# LEVEL

level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: NS
level_comment:
J Ne 1/2- from |DJ=0 d or |DJ=2 Q to g.s. if J|p(g.s.)=7/2- 
T from line-shape analysis in ({+48}Ca,X|g) 


level_energy_unit: KEV
level_comment:
J 3/2,7/2,11/2 from |DJ=0 d or |DJ=2 Q to g.s. if J|p(g.s.)=7/2-. Ne 3/2 since not populated in |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J from comparison of branching ratios and log| {Ift}'s for the decay of {+43}Ar and {+45}Ar and shell model predictions 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
$x<6341 {I140}, from Q(|b{+-})-S(n), where Q(|b{+-})=11510 {I140}, S(n)({+45}Ar)=5168.9 {I17} (2021Wa16) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
|DE not given; at E({+14}C)=75 MeV the {+16}O lines to 1550 and g.s. have about equal intensity; 1550 suggested as 2+ first excited state on the basis of systematics. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$ |s=11 mb {I2} 
$ Deformation length |d{-2}=0.88 fm {I9}, |b{-2}=0.21 {I2} 
J$ measured ({+46}Ar)|g(|q) consistent with 2+ 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
E$ 4982 {I12} (2005Ri11) 
$ |s=4.5 mb {I11} without any feeding corrections 
J$ measured ({+46}Ar)|g(|q) consistent with 3- 
$ Deformation length |d{-3}=0.63 fm {I8} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$First B(E2) (in e{+2}b{+2} units) obtained from best fit of theoretical and experimental angular distributions (2016Ca17); and the second value is determined as relative to 0.0473 {I20} in 2001Ra27 (At. Data and Nucl. Data Tables 78, 1) evaluation. 2016Ca17 note that this B(E2) value could be |?10% less if excitation of the second 2+ state is considered. These results are compared to B(E2)=0.0196 {I39} (1996Sc31: Phys. Rev. Lett. 77, 3967); 0.0218 {I31} (2003Ga20: Phys. Rev. C68, 014302) and 0.0577 {I+335-160} (2010Me07: Phys. Rev. C82, 024308). 2016Ca17 give an average B(E2)=0.0216 {I22} from their two values and those from 1996Sc31 and 2003Ga20 
$Experimental |s=40 mb {I5} (2016Ca17) 
T$deduced by compiler from B(E2)=0.0225 {I29} using E|g=1577 keV. B(E2)=0.0234 {I19} gives T{-1/2}=1.24 ps {I10}, whereas averaged B(E2)=0.0216 {I22} gives T{-1/2}=1.34 ps {I14}. Value is 1.59 ps {I32} in {+46}Ar Adopted Levels in the ENSDF database (July 2000 update), based on data from 1996Sc31 


level_energy_unit: KEV
level_spin_parity: (2+)
level_uncertain: ?
level_comment:
E$tentative level from 2003Do10: Nucl. Phys. A727, 195 
$The listed B(E2) value is for 0+ (g.s.) to 3489, (2+) level obtained from upper limit of intensity for the 1919|g which has a branching of |?40% as given in 2003Do10 
$Rounded energy from {+44}Ca Adopted Levels in the ENSDF database. This level is probably not populated in the present work 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: S
level_comment:
J L(n)=1 in {+2}H({+46}Ar,p). 3/2- in analogy with other N=29 isotones (2004We09) and systematics (2003Au02) 
T from 2004We09. Others: 1.25 s {I15} (2004Gr20) and 0.7 s (1995So03) 
%B-N Other: <1 (1995So03) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$Inclusive and ground-state |s|<0.48 mb {I3} for one-neutron pickup reaction (2016Ga14). Only an upper limit is given by the authors since presence of tail of unreacted {+46}Ar projectiles did not allow for clean particle identification. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$Measured partial cross section=2.6 mb {I5} 
$Inclusive |s=5.4 mb {I3} for one-proton removal, derived from yield of {+47}Ar reaction products and number of incoming {+48}K projectiles, 5% systematic uncertainty has been added in quadrature 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 381 ms {I35} (|b|g-setup), 412 ms {I19} (|b telescope), and 430 ms {I70} (|b|g with secondary ECR) in 2012We08, and 475 ms {I40} from implant-|b(t) in 2004Gr20 and 2003Gr22 
$%|b{+-}n: estimated by 2012We08 from the intensities of 2013|g from {+47}K |b{+-} decay and 3832|g from {+48}K |b{+-} decay. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from decay curves for six |g rays from the decay of {+50}Ar (2012We08). Earlier value was 86 ms {I30} from the |b- and delayed-neutron time-spectra (2003We09) 
$Theoretical T{-1/2}=41.8 ms, %|b{+-}n=28 (2019Mo01) 
$Theoretical T{-1/2}=55.2 ms, %|b{+-}n=4.0, %|b{+-}2n=0.5 (2016Ma12) 
%B-N$earlier value from the same group was 35 {i10} (2003We09) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_uncertain: ?
level_comment:
J$from shell-model predictions, but a 2+ state is also predicted near this energy (2015St10), thus 2+ is also possible 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|b{+-} is the only possible decay mode, followed by |b-delayed neutron emissions. 
$Theoretical T{-1/2}=15.9 ms, %|b{+-}n=40, %|b{+-}2n=1, %|b{+-}3n=0 (2019Mo01) 
$Theoretical T{-1/2}=15.1 ms, %|b{+-}n=72.4, %|b{+-}2n=1.4, %|b{+-}3n=0.5 (2016Ma12) 
T$half-life of {+52}Ar has not yet been measured. From time-of-flight of 620-650 ns (e-mail reply of Sept 23, 2009 from O. Tarasov to B. Singh), T{-1/2}>650 ns. From a general decreasing trend of half-lives with increasing neutron number, T{-1/2} for {+52}Cl is expected to be <50 ms, based on measured half-lives of 1.23 s for {+47}Ar, 475 ms for {+48}Ar, 170 ms for {+49}Ar, and 106 ms for {+50}Ar, available in literature. Other: 40 ms (2021Ko07,systematics) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Population |s=0.6 mb {I3}, deduced from subtraction of summed partial cross sections to the two excited states from the inclusive |s=1.9 mb {I1}, with the assumption that no other excited states are populated. Note that 2019Li10 give |s=0.7 mb {I3}. 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
$%|b{+-}n=26, %|b{+-}2n=34 (calculated,1997Mo25) 
$ Measured cross section=0.24 pb {I+28-16} using tungsten target (e-mail reply of Nov 11, 2009 from O. Tarasov, first author of 2009Ta24). 
E$ fragments observed by 2009Ta24 are assumed to be in the ground state of {+53}Ar. 
J$ 5/2- (syst,2011AuZY), 9/2+ (prediction,1997Mo25) 
T$ time-of-flight=620-650 ns (e-mail reply of Sept 23, 2009 from O. Tarasov). Actual half-life is expected to be much longer as suggested by systematics value of 3 ms (2011AuZY) and calculated value of 15 ms (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Only the |b{+-} decay mode is expected, accompanied by delayed neutron decays, thus 100% |b{+-} decay is assigned by inference. 
$A total of 13 event were assigned to {+54}Ar, two events each with tuned setting of spectrometer for {+50}S and {+53}Cl, one event for setting on {+54}Ar, and four each for setting on {+57}K and {+60}Ca, according to data in Table I and text of 2018Ta07. 
$Theoretical T{-1/2}(|b)=7.1 ms, %|b{+-}n=81, %|b{+-}2n=5, %|b{+-}3n=0, %|b{+-}4n=0, %|b{+-}5n=0 (2019Mo01) 
$Theoretical T{-1/2}(|b)=6.7 ms, %|b{+-}n=68.2, 68.1; %|b{+-}2n=3.7, 4.8; %|b{+-}3n=1.8, 1.6; %|b{+-}4n=0.007, 0.006; %|b{+-}5n=0 (2021Mi17, two values for a decay mode refer to different fission barriers). 
T$half-life of the {+54}Ar 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 Sc isotopes, the half-life is expected to be <20 ms from 106 ms for {+50}Ar, 236 ms for {+49}Ar, 416 ms for {+48}Ar and 1.23 s for {+47}Ar, assuming a decreasing trend of half-life as neutron number increases in neutron-rich nuclei. From systematics, T{-1/2}=5 ms in 2021Ko07. 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$3/2+ from systematics (2021Ko07) and theoretical prediction (2019Mo01) 
T$derived from distributions of the measured decay vertices (2019Ko18). 
${+31}K g.s. decays via 1p-decay channel to {+30}Ar ground state, which subsequently decays via 2p-channel to {+28}S ground state. The half-life of {+30}Ar is <10 ps (2015Mu13) 
$1p-decay energy=2.15 MeV {I15} (2019Ko18), resulting in a decay energy of 4.6 MeV {I2} for the 3p-decay to {+28}S ground state, with the known {+30}Ar 2p-decay energy of 2.45 MeV {I15} from 2018Xu04 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$Tentative assignment of 1p-decay of {+31}K level through the known states in {+30}Ar and {+29}Cl states from 2018Xu04 
E$from 3p-decay energy of |?9 MeV for this level and 4.6 MeV for g.s. (2019Ko18) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$Tentative assignment of 1p-decay of {+31}K level through the known states in {+30}Ar and {+29}Cl states from 2018Xu04 
E$from 3p-decay energy of |?16 MeV for this level and 4.6 MeV for g.s. (2019Ko18) 


level_energy_unit: KEV
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$deduced from distributions of the measured decay vertices (2019Ko18) 
$Decays via 1p-decay channel to {+30}Ar ground state, which further decays via 2p mode to {+28}S ground state with T{-1/2}<10 ps (2015Mu13) 
$1p-decay energy=2.15 MeV {I15} (2019Ko18), resulting in a decay energy of 4.6 MeV {I2} for the 3p-decay to {+28}S ground state, with the known {+30}Ar 2p-decay energy of 2.45 MeV {I15} from 2018Xu04 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
$S(p)=-2450 {I200} (syst, 2021Wa16) suggests that {+33}K is unbound for one-proton emission. 
T$estimated by 1996PoZZ from limit of detection. 
J$3/2+ from theory in 2019Mo01 and systematics in 2021Ko07 
$Theoretical T{-1/2}(|b decay)=36.3 ms (2019Mo01) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
T$upper limit estimated from expected cross sections (1996PoZZ) 
J$1+ proposed by 2003Au02 (also 2011AuZY) from systematics 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$Total decay energy E{-T}=608 {I17} 
$Mass excess=-1487 keV {I17}, deduced by 2024Dr01 from their measured total decay energy and mass of {+33}Ar from 2021Wa16 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_lifetime_unit: MS
level_comment:
MOMM1$ from |b-NMR spectroscopy (2006Me04). Other: 0.36 {I3} (1998Sc19,|b-NMR spectroscopy). Positive sign from analogy with mirror state of {+35}S g.s. 
%|ep: from 1980Ew02. 
J$log| {Ift}=4.85 to 1/2+, 5.07 to 3/2+ and 4.91 to (5/2)+; probable mirror state of {+35}S g.s. with J|p=3/2+ 
T$from 1998Sc19. Other: 190 ms {I30} (1980Ew02). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MS
level_comment:
%ECP,%ECA$from 1980Es01. 
J$spin from |b-radiation detected optical pumping from polarized nuclei (1975Sc20), parity from log| {Ift}=4.78 to 2+ state in {+36}Ar 
MOMM1$ optical pumping (1975Sc20) 
T$weighted average of 336 ms {I4} (1971Go18), 341 ms {I6} (1972Mi13), and 344 ms {I3} (1976Fr03). Others: 345 ms {I5} (1971Ja09) from the same group as 1972Mi13, 342 ms {I28} (1972Mo08), 265 ms {I25} (1967Be11) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: PS
level_comment:
J$ mirror state of 788, 3+ level in {+36}Cl 
T$ from plunger method in {+48}Ca({+37}Ca,X|g) (2010Be01) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
E$weighted average of 1706.8 {I6} ({+36}Ar({+3}He,t)) and 1706 {I3} ({+9}Be({+40}Ca,X|g)) 
J$ possible mirror state of 1951, 2- level in {+36}Cl 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$weighted average of: 1918.3 {I7} ({+36}Ar({+3}He,t)), 1916.4 {I14} ({+9}Be({+40}Ca,X|g)), and 1914 {I5} ({+9}Be({+37}Ca,X|g)) 
J$ possible mirror state of 1959, 2+ level in {+36}Cl 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$isobar analog state of {+36}Ca g.s.. Energy: 4289 {I8} (1995Ga16), 4290 {I23} (2001Lo11), 4286 {I8} (1997Tr05); E(level){-recalculated}=4281.9 {I8} 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: PS
level_comment:
T$from plunger method (2010Be01); other: 8 {I+5-4} ps (2007DoZV). 2010Be01 and 2007DoZV seem related but give discrepant T{-1/2} value; the newer value was adopted by evaluator 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$ possible mirror state of 1951, 2- in {+36}Cl, predicted level energy=1723 in {+36}K 
$ E(p)(c.m.)=48.4 {I8} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$ possible mirror state of 1959, 2+ in {+36}Cl, predicted level energy=1931 in {+36}K 
$ E(p)(c.m.)=259.9 {I9} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$ possible mirror state of 2468, 3- in {+36}Cl, predicted level energy=2186 in {+36}K 
$ E(p)(c.m.)=538.5 {I9} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$ possible mirror state of 2492, 2+ in {+36}Cl, predicted level energy=2288 in {+36}K 
$ E(p)(c.m.)=623.4 {I9} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$from Adopted Levels of {+36}K in ENSDF database 
$Mean square charge radius |d<r{+2}>({+39}K,{+36}K)=-0.16 fm{+2} {I5}(stat) {I8}(syst) (2015Ro12) 
$Isotope shift |d|n({+39}K,{+36}K)=-403 MHz {I5}(stat) {I4}(syst) (2015Ro12). Other |d|n({+37}K,{+36}K)=-139 MHz {I4}(stat) {I3}(syst) (2015Ro12) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|d|n{+39,36}=-403 MHz {I9}, |d<r{+2}>{+39,36}=-0.20 fm{+2} {I8} (stat) {I4} (syst) 
$R{-ch}=3.405 fm {I12} (stat) {I6} (syst) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
MOMM1$measured by optical pumping with radiative detection (1971Vo03); hyperfine splitting of {+37}K g.s. (1968Be19) 
MOME2$ |b-NQR method on polarized {+37}K nuclei produced in fragmentation reaction. The quoted uncertainty includes both the statistical and systematic resulting from the line shape of the |b-NQR spectrum presented in 2008Mi07. Other: 0.10 {I4} (1997Be35, optical isotope shift measurement using polarized {+37}K nuclei in magneto-optic trap at TISOL, TRIUMF) 
J$from L=0 in {+39}K(p,t) 
T$weighted mean of: 1.23 s {I2} (1958Sc29), 1.25 s {I4} (1964Ka24), and 1.223 s {I8} (1977Az01); others: 1.2 s {I2} (1951Bo56), 1.20 s {I12} (1958Su60), 1.15 s {I15} (1960Wa04) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
MOMM1$1971Ra22 measured g=+1.5 {I1} by time-dependent perturbed angular distribution based on which 2005St24 adopted the g-factor 
J$based on RUL and L=3 from {+36}Ar(d,n) 
T$weighted average of 9.6 ns {I14} (1967Go{+18,36}Ar(p,p)) and 10.5 ns {I5} (1971Ra{+22,40}Ca(p,|a)); other: >8.3 ns ({+36}Ar(d,n|g)) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$1/2-,3/2- from L=1 ({+36}Ar({+3}He,d)); |DJ=1, M1+E2 912|g connecting 5/2-,7/2-, 3082 with 1/2-,3/2-, 2170 (this level) selects 5/2- for 3082 and 3/2- for 2170 
T$from {+36}Ar(p,p); other: ls 69 ps ({+36}Ar(d,n|g)) 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
J$5/2,7/2,9/2 from D(+Q) |g from 7/2+, 4732 ({+36}Ar(p,p)); 5/2+,(7/2+,9/2+) from L=2(+4) in {+39}K(p,t); (5/2+,7/2+) from (Q+O) |g to 3/2+, g.s. ({+36}Ar(p,p)) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L=2 from |s(|q) and Ay(|q) ({+40}Ca(p,|a)) 
T$weighted average of 0.5 fs {I4} ({+36}Ar(p,p)) and 1.52 fs 14 ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J$from 1967Go18: 7/2-,5/2- from |DJ=0,1 M1+E2 1702|g to 7/2-, 1380 (1967Go18); |DJ=1, M1+E2 912|g connecting 7/2-,5/2-, 3082 (this level) with 3/2-,1/2-, 2170 level selects 5/2- for 3082 and 3/2- for 2170 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E,T$from {+37}Ca |e decay 
J$5/2+,7/2+ from L=2+4 ({+39}K(p,t)); 7/2+ excluded by log| {Ift}=4.9 from 3/2+ g.s. of {+37}Ca ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$weighted average of 3315 {I3} ({+36}Ar(p,p)) and 3315 {I2} ({+40}Ca(p,|a)) 
J$1/2-, 3/2- from L=1; 3/2- from |DJ=1 |g to 1/2+, 1370; also, the elastic scattering anomaly can Be fitted only for J|p=3/2- and |G=|G{-p}=2.2 {I3} keV thus excluding 1/2- (all arguments from {+36}Ar(p,p)) 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+,5/2+
level_comment:
E$weighted average of 3840 {I3} ({+37}Ca |e decay) and 3844 {I10} ({+36}Ar(p,p)) 
J$log| {Ift}=4.9 from 3/2+ g.s. of {+37}Ca ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$weighted average of 4496 {I3} ({+37}Ca |e decay), 4498 {I4} ({+40}Ca(p,|a)), and 4508 {I4} ({+36}Ar(p,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 5418 {I5} ({+36}Ar(p,p)) and 5424 {I3} ({+37}Ca |e decay) 
J$from L=2 ({+36}Ar(p,p)) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 5479.8 {I21} ({+37}Ca |e decay) and 5470 {I5} ({+36}Ar(p,p)) 
J$from L=2 ({+36}Ar(p,p)) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$weighted average of 5565 {I7} ({+36}Ar(p,p)) and 5569 {I5} ({+37}Ca |e decay) 
J$5/2-,7/2- from L=3 ({+36}Ar(p,p)); 7/2- excluded by log| {Ift}=6.2 from 3/2+ g.s. of {+37}Ca ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 6431 {I10} ({+36}Ar(p,p)) and 6432 {I3} ({+37}Ca |e decay) 
J$log| {Ift}=5.3 from 3/2+ g.s. of {+37}Ca ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 6678 {I10} ({+36}Ar(p,p)), 6684 {I5} ({+37}Ca |e decay), and 6670 {I20} ({+39}K(p,t)) 
J$from isobaric multiplet mass equation ({+39}K(p,t)) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$from {+36}Ar(p,p), 6740 {I5} from ({+37}Ca |e decay) 
J$log| {Ift}=6.4 from 3/2+ g.s. of {+37}Ca ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$from L=3 ({+36}Ar(p,p)) 
E$weighted average of 6912 {I10} ({+36}Ar(p,p)), 6912 {I5} ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)+
level_comment:
E$weighted average of 7093 {I15} ({+36}Ar(p,p)), 7071 {I5} ({+37}Ca |e decay) 
J$log| {Ift}=5.0 from 3/2+ g.s. of {+37}Ca ({+37}Ca |e decay) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from Adopted Levels, Gammas dataset; this value was used by 1979SoZT to assign other J|p values in this level scheme 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
E$also 1381 (1979SoZT); 1380 (1967Go18) 
J$from 1979SoZT: 5/2,7/2 from |g(|q) (no evidence shown) allows extracting L=3 (from L=0+3 for doublet in {+36}Ar(d,n) dataset); (7/2-) from analog level in mirror {+37}Ar nucleus 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E$also 2171 (1979SoZT); 2169 (1967Go18) 
J$from 1979SoZT: 3/2 from |DJ=1, D |g to (1/2+), 1369; 3/2- from L=1 (see {+36}Ar(d,n) dataset) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$based on measured L (same as the adopted values) 
S$|s(|q) indicates s(0)>>s(2), with (1d3/2){+2} transfer dominant 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from 1967Go18: L=2 from {+36}Ar({+3}He,d) (see dataset); the strength of 1380|g from 1380 level simultaneously selects 3/2+ for g.s. and 7/2- for 1380 level 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$others: 1368 {I3} (1967Go18) 
T$mean lifetime |t in ps: >1.5 (1988De03) 
J$from 1967Go18: 1/2+, 1/2-, 3/2-, or (5/2-) from respectively |DJ=1 E1 or M1 |g, |DJ=0 M1+E2 |g, or |DJ=2 E2(+M3) |g from 3/2-, 3311 (1967Go18); (1/2+) assuming this is the analog of 1/2+, 1410 in {+37}Ar (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
E$others: 1380 {I2} (1967Go18) 
J$from 1967Go18: based on RUL and L=3 from {+36}Ar({+3}He,d) (see dataset); the strength of 1380|g from this level to g.s. simultaneously selects 3/2+ for g.s. and 7/2- for 1380 level; also in 1988De03: based on RUL and L=3 from {+36}Ar(d,n) (see dataset) 
T$from 1967Go18; others: mean lifetime |t in fs: >200 (1988De03, from E(p)(lab)=1259); >400 (1988De03, from E(p)(lab)=2627) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
$E(p)(lab)=321.28 {I17} (weighted average of 321.28 {I16}, 321 {I2}, 321 {I5}) 
$E(p)(lab)=321.28 {I16} estimated by evaluators from E(level)=2170.18 {I13} (1988De03) 
$E(p)(lab)=321 {I2}, E(level)=2170 {I2} (1992Il03) 
$E(p)(lab)=321 {I5}, E(level)=2170 {I5} (1967Go18) 
J$from 1967Go18: 1/2-,3/2- from L=1; |DJ=1, M1+E2 912|g connecting 7/2-,5/2-, 3082 with 1/2-,3/2-, 2170 (this level) selects 5/2- for 3082 and 3/2- for 2170 
T$mean lifetime |t in fs: 150 {I+100-45} (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=1.2 {I3} meV (1992Il03) 
$|G{-|g}/|G>0.8 (1988De03) 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
$E(p)(lab)=439.56 {I15} (weighted average of 439.56 {I15}, 433 {I9}) 
$E(p)(lab)=439.56 15 ESTIMATED BY EVALUATORS FROM E(level)=2285.24 12 (1988De03) 
$E(p)(lab)=433 9, E(level)=2279 9 (1967Go18) 
J$from 1988De03: 5/2,7/2,9/2 from D(+Q) |g from 7/2+, 4732; 5/2+,(7/2+,9/2+) from L=2(+4) in {+39}K(p,t); (5/2+,7/2+) from (Q+O) |g to 3/2+, g.s. (1988De03; based on |d fits, they further conclude 7/2+,(5/2+) which however is not adopted here) 
T$mean lifetime |t in fs: >350 (1988De03) 
$|G{-|g}/|G>0.94 (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G<0.048 {I3} meV (1992Il03) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
$E(p)(lab)=917.56 {I9} (weighted average of 917.57 {I9}, 917.2 {I6}, 917 {I2}, 918 {I1}) 
$E(p)(lab)=917.57 9, E(level)=2750.22 8 (1988De03, ADJUSTED) 
$E(p)(lab)=917.52 7, E(level)=2750.27 6 (1988De03, ORIGINAL) 
$E(p)(lab)=917.2 6 ESTIMATED BY EVALUATORS FROM E(level)=2749.9 6 (1993Il02) 
$E(p)(lab)=917 2, E(level)=2750 2 (1992Il03) 
$E(p)(lab)=918 1, E(level)=2751 1 (1964Ar17) 
J$5/2,7/2,9/2 (1988De03, 1967Go24) from D(+Q) |g to 7/2-, 1380 (1988De03); 5/2+ from M1+E2 |g to 3/2+, g.s. (1967Go24); 1/2,3/2,5/2 (1967Go18) from D+Q |g to 3/2+, g.s.; (3/2-,5/2) (1967Go18) from |g to 7/2-, 1380 
T$mean lifetime |t in fs: 0.7 {I5} (1998Hi18, DSAM); 1.89 {I15} (1999Mo07, deduced from their measured (2J+1)|G{-p}|G{-|g}/|G and |G{-|g}/|G{-p} from other refs.); <3 (1988De03); <6 (1970An19); |>0.0008 (from |G |<0.8 keV, 1967Go18 citing 1964Ar17); adopted: 0.7 {I5} 
$(2J+1)|G{-p}|G{-|g}/|G=516 {I48} meV (1999Mo07), 416 {I60} meV (1967Go18) 
$|G{-p}= |<0.8 keV (1964Ar17), |G{-|g}=69 {I10} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
$E(p)(lab)=1258.64 {I13} (weighted average of 1258.64 {I13}, 1260 {I4}) 
$E(p)(lab)=1258.64 13 FROM E(level)=3081.99 9 (1988De03); E(p)(lab)=1258.73 13 (1988De03, ORIGINAL) 
$E(p)(lab)=1260 4, E(level)=3083 4 (1967Go18) 
J$from 1967Go18: 7/2-,5/2- from |DJ=0,1 M1+E2 1702|g to 7/2-, 1380 (1967Go18); |DJ=1, M1+E2 912|g connecting 7/2-,5/2-, 3082 (this level) with 3/2-,1/2-, 2170 level selects 5/2- for 3082 and 3/2- for 2170 
J$from 1988De03: 5/2 from D(+Q) |g to 3/2+, g.s. and D+Q |g to 7/2-, 1380; 5/2- based on RUL 
T$mean lifetime |t in fs: 10 {I4} (1988De03); 0.041 {I8} (1967Go18, |G=0.016 {I3} keV, tentative value); adopted 10 {I4} 
$(2J+1)|G{-p}|G{-|g}/|G=26 {I4} meV (1967Go18) 
$|G{-p}=0.016 {I3} keV, |G{-|g}=4.3 {I7} meV (1967Go18, tentative values) 


level_energy_unit: KEV
level_comment:
E$E(p)(lab)=1422.2 {I17}, E(level)=3241.1 {I20} (1993Il02, adjusted) 
E$E(p)(lab)=1422 2, E(level)=3241.1 17 (1993Il02, ORIGINAL) 
$(2J+1)|G{-p}|G{-|g}/|G=1.2 {I3} meV (1993Il02) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=1497.9 {I29} (weighted average of 1497.1 {I20}, 1494 {I4}, 1509 {I5}) 
$E(p)(lab)=1497.1 20 CALCULATED FROM E(level)=3314 2 (1988De03); E(p)(lab)=1497 2 (1988De03, ORIGINAL) 
$E(p)(lab)=1494 4, E(level)=3311 4 (1967Go18) 
$E(p)(lab)=1509 5, E(level)=3326 5 (1964St18) 
$E(p)(lab)=1494, E(level)=3311 (1961Ki08) 
J$from 1967Go18: 1/2-, 3/2- from L=1; the elastic scattering anomaly can Be fitted only for J|p=3/2- and |G=|G{-p}=2.2 {I3} keV thus excluding 1/2- 
J$from 1988De03: 1/2-, 3/2- from L=1; 3/2- from |DJ=1 |g to (1/2+), 1370 
J$from 1961Ki08: 1/2- from dispersion theory (single level approx.) 
T$2.2 {I3} keV (1967Go18); others: <3.0 keV (1964St18) 
L$from 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=62 {I8} meV (1967Go18) 
$|G{-p}=2.2 {I3} keV, |G{-|g}=15 {I2} meV (1967Go18) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$E(p)(lab)=1686 {I20}, E(level)=3498 {I19} (1967Go18, regarded as questionable); E(p)(lab)=1685, E(level)=3497 (1988De03, shown as coming from another reaction) 
$(2J+1)|G{-p}|G{-|g}/|G=16 {I6} meV (1967Go18) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=1815 {I15}, E(level)=3623 {I15} (1967Go18) 
$(2J+1)|G{-p}|G{-|g}/|G=28 {I6} meV (1967Go18) 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2042 {I10}, E(level)=3844 {I10} (1967Go18) 
$(2J+1)|G{-p}|G{-|g}/|G=42 {I12} meV (1967Go18) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=2163 {I15}, E(level)=3962 {I15} (1967Go18) 
T$10 {I4} keV (1967Go18) 
$|G{-p}=10 {I4} keV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=2203 {I4} (weighted average of 2199 {I10}, 2184 {I15}, 2206 {I5}) 
$E(p)(lab)=2199 10, E(level)=3997 10 (1970Th05) 
$E(p)(lab)=2184 15, E(level)=3982 15 (1967Go18) 
$E(p)(lab)=2206 5, E(level)=4004 5 (1964St18) 
T$35 keV (1964St18) 
L$from 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=140 {I42} meV (1967Go18, for unresolved 3982 and 3962 doublet) 
$|G{-p'}=35 keV (1967Go18 citing 1964St18) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
$E(p)(lab)=2333 {I15}, E(level)=4127 {I15} (1967Go18), denotes a pair of 
$According to 1967Go18, this energy denotes a pair of close levels 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=2491 {I20}, E(level)=4281 {I19} (1967Go18) 
$(2J+1)|G{-p}|G{-|g}/|G=46 {I24} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=2617.1 {I4} (weighted average of 2627.1 {I4}, 2631 {I5}) 
$E(p)(lab)=2627.1 4 FROM E(level)=4413.2 4 (1988De03); E(p)(lab)=2627.3 4 (1988De03, ORIGINAL) 
$E(p)(lab)=2631 5, E(level)=4417 5 (1967Go18) 
J$7/2 from |DJ=2 |g to 3/2+ g.s.; 7/2+ from RUL (1988De03) 
T$mean lifetime |t in fs: <3 (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=340 {I100} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=2647.0 {I5} (weighted average of 2647.0 {I5}, 2649 {I5}) 
$E(p)(lab)=2647.0 5, E(level)=4432.6 3 (1988De03, ADJUSTED) 
$E(p)(lab)=2647.2 5, E(level)=4432.4 3 (1988De03, ORIGINAL) 
$E(p)(lab)=2649 5, E(level)=4434 5 (1967Go18) 
J$|DJ=1 d(+Q) |g to (1/2+), 1371 
T$mean lifetime |t in fs: <5 (1988De03) 
$|G{-|g}/|G{-p'}=0.050 {I4} (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=226 milli-eV 68, 2J+1)|G{-p}|G{-p'}/|G=1.5 eV {I5} (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=2725 {I4} (weighted average of 2713 {I10}, 2740 {I20}, 2727 {I5}) 
$E(p)(lab)=2713 10, E(level)=4497 10 (1970Th05) 
$E(p)(lab)=2740 20, E(level)=4523 19 (1967Go18) 
$E(p)(lab)=2727 5, E(level)=4510 5 (1964St18) 
T$0.5 {I3} keV (1967Go18, reestimating data of 1964St18); 0.8 (1970Th05) 
L$from 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=58 {I46} meV (1967Go18) 
$|G{-p}=0.5 {I3} keV (1967Go18, reestimating data of 1964St18), |G{-|g}=29 {I23} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=2802 {I3} (weighted average of 2804 {I5}, 2800 {I10}, 2804 {I13}, 2800 {I5}) 
$E(p)(lab)=2804 5, E(level)=4585 5 (1988De03); E(level)=4586 5 (1988De03, ORIGINAL) 
$E(p)(lab)=2800 10, E(level)=4581 10 (1970Th05) 
$E(p)(lab)=2804 13, E(level)=4585 13 (1967Go18) 
$E(p)(lab)=2800 5, E(level)=4581 5 (1964St18) 
T$83 {I11} keV (1988De03); others: 90 keV (1964St18) 
L$from 1964St18 
$|G{-|g}/|G{-p'}<0.8 (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=1400 {I420} meV (1967Go18) 
$|G{-p}=90 keV (1967Go18 citing 1964St18), |G{-|g}=700 {I210} meV (1967Go18) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=2890.7 {I7} (weighted average of 2890.7 {I7}, 2893 {I15}, 2880 {I10}) 
$E(p)(lab)=2890.7 7, E(level)=4669.6 8 (1988De03, ADJUSTED) 
$E(p)(lab)=2890.4 6, E(level)=4669.9 7 (1988De03, ORIGINAL) 
$E(p)(lab)=2893 15, E(level)=4672 15 (1970Th05) 
$E(p)(lab)=2880 10, E(level)=4659 10 (1967Go18) 
$|G{-|g}/|G{-p'}=0.027 {I1} (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=106 {I40} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=2955.1 {I4} calculated from E(level)=4732.2 {I4} (1988De03); E(p)(lab)=2955.3 {I4} (1988De03, original) 
$E(p)(lab)=2944 10, E(level)=4721 10 (1967Go18) 
$|G{-|g}/|G{-p'}=0.24 {I1} (1988De03) 
J$from 1988De03: 7/2 from |DJ=2 |g to 3/2+, g.s.; 7/2+ based on RUL (1988De03) 
T$mean lifetime |t in fs: <6 (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=196 meV {I84}, (2J+1)|G{-p}|G{-p'}/|G=36 eV {I10} (1967Go18) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=2961.0 {I6} (weighted average of 2960.9 {I5}, 2960 {I10}, 2970 {I5}) 
$E(p)(lab)=2960.9 5, E(level)=4737.9 5 (1988De03); E(level)=4737.7 6 (1988De03, ORIGINAL) 
$E(p)(lab)=2960 10, E(level)=4737 10 (1970Th05) 
$E(p)(lab)=2970 5, E(level)=4747 5 (1964Va15) 
J$from 1964Va15: (p,p'|g(|q)) (they give A{-2}=+0.53 {I3}, A{-4}=-0.34 {I3} for 1970 {I30} |g ray from 2+ to g.s. in {+36}Ar) 
$|G{-|g}/|G{-p'}<0.0002 (1988De03) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=3040.0 {I8} (wt. Av of 3039.9 {I6}, 3039 {I10}, 3050 {I5}) 
$E(p)(lab)=3039.9 {I6}, E(level)=4814.7 {I6} (1988De03); E(level)=4814.5 {I6} (1988De03, original) 
$E(p)(lab)=3039 {I10}, E(level)=4814 {I10} (1970Th05) 
$E(p)(lab)=3050 {I5}, E(level)=4825 {I5} (1964Va15) 
$|G{-|g}/|G{-p'}<0.0002 (1988De03) 
J$from 1964Va15: (p,p'|g(|q)) (they give A{-2}=+0.56 {I2}, A{-4}=-0.56 {I2} for 1970 {I30} |g ray from 2+ to g.s. in {+36}Ar) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=3068.6 {I9} (weighted average of 3068.4 {I6}, 3068 {I10}, 3059 {I13}, 3081 {I5}) 
$E(p)(lab)=3068.4 6, E(level)=4842.5 6 (1988De03, ADJUSTED) 
$E(p)(lab)=3068.5 6, E(level)=4842.4 6 (1988De03, ORIGINAL) 
$E(p)(lab)=3068 10, E(level)=4842 10 (1970Th05) 
$E(p)(lab)=3059 13, E(level)=4833 13 (1967Go18) 
$E(p)(lab)=3081 5, E(level)=4855 5 (1964St18) 
J$from 1970Th05, 1964St18: 3/2+, 5/2+ from L=2 
T$0.20 {I8} keV (1967Go18, reestimating data of 1964St18), for J=3/2; multiply by 2/3 for J=5/2; 0.28 keV (1970Th05) 
L$from 1970Th05 and 1964St18 
$|G{-|g}/|G{-p'}=0.006 {I1} (1988De03) 
$(2J+1)|G{-p}|G{-|g}/|G=104 meV {I42}; (2J+1)|G{-p}|G{-p'}/|G=64 {I20} ev (1967Go18) 
$|G{-p}=0.20 {I8} keV (1967Go18, reestimating data of 1964St18), |G{-p'}=16 {I5} eV, |G{-|g}=26 {I11} meV (1967Go18); all values are for J=3/2 and should Be multiplied by 2/3 for J=5/2 (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=3249.8 {I11} (weighted average of 3249.6 {I6}, 3248 {I8}, 3250 {I10}, 3249 {I3}, 3269 {I5}) 
$E(p)(lab)=3249.6 6, E(level)=5018.7 6 (1988De03); E(level)=5018.5 6 (1988De03, ORIGINAL) 
$E(p)(lab)=3248 8, E(level)=5017 8 (1997Ka10) 
$E(p)(lab)=3250 10, E(level)=5019 10 (1970Th05) 
$E(p)(lab)=3249 3, E(level)=5018 3 (1967Go18) 
$E(p)(lab)=3269 5, E(level)=5038 5 (1964St18) 
J$3/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05,1964St18); in 1967Go18, the elastic scattering anomaly can Be fitted only for J|p=3/2+, |G=|G{-p}=600 eV {I150} and J|p=5/2+, |G=|G{-p}=400 eV {I100} 
T$1.3 {I1} keV (1997Ka10); 0.60 {I15} keV (1967Go18) for J=3/2; multiply by 2/3 for J=5/2; 0.60 keV (1970Th05); 4 keV (1964St18); adopted: 1.3 {I1} keV 
L$from 1970Th05 and 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=66 {I34} meV (1967Go18) 
$(2J+1)|G{-p}|G{-p'}/|G=3.2 {I12} ev (1967Go18) 
$|G{-p}=0.60 {I15} keV, |G{-p'}=1.6 {I3} eV, |G{-|g}=17 {I9} meV (1967Go18); all values are for J=3/2 and should Be multiplied by 2/3 for J=5/2 (1967Go18) 
$|G{-p}=1.3 {I1} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=3281.6 {I8} (weighted average of 3281.6 {I10}, 3284 {I2}, 3282 {I8}, 3278 {I3}, 3280 {I15}, 3280 {I3}) 
$E(p)(lab)=3281.6 10, E(level)=5049.8 12 (1988De03, ADJUSTED) 
$E(p)(lab)=3282.2 8, E(level)=5049.2 10 (1988De03, ORIGINAL) 
$E(p)(lab)=3284 2, E(level)=5052 2 (1997Ka10) 
$E(p)(lab)=3282 8, E(level)=5050 8 (1997Ka10) 
$E(p)(lab)=3278 3, E(level)=5046 3 (1976Ik03) 
$E(p)(lab)=3280 15, E(level)=5048 15 (1970Th05) 
$E(p)(lab)=3280 3, E(level)=5048 3 (1967Go18) 
J$in 1997Ka10,1992Wi13: 3/2+ from |s(|q) and analyzing power; in 1967Go18: the elastic scattering anomaly can Be fitted only for J|p=3/2+, |G=|G{-p}=40 {I20} eV and J|p=5/2+, |G=|G{-p}=27 {I13} eV, assuming L|<4 
T$0.048 {I11} keV (1997Ka10); 0.038 {I6} keV (1992Wi13); 0.04 {I2} keV (1967Go18); adopted weighted average: 0.040 {I5} keV for J=3/2; multiply by 2/3 for J=5/2; <0.6 keV (1970Th05) 
$(2J+1)|G{-p}|G{-|g}/|G=220 {I100} meV (1967Go18) 
$(2J+1)|G{-p}|G{-p'}/|G=1.6 {I6} ev (1967Go18) 
$|G{-p}=0.04 {I2} keV, |G{-p'}=0.42 {I14} eV, |G{-|g}=55 {I25} meV (1967Go18); all values are for J=3/2 and should Be multiplied by 2/3 for J=5/2 (1967Go18) 
$|G{-p}=0.048 keV {I11} (1997Ka10), 0.034 keV {I5} (1992Wi13) 
$|G{-|g}/|G{-p'}=0.07 {I2} (1988De03) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=3357 {I6} (weighted average of 3348 {I5}, 3350 {I10}, 3368 {I5}, 3340 {I20}) 
$E(p)(lab)=3348 5, E(level)=5114 5 (1967Go18) 
$E(p)(lab)=3350 10, E(level)=5116 10 (1970Th05) 
$E(p)(lab)=3368 5, E(level)=5134 5 (1964St18) 
$E(p)(lab)=3340 20, E(level)=5107 19 (1964Ar17) 
T$0.2 {I1} keV (1967Go18, reestimating data of 1964St18); <0.40 keV (1970Th05) 
L$from 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=100 {I60} meV (1967Go18) 
$|G{-p}=0.2 {I1} keV (1967Go18, reestimating data of 1964St18), |G{-|g}=50 {I30} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=3369 {I4} (weighted average of 3359 {I4}, 3362 {I10}, 3360 {I20}, 3375 {I5}, 3379 {I5}) 
$E(p)(lab)=3359 4, E(level)=5125 5 (1967Go18) 
$E(p)(lab)=3362 10, E(level)=5128 10 (1970Th05) 
$E(p)(lab)=3360 20, E(level)=5126 19 (1966Sk02) 
$E(p)(lab)=3375 5, E(level)=5141 5 (1964Va15) 
$E(p)(lab)=3379 5, E(level)=5145 5 (1964St18) 
J$from 1964Va15: (p,p'|g(|q)) (they give A{-2}=+0.15 {I1}, A{-4}=+0.41 {I1} for 1970 {I30} |g ray from 2+ to g.s. in {+36}Ar) 
T$0.5 {I2} keV (1967Go18, reestimating data of 1964St18); <0.70 keV (1970Th05) 
L$from 1970Th05 and 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=100 {I60} meV (1967Go18) 
$(2J+1)|G{-p}|G{-p'}/|G=708 {I106} ev (1967Go18) 
$|G{-p}=0.3 {I1} keV (1967Go18, reestimating data of 1964St18), |G{-p'}=200 {I110} eV, |G{-|g}=17 {I10} meV (1967Go18) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=3444 {I7} (weighted average of 3444 {I8}, 3442 {I15}) 
$E(p)(lab)=3444 8, E(level)=5208 8 (1967Go18) 
$E(p)(lab)=3442 15, E(level)=5206 15 (1970Th05) 
$(2J+1)|G{-p}|G{-|g}/|G=360 {I160} meV (1967Go18) 
$(2J+1)|G{-p}|G{-p'}/|G=6 {I4} ev (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3502 {I4} (weighted average of 3496 {I5}, 3496 {I10}, 3490 {I20}, 3511 {I5}, 3480 {I20}) 
$E(p)(lab)=3496 5, E(level)=5258 5 (1967Go18) 
$E(p)(lab)=3496 10, E(level)=5258 10 (1970Th05) 
$E(p)(lab)=3490 20, E(level)=5253 19 (1966Sk02) 
$E(p)(lab)=3511 5, E(level)=5273 5 (1964St18) 
$E(p)(lab)=3480 20, E(level)=5243 19 (1964Ar17) 
J$from L=1 (1964St18) and (p,p'|g(|q)) (1967Go18) 
T$18 keV (1970Th05); 17 keV (1964St18) 
L$from 1964St18 
$(2J+1)|G{-p}|G{-|g}/|G=278 {I120} meV (1967Go18) 
$(2J+1)|G{-p}|G{-p'}/|G=632 {I100} ev (1967Go18) 
$|G{-p}=17 keV (1967Go18 citing 1964St18), |G{-p'}=158 {I25} eV, |G{-|g}= 70 {I30} meV (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3558 {I5} (weighted average of 3558 {I6}, 3561 {I10}, 3560 {I20}, 3540 {I20}) 
$E(p)(lab)=3558 6, E(level)=5319 6 (1967Go18) 
$E(p)(lab)=3561 10, E(level)=5322 10 (1970Th05) 
$E(p)(lab)=3560 20, E(level)=5321 19 (1966Sk02) 
$E(p)(lab)=3540 20, E(level)=5301 19 (1964Ar17) 
J$from 1970Th05: 3/2+, 5/2+ from L=2 
$(2J+1)|G{-p}|G{-|g}/|G=96 {I48} meV (1967Go18) 
$(2J+1)|G{-p}|G{-p'}/|G=400 {I120} ev (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3582 {I6} (weighted average of 3580 {I9}, 3585 {I10}, 3580 {I20}) 
$E(p)(lab)=3580 9, E(level)=5340 9 (1967Go18) 
$E(p)(lab)=3585 10, E(level)=5345 10 (1970Th05) 
$E(p)(lab)=3580 20, E(level)=5340 19 (1966Sk02) 
J$from 1970Th05: 5/2-, 7/2- from L=3 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3660 {I5} (weighted average of 3658 {I6}, 3665 {I10}, 3670 {I20}) 
$E(p)(lab)=3658 6, E(level)=5416 6 (1967Go18) 
$E(p)(lab)=3665 10, E(level)=5423 10 (1970Th05) 
$E(p)(lab)=3670 20, E(level)=5428 19 (1966Sk02) 
J$from 1970Th05: 3/2+, 5/2+ from L=2 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3694 {I5} (weighted average of 3693 {I6}, 3696 {I10}) 
$E(p)(lab)=3693 6, E(level)=5450 6 (1967Go18) 
$E(p)(lab)=3696 10, E(level)=5453 10 (1970Th05) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3713 {I5} (weighted average of 3713 {I6}, 3714 {I10}, 3710 {I20}) 
$E(p)(lab)=3713 6, E(level)=5469 6 (1967Go18) 
$E(p)(lab)=3714 10, E(level)=5470 10 (1970Th05) 
$E(p)(lab)=3710 20, E(level)=5467 19 (1966Sk02) 
J$from 1970Th05: 3/2+, 5/2+ from L=2 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3811 {I7} (weighted average of 3815 {I10}, 3816 {I15}, 3810 {I20}, 3790 {I20}) 
$E(p)(lab)=3815 10, E(level)=5569 10 (1970Th05) 
$E(p)(lab)=3816 15, E(level)=5570 15 (1967Go18) 
$E(p)(lab)=3810 20, E(level)=5564 19 (1966Sk02) 
$E(p)(lab)=3790 20, E(level)=5544 19 (1964Ar17) 
J$from 1970Th05: 5/2-, 7/2- from L=3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=3968 {I9} (weighted average of 3970 {I10}, 3960 {I20}) 
$E(p)(lab)=3970 10, E(level)=5719 10 (1970Th05) 
$E(p)(lab)=3960 20, E(level)=5710 19 (1966Sk02) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=3987 {I9} (weighted average of 3989 {I10}, 3980 {I20}) 
$E(p)(lab)=3989 10, E(level)=5738 10 (1970Th05) 
$E(p)(lab)=3980 20, E(level)=5729 19 (1966Sk02) 
J$from 1970Th05: 5/2-, 7/2- from L=3 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4038 {I6} (weighted average of 4034 {I8}, 4042 {I10}, 4030 {I20}, 4060 {I20}) 
$E(p)(lab)=4034 8, E(level)=5782 8 (1997Ka10) 
$E(p)(lab)=4042 10, E(level)=5789 10 (1970Th05) 
$E(p)(lab)=4030 20, E(level)=5778 19 (1966Sk02) 
$E(p)(lab)=4060 20, E(level)=5807 19 (1964Ar17) 
J$3/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05) 
T$2.7 {I5} keV (1997Ka10); 0.8 keV (1970Th05) 
$|G{-p}=2.3 {I5} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4185 {I6} (weighted average of 4181 {I8}, 4192 {I10}, 4184 {I20}) 
$E(p)(lab)=4181 8, E(level)=5925 8 (1997Ka10) 
$E(p)(lab)=4192 10, E(level)=5935 10 (1970Th05) 
$E(p)(lab)=4184 20, E(level)=5928 19 (1967Go18) 
J$5/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05) 
T$11.4 {I23} keV (1997Ka10); 12 keV (1970Th05) 
$|G{-p}=11.0 {I22} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4275 {I6} (weighted average of 4274 {I8}, 4277 {I10}, 4270 {I20}) 
$E(p)(lab)=4274 8, E(level)=6015 8 (1997Ka10) 
$E(p)(lab)=4277 10, E(level)=6018 10 (1970Th05) 
$E(p)(lab)=4270 20, E(level)=6011 19 (1966Sk02) 
J$5/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05) 
T$6.7 {I13} keV (1997Ka10); 10 keV (1970Th05) 
$|G{-p}=5.0 {I10} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=4305 {I9} (weighted average of 4306 {I10}, 4300 {I20}) 
$E(p)(lab)=4306 10, E(level)=6046 10 (1970Th05) 
$E(p)(lab)=4300 20, E(level)=6040 19 (1966Sk02) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=4372 {I9} (weighted average of 4373 {I10}, 4370 {I20}) 
$E(p)(lab)=4373 10, E(level)=6111 10 (1970Th05) 
$E(p)(lab)=4370 20, E(level)=6109 19 (1966Sk02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=4388 {I9} (weighted average of 4387 {I10}, 4390 {I20}) 
$E(p)(lab)=4387 10, E(level)=6125 10 (1970Th05) 
$E(p)(lab)=4390 20, E(level)=6128 19 (1966Sk02) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=4487 {I9} (weighted average of 4489 {I10}, 4480 {I20}) 
$E(p)(lab)=4489 10, E(level)=6224 10 (1970Th05) 
$E(p)(lab)=4480 20, E(level)=6216 19 (1966Sk02) 
J$from 1970Th05: 3/2+, 5/2+ from L=2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=4541 {I9} (weighted average of 4541 {I10}, 4540 {I20}) 
$E(p)(lab)=4541 10, E(level)=6275 10 (1970Th05) 
$E(p)(lab)=4540 20, E(level)=6274 19 (1966Sk02) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4589 {I6} (weighted average of 4586 {I8}, 4593 {I10}) 
$E(p)(lab)=4586 8, E(level)=6319 8 (1997Ka10) 
$E(p)(lab)=4593 10, E(level)=6325 10 (1970Th05) 
J$5/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05) 
T$2.3 {I5} keV (1997Ka10); 3.0 keV (1970Th05) 
$|G{-p}=2.0 {I4} keV (1997Ka10) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E(p)(lab)=4613 {I9} (weighted average of 4614 {I10}, 4610 {I20}) 
$E(p)(lab)=4614 10, E(level)=6346 10 (1970Th05) 
$E(p)(lab)=4610 20, E(level)=6342 19 (1966Sk02) 


level_energy_unit: KEV
level_spin_parity: 5/2-,7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=4723 {I9} (weighted average of 4724 {I10}, 4720 {I20}) 
$E(p)(lab)=4724 10, E(level)=6453 10 (1970Th05) 
$E(p)(lab)=4720 20, E(level)=6449 19 (1966Sk02) 
J$from 1970Th05: 5/2-, 7/2- from L=3 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=4807 {I9} (weighted average of 4809 {I10}, 4800 {I20}) 
$E(p)(lab)=4809 10, E(level)=6536 10 (1970Th05) 
$E(p)(lab)=4800 20, E(level)=6527 19 (1966Sk02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4877 {I6} (weighted average of 4873 {I8}, 4882 {I10}) 
$E(p)(lab)=4873 8, E(level)=6598 8 (1997Ka10) 
$E(p)(lab)=4882 10, E(level)=6607 10 (1970Th05) 
J$3/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05) 
T$4.9 {I10} keV (1997Ka10); 1.2 keV (1970Th05) 
$|G{-p}=4.5 {I9} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4895 {I6} (weighted average of 4890 {I8}, 4901 {I10}, 4900 {I20}) 
$E(p)(lab)=4890 8, E(level)=6614 8 (1997Ka10) 
$E(p)(lab)=4901 10, E(level)=6625 10 (1970Th05) 
$E(p)(lab)=4900 20, E(level)=6624 19 (1966Sk02) 
J$5/2+ from |s(|q) and analyzing power (1997Ka10); 3/2+, 5/2+ from L=2 (1970Th05) 
T$2.9 {I6} keV (1997Ka10); 0.5 keV (1970Th05) 
$|G{-p}=1.1 {I2} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4902 {I6} (weighted average of 4898 {I8}, 4907 {I10}) 
$E(p)(lab)=4898 8, E(level)=6622 8 (1997Ka10) 
$E(p)(lab)=4907 10, E(level)=6631 10 (1970Th05) 
J$5/2- from |s(|q) and analyzing power (1997Ka10); 5/2-, 7/2- from L=3 (1970Th05) 
T$5.9 {I12} keV (1997Ka10); 0.3 keV (1970Th05) 
$|G{-p}=1.4 {I3} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=4963.2 {I19} (weighted average of 4963 {I2}, 4967 {I10}, 4965 {I15}) 
$E(p)(lab)=4963 2, E(level)=6685 2 (1970Th05) 
$E(p)(lab)=4967 10, E(level)=6689 10 (1970Th05) 
$E(p)(lab)=4965 15, E(level)=6687 15 (1967Go18) 
J$from 1992Wi13: 1/2+ from |s(|q) and analyzing power 
T$2.75 {I11} keV (1992Wi13); <0.6 keV (1970Th05) 
$|G{-p}=555 {I320} eV (1992Wi13) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5149 {I8} (weighted average of 5150 {I10}, 5147 {I15}) 
$E(p)(lab)=5150 10, E(level)=6867 10 (1970Th05) 
$E(p)(lab)=5147 15, E(level)=6864 15 (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5261 {I9} (weighted average of 5262 {I10}, 5259 {I20}) 
$E(p)(lab)=5262 10, E(level)=6976 10 (1970Th05) 
$E(p)(lab)=5259 20, E(level)=6973 19 (1967Go18) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=5471 {I8}, E(level)=7180 {I8} (1997Ka10) 
J$from 1997Ka10: 5/2+ from |s(|q) and analyzing power 
$|G{-p}=1.8 {I4} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=5523 {I8}, E(level)=7230 {I8} (1997Ka10) 
J$from 1997Ka10: 3/2+ from |s(|q) and analyzing power 
$|G{-p}=5.3 {I11} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p)(lab)=5655 {I8}, E(level)=7359 {I8} (1997Ka10) 
J$from 1997Ka10: 5/2+ from |s(|q) and analyzing power 
$|G{-p}=13.8 {I28} keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5771 {I8}, E(level)=7471 {I8} (1997Ka10) 
J$from 1997Ka10: 5/2+ from |s(|q) and analyzing power 
$|G{-p}=5.3 keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5795 {I8}, E(level)=7495 {I8} (1997Ka10) 
J$from 1997Ka10: 7/2- from |s(|q) and analyzing power 
$|G{-p}=0.1 keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5828 {I7} (weighted average of 5830 {I8}, 5818 {I20}) 
$E(p)(lab)=5830 8, E(level)=7529 8 (1997Ka10) 
$E(p)(lab)=5818 20, E(level)=7517 19 (1967Go18) 
J$from 1997Ka10: 3/2+ from |s(|q) and analyzing power 
$|G{-p}=4.2 keV (1997Ka10) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5942 {I8}, E(level)=7638 {I8} (1997Ka10) 
J$from 1997Ka10: 5/2+ from |s(|q) and analyzing power 
$|G{-p}=6.8 keV (1997Ka10) 
$ 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(lab)=5962 {I8}, E(level)=7657 {I8} (1997Ka10) 
J$from 1997Ka10: 3/2+ from |s(|q) and analyzing power 
$|G{-p}=1.9 keV (1997Ka10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2)+
level_comment:
E$from 1971Li34 and 1967Go18; other: 2280 (1980Ro01); also observed by 1995Ma36 (citing E(level) of 1998En04) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
E$from 1980Ro01, 1971Li34, and 1967Go18; also observed by 1995Ma36 (citing E(level) of 1998En04) 
$|G{-|g}/|G{-p}=0.52 {I23} (1995Ma36) 


level_energy_unit: KEV
level_comment:
E$other: 2970 (1971Li34) 
J$(9/2-) assumed by 1995Ma36 from analog of 3185 in {+37}Ar 
$|G{-|g}/|G{-p}>9 (1995Ma36) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)
level_comment:
E$from 1971Li34; also observed by 1995Ma36 (citing E(level) of 1998En04) 
$|G{-|g}/|G{-p}=0.41 {I14} (1995Ma36) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
T$measured by 2014Sh25. Both the statistical and systematic uncertainties are included, and discussed in detail in the paper. 
$The new half-life gives {Ift}=4605 s {I8}, F|t=4605.4 s {I82} (2014Sh25) or log| {Ift}=3.6632 {I8} for 3/2+ to 3/2+ (g.s. to g.s.) |b transition with a branching ratio of 97.99% {I14} adopted from a previous review 
$Deduced V{-ud}=0.981 {I+12-10} (2014Sh25) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d<r{+2}>({+47}K,{+37}K)=-0.163 fm{+2} {I40}(stat) {I199}(syst) (2014Kr04) for |d|n({+39}K,{+37}K)=-265 MHz {I4} from literature 
J$spin from fitting of hyperfine structure (2014Kr04) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from Adopted Levels of {+37}K in ENSDF database 
$Mean square charge radius |d<r{+2}>({+39}K,{+37}K)=-0.08 fm{+2} {I2}(stat) {I6}(syst) (2015Ro12) 
$Isotope shift |d|n({+39}K,{+37}K)=-264 MHz {I2}(stat) {I3}(syst) from weighted average of -264 Mhz {I3} reported by D.M. Rossi et al. (Rev. Sci. Instrum. 85, 093503 (2014)); and -265 Mhz {I4} in 1997Be35 (Phys. Rev. Lett. 79, 375 (1997)) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d|n{+39,37}=-264 MHz {I6}, |d<r{+2}>{+39,37}=-0.11 fm{+2} {I6} (stat) {I3} (syst) 
$R{-ch}=3.419 fm {I8} (stat) {I4} (syst) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: MIN
level_comment:
J$spin from atomic-beam magnetic resonance (1965Ph02) and fitting of hyperfine structure (2014Pa45,2014Kr04); parity from L({+3}He,|a)=L(d,t)=L(p,d)=2 from 3/2+ 
T$unweighted average of 7.67 min {I3} (1957Cl23), 7.67 min {I5} (1965Bo42), 7.70 min {I2} (1965Eb01), 7.60 min {I4} (1967Va27), and 7.613 min {I11} (1970Re13). Others: 7.4 min {I9} (2000Le02); 7.4 m {I13} (1968Ka15); 6.5 m {I15} (1965Ph02); 7.0 m {I10}, Nucl. Phys. 41, 364 (1963); 7.7 m {I3} (1956Gr07); Phys. Rev. 72, 639 (1947); 7.7 m {I1} (1937Ri01); 7.7 m {I1} (1937Hu01). 
MOMM1$atomic beam method (1982To02). Other: +1.3735 {I10} (1965Ph02), +1.3711 {I69} (2014Pa45). See also 2014StZZ compilation 
$<r{+2}>{+1/2}=3.426 fm {I5} (2013An02 evaluation) 
$Adopted (1977En02) neutron pickup spectroscopic factor (S)=2.0 {I3} for L=2 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M1
level_comment:
J$L({+3}He,t)=L(p,{+3}He)=0 from 0+; superallowed |b transition from 0+; analog of g.s. of {+38}Ar and {+38}Ca 
T$924.41 ms {I21} from average of 929.2 ms {I35} (1972Ha82), 925.6 ms {I7} (1975Sq01), 922.3 ms {I11} (1976Wi08), 921.71 ms {I65} (1978Wi04), 928.8 ms {I20} (1978Th02), 924.15 ms {I31} (1983Ko22), 924.4 ms {I6} (2000Bb01), 924.46 ms {I14} (2010Ba43), using the Normalised Residual Method (NRM) with a reduced |h{+2}=2.9, and weighted average gives 924.35 {I25} with a reduced |h{+2}=4.4. The evaluator has adopted 924.4 ms {I3} by considering results from both methods. Others (in ms): 948 {I10} (1961Ja22); 938 {I8} (1960Ja12); 944 {I12} (1960Li05); 970 {I7} (Nucl. Phys. 7, 296 (1958)); 951 {I7} (1957Cl23); 1954Kl36; Phys. Rev. 92, 1076 (1953). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_comment:
J$L(pol d,|a)=2 and analyzing power; 328.1|g |DJ=1 to 0+ 
T$from Recoil Distance Method (RDM) in ({+16}O,pn|g). Others: <35 ps from (|a,n|g), >2.8 ps from (d,|a|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor (S)=0.39 {I7} for L=2; 0.19 {I5} for L=0 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$L(d,|a)=L(p,{+3}He)=0+2 from 0+; unnatural parity from (pol d,|a); 1567.4|g |DJ=1 to 0+ 
T$from DSAM, weighted average of 37 fs {I17} from ({+3}He,|a|g) and 52 fs {I10} from (d,|a|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor (S)=0.72 {I10} for L=2; 0.04 {I2} for L=0 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,d)=L(d,t)=0+2 from 3/2+; natural parity from (pol d,|a); J=2 from |g(|q) in (d,|a|g) 
T$from DSAM, weighted average of 37 ps {I17} from ({+3}He,|a|g) and 63 fs {I15} (d,|a|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(p,d)=3 from 3/2+ and natural parity from (pol d,|a) gives 1-,3-,5-; 2613.0|g to 3+ and RUL rules out 1- and 5- 


level_energy_unit: KEV
level_spin_parity: (4)-
level_lifetime_unit: NS
level_comment:
J$L(p,d)=3 from 3/2+ and unnatural parity from (pol d,|a) gives 2-,4-; 4- is supported by J|p=(7)+ assignment for 3458 level; but 2- is supported by L(p,{+3}He)=1+3 from 0+ and L(d,t)=1 from 3/2+ for the 2613+2646 doublet and is not completely ruled out 
T$from |g(t) in ({+16}O,pn|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
J$L(p,d)=1+3 from 3/2+ and natural parity from (pol d,|a) gives 1-,3-,5-; 2697.9|g to 0+ and RUL rules out 3- and 5-. But L({+3}He,t)=(2,4) from 0+ is inconsistent. 


level_energy_unit: KEV
level_spin_parity: (1+,2-,3+)
level_lifetime_unit: PS
level_comment:
J$unnatural parity from (pol d,|a); J=1,2,3 from |g(|q) in (d,|a|g); L(p,{+3}He)=0+2 or 1+3 suggests 1+,2- 


level_energy_unit: KEV
level_spin_parity: (6)-
level_lifetime_unit: PS
level_comment:
J$|DJ=2, E2 |g to (4)-. J|p=4- if J(2646)=2- is not completely ruled out 
T$from RDM in ({+16}O,pn|g) 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
J$L(|a,d)=6 for a 3445 {I50} group is consistent with 3458 level rather than 3431 level and gives J|p=5+,6+,7+; unnatural parity from (pol d,|a) rules out 6+; J=7 is favored by measured magnetic moment and shell-model predictions. J=5 (for J(2646)=2) is not completely ruled out 
T$from timing in pulsed beam method using reaction {+24}Mg({+16}O,np|g) (1980Jo11). Other: 22.3 |ms {I4} (1983Va05), 22.5 |ms {I6} (1974Ya04), and 22.1 |ms {I7} (1974Va13) in ({+16}O,np|g), 22.1 |ms {I7} (1975Io01) in (|a,n|g) 
MOMM1$from g-factor=+0.548 {I2} measured using TDPAD method (1974Io01). |m=+2.740 {I10} if J(3458)=5. 


level_energy_unit: KEV
level_spin_parity: (3,5)-
level_lifetime_unit: PS
level_comment:
J$L(p,d)=3 from 3/2+; J=(3,5) from |g(|q) in ({+3}He,p|g) if J(2646)=4; possible natural parity from (pol d,|a). But 1086.3|g from (1+,2+) disfavors 5- 


level_energy_unit: KEV
level_spin_parity: (3)
level_lifetime_unit: PS
level_comment:
J$3690|g to 3+, 1074.3|g to 3- and RUL gives J=(2,3,4); J=(3,5) from |g(|q) in ({+3}He,p|g) if J(2646)=4. Note that J(2646)=2 is not completely ruled out. 


level_energy_unit: KEV
level_spin_parity: (1+:5+)
level_comment:
E$from 1975Co09 in ({+3}He,p|g). 1975Co09 also report 3738.9 {I17} from (d,|a) measurement 
J$3739|g to 3+ 


level_energy_unit: KEV
level_comment:
E$weighted average of 3840 {I3} from ({+3}He,p|g), 3842 {I4} from (p,d), and 3841.2 {I17} from (d,|a),(pol d,|a). 
J$unnatural parity from (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,t)=L({+3}He,|a)=L(p,d)=0+2 from 3/2+; L(d,|a)=L(p,{+3}He)=0+2 from 0+; unnatural parity from (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
E$weighted average of 4175.4 {I18} from ({+3}He,p|g), 4176 {I3} from (p,d), and 4173.8 {I20} from (d,|a),(pol d,|a). 
J$L(p,d)=0+2 from 3/2+; weak |b feeding (log| {Ift}=5.3) from 0+ 


level_energy_unit: KEV
level_spin_parity: (1+:5+)
level_comment:
E$weighted average of 4317 {I3} from ({+3}He,p|g), 4321 {I4} from (p,d), and 4318.0 {I21} from (d,|a),(pol d,|a). 
J$4318|g to 3+ 


level_energy_unit: KEV
level_spin_parity: (0-:4-)
level_lifetime_unit: PS
level_comment:
E$weighted average of 4331.0 {I15} from ({+3}He,p|g) and (d,|a|g), 4338 {I4} from (p,d), and 4336.7 {I21} from (d,|a),(pol d,|a). 
J$402|g to 2- 


level_energy_unit: KEV
level_spin_parity: (1+:5+)
level_comment:
E$weighted average of 4394.3 {I24} from ({+3}He,p|g) and 4395.0 {I21} from (d,|a),(pol d,|a). 
J$4394|g to 3+ 


level_energy_unit: KEV
level_spin_parity: (0:3+)
level_comment:
E$weighted average of 4409.2 {I13} from ({+3}He,p|g), 4405 {I4} from (p,d), and 4412.2 {I22} from (d,|a),(pol d,|a). 
J$2712|g to 1+ 


level_energy_unit: KEV
level_spin_parity: (1:5)-
level_comment:
E$weighted average of 4646 {I4} from (p,d) and 4639.0 {I22} from (d,|a),(pol d,|a). 
J$L(d,t)=3 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
J$L({+3}He,|a)=L(p,d)=0+2 from 3/2+ 
E$weighted average of 4662 {I15} from ({+3}He,|a), and 4664 {I3} from (d,|a),(pol d,|a), 4673 {I3} from (p,d) and 4671 {I11} from (p,{+3}He). 


level_energy_unit: KEV
level_spin_parity: (0:3+)
level_comment:
E$weighted average of 4724.4 {I19} from ({+3}He,p|g) and 4718 {I3} from (d,|a),(pol d,|a). 
J$1382|g to 1+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 4988.7 {I15} from ({+3}He,p|g), 4998 {I4} from (p,d), and 4990 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=0+2 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (1:5)-
level_comment:
E$weighted average of 5047.5 {I14} from ({+3}He,p|g) and 5049 {I3} from (d,|a),(pol d,|a). Other: 5058 {I4} from (p,d) 
J$L(p,d)=3 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (0+:4+)
level_comment:
E$weighted average of 5133.8 {I15} from ({+3}He,p|g), and 5131.3 {I23} from (d,|a),(pol d,|a) 
J$2732|g to 2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5234 {I15} from ({+3}He,|a), 5249 {I5} from (p,d) and 5257 {I3} from (d,|a),(pol d,|a) 
J$L(p,d)=L({+3}He,|a)=0+2 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
E$others: 5440 {I10} from ({+3}He,|a), 5449 {I4} from (p,d) could correspond to 5439 or 5459 in (d,|a),(pol d,|a) 
J$L({+3}He,|a)=2(+0) from 3/2+; L(p,d)=2+0 from 3/2+ for 5439 or 5459 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5626 {I4} from (p,d), and 5617 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=0+2 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_comment:
E$weighted average of 5680 {I5} from (p,d) and 5676 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=(1+3) from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5737 {I4} from (p,d) and 5730 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=2+0 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5809 {I6} from (p,d) and 5810 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=0+2 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5856 {I5} from (p,d), and 5851 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=2+0 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5976 {I5} from (p,d) and 5970 {I3} from (d,|a),(pol d,|a). 
J$L(p,d)=0+2 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
E$weighted average of 5991 {I5} from (p,d) and 5983 {I4} from (d,|a),(pol d,|a). 
J$L(p,d)=2+0 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: (7)+
level_lifetime_unit: US
level_lifetime_info: ;ISO=M2
level_comment:
T$from |g(t) in 1980Jo11. Others: 22.3 |ms {I4} (1983Va05), 22.5 |ms {I6} (1974Ya04), 22.1 |ms {I7} (1974Va13) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from 1977De02. Others: 0.10 ns {I6} (quoted by 1977De02 from thesis of 1973GoZQ), 0.51 ns {I11} (1971En02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$d|s/d|W=0.2 
$ B(>){-pn}=0.010 {I5} (1996An09) 
S$at 12|', 0.05 at 0|' 
$DWIA fit is poor for 1+ mainly due to the weakness of 460 peak. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=10 
$ B(>){-pn}=1.73 {I25} (1996An09), 1.63 {I9} (2002Or05) 
$ d|s/d|W=0.91 mb/sr (2002Or05) 


level_energy_unit: KEV
level_spin_parity: (7)+
level_comment:
$d|s/d|W=5.0 
E$this peak will be unresolved from 3400 and 3900 structure reported by 1996An09, thus its existence is considered as suspect by the evaluator 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$d|s/d|W=2.3 
$ B(>){-pn}=0.43 {I7} (1996An09) 
E$quadruplet, mostly 1+ states with some higher spin states 


level_energy_unit: KEV
level_comment:
E,L$L=1 gives J=1-,2-,3-; but J=4-,2- assignment in Adopted Levels. L=1 here is probably contributed partly by 2613, 3- level 


level_energy_unit: KEV
level_comment:
E$130 {I30} (1972Ro10), 138 {I10} (1972Fe06), 129 {I10} (1966Bl04) 
$Analog of g.s. of {+38}Ar and {+38}Ca 
S$others: 0.32 (1972Fe06), 0.31 {I14} (1966Bl04) 


level_energy_unit: KEV
level_comment:
E$450 {I30} (1972Ro10), 466 {I10} (1972Fe06), 458 {I15} (1966Bl04 
S$others: 0.19, 0.22 (1972Fe06); <0.06, 0.32 {I9} (1966Bl04) 


level_energy_unit: KEV
level_comment:
E$1700 {I30} (1972Ro10), 1700 {I15} (1972Fe06), 1704 {I15} (1966Bl04) 
S$others: 0.56, <0.05 (1972Fe06); 0.51 {I13}, <0.08 (1966Bl04) 


level_energy_unit: KEV
level_comment:
E$2400 {I30} (1972Ro10), 2400 {I10} (1972Fe06), 2405 {I15} (1966Bl04) 
S$others: 1.1, 0.27 (1972Fe06); 1.08 {I21}, <0.1 (1966Bl04). For J=2, S<0.3 for L=0; 4.4 or 3.1 for L=2 (1973Ro18) 


level_energy_unit: KEV
level_comment:
E$2640 {I30} (1972Ro10), 2630 {I10} (1972Fe06), 2655 {I15} (1966Bl04) 
E,L$L=1+3 (1972Fe06); 1 (1972Ro10). L=1 gives J=1-,2-,3- and L=1+3 gives J=2-; but J=4-,2- assignment in Adopted Levels. L=1 or 1+3 here is probably contributed partly by 2613, 3- level 
S$from 1972Fe06. Other: 0.14 for L=1 (1972Ro10) 


level_energy_unit: KEV
level_comment:
E$3440 {I30} (1972Ro10), 3420 {I10} (1972Fe06) 
L$according to 1972Fe06, L=0 is dominant 
S$others: 0.51, 0.07 (1972Fe06). For J=2, S=0.46 or 0.40 for L=0; 0.19 or 0.17 for L=2 (1973Ro18) 


level_energy_unit: KEV
level_comment:
E$5250 {I30} (1972Ro10), 5230 {I15} (1972Fe06) 
L$according to 1972Fe06, L=0 is dominant 
S$other: 0.18, 0.0 (1972Fe06) 


level_energy_unit: KEV
level_spin_parity: (4)-
level_comment:
E,L$L=1+3 gives J=2-; but (4)- assignment in Adopted Levels L=1+3 here is probably contributed partly by 2613, 3- level. Also (p,{+3}He) transfer process does not provide a strong argument for J|p assignments 
S$for L=1; 0.21 {I12} for L=3 


level_energy_unit: KEV
level_spin_parity: (1+,2-,3+)
level_comment:
S$for L=0+2, S=0.018 {I4} for L=0, 0.340 {I9} for L=2. For L=1+3, S=0.015 {I12} for L=1, 0.30 {I9} for L=3 


level_energy_unit: KEV
level_spin_parity: (2-,3+)
level_comment:
J$from L(p,{+3}He). J|p=(1+,2,3+) in Adopted Levels 
S$for L=1+3, S=0.0033 {I9} for L=1, 0.021 {I4} for L=3. For L=2+4, S=0.043 {I15} for L=2, 0.48 {I18} for L=4. For pure L=4, S=0.49 {I7} 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3+)
level_comment:
L$|s(|q) distribution inconsistent with L=6, J|p=7+ 
S$for L=2; 0.031 {I20} for L=0. For pure L=2, S=0.23 {I3} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$from 1977StZB. Others: 1963Ja14, 1965Is04, 1967He16, 1971Kr03 and 1974Sm02 
J$from Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
L$0+2 (1974Fr10), 2 (1971Su05,1977StZB) 
E$other: 1700 {I2} (1977StZB) 
$ <T{-20}>=+0.47 {I7} (1976Pe11) 


level_energy_unit: KEV
level_spin_parity: 4-,2-
level_comment:
J$(2,4)- (1976Pe11); L=1+3 (1983Bh05) gives 2- but with FWHM=135 keV, the 2646 peak in this work is not resolved from 2613, 3- level; also L=3 in 1971Su05 and L=(3) in 1977StZB 
E$other: 2647 {I2} (1977StZB) 
$ <T{-20}>=-1.05 {I13} (1976Pe11) 


level_energy_unit: KEV
level_spin_parity: 0-
level_comment:
E$other: 2994 {I4} (1977StZB) 
J$ from <T{-20}>(180|')=-1.08 {I9} (5.9 MeV), -0.98 {I5} (6.1 MeV), -1.03 {I3} (6.4 MeV), -1.00 {I5} (6.6 MeV) (1976Ri05). Other: <T{-20}>(3|')=-1.35 {I22} (7.5-8.0 MeV) (1976Pe11) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$1 from 328|g(|q); 1- gives an unacceptable solution based on substate population (1972Ha15) 
T$from 1973Ha56 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$1 from 1567|g(|q); 1- gives an unacceptable solution based on substate population (1972Ha15) 
T$weighted average of 76 fs {I20} (2007Pr03), 57 fs {I24} (1975Co09) and 45 fs {I10} (1973Ha56) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$1,2 from 1942|g(|q); J=1 is rejected by 2271|g(|q) (1972Ha15) 
T$weighted average of 66 fs {I15} (2007Pr03), 53 fs {I35} (1975Co09) and 62 fs {I17} (1973Ha56) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
T$weighted average of 317 fs {I44} (2007Pr03), 142 fs {I+45-38} (1975Co09) and 194 fs {I49} (1973Ha56) 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: FS
level_comment:
J$0,1 from |g(|q) (1972Ha15) 
T$weighted average of 90 fs {I28} (2007Pr03) and 152 fs {I35} (1973Ha56) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$1,3 from |g(|q) (1972Ha15) 
T$weighted average of 111 fs {I35} (2007Pr03) and 66 fs {I38} (1975Co09). Other: <104 fs (1973Ha56) 
$|g's to g.s., 2613 and 2646 shown by 1973Ha56 and 1972Ha15 are, instead, from 3688 level according to 1975Co09 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$population from 1978Ba35; yield/100 |p{+-} captures |?5 
L$from opening-angle distributions and recoil momentum distributions 


level_energy_unit: KEV
level_comment:
$Isotope shift=-983.8 MHz {I4}(stat){I18}(syst), |d<r{+2}>=-0.146 fm{+2} {I4}(stat){I16}(syst), with respect to {+47}K (2019Ko19) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$|d|n{+39,38}=-126.1 MHz {I19}, |d<r{+2}>{+39,38}=-0.075 fm{+2} {I18} (stat) {I14} (syst) 
$R{-ch}=3.4241 fm {I26} (stat) {I20} (syst) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$|d<r{+2}>=-0.089 fm{+2} {I25} with uncertainty deduced by quadratic addition of statistical uncertainty of 0.009 and systematic uncertainty of 0.023 relative to {+39}K (2014Bi10). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d<r{+2}>=0.011 fm{+2} {I25} with uncertainty deduced by quadratic addition of statistical uncertainty of 0.010 and systematic uncertainty of 0.023 relative to {+39}K (2014Bi10). 
$|d<r{+2}>=0.100 fm{+2} {I6} with uncertainty deduced by quadratic addition of statistical uncertainty of 0.005 and systematic uncertainty of 0.003 relative to {+38g}K (2014Bi10). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
J$optical spectroscopy (1937Ja02), atomic beam (1935Mi08), hyperfine structure (2014Pa45, 2014Kr04); L(p,t)=0 from 3/2+; L(pol d,{+3}He)=2 and L-1/2 from analyzing power; also L({+3}He,d)=L(d,n)=L(t,|a)=2 from 0+ 
$Experimental nuclear charge radius <r{+2}>{+1/2}=3.4349 fm {I19} (2013An02, evaluation) 
MOMM1$from atomic beam (1974Be50). Others: +0.2917 {I13} (2014Pa45, hyperfine structure), +0.39147 {I3} (1993Du08, atomic-beam laser spectroscopy), +0.39150731 {I12} (NMR, 1974Sa24 and 1974Sa25), 0.391427 {I27} (1973CoZB), 1983Ob03, 1973Ti03, 1972Ro40, 1972Za10, 1970ChYV, 1969Zi01, 0.39147 {I3} (NMR, 1968Br16), 1957Ka07, 1957Ri37, 1955Br11, 1954Br09, 1952Ei09, 1950Oc01, 1950Co65, 1939Ku10, 1937Ja02, 1937To04, 1935Mi08. Compilation: 2014StZZ 
MOME2$optical level crossing method (measured value of +0.057 {I4} by 1968Sc09, re-evaluated by 1998Ke05). Other re-evaluations of 1968Sc09 measurement: +0.0601 {I15} (1993Su36), +0.049 {I4} (1971St12, 1989Ra17). Compilation: 2016St14. Others: +0.059 {I6} (1971Sv02), 0.056 {I3} (1970Sc33), +0.053 {I8} (atomic beam, 1968Sp03), 1972Jo09, 1971Ch61, 1970Fi17, 1969Ne03, 1967Ba64, 1967Da04, 1964Ya03, 1963Ma42, 1962Ko22, 1961Fo11, 1960Bl15, 1957Bu19, 1957Ri37 
$Adopted (1977En02) proton stripping spectroscopic factor=1.0 {I2} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
J$L(d,n)=L({+3}He,d)=L(p,|a)=L(d,{+3}He)=L(t,|a)=0 from 0+; also L(d,d')=L(|a,|a')=L(p,t)=2 from 3/2+ 
T$weighted average of 64 fs {I9} from ({+39}K,|a|g), 62 fs {I21} from (|a,p|g), 59 fs {I14} from (p,|g):resonances, 64 fs {I6} from (n,n'|g), 57 fs {I12} from (p,p'|g) 
$B(E2)|^ from (e,e'). Other: 0.0034 from (|a,|a') 
$Adopted (1977En02) proton pick-up spectroscopic factor=3.3 {I4} 
$Adopted (1977En02) proton stripping spectroscopic factor=0.08 {I2} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$L(d,n)=L({+3}He,d)=L(p,|a)=L(d,{+3}He)=L(t,|a)=3 from 0+ and 2814.24|g M2+E3 to 3/2+; also L(d,d')=L(|a,|a')=L(p,t)=3 from 3/2+ 
T$weighted average of 56 ps {I6} from ({+35}Cl,d|g), 43 ps {I4} from ({+28}Si,|ap|g), 48 ps {I6} from ({+18}O,2np|g), 44 ps {I7} from (|a,p|g) and 49.2 ps {I35} from (p,p'|g) 
MOMM1$time-dependent recoil into gas method in heavy-ion reaction (1981Le19). Compilation: 2014StZZ 
$B(E3)|^ from (e,e'). Other: 0.00086 from (|a,|a') 
$Adopted (1977En02) proton pick-up spectroscopic factor=0.88 {I12} 
$Adopted (1977En02) proton stripping spectroscopic factor=0.48 {I12} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$L(d,n)=L({+3}He,d)=L(d,{+3}He)=1 from 0+; 3018.8|g E1(+M2) to 3/2+; J=3/2 from |g(|q,pol) in (|a,p|g) 
T$weighted average of 14 fs {I3} from ({+39}K,|a|g), 15.2 fs {I35} from (p,|g):resonances, 17 fs {I6} from (p,p'|g). Other: 15 fs {I3} from |G=0.030 eV {I5} from (|g,|g') 
$B(E3)|^ from (e,e'). Other: 0.00186 from (|a,|a') 
$Adopted (1977En02) proton pick-up spectroscopic factor=0.10 {I5} 
$Adopted (1977En02) proton stripping spectroscopic factor=0.02 {I1} 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
J$L(d,d')=L(|a,|a')=L(p,t)=3 from 3/2+; 783.36|g M1+E2 to 7/2- and 3597.25|g E3 to 3/2+; L(p,|a)=5 from 0+. But L(t,|a)=(2) is inconsistent with 9/2- 
T$weighted average of 41 ps {I3} from ({+35}Cl,d|g), 35 ps {I3} from ({+28}Si,|ap|g), 34 ps {I4} from ({+18}O,2np|g), 42 ps {I6} from (|a,p|g). Other: 63 ps {I19} from (p,p'|g) 
MOMM1$time-dependent recoil into gas method in heavy-ion reaction (1981Le19). Compilation: 2014StZZ 
$B(E3)|^ from (e,e'). Other: 0.00517 from (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
J$L(d,d')=L(|a,|a')=L(p,t)=3 from 3/2+; 3883.0|g E1(+M2) to 3/2+; J=5/2 from |g(|q,pol) in (|a,p|g). But L(d,{+3}He)=1 and L(t,|a)=(2) are inconsistent with 5/2- 
T$weighted average of 8 fs {I4} from ({+39}K,|a|g), 14 fs {I5} from (|a,p|g), 6.2 fs {I14} from (p,|g):resonances, 18 fs {I7} from (n,n'|g), and 15 fs {I8} from (p,p'|g). Other: 7.2 fs {I+14-10} from |G=0.063 eV {I10} from (|g,|g') 
$B(E3)|^=0.0066 {I7} from (e,e') for 3883+3939 doublet. Other: 0.00336 from (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=0(+2) from 3/2+; 1416.2|g M1+E2 to 1/2+; J=3/2 from |g(|q,pol) in (|a,p|g) 
T$weighted average of 87 fs {I21} from (|a,p|g) and 66 fs {I14} from (p,p'|g). Other: 23 fs {I+5-8} from |G=0.020 eV {I5} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$L(p,|a)=5 from 0+; 1129.93|g E2 to 7/2- and 346.72|g M1(+E2) to 9/2-. Also L(d,d')=L(|a,|a')=5 from 3/2+; L(d,|a)=4 from 7/2- 
T$weighted average of 7.9 ps {I11} from ({+28}Si,|ap|g) and 9.0 ps {I10} from ({+18}O,2np|g). Others: >4.2 ps from (|a,p|g), 0.83 ps {I29} from (p,p'|g) is discrepant. 
$B(E5)|^ from (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$L({+3}He,d)=L(d,n)=1 from 0+; J=3/2 from |g(|q,pol) in (|a,p|g) 
T$weighted average of 14 fs {I7} from (|a,p|g), 50 fs {I30} from (n,n'|g), 13 fs {I+26-9} from (p,|g):resonances and 35 fs {I10} from (p,p'|g). Other: 23 fs {I+12-6} from |G=0.020 eV {I7} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
J$L(d,{+3}He)=0 from 0+ 
T$weighted average of 80 fs {I21} from (|a,p|g), 62 fs {I50} from (n,n'|g), 55 fs {I10} from (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$L(d,d')=L(|a,|a')=L(p,t)=3 from 3/2+; J=7/2 from |g(|q,pol) in (|a,p|g) 
T$weighted average of 59 fs {I14} from (|a,p|g), 59 fs {I35} from (n,n'|g), 37 fs {I10} from (p,p'|g). 
$B(E3)|^=0.0076 {I10} from (e,e') for triplet of 4082, 4095, and 4126. Other: 0.00331 from (|a,|a') 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=1 from 0+. 877|g to 9/2- and 1660|g to 7/2- observed only in (p,p'|g) would rule out 1/2- but these placements are uncertain. 
T$weighted average of 0.243 ps {I21} from (n,n'|g) and 0.15 ps {I6} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$4514.0|g M1+E2 to 3/2+; 3586|g from the proton-unbound level at 8100 with J=9/2. But L(d,{+3}He)=(3) is inconsistent with 5/2+ 
T$weighted average of 17 fs {I7} from (|a,p|g) and 28 fs {I14} from (p,p'|g). Other: 29 fs {I+10-6} from |G=0.016 eV {I4} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
J$923.0|g M1 to 9/2-, 576.20|g M1(+E2) to 11/2- and 393.9|g M1(+E2) to 7/2-; also L(p,|a)=5 from 0+; L(p,t)=5 from 3/2+; L(d,|a)=4 from 7/2- 
T$weighted average of 0.20 ps {I5} from (|a,p|g), 0.12 ps {I3} from (p,p'|g) and 76 fs {I17} from (n,n'|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$L({+3}He,d)=3 from 0+; 1864.5|g and 552.44|g M1+E2 to 7/2-; J=7/2 from |g(|q,pol) in (|a,p|g). But L(p,t)=0(+2) is inconsistent 
T$weighted average of 111 fs {I28} from (|a,p|g) and 76 fs {I21} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$4737.9|g E2(+M1) to 3/2+; 3361|g from the proton-unbound level at 8100 with J=9/2; L(|a,|a')=2 
T$weighted average of 21 fs {I6} from (|a,p|g) and 24 fs {I7} from (p,p'|g). Other: 27 fs {I+30-9} from |G=0.017 eV {I9} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=0 from 3/2+; 4931.4|g M1+E2 to 3/2+ and 2407.4|g M1+E2 to 1/2+. But L(d,n)=1 from 0+ for unresolved 4928+5010 doublet is inconsistent. 
T$other: 64 fs {I17} from (p,p'|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$883.08|g M1(+E2) to 7/2-; 7/2 from |g(|q,pol) in (|a,p|g) 
T$other: 0.42 ps {I+17-10} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-,7/2-)
level_lifetime_unit: FS
level_comment:
J$from |g(|q) in (|a,p|g) and RUL. L(d,n)=1 for a 4928+5010 unresolved doublet suggests 1/2-,3/2-; which may correspond to a different or to the 5010.9 level 
T$other: <35 fs from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,{+3}He)=L(p,|a)=L(p,t)=L(t,|a)=2 and L+1/2 transfer from analyzing power. But L(|a,|a')=3 and L(e,e')=(3) from 3/2+ is inconsistent 
T$deduced from |G=0.35 eV {I3} in (|g,|g'). Others: 14 fs {I7} from (p,p'|g), <14 fs from (|a,p|g), <3.5 fs from (p,|g):resonances. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=0. But L(|a,|a')=L(e,e')=(3) is inconsistent and 5/2+ from ({+7}Li,{+8}Be) 
T$deduced from |G=0.33 eV {I3} in (|g,|g'). Others: <14 fs from (|a,p|g), <28 fs from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: FS
level_comment:
J$from |g(|q,pol) in (|a,p|g) and ({+28}Si,|ap|g) (also DCO). 
T$weighted average of 60 fs {I40} from (|a,p|g) and 113 fs {I35} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (3/2:9/2)-
level_comment:
E$from (t,|a), considered as a separate level from the 5354, 11/2- level since J|p=11/2- would require L(t,|a)=5 
J$L(|a,|a')=3 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$L(pol d,{+3}He)=L(t,|a)=2 and L+1/2 transfer from analyzing power. 
T$deduced from |G=0.23 eV {I2} from (|g,|g'). Others: 14 fs {I7} from (|a,p|g), <14 fs from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in (|a,p|g); also L({+3}He,d)=3 from 0+ 
T$other: 0.67 ps {I+42-21} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in (|a,p|g), ({+18}O,2np|g) and ({+28}Si,|ap|g) (also DCO). Also L(|a,|a')=5 from 3/2+; L(d,|a)=4 from 7/2- 
T$other: <2.1 ps from ({+28}Si,|ap|g) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)+
level_lifetime_unit: FS
level_comment:
E$5787.6 {I10} from (p,p'|g) 
J$5788.4|g to 3/2+, 2310|g from proton-unbound level at 8100 with J|p=9/2+, |g(|q) in (p,|g); negative parity is ruled out by RUL. 
T$weighted average of 35 fs {I17} from (|a,p|g) and 28 fs {I14} from (p,p'|g). Other: (2J+1)|*(0.82 {I12}) fs from (2J+1)|*|G/4=0.140 eV {I20} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$2987.3|g and 1676|g to 7/2-, 1280.7|g and 637.5|g to 9/2-, 2292|g from proton-unbound level at 8094 with J|p=3/2-; L(p,t)=3+5 implies 7/2-,9/2-. 
T$other: >0.52 ps from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$weighted average of 5827.0 {I10} from (p,|g):resonances and 5825.6 {I10} from (p,p'|g) 
J$L({+3}He,d)=L(d,{+3}He)=1 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
E$from (p,p'|g) 
J$L(|a,|a')=L(p,t)=3 from 3/2+; 2203|g from proton-unbound 8094, 3/2-; 1371|g and 727|g to 9/2- 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
E$5936.9 {I10} from (p,p'|g) 
J$L(d,{+3}He)=2 from 3/2+; J=5/2 from |g(|q) in (|a,p|g). But L(p,t)=3 is inconsistent 
T$deduced from |G=0.173 eV {I20} in (|g,|g'). Others: <24 fs from (|a,p|g), <14 fs from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (1/2+:7/2+)
level_lifetime_unit: FS
level_comment:
E$from (p,p'|g) 
J$6041|g to 3/2+, 1527|g to 5/2+, |g to 3/2+; L(p,t)=(0+2) from 3/2+ for a group at 6050 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$from (p,|g):resonances. The evaluator has considered this level as a separate level from the 6248.5 level in (|a,p|g) and (p,p'|g) based on non-observation of the 6246|g in the latter. It is also possible that the level in (p,|g):resonances is a doublet because of the observations of the same |g branches as from the 6248.5 level. 
J$L(d,{+3}He)=0 from 0+ for a group at 6263 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
E$See comments for 6246 level. 6244.0 {I10} from (p,p'|g) 
J$(3/2- to 11/2-) from 3434.2|g and 1568.2|g to 7/2- 
T$from (p,p'|g). Other: <35 fs from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E$from (p,p'|g). Others: 6331.6 {I20} from (|a,p|g), 6332 {I2} from (|g,|g') 
J$L(p,t)=0 from 3/2+ 
T$others: <55 fs from (p,p'|g), 0.178 fs {I14} deduced from |G=2.56 eV {I20} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: FS
level_comment:
J$from |g(|q,pol) in (|a,p|g) and ({+28}Si,|ap|g) (also DCO) 
T$other: <7 ns from |g|g(t) in ({+28}Si,|ap|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:
J$L(p,t)=2 from 3/2+; 6458|g to 3/2+; RUL 
T$other: (2J+1)(0.9 {I2}) fs from (2J+1)|*|G/4=0.14 eV {I3} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in (|a,p|g), ({+18}O,2np|g), ({+18}O,|a2n|g), and ({+28}Si,|ap|g) (also DCO) 
T$weighted average of 8.3 ps {I4} from ({+28}Si,|ap|g) and 11.8 ps {I21} from ({+18}O,|a2n|g). Other: >4.2 ps from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_lifetime_unit: FS
level_comment:
J$L(d,{+3}He)=2 from 0+ for a group at 6500 
T$other: (2J+1)(1.0 {I3}) fs from (2J+1)|*|G/4=0.11 eV {I3} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2+)
level_lifetime_unit: PS
level_comment:
J$|g to 3/2+; L(t,|a)=(1) suggests (1/2-,3/2-) for 6500 {I20} group 
T$other:(2J+1)(0.42 {I8}) fs from (2J+1)|*|G/4=0.27 eV {I5} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,{+3}He)=(2) from 0+ 
T$other: (2J+1)(0.60 {I12}) fs from (2J+1)|*|G/4=0.19 eV {I4} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2)
level_comment:
E$from (p,p'|g) 
J$L(d,{+3}He)=(3) suggests (5/2-,7/2-) for 7170 and/or 7200 levels; |g to 3/2+ disfavors 7/2- 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
E$from (p,|g):resonances, 7631.9 {I22} from E|g fit. 
J$5110|g to 1/2+ and 4819|g to 7/2-. See also comment for 7588 level 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E$possible doublet in (p,|g):resonances. 
J$2395|g to 3/2+, 4695|g to 3/2- and 2550|g to 9/2-; but (5/2-) is disfavored by 3620|g to 1/2+ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$7738.8 {I5} from (p,|g):resonances. 
J$3/2 from |g(|q) in (p,|g); L(d,n)=1 for a group at 7720 {I20} 
T$proton width from (p,|g):resonances. 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
E$two levels near this energy suggested in (|a,p|g) (1981No05), but there is no evidence for a doublet in other (HI,xn|g) studies such as in 1982VaZH in ({+28}Si,|ap|g). Only one level is included here with 1301|g and 1341|g from the same level 
J$1341.7|g stretched E2 to 13/2+, 1301.18|g M1+E2 to 15/2+ 
T$weighted average of 2.3 ps {I12} from ({+28}Si,|ap|g) and 0.94 ps {I28} from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
E$possible doublet in (p,|g):resonances. 
J$5274|g to 1/2+, 4983|g to 7/2-; but 3277|g to 9/2- favors 5/2-; possible doublet suggested in (p,|g):resonances. See also comment for 7756 level 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
E$possible doublet in (p,|g):resonances 
J$5324|g and 3751|g to 1/2+, 3963|g to 5/2- and 3332|g to 5/2+ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$5/2 from |g(|q) in (p,|g):resonances; negative parity is ruled out by RUL since it would require an unreasonably large M2 strength for 7867|g, estimated based on the large mixing ratio and resonance strength in (p,|g):resonances. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
E$from (p,|g):resonances. 7978.7 {I21} from E|g fit 
J$7978|g to 3/2+, 4960|g to 3/2- and 5164|g to 7/2-. L(d,{+3}He)=3 gives 5/2-,7/2- for a 8004 {I30} group 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
J$1653|g to 3/2+, 4964|g to 3/2-, 3469|g to 5/2+, 4100|g to 5/2-, 1737|g to (1/2+). See also comment for 7979 level 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
J$886.64|g stretched E2 to 15/2- and 252.10|g E1 to 17/2+ 
T$weighted average of 13.7 ps {I7} from ({+28}Si,|ap|g), 13.9 ps {I10} from ({+18}O,|a2n|g). 
MOMM1$transient-field method in heavy-ion fusion reaction (1992Pa01). Compilation: 2014StZZ 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$3/2 from |g(|q) in 1986Zi02 in (p,|g):resonances; 1547|g, 2203|g, 2591|g, 3083|g, 3967|g, 5279|g to 7/2-; positive parity would require an unreasonably large B(M2) for the 1547|g to 7/2- 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
J$3/2 and 9/2 from |g(|q) in 1986Zi02 in (p,|g):resonances; 4155|g to 11/2- rules out 3/2; J=9/2 implies l{-p}=4 or 5 proton capture with l{-p}=4 favored due to an improbably high value of reduced proton width for l{-p}=5 deduced using the resonance strength in 1970Ma31; negative parity would also require an unreasonably large B(M2) for the 3355|g to 5/2+. 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2+)
level_comment:
E$from (p,|g):resonances, 8253.9 {I20} from E|g fit. 
J$8253|g to 3/2+ 
$T{-1/2}=(2J+1)(0.13 {I3}) fs from (2J+1)|*|G/4=0.90 eV {I22} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (1/2:7/2+)
level_comment:
J$8390|g to 3/2+. L(d,{+3}He)=2 gives 3/2+,5/2+ for a 8411 {I30} group 
$T{-1/2}=(2J+1)(0.41 {I10}) fs from (2J+1)|*|G/4=0.28 eV {I7} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
J$8530|g to 3/2+, 5512|g to 3/2- and 5716|g to 7/2-. L(d,{+3}He)=2 gives 3/2+,5/2+ for a 8534 {I30} group 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of 4083.0 {I4} (1970Ma31) and 4082.1 {I11} (1970An19) 
J$3/2 from 3655|g(|q) from the level at 7739, J|p=3/2- in 1970Ma31 
T$from 1970Ma31 (tentative result) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J$7/2 and 11/2 from |g(|q) of 3973|g from the level at 8099, J|p=9/2(+) in 1986Zi02; 11/2 is excluded by the primary transition of 3976|g from the level at 8093, J|p=3/2- 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.54 {I17} 
$E(p)=1285.2 {I6}; also 1284 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.29 {I10} 
$E(p)=1368.5 {I8}, possible doublet; also 1368 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.6 {I5} 
E$weighted average of 7739.1 {I5} from |g cascade in 1970Ma31, and 7738.1 {I7} from 1970An19 
$E(p)=1393.4 {I6}; also 1392.6 {I7} (1970An19), 1394.3 {I10} (1970Ma31), 1394 {I2} (1974Ke10) 
J$3/2- from |s(|q) in (p,p) for 1394 proton resonance (1974Ke10); J=3/2 from |g(|q) in 1970Ma31 
T$|G=|G{-p} from 1974Ke10. Other: T{-1/2}<2.8 fs (1970An19) 
S$other: 2.7 eV {I8} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.27 {I6} 
$E(p)=1411.0 {I8}; also 1411 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.29 {I8} 
$E(p)=1428.6 {I8}; also 1427 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.87 {I23} 
$E(p)=1453.7 {I8}; also 1453 {I2} (1970Ma31), who suggests a possible doublet 
J$5/2- from 1984Ha27 is inconsistent 
S$other: 0.8 eV {I4} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.41 {I10} 
$E(p)=1477.6 {I8}; also 1477 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.60 {I19} 
$E(p)=1504.4 {I12}, possible doublet; also 1504 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.76 {I20} 
$E(p)=1526.3 {I10}; also 1527 {I2} (1970Ma31) 
J$from |g(|q) in 1986Zi02; 3/2-,5/2,(7/2+) in 1984Ha27; negative parity is ruled out by RUL 
S$other: 0.80 eV {I24} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.78 {I20} 
$E(p)=1618.4 {I8}; also 1620 {I2} (1970Ma31) 
S$other: 0.11 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.50 {I12} 
$E(p)=1639.7 {I8}; also 1640 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.0 {I4} 
J$(3/2,5/2) from 1984Ha27 
$E(p)=1644.6 {I8}; also 1644 {I2} (1970Ma31) 
S$other: 1.0 eV {I5} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.93 {I21} 
$E(p)=1653.8 {I8}; also 1654 {I2} (1970Ma31) 
J$3/2 from |g(|q) in 1986Zi02; 3/2-,5/2+ in 1984Ha27 
S$other: 0.9 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.50 {I12} 
$E(p)=1693.5 {I8}; 1695 {I2} (1970Ma31), probably 1693.5+1696.5 (evaluator) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.21 {I6} 
$E(p)=1696.5 {I10}; also 1695 {I2} (1970Ma31) 
S$other: 0.7 eV {I2} (1970Ma31) probably 1693.5+1696.5 (evaluators) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.3 {I4} 
$E(p)=1701.2 {I8}; also 1701 {I2} (1970Ma31) 
S$other: 1.9 eV {I6} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.52 {I25} 
J$(3/2-,5/2) from 1984Ha27 
$E(p)=1745.3 {I12}; also 1745 {I2} (1970Ma31) 
S$other: 1.9 eV {I6} (1970Ma31) probably 1743.4+1745.3 (evaluators) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.54 {I14} 
$E(p)=1757.4 {I10}; also 1757 {I2} (1970Ma31) 
J$3/2 from |g(|q) in 1986Zi02, positive parity would require an unreasonably large B(M2) for the 1547|g to 7/2-. Other: 3/2-,5/2+ in 1984Ha27 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.35 {I12} 
$E(p)=1763.5 {I10}; also 1763 {I2} (1970Ma31) 
J$3/2 and 9/2 from |g(|q) in 1986Zi02; 4155|g to 11/2- rules out 3/2; J=9/2 implies l{-p}=4 or 5 proton capture with l{-p}=4 favored due to an improbably high value of reduced proton width for l{-p}=5 deduced using the resonance strength in 1970Ma31; negative parity would require an unreasonably large B(M2) for the 3355|g to 5/2+. Other: 7/2-,(9/2+) in 1984Ha27 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.27 {I14} 
$E(p)=1772.3 {I10}, possible doublet; also 1773 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 
J$(1/2-,3/2,5/3+) in 1984Ha27 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.87 {I21} 
$E(p)=1782.8 {I8}; also 1782 {I2} (1970Ma31) 
S$other: 1.1 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.19 {I6} 
$E(p)=1803.7 {I10}; also 1802 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.52 {I17} 
$E(p)=1855.9 {I10}; also 1857 {I2} (1970Ma31), a triplet of 1854.7 {I3}, 1855.8 {I3} and 1857.3 {I3} is reported in 1986Zi02. 
S$other: 1.0 eV {I3} (1970Ma31) probably 1855.9+1858.0 (evaluators) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.2 {I4} 
$E(p)=1865.2 {I10}; also 1865 {I2} (1970Ma31) 
S$other: 1.4 eV {I5} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.7 {I9} 
$E(p)=1921.2 {I8}; also 1921 {I2} (1970Ma31) 
S$other: 3.0 eV {I10} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.4 {I5} 
$E(p)=1931.0 {I10}; also 1930 {I2} (1970Ma31) 
S$other: 1.2 eV {I6} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.37 {I12} 
$E(p)=1948.8 {I10}; also 1949 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.47 {I16} 
$E(p)=1963.7 {I10}; also 1964 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.9 {I3} 
$E(p)=1974.7 {I10}; also 1974 {I2} (1970Ma31) 
S$other: 1.2 eV {I6} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.62 {I21} 
$E(p)=2011.6 {I10}; also 2011 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.37 {I12} 
$E(p)=2017.9 {I10}; also 2017 {I2} (1970Ma31) 
S$other: 0.6 eV {I3} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.39 {I12} 
$E(p)=2051.5 {I10}; also 2051 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.1 {I4} 
$E(p)=2058.3 {I10}, also 2057 {I2} (1970Ma31) 
S$other: 1.2 eV {I6} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.52 {I17} 
$E(p)=2067.5 {I15}, possible doublet; also 2064 {I2} (1970Ma31) 
S$other: 0.8 eV {I4} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.2 {I4} 
$E(p)=2086.7 {I12}; also 2087 {I2} (1970Ma31) 
S$other: 1.2 eV {I6} (1970Ma31) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.37 {I12} 
$E(p)=2100.0 {I12}; also 2100 {I2} (1970Ma31) 
S$other: 1.0 eV {I5} (1970Ma31) probably 2100.0+2102.8 (evaluators) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.47 {I17} 
$E(p)=2139.6 {I12}; also 2140 {I2} (1970Ma31) 
S$other: 0.40 eV {I20} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.1 {I4} 
$E(p)=2206.4 {I12}; also 2205 {I2} (1970Ma31) 
S$other: 0.8 eV {I4} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=1.6 {I5} 
$E(p)=2261.0 {I13}; also 2259 {I2} (1970Ma31) 
S$other: 1.6 eV {I8} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2+)
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.62 {I21} 
$E(p)=2303.3 {I15}, possible doublet; also 2303 {I2} (1970Ma31) 
S$other: 2.0 eV {I10} (1970Ma31) probably 2303.3+2305.4 (evaluators) 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.58 {I20} 
$E(p)=2317.1 {I15}; also 2316 {I2} (1970Ma31) 
S$other: 0.8 eV {I4} (1970Ma31) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
BE2$weighted average of 0.00210 {I11} (1985De02), 0.00189 {I18} (1981Gr04) and 0.0022 {I5} (1970Pe03), with all values extracted from DWBA analysis. 
BM1$weighted average of 0.014 {I6} (1985De02) and 0.015 {I6} (1981Gr04). Note that 1985De02 and 1981Gr04 deduced B(M1) from measured B(E2) using the adopted T{-1/2}=52 fs {I14} at that time, while the currently adopted T{-1/2}=63 fs {I6}. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 2521.9 {I5} (1974Du01), 2522.2 {I6} (1986St02), 2522.3 {I6} (1969Ro15) 
T$weighted average of 53 fs {I12} (1986St02), 49 fs {I13} (1974Du01), 61 fs {I12} (1971Ta10), 73 fs {I22} (1969Ro15) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
E$weighted average of 2813.9 {I7} (1986St02) and 2813.9 {I4} (1969Ro15) 
T$from 1974Hu09. Others: >4.2 ps (1969Ro15), |<78 ps (1969Go04), <55 ps (1970Ho26), >0.7 ps (1971Ta10) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of 3018.6 {I5} (1974Du01), 3019.3 {I7} (1986St02), and 3019.5 {I5} (1969Ro15) 
T$weighted average of 35 fs {I14} (1986St02), 12 fs {I6} (1974Du01), 28 fs {I15} (1971Ta10). Other: <37 fs (1969Ro15) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of 3883.1 {I5} (1974Du01) and 3882.8 {I8} (1986St02) 
T$weighted average of 13 fs {I8} (1986St02) and 19 fs {I14} (1971Ta10). Other: <21 fs (1974Du01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of 3938.9 {I5} (1974Du01) and 3939.0 {I8} (1986St02) 
T$weighted average of 66 fs {I19} (1986St02), 62 fs {I14} (1974Du01), 71 fs {I21} (1971Ta10) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
E$weighted average of 3942.7 {I5} (1974Du01) and 3942.4 {I9} (1986St02) 
J$1968Lo03 propose 5/2,7/2 for a single level near 3940 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of 4082.5 {I5} (1974Du01) and 4082.8 {I8} (1986St02) 
T$weighted average of 37 fs {I14} (1986St02), 30 fs {I10} (1974Du01), 54 fs {I26} (1971Ta10) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
E$weighted average of 4125.8 {I5} (1974Du01) and 4126.7 {I9} (1986St02) 
T$weighted average of 40 fs {I21} (1986St02) and 31 fs {I10} (1974Du01). Other: 69 fs {I+29-26} (1971Ta10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|b{-L}{+p}=0.105 {I7} 
$|b{-2}: for real coupling; complex coupling gives 0.067 {I7}, but poor fit (1972El06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_comment:
E$separation energy=10.9|*10{+3} {I7} (1976Na20), 11.2|*10{+3} {I3} (1976Mo17) 
$2s orbital in 1976Mo17, but 1d{-3/2} orbital in 1976Na20 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_comment:
E$separation energy=14.4|*10{+3} {I3} (1976Na20), 14.9|*10{+3} {I8} (1976Mo17) 
$1d orbital in 1976Mo17, but 2s{-1/2} orbital (1976Na20) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_comment:
E$separation energy=35|*10{+3} {I1} (1976Na20), 41|*10{+3} (1976Mo17) 
$1p orbital (1976Na20,1976Mo17) 


level_energy_unit: KEV
level_comment:
E$separation energy=8.3|*10{+3} 
$1d{-3/2} orbital 
$Relative to IPSM: S=0.78 {I13} (without subtraction of background) 
S$ statistical uncertainty of 0.06 is included 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$separation energy=10.9|*10{+3} 
$2s{-1/2} orbital 
S$ statistical uncertainty of 0.03 is included 
$Relative to IPSM: S=0.60 {I10} (background subtracted) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$separation energy=10.9|*10{+3} 
$1f{-7/2} orbital 
S$ statistical uncertainty of 0.04 is included 
$Relative to IPSM: S=0.097 {I17} (without subtraction of background) 


level_energy_unit: KEV
level_energy_info: ;ERR=GT;ERR=?
level_comment:
E$separation energy>12|*10{+3} 
$1d{-5/2} orbital 
$Relative to IPSM: S=0.94 {I17} (without subtraction of background) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$separation energy=30.0|*10{+3} {I4}, statistical uncertainty of 0.3 MeV is included; 29.8|*10{+3} {I1} for 1p{-1/2} orbital with |G=8.5 MeV {I11} and 34.7|*10{+3} {I3} for 1p{-3/2} orbital with |G=9.4 MeV {I12} from 1990Vo13. 
$1p orbital 
T$ statistical uncertainty of 0.9 is included 
$Relative to IPSM: S=0.49 {I10} (background subtracted) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$separation energy=49.6|*10{+3} {I6}, statistical uncertainty of 0.6 MeV is included; 53.6|*10{+3} {I3} with |G=18.8 MeV {I14} from 1990Vo13. 
$1s{-1/2} orbital 
T$ statistical uncertainty of 0.9 is included 
$Relative to IPSM: S=0.78 {I14} (background subtracted) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from analyzing powers in 1987Me01, 1978Co13, 1977Be70 
S$others: 3.70 (1976Do05), 3.8 (1976Fr22), 3.6 (1969Do04), 3.93 (1968Ga13), 3.53 (1967Hi06), 3.8 (1962Cu07) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$weighted average of 2520 {I10} (1981De19) and 2520 {I15} (1976Do05). Note that 2550 in Table 1 of 1981De19 is a misprint. 
J$from analyzing powers in 1978Co13 
S$others: 1.0 (1978Co13), 1.65 (1976Do05), 1.1 (1969Do04), 1.35 (1967Hi06), 0.67 (1962Cu07) 


level_energy_unit: KEV
level_comment:
E$weighted average of 2813 {I10} (1981De19) and 2820 {I15} (1976Do05). 
S$for 1f{-7/2}. Other: 0.58 (1976Do05) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4090 {I30} (1981De19) and 4100 {I15} (1976Do05). 
S$others: <0.10 (1976Do05), 0.7 (1969Do04), 0.12 (1967Hi06) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 5258 {I10} (1981De19) and 5270 {I15} (1976Do05). 
S$others: 0.91 (1976Do05), 1.52 (1969Do04), 0.98 (1967Hi06) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 5595 {I10} (1981De19) and 5610 {I15} (1976Do05). 
S$others: 0.64 (1976Do05), 0.66 (1967Hi06) 


level_energy_unit: KEV
level_comment:
E$weighted average of 5943 {I10} (1981De19) and 5940 {I15} (1976Do05). 
S$for d{-3/2} 
L,S$other: L=1, C{+2}S=0.03 (1976Do05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 6328 {I15} (1981De19) and 6340 {I15} (1976Do05). 
S$others: 1.25 (1976Do05), 1.49 (1969Do04), 1.31 (1967Hi06) 


level_energy_unit: KEV
level_comment:
E$weighted average of 7191 {I25} (1981De19) and 7200 {I30} (1976Do05). 
S$for 1f{-5/2} 
L,S$other: L=2, C{+2}S=0.1 (1976Do05) 


level_energy_unit: KEV
level_comment:
E$weighted average of 8017 {I30} (1981De19) and 7900 {I30} (1976Do05). 
S$for 1f{-5/2} 
L,S$other: L=1, C{+2}S=0.01 for 2p{-3/2}, 0.2 for 1p{-1/2} (1976Do05) 


level_energy_unit: KEV
level_comment:
E$weighted average of 8204 {I30} (1981De19) and 8170 {I30} (1976Do05). 
S$others: 0.35 (1976Do05), 0.56 (1967Hi06) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$C{+2}S=3.9 
S$others: 1985Wi18 in ({+9}Be,{+10}B); 1984Ma06 in ({+10}B,{+11}C); 1980Ma31, 1980Gl07 in ({+11}B,{+12}C); 1980Ma31, 1979Bo13 in ({+13}C,{+14}N); 1984Ma06, 1980Dr09 in ({+14}C,{+15}N); 1979Bo13 in ({+14}N,{+15}O); 1979Bo13, 1978Ku10 in ({+15}N,{+16}O). Others: ({+37}Cl,{+38}Ar) (1997Wi17); ({+18}O,{+19}F) (1982Re14,1972Si02) 
$d|s/d|W (at 20|')=6 mb/sr (1980Dr09) 
$ ORIGIN OF OTHER C2S VALUES NEEDS TO BE CHECKED ?? 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$C{+2}S=0.71 
S$others: 1985Wi18 in ({+9}Be,{+10}B); 1984Ma06 in ({+10}B,{+11}C); 1980Ma31, 1980Gl07 in ({+11}B,{+12}C); 1980Ma31, 1979Bo13 in ({+13}C,{+14}N); 1984Ma06, 1980Dr09 in ({+14}C,{+15}N); 1979Bo13 in ({+14}N,{+15}O); 1979Bo13, 1978Ku10 in ({+15}N,{+16}O). Others: ({+37}Cl,{+38}Ar) (1997Wi17); ({+18}O,{+19}F) (1982Re14,1972Si02) 
$d|s/d|W (at 20|')=7 mb/sr (1980Dr09) 
$ ORIGIN OF OTHER C2S VALUES NEEDS TO BE CHECKED ?? 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
J$from combined analysis of (|a,|a') (from 1977Bo12) and their (d,|a) data, 1979Su04 strongly favor J=13/2 over 9/2 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$from |g|g(t) in 1978Eg02 
E$the ordering of the 1342-2490 cascade is not established in 1978Eg02 but the ordering given here is confirmed in later work of 1999AnZT 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
T$from 1978Eg02, determined from measured line shape of 3197|g in a separate experiment of {+27}Al+{+14}N reaction with E({+14}N)=33 MeV. 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
E$doublet near this energy proposed by 1981No05 in (|a,p|g) is not supported by detailed |g-ray studies of 1982VaZH 
T$from DSAM (1982VaZH); 1301 and 1342 |g rays have the same Doppler shapes thus no lifetime difference is found as claimed by 1981No05 in (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$from DSAM using 886.59|g in 1975Uh01. Note that ordering of 887-3197 cascade is reversed in 1975Uh01. Other: 13.2 ps {I21} from 1981No05 using recoil-distance method (RDM). 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
T$from 1975Ol01 based on re-analysis of data in 1974Ko04 which give T{-1/2}=11.2 ps {I11}. 1975Ol01 state that the revised value is obtained after accounting for the feeding from the longer lived 4831 level with T{-1/2}=20 ps {I5}. But the existence of the 4831 level is proposed by 1975Ol01 based on the 3197|g-887|g cascade from 8028 level, the ordering of which is however reversed in Adopted Gammas, resulting in no existence of such level but instead the short-lived 7142 level feeding the 3944 level. So the evaluator has considered that further revision is needed for the quoted T{-1/2} here. 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_comment:
T$1.9 ps {I10} in 1974Ko04 is retracted by 1977Wa14 from the same laboratory due to revised lifetime for 6475 level and its strong effect on the lifetime of 5718 level from the measurement of {+27}Al({+14}N,np|g) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_comment:
T$0.7 ps|<T{-1/2}|<2.1 ps in 1974Ko04 is replaced with T{-1/2}=11.8 ps {I21} from authors' later work in 1977Wa14 using {+27}Al({+14}N,np|g), with the earlier result found to be in error due to the presence of contaminant |g rays. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$or 38 ps {I17} from 1974Ko04 using RDM. 
G$relative to g factor of 15/2+ state in {+41}Ca measured in the same experiment (1992Pa01) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_comment:
E$doublet near this energy proposed by 1981No05 in (|a,p|g) is not supported by detailed |g-ray studies of 1982VaZH 
J$13/2+ from 1982VaZH 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_comment:
T$from RDM in 1977Wa14; this value replaces authors' previous result of 0.7 ps|<T{-1/2}|<2.1 ps from the measurement of {+24}Mg({+18}O,2np|g) in 1974Ko04, with the latter found to be in error due to the presence of contaminant |g rays. 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
T$from average of values for 887|g and 3197|g in cascade (1977Wa14). The 7142 level is expected to be of short half-life (see adopted levels). 
G$relative to g factor of 15/2+ state in {+41}Ca measured in the same experiment (1992Pa01) 


level_energy_unit: KEV
level_spin_parity: 13/2-
level_lifetime_unit: PS
level_comment:
J$1981No05 proposed 9/2 and rejected 13/2 since 13/2 gives an unusually low value of |?0.6 for the alignment parameter in |g(|q) as compared to that for other |g rays in {+39}K and for |g rays in neighboring nuclides. But analysis by 1982VaZH in {+28}Si({+16}O,|ap|g) rules out 9/2 and supports 13/2, the authors suggest that 1981No05 applied expected alignments too strictly to be realistic in (|a,p|g) reaction 
T$other: <140 ps (1974Al13) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$11/2+ proposed by 1981No05 is rejected in the work of 1982VaZH in {+28}Si({+16}O,|ap|g). See J|p comment for 5718 level 
T$other: <140 ps (1974Al13) 


level_energy_unit: KEV
level_spin_parity: 17/2+
level_lifetime_unit: PS
level_comment:
E$doublet of levels at 7774.9 and 7775.8 is proposed by 1981No05 based on differences in Doppler shifts for 1300.7|g and 1341.0|g and poor fit of the two |g rays in the level scheme. But the doublet is not supported in (HI,xn|g) study of 1982VaZH. Only one level is included in Adopted Levels with 1301|g and 1341|g from the same level. 
J$13/2+ proposed by 1981No05 is proven to be untenable by 1982VaZH in {+28}Si({+16}O,|ap|g). See J|p comment for 5718 level 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_comment:
J$(15/2,19/2)- proposed by 1981No05, but only 19/2- is supported in the work of 1982VaZH in {+28}Si({+16}O,|ap|g) 


level_energy_unit: KEV
level_comment:
$Isotope shift=-858.4 MHz {I6}(stat){I5}(syst), |d<r{+2}>=-0.074 fm{+2} {I5}(stat){I5}(syst), with respect to {+47}K (2019Ko19) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: Y
level_comment:
J$spin from fitting of hyperfine structure (2014Pa45,2014Kr04); unnatural parity in (pol d,|a); unique 3rd forbidden |b decays to 0+ in {+40}Ar and {+40}Ca; L(d,p)=L(p,d)=L(d,t)=3 
MOMM1$measured using nuclear magnetic resonance method in 1974Sa24. Others: -1.2982 {I4} (1952Ei09), 1.291 {I5} (1949Da01), with atomic beam magnetic resonance method. 
MOME2$measured using quadrupole resonance/optical level crossing in 1972Jo09 and 1971St12. Others: -0.073 {I1} (2008Py02,1998Ke05), -0.075 {I2} (1993Su36), with both re-evaluated data from 2013StZZ. See data also in 1962Bu10, 1968Ne05 
$%|b{+-}, %|e+%|b{++}: deduced from |g/|b{+-} (=I(electron capture to 1460.9 level in {+40}Ar)/I(|b{+-} to {+40}Ca g.s.))=0.1195 {I14}, and I(|b{++})/I(|b{+-})=1.12|*10{+-5} {I14} from evaluation of 1973EnVA, and |e/|b{++}(to {+40}Ar g.s.)=45.2 {I14} (3U theory), with all |b{++}) decay proceeding to {+40}Ar ground state. 
T$from 2004Ko09 and 2002Gr01 from measurements of specific activity of natural potassium salts using liquid-scintillation counting (LSC) technique. (2002Gr01 reported a value of 1.248|*10{+9} y {I2}, later adjusted to 1.248|*10{+9} y {I3} by 2004Ko09 to correct the quoted uncertainty on measured isotopic abundance of {+40}K). Both papers used natural abundance of {+40}K as 0.01167% {I2} (1975Ga24). The natural abundance of {+40}K=0.0117% {I1} (as recommended in the International Union of Pure and Applied Chemistry 70, 217 (1998), based on the measured value of 1975Ga24) would give about four times larger uncertainty on T{-1/2}. The earlier recommended values of 1.265|*10{+9} y {I13} (1999BeZS,1999BeZQ) based on recomputation of 1.277|*10{+9} y {I8} (evaluation by 1973EnVA); and 1.26|*10{+9} y {I1} (evaluation by 1990Ho28 from 14 different measurements out of a total of 34 measurements listed) are in good agreement. Variation of T{-1/2} due to environmental conditions has been studied by 2001No10, where no significant effect has been reported. Earlier (pre-1977) measurements of partial (|b{+-} and ce) and/or total T{-1/2} of {+40}K: 1977Ce04, 1972Go21, 1966Fe09, 1965Le15, 1965Br25, 1962Fl05, 1961Gl07, 1960Sa31, 1960Eg01, 1959Ke26, 1957We43, 1956Mc20, 1955Ba25, 1955Ko21, 1955Su38, 1953Bu58, 1950Sa52, 1947Gl07. Another 16 references (from 1931 to 1971) are listed by 1990Ho28 and in the 1978 Table of Isotopes (1978LeZA); but are not present in the NSR database. 
T$1.277|*10{+9} y {I8} from evaluation of 1973EnVA, where the |b{++} branch to the {+40}Ar ground state, whose intensity has been measured, was taken into account, but it appears that the corresponding |e decay was neglected. The |e/|b{++} ratio for this 3U transition has been estimated as follows. For a 1U transition, the theoretical value for this ratio is 8.5 and for a 2U transition it is 45.2. If the 3U ratio is larger by the same factor, 45.2/8.5, than the |e/|b{++} ratio is |?240. In the calculation of t{-1/2}, a value of 200 {I100} was used. The revised |b{+-}, |b{++}, and |e branchings are given in the corresponding tables and are based on the |g/|b{+-} and |b{++}/|b{+-} data in 1973EnVA. There are 1.5405|*10{+22} atoms of {+40}K per gram of natural K based on an average atomic mass of 39.095 and an atomic abundance of 1.178|*10{+-4} {I4} (1973EnVA). From the measured |b{+-} activity of 27.89 {I15} per second for 1 g of natural K and I(|b{+-})=89.14% {I11}, the total activity is 31.29 {I17} per s and T{-1/2}=4.0207|*10{+16} s or 1.274|*10{+9} y {I8}. With a later value of {+40}K/K=1.17|*10{+-4} {I1} (1990Ho28), T{-1/2}=3.992|*10{+16} s {I40} or 1.265|*10{+9} y {I13}. 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=0.56 10 (L=3) 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR=0.94 14 (L=3) 
$ ADOPTED (1977En02) PROTON PICKUP SPECTROSCOPIC FACTOR=2.5 7 (L=2) 
$Evaluated rms charge radius=3.4381 fm {I28} (2013An02) 
$|d<r{+2}>({+47}K,{+40}K)=-0.066 fm{+2} {I16}(stat) {I129}(syst) (2014Kr04) for |d|n({+39}K,{+40}K)=+125.6 MHz {I3} from literature 
$Dominant configuration=|p1d{-3/2}{+-1}~#|n(1f{-7/2} or 2p{-3/2}) (2014Pa45) from comparison with shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: NS
level_comment:
J$L(t,{+3}He)=L(p,d)=L(d,t)=3, L(d,{+3}He)=2; |p=natural in (pol d, |a), |g(circ pol) in (n,|g) E=thermal 
T$weighted average of 4.30 ns {I6} from (|a,n|g), 4.24 ns {I9} from (n,|g) E=thermal, 4.13 ns {I12} from (|g,|g) and 3.88 ns {I35} from (p,n|g). 
MOMM1$using TDPAD method (1974Br12) 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=SMALL (L=1) AND 0.56 10 (L=3) 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR=0.03 2 (L=1) AND 0.96 12 (L=3) 
$ ADOPTED (1977En02) PROTON PICKUP SPECTROSCOPIC FACTOR=2.5 7 (L=2) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=2, L(d,p)=L(p,d)=L(d,t)=1+3; |g(|q,pol) in (p,n|g), |g(circ pol) in (n,|g) thermal; |p=unnatural in (pol d,|a) 
T$weighted average of 0.28 ps {I7} from (|a,n|g), 0.40 ps {I8} from (d,p|g) and 0.22 ps {I4} from (p,n|g). 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=0.01 1 (L=1) AND 0.07 2 (L=3) 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR=0.02 1 (L=1) AND 0.77 9 (L=3) 
$ ADOPTED (1977En02) PROTON PICKUP SPECTROSCOPIC FACTOR=1.2 4 (L=2) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$L(|a,d)=L(t,{+3}He)=5, L(d,p)=L(p,d)=L(d,t)=3, L(d,{+3}He)=2; |g(|q,pol) in {+26}Mg({+16}O,np|g) 
T$weighted average of 0.78 ps {I18} from (|a,n|g), 1.07 ps {I23} from (d,p|g) and 0.73 ps {I18} from (p,n|g). Other: 2.3 ps {I10} from {+26}Mg({+16}O,np|g) 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=0.31 6 (L=3) 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR=0.88 10 (L=3) 
$ ADOPTED (1977En02) PROTON PICKUP SPECTROSCOPIC FACTOR=3.2 9 (L=2) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: US
level_comment:
J$L(p,{+3}He)=0; |g(|q) in (p,n|g); anti-analog state 
T$weighted average of 0.340 |ms {I7} in (p,n|g) and 0.294 |us {I23} in (n,2n|g) 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=0.06 2 (L=2) 
$ ADOPTED (1977En02) NEUTRON STRIPPING SPECTROSCOPIC FACTOR=0.10 3 (L=2) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,{+3}He)=2; |g(|q,pol) in (p,n|g) 
T$weighted average of 0.69 ps {I18} from (|a,n|g), 0.51 ps {I8} from (p,n|g). Other: 0.42 ps {I+29-15} from (d,p|g) 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=0.02 1 (L=0), 0.07 2 (L=2) 
$ ADOPTED (1977En02) NEUTRON stripping SPECTROSCOPIC FACTOR=0.01 1 (L=0), 0.02 1 (L=2) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1; |g(|q,pol) in (p,n|g) and |g(circ pol) in (n,|g) E=thermal; unnatural parity in (pol d,|a) 
$ ADOPTED (1977En02) NEUTRON stripping SPECTROSCOPIC FACTOR=0.52 13 (L=1) 
T$weighted average of 0.37 ps {I11} from (|a,n|g), 0.31 ps {I7} from (d,p|g) and 0.32 ps {I5} from (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(d,{+3}He)=0, L(|a,d)=3; |g(|q,pol) in (p,n|g) and also |g(circ pol) in (n,|g) 
T$from (|a,n|g). Others: 0.26 ps {I+15-10} from (d,p|g), 0.73 ps {I+26-19} from (p,n|g) 
$ ADOPTED (1977En02) NEUTRON stripping SPECTROSCOPIC FACTOR=0.37 10 (L=1) 
$ ADOPTED (1977En02) PROTON PICKUP SPECTROSCOPIC FACTOR=0.59 15 (L=0) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
J$L(t,{+3}He)=L(d,p)=1; |g(|q) in (p,n|g) and also |g|g(|q) in in (n,|g) E=thermal 
T$weighted average of 0.53 ps {I14} from (|a,n|g), 0.36 ps {I9} from (d,p|g) and 0.58 ps {I12} from (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: FS
level_comment:
J$L(d,t)=2; |p=unnatural in (pol d,|a); |g(|q,pol) in (p,n|g) 
T$weighted average of 59 fs {I17} from (|a,n|g) and 69 fs {I14} from (p,n|g). Other: 49 fs {I+55-29} from (d,p|g) 
$ ADOPTED (1977En02) NEUTRON PICKUP SPECTROSCOPIC FACTOR=0.86 22 (L=2) 
$ ADOPTED (1977En02) NEUTRON stripping SPECTROSCOPIC FACTOR=0.04 2 (L=2) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$L(t,{+3}He)=0+2; L(d,t)=2(+0); 646.223|g D to 0+ 
T$weighted average of 76 fs {I21} from (|a,n|g) and 94 fs {I19} from (p,n|g). Other: 0.23 ps {I+24-13} from (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(|a,d)=3; |g(|q,pol) in (|a,n|g) 
T$weighted average of 0.15 ps {I3} from (|a,n|g) and 0.155 ps {I29} from (p,n|g). Other: 0.22 ps {I+14-9} from (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1; |g|g(|q) in (n,|g) E=thermal; |g(|q) in (p,n|g); |p=unnatural in (pol d,|a) 
T$weighted average of 0.0.46 ps {I+30-18} from (|a,n|g), and 0.73 ps {I16} from (p,n|g), and 0.28 ps {I+28-11} from (d,p|g) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$this level is proposed in 2013Fi01 in (n,|g) E=thermal only based on the placement of a 2688.1|g from the 5111.9 level. But this level was neither observed in other work nor listed in Table 3 of populated levels in 2013Fi01. The evaluator have considered this level as questionable. 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
J$|g(|q,pol) in (|a,n|g); |p=unnatural in (pol d,|a) 
T$weighted average of 1.10 ns {I7} from ({+16}O,np|g) and 1.05 ns {I17} from (|a,n|g) 
MOMM1$using IPAD method (1976Bo21). Other: +4.4 {I11} (recoil into gas, 1981Le19) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$|g(|q) in (p,n|g); L(d,p)=2 
T$from (p,n|g). Other: 0.14 ps {I+8-5} in (d,p|g), 0.078 ps {I25} in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: PS
level_comment:
J$analyzing power in (pol d,|a); L(d,p)=1; isotropic |g(|q) in (p,n|g) 
T$from (p,n|g). Other: 0.22 ps {I+15-10} in (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$spin from |g(|q) in (p,n|g); L(t,{+3}He)=1 for a weak peak at 2724 indicates parity=-, while probable analog of the 10319, 1+ level in {+40}Ca according to 1979Gr09 in (e,e') suggests parity=+. 
T$from (p,n|g). Others: <50 fs in (|a,n|g), <83 fs in (d,p|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1 from 3/2+; 789|g to 2+, 2747.00|g D+Q to 4-; |g(|q) in (p,n|g) 
J$A2=+0.30 3, A4 AP 0 for 2717|g to 3- implies |DJ=0 
T$weighted average of 0.19 ps {I11} in (|a,n|g) and 0.123 ps {I31} in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g(|q) in (p,n|g); J=2- is ruled out by 1113.3|g to 0+ and RUL 
T$from (|a,n|g). Other: <24 fs from (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_lifetime_unit: PS
level_comment:
J$L(d,p)=1 from 3/2+; |g(|q) in (p,n|g) 
T$weighted average of 0.10 ps {I7} in (|a,n|g) and 0.16 ps {I5} in (p,n|g) 


level_energy_unit: KEV
level_spin_parity: (2-,3+)
level_lifetime_unit: FS
level_comment:
J$1027.09|g to 2+, 2185.70|g to 2-, 695.31|g and 2955.94|g to 3-; |p=unnatural in (pol d,|a) 
T$from (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 2-,3-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=1 from 3/2+; J|p=0-,1- ruled out by RUL for 1232.74|g and 3629.94|g to 4- 
J$ 1990En08 GIVE 3- 
T$from (d,p|g) 


level_energy_unit: KEV
level_spin_parity: (1-,2,3,4+)
level_comment:
J$1373.227|g and 3633.88|g to 3-, 249.54|g and 1704.73|g to 2+ 
J$J|p=(3,4)+ in 2004 evaluation with argument L(|a,d)=4 is erroneous since this level is not populated in (|a,d); also the 3663|g replaced by 1984Vo01 from this level to 4- ground state has been replaced by 2013Fi01 from 4463 level 


level_energy_unit: KEV
level_spin_parity: (1-,2,3-)
level_comment:
J$2001.24|g to 1-, 1813.94|g to 3-. J|p=2- preferred from |p=unnatural in (pol d,|a) for a level at 4118 {I10} if it is the same level 


level_energy_unit: KEV
level_spin_parity: 2
level_comment:
J$2467.31|g to 0+, 4110.39|g to 4-. J|p=2- preferred from |p=unnatural in (pol d,|a) for a level at 4118 {I10} if it is the same level 


level_energy_unit: KEV
level_spin_parity: (2-,3+)
level_comment:
J$1751.76|g and 4148.4|g to 4-, 3348.91|g to 2-; primary 3650.34|g from 1+,2+; |p=(unnatural) in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (1,2-)
level_comment:
J$1625.67|g to 0-. J|p=1+,2- preferred from |p=(unnatural) in (pol d,|a) for a level at 4255 {I10} if it is the same level 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_comment:
J$L(d,p)=1; 2149.93|g to 1-, 2183.70|g and 4223.66|g to 3-; J|p=(1,2)- from |g(circ pol) in (n,|g) E=thermal. J|p=2- preferred from |p=(unnatural) in (pol d,|a) for a level at 4255 {I10} if it is the same level 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$1486.7|g stretched E2 to 6+, 1822.9|g to 7+ 
T$from ({+16}O,np|g). The uncertainty may be larger since the lifetime is comparable to the stopping time in the tantalum stopper (1991Ja11). 


level_energy_unit: KEV
level_spin_parity: (1-,2,3,4-)
level_comment:
J$2416.06|g and 3663.32|g to 2-, 2393.84|g to 3-. J|p=(1-,2-,3-) preferred from L(d,p)=1 from 3/2+ for a level at 4466 {I5} if it is the same level 


level_energy_unit: KEV
level_spin_parity: (2-,3,4-)
level_comment:
J$4472.80|g to 4-, 1079.44|g to 2-. J|p=(2-,3-) preferred from L(d,p)=1 from 3/2+ for a level at 4466 {I5} if it is the same level 


level_energy_unit: KEV
level_spin_parity: (1-,2,3)
level_comment:
J$1961.11|g and 2577.63|g to 2+, 3737.01|g to 2-, 4506.96|g to 3-. J|p=2- preferred from L(d,p)=1 from 3/2+ for a level at 4544 {I5} and |p=unnatural for a level at 4535 {I10} in (pol d,|a) if they are the same level 


level_energy_unit: KEV
level_spin_parity: (0-:4-)
level_comment:
J$1058.03|g and 3743.2|g to 2-. J|p=2- preferred from L(d,p)=1 from 3/2+ for a level at 4544 {I5} and |p=unnatural for a level at 4535 {I10} in (pol d,|a) if they are the same level 


level_energy_unit: KEV
level_spin_parity: (2-:6-)
level_comment:
J$4662.1|g to 4-. J|p=2- preferred from L(d,p)=1 from 3/2+ for a level at 4662 {I5} and |p=unnatural for a level at 4663 {I10} in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (2-:5-)
level_comment:
J$4667.0|g to 4-, 2375.85|g to 3-. J|p=2- preferred from L(d,p)=1 from 3/2+ for a level at 4662 {I5} and |p=unnatural for a level at 4663 {I10} in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (1)+
level_comment:
E$from (d,p). Others: 4763 {I30} from (p,n), 4762 {I10} from (pol d,|a) 
J$L(d,p)=0 from 3/2+; J|p= 1+ preferred from |p=unnatural in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
E$from (d,p), 4942 {I10} from (pol d,|a) 
J$L(d,p)=1; J|p=2- preferred from |p=(unnatural) in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (2-,3+)
level_comment:
J$2644.0|g to 2-, 1953.74|g to 1+,2+, 5062.9|g to 4-. J|p=2-,3+ preferred from |p=unnatural for a level at 5068 {I10} in (pol d,|a) if it is the same level 


level_energy_unit: KEV
level_spin_parity: (0:3)-
level_comment:
E$from (d,p) 
J$L(d,p)=1. J|p=2- preferred from |p=unnatural for a level at 5068 {I10} in (pol d,|a) if it is the same level 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_comment:
J$L(d,p)=1 from 3/2+; 5111.5|g to 4-. J|p=2- preferred from |p=unnatural for a possible 5112+5132 doublet at 5111 {I10} in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: (0:3)-
level_comment:
J$L(d,p)=1. J|p=2- preferred from |p=unnatural for a possible 5112+5132 doublet at 5111 {I10} in (pol d,|a) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$3- is preferred by |g(|q) and |g(lin pol) in 1974Th07, but 4+ is possible 
$lifetime: 0.21 PS 5 (1971Ja15), 0.25 PS 8 (1971We09) 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
T$from mean lifetime of 1.51 ns {I25}, weighted average of 1.52 ns {I25} and 1.48 ns {I35} measured by 1973Gr19 using Recoil-Distance method (RDM). Other: 2.1 ps to 35 ns (1971Ja15) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$this level is proposed in 2013Fi01 only based on the placement of a 2688.1|g from the 5111.9 level. But this level was neither observed in other work nor listed in Table 3 of populated levels in 2013Fi01. The evaluator have considered this level as questionable. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_uncertain: S
level_comment:
E$S(n)=7799.62 {I6} (2012Wa38) 
J$s-wave capture in {+39}K (g.s. J|p=3/2+). From |g|g(|q)), an incoherent superposition of 1+ and 2+ is allowed, while from |g(circ pol), superposition is coherent, with either constructive or destructive interference 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$g|G{-n}|G{-|g}/|G=0.172 eV {I3} 
$E{-n}(lab)=9.386 {I9} 
$2g|G{-n}=54 eV {I6}, |G{-|g}=0.463 eV {I8} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$g|G{-n}|G{-|g}/|G=0.2577 eV {I15} 
$E{-n}(lab)=12.626 {I13} 
$2g|G{-n}=1.3 eV {I3}, |G{-|g}=0.488 eV {I5} 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
$g|G{-n}|G{-|g}/|G=0.1176 eV {I14} 
$E{-n}(lab)=14.302 {I21} 
$2g|G{-n}=0.81 eV {I17}, |G{-|g}=0.266 eV {I5} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.1496 eV {I19} 
$E{-n}(lab)=15.958 {I24} 
$2g|G{-n}=1.69 eV {I30}, |G{-|g}=0.291 eV {I4} 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$g|G{-n}|G{-|g}/|G=0.143 eV {I2} 
$E{-n}(lab)=16.715 {I14} 
$2g|G{-n}=0.320 eV {I1}, |G{-|g}=0.30 eV 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.246 eV {I4} 
$E{-n}(lab)=25.55 {I3} 
$2g|G{-n}=118.4 eV {I34}, |G{-|g}=0.396 eV {I7} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.184 eV {I8} 
$E{-n}(lab)=33.32 {I3} 
$2g|G{-n}=16.2 eV {I11}, |G{-|g}=0.301 eV {I14} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$g|G{-n}|G{-|g}/|G=0.63 eV {I3} 
$E{-n}(lab)=42.72 {I4} 
$2g|G{-n}=674 eV {I32}, |G{-|g}=0.973 eV {I4} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.386 eV {I10} 
$E{-n}(lab)=45.99 {I5} 
$2g|G{-n}=52 eV {I2}, |G{-|g}=0.626 eV {I17} 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
$g|G{-n}|G{-|g}/|G=0.220 eV {I8} 
$E{-n}(lab)=52.12 {I5} 
$2g|G{-n}=15.9 eV {I43}, |G{-|g}=0.362 eV {I13} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.261 eV {I9} 
$E{-n}(lab)=54.55 {I6} 
$2g|G{-n}=20.4 eV {I54}, |G{-|g}=0.429 eV {I15} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$g|G{-n}|G{-|g}/|G=0.55 eV {I5} 
$E{-n}(lab)=57.81 {I6} 
$2g|G{-n}=804 eV {I80}, |G{-|g}=1.47 eV {I13} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=0.076 eV {I8} 
$E{-n}(lab)=59.88 {I6} 
$2g|G{-n}=62 eV {I10}, |G{-|g}=0.203 eV {I21} 


level_energy_unit: KEV
level_spin_parity: 1
level_comment:
$g|G{-n}|G{-|g}/|G=0.67 eV {I8} 
$E{-n}(lab)=68.35 {I7} 
$2g|G{-n}=1454.00 eV {I18}, |G{-|g}=1.78 eV {I21} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$g|G{-n}|G{-|g}/|G=0.11 eV {I3} 
$E{-n}(lab)=87.71 {I9} 
$2g|G{-n}=350 eV {I40}, |G{-|g}=0.283 eV {I43} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.149 eV {I19} 
$E{-n}(lab)=99.20 {I10} 
$2g|G{-n}=142 eV {I32}, |G{-|g}=0.239 eV {I30} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$g|G{-n}|G{-|g}/|G=0.221 eV {I19} 
$E{-n}(lab)=102.0 {I2} 
$2g|G{-n}=45 eV {I13}, |G{-|g}=0.358 eV {I31} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$g|G{-n}|G{-|g}/|G=0.34 eV {I9} 
$E{-n}(lab)=108.7 {I2} 
$2g|G{-n}=1500 eV {I320}, |G{-|g}=0.96 eV {I24} 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
$g|G{-n}|G{-|g}/|G=0.308 eV {I21} 
$E{-n}(lab)=122.8 {I3} 
$2g|G{-n}=34 eV {I9}, |G{-|g}=0.503 eV {I36} 


level_energy_unit: KEV
level_spin_parity: (2)
level_comment:
$g|G{-n}|G{-|g}/|G=0.40 eV {I3} 
$E{-n}(lab)=126.2 {I3} 
$2g|G{-n}=53.0 eV {I56}, |G{-|g}=0.654 eV {I61} 


level_energy_unit: KEV
level_comment:
E$weighted average of 32 {I2} (1953Bu98), 28 {I2} (1959En57) and 30 {I5} (1974Fi08). 
L$ 3 (1959En57) 
$E(level)=27 (1959Da02) 


level_energy_unit: KEV
level_comment:
E$probable doublet: 2290+2291 (1974Fi08) 
$2286 {I8} (1959En57), 2292 {I5} (1974Fi08), 2286 (1959Da02) 
L$ (1) (1959En57) 


level_energy_unit: KEV
level_comment:
E$From 1974Fi08. 1959En57 report an uncertain level at 3021 {I8} 
L$ 1 for an uncertain level at 3021 from 1959En57 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_comment:
$Populated weakly in (p,n|g) (1973Da18); also reported by 1977St29 
J$from adopted level. Other: J|p=4,6 (1973Da18) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$B(>)(2730 level)/B(>)(2290 level)=0.73 {i5} (2014Ka27). Others quoted in 2014Ka27: 0.911 {i5} from (p,n) reaction (2009Bh09), 1.65 {i11} from analog states in {+40}Ti |b decay (1998Bh12). 


level_energy_unit: KEV
level_comment:
E$wide bump interpreted as spinflip giant-dipole resonance split into several states of J|p=0-,1-, and 2- (1988Vo06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
E$rounded value from Adopted Levels 
T$from 1972Ad01. Other: 0.26 |ms {I15} (1979Ha60) 
$isomeric cross sections: 36 mb 16 (1972Ad01), 15.1 mb 54 (1979Ha60) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
E$From 1970Ko13 
J$0+ is confirmed by characteristic L=0 shape and is consistent with its non-population in (d,|a) (1970Ko13). This state is interpreted as an anti-analog state (1970Ko13) 


level_energy_unit: KEV
level_spin_parity: 7+
level_lifetime_unit: NS
level_comment:
T$others: 1.10 ns {I8} (1976Ke02, RDM); 1.10 ns {I8}, 1.06 ns {I7} (apparent half-lives at 55|' and 0|', respectively, 1976Ra05 using RDM) 
$g-factor=0.63 {I15} (1981Le19), +0.59 {I10} (1976Bo21), +0.49 {I10} (1975Bo44) 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
T$the uncertainty may be larger since lifetime of the 4366 level is comparable to the stopping time in the tantalum stopper (1991Ja11). Other: <0.7 ps (1977Eg01) 


level_energy_unit: KEV
level_comment:
$B(>)=1.03 {I10} 
$Relative intensity=20.1% {i3} 
$B(>)=0.57 {I3} in {+40}Ti decay 
$B(>)(2730)/B(>)(2290)=1.65 {I11} in {+40}Ti decay is in severe disagreement with 0.911 {I5} from (p,n); 2730 and 2290 levels are identified with 2775 and 2333 levels, respectively 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
$|d|n{+39,40}=125.63 MHz {I9}, |d<r{+2}>{+39,40}=0.025 fm{+2} {I1} (stat) {I13} (syst) 
$R{-ch}=3.4386 fm {I1} (stat) {I9} (syst) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
MOME2$Mossbauer effect, recalculated by 1998Ke05. Others: +0.073 {I2} Mossbauer effect, recalculated by 1993Su05, +0.060 {I5} Mossbauer effect, recalculated by 1971St12, 1969Ne03, 1967Bo40, 1960Bl15, 1953Le33 
MOMM1$atomic-beam resonance method (1974Be50). Others: +0.21489274 {I12} (NMR 1974Sa24,1974Sa25), 0.2154 {I10} (1982To02), 1967Lu02, 1954Br09, 1936Ma03 
J$spin from atomic beam resonance method (1936Ma03). Parity from L({+3}He,d)=L(d,{+3}He)=2 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
BE2$weighted av of 0.0024 {I4} from (e,e') and 0.0029 {I10} and 0.00139 {I20} both from Coulomb Excitation 
T$the measured T{-1/2} values cluster into groups of values which differ significantly. The evaluators have adopted the weighted average of 0.35 ps {i14} from {+2}H({+40}Ar,n|g), 0.29 ps {I+21-10} from {+39}K(t,p|g), and 0.25 ps {I+14-10} from {+40}Ar(d,n|g) as they form the most consistent set of measured values. There are also several measurements which indicate a larger half-life including >6.9 ps from {+37}Cl(|a,|g): 3817 Resonance, 3.5 ps {I10} from {+38}Ar(|a,p|g), and >2.4 ps from {+41}K(p,p'|g),(p,p'). Other: 76 fs {I+21-4} from {+40}Ar(p,|g) 
J$from L(d,n)=L({+3}He,d)=L(d,{+3}He)=L(t,|a)=0 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
MOMM1$|g(|q,H,t), Time-dependent PAD method (1969Bl07). Other: +4.52 {I10} (1975Bo44). 
J$L(d,n)=L({+3}He,d)=L(d,{+3}He)=L(t,|a)=3; |g(|q,pol) in (|a,p|g) 
T$weighted average of 6.7 ns {I5} from {+41}Ar |b{+-} decay (109.61 min), 8.1 ns {I11} from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g), 8.3 ns {I7} from {+40}Ar(p,|g), 7.35 ns {I20} from {+41}K(p,p'|g),(p,p) Others: >3.5 ps from {+2}H({+40}Ar,n|g), >3.1 ps from {+37}Cl(|a,|g): 3817 Resonance, >3.1 ps from {+38}Ar(|a,p|g), >3.5 ps from {+39}K(t,p|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in {+38}Ar(|a,p|g) 
T$weighted average of 0.42 ps {I+20-14} from {+2}H({+40}Ar,n|g), 0.42 ps {I10} from {+38}Ar(|a,p|g), 0.40 ps {I15} from {+39}K(t,p|g), 0.35 ps {I5} from {+40}Ar(p,|g), 0.35 ps {I15} from {+40}Ar(d,n|g), 0.49 ps {I14} from {+41}K(p,p'|g),(p,p'). Other: 0.87 ps {I28} from {+37}Cl(|a,|g): 3817 Resonance, 0.59 ps {I17} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$from L({+3}He,d)=1 and |g(|q,pol) in {+38}Ar(|a,p|g) 
T$from {+40}Ar(p,|g). Others: >2.1 ps from {+2}H({+40}Ar,n|g), >1.7 ps from {+37}Cl(|a,|g): 3817 Resonance, >3.1 ps from {+38}Ar(|a,p|g), >1 ps from {+39}K(t,p|g), >1 ps from {+40}Ar(d,n|g), >2.8 ps from {+41}K(p,p'|g),(p,p'), >1.4 ps from {+37}Cl(|a,|g): 3817 Resonance 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
J$|g(|q) allows 1/2,3/2; 551|g from 5/2+; L(d,{+3}He)=0+1+2 for the unresolved triplet of levels 1560(L=2), 1582(L=1), 1593(L=0). 
T$weighted average of 97 fs {I35} from {+38}Ar(|a,p|g) and 83 fs {I28} from {+40}Ar(d,n|g). Others: 130 fs {I50} from {+41}K(p,p'|g),(p,p'), <0.24 ps from {+40}Ar(p,|g), 0.30 ps {I9} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g) and {+38}Ar(|a,p|g) 
T$weighted average of 1.6 ps {I4} from {+38}Ar(|a,p|g) and 1.25 ps {I35} from {+41}K(p,p'|g),(p,p'). Others: 5.4 ps {I22} from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g), >2.8 ps from {2}H({+40}Ar,n|g), >1.4 ps from {+37}Cl(|a,|g): 3817 Resonance, >3,5 ps from {+39}K(t,p|g), >0.17 ps from {+40}Ar(p,|g), >4.9 ps from {+40}Ar(d,n|g), 2.7 ps {I17} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in {+38}Ar(|a,p|g) 
T$weighted average of 0.83 ps {I21} from {+38}A(|a,p|g), 0.90 ps {I28} from {+39}K(t,p|g), and 0.83 ps {I21} from {+41}K(p,p'|g),(p,p'). Others: 0.07 ps {I+14-7} from {+2}H({+40}Ar,n|g), 1.4 ps {I7} from {+37}Cl(|a,|g): 3817 Resonance, 49 fs {I28} from {+40}Ar(p,|g), 0.24 ps {I6} from {+40}Ar(d,n|g), 0.83 ps {I28} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$3/2+,5/2+ from |g(|q,pol) in {+38}Ar(|a,p|g), |g from 7/2- 
T$weighted average of 0.55 ps {I+21-14} from {+2}H({+40}Ar,n|g), 0.25 ps {I9} from {+40}Ar(d,n|g), 0.21 ps {I6} from {+41}K(p,p'|g),(p,p'). Others: 0.29 ps {I6} from {+37}Cl(|a,|g): 3817 Resonance, 76 fs {I21} from {+38}Ar(|a,p|g), <0.18 ps from {+40}Ar(p,|g), 0.25 ps {I7} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
J$3/2 from |g(|q) in {+38}Ar(|a,p|g), |p from L({+3}He,d)=1 
T$weighted average of 1.7 ps {I6} from {+38}Ar(|a,p|g), 1.94 ps {I14} from {+40}Ar(p,|g). Others: >2.1 ps from {+2}H({+40}Ar,n|g), >1.25 ps from {+37}Cl(|a,|g): 3817 Resonance, >2.1 ps from {+40}Ar(d,n|g), 0.22 ps {I8} from {+41}K(p,p'|g),(p,p'), 1.5 ps {I7} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$from L({+3}He,d)=3 and |g(|q,pol) in {+38}Ar(|a,p|g) 
T$weighted average of 0.54 ps {I15} from {+38}Ar(|a,p|g) and 0.59 ps {I14} from {+41}K(p,p'|g),(p,p'). Others: 0.34 ps {I10} from {+37}Cl(|a,|g): 3817 Resonance, <0.21 ps from {+40}Ar(p,|g), 0.062 ps {I21} from {+40}Ar(d,n|g), 0.18 ps {I10} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_lifetime_unit: PS
level_comment:
J$from 847|g to 1/2+ and RUL for 742|g to 5/2+. 
T$from {+41}K(p,p'|g),(p,p'). Others: 0.16 ps {I3} from {+37}Cl(|a,|g): 3817 Resonance, 0.15 ps {I3} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$from |g(|q,pol) in {+38}Ar(|a,p|g) 
T$from {+38}Ar(|a,p|g). Others: >2.1 ps from {+37}Cl(|a,|g): 3817 Resonance, >2.8 ps from {+41}K(p,p'|g),(p,p'), 1.7 ps {I10} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in {+38}Ar(|a,p|g) 
T$weighted average of 0.16 ps {I6} from {+38}Ar(|a,p|g) and 0.15 ps {I4} from {+41}K(p,p'|g),(p,p'). Others: 0.43 ps {I10} from {+37}Cl(|a,|g): 3817 Resonance, 0.29 ps {I6} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
MOMM1$|g(|q,H,t), recoil into gas or vacuum (1981Le19) 
J$from |g(|q,pol) in {+38}Ar(|a,p|g) and {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g). 
T$from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g). Other: >3.1 ps from {+38}Ar(|a,p|g), >4.9 ps from {+39}K(t,p|g) 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: FS
level_comment:
J$from L({+3}He,d)=1. {I1}/2- is favored in (p,p'|g) from comparisons with Hauser-Feshbach calculations, but 3/2- is favored by |g from 5/2+ resonance in (p,|g) 
T$from {+40}Ar(p,|g). Other: 0.19 ps {I8} from {+37}Cl(|a,|g): 4013 Resonance, 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_lifetime_unit: PS
level_comment:
J$|g(|q,pol) in (|a,p|g) give 3/2-,7/2-. |g from (7/2+) 
T$weighted average of 0.52 ps {I15} from {+38}Ar(|a,p|g) and 0.59 ps {I28} from {+41}K(p,p'|g),(p,p'). Others: 0.62 ps {I28} from {+37}Cl(|a,|g): 3817 Resonance, <0.54 ps from {+40}Ar(p,|g), 0.83 ps {I35} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_comment:
J$from L({+3}He,d)=2; 1079|g to 7/2+, 1463|g to 7/2- 
T$from {+41}K(p,p'|g),(p,p'). Others: <31 fs from {+37}Cl(|a,|g): 3817 Resonance, <69 fs from {+38}Ar(|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 11/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in {+38}Ar(|a,p|g) 
T$weighted average of 0.48 ps {I6} from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g), 0.46 ps {I12} from {+38}Ar(|a,p|g) and 0.53 ps {I21} from {+41}K(p,p'|g),(p,p'). 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
MOMM1$|g(|q,H,t), recoil into gas or vacuum (1981Le19) 
J$from |g(|q,pol) in {+38}Ar(|a,p|g). 
T$from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g). Other: >3.1 ps from {+38}Ar(|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
J$from L({+3}He,d)=1. {I1}/2- is favored in (p,p'|g) from comparisons with Hauser-Feshbach calculations, but 3/2- is favored by |g from from 5/2+ resonance in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$5/2-,9/2- from |g(|q,pol) in {+38}Ar(|a,p|g), 998|g to 5/2+ and 381|g to 11/2- 
T$weighted average of 0.16 ps {I6} from {+38}Ar(|a,p|g) and 0.12 ps {I8} from {+41}K(p,p'|g),(p,p'). Others: 0.08 ps {I5} from {+37}Cl(|a,|g): 3817 Resonance, 0.17 ps {I4} from {+37}Cl(|a,|g): 4013 Resonance 


level_energy_unit: KEV
level_comment:
J$L({+3}He,d)=1 for 3619 {I10} group corresponds 3612.77 and/or 3626.1 level. 
$1990En08 ASSIGNED L(3HE,D)=1 TO 3626 LEVEL ONLY 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2+)
level_comment:
J$from 685|g to (7/2-), 2150|g to 7/2+, 3827|g to 3/2+ 
J$1990En08 GIVES (5/2+,7/2) WHICH APPEARS TO BE A MISPRINT 


level_energy_unit: KEV
level_spin_parity: (11/2,15/2)
level_lifetime_unit: PS
level_comment:
J$from |g(|q) in {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g) 
T$from {+38}Ar(|a,p|g). Other: >0.14 ps from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g) 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,pol) in {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g) 
T$from {+38}Ar(|a,p|g). Other: <0.14 ps from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g) 


level_energy_unit: KEV
level_comment:
J$L({+3}He,d)=1+3 implies 1/2-,3/2- and 5/2-,7/2- doublet 
E$this group is most likely different from 4927.8 level 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_comment:
E$4900, L=2 in (d,{+3}He). In (p,|a) E=4900 corresponds to 4922 and/or 4928 
J$from L(d,{+3}He)=2; 3253|g to 7/2+, 3335|g to 1/2+, 3634|g to 7/2- 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
MOMM1$|g(|q,H,t), recoil into gas or vacuum (1981Le19) 
J$from |g(|q,pol) in {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g) 
T$from {+26}Mg({+18}O,p2n|g),{+27}Al({+16}O,2p|g). Other: >3.1 ps from {+38}Ar(|a,p|g) 


level_energy_unit: KEV
level_comment:
J$doublet group in ({+3}He,d) assigned as L=1+3. The L=1 component may be associated with 5557.38 level 


level_energy_unit: KEV
level_comment:
E$8000 in (d,{+3}He) 
J$L({+3}He,d)=(3) gives (5/2-,7/2-); but L(d,{+3}He)=(2) gives (3/2+,5/2+). There may be two levels near this energy 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 9.5 ps {I40} (1973Go31) and 4.2 ps {I21} (1976Me09). Other: <35 ps (1974Li07) 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 152.5 ps {I35} (1981Le19), 159 ps {I10} (1976Me09), 138 ps {I7} (1973Go31), 159 ps {I8} (1974Li07) 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 55.5 ps {I14} (1981Le19), 53.0 ps {I15} (1978Cl09), 47 ps {I3} (1976Me09), 50.3 ps {I24} (1976Ra05), 51 ps {I6} (1974Li07), 47.0 ps {I14} (1973Go31) 


level_energy_unit: KEV
level_spin_parity: 19/2-
level_lifetime_unit: PS
level_comment:
G$other: |?0.33 (1976Ra05) 
T$weighted average of 73.5 ps {I21} (1981Le19), 67.2 ps {I21} (1978Cl09), 66 ps {I10} (1976Me09), 74 ps {I6} (1976Ra05), 70 ps {I5} (1974Li07), 97 ps {I14} (1973Go31) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
J$1971Pi12 give (1/2,3/2) 
E$uncertainty of 0.1 appears too low, increased to 0.5 by the evaluators based on the uncertainty of neighboring levels 


level_energy_unit: KEV
level_comment:
E$this level presumably differs from 4026.94 {I6} in (n,|g) (1984Kr05) since the decay branchings differ significantly, {Ie.g.} no evidence of a 2470|g in (p,|g) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
$E(p)(LAB)=974.3 
$S(p,|g)=0.7 {I2} 
J$|g to 1/2+ disfavors 5/2- 
L$others: 972 (2008Vo08) 973 {I1} (1961Ar10), 977 (1963Ko22) 
S$other: 1.0 (2008Vo08). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=986.2 
$S(p,|g)=1.6 {I3} 
J$|g's to 1/2+,5/2+ and 5/2- 
L$others: 984 (2008Vo08), 985 (1961Ar10), 988 (1963Ko22) 
S$other: 1.1 (2008Vo08). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1063.0 
$S(p,|g)=0.4 
L$others: 1061 (1961Ar10), 1066 (1963Ko22), 1058 (1963Co04), 1061 (2008Vo08) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
$E(p)(LAB)=1069.5 
$S(p,|g)=0.7 {I2} 
J$|g to 1/2+ disfavors 5/2- 
L$others: 1068 (1961Ar10), 1074 (1963Ko22), 1066 (1963Co04), 1068 (2008Vo08) 
S$other: 0.4 (2008Vo08) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1076.7 
$S(p,|g)=0.6 
L$others: 1074 (1961Ar10), 1079 (1963Ko22), 1074.6 (1970Ko28), 1072 (1963Co04), 1074 (2008Vo08) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1082.9 
$S(p,|g)=1.0 {I2} 
J$|g to 7/2- disfavors 3/2+ 
L$ 1081.7 (1970Ko28), 1082.9 3 (1967Bl26), 1082 (1963Co04) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=1087.1 
$S(p,|g)=2.1 {I3} 
J$3/2- (1971Pi12) 
T$|G from 1967Bl26; |G{-p}/|G=0.49 {I16}, |G{-|a}=0.032 eV {I12} (1967Bl26), |G{-|g}=1.7 eV (2008Vo03). 
L$others: 1086 (1961Ar10), 1091 (1963Ko22), 1086.2 (1970Ko28), 1086.5 3 (1967Bl26), 1092 (1963Co04), 1086 (2008Vo08). 
S$others: 3.6 (2008Vo08), 2.4 {I4} (2008Vo03). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1096.2 
$S(p,|g)=0.4 {I2} 
L$doublet: 1096.2+1096.4 
L$others: 1096 (1961Ar10), 1098 (1963Co04), 1096 (2008Vo03). 
S$from 2008Vo03. 


level_energy_unit: KEV
level_spin_parity: 3/2(-)
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=1101.7 
$S(p,|g)=8.0 {I10} 
J$p|g(|q) (1964Ar13). 
T$|G from 1967Bl26. |G{-p}/|G=0.58 {I8}, |G{-|a}=0.040 eV {I10} (1967Bl26), |G{-|g}=3.4 (2008Vo03). 
L$from 1967St30. 1102.4 {I5} in 1989Sm06. Others: 1101 (1961Ar10), 1106 (1963Ko22), 1101.0 (1970Ko28,1971Ko32), 1101.8 {I3} (1967Bl26), 1104 (1963Co04), 1102 (2008Vo08,2008Vo03,2014Ka35). 
$Possible IAR of 520 in {+41}Ar 
S$other: 8.0 (2008Vo08), 8.0 {I5} (2008Vo03). 
L$ 1970Ko28 SHOW 10 TRANSITIONS FROM THIS LEVEL TO BOUND LEVELS. BRANCHING RATIOS ARE IN REASONABLE AGREEMENT WITH THOSE FROM 1989Sm06 


level_energy_unit: KEV
level_spin_parity: 3/2,5/2+
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=1108.9 
$S(p,|g)=2.1 {I3} 
J$1964Ar13 and 1971Pi12 give 3/2 
T$|G from 1967Bl26. |G{-p}/|G=0.70 {I15}, |G{-|a}=0.019 eV {I6} (1967Bl26), |G{-|g}=1.1 (2008Vo03). 
L$others: 1108 (1961Ar10,2014Ka35), 1112 (1963Ko22), 1107.6 (1970Ko28), 1108.4 {I3} (1967Bl26), 1118 (2008Vo08). 
S$others: 3.1 (2008Vo08), 2.0 {I3} (2008Vo03), 2.0 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: GE 3/2
level_comment:
$E(p)(LAB)=1118.7 
J$not 1/2 from p|g(|q) (1964Ar13), 1971Pi12 give 3/2 for 1118.4 {I6} resonance 
L$others: 1118 (1961Ar10, 2014Ka35), 1123 (1963Ko22), 1118.1 (1970Ko28), 1114 (1963Co04), 1118 (2008Vo03, reported as quadruplet). 
S$2.2 {I3} for quadruplet at 1118 keV (2008Vo03), 3.0 for level at 1118 keV (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1140.0 
L$others: 1139 (1961Ar10,2014Ka35), 1141 (1963Ko22), 1136 (1963Co04), 1139 (2008Vo08). 
S$1.4 for level at 1139 keV (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1152.1 
$S(p,|g)=1.0 
L$others: 1152 (1961Ar10,2008Vo08,2014Ka35), 1159 (1963Ko22), 1149 (1963Co04) 
S$other: 1.7 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
$E(p)(LAB)=1162.8 
$S(p,|g)=0.9 {I3} 
J$|g to 1/2+ disfavors 5/2- 
L$others: 1162 (1961Ar10,2008Vo08), 1164 (1963Ko22), 1162.8 {I3} (1967Bl26), 1161 (2014Ka35) 
S$others: 1.2 (2008Vo08), 0.7 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
$E(p)(LAB)=1179.5 
$S(p,|g)=2.3 {I5} 
L$others: 1179 (1961Ar10), 1184 (1963Ko22), 1179.2 {I3} (1967Bl26), 1175 (1963Co04), 1177 (2014Ka35). 
S$other: 1.6 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1186.3 
$S(p,|g)=1.5 
L$others: 1186 (1961Ar10,2008Vo08), 1182 (1963Co04), 1184 (2014Ka35). 
S$other: 1.6 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1194.0 
$S(p,|g)=0.8 
L$others: 1194 (1961Ar10,2014Ka35), 1192 (1963Ko22), 1191 (1963Co04) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1195.7 
$S(p,|g)=0.6 
L$others: 1200 (1961Ar10,1963Ko22, 2008Vo08), 1196 (1963Co04), 1199 (2014Ka35). 
S$other: 0.4 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1207 
$S(p,|g)=1.2 
L$others: 1205 (1963Ko22), 1204 (1963Co04,2014Ka35), 1207 (2008Vo08). 
S$other: 0.5 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1217 
$S(p,|g)=0.3 
L$others: 1212 (1963Ko22), 1215 (1963Co04), 1217 (2008Vo08,2014Ka35). 
S$other: 0.6 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
$E(p)(LAB)=1241.1 
$S(p,|g)=2.4 {I5} 
L$others: 1240 (1961Ar10), 1246 (1963Ko22), 1236 (1963Co04), 1238 (2014Ka35) 
S$other: 2.0 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1244.9 
$S(p,|g)=1.3 
L$others: 1244 (1961Ar10), 1250 (1963Ko22), 1247 (1963Co04), 1244 (2008Vo08), 1241 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1258 
$S(p,|g)=0.3 
L$others: 1265 (1963Ko22), 1258 (1963Co04, 2008Vo08), 1256 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1262 
$S(p,|g)=0.8 
L$others: 1269 (1963Ko22), 1263 (1963Co04), 1268 (2008Vo08), 1260 (2014Ka35) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1270.2 
$S(p,|g)=0.7 
L$others: 1268 (1961Ar10, 2008Vo08), 1275 (1963Ko22), 1274 (1963Co04), 1266 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1284.5 
$S(p,|g)=2.2 
L$others: 1283 (1961Ar10, 2008Vo08), 1293 (1963Ko22), 1263 (1963Co04) 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2)
level_comment:
$E(p)(LAB)=1294.4 
$S(p,|g)=2.5 {I5} 
J$|g to 1/2+ disfavors 5/2-. 7/2- is not completely excluded but very unlikely 
L$others: 1293 (1961Ar10, 2008Vo08,2014Ka35), 1300 (1963Ko22,1963Co04) 
S$others: 1.1 (2008Vo08), 2.6 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: 3/2
level_comment:
$E(p)(LAB)=1305.2 
$S(p,|g)=2.1 {I5} 
L$others: 1303 (1961Ar10, 2008Vo08), 1311 (1963Ko22), 1316 (1963Co04), 1302 (2011Ka24,2014Ka35) 
S$others: 1.4 (2008Vo08), 3.1 (2011Ka24), 3.9 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
$E(p)(LAB)=1323.6 
$S(p,|g)=0.8 {I3} 
J$|g to 1/2+ disfavors 5/2- 
L$others: 1321 (1961Ar10, 2008Vo08), 1318 (2014Ka35) 
S$others: 0.9 (2008Vo08), 1.3 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1331 
$S(p,|g)=2.3 
L$others: 1331 (1963Ko22,1963Co04), 1333 (2008Vo08), 1332 (2014Ka35). 
S$other: 0.8 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_comment:
$E(p)(LAB)=1337.2 
$S(p,|g)=1.0 {I3} 
L$others: 1336 (1961Ar10), 1338 (1963Ko22), 1346 (1963Co04), 1338 (2014Ka35) 
S$other: 1.7 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1351.6 
$S(p,|g)=0.9 
L$others: 1349 (1961Ar10,1963Ko22, 2008Vo08), 1351 (1963Co04), 1352 (2014Ka35) 
S$other: 1.6 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1357.2 
$S(p,|g)=1.1 
L$others: 1358 (1961Ar10, 2008Vo08), 1356 (1963Co04), 1359 (2014Ka35) 
S$other: 1.1 (2014Ka35) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
$E(p)(LAB)=1363.7 
$S(p,|g)=1.5 {I5} 
L$others: 1365 (1961Ar10, 2008Vo08,2014Ka35), 1363 (1963Ko22), 1366 (1963Co04) 
S$others: 0.3 (2008Vo08), 1.0 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1373.7 
$S(p,|g)=1.2 {I4} 
J$5/2- is not completely excluded but very unlikely 
L$others: 1372 (1961Ar10, 2008Vo08), 1378 (1963Co04), 1371 (2014Ka35) 
S$other: 2.3 (2008Vo08), 1.1 (2014Ka35) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2,5/2)
level_comment:
$E(p)(LAB)=1384.2 
$S(p,|g)=1.9 {I5} 
J$|g to 1/2+ disfavors 5/2-. 7/2- is not completely excluded but very unlikely 
L$others: 1386 (1963Ko22), 1385 (2014Ka35). 2008Vo08 give a resonance at Ep=1387 with S=5.6 
S$other: 0.5 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1389.3 
L$others: 1391 (1963Ko22), 1389 (1963Co04), 2008Vo08 give a resonance at Ep=1387 with S=5.6 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1410.2 
$S(p,|g)=2.1 {I5} 
L$others: 1401 (1963Ko22), 1416 (1963Co04), 1408 (2008Vo08), 1406 (2014Ka35) 
S$others: 0.9 (2008Vo08), 2.1 (2014Ka35) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2+)
level_comment:
$E(p)(LAB)=1422.1 
$S(p,|g)=2.4 {I8} 
L$others: 1417 (1963Ko22), 1420 (1963Co04), 1420 (2008Vo08), 1418 (2014Ka35) 
S$others: 0.7 (2008Vo08), 1.2 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
$E(p)(LAB)=1427.1 
$S(p,|g)=2.6 {I9} 
L$others: 1429 (1963Ko22), 1424 (1963Co04), 1428 (2008Vo08), 1425 (2014Ka35) 
S$others: 1.4 (2008Vo08), 2.5 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
$E(p)(LAB)=1429.8 
$S(p,|g)=2.2 {I5} 
L$others: 1433 (1963Ko22), 1434 (1963Co04,2008Vo08), 1431 (2014Ka35) 
S$others: 0.5 (2008Vo08), 0.4 (2014Ka35) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1436.1 
$S(p,|g)=3.0 
L$others: 1437 (1963Ko22), 1441 (1963Co04, 2011Ka24,2014Ka35) 
S$from 2011Ka24. Other 3.7 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1447.0 
$S(p,|g)=2.2 {I5} 
L$others: 1443 (1963Ko22), 1449 (1963Co04,2014Ka35), 1444 (2008Vo08). 
S$others: 1.9 (2008Vo08), 0.9 (2014Ka35) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2,7/2-)
level_comment:
$E(p)(LAB)=1454.0 
$S(p,|g)=1.0 {I2} 
L$others: 1454 (1963Co04,2014Ka35), 1458 (2008Vo08). 
S$others: 0.5 (2008Vo08), 1.9 (2014Ka35) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1459.7 
$S(p,|g)=1.8 {I4} 
L$others: 1463 (1963Co04), 1466 (2008Vo08), 1462 (2014Ka35) 
S$others: 1.3 (2008Vo08), 2.3 (2014Ka35) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1475 
$S(p,|g)=3.8 
L$others: 1477 (2008Vo08), 1474 (2014Ka35) 
S$other: 4.2 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2,5/2+)
level_comment:
$E(p)(LAB)=1491.0 
$S(p,|g)=1.0 {I2} 
L$others: 1486 (1963Co04), 1488 (2008Vo08), 1493 (2014Ka35). 
S$others: 0.8 (2008Vo08), 2.1 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1499.4 
$S(p,|g)=1.3 {I4} 
L$others: 1495 (1963Co04), 1496 (2008Vo08), 1501 (2014Ka35) 
S$others: 0.99 (2008Vo08), 1.8 (2014Ka35). 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
$E(p)(LAB)=1509.9 
$S(p,|g)=2.4 {I6} 
L$others: 1509 (1963Co04), 1510 (2008Vo08) 
S$other: 1.2 (2008Vo08). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_comment:
$E(p)(LAB)=1513.7 
$S(p,|g)=2.2 {I6} 
L$others: 1515 (1963Co04), 1517 (2008Vo08), 1513 (2014Ka35) 
S$others: 1.3 (2008Vo08), 3.0 (2014Ka35). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1559.2 
$S(p,|g)=3.0 
L$others: 1554 (1963Co04), 1556 (2008Vo08), 1551 (2014Ka35) 
S$other: 4.2 (2014Ka35) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1570.7 
$S(p,|g)=2.6 
L$others: 1567 (1963Co04), 1571 (2008Vo08,2014Ka35). 
S$other: 0.9 (2014Ka35) 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1584 
$S(p,|g)=4.9 
L$other: 1583 (2011Ka24,2014Ka35). 
S$from 2011Ka24. Other: 6.7 (2014Ka35) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$E(p)(LAB)=1592.0 
$S(p,|g)=5.2 {I15} 
L$others: 1600 (1971Ko32), 1598 (1963Co04), 1590 (2008Vo08), 1597 (2014Ka35) 
S$others: 4.1 (2008Vo08). 11.3 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$E(p)(LAB)=1605.4 
$S(p,|g)=8.5 
J$from 1971Ko32, 1971Pi12 give (3/2) 
$Possible IAR of 1030 in {+41}Ar 
L$from 1971Pi12. Others: 1602 (1963Co04, 2008Vo08), 1600 (1971Ko32), 1597 (2011Ka24). 
S$other: 10.3 (2011Ka24). 


level_energy_unit: KEV
level_comment:
$E(p)(LAB)=1648 
$S(p,|g)=3.2 
L$others: 1648 (2008Vo08), 1649 (2014Ka35) 
$|G{-|g}=0.8 eV (2008Vo08). 
S$other: 1.2 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1656 
$S(p,|g)=0.2 
$|G{-|g}=0.1 eV (2008Vo08). 
S$other: 1.2 for a level at Ep=1660 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1752 
$S(p,|g)=0.5 
$|G{-|g}=0.3 eV (2008Vo08). 
S$other: 2.1 for a level at Ep=1749 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1764 
$S(p,|g)=1.5 
$|G{-|g}=0.4 eV (2008Vo08). 
S$other: 4.2 for a level at Ep=1765 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1772 
$S(p,|g)=1.0 
$|G{-|g}=0.5 eV (2008Vo08). 
S$other: 3.6 for a level at Ep=1773 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1795 
$S(p,|g)=0.7 
$|G{-|g}=0.2 eV (2008Vo08). 
S$other: 6.3 for a level at Ep=1798 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1804 
$S(p,|g)=4.6 
$|G{-|g}=2.4 eV (2008Vo08). 
S$other: 1.0 for a level at Ep=1803 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1814 
$S(p,|g)=2.4 
$|G{-|g}=0.6 eV (2008Vo08). 
S$other: 1.6 for a level at Ep=1816 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$E(p)(LAB)=1839 
$S(p,|g)=3.9 {I4} 
$|G{-|g}=0.8 eV (2008Vo08), 1.0 (2008Vo03). 
J$from |g(|q) in 2008Vo03. 
S$from 2008Vo03. Others: 3.2 (2008Vo08), 5.8 for a level at Ep=1835 (2011Ka24), 7.2 for a level at 1835 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$E(p)(LAB)=1842 
$S(p,|g)=3.3 {I3} 
S$from 2008Vo03. Others: 3.0 (2008Vo08), 5.0 (2014Ka35). 
$|G{-|g}=0.8 (2008Vo03). 
J$from |g(|q) in 2008Vo03. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$E(p)(LAB)=1859 
$S(p,|g)=0.8 {I2} 
$|G{-|g}=0.2 eV (2008Vo08). 
S$from 2008Vo03. Others: 0.8 (2008Vo08), 1.7 for a level at Ep=1856 (2014Ka35). 
J$from |g(|q) in 2008Vo03. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$E(p)(LAB)=1870 
$S(p,|g)=2.8 {I3} 
L,J$from 1971Ko32. This resonance exhibits a multiplet structure. Other: Ep=1875 (2003Vo08,2008Vo08) 1868 (2011Ka24,2014Ka35). 
$Possible IAR of 1350 in {+41}Ar 
$|G{-|g}=1.0 eV (2008Vo08), 0.7 (2008Vo03). 
S$from 2008Vo03. Other: 3.9 (2008Vo08), 5.6 (2011Ka24), 6.9 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$E(p)(LAB)=1896 
$S(p,|g)=4.1 {I4} 
$|G{-|g}=1.1 eV (2008Vo08), 1.0 (2008Vo03). 
S$from 2008Vo03. Others: 4.4 (2008Vo08), 5.4 (2011Ka24), 6.6 (2014Ka35) 
J$3/2 from |g(|q) in 2008Vo03, |p from consideration of RUL of depopulating transitions (2008Vo03). 
L$other: 1890 (2011Ka24,2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1909 
$S(p,|g)=0.6 
$|G{-|g}=0.3 eV (2008Vo08). 
S$others: 5.9 for a level at Ep=1907 (2011Ka24), 7.3 for a level at Ep=1907 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1916 
$S(p,|g)=4.0 
$|G{-|g}=3.0 eV (2008Vo08). 
S$others: 7.0 for a level at Ep=1917 (2011Ka24), 4.2 for a level at Ep=1917 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1931 
$S(p,|g)=0.7 
$|G{-|g}=0.4 eV (2008Vo08). 
S$other: 4.9 for a level at Ep=1934 (2011Ka24), 6.0 for a level at 1934 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1959 
$S(p,|g)=3.8 
$|G{-|g}=1.9 eV (2008Vo08). 
S$other: 3.5 for a level at Ep=1964 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=1985 
$S(p,|g)=5.0 
$|G{-|g}=2.5 eV (2008Vo08). 
S$other: 1.5 for a level at Ep=1988 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2003 
$S(p,|g)=2.7 
$|G{-|g}=1.4 eV (2008Vo08). 
S$other: 1.3 for a level at Ep=2005 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2089 
$S(p,|g)=2.3 
$|G{-|g}=0.6 eV (2008Vo08). 
S$other: 6.3 (2011Ka24), 7.7 (2014Ka35). 
L$other: 2090 (2011Ka24,2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2101 
$S(p,|g)=1.5 
$|G{-|g}=0.4 eV (2008Vo08). 
S$other: 3.9 for a level at Ep=2100 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2206 
$S(p,|g)=1.3 
$|G{-|g}=0.7 eV (2008Vo08). 
S$other: 6.5 for a level at Ep=2209 (2011Ka24), 8.2 for a level at Ep=2209 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2214 
$S(p,|g)=1.4 
$|G{-|g}=0.7 eV (2008Vo08). 
S$other: 4.7 for a level at Ep=2220 (2011Ka24), 5.8 for a level at Ep=2220 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2225 
$S(p,|g)=3.7 
$|G{-|g}=1.9 eV (2008Vo08). 
S$other: 2.5 for a level at Ep=2229 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2260 
$S(p,|g)=1.4 
$|G{-|g}=0.4 eV (2008Vo08). 
S$other: 2.8 for a level at Ep=2259 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2293 
$S(p,|g)=1.4 
$|G{-|g}=0.4 eV (2008Vo08). 
S$other: 4.3 for a level at Ep=2290 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2300 
$S(p,|g)=1.4 
$|G{-|g}=0.4 eV (2008Vo08). 
S$other: 3.7 for a level at Ep=2301 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2326 
$S(p,|g)=7.0 
L,S$S=2.3 for a level at Ep=2330 (2008Vo03). 
S$other: 5.7 (2011Ka24) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2347 
$S(p,|g)=3.2 
$|G{-|g}=1.6 eV (2008Vo08). 
L,S$S=4.2 for a level at Ep=2348 (2008Vo03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2357 
$S(p,|g)=4.3 
$|G{-|g}=2.2 eV (2008Vo08). 
L$other: 2360 (2011Ka24,2014Ka35) 
S$others: 6.8 (2011Ka24), 8.9 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2377 
$S(p,|g)=11.7 
L,S$S=1.3 for a level at Ep=2380 (2008Vo03). 
S$other: 9.3 (2011Ka24) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2414 
$S(p,|g)=2.0 
$|G{-|g}=1.0 eV (2008Vo08). 
S$other: 7.7 for a level at Ep=2413 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2422 
$S(p,|g)=3.3 
$|G{-|g}=1.7 eV (2008Vo08). 
L$others: 2421 (2011Ka24,2014Ka35) 
S$others: 11.4 (2011Ka24), 14.0 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2444 
$S(p,|g)=2.5 
$|G{-|g}=0.6 eV (2008Vo08). 
S$other: 7.5 for a level at Ep=2445 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2458 
$S(p,|g)=2.2 
$|G{-|g}=0.6 eV (2008Vo08). 
S$other: 5.6 for a level at Ep=2461 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2466 
$S(p,|g)=1.1 
$|G{-|g}=0.6 eV (2008Vo08). 
S$other: 5.6 for a level at Ep=2467 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2472 
$S(p,|g)=4.0 
$|G{-|g}=2.0 eV (2008Vo08). 
L$other: 2474 (2011Ka24,2014Ka35) 
S$other: 3.6 (2011Ka24), 7.5 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2500 
$S(p,|g)=2.6 
$|G{-|g}=1.3 eV (2008Vo08). 
L$other: 2494 (2011Ka24,2014Ka35) 
S$other: 3.1 (2011Ka24), 7.5 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2513 
$S(p,|g)=2.5 
$|G{-|g}=1.3 eV (2008Vo08). 
L,S$S=9.2 for level at Ep=2515 (2011Ka24), S=13.5 for level at Ep=2515 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2519 
$S(p,|g)=2.0 
$|G{-|g}=1.0 eV (2008Vo08). 
L,S$S=9.2 for level at Ep=2515 (2011Ka24), S=3.9 for level at Ep=2523 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2549 
$S(p,|g)=5.0 
$|G{-|g}=0.3 eV (2008Vo08). 
L$other: 2544 (2011Ka24, 2014Ka35). 
S$other: 5.9 (2011Ka24), 7.5 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2569 
$S(p,|g)=9.0 
$|G{-|g}=0.5 eV (2008Vo08). 
L$other: 2562 (2011Ka24,2014Ka35) 
S$other: 4.9 (2011Ka24), 6.0 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2584 
$S(p,|g)=2.0 
$|G{-|g}=0.5 eV (2008Vo08). 
L,S$S=5.2 for level at Ep-2586 (2011Ka24), S=6.7 for level at Ep-2586 (2014Ka35) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E(p)(LAB)=2588 
$S(p,|g)=1.4 
$|G{-|g}=0.7 eV (2008Vo08). 
L,S$S=5.2 for level at Ep-2586 (2011Ka24), S=6.7 for level at Ep-2586 (2014Ka35) 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=4.2 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=2.45 mb/sr 
E$analog of {+41}Ar ground state with J|p=7/2- (1975Me10). 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=0.46 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=0.254 mb/sr 
E$analog of {+41}Ar 167-keV level with J|p=7/2- (1975Me10). 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=0.90 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=0.66 mb/sr 
E$analog of {+41}Ar 516-keV level with J|p=3/2- (1975Me10). 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=0.80 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=0.44 mb/sr 
E$analog of {+41}Ar 1035-keV level with J|p=(3/2)+ (1975Me10). 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=1.9 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=0.97 mb/sr 
E$analog of {+41}Ar 1354-keV level with J|p=3/2- (1975Me10). 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=0.18 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=0.064 mb/sr 
E$analog of {+41}Ar 1635-keV level with J|p=3/2- (1975Me10). 


level_energy_unit: KEV
level_comment:
$1978En02 give (2J+1)S=0.16, 0.10 (C{+2}=1/5 for T=5/2) 
$d|s/d|W=0.046 mb/sr 
E$analog of {+41}Ar 1869-keV level with J|p=1/2+ (1975Me10). 


level_energy_unit: KEV
level_spin_parity: 7/2-,9/2-
level_uncertain: S
level_comment:
E$S(n)=10095.37 {I6} (2012Wa38). Observed deexcitation intensity is 70% of g.s. feeding. 
J$s-wave capture in {+40}K (g.s. J|p=4-), but population of mainly the levels of J<11/2 shows that the dominant component is 7/2- (1984Kr05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2(+),9/2+
level_comment:
$E(n)(LAB)=20.9 
$g|G{-n}|G{-|a0}/|G=0.27 eV {I3} 
$g|G{-n}|G{-p}/|G=0.017 {I5} 
J$from comparison of |a and proton yield to estimated spin dependent values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
BE2$other: 0.0034 {I13} (quoted by 1978En02 from Richter, Darmstadt Report IKDA 1978). 
$Using mean lifetime of 440 fs {I40}, 1981Gr04 deduce B(M1)(|^)=0.067 {I6} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
T$weighted average of 8.04 ns {I35} (1986St10), 7.14 ns {I35} (1977Ay01), 7.1 ns {I3} (1974Ko10), 7.3 ns {I2} (1969Bl07) 
$|s{-p'}=4.9 {I6} 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_lifetime_unit: FS
level_comment:
$|s{-|g}=2.6 {I4} 
J$Hauser-Feshbach analysis gives 3/2,5/2,7/2, but 5/2- and 7/2 are excluded due to unacceptably large transition strengths. 5/2+ is also less likely from E2 transition strength 
$|s{-p'}=1.9 {I3} 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2,7/2)
level_lifetime_unit: FS
level_comment:
$|s{-|g}=0.97 {I16} 
J$3/2- and 9/2- are allowed by Hauser-Feshbach analysis but 9/2- is unacceptable and 3/2- is less likely from transition strengths 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
BE2$values of 1968An20 and 1977Li20 have been adjusted by the evaluators to account for a change in the B(E2) value of the normalizing transitions. 1968An20 normalize to B(E2)(|^)=0.024 for the g.s. to 1630-keV level in {+20}Ne, the value is now known to be 0.033. 1977Li20 normalize to B(E2)(|^)=11.3 W.u. for the g.s. to 203 level in {+127}I, the value is now known to be 13.3. 
BE2$value from 1977Li22 deduced from B(E2)(W.u.)(|^)=1.4 {I2} (1977Li22) 


level_energy_unit: KEV
level_comment:
E$1969Yn01 report two levels 1270 {I40} with L=0 and 1290 {I40} with L=(3). 
S$other: 0.17 for L=0, fit improves if an L=3 component with C{+2}S=0.36 is included (1969Yn01). 


level_energy_unit: KEV
level_comment:
E$triplet of 1560+1582+1593 levels 
S$0.17 for L=0 (1593 level); 0.10 for L=1 (1582), 0.16 for L=2 (1560 level) (1976Do05). C{+2}S=0.4 fit with L=0 for the multiplet (1969Yn01) 
E$other: 1590 {I40} (1969Yn01). 


level_energy_unit: KEV
level_comment:
L$L=1 dominates (1976Bo01) but DWBA code LOLA fits the |s(|q) distribution poorly, in particular the experimental oscillations are out of phase with the predicted angular shape. Analysis of |s(|q) distribution of 1976Bo01 by 1977Fu07 suggest that fit is improved by including spin-flip (helicity) contribution 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
$d|s/d|W=6.0 
T$from 1972Gr04. 1977Li22 consider this measurement as questionable since no 980|g was observed in their {+44}Ca(p,|a|g) spectrum 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=1101.8 
$|G{-p}/|G=0.58 {I8}, |G{-|a}=0.064 {I24} eV (1967Bl26) 
L$other: 1102 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_comment:
$E(p)(LAB)=1108.4 
$|G{-p}/|G=0.70 {I15}, |G{-|a}=0.019 {I6} eV (1967Bl26) 
L$other: 1108 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1731.0 
T$for 1/2-; 21 eV for 3/2- 
$|G{-p}=30,20 eV, |G{-|a}=2,1 eV 
L$other: 1731 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1835.3 
$|G{-p}=70 eV 
$Pol=+0.056 {I8} for 1840 {I7} (1967Br08) 
L$other: 1835 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1851.4 
$|G{-p}=30 eV 
$Pol=+0.061 {I7} for 1850 {I7} (1967Br08) 
L$other: 1850 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1873.8 
$|G{-p}=1250 keV 
$1968Sc11 report E(p)=1880, L=1, |G=23.0 keV, |G{-p}=2.50 keV. 
$1963Co04 report 1875 {I8}, L=1, |G=3 keV {I1}, S=0.5 
$Pol=-0.059 {I9} for 1870 {I7} (1967Br08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1884.3 
$|G{-p}=30 eV, |G{-|a}=1 eV 
L$other: 1885 (2014Ka35). 
L,T$1968Sc11 report Ep=1880, |G=23, |G{-p}=2.5, L=0 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1897.4 
$|G{-p}=400 eV, |G{-|a}=3 eV 
$1963Co04 report 1890 {I8}, L=1, |G=6 keV {I2}, S=0.5 
$Pol=-0.118 {I14} for 1900 {I7} (1967Br08) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1913.8 
$|G{-p}=125 eV, |G{-|a}=5 eV 
$Pol=-0.083 {I11} for 1910 {I7}; J|p=3/2- (1967Br08) 
L$other: 1914 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1931.8 
$|G{-p}=45 eV 
$Pol=-0.045 {I10} for 1930 {I7}; J|p=3/2- (1967Br08) 
L$other: 1932 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=1958.1 
$|G{-p}=60 eV, |G{-|a}=2 eV 
$Pol=-0.030 {I12} for 1960 {I7}; J|p=3/2- (1967Br08) 
L$other: 1959 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+,3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=2123.5 
T$for 1/2+; 36 eV for 3/2- 
$|G{-p}=20,35 eV, |G{-|a}=3,1 eV 
L$other: 2123 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=2444.9 
$|G{-p}=750 eV, |G{-|a}=6 eV, |G{-n}=1 eV 
L$others:2440, |G{-n}<0.3 keV (1968Yo05); 2443 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=2464.2 
$1968Sc11 report E(p)=2460, L=0, |G=16.0 keV, |G{-p}=4.25 keV 
$|G{-p}=340 eV, |G{-|a}=18 eV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+,3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=2480.4 
T$for 1/2+; 270 eV for 3/2- 
$|G{-p}=170,270 eV, |G{-|a}=6,2 eV 
L$other: 2479 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-,3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=2544.6 
T$for 1/2-; 70 eV for 3/2- 
$|G{-p}=40,20 eV, |G{-|a}=100,30 eV, |G{-n}=60,20 eV 
L$others: 2540 (1968Yo05), 2545 (2015Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=2581.6 
$|G{-p}=250 eV, |G{-|a}=13 eV, |G{-n}=4 eV 
L$others: 2580 {I20} (1966Sk02), 2582 (2014Ka35). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3380 
$1968Sc11 report E(p)=3390, L=1, |G{-p}=7.50 keV 
L$other: 3390 (1972Bu06) 
J$from L=1 (1972Bu06). 
$Possible IAR of 2740, 3/2- level in {+41}Ar (1972Bu06) 
$|G{-n}=12 keV (1968Yo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3480 
$1968Sc11 report E(p)=3490, L=1, |G{-p}=7.0 keV. 
L$others: 3490 (1972Bu06), 3450 {I20} (1966Sk02) (doublet) 
$|G{-n}<2 keV (1968Yo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3550 
$1968Sc11 report tentative resonance at E(p)=3540 with L=2, |G{-p}=6.0 keV 
L$others: 3570 (1972Bu06), 3550 {I20} (1966Sk02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3600 
$L=1, |G{-p}=3.60 keV (1968Sc11) 
L$others: 3600 (1972Bu06), 3600 {I20} (1966Sk02) 
J$from L=1 (1972Bu06) 
$Possible IAR of 2955, 3/2- level in {+41}Ar (1972Bu06) 
$|G{-n}=3 keV (1968Yo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3640 
$1968Sc11 report E(p)=3650, L=1, |G{-p}=7.70 keV. |G{-n}=8 keV (1968Yo05) 
L$others: 3650 (1972Bu06), 3670 {I20} (1966Sk02) 
J$3/2- from L=1 (1972Bu06) 
$Possible IAR of 3017, 3/2- level in {+41}Ar (1972Bu06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3750 
$1968Sc11 report E(p)=3740, L=0, |G{-p}=3.00 keV. 
L$other: 3760 {I20} (1966Sk02) 
$|G{-n}=3 keV (1968Yo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3880 
$1968Sc11 report tentative resonance at E(p)=3880 with L=2, |G{-p}=3.00 keV. 
$|G{-n}=6 keV (1968Yo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=3960 
$L=0, |G{-p}=5.50 keV (1968Sc11) 
L$others: 3960 (1972Bu06), 3980 (1967Sl05) 
J$from L=1 (1972Bu06) 
$Possible IAR of 3335, 3/2- level in {+41}Ar (1972Bu06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=4020 
$1968Sc11 report E(p)=4030, L=0, |G=17.0 keV, |G{-p}=4.50 keV 
$|G{-n}=8 keV (1968Yo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=4060 
$1968Sc11 report E(p)=4070, L=1, |G{-p}=3.50 keV |G{-n}=8 keV (1968Yo05) 
L$others: 4070 (1972Bu06), 4090 (1967Sl05) 
J$from L=1 (1972Bu06) 
$Possible IAR of 3438, 3/2- level in {+41}Ar (1972Bu06) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
$E(p)(LAB)=5210 
T$from 1972Bu06. |G{-p}=5.0 eV (1972Bu06) 
J$from L=2 (1972Bu06) 
L$other: 5240 (1967Sl05) 
$Possible IAR of 4577, 5/2+ level in {+41}Ar (1972Bu06) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d|n{+39,41}=235.47 MHz {I9}, |d<r{+2}>{+39,41}=0.135 fm{+2} {I1} (stat) {I26} (syst) 
$R{-ch}=3.4546 fm {I1} (stat) {I37} (syst) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: H
level_comment:
$The rms charge radius (<r{+2}>){+1/2}: 3.4517 fm {I70} (2013An02 evaluation) 
$|d<r{+2}>({+47}K,{+42}K)=+0.034 fm{+2} {I6}(stat) {I89}(syst); |d<r{+2}>({+47}K,{+42}K)=+0.026 fm{+2} {I23}(stat) {I88}(syst) for |d|n({+39}K,{+42}K)=+351.7 MHz {I19} from literature; |d|n({+47}K,{+42}K)=-506.7 MHz {I7}(stat) {I19}(syst) (2014Kr04). 
J$spin from fitting of hyperfine structure (2014Pa45,2014Kr04) with spin of 1 or 2; former is excluded in the analysis. Also atomic-beam method (1969Ch20,1973CoZG). Parity from L(|a,d)=1 and L(d,p)=3 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0007 and an uncertainty of 0.0057 due to hyperfine anomaly are added in quadrature (2014Pa45). In 1969Ch20, |m is from atomic beam method. 
$Dominant configuration=|p1d{-3/2}{+-1}~#|n(1f{-7/2} or 2p{-3/2}) (2014Pa45) from comparison with shell-model calculations 
T$weighted average of 12.339 h {I11} (2005Li66), 12.321 h {I25} (2004Un01), 11.97 h {I12} (1994Mi03), 12.361 h {I3} (1967Go21) and 12.358 h {I7} (1962Me06), with uncertainty increased to 0.007 in 1967Go21. Others: 12.37 h {I9} (1959Ma27), 12.46 h {I7} (1957Wr37), 12.516 h {I7} (1953Bu58), 12.44 h {I8} (1953Ka26), 12.44 h {I10} (1947Si08), 12.47 h {I7} (1962Mo21), 12.5 h {I2} (1951Si25), 12.4 h {I2} (1937Hu01) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.34 {I9} (L=3) 
$Adopted (1977En02) proton-pickup spectroscopic factor=0.46 {I12} (L=2) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$|g(|q,lin pol); L(d,p)=3 and L(d,{+3}He)=2 
T$weighted average of 133 ps {I9} in ({+18}O,np|g) and 123 ps {I28} in ({+18}O,n2p|g) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$|DJ=2 |g to 4+ 
T$weighted average of 1.17 ns {I8} in ({+18}O,np|g) and 0.76 ns {I21} in ({+18}O,n2p|g) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J,E$gammas to 3- and 4+; primary |g from 1+,2+; unnatural-parity state from (pol d,|a), assuming that same level is populated in (d,|a) and (n,|g). J|p=(2,4)- suggested by 1982Ba55 in (pol d,|a) was based on L(d,|a)=3 and unnatural-parity, but |g to 4+ forbids 2- and primary |g from 1+,2+ does not allow 4-. The 2056-keV peak in (d,|a) was weakly populated in the work of 1977Pa24, it is possible that L(d,|a)=4 can also be consistent with the observed |s(|q) pattern, which will give a unique choice of 3+, when combined with unnatural parity assignment for this state. Another unlikely possibility is that the level populated in (d,|a) is different from that in (n,|g) giving a (2,4)- level at 2056 keV in (d,|a) and a 2+ or 3+ level at 2049 in (n,|g) 


level_energy_unit: KEV
level_comment:
L,S$for 1249 group in 1978Li27. Also L=1 quoted by 1982Ba55 from a priv comm from Summers-Gill (at McMaster) 
S$0.4 for 1260 group (1969Ly02) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$1776 (1958MoZZ) adjusted to 1787 by 1978En02. This level is considered as uncertain (evaluators) since it is not reported in any other study 


level_energy_unit: KEV
level_comment:
E,L,S$this level is associated with 699, 5- level in Adopted dataset. May contain contribution from 639, 3- level 


level_energy_unit: KEV
level_spin_parity: (2,4)-
level_comment:
$d|s/dW=60 
J,L$3+ in Adopted Levels based on |g decays and feeding, and |p=unnatural in (pol d,|a) (1982Ba55). J|p=(2,4)- was assigned by 1982Ba55 from L(d,|a)=3 in 1977Pa24 and unnatural parity state in their work. The 2056-keV peak was weakly populated in the work of 1977Pa24, and in evaluators' opinion L(d,|a)=4 can also satisfy the angular distribution pattern in 1977Pa24, which can give 3+. Other possibility is that level populated in (d,|a) is different from that in (n,|g) 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=2.030 {I2} 
$2g|G{-n}=4.18 eV {I4} 
$g|G{-n}|G{-|g}/|G (meV)=198.8 {I11} 
$|G{-|g}=0.352 eV 4 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=5.514 {I6} 
$2g|G{-n}=92.2 eV {I18} 
$g|G{-n}|G{-|g}/|G (meV)=260 {I26} 
$|G{-|g}=0.70 eV 7 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=13.341 {I13} 
$2g|G{-n}=5.9 eV {I12} 
$g|G{-n}|G{-|g}/|G (meV)=214.0 {I22} 
$|G{-|g}=0.369 eV 4 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=15.022 {I15} 
$2g|G{-n}=4.8 eV {I12} 
$g|G{-n}|G{-|g}/|G (meV)=137.6 {I23} 
$|G{-|g}=0.389 eV 7 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=16.710 {I17} 
$2g|G{-n}=256 eV {I11} 
$g|G{-n}|G{-|g}/|G (meV)=293 {I12} 
$|G{-|g}=0.78 eV 3 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=20.298 {I20} 
$2g|G{-n}=32.6 eV {I8} 
$g|G{-n}|G{-|g}/|G (meV)=266 {I4} 
$|G{-|g}=0.722 eV 12 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=25.118 {I25} 
$2g|G{-n}=110 eV {I21} 
$g|G{-n}|G{-|g}/|G (meV)=162 {I7} 
$|G{-|g}=1.30 eV 5 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=27.12 {I3} 
$2g|G{-n}=23.0 eV {I8} 
$g|G{-n}|G{-|g}/|G (meV)=255 {I6} 
$|G{-|g}=0.297 eV 8 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=38.56 {I4} 
$2g|G{-n}=830 eV {I15} 
$g|G{-n}|G{-|g}/|G (meV)=942 {I41} 
$|G{-|g}=1.51 eV 7 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=42.35 {I4} 
$2g|G{-n}=270 eV {I130} 
$g|G{-n}|G{-|g}/|G (meV)=570 {I19} 
$|G{-|g}=0.92 eV 3 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=55.43 {I6} 
$2g|G{-n}=80 eV {I24} 
$g|G{-n}|G{-|g}/|G (meV)=210 {I11} 
$|G{-|g}=0.242 eV 13 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=58.20 {I6} 
$2g|G{-n}=270 eV {I26} 
$g|G{-n}|G{-|g}/|G (meV)=388 {I24} 
$|G{-|g}=1.04 eV 6 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=70.45 {I7} 
$2g|G{-n}=46.6 eV {I5} 
$g|G{-n}|G{-|g}/|G (meV)=242 {I17} 
$|G{-|g}=0.39 eV 3 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=75.50 {I8} 
$2g|G{-n}=420 eV {I120} 
$g|G{-n}|G{-|g}/|G (meV)=163 {I24} 
$|G{-|g}=0.44 eV 7 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=79.83 {I8} 
$2g|G{-n}=710 eV {I120} 
$g|G{-n}|G{-|g}/|G (meV)=564 {I76} 
$|G{-|g}=0.90 eV 12 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=83.41 {I8} 
$2g|G{-n}=360 eV {I120} 
$g|G{-n}|G{-|g}/|G (meV)=601 {I29} 
$|G{-|g}=0.69 eV 3 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=90.53 {I9} 
$2g|G{-n}=130 eV {I60} 
$g|G{-n}|G{-|g}/|G (meV)=251.8 {I21} 
$|G{-|g}=0.41 eV 3 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=100.61 {I10} 
$2g|G{-n}=450 eV {I150} 
$g|G{-n}|G{-|g}/|G (meV)=526 {I41} 
$|G{-|g}=0.85 eV 7 


level_energy_unit: KEV
level_comment:
$E{-n}(lab)=116.44 {I24} 
$2g|G{-n}=590 eV {I200} 
$g|G{-n}|G{-|g}/|G (meV)=550 {I56} 
$|G{-|g}=0.63 eV 6 


level_energy_unit: KEV
level_comment:
$Isotope shift=-505.5 MHz {I6}(stat){I3}(syst), |d<r{+2}>=0.023 fm{+2} {I5}(stat){I3}(syst), with respect to {+47}K (2019Ko19) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$|d|n{+39,42}=352.4 MHz {I10}, |d<r{+2}>{+39,42}=0.128 fm{+2} {I10} (stat) {I38} (syst) 
$R{-ch}=3.4536 fm {I15} (stat) {I55} (syst) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: H
level_comment:
MOMM1$ABLDS method (1982To02,1982Du06). Other: 1959Pe26 
$Evaluated rms charge radius=3.4556 fm {I86} (2013An02) 
$Adopted (by 1977En02) spectroscopic factor S=4.0 {I15} (proton pickup) 
$The rms charge radius (<r{+2}>){+1/2}=3.4558 fm {I2} from 1989OtZZ evaluation 
$|d<r{+2}>({+47}K,{+43}K)=+0.049 fm{+2} {I19}(stat) {I69}(syst) (2014Kr04) for |d|n({+39}K,{+43}K)=+459.0 MHz {I12} from literature 
T$weighted average of 21.75 h {I50} (1963Ho17), 22.1 h {I1} (1972Em01), and 22.6 h {I2} (1972Wa20). Other: 1955Ne01, 1969Ta07 
J$spin from atomic-beam method; also from fitting of hyperfine structure (2014Pa45,2014Kr04); parity from L(t,p)=0; L(d,{+3}He)=L(t,|a)=2 
$Configuration=|p1d{-3/2}{+-1} (92%) (2014Pa45) from shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
MOMM1$TDPAD method (1983Ra37). Others: 1976We23, 1976De41 
J$L(d,{+3}He)=L(t,|a)=3; 5/2 ruled out by |DJ=2 to 3/2+ from |g(|q,pol) in (|a,p|g) 
T$from p|g(t) in (|a,p|g). 


level_energy_unit: KEV
level_spin_parity: 5/2(+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$|g decays to 3/2-, 3/2+, 7/2- and 7/2+; L(t,|a)=(2). But the parity is inconsistent with log| {Ift}=5.8 from 5/2(-) parent. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)
level_comment:
J$|g to 3/2+; log| {Ift}=7.4 from 5/2(-) parent. L(t,|a)=(2) for a 2180 group gives (3/2+,5/2+) for one of the levels near this energy 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_comment:
J$probably high spin formed in coupling an f{-7/2} proton with four f{-7/2} neutrons in a 4{++} configuration 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
J$|g decays to 3/2-, 3/2+ and (5/2,7/2)+; L(t,p)=2 from 3/2+; log| {Ift}=5.1 from 5/2(-) parent is inconsistent with positive parity 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
J$|DJ=2 stretched quadrupole to (11/2+) from DCO ratios possible positive-parity yrast band member in 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$|g transitions to 3/2+, 3/2- and (5/2,7/2)+; L(d,{+3}He)=(2); log| {Ift}=5.6 from 5/2(-) is inconsistent with positive parity 


level_energy_unit: KEV
level_spin_parity: (19/2-)
level_comment:
J$comparison with negative-parity levels of {+45}Sc suggests that the 1816 keV transition corresponds to the decay of a 19/2- level to the 15/2- level at 3116 keV (1998Mo16). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: NS
level_comment:
T$from p|g(t). Weighted average of 202 ns {I4} (1983Ra37,1984Ra23), 184 ns {I10} (1977Po07), 165 ns {I17} (1976De41), 205 ns {I10} (1975Bo30,1978MeZX) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d|n{+39,43}=459.0 MHz {I12}, |d<r{+2}>{+39,43}=0.165 fm{+2} {I11} (stat) {I49} (syst) 
$R{-ch}=3.4590 fm {I16} (stat) {I71} (syst) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MIN
level_comment:
$Evaluated rms charge radius (<r{+2}>){+1/2}=3.456 fm {I10} (2013An02) 
$Evaluated change in charge radius |d<r{+2}>({+39}K,{+44}K)=+0.148 fm{+2} {I11} (2013An02) 
J$spin from laser spectroscopy (1982To02,1982Du06); parity from allowed |b{+-} decay to |p=- level at 5561 (log {Ift}=4.5 {I+5-2}); fit of |s(|q) data in (t,{+3}He) with CCBA calculations and assumed L=1+3 suggests 2-, although with a poor fit. 
T$weighted average of 22.0 min {I5} (1954Co70) and 22.15 min {I20} (1973In02). Others: 1961Hi17, 1960Su05, 1954An25, 1937Wa06 
MOMM1$from laser spectroscopy: 1982To02, 1982Du06. See also 2019StZV compilation. Other: -0.8567 {I43} from laser spectroscopy in 2014Pa45 
$Measured |d<r{+2}>({+47}K,{+44}K)=+0.036 fm{+2} {I5}(stat) {I51}(syst) from |d|n({+47}K,{+44}K)=-292.1 MHz {I5}(stat) {I10}(syst) (2014Kr04). 
$Measured |d<r{+2}>({+39}K,{+44}K)=0.163 fm{+2} {I7}(stat) {I60} (syst) from |d|n({+39}K,{+44}K)=565.1 MHz {I8} (2021Ko08); |d<r{+2}>({+47}K,{+44}K)=0.0464 fm{+2} {I51}(stat){I21}(syst) from |d|n({+47}K,{+44}K)=-293.19 MHz {I56}(stat){I23}(syst) (2019Ko19) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$1,2,3+ from 1703.4|g from 1+, 182.6|g to 2- not pure E2 from RUL; 1- predicted in shell-model calculations (1980Jo09). 
$Level is weakly populated in (t,{+3}He). 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$fit of |s(|q) data in (t,{+3}He) with CCBA calculations and assumed L=1+3 suggests 2-, but as stated by 1985Aj03, fits for 3+ and 3- could not be excluded; 1980Ma13 in (p,|an|g) proposed (3-) based on shell-model calculations by 1980Jo09, and an analogous state at 587, 3- in {+46}K. J|p=2- is unlikely as it would require 137.25|g from 520, (4-) level to be E2, with B(E2)|>1244, exceeding RUL=100 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$from fit of |s(|q) data in (t,{+3}He) with CCBA calculations and assumed L=3+5. J|p=(4-) also proposed in (p,|an|g) (1980Ma13) based on shell-model calculations in 1980Jo09, and an analogous state at 681, (4-) in {+46}K. 


level_energy_unit: KEV
level_spin_parity: (5-)
level_comment:
J$from fit of |s(|q) data in (t,{+3}He) with CCBA calculations and assumed L=5. J|p=(5-) also proposed in (p,|an|g) (1980Ma13) based on shell-model calculations by 1980Jo09, and an analogous state at 885, 5- in {+46}K. 


level_energy_unit: KEV
level_spin_parity: (3)
level_comment:
J$fit of |s(|q) data in (t,{+3}He) with CCBA calculations and assumed L=2+4 suggests 3+, but 3- is not completely excluded. Shell-model calculations predict 4- (1980Jo09) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$fit of |s(|q) data in (t,{+3}He) with CCBA calculations and assumed L=4 suggests 4+ more likely than 3-, while excluding 3+. Also, possible (4+) from shell-model calculations (1980Jo09) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$from fit of |s(|q) data in (t,{+3}He) with CCBA calculations suggest (4+,3-); and 1051.3|g to 2-. Also, 3- from shell-model calculations (1980Jo09) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$from fit of |s(q) data in (t,{+3}He) with CCBA calculations and assumed L=1+3. Also, 2- from shell-model calculations (1980Jo09) 


level_energy_unit: KEV
level_comment:
J$2-,3,4,5- suggested from 227.4|g to (3-) and 721.2|g to (4-). Possible (5+) from shell-model calculations (1980Jo09) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$3-,4,5,6,7- suggested from 556.3|g to (5-). Possible (6+) from shell-model calculations (1980Jo09) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$J=1 from allowed or forbidden (log {Ift}=6.47) |b{+-} transition from 0+ parent; 1460.0|g to 2-; negative parity from 408.1|g to (3-) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
E$from energy consideration, this level may be the same as the 1459.39, (1-) populated in {+44}Ar |b{+-} decay, but different J|p assignments suggest two different levels 
J$from fit of |s(|q) data in (t,{+3}He) to CCBA calculations, excluding fit to L=1, J|p=1-. 


level_energy_unit: KEV
level_spin_parity: 5+,4-
level_comment:
E,J$from fit of |s(|q) data to CCBA calculations for possible unresolved states; L-transfers not listed (1985Aj03). Note that J|p=5+,4- in Fig. 6 of 1985Aj03, but 5+,4 in authors' Table IV. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MIN
level_comment:
J J from AB (1976Fu06,1967Ga08); |p=+ from L=2 in (t,|a),(d,{+3}He) 
T weighted av of 17.81 min {I25} (1980Hu10; |DT{-1/2} statistical only, {+45}K |b{+-} decay), 20 min {I2} (1967Ga08; av from decay curve of atoms collected from AB; |?3 T{-1/2}), 20 min {I1} (1964Mo18; chem, NaI), and 16.3 min {I3} (1965Ch07; chem, 4|p|b pc; 5 T{-1/2}). 17.81 min {I61} is the mean of 17.79 min {I61} (NRM) and 17.83 min {I24} (RT) with uncertainty from NRM 
MOMM1 AB; {+39}K standard 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J |<7/2+ from D,E2 |g to 3/2+. (3/2 to 9/2) from D |g from (5/2-,7/2-). 5/2+ from theory (1980Jo09) 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2,5/2(+)
level_comment:
J |g to 1/2+. L(t,|a)=0; however, 1980Jo09 note that the evidence for L=0 pickup is weak and that this state may Be the second 3/2+ and that the calculations suggest the second 1/2+ state is at 2.3 MeV. 1986Ku01 note that their pure shell-model calculations reproduce the experimental excitation energy for J|p=1/2+ 


level_energy_unit: KEV
level_comment:
If J|p({+45}Ar g.s.)=7/2-, then the 3690 state observed in (p,|a) and this state are not the same since J|p(3707)=5/2-,7/2- from |g to 3/2+ and log| {Ift}=4.7 {I1} from {+45}Ar g.s. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d<r{+2}>({+47}K,{+45}K)=+0.072 fm{+2} {I21}(stat) {I33}(syst) (2014Kr04) for |d|n({+39}K,{+45}K)=+661.7 MHz {I16} from literature 
J$spin from fitting of hyperfine structure (2014Pa45,2014Kr04) 
$Configuration=|p1d{-3/2}{+-1} (88-90%) (2014Pa45) from shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d|n{+39,45}=661.7 MHz {I16}, |d<r{+2}>{+39,45}=0.203 fm{+2} {I15} (stat) {I70} (syst) 
$R{-ch}=3.4644 fm {I22} (stat) {I102} (syst) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
T$unweighted average of 95 s {I5} from decay of 1345|g (1968YaZZ), and 115 s {I4} from decays of 1347|g and |b{+-}>3 MeV (1966Pa20). 
J L=(1+3) in (p,{+3}He), (d,|a) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$|d<r{+2}>({+47}K,{+46}K)=-0.002 fm{+2} {I4}(stat) {I16}(syst); |d<r{+2}>({+47}K,{+46}K)=+0.026 fm{+2} {I21}(stat) {I16}(syst) for |d|n({+39}K,{+46}K)=+762.8 MHz {I15} from literature; |d|n({+47}K,{+46}K)=-91.6 MHz {I5}(stat) {I3}(syst) (2014Kr04). 
J$ spin from fitting of hyperfine structure (2014Pa45,2014Kr04) with spin of 1 or 2; latter is excluded in the analysis 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0007 and an uncertainty of 0.0052 due to hyperfine anomaly are added in quadrature (by compiler) 
$Dominant configuration=|p1d{-3/2}{+-1}~#|n(1f{-7/2} or 2p{-3/2}) (2014Pa45) from comparison with shell-model calculations 


level_energy_unit: KEV
level_comment:
$Isotope shift=-95.81 MHz {I55}(stat){I6}(syst), |d<r{+2}>=0.0363 fm{+2} {I50}(stat){I5}(syst), with respect to {+47}K (2019Ko19) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$|d|n{+39,46}=764.1 MHz {I14}, |d<r{+2}>{+39,46}=0.150 fm{+2} {I13} (stat) {I80} (syst) 
$R{-ch}=3.4568 fm {I19} (stat) {I116} (syst) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: S
level_comment:
J$from the Adopted Levels of {+46}K in the ENSDF database 
T$from |g(t) measurements in 2019Po06. Result is a weighted average of |g(t) measurements for 29 strong |g transitions. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
J J=1/2 from ABLS (1982To02). J|p=1/2+ from L=0 
T weighted average of 17.5 s {I4} (1981HuZT. |b(t), 4|p|b, or |g(t)) and 17.5 s {I3} (1964Ku02. |g(t); E|g>1.85 MeV, NaI. Chem). Other: 18.0 s {I10} (1970Wa29. |g(t)) 
MOMM1 ABLS. {+39}K standard 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: NS
level_comment:
J (7/2-) from |s(|q) and A(|q) in (d,{+3}He),(pol d,{+3}He). Either 7/2- or 5/2+; a pure L=3 transfer does not reproduce |s(|q) (1987Og01) in (t,|a). 7/2- from comparison of experimental to calculated decay patterns (2004We09) in |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E weighted av of 0 {I10} (1967Bj04), 0 {I10}, (1968Sa09), 0 {I20} (1976Do05), and 0 {I20} (1987Og01) 
J from the Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E weighted av of 359 {I7} (1966Wi11), 359 {I10} (1967Bj04), 359 {I8} (1968Sa09), 360 {I20} (1976Do05), and 360 {I20} (1987Og01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$spin from observation of three resonances in figure 3 of 2014Pa45 (Figure 1 of 2013Pa11); also 2014Kr04 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0002 and an uncertainty of 0.0058 due to hyperfine anomaly are added in quadrature (by compiler) 
$Dominant configuration=|p2s{-1/2}{+-1} while |p1d{-3/2}{+-1} contributes 13% (2014Pa45) from comparison with shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$ spin from hyperfine structure 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0001 and an uncertainty of 0.0058 due to hyperfine anomaly are added in quadrature (by compiler) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-res}(c.m.)=2680 {I108}(syst){I20}(stat) 
$isobaric analogue state in {+47}Ar at E{-x}=0 {I91}(syst){I28}(stat) 
$|G{-p}=4.3 keV {I4}, S=0.27 {I3}(syst){I+21-13}(stat) 
$T{-z}=11/2 ({+47}Ar) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-res}(c.m.)=2990 {I+117-124}(syst){I20}(stat) 
$isobaric analogue state in {+47}Ar at E{-x}=310 {I+91-92}(syst){I28}(stat) 
$|G{-p}=20 keV {I2}, S=0.027 {I6}(syst){I+13-7}(stat) 
$T{-z}=9/2 ({+47}K) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-res}(c.m.)=3280 {I+125-127}(syst){I20}(stat) 
$isobaric analogue state in {+47}Ar at E{-x}=600 {I+92-93}(syst){I28}(stat) 
$|G{-p}=8.0 keV {I8}, S=0.008 {I2}(syst){I+5-6}(stat) 
$T{-z}=9/2 ({+47}K) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-res}(c.m.)=3650 {I+137-147}(syst){I20}(stat) 
$isobaric analogue state in {+47}Ar at E{-x}=970 {I+95-99}(syst){I28}(stat) 
$|G{-p}=24 keV {I2}, S=0.42 {I5}(syst){I9}(stat) 
$T{-z}=11/2 ({+47}Ar) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|d|n{+39,47}=858.4 MHz {I9}, |d<r{+2}>{+39,47}=0.133 fm{+2} {I8}(stat) {I90} (syst) 
$R{-ch}=3.4543 fm {I12} (stat) {I130} (syst) 


level_energy_unit: KEV
level_spin_parity: 1(-)
level_lifetime_unit: S
level_comment:
J$spin=1 from hyperfine structure (2014Kr04); parity from strong |b{+-} feeding to (2-) levels (6895 and 7401) in {+48}Ca 
T$from 1975Mu08. Others: 6.9 s {I2} (1981HuZT), 6 s {I1} (1978De17), 1973RaYT, 1972RiZJ 
%B-N$from simultaneous |b{+-} and n measurements (1982Ca04) 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely (2014Pa45). Statistical uncertainty of 0.0003 and an uncertainty of 0.0045 due to hyperfine anomaly are added in quadrature. Not listed in 2019StZV 
MOMM1$no value for {+48}K in 2019StZV compilation 
$|d<r{+2}>({+47}K,{+48}K)=+0.186 fm{+2} {I3}(stat) {I16}(syst); |d|n({+47}K,{+48}K)=+67.9 MHz {I4}(stat) {I3}(syst) (2014Kr04) 
$|d|n{+39,48}=926.4 MHz {I9}, |d<r{+2}>{+39,48}=0.328 fm{+2} {I8}(stat) {I99} (syst) (2021Ko08) 
$R{-ch}=3.4825 fm {I12} (stat) {I142} (syst) (2021Ko08) 
$Configuration=|p2s{-1/2}{+-1}~#|n(pf) (2014Pa45) from comparison with shell-model calculations 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5+)
level_lifetime_unit: NS
level_comment:
T$unweighted average of 13 ns {I2} in {+198}Pt({+48}Ca,X|g) (2004IsZX) and 7.1 ns {I5} in {+238}U({+48}Ca,X|g) (2011Kr12) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$2004IsZX propose this 1- level at E=x, on which all higher levels are based, while it has been resolved to be the g.s. by 2011Kr12 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
E,J$the (1-) state at E=x proposed in 2004IsZX is resolved by 2001Kr12 to be the ground state based on observed |g-decay pattern of the (5+) isomer and information from {+48}K |b{+-} decay 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: S
level_comment:
$ $ |pd{-3/2}{+-1} or |ps{-1/2}{+-1} state 
J$ from shell-model predictions in 2010Br14, but another calculation (2009No01) gives 3/2+ as g.s. and 1/2+ slightly above this energy. |<5/2 from log| {Ift}=6.1 to 3/2+ in |b{+-} decay to {+49}Cr. 3/2+ from log| {Ift}=5.4 to 1/2 (5.3 MeV) and log| {Ift}=4.5 to 5/2+ in |b{+-} decay to {+49}Cr. Note, however, that correspondence between unbound states observed in {+49}K |b{+-} decay and {+48}Ca(n,X),(n,|g) should not be considered as well established 
T$ from |b and neutron counting (1982Ca04). Other: 1.10 s {I30} (1978De17, decay curve for |g rays from {+49}K decay) 
%B-N$ If %|b{+-}n({+9}Li)=50% {I4} (1982Ca04). Other: 90% {I14} (1983La23. Ir(p,X) E=10 GeV. |bn-coin, 4|p scin) 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: NS
level_comment:
$ $ |pd{-3/2}{+-1} or |ps{-1/2}{+-1} state 
T$ >3 ns from recoil-distance method, <13 ns from |g|g time distribution of 771-92 |g|g events (2010Br14) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: PS
level_comment:
T$from recoil-distance method (2010Br14). Effective half-life, includes feeding from higher-lying stated 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
T$ from thick-target data where 575|g appears as a narrow line (2010Br14). The fit to the ratio I{-after}/[I{-before}+I{-after}] gave T{-1/2}=3.4 ps {I7} for 575.5|g which could imply T{-1/2} is much shorter than 2.2 ps for the 863-keV state which is populated by 575|g 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
$ Configuration=|pd{-3/2}{+-1} state 
T$ >3 ns from recoil-distance method, <13 ns from |g|g time distribution of 771-92 |g|g events (2010Br14) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
$ Configuration=|pf{-7/2} state 
T$ from thick-target data where 1241|g appears as a narrow line (2010Br14) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|d<r{+2}>({+47}K,{+49}K)=+0.342 fm{+2} {I4}(stat) {I32}(syst); |d|n({+47}K,{+49}K)=+135.3 MHz {I5}(stat) {I6}(syst) (2014Kr04) 
J$spin from observation of three resonances in figure 3 of 2014Pa45 (Figure 1 of 2013Pa11) 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0008 and an uncertainty of 0.0040 due to hyperfine anomaly are added in quadrature (by compiler) 
$Dominant configuration=|p2s{-1/2}{+-1} while |p1d{-3/2}{+-1} contributes 15-21% (2014Pa45) from comparison with shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$ spin from appearance of three resonances in figure 1 of 2013Pa11 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0008 and an uncertainty of 0.0040 due to hyperfine anomaly are added in quadrature (by compiler) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|d|n{+39,49}=994.2 MHz {I11}, |d<r{+2}>{+39,49}=0.491 fm{+2} {I10} (stat) {I108} (syst) 
$R{-ch}=3.5057 fm {I15} (stat) {I154} (syst) 


level_energy_unit: KEV
level_spin_parity: 0(-)
level_lifetime_unit: MS
level_comment:
$|d<r{+2}>({+47}K,{+50}K)=+0.438 fm{+2} {I8}(stat) {I47}(syst); |d|n({+47}K,{+50}K)=+206.5 MHz {I9}(stat) {I9}(syst) (2014Kr04, 2014Pa45); collinear laser spectroscopy at ISOLDE-CERN 
$Theoretical T{-1/2}=684.6 ms, %|b{+-}n=19 (2019Mo01) 
$Theoretical T{-1/2}=215 ms, %|b{+-}n=2.4, %|b{+-}2n=0.3 (2016Ma12) 
%B-N$from 1982Ca04. Other: 28 {i4} (1983La23) 
J$spin from observation of only one line in the laser hyperfine structure, as shown in figure 3 in 2014Pa45, and figure 4 in 2014Kr04 
$Dominant configuration=|p1d{-3/2}{+-1}~#|n2p{-3/2}{+-1} (2014Pa45) from shell-model calculations. See also 1998Ba80 and 1991Wa23 
T$from |b{+-}n coincidence decay curve (1983La23). Other: 470 ms {i20} (1983HuZW, 1981HuZT, from |g decay curve) 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
J$171.4|g to 0(-), possibly E2. (3-) proposed in 2010Da06, 2009Cr03, 1999DaZQ, with (1-) for the g.s. 
T$from IT decay (2012Ka36, 1999DaZQ) 


level_energy_unit: KEV
level_spin_parity: 0(-)
level_comment:
J$(1-) proposed by 2009Cr03 and 1999DaZQ based on |ps{-1/2}{+-1}~#|np{-3/2}{+-1} configuration. (0-) proposed by 1998Ba80. Spin=0 measured in hyperfine structure 


level_energy_unit: KEV
level_spin_parity: (1,2-)
level_uncertain: ?
level_comment:
E$ ordering of the 127.4-44 |g cascade is not established. Reverse ordering is proposed by 2009Cr03 giving a level at 128 keV, instead 
J$(1-) suggested by 1999DaZQ from multipolarity assignments 


level_energy_unit: KEV
level_spin_parity: (1,2-)
level_uncertain: ?
level_comment:
E$level considered as uncertain by the evaluators in view of weak and unknown ordering of the 101-70 |g cascade. Also 2009Cr03 do not report 70|g and 101|g 
J$(1-) suggested by 1999DaZQ from multipolarity assignments 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: NS
level_lifetime_info: ;ISO=M
level_comment:
T$weighted average of 125 ns {I40} (1999DaZQ, from |g-ray decay curve); 138 ns {I+50-41} (2012Ka36, |g-decay curve). Other: <500 ns (2009Cr03) 
J$3- proposed by 2009Cr03 and 1999DaZQ based on (E2) multipolarity of 171|g and J|p(g.s.)=(1-) 
$Number of implanted fragments=2.0|*10{+4} (2012Ka36) 


level_energy_unit: KEV
level_spin_parity: 0-
level_comment:
$|d|n{+39,50}=1065.3 MHz {I10}, |d<r{+2}>{+39,50}=0.592 fm{+2} {I9} (stat) {I116} (syst) 
$R{-ch}=3.5201 fm {I13} (stat) {I165} (syst) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K, Collinear Laser Spectroscopy (CLS, 2013Pa11). 
$|d<r{+2}>({+47}K,{+51}K)=+0.538 fm{+2} {I13}(stat) {I61}(syst); |d|n({+47}K,{+51}K)=+273.2 MHz {I14}(stat) {I11}(syst) (2014Kr04) 
J$ Spin from fitting of hyperfine structure with assumed spins of 3/2, 5/2 and 7/2 and comparison of intensity ratios of lines in these spectra (2013Pa11). J=5/2 and higher values are excluded at 95% confidence level. Comparison of experimental magnetic moments for different spin values (3/2+, 5/2+, 7/2+) with those calculated from shell model with three different interactions shows agreement only for 3/2+. Appearance of four resonances in figure 3 in 2014Pa45, figure 1 in 2013Pa11, and figure 4 in 2014Kr04 rules out J=1/2 for which maximum of three resonances are expected 
$Configuration=|p1d{-3/2}{+-1} (90-93%) (2014Pa45) from comparison with shell-model calculations 
T from multiscaling of neutron coincidences in 1983La23. Other: 380 ms {I30} (|b or |g multiscaling, 1981HuZT). 
%B-N Weighted average of 63 {I8} (|b-|g-n coin,2006Pe16) and 68 {I10} (|b-n coin,Scin, 1983La23). Others: 47 {I5} (simultaneous |b and neutron (scin in {+3}He long counter) measurements,1982Ca04, 1981HaZC) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d<r{+2}>({+47}K,{+51}K)=+0.538 fm{+2} {I13}(stat) {I61}(syst); |d|n({+47}K,{+51}K)=+273.2 MHz {I14}(stat) {I11}(syst) (2014Kr04) 
J$ spin from fitting of hyperfine structure with assumed spins of 3/2, 5/2 and 7/2 and comparison of intensity ratios of lines in these spectra (2013Pa11). J=5/2 and higher values are excluded at 95% confidence level. Comparison of experimental magnetic moments for different spin values (3/2+, 5/2+, 7/2+) with those calculated from shell model with three different interactions shows agreement only for 3/2+. Appearance of four resonances in figure 3 in 2014Pa45, figure 1 in 2013Pa11, and figure 4 in 2014Kr04 rules out J=1/2 for which maximum of three resonances are expected 
MOMM1$deduced from hyperfine parameters measured relative to those for {+39}K whose parameters are known very precisely. Statistical uncertainty of 0.0022 and an uncertainty of 0.0015 due to hyperfine anomaly are added in quadrature by evaluators. 
$Configuration=|p1d{-3/2}{+-1} (90-93%) (2014Pa45) from comparison with shell-model calculations 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|d|n{+39,51}=1130.6 MHz {I14}, |d<r{+2}>{+39,51}=0.716 fm{+2} {I13} (stat) {I124} (syst) 
$R{-ch}=3.5377 fm {I18} (stat) {I176} (syst) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$removal of d{-3/2} proton from comparison of parallel momentum distribution with DWIA calculations. 
$|s=5.2 mb {I4} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$removal of s{-1/2} proton from comparison of parallel momentum distribution with DWIA calculations. 
$|s=1.7 mb {I2} 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
Other: %|b{+-}n|?64, %|b{+-}2n|?21 estimated from P{-n}(%)=%|b{+-}n+2*%|b{+-}2n=107 {I20} in 1985Hu03. 
T Weighted average of 118 ms {I6} (2006Pe16), 110 ms {I30} (1985Hu03), and 105 ms {I5} (1983La23) 
J estimated from systematic trends in neighboring nuclides with the same Z or N (2012Au07). 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$supported by unrealistically small/large charge radii for J=1 or J=3 possibilities (2021Ko08) 
$|d|n{+39,52}=1198 MHz {I5}, |d<r{+2}>{+39,52}=0.79 fm{+2} {I5} (stat) {I13} (syst) for J=2. Others: |d|n{+39,52}=1119 MHz {I5} and |d<r{+2}>{+39,52}=1.54 fm{+2} {I5} (stat) {I13} (syst) for J=1 ; |d|n{+39,52}=1237 MHz {I5} and |d<r{+2}>{+39,52}=0.43 fm{+2} {I5} (stat) {I13} (syst) for J=3 
$R{-ch}=3.549 fm {I7} (stat) {I19} (syst), for J=2. Others: R{-ch}=3.652 fm {I6} (stat) {I18} (syst), for J=1 R{-ch}=3.497 fm {I7} (stat) {I19} (syst), for J=3. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$removal of d{-3/2} proton from comparison of parallel momentum distribution with DWIA calculations. 
$|s=3.8 mb {I3} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$removal of s{-1/2} proton from comparison of parallel momentum distribution with DWIA calculations. 
$|s=1.5 mb {I2} 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MS
level_comment:
T from 1983La23. 
J$Estimated from trends in neighboring nuclides with the same Z and n parities (2012Au07). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$Theoretical T{-1/2}=9.2 ms, %|b{+-}n=87, %|b{+-}2n=7, %|b{+-}3n=1, %|b{+-}4n=0 (2019Mo01). 
$Theoretical T{-1/2}=9.9 ms, %|b{+-}n=82.6, 80.5; %|b{+-}2n=5.3, 7.8; %|b{+-}3n=1.5, 1.2; %|b{+-}4n=0 (2021Mi17). 
$Measured production |s=4|*10{+-11} mb {I+3-2} (read by the evaluator from Fig. 2 in 2009Ta05). 
E$fragment observed by 2009Ta05 is assumed to be in the ground state of {+55}K. 
J$others: 3/2+ (syst, 2021Ko07), 1/2+ (theory, 2019Mo01) 
T$experimental half-life of {+55}K g.s. is unknown. Lower limit of |?360 ns is estimated from time-of-flight as in 2005St29 (from the same lab as 2009Ta05). From a trend of decreasing half-lives with increasing neutron number in neutron-rich nuclei, evaluator estimates T{-1/2}<10 ms from known half-lives of 110 ms for {+52}K, 30 ms for {+53}K and 10 ms for {+54}K. Other: 10 ms (syst, 2021Ko07) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
E$from E|g 
T$mean lifetime |t<53 ps, estimated from peak-shape analysis in {+1}H({+56}Ca,2p) (2022Ko06) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$Measured inclusive |s=5.3 mb {I5} (2022Ko06). 
$Measured exclusive |s=3.5 mb {I7} (2022Ko06). 
$Spectroscopic factor=3.09 {I62} (2022Ko06) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$Measured exclusive |s=1.7 mb {I5} (2022Ko06) 
E$from E|g 
T$mean lifetime |t<53 ps, estimated from peak-shape analysis in {+1}H({+56}Ca,2p|g) (2022Ko06) 
$Spectroscopic factor=1.31 {I42} (2022Ko06) 


level_energy_unit: KEV
level_comment:
$As |b{+-} is the only possible decay mode, followed by |b{+-}-delayed-neutrons, 100% |b{+-} decay is assigned by inference. 
$Theoretical T{-1/2}=3.9 ms, %|b{+-}n=51, %|b{+-}2n=34, %|b{+-}3n=1, %|b{+-}4n=0, %|b{+-}5n=0 (2019Mo01). 
$Theoretical T{-1/2}=7.3 ms, %|b{+-}n=18.9, 21.2; %|b{+-}2n=65.3, 62.8; %|b{+-}3n=2.0, 2.3; %|b{+-}4n=0.34, 0.21; %|b{+-}5n=0 (2021Mi17). 
$Measured cross section=8|*10{+-11} mb {I3} for W target (read by the evaluator from Fig. 8 in 2009Ta24). 
E$fragment observed by 2009Ta05, 2009Ta24 is assumed to be in the ground state of {+56}K. 
J$1- or 2- from |W{-p}=1/2+ and |W{-n}=3/2- (theory,2019Mo01); 2- from systematics (2021Ko07) 
T$>620 ns estimated from time-of-flight of 620-650 ns (from (e-mail reply of Sept 23, 2009 from O. Tarasov). Actual half-life is expected to be much longer as suggested by theoretical values of 3.9 ms (2019Mo01), 7.3 ms (2021Mi17), and 5 ms from systematics (2021Ko07). From a decreasing trend of half-lives with increasing neutron number in neutron-rich nuclei, T{-1/2} of {+56}K is expected to be <10 ms from known half-lives of 10 ms for {+54}K, 30 ms for {+53}K and 110 ms for {+52}K. 


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 eight events were assigned to {+57}K, as in the text of 2018Ta17. In Table I of the paper, six events are assigned for tuned setting of the spectrometer for {+60}Ca, and one event for setting on {+57}K. 
$Theoretical T{-1/2}(|b)=5.6 ms, %|b{+-}n=69, %|b{+-}2n=24, %|b{+-}3n=5, %|b{+-}4n=0, %|b{+-}5n=0, %|b{+-}6n=0 (2019Mo01) 
$Theoretical T{-1/2}(|b)=5.6 ms, %|b{+-}n=41.2, 45.9; %|b{+-}2n=43.2, 37.8; %|b{+-}3n=4.3, 3.8; %|b{+-}4n=0.41, 0.49; %|b{+-}5n=0.010, 0.004; %|b{+-}6n=0 (2021Mi17); two values for different fission barriers. 
$The observed events are assumed to correspond to the {+57}K g.s. 
T$half-life of the {+57}K 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 <10 ms from 10 ms for {+54}K, 30 ms for {+53}K, 110 ms for {+52}K, and 365 ms for {+51}K, assuming a decreasing trend of half-life as neutron number increases in neutron-rich nuclei. From systematics, T{-1/2}=2 ms in 2021Ko07. 
J$1/2+ (2019Mo01, theory); 3/2+ (syst, 2021Ko07) 


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. 
$Only one event was assigned to {+59}K, with tuned setting of the spectrometer for {+60}Ca (2018Ta17) 
$Theoretical T{-1/2}(|b)=2.9 ms, %|b{+-}n=31, %|b{+-}2n=45, %|b{+-}3n=22, %|b{+-}4n=1, %|b{+-}5n=0, %|b{+-}6n=0 (2019Mo01) 
$Theoretical T{-1/2}(|b)=3.48 ms, %|b{+-}n=15.4, 21.8; %|b{+-}2n=48.9, 37.0; %|b{+-}3n=22.5, 38.4; %|b{+-}4n=1.8, 2.2; %|b{+-}5n=0.42, 0.6; %|b{+-}6n=0.002, 0.006; %|b{+-}7n=0.0 (2021Mi17); two values for different fission barriers. 
$The observed event is assumed to correspond to the {+59}K g.s. 
T$half-life of the {+59}K 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 <10 ms from 10 ms for {+54}K, 30 ms for {+53}K, 110 ms for {+52}K, and 365 ms for {+51}K, assuming a decreasing trend of half-life as neutron number increases in neutron-rich nuclei. From systematics, T{-1/2}=2 ms in 2021Ko07. 
J$1/2+ (2019Mo01, theory); 3/2+ (syst, 2021Ko07) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
T$upper limit estimated from expected cross sections (1996PoZZ) 
${+34}Ca is a candidate for two-proton emission since S(2p) is negative 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: MS
level_comment:
T$from decay curve of |b-delayed protons in 1999Tr04. Other: 50 ms {I30} from 1985Ay01. 
J$ probable mirror state of 1/2+ ground state of {+35}P. 
$%|ep, %|e2p: from 1999Tr04 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$from L=2 transfer from 3/2+ g.s. of {+37}Ca and in agreement with J|p=1/2+ for the mirror nucleus {+35}P (2023La09). 
$configuration=|n2s{-1/2} 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$from L transfer and comparison to the mirror nucleus {+35}P 
E$large uncertainty results from high density of unresolved states above 3 MeV (2023La09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$%|ep: from 2007Do11. Others: 54.3% {i15} (2001Lo11) is an earlier measurement from GANIL, same lab as 2007Do17, 57% {I5} (or 14) (1997Tr05,1995Tr02), |?20 (1981Ay01). 
T$from timing of |b(proton) correlated events. Weighted average of 100.1 ms {I23} (2007Do17) and 102 ms {I2} (1995Tr02,1997Tr05). Other: 100 ms {I+90-40} (1981Ay01). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$ from systematics and shell model calculations. 
E$ from mirror energy difference |DE{-M}=E({+36}Ca)-E({+36}S)=-246 {3} for the first excited 2+ states in {+36}Ca and {+36}S. The energy of the 2+ excited state in {+36}S is at 3291 keV from Adopted Levels. 2007Do11 interpret this large |DE{-M} value in terms of detailed shell-model calculations using {+16}O core, the {Isd} shell isospin symmetric interaction, and experimental single particle energies from {+17}O and {+17}F. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$ from systematics and shell model calculations. 
E$ mirror energy difference |DE{-M}=E({+36}Ca)-E({+36}S)=-262 {I11} for the first excited 2+ states in {+36}Ca and {+36}S. The energy of the 2+ excited state in {+36}S is at 3291 keV in Adopted Levels. 2007Do11 interpret this large |DE{-M} value in terms of detailed shell-model calculations using {+16}O core, the {Isd} shell isospin symmetric interaction, and experimental single particle energies from {+17}O and {+17}F. 
$ One-neutron knockout cross section=5.3 mb {I20} (2007Bu15, preliminary value) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$predicted from mirror state in {+36}S and shell-model calculations (2012Bu15) 
S$lower limit assuming no proton emission (2012Bu15) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$E{-r}=445 {I7} 
$Calculated |G{-|g}=0.99 meV, resonance strength |w|g=0.102 meV {I50} 
$|G{-p}=0.20 meV from calculated |G{-|g} and measured %p (2021La04) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$4706 {I100} 
$E{-r}=2106 {I100} 
$Calculated |G{-|g}=7.4 meV, resonance strength |w|g=4.6 meV {I25} 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Level observed in {+1}H({+38}Ca,t) reaction 
L$from (p,t) (2022La10) 
$Proposed configuration from shell-model: |p(d{-5/2},s{-1/2},d{-3/2},f{-7/2},p{-3/2},p{-1/2},f{-5/2}) ~# |n(d{-5/2},s{-1/2},d{-3/2}), listed with normal occupancy values of the orbits and their calculated excesses or reductions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
J$from 2022La10 
$Two-proton decay of this level observed by 2022La10 through the observation of ({+36}Ca)p-coin and ({+36}Ca)2p-coin, with proton energies of 1.7 MeV {I3} and 3.4 MeV {I3}, corresponding to the expected energies of 1.47 MeV and 3.65 MeV, respectively, from the sequential 2p-decay to {+34}Ar g.s. through the 1.55-MeV,(1/2+) state in {+35}K 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$Deformation correction deduced from measured B(E2), |b{-2} = 0.139 in 2023Dr01. The charge radius |dR{-ch}=0.012 fm {I2}. 
$The p/|g branching ratio B{-p} = 0.087 {I8} measured in 2023Dr01 in neutron knockout experiment. 
$|s =22.4 mb {I34} measured from laboratory scattering angles |q=0|' to |q{-max}=55|' mrad at 70.5 MeV/nucleon mid-target energy.and corrected for the proton branch. 
$The gamma partial width |G{-|g}=5.6 meV {I8} deduced from measured B(E2) in 2023Dr01. 
$The proton partial width |G{-p}=0.53 meV {I9} deduced using |G{-|g} and B{-p} in 2023Dr01. 
$The total width |G=6.1 meV {I8} (2023Dr01). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$two-neutron removal cross section = 0.292 mb {I8} (stat) {I8} (syst) (2023Be26), includes contribution from excited 0+ level. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
%ECP$others: 72.2 {I43} (2007Do17), 76 {I3} (1974Se11). 
J$ mirror state of 3/2+ ground state of {+37}Ca 
T$from 1995Tr03. Others: 181.7 ms 36 (2007Do17), 177 ms {I5} (1966Po12), 173 ms {I4} (1964Ha42) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$ possible mirror of 3103.5, 7/2- in {+37}Cl 
T$ estimated (by 2009AmZZ) as greater than a few picoseconds from Doppler-shift in energy between the two sets of rings in SeGA array 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
T$ estimated (by 2009AmZZ) as greater than a few picoseconds from Doppler-shift in energy between the two sets of rings in SeGA array 
$ Deduced E(resonance)=106 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
MOMM1$from HF spectrum measurement (2019Kl06), value is relative to reference of |m({+43}Ca)=-1.317643 {I7} 
J$from the Adopted Levels of {+37}Ca in the ENSDF database (2012 update). 
MOME2$from HF spectrum measurement (2019Kl06). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 443.63 ms {I35} (2015Bl02), 443.77 ms {I36} (2011Pa38), 443.8 ms {I19} (2010Bl09), 430 ms {I12} (1980Wi13), 450 ms {I70} (1972Zi02), 439 ms {I12} (1969Ga27), and 470 ms {I20} (1968Ka15). Other: 660 ms {I50} (1957Cl23), based on the observation of a 3.5 MeV |g which could not be confirmed in the studies afterwards. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(p,t)=2 from 0+; Coulomb excitation from 0+ 
T$from B(E2)|^. Other: 68 fs {I+30-28} from DSAM in ({+3}He,n|g) 
$B(E2)|^ from 1999Co23 in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2; L({+3}He,n)=2 or 2+3 for a doublet; Coulomb excitation from 0+ 
T$from B(E2)|^ and adopted |g-ray branching ratios. Other: <5.5 fs from DSAM in ({+3}He,n|g) 
$B(E2)|^ from 1999Co23 in Coulomb excitation. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: PS
level_comment:
J$systematics of even-even nuclides; L({+3}He,n)=2+3 for a doublet composed of 3684 and 3703 levels. L(p,t) also shows some evidence of presence of L=3 component 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$other: 4751 {I5} from ({+3}He,n) 
J$L({+3}He,n)=0 from 0+. L(p,t)=(3) is inconsistent. There may be a doublet near this energy, but due to tentative nature of L(p,t), the evidence for two levels is not sufficient. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
E$from ({+3}He,n) 
J$L({+3}He,n)=3,(2+4). This group may be a doublet in ({+3}He,n); L=(2+4) may correspond to 4899, 2+ level from (p,t) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(MAX)=0.46 
E$weighted average of 3070 {I30} (1986Al15) and 3060 {I50} (1969Sh04). 
L$0 in 1977Bo16 and 1969Sh04, but |s(|q) distribution in 1986Al15 does not show characteristic L=0 shape 


level_energy_unit: KEV
level_comment:
$d|s/d|W(MAX)=0.43 
E,L$1969Sh04 observe a doublet structure of E=3690 {I30} at some angles, however the |s(|q) distribution for the group is consistent with DWBA for L=2. |s(|q) distribution in 1977Bo16 fits L=2 uniquely, in 1986Al15 it fits L=2 or L=2+3 


level_energy_unit: KEV
level_comment:
$d|s/d|W(MAX)=0.18 
E$weighted average of 4390 {I30} (1986Al15) and 4450 {I40} (1969Sh04) 
L$other: 3 (1977Bo16) 


level_energy_unit: KEV
level_comment:
$d|s/d|W(MAX)=0.29 
E,L$this level in 1986Al15 and the level at 4920 {I30} in 1969Sh04 could be doublet; L=(2+4) could correspond to 4899, 2+ level in (p,t) 
L$other: 3 (1977Bo16) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|s (mb)=21 {I5} 
J$1999Co23 have considered the possibility that this level may be 3-; but the deduced B(E3) (from cross section) disagrees with RUL, concluding, therefore, that most of the strength must come from 2+ 


level_energy_unit: KEV
level_comment:
E$weighted average of 2215 {I3} (2017Lo05) and 2206 {I5} (1972Pa02). Others: 2200 {I30} (1977Ku01), 2200 {I30} (1966Ha32) 


level_energy_unit: KEV
level_comment:
E$from 2017Lo05 and 1972Pa02. Others: 3690 {I30} (1977Ku01), 3720 {I30} (1966Ha32) 
L$|s(|q) in 1977Ku01 differs somewhat from L=2 for 2206 group; the difference may be due to the presence of a 3720, 3- unresolved group. Others: L=3 for 3720 {I30} (1966Ha32), 3,2 for 3695 {I5} (1972Pa02) 


level_energy_unit: KEV
level_comment:
E$weighted average of 4387 {I4} (2017Lo05) and 4381 {I5} (1972Pa02). Others: 4370 {I30} (1977Ku01), 4360 {I40} (1966Ha32), 
L$0 from 1966Ha32, (2) from 1972Pa02 


level_energy_unit: KEV
level_comment:
E$weighted average of 4904 {I4} (2017Lo05) and 4899 {I5} (1972Pa02). Others: 4890 {I30} (1977Ku01), 4840 {I40} (1966Ha32) 
L$(2) from 1972Pa02 and 1966Ha32 


level_energy_unit: KEV
level_comment:
E$weighted average of 6277 {I3} (2017Lo05) and 6280 {I8} (1972Pa02). Other: 6270 {I30} (1977Ku01) 
L$(0) from 1972Pa02 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|s=17.5 mb {I19} measured from laboratory scattering angles |q=0|' to |q{-max}=55|' mrad at 62.6 MeV/nucleon mid-target energy and corrected for the feeding from 1486|g. Other: 16.0 mb {I15} not corrected for the feeding. 
$B(E2) = 0.0108 {I10} not corrected for the feeding. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4-)
level_comment:
J$From the characteristics of 489|g observed and comparison with the mirror {+38}Ar level systematics in 2022Ga31. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
J$L(pol p,d)=L(pol d,t)=L(pol {+3}He,|a)=2 and L-1/2 transfer from analyzing power 
T$weighted average of 860.7 ms {I10} (2010Bl09), 860.4 ms {I30} (1973Al11) and 859.4 ms {I16} (1977Az01). Others: 0.76 s {I20} (1994Ha07), 0.95 s {I4} (1964Ba24), 0.89 s {I5} (1960Wa04), 0.873 s {I8} (1960Li05), 0.860 s {I5} (1958Mi85), 0.876 s {I12} (1958Cl41), 0.90 s {I1} (1954Kl36), 1.00 s {I3} (1953Su81), 1.00 s {I5} (1953Br07), 1.06 s {I3} (1943Hu02) 
MOMM1$using NMR technique with a polarized proton beam; also 1976Mi21 and 1980HuZX. Compilation: 2014StZZ. 
MOME2$using |b-NMR method (1999MaZI). Also Q=0.040 {I6} (1999MaZK) by the same group. Compilation: 2016St14 
$Experimental nuclear charge radius <r{+2}>{+1/2}=3.460 fm {I3} (2013An02, evaluation) 
$|D<r{+2}>({+40}Ca,{+39}Ca)=-0.127 fm{+2} {I18}; |D<r{+2}>({+41}Ca,{+39}Ca)=-0.115 fm{+2} {I18} (1996Ve04) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_comment:
J$L(pol p,d)=L(d,t)=L({+3}He,|a)=3 and L+1/2 transfer from analyzing power 
T$other: >12 ps in ({+3}He,|a|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
J$L(pol p,d)=L(d,t)=L({+3}He,|a)=1 and L+1/2 transfer from analyzing power 
T$from ({+3}He,|a|g). Other: <7.6 ps in (|a,n|g). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
J$3640|g(|q) and 843|g(|q) in 1970Ba08 in ({+3}He,|a|g) is consistent with 3/2,5/2,9/2 with best fit for 9/2; 1980Oh06 in (p,d) interpret this state as 9/2- state populated by L=2, J=3/2 transfer from 3740, 3- state in {+40}Ca 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_lifetime_unit: PS
level_comment:
J$798.0|g to 3/2- and 3823.4|g to 3/2+. L(d,t)=(0) suggests (1/2+), but L(p,d)=(3) suggests (5/2-,7/2-) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,d)=L(d,t)=L({+3}He,|a)=1 for a single state around 3950 could be for the 3936+3950 double; possible analog state of the 4083, 3/2- level in {+39}K from 1974Ke09 in (|a,n|g). 
T$from ({+3}He,|a|g). Other: <3.5 ps in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: PS
level_comment:
J$3952|g to 3/2+, 1155.3|g to 7/2-; 1155|g(|q) and 3952|g(|q) in ({+3}He,|a|g) is consistent with 1/2,3/2,5/2, but 3952|g is most likely a doublet with 3939|g from 3939 level observed in ({+3}He,|a|g). L(p,d)=L(d,t)=L({+3}He,|a)=1 for a single state around 3950 could be for the doublet 
T$other: 0.75 ps {I+28-24} from ({+3}He,|a|g) 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
E$weighted average of 4320 {I15} in (d,t), 4320 {I20} in ({+3}He,|a) and 4340 {I10} in (p,d) 
J$L(p,d)=3. But L(d,t)=(2) is inconsistent 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 4432 {I10} in (p,d), 4430 {I20} in ({+3}He,|a), and 4460 {I15} in (d,t) 
J$L(p,d)=L(d,t)=L({+3}He,|a)=2 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$weighted average of 4487 {I10} in (p,d), 4490 {I20} in ({+3}He,|a) 
J$L(pol p,d)=3 and L+1/2 transfer from analyzing power 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 4926 {I10} in (p,d), 4920 {I20} in ({+3}He,|a), and 4940 {I15} in (d,t) 
J$L(p,d)=2 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 5128 {I10} in (p,d), 5130 {I20} in ({+3}He,|a), and 5130 {I15} in (d,t) 
J$L(pol p,d)=L(pol {+3}He,|a)=L(d,t)=2 and L+1/2 transfer from analyzing power. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
E$weighted average of 5316 {I10} in (p,d) and 5320 {I15} in (d,t) 
J$L(pol p,d)=3 and L+1/2 transfer from analyzing power. But L(d,t)=2 is inconsistent 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 5484 {I10} in (p,d), 5490 {I20} in ({+3}He,|a), and 5490 {I15} in (d,t) 
J$L(pol p,d)=2 and L+1/2 transfer from analyzing power 


level_energy_unit: KEV
level_spin_parity: 1/2,3/2-
level_comment:
E$weighted average of 5790 {I10} in (p,d), 5760 {I20} in ({+3}He,|a), and 5790 {I15} in (d,t) 
J$L(p,d)=L(d,t)=L({+3}He,|a)=1 


level_energy_unit: KEV
level_comment:
E$weighted average of 6009 {I10} in (p,d), 6000 {I20} in ({+3}He,|a), and 6010 {I15} in (d,t) 
J$1/2-,3/2- from L(d,t)=1; 3/2+,5/2+ from L({+3}He,|a)=2; (7/2-) from L(pol p,d)=(3) and L+1/2 from analyzing power. It is possible that there are three separate levels near this energy 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$weighted average of 6158 {I10} in (p,d), 6150 {I20} in ({+3}He,|a), 6160 {I15} in (d,t) and 6157 {I13} in {+1}H({+38}K,|g) E=res. 
J$L(pol p,d)=L(pol {+3}He,|a)=L(d,t)=2 and L+1/2 transfer from analyzing power 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$from (p,d). Other: 6286 {I13} from {+1}H({+38}K,|g) E=res 
J$L(p,d)=2. (5/2+) from expected L=0 resonances from 3+ g.s. in {+38}K in {+1}H({+38}K,|g) E=res 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
E$weighted average of 6467 {I10} in (p,d), 6450 {I30} in (d,t) and 6450 {I2} in {+1}H({+38}K,|g) E=res. 
J$L(p,d)=L(d,t)=2. (5/2+) from expected L=0 resonances from 3+ g.s. in {+38}K in {+1}H({+38}K,|g) E=res 


level_energy_unit: KEV
level_comment:
$d|s/d|W(mb/sr)=3.6 {I2} 
L$0 also from 1984Ra22 
$B(>)=0.27 (normalized value to |b-decay) (1984Ra22) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(mb/sr)=1.7 {I1} 
E$other: 5300 for the 5100+5500 doublet (1984Ra22) 
L$0 for the 5100+5500 doublet (1984Ra22) 
$B(>)=0.19 {I2} (1984Ra22) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(mb/sr)=1.70 {I15} 
E$other: 8100 (1984Ra22) 
L$other: (0+1) (1984Ra22) 
$B(>)=0.20 {I3} (1984Ra22) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W(mb/sr)=0.9 {I1} 
E$other: 9000 (1984Ra22) 
L$other: (0+1) (1984Ra22) 
$B(>)=0.10 {I2} (1984Ra22) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
S$others: 4.0 (1980Oh06), 7.0 (1975Ka10), 1.96 or 1.41 or 1.34 (1989Ab01), 3.0 (1984Sm04), 2.98 (1980Ho18), 4.3 (1975Ro27), 4.2 (1972Ma23),3.7 (1968Ko11) 
$ d|s/d|W(max)=3.4 mb/sr 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
S$others: 0.48 or 1.20 or 0.56 (1989Ab01), 1.4 (1975Ka10), 1.5 (1975Ro27), 1.9 (1972Ma23), 1.82 (1968Ko11) 
$ d|s/d|W(max)=0.80 mb/sr 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
S$others: 0.20 (1989Ab01), 0.17 (1975Ka10), 0.21 (1972Ma23), 0.58 (1968Ko11) 
$ d|s/d|W(max)=0.75 mb/sr 


level_energy_unit: KEV
level_comment:
$ 1980Oh06 interpret this state as 9/2- state populated by L=2, J=3/2 transfer from 3740, 3- state in {+40}Ca with C{+2}S=1.86 
$ d|s/d|W(max)=0.038 mb/sr 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
L$2 from 1968Ko11 
S$others: 0.95 (1975Ka10), 1.1 (1972Ma23), 1.48 (1968Ko11) 
$ d|s/d|W(max)=0.90 mb/sr 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
L$ 2 for 6910 group in 1975Ka10 
S$others: 0.14 (1975Ka10) for L=2, J|p=5/2+ 
$ d|s/d|W(max)=0.15 mb/sr 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$ 7920 (1972Ma23) and 7970 (1975Ka10) probably correspond to 7924+7972 doublet 
S$others: 0.33 (1975Ka10,1972Ma23) 
$ d|s/d|W(max)=0.43 mb/sr 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$from L-1/2 transfer based on analyzing power (1980Lu03) 
L$from 1965Ya04, 1965Bo15, 1965Gl02, 1965Cl04, 1971Ra35, 1981Gr05 
S$others: 6.6 (1968Ly01), 4.2 (1965Ya04), 4.0 (1965Cl04), 4.3 (1971Ra35), 10 (1973Ro18), 9.2 (1975Ap01), 8.0 (1980Lu03), 0.8 (1981Gr05) 


level_energy_unit: KEV
level_comment:
E$other: 2470 {I30} (1965Ya04) 
L$from 1965Ya04, 1965Bo15, 1965Gl02, 1965Cl04, 1971Ra35, 1981Gr05 
S$others: 1.6 (1968Ly01), 1.9 (1965Ya04), 1.3 (1971Ra35), 3.0 (1973Ro18), 3.9 (1975Ap01), 3.5 (1980Lu03), 0.6 (1981Gr05) 


level_energy_unit: KEV
level_comment:
E$other: 2800 {I30} (1965Ya04) 
L$from 1965Ya04, 1965Bo15, 1965Gl02, 1971Ra35 
S$other: 0.43 (1971Ra35) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$from L+1/2 transfer based on analyzing power (1980Lu03) 
S$other: 3.9 (1980Lu03) 
L$ 2 (1965Gl02) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E$weighted average of values from 1973BoXR, 1973Ke05 and 1976Ve01. 
E$2467 {I1} (1973Ke05), 2467.9 {I10} (1976Ve01) 
T$from 1988Al05 (including 5% uncertainty due to stopping power). Others: 180 fs {I55} (1973Ke05), 159 fs {I+28-21} (1983Ma47), 250 fs {I6} (1973BoXR) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$weighted average of values from 1973BoXR, 1973Ke05 and 1976Ve01. 
E$2795 {I1} (1973Ke05), 2797.6 {I13} (1976Ve01) 
J$7/2 from 2797|g(|q) in 1968Le06 
T$from 1983Ma47. Others: >11 ps (1973Ke05), >5.5 ps (1973BoXR) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: PS
level_comment:
J$1155|g(|q) and 3953|g(|q) is consistent with 1/2,3/2,5/2; but 3952|g is most likely a doublet with 3939|g from 3939 level. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: S
level_comment:
E$E(p){-cm}= 386 keV {I13}. 
$|w|g<1.16 meV with a single-sided 68% C.L. or <3.5 meV with a 95% C.L. (2016Lo03) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: S
level_comment:
E$E(p){-cm}= 515 keV {I13}. 
$|w|g<8.6 meV with a single-sided 68% C.L. or <26 meV with a 95% C.L. (2016Lo03) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
E$E(p){-cm}= 679 keV {I2}. 
$|w|g=120 meV {I+50-30}(stat){I+20-60}(sys) at the 68% C.L. Possible misprint in text at pg 3 in 2016Lo03 with |w|g=120 meV {I+20-30}(stat) {I+20-60}(sys) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: S
level_comment:
E$E(p){-cm}= 386 keV {I13}. Resonance energy given by the authors (2016Lo03) but was not observed due to beam intensities and measurement times 
$|w|g<1.16 meV with a single-sided 68% C.L. or <3.5 meV with a 95% C.L. 2018Ch08 report <2.54 meV with a 90% C.L. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: S
level_comment:
E$E(p){-cm}= 515 keV {I13}. Resonance energy given by the authors (2016Lo03) but was not observed due to beam intensities and measurement times 
$|w|g<8.6 meV with a single-sided 68% C.L. or <26 meV with a 95% C.L. 2018Ch08 report <18.4 meV with a 90% C.L. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
MOME2$from HF spectrum measurement (2019Kl06). 
J$from the Adopted Levels of {+39}Ca in the ENSDF database (2018 update). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
E$from literature, energy of transition depopulating this level is shifted due to lifetime effects. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2-)
level_lifetime_unit: PS
level_comment:
T$from |t=22 ps {I+6-7} where statistical ( 1 ps ) and systematic (+4-6 ps) uncertainties are added in quadrature. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: PS
level_comment:
T$from |t=37 ps {I+2-5} where statistical ( 1 ps ) and systematic (+2-5 ps) uncertainties are added in quadrature. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Double |b decay (|e|e) is possible, but only limits have been set on half-life from measurements 
$T{-1/2}: experimental limits from 2|e|e decay (2001Be79,1999Be64): >3.0|*10{+21} y for 0-neutrino mode; >5.9|*10{+21} y for 2-neutrino mode 
$Evaluated rms charge radius=3.4776 fm {I19} (2013An02) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.85 {I9} (L=3) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_comment:
J$L(|a,|a')=L({+3}He,n)=L(p,t)=0 from 0+; E0 excitation in (e,e') 
T$weighted average of 2.21 ns {I10} in (n,n') and 2.15 ns {I8} in (p,p'|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.01 {I1} (L=3) 
$Adopted (1977En02) proton stripping spectroscopic factor<0.7 (L=2) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L({+3}He,n)=L(p,t)=3 from 0+; E3 excitation in (e,e') 
MOMM1$from tilted-foil hyperfine field IPAC in (|a,|a')(1979Ni04) and recoil into gas in (|a,|a') (1976Ja16). Other: 1.56 {I30} (IMPAC, relative to g-factor for 4491 level in (|a,|a'), 1987Ma25) 
T$from (p,p'|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.16 {I4} (L=0), 0.48 {I13} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.01 {I1} (L=1), 0.55 {I6} (L=3) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=L({+3}He,n)=L(p,t)=2 from 0+; E2 excitation in (e,e') and (|g,|g') 
T$weighted average of 40 fs {I7} in (p,|g), 29 fs {I+10-6} in (|g,|g'), 36 fs {I14} in (n,n'|g), and 33 fs {I7} in (p,p'|g) 
$Adopted (1977En02) neutron stripping spectroscopic factor<0.2 (L=2) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(p,t)=5 from 0+; E5 excitation in (e,e') 
T$weighted average of 295 ps {I5} in (|a,|a'|g), 272 ps {I8} in (p,p'|g), and 0.38 ns {I8} in (HI,xn|g) 
MOMM1$IPAD method in (p,p'|g) (1974He13) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.96 {I19} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.84 {I9} (L=3) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=L({+6}Li,d)=L(p,p')=2 from 0+; E2 excitation in (e,e') 
T$weighted average of 0.15 ps {I7} in (p,|g) and 94 fs {I17} in (p,p'|g) and 79 fs {I+11-9} in (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L({+6}Li,d)=L(p,p')=4 from 0+; |g(|q) in (p,'|g) 
T$weighted average of 0.19 ps {I4} in (n,n'|g), 0.225 ps {I35} in (p,p'|g), and 0.16 ps {I+13-4} in (p,|g) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$spin from |g(|q) in (HI,xn|g) and |g|g(|q) in (p,|g); parity from L(d,n)=L({+3}He,d)=3 from 3/2+ and L(d,t)=L({+3}He,|a)=2 from 7/2- 
T$from (p,p'|g). Other: 69 fs {I55} in (p,|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.77 {I13} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.91 {I10} (L=3) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=2 from 0+; E2 excitation in (e,e') 
T$weighted average of 42 fs {I15} from (p,p'|g) and 38 fs {I+20-10} from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$L(p,t)=L({+6}Li,d)=1 from 0+ 
T$weighted average of 42 fs {I14} from (p,p'|g) and 15.2 fs {I+23-18} (|g,|g') 
$2004To07 in (HI,xn|g) propose this as 1- member of K|p=0- band, not observed by 2004To07 
$Adopted (1977En02) neutron pickup spectroscopic factor<0.01 (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.05 {I2} (L=1), <0.13 (L=3) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$L({+3}He,d)=3 and L(d,n)=1+3 from 3/2+; analyzing power in (pol p,p') 
T$from (p,p'|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.14 {I4} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.05 {I2} (L=1), 0.24 {I4} (L=3) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(|a,|a')=L(p,t)=L({+6}Li,d)=3 from 0+ 
T$weighted average of 0.27 ps {I8} in (p,|g) and 0.35 ps {I4} in (p,p'|g) 
$2004To07 in (HI,xn|g) propose this as (3-) member of K|p=0- band, not observed by 2004To07 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.05 {I2} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.50 {I7} (L=1), <0.1 (L=3) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$L({+6}Li,d)=4 from 0+; 913.3|g stretched E2 to 2+; band assignment in (HI,xn|g). 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=L(p,t)=L({+6}Li,d)=L(pol p,p')=3 
T$from (p,p'|g) 
$2004To07 in (HI,xn|g) propose this as possible (3-) member of K|p=0- band, not observed by 2004To07 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.04 {I1} (L=0), 0.24 {I4} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.18 {I2} (L=1), <0.2 (L=3) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
J$from analyzing power in (pol p,p') with L=3; L({+3}He,d)=1 and L(d,n)=1+3 from 7/2+. 
T$from (p,p'|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.20 {I4} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.16 {I2} (L=1), 0.44 {I8} (L=3) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(p,t)=L({+6}Li,d)=L(p,p')=2 from 0+ 
T$from (|g,|g'). Others: <35 fs from (p,|g), <10 fs from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,|a)=2 from 7/2-; 2439.8|g to 5-, 1301.8|g, 1682.4|g and 3026.8|g to 2+ 
T$from (p,|g). Other: 104 fs {I28} from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$L(p,t)=L({+3}He,n)=1 from 0+ 
T$from (|g,|g'). Other: <10 fs from (p,p'|g) 
$Adopted (1977En02) neutron pickup spectroscopic factor=0.06 {I2} (L=2) 
$Adopted (1977En02) proton stripping spectroscopic factor=0.40 {I7} (L=1), <0.5 (L=3) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$1899.8|g and 7112.9|g to 0+, 1485|g and 3206.8|g to 2+; L({+3}He,d)=1 from 3/2+; L(d,n)=1(+3) from 3/2+ 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
J$L(p,p')=5 from 0+; L(d,t)=L({+3}He,|a)=0+2 from 7/2- 
T$weighted average of 35 fs {I21} in (p,p'|g) and 76 fs {I28} in (p,|g) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: PS
level_comment:
J$|g to 4+ and band assignment in (HI,xn|g) 
$2004To07 in (HI,xn|g) proposed this as (5-) member of K|p=0- band 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=1 from 3/2+; L({+3}He,|a)=2; L(p,p')=3; not 3- from (p,|g) 
T$weighted average of 0.22 ps {I7} in (p,|g) and 0.149 ps {I35} in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L({+6}Li,d)=4. Note that L(p,t)=(2) is inconsistent and tentative. 
T$from (p,p'|g). Other: 0.18 ps {I+10-5} in (p,|g) 
J$ 1990En08 ASSIGNED 3+ BASED ON J=2,3 FROM G DECAY MODE; BUT G'S TO 2+, 3- AND 3+ ALLOW 4+ ALSO 


level_energy_unit: KEV
level_spin_parity: (2-,3,4+)
level_lifetime_unit: PS
level_comment:
J$1993.6|g and 2374.2|g to 2+ and 2009.5|g to 4-. However, L(p,t)=0 for a level at 7625 could indicate there may be a separate level, if this assignment is correct. 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,n)=1 and L({+3}He,d)=3 from 3/2+; 2080.6|g to 4-; analog of the 29.8, 3- level in {+40}K, see 1966Er05 in ({+3}He,d) 
T$from (p,|g). Other: <10 fs in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (3,4,5-)
level_lifetime_unit: FS
level_comment:
J$2155.8|g to 4- and 4032.5|g to 3-; J=(3,4,5) from |g feeding in (p,|g) (1990Ki07) 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=L(p,p')=4 from 0+. Note that L(p,t)=(3) is inconsistent and tentative. 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=L({+6}Li,d)=L({+3}He,n)=L(p,p')=2 from 0+; E2 excitation in (|g,|g'); but L(p,t)=4 from 0+ for a level at 8085 is inconsistent and it could imply that there may be a separate level if the assignment is correct. 
T$from (|g,|g'). Other: <28 fs in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$spin=1 from dipole excitation in (|g,|g'); L(p,p')=3 and L({+6}Li,d)=1 from 0+ 
T$from (|g,|g'). Other: <14 fs in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$2505.3|g and 4229.4|g to 2+ and 2521.2|g to 4-. Possible 3643.1|g to 5- would disfavor 2- and 3+. L(d,n)=1+3 from 3/2+ for 8113 and 8135 doublet 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (LE 3)-
level_comment:
E$from (p,p') 
J$L(d,n)=1 from 3/2+; 1315|g and 2364|g to 1-. But L({+6}Li,d)=4 from 0+ is suggested for a 8270 group 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_lifetime_unit: FS
level_comment:
J$8322.2|g to 0+, 2038.0|g and 4586.2|g to 3- 
T$weighted average of 83 fs {I28} in (p,|g) and 42 fs {I21} in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L({+3}He,|a)=2 from 7/2-, L(p,p')=3 from 0+, L(d,n)=1+3 from 3/2+; M2 excitation in (e,e'); analog of the 800, 2- level in {+40}K, see 1966Er05 in ({+3}He,d) 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: (1-,2-,3-)
level_lifetime_unit: FS
level_comment:
J$2581.3|g to 1-, 4747.0|g to 3-; L({+3}He,|a)=(2) from 7/2-. But L(p,t)=0 from 0+ for a level at 8483 is inconsistent and it is unlikely the same level based on RUL for the 4747.0|g, unless L(p,t)=0 is questionable. 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(p,t)=L(p,p')=5 from 0+, L(d,n)=L({+3}He,d)=3 from 3/2+; analog of the 891, 5- level in {+40}K, see 1966Er05 in ({+3}He,d) 
T$from (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L({+6}Li,d)=2 from 0+; 3722.1|g, 5581.8|g and 8933.7|g to 0+, 2352.2|g and 5197.8|g to 3-, 2905.0|g to 3+ 


level_energy_unit: KEV
level_spin_parity: 4-
level_comment:
J$L(d,t)=L({+3}He,|a)=0 from 7/2-, L(p,p')=5 from 0+. 2004To07 in (HI,xn|g) propose (7-) for this level, but |g's to 3- and 4- states are inconsistent with this assignment. 


level_energy_unit: KEV
level_spin_parity: (7-)
level_uncertain: ?
level_comment:
E$it is possible that this level is the same as the 9031.9 seen in other reactions and the 4542|g reported by 2004To07 in (HI,xn|g) could correspond to 4540.2|g in (p,|g). But the most intense 3418|g from 9031.9 level is not reported by 2004To07 
J$band assignment in (HI,xn|g) 


level_energy_unit: KEV
level_spin_parity: (2,3)-
level_comment:
J$2096.0|g to 4-, 2259.2|g and 3307.0|g to 1-; L(d,n)=1 from 3/2+ 
E$ 9197 10 IN 1990En08 (FROM 1966Gr03) IS PROBABLY SAME AS 9209.8 
E$1969Fu01 in (d,n) make their 9228 level correspond to 9211 level in (p,p') 


level_energy_unit: KEV
level_spin_parity: (1-,2,3-)
level_comment:
J$2276.1|g to 1- and 2941.4|g to 3-. Possible 9225.6|g to 0+ would disfacvor 3- 
J$ BUT L=1 FROM 3/2+ FOR 9228 (IN G) 


level_energy_unit: KEV
level_spin_parity: (7)-
level_comment:
E$from (p,p') 
J$L(p,p')=7. But L({+6}Li,d)=6 for a 9240 group 
E$ 9237 3 IN 1990En08 (FROM 1972Gr26) IS PROBABLY SAME AS 9246.0 OR A MIXTURE OF 9227.4+9246.0 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$log| {Ift}=5.4 from 4-; 937.7|g to 2-, 4113.5|g to 2+ 
$|G{-|a}/|G{-p}=0.0119 {I5} from {+40}Sc |e decay 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$9403.7|g to 0+, 2822.2|g, 3119.6|g and 5667.7|g to 3-, 2291.1|g to 4-; L(p,p)=1 from 3/2+; |g|g(|q) in (p,|g) give J=2 
T$from (p,p),(p,|a): resonances 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$from (p,|g). Other: 9535.2 {I14} in (p,p):resonances 
J,T$from (p,p),(p,|a):resonances. L(p,p)=L(d,n)=1 from 3/2+ 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$log| {Ift}=5.6 from 4-; L(p,p)=1 from 3/2+; |g|g(|q) in (p,|g) gives J=3 
T$from (2J+1)|*|G=3.4 keV for the 9603+9605 levels in (p,p),(p,|a):resonances, and |G=0.19 keV {I5} from (|g,|g') for the 9605 level. 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_lifetime_unit: KEV
level_comment:
J$|g's to 0+ and 2+; M1 or E2 excitation in (e,e'). L({+6}Li,d)=2 for a 9870 group and a doublet at 9868 suggested by 1980St17 in (e,e') could indicate there is a separate level with J|p=2+ 
T$from (|g,|g') 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$spin=4 from |g|g(|q) in (p,|g); observed |a decay from this level in {+40}Sc |e decay implies |p=natural 


level_energy_unit: KEV
level_spin_parity: (3-,4+,5-)
level_comment:
E$from {+40}Sc |e decay 
J$log| {Ift}=7.3 from 4-; observed |a decay from this level in {+40}Sc |e decay implies |p=natural 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$T=0+1 
J$|g's to 1-, 3-, 3+; L(p,p)=1 from 3/2+ for 10263+10268; |p=natural from (p,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$$ from (p,p),(p,|a):resonances 
J$(1,3)- in (p,p),(p,|a):resonances with L(p)=1 from 3/2+; log| {Ift}=6.2 from 4- 


level_energy_unit: KEV
level_spin_parity: (3,5)-
level_comment:
E$from (p,|g) 
J$log| {Ift}=5.7 from 4-; |a decay of this level in {+40}Sc |e decay implies |p=natural 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$(1-,2,3,4+) from 5118.0|g and 6842.8|g to 2+, 7010.5|g to 3-; J|p=(4+,5-) from (p,p),(p,|a):resonances for a level at 10751 


level_energy_unit: KEV
level_spin_parity: (3-,4+,5-)
level_comment:
J$log| {Ift}=6.3 from 4-; L({+6}Li,d)=5 for 10800 group; |a decay of this level in {+40}Sc |e decay implies |p=natural 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
E$from (p,|g) 
J$log| {Ift}=7.2 from 4-; |a decay of this level in {+40}Sc |e decay implies |p=natural; 4079.1|g, 5358.2|g to 2+ 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
E$from 1970De30 in (p,p),(p,|a):resonance. 11088 {I12} in {+40}Sc |e decay 
J$log| {Ift}=7.1 from 4-; 4+(1-,3-) for a 11901 level from 1970De30 in (p,p),(p,|a):resonance. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_comment:
E$from (p,p),(p,|a):resonances 
J$log| {Ift}=5.5 from 4-; |a decay of this level in {+40}Sc |e decay implies |p=natural; (1,2-,3) from (p,p),(p,|a):resonances 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: EV
level_comment:
J$L({+3}He,n)=0; IAR state 
$%|a=93 {I9} to {+36}Ar g.s.; %|a<3% to first 2+ in {+36}Ar; %p<5% ro {+39}K g.s. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (4+)
level_comment:
J$L({+6}Li,d)=4, but L(|a,|a')=3 for a 12450 group is inconsistent and could indicate there may be a separate level 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(LAB)=1006 {I3} 
$%p=0.072 {I11}, %|a=8.2|*10{+-4} {I20} 
$E|a=2089 {I6}. |G{-|a}/|G{-p}=0.0119 {I5} 
E$weighted average of 9360 {I3} (from E(p)) and 9362 {I6} (from E|a) 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
$E(p)(LAB)=1752 {I4} 
$%p=0.0013 {I4}, %|a=1.9|*10{+-4} {I10} 
E$weighted average of 10126 {I4} (from E(p)) and 10129 {I8} (from E|a) 
$E|a=2780 {I8}. |G{-|a}/|G{-p}=0.14 {I5} 


level_energy_unit: KEV
level_spin_parity: (3,5)-
level_comment:
$E(p)(LAB)=2089 {I4} 
$%p=0.0094 {I14}, %|a=7.8|*10{+-4} {I20} 
E$weighted average of 10471 {I4} (from E(p)) and 10465 {I7} (from E|a) 
$E|a=3082 {I7}. |G{-|a}/|G{-p}|>1 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(LAB)=2211 {I10} 
$%p=3.5|*10{+-4} {I20}, %|a=6.9|*10{+-4} {I20} 
E$weighted average of 10596 {I10} (from E(p)) and 10599 {I7} (from E|a) 
$E|a=3203 {I7}. |G{-|a}/|G{-p}=2.0 {I7} 


level_energy_unit: KEV
level_spin_parity: (3-,4+,5-)
level_comment:
$E(p)(LAB)=2423 {I9} 
$%p=8|*10{+-4} {I3}, %|a=4.2|*10{+-4} {I20} 
E$weighted average of 10814 {I9} (from E(p)) and 10819 {I7} (from E|a) 
$E|a=3401 {I7}. |G{-|a}/|G{-p}|>0.5 


level_energy_unit: KEV
level_spin_parity: (3-,4+,5-)
level_comment:
$E(p)(LAB)=2912 {I5} 
$%p=5.1|*10{+-4} {I20}, %|a=2.4|*10{+-4} {I10} 
E$weighted average of 11315 {I5} (from E(p)) and 11306 {I7} (from E|a) 
$E|a=3839 {I7}. |G{-|a}/|G{-p}|>1 


level_energy_unit: KEV
level_spin_parity: (3,5)-
level_comment:
$E(p)(LAB)=3308 {I10} 
$%p=7|*10{+-4} {I3}, %|a=9|*10{+-5} {I10} 
E$weighted average of 11723 {I4} (from E(p)) and 11727 {I7} (from E|a) 
$E|a=4218 {I7}. |G{-|a}/|G{-p}|>0.2 


level_energy_unit: KEV
level_spin_parity: (3,5)-
level_comment:
$E(p)(LAB)=3584 {I10} 
$%p=1.0|*10{+-4} {I10}, %|a=5.0|*10{+-4} {I20} 
$E|a=4462 {I7}. |G{-|a}/|G{-p}=5 {I2} 


level_energy_unit: KEV
level_spin_parity: (3,5)-
level_comment:
$E(p)(LAB)=3649 {I10} 
$%p=1.2|*10{+-4} {I10}, %|a=1.6|*10{+-4} {I10} 
$E|a=4519 {I9}. |G{-|a}/|G{-p}=1.3 {I7} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$B(E3)=0.0164 {I17} (same for 3 sets), 0.0171 {I17} (same for 2 sets), 0.0179 {I18}, 0.0197 {I20}, with different optical model parameter sets (2010Kr06). 
$|b{-3}R=0.49 ({+6}Li,1982Co12); 1.15 ({+11}B,1981Hn01); 1.29 {I18} ({+28}Si,1986Vi02) 
$|b{-3}R(p,p')/|b{-3}R({+13}C,{+13}C')=1.3 (1977Bo17) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_comment:
$|b{-5}R=0.53 ({+6}Li,1982Co12); 1.15 ({+11}B,1981Hn01) 
$|b{-5}R(p,p')/|b{-5}R({+13}C,{+13}C')=1.9 (1977Bo17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$E|a(lab)=5497 
E$from 1982Pr05 
J$isotropic angular distribution of capture |g rays (1982Pr05) 
$|G{-|a0}=80 ev {I10}, |G=81 ev {I10} (1987He05) 
$Proton decay to 2522 level in {+39}K based on observed 2522.4 {I2} |g ray in 1982Pr05; |a decay to 2814 level in {+39}K based on observed 2814 |g ray in 1987He05. 
$1982Pr05 have tentative evidence for four weaker |g-decay branches from this level with E|g=1504, 1611, 2013 and 2202 and |DE|g=3 keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$unresolved multiplet with L=0 from |s(|q) distribution and cross section below 3% of that to g.s. (1975Fo04). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$3904.39 {I4} (1990Ki07), 3904.37 {I6} (1988Sc23) 
T$from 1971Ma03 by DSAM. Others: 13 fs {I4} (1968Do12), 17 fs {I4} (1968Li12) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
E$5278.80 {I6} (1990Ki07), 5279.0 {I3} (1988Sc23) 
T$from 1968Do12 by DSAM. Other: |>0.13 ps (1968Li12) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: FS
level_comment:
E$5613.52 {I3} (1990Ki07), 5613.59 {I15} (1988Sc23) 
T$from 1968Li12 by DSAM. Other: >0.55 ps (1968Do12) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
E$6285.15 {I4} (1990Ki07), 6285.17 {I10} (1988Sc23) 
T$weighted average of 0.26 ps {I+11-6} (1968Do12), and 0.35 ps {I21} (1968Li12) 
J$spin from |g|g(|q) and |g(pol) together (1967Le12) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
E$7466.35 {I7} (1990Ki07), 7466.7 {I3} (1988Sc23) 
T$weighted average of 7 fs {I4} (1968Do12) and 18 fs {I14} (1990Ki07) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
E$7561.17 {I7} (1990Ki07), 7561.3 {I3} (1988Sc23) 
T$from 1968Do12 by DSAM. Other: 36 fs {I13} (1968Li12) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LE
level_comment:
E$from 1990Ki07. Other: 7695.07 {I15} from 1988Sc23) is discrepant and is probably a typo. 
T$from 1968Li12 by DSAM 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$S(P,G)=2.4 {I10} 
$E(p)(lab)=1307.7 {I4} 
J$parity from Adopted Levels, but positive parity from 1967Le12 based on a resonance formation fit 


level_energy_unit: KEV
level_spin_parity: (3,4,5)-
level_comment:
$E(p)(lab)=3804 {I3} 
$|G{-p}(to 3352)=0.07 keV {I3} 
$Resonance strengths: 0.9 eV {I4} to g.s., 1.0 eV {I5} (first 2+ to g.s.), 2.3 eV {I8} (first 3- to g.s.) (1985Se16). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=3815 {I3} 
$|G{-p}(to 3352)=0.66 keV {I13} 
$Resonance strengths: 0.7 eV {I3} to g.s., 1.2 eV {I6} (first 2+ to g.s.), 0.5 eV {I2} (first 3- to g.s.) (1985Se16). 


level_energy_unit: KEV
level_comment:
$E(p)(lab)=3841 {I3} 
$|G{-p}(to 3352)=0.030 keV {I17} 
$Resonance strengths: 0.7 eV {I3} to g.s., 1.5 eV {I6} (first 2+ to g.s.), 1.1 eV {I5} (first 3- to g.s.) (1985Se16). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=0.8 
J$from (1-,2) in 1987WaZI, 1- in 1970De30 
E$analog of 2757 level in {+40}K (1970De30) 
$E(p)(lab)=1919.1 {I5}, |G{-p}=1.6 keV (1987WaZI) 
$E(p)(lab)=1921 {I2}, S{-|a}=3.4 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=3.4 
E$may be the same level as 10275 
$E(p)(lab)=2002 {I2}, S{-|a}=3.4 eV (1970De30); this resonance may be the same as 1997 in 1987WaZI 


level_energy_unit: KEV
level_spin_parity: (1,3)-
level_comment:
J$from (1-,3-) in 1987WaZI and (1,3)- from 1970De30 
$E(p)(lab)=2057.1 {I5}, |G{-p}=0.11 keV, |G{-|a}=0.001 keV (1987WaZI) 
$E(p)(lab)=2059 {I2}, S{-|a}=22 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1,3)-
level_comment:
$S{-p}=27 
J$1- in 1987WaZI, 3- in 1970De30 
$E(p)(lab)=2088.8 {I5}, |G{-p}=1.1 keV, |G{-|a}=0.0050 keV (1987WaZI) 
$E(p)(lab)=2089 {I2}, S{-|a}=1.7 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J$(0+,1-,2+) from (p,|a) in 1970De30 
$E(p)(lab)=2145.8 {I5}, |G{-p}=0.50 keV, |G{-|a}=0.0028 keV (1987WaZI) 
$E(p)(lab)=2147 {I2}, S{-|a}=8.8 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1,3)-
level_comment:
$S{-p}=3.1 
J$1- in 1987WaZI, 3- in 1970De30 
$E(p)(lab)=2173.1 {I5}, |G{-p}=0.15 keV, |G{-|a}=0.001 keV (1987WaZI). 
$E(p)(lab)=2174 {I2}, S{-|a}=6.5 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J$also from 1970De30 
$E(p)(lab)=2244.4 {I5}, |G{-p}=1.2 keV, |G{-|a}=0.010 keV (1987WaZI). 
$E(p)(lab)=2245 {I2}, S{-|a}=18 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$from (p,|a) in 1970De30. Other: 0+ from (p,p') in 1987WaZI 
$E(p)(lab)=2270.3 {I5}, |G{-p}=0.16 keV, |G{-|a}=0.025 keV (1987WaZI) 
$E(p)(lab)=2272 {I2}, S{-|a}=41 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$from 1987WaZI, (1,3)- from (p,|a) in 1970De30 
$E(p)(lab)=2326.4 {I5}, |G{-p}=0.15 keV, |G{-|a}=0.0050 keV (1987WaZI) 
$E(p)(lab)=2327 {I2}, S{-|a}=63 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$S{-p}=15 
J$from 1987WaZI. Other: 1- from (p,p) in 1970De30, 0+ and 2+ favored in (p,|a) in 1970De30 
E$1970De30 suggest it could be the analog of 3230, 1- level in {+40}K; however, the 3230 level has J|p=2- from Adopted Levels of {+40}K. It could be that this level in 1970De30 corresponds to the 10618.8, 2- level above from 1987WaZI 
$E(p)(lab)=2352.2 {I5}, |G{-p}=0.030 keV, |G{-|a}=0.0080 keV (1987WaZI) 
$E(p)=2354 {I3}, S{-|a}=14 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$3 is also possible (1987WaZI) 
$E(p)(lab)=2364.7 {I5}, |G{-p}=1.1 keV, |G{-|a}=0.0015 keV (1987WaZI) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
J$3 is also possible (1987WaZI) 
$E(p)(lab)=2387.6 {I5}, |G{-p}=0.59 keV, |G{-|a}=0.0050 keV (1987WaZI) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$S{-p}=1.2 
J$(1,3)- for 2390 resonance in (p,|a) but (1,2)+ and L(p,p)=0 for 2390 resonance in (p,p) in 1970De30. The 2390 resonance in (p,|a) in 1970De30 could correspond to the 2387.5 resonance in 1987WaZI 
$E(p)(lab)=2389.1 {I5}, |G{-p}=0.350 keV, |G{-|a}=0.004 keV (1990Bu02) 
$E(p)(lab)=2390 {I3}, S{-|a}=16 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$S{-p}=17 
J$from 1987WaZI, 1- from (p,p) in 1970De30 
$E(p)(lab)=2398.4 {I5}, |G{-p}=2.0 keV (1987WaZI) 
$E(p)(lab)=2400 {I3}, S{-|a}<1 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=0.5 
J$also from 1970De30 
$E(p)(lab)=2407.6 {I5}, |G{-p}=1.5 keV, |G{-|a}=0.060 keV (1987WaZI) 
$E(p)(lab)=2408 {I3}, S{-|a}=200 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$S{-p}=0.7 
J$from 1987WaZI, (1,2)+ in 1970De30 
$E(p)(lab)=2425.5 {I5}, |G{-p}=1.1 keV (1987WaZI) 
$E(p)(lab)=2426 {I3}, S{-|a}<1 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=1.5 
J$also from 1970De30 
$E(p)(lab)=2473.9 {I5}, |G{-p}=2.2 keV, |G{-|a}=0.0060 keV (1987WaZI). 
$E(p)(lab)=2475 {I3}, S{-|a}=16 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$S{-p}=35 
J$1- in 1987WaZI; later corrected to 3- by the same group Other: 1- from (p,p) in 1970De30, (1-,2+) from (p,|a) in 1970De30 but 2+ is favored 
E$1970De30 suggest it could be the analog of 3365, 1- level in {+40}K 
$E(p)(lab)=2515.4 {I5}, |G{-p}=1.0 keV, |G{-|a}=0.010 keV (1987WaZI). 
$E(p)(lab)=2514 {I3}, S{-|a}=77 eV (1970De30); it could also correspond to the 2513.0 resonance in 1990Bu02 


level_energy_unit: KEV
level_spin_parity: 0(+)
level_comment:
J$from 1987WaZI, (1-,2+) from (p,|a) in 1970De30 
$E(p)(lab)=2538.1 {I5}, |G{-p}=0.50 keV, |G{-|a}=0.20 keV (1987WaZI) 
$E(p)(lab)=2539 {I3}, S{-|a}=220 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$S{-p}=13 
J$from 1987WaZI, (1-) from (p,p)in 1970De30 
$E(p)(lab)=2552.0 {I5}, |G{-p}=6.0 keV (1987WaZI) 
$E(p)(lab)=2552 {I3}, S{-|a}<1 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$3(-) from 1987WaZI and (3-,4+) from (p,|a) in 1970De30 
$E(p)(lab)=2569.2 {I5}, |G{-p}=0.025 keV, |G{-|a}=0.0009 keV (1987WaZI) 
$E(p)(lab)=2569 {I3}, S{-|a}=24 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=30 
J$from (1-,2-) in 1987WaZI and 1- in 1970De30 
E$analog of 3481 level in {+40}K (1970De30) 
$E(p)(lab)=2588.7 {I5}, |G{-p}=2.5 keV (1987WaZI) 
$E(p)(lab)=2588 {I3}, S{-|a}=10 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$also from (p,|a) in 1970De30 
$E(p)(lab)=2598.2 {I5}, |G{-p}=0.040 keV, |G{-|a}=0.005 keV (1990Bu02) 
$E(p)(lab)=2599 {I3}, S{-|a}=24 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=6.9 
J$also from 970De30 
$E(p)(lab)=2652.9 {I5}, |G{-p}=5.0 keV, |G{-|a}=0.040 keV (1987WaZI) 
$E(p)(lab)=2652 {I3}, S{-|a}=110 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
J$1+,2+ in 1987WaZI; later corrected to 3+ by the same group 
$E(p)(lab)=2653.9 {I5}, |G{-p}=0.70 keV (1987WaZI) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=15 
$E(p)(lab)=2671.3 {I5}, |G{-p}=2.0 keV, |G{-|a}=0.0080 keV (1987WaZI) 
$E(p)(lab)=2673 {I3}, S{-|a}=53 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=30 
J$also from 1970De30 
$E(p)(lab)=2689.9 {I5}, |G{-p}=7.0 keV (1987WaZI) 
$E(p)(lab)=2689 {I3}, S{-|a}=100 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 0(+)
level_comment:
$E(p)(lab)=2692.7 {I5}, |G{-p}=0.20 keV, |G{-|a}=0.020 keV (1987WaZI) 
$E(p)(lab)=2695 {I3}, S{-|a}=27 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$S{-p}=20 
E$analog of 3630 level in {+40}K (1970De30) 
$E(p)(lab)=2735 {I3}, S{-|a}<1 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1,3)-
level_comment:
J$also from 1970De30 
$E(p)(lab)=2739.2 {I5}, |G{-p}=0.20 keV, |G{-|a}=0.0020 keV (1987WaZI). 
$E(p)(lab)=2742 {I3}, S{-|a}=35 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$S{-p}=2.1 
J$from 1987WaZI, (1,3)- in 1970De30 
$E(p)(lab)=2747.7 {I5}, |G{-p}=5.0 keV, |G{-|a}=0.010 keV (1987WaZI). 
$E(p)(lab)=2750 {I3}, S{-|a}=9 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1,3)-
level_comment:
$S{-p}=0.7 
J$(1-) from 1970De30, 3(-) in 1987WaZI, L(p,p)=1 from 3/2+ 
$E(p)(lab)=2765.1 {I5}, |G{-p}=0.10 keV, |G{-|a}=0.012 keV (1987WaZI) 
$E(p)(lab)=2767 {I3}, S{-|a}=270 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$S{-p}=1.0 
J$2+ from 1970De30 
$E(p)(lab)=2785.9, |G{-p}=0.50 keV, |G{-|a}=0.002 keV (1990Bu02) 
$E(p)(lab)=2789 {I3}, S{-|a}=6 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: (1+)
level_comment:
J$0,2 are also possible (1987WaZI) 
$E(p)(lab)=2826.1 {I5}, |G{-p}=0.35 keV (1987WaZI) 
$E(p)(lab)=2825 {I3}, S{-|a}=11 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 0(+)
level_comment:
J$from 1987WaZI, 4+(1-,3-) from (p,|a) for a 11091 level in 1970De30 could indicate a different level 
$E(p)(lab)=2831.9 {I5}, |G{-p}=0.10 keV, |G{-|a}=0.0060 keV (1987WaZI) 
$E(p)(lab)=2834 {I3}, S{-|a}=6.1 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 0-
level_comment:
$S{-p}=5.2 
E$analog of 3768 level in {+40}K (1970De30) 
$E(p)(lab)=2855 {I3}, S{-|a}<1 eV (1970De30); it could correspond to the 2850.1 resonance in 1987WaZI 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$also from 1970De30 
$E(p)(lab)=2862.3 {I5}, |G{-p}=0.040 keV, |G{-|a}=0.006 keV (1990Bu02) 
$E(p)(lab)=2865 {I3}, S{-|a}=21 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$also from 1970De30 
$E(p)(lab)=2872.7 {I5}, |G{-p}=0.11 keV, |G{-|a}=0.0014 keV (1987WaZI) 
$E(p)(lab)=2875 {I3}, S{-|a}=19 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$also from 1970De30 
$E(p)(lab)=2912.0 {I5}, |G{-p}=0.080 keV, |G{-|a}=0.0030 keV (1987WaZI) 
$E(p)(lab)=2914 {I3}, S{-|a}=31 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$S{-p}=175 
E$analog of 3867 level in {+40}K (1970De30) 
J$also from 1970De30 
$E(p)(lab)=2958.4 {I5}, |G{-p}=2.8 keV, |G{-|a}=0.0014 keV (1987WaZI). 
$E(p)(lab)=2962 {I3}, S{-|a}<1 eV (1970De30). |G{-p}=25 keV from S{-p}=175 keV assuming |G=|G{-p} is much greater than |G{-p}=2.8 keV, which could indicate a different level at 11317 {I3} 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$S{-p}=3 
J$from 1987WaZI, (1,2,3)- in 1970De30 
$E(p)(lab)=2977.6 {I5}, |G{-p}=3.0 keV (1987WaZI). 
$E(p)(lab)=2972 {I3}, S{-|a}<1 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$also from 1970De30 
$E(p)(lab)=2993.4 {I5}, |G{-p}=0.080 keV, |G{-|a}=0.012 keV (1987WaZI) 
$E(p)(lab)=2996 {I3}, S{-|a}=190 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$also from 1970De30 
$E(p)(lab)=3011.4 {I5}, |G{-p}=0.325 keV, |G{-|a}=0.016 keV (1990Bu02) 
$E(p)(lab)=3013 {I3}, S{-|a}=190 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$(1-,2+) from 1970De30 
$E(p)(lab)=3070.5 {I5}, |G{-p}=0.475 keV, |G{-|a}=0.041 keV (1990Bu02) 
$E(p)(lab)=3073 {I3}, S{-|a}=440 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=3079.5 {I5}, |G{-p}=4.0 keV, |G{-|a}=0.030 keV 
$E(p)(lab)=3083 {I3}, S{-|a}=52 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
J$from 1987WaZI, but |p=natural from (p,|a) in 1970De30 is inconsistent 
$E(p)(lab)=3100.8 {I5}, |G{-p}=0.80 keV 
$E(p)(lab)=3099 {I3}, S{-|a}=18 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$(1-,2+) from 1970De30 
$E(p)(lab)=3121.2 {I5}, |G{-p}=1.4 keV, |G{-|a}=0.0040 keV 
$E(p)(lab)=3119 {I3}, S{-|a}=400 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$(0+,1-,2+) from (p,|a) in 1970De30 
$E(p)(lab)=3132.2 {I5}, |G{-p}=2.500 keV, |G{-|a}=0.065 keV (1990Bu02) 
$E(p)(lab)=3134 {I3}, S{-|a}=360 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$also from (p,|a) in 1970De30 
$E(p)(lab)=3165.7 {I5}, |G{-p}=0.10 keV, |G{-|a}=0.0050 keV 
$E(p)(lab)=3169 {I3}, S{-|a}=70 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$also from (p,|a) in 1970De30 
$E(p)(lab)=3188.3 {I5}, |G{-p}=0.200 keV, |G{-|a}=0.015 keV (1990Bu02) 
$E(p)(lab)=3192 {I3}, S{-|a}=170 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$E(p)(lab)=3199.0 {I5}, |G{-p}=5.0 keV, |G{-|a}=0.34 keV 
$E(p)(lab)=3200 {I3}, S{-|a}=950 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$also from (p,|a) in 1970De30 
$E(p)(lab)=3212.5 {I5}, |G{-p}=1.030 keV, |G{-|a}=0.140 keV (1990Bu02) 
$E(p)(lab)=3214 {I3}, S{-|a}=1500 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2(+)
level_comment:
$E(p)(lab)=3217.3 {I5}, |G{-p}=0.026 keV, |G{-|a}=0.10 keV 
$E(p)(lab)=3221 {I3}, S{-|a}=57 eV (1970De30) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=3385.5 {I5}, |G{-p}=0.070 keV, |G{-|a}=0.015 keV (1990Bu02) 
$ 1987WaZI GIVE EP(LAB)=3385.2, |G{-p}=0.80 KEV, |G{-|a}=0.010 KEV 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=3502.1 {I5}, |G{-p}=0.750 keV, |G{-|a}=0.320 keV (1990Bu02) 
$ 1987WaZI GIVE |G{-p}=0.24 KEV, |G{-|a}=0.60 KEV 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$E(p)(lab)=3504.8 {I5}, |G{-p}=0.050 keV, |G{-|a}=0.50 keV 
J$2+ in 1987WaZI; later corrected to 4+ by the same group 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=3513.7 {I5}, |G{-p}=0.30 keV, |G{-|a}=0.050 keV 
J$1- in 1987WaZI, later corrected to 3- by the same group 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=3572.0 {I5}, |G{-p}=0.770 keV, |G{-|a}=0.975 keV (1990Bu02) 
$ 1987WaZI GIVE |G{-p}=1.3 KEV, |G{-|a}=0.60 KEV 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=3581.9 {I5}, |G{-p}=3.5 keV, |G{-|a}=0.030 keV 
J$1- in 1987WaZI; later corrected to 3- by the same group 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$E(p)(lab)=3632.6 {I5}, |G{-p}=0.010 keV, |G{-|a}=0.030 keV 
J$2+ in 1987WaZI, later corrected to 3- by the same group 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$E(p)(lab)=3835.5 {I5}, |G{-p}=1.1 keV, |G{-|a}=0.01 keV 
J$2+ in 1987WaZI; later corrected to 4+ by the same group 
$|G{-a} of 0.10 listed in 1987WaZI was later corrected to 0.01 by the same group 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$E(p)(lab)=3998.2 {I5}, |G{-p}=0.425 keV, |G{-|a}=0.009 keV (1990Bu02) 
$ 1987WaZI GIVE |G{-p}=0.20 KEV, |G{-|a}=2.5 KEV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2)-
level_comment:
S$for L=3; 0.01 for L=1 
$S=0.58 {I18} for L=3 
$((2J{-f}+1)/(2J{-i}+1))S=0.02 for L=1; ; 0.72 {I22} for L=3 


level_energy_unit: KEV
level_spin_parity: (2)-
level_comment:
E$triplet: 9405+9412+9419 
$S=0.43. S=0.35 for 9404, (3)- level with L=1 
$((2J{-f}+1)/(2J{-i}+1))S=1.14 for 9404+9408 


level_energy_unit: KEV
level_spin_parity: (0)-
level_comment:
$S=0.44 {I8} 
$((2J{-f}+1)/(2J{-i}+1))S=0.11 {I2} 
E$from 1969Fu01. Several levels near this energy in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{-0}=0.0105 {I35} 
S$unweighted average of 0.0140 eV {I13} (2002Ha13) and 0.007 eV {I3} (1982Mo05) 
T$using adopted branching |G{-0}/|G=0.877 {I8} 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{-0}=0.039 {I12} 
J$2+ from 1982Mo05, but measured intensity ratio in 2002Ha13 is consistent with J=1 
S$unweighted average of 0.027 eV {I7} (2002Ha13) and 0.050 eV {I6} (1982Mo05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{-0}=0.189 {I20} 
S$weighted average of 0.221 eV {I36} (2002Ha13), 0.190 eV {I20} (1982Mo05), 0.13 eV {I6} (1977La15), 0.18 eV {I3} (1968Me06) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
$|G{-0}=0.452 {I20} 
S$weighted average of 0.49 eV {I7} (2002Ha13), 0.450 eV {I20} (1982Mo05), 0.41 eV {I8} (1977La15), 0.47 eV {I6} (1968Me06) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{-0}=0.187 {I17} 
T$using adopted branching |G{-0}/|G=1. 1982Mo05 report |G{-0}/|G=0.84 {I6} without indicating the observation of other |g branches other than the ground transition and no such observation is from other studies. So this |g branching value is not considered in Adopted Gammas. 
S$weighted average of 0.176 eV {I32} (2002Ha13) and 0.190 eV {I17} (1982Mo05) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$|G{-0}=0.128 {I34} 
S$unweighted average of 0.161 eV {I13} (2002Ha13) and 0.094 eV {I12} (1982Mo05) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$|G{-0}=1.36 {I25} 
E$from 1982Mo05. Other: 9864.6 (1987Gu01) 
T$weighted average of 0.100 keV {I24} (1987Gu01) and 0.110 keV {I30} (1962Ra07). Most of the |G is ascribed to proton decay (1962Ra07) 
S$from 1962Ra07. |G{-0}{+2}/|G=44 meV {I18} from (1982Mo05) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_comment:
$|G{-0}=0.80 {I26} 
E$from 1987Gu01. 
T$weighted average of 0.90 keV {I21} (1987Gu01) and 1.06 keV {I20} (1962Ra07). Most of the width is ascribed to proton decay (1962Ra07) 
S$from 1962Ra07 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: EV
level_comment:
$|G{-0}=5.5 {I8} 
E,J$from 1982Mo05. Other: 10321.0 (1987Gu01). J|p=1+ in Adopted Levels. J|p=2+ from 1961Ec03. 
S$from 1982Mo05. Others: 6.6 eV {I8} (1987Gu01), 3.60 eV {I24} (1961Ec03) 
$|G from 1982Mo05. Others: 91 eV {I15} (1987Gu01), 10.3 eV {I17} (1961Ec03) 
$|G{-|g}=6.4 eV {I9} (1982Mo05), 4.5 eV {I6} (1961Ec03) 
$|G{-p}=20 eV {I5} (1982Mo05), 5.8 eV {I18} (1961Ec03) 
$|G{-0}/|G=0.21 {I2} (1982Mo05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$E=3352 {I5} (1984Ha29) 
E$from 1984Ha29 
$Monopole matrix element M(E0)=2.66 e*fm{+2} {I41}, weighted average of 2.53 e*fm{+2} 41 (1978Gr02), 3.6 fm{+2} {I11} (1968St20). From monopole strength |r{+2}{E0}=[M(E0)]{+2}/[e{+2}R{+4}] where R=R{-0}A{+1/3} with R{-0}=1.2 fm, one gets |r{+2}{E0}=0.025 {I8} 
$Width of e{++}e{+-} pair emission |G{-|p}=3.7|*10{+-7} eV {I23} (1970St10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$E=3740 {I100}, J|p=3- (1970It01) 
T$from B(E3)|^. Other: 30 ps {I6} from |G{-|g} in 1970St10 
$B(E3)|^=0.0167 {I16}, unweighted average of 0.0100 {I11} (1963Bl04, from |b{-3}=0.066 {I7}), 0.0190 {I21} (1956He83, from |b{-3}=0.125 {I14} with 10% uncertainty from normalization added by the evaluator), 0.0211 {I25} (1969Ei03), 0.0149 {I7} (1973Ha13), 0.0183 {I7} (1970It01, average of 0.0185 {I7} and 0.0180 {I7}), 0.0166 {I12} (1971He08, from B(E3)(W.u.)=24.9 {I18}) 
$|G{-|g}=15 |meV {I3} (1970St10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
$E=3900 {I100} (1970It01) 
T$from B(E2)|^. Other: 29 fs {I6} from |G{-|g} in 1970St10. 
$B(E2)|^=0.0088 {I10}, weighted average of 0.015 {I5} (1963Bl04, from |b{-2}=0.016 {I5}), 0.0084 {I10} (1969Ei03), 0.0090 {I10} (1973Ha13). Other: 0.012 (1970It01, from B(E2)(W.u.)=3.0) 
$|G{-|g}=0.016 eV {I3} (1970St10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_comment:
$E=4490 {I100}, J|p=5- (1970It01) 
J$from 1970It01 and 1963Bl04 
$B(E5)|^=2.12|*10{+-4} {I22}, weighted average of 2.07|*10{+-4} {I22} (1963Bl04, from |b{-5}=0.048 {I5}), 2.8|*10{+-4} {I8} (1970It01, from B(E5)(W.u.)=17 {I5} average of 20 {I+9-5} and 16.3 {I45}). Others: 1.62|*10{+-4} {I10} or 2.95|*10{+-4} {I25} (1971He08, depending on shape factor) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$E=6290 {I100}, J|p=3- (1970It01) 
E$from B(E3)|^ here and the adopted |g branchings in Adopted Gammas 
$B(E3)|^=0.0031 {I3} (1970It01, from B(E3)(W.u.)=4.6 {I4}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
E,J$from 1963Bl04. This level could correspond to the 6931, 3- or the 6938 level in Adopted Levels. 1969Ei03 report a composite of 6930,3- and 6910,2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E,J$from 1978Gr03. 1969Ei03 report a composite of 6930,3- and 6910,2+ 
$|G{-0}=0.190 eV {I6} (1978Gr03) 
$B(E2)|^=0.00070 {I9} (1969Ei03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
E,J$from 1969Ei03. According to 1969Ei03, it could be an unresolved triplet of 6910 (2+), 6930 (3-) and 6950 (1-). Other: 6900 reported in 1963Bl04 
$B(E3)|^=0.0011 {I3} (1963Bl04, from |b{-3}=0.007 {I2}), while 0.0092 {I13} from 1969Ei03 for the 6930 component of the 6910+6930 composite; however, T{-1/2}=1.4 ps {I6} and no observation of g.s. transition from the 6931.29, J|p=3- level in |g studies indicates a much smaller B(E3)|^. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
$E=6940 {I70} (1971Fa15) 
$E=6950 {I100} (1970It01) 
E,J$from 1978Gr03. E=6940 {I70} from 1971Fa15, 6950 {I100} from 1970It01 
$|G{-0}=0.51 eV {I5} (1978Gr03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+,4+)
level_comment:
$E=7900 {I100} (1970It01) 
J$from 1970It01; 4+ from 1963Bl04; could correspond to the 7872, 2+ level or 7928, 4+ level in Adopted Levels 
$B(E4)|^=0.00028 {I5} (1963Bl04, from |b{-4}=0.011 {I2}). Others: B(E2)|^=0.0053 or B(E4)|^=0.00053 from B(E2)(W.u.)=1.3 or B(E4)(W.u.)=5 in 1970It0) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_comment:
$E=8500 {I100} (1970It01) 
J$from 1963Bl04. Other: (2+,4+,5-) (1970It01) 
$B(E5)|^=1.16|*10{+-4} {I13} (1963Bl04, from |b{-5}=0.027 {I3}). Other: B(E2)|^=0.0016 or B(E5)|^=0.00012 from B(E2)(W.u.)=0.4 or B(E5)(W.u.)=7.0 in 1970It01 


level_energy_unit: KEV
level_spin_parity: 1+,2+
level_comment:
$E=9870 {I10}, Darmstadt=9868 (1995Pe01) 
$E=9868 {I5}, probably a doublet of 2+ and 1+ separated by 5 keV (1980St17) 
E,J$from 1980St17, probably a doublet of 2+ and 1+ separated by 5 keV. Other: 9870 {I10} with J|p=1+,2+ from 1995Pe01. 
$B(M1)|^=0.32 {I9} (1995Pe01), 0.43 {I4} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$E=10320 {I10}, Darmstadt=10318 (1995Pe01) 
$E=10319 {I5}, B(M1)=1.12 {I7} (1980St17, probably quoted from 1979Gr09) 
$E=10319 {I5}, B(M1)=1.12 {I7} (1979Gr09) 
$E=10340 {I60}, width=7.0 eV {I+29-22} (1971Fa15) 
E$from 1979Gr09, probably the isobaric analog of the 2730 level in {+40}K 
$B(M1)|^=1.06 {I8} (1995Pe01), 1.11 {I5} (quoted by 1995Pe01 from Darmstadt group), 1.12 {I7} (1979Gr09) 
$|G=7.0 eV {I+29-22} (1971Fa15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$from 1974Na15, 1d{-3/2} state, |DE=1.4 MeV 
$|G=9.2 MeV {I13} (1974Na15) 
$E=10.4E3 {I14}, width=9.2 MeV {I13}, 1d{-3/2} state (1974Na15) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$E=10670 {I10}, Darmstadt=10676 (1995Pe01) 
E,J$from 1995Pe01. Other: 10676 (quoted by 1995Pe01 from Darmstadt group) 
$B(M2)|^=0.16 {I5} (1995Pe01), 0.15 {I3} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$11760 {I10}, Darmstadt=11775 (1995Pe01) 
E,J$from 1995Pe01. Other: 11775 (quoted by 1995Pe01 from Darmstadt group) 
$B(M1)|^=0.35 {I3} (1995Pe01) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$12040 {I10}, Darmstadt=12044 (1995Pe01) 
E,J$from 1995Pe01. Other: 12044, J|p=2- (quoted by 1995Pe01 from Darmstadt group); J|p=2+ in Adopted Levels 
$B(M1)|^=0.09 {I4} (1995Pe01) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$E=12350 {I10}, Darmstadt=12332 (1995Pe01) 
E,J$from 1995Pe01. Other: 12332, J|p=(1-,2+) (quoted by 1995Pe01 from Darmstadt group) 
$B(M2)|^=0.41 {I21} (1995Pe01) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$E=12750 {I10}, Darmstadt=12749 (1995Pe01) 
E,J$from 1995Pe01. Other: 12749 (quoted by 1995Pe01 from Darmstadt group) 
$B(M2)|^=0.13 {I6} (1995Pe01), 0.06 {I6} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_spin_parity: 1+,2-
level_comment:
$E=12830 {I10}, Darmstadt=12830 (1995Pe01) 
E,J$from 1995Pe01, 2- is less probable. Other: 12830 (quoted by 1995Pe01 from Darmstadt group) 
$B(M1)|^=0.14 {I3} (1995Pe01), 0.06 {I4} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$E=13050 {I10}, Darmstadt=13049 (1995Pe01) 
E,J$from 1995Pe01. Other: 13049 (quoted by 1995Pe01 from Darmstadt group) 
$B(M1)|^=0.26 {I4} (1995Pe01), 0.25 {I2} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$E=13150 {I10}, Darmstadt=13147 (1995Pe01) 
E,J$from 1995Pe01. Other: 13147 (quoted by 1995Pe01 from Darmstadt group) 
$B(M2)|^=0.48 {I6} (1995Pe01), 0.34 {I9} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$E=13480 {I10} (1995Pe01) 
E,J$from 1995Pe01. Other: 13480, J|p=2-,(1+) (quoted by 1995Pe01 from Darmstadt group) 
$B(M1)|^=0.26 {I10} (1995Pe01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E=13.6E3 {I4}, width=12.0 MeV {I9}, 2s{-1/2} state (1974Na15) 
E$from 1974Na15, 2s{-1/2} state, |DE=0.4 MeV 
$|G=12.0 MeV {I9} (1974Na15) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
$E=13670 {I10}, Darmstadt=13666 (1995Pe01) 
E,J$from 1995Pe01. Other: 13666 (quoted by 1995Pe01 from Darmstadt group) 
$ B(M2)|^=0.66 {I16} (1995Pe01), 0.27 {I6} (quoted by 1995Pe01 from Darmstadt group) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$E=13900 {I100} (1964Ho06) 
E,J$from 1964Ho06, |DE=100 keV 
$B(E2)|^=7.3|*10{+-4} {I8} (1964Ho06, from B(E2)(W.u.)=0.18 {I2}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
S,L$from 1990Ol02, 5% uncertainty in |b{-L}. Others: |b{-L}=0.359 {I21} (1977Ba49), 0.33 (1987Al03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
J$from (pol p,p') (1968Wi05,1982Ho13,1982Bl10,1987Fr05,1989Le04) 
S$others: 1.40, 1.38, 1.35, 1.32 from E=25, 30, 35, 40 MeV data (1972Gr26) 
$B(E3)(W.u.)=28.7 {I20} (1972Gr26) 
$Other |b{-3}=0.340 (1982Bl10) 
$ d|s/d|W=11300 |mb/sr, %EWSR=22.1 (1972Gr26) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
J$from (pol p,p') (1987Fr05,1984Ho16) 
S$others: 0.42, 0.43, 0.42, 0.43 from E=25, 30, 35, 40 MeV data (1972Gr26), 0.43 (1984Ho16) 
$Other |b{-2}=0.133 (1982Bl10) 
$ d|s/d|W=2240, %EWSR=3.2 (1972Gr26) 
$B(E2)(W.u.)=2.05 {I20} (1972Gr26) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_comment:
J$from (pol p,p') (1987Fr05,1982Bl10) 
S$others: 0.91, 0.86, 0.83, 0.80 from E=25, 30, 35, 40 MeV data (1972Gr26) 
$Other |b{-5}=0.215 (1982Bl10) 
$d|s/d|W=1560, %EWSR=6.4 (1972Gr26) 
$B(E5)(W.u.)=20.6 {I21} (1972Gr26) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
S$others: 0.14, 0.15, 0.12 from E=30, 25, 40 MeV data (1972Gr26), 0.11 (1984Ho16) 
$d|s/d|W=575 
$B(E2)(W.u.)=0.26 {I5}, %EWSR=0.3 (1972Gr26) 


level_energy_unit: KEV
level_comment:
S$others: 0.15, 0.16, 0.13 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.2 (1972Gr26) 
$d|s/d|W=122 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
S$others: 0.36, 0.42, 0.31 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=1.2 (1972Gr26) 
$d|s/d|W=194 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$from (pol p,p') (1982Ho13) 
S$others: 0.20, 0.23, 0.17 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.7 (1972Gr26) 
$d|s/d|W=268 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
S$others: 0.46, 0.43, 0.41, 0.40 from E=25, 30, 35, 40 MeV data (1972Gr26) 
$d|s/d|W=1471 
$B(E3)(W.u.)=3.1 {I3}, %EWSR=3.4 (1972Gr26) 


level_energy_unit: KEV
level_comment:
S$others: 0.17, 0.18, 0.17 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.5 (1972Gr26) 
$d|s/d|W=114 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
S$others: 0.41, 0.36, 0.33, 0.32 from E=25, 30, 35, 40 MeV data (1972Gr26) 
$d|s/d|W=975 
$B(E3)(W.u.)=2.5 {I3}, %EWSR=2.4 (1972Gr26) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$from (pol p,p') (1982Ho13) 
S$others: 0.24, 0.27, 0.21 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=1.1 (1972Gr26) 
$d|s/d|W=410 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
S$others: 0.44, 0.43, 0.42, 0.45 from E=25, 30, 35, 40 MeV data (1972Gr26), 0.42 (1984Ho16) 
$d|s/d|W=2316 
$B(E2)(W.u.)=2.25 {I23}, %EWSR=5.7 (1972Gr26) 


level_energy_unit: KEV
level_comment:
L$other: 3 (1965Gr11) 
S$others: 0.32, 0.40, 0.27 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=1.2 (1972Gr26) 
$d|s/d|W=164 


level_energy_unit: KEV
level_comment:
L$1972Gr26 did not resolve the 7278 and 7301 level and assigned L=(0,2) for a level at 7292 with %EWSR=0.3 
S$others: 0.10, 0.10, 0.09 from E=30, 25, 40 MeV data (1972Gr26) 
$d|s/d|W=25 {I4} 


level_energy_unit: KEV
level_comment:
S$others: 0.17, 0.20, 0.15 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.5 (1972Gr26) 
$d|s/d|W=33 {I5} 


level_energy_unit: KEV
level_comment:
E,L$1972Gr26 did not resolve this level from 7561 but assigned L=3 and (4), respectively 
S$others: 0.17, 0.19, 0.15 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.7 (1972Gr26) 
$d|s/d|W=221 


level_energy_unit: KEV
level_comment:
S$others: 0.20, 0.23, 0.19 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.8 (1972Gr26) 
$d|s/d|W=146 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$d|s/d|W=696 
S$others: 0.25, 0.28, 0.23 from E=30, 25, 40 MeV data (1972Gr26) 
$B(E2)(W.u.)=0.92 {I15}, %EWSR=1.8 (1972Gr26) 


level_energy_unit: KEV
level_comment:
$d|s/d|W=333 
$B(E4)(W.u.)=2.2 {I2}, %EWSR=1.7 (1972Gr26) 
S$others: 0.31, 0.34, 0.29 from E=30, 25, 40 MeV data (1972Gr26) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$d|s/d|W=269 
S$others: 0.17, 0.18, 0.16 from E=30, 25, 40 MeV data (1972Gr26), 0.21 (1984Ho16) 
$B(E2)(W.u.)=0.38 {I6}, %EWSR=1.0 (1972Gr26) 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
S$others: 0.17, 0.19, 0.15 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.7 (1972Gr26) 
$d|s/d|W=115 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$very weak state and assignment is tentative (1975No04). 
E$unresolved from 8196 in 1972Gr26, %EWSR=0.8 
S$others: 0.22 from E=25 data (1972Gr26) 
$d|s/d|W=15 {I4} 


level_energy_unit: KEV
level_comment:
E$unresolved from 8359 in 1972Gr26, but they assigned L=4 for E=8366 and associated it with a previously reported 8371 level. 
S$others: 0.32, 0.31, 0.31, 0.33 from E=25, 30, 35, 40 MeV data (1972Gr26) 
$d|s/d|W=348 
$B(E4)(W.u.)=2.0 {I2}, %EWSR=2.1 (1972Gr26) 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
J$from (pol p,p') (1985Ho14,1982Ho13) 
S$others: 0.27, 0.29, 0.25 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=1.7 (1972Gr26) 
$d|s/d|W=279 


level_energy_unit: KEV
level_comment:
E$8535 (1972Gr26) 
$d|s/d|W=169 
S$for E=8535, others: 0.20, 0.23, 0.18 from E=30, 25, 40 MeV data (1972Gr26) 
$%EWSR=0.6 (1972Gr26) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$from 1982Ho13 and 1984Ho16 
S$others: 0.18, 0.17, 0.17 from E=30, 25, 40 MeV data (1972Gr26), 0.16 (1984Ho16) 
$%EWSR=1.1 (1972Gr26) 
$d|s/d|W=439 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
S$others: 0.15, 0.17, 0.14 from E=30, 25, 40 MeV data (1972Gr26), 0.12 (1984Ho16) 
$%EWSR=0.9 (1972Gr26) 
$d|s/d|W=392 


level_energy_unit: KEV
level_comment:
S$others: 0.10, 0.10, 0.09 from E=30, 25, 40 MeV data (1972Gr26) 
S$0.28 for L=6 
$%EWSR=0.1 (1972Gr26) 
$d|s/d|W=42 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
E$doublet 
L$0,1 (1984Ho16) for second component 
S$from 1984Ho16 for a doublet at 9868 
J$1+ in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from lifetime=47 fs {I10}, weighted average of 64 fs {I19} (1968Ma05), 0.07 ps {I5} (1969Po04), 30 fs {I20} (1973Te04), 48 fs {I10} (1971Ma03), 40 fs {I16} (1972Si01) 


level_energy_unit: KEV
level_spin_parity: 5
level_lifetime_unit: PS
level_comment:
T$|t=392 ps 12 (1969Ma19, delayed coincidence), >7 ps (1969Po04) 
T$from 1969Ma19 by delayed coincidence. Other: >7 ps (1969Po04) 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: PS
level_comment:
T$|t=2.6 ps +14-7 (1968Ma05), 1.47 ps 30 (1969Po04), 1 ps (1973Te04), 
T$from 1969Po04. Other: 1.8 ps {I+10-5} (1968Ma05), 0.7 ps (1973Te04) 
J$1 is not ruled out; adopted J|p=0+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
T$from lifetime=135 fs {I26}, weighted average of 190 fs {I30} (1968Ma05), 150 fs {I70} (1969Po04), 110 fs {I20} (1973Te04) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
T$from lifetime=324 fs {I50}, weighted average of 260 fs {I80} (1968Ma05), 0.41 ps {I10} (1969Po04), 330 fs {I50} (1973Te04), 340 fs {I80} (1972Si01), 310 fs {I60} (1971Ma03) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$stretched dipole to J=3 and |g to J=5 
T$from lifetime=0.99 ps {I15}, weighted average of 0.95 ps {I+28-19} (1969An09), 0.83 ps {I20} (1969Po04), 1.10 fs {I15} (1973Te04) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$assigned to this level which was not resolved from 5613 by 1966Gr03 
T$from lifetime=61 fs {I22}, weighted average of 76 fs {I21} (1969An09), 30 fs {I30} (1973Te04). Other: T{-1/2}<70 fs (1969Po04) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
T$from 1969An09. Other: 10 fs {I10} (1973Te04), <70 fs (1969Po04) 
T$|t=0.06 ps 2 (1969An09), <0.10 ps (1969Po04), 15 fs 15 (1973Te04) 


level_energy_unit: KEV
level_spin_parity: 2,3
level_lifetime_unit: FS
level_comment:
T$from lifetime=246 fs {I30}, weighted average of 0.26 ps {I3} (1969An09), 0.17 ps {I9} (1969Po04), 240 fs {I30} (1973Te04) 
E$6025+6029 not resolved in 1966Gr03 
J$2- in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 2,3
level_lifetime_unit: PS
level_comment:
T$from lifetime=0.58 ps {I12}, weighted average of 0.56 ps {I19} (1969An09), 0.44 ps {I+17-12} (1969Po04), 0.70 fs {I12} (1973Te04) 
J$3+ in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 3
level_lifetime_unit: PS
level_comment:
T$from lifetime=0.50 ps {I5}, weighted average of 410 fs {I12} (1968Ma05), 0.57 ps {I10} (1969Po04), 0.50 fs {I5} (1973Te04) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
T$|t=0.19 ps 6 (1969An09), 170 fs 30 (1973Te04) 
T$from lifetime=174 fs {I30}, weighted average of 0.19 ps {I6} (1969An09), 170 fs {I30} (1973Te04) 


level_energy_unit: KEV
level_spin_parity: 2,3
level_lifetime_unit: FS
level_comment:
J$3- in Adopted Levels 
T$from lifetime=250 fs {I40}, weighted average of 0.25 ps {I7} (1969An09), 250 fs {I40} (1973Te04) 
T$|t=0.25 ps 7 (1969An09), 250 fs 40 (1973Te04) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
T$|t=120 fs 40 (1973Te04), 185 fs 65 (1972Si01) 
J$from 1972Si01 
T$from lifetime=138 fs {I40}, weighted average of 120 fs {I40} (1973Te04), 185 fs {I65} (1972Si01) 


level_energy_unit: KEV
level_comment:
L$1966Ni02, 1980Wi12 and 1989Ec01 
S$other: 0.32 (1968Ha31), 0.21 (1980Wi12, average of two values for different potentials). |DS=0 (1992Mo17) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_comment:
$1976Mo07 observed |a decay to {+36}Ar (g.s.,1970 and 4300 (multiplet)) and p decay to {+39}K (g.s.,2520 and higher levels) for a resoance at E=13.5-15.6 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_comment:
$1976Mo07 observed |a decay to {+36}Ar (g.s.,1970 and 4300 multiplet) and p decay to {+39}K (g.s.,2520 and higher levels) for a resoance at E=15.6-22.5 MeV 
L$2 from 1978Ta05, a weak L=0 component is also suggested in 1980Le25 from DWBA analysis. 


level_energy_unit: KEV
level_comment:
$%EWSR=0.2 (1981Va09) 
$E=3350 {I20}, L=0, |b{-L}*R=0.07 (1981Va09) 
$E=3350 (1974De42), 3350 (1970Sc24) 


level_energy_unit: KEV
level_comment:
S$others: 0.88 (1970Br07), 0.85 (1965Sp01), 0.90 (sharp cut-off) or 0.97 (smooth cut-off) (1968Bu10), 0.85 (1965Sp01) 
$%EWSR=11.6 (1981Va09) 
$E=3740 {I20}, L=3, |b{-L}*R=0.90 (1981Va09) 
$L=3 (1976Ru02,1974De42) 
$L=3, |b{-L}*R=0.88 (1970Br07) 
$E=3740 (1970Sc24) 
$L=3, |b{-L}*R=0.90 and 0.97 (1968Bu10) 
$E=3730 {I30}, L=3 (1967Li13) 
$E=3730, L=3, |b{-L}*R=0.85 (1965Sp01) 
$E=3730 {I30}, L=3 (1965Ba03) 


level_energy_unit: KEV
level_comment:
S$others: 0.34 (1965Sp01), |b{-L}=0.097 (1967Li13) 
$%EWSR=3.4 (1981Va09) 
$E=3900 {I20}, L=2, |b{-L}*R=0.37 (1981Va09) 
$L=2 (1976Ru02) 
$E=3900 (1970Sc24) 
$E=3900 {I30}, L=2, |b{-L}=0.097 (1967Li13) 
$E=3900, L=2, |b{-L}*R=0.34 (1965Sp01) 
$E=3900 {I30}, L=2 (1965Ba03) 


level_energy_unit: KEV
level_comment:
S$others: 0.38 (1970Br07), 0.53 (sharp cut-off) or 0.58 (smooth cut-off) (1968Bu10), 0.35 (1965Sp01) 
$%EWSR=0.2 (1981Va09) 
$E=4490 {I20}, L=5, |b{-L}*R=0.39 (1981Va09) 
$L=5 (1976Ru02,1974De42) 
$L=3, |b{-L}*R=0.38 (1970Br07) 
$E=4490 (1970Sc24) 
$L=5, |b{-L}*R=0.53 and 0.58 (1968Bu10) 
$E=4480 {I30}, L=5 (1967Li13) 
$E=4480, L=5, |b{-L}*R=0.35 (1965Sp01) 
$E=4480 {I30}, L=5 (1965Ba03) 


level_energy_unit: KEV
level_comment:
E$5250 {I20} in 1981Va09 and 5260 {I30} in 1967Li13 for the 5250+5280 doublet. 
$E=5250 {I20} (1981Va09), 5250 (1974De42), 5210+5250+5280 (1970Sc24) 
$E=5260 {I30} (1967Li13), 5250 (1965Sp01) 


level_energy_unit: KEV
level_comment:
L$assignment of L=4 in 1965Ba03 is erroneous according to 1967Li13 of the same authors 
S$others: |b{-L}=0.046 (1967Li13) 
$%EWSR=0.6 (1981Va09) 
$E=5630 {I20}, L=2, |b{-L}*R=0.13 (1981Va09) 
$E=5610+5620 (1970Sc24) 
$E=5620 {I30}, L=(2), |b{-L}=0.046 (1967Li13) 
$E=5620 (1965Sp01) 
$E=5620 {I30}, L=4 (1965Ba03), L=4 erroneously assigned (1967Li13, same authors) 


level_energy_unit: KEV
level_comment:
L$(1) from 1981Va09; L=1 from 1967Li13 and 1965Ba03. Other: L=3 with |b{-L}R=0.18 (1965Sp01) 
$E=5910 {I20}, L=(1) (1981Va09), 5900 (1974De42), 5910 (1970Sc24) 
$E=5900 {I30}, L=1 (1967Li13) 
$E=5900, L=3, |b{-L}*R=0.18 (1965Sp01) 
$E=5890 {I30}, L=1 (1965Ba03) 


level_energy_unit: KEV
level_comment:
E$from 1967Li13. Also reported in 1974De42 and 1970Sc24; not reported in 1981Va09 
$E=6030 (1974De42), 6030 (1970Sc24) 
$E=6020 {I30} (1967Li13) 


level_energy_unit: KEV
level_comment:
S$other: 0.40 (1965Sp01). 
$%EWSR=3.1 (1981Va09) 
$E=6290 {I20}, L=3, |b{-L}*R=0.36 (1981Va09) 
$L=3 (1976Ru02,1974De42) 
$E=6290 (1974De42), 6290 (1970Sc24) 
$E=6290 {I30},L=3 (1967Li13) 
$E=6280, L=3, |b{-L}*R=0.40 (1965Sp01) 
$E=6290 {I30}, L=3 (1965Ba03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$%EWSR=2.4 (1981Va09) 
$E=6570 {I20}, L=3, |b{-L}*R=0.31 (1981Va09) 
$L=3 (1976Ru02,1974De42) 
$E=6580 (1974De42) 
$E=6580 {I30}, L=3 (1967Li13) 
$E=6580, L=3, |b{-L}*R=0.31 (1965Sp01) 
$E=6560 {I30}, L=3 (1965Ba03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E,L,S$from 1961Sa04 and 1970Br07 only. A level at 6790 with adopted J|p=(2-) is reported in 1970Sc24. 
$L=3, |b{-L}*R=0.41 (1970Br07) 
$E=6790, adopted J|p=(2-) (1970Sc24) 


level_energy_unit: KEV
level_comment:
E$multiplet since several levels near this energy in Adopted Levels 
S$others: 0.21 for L=2 and 0.36 for L=3 (1965Sp01) 
L$others: L=1+(2) from 1967Li13 and 1965Ba03; none adopted by the evaluator since this level could be an unresolved multiplet. 
$E=6940 {I20}, L=(3), |b{-L}*R=0.37 (1981Va09) 
$E=6910+6930+6940 (1970Sc24) 
$E=6940 {I30}, L=1 (1967Li13) 
$E=6940, |b{-L}*R=0.21 for L=2 and 0.36 for L=3, L=1 possible (1965Sp01) 
$E=6940 {I30}, L=1 (1965Ba03) 


level_energy_unit: KEV
level_comment:
E$from 1967Li13. 
L$the assignment of L=(6) in 1965Ba03 should be discarded according to 1967Li13 of the same authors as 1965Ba03 
$E=7110 (1970Sc24) 
$E=7110 {I30} (1967Li13) 
$E=7120 {I30}, L=(6) (1965Ba03) 


level_energy_unit: KEV
level_comment:
L$from 1981Va09. Other: 4 (1965Ba03) 
S$other: |b{-L}=0.078 (1967Li13) 
$%EWSR=3.9 (1981Va09) 
$E=7900 {I20}, L=2, |b{-L}*R=0.28 (1981Va09) 
$E=7870 {I30}, L=(2), |b{-L}=0.078 (1967Li13) 
$E=7920 {I30} (1965Ba03) 


level_energy_unit: KEV
level_comment:
E$from 1967Li13 
L$from 1965Sp01, 1966Be19, 1967Li13 
S$from 1965Sp01. Other: |b{-L}=0.094 (1967Li13) 
$E=7870+7920 (1970Sc24) 
$E=7940 {I30}, L=4, |b{-L}=0.094 (1967Li13) 
$E=7920, L=4, |b{-L}*R=0.29 (1965Sp01) 


level_energy_unit: KEV
level_comment:
S$others: 0.24 (1965Sp01), |b{-L}=0.083 (1967Li13) 
$%EWSR=2.5 (1981Va09) 
$E=8100 {I20}, L=2, |b{-L}*R=0.22 (1981Va09) 
$E=8100 (1970Sc24) 
$E=8100 {I30}, L=(2), |b{-L}=0.083 (1967Li13) 
$E=8110, L=2, |b{-L}*R=0.24 (1965Sp01) 
$E=8090 {I30}, L=2 (1965Ba03) 


level_energy_unit: KEV
level_comment:
L$the assignment of L=5 by 1965Ba03 is incorrect according to 1967Li13 of the same authors as 1965Ba03 
S$others: 0.24 (1965Sp01), |b{-L}=0.083 (1967Li13) 
$%EWSR=1.1 (1981Va09) 
$E=8380 {I20}, L=4, |b{-L}*R=0.21 (1981Va09) 
$E=8380 (1970Sc24) 
$E=8380 {I30}, L=4, |b{-L}=0.083 (1967Li13) 
$E=8380, L=4, |b{-L}*R=0.24 (1965Sp01) 
$E=8370 {I30}, L=5 (1965Ba03), L=5 discarded by 1967Li13 of the same authors 


level_energy_unit: KEV
level_comment:
S$other: 0.19 (1965Sp01) 
$%EWSR=1.6 (1981Va09) 
$E=8600 {I20}, L=2, |b{-L}*R=0.17 (1981Va09) 
$E=8600 {I30} (1967Li13) 
$E=8590, L=2, |b{-L}*R=0.19 (1965Sp01) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
T$0.52 MeV {I8} from E=117 MeV data (1981Lu05). 
L$from 1981Va09. Other: 1 (1981Lu05) 
$%EWSR=0.4 (1981Va09) 
$E=10.6 {I2}, width=0.48 MeV {I5}, L=1 (1981Lu05), 99 MeV data 
$E=10.6 {I2}, width=0.52 MeV {I8}, L=1 (1981Lu05), 117 MeV data 
$E=10590 {I20}, L=(3), |b{-L}*R=0.10 (1981Va09) 


level_energy_unit: KEV
level_comment:
L$other: 0 (1983Br21) 
$%EWSR=1.5 (1981Va09) 
$E=11690 {I20}, L=2, |b{-L}*R=0.14 (1981Va09); E=11680, L=0 (1983Br21) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
T$0.36 MeV {I6} from E(beam)=117 MeV data (1981Lu05). 
L$from 1981Lu05 and 1983Br21. Other: L=(2) from 1981Va09 with |b{-L}R=0.07. other: 0+2 from |a decay to {+36}Ar g.s. (1982Zw01,1983Br21,1985Zw02) 
$%EWSR|?7 (1981Lu05) 
$E=13.8 {I3}, width=0.40 MeV {I8}, L=0 (1981Lu05), 99 MeV data 
$E=13.9 {I3}, width=0.36 MeV {I6}, L=0 (1981Lu05), 117 MeV data 
$E=13400 {I50}, L=(2), |b{-L}*R=0.07 (1981Va09); E=13260, L=0 (1983Br21) 


level_energy_unit: KEV
level_comment:
L$(0) from 1981Va09; L=0 from 1983Br21. 
$E=14070 {I50}, L=(0), |b{-L}*R=0.05 (1981Va09); E=14170, L=0 (1983Br21) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$others: 14.5 MeV {I3} (1981Lu05), average energy of 14300 for an excitation region of 13.3-15.3 MeV (1979Ro09) 
T$0.51 MeV {I7} from E(beam)=117 MeV data (1981Lu05). 
L$other: 1+2 for an excitation region with average energy of 14.3 MeV (1979Ro09) 
$|b{-L}{+2}=0.0041 for L=1 and 0.0036 for L=2 (1979Ro09) 
$E=14.5 {I3}, width=0.68 MeV {I8}, L=2 (1981Lu05), 99 MeV data 
$E=14.6 {I3}, width=0.51 MeV {I7}, L=2 (1981Lu05), 117 MeV data 
$E=14850 {I50}, L=2, |b{-L}*R=0.09 (1981Va09) 
$<E>=14300, |b{-L}{+2}=0.0041 for L=1 and 0.0036 for L=2 (1979Ro09) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
T$Other: 0.65 MeV from 1981Va09 
L$from 1981Lu05. Other: 1+2 (1979Ro09) with |b{-L}{+2}=0.0033 for L=1 and 0.0024 for L=2; 2 (1981Va09) with |b{-L}R=0.15 
$E=15.8 {I4}, width=0.63 MeV {I10}, L=3 (1981Lu05) 
$E=16000 {I50}, L=2, width=0.65 MeV, |b{-L}*R=0.15 (1981Va09) 
$<E>=16000, |b{-L}{+2}=0.0033 for L=1 and 0.0024 for L=2 (1979Ro09) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
T$2.53 MeV {I40} from E=117 MeV data and 2.56 MeV {I40} from E=130 data (1981Lu05), 3.26 MeV (1981Va09), 3.5 MeV {I3} (1975Mo04), 3.5 MeV {I3} (1976Yo02), 2.9 MeV {I6} (2001Yo07) 
S$other: 0.72 (1976Yo02), |b{-L}{+2}=0.0164 (1979Ro09), |b{-L}=0.14 (1974Ru01) 
$%EWSR=108 {I12} (2001Yo07) 
$E=17500 {I400}, width=4.95 MeV {I25} (1997Yo07) 
$E=17.84 MeV {I43}, width=2.89 MeV {I60}, L=2 (2001Yo07) 
$E=17.8 {I3}, width=2.25 MeV {I20}, L=2 (1981Lu05), 99 MeV data 
$E=17.7 {I2}, width=2.53 MeV {I40}, L=2 (1981Lu05), 117 MeV data 
$E=18.0 {I3}, width=2.56 MeV {I40}, L=2 (1981Lu05), 130 MeV data 
$E=18000 {I50}, L=2, width=3.26 MeV, |b{-L}*R=0.69 (1981Va09) 
$E=17.7 {I3}, width=2.5 MeV {I40} (1981Yo04) 
$E=17.9, width=3.5 MeV {I3} (1975Mo04) 
$<E>=18500, |b{-L}{+2}=0.0164 for L=2 (1979Ro09) 
$E=18.1 {I3}, width=3.5 MeV {I3}, |b{-L}*R=0.73 (1976Yo02), 96 MeV data 
$E=17.9 {I3}, width=3.4 MeV {I3}, |b{-L}*R=0.71 (1976Yo02),115 MeV data 
$E=18.25 {I25}, |b{-L}=0.14 for L=2 (1974Ru01) 


level_energy_unit: KEV
level_comment:
L$from 1979Ro09 and 1981Va09 
S$other: |b{-L}{+2}=0.0019 for L=0 and 0.0018 for L=2 (1979Ro09) 
$E=21100 {I50}, L=(2), width=1.95 MeV, |b{-L}*R=0.20; or L=(0), |b{-L}*R=0.18 (1981Va09) 
$<E>=21000, |b{-L}{+2}=0.0019 for L=1 and 0.0018 for L=2 (1979Ro09) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E,T,L$from 1997Yo07, 2001Yo07 
$%EWSR=62 {I+10-20} (2001Yo07) 
$E=23.36 MeV {I70}, width=5.34 MeV {I90}, L=1 (2001Yo07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_comment:
E,J$possible doublet or triplet, but from decay mode and DWBA fit to |s(|q), principally 1- (1968Ko02) 


level_energy_unit: KEV
level_comment:
$INTEGRATED=7.1 
E$others: 5247 {I10} for the triplet of 5212, 5249 and 5279 levels in Adopted Levels (1974De20), 5250 {I10} (1972Sc19) 


level_energy_unit: KEV
level_comment:
$INTEGRATED=1.53 
E$others: 6498 {I10} for the doublet of 6508 and 6543 levels in Adopted Levels (1974De20), 6510 {I10} (1972Sc19) 


level_energy_unit: KEV
level_comment:
$INTEGRATED=1.87 
E$others: 6911 {I11} for the triplet of 6909, 6931 and 6950 levels in Adopted Levels (1974De20) 


level_energy_unit: KEV
level_comment:
$INTEGRATED=0.79 
E$possibly 7113.1, 1- and 7113.7, 4- levels in Adopted Levels. Others: 7105 {I8} (1974De20) 


level_energy_unit: KEV
level_comment:
$INTEGRATED=0.30 
E$others: 7400 (1974De20) 
L$1974De20 quote L=6 from previous work for a 7400 level but no reference for that assignment is found. 


level_energy_unit: KEV
level_comment:
$INTEGRATED=0.89 
E$The 7453 {I9} reported in 1974De20 is considered as the same level as the 7477 level based on the fact that many levels above 6000 in 1974De20 are about 10 keV lower than values in 1974Se05 


level_energy_unit: KEV
level_comment:
$INTEGRATED=1.21 
E$others: 7619 {I15} (1974De20) 
L$from 1977SeZR. Brackets are added by the evaluator since it is inconsistent with J|p=(2-,3,4+) for the 7623.1 level from |g decay modes in (p,p'|g); however, if this assignment is correct it could indicate they are two separate levels 


level_energy_unit: KEV
level_comment:
$INTEGRATED=3.0 
E$this level corresponds to the 7702, 0+ level in Adopted Levels. Others: 7685 {I12} (1974De20); 1972Sc19 report a 3- level at 7690 {I30}, but 1974Se05 point out that it was misassigned by 1972Sc19 as the 3- level seen in {+3}He,d) at 7695 and is considered as the same level as the 7698 level. 


level_energy_unit: KEV
level_comment:
$INTEGRATED=0.28 
L$from 1977SeZR, inconsistent with the assignment of J|p=(1-,2-,3-) in Adopted Levels, see comments for this assignment. 


level_energy_unit: KEV
level_comment:
$T=2 IAR state (1979Fr04,1970Mc04) 
E$from 1974De20 
$93% {I9} |a decay to {+36}Ar g.s.; <3% |a decay to first 2+ in {+36}Ar; <5% p decay to {+39}K g.s. (1979Fr04). Others: 1970Mc04, 1970Ha10 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E,J$2004To07 propose this level as the 5- member of negative-parity band, based on systematics. These authors do not find any feeding transition to this level. 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
E$8465 {I12} (1966Er05), 8435 {I9} (1967Se10), 8460 (1968Ba64) 
E$from 1967Se10. 8465 {I12} from 1966Er05. According to 1973Te04 in ({+3}He,d|g) this level probably corresponds to 8425 level in their |g-ray study 


level_energy_unit: KEV
level_spin_parity: 2-
level_comment:
E$according to 1973Te04 this level is strongly fed in ({+3}He,d); probably corresponds to 8435 {I9} from 1967Se10 in ({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from Adopted Levels of {+40}Ca in ENSDF database, as quoted by 2022Gr04 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_comment:
$E{-r}=535.6 {I9} 
$|w|g=0.141 meV {14} from 3736|g yield, 0.138 meV {I14} from 3904|g yield, 0.139 meV {I20} from 8858|g yield. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: Y
level_comment:
J$from L(d,p)=3 and (pol d,p); configuration=|pf7/2 
MOMM1,MOME2$See compilation in 2014StZZ and recommended Q in 2013StZZ 
T$From a combination of methods consisting of triple-to-double coincidence ratios method (TDCR) with the liquid scintillation counting and the thermal ionization mass spectrometry (TIMS) with isotope dilution for absolute isotopic composition (2012Jo04). Others: 1.03|*10{+5} y {I7} (1991Kl06, 1990Fi13), 1.01|*10{+5} y {I10} (1991Pa10), 1.03|*10{+5} y {I4} (1989Ku33), 1.03|*10{+5} y {I4} (1974Ma30) revised to 1.14|*10{+5} y {I5} by 1991Kl06, 1.3|*10{+5} y {I2} (1972Em01), 0.75|*10{+5} y {I11} (1962Dr02) revised to 1.60|*10{+5} y {I30} by 1991Kl06, 1.1|*10{+5} y {I3} (1953Br71) revised to 1.90|*10{+5} y {I60} by 1991Kl06 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 0.42 ps {I10} from {+38}Ar(|a,n|g), 0.28 ps {I9} from {+41}K(p,n|g), and 0.47 ps {I5} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g), all from DSAM. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: NS
level_comment:
T$weighted average of 0.46 ns {I5} from (HI,xn|g), 0.56 ns {I14} from {+41}K(p,n|g), and 0.506 ns {I12} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: >3.1 ps from {+38}Ar(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$weighted average of 2.4 ps {I6} from {+38}Ar(|a,n|g) and 4.4 ps {I6} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: >0.5 ps from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
J$L({+3}He,d)=1+3 for a 2587 group from 4- target implying |p=+ is discrepant 
T$weighted average of 0.107 ps {i28} from {+38}Ar(|a,n|g) and 0.180 ps {i20} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: 66 ps {i21} from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
J$From L(p,t)=1+3 from 7/2- target. L({+3}He,|a)=3 for a 2610 group implying |p=- is discrepant 
T$weighted average of 0.27 ps {i7} from {+38}Ar(|a,n|g) and 0.39 ps {i5} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: 0.111 ps {i35} from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
E$2680 in ({+3}He,|a) 
J$L(d,p)=0 
T$weighted average of 1.7 ps {i5} from {+38}Ar(|a,n|g) and 2.8 ps {i6} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: 0.28 ps {I+29-18} from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
T$from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Others:< 14 fs from {+38}Ar(|a,n|g),|< 14 fs from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
T$weighted average of 24 fs {I7} from {+38}Ar(|a,n|g) and 41 fs {I13} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: <28 fs from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
E$3080 in (p,d) 
T$weighted average of 0.49 ps {I14} from {+38}Ar(|a,n|g) and 1.12 ps {I+19-15} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_comment:
J$(5/2-,7/2-) from L({+3}He,|a)=(3) for a 3210 group is in disagreement 
T$weighted average of 35 fs {I14} from {+38}Ar(|a,n|g), 40 fs {I20} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g) and 19 fs {I17} from {+41}K(p,n|g). 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$from (HI,xn|g). Others: >3.1 ps {+38}Ar(|a,n|g), < 2.8 ns {+39}K({+7}Li,|an|g),{+40}Ca({+3}He,2p|g). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_comment:
E$3450 in (d,t) 
J$L(d,p)=0 
T$from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). Other: <69 fs from {+38}Ar(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
E$3510 in (p,d) 
T$weighted average of 0.24 ps {I8} from {+38}Ar(|a,n|g) and 0.30 ps {I6} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
J$5/2-,7/2- from L({+3}He,|a)=3 for a 3527 {I12} group is in disagreement 
T$weighted average of 69 fs {I42} from {+38}Ar(|a,n|g) and 33 fs {I17} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: FS
level_comment:
E$3686 in (pol d,p),(d,p) 
T$weighted average of 44 fs {I12} from {+38}Ar(|a,n|g) and 53 fs {I28} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_comment:
T$weighted average of 52 fs {i14} from {+38}Ar(|a,n|g) and 38 fs {i14} from {+41}K(p,n|g). Other: 0.26 ps {i5} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|p=+ is also supported by L({+3}He,d)=1 from 4- target and L({+3}He,p)=0+2 from 3/2+ target. 5/2+ was proposed in an earlier (pol d,p) study (1972Ko41), but this level was not reported in recent (pol d,p) work (1994Uo01,1990Ec01) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: NS
level_comment:
T$weighted average of 3.00 ns {I10} from (HI,xn|g) and 3.8 ns {I6} from {+39}K({+7}Li,|an|g),{+40}Ca({+3}He,2p|g). Other: >3.12 ps from {+38}Ar(|a,n|g). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$4120 in (p,d) 
J$L(d,p)=2; |g to 7/2-; RUL. |p=- from L({+3}He,|a)=3 for a 4108 {I15} group is in disagreement 
T$other: < 28 fs from {+38}Ar(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)
level_lifetime_unit: FS
level_comment:
E$4198 in (pol d,p),(d,p); 4150 in (d,t) 
J$|g's to 3/2+ and 5/2+; |p=+ from L(d,t)=2 for a 4150 group, but |p=- from L(d,p)=1 for a tentative group at 4198 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2,9/2)-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$(3/2 to 11/2)- from L(p,t)=L(p,p')=2 from 7/2- target; 5/2,7/2,9/2 from |g(|q) in (|a,n|g); (9/2)+ from L(d,p)=4 and (pol d,p), is in disagreement 
T$other: < 49 fs from {+38}Ar(|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: PS
level_comment:
E$4367 in (pol d,p),(d,p) 
J$|p=(+) from L(|a,|a')=(3) from 7/2- target for a 4343 {I5} group is in disagreement 
T$weighted average of 125 fs {I35} from {+38}Ar(|a,n|g) and 132 fs {I35} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
T$weighted average of 28 fs {I24} from {+38}Ar(|a,n|g) and 42 fs {I10} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$weighted average of 97 fs {I28} from {+38}Ar(|a,n|g) and 87 fs {I31} from {+40}Ca(d,p|g),{+2}H({+40}Ca,p|g). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: FS
level_comment:
J$L({+3}He,p)=0+2 from 3/2+ target; L({+3}He,d)=L(d,n)=1+3 from 4- target; L(|a,|a')=3 from 7/2- target; L(p,t)=3 for a doublet from 7/2- target. Based on all the L-transfers both levels of the doublet at 4728 and 4730 are of positive parity; with most likely spin of 5/2 for 4730 and 3/2 for 4728. But (9/2)+ from L(d,p)=4 and (pol d,p) is in disagreement 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
J$L(|a,{+3}He)=3. |p=(+) from L(p,p')=(3,5) from 7/2- target for a 5682 {I5} group is in disagreement 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$L=2 {I5852} group in (p,d) and ({+3}He,|a) is associated with 5819, T=3/2 analog state, based on large (L=2) C{+2}s factors 
J$|g(|q) in ({+3}He,|a|g) 
T$from {+42}Ca({+3}He,|a|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$6851 {I15} in (p,d) and ({+3}He,|a) differs significantly, but most likely these correspond to the 6822 level seen in ({+3}He,|a|g) 
J$L({+3}He,|a)=L(p,d)=0 
T$from {+42}Ca({+3}He,|a|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_comment:
J$L({+3}He,|a)=2. (7/2+,9/2+) from L(|a,{+3}He)=(4) for a 6980 group is in disagreement 
E$6980 in (|a,{+3}He) 


level_energy_unit: KEV
level_comment:
L$Fraction of L values:0.50 {I10} (L=0), 0.50 {I10} (L=2) 
E$5759 in 1966Se08 corresponds to 5730+5759 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=216.15 
$|G{-n}=7.4 
T$Other: 5.65 keV (1972Ne04) 
S$216.15 (1974Si26) and 220.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=241.80 
$|G{-n}=20.0 
S$241.80 (1974Si26) and 250.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=290.95 
$|G{-n}=1.8 
T$Other: 2.19 keV (1972Ne04) 
S$290.95 (1974Si26) and 299.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=326.35 
$|G{-n}=14.2 
T$Other: 13.65 keV (1972Ne04) 
S$326.35 (1974Si26) and 338.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=354.50 
$|G{-n}=1.61 
T$Other: 1.50 keV (1972Ne04) 
S$354.50 (1974Si26) and 360.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=435.00 
$|G{-n}=8.2 
T$Other: 13.38 keV (1972Ne04) 
S$435.00 (1974Si26) and 448.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2
level_comment:
$E(n)(lab)=501.50 
$|G{-n}=8.1 
T$Other: 10.65 keV (1972Ne04) 
S$501.50 (1974Si26) and 504.0 (1972Ne04) are probably the same levels 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.39 ps {I6} (1987Ta03), 0.40 ps {I7} (1980Sa14), 0.55 ps {I7} (1978Be20), 0.55 ps {I5} (1975Ta13), 0.32 ps {I10} (1971La07) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 4.6 ps {I6} (1978BeE20) and 3.8 ps {I11} (1975Ta13). Others: > 1.0 ps (1987Ta03), |> 1.0 ps (1971La07) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 2.7 ps {I+7-5} (1975Ta13) and 3.1 ps {I9} (1978Be20). Other: 0.33 ps {I10} (1971La07) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 0.17 ps {I3} (1975Ta13) and 0.067 ps {I+28-25} (1987Ta03). Other: |< 35 fs (1971La07) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
S$1990Ec01 quote value from a thesis by N. Seichert (University of Munich 1982) from 21 MeV data. Others: 6.8 (1990En08). C{+2}S=0.59 (1984Ha26), 0.57 (1978Vo04), 0.77 (1994Uo01) 


level_energy_unit: KEV
level_comment:
L,J$from 1990En08. 1990Ec01 give L=2, J|p=5/2+ and assign as pure CCBA. 1994Uo01 assign 3/2+ with C{+2}S=0.038 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
S$0.16 (1990En08). C{+2}S=0.14 (1994Uo01), possible misprint for energy level(5601.7) in 1994Uo01, evaluators assume it is 4601.7 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$(1/2-) (1994Uo01), C{+2}S=(0.028) for 5404 level. However, 1994Uo01 associate 5404 group with 5451.7 from 1990Ec01. J|p=5/2+ in Adopted Levels 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$C{+2}S=0.077 (1994Uo01) for 8697 level. But 8697 group in 1994Uo01 should be associated with 8700 level of 1990Ec01 


level_energy_unit: KEV
level_comment:
$C{+2}S=2.7 {I4} 
S$0.60 {I11} for excitation to 780, 1/2+ level in {+27}Si; 0.55 {I10} for excitation to 960, 3/2+ level in {+27}Si. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
E$E=2875 {I12} with L=2 (1975Gr14) 
J$From 1975Gr14. A preference of 7/2+ over 9/2+ is shown by the authors (1975Gr14), since S=0 state are expected to be populated more strongly than S=1 states in ({+3}He,t) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$E=4098 {I8} with L=2 (1975Gr14) 
E$Strongest peak known to have pure > nature 
E$possible analog state of 4245 level in {+41}Sc 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$E=5822 {I10} with L=0 (1975Gr14) 
E$Isobaric analog state (IAS) (2004Fu28) 
E$Analog of {+41}K g.s. (1975Gr14,1975Ta05) 
E$possible analog state of 5941 level in {+41}Sc 


level_energy_unit: KEV
level_comment:
L$1969Yn01 list L=1 in Table II, but no |s(|q) distribution is shown in Figure 4 of their paper. This level is populated weakly in (d,t) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
J,L,S$This level could be fitted with L=3 with J|p=(5/2-,7/2-) and C{+2}S= 0.13. J|p=7/2- in (p,t) and ({+3}He,|a|g) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
L$1969Yn01 list L=2 in Table II, but no |s(|q) distribution is shown in figure 4 of their paper. The authors state that this state was not excited with sufficient intensity to extract a reliable |s(|q) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$Level decays principally (98% {I1}) to {+40}Ca g.s. through 180-keV s-wave neutron branch. |g transitions from this level were not determined. However authors (1975Ta05) conclude that a weak |g decay branch does exist 


level_energy_unit: KEV
level_spin_parity: 11/2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 21.1 ps {I10} (1978Cl09), 17.3 ps {I28} (1976Me09), 19.4 ps {I35} (1974Li07), 20.5 ps {I14} (1973Go31) 


level_energy_unit: KEV
level_spin_parity: 15/2+
level_lifetime_unit: NS
level_comment:
G$From (1975Yo05). Other: +0.32 {I4} (1975Uh02) 
T$Weighted average of 3.19 ns {I21} (1976Ra05), 2.98 ns {I35} (1976Me09), 2.88 ns {I14} (1975Ki05), 3.05 ns {I21} (1974Li07), 3.12 ns {I35} (1973Go31) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_comment:
T$from DSAM (2017Da13). Uncertainty from stopping powers, estimated by the authors as |?5%, is not included. This value can be compared to 1.80 ps {I55} (1974Li07: Nucl. Phys. A223, 445), 1.21 ps {I31} (1976Li17: J. Phys. g{-2}, 577), and 1.5 ps {I3} in {+41}Ca Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$The rms charge radius (<r{+2}>){+1/2}: 3.5081 fm {I21} (2013An02 evaluation) 
J$L(t,p)=L(p,t)=0 from 0+ 
$Adopted (1977En02) neutron-stripping spectroscopic factor=1.6 {I2} (L=3) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.58 {I6} (L=3) 
$Adopted (1977En02) proton-stripping spectroscopic factor=3.2 {I4} (L=2) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,t)=2 from 0+ 
T$weighted average of 0.62 ps {I21} (|a,p|g), 0.97 ps {I22} (|g,|g), 1.11 ps {I21} (p,p'|g) and 0.825 ps {I28} (coulomb excitation) 
MOMM1$from transient field integral perturbed angular correlation (2003Sc21) 
MOME2$reorientation method (1973To07) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.04 {I2} (L=1), 0.48 {I12} (L=3) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.18 {I3} (L=3), small (L=1) 
$Adopted (1977En02) proton-stripping spectroscopic factor=0.04 {I3} (L=2) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,t)=0 from 0+ 
T$from (p,p'|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.18 {I5} (L=3) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.05 {I2} (L=3) 
$Adopted (1977En02) proton-stripping spectroscopic factor=0.3 {I2} (L=2) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(t,p)=L(p,t)=2 from 0+ 
T$weighted average of 114 fs {I30} (|a,p|g) and 210 fs {I50} (p,p'|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.56 {I14} (L=3), small (L=1) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.16 {I7} (L=3), (0.0) (L=1) 
$Adopted (1977En02) proton-stripping spectroscopic factor=0.05 {I5} (L=2) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(p,t)=4 from 0+ 
T$weighted average of 3.5 ps 3 ({+18}O,2np|g), 2.63 ps 28 ({+16}O,2p|g) and 1.6 ps 7 (|a,p|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.03 {I1} (L=1), 0.86 {I22} (L=3) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.59 {I10} (L=3), 0.01 (L=1) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J$L(|a,{+2}He)=L(|a,|a')=6 from 0+ 
T$weighted average of 5.30 ns 16 (|a,p|g) and 5.27 ns 14 (|a,|a') 
MOMM1$DPAD (1975Yo02) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=1.2 {I3} (L=3) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.99 {I18} (L=3) (L=3), 0.01 (L=1) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=L(p,t)=4 from 0+ 
T$weighted average of 118 fs 21 (|a,p|g) and 210 fs +100-70 (p,p'|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.22 {I6} (L=3), small (L=1) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.08 {I2} (L=3), 0.00 (L=1) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(t,p)=L(|a,|a')=2 from 0+ 
T$weighted average of 118 fs 21 in (|a,p|g) and 230 fs 50 in (p,p'|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=0.01 {I1} (L=1), 0.01 {I1} (L=3) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.01 (L=3), 0.01 {I1} (L=1) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$ B(E3) from (e,e') 
J$L(t,p)=L(p,t)=3 from 0+ 
T$weighted average of 0.23 ps 7 (|a,p|g) and 0.45 ps 14 (p,p'|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=small (L=0 and L=2) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.26 {I17} (L=0), 0.12 {I3} (L=2) 
$Adopted (1977En02) proton-stripping spectroscopic factor=0.28 {I4} (L=1+3) 


level_energy_unit: KEV
level_spin_parity: 4-
level_lifetime_unit: PS
level_comment:
J$|g(|q,lin pol) in ({+18}O,|a2n|g) and (|a,p|g); L({+3}He,d)=3; L({+3}He,|a)=0(+2); |s(|q) and Ay(|q) in (pol p,|a) 
T$from (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_comment:
J$L(p,t)=L(p,p')=L(|a,|a')=5 from 0+; |s(|q) and Ay(|q) in (pol p,|a); also |g(|q,lin pol) 
T$from (|a,p|g) 
$Adopted (1977En02) neutron-stripping spectroscopic factor=small (L=2) 
$Adopted (1977En02) neutron-pickup spectroscopic factor=0.43 {I13} (L=2) 
$Adopted (1977En02) proton-stripping spectroscopic factor=0.46 {I9} (L=3) 


level_energy_unit: KEV
level_spin_parity: (3,4)-
level_comment:
J$L(d,p)=0+2 from 7/2- this level was not adopted by 1990En08 since the (d,p) cross section is small. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(|a,|a')=3. This requires E3 to g.s. 
E$if T{-1/2}<50 fs then E3 50% to g.s. is unlikely. In that case another level of J|p=2+ is required. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$|g to 4+. L(t,p)=L(|a,|a')=2. It is assumed that the level at 5200 {I5} in (t,p) and 5205 {I5} in (|a,|a') is the same as 5210 {I2} in (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$gammas to 2+ and 4+; L(p,t)=2. It is assumed that the level at 5213 in (p,t) is the same as this level. See also comment for 5210 level 
J$ PRIMARY G FROM (1-,2+) 


level_energy_unit: KEV
level_spin_parity: (3-,4-)
level_comment:
J$L({+3}He,|a)=(0+2) from 7/2-. It is assumed that the level at 5610 {I20} in ({+3}He,|a) is the same as the level at 5601 {I2} in (|a,p|g) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$L(|a,|a')=L(p,t)=3. It is assumed that the level at 5665 {I2} in (|a,p|g) is the same as 5667 {I5} in (|a,|a') and 5664 in (p,t) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
J$gammas to 2+ and 3-; L(d,p)=0+2. It is assumed that the level at 5670 {I2} in (|a,p|g) is the same as 5669 {I10} in (d,p) 


level_energy_unit: KEV
level_spin_parity: 7-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 |g to 5-; |g to 6+ from |g(|q,lin pol,DCO) 
T$from (|a,p|g). Other: 10.5 ps {I10} is reported in ({+16}O,2p|g) using RDM. It may suggest two closely spaced levels. 


level_energy_unit: KEV
level_spin_parity: (1,2,3-)
level_comment:
J$gammas to 0+ and 2+. If this level is the same as 5860 in (t,p) with L=0, then placement of 4028.5|g is incorrect as it would be E0 


level_energy_unit: KEV
level_spin_parity: (4+,5,6-)
level_comment:
J$gammas to 4- and 6+; 5- or 6- are supported by 11/2- transfer in (|a,p) from 3/2+ 
J$4+ IN 1990En08 


level_energy_unit: KEV
level_comment:
J$L(d,p)=1 from 7/2-. L(p,d)=0+2 from 7/2- is incompatible. L(t,p)=(0) suggests (0+) and L({+3}He,|a)=(4) suggests (4+) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
J$L(d,p)=1 from 7/2-; J{-n}=1/2+3/2 in (pol d,p); |g transitions to 5- in (|a,p|g). But 3/2+ transfer in (|a,p) from 3/2+ favors 3+. 


level_energy_unit: KEV
level_spin_parity: 10-
level_lifetime_unit: PS
level_comment:
J$from |g(|q,lin pol,DCO) 
T$weighted average of 2.6 ps {I11} in ({+18}O,2np|g) and 1.5 ps {I8} in ({+16}O,2p|g) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from 1969Ha02,1971Ha12. Other: 0.69 ps {I21} (quoted by 1971Ha12 from Carlsson (priv comm)) 
$ 1969Ca24: priv. comm. from Carlsson quoted by 1969Fl03 and 1971Ha12 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$average of 0.11 ps {I3} (1969Ha02), 0.118 ps {I28} (1971Ha12). Other: 0.125 ps {I21} (quoted by 1971Ha12 from Carlsson (priv comm)) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$from 1973Mc16. Others: 24 ps {I7} (1969Ha02), 1.3 ps {I+14-7} (1971Ha12), 2.0 ps {I+14-7} (quoted by 1971Ha12 from Carlsson (priv comm)), 8.0 ps {I17} (1970Co32) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
T$from 1970Ma39. Others: 3.7 ns {I5} (1969Ha02), 5.3 ns {I3} (quoted by 1971Ha12 from Carlsson (priv comm)), 5.52 ns {I15} (1970No04) in {+40}Ca(|a,2p|g) 
$g=-0.42 {I3} (1970Ma39), -0.50 {I+2-3} (1971No06,1972No09), -0.415 {I15} (1975Yo02) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$average of 0.10 ps {I3} (1969Ha02), 0.125 ps {I21} (1971Ha12). Other: 0.17 ps {I3} (quoted by 1971Ha12 from Carlsson (priv comm)) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$average of 0.25 ps {I7} (1969Ha02), 0.20 ps {I7} (1971Ha12). Other: 0.28 ps {I7} (quoted by 1971Ha12 from Carlsson (priv comm)) 


level_energy_unit: KEV
level_spin_parity: (1,2,3-)
level_comment:
E$If this level is the same as 5860 in (t,p) with L=0, then placement of 4029|g is incorrect as it would be E0 


level_energy_unit: KEV
level_comment:
$d|s/d|W=0.81 {I17} 
|s(exp)/|s(dw)=0.0027 (1977Bo16) for d{-3/2}{+2} 
d|s/d|W=0.78 mb/sr (1977Bo16) 


level_energy_unit: KEV
level_comment:
$|S15 {I1} 
$E$3186 6 (1967Wi15) 
L$6 assigned by 1967Wi15, but none assigned by 1967Bj06 in their |s(|q) distribution 


level_energy_unit: KEV
level_comment:
$|S21 {I3} 
$E$5471 9 (1967Wi15) 
L$4 assigned by 1967Wi15, but none assigned by 1967Bj06 in their |s(|q) distribution 


level_energy_unit: KEV
level_comment:
$|S52 {I3} 
$E$6920 4 (1967Wi15) 
L$2 assigned by 1967Wi15 for a 6920 group, but none assigned by 1967Bj06 in their |s(|q) distribution for 6880+6910+6940 


level_energy_unit: KEV
level_comment:
$|S78 {I4} 
L$2 assigned by 1967Wi15, but none assigned by 1967Bj06 in their |s(|q) distribution 
$E$7385 5 (1967Wi15) 


level_energy_unit: KEV
level_comment:
E,L$from 1980Va17 
N=350 {I200} for |nf{-7/2}{+2}, 43 {I20} for |nf{-7/2}p{-3/2}, 60 {I30} for |np{-3/2}{+2} (1980Va17) 


level_energy_unit: KEV
level_comment:
$NORMALIZATION=30 {I4} 
E$5010 {I70} (1980Va17) 
N=190 {I70} for |nf{-7/2}{+2}, 28 {I8} for |nf{-7/2}p{-3/2}, 190 {I70} for |nf{-7/2}|nf{-5/2} (1980Va17) 


level_energy_unit: KEV
level_comment:
$NORMALIZATION=6 {I1} 
E$7400 (1978Ja10), 7510 {I50} (1980Va17) 
L$in 1980Va17, L=6 fits well, but L=5 and 7 cannot be discarded 
N(for L=6)=70 {I20} for |nf{-7/2}{+2}, 17 {I6} for |nf{-7/2}|nf{-5/2} (1980Va17) 


level_energy_unit: KEV
level_comment:
E$9040 (1978Ja10), 9111 {I50} (1980Va17) 
L$from 1980Va17, L=6 is less probable 
N(for L=6)=80 {I30} for |nf{-7/2}{+2}, 18 {I5} for |nf{-7/2}|nf{-5/2}. N(for L=7)=34 {I7} for |nf{-7/2}g{-9/2}. N(for L=8)=6 {I2} for |ng{-9/2}{+2} (1980Va17) 


level_energy_unit: KEV
level_comment:
E$9510 {I50} (1980Va17) 
L$from 1980Va17, L=5 fits slightly better than L=6 
N(for L=5)=18 {I4} for |nf{-7/2}|ng{-9/2}, 65 {I10} for |np{-3/2}|ng{-9/2}. N(for L=6)=30 {I6} for |nf{-7/2}|nf{-5/2} (1980Va17) 


level_energy_unit: KEV
level_comment:
E$9990 {I50} (1980Va17) 
L$from 1980Va17, L=6 is less probable 
N(for L=6)=18 {I4} for |nf{-7/2}|nf{-5/2}. N(for L=7)=32 {I6} for |nf{-7/2}g{-9/2}. N(for L=8)=6 {I2} for |ng{-9/2}{+2} (1980Va17) 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=2.8 eV 
$E(p)(LAB)=1187.1 {I15} 
A{-2}=-0.44 {I8}, A{-4}=+0.05 {I13}, A{-6}=-0.09 {I11} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=6.0 eV 
$E(p)(LAB)=1226.0 {I15} 
A{-2}=-0.46 {I7}, A{-4}=+0.14 {I11}, A{-6}=-0.11 {I10} 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=7.4 eV 
$E(p)(LAB)=1237.2 {I15} 
A{-2}=-0.40 {I5}, A{-4}=+0.23 {I8}, A{-6}=-0.11 {I7} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=15 eV 
$E(p)(LAB)=1241.6 {I15} 
A{-2}=-0.85 {I5}, A{-4}=+0.11 {I7}, A{-6}=-0.04 {I6} 


level_energy_unit: KEV
level_spin_parity: 0+,1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=2.7 eV 
$E(p)(LAB)=1258.7 {I15} 
A{-2}=-0.11 {I5}, A{-4}=+0.07 {I8}, A{-6}=-0.09 {I7} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=7.1 eV 
$E(p)(LAB)=1264.3 {I15} 
A{-2}=-0.96 {I3}, A{-4}=+0.15 {I5}, A{-6}=-0.06 {I4} 


level_energy_unit: KEV
level_spin_parity: (1-),2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=1.1 eV 
$E(p)(LAB)=1277.0 {I15} 
A{-2}=+0.32 {I7}, A{-4}=-0.21 {I9}, A{-6}=+0.09 {I9} 


level_energy_unit: KEV
level_spin_parity: 0+,1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=14 eV 
$E(p)(LAB)=1296.5 {I15} 
A{-2}=-0.05 {I5}, A{-4}=-0.03 {I7}, A{-6}=+0.06 {I6} 


level_energy_unit: KEV
level_spin_parity: 0+,1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=2.2 eV 
$E(p)(LAB)=1304.4 {I15} 
A{-2}==0.65 {I7}, A{-4}=-0.04 {I8}, A{-6}=+0.07 {I8} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=6.9 eV 
$E(p)(LAB)=1309.9 {I15} 
A{-2}=-0.83 {I4}, A{-4}=+0.13 {I6}, A{-6}=-0.05 {I5} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=4.2 eV 
$E(p)(LAB)=1324.0 {I15} 
A{-2}=-0.96 {I3}, A{-4}=+0.08 {I6}, A{-6}=-0.03 {I5} 


level_energy_unit: KEV
level_spin_parity: 0+,1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=3.3 eV 
$E(p)(LAB)=1326.6 {I15} 
A{-2}=-0.06 {I9}, A{-4}=-0.15 {I12}, A{-6}=+0.08 {I10} 


level_energy_unit: KEV
level_spin_parity: (1-,3-,4+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=2.8 eV 
$E(p)(LAB)=1327.7 {I15} 
A{-2}=+0.95 {I34}, A{-4}=-0.34 {I35}, A{-6}=+0.18 {I30} 


level_energy_unit: KEV
level_spin_parity: (3-,4+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=3.2 eV 
$E(p)(LAB)=1330.2 {I15} 
A{-2}=+2.0 {I4}, A{-4}=-0.10 {I34}, A{-6}=-0.39 {I34} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=9.0 eV 
$E(p)(LAB)=1345.1 {I15} 
A{-2}=-1.02 {I3}, A{-4}=+0.04 {I5}, A{-6}=+0.04 {I4} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=13 eV 
$E(p)(LAB)=1346.5 {I15} 
A{-2}=+1.53 {I18}, A{-4}=-0.12 {I16}, A{-6}=+0.28 {I13} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=13 eV 
$E(p)(LAB)=1352.2 {I15} 
A{-2}=-1.01 {I4}, A{-4}=+0.03 {I7}, A{-6}=-0.04 {I6} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=20 eV 
$E(p)(LAB)=1355.0 {I15} 
A{-2}=-0.44 {I7}, A{-4}=-0.01 {I11}, A{-6}=+0.08 {I9} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=16 eV 
$E(p)(LAB)=1357.4 {I15} 
A{-2}=-1.05 {I5}, A{-4}=+0.08 {I9}, A{-6}=+0.03 {I7} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=18 eV 
$E(p)(LAB)=1368.4 {I15} 
A{-2}=-0.83 {I4}, A{-4}=+0.02 {I7}, A{-6}=-0.04 {I6} 
|G=170 eV {I50} (|G{-|a}=5 eV {I2}, |G{-n}<3 eV, |G{-p}=160 eV {I50}) (1970De11) 
E$possible analog of 1913 level in {+42}K 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=17 eV 
$E(p)(LAB)=1372.0 {I15} 
A{-2}=-0.86 {I5}, A{-4}=0.00 {I9}, A{-6}=-0.07 {I7} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=12 eV 
$E(p)(LAB)=1390.9 {I15} 
A{-2}=-0.17 {I3}, A{-4}=+0.01 {I4}, A{-6}=-0.05 {I3} 


level_energy_unit: KEV
level_spin_parity: 1-,(2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=3.5 eV 
$E(p)(LAB)=1392.6 {I15} 
A{-2}=-0.56 {I3}, A{-4}=0.00 {I4}, A{-6}=+0.02 {I3} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=20 eV 
$E(p)(LAB)=1393.9 {I15} 
A{-2}=-0.28 {I3}, A{-4}=-0.03 {I4}, A{-6}=+0.03 {I3} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=27 eV 
$E(p)(LAB)=1395.9 {I15} 
A{-2}=-0.81 {I3}, A{-4}=+0.05 {I5}, A{-6}=-0.06 {I4} 
|G=40 eV {I10} (|G{-|a}=14 eV {I5}, |G{-n}<4 eV, |G{-p}=25 eV {I10}) (1970De11) 
E$possible analog of 1927 level in {+42}K 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=4.5 eV 
$E(p)(LAB)=1400.1 {I15} 
A{-2}=+1.87 {I16}, A{-4}=+0.40 {I14}, A{-6}=-0.11 {I13} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=2.4 eV 
$E(p)(LAB)=1410.3 {I15} 
A{-2}=+1.12 {I22}, A{-4}=-0.75 {I24}, A{-6}=+0.20 {I20} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=4.2 eV 
$E(p)(LAB)=1411.1 {I15} 
A{-2}=-0.85 {I5}, A{-4}=-0.09 {I8}, A{-6}=+0.05 {I7} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=20 eV 
$E(p)(LAB)=1447.0 {I15} 
A{-2}=+0.03 {I2}, A{-4}=+0.07 {I3}, A{-6}=+0.03 {I3} 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=34 eV 
$E(p)(LAB)=1452.9 {I15} 
A{-2}=+0.78 {I3}, A{-4}=-0.03 {I4}, A{-6}=+0.17 {I4} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=4.7 eV 
$E(p)(LAB)=1465.7 {I15} 
A{-2}=-0.05 {I7}, A{-4}=-0.28 {I10}, A{-6}=+0.04 {I9} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=28 eV 
$E(p)(LAB)=1467.4 {I15} 
A{-2}=-0.10 {I2}, A{-4}=-0.04 {I3}, A{-6}=+0.04 {I3} 


level_energy_unit: KEV
level_spin_parity: (0+,1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=2.2 eV 
$E(p)(LAB)=1485.8 {I15} 
A{-2}=+0.05 {I4}, A{-4}=-0.19 {I5}, A{-6}=+0.15 {I5} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=13 eV 
$E(p)(LAB)=1491.8 {I15} 
A{-2}=-0.34 {I4}, A{-4}=+0.21 {I6}, A{-6}=-0.20 {I5} 


level_energy_unit: KEV
level_spin_parity: (0+,1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=12 eV 
$E(p)(LAB)=1496.3 {I15} 
A{-2}=-0.02 {I7}, A{-4}=-0.04 {I10}, A{-6}=+0.05 {I9} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=30 eV 
$E(p)(LAB)=1497.4 {I15} 
A{-2}=-0.67 {I3}, A{-4}=+0.02 {I4}, A{-6}=+0.02 {I4} 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=9.2 eV 
$E(p)(LAB)=1516.0 {I15} 
A{-2}=-1.11 {I2}, A{-4}=+0.24 {I4}, A{-6}=-0.03 {I4} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=27 eV 
$E(p)(LAB)=1532.5 {I15} 
A{-2}=+0.15 {I3}, A{-4}=+0.05 {I4}, A{-6}=+0.03 {I4} 


level_energy_unit: KEV
level_spin_parity: 0+,1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=12 eV 
$E(p)(LAB)=1538.4 {I15} 
A{-2}=-0.01 {I5}, A{-4}=-0.14 {I6}, A{-6}=+0.08 {I6} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=18 eV 
$E(p)(LAB)=1543.0 {I15} 
A{-2}=+0.32 {I10}, A{-4}=+0.33 {I12}, A{-6}=-0.06 {I11} 


level_energy_unit: KEV
level_spin_parity: (1-),2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=18 eV 
$E(p)(LAB)=1544.8 {I15} 
A{-2}=+0.18 {I9}, A{-4}=+0.44 {I12}, A{-6}=-0.10 {I11} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=210 eV 
$E(p)(LAB)=1558.7 {I15} 
A{-2}=+0.04 {I3}, A{-4}=+0.05 {I3}, A{-6}=+0.02 {I4} 
|G=300 eV {I100} (|G{-|a}=100 eV {I70}, |G{-n}<4 eV, |G{-p}=200 eV {I7}) for J=1; |G=180 eV {I60} (|G{-|a}=60 eV {I40}, |G{-n}<4 eV, |G{-p}=120 eV {I40}) (1970De11) 
E$possible analog of 2061 level in {+42}K 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=12 eV 
$E(p)(LAB)=1566.0 {I15} 
|G=170 eV {I70} (|G{-|a}=5 eV {I3}, |G{-n}=26 eV {I15}, |G{-p}=140 eV {I60}) for J=1; |G=100 eV {I50} (|G{-|a}=3 eV {I2}, |G{-n}=16 eV {I10}, |G{-p}=85 eV {I40}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=5.7 eV 
$E(p)(LAB)=1571.8 {I15} 
|G=110 eV {I50} (|G{-|a}<4 eV, |G{-n}=11 eV {I7}, |G{-p}=95 eV {I50}) for J=1; |G=63 eV {I30} (|G{-|a}<2 eV, |G{-n}=6 eV {I4}, |G{-p}=56 eV {I30}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=3.5 eV 
$E(p)(LAB)=1583.4 {I15} 
A{-2}=-0.81 {I4}, A{-4}=+0.18 {I7}, A{-6}=-0.03 {I6} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=5.5 eV 
$E(p)(LAB)=1585.0 {I15} 
A{-2}=-0.69 {I5}, A{-4}=+0.23 {I9}, A{-6}=-0.10 {I7} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=12 eV 
$E(p)(LAB)=1590.2 {I15} 
A{-2}=+0.26 {I8}, A{-4}=-0.06 {I10}, A{-6}=+0.11 {I9} 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=8.7 eV 
$E(p)(LAB)=1597.7 {I15} 
A{-2}=+1.61 {I16}, A{-4}=+0.64 {I16}, A{-6}=-0.17 {I16} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=4.6 eV 
$E(p)(LAB)=1604.8 {I15} 
A{-2}=+0.50 {I8}, A{-4}=-0.04 {I10}, A{-6}=+0.05 {I9} 


level_energy_unit: KEV
level_spin_parity: (1-),2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=7.7 eV 
$E(p)(LAB)=1606.4 {I15} 
A{-2}=-0.27 {I6}, A{-4}=+0.21 {I9}, A{-6}=+0.07 {I8} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=11 eV 
$E(p)(LAB)=1614.3 {I15} 
A{-2}=-0.78 {I7}, A{-4}=+0.05 {I12}, A{-6}=+0.04 {I8} 


level_energy_unit: KEV
level_spin_parity: (1-,2+,3-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=43 eV 
$E(p)(LAB)=1647.7 {I15} 
A{-2}=+0.60 {I7}, A{-4}=+0.01 {I7}, A{-6}=-0.14 {I7} 


level_energy_unit: KEV
level_spin_parity: 1-,(2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=5.7 eV 
$E(p)(LAB)=1658.1 {I15} 
A{-2}=-0.63 {I7}, A{-4}=-0.02 {I11}, A{-6}=+0.04 {I10} 


level_energy_unit: KEV
level_spin_parity: (1-),2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=18 eV 
$E(p)(LAB)=1664.9 {I15} 
A{-2}=-0.39 {I5}, A{-4}=+0.02 {I7}, A{-6}=+0.03 {I7} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=81 eV 
$E(p)(LAB)=1673.8 {I15} 
A{-2}=-0.45 {I3}, A{-4}=-0.08 {I5}, A{-6}=+0.02 {I5} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=130 eV 
$E(p)(LAB)=1686.8 {I15} 
A{-2}=-0.56 {I4}, A{-4}=-0.03 {I6}, A{-6}=+0.11 {I5} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=19 eV 
$E(p)(LAB)=1696.8 {I15} 
A{-2}=-0.26 {I7}, A{-4}=+0.01 {I11}, A{-6}=+0.04 {I9} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=9.0 eV 
$E(p)(LAB)=1705.8 {I15} 
A{-2}=+0.03 {I7}, A{-4}=-0.54 {I10}, A{-6}=-0.06 {I11} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=62 eV 
$E(p)(LAB)=1708.4 {I15} 
A{-2}=-0.70 {I3}, A{-4}=-0.02 {I5}, A{-6}=+0.02 {I5} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=260 eV 
$E(p)(LAB)=1734.8 {I15} 
A{-2}=-1.00 {I3} 
|G=430 eV {I360} (|G{-|a}=310 eV {I350}, |G{-n}<9 eV, |G{-p}=120 eV {I30}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=22 eV 
$E(p)(LAB)=1741.6 {I15} 
A{-2}=+0.30 {I10}, A{-4}=-0.77 {I13}, A{-6}=+0.16 {I11} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=180 eV 
$E(p)(LAB)=1745.1 {I15} 
A{-2}=-0.69 {I4}, A{-4}=-0.06 {I7}, A{-6}=+0.07 {I7} 
|G=320 eV {I80} (|G{-|a}=95 eV {I50}, |G{-n}=21 eV {I10}, |G{-p}=200 eV {I50}) (1970De11) 
E$possible analog of 2227 level in {+42}K 


level_energy_unit: KEV
level_spin_parity: (2+,3-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=8.9 eV 
$E(p)(LAB)=1754.1 {I15} 
A{-2}=+0.40 {I16}, A{-4}=-0.77 {I22}, A{-6}=+0.07 {I19} 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=38 eV 
$E(p)(LAB)=1770.5 {I15} 
A{-2}=+0.25 {I7}, A{-4}=-0.08 {I9}, A{-6}=+0.06 {I9} 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=11 eV 
$E(p)(LAB)=1777.6 {I15} 
A{-2}=+0.26 {I5}, A{-4}=-0.11 {I6}, A{-6}=+0.06 {I6} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=130 eV 
$E(p)(LAB)=1786.2 {I15} 
A{-2}=+0.36 {I3}, A{-4}=+0.03 {I3}, A{-6}=+0.03 {I3} 


level_energy_unit: KEV
level_spin_parity: 0+,1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=34 eV 
$E(p)(LAB)=1795.5 {I15} 
A{-2}=-0.14 {I9}, A{-4}=+0.20 {I12}, A{-6}=+0.05 {I12} 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=29 eV 
$E(p)(LAB)=1798.6 {I15} 
A{-2}=+1.19 {I12}, A{-4}=-0.04 {I12}, A{-6}=+0.24 {I12} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=9.4 eV 
$E(p)(LAB)=1806.1 {I15} 
A{-2}=-1.06 {I6}, A{-4}=+0.09 {I10}, A{-6}=+0.06 {I9} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=23 eV 
$E(p)(LAB)=1817.5 {I15} 
A{-2}=+0.31 {I7}, A{-4}=+0.05 {I9}, A{-6}=+0.06 {I10} 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=39 eV 
$E(p)(LAB)=1837.1 {I15} 
A{-2}=-0.20 {I6}, A{-4}=+0.03 {I9}, A{-6}=+0.06 {I7} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=34 eV 
$E(p)(LAB)=1850.2 {I15} 
A{-2}=+0.11 {I4}, A{-4}=-0.09 {I5}, A{-6}=+0.12 {I5} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=41 eV 
$E(p)(LAB)=1859.5 {I15} 
A{-2}=-0.09 {I8}, A{-4}=-0.17 {I11}, A{-6}=+0.22 {I11} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=70 eV 
$E(p)(LAB)=1869.1 {I15} 
A{-2}=-0.09 {I4}, A{-4}=0.00 {I6}, A{-6}=-0.03 {I5} 
|G=770 eV {I300} (|G{-|a}=27 eV {I20}, |G{-n}=78 eV {I60}, |G{-p}=660 eV {I290}) (1970De11) 
E$possible analog of 2356 level in {+42}K 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=39 eV 
$E(p)(LAB)=1880.3 {I15} 
|G=810 eV {I90} (|G{-|a}=14 eV {I5}, |G{-n}=55 eV {I30}, |G{-p}=740 eV {I80}) (1970De11) 
E$possible analog of 2389 level in {+42}K 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=240 eV 
$E(p)(LAB)=1884.7 {I15} 
A{-2}=+0.10 {I4}, A{-4}=+0.09 {I5}, A{-6}=+0.03 {I5} 


level_energy_unit: KEV
level_spin_parity: (1-),2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=24 eV 
$E(p)(LAB)=1892.1 {I15} 
A{-2}=-0.47 {I7}, A{-4}=+0.14 {I10}, A{-6}=-0.03 {I10} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=200 eV 
$E(p)(LAB)=1896.0 {I15} 
A{-2}=-0.61 {I5}, A{-4}=-0.33 {I7}, A{-6}=+0.07 {I6} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=130 eV 
$E(p)(LAB)=1903.8 {I15} 
A{-2}=+1.07 {I10}, A{-4}=+0.16 {I10}, A{-6}=+0.35 {I10} 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=53 eV 
$E(p)(LAB)=1922.8 {I15} 
A{-2}=-0.07 {I5}, A{-4}=-0.23 {I8}, A{-6}=-0.02 {I7} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=150 eV 
$E(p)(LAB)=1927.8 {I15} 
A{-2}=-0.19 {I3}, A{-4}=-0.09 {I4}, A{-6}=+0.05 {I4} 
|G=210 eV {I70} (|G{-|a}=80 eV {I50}, |G{-n}<5 eV, |G{-p}=130 eV {I50}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=240 eV 
$E(p)(LAB)=1932.4 {I15} 
|G=380 eV {I120} (|G{-|a}=120 eV {I80}, |G{-n}=7 eV {I5}, |G{-p}=250 eV {I90}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=5 eV {ILT} 
$E(p)(LAB)=1937 {I3} 
E,J$from {+41}K(p,n) (1970De11) 
|G=105 eV {I50} (|G{-|a}<5 eV, |G{-n}<10 eV, |G{-p}=100 eV {I50}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=220 eV 
$E(p)(LAB)=1945.3 {I15} 
A{-2}=-0.71 {I2}, A{-4}=-0.02 {I4}, A{-6}=+0.05 {I4} 
|G=850 eV {I110} (|G{-|a}=84 eV {I30}, |G{-n}=21 eV {I10}, |G{-p}=740 eV {I100}) (1970De11) 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=110 eV 
$E(p)(LAB)=1952.6 {I15} 
A{-2}=-0.40 {I4}, A{-4}=+0.04 {I6} 
|G=480 eV {I60} (|G{-|a}=40 eV {I20}, |G{-n}<4 eV, |G{-p}=440 eV {I50}) (1970De11) 
E$possible analog of 2470 level in {+42}K 


level_energy_unit: KEV
level_spin_parity: (1-,3-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=13 eV 
$E(p)(LAB)=1973.3 {I15} 
A{-2}=+0.85 {I6}, A{-4}=-0.21 {I6}, A{-6}=+0.04 {I6} 


level_energy_unit: KEV
level_spin_parity: (0+),1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=19 eV 
$E(p)(LAB)=1978.3 {I15} 
A{-2}=+0.23 {I6}, A{-4}=-0.02 {I7}, A{-6}=-0.09 {I7} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=230 eV 
$E(p)(LAB)=1997.1 {I15} 
A{-2}=+0.01 {I2}, A{-4}=-0.27 {I3}, A{-6}=+0.11 {I3} 


level_energy_unit: KEV
level_spin_parity: (1-),3-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=14 eV 
$E(p)(LAB)=2009.5 {I15} 
A{-2}=+0.83 {I11}, A{-4}=+0.11 {I12}, A{-6}=+0.11 {I11} 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=31 eV 
$E(p)(LAB)=2037.0 {I15} 
A{-2}=-0.89 {I6}, A{-4}=-0.18 {I10}, A{-6}=+0.07 {I9} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=120 eV 
$E(p)(LAB)=2040.0 {I15} 
A{-2}=+0.62 {I8}, A{-4}=-0.21 {I10}, A{-6}=+0.27 {I9} 


level_energy_unit: KEV
level_spin_parity: 1-,2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=180 eV 
$E(p)(LAB)=2043.8 {I15} 
A{-2}=-0.26 {I7}, A{-4}=0.00 {I10}, A{-6}=+0.05 {I9} 


level_energy_unit: KEV
level_spin_parity: (1-,2+,3-)
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=78 eV 
$E(p)(LAB)=2071.2 {I15} 
A{-2}=+0.51 {I7}, A{-4}=+0.10 {I9}, A{-6}=+0.21 {I8} 


level_energy_unit: KEV
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=250 eV 
$E(p)(LAB)=2077.7 {I15} 
A{-2}=+0.92 {I4}, A{-4}=-0.11 {I5}, A{-6}=+0.17 {I5} 


level_energy_unit: KEV
level_spin_parity: (0+,1-),2+
level_comment:
$(2J+1)|G{-P}|G{-|a}/|G=200 eV 
$E(p)(LAB)=2093.8 {I15} 
A{-2}=-0.23 {I4}, A{-4}=+0.17 {I6}, A{-6}=+0.21 {I5} 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
Spin of transferred neutron=1/2+3/2 (1978Vo04) 
L$1(+3) (1975Ha14) 
S$0.18 (L=1), 0.26 (L=3) (1975Ha14) 


level_energy_unit: KEV
level_spin_parity: 3+,4+
level_comment:
$Pure p{-1/2} neutron transfer is indicated by observation of the 7643 group at three most forward angles only (1978Vo04) 
L$1+3 (1975Ha14) 
S$0.45 (L=1), 0.39 (L=3) (1975Ha14) 


level_energy_unit: KEV
level_spin_parity: (3,4)+
level_comment:
Spin of transferred neutron=(1/2) (1978Vo04) 
L$1+3 (1975Ha14) 
S$0.47 (L=1), 0.94 (L=3) (1975Ha14) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_comment:
Assignment as isoscalar E1 transition is based on similarity of q-dependence of form factor with isoscalar E1 transitions of 5900 and 6950 in {+40}Ca. 


level_energy_unit: KEV
level_comment:
E$doublet. Others: 3250+3300 (1970La22), 3260 (1968Ba28); 3250+3297 (1956Br08), 3191+3250+3297 in 1969Ko03 
B(E2)(W.u.)=0.35 {I5}, B(E6)(W.u.)=0.32 {I5} (1971Ma53) 


level_energy_unit: KEV
level_comment:
E$ 4940 25 (1971Ma53) 
L$from 1971Ma53. L=2,3 in 1968Ba28 
B(E2)(W.u.)=1.2 {I2} (1971Ma53), 1.5 {I5} (1968Ba28) 


level_energy_unit: KEV
level_comment:
S$20% of the observed strength due to {+43}Ca g.s. from {+44}Ca(d,t) has been subtracted 
S$1.0 (1969Yn01), 1.08 (1964Bj02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
$ Transition to 5.76 MeV, 0+ state is much stronger than for g.s. The 5.76 MeV state is dominated by two neutrons in the 2p{-3/2} shell 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$<Q{+2}>=0.0480 e{+2}b{+2} {I20} (2018Ha10), triaxial parameter <cos(3|d)>=0.06 {I10} (2016Ha23,2018Ha10) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
$<Q{+2}>=0.131 e{+2}b{+2} {I25} (2018Ha10), triaxial parameter <cos(3|d)>=0.79 {I13} (2016Ha23,2018Ha10) 
$Deduced |b{-2}=0.43 {I2}, |g=13|' {I+5-6} (2016Ha23), suggesting superdeformed nature of the state 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$Deduced |b{-2}=0.45 {I2} (2016Ha23), suggesting superdeformed nature of the state 
T$0.214 ps {I47}, deduced by compiler from B(E2)|_(2424|g)=0.00082 {I8} and branching ratio=0.26 {I5} for 2424|g (2016Ha23). Others: 0.178 ps {I60} deduced from B(E2)|_ for 899|g; 0.114 ps {I50} in {+42}Ca Adopted Levels in the ENSDF database. Note that 1969Ko03 (Phys. Rev. 177, 1725) measured T{-1/2}=0.21 ps {I5} from DSAM in (p,p'|g) which may have been used by 2016Ha23 in their GOSIA analysis 
$Diagonal E2 matrix element=-0.55 eb {I15} 
$<Q{+2}>=0.144 e{+2}b{+2} {I25} (2018Ha10) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Evaluated rms charge radius=3.4954 fm {I19} (2013An02) 
MOMM1$optical method (1972Ol01). Other: -1.317643 {I7} (NMR,1973Lu08) 
MOME2$from CFBLS method (revised value by 1993Su36 from -0.043 {I9} (1991Si14). Other measurements: -0.062 {I12} (ABMR-LIRF, 1982Ay02), -0.065 {I20} (ABMR, laser spectroscopy, 1979Gr05), -0.040 {I8} (optical isotope shift method, 1980Be13,1981Ar15). Recalculations and analyses: -0.0552 {I11} (2002Mi37), -0.0408 {I8} (1993Su36,2008Py02), -0.049 {I5} (1984Sa10,1983Ar25,1982Ol05). 
$Measured |D<r{+2}>({+43}Ca-{+40}Ca)=0.117 fm{+2} {I25} (1981Wo02), 0.1254 fm{+2} {I32} (1984Pa12), 0.1215 fm{+2} {I4} (1991Si14). 
$Adopted (by 1977En02) spectroscopic factor S=0.58 {I6} (neutron stripping); 3.1 {I3} (neutron pickup) 
J$L(d,p)=L(d,t)=L(|a,{+3}He)=L(p,d)=L(pol {+3}He,|a)=3; J from optical spectroscopy (1954Ke14); L(|a,d)=5 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: PS
level_comment:
$Adopted (by 1977En02) spectroscopic factor S<0.02 (neutron stripping); 0.17 {I8} (neutron pickup) 
J$L(d,t)=L(|a,{+3}He)=L(p,d)=L(d,t)=L(pol {+3}He,|a)=3; |g(|q) and |g(lin pol) in (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
$Adopted (by 1977En02) spectroscopic factor S=0.04 {I2} (neutron stripping); 0.10 {I3} (neutron pickup) 
J$L(d,p)=L(|a,{+3}He)=L(d,t)=L(p,d)=L(pol {+3}He,|a)=1; |DJ=2 to 7/2- from |g(|q) and |g(lin pol) in (|a,n|g) 
T$other: 160 ps {I10} from p'|g(t) in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_comment:
$Adopted (by 1977En02) spectroscopic factor S=0.11 {I2} (neutron stripping); 2.2 {I4} (neutron pickup) 
J$L(d,p)=L(d,t)=L(|a,{+3}He)=L(p,d)=L(pol {+3}He,|a)=2; L({+3}He,p)=0; |DJ=1 to 5/2- from |g(|q) and |g(lin pol) in (|a,n|g) 
T$weighted average of 48 ps {I4} from (|a,n|g) and 51 ps {I8} from ({+19}F,2pn|g) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
$Adopted (by 1977En02) spectroscopic factor S=0.05 {I2} (neutron stripping); 1.0 {I2} (neutron pickup) 
J$L(d,p)=L(d,t)=L(p,d)=L(pol {+3}He,|a)=0 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: PS
level_comment:
Adopted (by 1977En02) spectroscopic factor S=0.72 {I9} (neutron stripping); 0.19 {I6} (neutron pickup) 
J$L(d,p)=L(|a,{+3}He)=L(d,t)=L(p,d)=L(pol {+3}He,|a)=1; L(|a,|a')=2+4 and |g to 7/2- reject 1/2- 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: FS
level_comment:
J$L(d,d')=4; L(|a,|a')=2+4; |DJ=1 to 5/2- from |g(|q) and |g(lin pol) in (|a,n|g) 
T$from DSAM in (p,p'|g) 


level_energy_unit: KEV
level_spin_parity: 3/2-,5/2-
level_lifetime_unit: FS
level_comment:
J$|DJ=0 or 1 to 3/2- and 5/2- from |g(|q) and |g(lin pol) in (|a,n|g); positive sign gives unacceptable M2 strength from (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=L(d,t)=L(p,d)=2; L(|a,|a')=2+4 is presumed to be in error or for a different level at 2694 {I5} 


level_energy_unit: KEV
level_spin_parity: 15/2-
level_lifetime_unit: PS
level_comment:
J$|DJ=2 to 11/2- from |g(|q) and |g(lin pol) in (|a,n|g) and from DCO in ({+18}O,|an|g) 
T$weighted average from ({+19}F,2pn|g) 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: PS
level_comment:
J$L(p,d)=L(d,t)=2 and |g to 7/2-. L(d,p)=0 suggests 1/2+. L(|a,d)=4+6 from 3/2+ is inconsistent with J=5/2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
J$L(d,p)=1. |g(circ pol) in (pol n,|g) does not allow 3/2-. |g(|q) of 2504|g in ({+3}He,|a|g) is inconsistent with J=1/2. It is possible that the level seen in ({+3}He,|a|g) is different from that in (n,|g) and (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)
level_comment:
E$not resolved from 3028.6; |g decay seen only in ({+3}He,|a|g) 
J$|g decays to 3/2+,3/2- L(p,d)=0+2 implies the presence of a doublet 


level_energy_unit: KEV
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$probable 1/2+ from L(p,d)=0 or 0(+2) 
E$population in (|a,n|g) is considered suspect (evaluators) 


level_energy_unit: KEV
level_spin_parity: (11/2:17/2)+
level_comment:
J$L(|a,d)=6 from 3/2+; L(|a,|a')=3+5. L(|a,{+3}He)=(4) implying (7/2+,9/2+) is inconsistent with either of the J|p values for 3278 or 3270 levels 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=1. |g(circ pol) in (pol n,|g) does not allow 1/2-. L(|a,|a')=3+5 for 3277+3297 is inconsistent with |p=- 


level_energy_unit: KEV
level_spin_parity: 13/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(|a,|a')=3+5 and |DJ=2 to 9/2+ from |g(|q) and |g(lin pol) in (|a,n|g) 
T$From ({+19}F,2pn|g). >3.5 ps from (|a,n|g) 


level_energy_unit: KEV
level_spin_parity: (7/2,9/2)+
level_comment:
E$possible doublet as suggested in (|a,{+3}He) and in 1990En08 evaluation. See also J|p comment 
J$L({+3}He,p)=2 from 3/2+; L(|a,|a')=3+5; L(|a,{+3}He)=(4). L(d,p)=(1) from 1974Br19 is in disagreement but L(d,p)=4 is also suggested by 1966Do02. Similarity to 4984, 9/2+ state in {+41}Ca indicates 4p-1h component in this level (1968Do02) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$L(d,p)=L(|a,{+3}He)=1. |g(circ pol) in (pol n,|g) does not allow 3/2-. Not compatible with L(d,t)=2 or L(p,d)=(2,3) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2+
level_uncertain: ?
level_comment:
J$L(d,t)=2 and L(p,d)=(2,3) 
E$this level corresponds to 4207.1 if L transfer in (d,t) and (p,d) is ignored (1978En02) 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_comment:
J$L(d,t)=2. L(d,p)=1 in 1974Br19 suggests 1/2-,3/2-. In another experiment L(d,p)=2 is also suggested by 1966Do02 


level_energy_unit: KEV
level_spin_parity: (7/2 : 13/2)+
level_comment:
J$L(|a,d)=4+6 from 3/2+ 
J$L(A,D)=2+4 IMPLYING (3/2 TO 9/2)+ AS QUOTED BY 1990En08 SEEMS TO BE A MISPRINT 


level_energy_unit: KEV
level_spin_parity: (3/2)+
level_comment:
J$L(p,d)=L(d,t)=L({+3}He,|a)=2. Strong L({+3}He,p)=0 from 3/2+ indicates IAS of {+43}K g.s., J|p=3/2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W=18 
Weak population is consistent with configuration=1f{-7/2}{+4}1d{-3/2}{+-1}, J=3/2, T=3/2 as proposed by 1966Do02 in (d,p) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$d|s/d|W=4 {ILT} 
Very weak population suggests a configuration more complicated than 1f{-7/2}{+4}1d{-3/2}{+-1}; J=3/2,T=3/2, proposed by 1966Do02 in (d,p). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$d|s/d|W=46 
Strongest transition below 6 MeV. Strong population relative to the 990 group is consistent with configuration=1f{-7/2}{+4}1d{-3/2}{+-1}; J|p=3/2+, T=3/2. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
This group is assigned to {+39}Ca g.s. in 1972Ma23. 1968Sm05 assign this group as L=2, S=0.53 for 3/2,0.37 for 5/2 in {+43}Ca. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
L$from 1972Ma23 
1978En02 quote S=0.9 (C{+2}=1/6 for T=5/2) 
Possible IAS of 561 in {+43}K (1972Ma23) 


level_energy_unit: KEV
level_spin_parity: (7/2)-
level_comment:
L$from 1972Ma23 
E$8750 50 (1968Sm05) 
1978En02 quote S=0.42 (C{+2}=1/6 for T=5/2) 
Possible IAS of 738 in {+43}K (1972Ma23) 


level_energy_unit: KEV
level_comment:
$|G{-|g}=0.56 eV {I10} 
$E{-n}(lab)=9.143 {I4} 
$g|G{-n}=1.0 eV {i5} 
$g|G{-n}|G{-|g}/|G=0.36 eV {i4} 


level_energy_unit: KEV
level_comment:
$|G{-|g}=0.645 eV {I80} 
$E{-n}(lab)=9.345 {I4} 
$g|G{-n}=3 eV {i1} 
$g|G{-n}|G{-|g}/|G=0.53 eV {i6} 


level_energy_unit: KEV
level_comment:
$|G{-|g}=0.435 eV {I50} 
$E{-n}(lab)=22.71 {I1} 
$g|G{-n}=20 eV {i5} 
$g|G{-n}|G{-|g}/|G=0.42 eV {i5} 


level_energy_unit: KEV
level_comment:
$|G{-|g}=0.44 eV {I5} 
$E{-n}(lab)=82.63 {I4} 
$g|G{-n}=200 eV {i50} 
$g|G{-n}|G{-|g}/|G=0.44 eV {i5} 


level_energy_unit: KEV
level_comment:
$|G{-|g}=1.63 eV {I18} 
$E{-n}(lab)=156.8 {I3} 
$g|G{-n}=300 eV {i50} 
$g|G{-n}|G{-|g}/|G=1.62 eV {i18} 


level_energy_unit: KEV
level_comment:
$|G{-|g}=1.9 eV {I2} 
$E{-n}(lab)=174.4 {I10} 
$g|G{-n}=2500 eV {i500} 
$g|G{-n}|G{-|g}/|G=1.9 eV {i2} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$The rms charge radius <r{+2}>{+1/2}=3.5179 fm {I21} (2013An02 evaluation) 
$Evaluated change in charge radius |d<r{+2}>({+44}Ca-{+40}Ca)=+0.283 fm{+2} {I6} (2013An02) 
$|d<r{+2}>({+40}Ca-{+44}Ca)=0.288 fm{+2} {I2}(stat){I6}(syst) (2016Ga34), 0.2904 fm{+2} {I10} (1998No10). 
$|d|n({+40}Ca-{+44}Ca)=851.1 MHz {I6}(stat){I21}(syst) (2016Ga34) 
J$L(t,p)=L(|a,{+2}He)=L({+6}Li,d)=L(d,{+6}Li)=0 from 0+. 
$Adopted (1977En02) spectroscopic factors S: 3.1 {I3} (L=3) (neutron stripping); 0.50 {I13} (L=3) (proton pickup). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L({+6}Li,d)=L(|a,|a')=L(d,d')=L(p,p')=L(e,e')=2 from 0+ 
T$weighted average of 3.5 ps {I7} from DSAM in (|a,p|g); 2.0 ps {I+8-5} from DSAM in (p,p'|g); 3.05 ps {I28} from DSAM in Coul. ex. (2003Sc21); 3.19 ps {I27} from DSAM in Coul. ex. (1973Fi15); and 2.88 ps {I12} from adopted B(E2)|^=0.0475 {I20} in Coulomb excitation. 
MOMM1$from transient field method in 2003Sc21. 
MOME2$from Coulomb excitation in 1973To07. 
BE2$weighted average of 0.0550 {I20} (1989It02) and 0.048 {I3} (1971He08) in (e,e'), 0.0475 {I36} (2016Ca17), 0.0473 {I20} (1973To07) and 0.049 {I5} (1972Bi17) in Coulomb excitation 
$Adopted (1977En02) spectroscopic factors S: 0.41 {I11} (L=3) and 0.08 {I2} (L=1) (neutron stripping); 0.18 {I3} (L=3) (proton pickup). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_uncertain: ?
level_comment:
E$from (pol {+3}He,{+3}He') only; this level is not seen in other studies 
J$from analyzing power in (pol {+3}He,{+3}He') 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$L({+6}Li,d)=L(d,{+6}Li)=0 from 0+; p-1883|g(|q) is isotropic in (p,p'|g). 
T$other: >1.4 ps from DSAM in (p,p'|g) 
$Adopted (1977En02) spectroscopic factors S: 0.39 {I10} (L=3) (neutron stripping); 0.12 {I3} (L=3) (proton pickup). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L({+6}Li,d)=L(e,e')=L(p,p')=L(|a,|a')=4 from 0+. 
T$others: 2.6 ps from B(E2)|^(from 2+,1157)=0.021 in ({+16}O,{+16}O'); 16 ps {I5} from RDM in ({+19}F,2p|g) is discrepant. 
$Adopted (1977En02) spectroscopic factors S: 0.14 {I4} (L=3) and 0.01 {I1} (L=1) (neutron stripping); 0.09 {I3} (L=3) (proton pickup). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L({+6}Li,d)=L(t,p)=L(p,p')=L(|a,|a')=2 from 0+ 
T$from B(E2) in (e,e') in 1989It02. 
BE2$from 1989It02 in (e,e') 
$ Adopted (1977En02) spectroscopic factors S: 0.51 {I13} (L=3) and <0.02 (L=1) (neutron stripping); 0.19 {I3} (L=3) (proton pickup). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
J$L(t,p)=L(|a,|a')=4 from 0+. 
$Adopted (1977En02) spectroscopic factors S: 0.91 {I23} (L=3) (neutron stripping); <0.04 (L=3) (proton pickup). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: PS
level_comment:
J$L(|a,{+2}He)=6 from 0+; 1001.869|g, |DJ=2 to 4+. 
T$other: <17 ps from RDM in ({+19}F,2p|g), <0.76 ns from |g|g(t) in (n,|g) E=thermal. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$L(e,e')=L(p,p')=L(d,d')=L(|a,|a')=3 from 0+. 
T$from adopted B(E3)|^=0.0072 {I12} and |g-branching ratios. Other: <0.35 ns from |g|g(t) in (n,|g) E=thermal. 
BE3$unweighted average 0.0095 {I9} (1989It02) and 0.00559 {I23} (1971He08) in (e,e'), 0.0065 {I9} (1969BeYW) in (|a,|a') 


level_energy_unit: KEV
level_spin_parity: (2+,3,4+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$1074|g to 4+, 2200|g to 2+. L(d,{+2}He)=2 from 0+ for a 3370 group suggest |p=-, but L(t,|a)=3 from 7/2- for a 3360 group suggests |p=+ 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
J$3661|g D to 0+; 353.67|g to 3- is not M2 since it would require a T{-1/2}>0.3 ns or width |G<1.5|*10{-6} eV which is significantly smaller than observed |G{-|g}=0.08 eV in (|g,|g') 
T$5.8 fs from |G{-|g}=0.08 eV in (|g,|g'), but it would require a B(E2)(W.u.)(354|g)=3800 exceeding RUL=100, which constrains T{-1/2}>0.22 ps or a width |G<0.0021 eV 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$L(e,e')=L(|a,|a')=5 from 0+. 
T$from DSAM in ({+14}C,|a2n|g). 
BE5$unweighted average of 0.000096 {I8} (1989It02) and 0.000053 {I5} (1971He08) in (e,e'), and 0.000101 {I16} (1969BeYW) in (|a,|a') 


level_energy_unit: KEV
level_spin_parity: (2+,3,4+)
level_comment:
E$this level is probably different from 4092 level (see discussion in 1976Co06 in {+44}K |b{+-} decay). 
J$1810.4|g to 4+, 2937.8|g to 2+ 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$L(d,p)=1 from 7/2-; |DJ=2 to 0+ from p|g(|q) in (p,p'|g). But J=1 is expected from population in (|g,|g'), although, a 2+ level could also be populated weakly either directly or from deexcitation of a higher J=1 level 
T$from 30 fs {+8-5} deduced from |G{-|g0} for J=1 in (|g,|g') with a correcting factor of 5/3 due to the change of spin from 1 to 2, since (2J+1)|G{-g0} is proportional to measured |g-ray yield (2011Is01). Other: <0.69 ns from |g|g(t) in (n,|g) E=thermal 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$L(t,p)=L(|a,|a')=2 from 0+. But 3-,4- from L(d,{+3}He)=0 from 7/2- for a group at 4480 is inconsistent 


level_energy_unit: KEV
level_spin_parity: 8+
level_lifetime_unit: PS
level_comment:
J$1802.59|g E2, |DJ=2 {I6}+ and member of g.s. band in ({+18}O,2p2n|g). 
T$from DSAM in ({+14}C,|a2n|g). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
T$deduced from |G=0.228 eV {I40} in (|g,|g'). 
J$parity from 4053|g M1+E2 to 2+. L(|a,{+2}He)=4+5 from 0+ for a 5210 group is inconsistent 


level_energy_unit: KEV
level_spin_parity: 2+,3+,4+,5+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$L(d,p)=1 from 7/2- for a group at 5343 {I10}. Other: 3- for a group at 5235 {I5} in (p,p') is inconsistent 


level_energy_unit: KEV
level_spin_parity: 3-,4-
level_comment:
E$weighted average of 5405 {I10} from (d,p), 5407 {I5} from (|a,|a'), and 5404 {I12} from (t,|a) 
J$L(t,|a)=L(d,{+3}He)=0 from 7/2- 


level_energy_unit: KEV
level_spin_parity: (1 : 6)-
level_comment:
E$weighted average of 5646 {I20} in (t,p), 5666 {I10} in (d,p), 5654 {I5} from (|a,|a'), and 5660 {I12} from (t,|a) 
J$L(t,|a)=2 from 7/2- 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$E0 branching=0.00088 {I14} (1976Ul01) from measurement of pair production (e+, e-) of E0 transition. 
$|r=0.30 {I10} (1976Ul01) 


level_energy_unit: KEV
level_comment:
$B(EL)|^=0.0508 
$B(E2)|^: other: 0.051 {I10} (quoted by 1989It02 from 1969BeYW) 
$g-factor=-0.28 {I11} (1979Ni04) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$%EWSR=68 for E2 strength (ISGQR) (2017Bu16) 
$%EWSR=77 {I14} and rms width=5.1 MeV {I+13-12} for E=17.2|*10{+3} {I5} from DWBA analysis (2017Bu16) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$others: 19.5E3 {I1} (2020Ho01) 
$%EWSR=75 {I11} for E0 strength (ISGMR) from DWBA analysis (2017Bu16), 88 {I4} (2020Ho01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
$|d{-N}=0.29 
$B(E2)|^(from 2+,1157)=0.0216 
S$0.30 fm (DWBA). 1.01 fm for transition from 2+,1157 (1982Re03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|d{-N}=0.32 
$B(E2)|^(from 2+,1157)=0.0060 
S$0.37 fm (DWBA). 0.71 fm for transition from 2+,1157 (1982Re03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_comment:
$|d{-N}=0.33 
$B(E2)|^(from 3-,3308)=0.00132 
S$0.47 fm (DWBA). 0.30 fm for transition from 3-,3308 (1982Re03) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$weighted average of 3.05 ps {I28} (2003Sc21) and 3.19 ps {I27} (1973Fi15), both by DSA. Other: 2.88 ps {I12} from B(E2)|^=0.0475 {I20} 
BE2$weighted average of 0.0475 {I36} (2016Ca17), 0.0473 {I20} (1973To07), and 0.049 {I5} (1972Bi17). Other: 0.035 (1961An07) 
$g-factor=+0.17 {I3} (2003Sc21), +0.12 {I5} (2003Ta05) 
$Experimental |s=53 mb {I4} (2016Ca17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d|n{+40,44}=851.1 MHz {I6} (stat) {I21} (syst) 
$|d<r{+2}>{+40,44}=0.288 fm {+2} {I2} (stat) {I6} (syst) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: D
level_comment:
J J=7/2 from ABLDF (1979Be47). |p=- from L(d,p)=3. 
T weighted ave. (int.) of 162.67 d {I25} (1994Lo04. Liquid scin; inorganic and organic samples. 3 T{-1/2}'s) and 162.6 d {I1} (1965An07; 4|p|b pc, 5.8 T{-1/2}'s). Others: see 1992Bu01. 
MOMM1,MOME2$ABLDF; {+43}Ca standard; Sternheimer correction applied for Q. Other |m=-1.316 {I16} (1982An15). 


level_energy_unit: KEV
level_comment:
This state which is observed in (d,p) at 7 MeV is probably not the same as the 1554-keV state observed in ({+14}C,n|a|g) and ({+3}He,{+6}He) since the (d,p) reaction at 7 MeV is unlikely to populate an 11/2- state (L=5 required). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
May Be the same as the previous state; however, the large L transfer noted in ({+3}He,{+6}He) would indicate that it is not 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)
level_uncertain: ?
level_comment:
Tentatively proposed by 1980Hu10 on basis of doublet nature of 2354|g in |g|g-coin where a contribution of a 2349|g is assumed 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$from {+45}Ca Adopted Levels in ENSDF database 
MOMM1,MOME2$from collinear laser spectroscopy (2015Ru02) Others: |m=-1.3278 {I9} (1981Ar15: Hyperfine Int. 9, 159). Q=+0.046 {I14} (1983Ar25: Zeit. Phys. A314, 302) 
MOME2$ recalculated and recommended value based on 1983Ar25 measurement: +0.038 {I12} (2013StZZ: Rept INDC(Nuclear Data Sheets)-0650) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
$B(GT)=0.008 {i5}, extracted from observed count of 174|g, where uncertainty is from statistical and systematic contributions 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$|d|n{+40,45}=1103.5 MHz {I7} (stat) {I25} (syst) 
$|d<r{+2}>{+40,45}=0.125 fm {+2} {I3} (stat) {I8} (syst) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J L=2 in (t,p), (|a,{+2}He) and (p,t) 
T$from Coul. ex. if B(E2)=0.0178 {I13} (1975Ku17), T{-1/2}>5.5 ps from (t,p|g) (1974Be28) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
E$weighted average of values from (t,p|g) (E|g plus adopted 1346.0 level), (p,p'), and (p,t). 
J L=0 in (t,p) and (p,t) 
T$from (t,p|g) (1974Be28) 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: NS
level_comment:
J L=6 in (|a,{+2}He) and (p,t) 
T$weighted average of 10.3 ns {I10} (p,p2n|g) (1975Bi01) and 10.5 ns {I6} (|a,|a2n|g) (1975Ku17) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of values from {+46}K |b{+-} decay: data set #1, (t,p), (p,p'), (d,d'), and (p,t) (3020.5 {I21} from {+46}K |b{+-} decay: data set #1 based on E|g's and 1346.0 {I3} for first excited state (evaluator)). 
J L=2 in (t,p) and (p,t) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3-)
level_uncertain: ?
level_comment:
J$based on log| {Ift}. 
Not found in any other data and not adopted; does not seem to correspond to J=2+ 4430.2 {I9} adopted level. 


level_energy_unit: KEV
level_spin_parity: 5-,6+,8+
level_comment:
Configuration (|n p{-1/2}){+-1}(|n g{-9/2}){+-1}, (|n g{-9/2}){+-1}(|n d{-5/2}){+-1} or (|n g{-9/2}){+-2} 


level_energy_unit: KEV
level_spin_parity: 6+,8+,7-
level_comment:
Configuration (|n g{-9/2}){+-1}(|n d{-5/2}){+-1} (|n g{-9/2}){+-2} or (|n f{-5/2}){+-1}(|n g{-9/2}){+-1} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$ recoil distance Doppler shift method (2009Me23) with gate on total kinetic energy gating loss (TKEL) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|d|n{+40,46}=1301.0 MHz {I6} (stat) {I30} (syst) 
$|d<r{+2}>{+40,46}=0.125 fm {+2} {I2} (stat) {I8} (syst) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: D
level_comment:
J J=7/2 from ABLFS (1982An15). |p=- from L({+3}He,|a)=3 
T weighted av of 4.535 d {I4} (1964Gi04. |?9 T{-1/2}'s; NaI, 1.15|<E|g|<1.52 MeV), 4.530 d {I4} (1968Re04. 3.3 T{-1/2}'s; 4|p|g ic), and 4.540 d {I3} (1969Bu14. |?6 T{-1/2}'s; NaI, 1.19 MeV|<E|g|<1.39 MeV). 4.536 d {I3} is the arithmetic mean of 4.5360 d {I21} (NRM) and 4.5352 d {I29} (RT) with uncertainty from RT; LWM gives 4.5360 d {I21}. Others: see 1995Bu05 
MOMM1,MOME2$ABLFS; {+43}Ca standard. |m: not corrected for hyperfine anomaly. Q: "Sternheimer" or other polarization correction included. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_uncertain: ?
level_comment:
Not included in decay scheme by 1984Al18 due to the uncertain placement of the 2511|g. See discussion on possible J|p's and configuration of this state by 1984Al18. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J from J-dependence of A(|q) (1971Ma58; E|?20 MeV, Si telescopes; POL|?80%). Confirmed by 1977Wi12. 
S other: 6.22 (1977Wi12) 


level_energy_unit: KEV
level_spin_parity: 1/2+&3/2-
level_comment:
Unresolved group. Probably includes 2849- and 2874-keV states seen in (d,p). However, data are discrepant in various stripping and pickup reactions; see comments in Adopted Levels 
J,L from DWBA comparison to |s(|q) and A(|q) (1977Wi12). L(p,d)=(1)+? from forward peaking of |s(|q) (1972Ma23) 
S from 1977Wi12 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
Probable doublet consisting of the 4960 and 4980 states observed in ({+3}He,|a) (evaluator). 4960 state weakly populated 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J 1972Ma23 suggested that this state is possibly the IAS({+47}K; 5465; 5/2+). However, L=(3) is not consistent with this suggestion. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J from characteristic shape of A(|q) (1985Ha08) 
Main component of 1f7/2. Using the isospin-dependent potential, C{+2}S=87% of shell-model sum rule 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
Main component of 2d3/2(T<). Using the isospin-dependent potential, C{+2}S=63% of shell-model sum rule 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
Main component of 2s1/2(T<). Using the isospin-dependent potential, C{+2}S=78% of shell-model sum rule 
For the |?2.6-MeV doublet, A(|q) indicates that the 1/2+ member is weakly excited (1985Ha08) 


level_energy_unit: KEV
level_spin_parity: 13/2
level_comment:
J From CRC analysis. 13/2- if (({+48}Ca 3-) (|n 1f7/2){+-1}); 13/2+ if (({+48}Ca 4+) (|n 1f7/2){+-1}). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$ other: L=2 momentum distribution in knock-out from d{-3/2} orbital (2009Ma16) 
$ Measured cross section=21 mb {I4} (2009Ma16) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_lifetime_info: ;ERR=GT
level_comment:
J$ other: L=0 momentum distribution in knock-out from s{-1/2} orbital (2009Ma16) 
$ Measured cross section=15 mb {I3} (2009Ma16) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
J$from {+47}Ca Adopted Levels in ENSDF database 
MOMM1,MOME2$from collinear laser spectroscopy (2015Ru02) Other: |m=-1.380 {I24} (1982An15: Phys. Rev. C 26, 2194). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$Level populated by removal of f{-7/2} neutron from {+48}Ca g.s. 
$Measured cross section=70.6 mb {I+84-96} (2017Cr03) 
$C{+2}S=6.4 {I+8-9} (2017Cr03) 
$C{+2}S(normalized)=9.3 {I+11-13}(stat) {I19}(syst) (2017Cr03), using a quenching factor of 0.69 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$Measured cross section |< 1.4 mb (2017Cr03) 
$C{+2}S |< 0.1 (2017Cr03) 
$C{+2}S(normalized) |<0.2 (2017Cr03), using a quenching factor of 0.66 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
$Level populated by removal of d{-3/2} neutron from {+48}Ca g.s. 
$Measured cross section=9.4 mb {I+31-19} (2017Cr03) 
$C{+2}S=1.3 {I+4-3} (2017Cr03) 
$C{+2}S(normalized)=1.9 {I+6-4}(stat) {I4}(syst) (2017Cr03), using a quenching factor of 0.65 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$Level populated by removal of s{-1/2} neutron from {+48}Ca g.s. 
$Measured cross section=10.5 mb {I+14-13} (2017Cr03) 
$C{+2}S=0.8 {I1} (2017Cr03) 
$C{+2}S(normalized)=1.3 {I2}(stat) {I2}(syst) (2017Cr03), using a quenching factor of 0.65 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$ratio of Fermi to Gamow-Teller matrix elements y=0.098 {I37} (2024Ko08), implying a Coulomb mixing matrix element of 101 keV {I37} 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$|d|n{+40,47}=1524.8 MHz {I8} (stat) {I35} (syst) 
$|d<r{+2}>{+40,47}=0.002 fm {+2} {I3} (stat) {I9} (syst) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: Y
level_comment:
%B-,%2B-$From T{-1/2}(2|b{+-})=3.7|*10{+19} y {I+33-12} and T{-1/2}=2.9|*10{+19} y {I+42-11}. See footnote comments for T{-1/2}. 
$Nuclear rms charge radius=3.4771 fm {I20} (2013An02). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$3831.4|g E2 to 0+. 
T$weighted average of 35 fs {I3} from |G{-|g0} in (|g,|g') (2002Ha13), 42 fs {I9} from DSAM in (n,n'|g) (1992Va06), and 37 fs {I17} from DSAM in (p,p'|g) (1970Be39). 
$B(E2)|^=0.0082 {I5} from (e,e') (1985Wi06), but it is discrepant with 0.0140 {I15} from (|a,|a'):giant res (2011Lu07) and 0.0131 {I12} from ({+6}Li,{+6}Li') (2010Kr06). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
J$from observation of E0 e+/e- pair emission to g.s. in (p,p'|g); L(t,p)=0 from 0+. 
T$from p|g(t) in (p,p'|g) (1970Be39). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
J$4507.3|g E3 to 0+. 
T$from DSAM in (p,p'|g) (1970Be39). Other: 7.2 ps {I+26-20} from adopted B(E3)|^=0.0069 {I10}. 
$B(E3)|^=0.0069 {I10}, unweighted average of 0.0065 {I10} from (e,e'), 0.0054 {I8} from (|a,|a'):giant res, 0.0087 {I8} from ({+6}Li,{+6}Li'). 


level_energy_unit: KEV
level_spin_parity: 3(+)
level_lifetime_unit: PS
level_comment:
J$spin=3 from |g|g(|q) in (p,p'|g) and |g(|q) in (n,n'|g); L(p,p')=(4) from 0+. 
T$unweighted average of 3.7 ps {I+9-4} from (n,n'|g) (1992Va06) and 1.2 ps {I4} from (p,p'|g) (1972Ta23). 


level_energy_unit: KEV
level_spin_parity: 3,4,5
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
J$D |g to 4+. Results are discrepant in the various experiments: 3,5 from |g(|q) in (n,n'|g); 5+ from DWBA fit to Coulomb form factors and RPA calculation (unnatural |p state from absence of longitudinal form factor) in (e,e'); 5- from L(p,p')=5 and observance of peak in (|a,|a') (natural |p state) (1988Fu01); (4) from comparison of |s(|q) and analyzing powers to those of known states in (p,p') (1984Se10),(pol p,p'); 3- from L(|a,|a')=3. 
T$from direct timing in (p,p'|g) (1977Lo06). 


level_energy_unit: KEV
level_spin_parity: 4(-)
level_lifetime_unit: PS
level_comment:
J$spin=4 from |g(|q) in (n,n'|g); 4- from DWBA fit to the Coul. form factors and RPA calc. in (e,e') (unnatural parity state from absence of longitudinal form factor). Other: (5+) from (p,p') for a group at 5257 {I5} is discrepant 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$weighted average of 5459 {I10} from (t,p) and 5462 {I7} from (p,p'). 
J$L(t,p)=L(p,p')=0 from 0+. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: FS
level_comment:
J$L(|a,|a')=(2) from 0+; 2273.1|g to 2+, 1597.8|g to 3-. Other: 4- from DWBA fit to Coulomb form in (e,e') (unnatural |p state from absence of longitudinal form factor) and (4-) from DWBA analysis in (p,p') (unnatural |p state since peak not observed in (|a,|a')) are discrepant. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: FS
level_comment:
J$2,3,4 from |g(|q) in (n,n'|g); (2- and 5+) doublet from DWBA analysis in (p,p') with unnatural |p state since peak not observed in (|a,|a') (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E$weighted average of 6893 {I9} from (e,e') and 6898 {I7} from (p,p'). 
J$the 5+ member of (2- and 5+) doublet (see comment on J|p(6895.87)); J|>3 {I1} from comparison of |s(|q) and analyzing power to those of known states in (p,p') (1984Se10); . 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
J$(4-) from DWBA fit to the Coulomb form factors and RPA calculations in (e,e') (unnatural |p state from absence of longitudinal form factor) discrepant. But L(p,p')=(3) favors (3-) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$weighted average of 7476 {I7} from (e,e') and 7468 {I5} from (p,p'). 
J$L(p,p')=4 from 0+ and natural parity due to presence in (|a,|a') measured by 1988Fu01 in (p,p'). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,p'). Other: 7658 from {+48}K |b{+-} decay, 7657 {I10} from (e,e') 
J$also from analysis of |s(|q) in (p,p') 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$from (p,p'). Others: 7650 {I20} from (t,p) and 7657 {I10} from (e,e'). 
J$L(p,p')=3 from 0+ and natural parity 
$B(E3)|^|?0.0014 from (e,e'). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1+,2+)
level_comment:
$B(M1)|^<0.05 from (e,e'). 
$15 additional states reported in (p,p') by 1983Cr01 between 7.7 MeV and 12.7 MeV, seven of which appear to correspond to states observed in (e,e'). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$weighted average of 7791 {I7} from (e,e') and 7784 {I10} from (p,p'). 
J$L(|a,|a')=3 from 0+. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,p') 
J$L(p,p')=4 from 0+ and not clearly seen in |a spectrum (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: (1)
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,p') 
J$from analysis of |s(|q) in (p,p'); |g to 0+. Other: (1-,2+) from (e,e') for a group at 8038 {I15} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (|a,|a'|g) 
J$from |a|g(|q) in (|a,|a'|g). 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,p'). 
J$L(p,p')=4 from 0+ and natural parity 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-,2,3)
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$reported by 1969Te03 as the same level at 8276 {I10} seen in their (p,p') measurement, however, while the level seen in thier (p,p') could correspond to the 8283 {I8} level with J|p=4+ from 1988Fu01 in (p,p') and the level seen in (p,p'|g) by 1969Te03 with a different J|p could be a separate level. 
J$8275|g to 0+, 1456|g to (3-) 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$1- and (6)+ doublet from L(p,p')=1+6 and natural |p state from presence of peak in (|a,|a') spectra; 8385.3|g E1 to 0+. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$weighted average of 8435 {I5} from (e,e'), and 8441 {I8} from (p,p'). 
J$L(p,p')=3 from 0+ and natural parity (1988Fu01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2)
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+48}K |b{+-} decay 
J$4635|g to 2+, 8466|g to 0+. 


level_energy_unit: KEV
level_spin_parity: 3+,4+,5+
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,p'). Other: 8477 {I15} from (e,e') 
J$L(p,p')=4 from 0+. 


level_energy_unit: KEV
level_spin_parity: (1-,2+)
level_comment:
J$8517.1|g to 0+; (1-,2+) is most likely from |g excitation. 
T$4.6 fs {I8} if J|p=1- or 11.4 fs {I28} if J|p=2+ from |G{-|g0} in (|g,|g') assuming |G{-|g0}/|G=1. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from (p,p'). Other: 8518 {I8} from (e,e') 
J$L(p,p')=3 from 0+ and natural parity 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2+)
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+48}K |b{+-} decay 
J$possible 4247|g to 0+. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_comment:
E$weighted average of 8557 {I14} from (e,e'), and 8565 {I7} from (p,p'). 
J$other: (6) assigned by 1988Fu01 based on L(p,p')=(6) from 0+ and uncertain existence of this state in the (|a,|a') spectra in 1988Fu01 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$weighted average of 8605 {I6} from (e,e') and 8609 {I6} from (p,p'). 
J$L(p,p')=3 from 0+ and natural parity 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
E$weighted average of 8804 {I9} from (e,e') and 8806 {I5} from (p,p'). 
J$L(p,p')=5 from 0+; 5- from DWBA analysis in (e,e') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1,2,3)
level_uncertain: ?
level_comment:
E LEVEL ENERGY HELD FIXED IN LEAST-SQUARES ADJUSTMENT 
E$from {+48}K |b{+-} decay. Other: 8964 {I10} from (p,p') 
J$8966|g to 0+ 


level_energy_unit: KEV
level_comment:
J$(8-) from DWBA fit to the Coulomb form factors and RPA calculations in (e,e'); unnatural parity state from absence of longitudinal form factor; L(p,p')=(8), J|p=(7-) from comparison to DWBA in (p,p'). See also J|p comment for 9123 level. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
J$L(p,p')=3+(7) from 0+ (natural |p from presence of peak in (|a,|a')) in (p,p') for the doublet. 9229 state appears to be the high-spin member. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7-)
level_comment:
J$(7,8,9) from comparison of |s(|q) and analyzing power to those of known states in (p,p'),(pol p,p'); (6-,7-) from comparison to DWBA in (p,p'),(|a,|a'). See comment on J|p(9211). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$9294.3|g E1 to 0+. L(p,p')=1+(8) (natural |p state from presence of peak in (|a,|a')) in (p,p') for the doublet. 9296 state appears to be the L=8 member. 


level_energy_unit: KEV
level_spin_parity: (8-)
level_comment:
J$(8-) from DWBA fit to the Coulomb form factors and RPA calculations in (e,e') unnatural |p state from absence of longitudinal form factor; (7,8,9) from comparison of |s(|q) and analyzing power to those of known states and (8-) from comparison to DWBA in (p,p'). See comment for J|p(9295.3). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$B(M1)|^=3.9 {I3} from (e,e'). 
E$weighted average of 10227 {I5} from (e,e') and 10211 {I10} from (p,p'). 
J$L(p,p')=0 from 0+; unnatural parity state from absence of peak in (|a,|a'). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_comment:
J,ISPIN$momentum transfer dependence favors an E1 excitation and small |G implies an isobaric analog resonance in (e,e'n). 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$B(M1)|^=3.9 {I3} 
E$from 1980St17. 
J$based on dependence of strength on momentum transfer (1980St17). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
E,J$from 1984De19. (|p{++},|p{++}) peak heavily contaminated by {+16}O 9.85-MeV state. Excitation function shows similar anomalous behavior to that for the {+12}C 15.1-MeV, 1+, T{->} state. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$from 1972Gr27. Others: 3818 {I10} (1966La05), 3833 {I4} (1966Ma13), 3835 {I10} (1969Te03), and 3832 {I7} (1988Fu01), 3832 (1984Se10). 
S$others: 0.70 (1972Gr27), 0.61 (1985Se14), 0.95 (1969Te03). 
$M{-n}=9.46 fm{+2} {I21}, M{-p}=4.04 fm{+2}. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
E$weighted average of 4272 {I10} (1966La05), 4284 {I6} (1966Ma13), 4286 {I10} (1969Te03), and 4284 {I7} (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$from 1972Gr27. Others: 4498 {I10} (1966La05), 4506 {I4} (1966Ma13), 4512 {I10} (1969Te03), and 4507 {I7} (1988Fu01), 4507 (1984Se10) 
S$others: 0.81 (1972Gr27), 0.84 (1985Se14), 1.09 (1969Te03). 
$May contain a small contribution from the 4503, 4+, state (1988Fu01). 
$M{-n}=36.3 fm{+3} {I12}, M{-p}=31.78 fm{+3}. 1994Fe05 investigated the possibility of contributions to |s(|q) and the analyzing power from the 4503,4+, state and found the effect to be negligible. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
E$weighted average of 4604 {I10} (1966La05), 4613 {I4} (1966Ma13), 4619 {I10} (1969Te03), 4608 {I4} (1972Gr27), and 4612 {I7} (1988Fu01). Other: 4613 (1984Se10) 
J$2 from 1969Te03 is discrepant 
L,S$from 1972Gr27. Other: |b{-L}R=0.44 (1969Te03) 
CONF$(|n,p{-3/2}f{-7/2}){+-1} (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
E$from 1972Gr27. Others: 5130 {I20} (1966La05), 5146 {I5} (1966Ma13), and 5152 {I10} (1969Te03), 5147 {I7} (1988Fu01), 5147 (1984Se10) 
J$other: (4) from 1984Se10 is inconsistent 
S$other: 0.22 (1972Gr27), 0.83 (1969Te03) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E$weighted average of 5266 {I10} (1966La05), 5265 {I10} (1969Te03), 5252 {I5} (1972Gr27), and 5260 {I7} (1988Fu01). 
J$4- may also fit |s(|q) (evaluator). 
L$from 1972Gr27. 
S$other: 0.11 (1972Gr27) 
CONF$(|n,p{-3/2}f{-7/2}){+-1} (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$weighted average of 5368 {I5} (1966Ma13), 5376 {I10} (1969Te03), 5368 {I3} (1972Gr27), and 5370 {I7} (1988Fu01). Other: 5370 {I20} (1966La05), 5368 (1984Se10). 
J$other: (4) from 1969Te03 is discrepant 
S$other: 0.46 (1972Gr27) 
$M{-n}=18.4 fm{+3} {I6}, M{-p}=16.23 fm{+3}. 


level_energy_unit: KEV
level_spin_parity: 5-
level_comment:
E$from 1972Gr27. Others: 5724 {I10} (1966La05), 5728 {I8} (1966Ma13), 5737 {I10} (1969Te03), and 5730 {I7} (1988Fu01), 5729 (1984Se10). 
J$other: (3) from 1969Te03 is discrepant 
S$other: 0.46 (1972Gr27) 
$M{-n}=315 fm{+5} {I26}, M{-p}=328.5 fm{+5}. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_comment:
E$from 1972Gr27. Others: 6096 {I10} (1966La05), 6106 {I7} (1966Ma13), 6108 {I10} (1969Te03), and 6105 {I7} (1988Fu01), 6104 (1984Se10). 
J$other: (4) from 1984Se10 
S$other: 0.15 (1972Gr27) 
CONF$-0.896|p(f{-7/2},(s{+-}{-1/2}){+1}{-2}){-4-} + 0.441|p(f{-7/2},(d{+-}{-3}){+1}{-1/2}){-4-} (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$from 1972Gr27. Others: 6340 {I20} (1966La05), 6338 {I10} (1966Ma13), 6351 {I10} (1969Te03), and 6345 {I7} (1988Fu01), 6342 (1984Se10). 
S$other: 0.37 (1972Gr27) 
$M{-n}=100 fm{+4} {I3}, M{-p}=49.25 fm{+4}. 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$from 1972Gr27. Others: 6654 {I10} (1969Te03), 6648 {I7} (1988Fu01), 6648 (1984Se10) 
S$other: 0.25 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: (5+)
level_comment:
E$weighted average of 6897 {I8} (1972Gr27), 6896 {I10} (1969Te03), and 6899 {I7} (1988Fu01). Other: 6897 (1984Se10) 
J$data appear to be consistent with the assumption that this peak is a multiplet consisting of a 2- and a 5+ state; |>3 from 1984Se10 
L$other: 5 from 1972Gr27. 
S$other: 0.15 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$weighted average of 7305 {I10} (1969Te03), 7298 {I5} (1972Gr27), 7303 {I7} (1988Fu01), and 7285 {I10} (2017Ma28). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_comment:
E$from 1972Gr27. Others: 7402 {I10} (1969Te03) and 7399 {I7} (1988Fu01). 
L$from 1972Gr27, inconsistent with J|p=(2-) from 1988Fu01. Other: 1,2 from 1988Fu01 with L=2 inconsistent with J|p=(2-) 
S$other: 0.15 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 3-,1+
level_comment:
$|s{-M1}(0|')(mb/sr)=0.015 {I9} 
E$weighted average of 7652 {I10} (1969Te03) and 7648 {I10} (2017Ma28). 
J$from 2017Ma28 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$from 1972Gr27. Others: 7666 {I10} (1969Te03), 7661 {I7} (1988Fu01), 7659 (1984Se10). 
S$other: 0.49 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
S$other: 0.22 (1972Gr27) 
E$weighted average of 7784 {I10} (1969Te03), 7801 {I8} (1972Gr27), and 7800 {I7} (1988Fu01). Other: 7800 (1984Se10) 


level_energy_unit: KEV
level_spin_parity: (0,1)
level_comment:
E$weighted average of 8041 {I10} (1969Te03) and 8047 {I8} (1972Gr27). Other: 8047 (1984Se10) 
J$from 1984Se10 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
E$weighted average of 8276 {I10} (1969Te03), 8269 {I6} (1972Gr27), and 8283 {I8} (1988Fu01). Other: 8269 (1984Se10) 
S$other: 0.22 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 1-&(6)+
level_comment:
E$weighted average of 8384 {I10} (1969Te03), 8385 {I10} (1972Gr27), 8388 {I8} (1988Fu01), and 8385 {I10} (2017Ma28). Other: 8385 (1984Se10) 
J$1-,3- from 2017Ma28 
S$other: 0.25 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$weighted average of 8527 {I10} (1969Te03), 8522 {I5} (1972Gr27), 8524 {I8} (1988Fu01), and 8520 {I10} (2017Ma28). 
J$other: 3-,1+ from 2017Ma28. 
S$other: 0.26 (1972Gr27) 
$|s{-M1}(0|')(mb/sr)=0.012 {I5} 
$B(M1)|^=0.007 {I3} for J|p=1+ (2017Ma28) 


level_energy_unit: KEV
level_spin_parity: (6)
level_comment:
E$weighted average of 8562 {I7} (1972Gr27) and 8570 {I8} (1988Fu01). Other: 8572 (1984Se10) 
J$6- from (e,e') studies; but the existence of this L(p,p')=(6) state in (|a,|a') spectra is uncertain (1988Fu01) and thus a tentative J=(6) is assigned by 1988Fu01; . Other: (3) from 1984Se10 discrepant. 
S$other: 0.27 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
E$weighted average of 8603 {I10} (1969Te03), 8608 {I6} (1972Gr27), and 8615 {I8} (1988Fu01). Other: 8609 (1984Se10) 
S$other: 0.27 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
S$other: 0.07 (1972Gr27) 
E$weighted average of 8680 {I7} (1972Gr27), 8672 {I10} (1969Te03) and 8685 {I8} (1988Fu01). 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 8888 {I10} (1969Te03), 8885 {I6} (1972Gr27), 8883 {I8} (1988Fu01), and 8893 {I10} (2017Ma28). Other: 8885 (1984Se10) 
L$other: (5) from 1972Gr27 is inconsistent 
S$other: 0.30 (1972Gr27) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$weighted average of 9049 {I10} (1982Be14), 9049 {I9} (1988Fu01), and 9043 {I10} (2017Ma28). Other: 1-,2+ from 2017Ma28 


level_energy_unit: KEV
level_spin_parity: 1-&(8-)
level_comment:
E$weighted average of 9285 {I10} (1982Be14), 9297 {I9} (1988Fu01), and 9298 {I10} (2017Ma28). 
J$other: 1-,2+ from 2017Ma28 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E$weighted average of 9461 {I10} (1982Be14), 9461 {I9} (1988Fu01), and 9475 {I10} (2017Ma28). 
J$other: 1-,3- from 2017Ma28 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E$weighted average of 9536 {I10} (1982Be14), 9537 {I9} (1988Fu01), and 9548 {I10} (2017Ma28). 
J$other: 1-,3- from 2017Ma28 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$weighted average of 10212 {I10} (1982Be14) and 10210 {I10} (1988Fu01). Other: 10220 {I40} (1984Se10), 10230 (2016Bi05). 
J$J=1,2 from |s(|q), unnatural parity state from absence of peak in (|a,|a') spectra, |=2- or 1- from comparison to {+40}Ca(p,p') (1982Fu02); 1+ from |DL=0 spin-flip transition (2016Bi05) 
L$from characteristic very sharp forward peaking of |s(|q) (1983Cr01). Other: 1 from 1988Fu01 inconsistent with J|p=1+ 
$B(M1)=3.85 {I32}-4.63 {I38} |m{-N}{+2} (2016Bi05). The range is due to taking into consideration two extreme factors; with and without quenching factor: 3.85 {I32} |m{-N}{+2} is the value without quenching and 4.63 {I38} |m{-N}{+2} is with quenching. 
$Little evidence for splitting of the magnetic dipole (1991Ba26,1990Ba14); see {+48}Ca(pol p,p'): GDR,GQR. 
$1983Cr01 observed 15 additional states between 7.7 MeV and 12.7 MeV. Seven of these states are within 42 keV of those reported by 1983St09. The others observed by 1983Cr01 and reported by 1983St09 do not appear to be correlated in energy. 1983Cr01 place an upper limit of 5% of the reported B(M1)|^ strength to any other level. 


