1974Vi02) 
$S{-p|g}=0.091 eV {I15} (1975Ob02), 0.08 eV {I2} (1972Co13; renormlaized from 0.18 eV {I6}) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$E(p)=994 {I3} (1975Ob02). 1997Br07 legitimately criticizes if this this level truly exists. 
$|G=4.0 keV {I8} from 1975Ob02 
$S{-p|g}=<0.3 eV (1975Ob02) 


level_energy_unit: KEV
level_comment:
E$E(p)=1056.5 {I6} (1972Co13) 
$S{-p|g}=0.49 eV {I15} (1972Co13; renormlaized from 1.1 eV {I3}), 0.55 eV 6 (1975Ob02) 


level_energy_unit: KEV
level_comment:
E$E(p)=1088.4 {I7}, weighted average of 1089.6 {I6} (1972Co13), 1088.0 {I5} (1961An01), 1087 {I1} (1974Vi02) 
$S{-p|g}=0.17 eV {I5} (1972Co13; renormlaized from 0.38 eV {I12}), 0.19 eV {I6} (1975Ob02) 
$Corrected half-width <0.30 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
E$E(p)=1117.7 {I10}, unweighted average of 1120.7 {I6} (1972Co13), 1116.2 {I5} (1961An01), 1117 {I1} (1974Vi02), 1117 {I1} (1972Le29) 
J$from |g(|q) in 1963Sp03 
$S{-p|g}=1.6 eV {I4} (1963Sp03), 1.3 eV {I4} (1972Co13; renormlaized from 3.0 eV {I9}), 1.04 eV {I13} (1975Ob02), 1.7 eV 7 (1972Le29) 
$Corrected half-width <0.15 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 4
level_comment:
E$E(p)=1150.0 {I7} (1981He09). See comments for 9978.2 level 
J$from |g(|q) 1981He09 
$S{-p|g}=0.11 eV {I3} (1981He09). See comments for 9978.2 level for other values undivided for the doublet 
$Corrected half-width <0.16 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$E(p)=1150.5 {I7} (1981He09). The doublet of 1150.0+1150.5 is only identified by 1981He09. Others (unresolved doublet): 1150.5 {I6} (1972Co13), 1146 {I1} (1972Le29), 146 {I1} (1972Le29), 1147.5 {I5} (1961An01) 
J$from |g(|q) 1981He09 and |g|g(|q) in 1965An08. But J=2 from |g(|q) in 1970Ho25 is inconsistent 
$S{-p|g}=1.0 eV {I2} (1981He09). Others: 4.2 eV {I9} (1963Sp03), 1.3 eV {I3} (1965An08), 1.7 eV {I7} (1972Co13; renormlaized from 3.9 eV {I12}), 5.4 eV {I22} (1972Le29), 1.85 eV {I22} (1975Ob02) undivided between 9977.7 and 9978.2 doublet. 
$1963Sp03 also studied the decay scheme for this doublet without knowing the structure well at all. 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$E(p)=1155.1 {I6} (1972Co13), 1151 {I1} (1972Le29) 
J$from |g(|q) (1970Ho25) 
$S{-p|g}=0.7 eV {I2} (1972Co13; renormlaized from 1.5 eV {I5}), 0.66 eV {I8} (1975Ob02), 1.3 eV {I5} (1972Le29) 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$E(p)=1248.3 {I11}, unweighted average of 1251.4 {I6} (1972Co13), 1246.5 {I6} (1961An01), 1247.4 {I15} (1973Ve08), 1248 {I1} (1972Le29). Other: 1247 (1976Ve03). 
J$spin from |g(|q) 1973Ve08 and |g|g(|q) in 1965An08 
$S{-p|g}=1.27 eV {I16} (corrected value 1997Br07). Other: 4.9 eV {I15} (1972Co13; renormlaized from 11 eV {I3}), 4.6 eV {I6} (1975Ob02), 4.3 eV {I5} (1986Zi08), 5.2 eV {I11} (1973Ve08; renormlaized from 11.8 eV {I24}), 9.2 eV 37 (1972Le29), 2.0 eV {I4} (1965An08) 
$Corrected half-width 1.5 keV {I3} (1961An01) 
$|G{-|g}=0.86 eV {I11} (1986Zi08) 
$g.s. transition is considered one of the strongest M2 transitions known 


level_energy_unit: KEV
level_spin_parity: 4
level_comment:
E$E(p)=1278.5 {I10}, weighted average of 1278.2 {I10} (1997Br07), 1279.1 {I15} (1973Ve08) 
J$spin from |g(|q) in 1997Br07 
$S{-p|g}=0.11 eV {I2} (1973Ve08; renormlaized from 0.25 eV {I5}) 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$E(p)=1399.6 {I6}, weighted average of 1400.1 {I6} (1972Co13), 1399.3 {I8} (1973Ve08), 1400 {I1} (1974Vi02), 1398 {I1} (1972Le29). Other: 1396.5 {I7} (1961An01) is discrepant 
J$spin from |g(|q) in 1974Vi02 and 1973Ve08 
$S{-p|g}=0.6 eV {I2} (1972Co13; renormlaized from 1.3 eV {I4}), 0.7 eV {I2} (1975Ob02), 0.6 eV {I2} (1973Ve08; renormlaized from 1.3 eV {I3}), 1.8 eV {I7} (1972Le29) 
$Corrected half-width <0.30 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$E(p)=1402.3 {I6}, weighted average of 1402.9 {I6} (1972Co13), 1401.9 {I15} (1973Ve08), 1402 {I1} (1974Vi02), 1401 {I1} (1972Le29). Other: 1398.7 {I7} (1961An01) seems discrepant. 
J$spin from |g(|q) 1973Ve08 
$S{-p|g}=2.2 eV {I7} (1972Co13; renormlaized from 5.0 eV {I15}), 2.0 eV {I6} (1975Ob02), 1.7 eV {I4} (1973Ve08; renormlaized from 3.8 eV {I8}), 5.8 eV {I23} (1972Le29) 
$Corrected half-width <0.35 keV (1961An01) 


level_energy_unit: KEV
level_comment:
E$E(p)=1405.1 {I15} (1973Ve08). Other: 1404 (1972Le29) 
$S{-p|g}=0.11 eV {I5} (1973Ve08; renormlaized from 0.25 eV {I10}) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$E(p)=1410.6 {I6}, weighted average of 1411.4 {I6} (1972Co13), 1410.6 {I8} (1973Ve08), 1410 {I1} (1974Vi02), 1409 {I1} (1972Le29). 
J$spin from |g(|q) in 1973Ve08; parity from |g(|q,pol) in 1968Do14. 
$S{-p|g}=0.9 eV {I3} (1972Co13; renormlaized from 2.0 eV {I6}), 0.5 eV {I1} (1975Ob02), 0.4 eV {I1} (1973Ve08; renormlaized from 1.0 eV {I2}), 1.5 eV {I6} (1972Le29) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
E$E(p)=1437.3 {I}, weighted average of 1438.3 {I7} (1972Co13), 1436.3 {I7} (1961An01), 1437.3 {I15} (1973Ve08), 1437 {I1} (1972Le29). 
J$spin from |g(|q) in 1974Gr15, 1973Ve08 and 1972Co13 
$S{-p|g}=4.9 eV {I15} (1972Co13; renormlaized from 11 eV {I3}), 4.8 eV {I6} (1975Ob02), 3.7 eV {I8} (1973Ve08; renormlaized from 8.3 eV {I17}), 20 eV {I8} (1972Le29), 3.0 eV {I7} (1965An08) 
$Corrected half-width <0.20 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$E(p)=1468.5 {I7}, weighted average of 1468.6 {I7} (1961An01), 1469.0 {I15} (1973Ve08), 1468 {I1} (1972Le29). 
J$from |g|g(|q) in 1965An08 
$S{-p|g}=0.07 eV {I1} (1973Ve08; renormlaized from 0.15 eV {I3}), 0.5 eV {I2} (1965An08) 
$Corrected half-width <0.25 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$E(p)=1472.5 {I7}, weighted average of 1473.1 {I6} (1972Co13), 1472.1 {I15} (1973Ve08), 1471 {I1} (1972Le29). 
J$from |g(|q) 1973Ve08 
$S{-p|g}=1.1 eV {I3} (1972Co13; renormlaized from 2.4 eV {I7}), 1.2 eV {I2} (1975Ob02), 0.7 eV {I1} (1973Ve08; renormlaized from 1.5 eV {I3}), 2.4 eV {I10} (1972Le29) 


level_energy_unit: KEV
level_comment:
E$E(p)=1474.3 {I15} (1973Ve08), 1474 (1972Le29) 
$S{-p|g}=0.17 eV {I7} (1973Ve08; renormlaized from 0.38 eV {I15}) 


level_energy_unit: KEV
level_comment:
E$E(p)=1514.7 {I15} (1973Ve08) 
$S{-p|g}=0.8 eV {I2} (1975Ob02), 1.0 eV {I2} (1973Ve08; renormlaized from 2.2 eV {I5}) 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
E$E(p)=1555.5 {I7}, weighted average of 1556.6 {I6} (1972Co13), 1553.9 {I8} (1961An01), 1555.4 {I15} (1973Ve08), 1555 {I1} (1972Le29). 
J$spin from |g|g(|q) in 1965An08 
$S{-p|g}=4.0 eV {I12} (1972Co13; renormlaized from 9 eV {I3}), 4.2 eV {I5} (1975Ob02), 3.8 eV {I8} (1973Ve08; renormlaized from 8.7 eV {I18}), 11 eV {I5} (1972Le29), 2.3 eV {I5} (1965An08) 
$Corrected half-width<0.40 keV (1961An01) 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
E$E(p)=1582.4 {I6}, weighted average of 1582.9 {I6} (1972Co13), 1581.5 {I8} (1961An01), 1581.1 {I15} (1973Ve08), 1583 {I1} (1972Le29). 
J$spin from |g(|q) in 1974Gr15, 1973Ve08 and 1972Co13 
$S{-p|g}=3.5 eV {I11} (1972Co13; renormlaized from 2.4 eV {I7}), 4.6 eV {I6} (1975Ob02), 3.5 eV {I7} (1973Ve08; renormlaized from 7.9 eV {I16}), 15 eV {I6} (1972Le29), 2.5 eV {I6} (1965An08) 
$Corrected half-width <0.55 keV (1961An01) 


level_energy_unit: KEV
level_comment:
E$E(p)=1697.9, weighted average of 1696.9 {I10} (1997Br07), 1698.9 {I10} (1972Co13) 
$S{-p|g}=0.4 eV {I1} (1972Co13; renormlaized from 0.9 eV {I3}), 0.70 eV {I15} (1975Ob02) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$E(p)=1746.9 {I10} (1972Co13) 
$S{-p|g}=1.3 eV {I4} (1972Co13; renormlaized from 2.9 eV {I9}), possibly due to {+13}C(p,|g){+14}N contamination (1975Ob02), or {+23}Na(p,|g) (1997Br07). Level not observed in 1975Bo42. 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E$E(p)=1764.9 {I10}, weighted average of 1765.5 {I10} (1997Br07), 1764.2 {I10} (1972Co13) 
J$spin=5 from |g(|q) in 1997Br07, parity from rejecting L=5 as a result of strong centrifugal barrier. Other: 2+,(3-) from 1972Co13 based on 10571|g to 0+, 8342|g to 2+, 6114|g to 4+, 5151|g to 3+ and estimated strengths, however, 10571|g and 8342|g are not seen from this resonance by much more detailed study of 1997Br07. It is probably there are two different resonances around this energy. 
$S{-p|g}=0.4 eV {I1} (1972Co13; renormlaized from 0.9 eV {I3}) 


level_energy_unit: KEV
level_comment:
E$E(p)=1891.5 {I10} (1972Co13). Other: 1891 {I3} (1973Ko28) 
$S{-p|g}=1.0 eV {I3} (1972Co13; renormlaized from 2.2 eV {I7}); 14 eV (1965Sp05) is discrepant 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$E(p)=1953.9 {I10}, weighted average of 1953.7 {I10} (1997Br07) and 1954.0 {I10} (1972Co13). Other: 1952 (1973Ko28) 
J$from |g(|q) in 1997Br07 
$S{-p|g}=6.4 eV {I19} (1997Br07), 3 eV {I1} (1972Co13; renormlaized from 7 eV {I2}) 


level_energy_unit: KEV
level_comment:
E$E(p)=1976.6 {I10}, weighted average of 1976.6 {I10} (1997Br07), 1977.1 {I10} (1972Co13), 1975 {I2} (1973Ko28) 
$S{-p|g}=6.7 eV {I20} (1997Br07), 1.7 eV {I5} (1972Co13; renormlaized from 3.9 eV {I12}) 


level_energy_unit: KEV
level_comment:
E$E(p)=1981.7 {I10} (1997Br07). Others: 1983.6 {I10} (1972Co13) and 1981 (1973Ko28) could be the unresolved 1981.7+1982.5 doublet that is divided in 1997Br07 
$S{-p|g}=9.3 eV {I28} (1997Br07), 3.5 eV {I11} (1972Co13; renormlaized from 8 eV {I3}) 


level_energy_unit: KEV
level_comment:
E$E(p)=1990.2 {I10}, weighted average of 1989.5 {I10} (1997Br07) and 1990.9 {I10} (1972Co13). Other: 1989 (1973Ko28) 
$S{-p|g}=2.3 eV {I7} (1972Co13; renormlaized from 5.3 eV {I16}) 


level_energy_unit: KEV
level_comment:
E$E(p)=2026.6 {I10} (1972Co13). Others: 2023 (1970Fo13); 2023 {I2} (1973Ko28). Note that this resonance is considered as different from E(p)=2024.7 {I10} in 1997Br07 based on |g-decay patterns, also considering that 1970Fo13 report two resonances at E(p)=2020 and 2023, respectively, which are also seen by 1988Fa01 in (p,p):resonance 
$S{-p|g}=7 eV {I2} (1972Co13; renormlaized from 15 eV {I5}), 7 (1965Sp05) 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$E(p)=2136.5 {I10} (1997Br07). Other: 2133 (1970Fo13) 
J$from |g(|q) in 1997Br07 
$S{-p|g}=6.2 eV {I19} (1997Br07) 


level_energy_unit: KEV
level_spin_parity: 4
level_comment:
E$E(p)=2215.2 {I10} (1997Br07). Other: 2212 (1970Fo13) 
J$from |g(|q) 1997Br07, 
$1997Br07 reject negative parity based on the argument of B(M2)(W.u.)>RUL for 4344|g to 2+ transition, which however is not a valid argument since T{-1/2} is unknown and M2 is still likely for a T{-1/2}>10 fs. 
$S{-p|g}=5.4 {I16} (1997Br07) 


level_energy_unit: KEV
level_spin_parity: 3
level_comment:
E$E(p)=2300.2 {I10} (1997Br07). Other: 2301 (1970Fo13) 
J$from |g(|q) in 1997Br07 
$S{-p|g}=4.9 eV {I15} (1997Br07) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E$E(p)=2896.3 {I10} (1997Br07) 
J$spin=5 from |g(|q) 1997Br07; |p=- would require L=5 capture which is effectively suppressed by the centrifugal barrier (1997Br07). L=4 for |p=+ 
$S{-p|g}=6.1 {I18} (1997Br07) 


level_energy_unit: KEV
level_spin_parity: 5+
level_comment:
E$E(p)=2924.3 {I10} (1997Br07) 
J$spin=5 from |g(|q) 1997Br07; |p=- would require L=5 capture which is effectively suppressed by the centrifugal barrier (1997Br07). L=4 for |p=+ 
$S{-p|g}=2.5 {I8} (1997Br07) 


level_energy_unit: KEV
level_spin_parity: 2,3,4
level_comment:
E$E(p)=3282.8 {I10} (1997Br07). Other: 3283 {I3} (1973Ve06) 
J$spin=2,3,4 from |g(|q) 1973Ve06; 4- with l{-p}=3 from (p,p) elastic scattering (1973Ve06) 
$S{-p|g}=3.1 eV {I6} (1973Ve06; renormlaized from 7.0 eV {I14}) 
$|G=0.47 keV {I5} (1973Ve06) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$from 2006Tr03. Other: 12049 {I3} from E(p)=3289 {I3} (1973Ve06) 
J$from |g(|q) 1973Ve06; analog of 5073, 0+ level in {+32}P 
$S{-p|g}=1.1 eV {I2} (1973Ve06; renormlaized from 2.4 eV {I5}) 
$|G<0.17 keV (1973Ve06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_uncertain: S
level_comment:
$E(p)(c.m.)=159, |G{-|a}/|G=0.37 {I13}, |G{-|g}/|G=0.75 {I19} (1995Ro22), but the authors don't explain why the sum of |a and |g decay branches is greater 100%. In Adopted Levels, the evaluator has adopted %|a and %|g deduced from the ratio of |G{-|a}/|G and |G{-|g}/|G here. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_uncertain: ?
level_comment:
E$E(p)=355 (1963Ku24); E(p)(c.m.)=344 (1995Ro22). 
J$from 1995Ro22 
$|G{-|a}/|G|<0.05; |G{-|g}/|G=1.2 {I3} (1995Ro22) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E$E(p)=384 (1963Ku24); E(p)(c.m.)=371 (1995Ro22) 
J$from 1995Ro22 
$|G{-|a}/|G=1.00 {I8}; |G{-|g}/|G<0.15 (1995Ro22) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
E$E(p)=439 (1963Ku24); E(p)(c.m.)=425 (1995Ro22) 
J$from 1995Ro22 
$|G{-|a}/|G|<0.13; |G{-|g}/|G=1.03 {I26} (1995Ro22) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_comment:
E$E(p)=541 (1963Ku24); E(p)(c.m.)=524 (1995Ro22) 
J$from 1995Ro22 
$|G{-|a}/|G|<0.02; |G{-|g}/|G<0.05 (1995Ro22) 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=618.7 {I9} (1963Ku24); E(p)(c.m.)=600 (1995Ro22) 
S$other: 0.022 eV {I7} (2011Mo12) 
J,T$from 1963Ku24, spin from |s(|q) 
$A{-2}=+1.22 {I8}, A{-4}=+1.32 {I45} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$E(p)=641 (1963Ku24), 642 (1973Sh07) 
J$spin from |s(|q) in 1963Ku24 
T$from 1973Sh07 
S$from 2011Mo12. Other: 1.35 (1963Ku24) 
$A{-2}=+0.61 {I5} 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=1024 {I10} (1960Cl02), 1014 {I10} (1967Ri07), 1020 (1968Gu01) 
J$1- also from |s(|q) of (p,|a) in 1968Gu01 
T$others: |>3 keV (1960Cl02), 3 keV (1968Gu01) 
S$other: 26 eV (1960Cl02) 
$|G{-|a}=35 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E(p)=1161 {I10} (1960Cl02), 1158 (1968Gu01) 
T$from 1960Cl02. Other: 2 keV (1968Gu01) 
J$from |s(|q) of (p,|a) in 1968Gu01 
S$from 1960Cl02 
$|G{-|a}=3.1 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
E$E(p)=1247.4 {I15} (1973Ve08), 1250 {I3} (1988Fa01) 
J,T$from 1973Ve08 
$|G{-p}=1.50 keV {I15} (1988Fa01), 1.60 keV {I24} (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LE
level_comment:
E$E(p)=1399.3 {I8} (1973Ve08), 1403 {I3} (1988Fa01), 1403 {I6} (1967Ve05), 1404 {I10} (1960Cl02), 1400 {I10} (1967Ri07) 
J,T$from 1973Ve08 
$|G{-p}|<10 eV (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_comment:
E$E(p)=1401.9 {I15} (1973Ve08), 1403 {I3} (1988Fa01), 1403 {I6} (1967Ve05), 1404 {I10} (1960Cl02), 1400 {I10} (1967Ri07), 1404 (1968Gu01) 
J$2+,3- |s(|q) (1967Ve05); 2+,3- in 1968Gu01; 3- in 1988Fa01 
J,T$from 1973Ve08 
T$from 1973Ve08. Others: |<0.7 keV (1967Ve05), |?6 keV (1960Cl02), 1.5 keV (1968Gu01), 1.8 keV (1967Ri07) 
S$others: 33 eV (1960Cl02), 11 (1967Ri07) 
$|G{-p}=16 eV {I2} (1988Fa01), 16 eV {I6} (1973Ve08) 
$|G{-|a}=49 eV {I17} (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$E(p)=1405.1 {I15} (1973Ve08) 
J,T$from 1973Ve08, with J|p from analysis of |s(|q) and L(p,p)=1 from 1/2+ of {+31}P g.s. 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: EV
level_comment:
E$E(p)=1437.3 {15} (1973Ve08), 1438 {I3} (1988Fa01) 
J$from 1973Ve08 
$|G{-p}=35 eV {I4} (1988Fa01), 45 eV {I20} (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_comment:
E$E(p)=1469.0 {I15} (1973Ve08), 1470 {I6} (1967Ve05), 1468 (1968Gu01), 1468 {I7} (1966Ve10) 
J$spin from |s(|q) in 1967Ve05; 3- also in 1968Gu01. 
T$from 1973Ve08. Others: |<0.55 keV (1967Ve05), <=1 keV (1968Gu01) 
S$from 1967Ve05 
$|G{-p}=9 eV {I4}, |G{-|a}=170 eV {I60} (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=1474.3 {I15} (1973Ve08), 1476 {I6} (1967Ve05), 1474 {I10} (1960Cl02), 1466 {I10} (1967Ri07), 1475 (1968Gu01) 
J$from 1973Ve08. Other: J=2 also from 1967Ve05; 2+,3- from |s(|q) in 1968Gu01 
T$others: |<0.45 keV (1967Ve05), |<2.4 keV (1960Cl02), 1.5 keV (1968Gu01) 
S$from 1967Ve05. Others: 16 eV (1967Ri07), 8.5 eV (1960Cl02) 
$|G{-|a}=11.3 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
E$E(p)=1514.8 {I15} (1973Ve08), 1514 {I6} (1967Ve05), 1514 {I10} (1960Cl02), 1513 {I10} (1967Ri07), 1515 (1968Gu01), 1509 {I7} (1966Ve10) 
J$spin=1 from |s(|q) in 1967Ve05, L(p,p)=1 (1973Ve08) 
T$from 1967Ve05. Others: 7 keV {I2} (1960Cl02), 8 keV (1968Gu01), 8.3 keV (1967Ri07) 
S$from 1967Ve05. Others: 770 eV (1960Cl02), 690 (1967Ri07) 
$|G{-|a}=1.03 keV (1960Cl02), 3.8 keV {I6} (1973Ve08) 
$|G{-p}=3.8 keV {I6} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: EV
level_comment:
E$E(p)=1555.4 {I15} (1973Ve08), 1557 {I3} (1988Fa01) 
J,T$from 1973Ve08 
$|G{-p}=25 eV {I3} (1988Fa01), 30 eV {I10} (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: EV
level_comment:
E$E(p)=1581.1 {I15} (1973Ve08), 1583 {I3} (1988Fa01) 
J$from 1973Ve08 and 1988Fa01 
$|G{-p}=12 eV {I2} (1988Fa01), 25 eV {I+20-10} (1973Ve08) 


level_energy_unit: KEV
level_spin_parity: 0+,1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=1643 {I6} (1967Ve05), 1640 {I10} (1960Cl02), 1639 {I10} (1967Ri07), 1642 (1968Gu01), 1642 {I7} (1966Ve10) 
J$spin=0,1 from |s(|q) in 1967Ve05; 1- from 1968Gu01 
T$others: |<2.3 keV (1967Ve05), |?4.2 keV (1960Cl02), 6 keV (1968Gu01) 
S$from 1967Ve05. Others: 40 (1967Ri07), 58 eV (1960Cl02) 
$|G{-|a}=77 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=1715 {I6} (1967Ve05), 1710 {I10} (1960Cl02), 1715 {I10} (1967Ri07), 1715 (1968Gu01), 1713 {I7} (1966Ve10) 
J$spin from |s(|q) (1967Ve05) 
T$others: |<1.2 keV (1967Ve05), |<5.5 keV (1960Cl02), 2.5 keV (1968Gu01) 
S$from 1967Ve05. Others: 9 eV (1960Cl02); 26.5 eV from 1967Ri07 seems discrepant 
$|G{-|a}=12 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=1817 {I6} (1967Ve05), 1811 {I10} (1960Cl02), 1815 {I10} (1967Ri07), 1814 (1968Gu01), 1816 {I7} (1966Ve10) 
J$spin from |s(|q) (1967Ve05); 3- also from |s(|q) of (p,|a) in 1968Gu01 
T$others: |<1.6 keV (1967Ve05), |?4.7 keV (1960Cl02), 3 keV (1968Gu01) 
S$from 1967Ve05. Others: 26 eV (1960Cl02), 16 (1967Ri07) 
$|G{-|a}=35 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$E(p)=1896 {I6} (1967Ve05), 1892 {I10} (1960Cl02), 1891 {I10} (1967Ri07), 1892 (1968Gu01), 1893 {I7} (1966Ve10) 
J$spin from |s(|q) in 1967Ve05; 1- in 1968Gu01; 2+,1- in 1967Ri07 
T$weighted average of 24 keV {I3} (1967Ve05) and 27 keV {I2} (1960Cl02). Others: 24 keV (1968Gu01), 20 keV (1967Ri07) 
S$others: 730 eV (1960Cl02); 1750 eV {I250} (1967Ve05) seems discrepant 
$|G{-|a}=970 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 2+,(1-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=1976 {I10} (1960Cl02), 1971 {I10} (1967Ri07), 1976 (1968Gu01) 
T$other: |<2.8 keV (1960Cl02) 
S$other: 17 eV (1960Cl02) 
$|G{-|a}=23 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E$E(p)=1989 {I3} (1988Fa01), 1990 {I10} (1960Cl02), 1985 {I10} (1967Ri07), 1983 (1968Gu01) 
T$others: |<3.6 keV (1960Cl02), 5 keV (1968Gu01) 
J$other: 2+ from 1988Fa01 is in disagreement 
S$other: 30 eV (1960Cl02) 
$|G{-p}=80 eV {I8} (1988Fa01), |G{-|a}=40 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E(p)=2022 {I3} (1988Fa01), 2018 {I10} (1960Cl02), 2004 {I10} (1967Ri07), 2018 (1968Gu01) 
T$other: |<3 keV (1960Cl02), 4 keV (1968Gu01) 
J$1- also from |s(|q) of (p,|a) in 1968Gu01 
S$other: 23 eV (1960Cl02) 
$|G{-p}=19 keV {I4} (1988Fa01), |G{-|a}=31 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=2023 {I3} (1988Fa01), 2020 (1968Gu01), 2011 {I10} (1967Ri07) 
J,T$from |s(|q) of (p,|a) in 1968Gu01, but 2+ from 1988Fa01; 1- and |G|?4 keV from 1967Ri07 
$|G{-p}=0.17 keV {I2} (1988Fa01) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$E(p)=2029 {I10} (1960Cl02), 2015 {I10} (1967Ri07) 
T$from 1960Cl02. Other: |?4 keV (1967Ri07), 18 keV {I2} (1960Cl02) 
S$from 1960Cl02 
$|G{-|a}=0.6 keV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 2+,(3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E(p)=2031 {I10} (1960Cl02), 2019 {I10} (1967Ri07) 
T$other: |?6 keV (1960Cl02) 
S$other: 120 eV (1960Cl02) 
$|G{-|a}=160 eV (1960Cl02) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E(p)=2041 {I10} (1960Cl02), 2027 {I10} (1967Ri07) 
T$other: |?6 keV (1960Cl02) 
S$from 1960Cl02 
$|G{-|a}=27 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=2109 {I10} (1960Cl02), 2115 {I10} (1967Ri07) 
T$other: |<4 keV (1960Cl02) 
S$other: 1.3 eV (1960Cl02) 
$|G{-|a}=1.7 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$E(p)=2434 {I10} (1960Cl02), 2448 {I10} (1967Ri07) 
T$from 1960Cl02. Other: 9 keV (1967Ri07) 
S$other: 407 eV (1960Cl02) 
$|G{-|a}=540 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E(p)=2644 {I10} (1960Cl02), 2662 {I10} (1967Ri07) 
T$other: |?5 keV (1960Cl02) 
S$other: 23 eV (1960Cl02) 
$|G{-|a}=31 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: (0+,1-)
level_lifetime_unit: KEV
level_comment:
E$E(p)=2779 {I10} (1960Cl02), 2808 {I10} (1967Ri07) 
T$from 1960Cl02. Other: 6.1 keV (1967Ri07) 
S$other: 120 eV (1960Cl02) 
$|G{-|a}=160 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$E(p)=2805 {I10} (1960Cl02), 2831 {I10} (1967Ri07) 
T$from 1960Cl02. Other: 10.7 keV (1967Ri07) 
S$other: 136 eV (1960Cl02) 
$|G{-|a}=180 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$E(p)=2874 {I10} (1960Cl02), 2907 {I10} (1967Ri07) 
T$other: |?5 keV (1960Cl02) 
S$other: 22 eV (1960Cl02) 
$|G{-|a}=29 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: KEV
level_comment:
E$E(p)=2922 {I10} (1960Cl02), 2950 {I10} (1967Ri07) 
T$from 1960Cl02. Other: 8.0 keV (1967Ri07) 
S$other: 273 eV (1960Cl02) 
$|G{-|a}=360 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 2+,(1-)
level_lifetime_unit: KEV
level_comment:
E$E(p)=3008 {I10} (1960Cl02), 3040 {I10} (1967Ri07) 
T$from 1960Cl02. Other: 30 keV (1967Ri07) 
S$other: 1370 eV (1960Cl02) 
$|G{-|a}=1830 eV (1960Cl02) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$E(p)=3119 {I10} (1960Cl02), 3119 (1967Ri07), 3148 {I10} (1967Ri07) 
T$from 1960Cl02. Other: 7.6 keV (1967Ri07) 
S$other: 156 eV (1960Cl02) 
$|G{-|a}=208 eV (1960Cl02) 


level_energy_unit: KEV
level_comment:
L$1 from 1976Uz01 disagrees with 3 from 1987Mi11 
S$0.02 for L=1 (1976Uz01), 0.21 for L=3 (1987Mi11) 


level_energy_unit: KEV
level_comment:
L$1 from 1976Uz01 disagrees with 3 from 1987Mi11 
S$0.07 for L=1 (1976Uz01), 0.31 for L=3 (1987Mi11) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from DSAM in 1980Ba40, |t=236 fs {I16}. Others: |t=230 ps {I60} (1971Ga01), 236 fs {I18} (1988Si14) 
$g-factor=+0.47 {I9} (1979Za01), using IMPAC technique and a lifetime value of 230 fs {I16} 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$spin=4 from |a-2228|g(|q) and J(2230)=2, with 2228|g the sum of 4458 to 2230 and 2230 to g.s. transitions (1969Ga04) 
T$from |t=0.198 fs {I29}, weighted average of 0.207 fs {I29} from DSAM in 1988Si14 and 0.18 ps {I4} in 1971Ga01. The value from 1971Ga01 is obtained by combining value measured by 1971Ga01 and reanalysis of their earlier measurement in 1969Ga04. 
$g-factor=+0.40 {I15} (1988Si14), using transient field technique and a known g-factor=0.50 {I3} for 2230 level. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$not reported in 1972Ma36, but 1976Pe05 claim that this level was wrongly identified as 4700 level by 1972Ma36 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$weighted average of 1.01 ps {I26} (1973Ca18) and 0.87 ps {I7} (2017Pe14) 
T$|t=1.46 fs {I37} (1973Ca18), 1.260 fs {I91} (2017Pe14) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$unweighted average of 44 fs {I26} (1973Ca18) and 98 fs {I11} (2017Pe14) 
T$|t=64 fs {I18} (1973Ca18), 142 fs {I15} (2017Pe14) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$unweighted average of 46 fs {I12} (1973Ca18) and 45 fs {I6} (2017Pe14) 
T$|t=66 fs {I17} (1973Ca18), 65 fs {I9} (2017Pe14) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$spin=1 from n|g(|q) in 1972Ga43 
T$from DSAM in 1972Ga43. Other: <7fs (1973Ca18) 
T$|t<10 fs (1973Ca18) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_comment:
$|G=0.0031 eV {I5} 
T$weighted average of 147 fs {I24} (2002Ba28), 229 fs {I56}, and 187 fs {I63} (1964Bo22) 
T$|t=212 FS 35 (2002Ba28), 330 FS 80 (1964Ma01), 270 FS 90 (1964Bo22) 


level_energy_unit: KEV
level_spin_parity: 2
level_lifetime_unit: FS
level_comment:
$|G=0.0144 eV {I22} 
$|G{-|g0}=0.0124 eV {I21}, |G{-|g1}=0.00198 eV {I51} 
T$|t=45.7 FS 69 (2002Ba28) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
$|G=0.0483 eV {I80} 
$|G{-|g0}=0.0379 eV {I73}, |G{-|g1}=0.0104 eV {I33} 
T$|t=13.6 FS 23 (2002Ba28) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
$|G=3.52 eV {I52} 
$|G{-|g0}=3.044 eV {I508}, |G{-|g1}=0.480 eV {I114}; |G{-|g0}=2.6 eV {I3} (1984Be26) 
T$|t=0.19 FS 3 (2002Ba28) 
J$from 1984Be26 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_comment:
$|G=0.351 eV {I64} 
$|G{-|g0}=0.231 eV {I50}, |G{-|g1}=0.115 eV {I40}; |G{-|a}=0.0054 eV from {+28}Si(|a,|g) 
T$|t=1.87 FS 35 (2002Ba28) 
T$includes |G{-|a}=0.0054 eV from {+28}Si(|a,|g) (2002Ba28) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
$|G=0.109 eV {I36} 
$|G{-|g0}=0.043 eV {I13}, |G{-|g1}=0.066 eV {I33}; |G{-|g0}=0.36 eV {I11} from 1984Be26 is inconsistent 
T$|t=6.1 FS 20 (2002Ba28) 
J$from 1984Be26 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$spin=2 from p|g(|q) in 1966Po01 and 1982Go13 
T$weighted average of 55 fs {I7} (1971In02) and 51 fs {I4} (1970Ol01) 
T$|t=80 FS 10 (1971In02), 74 FS 6 (1970Ol01) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$spin=1 from p|g(|q) in 1966Po01 and 1982Go13 
T$weighted average of 0.28 ps {I7} (1971In02) and 0.34 ps {I6} (1970Ol01) 
T$|t=0.4 PS 1 (1971In02), 0.49 PS 9 (1970Ol01) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1966Po01 
J$spin=3 from p|g(|q) in 1966Po01 
T$from 1970Ol01 
T$|t=0.19 PS 2 (1970Ol01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1966Po01 
J$spin=1 from p|g(|q) in 1966Po01 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from DSAM in 1977Sc36, |t=240 ps {I27}. Other: |t=242 fs {I11} deduced by 1977Sc36 from their measured B(E2)|^ extracted from |g-ray yield; |t=258 fs {I8} from DSAM in 2006Sp01, but the uncertainty of about 3% is considered too small for DSAM and likely doesn't include the systematic uncertainty from stopping power theory which could be 10-20%; |t=250 fs {I12} from the average B(E2)|^=0.0298 {I6} below 
$Static quadrupole moment Q=-0.160 {I22} (1982Ve09,constructive), -0.18 {I4} (1981Da08), -0.15 {I10} (1980Ba40), -0.175 {I5} (1971Ha47), -0.20 {I6} (1970Na05), <0.25 (1970Ha24). Other: -0.133 {I22} (1982Ve09,destructive); -0.066 {I17} from 1974Ol02 is discrepant with all other studies. -0.16 {I2} from 2021StZZ compilation, which has adopted the value from 1982Ve09 
$1974Ol04 attribute the discrepancy in Q to the smaller internucleon separation distances involved in previous studies 
$B(E2)|^=0.0297 {I13}, weighted average of 0.0292 {I17} (1982Ve09,constructive), 0.0334 {I70} (1980Ba40), 0.0300 {I13} (1977Sc36), 0.0305 {I16} (1974Ol02), 0.0284 {I20} (1971Ha47), all determined from |g-ray or {+32}S yield. Other: 0.0307 {I17} (1982Ve09,destructive). 
$B(E2)|^=0.0298 {I6} from average lifetime in 2006Sp01; 0.0090 in 1989Al14 is likely in error 
$g-factor=+0.44 {I10} (2006Sp01), using transient-field technique 
$Deformation parameters |b{-2}(Coulomb)=0.29, |b{-2}(nucleon)=0.27 (1989Al14) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$B(E3)|^=0.0070 {I5} (1991Al19) 
$Deformation parameters |b{-3}(Coulomb)=0.39 {I1}, |b{-3}(nucleon)=0.39 {I1} (1991Al19) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$spin from microwave absorption (1948To13, 1952Es07) and NMR (1953We51); L(pol d,t)=2 from 0+ and L-1/2 transfer from analyzing powers. 
MOMM1$evaluated value from 2019StZV based on measured value of 0.6432574 {I107} using nuclear magnetic resonance (NMR) in 2005An15, with more accurately estimated shielding constant than old values as claimed by the authors. Others: +0.6438212 {I14} (1973Lu06), +0.64348 {I9} (1953We51), +0.634 {I10} (1952Es07), +0.64292 {I14} (1951Dh01), all using NMR. 
MOME2$as adopted in 2021StZZ and 2018Py01 evaluations, which is the revised value of -0.0678 {I13} calculated by 1990Su19 using multi-configurational Hartree-Fock (MCHF) calculations and measured hyperfine structure data in 1989Tr06. This revision was made by 2014St28, by using the coupled-cluster theory and accurate values of sulfur quadrupole couplings of Cs and SiS from the analysis of rotational spectra data in 2007Mu22 and 2005Mu32. Others: -0.084 {I8} (collinear laser spectroscopy, 1986El09), -0.064 {I10} (microwave spectroscopy, 1954Bi40), -0.056 (1962Ko22, value of 1954Bi40 reanalyzed), -0.06 (1953Bu92), -0.050 (1953De16), -0.05 {+5-3} (1948To13). Theory: -0.0663 {I2} (Hartree-Fock-density functional, 2000Ba85). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J$L(d,t)=L(d,p)=L(p,d)=L({+3}He,|a)=0 from 0+; also from |g(circ pol) in (n,|g) E=thermal. 
T$from |t=1.69 ps {I10}, weighted average of 2.0 ps {I3} (1973Wa10) and 1.69 ps {I10} (1977He12) in ({+32}S,p|g), 1.66 ps {I34} (1969Ra29), 1.81 ps {I36} and 1.65 ps {I33} (1969Br28, different stopping materials), and 1.70 ps {I45} (1973Ca20) in (|a,n|g), 1.73 ps {I+110-45} (1969Va28) and 0.9 ps {I+5-4} (1970Cu01) in (d,p|g), 1.69 ps {I18} (1977Sc36) in Coulomb excitation, all by DSAM. 
BE2$from Coulomb excitation (1961An09) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,t)=2 and L+1/2 transfer from analyzing powers. 
T$from |t=136 ps {I20}, weighted average of 125 fs {I37} (1969Br28), 182 fs {I22} (1969Ra29), 90 fs {I20} (1970Ka08), and 189 fs {I50} (1973Ca20) in (|a,n|g), 150 fs {I45} (1969Va28) and 150 fs {I30} (1970Cu01) in (d,p|g), and 80 fs {I60} (1977Sc36) in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,t)=2 and L-1/2 transfer from analyzing powers; spin=3/2 also from |g|g(|q) in (n,|g) E=thermal. 
T$from |t=169 fs {I25}, weighted average of 202 fs {I26} (1977He12) in ({+32}S,p|g), 178 fs {I53} (1969Br28), 183 fs {I25} (1969Ra29), 145 fs {I25} (1970Ka08), and 198 fs {I50} (1973Ca20) in (|a,n|g), and 140 fs {I30} (1969Va28) and 140 fs {I40} (1970Cu01) in (d,p|g). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,t)=2 and L+1/2 transfer from analyzing powers; also from |g(|q,pol) in (|a,n|g). 
T$from |t=17 fs {I6}, weighted average of 33 fs {I13} (1969Br28) and 34 fs {I14} (1973Ca20) in (|a,n|g), 13 fs {I5} (1969Va28) in (d,p|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in (|a,n|g); also L(d,p)=L(p,d)=L({+3}He,|a)=3 from 0+. 
T$from |t=40.9 ps {I20}, weighted average of 38 ps {I11} (1969Br20), 36 ps {I8} (1970Ka08), 40.5 ps {I20} (1970Ra24, RDM), 44 ps {I4} (1971Br23, RDM) in (|a,n|g). Other: >5 ps from (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q,pol) in (|a,n|g). Other: (3/2) from a fit to |s(|q) in (d,|a) for a level at 2969 {I8} by 1969Bo30 is in disagreement; L({+3}He,p)=(3) from 1/2+ suggests |p=(-) for a group at 2974 {I12} 
T$from |t=85 fs {I12}, weighted average of 90 fs {I31} (1969Br28), 82 fs {I12} (1969Ra29), 94 fs {I24} (1973Ca20) in (|a,n|g), 86 fs {I25} (1969Va28) in (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$from |g(circular pol) in (n,|g) E=thermal and |g(|q) in (d,p|g); also L(d,p)=L(p,d)=L({+3}He,|a)=1 from 0+ 
T$from |t=38 fs {I7}, weighted average of 48 fs {I18} (1973Ca20) in (|a,n|g), 43 fs {I7} (1989Ko53) in (n,|g) E=thermal, 28 fs {I9} (1969Va28) and 40 fs {I+20-10} (1970Cu01) in (d,p|g). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$tentatively proposed in ({+12}C,|apn|g) (2014Bi16) based on |g|g(|q)(DCO), |g|g(lin pol), and comparisons with shell-model calculations. Other: (9/2+) proposed in ({+18}O,X|g) (2009Ch43) based on qualitative |g|g(lin pol) results. 2014Bi16 point out that for J|p(3780)=(9/2+) proposed by 2009Ch43, the experimental and calculated excitation energies show large differences while they match reasonably well for J|p(3780)=(5/2+). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,t)=2 and L+1/2 transfer from analyzing powers; spin=5/2 also from |g(|q) and |g|g(|q) in (|a,n|g) 
T$from |t=44 fs {I12} (1973Ca20) in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$spin=3/2,5/2 from |g(|q) in (|a,n|g) and |g|g(|q) in (d,p|g); 1209|g to 7/2- and 3303|g to 1/2+ cannot be pure M2 (|DJ=2) based on RUL; 3/2- is ruled out since it would require a large B(M2)(W.u.) for 4144|g exceeding RUL=3 based on |d(Q/D) values for J=3/2 from (|a,n|g) and (d,p|g). Other: L({+3}He,p)=(1) from 1/2+ giving parity=(-) for a group at 4151 {I12} is inconsistent 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$spin=3/2 from |g|g(|q) in (n,|g) E=thermal; L(d,p)=1 from 0+ 
T$weighted average of 32 fs {I9} (1973Ca20) from (|a,n|g) and 17 fs {I8} (1989Ko53) from (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2
level_lifetime_unit: FS
level_comment:
J$spin=1/2,3/2 from |g(|q) in (|a,n|g); 1/2- is excluded based on |d solution for J|p=1/2- which would require M2,E3 or M3 strengths exceeding RUL 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$5/2-,9/2- from |g(|q,lin) in (|a,n|g); 5/2- ruled out based on |g(|q) (1975Bu15) in (|a,n|g) giving an |d(M2/E1)>+5.6 for 1761|g which would require a large B(M2)(W.u.) greatly exceeding RUL. 
T$from |t=110 fs {I29}, weighted average of 82 fs {I21} (1973Ca20) in (|a,n|g), 130 fs {I40} (2017Ay04) in ({+14}N,|ap|g), and 190 fs {I40} (2014Bi16) in ({+12}C,|apn|g). 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,n|g). 
J$allowed |b-decay from 3/2+ parent, log| {Ift}=5.4. L(d,p)=(0) for a composite structure suggests (1/2+). 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
J$tentatively proposed in ({+12}C,|apn|g) based on |g|g(|q)(DCO) and |g|g(lin pol) of 1015.3|g M1(+E2) to 3780, (5/2+) level. See also comments for J|p(3780). Other: (11/2-) proposed in ({+18}O,X|g) based on qualitative |g|g(lin pol) result of 1015.3|g which suggests Mult(1015.3|g)=(E1). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
J$from |g(|q,pol) in (|a,n|g). But L(pol d,t)=(2) from 0+ for a group at 4868 {I20} (with T=1/2) suggests (3/2+,5/2+), which may indicate a different level 
T$from |t=328 fs {I50}, weighted average of 400 ps {I100} from ({+14}N,|ap|g), 300 ps {I50} from ({+12}C,|apn|g), and 360 ps {I90} from (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,n|g). Others: 4941 {I6} from (d,p); 4945 {I3} from (p,d) 
J$L(d,p)=L(p,d)=3 from 0+. Other: L({+3}He,p)=(1) from 1/2+ suggests (1/2-,3/2-,5/2-) for a group at 4932 {I12} 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_comment:
E$weighted average of 5177 {I6} from (d,p), 5179 {I4} from (p,d), and 5176 {I20} from ({+3}He,|a) 
J$L({+3}He,|a)=(3) from 0+; L(p,d)=(3,4) from 0+. 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$others: 5209 from (|a,n|g), 5210 {I6} from (d,p) 
J$5208.5|g to 3/2+, with Mult=M2 ruled out by RUL 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$others: 5276 {I6} from (d,p), 5273 {I4} from (p,d). This level is considered tentative in (n,|g) E=thermal due to the tentative placement of 5269.8|g by 1985Ke08 
J$possible 5269.8|g to 3/2+ 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2+)
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,n|g). 
J$5282|g to 3/2+, with Mult=M2 ruled out by RUL. Other: L({+3}He,|a)=(2) from 0+ for a group at 5285 {I20}, likely a doublet of 5282+5286 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 5340 {I6} from (d,p) and 5343 {I4} in (p,d). Note that a 5351 {I6} level is also reported in (d,p) but no similar level is reported in (p,d). It also could be possible that the 5343 {I4} level in (p,d) is a doublet of 5340+5351 in (d,p) 
J$L(p,d)=2 from 0+. 


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 (n,|g) E=thermal. Other: 5351 {I6} from (d,p) 
J$430.3|g to 1/2-, 1413.9|g to 3/2+ 


level_energy_unit: KEV
level_comment:
E$weighted average of 5414 {I15} from ({+3}He,p), 5399 {I6} from (d,p), 5401 {I4} from (p,d), and 5391 {I20} from ({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J$L(d,p)=(0) from 0+. L(p,d)=0 for a group at 5617 {I14} and L({+3}He,|a)=0 for a group at E=5620 {II15}, both likely a triplet of 5597+5613+5622 in (d,p). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$spin=1/2 from |g|g(|q) in (n,|g) E=thermal; L(d,p)=L({+6}Li,d)=1 from 0+. Other: L({+3}He,p)=1 from 1/2+ for a group at E=5725 {I12} gives (1/2,3/2,5/2)- 


level_energy_unit: KEV
level_comment:
E$from (d,p). Other: 5882 {I15} from ({+3}He,p) could be a doublet of 5864+5888; 1985Ke08 in (n,|g) E=thermal tentatively place a 2775.65|g from 8642 level, making a tentative final level of 5866, but this |g is not confirmed in other studies. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$weighted average of 5911 {I12} from ({+3}He,p), 5915 {I6} from (d,p), and 5916 {I4} from (p,d) 
J$L(p,d)=0 from 0+. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from ({+3}He,p|g). Others: 6079 {I6}, tentative in (d,p) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 6326 {I6} from (d,p) and 6330 {I12} from (d,t). 
J$L(pol d,t)=2 an L+1/2 from analyzing powers 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 6360 {I6} from (d,p) and 6362 {I4} from (p,d). Other: 6361 {I20} from ({+3}He,|a) 
J$L(p,d)=L({+3}He,|a)=2 from 0+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2:7/2)(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from ({+3}He,p|g). Other: 6372 {I6} from (d,p) could be the same level; 6376 {I12} from ({+3}He,p) could be a doublet of 6360+6372 in (d,p) 
J$L({+3}He,p)=(2) from 1/2+ suggests (1/2 to 7/2)(+) for a group at 6376 {I12}; 6380|g to 3/2+ 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (d,p). Other: 6486.6 from a tentative placement of 6485.93|g in (n,|g) E=thermal 
J$L(d,p)=(0). 


level_energy_unit: KEV
level_spin_parity: (11/2)-
level_lifetime_unit: PS
level_comment:
J$1795.0|g M1+E2, |DJ=1 to 9/2-, assuming spin ascends as excitation energy rises in fusion-evaporation reaction ({+14}N,|ap|g) 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (d,p). Other: 6708.29 from a tentative placement of 6707.56|g in (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
E$from (d,p); not seen in (p,d). 
J$L(pol d,t)=2 and L-1/2 from analyzing powers for a group at 6852 {I34} with T=3/2, which could be a doublet of 6892+6903 in (d,p). 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
E$weighted average of 6903 {I6} from (d,p) and 6905 {I4} from (p,d) 
J$L(p,d)=2 from 0+; L(pol d,t)=2 and L-1/2 from analyzing powers for a group at 6852 {I34}, which could be a doublet of 6892+6903 in (d,p). 
ISPIN$from (pol d,t) and ({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 6965 {I6} from (d,p) and 6967 {I4} from (p,d). Others: 6977 {I12} from ({+3}He,p); 6958.87 from a tentative placement of 6958.08|g in (n,|g) E=thermal 
J$L({+3}He,p)=2 from 1/2+. 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
J$1278.2|g M1+E2, |DJ=1 to 9/2+; 2133.2|g D, |DJ=1 to 11/2- 
T$other: >0.7 ps from ({+13}C,2n|g|g) is discrepant 


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$from (n,|g) E=thermal. Other: 7017 {I6} from (d,p) 
J$a possible weak primary 1624.9|g from 1/2+ capture state in (n,|g) E=thermal 


level_energy_unit: KEV
level_comment:
E$weighted average of 7038 {I5} from (p,d) and 7037 {I6} from (d,p). Other: 7052 {I15} from ({+3}He,p) 


level_energy_unit: KEV
level_comment:
J$L({+3}He,p)=(2) from 1/2+ gives (1/2 to 7/2)(+) for a group at 7153 {I15}, which could be a doublet of 7133+7164 in (d,p) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: FS
level_comment:
J$2450.9|g E2, |DJ=2 to 9/2-; 2313.7|g M1+E2 to 11/2-. Other: 11/2+ from ({+12}C,|apn|g) is in disagreement. 
T$other: <55 fs from ({+12}C,|apn|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$others: 7190 {I6} from (d,p), 7193 {I5} from (p,d), 7206 {I15} from ({+3}He,p) 
J$spin=3/2 from |g|g(|q) in (n,|g) E=thermal; L(d,p)=1 from 0+. 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E$from (p,d). 
J$L(p,d)=2 from 0+; L(pol d,t)=2 and L+1/2 from analyzing powers for a group at 7330 {I30} with T=3/2, which could be a doublet of 7330+7339. 


level_energy_unit: KEV
level_comment:
E$from (d,p) 
J$L({+3}He,|a)=(3) from 0+ gives (5/2-,7/2-) for a group at 7348 {I20}, which could be a doublet of 7353+7359 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_comment:
E$other: 7413 {I6} from (d,p) 
J$1/2,3/2 from |g|g(|q) with 1/2 preferred and also strong primary 1225.7|g from 1/2+ capture state in (n,|g) (E=thermal). 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
E$others: 7482 {I6} from (d,p), 7498 {I15} from ({+3}He,p) 
J$weak primary 1153.2|g from 1/2+ capture state in (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
E$others: 7503 {I6} from (d,p), 7521 {I15} from ({+3}He,p) 
J$primary 1135.3|g from 1/2+ capture state in (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$this level may be the same as 7615.7 in (n,|g) E=thermal by energy, however, J|p=5/2-,7/2- implied from L(d,p)=3 and J|p=(1/2,3/5,5/2+) implied from primary |g transition indicates two different levels. 
J$L(d,p)=3 from 0+. 


level_energy_unit: KEV
level_comment:
J$L({+3}He,p)=0 from 1/2+ gives (1/2+,3/2+) for a group at 7909 {I12} which is probably a doublet of 7892+7906 in (d,p) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res. Other: 8329 {I12} from ({+3}He,p) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g),(n,n):resonances. Other: 8670 {I10} from (d,p), 8672 from (n,|g) E=res 
J$L(d,p)=1 from 0+ gives 1/2-,3/2-; 1/2- is ruled out since 6703|g and 5803|g to 5/2+ cannot be M2 based on RUL. Other: 1/2- from R-matrix analysis in (n,|g),(n,n):resonances is in disagreement 
$|G=32.9 eV {I5} from |G{-n}=31.8 eV {I5}, |G{-g}=1.12 eV {I6} in (n,|g),(n,n):resonances 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g):resonances. Other: 8685 from (n,|g) E=res 
J$2973|g to 1/2- and 7842|g to 1/2+ cannot be M2 based on RUL; L=2 from 0+ gives 3/2+,5/2+ in (n,|g),(n,n):resonances 
$|G{-n}=2.0 eV {I4}/(2J+1)=0.50 eV {I10} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$(n,|g):resonances. Others: 8752 {I3} from (d,p); 8745 from (n,|g) E=res deduced from measured E{-R}=103 keV with no uncertainty 
J$also L(d,p)=0 from 0+ 
$|G=15.0 keV {I1} from |G{-n}=30.0 {I2}/(2J+1) keV, |G{-|g}=4.29 eV {I32} in (n,|g):resonances 
$|G=20 keV {I3} from (d,p), based on re-analysis by 1976Bo18 of (n,|g):resonances data in 1950Ba88, and comparison with corresponding measured (d,p) cross sections by 1976Bo18. 


level_energy_unit: KEV
level_comment:
J$L(pol d,t)=2 and L+1/2 from analyzing powers gives 5/2+ for a group at 8794 {I22} with T=3/2, which could be a doublet of 8782.3+8809.1 levels 
$|G{-n}<6/(2J+1) eV 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$L=1 from 0+ in (n,|g),(n,n):resonances 
$|G=10.5 eV {I5} if J=1/2, 5.3 eV {I3} if J=3/2 from |G{-n}=18.8 {I10}/(2J+1) eV, |G{-|g}=2.28 {I16}/(2J+1) eV. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g):resonances. Other: 8838 {I10} from (d,p), 8845 from (n,|g) E=res 
J$from R-matrix analysis in (n,|g),(n,n):resonances and analysis of resonance data in (n,|g) E=res. Other: L(d,p)=1 from analysis of neutron resonance data (1976Bo18) 
$|G=3.120 keV {I12} from |G{-n}=6.240 {I24}/(2J+1) keV, |G{-|g}=0.65 eV {I7} in (n,|g),(n,n):resonances 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$from (n,|g):resonances. Other: 8910 {I2} from (d,p) 
J$also L(d,p)=1 from 0+ 
$|G=1.63 keV {I1} from |G{-n}=3.256 keV {I18}/(2J+1) keV, |G{-|g}=4.53 eV {I33} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$from (n,|g):resonances. Other: 8926 {I2} from (d,p) 
J$also L(d,p)=1 from 0+ 
$|G=1.144 eV {I4} from |G{-n}=4.568 {I16}/(2J+1) keV, |G{-|g}=2.03 eV {I17} 


level_energy_unit: KEV
level_comment:
E$from (n,|g):resonances. Other: 8939 {I10} from (d,p) 
$|G<6.1 eV from |G{-n}=8 {I2}/(2J+1) eV, |G{-|g}=4.26 {I34}/(2J+1) eV, and J|>1/2. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g),(n,n):resonances. Other: 9010 {I10} from (d,p), 9010 from (|a,|g):res 
J$also L(d,p)=0 from 0+. 1/2+ also from (|a,|g):res 
$|G=7.971 keV {I14} from |G{-n}=15.938 {I28}/(2J+1) keV, |G{-|g}=2.43 eV {I61}. Other: 13 keV {I3} (1976Bo18) from re-analysis of (n,|g):resonances data in 1950Ba88, and comparison with corresponding measured (d,p) cross sections by 1976Bo18 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$from (n,|g):resonances. Other: 9035 {I10} from (d,p) 
J$L(d,p)=2 from 0+ 
$|G=7.8 eV {I5} if J=3/2, 5.2 eV {I3} if J=5/2 from |G{-n}=27.2 {I20}/(2J+1) eV, |G{-|g}=3.86 {I30}/(2J+1) eV. 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$from (n,|g):resonances. Other: 9138 {I10} from (d,p) 
J$L(d,p)=2 from 0+. 
$|G{-n}<53.2 {I38}/(2J+1) eV 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g):resonances. Others: 9211 {I2} from (d,p), 9200 from (|a,|g):res 
J$also L(d,p)=2 from 0+ 
$|G=1.285 keV {I61} from |G{-n}=7.710 {I36}/(2J+1) keV, |G{-|g}=1.03 eV {I10} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from Breit-Wigner analysis in (n,|g) (resonance). 
$|G=32.0 eV {I16} from |G{-n}=124.8 {I64}/(2J+1) eV, |G{-|g}=0.78 eV {I9} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from Breit-Wigner analysis in (n,|g) (resonance). 
$|G=416 eV {I8} from |G{-n}=1660 {I32}/(2J+1) eV, |G{-|g}=0.67 eV {I20} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$from (n,|g):resonances. Others: 9318 {I3} from (d,p) 
J$also L(d,p)=0 from 0+ 
T$from |G{-n}=22.558 {I176}/(2J+1) keV, |G{-|g}=2.23 eV {I11}. Other: 10 keV {I3} (1976Bo18) from re-analysis of (n,|g):resonances data in 1950Ba88, and comparison with corresponding measured (d,p) cross sections by 1976Bo18 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g):resonances. Others: 9345 from (|a,|g):res 
$|G=3.78 keV {I5} from |G{-n}=7.558 {I98}/(2J+1) keV, |G{-|g}=1.00 eV {I33} 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_comment:
E$it could be the same level as 9345.4 in (n,|g),(n,n):resonances based on energy agreement, but their J|p assignments are in disagreement 
J$L(d,p)=3 from 0+ 


level_energy_unit: KEV
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (n,|g):resonances. Others: 9352 from (|a,|g):res 
$|G{-n}<48/(2J+1) eV 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$from (n,|g):resonances. 
$|G=1.257 keV {I16} from |G{-n}=5.028 {I64}/(2J+1) keV, |G{-|g}=0.39 eV {I11} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$from (n,|g):resonances. Other: 9400 {I3} from (d,p) 
J$from Breit-Wigner analysis in (n,|g) (resonance) and L(d,p)=2 from 0+. 
$|G=149 eV {I12} from |G{-n}=5928 {I48}/(2J+1) keV, |G{-|g}=1.46 eV {I16} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$other: L(pol d,t)=2 and L+1/2 from analyzing powers for a group at 9426 {I25} with T=3/2, which could be a doublet 
$g|G{-n}=96 {I4}/(2J+1) eV 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$from (n,|g):resonances. Other: 9436 {I3} from (d,p) 
$|G=588 eV {I5} from |G{-n}=3528 {I30}/(2J+1) keV, |G{-|g}=0.41 eV {I11} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$from (n,|g):resonances. Other: 9539 {I5} from (d,p) 
$|G=3.011 keV {I55} from |G{-n}=12.040 {I220}/(2J+1) keV, |G{-|g}=1.29 eV {I14} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$from (n,|g):resonances. Other: 9564 {I5} from (d,p) 
$|G=1.091 keV {I12} from |G{-n}=6540 {I72}/(2J+1) eV, |G{-|g}=0.73 eV {I40} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$L(d,p)=0 from 0+ 
$|G=10 keV {I4} (1976Bo18) from re-analysis of (n,|g):resonances data in 1950Ba88, and comparison with corresponding measured (d,p) cross sections by 1976Bo18. However, 9598.05 neutron resonance in 2018MuZY is assigned J|p=1/2- 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$L(d,p)=1 from 0+ 
$|G=11 keV {I4} (1976Bo18) from re-analysis of (n,|g):resonances data in 1950Ba88, and comparison with corresponding measured (d,p) cross sections by 1976Bo18. However, 9665.54 neutron resonance in 2018MuZY is assigned J|p=5/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$from (n,|g):resonances. Others: 9701 {I5} from (|a,n):res 
J$spin=3/2 also from (|a,|g):res 
T$from |G{-|a}=0.05 keV {I1}, |G{-n}=2.15 keV {I43} in (|a,n):res, |G{-|g}=0.55 eV {I28} in (n,|g),(n,n):resonances. But |G{-n}=1752 {I56}/(2J+1) eV=0.438 keV {I14} in (n,|g),(n,n):resonances is in disagreement 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$from (n,|g):resonances. Others: 9810 {I5} from (|a,n):res 
T$from |G{-|a}=0.020 keV {I4}, |G{-n}=0.98 keV {I20} in (|a,n):res. But |G{-n}=1368 {I46}/(2J+1) eV=0.342 keV {I12} from (n,|g),(n,n):resonances is in disagreement 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: PS
level_comment:
J$1173.2|g and 1995.1|g D, |DJ=1 to 15/2+ and 15/2-, respectively; 17/2+ proposed in ({+14}N,|ap|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E$from (n,|g),(n,n):resonances. Other: 9930 {I6} from (|a,n):res 
J$spin=5/2 also from (|a,|g):res 
T$from |G{-|a}=0.010 keV {I2}, |G{-n}=0.99 keV {I20} in (|a,n):res. But |G{-n}=2244 {I168}/(2J+1) eV=0.37 keV {I3} from (n,|g),(n,n):resonances is in disagreement 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E$from (n,|g):resonances. Other: 10001 {I7} from (|a,n):res 
J$spin=1/2 also from (|a,n):res 
T$from |G{-|a}=0.080 keV {I16}, |G{-n}=4.69 keV {I9} in (|a,n):res. But |G{-n}=1362 {I110}/(2J+1) eV=0.68 keV {I6} from (n,|g),(n,n):resonances is in disagreement 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$from (n,|g):resonances. Other: 10025 {I7} from (|a,n):res 
J$spin=3/2 also from (|a,n):res 
T$from |G{-|a}=0.120 keV {I24}, |G{-n}=6.5 keV {I13} in (|a,n):res. But |G{-n}=12240 {I248}/(2J+1) eV=3.06 keV {I6} from (n,|g),(n,n):resonances is in disagreement 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res 
J$spin=1/2 from |g(|q) in (|a,|g):res; 8084|g to 5/2+ 


level_energy_unit: KEV
level_comment:
J$(5/2) from the analysis of the resonance data in (|a,n):res for a group at 10081 {I7}, which could be a doublet of 10076.4 and 10083.5 in (n,|g):res. 
$|G{-|a}=0.020 keV {I4}, |G{-n}=0.98 keV {I20} for 10081 {I7} from (|a,n):res 


level_energy_unit: KEV
level_comment:
J$5/2 from analysis of (|a,n):res data for a group at 10134 {I8}, which could be a doublet of 10129.2+10132.4 in (n,|g):res 
$|G{-n}=1.055 {I146}/(2J+1) keV in (n,|g),(n,n):res 
$|G{-|a}=0.080 keV {I10}, |G{-n}=4.9 keV {I10} in (|a,|g):res 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: KEV
level_comment:
E$from (n,|g):res. Other: 10184 {I9} from (|a,n):res 
T$from |G{-|a}=0.15 keV {I3}, |G{-n}=6.2 keV {I12} in (|a,n):res. Other: |G{-n}=18.47 {I151}/(2J+1) keV=4.6 keV {I4} from (n,|g),(n,n):resonances 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E,J$from (n,|g):res. Other: 10223 with J=3/2 from (|a,n):res 
$|G{-n}=44.18 {I166}/(2J+1) keV=7.36 keV {I28} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$L(pol d,t)=2 and L+1/2 from analyzing powers gives 5/2+ for a group at 10356 {I30} with T=3/2, which could be a multiplet based on energy agreement 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res 
J$spin=3/2 from |g(|q); 7472|g to 7/2+. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res 
J$3/2 from the analysis of the resonance data in (|a,n):res; 5/2 from from |g(|q) in (|a,|g):res; 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2(+)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res 
J$5/2 from |g(|q) in (|a,|g):res; (1/2-,5/2+) from analysis of (|a,n):res data 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2(-)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|g):res 
J$spin from |g(|q) in (|a,g):res; 5042|g to 1/2-. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
E$others: 841.1 {I3} (1973Ca20), 840.3 {I3} (1972Hi06) 
T$from |t=1.70 ps {I33}, weighted average of 1.66 ps {I34} (1969Ra29), 1.81 ps {I36} and 1.65 ps {I33} (1969Br28, different stopping materials), 1.70 ps {I45} (1973Ca20). Other: 1.8 ps<|t<5.4 ps (1970Ka08) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$others: 1968.0 {I6} (1973Ca20), 1966.5 {I3} (1972Hi06) 
J$spin=5/2 from |g(|q) in 1977St02; 1966|g M1+E2 to 3/2+ 
T$from |t=147 fs {I24}, unweighted average of 125 fs {I37} (1969Br28), 182 fs {I22} (1969Ra29), 90 fs {I20} (1970Ka08), and 189 fs {I50} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E$others: 2313.7 {I5} (1973Ca20), 2312.6 {I4} (1972Hi06) 
J$from |g(|q,pol) in 1975Bu15 
T$from |t=169 fs {I25}, weighted average of 178 fs {I53} (1969Br28), 183 fs {I25} (1969Ra29), 145 fs {I25} (1970Ka08), and 198 fs {I50} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$others: 2868.2 {I3} (1973Ca20), 2866.2 {I4} (1972Hi06) 
J$from |g(|q,pol) in 1973Bu05 and 1975Bu15 
T$from |t=33 fs {I13}, weighted average of 33 fs {I13} (1969Br28) and 34 fs {I14} (1973Ca20). Others: |t<15 fs (1970Ka08), <15 fs (1969Ra29) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
E$others: 2935.0 {I5} (1973Ca20), 2934.3 {I5} (1972Hi06), 2934.5 {I15} (1969Br20) 
J$from |g(|q) in 1973Ca20 and |g(|q,pol) in 1975Bu15 
T$from |t=40.9 ps {I20}, weighted average of 38 ps {I11} (1969Br20), 36 ps {I8} (1970Ka08), 40.5 ps {I20} (1970Ra24, RDM), 44 ps {I4} (1971Br23, RDM). Others: |t>5.5 ps (1973Ca20), >10 ps (1969Br28), >4 ps (1969Ra29) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
E$others: 2971.0 {I5} (1973Ca20), 2968.7 {I4} (1972Hi06) 
J$from |g(|q) in 1972Hi06 and 1973Ca20 and |g(|q,pol) in 1975Bu15 
T$from |t=85 fs {I12}, weighted average of 90 fs {I31} (1969Br28), 82 fs {I12} (1969Ra29), 94 fs {I24} (1973Ca20). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E$others: 3221.0 {I5} (1973Ca20), 3219.0 {I10} (1972Hi06) 
T$from |t=48 fs {I18} (1973Ca20). Other: |t<65 fs (1969Ra29) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$others: 3833.0 {I10} (1973Ca20), 3830 {I2} (1972Hi06) 
J$spin=5/2 from n|g(|q) and |g|g(|q) in 1977St02; (3/2,5/2,7/2) from |g(|q) in 1973Ca20; 3/2,5/2 from |g(|q) in 1972Hi06; 3832|g M1+E2 to 3/2+ 
T$from |t=44 fs {I12} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E$others: 3935.0 {I5} (1973Ca20), 3934 {I3} (1972Hi06) 
J$spin=3/2 from |g(|q) in 1975Bu15; (1/2,3/2,5/2) from |g(|q) in 1973Ca20; 3935|g M1+E2 to 3/2+ 
T$from |t=35 fs {I10} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
E$others: 4049.8 {I5} (1973Ca20), 4047.6 {I10} (1972Hi06) 
J$from |g|g(|q) in 1977St02 and |g(|q,pol) in 1973Bu05 and 1975Bu15. Other: 5/2,9/2 from |g(|q) in 1972Hi06 and 1973Ca20 
T$from |t=305 fs {I77} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1973Ca20. Other: 4053 {I3} (1972Hi06) 
J$1972Hi06 states their |g(|q) is compatible with J=1/2,3/2 
T$from |t=18 fs {I12} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
E$others: 4096.0 {I5} (1973Ca20), 4093.8 {I10} (1972Hi06) 
J$from |g|g(|q) in 1977St02 and |g(|q,pol) in 1973Bu05 and 1975Bu15 
T$from |t=45 fs {I12} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_lifetime_unit: FS
level_comment:
E$others: 4145.0 {I5} (1973Ca20), 4142 {I3} (1972Hi06) 
J$spin=3/2,5/2 from |g(|q) in 1972Hi06 and 1973Ca20; 1/2,3/2,5/2 from |g|g(|q) in 1977St02 
T$from |t=34 fs {I10} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2
level_lifetime_unit: FS
level_comment:
E$other: 4376 {I1} (1973Ca20) 
J$spin=3/2,5/2 from |g(|q) in 1975Bu15; the authors note that their |g(|q) data is not in agreement with L(p,d)=0 for the same level in (p,d), which gives J|p=1/2+ 
T$from |t=34 fs {I15} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2
level_lifetime_unit: FS
level_comment:
E$other: 4425 {I2} (1973Ca20) 
J$spin=1/2,3/2 from |g(|q) in 1975Bu15 
T$from |t=27 fs {I14} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
E$other: 4732 {I1} (1973Ca20) 
J$5/2-,9/2- from |g(|q,pol) in 1975Bu15; 5/2- is ruled out since the corresponding |d(M2/E1)(1761|g)>+5.6 from 1975Bu15 is ruled out by RUL. 
T$from |t=82 fs {I21} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
E$other: 4868 {I1} (1973Ca20) 
J$from |g(|q,pol) in 1973Bu05 and 1975Bu15. Others: 7/2,11/2 from |g(|q) in 1973Ca20; 5/2,7/2,11/2 from |g(|q) in 1977St02 
T$from |t=360 fs {I90} (1973Ca20) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1973Ca20 
T$from |t=130 fs {I44} (1973Ca20) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1973Ca20 
T$from |t=39 fs {I16} (1973Ca20) 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from 1973Ca20 
T$from |t=31 fs {I11} (1973Ca20) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
T$from DSAM in 1989Ko53 
J$from |g circular polarization of transition from 8646 keV level (1969Ko05,1965Ko10,1961Ve03) and |g|g(|q) (1959Ma21 and 1967Ka03). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$1985Ke08 also report a level at E=5621 based on the placement of a 3020.38|g from 8642 level, but this placement is not confirmed in any other study and the same transition is placed from 5888 level to 2868 level by 1985Ra15 and 1985Gu20, which is adopted by the evaluators. Therefore, the 5621 level proposed in 1985Ke08 is omitted by the evaluators. 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$|t>1 ps is expected with a typical stopping time >1.3 ps of recoils in Bi backing, since all de-exciting transitions were observed without significant Doppler broadening (2016Fu09). 


level_energy_unit: KEV
level_comment:
$(d|s/d|W){-max}=0.0178 mb/sr at |q=22.5|' 
$Deformation parameter |b{-2}=-0.20 from analysis of |s(|q) (1968Co25) 


level_energy_unit: KEV
level_comment:
E$weighted average of 2868 {I12} (1971Gr04) and 2870 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.017 mb/sr at |q=30|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 2934 {I12} (1971Gr04) and 2938 {I15} (1971Kn04) 
L$for 2934+2974 doublet (1971Gr04) 
$(d|s/d|W){-max}=0.071 mb/sr at |q=37.5|' for 2934+2974 


level_energy_unit: KEV
level_comment:
E$weighted average of 3223 {I12} (1971Gr04) and 3220 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.207 mb/sr at |q=15|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 3832 {I12} (1971Gr04) and 3843 {I15} (1971Kn04) 
$L|<(3) 
$(d|s/d|W){-max}=0.019 mb/sr at |q=30|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 3939 {I12} (1971Gr04) and 3947 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.054 mb/sr at |q=30|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 4059 {I12} (1971Gr04) and 4068 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.198 mb/sr at |q=7.5|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 4146 {I12} (1971Gr04) and 4158 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.052 mb/sr at |q=15|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 4214 {I12} (1971Gr04) and 4224 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.161 mb/sr at |q=7.5|' 


level_energy_unit: KEV
level_comment:
E$4746 {I12} in 1971Gr04 could correspond to 4742+4761 in 1971Kn04 
$(d|s/d|W){-max}=0.078 mb/sr at |q=7.5|' for a group at 4746 {I12} 


level_energy_unit: KEV
level_comment:
E$weighted average of 4933 {I12} (1971Gr04) and 4931 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.100 mb/sr at |q=15|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 5281 {I12} (1971Gr04) and 5294 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.188 mb/sr at |q=7.5|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 5487 {I12} (1971Gr04) and 5495 {I15} (1971Kn04) 
$(d|s/d|W){-max}=1.48 mb/sr at |q=7.5|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 5723 {I12} (1971Gr04) and 5728 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.201 mb/sr at |q=7.5|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 6370 {I12} (1971Gr04) and 6384 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.209 mb/sr at |q=30|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 6684 {I12} (1971Gr04) and 6697 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.170 mb/sr at |q=22.5|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 6900 {I12} (1971Gr04) and 6912 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.131 mb/sr at |q=22.5|' 


level_energy_unit: KEV
level_comment:
E$weighted average of 6973 {I12} (1971Gr04) and 6983 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.140 mb/sr at |q=22.5|' 


level_energy_unit: KEV
level_comment:
E$probable doublet of 7163 {I12} in 1971Gr04 could correspond to 7153+7383 in 1971Kn04 
$(d|s/d|W){-max}=0.294 mb/sr at |q=30|' for a group at 7163 {I12} 


level_energy_unit: KEV
level_comment:
E$weighted average of 7346 {I12} (1971Gr04) and 7351 {I15} (1971Kn04) 
$(d|s/d|W){-max}=0.199 mb/sr at |q=22.5|' 


level_energy_unit: KEV
level_comment:
E$probable doublet of 7463 {I12} in 1971Gr04 could correspond to 7435+7473 in 1971Kn04 
$(d|s/d|W){-max}=0.238 mb/sr at |q=22.5|' for a group at 7463 {I12} 


level_energy_unit: KEV
level_comment:
E$weighted average of 7902 {I12} (1971Gr04) and 7920 {I15} (1971Kn04) 
$(d|s/d|W){-max}=1.03 mb/sr at |q=7.5|' 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$1/2+,3/2 from the Adopted Levels, but 7/2+ quoted in the level scheme and (7/2+,9/2+) quoted in the text in 1978Ok02. It is unclear how this J|p is assigned and where it is taken from in 1978Ok02. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
J$5/2+ in Adopted Levels, but 3/2- quoted in 1978Ok02. It is unclear how J|p=3/2- is assigned and where it is taken from in 1978Ok02 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
J$1978Ok02 propose |p=+ by considering 8085|g to 5/2+ can only be E2, but there is no supporting evidence in 1978Ok02. 
S$other: 3344 (1971Mc23). 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_comment:
J$(3/2-,7/2-) from 1975Sa05, 3/2 from 1975Ba01 and 1971Mc23. 
S$others: 3755 (1975Sa05), 3759 (1971Mc23). 
$|G{-|a}=2.18 keV {I44}, |G{-n}=4.1 keV {I8}. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
J$3/2 from fit to resonance data in 1971Mc23 and 1975Ba01, but 5/2 from |g(|q) in 1978Ok02. |p=- is proposed in 1978Ok02 assuming 6281|g and 7266|g to 3/2- are M1+E2. 
S$others: 3844 (1971Mc23), 3845 (1978Ok02). 
$|G{-|a}=0.030 keV {I6}, |G{-n}=4.0 keV {I8}. 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_comment:
J$(1/2-,3/2+) from 1975Sa05, 3/2 from 1975Ba01 and 1971Mc23. 
S$others: 4020 (1975Sa05), 4011 (1971Mc23). 
$|G{-|a}=0.55 keV {I11}, |G{-n}=14.4 keV {I29}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2(+)
level_comment:
J$5/2 from |g(|q) in 1978Ok02; (1/2-,5/2+) from 1975Sa05. But 1978Ok02 propose |p=- considering 4986|g to 1/2- is E2. 
S$other: 4091 (1971Mc23, 1978Ok02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2
level_comment:
J$1978Ok02 propose |p=- by assuming 6551|g to 3/2- is M1+E2 and 7909|g to 5/2+ is E1 
S$doublet with 4171 in 1978Ok02. Other: 4149 (1971Mc23). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2
level_comment:
J$1978Ok02 propose |p=+ by assuming 7909|g to 5/2+ and 9938|g to 1/2+ are M1+E2. 
S$doublet with 4153 in 1978Ok02. Other: 4169 (1971Mc23). 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_comment:
J$other: (3/2,5/2) from 1971Mc23. 
S$other: 4407 (1971Mc23). 
$|G{-|a}=0.170 keV {I34}, |G{-n}=3.8 keV {I8}. 


level_energy_unit: KEV
level_spin_parity: 3/2(+)
level_comment:
J$(3/2+,7/2-) from 1975Sa05, 3/2 from 1975Ba01, (3/2,5/2) from 1971Mc23. 
S$others: 4425 (1975Sa05), 4424 (1971Mc23). 
$|G{-|a}=0.34 keV {I7}, |G{-n}=4.8 keV {I10}. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
J$(5/2+,9/2+) from 1975Sa05, (5/2) from 1975Ba01 and 1971Mc23. 
S$others: 4495 (1975Sa05), 4502 (1971Mc23). 
$|G{-|a}=0.22 keV {I5}, |G{-n}=2.8 keV {I6}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
E,J$E{-R}=103 keV, s{-1/2}-wave resonance from analysis of resonance data (1988Ki02,1992Ki03). The s-wave resonance at E{-R}=111 keV in 1967Be36 is considered as the same resonance based on agreements of energy and J|p as well as |g-decay pattern. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$others: 790 {I50} (1949Da16), 841 {I8} (1967Mo04) 
L$also from 1953Ho80, 1966Sc09, 1973Or04, 1970Bo36. 
S$others: 0.24 {I3} (1973Or04), 0.80 (1970Bo36) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$from 1990Pi05. Others: 3222 {I6} (1958En51), 3224 {I8} (1967Mo04), 3150 {I50} (1949Da16) 
E$3252 in 1973Or04 is likely a misprint 
L$also from 1953Ho80, 1966Sc09, 1970Bo36, 1973Or04 
S$others: 1.26 (1970Bo36), 0.13 {I2} (1973Or04) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$4732 and 4747 cannot be resolved in 1973Or04 
L$from 1973Or04 for unresolved 4732+4747 peaks. The J|p assignments for 4732 and 4747 levels suggest L=0 belongs to only the 4747 level 
S$from 1973Or04 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$others: 4890 (1953Ho80); 4919+4941 not resolved in 1971Me12 
L$also from 1953Ho80, 1973Or04 
S$other: 0.035 {I10} (1973Or04) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$from 1990Pi05. Other: 5711 {I6} (1958En51) 
L$also from 1953Ho80, 1973Or04. 
S$other: 0.11 {I2} (1973Or04) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E,L$other: 8749 {I10} with L=0 (1975Li09) 
$|G=20 keV {I3} deduced by 1976Bo18 from reanalysis of neutron resonance data in 1950Ba88, as compared with the cross-section data in their (d,p) experiment 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E,L$other: 9005 {I10} with L=0 (1975Li09) 
$|G=13 keV {I3} deduced by 1976Bo18 from reanalysis of neutron resonance data in 1950Ba88, as compared with the cross-section data in their (d,p) experiment 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E,L$other: 9320 {I10} with L=0 (1975Li09) 
$|G=10 keV {I3} deduced by 1976Bo18 from reanalysis of neutron resonance data in 1950Ba88, as compared with the cross-section data in their (d,p) experiment 


level_energy_unit: KEV
level_comment:
$|G=10 keV {I4} deduced by 1976Bo18 from reanalysis of neutron resonance data in 1950Ba88, as compared with the cross-section data in their (d,p) experiment 


level_energy_unit: KEV
level_comment:
$|G=11 keV {I4} deduced by 1976Bo18 from reanalysis of neutron resonance data in 1950Ba88, as compared with the cross-section data in their (d,p) experiment 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: PS
level_comment:
J$from 1966Be15 
T$from |t=1.10 ps {I+50-40}, weighted average of 1.73 ps {I+110-45} (1969Va28) and 0.9 ps {I+5-4} (1970Cu01) by DSAM. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$tentative level from 1966Od01. 1967Mo04 argued that the 1.35 MeV level observed in 1966Od01 was due to levels in {+34}S at E{-x}=4.08 and 4.12 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$2017Ka41 label this |g as the transition from the first excited level to g.s., but such level is not seen in any other work. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$from 1966Be15, 1966Od01 and 1977So07; parity from the Adopted Levels 
T$from |t=150 fs {I30}, weighted average of 150 fs {I45} (1969Va28) and 150 fs {I30} (1970Cu01) by DSAM 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$from 1966Be15 and 1977So07. Other: 3/2,5/2 from 1966Od01. Parity from the Adopted Levels 
T$from |t=140 fs {I30}, weighted average of 140 fs {I30} (1969Va28) and 140 fs {I40} (1970Cu01) by DSAM 


level_energy_unit: KEV
level_spin_parity: 7/2
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$from 1966Be15 and 1966Od01. Other: 3/2,7/2 from |g(|q) in 1977So07 
T$from |t>7 ps in 1969Va28. Others: |t>1.4 ps (1970Cu01), |t<10 ns (1966Be15) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_lifetime_unit: FS
level_comment:
J$from 1966Be15, 1966Od01 and 1977So07 
T$from |t=31 fs {I9}, weighted average of 28 fs {I9} (1969Va28) and 40 fs {I+20-10} (1970Cu01) by DSAM 


level_energy_unit: KEV
level_comment:
J$1975VaYG propose 7/2 based on their |g(|q) and |g|g(|q) combined with previous work. However, as also stated in 1975VaYG, only J=1/2 is excluded from their analysis of |g|g(|q). 1975VaYG reject J=9/2 assigned by 1973Bu05 (also 1975Bu15) from |g(|q,pol) in (|a,n|g), by arguing that the resulting |d(1966|g) for J=9/2 is in disagreement with |d(1966|g) from 977|g-1966|g(|q), which however does not seem a strong argument for rejection of J=9/2. Besides, A{-2}=+0.31 {I12} and A{-4}=-0.26 {I16} of 2081|g from this level to 1966 with J=5/2 seems to be consistent with |DJ=0 or 2, which is also in agreement with the assignment of J(4047)=5/2,9/2 by 1973Ca20 in (|a,n|g). J=9/2 is also confirmed by 1977St02 in (|a,n|g) based on |g|g(|q) 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
J$spin=3/2,5/2 from 3370|g(|q) in 1977So07; 5/2 is excluded by 1977So07 as it would require an E3 or M3 strength for 3370|g that exceeds RUL. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+,3/2)
level_comment:
E$from 1977So07 
J$spin=1/2,3/2,5/2 from |g(|q) in 1977So07; 5/2 and 1/2- is excluded by 1977So07 as the |d solutions for those J|p would require M2, E3 or M3 strengths that exceed RUL, by using measured T{-1/2} from 1973Ca20 in (|a,n|g) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$doublet (1968Du04); the higher-energy component could correspond to 2970 level from 1970Le14 
L$(3) in 1968Du04 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$ <r{+2}>{+1/2}=3.2847 fm {I21} (2004An14 evaluation and its 2008 update on webpage: http://cdfe.sinp.msu.ru) 
J$ microwave spectroscopy measurement (1948To10) shows no hyperfine structure 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|b{-2}(p,p')=0.28 {I1} (1985Al03); 0.24 {I2} (1999Ma63 by reanalysing 1985Al03 data with Becchetti-Greenless optical potential) 
MOMM1$from 1979Za01 by perturbed angular correlation after ion implantation method. 
MOME2$+0.06 {I4} in 1980Ba40 by Coulomb excitation reorientation method recalculated by 1981Sp07 as 0.04 {I3}. See also 1989Ra17 evaluation 
J$E2 |DJ=2 |g to 0+, g.s. ({+31}P(|a,p|g), {+24}Mg({+16}O,|a2p|g)) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 440 {I50} (1970Gr11), 400 {I32} (1970Ra17), 400 {I40} (1974Gr06), 460 {I95} (1970Br18), 467 {I90} (1970Cu02); from {+32}S(t,p|g): 490 {I30} (1977He12); from {+34}S(e,e'): 486 {I17} (1985Wo06); from {+34}S(|a,|a'): 442 {I25} (1980Ba40); from {+28}Si({+34}S,{+34}S'): 462 {I26} (1977Sc36). Weighted average (external uncertainty) |t: 459 fs {i11}. Others T{-1/2}: 350 fs {i60} (1969Gr03, from {+31}P(|a,p|g)); 380 fs {i60} (1974Ol02, from {+206}Pb({+34}S,{+34}S'|g)); 307 fs {i17} (2001Ra27 evaluation, total of 14 measurements are listed in this evaluation) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$E2 |DJ=2 |g to 0+, g.s. ({+24}Mg({+16}O,|a2p|g)) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 218 {I30} (1970Gr11); 175 {I25} (1970Ra17); 190 {I40} (1970Br18). From {+31}P(|a,p|g): 192 {I13} (1977He12). From {+34}S(e,e'): 216 {I25} (1985Wo06). Weighted average: 196 {I10}. Others (from {+31}P(|a,p|g)): 145 {I20} (1974Gr06); 144 {I28} (1970Cu02); 120 {I30} (1969Gr03). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L=0 in {+32}S(t,p) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 1600 {I130} (1970Gr11); 1890 {I500}. Weighted average: 1618 {I126} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$D |DJ=1 |g to 0+, g.s. (1970Mo09, 1971Mu03); |p=+ from L=0 in {+35}Cl(d,{+3}He) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): <33 (1970Gr11); <24 (1970Ra17); |<50 (1974Gr06). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$E2 |DJ=2 |g to 0+, g.s. ({+31}P(|a,p|g)), or L=2 in {+32}S(t,p) 
T$mean lifetime |t in fs ({+31}P(|a,p|g)): 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:
J$L=3 in {+32}S(t,p), and also from {+34}S(p,p'),(pol p,p') 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 125 {I20} (1970Gr11); 135 {I17} (1970Ra17); 145 {I50} (1971So01); 115 {I10} (1974Gr06). Weighted average: 121 {I8} 
$ Adopted B(E3)=0.008 {I2} (2002Ki06 evaluation) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$E2 |DJ=2 |g to 2+, 2127 and test of spin hyphotheses ({+31}P(|a,p|g)); also J=4 in {+34}S(n,n),(n,n') 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 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:
J$M1+E2 |DJ=1 |g to 2+, 3303 and test of spin hyphotheses (1971Mu03) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 57 {I22} (1970Ra17). Others: <85 (1970Gr11), |<70 (1974Gr06). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$E2 |DJ=2 |g to 0+ g.s. {+31}P(|a,p|g) 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): <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:
J$D+Q |DJ=0 |g to 2+, 2127; |p=(-) based on statement in {+34}S(|a,|a') 
T$mean lifetime |t in fs, from {+31}P(|a,p|g): 24 {I10} (1970Gr11). Other: |<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 ({+31}P(|a,p|g)) 
T$mean lifetime |t in fs from {+31}P(|a,p|g): |<70 (1974Gr06) 


