# LEVEL

level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 2,3(+),4+
level_comment:
E$unresolved multiplet of known 3986, 4088 and 4142 levels 
$This level is populated in BR=0.25 {I4} of 1n-knockout reactions at E/A |?700 MeV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$The E{-x}=1766 state is fed by |g-ray decay from {+16}C*(3986,4088,4142) (|S=2.2%) however an additional 7.2% {I4} of feeding from other cascades is unobserved. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
BE2$From |d{-n}=1.25 fm {I30}, |d{-p}=1.07 fm {I26} and M{-n}/M{-p}=1.95 {I47}. Also B(E2:0{++}|)2{++})=5|*B(E2:2{++}|)0+)=21.7 e{+2}fm{+4} {I+114-93} =0.0022 e{+2}b{+2} {I+11-9} 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E$Potential (1/2{+-}{-|s}){+2}(1/2{++}{-|s}){+2}-bond molecular bandhead. 
J$Comparison with an AMD calculation may suggest J|p=0{++}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MS
level_comment:
T$193 ms {I6} is accepted. This is the weighted average of the values 193 ms {I6} (1995Sc03) 191 ms {I12} (P.L. Reeder et al., Int. Conf. on Nucl. Data for Science and Technology, May 9-13, 1994, Gatlinburg, Tennessee ), 180 ms {I31} (1988Sa04), 202 ms {I17} (1986Cu01), 220 ms {I80} (1986Du07). See other reported values 174 ms {I31} (1991Re02) and 188 ms {I10} (1995ReZZ,2008ReZZ). Also see 191 ms {I6} from analysis given in 2015Bi05. 
%B-N$The experimental works of (1988Mu08) and (1995Sc03) found %|b{+-}n<11% and (10.8 {I22})%, respectively, but in those cases the detectors had rather high energy thresholds. In the works of Reeder et al., a zero-threshold {+3}He counter was used. The evaluator favors the latest published value from 1994 Gatlinburg (26.0 {I18})%, but see also associated values of (32.0 {I27})% (1991Re02) and (28.4 {I13})% from unpublished comments (1995ReZZ,2008ReZZ). 
%|b{+-}n from 1994 Reeder 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
E$from weighted average of all reported values: E{-x}= 210 keV {I4} (2005El07), 212 keV {I8} (2008Su12), 218 keV {I1} (2015Sm03), 201 keV {I15} (2008St18), and 217 keV {I2} (2013Ue01). 
T$from (2015Sm03). See also T{-1/2}=404 ps {I15} ({I25} ps {Isys.}) (2008Su12). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
E$from weighted average of reported values at: E{-x}= 331 keV {I6} (2005El07), 333 keV {I10} (2008Su12), 332 keV {I1} (2015Sm03), 329 keV {I5} (2008St18), 331 keV {I2} (2013Ue01). See also E{-x}= 310 keV {I40} (2007Bo10), 292 keV {I20} (1977No08), 295 keV {I10} (1982Fi10), 
T$from (2015Sm03). See also T{-1/2}=13.1 ps {I4} ({I3.3} ps {Isys.}) (2008Su12). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: MEV
level_comment:
E$from Method of Best Representation averaging technique (2014Bi14). E{-x}=2060 keV 50 (2007Bo10) and 2200 keV {I30} (2008Sa03). 
T$From (2008Sa03), see also |G=250 keV {I100} (2007Bo10). 
J$from (2008Sa03): DWBA analysis of |s(|q). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: MEV
level_comment:
E$from Weighted Average of E{-x}=3050 keV {I30} (2008Sa03) and 3100 keV {I20} (2007Bo10). 
T$From (2007Bo10). 
J$From (2008Sa03): DWBA analysis of |s(|q). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$ Possible configuration=d{-5/2}; |b{-2}=0.52 {I4}, deduced from integrated experimental cross section for this level from 0|'-1.7|' and an assumed J{+|p} of 5/2+. 
$Cross sections: 33 mb {I4} in ({+19}C,2n{+17}C) reaction, 13.8 mb {I15} in (p,p') 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$|s (mb)=0.40 {I4} 
$ Resonance energy (c.m.)=550 {I20} (1770 {I10}, 2+ excitation energy in {+16}C) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MEV
level_comment:
$|s (mb)=0.8 {I1} 
J$ from comparisons with structure calculations 
$ Resonance energy=3630 {I90} (1770 {I10}, 2+ excitation energy in {+16}C) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
$ Configuration of state suggested to have small [d{-5/2}{+3}]{-1/2} admixture. 
E$uncertainty of 6 keV is also stated in the abstract of (2005El07). 
$Cross sections: 37 mb {I4} in ({+19}C,2n{+17}c) reaction, |?1.5 mb in (p,p') 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_comment:
T$the quoted uncertainty is statistical. The systematics uncertainty is 24 ps (2008Su12) 
E$configuration=|n{-1/2}[211] with less mixing from the |n{-1/2}[220] (1d{-5/2}) and |n{-1/2}[200] (1d{-3/2}) orbitals 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MEV
level_comment:
E,T$from E{-n}=1.86 MeV {I1} that populated {+16}C{-g.s.} (2013Ue01). See also E{-n}=1.80 MeV {I2} (1996Ra02). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MEV
level_comment:
E,T$from E{-n}=3.01 MeV {I1} that populated {+16}C{-g.s.} (2013Ue01). See also E{-n}=2.91 MeV {I5} (1996Ra02). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from 1995Sc03. Others: 66 ms {I+25-15} (1988Mu08), 78 ms {I+20-15} (1989Le16), 95 ms {I10} (1991Pr03), 92 ms 5 (2008ReZZ, see also 1991Re02, 2005ReZZ). See also 2012Ch48. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
T$from (2008On02, 2009On02), recoil-shadow method. The statistical uncertainty of 0.9 ps and systematic uncertainty of 4.4 ps in mean lifetime were combined in quadrature. 


level_energy_unit: KEV
level_comment:
$A g.s. transition is shown in the level/transition diagram of 2009On02 but is absent in 2008On02. The measured spectrum does not show strong support for this transition. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
$The mean lifetime |t=22.4 ps {I9}(stat) {I+33-22}(syst) is deduced corresponding to T{-1/2}=15.5 ps {I6}(stat) {I+23-15}(syst). 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: MS
level_comment:
T$from the weighted average of 49 ms {I4} (1988Du09: see also preliminary value 30 ms {I10} in 1988DuZT), 45.5 ms {I40} (1995Oz02) and 44.1 ms {I42} (Reeder et al., Int. Conf. on Nucl. Data for Science and Technology, May 9-13, 1994, Gatlinburg, Tennessee: see also 44 ms {I4} in the unpublished private communications of (2008ReZZ)/(1995ReZZ) and 45.5 ms {I40} (1994RaZW)). Also see 46.2 ms {I40} in (2015Bi05). 
J$from analysis of breakup fragment momentum distributions in 2001Ma08. 
$Decay: Studies of the |b-delayed neutron emission have been carried out in (1991Re02: |b{+-}n=|b{-1n}+2(|b{-2n})+3(|b{-3n})...=(53 {I26})%), (1995ReZZ/2008ReZZ: |b{+-}n=(66 {I9})%), and (1988Du09: |b{-1n}=(47 {I3})% and |b{-2n}=(7 {I3})%. Analysis of |b-|g coincidences indicate the |b{-1n} decay populates {+19}N*(6400,6508,7025), which subsequently neutron decay to {+18}B*(115,587) see (1995Oz02). There is evidence for additional branches that |b-2n decay to {+17}B with |b-2n=(7 {I3})% (1988Du09). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
E$from (2015Wh02). See also 2005El07: 197 keV {I6}, 2015Va09: 198 keV {I10}, and 2008St18: 201 keV {I15}. 
T$Analysis of the spectra using lineshape and recoil-distance techniques indicate T{-mean}=198 ns {I10} and 190 ns {I10} values, respectively (2015Wh02). Additional systematic uncertainties give final uncertainties of T{-mean}=198 ns {I12} and 190 ns {I13} for the two methods, respectively. The authors give a recommended value T{-mean}=194 ns {I15}. 
J$from 2015Wh02, based on the B(M1) value; E2 components are excluded and neglected. 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$from E|g=72 keV {I4} to E{-x}=209 keV {I2} 
$The J|p of this state had initially been suggested as 5/2+ based on expectations from shell model analysis. In this case |b{-2}=0.29 {I3}; deduced from integrated experimental cross section for this state from 0|'-1.7|' and distorted wave analysis (2005El07). However, subsequent observations and discussion in (2011Oz01, 2012Ko38, 2013Th06) support the notion that the first J|p=5/2+ state must be unbound. 
$Cross section: 4.2 mb {I5} in (p,p') 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_uncertain: ?
level_comment:
$Configuration of state suggested as mixture of d{-5/2}{+5}, d{-5/2}{+5}~#s{-1/2}{+2} and d{-5/2}{+4}~#s{-1/2} configurations (2001Ma08). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_uncertain: ?
level_comment:
$|b{-2}=0.29 {I3}; deduced from integrated experimental cross section for this state from 0|'-1.7|' and distorted wave analysis (2005El07). 
$Cross section: 4.2 mb {I5} in (p,p') 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MEV
level_comment:
$|s (mb)=8.6 {I4} 
$Resonance energy(c.m.)=880 keV {I10} (g.s. in {+18}C) 
J$from DWBA analysis of angular distribution. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: NS
level_comment:
T$Analysis of the spectra using lineshape and recoil-distance techniques indicate T{-mean}=198 ns {I10} and 190 ns {I10} values, respectively (2015Wh02). Additional systematic uncertainties give final uncertainties of T{-mean}=198 ns {I12} and 190 ns {I13} for the two methods, respectively. The authors give a recommended value T{-mean}=194 ns {I15}. 
J$from 2015Wh02, based on the B(M1) value; E2 components are excluded and neglected. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$deduced from E({+18}C+n)=76 keV {I14} and S(n)=577 keV {I94} (from http://amdc.in2p3.fr/masstables/Ame2003/rct2.mas03). Rounded value of S(n) is 580 keV {I90} in published 2012Wa38 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$3/2+ or 5/2+ from shell-model predictions; the latter would require 201|g to be E2 and corresponding half-life|?1 |ms for 201 level 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from weighted average of: 16 ms {I+14-4} (1989Le16), 14 ms {I+6-5} (1990Mu06),16.7 ms {I35} (1995ReZZ, 2008ReZZ), 22 ms {I+15-7} (2003Yo02), see also 16.2 ms {I35} in the review of (2015Bi05). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$from the E{-|g} measurements of 2011Pe21 using Doppler corrected germanium spectra. 
T$from 2011Pe21. The mean lifetime |t=9.8 ps {I28}(stat) {I+5-11}(syst) is deduced corresponding to T{-1/2}=6.8 ps {I19}(stat) {I+5-11}(syst). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$from 2011Pe21. The mean lifetime |t=9.8 ps {I28}(stat) {I+5-11}(syst) is deduced corresponding to T{-1/2}=6.8 ps {I19}(stat) {I+5-11}(syst). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$From 2003Yo02. Other value: 9 ms {I3} (1998Yo06). 
%B-N$From 2003Yo02. Total neutron emission probability p{-n}>60 (1998Yo06) 
%B-2N$From 2003Yo02 
$Measured reaction cross section=1.34 b {I27} (2010Ta04 - assuming no excited states in {+22}C). 
$Deduced rms radius=5.4 fm {I9} (2010Ta04) 
$Halo structure of {+22}C is suggested in 2010Ta04 from comparison of measured reaction cross sections for {+22}C, {+20}C and {+19}C isotopes and from deviation of systematic trend for measured rms radius in C isotopes. The two-valence neutrons in {+22}C preferentially occupy the 1s{-1/2} orbital (from Glauber model calculation - 2010Ta04). Also supported in 2012Ko38 from two-neutron removal reaction studies of {+22}C on a carbon target. 
$Two-neutron removal cross section 266 mb {I19}, measured from the C({+22}C,{+20}C), E=240 MeV/A, knock-out reaction (2012Ko38). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E from E{-res}=1.49 MeV {I6}, see comments. 
E there are essentially three high resolution measurements of the {+11}N ground state mass. They do not have overlap in their uncertainties. The measured values, in the {+10}C+p relative energy system, are E{-res}=1.54 MeV {I2} (2006Ca05) from {+1}H({+10}C,{+1}H), 1.63 MeV {I5} (2000Ol01) from {+10}B({+14}N,{+13}B) and 1.31 MeV {I5} (2003Gu30) from {+14}N({+3}He,{+6}He). In this situation, the evaluator has taken the unweighted average and assigned an uncertainty of 60 keV. This yields reasonable agreement with each value and the average. Other reported values are E{-res}=1.27 MeV {I+18-5} (2006Ma62) and 1.45 MeV {I40} (1998Az01). 
WIDTH From (2006Ca05). The measured widths are in poor agreement. Reported values are |G=0.83 MeV {I3} (2006Ca05) from {+1}H({+10}C,{+1}H), 1.44 MeV {I20} (2000Ma62) from {+1}H({+10}C,{+1}H), >400 keV (1998Az01) from {+9}Be({+12}N,{+10}C+p), 0.4 MeV {I1} (2000Ol01) from {+10}B({+14}N,{+13}B) and 0.24 MeV {I24} (2003Gu30) from {+14}N({+3}He,{+6}He). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MEV
level_comment:
E E{-res.}=2220 keV {I30} from the weighted average of E{-res.}=2240 keV {I50} from {+1}H({+10}C,p), E{-res.}=2160 keV {I50} from {+10}B({+14}N,{+13}B), E{-res.}=2180 keV {I50} from {+12}C({+14}N,{+15}C). The value E{-res.}=2310 keV {I20} from {+14}N({+3}He,{+6}He) was not included in the average because it is significantly larger and has no overlap with other values. 
WIDTH From the unweighted average of |G=960 keV {I160} from {+1}H({+10}C,p), 250 keV {I80} from {+10}B({+14}N,{+13}B), 440 keV {I80} from {+12}C({+14}N,{+15}C) and 730 keV {I60} from {+14}N({+3}He,{+6}He). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E E{-res.}=3690 keV {I30} from the weighted average of E{-res.}=3750 keV {I50} from {+1}H({+10}C,p), E{-res.}=3610 keV {I50} from {+10}B({+14}N,{+13}B), E{-res.}=3630 keV {I50} from {+12}C({+14}N,{+15}C), E{-res.}=3780 keV {I50} from {+14}N({+3}He,{+6}He). 
WIDTH From the weighted average of |G=600 keV {I50} from {+1}H({+10}C,p), 500 keV {I80} from {+10}B({+14}N,{+13}B), 400 keV {I80} from {+12}C({+14}N,{+15}C) and 560 keV {I170} from {+14}N({+3}He,{+6}He). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E E{-res.}=4350 keV {I30} from the weighted average of E{-res.}=4330 keV {I50} from {+1}H({+10}C,{+1}H), E{-res.}=4330 keV {I50} from {+10}B({+14}N,{+13}B), E{-res.}=4390 keV {I50} from {+12}C({+14}N,{+15}C). The value E{-res.}=4560 keV {I10} from {+14}N({+3}He,{+6}He) was not included in the weighting because it is significantly larger and has no overlap with other values. 
WIDTH From the weighted average of |G=450 keV {I80} from {+10}B({+14}N,{+13}B) and 300 keV {I50} from {+14}N({+3}He,{+6}He). Also see |G|?270 from {+1}H({+10}C,p) and |<220 keV from {+12}C({+14}N,{+15}C). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
E from E{-res.}=5910 keV {I30} from the weighted average of E{-res.}=5870 keV {I150} from {+12}C({+14}N,{+15}C), E{-res.}=5980 keV {I100} from {+10}B({+14}N,{+13}B), E{-res.}=5910 keV {I30} from {+14}N({+3}He,{+6}He). 
WIDTH See 100 keV {I60} from {+10}B({+14}N,{+13}B), 700 keV {I200} from {+12}C({+14}N,{+15}C) and 1.30 MeV {I9} from {+14}N({+3}He,{+6}He). 
J|p: (5/2-) from {+10}B({+14}N,{+13}B) and DWBA analysis in {+14}N({+3}He,{+6}He). Also see (7/2-) from {+12}C({+14}N,{+15}C). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_comment:
E from E{-res.}=6.57E3 keV 10 from the weighted average of E{-res.}=6540 keV {I100} from {+10}B({+14}N,{+13}B), E{-res.}=6800 keV {I300} from {+14}N({+3}He,{+6}He). 
WIDTH From {+10}B({+14}N,{+13}B). 
J|p: from DWBA analysis in {+14}N({+3}He,{+6}He). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_comment:
E from {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}, see comments in the adopted levels data set. 
For {+1}H({+10}C,p) the reported ground state energy E{-res}=1.54 MeV {I2} from (2006Ca05) lies above the adopted ground state energy E{-res}=1.49 MeV {I6}. The energies of higher excited states are deduced assuming {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}. 
E from E{-res}=1.54 MeV {I2} (2006Ca05). See also 1.27 MeV {I+18-5} (2000Ma62) and E{-res}=1.30 MeV {I4} (1996Ax01); (2000Ma62) is a reanalysis of (1996Ax01) with additional data. The two experimental results (2006Ca05) and (2000Ma62) are in poor agreement; the precision of (2006Ca05) was found to dominate any weighting. 
WIDTH From |G=0.83 MeV {I3} (2006Ca05), also see |G=1.44 MeV {I20} (2000Ma62) and |G=0.90 MeV {I+10-20} (1996Ax01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MEV
level_comment:
E from E{-res}=2.24 MeV {I5} and {+11}N{-g.s.}=E{-res.}=1.49 MeV {I6}. 
E from weighted average of E{-res}=2.27 MeV {I5} (2006Ca05) and 2.01 MeV {I+15-5} (2000Ma62); see also E{-res}=2.04 MeV {I4} (1996Ax01). 
WIDTH From |G=1.15 MeV {I25} (2006Ca05) and 0.84 MeV {I20} (2000Ma62), also see |G=0.69 MeV {I+5-10} (1996Ax01). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MEV
level_comment:
E from E{-res}=3.75 MeV {I5} (2000Ma62) and {+11}N{-g.s.}=E{-res.}=1.49 MeV {I6}; see also E{-res}=3.72 MeV {I4} (1996Ax01). 
WIDTH From (2000Ma62), also see |G=0.60 MeV {I+10-4} (1996Ax01). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E from E{-res}=4330 MeV {I50} (2000Ma62) and {+11}N{-g.s.}=E{-res.}=1.49 MeV {I6}; see also E{-res}=4.32 MeV (1996Ax01). 
WIDTH From (2000Ma62); also see |G=70 keV (1996Ax01). 
J|p: from (2000Ma62). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=GT
level_uncertain: ?
level_comment:
E from {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}, see comments in the adopted levels data set. 
For {+9}Be({+12}N,{+11}N) the reported ground state energy E{-res}=1.45 MeV {I40} from (1998Az01) lies below the adopted ground state energy E{-res}=1.49 MeV {I6}. The energies of higher excited states are deduced assuming {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}. 
E from E{-res}=1.45 MeV {I40}. Ambiguity exists in determining the {+11}N parent level, since reactions involving higher lying {+11}N that decay to excited states in {+10}C are not distinguishible from population and decay of the {+11}N ground state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E from the known E{-res}|?2240 keV (1974Be20) and {+11}N{-g.s.}=E{-res.}=1.49 MeV {I6}; the value was fixed in the analysis. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_comment:
E from {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}, see comments in the adopted levels data set. 
For {+10}B({+14}N,{+13}B)) the reported ground state energy E{-res}=1.63 MeV {I5} from (2000Ol01) lies above the adopted ground state energy E{-res}=1.49 MeV {I6}. The energies of higher excited states are deduced assuming {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}. 
E |G: from E{-res}=1.63 MeV {I5} (2000Ol01) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MEV
level_comment:
E from {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}, see comments in the adopted levels data set. 
For {+12}C({+14}N,{+15}C) the ground state is not observed. The energies of higher excited states are deduced assuming {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}. 
E |G: from E{-res}=2.18 MeV {I5} (1998Le06) and {+11}N{-g.s.}=E{-res.}=1.49 MeV {I6}. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_comment:
E from {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}, see comments in the adopted levels data set. 
For {+14}N({+3}He,{+6}He) the reported ground state energy E{-res}=1.31 MeV {I5} from (2003Gu06) lies above the adopted ground state energy E{-res}=1.49 MeV {I6}. The energies of higher excited states are deduced assuming {+11}N{-g.s.}=E{-res}=1.49 MeV {I6}. 
E |G: from E{-res}=1.31 MeV {I5} (2003Gu06). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MEV
level_comment:
E from E{-res}=2.31 MeV {I2} (2003Gu06) and {+11}N{-g.s.}=E{-res.}=1.49 MeV {I6}; see also E{-res}=2.24 MeV {I10} (1974Be20). 
WIDTH From |G=0.74 MeV {I10} (1974Be20) and 0.73 MeV {I6} (2003Gu06). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-T} (keV): (p+{+10}C) total kinetic energy: Appears to decay via both p{-0} and p{-1} to {+10}C*(3345). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
J$Deduced from comparison between the momentum correlations of the two protons emitted by the decay of this state with those of {+12}O{-g.s.} and {+16}Ne{-g.s.}, which are known {+2}He emitters. This comparison indicates a significant 1{Is}{-1/2}{+2} decay component, which confirms the J{+|p}=3/2{+-} for this state. 
$Decays to {+9}B{-g.s.}+2p via {+2}He decay. The diproton nature of this 2p decay is identified by comparing the momentum correlations observed for the two protons from the decay of this state with those of the ground state systematics of known diproton emitters in this mass region. If the 2p decay were to be of democratic nature, one would have expected to see a wide {+10}C* {Is}-wave resonance with J{+|p}=1{+-} or J{+|p}=2{+-}, which would act as an intermediate state in such a decay. Such a state is not present, which supports the diproton nature of this state's decay. 
$Deduced a Thomas-Ehrman shift of 542 keV {I12} for this state. 
$This state has an |a-cluster structure. 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_comment:
E$E{-x}=6433 keV {I104} deduced from a total decay energy of 4081 keV {I104}. 
$Decays to {+9}B{-g.s.}+2p, or to {+10}C*(5222 keV, 2{++})+p. The {+10}C*(5222 keV, 5/2{++}) state decays via proton emission to {+9}B{-g.s.}. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
T$Deduced from R-matrix lineshape for diproton emission to {+9}B*(2345 keV, 5/2{+-}). 
$Decays to {+9}B*(2345 keV, 5/2{+-})+2p. The 2p emission is of democratic nature. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MS
level_comment:
$T{-1/2}: The half-life of {+12}N is 11.000 ms {I16} (1978Al01). Other values are reported at T{-1/2}=10.95 ms {I5} (1963Fi05), 11.43 {I5} (1958Ve20), 11.0 {I1} (1963Pe10), 11.1 ms {I2} (1962Po02) and 11.2 {I4} (1959Fa03). 
${+12}N decays to {+12}C*(0,4.44,7.65,10.3,12.71,15.11). 
MOMM1$ See also |m=4573 {I5} (1968Su05). 
MOME2$See also Q=0.0103 {I7} (1994OhZY) and [+0.049 {I6} or -0.010 {I6}] (1980Ra05). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
E$From (1974Fu11, 1976Ma15, 1983St10, 2013So11, 2015Ch50) 
WIDTH$From (1976Ma15,1983St10,2013So11,2015Ch50) and {+10}B({+3}He,n) references in (1980Aj01). 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: MEV
level_comment:
E$From (1974Fu11, 1976Ma15, 1983St10, 1996An08, 2015Ch50) 
WIDTH$From (1974Fu11, 1976Ma15, 1983St10, 1996An08, 2015Ch50) using the Method of Best Representation averaging technique. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From E(2p+{+10}B*(1740))=1.165 MeV {I20} and |DM=29534 keV {I29}. 
$|G: Deduced after correcting for experimental resolution. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
J$From L=0 {+15}N(p,t) (1968Fl03) 
T$From the average of T{-1/2}=9.9502 min {I32} (2022Lo14), 9.962 min {I20} (1989KaYR), 9.967 min {I10} (1980An40), 9.965 min {I10} (1977Az01), 10.0 min {I5} (1973SiYS), 9.963 min {I9} (1968Ri15), 10.05 min {I5} (1965Bo42), 9.96 min {I2} (1965Eb01), 9.965 min {I5} (1960Ja12), 9.93 min {I5} (1960Ki02), 9.96 min {I3} (1958Ar15), 9.96 min {I3} (1957Da08, 1958Da09), 10.02 min {I10} (1957De22), 10.07 min {I6} (1957No17), 10.08 min {I4} (1955Wi43), 10.05 min {I3} (1953Ch34), 10.05 min {I10} (1950Ho01), 10.2 min {I1} (1948Co24) 10.13 min {I10} (Siegbahn, Arkiv. f. Ast. Math-Fys. 32|a No. 9 (1945)) 9.93 min {I3} (1939Wa09). 
T$See also 12.3 min |+5.4% (1961Ra06), 9.9670 min {I37} (DDEP) and 9.9647 min {I39} (2008Se10) 
T$In (1935Ru01), Rutherford discusses |b decay. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p 
E$From the average of E{-x}=2367.6 keV {I9} from references in {+12}C(p,|g), 2369 keV {I3} from (1953Ja04) in {+12}C(p,p):res and 2368.2 keV {I28} from (1974Bl06) {+12}C({+3}He,d). 
J$From L=0 {+12}C(p,p):res (1951Ja21) 
WIDTH$From the average (external errors) of |G=36.15 keV {I54} (1973Cl04) {+12}C(d,n), 36.1 keV {I28} (1974Bl06) {+12}C({+3}He,d), 34.5 keV {I9} (1953Hu18,1973Cl04) {+12}C(p,|g), 33.7 keV {I20} (1968Bl17) {+12}C(p,|g) 31.4 keV {I9} (1968Ri16) {+12}C(p,|g), 33.3 keV {I18} (1974Bl06) {+12}C(p,|g), 36 keV {I2} (1974Ro29) {+12}C(p,|g), 34.9 keV {I2} (2023Sk02) {+12}C(p,|g) 35.2 keV {I5} (2023Cs01) {+12}C(p,|g) and 34.0 keV {I2} (2023Ke11: includes 2008Bu19) {+12}C(p,|g). Note: uncertainty surrounds some |G values related to assigning the values as lab or c.m. frame values. Table 1 of (1992Hi14) is helpful for resolving some issues. 
WIDTH$In (1991Aj01) |G=31.7 keV {I8} was determined by averaging only (1974Bl06) and (1968Ri16) values from {+12}C(p,|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p 
E$From E{-x}=3499 keV {I6} (1966Ar03) {+12}C(p,p):res and 3500.4 keV {I8} from references in {+12}C(p,|g). 
J$From L=0,2 {+11}B({+3}He,n) (1971Hs03) 
WIDTH$From the average of |G=60 keV {I3} (1974Ro29) {+12}C(p,|g), 61.9 keV {I40} (1968Bl17) {+12}C(p,|g), 55.2 keV {I3} (2023Ke11) {+12}C(p,|g), 53.2 keV {I7} (2023Cs01) {+12}C(p,|g), and 63 keV {I4} (2005Kn02) {+13}O |b-p. 
WIDTHG0$From the R-matrix analysis in (2023Ke11) as detailed above. In (1991Aj01) the analysis of (1952Se01, 1963Yo06) data given in (1980Ba54) was accepted. 
WIDTHG1$From |G{-|g0}, I(|g0)=92% {I1} and I(|g1)=8% {I1} from (1974Ro29). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From the average of E{-x}=3544.4 keV {I5} from the (2023Ke11) analysis of (1976Me22) {+12}C(p,p):res and 3549.1 keV {I50} (1974Bl06) {+12}C({+3}He,d). 
J$From phase-shift analysis of {+12}C(p,p) (1951Ja21). 
WIDTH$From the (2023Ke11) R-matrix analysis of (1976Me22) {+12}C(p,p):res. See also 47 keV {I7} from (1974Bl06). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Mode: p 
E$From the weighted average (external errors) of E{-x}=6378 keV {I8} (1956Re39) {+12}C(p,p):res, 6353 keV {I9} (1971Hs03) {+11}B({+3}He,n) and 6380 keV {I30} (1968Fl03) {+15}N(p,t). 
J,WIDTH$From phase-shift analysis (1956Re39) {+12}C(p,p):res 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From the average of E{-x}=6890 keV {I6} from values in {+12}C(p,p):res and 6875 keV {I10} (1971Hs03) in {+11}B({+3}He,n). 
J$From phase-shift analysis of angular distributions and |s(E) in (1956Re39) {+12}C(p,p),(p,p{-1}|g(|q)). 
WIDTH$From the average of |G=115 keV {I5} (1963Ni05) {+12}C(p,p):res, 110 keV {I15} (1962Cl12) {+14}N({+3}He,|a) and 120 keV {I30} (1974Ho06) {+10}B({+6}Li,t). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From the average of E{-x}=7145 keV {I9} (1971Hs03) {+11}B({+3}He,n), 7155 keV {I9} (1963Ba36) {+12}C(p,p):res and 7166 keV {I8} (1962Cl12) {+14}N({+3}He,|a) 
J$From phase-shift analysis in (1963Ba36, 1963Ni05) {+12}C(p,p):res 
WIDTH$From (1963Ni05) {+12}C(p,p):res 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From the average of E{-x}=7363 keV {I8} (1971Hs03) {+11}B({+3}He,n), 7.38 MeV {I1} (1963Ba36) {+12}C(p,p), 7380 keV {I20} (1968Fl03) {+15}N(p,t) and 7388 keV {I8} (1962Cl12) {+14}N({+3}He,|a). 
J$From phase-shift analysis of {+12}C(pol. p,p) (1968Be31). L=2 {+15}N(p,t) (1968Fl03). 
WIDTH$From the average (external errors) of |G=69 keV {I5} (1963Ni05) {+12}C(p,p):res, 104 keV {I20} (2005Kn02) {+13}O |b-p and 45 keV {I10} (1962Cl12) {+14}N({+3}He,|a). 
WIDTH$In (1970Aj04) the value |G=75 keV {I5} from (1963Ni05) is listed, but this value, given in the abstract of (1963Ni05) was |G{-lab}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
$Decay Mode: p 
E,T$From (1962Sh22, 1966Ba35) {+12}C(p,p):res. See also E{-x}=8200 keV {I22} from (1971Hs03) {+11}B({+3}He,n), but note that data supporting this value is not shown in the article. 
J$From phase-shift analysis of {+12}C(p,p) (1962Sh22). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From (1971Hs03) {+11}B({+3}He,n) 
J$From L=0 {+15}N(p,t) (1968Fl03) and phase-shift analysis of {+12}C(p,p) (1962Sh22). 
WIDTH$From (2005Kn02) {+13}O |b-p. See also 230 keV from {+12}C(p,p):res. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From (1974Ho06) {+10}B({+6}Li,t) 
J$In (1974Ho06) comparison of angular distributions in {+10}B({+6}Li,{+3}He) and {+10}B({+6}Li,t) indicates the state is the analog of {+13}C{+*}(9.5 MeV), which is presently identified as 9/2{++}. See also L=4 in {+12}C({+3}He,d) (1980Pe13). 
WIDTH$See also 0.40 MeV {I5} in {+12}C({+3}He,d) (1969Fo02). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Mode: p 
E$From (1971Hs03) {+11}B({+3}He,n). See also E{-x}=9520 keV {I20} from (1966Ch18) {+11}B({+3}He,n). 
J$From L=0,2 {+11}B({+3}He,n) (1971Hs03) and phase-shift analysis of {+12}C(p,p) (1962Sh22). 
WIDTH$From (1962Sh22) {+12}C(p,p):res. See also |G=143 keV {I18} (2005Kn02) {+13}O |b-p, but note the fit in this region is rather poor. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p 
E,WIDTH$From (1973Me12) {+12}C(p,|g). For J{+|p}=3/2+, |G{-lab}=280 keV {I100} and for J{+|p}=1/2+, |G{-lab}=300 keV {I100}. 
J$From {+12}C(p,|g{-0}) (1973Me12) where |q{-|g}=90|' and |g{-0} to {+13}N{-g.s.}(J|p=1/2-) is observed. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Mode: p 
E,WIDTH$From (1968Be31) {+12}C(p,p):res where the 5/2- and 7/2- doublet partners are both analyzed. In (1968Be31) the authors find the level energies do not differ by more than 2 keV. See also E{-x}=10381 keV {I8} (1971Hs03) {+11}B({+3}He,n) and 10350 keV {I20} (1966Ch18) {+11}B({+3}He,n). 
J$From phase-shift analysis of {+12}C(pol. p,p) (1968Be31). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Mode: p 
E,WIDTH$From (1968Be31) {+12}C(p,p):res. See above comment. 
J$From phase-shift analysis of {+12}C(pol. p,p) (1968Be31). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E$From (1971Hs03) {+11}B({+3}He,n) 
J$From L=0 {+15}N(p,t) (1968Fl03). 
WIDTH$From (1980Pe13) {+12}C({+3}He,d) 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
$Decay Modes: p, |a 
E,J,T$Deduced in (2024Bi01) {+13}O |b{++}+|e; if decay from this state is visible in the delayed proton spectrum of (2005Kn02), then (2024Bi01) suggest |G<40 keV. 
$Suggested to decay via |a{-0}+{+9}B{-g.s.}, p+{+12}C{-g.s.} and p+{+12}C(7654.7 MeV). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From (1971Hs03) {+11}B({+3}He,n). See also E{-x}=11490 keV {I50} (1973Me03) {+12}C(p,p):res. 
J$From phase-shift analysis of {+12}C(pol.p, p),(pol. p,p') (1973Me03) 
WIDTH$From (1973Me03) {+12}C(p,p):res. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E,J,WIDTH$From (1973Me03) {+12}C(p,p):res 
J$From phase-shift analysis of {+12}C(pol.p, p),(pol. p,p') (1973Me03). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p 
E,WIDTH$From (1973Me03) {+12}C(p,p):res where the 3/2+ and 3/2- doublet partners are both analyzed. 
J$From phase-shift analysis of {+12}C(pol.p, p),(pol. p,p') (1973Me03). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E,WIDTH$From (1973Me03) {+12}C(p,p):res. Other results associated with J|p=3/2- but reported with energies near the next highest level are E{-x}=11878 keV {I12} (1971Hs03) {+11}B({+3}He,n), 11850 keV {I40} (1969Ba06) {+13}C({+3}He,t) and 11880 keV {I40} (1968Fl03) {+15}N(p,t); these likely correspond to unresolved 3/2{+-} and 1/2{++} states. 
WIDTH$See also 98 keV (2004Fu12) {+13}C({+3}He,t). {+13}C({+3}He,t) 
J$From phase-shift analysis of {+12}C(pol.p, p),(pol. p,p') (1973Me03). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E,WIDTH$From (1973Me03) {+12}C(p,p):res 
J$From phase-shift analysis of {+12}C(pol. p,p) (1973Me03); see also J|p=3/2- from L=0,2 {+11}B({+3}He,n) (1971Hs03) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E,WIDTH$From (1973Me03) {+12}C(p,p):res. See also E{-x}=12130 keV {I60} (1972Ma72) {+16}O(p,|a). 
J$From phase-shift analysis of {+12}C(pol.p, p),(pol. p,p') (1973Me03). 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_uncertain: ?
level_comment:
$Decay Modes: p, |a 
E,J$Deduced in (2024Bi01) {+13}O |b{++}+|e 
$Suggested to decay via |a{-0}+{+9}B{-g.s.}, |a{-1}+{+9}B(1.8 MeV) and p+{+12}C(7654.7 MeV). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=GT
level_comment:
E,WIDTH$From (1971Hs03) {+11}B({+3}He,n). 
$Decay Mode: p 
E$See nearby E{-x}=13260 keV {I100} with |G|?520 keV reported in (2005Kn02) {+13}O |b-p. 


level_energy_unit: KEV
level_spin_parity: [1/2-,5/2-]
level_uncertain: ?
level_comment:
$Decay Modes: p, |a 
E,J$Deduced in (2024Bi01) {+13}O |b{++}+|e 
J$1/2{+-} for |a{-4} decay through {+9}B(2.78:1/2{+-}) is preferred. 
$Suggested to decay via |a{-1}+{+9}B(1.8 MeV), |a{-0}+{+9}B(2.75 MeV) or |a{-0}+{+9}B(2.78 MeV) and p+{+12}C{-g.s.}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
$Decay Modes: |g, p 
E,WIDTH$From (1973Me12) {+12}C(p,|g) 
J$From {+12}C(p,|g{-0}) (1973Me12) where detector(|q)=90|' and |g{-0} to {+13}N{-g.s.}(J|p=1/2-) is observed; also strong interference with J|p=3/2{++} states at {+13}N{+*}(11.74, 14.05); assumed component of GDR. 
WIDTH$See also |G|?7.9 MeV (1994Ha41) {+13}C(|p{++},|p{+0}) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
$Decay Mode: p 
E,WIDTH$From (2009Ch38) {+9}Be({+10}C,{+13}N) 
WIDTH$See also |G|?500 keV (1961Na02) {+12}C(p,p):res. and |G|? few hundred keV (1972Ma21) {+16}O(p,|a) 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_uncertain: ?
level_comment:
$Decay Modes: p, |a 
E,J$Deduced in (2024Bi01) {+13}O |b{++}+|e 
$Suggested to decay via |a{-0}+{+9}B{-g.s.}, |a{-1}+{+9}B(1.8 MeV), |a{-0}+{+9}B(2.75 MeV) and p+{+12}C(7.6547 MeV). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p, |a 
E$From (1976Me18) {+12}C(p,p):res. See also E{-x}=14050 keV {I80}. 
J$From phase-shift analysis of {+12}C(pol. p,p) (1976Me18). 
WIDTH$From the average of |G=157 keV {I18} (1973Me12) {+12}C(p,|g) and 180 keV {I35} (1976Me18) {+12}C(p,p):res. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p, |a 
E,WIDTH$From (1973Hu07) {+12}C(p,p):res. 
E$See also E{-x}=15064 keV {I4} (1969Le18) and 15068 keV {I8} (1969Ad02). 
WIDTH$See also |G=1.10 keV {I9} (1975Hi07) {+12}C(p,|a). Beginning in (1981Aj01) the value |G=0.86 keV {I12} was given in the evaluations. This value is derived in (1977Ma16) using their measured |G{-p0}|G{-|g0}/|G=5.79 eV {I20} value. 
J$From L=0 {+11}B({+3}He,n) (1971Hs03) and phase-shift analysis of (1969Le18) 
WIDTHP,WIDTHA$Branching ratios for p- and |a-decay branches are from (1973Ad02); partial widths are deduced using these and |G=0.932 keV {I28}. 
WIDTHP$See also |G{-p}(|){+12}C(9.6 MeV))/|G=0.096 {I14} and |G{-p}(|){+12}C(10.8 MeV))/|G=0.164 {I36} 1967AdZY; these imply |G{-p} (|){+12}C(9.6 MeV))=89.5 eV {I5} and |G{-p}(|)10.8 MeV)=153 eV {I34}. Hence |G{-p}=651 eV {I40} for all proton branches. 
WIDTHG0$|G|g{-0}=24.5 eV {I15} is obtained by combining |G{-p0}/|G=0.236 {I12} (1973Ad02) with |G{-p0}|G|g0/|G=5.79 eV {I20} (1975Ma21). 
WIDTHG$|G|g=44.1 eV {I35} from |G|g{-0}=24.5 eV {I15} |G|g{-1}|<2.82 eV {I30} and |G|g{-(2+3)}=19.6 eV {I14} (1975Ma21,1973Ad02) 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MEV
level_comment:
$Decay Modes: |g, p 
E,WIDTH$From (1973Me12) {+12}C(p,|g) 
J$From {+12}C(p,|g{-0}) (1973Me12) |q{-|g}=90|' and |g{-0} to {+13}N{-g.s.}(J|p=1/2-) is observed. See also (3/2-) in (2005Kn02) {+13}O |b-p; but note the reported %I|b=0.004 {I3} intensity corresponds to perhaps three counts in a region where no background contribution is considered. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, |a 
E$From the average of E{-x}=16010 keV {I40} (1973Me12) {+12}C(p,p):res and E{-x}=15980 keV {I50} (1969Ba06) {+13}C({+3}He,t). See also E{-x}=16 MeV and |G=500 keV (1964Da03) {+12}C(p,p):res. 
J$From phase-shift analysis of {+12}C(pol. p,p) (1976Me18). 
WIDTH$From (1973Me12). See also |G|?100 keV (1969Le18) {+12}C(p,|a) and |?163 keV (2004Fu12) {+13}C({+3}He,t). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From (2004Fu12) {+13}C({+3}He,t). 
$Decay Modes: |g, p 
E,J$(1988Vo08) {+12}C({+13}C,{+12}B) suggests a broad (5/2{++}) GDR component near E{-x}=16.2 MeV. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E$From the average of E{-x}=18150 keV {I30} (1976Me18) {+12}C(p,p):res and 18120 keV {I20} (2004Fu12) {+13}C({+3}He,t). 
J$From phase-shift analysis of {+12}C(pol. p,p) (1976Me18). 
WIDTH$From the average of |G=322 keV {I75} (1976Me18) and 276 keV {I41} (2004Fu12). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, |a 
E,WIDTH$From (1976Me18) {+12}C(p,p):res. See also E{-x}=18232 keV and |G=300 keV in (1969Le18) {+12}C(p,|a) 
J$From phase-shift analysis of {+12}C(pol. p,p) (1976Me18). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, |a 
E,WIDTH$See comments in {+12}C(p,p):res. Values are apparently from (1968Sn03) and a private communication reported in (1970Aj04). See also E{-x}=18370 keV {I10} (2004Fu12) {+13}C({+3}He,t) and 18440 keV {I40} (1969Ad02) {+11}B({+3}He,n). 
J$From phase-shift analysis of {+12}C(p,p) (1969Le18). 


level_energy_unit: KEV
level_spin_parity: (3/2-,7/2+)
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, |a 
E$From the average of E{-x}=18960 {I9} see comments in {+12}C(p,p):res and 18980 keV {I20} (1969Ad02) {+11}B({+3}He,n). 
J$From phase-shift analysis in (1969Le18) {+12}C(p,p) 
WIDTH$See discussion in {+12}C(p,p):res related to (1968Sn03). See also |G=40 keV {I20} (1969Ad02). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, |a 
E,WIDTH$From (2004Fu12) {+13}C({+3}He,t) 
J$From phase-shift analysis of {+12}C(p,p) (1969Le18). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Modes: p, |a 
E$From (1969Le18) {+12}C(p,p),(p,|a). 
J$From (1979Ga13) analysis of |s(|q) and A{-y}(|q) from {+12}C(pol. p,p),(pol. p') See also 3/2{++} in phase-shift analysis (1969Le18). 
WIDTH$From (1979Ga13) {+12}C(p,p):res. See also |G=520 keV (1969Le18) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E,WIDTH$From (1979Ga13) {+12}C(p,p):res. 
$Decay Mode: p 
J$From (1979Ga13) analysis of |s(|q) and A{-y}(|q) from {+12}C(pol. p,p),(pol. p') 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Modes: |g, p, (n) 
E$From (1973Me12) {+12}C(p,p):res 
E$In {+12}C(p,|g) broad |G|?1.2-4.0 MeV groups are reported with E{-x} ranging from 20.0 MeV to 20.8 MeV. 
J$From (1979Ga13) analysis of |s(|q) and A{-y}(|q) from {+12}C(pol. p,p),(pol. p') 
WIDTH$From (1979Ga13) {+12}C(p,p):res. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$Decay Mode: p 
E,WIDTH$From (2004Fu12) {+13}C({+3}He,t). The previous evaluation accepted a state at E{-x}=21.4 MeV with |G=750 keV (1979Ga13) {+12}C(p,p):res; the evaluator assumes (2004Fu12) observed the same level. 
J$From (1979Ga13) analysis of |s(|q) and A{-y}(|q) from {+12}C(pol. p,p),(pol. p') 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_comment:
$Decay Mode: p 
E$From {+12}C(p,p):res. See for discussion on (1964Ta15) analysis of (1963Di16) data and see (1979Ga13). 
J$From (1979Ga13) analysis of |s(|q) and A{-y}(|q) from {+12}C(pol. p,p),(pol. p') and (1964Ta15). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$Decay Modes: |g, p 
E,WIDTH$From (2004Fu12) {+13}C({+3}He,t). The previous evaluation accepted a state at E{-x}=22.4 MeV {I5} with |G|?1 MeV (1973Me12, 1979Ga13) {+12}C(p,p):res; the evaluator assumes (2004Fu12) observed the same level. 
J$From (1979Ga13) analysis of |s(|q) and A{-y}(|q) from {+12}C(pol. p,p),(pol. p') 
E,J$(1988Vo08) {+12}C({+13}C,{+12}B) suggests a broad (3/2{++}) GDR component near E{-x}=22.5 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Modes: |g, p, {+3}He 
E$From E{-x}=23.2 MeV (1976Be28) {+12}C(p,|g), 23.25 MeV (1987Ba34) {+10}B({+3}He,{+3}He) and 23.3 MeV (1966Pa10) {+10}B({+3}He,p{-0}). In the prior evaluation the (p,|g) resonance was listed separately with E{-x}=23 MeV. 
J$From L=1 and R-matrix analysis in (1987Ba34) {+10}B({+3}He,{+3}He) 
WIDTH$From |G=500 keV (1987Ba34) {+10}B({+3}He,{+3}He) and |G=500 keV (1966Pa10) {+10}B({+3}He,p{-0}). See also |G|?1 MeV (1976Be28) {+12}C(p,|g). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, {+3}He 
E$From (1964Ku09) {+10}B({+3}He,p) 
J$From L=1 and R-matrix analysis in (1987Ba34) {+10}B({+3}He,{+3}He) 
WIDTH$From (1956Sc01) {+10}B({+3}He,p) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 13/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Mode: {+3}He 
E,WIDTH$From (1987Ba34) {+10}B({+3}He,{+3}He) 
J$From L=3 and R-matrix analysis in (1987Ba34) {+10}B({+3}He,{+3}He) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$Decay Modes: (p), n, {+3}He, |a 
E,WIDTH$From (1966Lo16) {+12}C(p,p):res. In the previous evaluation, |G=700 keV from (1987Ba34) was listed, but this resonance was not covered in the energy range of that study; inclusion of the resonance did improve the fit in that study, but the value is not accepted here. Other reported widths are |G=750 keV (1970Gi04) {+10}B({+3}He,|a), |<500 keV (1966Lo16) {+12}C(p,p):res. 
J$From Legendre polynomial analysis of {+10}B({+3}He,|a) in (1987Ba34) and scattered proton polarization results from {+12}C(p,p) (1966Lo16). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$Decay Modes: |g, p, {+3}He 
E$From (2004Fu12) {+13}C({+3}He,t). See also E{-x}=24.5 MeV (1963Fi07,1991Co07) {+12}C(p,|g). 
WIDTH$From (2004Fu12) {+13}C({+3}He,t). See also |G=3.5 MeV (1991Co07). 


level_energy_unit: KEV
level_spin_parity: (3/2)-
level_lifetime_unit: KEV
level_comment:
$Decay Modes: p, {+3}He 
E,WIDTH$From (1964Ku09) 
J$From (1967Sc11) where L=1 waves in the entrance and exit channels are found in {+12}C(p,p'){+12}C(15.11 MeV: 1{++}), 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$Decay Modes: |g, p, (n), d, {+3}He, |a 
E,WIDTH$From discussion in (1972Be56) finding {+10}|B({+3}He,X) where X=|a{-0}, d{-0}, p{-0,2,3} |g{-0} and (n). 
J$7/2- is found by (1970Gi04), where both Legendre polynomial analysis of {+10}B({+3}He,|a) and analyzing power data in {+12}C(pol. p,p) are discussed. However, the level is found to |g decay to {+13}C{-g.s.} so this is unlikely. See also J|<3/2 (1966Pa10) {+10}B({+3}He,p) and see discussion in (1972Be56). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$Decay Modes: p, (n) 
E,WIDTH$From (2004Fu12) {+13}C({+3}He,t). See also E{-x}=26.87 MeV (1964Ta15) analysis of (1963Di16) and 26.84 (1966Cr04) in {+12}C(p,p):res 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$Decay Modes: (|g), p, {+3}He, (|a) 
E$From discussion in (1972Be56) finding {+10}|B({+3}He,X) where X=|a{-0}, p{-0} and |g{-0}, and (1966Pa10) {+10}B({+3}He,p). 
J$9/2+ is found by (1970Gi04), where both Legendre polynomial analysis of {+10}B({+3}He,|a) and analyzing power data in {+12}C(pol. p,p) are discussed. However, the level is found to |g decay to {+13}C{-g.s.} so this is unlikely. See also J|<7/2 (1966Pa10) {+10}B({+3}He,p) and see discussion in (1972Be56). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
$Decay Modes: |g, p 
E$From the average of E{-x}=31.4 MeV (1976Fe11) {+12}C(p,p'|g(4.44)) and 31.9 MeV from the average of (1963Fi07, 1976Fe11, 1991Co07) values in {+12}C(p,|g). In earlier evaluations this level is listed with E{-x}=31 MeV. The level appears distinct from the E{-x}=32 MeV level, since it is not populated in {+10}B({+3}He,p) reactions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$Decay Modes: |g, d, {+3}He, |a 
E,WIDTH$From discussion in (1972Be56) finding {+10}|B({+3}He,X) where X=|a{-0}, d{-4,5} and |g{-0}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$The authors suggest this level may not be strongly populated in this reaction since its {+13}C{+*}(8.86) analog is weakly populated in ({+6}Li,{+3}He). This level cannot be resolved from {+13}N{+*}(9.00) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
J$From Adopted Levels 
T$T{-1/2} from (1980An40). 
$(1953Ch34): T{-1/2}=602.9 s {I19} 
$(1957De22): T{-1/2}=10.02 min {I10} 
$(1958Ar15): T{-1/2}= 597.6 s {I18} 
$(1980An40): T{-1/2}=598.02 s {I61} from |t{-m}=862.76 s {I88} 
$(1974Ro29): C{+2}S=0.49 {I15} L=1 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E$E{-p}=459.7 keV {I9} from the average (external errors) of E{-res}=456.0 keV {I20} (1949Fo18), E{-p}=456.8 keV {I5} (1953Hu18) E{-res}=457 keV {I1} (1974Ro29), E{-c.m.}=426.1 keV {I4} (E{-p}=461.9 {I4}) (2023Sk02) E{-p}=460.3 keV {I5} (2023Cs01) and E{-p}=459.8 keV {I8} (2023Ke11: includes global analysis of data). 
T$From weighted average (external errors) of |G{-lab}=37.4 keV {I10} (1953Hu18, 1973Cl04), |G{-c.m.}=33.7 keV {I20} (1968Bl17), |G{-lab}=34 keV {I1} (1968Ri16), |G{-c.m.}=33.3 keV {I18} (1974Bl06), |G{-(lab)}=39 keV {I2} (1974Ro29), |G{-c.m.}=34.9 keV {I2} (2023Sk02), |G{-lab}=38.2 keV {I5} (2023Cs01) and |G{-c.m.}=34.0 keV {I2} (2023Ke11: includes 2008Bu19). See also |G{-p}=33.5 keV {I10} obtained from a global analysis in (2022Ar03). Note: some inconsistencies exist in the literature related to assigning the values as lab or c.m. frame values. Table 1 of (1992Hi14) is helpful for resolving some issues. 
WIDTHG0$Weighted average (external errors) of |G{-|g}=0.45 eV {I5} (1968Ri16-c.m. value), |G{-|g}=0.53 eV {I5} (1992Hi14-c.m. value), |G{-|g}=0.49 eV {I3} (2023Sk02-c.m. value); |G{-|g}=0.48 ev {I2} (2023Ke11-c.m. value: includes 2008Bu19); see also |G{-|g0}=0.63 eV (1949Fo18-lab value). As with |G, there are some inconsistencies with determining the reference frame of the widths. 
J$From R-matrix analysis in (2023Ke11) 
$C{+2}S=1.02 {I15} (1974Ro29) 
$(1949Fo18): E{res}=456.0 keV {I20}, |G=35 keV and |w|g=0.63 eV 
$(1951Se67,1952Se01): E{-p}=0.45 MeV, |G{-lab}=35 keV and |w|g=0.67 eV (implies |G{-|g0}=0.67 eV) 
$(1953Hu18): E{-p}=456.8 keV {I5} and |G{-lab}=39.5 keV {I10} (analysis in (1973Cl04) deduced |G{-lab}=37.4 keV {I13} after correcting for target thickness effects). 
$(1968Bl17): E{-p}=459 keV and |G{-c.m.}=33.7 keV {I20} (Uncertainty given in (1970Aj04) from (1968Bl18), see also (1973Cl04) where |g uncertainty of 2 keV is given). 
$(1968Ri16): |G{-lab}=34 keV {I1}, |t=1.47 fs {I15} and |G{-|g}=0.45 eV {I5}. A private communication in (1973Cl04) establishes this |G is a lab value. 
$(1974Bl06): |G{-c.m.}=33.3 keV {I18} (assumed lab in (1976Aj04)). (see for discussion on |G variation in prior measurements) 
$(1974Ro29): E{-res}=457 keV {I1}, |G{-(lab)}=39 keV {I2}, L=0, C{+2}S=1.02 {I15}, |q{+2}(l=0)|?0.81 A lab report (1975FoZD) indicates |G{-|g0}=0.64 eV {I7}. 
$(1992Hi14): E{-p}|?424, |G{-c.m.}|?36.4 and |G{-|g}=0.53 eV {I5}. 
$(2008Bu19): |G{-p}=35.0 keV {I10} and |G{-|g}=0.65 eV {I7} (assumed c.m.) 
$(2023Sk02): E{-c.m.}=426.1 keV {I4}, |G{-c.m.}=34.9 keV {I2} and |G{-|g}=0.49 eV {I3}. 
$(2023Cs01): E{-p}=459.8 keV {I8} and |G{-lab}=38.2 keV {I5}. 
$(2023Ke11): E{-p}=460.3 keV {I5}, |G{-p}=34.0 keV {I2} and |G{-|g}=0.48 eV {I3}. 
$See additional discussion in (2017Mu06) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$From E{-p}=1687.8 keV {I8} the weighted average of E{-p}=1687 keV {I1} (1991Po18), E{-p}=1688.7 keV {I7} (1989Ki21: thick target), E{-p}=1689 keV {I2} (1989Ki21: thin target), E{-p}=1685.1 keV {I7} (2023Cs01) and E{-p}=1688.8 keV {I5} (2023Ke11). 
WIDTH$From |G{-c.m.}=61.9 keV {I40} (1968Bl17), |G{-lab}=65 keV {I3} (1974Ro29), |G{-lab}=57.6 keV {I8} (2023Cs01) and |G{-c.m.}=55.2 keV {I3} (2023Ke11). See also |G=65.6 keV {I18} (1989Ki21: thick target - taken as lab), see also |G=74 keV {I9} (1949Va03), |G{-lab}=70 keV {I10} (1951Se67,1952Se01) and |G=62.2 keV {I15} (1991Po18-reference frame is unclear) 
J$From phase-shift analysis in (1974Ro29) 
WIDTHG0$From the R-matrix analysis in (2023Ke11) as detailed above. In (1991Aj01) the analysis of (1952Se01, 1963Yo06) cross sections given in (1980Ba54) was accepted; see discussion in (1991Aj01). See also |G{-|g0}=0.70 eV from |w|g=1.39 eV (1951Se67,1952Se01) as quoted in (1954Wo09), and see |w|g=1.06 and |G{-|g}=0.53 eV in (1963Yo06). 
WIDTHG1$From |G{-|g0} and I|g1=8% {I1} from (1974Ro29). 
$1949Va03: E{-res}=1697 keV {I12}, |G=74 keV {I9}, ratio of yield from E{-res}=1697 keV {I12} and E{-res}=456 keV is R=1.3 {I2}, which is used to deduce |G|g=1.3 eV {I2} (this may be a typo). 
$(1951Se67,1952Se01): E{-p}=1.698 MeV {I5} and |G{-lab}=70 keV {I10} and |w|g=1.39 eV (implies |G{-|g0}=0.70 eV) 
$(1954Wo09): |G{-|g1}=0.04 eV 
$(1963Yo06): |s=37 |mb, |w|g=1.06 eV, |G{-|g}=0.53 eV (no participation of {+13}N{+*}(3.56: 5/2+); |s|<0.16 |mb ; |w|g<0.006 eV); |d(M2/E1)=-0.092 from A{-2}/A{-0}=-0.65 
$(1968Bl17): E{-p}=1697 keV and |G{-c.m.}=61.9 keV {I40} (Uncertainty given in (1970Aj04) from (1968Bl18)) 
$(1974Ro29): E{-res}=1699 keV {I2}, |G{-lab}=65 keV {I3}, L=1, C{+2}S<0.5 and |d{-R}(M2/E1)=-0.09 {I2} from {Ia2}=-0.64 {I4} 
$(1989Ki21: thick target): E{-p}=1688.7 keV {I7} and |G=65.6 keV {I18} 
$(1989Ki21: thin target):E{-p}=1689 keV {I2}; in this work the energy shift is attributed to the thick target measurement methodology. 
$(1991Po18: see important discussion): E{-p}=1687 keV {I1}. |G{-lab}=63.6 keV {I16} and |G{-lab}=62.2 keV {I15} were deduced from separate configurations. 
$(2008Bu19): |G{-p}=62 keV (2008Bu19) (assumed c.m.). 
$(2023Cs01): E{-p}=1685.1 keV {I7} and |G{-lab}=57.6 keV {I8}. 
$(2023Ke11): E{-p}=1688.8 keV {I5}, |G{-c.m.}=55.2 keV {I3}, |G{-|g}(M1)=0.49 eV {I3} and |G{-|g}(E2)=7.2|*10{+-4} eV {I11}. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_lifetime_unit: MEV
level_comment:
E$E{-res}=9.01 MeV {I15} from E{-res}=9.01 MeV {I15} (1972Ha32,1973Me12) and E{-p}=9.01 MeV {I15} (1976Be28). 
T$From |G{-lab}=0.28 MeV {I10} (1972Ha32,1973Me12) 
WIDTHG0$From (1973Me12); see other discussion in (2008Bu19). 
$(1972Ha32,1973Me12): E{-res}=9.01 MeV {I15}, |G{-lab}=0.28 MeV {I10}, detector |q=90|' gives |p=+, J|p=(1/2+,3/2+) and |G{-p0}|G{-|g0}=0.17 keV{+2} {I9} 
$(1973Me12): |G{-|g0}|>0.6 eV 
$(1976Be28): E{-p}=9.01 MeV {I15} and |G|?300 keV 
$(2008Bu19): E{-c.m.}=8.371 MeV accounting for the tail of this resonance in the E{-p}|<2 MeV region suggests |G{-|g}=6 keV (assumed lab). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,T$From (1972Ha32,1973Me12) 
WIDTHG0$From (1973Me12) 
$(1972Ha32,1973Me12): E{-res}=10.62 MeV {I12}, |G{-lab}=220 keV {I50}, J|p=3/2{++} and |G{-p0}|G{-|g0}=0.28 keV{+2} {I10}. 
$(1973Me12): |G{-|g0}|?4.2 eV 
$(1976Be28): See discussion on J|p assignments of {+13}N{+*}(11.74, 14.05) and other nearby levels. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,T$From (1973Me12) 
J$From (1973Me12) {+12}C(p,|g{-0}); L=0,2, strong interference with J|p=3/2{++} states at {+13}N{+*}(11.74, 14.04), assumed component of GDR. 
WIDTHG0$From (1973Me12) 
$(1973Me12): E{-p}=12.5 MeV {I2}, |G=7 MeV, |G{-|g0}|> 1.1 keV. 
$(1963Fi07): E{-x}=13 MeV 
$(1991Co07): E{-x}=14.0 MeV, |G=12 MeV {+12}C(p,|g{-0}) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,T$From (1972Ha32,1973Me12) 
WIDTHG0$From (1973Me12) 
$(1972Ha32,1973Me12): E{-res}=13.12 MeV {I9}, |G{-lab}=170 keV {I20} J|p=3/2{++} and |G{-p0}|G{-|g0}=0.47 keV{+2} {I12} 
$(1973Me12): |G{-|g0}=3.7 eV {I10}; associated with the J|p=3/2{++} state from (1969Le18) (p,p) phase-shift analysis. 
$(1976Be28): See discussion on J|p assignments of {+13}N{+*}(11.74, 14.05) and other nearby levels. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$(1968Di04): |G{-p}|G|g/|G=5.5 eV {I8}, J|p=3/2- from |g(|q), T=3/2 I(E2/M1)=-0.095 {I7}, |G{-|g1}/|G{-|g0}<0.14, (|G{-|g2}+|G{-|g3})/|G{-|g0}=0.84 {I8} 
$(1975Ma21,1977Ma16) |G{-p}|G|g/|G=5.79 eV {I20}, I(E2/M1)=0.013 {I5}. Using |G{-p0}/|G=0.236 {I12} from (1973Ad02) they deduced |G{-|g0}(M1)=24.2 eV {I15}, |G{-|g0}(E2)=0.32 eV {I12}, B(M1)W=0.342 {I21} and B(E2)W=0.28 {I11} for the ground state transition. They also measured {+11}B({+3}He,n|g) and determined relative transition strengths for |g{-0}, |g{-1} and |g{-2}. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MEV
level_comment:
E,J,T$From (1972Ha32,1973Me12) 
WIDTHG0$From (1973Me12) 
$(1972Ha32,1973Me12): E{-res}=14.5 MeV {I2}, |G{-lab}=0.38 MeV {I15}, |G{-p0}|G{-|g0}=0.21 keV{+2} {I8}. Possible doublet. 
$(1973Me12): |G{-|g0}|>0.5 eV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
E$From average of measured values listed below. 
E$In (1981Aj01) an additional level at E{-p}|?20 MeV was deduced based a peak seen in Figure 11 of (1976Be28). However, those authors indicated, "at lower energies the |g{-2+3} pulses are completely submerged in the sea of inelastic |g rays"; therefore there seems to be evidence for only one level in this region. 
$(1963Fi07): E{-x}=20 MeV {+12}C(p,|g{-0}) 
$(1976Fe11): E{-p}=20 MeV {+12}C(p,|g{-0,2+3}) 
$(1976Be28): E{-x}|?20.8 MeV and |G|?4 MeV. 
$(1988Ha04): E{-x}|?20.40 MeV and |G|?3.5 MeV (GDR). 
$(1991Co07): E{-x}=20.6 MeV with |G=1.2 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: MeV
level_lifetime_info: ;ERR=?
level_comment:
E$From (1963Fi07, 1991Co07) 
T$From (1991Co07) 
$(1963Fi07): E{-x}=24.5 MeV (|g{-2}) and uncertain E{-x}=24 MeV (|g{-0}) 
$(1991Co07): E{-x}=24.5 MeV with |G=3.5 MeV {+12}C(p,|g{-2+3}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
T |G=broad 
E$From average (1963Fi07, 1976Fe11). 
$(1963Fi07): E{-x}=32.5 MeV {+12}C(p,|g{-0}) 
$(1976Fe11): E{-p}=32 MeV {+12}C(p,|g{-0,2+3}) 
$(1991Co07): E{-x}=32.0 MeV, |G=10 MeV {+12}C(p,|g{-0}) and E{-x}=35.0 MeV, |G=14 MeV {+12}C(p,|g{-2+3}) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)-
level_comment:
E$Reported as 10.833 MeV in (1981Pe08) 
J$(1981Pe08) indicate L=2, which implies (3/2,5/2)-, but this disagrees with the J|p=1/2- from their {+12}C({+3}He,d) result in (1980Pe13). 
$%p{-0}=5 {I1}, %p{-1}=54 {I9}, %p{-2}=43 {I16} (2004Fu12) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$%p{-0}=16 {I2}, %p{-1}=13 {I2}, %p{-2}=3 {I1} (2004Fu12) 
E$(2004Fu12) report this state has a considerable amount of the isospin violation component in the wave function, surpassing the weak |g-ray decay rates, as the 15060, T=3/2 state in {+13}N decays to the forbidden T=0 states in {+12}C. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
E$Observed in (1966Ba44: E{-x}=3.6 MeV {I1} likely unresolved states) 
S$See also S=0.21 (1975Ro27) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
E$Observed in (1966Ba44: E{-x}=11.9 MeV {I2}, likely unresolved states) 
S$See also S=1.29 (1975Ro27) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$This state is not associated with any Adopted Level because inadequate detail for association is given in the literature. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
T$See 104 keV {I20} in (2005Kn02) 
$%I|b-p0=0.009 {I4} and %I|b-p1=0.235 {I29}; this implies %p{-0}=3.6 and %p{-1}=96.4 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
T$From (2005Kn02) 
$%I|b-p0=0.519 {I40} and %I|b-p1=0.441 {I29}; this implies %p{-0}=54.1 and %p{-1}=45.9 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
T$See 143 keV {I18} in (2005Kn02) 
$%I|b-p0=0.137 {I12} and %I|b-p1=0.104 {I11}; this implies %p{-0}=56.9 and %p{-1}=43.1 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
T$Deduced in (2024Bi01); if this state is observed in (2005Kn02) (2024Bi01) suggest |G<40 keV. 
$Suggested to decay via |a{-0}+{+9}B{-g.s.}, p+{+12}C{-g.s.} and p+{+12}C(7654.7 MeV). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
WIDTH$See 315 keV {I112} (2005Kn02). 
J$In (2024Bi01), decay to p+{+12}C(7654.7 MeV) is reported for a state in this energy region; they suggest the J|p=3/2- state near E{-x}=11.8 MeV was involved. 
$I|b-p0=0.015 {I4} and %p{-1}|<0.002; this implies %p{-0}=100. A small branch via p{-2} decay is reported in (2024Bi01). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=GT
level_comment:
E$See 13.26 MeV {I10} deduced from E{-p} in (2005Kn02) 
WIDTH$See 521 keV {I210} (2005Kn02). 
J$See (-) in (2005Kn02). 
$%I|b-p0=0.011 {I3}; this implies %p{-0}=100 


level_energy_unit: KEV
level_spin_parity: [1/2-,5/2-]
level_comment:
J$1/2{+-} for |a{-4} decay through {+9}B(2.78:1/2{+-}) is preferred. 
$Suggested to decay via |a{-1}+{+9}B(1.8 MeV), |a{-0}+{+9}B(2.75 MeV) or |a{-0}+{+9}B(2.78 MeV) and p+{+12}C{-g.s.}. 


level_energy_unit: KEV
level_spin_parity: [3/2-]
level_comment:
$Suggested to decay via |a{-0}+{+9}B{-g.s.}, |a{-1}+{+9}B(1.8 MeV), |a{-0}+{+9}B(2.75 MeV) and p+{+12}C(7654.7 MeV). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$%I|b-p0=0.0048 {I7}, %I|b-p1=0.0029 {I5} and %I|b-p2=0.0011 {I2}; when |g and |a decay are considered, this implies %|g=4.9%, %|a=53.4, %p{-0}=22.8, %p{-1}=14.0 and %p{-2}=4.9 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MEV
level_comment:
E$deduced from E{-p} 
J$If populated in this (2005Kn02), the transition is allowed and |p=-; however the evaluator expresses reservations upon consideration of the background near where perhaps three or four counts attributed to this broad state are identified. The evaluator discounts the merit of any J|p constraints based on the suggestion this is an allowed transition. 
$%I|b-p0=0.004 {I3} and %p{-1}|<0.0004; this implies %p{-0}=100. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$C{+2}S(phenomenological)=1.14 {I16}(exp.) {I15}(analysis), also see C{+2}S(microscopic)=1.58 {I22}(exp.) {I2}(analysis). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$C{+2}S(phenomenological)=0.94 {I19}(exp.) {I7}(analysis), also see C{+2}S(microscopic)=1.00 {I20}(exp.) {I1}(analysis). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
S,T$From (1964Ku09): ({+3}He,p) resonance to {+12}C(15.1 MeV) 
$(1966Ba01) suggest no evidence of a GDR at E{-x}|? 26 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: GE3/2
level_comment:
S$From (1966Pa10): ({+3}He,p) resonance to {+12}C(0,4.44,9.6 MeV). See also (1972Be56) where E{-{+3}He}(res)=5.6 is reported for p{-0,2,3}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: GE7/2
level_comment:
S$From (1966Pa10): ({+3}He,p{-0}) resonance. See also (1972Be56) where E{-{+3}He}(res)=5.5 is reported for p{-0}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
WIDTH$Broad 
S$From (1972Be56) for d{-0}. See also (1965Pa10) where E{-{+3}He}(res)=5.8 is reported. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2,7/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
WIDTH$|G{-3He}=0.35 MeV (1987Ba34) 
E$The upper energy covered in (1987Ba34) was E({+3}He)=3.3 MeV. The authors found an improved fit by including this resonance. Fit values should be considered tentative. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: MEV
level_comment:
S$From (1965Pa05, 1970Gi04). 
J,T$From R-matrix analysis in (1970Gi04). |G from 1.2-1.5 MeV. 
WIDTH$Broad (1965Pa05). See also (1972Be56) where E{-{+3}He}(res)=5.6 is reported for |a{-0}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: MEV
level_comment:
S,J,T$From R-matrix analysis in (1970Gi04). |G from 2.0-2.5 MeV. See also (1972Be56) where E{-{+3}He}(res)=8.5 is reported for |a{-0}. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,T,J,L$ and T from (1969Ad02) 
$(1968Co27): |G{-|g0}/|G{-p0}=0.12 {I2}. 
$(1969Ad02): |G<15 keV; |G{-p0}/|G=0.202 {I20} and |G{-p1}/|G=0.121 {I15} from (1969Ad01). 
$(1973Ad02) Measured Branching ratios to {+12}C and {+9}B states. Assuming |G=0.82 keV {I20} from (1973Ad02,1968Co27,1968Di04), {+12}C(0)=23.6% {I12} and |G{-p0}=0.19 keV {I5}, {+12}C(4.44)=15.0% {I10} and |G{-p1}=0.12 keV {I3}, {+12}C(7.65)=5.3% {I15} and |G{-p2}=0.043 keV {I16}, {+9}B(0)=4.9% {I27} and |G{-|a0}=0.040 keV {I24}, {+9}B(1.6)=3.9% {I39} and |G{-|a1}=0.032 keV {I32}, {+9}B(2.36)=7.2% {I45} and |G{-|a2}=0.059 keV {I40}, |G{-|g0}=23.3 eV {I36}. 
$(1975Ma21):|G{-p}|G{-|g0}/|G=5.79 eV {I20} and 0.013 {I5} for the E2/M1 intensity ratio from {+12}C(p,|g). In (1975Ma21) |G{-|g0}=24.5 eV {I15} and reduced M1 and E2 transition strengths are deduced after making several assumptions. Using relative intensities measured via {+11}B({+3}He,n|g) and with |q{-|g}=125|' and |q{-n}=0|', they obtained |G|g0(M1)=24.2 eV {I15}, |G|g0(E2)=0.32 eV {I12}, |G|g1(E1)|<2.18 eV {I30} and |G|g2(M1)=19.6 eV {I14}. 
$(1977Ma16): |G{-|g0}/|G{-p0}=0.121 {I11}. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$From E{-res}=461 keV {I3} (1953Ja04) 
$|q{+2}=0.54 (1953Ja04 |* 0.66 ) 
$(1951Ja21): E{-x}=2379 keV, |G=33 keV 
$(1953Ja04): E{-res}=461 keV {I3}, J|p=1/2+ and |G=31 keV from phase-shift analysis 
$(1954Mi05): E{-res}=462 keV {I4} and |G{-c.m.}=32 keV. 
$(1976Me22): E{-c.m.}=424 keV with |G{-c.m.}=33 keV (1976Me22) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|q{+2}=0.031 (1953Ja04 value |* 0.66 ) 
E,J,T$From E{-p}=1686 keV {I6} (1966Ar03) 
$(1951Ja21): E{-x}=3501 keV, |G=42 keV. 
$(1953Ja04) E{-res}=1698 keV, J|p=3/2- and |G=55 keV. 
$(1966Ar03): E{-p}=1686 keV {I6}, J|p=3/2- and |G=63 keV. They also report |DE(3/2-,5/2+)=48 keV {I2} and reduced width values. 
$(1976Me22): E{-c.m.}=1558 keV with |G{-c.m.}=55 keV. 
$(1992Ba30): E{-res}=1685 keV {I6} J=3/2- from phase-shift analysis. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E$E{-res}=1735.5 keV {I5} from the average of E{-p}=1734 keV {I6} (1966Ar03), E{-p}=1736 keV {I8} (1992Ba30) and E{-p}=1735.5 keV {I5} from the (2023Ke11) analysis of (1976Me22). 
J,T$From the (2023Ke11) R-matrix analysis of (1976Me22). 
$|q{+2}=0.21 (1953Ja04 value |* 0.66 ) 
$(1951Ja21): E{-x}=3549 keV, |G=40 keV (1951Ja21) 
$(1953Ja04) E{-res}=1748 keV, J|p=5/2+ and |G=61 keV, 
$(1966Ar03): E{-p}=1734 keV {I6}, J|p=5/2+ and |G=74 keV. They also report |DE(3/2-,5/2+)=48 keV {I2} and reduced width values. 
$(1976Me22): E{-c.m.}=1604 keV with |G{-c.m.}=50 keV. A subsequent reanalysis in (2023Ke11) resulted in E{-p}=1735.5 keV {I5} with J|p=5/2+, and |G=49.0 keV {I5}. 
$(1992Ba30): E{-res}=1736 keV {I8} J=5/2+ from phase-shift analysis. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$From E{-res}=4808 keV {I8} (1956Re39). 
$|q{+2}=0.0031 (1956Re39) 
$(1956Re39): E{-res}=4808 keV {I8}, J|p=5/2+, |G{-lab}=12 keV and |q{+2}=0.0031 from phase-shift analysis 
$(1966Ba35): E{-res}=4.80 MeV, J|p=5/2+ and |G{-lab}=12 keV. See also (1967Ba84) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$|q{+2}=0.13 (1963Ba36) 
E$From E{-res}=5363 keV {I6} from the average of E{-res}=5370 keV {I8} (1956Re39), E{-res}=5.35 MeV {I1} (1963Ba36) and E{-p}=5374 keV {I20} (1967Du12). 
J$From phase-shift analysis of angular distributions and |s(E) in (1956Re39) {+12}C(p,p),(p,p{-1}|g(|q)). See also (1965Be12). 
T$From (1963Ni05) 
WIDTHP0$See also |G{-p0}=46 keV (1963Ni05). 
$(1956Re39): E{-res}=5370 keV {I8}, J|p=3/2+ and |G{-lab}=125 keV. 
$(1956Sc29): E{-res}=5.30 keV, L:J|p=2:3/2+, |G=50 keV. 
$See unpublished results in (1959Aj76). 
$(1960Yo05): E{-res}=5.37 MeV. 
$(1961Ad04): E{-res}=5.63 MeV and |G{-lab}=140 keV. 
$(1962Sh22): E{-res}=5.38 MeV, J|p=3/2+, |G=115 keV and |q{+2}=0.01 from phase-shift analysis 
$(1961Ba25, 1961Mc11): E{-res}=5.4 MeV 
$(1963Ba36): E{-res}=5.35 MeV {I1}, J|p=3/2+, |G{-c.m.}=114 keV |G{-p0}=51 keV, |G{-p1}=63 keV. 
$(1963Ni05): E{-p}=5.38 MeV, J|p=3/2+, |G{-c.m.}=115 keV {I5} and |G{-p0}=46 keV (1963Ni05). 
$(1966Ba35): E{-res}=5.30 MeV, J|p=3/2+ and |G{-lab}=74 keV. 
$(1967Du12): E{-p}=5374 keV {I20} 
$(1968Be31): E{-res}=5.38 MeV, J|p=3/2+ 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
E,J$From E{-res}=5.65 MeV {I1} (1963Ba36). 
T,WIDTHP1$From (1963Ni05). 
$|q{+2}=0.016 (1963Ba36) 
$(1960Yo05): E{-res}=5.69 MeV (1960Yo05) 
$(1963Ba36): E{-res}=5.65 MeV {I1}, J|p=7/2+, |G{-c.m.}=7.7 keV |G{-p0}=0.03 keV, |G{-p1}=7.4 keV. |G{-p0}=0.03 keV may be a typo since the value |G{-p0}=0.3 keV gives the better accounting. Phase-shift and interference analysis. 
$(1963Ni05) E{-p}=5.68 MeV, J|p=(7/2+), |G{-c.m.}=9.0 keV {I5} and |G{-p0}=0.36 keV. Phase-shift analysis. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
E$From (1963Ba36). 
J$From polarization data in (1968Be31). See discussion in (1966Sh10). 
T,WIDTHP0$From (1963Ni05). See also |G{-c.m.}=61 keV, |G{-p0}=5.0 keV, |G{-p1}=56 keV (1963Ba36) and |G{-lab}=70 keV and |G{-p0}/|G=0.08 (1968Be31). 
$|q{+2}=0.069 (1963Ba36) 
$(1956Br27) E{-res}=5891 keV, |G{-lab}= 55 keV 
$(1956Sc29): E{-res}=5.85 keV, L:J|p=1:3/2-, |G=50 keV 
$See unpublished results in (1959Aj76) 
$(1960Yo05): E{-res}=5.93 MeV 
$(1961Ad04): E{-res}=5.89 MeV, |G{-lab}=70 keV 
$(1961Ba25,1961Mc11): E{-res}=5.9 MeV 
$(1962Sh22): E{-res}=5.90 MeV, J|p=5/2+, |G=80 keV and |q{+2}=0.01 from phase-shift analysis 
$(1963Ba36): E{-res}=5.89 MeV {I1}, J|p=(5/2-,7/2-), |G{-c.m.}=61 keV, |G{-p0}=5.0 keV, |G{-p1}=56 keV 
$(1963Ni05): E{-p}=5.90 MeV, J|p=5/2-, |G{-c.m.}=69 keV {I5} and |G{-p0}=6.9 keV. (note:|G{-lab}=75 keV {I5} is listed in the abstract as |G{-c.m.}. The issue is clear in the conclusions paragraph). 
$(1966Ba35): E{-res}=5.88 MeV, J|p=5/2- and |G{-lab}=70 keV. 
$(1968Be31): E{-res}=5.88 MeV, J|p=5/2-, |G{-lab}=70 keV and |G{-p0}/|G=0.08 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E{-res}|?6530 from average of E{-res}=6.65, 6.6, 6.35 MeV 
J$From (1962Sh22,1966Ba35) 
T$From average of |G=1400 keV (1962Sh22) and |G{-lab}=1.72 MeV (1966Ba35). See also |G=350 keV (1956Sc29) 
$|q{+2}=0.14 (1962Sh22) 
$(1956Sc29): E{-res}=6.65 keV, L:J|p=2:3/2+, |G=350 keV. 
$(1961Ba25, 1961Mc11): E{-res}=6.65 MeV 
$(1961Na02): E{-res}=(6.65) MeV 
$(1962Sh22): E{-res}=6.6 MeV, J|p=3/2+, |G=1400 keV and |q{+2}=0.14 from phase-shift analysis 
$(1966Ba35): E{-res}=6.35 MeV, J|p=3/2+ and |G{-lab}=1.72 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,T$From E{-res}|?7540 keV, |G from |G{-lab}|?250 keV 
$|q{+2}=0.02 (1962Sh22) 
$(1961Ad04): E{-res}=7.55 MeV, |G{-lab}=255 keV 
$(1961Ba25, 1961Mc11, 1961Mc16): E{-res}=7.6 MeV 
$(1962Sh22): E{-res}=7.53 MeV, J|p=1/2-, |G=225 keV and |q{+2}=0.02 from phase-shift analysis 
$(1966Ba35): E{-res}=7.53 MeV, J|p=1/2- and |G{-lab}=250 keV 
$(1973Be37): E{-res.}=7575 keV and |G=0.25 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$From E{-res}=8170 keV. 
$|q{+2}=0.001 (1962Sh22) 
$|G{-p1}/|G=0.72 (1972Be15) 
$(1961Ad04): E{-res}=8.17 MeV, |G{-lab}=38 keV 
$(1961Ba25, 1961Mc11, 1961Mc16): E{-res}=8.2 MeV 
$(1962Sh22): E{-res}=8.17 MeV, J|p=3/2-, |G=30 keV and |q{+2}=0.001 from phase-shift analysis 
$(1966Ba35): E{-res}=8.16 MeV, J|p=3/2- and |G{-lab}=30 keV 
$(1972Be15): E{-res}=8.18, |G{-lab}|?28 keV and |G{-p1}/|G=0.72 


level_energy_unit: KEV
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level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|G{-p0}/|G=0.26 (1968Be31) 
E,J,T$From E{-res}|?9130 keV (1968Be31) 
E$In (1966Sw04) a doublet was identified around E{-res}=9.12 MeV. Previously, only the J|p=7/2- state had been identified. Later, (1967Sw02) identified the doublet members at E{-p}= 9145 and 9152 keV via phase-shift analysis with J|p=5/2- and 7/2- and with |G{-lab}=12 and 90 keV, respectively. 
E$In (1968Be31) E{-res}=9.13 MeV, J|p=5/2- from polarization data , |G{-lab}=33 keV and |G{-p0}/|G=0.26. The level energies of the doublet states differ by less than 2 keV. 
$(1961Ad04): E{-res}=9.12 MeV, |G{-lab}=70 keV 
$(1961Ba25, 1961Mc11, 1961Mc16): E{-res}=9.2 MeV 
$(1961Na02): E{-res}=9.1 MeV, |G=150 keV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|G{-p0}/|G=0.81 (1968Be31) 
E,J,T$From E{-res}|?9130 keV (1968Be31) 
E$In (1966Sw04) a doublet was identified around E{-res}=9.12 MeV. Previously, only the J|p=7/2- state had been identified. Later, (1967Sw02) identified the doublet members at E{-p}=9145 and 9152 keV via phase-shift analysis with J|p=5/2- and 7/2- and with |G{-lab}=12 and 90 keV, respectively. 
E$In (1968Be31) E{-res}=9.13 MeV, J|p=7/2- from polarization data, |G{-lab}=82 keV and |G{-p0}/|G=0.81 
$(1961Ad04): E{-res}=9.12 MeV, |G{-lab}=70 keV 
$(1961Ba25, 1961Mc11, 1961Mc16): E{-res}=9.2 MeV 
$(1961Na02): E{-res}=9.1 MeV, |G=150 keV 
$(1962Sh22): E{-res}=9.14 MeV, J|p=7/2-, |G=73 keV and |q{+2}=0.01 from phase-shift analysis 
$(1966Ba35): E{-res}=9.13 MeV, J|p=7/2- and |G{-lab}=84 keV 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From E{-res}=10.35 MeV {I5} (1973Me03). In (1976Aj04) values from the E{-p}=9.5-11.5 MeV phase-shift analysis of (1973Me03) were accepted; we continue this acceptance and note that averaging with other values would have little impact. 
$(1961Mc16): E{-res}=10.3 MeV 
$(1961Na02): E{-res}=10.5 MeV, |G=700 keV 
$(1972Wi26): E{-res}=10.25 MeV {I10}, J|p=5/2+, |G=0.45 MeV {I10} and |G{-p0}/|G=0.65 {I15} 
$(1973Me03): E{-res}=10.35 MeV {I5}, J|p=5/2+, |G{-c.m.}=430 keV {I35} and |G{-p0}/|G=0.70 {I5}. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
E,J,T$E{-res}=10.58 MeV {I3} (1973Me03). The E{-p}=9.5-11.5 MeV phase-shift analysis of (1973Me03) is accepted. See comment on E{-x}=10.49 MeV. 
$(1961Ad04): E{-res}=10.51 MeV, |G{-lab}=85 keV 
$(1961Ba25, 1961Mc11, 1961Mc16): E{-res}=10.5 MeV 
$(1972Wi26): E{-res}=10.51 MeV {I2}, J|p=5/2-, |G=120 keV {I30} and |G{-p0}/|G=0.55 {I5} 
$(1973Me03): E{-res}=10.58 MeV {I3}, J|p=5/2-, |G{-c.m.}=115 keV {I30} and |G{-p0}/|G=0.60 {I4} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$E{-res}=10.62 MeV {I4}, J|p=3/2+, |G{-c.m.}=250 keV {I30} and |G{-p0}/|G=0.30 {I5} from the E{-p}=9.5-11.5 MeV phase-shift analysis of (1973Me03) are acccepted. See comment on E{-x}=10.49 MeV. 
$See also E{-res}=10.70 MeV {I5}, J|p=3/2+, |G=250 keV {I50} and |G{-p0}/|G=0.62 {I10} (1972Wi26) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E,J,T$E{-res}=10.62 MeV {I5}, J|p=3/2-, |G{-c.m.}=530 keV {I80} and |G{-p0}/|G=0.55 {I5} from the E{-p}=9.5-11.5 MeV phase-shift analysis of (1973Me03) are acccepted. See comment on E{-x}=10.49 MeV. 
$See also E{-res}=10.54 MeV {I50}, J|p=3/2-, |G=230 keV {I50} and |G{-p0}/|G=0.45 {I10} (1972Wi26) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$E{-res}=10.75 MeV {I4}, J|p=1/2+, |G{-c.m.}=380 keV {I50} and |G{-p0}/|G=0.35 {I5} from the E{-p}=9.5-11.5 MeV phase-shift analysis of (1973Me03) are acccepted. See comment on E{-x}=10.49 MeV. 
$See also E{-res}=10.74 MeV, |G{-lab}=140 keV (1961Ad04) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
E$From E{-res}=11.05 MeV {I5} (1973Me03). The E{-p}=9.5-11.5 MeV phase-shift analysis of (1973Me03) is acccepted. See comment on E{-x}=10.49 MeV. 
$(1961Ad04): E{-res}=10.99 MeV, |G{-lab}= 150 keV 
$(1961Mc16) E{-res}=11.0 MeV 
$(1973Me03): E{-res}=11.05 MeV {I5}, J|p=7/2-, |G{-c.m.}=250 keV {I30} and |G{-p0}/|G=0.30 {I5} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From E{-res}=13.13 MeV {I2}, J|p=3/2+, |G{-c.m.}=180 keV {I35} and |G{-p0}/|G=0.29 {I7} phase-shift analysis (1976Me18). The authors suggest a |<70 keV systematic error in (1969Le18). 
$See also E{-res}=13.2 MeV, |G=500 keV (1961Na02) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_uncertain: ?
level_comment:
E$See E{-res}=13.7 MeV, |G=500 keV (1961Na02) 
$This resonance does not appear in the (1981Aj01) evaluation or later. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E,ISPIN$From E{-p}=14230.75 keV {I20} and T=3/2 (1973Hu07) 
E$See also E{-p}=14232.5 keV {I22} (1975Go03); |G{-p}/|G=0.18 was used in the fit. 
T$From |G=1010 eV {I30} and |G{-p}=285 eV {I15} (both lab frame) (1980Th05). Atomic excitations were taken into account, See also (1983Wi04,1992Wi13). 
T$See also |G{-c.m.}=1.10 keV {I9}, |G{-p}=210 eV {I11} and |G{-p}/|G=0.191 {I17} (1975Hi07). 
J$From phase-shift analysis in (1969Le18). 
$p decay to {+12}C(0,4.4, 7.65, 9.65) is observed in (1977Ma16) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
E$From average of E{-res}=15.27 MeV {I3} (1973Me12) and E{-res}=15.24 MeV {I4} (1976Me18) 
J$From phase-shift analysis in (1969Le18). 
T$From (1973Me12). See also (1976Me18). 
E$A second state near E{-x}=16 MeV with |G|?500 keV had previously been adopted, apparently based on (1964Da03) and (1961Na02); however this seems unwarranted. In (1964Da03) the authors indicate improved data are necessary, and in (1961Na02,1967Ku02,1976Be28) the associated peaks are rather narrow. 
$(1973Me12): E{-res}=15.27 MeV {I3}, |G{-c.m.}=130 keV {I30} and |G{-p}(12.71)=30 keV. 
$(1976Me18): E{-res}=15.24 MeV {I4}, J|p=7/2+, |G{-c.m.}=135 keV {I90} and |G{-p0}/|G=0.05 {I4} 
$(1961Na02): E{-res}=15.1 MeV (1961Na02) 
$(1967Ku02): E{-p}=15.2 MeV and T=(1/2) (1967Ku02) 
$(1976Be28) E{-p}=15.27 MeV (1976Be28). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From E{-res}=17.58 MeV {I3} phase-shift analysis in (1976Me18). 
$(1962Wa31): E{-p}=17.5 MeV and |G{-c.m.}=0.33 MeV {I10} 
$(1976Me18): E{-res}=17.58 MeV {I3}, J|p=3/2+, |G{-c.m.}=322 keV {I75} and |G{-p0}/|G=0.08 {I2} 
$See also table 13.25 of (1970Aj04) where E{p}=17.27 MeV {I5} and |G{-c.m.}|?400 keV from (1968Sn03) and a 1968 Private Communication with Snover are referenced. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E,J,T$From E{-res}=17.60 MeV {I2}, J|p=1/2-, |G{-c.m.}=225 keV {I50} and |G{-p0}/|G=0.24 {I6} phase-shift analysis in (1976Me18). 
E$See also E{-p}=17.6 MeV and T=(1/2) (1967Ku02) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,T$From E{-p}=17.857 MeV in (1970Aj04) Table 13.25. 
E$In (1970Aj04), E{-p}=17857 keV {I5} and |G=66 keV {I8} are given in Table 13.25; the values appear connected with (1968Sn03) a 1968 Private Communication with Snover. 
J$From phase-shift analysis in (1969Le18). 
$(1967Ku02): E{-x}=18.43 MeV {I2}, |G|?30 and T=3/2 
$(1962Wa31): E{-p}=18.05 MeV and |G{-c.m.}|<200 keV 
$(1976Be28): E{-p}=17.87 MeV 


level_energy_unit: KEV
level_spin_parity: 3/2- , 7/2+
level_lifetime_unit: KEV
level_comment:
E,T$From E{-p}=18.460 MeV in (1970Aj04) Table 13.25. 
E$In (1970Aj04), E{-p}=18460 keV {I10} and |G=23 keV {I5} are given in Table 13.25; the values appear connected with (1968Sn03) and a 1968 Private Communication with Snover. 
J$From phase-shift analysis in (1969Le18). 
$(1967Ku02): E{-x}=18.98 MeV {I2}, |G|?10 keV, L=(1) and T=3/2 
$(1976Be28): E{-p}=18.46 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$From E{-x}=19.9 MeV, J|p=7/2+, |G=0.75 MeV polarization data in (1979Ga13); see also E{-p}=19.3 MeV and |G{-c.m.}|<200 keV (1962Wa31) 
E$Several earlier Ajzenberg-Selove evaluations associate this state with resonances observed near E{-c.m.}=19.8 MeV; see (1965Ma26,1966Lo16,1967Sc11), but these appear to be misplaced. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,T$From E{-x}=20.2 MeV, J|p=5/2-, |G=1.0 MeV polarization data in (1979Ga13). 
E$See also (1963Me04) who suggested resonances near E{-p}=20 MeV based on their analysis of {+12}C(p,p'|g(12.7,15.1)). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$From E{-p}=20.5 MeV {I30} (1973Me12) 
J,T$From E{-x}=20.9 MeV polarization data in (1979Ga13) 
$(1966Lo16): E{-c.m.}=19.0 MeV, J|p=(5/2,9/2) and |G=1.5 MeV 
$(1967Sc11) find E{-x}=20.9 MeV, J|p=5/2+, L=2,0 
$(1973Me12): E{-p}=20.55 MeV {I30}, J|p=(5/2+), |G=1.1 MeV, |G{-p0}|?110 keV, |G{-p15.11}|?400 keV 
$(1976Fe11): E{-p}=20 MeV 
$(1976Be28): E{-p}=20.5 MeV, J|p=(3/2+). 
$(1979Ga13): E{-x}=20.9 MeV, J|p=1/2+, |G=1.2 MeV 
$See (1963Me04) who suggested a resonance near E{-p}=20 MeV Based on their analysis of {+12}C(p,p'|g(12.7,15.1)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_comment:
E$From (1964Ta15) analysis of (1963Di16) E{-c.m.}=19.75 MeV, J|p=(3/2+) and |G{-c.m.}=2.49 MeV are deduced. 
$(1965Ma26):See E{-c.m.}=19.8 MeV. 
$(1979Ga13): polarization data suggest a state around 21.7 MeV with J|p=3/2+ 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
E$From E{-p}=22.2 MeV {I5} (1973Me12) 
J,T$From E{-x}=22.4 MeV polarization data in (1979Ga13) 
E$Resonances at several energies around E{-x}=22 MeV have been reported in (1963Di16, 1964Ta15, 1965Ma26, 1967Sc11). In (1970Aj04) Table 13.25 proton resonances were listed at E{-x}=21.99 and 22.6 MeV. However, guided by the discussion and analysis of (1979Ga13, 1981Aj01), we accept only the E{-x}=22.4 MeV J{+|p}=1/2+ state. Along with the accepted states reported in (1979Ga13), their analysis indicated additional states around 21.7 with J|p=3/2+ and above 22.7 with 3/2+. 
$(1964Ta15) analysis of (1963Di16): E{-c.m.}=20.05 MeV, J|p=(5/2+) and |G{-c.m.}=1.46 MeV 
$(1965Ma26): E{-c.m.}=20.01 MeV 
$(1967Sc11): E{-x}=22.5 MeV, J|p=5/2-, L=1 
$(1966Lo16): E{-c.m.}=20.8 MeV, J|p=(5/2,9/2) and |G=0.5 MeV 
$(1973Me12): E{-p}=22.2 MeV {I5}, J|p=(5/2-), |G|?2 MeV, |G{-p0}|?200 keV, |G{-p15.11}|?450 keV. 
$(1979Ga13): E{-x}=22.4 MeV, J|p=1/2+, |G|?1.0 MeV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,J,T$From E{-c.m.}=22.2 MeV, J|p=7/2 and |G=0.5 MeV polarization data in (1966Lo16). 
E$See also E{-p}=23.8 MeV (1975Sl02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
E$From average of E{-x}=25.5 MeV (1967Sc11) and E{-p}=25.9 MeV (1975Sl02). 
J$From E{-x}=25.5 MeV, J|p=3/2-, L=1 Legendre polynomial angular correlation analysis in (1967Sc11) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$From (1964Ta15) analysis of (1963Di16) where E{-c.m.}=24.93 MeV and |G{-c.m.}=2.17 MeV are deduced. 
$(1965Ma26): E{-c.m.}=24.9 MeV (1965Ma26). 
$(1976Fe11): E{-p}=27 MeV 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
WIDTH,WIDTHP0$From (1975Hi07) analysis (p,p) and (p,|a) data. 
E$From (1969Le18); see also |G=1.22 keV and |G{-p}=0.24 keV from their analysis of (p,p) and (p,|a) data 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MIN
level_comment:
T$From T{-1/2}=597.9 s {I3} (1960Ja12), T{-1/2}=9.963 min {I9} (1968Ri15). 
S$From (1971Mu18). See also S=0.34 (1984Sc04). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J,L,S$From finite-range DWBA (1973Sc26:E=36 MeV); see also S=0.72 from (1979Ze01:E=48 MeV) and S=0.38 {I5} from (1986Co02:E=34 MeV). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2+)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
J,L$The discussion of (1987Ad07) and (1988Vo08) associates this state with the J|p=3/2+ GDR at E{-x}=21.7 MeV; however Table 6 of (1988Vo08) shows J; L=5/2+; 2, which appears to be a typo. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$Spin transfer coefficient for J|p=3/2- state D{-NN}(0|')=-0.33 {I5} (1984Ta07). 
E$From (1966Ri09). See also 3.5 MeV {I1} (1970Cl01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
E$From (1984Ta07). 
$Spin transfer coefficient D{-NN}(0|')=-0.36 {I8} (1984Ta07). 
$|s(|q=0|')=1.85 mb/sr {I11} for known T=3/2 state at E{-x}=15.06 MeV. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
$The slope of the shape function is characterized with the parameter {Ia'}=-0.0290 {I8}(stat) {I6}(syst) (2014Ge07) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
S$ consistent with B(>)=2.73 from |b-decay (1981He19). The differential cross section of this state is dominated by an angular momentum transfer of |DL=0. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
$|w|g=0.84 eV {I13}, |w|g0=353 eV {I64} 
$|w|g and |w|g0 from (1990Go25). The ground state |g-ray branching is from analysis of (1969Si04, R.P. Beukens, Ph.D thesis, University of Toronto (1976) and 1990Go25). |G, |G{-|g0}, |G{-|g} and |G{-p} are derived in (2015Sz03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_comment:
J$from (1969Ph02). 
$|w|g=0.270 eV {I40}, |w|g0=119 eV {I21} 
$|w|g and |w|g0 from (1990Go25). The ground state |g-ray branching is from analysis of (1969Si04, R.P. Beukens, Ph.D thesis, University of Toronto (1976) and 1990Go25). |G, |G{-|g0}, |G{-|g} and |G{-p} are derived in (2015Sz03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (9/2)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
J$analyzing power data in 2014Ro26 seem to rule out 7/2+ and 9/2+ proposed earlier. These data could not test 5/2- proposed earlier 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=?
level_comment:
$S({Il}=0)=0.03 {I2}, S({Il}=2)=0.14 {I1}. It is possible that S({Il}=2)=0.14 {I1} is for the 5270 level 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
E$weak compared to E3 population of 5.270 MeV state. The coupling to this state was omitted from the |a calculation. Unresolved from 5270 (5/2+) state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$|d{-3}=1.71 fm 
E$unresolved from 7301 (3/2+) and 7565 (7/2+) states. |d{-3} for 7155 and 7565 states are held equal. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
E$weak compared to the E3 population of the 7155 MeV and 7565 MeV states. The coupling to this state was omitted from the |a calculation. Unresolved from 7155 (5/2+) and 7565 (7/2+) states. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_comment:
$|d{-3}=1.71 fm 
E$unresolved from 7155 (5/2+) and 7301 (3/2+) states. |d{-3} for 7155 and 7565 states are held equal. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
E$weakly populated. The coupling to this state was omitted from the |a calculation, and all the stregth in this region was assigned to the 8312 state. Unresolved from 8312 (1/2+) state. 


level_energy_unit: KEV
level_spin_parity: 7/2(+)
level_lifetime_unit: KEV
level_comment:
E$ E{-|a}=336.7 keV {I10} (2023Bo19). 
J$ J{+|p}=7/2({++}) from (1991HaZU) supported by (2023Bo19) to meet the Wigner limit for the deduced proton spectroscopic factor for this state. 
S$ calculated for {Il}{-|a}=2 and J{+|p}=7/2{++} (2023Bo19). 
$|w|g=6.3|*10{+-7} eV {I9} measured directly by (2023Bo19). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E$ E{-|a}=411.0 keV {I10} (2023Bo19). 
J$ from the Adopted Levels of {+15}N in ENSDF (1991Aj01). 
S$ calculated for {Il}{-|a}=1 and J{+|p}=1/2{+-} (2023Bo19). 
$ C{+2}S{-p}=1.1|*10{+-2} calculated for {Il}{-p}=1 and J{+|p}=1/2{+-} (2023Bo19). 
$ |w|g=1.6|*10{+-5} eV {I3} measured directly by (2023Bo19). 


level_energy_unit: KEV
level_spin_parity: (0-,1-)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$ calculated levels: 0.00 and 0.03 MeV with configurations: p{+-1}{-1/2}~#s{-1/2|L}, J|p=0- and p{+-1}{-1/2}~#s{-1/2|L}, J|p=1- 


level_energy_unit: KEV
level_spin_parity: (1-,2-)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$ calculated levels: 6.71 and 6.93 MeV with configurations: p{+-1}{-3/2}~#s{-1/2|L}, J|p=1- and p{+-1}{-3/2}~#s{-1/2|L}, J|p=2- 


level_energy_unit: KEV
level_spin_parity: (1+,2+)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$ calculated levels: 11.00 and 11.05 MeV with configurations: p{+-1}{-1/2}~#p{-3/2|L}, J|p=2+ and p{+-1}{-1/2}~#p{-1/2|L}, J|p=1+ 


level_energy_unit: KEV
level_spin_parity: (2+,3+)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$ calculated levels: 17.56 MeV with configurations: p{+-1}{-3/2}~#p{-3/2|L}, J|p=3+ and p{+-1}{-3/2}~#p{-1/2|L}, J|p=2+ 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$ from 2007OnAA. The systematic and statistical uncertainties given by 2007OnAA were added in quadrature. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
T$ recoil-shadow method (2008Su12), the quoted uncertainty is statistical. The systematics uncertainty is +8-5 ps 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: S
level_comment:
$Square of ANC: C{+2}{-d5/2}=0.19 fm {+-1} {I2}, halo radius: R{-rms}{+valence}=3.85 fm {I31}, matter radius: R{-rms}{+matter}=2.52 fm {I3} 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: US
level_comment:
T$measured by 2013So20 from |g(t). This value is in agreement with the previous value of 5.25 |ms {I6} given in {+16}N Adopted Levels in the ENSDF database (taken from 1967Be14 (Phys. Rev. 155, 1967)), but more precise by a factor of two. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0-
level_lifetime_unit: US
level_lifetime_info: ;ERR=?
level_comment:
$Populated in {Il}=0 reactions to {+16}N(120,397). 
$At E({+15}N)=7.9 MeV/nucleon, the isomeric ratios {+16m}N/{+16}N{-g.s.}(E{-|g}:120 vs 1755 keV)=43% {I8} and {+16m}N/{+16}N{-g.s.}(E{-|g}:120 vs 2742 keV)=39% {I4} are deduced 
$At E({+15}N)=13.2 MeV/nucleon, the isomeric ratios {+16m}N/{+16}N{-g.s.}(E{-|g}:120 vs 1755 keV)=22% {I2} and {+16m}N/{+16}N{-g.s.}(E{-|g}:120 vs 2742 keV)=25% {I2} are deduced 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_comment:
T$weighted average of: 4174 ms {I4} (1976Oh05), 4169 ms {I8} (1972Al42) 4160 ms {I31} (1965Do13), other: 4230 ms {I490} (1991Re02) 
%|b{+-}n from 1976Al02 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: S
level_lifetime_info: ;ERR=?
level_comment:
MOMM1$ |b-NMR method, g({+17}N)=0.7102 {I7}, sign is not determined in this measurement 
J,T$ from {+17}N adopted levels in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
J$One proton removal from the |p0{Ip}{-1/2} orbital of {+17}N leads to {+16}C{-g.s.}. On the other hand, proton removal from the |p0{Ip}{-3/2} orbital mostly populates unbound {+16}C states. 
$The small (8%) spectroscopic factor for the {+16}C*(1766, 2{++}{-1}) state indicates that proton excitation in that state is negligible and that neutron excitation plays a more dominant role. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: MS
level_comment:
J$From {+18}N |b{+-} decay to {+18}O{-g.s.} (1982Ol01) 
T$From (2005Li60), See also 620 ms {I8} (2007Bu01), 625 ms {I30}, 635 ms {I40} and 609 ms {I60} (2007Lo05), 620 ms {I14} (1999Og03), 0.63 s {I2} (1994Sc01), 658 ms {I44} (1994ReZZ), 624 ms {I12} (1982Ol01) and 0.63 s {I3} (1964Ch19). 
MOMM1$From |b-NMR (2009De34) and (2019StZV). See also |m=0.3279 {I13} (1998Og04) and (-)0.135 {I15} (1999Ne01). 
MOME2$From (1999Og03) and (Priv. comm. Nick Stone (2021)). This is an update of (2014StZZ). See also +0.027 {I4} (1999Ne01). See other discussion in (2003Um02). 


level_energy_unit: KEV
level_spin_parity: (1-)
level_comment:
$The authors indicate J{+|p}=(1-) in the summary; though in the discussion and in Table I they suggest a possible doublet with J{+|p}=(0- and 1-) and S=0.72 {I14}, assuming equivalent values of S for 0- and 1- states . 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2-)
level_lifetime_unit: NS
level_comment:
T$From recoil-distance method (2008Wi05) 
$Configuration: 68% |p(p{-1/2})~#|n(d{-5/2}){+3}; 16% |p(p{-1/2})~#|n[(d{-5/2})(s{-1/2}){+2}] 


level_energy_unit: KEV
level_comment:
$R{+m}{-r.m.s.}=2.65 fm {I2} (2001Oz03), see also R{-rms}{+p}=2.53 fm {I3} and R{-rms}{+m}=2.68 fm {I2} (2019Ba11). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
MOMM1$ |b-NMR method, g({+18}N)=0.3273 {I4}, sign is not determined in this measurement 
J$From Adopted Levels 
A long lived isomer in {+18}N could influence these measurements (1999Og03). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
$|s (mb)=41 {I10} 
$Cross section value deduced by the compilers from total cross section of 65 mb {I10}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2-)
level_comment:
$|s (mb)=6 {I2} 
S$<6 mb {I2}. 
$This level is populated in Branching<0.09 {I2} of 1n-knockout reactions at E/nucleon|?700 MeV. 


level_energy_unit: KEV
level_spin_parity: (3-)
level_comment:
$|s (mb)=15 {I2} 
S$>15 mb {I2}. 
$This level is populated in Branching>0.23 {I1} of 1n-knockout reactions at E/nucleon|?700 MeV. If this is the only level populated then Branching<0.32 {I4} 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$Half-lives of 630 ms {I20} (1994Sc01), 619 ms {I2} (2005Li05), and 625 ms {I30}, 635 ms {I40} and 609 ms {I60} (2007Lo05) were determined in this reaction. 
%B-N$Analysis of fast neutrons measured by (2005Li60) and (2007Lo05) indicates consistency with %|b{+-}n|>7% 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$Deduced discrete |b{+-}|a decay branches and normalized to %|b{+-}|a=12.2 from (1989Zh04). 
T$From (2007Bu01) 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: PS
level_comment:
E$see also E{-x}=2404.6 keV {I13} deduced by (2020Zi03). 
T$From |t=0.16{++74}{--10} ps and E|g=1663.0 keV {I8} (2020Zi03,2021Zi01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MS
level_comment:
$See also P{-n}=(33 {I+34-11})% (1988Mu08), P{-n}=(62.4 {I26})% (1991Re02) and (1993ReZX). 
T$From (2006Su12). Previous results are 0.32 sec {I10} (1986Du07), 0.21 sec {I+20-10} (1988Mu08), 0.235 sec {I32} (1988Sa04), 0.300 sec {I80} (1988DuZT), 0.329 sec {I19} (1991Re02), 0.255 sec {I10} (P.L. Reeder et al., Int. Conf. on Nucl. Data for Science and Technology, May 9-13, 1994, Gatlinburg, Tennessee) and 0.271 sec {I8} (1995ReZZ). See also (1984Kl06, 1986JeZY,1987BaZI,1987DuZU,1987MiZU,1988BaYZ, 1994KiZU) and (1988Wa17, 1982CuZZ: theory). 
${Ig}-factor(=0.61 {I3}) (2004Ka22) is significantly smaller than the value of {Ig}({+17}N{-g.s.}) which contradicts the shell-model predictions. 
MOMM1$An upper limit {|}|m({+19}N){|}|<0.32 |m{-N} was deduced in (2004Ue03). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: MS
level_comment:
$%|b{+-}n: From (2006Su12). 
J$From (2008So09). See also (2012Yu07). 
T$Weighted average of 136 ms {I3} (2006Su12), 129 ms {I8} (P.L. Reeder et al., Int. Conf. on Nucl. Data for Science and Technology, May 9-13, 1994, Gatlinburg, Tennessee ), 70 ms {I40} (1988DuZT), 100 ms {I+30-20} (1988Mu08,1990Mu06); see also (1989MuZT,1990St08). Others: 142 ms {I19} (1991Re02) and 130.0 ms {I66} (unpublished private communications of (2008ReZZ)/(1995ReZZ)). 
$The delayed neutron probability, P{-n}, has been reported as 57% {I+11-7} (1988Mu08,1990Mu06), 66.1% {I50} (1991Re02), 46% {I11} (2006Su12). A reanalysis of (1991Re02) to include data published in the International conference on nuclear data for science and technology: nuclear data for the twenty-first century, Gatlinburg, TN, U.S.A.,9-13 May 1994) estimated P{-n}=52.0% {I33}. 
$The measurements of (2006Su12) provide the only quantitative measure of {+20}O and {+19}O spectroscopy for levels and transitions involved in the decay. The %|b{+-}1n=42.9 {I14} is deduced; furthermore, only {+19}O*(96,1472) levels are fed in the 1n decay. Beta-decay to neutron bound levels in {+20}O is found to comprise 53.8% {I13} of decays with an additional upper limit of 3.3% feeding {+20}O{-g.s.} directly. 
$The P{-n}=P{-1n}+2P{-2n}=52.0% {I33} value from the revised zero-threshold measurement of (1991Re02) can be combined with P{-1n}=42.9% {I14} from (2006Su12) to estimate the value of P{-2n}|?4.5%. The P{-2n} contribution in the decay was not considered when the limit on direct feeding of {+20}Og.s. was deduced. See also (1987BaZI,1987DuZU,1988BaYZ,1993ReZX,1994KiZU). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$The authors stated that due to the limited resolution of the gamma calorimeter, the first and the second excited states could not be separated. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$The authors attribute most of the cross section to the 850-level, and they did not attempt to deconvolute the two observed peaks. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MS
level_comment:
T$Weighted average of 83 ms {I8} (2009Li51), which replaced their earlier result of 82.9 ms {I19} (2008Lo06), 95 ms {I+15-11} (1990Mu06) 61 ms {I23} (1991Re02), 83.6 ms {I67} (1995ReZZ,1991Re02). 
%B-N$Weighted average of 90.5 {I42} (2009Li51), 84 {I9} (1990Mu06), 76 {I15} (1991Re02,1995ReZZ), and 78 {I7} (1995ReZZ). 
%B-2N$|b-delayed two-neutron emission is energetically possible. A search for the 1356|g in {+19}F proved negative (2009Li51). 
J$From comparison of one-neutron removal cross sections to extended Glauber model calculations, weighted by shell model spectroscopic factors (2004Sa14,2000Sa47). 
$Measured one-neutron removal cross section=140 mb {I44} (2004Sa14) in C({+21}N,{+20}N) reaction at 43 MeV/nucleon 
$Measured interaction |s=1114 mb {I9} (2001Oz03) in C({+21}N,X) at E=1005 MeV/nucleon. Deduced matter radius=2.75 fm {I3} (2001Oz03) 
$Measured |s=2.12 b {I7} at 34.20 MeV/nucleon and 2.16 b {I3} at 39.15 MeV/nucleon in Si({+21}N,X) reaction (2006Kh08); deduced strong absorption r{-0}{+2}=1.231 fm{+2} {I15} (2006Kh08) 
E$Least-squares fit to |g-rays from 2008So09 and 2010El05. 


level_energy_unit: KEV
level_spin_parity: (0-)
level_lifetime_unit: MS
level_comment:
T$Weighted average of 24.5 ms {I65} (symmetric value of 24 ms {I+7-6} 1990Mu06), 31 ms {I5} (2001Pe14), 16.5 ms {I+85-48} (2003Yo02 - used symmetric value of 18.3 ms {I66}), 14 ms {I6} (1995ReZZ), and 24 ms {I3} (3198|g-t), 22 ms {I4} (1845n-t), 21 ms {I7} (total |b-t) - all from 2010Su03. Uncertainty is the lowest experimental value. 2010Su03 adopted a {+22}N half-life of 20 ms {I2}, deduced (procedure not described) from measured values of neutron- (five), |g-ray (two) gated decay, and total |b-decay (one) curves. 
%B-N$Weighted average of 35 {I5} (1990Mu06), 37 {I14} (2001Pe14), 41 {I+12-10} (2003Yo02), 33 {I3} (2010Su03), 34 {I14} (2008ReZZ). 
%B-2N$From 2010Su03. Other: <13 (2003Yo02) 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$ unbound state, deduced from observed E(n)(c.m.)=650 {I50} (width=60 keV). S(n)({+22}N)=1280 {I210} (2012Wa38) 
E,J$ first 3- state from shell-model predictions (2009St20) 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$ unbound state, E(n)(c.m.)=650 {I50}. S(n)({+22}N)=1280 {I210} (2012Wa38). 
E,J$ first 3- state from shell-model predictions (2009St20) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
$<r{+2}>{+1/2}({+23}N)=3.41~fm~{I23} (matter radius) (2001Oz03). 
J$1/2- from shell model calculations (2017Jo06). 2015Zh05 assumes {+21}N core and two valence neutrons, where J{+|p}({+21}N) assigned as (1/2-) in 2015Fi05. 
T$From |b-n(t) coin 2003Yo02. Other: 14.5~ms~{I14} (1998Yo06 - same research group of 2003Yo02) 
$Neutron Emission Probability %p{-n} |? 58~{I10} (From Fig. 5b - %Pn=|S i |* %Pin (2003Yo02)). Other: 80~{I21} (1998Yo06 - same research group of 2003Yo02). 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 3/2-
level_comment:
E$Decay Energy=1070~keV~{I100}. Sn({+23}N)=2460~keV~{I380} (2012Ga45) gives an excitation energy of 3530~keV~{I400} (100 (stat)+400 (sys)) (Sn+Decay energy). In 2016-AME Sn({+23}N)=3120~keV~{I470} (2017Wa10). 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 3/2-
level_comment:
E$Decay Energy=2500~keV~{I+500-700}. Sn({+23}N)=2460~keV~{I380} (2012Ga45) gives an excitation energy of 4960~keV~{I+630-800} (Sn+Decay energy). In 2016-AME Sn({+23}N)=3120~keV~{I470} (2017Wa10). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-rel.}(2p+{+9}C) (MeV)=4.16 {I} 
E$(2019We03) observe a peak near E{-res}(2p+{+9}C)|?4.5 MeV that is reasonably explained assuming a four resonance multiplet. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-rel.}(2p+{+9}C) (MeV)=4.16 
E$(2019We03) observe a peak near E{-res}(2p+{+9}C)|?4.5 MeV that is reasonably explained using a four resonance fit. The fit, which is guided by theory, is found to be favorable but not uniquely constrained. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MEV
level_uncertain: ?
level_comment:
$E{-res}({+10}C+2p)(keV)=3.26E3 {I11} 
E$From E=1.62 MeV {I3}(stat) {I10}(syst) (2016Su05). 
T$From |G=1.2 MeV {I1}(stat) {I+3-7}(syst) (2016Su05). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MEV
level_comment:
E$From E=1.62 MeV {I3}(stat) {I10}(syst). 
T$From |G=1.2 MeV {I1}(stat) {I+3-7}(syst). 
$Discussion is given that considers any evidence that this state may be a doublet. No evidence as such is found in the present results. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From E(2p+{+10}C)=1.638 MeV {I24}; corresponds to |DM=31.914 MeV {I24}. 
T$The observed |G is |?230 keV, however analysis of the experimental resolution yields |G<72 keV. This is much narrower than prior measurements. 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_lifetime_unit: MEV
level_comment:
E$The group may correspond to either: a J{+|p}=0+ state previously reported at E{-x}|?1.6 MeV [E(2p+{+10}C)|?3.4 MeV] (2016Su05), a J{+|p}=1- state predicted at 3.26 MeV (2019Wa16) or the p{-1} proton decay branch from the known E(2p+{+10}C)|?4.8 MeV state to the {+10}C*(3.353 MeV) excited state. If the later is the case, then its branching ratio is (27 {I1})%. 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$E{-T} (MeV): (2p+{+10}C) total kinetic energy: From 2p+2|a. Note: in this case E{-x}=7972 keV + (Q{-2p}({+10}C)=3820 keV) - 1718 keV=10074 keV. 
$Found to have decays with |?50% of involving a {+6}Be{-g.s.}, 20% involving a {+9}B{-g.s.}, 9% involving {+6}Be{-g.s.}+{+6}Be{-g.s.} and |?6% involving |a+{+8}C{-g.s.}. 
$Comparison with {+12}N suggests this group is not a singlet state. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: MS
level_comment:
MOME2$From reanalysis of (1999Ma46). 
J$Allowed {Ift} values to {+13}N J|p=1/2-, 3/2-, 5/2- states (1970Es03) 
T$From weighted average of 8.7 ms {I4} (1965Mc09), 8.95 ms {I20} (1970Es03) and 8.55 ms {I5} (1990As01). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). See also E{-x}=2400 keV {I50} (1991Go13,1991GoZR) {+16}O({+3}He,{+6}He), E{-x}=2690 keV {I50} (2007Sk02) {+1}H({+12}N,p), and E{-x}=2690 keV {I50} from the (2007GuZW: |DE estimated by evaluator) {+16}O({+3}He,{+6}He) conference proceedings. Other values reported near this energy are E{-x}=2.82 MeV {I24} (1978Co15) {+12}C(p,|p{+-}) and E{-x}=2.8 MeV {I3} (2012Su21) {+1}H({+14}O,d). 
T$See also |G=0.45 MeV {I10} (2007Sk02), <300 keV (2012Su21) and <100 keV (2007GuZW: est.) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). See also E{-x}=2956 keV {I15} and |G<50 keV (2013So11) {+9}Be({+13}O,{+13}O). Ambiguity exists in the level energies obtained from the {+13}C(|p{++},|p{+-}) reaction. A narrow resonance is reported in (1984Se15) with E{-x}=2.75 MeV {I4} and in (1993Wa07) with 3.10 MeV {I7}; we associate these observations with either or both of the E{-x}=3006 keV and 3051 keV adopted levels of this evaluation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). See also E{-x}=3025 keV {I16} and |G<50 keV (2013So11) {+9}Be({+13}O,{+13}O) and E{-x}=3038 keV {I9} (2019We11) {+9}Be({+13}O,{+13}O). Also see E{-x}=2750 keV {I40} (1984Se15) and 3100 keV {I70} (1993Wa07) both from {+13}C(|p{++},|p{+-}), and 3120 keV {I50} (2007GuZW:|DE est.) {+16}O({+3}He,{+6}He). 
T$See also |?0.43 MeV (2007GuZW:est.). 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_lifetime_unit: KEV
level_uncertain: ?
level_comment:
E,J,T$From R-matrix analysis in (2007Sk02) {+1}H({+12}N,p). See also E{-x}=3120 keV {I50} and |G=0.43 MeV {I10} (2007GuZW:est.) {+16}O({+3}He,{+6}He). 
E$This level is listed because of the significant energy difference between 3290 and the nearest level at E{-x}=3051 keV and because of the broad width of the group reported in (2007GuZW) that may suggest both groups were populated in that study. But, its existence is rather uncertain. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). See also E{-x}=3669 keV {I13} and |G<50 keV (2013So11) {+9}Be({+13}O,{+13}O), E{-x}=3701 keV {I10} (2019We11) {+9}Be({+13}O,{+13}O). Also see E{-x}=3800 keV {I50} and |G|?160 keV (2007GuZW: |DE and |G est.) {+16}O({+3}He,{+6}He) where the unresolved {+13}O{+*}(3692+3721) states may have been observed. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+,5/2-)
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). See also E{-x}=3800 keV {I50} and |G|?160 keV (2007GuZW: |DE and |G est.) {+16}O({+3}He,{+6}He) where the unresolved {+13}O{+*}(3692+3721) states may have been observed. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). 
E$See also E{-x}=4.21 MeV (1984Se15) and 4500 keV {I90} (1993Wa07) discrepant values reported in {+13}C(|p{++},|p{+-}), 4.2 MeV {I3} (2012Su21) {+1}H({+14}O,d) and 4410 keV {I50} (2007GuZW: |DE est.) {+16}O({+3}He,{+6}He). 
J$See also (1/2-,3/2,5/2+) (2012Su21) and (1/2-) from (1993Wa07) 
T$See also |G=0.6 MeV {I4} (1993Wa07), <500 keV (2012Su21) and |?0.43 MeV (2007GuZW: est.) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). See also E{-x}=4.95 MeV {I10} and |G|?280 keV (2007GuZW: |DE and |G estimated by evaluator.) {+16}O({+3}He,{+6}He). 


level_energy_unit: KEV
level_spin_parity: (7/2+,7/2-)
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2021Ch45) {+9}Be({+13}O,{+13}O). 
E$(2021Ch45) suggests two states in this region: one at E{-x}=5951 keV {I18} along with a questionable state at |?6.2 MeV; both have broad widths of around 1 MeV. Other reactions have reported broad states near E{-x}|?6 MeV, but none have suggested or resolved two states. We associate all firm states reported in this region with the lower level reported in (2021Ch45), but highlight that the associations may be different if both states are found to exist. Other energies reported near E{-x}=6 MeV are 6020 keV {I80} (1984Se15) and 6100 keV {I90} (1993Wa07) both from {+13}C(|p{++},|p{+-}), 6.00 MeV {I10} (2007GuZW: |DE est.) {+16}O({+3}He,{+6}He) and 6 MeV (2007TaZR) {+13}C({+11}B,{+11}Li). 
T$Other reported widths are |G|?1.2 MeV (1984Se15) and |G=0.6 MeV {I4} (1993Wa07) from {+13}C(|p{++},|p{+-}); (1984Se15) suggest the group may correspond to one or more unresolved states. See also |G|?1.0 MeV (2007GuZW: est.) 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E,T$From (1993Wa07) {+13}C(|p{++},|p{+-}). See also E{-x}=8.8 MeV {I5} and |G=3.0 MeV {I6} (1991Mo02) and E{-x}=8.8 MeV (2007TaZR) {+13}C({+11}B,{+11}Li). 
E$Suggested GDR~#IAS (GDR built on isobaric analog states) see (2007TaZR, 1984Se15). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E$Q(g.s)=-18.9 MeV {I1} (1993Wa07,1991Mo02). 
T$The value |G=400 keV {I60} is reported in (1993Wa07), but this would imply a particle unbound level. 


level_energy_unit: KEV
level_comment:
WIDTH$NARROW 
E$From E{-x}=2.75 MeV {I4} in (1984Se15). See also E{-x}=3.10 MeV {I9} from Q=-22.0 MeV {I6} (1993Wa07). 
T$In (1984Se15) a peak with a narrower width than the g.s. is observed; subsequent results from (2021Ch45) {+9}Be({+13}O,{+13}O) support the existence of narrow states (|?50 keV) in this region. The other width reported for this state is |G=0.60 MeV {I40} (1993Wa07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-)
level_comment:
E$From (1984Se15). See also E{-x}=4500 keV {I90} from Q=-23.4 MeV (1993Wa07). 
J$Based on similarities with {+12}C(|p{++},|p{+-}){+12}O(g.s.) and {+14}C(|p{++},|p{+-}){+17}O(5.9 MeV) (1984Se15). 
T$In (1984Se15) a peak with a similar width to the g.s. is observed. The only width reported for this state in {+13}C(|p{++},|p{+-}) is |G=0.60 MeV {I40} in (1993Wa07). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
E$From (1984Se15). See also E{-x}=6.10 MeV {I9} from Q=-25.0 MeV {I8} (1993Wa07) and see also 5.1 MeV from Q=-24.0 MeV {I5} in (1991Mo02). 
T$From (1984Se15). The other width reported for this state is |G=0.60 MeV {I40} (1993Wa07). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E,T$From Q=-27.6 MeV {I2} (1993Wa07). See also Q=-27.7 MeV {I5} and |G=3.0 MeV {I6} (1991Mo02), and Q=-27.4 MeV {I5} and |G=2 MeV {I1} (1989Mo09). Suggested GDR~#IAS resonance. 


level_energy_unit: KEV
level_spin_parity: 1/2+,(1/2-:5/2+)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=LT
level_comment:
J|p=1/2+,(1/2-,3/2-,3/2+,5/2+). 
$The authors suggest this state corresponds to the 2.7 MeV J|p=1/2+ level of (2007Sk02), though participation of a second |DL=1 or 2 state can not be ruled out. Discussion on the spectroscopic factors for the various doublet combination is given in Table 1. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$C{+2}S(phenomenological)=1.69 {I17} (experimental) {I20} (analysis). C{+2}S(microscopic)=1.89 {I19} (experimental) {I22} (analysis). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$See also E{-x}=2.40 MeV {I5} (1991Go13,1991GoZR). 
T$The |?250 keV width observed in the spectrum suggests |G<100 keV. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$Weighted average: 70.59 s {I3} (1973Cl12), 70.613 s {I25} (1978Wi04). Others: 70.43 s {I18} (1974Az01), 70.48 s {I5} (1972Al01) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
S$apparent B(GT)=0.007 {i1}, deduced from proportionality of the extrapolated cross sections in the present ({+3}He,t) experiment. The real B(GT) value could could not be determined in this reaction. The B(GT) value deduced from log| {Ift} value in {+14}N g.s. to {+14}O g.s. decay is 0.681|*10{+-4} {I9} 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$deduced by combining present measurements, T{-1/2}(|b)=70.610 s {I30} and T{-1/2}(|g)=70.632 s {I94}, with prior measurements. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
|w|g=13.1|*10{+-3} eV {I6} (E.G. Adelberger et al., arXiv: 1004.2318) for E(p)(lab)=278-keV resonance 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
|w|g=0.364 eV {I21} for E(p)(lab)=1058-keV resonance. Normalized to |w|g=13.1|*10{+-3} eV {I6} for {+15}O*(7556). Analysis of prior work results in a recommended value |w|g=0.353 eV {I18}. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
T$from |G(l=0,s=1.5)=2.93 keV {I2} (stat) {I6} (syst) {I0} (model) and |G(l=2,s=1.5)=0.91 keV {I3} {I10} {I1} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$from E{+res}{-cm}=259.1 keV {I7} (HPGe near |?1.62 cm). See also E{+res}{-cm}=259.6 keV {I6} (HPGe far |?21.62 cm). 
$|w|g=12.60|+0.15(stat)|+0.55(sys) meV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$From the lifetime |t=7.5 fs {I30}, which is the average of |t=7.1 fs {I+48-23} (molybdenum), 7.1 fs {I55} (tantalum) and 8.0 fs {I67} (tungsten). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$From |t=0.7 fs {I5}, which is the average of |t=0.4 fs {I+7-4} (molybdenum), 1.4 fs {I10} (tantalum) and 0.6 fs {I+9-6} (tungsten). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$From |t=0.6 fs {I4}, which is the average of |t=0.2 fs {I+7-2} (molybdenum), 0.7 fs {I+9-7} (tantalum) and 0.9 fs {I6} (tungsten). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
$Multipolarity=M2. Total cross section is 12% M1 and 88% M2. This gives B(M1)|^=0.13 |m{+2}{-n} 3 and B(M2)|^=341 |m{+2}{-n} 51 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E$ |DE{-level} deduced by compilers from adding 1.6 (statistical) and 0.5 (systematic) uncertainties in quadrature. Expected spin-flip M1 transition between g.s. doublet members beyond detection limits. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
E$ From least-squares fit to 6534 and 6560 |g rays, holding 26.4 level energy fixed. 
T$ based on single-particle estimation. 
$ Configuration={+16}{-|L}O[(p{-3/2}){-n}{+-1}(s{-1/2}){-|L}]{-1-} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_uncertain: ?
level_comment:
Not listed in global R-matrix parameter table. 
(1982Aj01) had listed a (0+,1-) state observed in (1982Am02), but later this state was correlated with a 2+ state observed in {+15}N(p,p). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
|w|g=22.7 eV {I14} for E(p)(lab)=430-keV resonance. Normalized to |w|g=13.1|*10{+-3} eV {I6} for {+15}O*(7556). Analysis of prior work yields a recommended value of 21.9 eV {I10}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
|w|g=362 eV {I20} for E(p)(lab)=897-keV resonance. Normalized to |w|g=13.1|*10{+-3} eV {I6} for {+15}O*(7556). Analysis of prior work yields a recommended value of 362 eV {I20}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5-
level_lifetime_unit: KEV
level_comment:
$|G{-|a0}/|G=0.951 {I49} and |G{-|a1}/|G<0.05 from present |G{-|a0}/|G=1.02 {I14}, |G{-|a1}/|G=0.11 {I5}, and comparison with previous results. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 6+
level_lifetime_unit: KEV
level_comment:
$|G{-|a0}/|G=0.982 {I48} and |G{-|a1}/|G<0.02 from present |G{-|a0}/|G=1.02 {I9}, |G{-|a1}/|G<0.02, and comparison with previous results. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
S$0.10 {I+8-6}. 
$The |a reduced width, |g{-|a}{+2}=174 keV {I28} from linewidth analysis; 30 keV {I22} from DWBA analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: KEV
level_comment:
S$0.19 {I+17-8}. 
$The |a reduced width, |g{-|a}{+2}=60 keV {I14} from linewidth analysis; 20.1 keV {I79} from DWBA analysis. 


level_energy_unit: KEV
level_comment:
$Observed in {+12}C+|a -->{+8}Be{-g.s.}+{+8}Be{-g.s.}, {+12}C+|a --> |a+{+12}C*(7.65), {+12}C+|a -->|a+{+12}C*(9.64). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_comment:
E$likely correspond to previously unresolved state reported at 14620 with |G=490 keV {I15} and J|p=4(+). 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: KEV
level_comment:
E$likely correspond to previously unresolved state reported at 14660 with |G=670 keV {I15} and J|p=5-. 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: KEV
level_comment:
$The angular distribution is not well fitted with L=0,2,4 or 6 components. In 1993Ti07, the E{-x}=14815.3 keV state is reported with J|p=6+. That state has a significant decay component to {+12}C*(4.44 MeV: J|p=2+) which may explain the poor fit obtained in the present work. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: PS
level_comment:
$S(|a)=0.05 {I+3-2}. 
$May contain a small contribution from the weakly populated and unresolved {+16}O*(6049) J|p=0+ state. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E,J$The |a{-0} decay strength is centered at E{-x}=15090 keV {I7} with |G=162 keV {I4} and {Il}=1+5 deduced from the angular distribution. The |a{-1} decay strength is centered at E{-x}=15046 keV {I8} with |G=216 keV {I10} and {Il}=0,2. 
$The data suggests contributions from an unknown level near E{-x}= 15 MeV with J|p=2{++},3{+-}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_comment:
$Decays via |a+{+12}C. 
J$The observed intensities are consistent with J{+|p}=3+. The authors listed the 11097 keV as a J{+|p}=3+ state, however ENSDF indicates J{+|p}=4+. The authors are unable to resolve the difference in these states due to experimental uncertainty; hence E{-x}=11.080 MeV is assumed. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_comment:
WIDTH$|G{-|a1}/|G=0.46 {I8} and |G{-|a0}/|G|?0 [while not in the text, the compiler assumes |G{-p0}/|G|=0.54 {I8}]. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
J$Theory (i.e. 2008Fu11) predicts a level with an |a condensate configuration at E{-x}=15.1 MeV, and the authors suggest the present level could be the 0{-6}{++} state with a configuration analogous to that of the Hoyle state condensate of |a particles. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$This state could correspond to the E{-x}({+16}O)=16.44 MeV, J{+|p}=2{++} identified by (1993Ti07). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$This state is an unresolved doublet. 
T$The width is deduced from the FWHM of a single Gaussian fit to the unresolved doublet. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
E$From recoil corrected E{-|g}. 
$T{-1/2}: weighted average of 170 ps {I7} from {+14}N(|a,p) (1974Sc09) and 180.4 ps {I20} from {+16}O(d,p) (see discussion). 
J$From {+16}O(d,p) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
E$From recoil corrected least squares fit E{-|g}=2184.49 {I5} and 870.732 {I20}. See also 3054.98 {I20} from {+16}O(d,p) (2015Pi05) 
T$From 80 fs {I+60-40} from {+14}C(|a,n) (1964Al11) and 110 fs {I+28-21} from {+181}Ta({+18}O,{+17}O|g) (2020Zi03). 
J$From {+17}N |b- decay. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: EV
level_comment:
E$From 3842.76 keV {I42} from {+16}O(d,p) (1990Pi05), 3842.9 keV {I4} from {+19}F(d,|a) (2015Fa12), 3844 keV {I7} from {+12}C({+6}Li,p) (1986Sm10) 
T$From {+17}O(|g,|g') (1994Mo18) 
J$From {+14}C({+6}Li,t) (1981Cu11) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
WIDTHG$From (1992Ig01). See also |G{-|g}<4.0 eV (1971Al09) and |G{-|g0}=0.42 eV (1978Ho16). 
E$From 4551.4 keV {I7} from {+19}F(d,|a) (2015Fa12), 4553.8 keV {I16} from {+16}O(d,p) (1990Pi05), 4551 keV {I4} from {+16}O(n,n) (1958Hu18), 4555 keV {I8} from {+12}C({+6}Li,p) (1986Sm10) and 4544 keV {I10} from {+16}O(n,n) (1971Al09). 
WIDTH$ weighted average of 39 keV {I3} from {+16}O(n,n) (see discussion), 40 keV {I5} from {+16}O(d,p) (1957Br82), and 38.1 keV {I28} from {+19}F(d,|a) (2015Fa12). 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E$From 5089 keV {I1} from {+2}H({+16}O,p) (2013Al14), 5082 keV {I8} from {+16}O(n,n) (1958Hu18), 5084.4 keV {I9} from {+16}O(d,p) (1990Pi05) and 5087.7 keV {I10} from {+19}F(d,|a) (2015Fa12) 
WIDTH$ weighted average of 90 keV {I5} (lab) from {+16}O(n,n) (see discussion), 95 keV {I5} from {+16}O(d,p) (1957Br82), and 88 keV {I3} from {+19}F(d,|a) (2015Fa12). 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From average of 5217 keV {I8} from {+12}C({+6}Li,p) (1986Sm10), 5216.5 keV {I4} from {+19}F(d,|a) (2015Fa12) and 5215.77 keV {I45} from {+16}O(d,p) (1990Pi05). 
WIDTH$ This level is not observed in {+16}O(n,n) (1973Fo11) leading to a width estimate of |G<0.1 keV. 
J$From {+17}O(e,e') (1987Ma52) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$From discrepant values of 5380 keV {I9} from {+12}C({+6}Li,p) (1986Sm10), 5377.9 keV {I35} from {+16}O(n,n) (see discussion), 5379.2 keV {I14} from {+16}O(d,p) (1990Pi05) and 5388.8 keV {I6} from {+19}F(d,|a) (2015Fa12) 
WIDTH$ weighted average of 31 keV {I4} from {+16}O(n,n) (see discussion), 28 keV {I7} from {+16}O(d,p) (1957Br82), and 39.0 keV {I21} from {+19}F(d,|a)) (2015Fa12). 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
E$From 5697 keV {I2} from {+16}O(n,n) (1973Fo11) 5697.5 keV {I5} from {+19}F(d,|a) (2015Fa12) and 5697.26 keV {I33} from {+16}O(d,p) (1990Pi05) 
WIDTH$From {+16}O(n,n) (1973Fo11) 
J$From {+16}O(d,p) (1956Gr37,1961Ke02,1963Ya03,1964Sc12) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From 5732.79 keV {I52} from {+16}O(d,p) (1990Pi05), 5731.6 keV {I4} from {+19}F(d,|a) (2015Fa12) and 5733 keV {I2} from {+16}O(n,n) (1973Fo11) 
WIDTH$From {+16}O(n,n) (1973Fo11) 
J$From {+17}O(e,e') (1987Ma52) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E$From 5869.7 keV {I6} {+19}F(d,|a) (2015Fa13), 5869.07 keV {I55} from {+16}O(d,p) (1990Pi05) 
WIDTH$From {+16}O(n,n) (1973Fo11) 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E$From 5931.0 keV {I11} from {+19}F(d,|a) (2015Fa12) and 5939 keV {I4} from {+16}O(n,n) (1973Fo11) 
WIDTH$ weighted average of 32 keV {I3} from {+16}O(n,n) (1973Fo11), 23 keV {I10} from {+16}O(d,p) (1957Br82), and 33 keV {I5} from {+19}F(d,|a) (2015Fa12). 
J$From {+16}O(n,n) (1973Jo01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$|G |? |G{-n} (2012La29) 
E$From 6356 keV {I8} from {+16}O(n,n) (1973Fo11) and 6363.4 keV {I31} from {+19}F(d,|a) (2015Fa12) 
WIDTH$ weighted average of 83 keV {I+9-12} from {+13}C({+6}Li,d) (2012La29), 124 keV {I12} from {+16}O(n,n) (1973F011) and 136 keV {I5} from {+19}F(d,|a) (2015Fa12). 
J$From {+16}O(n,n) (1973Jo01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$Average of 6860.7 keV {I4} from {+19}F(d,|a) (2015Fa12) and 6860.3 keV {I7} from {+13}C(|a,n) (1993Br17) 
WIDTH$From {+16}O(n,n) (1973Fo11). 
J$from {+12}C({+6}Li,p),({+7}Li,d) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From average of 6972.6 keV {I4} from {+19}F(d,|a (2015Fa12) and 6972.1 keV {I8} from {+13}C(|a,n) (1993Br17). 
WIDTH$From {+16}O(n,n) (1973Fo11). 
J$From {+17}O(e,e') (1972Ma52). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
WIDTHA$From (1973J011). See also |G{-a}=3.4 eV (2020Me09) and |G{-n}/|G{-|a}=1300 (1957Wa46). 
E$From {+16}O(n,n) (1980Ci03). See also 7166.5 keV {I15} from {+13}C(|a,n)) (1973Ba10) and 7165.4 keV {I18} from {+19}F(d,|a) (2015Fa12) 
WIDTH$ From {+16}O(n,n) (1980Ci03). See also 1.5 keV {I2} from {+13}C(|a,n) (1973Ba10) 
J$From {+16}O(n,n) (1973Jo01) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=0.00043 from |G{-n}=280 keV |G{-|a}=0.12 keV (1973Jo01). See also |G{-n}=400 keV and |G{-|a}=0.09 keV (2008Pe09) and |G{-n}=340 keV and |G{-|a}=0.14 keV (2008He11, 2012La29). and |G{-|a}=0.073 keV (2020Me09). 
E$From average of 7216 keV {I4} from {+19}F(d,|a) (2015Fa12) and 7202 keV {I10} from {+16}O(n,n) (1973Fo11) 
WIDTH$ weighted average of 280 keV {I28} from {+16}O(n,n) (1973Fo11) and 262 keV {I7} from {+19}F(n,t) (2015Fa12). 
J$From {+16}O(n,n) (1973Fo11, 1973Jo01) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G|?0.02 from |G{-n}=0.50 keV |G{-|a}=0.01 keV (1973Jo01) See also |G{-n}/|G{-|a}=450 (1957Wa46), |G{-n}=0.41 keV |G{-|a}=0.011 keV (2008He11, 2012La29). 
E$Average of 7379.20 keV {I19} from {+16}O(n,n) (1980Ci03) and 7380.9 keV {I15} from {+13}C(|a,n) (1973Ba10). See also 7379 keV {I3} from {+16}O(n,|g),(n,n) (1973Fo11) 
WIDTH$ weighted average of 0.6 keV {I+2-1} from {+13}C(|a,n) (1973Ba10) and 0.64 keV {I23} from {+16}O(n,n) (1980Ci03) 
J$From {+16}O(n,n) (1970Fo03,1957Wa46). and {+13}C(|a,n) (1973Ba10) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G|?0.0027 from |G{-n}=1.2 keV |G{-|a}=3.2 eV (1973Jo01) 
E$From 7382.16 keV {I14} {+16}O(n,n) (1980Ci03) and 7383.9 keV {I15} from {+13}C(|a,n) (1973Ba10). See also 7382 keV {I3} from {+16}O(n,|g),(n,n) (1973Fo11) 
WIDTH$ weighted average of 0.8 keV {I+3-2} from {+13}C(|a,n) (1973Ba10) and 0.96 keV {I20} from {+16}O(n,n) (1980Ci03). 
J$From {+16}O(n,n) (1970Fo03,1957Wa46). and {+13}C(|a,n) (1973Ba10). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$Average of 7510 keV {I30} from {+19}F(d,|a) (Bu51), 7530 keV {I50} from {+16}O(d,p) (Bu51) 7559 keV {I20} from {+16}O(n,n) (1973Fo11) 
WIDTH$From {+16}O(n,n) (1973Fo11) 
J$From {+16}O(n,n) (1973Fo11). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$Average of 7572.9 keV {I21} from {+13}C(|a,n) (1973Ba10, 1993Br17) and 7573.5 keV {I6} from {+15}F(d,|a) (2015Fa12). 
WIDTH$ This level is not observed in {+16}O(n,n) (1973Fo11) leading to a width estimate of |G<0.1 keV. 
J$From {+12}C({+6}Li,p)({+7}Li,d) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
E$From {+16}O(n,n) (1980Ci03). See also 7689.2 keV {I6} from from {+19}F(d,|a) (2015Fa12). 
WIDTH$ From {+16}O(n,n)(1980Ci03). See also 12 keV {I4} from {+19}F(d,|a) (2015Fa12). 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=7.39 From |G{-|a}=6.7 keV and |G{-n}=84 keV (1973Jo01). See also |G{-n}/|G{-|a}=10 (1957Wa46). 
E$Average of 7952 keV {I8} from {+13}C(|a,n) (1973Ba10) and 7958 keV {I8} from {+16}O(n,n) (1973Fo11) 
WIDTH$ weighted average of 79 keV {I10} from {+13}C(|a,n) (1967Se07) and 90 keV {I9} from {+16}O(n,n) (1973Fo11). 
J$From {+16}O(n,n) (1973Fo11, 1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=0.053 From |G{-|a}=14 keV and |G{-n}=250 keV (1973Jo01). See also |G{-|a}/|G=0.059 {I7} (1973Fo11). 
E,J,WIDTH$From {+16}O(n,n) (1973Fo11, 1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=7.39 From |G{-|a}=15 keV and |G{-n}=71 keV (1973Jo01). 
E$Average of 8060 keV {I8} from {+16}O(n,n) (1973Fo11) and 8079 keV {I8} from {+13}C(|a,n) (1973Ba10). 
WIDTH$ weighted average of 71 keV {I8} from {+13}C(|a,n) (1967Se07) and 85 keV {I9} from {+16}O(n,n) (1973Fo11, 1973Jo01). 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_uncertain: ?
level_comment:
E,J,WIDTH,WIDTHA$From (1973Fo11). See global R-matrix analysis in (1973Jo01). This level was included in (1977Aj02) but was later dropped. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=7.69 From |G{-|a}=4 keV and |G{-n}=48 keV (1973Jo01). See also |G{-|a}/|G=0.077 {I8} (1973Fo11). 
E$From 8199 keV {I8} from {+13}C(|a,n) (1973Ba10), 8192 keV {I10} from {+15}N({+3}He,p) (1972Le01), 8210 keV {I25} from {+12}C({+6}Li,p) (1986Sm10), 8199 keV {I10} from {+16}O(n,|g),(n,n) (1973Fo11) and 8209 keV {I10} from {+16}O(n,n) (1960Ts02). 
WIDTH$From 71 keV {5} from {+13}C(|a,n) (1967Se07), |G=52 keV in {+16}O(n,n) (1973Fo11), and |G{-|a}=4 keV and |G{-n}=48 keV (1973Jo01). In (1977Aj02) and later, the value |G=60 keV was given. 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=10 keV and |G{-|a}=2.2 keV from (1973Jo01), |G{-n}/|G{-|a}=6.7 (1957Wa46) and |G{-|a}/|G=0.44 (1965Ba32). 
E,WIDTH$From {+16}O(n,n) (1980Ci03). See also E{-x}=8350 keV {I4} and |G=9 keV {I3} in {+13}C(|a,n) (1973Ba10,1967Se07). 
J$From {+17}O(e,e') (1987Ma52). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=4.8 and |G{-|a}=0.54 from (1973Jo01), |G{-n}=3.84 keV and |G{-|a}=0.16 keV (1967Se07), |G{-n}/|G{-|a}=19 (1957Wa46) and |G{-|a}/|G=0.08 (1965Ba32). 
E$From {+16}O(n,n) (1980Ci03). See also 8408 keV {I3} from {+13}C(|a,n) (1973Ba10). 
WIDTH$ From {+16}O(n,n) (1980Ci03). See also 5 keV {I2} from {+13}C(|a,n),(|a,|a) (1965Ba32), and 4 keV {I3} from {+13}C(|a,n) (1967Se07). 
J$From {+16}O(n,n) (1973Jo01) 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=small and |G{-|a}=7.6 keV from (1973Jo01), |G{-n}/|G{-|a}=31 (1957Wa46) and |G{-|a}/|G=0.97 (1965Ba32). This is very poor agreement. 
E$From {+16}O(n,n) (1980Ci03). See also 8473 keV {I3} {+13}C(|a,n) (1973Ba10) and other similar values in {+12}C({+6}Li,p),({+7}Li,d). 
WIDTH$From {+16}O(n,n) (1980Ci03). See also 7 keV {I3} in {+13}C(|a,n) (1967Se07) and {+13}C({+6}Li,d) (1978Ar15). 
J$Private communication D.J. Millener (2021). In (1993Ti03) the J{+|p} of this level was listed as 9/2+ with a footnote reading "private communication with D.J. Millener"; however, this message did not convey the intended communication. Prior evaluations confirmed the presence of a J{+|p}=7/2+ state at this energy based on, for example, {+13}C(|a,n) (1957Wa46, 1965Ba52) and {+16}O(n,n) (1973Jo01). Millener had suggested the presence of an additional J{+|p}=9/2+ state in this region based on the {+17}O(e,e') data of (1987Ma52) and {+14}C({+6}Li,t) (1981Cu11, 1983Cu02, 1983Cu04). We accept this interpretation and list a 7/2+ and 9/2+ doublet. 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=3.4 keV and |G{-|a}=1.9 keV from (1973Jo01), |G{-n}= 4.57 keV and |G{-|a}=0.43 keV (1967Se07), |G{-n}/|G{-|a}=2.8 (1957Wa46) and |G{-|a}/|G=0.26 (1965Ba32). 
E$From {+16}O(n,n) (1980Ci03). See also 8507 keV {I12} from {+13}C(|a,n) (1973Ba10) and 8492 keV {I10} {+15}N({+3}He,p) (1972Le01). 
WIDTH$ From {+16}O(n,n) (1980Ci03). See also 5.0 keV {I15} from {+13}C(|a,n),(|a,|a) (1965Ba32) and 5 keV {I3} from {+13}C(|a,n) (1967Se07). 
J$From {+16}O(n,n) (1973Jo01) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=42 keV and |G{-|a}=1.8 keV from (1973Jo01), |G{-n}/|G{-|a}=17 (1957Wa46) and |G{-|a}/|G=0.06 (1965Ba32). 
E$From {+16}O(n,n) (1980Ci03). See also 8702 keV {I12} from {+12}C({+6}Li,p) (1986Sm10) and 8698 keV {I5} from {+13}C(|a,n) (1973Ba10). 
WIDTH$ from {+16}O(n,n) (1980Ci03). See also 50 keV {I3} from {+13}C(|a,n) (1967Se07). 
J$From {+16}O(n,n) (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
WIDTHA$|G{-|a}/|G |? 1 (1965Ba32). 
E$From 8858 keV {I10} {+16}O(n,n) (1960Ts02) 8880 keV {I70} {+14}N(|a,p) (1969Ba17), 8890 keV {I40} {+16}O(|a,{+3}He) 8900 keV {I20} {+17}O(e,e') (1987Ma52) 8900 keV {I10} {+15}N({+3}He,p) (1972Le01). 
WIDTH$From {+13}C({+6}Li,d) (1978Ar15) 
J$From (7/2-) in {+13}C({+6}Li,d) (1978Ar15) and (9/2-) in {+17}O(e,e') (1987Ma52) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$See |G{-n}/|G{-|a}=3.5 (1957Wa46) and |G{-|a}/|G=0.5 (1965Ba32). 
E$From 8905 keV {I8} from {+12}C({+6}Li,p) (1986Sm10), 8890 keV {I30} from {+15}N(|a,d) (1969Lu07) 8896 keV {I8} from {+13}C(|a,n) (1973Ba10). 
J,WIDTH$From {+13}C(|a,n) (1971Ba06,1967Se07). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$|G{-n}/|G=0.894 from |G{-n}=23.5 keV and |G=26.3 keV (1980Ci03). See also |G{-n}=23 keV and |G{-|a}=2.3 keV from (1973Jo01), |G{-n}/|G{-|a}=35 (1957Wa46) and |G{-|a}/|G=0.04 (1965Ba32). 
E$From average of 8970 keV {I4} from {+13}C(|a,n) (1973Ba10) and 8968.5 keV {I16} from {+16}O(n,n) (1980Ci03) 
WIDTH$weighted average of 21 keV {I3} from {+13}C(|a,n) (1967Se07) and 26.3 keV {I19} from {+16}O(n,n) (1980Ci03). 
J$From {+16}O(n,n) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=0.45 (1968Ke02). 
WIDTHG0$From |G{-|a}|G{-|g1}/|G=0.65 eV {I7} (1983Ra29). Using |G{-|a}/|G=0.45 gives |G{-|g1}=1.44 eV {I26} 
E,WIDTH$From {+13}C(|a,n) (1973Ba10, 1967Se07) 
J$From {13}C(|a,|g) (1983Ra29). 
$The lower member of the 9.15 MeV doublet appears to be populated mainly via |g, n and |a reactions on {+17}O, {+16}O and {+13}C, respectively; whilst the higher member is populated via transfer reactions on {+13}C and {+15}N. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
E$From average of 9160 keV {I10} from {+15}N({+3}He,p) (1972Le01) and 9137 keV {I30} from {+15}N(|a,d) (1969Lu07). 
J$From {+15}N(|a,d) 
$See doublet comment on 9146 keV state. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|G{-|a}/|G |? 0.98 from {+13}C(|a,|a{-0}) (1968Ke02); the resonance was not observed in the (|a,n) channel. 
E$From {+12}C({+6}Li,p) (1986Sm10). See also (2008Cr03) 
J,WIDTH$From {+13}C({+6}Li,d) (1978Ar15) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=3.86 keV and |G{-|a}=0.14 keV from (1967Se07), |G{-|a}/|G=0.20 (1968Ke02). 
E,WIDTH$From {+16}O(n,n) (1980Ci03). See also |G=4 keV {I3} from {+13}C(|a,n) (1967Se07). 
J$From {+13}C(|a,n) (1967Se07). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$|G{-|a}/|G=0.85 (1968Ke02) 
E$From 9491 keV 4 {+13}C(|a,n) (1973Ba10), 9487 keV {I8} {+12}C({+6}Li,p) (2008Cr03), and {+15}N({+3}He,p) (1972Le01). 
WIDTH$From {+13}C(|a,n) (1967Se07) 
J$From {+15}N({+3}He,p) (1972Le01). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-|a}/|G=0.70 (1968Ke02). This is rather poor agreement. 
E,WIDTH$From {+16}O(n,n) (1981Ci03) 
J$From {+13}C(|a,n) (1971Ba06) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-|a}/|G=0.90 (1968Ke02). 
E,WIDTH$From {+16}O(n,n) (1981Ci03) 
J$From {+13}C(|a,n) (1971Ba06) 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-n}=3.86 keV and |G{-|a}=0.14 keV (1967Se07). 
E,J,WIDTH$From {+16}O(n,n) (1981Ci03). In (1971Aj02) a single level was indicated at E{-x}=9.88 MeV with J{+|p}=9/2+. In {+13}C(|a,n) (1973Ba10,1977Aj01) a doublet was identified at this energy. Finally, (1981Ci03) resolved the present two states at E{-n}=6076 and 6095 keV (E{-x}=9862 and 9879) with J{+|p}=(5/2-) and (1/2-), respectively. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$|G{-|a}/|G=0.78 (1968Ke02). 
E,WIDTH$From {+13}C(|a,n) (1973Ba10). 
J$From (1971Ba06). See also 7/2+ in {+13}C(|a,n) (1968Ke02) and {+13}C({+6}Li,d) (1978Ar15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_uncertain: ?
level_comment:
$|G{-|a}/|G=0.85 (1968Ke02). 
E,WIDTH$From {+13}C(|a,n) (1968Ke02,1971Ba06) and {+13}C({+6}Li,d) (1978Ar15) 
J$From {+13}C({+6}Li,d) (1978Ar15) 
$Note: between 1971Aj02 and 1977Aj01 this level was dropped without explanation. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
WIDTHN$From (1980Ci03). See also |G{-|a}/|G=0.15 (1968Ke02). 
E,WIDTH$From {+16}O(n,n) (1980Ci03) . See also 50 keV {I3} from {+13}C(|a,n) (1967Se07). 
J$From {+13}C(|a,n),(|a,|a) (1968Ke02) 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_lifetime_unit: KEV
level_comment:
E$From average of 10422.3 keV {I20} {+13}C(|a,n) (1975Be44) and 10419 keV {I3} from {+13}C(|a,|g) (1974Be32) 
WIDTH$From {+13}C(|a,n) (1963Sp02) 
J$From {+13}C(|a,n) (1970Ro08) 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_comment:
WIDTHN0$From (1980Ci03). Note: the {In{-1}} decay channel is open. 
E$From 10558.5 keV {I2} {+13}C(|a,n) (1975Be44) and 10562.6 keV {I6} {+16}O(n,n) (1980Ci03) 
WIDTH$weighted average of 45 keV {I20} from {+13}C(|a,n),(|a,|a), 51 keV {I2} from {+13}C(|a,n), and 42.5 keV {I11} from {+16}O(n,n). 
J$From {+16}O(n,n) (1970Lu16) 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E$From {+12}C({+6}Li,p) (1986Sm10). Note: between 1971Aj02 and 1977Aj01 this level was dropped without explanation. Since then it has been reported in (1986Sm10, 2008Cr03). 
WIDTH$From {+13}C(|a,n),(|a,|a) (1968Ke02) 
J$From {+14}N(|a,p) (1968Ke02) 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_comment:
$|G{-n0}/|G=63.3 from |G{-n0}=26.4 keV 9 and |G=41.7 keV {I14} (1980Ci03) 
E$From average of 10918.9 keV {I13} {+16}O(n,n) (1981Ci03) and 10905 keV {I2} from {+13}C(|a,n) (1975Be44). 
WIDTH$ weighted average of 46 keV {I2} from {+13}C(|a,n) (1975Be44), 60 keV {I20} from {+13}C(|a,n),(|a,|a) (1968Ke02), and 41.7 keV {I14} from {+16}O(n,n) (1980Ci03). 
J$From {+16}O(n,n) (1980Ci03) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$From average of 11036 keV {I2} {+13}C(|a,n) (1975Be44) and 11032 keV {I4} {+15}N({+3}He,p) (1972Le01) 
WIDTH$From {+13}C(|a,n) (1975Be44) 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+18}O({+3}He,|a) (1969De06). 
WIDTHN$Decay branching ratios reported in the literature are |G{-n0}/|G=0.79 {I7} (1980Ci03, 1981Hi01) and |G{-n0}/|G=0.91 {I15} and |G{-n(1+2)}/|G=0.05 {I2} (1973Ad02). In Table 17.11 of (1982Aj01), Fay adopted |G{-n0}/|G=0.81 {I6} and |G{-n(1+2)}/|G=0.05 {I2}, this is accepted. 
WIDTHA0$In (1976Mc11), (|G{-|a0}|G{-n0}){+1/2}/|G=0.23 is reported. Discussion in footnote f of Table 17.11 in (1986Aj04) indicates the above relation is incorrect, but rather (|G{-|a0}|G{-n0})/|G=0.27 keV |+20% is the correct relationship. We note (1986Aj04) used the former relation, while (1993Ti07) accepted the later. We accept (|G{-|a0}|G{-n0})/|G=0.27 keV {I6}. 
WIDTHA0$Using this and |G{-n0}/|G=0.81 {I6}, we find |G{-|a0}=0.33 keV {I8}. Taking this and |G=2.4 keV {I3} gives |G{-|a0}/|G=0.14 {I4}. 
WIDTHA0$The value |G{-|a0}/|G=0.07 {I1} sometimes appears in the literature based on (|G{-|a0}|G{-n0}){+1/2}/|G=0.23 given in (1976Mc11 and an earlier McDonald BAPS talk) and based on |G{-n0}/|G=0.91 {I15} from (1972ad03); this was used by (1972Ad03) along with |G=5.0 keV {I11} (1976Mc11,BAPS) to obtain |G{-|a0}=0.3 keV, but the agreement with the present analysis is purely accidental and by chance. 
WIDTHG1$Subsequently, (|G{-|a0}|G{-|g1})/|G=1.46 eV {I26} is given in (1983Ra29). Using |G{-|a0}/|G=0.14 {I4} gives |G{-|g1}=10.5 eV {I35}. Note: a previous value that agrees by chance |G{-|g1}= 11.6 eV {I18} was obtained in (1983Ra29) using |G{-|a0}=0.3 keV and |G=2.4 keV {I3}. 
E$From {+16}O(n,n) (1980Ci03,1981Hi01). See also 11076 keV {I5} {+13}C(|a,n) (1976Mc11) 11075 keV {I4} {+15}N({+3}He,p) (1972Le01) and 11082 keV {I6} {+18}O({+3}He,|a) (1969De06). 
WIDTH$From {+16}O(n,n) (1980Ci03,1981Hi01). See also 5.0 keV {I11} from {+13}C(|a,n) (1976Mc11, and earlier 1971 BAPS). 
J$From {+18}O(d,t) (1981Ma14) 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: GE3/2
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$From {+16}O(n,n) (1961Fo07, 1959Ha13, 1970Lu16). See also 11410 from {+18}O(d,t) (1977Ma10) and 11578 keV from {+16}O(n,|a) (1963Da12) 
J,WIDTH$From {+16}O(n,n). See also |?126 keV from {+16}O(n,|a) (1963Da12). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
E$From average of 11815 keV {I13} {+12}C({+6}Li,p),({+7}Li,d) (2008Cr03) and 11816 keV {I15} {+13}C(|a,n) (1963Sp02) 
J$From (2008Cr03) 
WIDTH$From {+13}C(|a,n) (1963Sp02) 


level_energy_unit: KEV
level_spin_parity: GE3/2
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_uncertain: ?
level_comment:
E,WIDTH$From {+17}O(e,e') (1977No06) 
J$From {+16}O(n,n) (1961Fo07). See also discussion on E{-x}=12007 keV. 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,J,WIDTH$From {+12}C({+6}Li,p)({+7}Li,d) (1986Sm10,2008Cr03), and {+13}C(|a,n) (1963Sp02). 
$In previous reviews, a broad state bear 12.0 MeV was listed. In the present evaluation, we find evidence for a broad state near 11.95 MeV and a narrow state at 12007 keV 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+18}O(d,t) (1977Ma10). 
E$From average of 12109 keV {I20} {+13}C(|a,n) (1963Sp02) and 12120 keV {I10} {+18}O(d,t) (1977Ma10) 
WIDTH$From {+13}C(|a,n) (1963Sp02) 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E$From average of 12220 keV {I20} {+17}O(e,e') (1987Ma52), 12239 keV {I16} {+12}C({+6}Li,p) (1986Sm10,2008Cr03), 12220 keV {I26} {+12}C({+7}Li,d) (2008Cr03). 
J$From {+12}C({+6}Li,p),({+7}Li,d) (2008Cr03) 
WIDTH$From {+17}O(e,e') (1987Ma52) 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From average of 12428 keV {I13} {+12}C({+6}Li,p) (1986Sm10, 2008Cr03), 12420 keV {I26} {+12}C({+7}Li,d) (2008Cr03) and 12421 keV {I15} {+13}C(|a,n) (1963Sp02) 
J,WIDTH$From {+12}C({+6}Li,p),({+7}Li,d) (1986Sm10) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+18}O({+3}He,t) (1969De06), {+18}O(d,t) (1981Ma14) {+16}O(n,n) (1976Mc11, 1981Hi01). 
WIDTHN0$from (1980Ci03) 
E,WIDTH$From {+16}O(n,n) (1980Ci03,1981Hi01). See also 12458 keV {I5} in {+13}C(|a,n) (1976Mc11) and 12471 keV {I5} in {+18}O({+3}He,|a) (1969De06) 
WIDTH$weighted average of 8 keV {I2} from {+13}C(|a,n) and 6.9 keV {I11} from {+16}O(n,n). 
J$From {+13}C(|a,n) (1976Mc11) 


level_energy_unit: KEV
level_spin_parity: (3/2-,9/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E,J,WIDTH$From {+13}C(|a,n) (1969Sp02,1970Ro08). See also 12660 keV {I50} {+17}O(e,e') (1977No06) 
WIDTH$Beginning in (1971Aj02) the |G for this level was listed at |?5 keV attributed to {+13}C(|a,n) (1969Sp02). However this was a typo. (1969Sp02) report |?75 keV. Also see |?90 keV {+17}O(e,e') and |?95 keV in {+16}O(n,n). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
ISPIN$From {+18}O(d,t) (1977Ma10) 
E$From {+12}C({+6}Li,p),({+7}Li,d) (2008Cr03), where it is best resolved. See also 12760 keV {I10} from {+18}O(d,t) (1977Ma10: uncertainties seem underestimated) and 12813 keV {I25} from {+13}C(|a,n) (1963Sp02: the peak is poorly resolved). 
WIDTH$From {+12}C({+6}Li,p),({+7}Li,d) (2008Cr03) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+13}C(|a,n) (1976Mc11), {+18}O({+3}He,|a) (1969De06), {+16}O(n,n) (1981Hi01). 
WIDTHN0$from (1981Hi01) 
E$From 12964 keV {I6} {+16}O(n,n) (1981Hi01) 12944 keV {I6} {+13}(|a,n) (1976Mc11) 12950 keV {I8} {+18}O({+3}He,|a) (1969De06). 
J$From {+18}O(d,t), {+18}O({+3}He,|a). 
WIDTH$From {+16}O(n,n) (1976Mc11) 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+13}C(|a,n) (1976Mc11) and {+18}O({+3}He,|a) (1969De06). 
WIDTHN0$from (1981Hi01) 
E,J,WIDTH$From {+16}O(n,n) (1976Mc11,1980Ci03,1981Hi01). Others 12993 keV {I6} {+13}C(|a,n) and 12994 {I8} {+18}O({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_comment:
E$From weighted average of 13070 keV {I26} {+12}C({+6}Li,p) (2008Cr03), 13060 keV {I26} {+12}C({+7}Li,d) (2008Cr03) and 13077 keV {I15} {+13}C(|a,n) (1963Sp02). 
WIDTH$From {+13}C(|a,n) (1963Sp02). 
J$From {+17}O(|g,n) (1985Ju02) 


level_energy_unit: KEV
level_spin_parity: (11/2-,13/2-)
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From {+17}O(e,e') (1987Ma52) 
J$The J{+|p}=11/2-,13/2- interfering doublet at 13.6 MeV is discussed in (1987Ca30). In {+13}C({+6}Li,d) (1978Ar15) E{-x}=13580 keV {I20}, J{+|p}=(13/2-) and a broader |?200 keV width are preferred. On the other hand in {+17}O(e,e') (1987Ma52) the same E{-x} is found with a narrower |G=68 keV and a preference of (11/2-). With no substantially new results, we maintain the interpretation of (1993Ti07) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+16}O(n,n) (1981Hi01), {+18}O({+3}He,|a) (1969De06), {+18}O(d,t) (1981Ma14). 
WIDTHN0$From (1981Hi01) 
E$From 13641.9 keV {I24} (1981Hi01). See also 13640 keV {I5} {+18}O({+3}He,|a) (1969De06) 
WIDTH$From {+16}O(n,n) (1981Hi01) 
J$From {+14}C({+6}Li,t) (1981Cu11,1983Cu02,1983Cu04), {+18}O(d,t) (1981Ma14) 


level_energy_unit: KEV
level_spin_parity: (9/2+,11/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E,J,WIDTH$from {+13}C({+6}Li,d) (1978Ar15). 
WIDTH$from |G=200 keV (1978Ar15) and |G|?100 keV {+17}O(e,e') (1977No06) 
J$(11/2+) is slightly preferred. 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+16}O(n,n) (1981Hi01), {+18}O({+3}He,|a) (1969De06). 
WIDTHN0$From (1981Hi01) 
E,WIDTH$From {+16}O(n,n) (1981Hi01). See also 14219 keV {I8} in {+18}O({+3}He,|a) (1969De06) 
J$From {+17}O(e,e'). See also (7/2-) in {+16}O(n,n). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From {+16}O(n,n) (1981Hi01). See also 14282 keV {I12} {+18}O({+3}He,|a) (1969De06) 
ISPIN$From {+16}O(n,n) (1981Hi01) and {+18}O({+3}He,|a) (1969De06). In (1990Mc06), T=1/2 is assigned based on {+17}O(|g(14380 keV),n{-0}), but those results appear uncertain because of persistent energy calibration issues. 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+17}O(e,e') (1983Ra27). 
E,J,WIDTH$From {+17}O(e,e') (1987Ma52). See also 14720 keV {I26} {+12}C({+7}Li,d) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$From {+17}O(e,e') (1977No06) 
WIDTH$From {+16}O(n,n) (1961Fo07) 
J$From {+14}C({+6}Li,t), see (1981Cu11,1983Cu02,1983Cu04) 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_comment:
E$From {+12}C({+6}Li,p)({+7}Li,d) (2008Cr03) 
J$From {+14}N({+6}Li,{+3}He) (1984Et01) 
WIDTH$Narrow, see (2008Cr03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E,WIDTH$From 14967 keV and |G|?180 keV {+16}O(n,n) (1961Fo07) and 14981 keV and |G|?100 keV {+15}N(d,|a) (1966Ti03) 


level_energy_unit: KEV
level_spin_parity: (9/2+,11/2+)
level_lifetime_unit: MEV
level_comment:
E,J,WIDTH$From (1978Ar15). 11/2+ is preferred in (1978Ar15). See also (5/2-,7/2-) in (1966Ti03) {+15}N(d,|a) 


level_energy_unit: KEV
level_comment:
ISPIN$From {+18}O({+3}He,|a) (1969De06). 
E$From 15070 keV {I26} {+12}C({+7}Li,d) (2008Cr03) and 15101 keV {I8} {+18}O({+3}He,|a) (1969De06). 
WIDTH$narrow; see {+17}O(e,e') (1983Ra27). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+16}O(n,n) (1981Hi01). In (1990Mc06), T=1/2 is assigned, but those results appear uncertain because of persistent energy calibration issues. 
E,WIDTH$From (1981Hi01) 
J$From {+17}O(e,e') (1983Ra27), {+14}C({+6}Li,t) (1981Cu11,1983Cu02,1983Cu04) and {+16}O(n,n') (1981Hi01). See also (5/2-,7/2-) for a broad level at 15.15 MeV reported in {+15}N(d,|a) (1966Ti03). 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From average of 15780 keV {I20} {+16}O(e,e') (1986Ma48) and 15800 keV {I26} {+12}C({+7}Li,d) (2008Cr03) 
WIDTH$From (1986Ma48) 
J,ISPIN$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). The state was initially identified in {+17}O(e,e') (1986Ma48) as (9/2-; T=3/2). 


level_energy_unit: KEV
level_spin_parity: (9/2+,11/2+)
level_lifetime_unit: MEV
level_comment:
E,J,WIDTH$From (1978Ar15). 9/2+ is preferred. See also |?15.8 MeV and |G|?300 keV (1976Ca28). 
$(1990Mc06) suggest a broad T=1/2 state in {+17}O(|g,n) around E{-x}=15.6 MeV. It may be this state? 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+16}O(n,n) (1981Hi01). 
E,WIDTH$From (1981Hi01) {+16}O(n,n),(n,n). See also 16.50 MeV {I2} and |< 20 keV from {+17}O(e,e') (1986Ma48). 
J$From (1981Cu11,1983Cu02,1983Cu04) {+14}C({+6}Li,t). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
ISPIN$From {+18}O(d,t) (1977Ma10, 1981Ma14) 
E$From 16.52 MeV {I5} {+17}O(e,e') (1977No06) and 16580 keV {I10} (1977Ma10). 
J$ From {+18}O(d,t) (1981Ma14) 
WIDTH$From {+17}O(e,e') (1977No06) 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,WIDTH$From {+17}O(e,e') (1986Ma48) 
J,ISPIN$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). The state was initially identified in {+17}O(e,e') (1986Ma48) as (7/2-; T=3/2). Also see (7/2-) in {+16}O(p,|p+) (1988Hu02)and ((11/2- preferred),13/2-) in {+13}C({+6}Li,d) (1978Ar15). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From 18122 keV {I4} {+16}O(n,n) (1981Hi01). See also 18140 keV {I10} {+18}O(d,t) (1977Ma10) and 18.09 MeV {I7} {+17}O(|g,p) (1992Zu01) 
J$From {+18}O(d,t) (1981Ma14). 
ISPIN$From {+18}O(d,t) (1977Ma10, 1981Ma14), {+16}O(n,n) (1981Hi01). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From {+17}O(e,e') (1986Ma48). Also see 18.5 MeV (1990Mc06) from reanalysis of 19.0 MeV in {+17}O(|g,n) (1979Jo05) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
WIDTHG$From (1980Li05) 
E,WIDTH$From 19760 keV {I60} {+14}N(t,|g) (1980Li05) and 19850 keV {I40} {+17}O(e,e') (1986Ma48). |G from 0.55 MeV {I5} from (1980Li05) and 0.53 MeV {I15} from (1986Ma48). 
J$From (1980Li05). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: KEV
level_comment:
E,WIDTH$From {+17}O(e,e') (1986Ma48). 
J,ISPIN$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). The state was initially identified in {+17}O(e,e') (1986Ma48) as (13/2-; T=1/2). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_lifetime_unit: KEV
level_comment:
WIDTHG1$From (1980Li05) 
E,WIDTH$From {+14}N(t,|g) (1980Li05), see also 20.33 MeV {I7} (1992Zu01) 
J$5/2- from (1980Li05); E1 to {+17}O(0:5/2+). See also (7/2-) in {+17}O(|g,p) (1992Zu01) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
ISPIN$From {+16}O(n,n) (1970Bo30). 
WIDTHG1$From (1980Li05) 
WIDTHN$|G{-n}|?|G {+16}O(n,n) (1970Bo30) 
E,J,WIDTH$ from {+14}N(t,|g) (1980Li05). M1 to {+17}O(871:1/2+) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,WIDTH$From {+17}O(e,e') (1986Ma48). 
J,ISPIN$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). The state was initially identified in {+17}O(e,e') (1986Ma48) as (11/2-; T=3/2). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_comment:
E,J,WIDTH$From {+14}N(t,|g) (1980Li05). E1 to {+17}O(0:5/2+, 871:1/2+); see also 7/2- from {+17}O(|g,n/p) 
WIDTHG$From (1980Li05) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$C{+2}S=0.30 
E$See also 6862 keV {I13} (2008Cr03). 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+2},1d{-5/2}{+3}-(3p-2h) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$C{+2}S=0.25 
E$from (2008Cr03). 
E$See also doublet 7580 keV {I16} (1986Sm10). 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+2},1d{-5/2}{+3}-(3p-2h) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$C{+2}S=0.81 
E$weighted average of 8476 keV {I12} (1986Sm10) and 8470 keV {I13} (2008Cr03). 
E$See also 8.46 MeV (1968Me10) which is suspected to be the 7/2+ member of a k=1/2+ rotational band starting at the 6.37 MeV 1/2+ level in {+17}O. 
$Configuration={+12}C g.s.+ 1p{-1/2}{+2},1d{-5/2}{+3}-(3p-2h) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$C{+2}S=0.23 
E$from (2008Cr03). 
E$See also 11815 keV {I20} (1986Sm10). 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+0},1d{-5/2}{+5}-(5p-4h) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$C{+2}S=0.28 
E$weighted average of 12020 keV {I20} (1986Sm10) and 12000 keV {I26} (2008Cr03). 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+0},1d{-5/2}{+5}-(5p-4h) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$C{+2}S=1.32 
E$weighted average of 12250 keV {I20} (1986Sm10) and 12220 keV {I26} (2008Cr03). 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+3},1d{-5/2}{+2}-(2p-1h) (2008Cr03). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$C{+2}S=0.20 
E$weighted average of 12430 keV {I15} (1986Sm10) and 12420 keV {I26} (2008Cr03). 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+0},1d{-5/2}{+5}-(5p-4h) (2008Cr03). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$from (2008Cr03). 
WIDTH$Estimated based on the FWHM of the peak in the {+12}C({+7}Li,d) reaction (2008Cr03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_comment:
$|G|?83 keV {I+9-12}, |G|?|G{-n} (2012La29). 
$ANC{+2}=6.7 fm{+-1} {I+9-6} (2012La29). 
$The results of (2003Ka51,2003Ku03,2003Ku36) indicate S{-|a}(6.356)/S{-|a}(3.055)=0.044. 
$See also S{-|a}=0.36-0.40 for N=4 (2003Ke10: calculated values in Table 3). 


level_energy_unit: KEV
level_spin_parity: (11/2-,13/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
WIDTH$From (1978Ar15) 
E$See also 13.6 MeV {I1} (1978Ar15). 
J$13/2- is preferred in (1978Ar15) based on expected systematics. 


level_energy_unit: KEV
level_spin_parity: (9/2+,11/2+)
level_lifetime_unit: MEV
level_comment:
E$15.0 MeV {I1} at E({+6}Li)=26 MeV, 15.15 MeV {I15} at E({+6}Li)=29 MeV. 
WIDTH$0.37 MeV {I15} at E({+6}Li)=26 MeV, 0.40 MeV {I15} at E({+6}Li)=29 MeV. 
J$11/2+ is preferred in (1978Ar15) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
$C{+2}S=8.8 
$Unresolved. 
S$10.5 for set II. 
$For 14.76-MeV; J{+|p}=9/2- state: C{+2}S=4.3|*10{+3} for set I and 4.0|*10{+3} for set II. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E$See also 11.075 MeV {I5} (Barnes et al., Proc. Intern. Conf. on Nucl. Phys., Gatlinburg, Tennessee, 12-17 Sept. 1966 (Academic, New York, 1967) p.884: {+15}N({+3}He,p)). 
J,ISPIN$See also (1973Ad02). 
T$A variety of widths and branching ratios from (1973Ad02) became associated with this reaction and level, but the width |G= 5 keV {I1} from McDonald et al., Bull. Amer. Phys. Soc. 16, 489 (1971) is from {+13}C(|a,n) and later published in (1966Mc11). The branching ratios and partial widths from (1973Ad02) are are discussed in {+18}O({+3}He,|a). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_comment:
E$See also 7.6 MeV {I2} (1962Ha40). 
$Dominant configuration: (d{-5/2}){+2}{-5}p{-1/2}{+-1}. See also (1966Ri04). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
E$See also 9.0 MeV {I2} (1962Ha40). 
$Dominant configuration: (d{-5/2}){+2}{-5}p{-1/2}{+-1}. See also (1966Ri04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
L$See also (1961Ar06,1963Ro12). 
$Spectroscopic factor (DWBA) S(1/2+)=0.29 {I5} (1978Fo05). The ratio of S(1/2+)/S(5/2+)=0.195 {I15} which is in disagreement with the theoretical value of 0.267 (1976La13). 


level_energy_unit: KEV
level_spin_parity: (1/2)-
level_lifetime_unit: KEV
level_comment:
WIDTH$from (McDonald et al., Bull. Amer. Phys. Soc. 16, 489 (1971) {+13}C(|a,n))). See also <20 keV (D.C. Hensly, Ph.D. thesis, Caltech (1969) unpublished). 
$|G{-n0}/|G=91 {I15} and |G{-n(1+2)}/|G=0.05 {I2} were deduced in (1973Ad02). Also |q{+2}(g.s.)/|q{+2}(6.13)=0.31 {I14} (1973Ad02); these compare with |q{+2}(g.s.)/|q{+2}(6.05)=3.4 {I14} and |q{+2}(g.s.)/|q{+2}(6.13)=0.32 {I14} (1970Mc02). 
$The value |G{-|a0}=0.3 keV is deduced using the measured (1973Ad02) neutron branching ratios and the width from McDonald; however in the present evaluation we adopt a different |G=2.4 keV {I3} and |G{-n0}/|G=81 {I6}. This changes the interpretation. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$C{+2}S=0.7 {I2} 
E$The authors deduced a {+17}O mass excess that differs by 5 keV {I2} when compared with (2017Wa10); this implies an unaccountable systematic error. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$ANC{+2}=3.6 fm{+-1} {I7} is deduced by (2015Av02). See also ANC{+2}=0.89 fm{+-1} {I23} (2006Jo11). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2,13/2)
level_comment:
E,J$Analysis of the angular distributions in (1987Ca30) concluded this peak corresponds to an unresolved doublet with (11/2,13/2). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2,11/2)
level_comment:
E,J$Analysis of the angular distributions in (1987Ca30) concluded this peak corresponds to an unresolved doublet with (7/2,11/2). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$ strongest population of this state is consistent with configuration={+16}O (6+,16.29 MeV)~#p{-1/2} in a weak coupling scheme 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$|t{-m}=253 ps {I6} 
$The Q(|b{+-})value for neutron transfer to this state is 1.61 MeV (1977Sw05). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$C{+2}S=0.53 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+2},1d{-5/2}{+3}-(3p-2h) 
E$See also 6.87-MeV:J{+|p}=7/2 (1971Sc21). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$C{+2}S=0.59 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+2},1d{-5/2}{+3}-(3p-2h) 
E$See also 7.56-MeV:J{+|p}=9/2 (1971Sc21). 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_comment:
$C{+2}S=1.06 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+2},1d{-5/2}{+3}-(3p-2h) 
E$See also triplet 8.40-MeV:J{+|p}=5/2, 8.47-MeV:J{+|p}=9/2 and 8.50-MeV:J{+|p}=5/2 (1971Sc21). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$triplet. See also triplet 8.87-MeV:J{+|p}=3/2, 8.88-MeV:J{+|p}=7/2 and 8.95-MeV:J{+|p}=7/2 (1971Sc21). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_comment:
$C{+2}S=0.96 
$Configuration={+12}C{-g.s.}+1p{-1/2}{+0},1d{-5/2}{+5}-(5p-4h) 
E$See also 11.88-MeV (1971Sc21). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$measured. May correspond to the known levels of {+17}O*(7.29-MeV:J{+|p}=3/2+ and 7.38-MeV:J{+|p}=5/2+)) (1975Ve10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=2233 
E$from E{-|a}=2233 keV. 
WIDTH$from |G{-lab}=110 keV with |G{-|a}/|G=0.05. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2663 
E$from E{-|a}=2663 keV. 
WIDTH$from |G{-lab}=7 keV {I2} with |G{-|a}/|G=0.08. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2800 
E$from E{-|a}=2800 keV. 
WIDTH$from |G{-lab}=6.7 keV {I20} with |G{-|a}/|G=0.26. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=3290 
E$from E{-|a}=3290 keV. 
WIDTH$from |G{-lab}=130 keV with |G{-|a}/|G=0.50. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=3305 
E$from E{-|a}=3305 keV; not observed in {+13}C(|a,n). 
WIDTH$from |G{-lab}=8 keV with |G{-|a}/|G=1.00. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=3690 
E$from E{-|a}=3690 keV; observed via {+13}C(|a,|a{-0}) only. 
WIDTH$See also |G{-|a}/|G=0.98 (1968Ke02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=4420 
E$from E{-|a}=4420 keV. This level is associated with E{-x}=9786 keV in adopted levels. 
WIDTH$See also |G{-|a}/|G=0.90 (1968Ke02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=4580 
E$from E{-|a}=4580 keV. 
WIDTH$See also |G{-|a}/|G=0.18 (1968Ke02). 
J$A doublet was populated and identified as J{+|p}=9/2+. Two levels were subsequently identified with (5/2-) and (1/2-). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=4700 
E$from E{-|a}=4700 keV. 
WIDTH$See also |G{-|a}/|G=0.78 (1968Ke02). 
J$Associated with 9976 keV: 5/2+ level in adopted levels. 


level_energy_unit: KEV
level_comment:
$E{-|a}(res) (keV)=656.0 {I7} 
E$from E{-|a}=656.0 keV {I7} (1993Br17). 
$(|w|g){-n}=1.85|*10{+-4} eV {I20}, (|w|g){-|g}<5 |meV (1993Br17). 


level_energy_unit: KEV
level_comment:
$E{-|a}(res) (keV)=802.2 {I8} 
E$from E{-|a}=802.2 keV {I8} (1993Br17). 
$(|w|g){-n}=4.54|*10{+-4} eV {I35}, (|w|g){-|g}<8 |meV (1993Br17). 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=1056.3 {I15} 
E$from E{-|a}=1056.3 keV {I15} (1973Ba10). See also E{-|a}(keV)=1056 (1976Ra36), 1054 (2005Ha69). 
WIDTH$See also |G=5 keV (1957Wa46), |G{-n}/|G{-|a}=(1300) (1957Wa46). 
$|w|g=12.1 eV {I6} (2005Ha69), 11.9 eV {I6} (Deduced from the resonance yield, 4434|+135 n/|mC (1992Br05, 1973Ba10), and the stopping power in {+13}C (Ziegler, The Stopping and Range of Ions in Matter, Vol. 3 (1977)); see (1993Br17)). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$authors (2008Pe09) listed the value from (1993Ti07). Involvement in {+13}C(|a,n) is suggested from its population in {+13}C({+7}Li,t). 
WIDTH$|G{-n}=400 keV, |G{-|a}=0.09 keV (2008Pe09) which is consistent with (1966Li03: |G{-n}/|G>0.99 in {+16}O+n measurement). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=1336.7 {I15} 
E$from E{-|a}=1336.7 keV {I15} (1973Ba10). See also E{-|a}=1336 keV (2005Ha69). 
WIDTH$See also |G(keV)=3 (1969Sc04), |<4 (1957Wa46), |G{-n}/|G{-|a}=(450) (1957Wa46). 
$|w|g=33.3 eV {I18} (2005Ha69). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E{-|a}(res) (keV)=1587.9 {I25} 
E$from E{-|a}=1587.9 keV {I21}, which is the average of (1973Ba10: 1590 keV {I2}) and (1993Br17: 1585.7 keV {I15}). See also E{-|a}=1590 keV (2005Ha69). 
WIDTH$See also |G(keV)=3 (1969Sc04), |<4 (1957Wa46). 
$|w|g=10.8 eV {I5} (1993Br17), 11.5 eV {I12} (2005Ha69). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E{-|a}(res) (keV)=1745 {I6} 
E$from E{-|a}=1745 keV {I6} (1973Ba10). 
WIDTH$See also |G=22 keV (1957Wa46,1969Sc04). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2083 {I8} 
E$from E{-|a}=2083 keV {I8} (1973Ba10). See also E{-|a}(keV)=2090 (1956Bo61), 2080 (1967Se07), 2075 (1973Bu14). 
E$triplet (1957Wa46). 
WIDTH$See also |G(keV)=75 (1973Ba10), 110 (1957Wa46,1969Sc04), |G(lab)=100 keV (1956Bo61), |G{-n}/|G{-|a}=10 (1957Wa46). 
J$See also (1973Bu14). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2250 {I8} 
E$from E{-a}=2250 keV {I8} (1973Ba10). See also E{-|a}(keV)=2250 (1956Bo61,1967Se07), 2240 (1963Bu14). 
WIDTH$See also |G(keV)=70 (1957Wa46, 1969Sc04), 110 (1973Ba10), |G(lab)=100 keV (1956Bo61), |G{-n}/|G{-|a}=10 (1957Wa46). 
J$See also (1973Bu14) who suggest the |p is ambiguous. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2407 {I8} 
E$from 2407 keV {I8} (1973Ba10). See also E{-|a}(keV)=2410 (1967Se07), 2420 (1956Bo61), 2430 (1973Bu14), 2440 (1954Tr09). 
WIDTH$See also |G(keV)=60 (1957Wa46,1969Sc04), 70 (1973Ba10), |G(lab)=80 keV (1956Bo61), |G{-n}/|G{-|a}=13 (1957Wa46). 
J$See also (1973Bu14) who suggest the |p is ambiguous. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2604 {I4} 
E$from E{-|a}=2604 keV {I4} (1973Ba10). See also E{-|a}(keV)=2610 (1967Se07), 2605 (1956Bo61), E{-n}=4440 keV (1956Be98: Fig. 5 top). 
WIDTH$See also |G(keV)=18 (1957Wa46,1969Sc04), 15 (1973Ba10), |G(lab)|<6 keV (1956Bo61), |G{-n}/|G{-|a}=6.7 (1957Wa46). 
J$See also (1973Bu14) who suggest the |p is ambiguous. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2680 {I3} 
E$from E{-|a}=2680 keV {I3} (1973Ba10). See also E{-|a}(keV)=2680 (1967Se07), 2660 (1954Tr09), 2690 (1956Bo61), E{-n}=4530 keV (1956Be98: Fig. 5 top). 
WIDTH$See also |G(keV)=8 (1973Ba10), 11 (1957Wa46), |G(lab)=10 keV (1956Bo61), |G{-n}=3.84 keV and |G{-|a}=0.16 keV (1967Se07), |G{-n}/|G{-|a}=19 (1957Wa46). 


level_energy_unit: KEV
level_spin_parity: 7/2
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2765 {I3} 
E$from E{-|a}=2765 keV {I3} (1973Ba10). See also E{-|a}(keV)=2770 (1967Se07), 2775 (1956Bo61), 2760 (1954Tr09), E{-n}=4590 keV (1956Be98: Fig. 5 top). 
E$doublet (1957Wa46). 
WIDTH$See also |G(keV)=8 (1973Ba10), 9 (1957Wa46), |G(lab)=10 keV (1956Bo61), |G{-n}/|G{-|a}=31 (1957Wa46). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2-)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=2809 {I3} 
E$from E{-|a}=2809 keV {I3} (1973Ba10). See also E{-|a}(keV)=2810 (1967Se07), 2825 (1956Bo61), E{-n}=4630 keV (1956Be98: Fig. 5 top). 
WIDTH$See also |G(keV)=6 (1973Ba10), 11 (1957Wa46), |G(lab)|<7 keV (1956Bo61), |G{-n}=4.57 keV and |G{-|a}=0.43 keV (1967Se07), |G{-n}/|G{-|a}=2.8 (1957Wa46). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=3059 {I5} 
E$from E{-|a}=3059 keV {I5} (1973Ba10). See also E{-|a}(keV)=3070 (1967Se07), 3090 (1956Bo61), 3100 (1971Ba06), E{-n}=4850 keV (1956Be98: Fig. 5 top). 
E$triplet (1957Wa46). 
WIDTH$See also |G(keV)=50 (1973Ba10), 85 (1957Wa46), |G(lab)=90 keV (1956Bo61), |G{-n}/|G{-|a}=17 (1957Wa46). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=3318 {I8} 
E$from E{-|a}=3318 keV {I8} (1973Ba10). See also E{-|a}(keV)=3320 (1967Se07), 3300 (1954Tr09), 3330 (1956Bo61), 3360 (1971Ba06), E{-n}=5080 keV (1956Be98: Fig. 5 top). 
WIDTH$See also |G(keV)=115 (1973Ba10), 110 (1957Wa46), |G(lab)=150 keV (1956Bo61), |G{-n}/|G{-|a}=3.5 (1957Wa46). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=3415 {I4} 
E$from E{-|a}=3415 keV {I4} (1973Ba10). See also E{-|a}(keV)=3420 (1956Bo61, 1967Se07,1971Ba06), E{-n}=5130 keV (1956Be98: Fig. 5 top). 
WIDTH$See also |G(keV)=14 (1973Ba10), 35 (1957Wa46). |G(lab)=30 keV (1956Bo61), |G{-n}/|G{-|a}=35 (1957Wa46). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=3645 {I4} 
E$from E{-|a}=3645 keV {I4} (1973Ba10). See also E{-|a}(keV)=3650 (1967Se07), 3670 (1956Bo61), 3640 (1971Ba06). 
WIDTH$See also |G=9 keV (1973Ba10), |G(lab)|<8 keV (1956Bo61) 


level_energy_unit: KEV
level_spin_parity: 5/2
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=3714 {I4} 
E$from E{-|a}=3714 keV {I4} (1973Ba10). See also E{-|a}(keV)=3720 (1967Se07,1971Ba06), 3730 (1956Bo61), E{-n}=5380 keV (1956Be98: Fig. 5 top). 
WIDTH$See also |G=8 keV (1973Ba10), |G(lab)|<5 keV (1956Bo61), |G{-n}=3.86 keV and |G{-|a}=0.14 keV (1967Se07). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=4096 {I4} 
E$from E{-|a}=4096 keV {I4} (1973Ba10). See also E{-|a}(keV)=4120 (1967Se07), 4125 (1956Bo61), 4110 (1971Ba06). 
WIDTH$See also |G=16 keV (1973Ba10), |G(lab)=15 keV (1956Bo61). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=4394 {I5} 
E$from E{-|a}=4394 keV {I5} (1973Ba10). See also E{-|a}=4380 keV (1971Ba06). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=4420 
E$from E{-|a}=4420 keV (1956Bo61,1967Se07,1971Ba06), This level is associated with E{-x}=9786 keV in adopted levels. 
WIDTH$See also |G(lab)=25 keV (1956Bo61). 
$It appears this level is not real. No single experiment reports more than two of the three levels at 9.72, 9.74 and 9.77 MeV. The energies of these levels are better resolved in {+16}O(n,n) (1980Ce03). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_uncertain: ?
level_comment:
$E{-|a}(res) (keV)=4465 {I15} 
E$from E{-|a}=4465 keV {I15} (1973Ba10). See also E{-|a}(keV)=4500 (1956Bo61), (4490) (1967Se07). 
WIDTH$See also |G(lab)=70 keV (1956Bo61). 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=4583 {I5} 
E$from E{-|a}=4583 keV {I5} (1973Ba10). See also E{-|a}=4580 keV (1971Ba06). 


level_energy_unit: KEV
level_spin_parity: 9/2
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=4600 {I15} 
E$from E{-|a}=4600 keV {i15} (1973Ba10). See also E{-|a}(keV)=4620 (1967Se07), 4630 (1956Bo61). 
WIDTH$See also |G(keV)|?10 (1973Ba10), |G(lab)=15 keV (1956Bo61), |G{-n}=4.7 keV and |G{-|a}=0.3 keV (1967Se07). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$E{-|a}(res) (keV)=4730 {I20} 
E$from E{-|a}=4730 keV {I20} (1973Ba10). See also E{-|a}(keV)=4750 (1956Bo61), 4700 (1971Ba06), (4770) (1967Se07). 
WIDTH$See also |G(lab)=200 keV (1956Bo61). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$E{-|a}(res) (keV)=4820 {I20} 
E$from E{-|a}=4820 keV {I20} (1973Ba10). See also E{-|a}=(4850) keV (1967Se07). 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2-)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=4993 {I5} 
E$from E{-|a}=4993 keV {I5} (1973Ba10). See also E{-|a}(keV)=4980 (1971Ba06), 4995 (1970Ro08), 5040 (1967Se07), 5050 (1956Bo61). 
WIDTH$See als 45 keV (1973Ba10), |G(lab)=65 keV (1956Bo61). 


level_energy_unit: KEV
level_spin_parity: (5/2+,7/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-|a}(res) (keV)=5200 {I15} 
E$from E{-|a}=5200 keV {I15} (1973Ba10). See also E{-|a}=5185 keV (1970Ro08). 


level_energy_unit: KEV
level_spin_parity: (5/2-,7/2-)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=5314.0 {I25} 
E$from E{-|a}=5314.0 keV {I25} (1975Be44). See also E{-|a}(keV)=5317 {I10} (1963Sp02), 5325 {I10} (1973Ba10), 5290 (1967Se07), 5370 (1970Ro08). 
WIDTH$See also |G(keV)=11 {I9} (1975Be44), 23 keV (1973Ba10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+,7/2-)
level_comment:
$E{-|a}(res) (keV)=5413 
E$from E{-|a}=5413 keV, which is the average of (1967Se07: 5410 keV) and (1970Ro08: 5415 keV). 


level_energy_unit: KEV
level_spin_parity: (7/2-,9/2+)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=5492.0 {I25} 
E$from E{-|a}=5492.0 keV {I25} (1975Be44). See also E{-|a}(keV)=5496 {I10} (1963Sp02), 5540 (1970Ro08). 
WIDTH$See also |G=50 keV {I20} (1963Sp02). 


level_energy_unit: KEV
level_spin_parity: (1/2+,7/2-)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=5779.0 {I25} 
E$from E{-|a}=5779.0 keV {I25} (1975Be44). See also E{-|a}(keV)=5771 {I10} (1963Sp02), 5790 (1970Ro08). 
WIDTH$See also |G=85 keV {I30} (1963Sp02). 


level_energy_unit: KEV
level_spin_parity: (5/2)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=5945 {I3} 
E$from E{-|a}=5945 keV {I3} (1975Be44). See also E{-|a}(keV)=5945 {I10} (1963Sp02), 5995 (1970Ro08). 
WIDTH$See also |G=55 keV {I20} (1963Sp02). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=6117 {I3} 
E$from E{-|a}=6117 keV {I3} (1975Be44). See also E{-|a}=6107 keV {I10} (1963Sp02). 
WIDTH$See also |G=45 keV {I10} (1963Sp02). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=6169 
E$from E{-|a}=6169 keV which is calculated from the E{-x} given in (1976Mc11); see also E{-|a}=6220 keV (1970Ro08). 
J$See also (3/2-,7/2+) (1970Ro08). 
WIDTH$From (1976Mc11). A preliminary result, 5 keV {I1}, from a BAPS was picked up by (1973Ad02: {+18}O({+3}He,|a) and used to derive various partial widths. See also (|G{-|a0}|G{-n0}){+1/2}/|G{-tot}=0.23 (1976Mc11) which corresponds to |G{-|a0}/|G=0.06 {I2} when combined with the value |G{-n0}/|G=0.91 {I15} (1973Ad02). 


level_energy_unit: KEV
level_spin_parity: (3/2-,7/2+)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=6380 {I3} 
E$from E{-|a}=6380 keV {I3} (1975Be44). See also E{-|a}(keV)=6367 {I10} (1963Sp02), 6480 (1970Ro08). 
WIDTH$See also |G=100 keV {I30} (1963Sp02). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=6883 {I3} 
E$from E{-|a}=6883 keV {I3} (1975Be44). See also E{-|a}=6878 keV {I10} (1963Sp02). 
WIDTH$See also |G=120 keV {I30} (1963Sp02). 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=7136 {I15} 
E$from E{-|a}=7136 keV {I15} (1963Sp02). See also E{-|a}=7160 keV (1970Ro08). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=7976 
E$from E{-|a}=7976 keV which is calculated from the E{-x} given in (1976Mc11). See also E{-|a}=8000 keV (1970Ro08). 
J$See also (3/2-,9/2+) (1970Ro08). 


level_energy_unit: KEV
level_spin_parity: (3/2-,9/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
$E{-|a}(res) (keV)=8253 {I15} 
WIDTH$Beginning in (1971Aj02) the |G for this level was listed at |?5 keV attributed to {+13}C(|a,n) (1969Sp02). However this was a typo. (1969Sp02) report |?75 keV. 
E$from E{-|a}=8253 keV {I15} (1963Sp02). See also E{-|a}=8328 keV (1970Ro08). 


level_energy_unit: KEV
level_spin_parity: (1/2+,7/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=GE
level_comment:
$E{-|a}(res) (keV)=8590 {I20} 
E$from E{-|a}=8590 keV {I20} (1963Sp02). See also E{-|a}=8657 keV (1970Ro08). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-|a}(res) (keV)=8612 
E$from E{-|a}=8612 keV which is calculated from the E{-x} given in (1976Mc11). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E{-|a}(res) (keV)=8676 
E$from E{-|a}=8676 keV which is calculated from the E{-x} given in (1976Mc11). See also 13027 keV {I20} (1963Sp02: E{-|a}=8720 keV {I20}) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$C{+2}S{-|a}=0.29 
$S{-|a}=0.29 {I11}, ANC{+2}=4.5 fm{+-1} {I22} and |g{-|a}{+2} (reduced |a width)=13.5 keV {I66} from (2008Pe09). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$C{+2}S{-|a}=0.24 
E$from (1993Ti07). 
$|G{-n}=400 keV, |G{-|a}=0.09 keV (2008Pe09) which are consistent with the {+16}O+n measurement in (1966Li03: |G{-n}/|G>0.99). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$S{-|a}=0.39 {I12} 
S$for N=4; ANC{+2}=4.5 fm{+-1} {I14}. For N=3, S{-|a}=0.72 {I22}; ANC{+2}=5.1 fm{+-1} {I15} (2017Me04). 
$S{-|a}=0.37 {I12}; ANC{+2}=4.0 fm{+-1} {I11} (2012Gu18). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-res}(lab) (MeV)=3.6 {I1} 
E$from E({+3}He)=3600 keV {I100} (1976Ch04). See also E{-res}=3600 keV (Ke70,1971Ke08,1972Ke08). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-res}(lab) (MeV)=4.1 {I1} 
E$From E({+3}He)=4100 keV {I100} (1976Ch04). See also E{-res}=4100 keV (Ke70,1970Ho08,1971Ke08,1972Ke08). 
J$(1970Ho08) however suggests (1/2-,3/2-). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=AP
level_comment:
$E{-res}(lab) (MeV)=5.1 {I1} 
E$from E({+3}He)=5100 keV {I100} (1976Ch04). See also E{-res}=5100 keV (Ke70,1972Ke08). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: PS
level_comment:
WIDTH$from |t=245 ps {I10} (1974Sc09). See also |t=434 ps {I11} (1962Ga15, 1962Ga16). 
L$from (1961Ya02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2,9/2,11/2)
level_comment:
J$from (1969Ro07) on the basis of a possible statistical compound nuclear mechanism and the use of the (2J+1) rule. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$E{-res} (keV)=1360 
E$from E{-d}=1360 keV (1957Bo04); see also E{-d}|?1400 keV (1977Ca03: {+15}N(d,d)). 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
$E{-res}=1700 {IAP} 
E$from E{-d}|?1700 keV, which is a likely multiplet corresponding to states around E{-d}=1.6-1.8 MeV. (1965Ma59). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=433 {I4} 
E$from E{-n}=433 keV {I4} (1958Hu18). See also E{-n}(keV)=440 (1950Bo95,1951Bo45), 442 (1955Ok01,1964St25). 
WIDTH$From |G{-lab}=41 keV {I3}. See also |G{-lab}(keV)=45 (1950Bo95), 40 (1951Bo45), 48 (1955Ok01), 46 (1964St25) and |G{-n}=45 keV (1973Jo01). 
L$See (1953Ad02,1955Ok01,1958Hu18,1964St25). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=998 {I8} 
E$from E{-n}=998 keV {I8} (1958Hu18). See also E{-n}=1000 keV (1950Bo95, 1951Bo45, 1958La09, 1958St28, 1964St25). 
WIDTH$From |G{-lab}=96 keV {I5}. See also |G{-lab}=100 keV (1950Bo95, 1951Bo45, 1958St28, 1964St25) and |G{-n}=96 keV (1973Jo01). 
L$See (1953Ad02,1958Fo67,1958Hu18,1964St25). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=1312.0 {I35} 
E$from E{-n}=1312.0 keV {I35} (Davis, et al., PLB 27, 636 (1968)). See also E{-n}(keV)=1310 {I8} (1958Hu18), 1300 (1950Bo95), 1320 (1951Bo45), 1312 (1958St28,1964St25). 
WIDTH$From |G{-lab}=33 keV {I4}. See also |G{-lab}=40 keV (1950Bo95), 35 keV (1951Bo45), 42 keV (1964St25), 44 keV (1958St28) and |G{-n}=41.5 keV (1973Jo01). 
L$See (1953Ad02,1958Hu18,1964St25). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=1651 {I2} 
E$from E{-n}=1651 keV {I2} (1973Fo11). See also E{-n}(keV)=1651 {I6} (1958Hu18), 1660 (1951Bo45,1958La09), 1651 (Jo68: Johnson, et al., Neutron Cross Sections and Technology, Proc. Conf.; NBS Special Publication 299 Vol. II, 851 (1968)). 
WIDTH$See also |G{-lab}|<7 keV (1951Bo45,1958Hu18), |G{-lab}=4 keV (Jo68) and |G{-n}=3.4 keV (1973Jo01). 
L$See (1951Bo45: >0) and (1958Hu18: |>1). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E{-n}(res) (keV)=1689 {I2} 
E$from E{-n}=1689 keV {I2} (1973Fo11). See also E{-n}=1689 keV (Jo68). 
WIDTH$See also |G{-lab}<1 keV (Jo68). 
J$|=1/2+ (1973Fo11). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=1833 {I2} 
E$from E{-n}=1833 keV {I2} (1973Fo11). See also E{-n}(keV)=1830 {I6} (1958Hu18), 1840 (1951Bo45), 1833 (Jo68). 
WIDTH$See also |G{-lab}(keV)|<10 (1951Bo45), |<8 (1958Hu18), |G=7 keV (Jo68) and |G{-n}=6.6 keV (1973Jo01). 
L$See also (1951Bo45: >0), (1958Hu18: |>1). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=1908 {I4} 
E$from E{-n}=1908 keV {I4} (1973Fo11). See also E{-n}(keV)=1903 {I11} (1958Hu18), 1910 (1951Bo45,1964St25), 1906 (Jo68), 1900 (Ba52: Baldinger, et al., Helv. Phys. Acta 25, 142 (1952)). 
WIDTH$See also |G{-lab}=30 keV (1951Bo45,1964St25), 28 keV {I5} (1958Hu18) and |G{-n}=31.5 keV (1973Jo01). 
L$See (1951Bo45,1958Hu18,1964St25). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=2351 {I8} 
E$from E{-n}=2351 keV {I8} (1973Fo11). See also E{-n}(keV)=2370 {I20} (1958Hu18), 2370 (1951Bo45,1964St25), 2350 (Ba52,Jo68). 
WIDTH$See also |G{-lab}(keV)=120 (1951Bo45,1964St25), 140 {I50} (1958Hu18), 180 (Ba52) and |G{-n}=124 keV (1973Jo01). 
L$See (1951Bo45,1958Hu18,1964St25). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E{-n}(res) (keV)=2889 {I2} 
E$from E{-n}=2889 keV {I2} (1973Fo11). See also E{-n}=2889 keV (Jo68). 
WIDTH$See also |G{-lab}<1 keV (Jo68). 
J$|=1/2+ (1973Fo11). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=3211.70 {I17} 
E$from E{-n}=3211.70 keV {I17} (1980Ci03). See also E{-n}(keV)=3211 {I3} (1973Fo11), 3213 (Jo68). 
WIDTH$See also |G{-lab}=2 keV (Jo68), |G=5 keV (1957Wa46), 1.3 keV {I4} (1973Fo11), |G{-n}=1.4 keV and |G{-|a}=0.0027 keV (1973Jo01), |G{-n}/|G{-|a}=(1300) (1957Wa46) and |G{-n0}=1.38 keV {I5} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=3250 {I10} 
E$from E{-n}=3250 keV {I10} (1973Fo11). See also E{-n}(keV)=3330 {I30} (1958Hu18), 3290 {I20} (1966Li03), 3350 (1967Jo12), 3330 (Ba52). 
WIDTH$See also |G{-lab}=200 keV {I40} (1958Hu18), 220 keV (Ba52), |G=500 keV (1967Jo12), 400 keV {I30} (1966Li03), |G{-n}=280 keV and |G{-|a}=0.12 keV (1973Jo01) and |G{-n}/|G>0.99 (1966Li03). 
J$See also (1966Li03,1967Jo12). 
L$from (1958Hu18,1967Jo12). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=3438.38 {I19} 
E$from E{-n}=3438.38 keV {I19} (1980Ci03). See also E{-n}(keV)=3438 {I3} (1973Fo11), 3442 (Jo68). 
WIDTH$See also |G(keV)=0.5 {I2} (1973Fo11), 0.5 (1970Fo03), |<4 (1957Wa46), |G{-n}=0.5 keV and |G{-|a}=0.01 keV (1973Jo01), |G{-n}/|G{-|a}=(450) (1957Wa46) and |G{-n0}=0.64 keV {I23} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=3441.73 {I14} 
E$from E{-n}=3441.73 keV {I14} (1980Ci03). See also E{-n}(keV)=3441 {I3} (1973Fo11), 3440 (1961Fo07), 3444 (Jo68). 
WIDTH$See also |G(keV)=1.1 {I3} (1973Fo11), 1.1 (1970Fo03), |<8 (1961Fo07), |G{-n}=1.2 keV and |G{-|a}=0.0032 keV (1973Jo01) and |G{-n0}=0.96 keV {I20} (1980Ci03). 
L$see (1970Fo03). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=3630 {I20} 
E$from E{-n}=3630 keV {I20} (1973Fo11). See also E{-n}(keV)=3770 {I20} (1966Li03), 3600 (1964St25), (3600) (1961Fo01), 3643 (Jo68), 3750 (1967Jo12). 
WIDTH$See also |G(keV)=360 {I30} (1966Li03), 600 (1961Fo07,1964St25), 405 (1967Jo12), |G{-n}=500 keV and |G{-|a}=0.08 keV (1973Jo01) and |G{-n}/|G>0.99 (1966Li03). 
J$See also (1966Li03,1967Jo12). 
L$from (1964St25,1967Jo12). 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_uncertain: ?
level_comment:
$E{-n}(res) (keV)=3745 {I10} 
$(1973Fo11) indicates this level does not exist. 
E$from E{-n}=3745 keV {I10} (1960Ts02). See also E{-n}=3770 keV (1961Fo07,1964St25), 3772 keV (1967Jo12). 
WIDTH$from (1960Ts02). See also |G=25 keV (1961Fo07,1964St25), 22 keV (1957Wa46), 3 keV (1967Jo12). 
J$See (1957Wa46,1960Ts02,1961Fo07,1964St25,1967Jo12). 
L$See (1964St25,1967Jo12). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=3767.76 {I22} 
E$from E{-n}=3767.76 keV {I22} (1980Ci03). See also E{-n}(keV)=3780 {I10} (1966Li03), 3765 {I3} (1969Da13), 3766 {I4} (1973Fo11), 3769 (1967Jo12). 
WIDTH$See also |G(keV)=14 keV (1967Jo12), <23 (1966Li03), 18 keV {I2} (1973Fo11), |G{-n}=18 keV and |G{-|a}=0.01 keV (1973Jo01), |G{-n}/|G>0.99 (1966Li03) and |G{-n0}=13.0 keV {I6} (1980Ci03). 
J$See also (1966Li03,1967Jo12). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_uncertain: ?
level_comment:
$E{-n}(res) (keV)=3800 {I80} 
E$from E{-n}=3800 keV {I80} (1958Hu18). See also E{-n}=3800 keV (Ba52). 
WIDTH$from |G{-lab}=800 keV {I200} (1958Hu18). See also |G{-lab}=800 keV (Ba52). 
J$See (Ba52,1958Hu18) 
L$from (1958Hu18). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4053 {I8} 
E$from E{-n}=4053 keV {I8} (1973Fo11). 
J$See also (1973Fo11). 
WIDTH$See also |G{-n}=84 keV and |G{-|a}=6.7 keV (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4090 {I50} 
E$from E{-n}=4090 keV {I50} (1973Fo11). See also E{-n}(keV)=3920 {I20} (1966Li03), 4000 (1967Jo12), (3980) (1961Fo07). 
WIDTH$See also |G(keV)=245 {I30} (1966Li03), 110 (1957Wa46: triplet), |G{-n}=250 keV and |G{-|a}=14 keV (1973Jo01), |G{-n}/|G{-|a}=10 (1957Wa46) and |G{-n}/|G>0.95 (1966Li03). 
J$See also (1966Li03,1967Jo12,1973Fo11). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4162 {I8} 
E$from E{-n}=4162 keV {I8} (1973Fo11). See also E{-n}(keV)=4200 {I10} (1960Ts02), 4175 {I10} (1966Li03), 4180 (1967Jo12), 4200 (1961Fo07). 
WIDTH$See also |G(keV)=75 {I20} (1966Li03), 80 (1961Fo07) and 70 (1957Wa46), |G{-n}=71 keV and |G{-|a}=15 keV (1973Jo01), |G{-n}/|G{-|a}=10 (1957Wa46) and |G{-n}/|G>0.90 (1966Li03). 
J$See also (1966Li03,1967Jo12). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4290 {I20} 
E$from E{-n}=4290 keV {I20} (1973Fo11). 
WIDTH$See also |G{-n}=68 keV and |G{-|a}=0.8 keV (1973Jo01). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-n}(res) (keV)=4320 {I14} 
E$from E{-n}=4320 keV {I10}, which is the average of (1960Ts02: 4330 keV {I10}) and (1973Fo11: 4310 keV {I10}). See also E{-n}=4320 keV (1961Fo07). 
WIDTH$Deduced, in part, from (1961Fo07). See also |G|?90 keV (1960Ts02), 60 keV (1957Wa46,1961Fo07), |G{-n}=48 keV and |G{-|a}=4 keV (1973Jo01) and |G{-n}/|G{-|a}=13 (1957Wa46). 


level_energy_unit: KEV
level_spin_parity: 1/2
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4463.41 {I26} 
E$from E{-n}=4463.41 keV {I26} (1980Ci03). See also E{-n}(keV)=4400 {I40} (1958Hu18), 4400 (Ba52,1958Hu18), 4470 (1960Ts02: group), 4450 (1964St25), 4440 (1956Be98). 
WIDTH$See also |G=18 keV (1957Wa46), |G{-lab}=280 keV {I80} (1958Hu18), 280 keV (Ba52), |G{-n}=10 keV and |G{-|a}=2.2 keV (1973Jo01), |G{-n}/|G{-|a}=6.7 (1957Wa46) and |G{-n0}=8.1 keV {I3} (1980Ci03). 
J$See (Ba52,1958Hu18,1964St25,1973Jo01). 
L$from (1958Hu18,1964St25). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4527.12 {I7} 
E$from E{-n}=4527.12 keV {I7} (1980Ci03). See also E{-n}=4530 keV (1956Be98,1961Fo07). 
WIDTH$See also |G|<10 keV (1961Fo07), 11 keV (1957Wa46), |G{-n}=4.8 keV and |G{-|a}=0.54 keV (1973Jo01), |G{-n}/|G{-|a}=19 (1957Wa46) and |G{-n0}=4.75 keV {I11} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4594.83 {I9} 
E$from E{-n}=4594.83 keV {I9} (1980Ci03). See also E{-n}(keV)=4625 {I10} (1960Ts02), 4600 (1961Fo07), 4590 (1956Be98). 
WIDTH$See also |G|<11 keV (1961Fo07), 9 keV (1957Wa46: doublet), |G{-|a}=7.6 keV (1973Jo01), |G{-n}/|G{-|a}=31 (1957Wa46) and |G{-n0}=1.18 keV {I4} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4631.78 {I12} 
E$from E{-n}=4631.78 keV {I12} (1980Ci03). See also E{-n}(keV)=4705 {I10} (1960Ts02), 4630 (1956Be98), 4640 (1961Fo07). 
WIDTH$See also |G|<13 keV (1961Fo07), 11 keV (1957Wa46), |G{-n}=3.4 keV and |G{-|a}=1.9 keV (1973Jo01), |G{-n}/|G{-|a}=2.8 (1957Wa46) and |G{-n0}=2.86 keV {I8} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=4829.9 {I4} 
E$from E{-n}=4829.9 keV {I4} (1980Ci03). See also E{-n}=4845 keV {I10} (1960Ts02), 4840 (1961Fo07), 4850 (1956Be98). 
WIDTH$See also |G(keV)|?90 (1960Ts02), 55 (1961Fo07), 85 (1957Wa46: triplet), |G{-n}=42 keV and |G{-|a}=1.8 keV (1973Jo01), |G{-n}/|G{-|a}=17 (1957Wa46) and |G{-n0}=48.9 keV {I11} (1980Ci03). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E{-n}(res) (keV)=5010 {I10} 
E,WIDTH$from (1960Ts02: 5010 keV {I10}). See also 5080 (1956Be98). 
E$In past evaluations, information from {+16}O(n,|a) and {+13}C(|a,n) is peppered into the {+16}O(n,n) dataset. It is usually harmless; however, in the present case we associate the 8858 keV level with the narrow (7/2-,9/2-) member of the E{-x}=8.9 MeV doublet. The broad 3/2+ member of this doublet is not reported in (n,n'). The |G{-n}=68 keV and |G{-|a}=9.7 keV (1973Jo01), and |G|?110 keV and |G{-n}/|G{-|a}=3.5 (1957Wa46), etc. parameters accociated with E{-x}=8.9 MeV; J{+|p}=3/2+ are from {+16}O(n,|a) and {+13}C(|a,n) (1957Wa46,1973Ba10). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=5127.0 {I16} 
E$from E{-n}=5127.0 keV {I16} (1980Ci03). See also E{-n}(keV)=5122 {I4} (1969Da13), 5110 (1961Fo07), 5130 (1956Be98) 
WIDTH$See also |G(keV)=28 (1961Fo07), 35 (1957Wa46), |G{-n}=23 keV and |G{-|a}=2.3 keV (1973Jo01), |G{-n}/|G{-|a}=35 (1957Wa46) and |G{-n0}=23.5 keV {I19} (1980Ci03). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=5368.90 {I9} 
E$from E{-n}=5368.90 keV {I9} (1980Ci03). 
WIDTH$see also |G{-n0}=2.37 keV {I8} (1980Ci03). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-n}(res) (keV)=5610 
E$from E{-n}=5610 keV (1973Jo01). See also E{-n}=5630 keV (1961Fo07). 
$|G=|G{-n}=120 keV (1973Jo01). See also 140 keV (1961Fo07). 


level_energy_unit: KEV
level_spin_parity: GE5/2
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=5919.67 {I14} 
E$from E{-n}=5919.67 keV {I14} (1980Ci03). See also E{-n}(keV)=5914 {I5} (1969Da13), 5900 (1961Fo07). 
WIDTH$See also |G=28 keV (1961Fo07) and |G{-no}=18.0 keV {I6} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: GE3/2
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=5995.68 {I15} 
E$from E{-n}=5995.68 keV {I15} (1980Ci03). See also E{-n}=5990 keV (1961Fo07). 
WIDTH$See also |G=28 keV (1961Fo07) and |G{-n0}=10.3 keV {I3} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=6076.08 {I15} 
E$from E{-n}=6076.08 keV {I15} (1980Ci03). 
WIDTH$See also |G{-n0}=3.37 keV {I20} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=6094.8 {I10} 
E$from E{-n}=6094.8 keV {I10} (1980Ci03). See also E{-n}=6080 keV (1961Fo07). 
WIDTH$See also |G=25 keV (1961Fo07) and |G{-n0}=10.9 keV {I12} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=6404.6 {I5} 
E$from E{-n}=6404.6 keV {I5} (1980Ci03). See also E{-n}(keV)=6395 {I7} (1969Da13), 6390 (1961Fo07). 
WIDTH$See also |G=38 keV (1961Fo07) and |G{-n0}=22.3 keV {I6} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=6820.7 {I6} 
E$from E{-n}=6820.7 keV {I6} (1980Ci03). See also E{-n}(keV)=6807 {I7} (1969Da13), 6830 (1959Ha13), 6790 (1961Fo07), 6860 (1970Lu16). 
WIDTH$See also |G=40 keV (1961Fo07) and |G{-n0}=17.2 keV {I7} (1980Ci03). 
J$from (1970Lu16). See also (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=7199.3 {I13} 
E$from E{-n}=7199.3 keV {I13} (1980Ci03). See also E{-n}(keV)=7200 {I8} (1969Da13), 7200 (1970Lu16), 7180 (1961Fo07). 
WIDTH$See also |G=70 keV (1961Fo07) and |G{-n0}=26.4 keV {I9} (1980Ci03). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=7373.31 {I18} 
E$from E{-n}=7373.31 keV {I18} (1980Ci03,1981Hi01); see also E{-n}=7400 keV (1959Ha13), 7440 keV (1970Lu16). See also E{-x}=11076 keV {I5} (1976Mc11: {+13}C(|a,n)). 
WIDTH$from (1980Ci03,1981Hi01). See also |G=5.0 keV {I11} (1976Mc11) and |G{-n0}=1.88 keV {I12} (1980Ci03,1981Hi01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: GE3/2
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-n}(res) (keV)=7837 
E$from E{-n}=7837 keV, which is the average of (1961Fo07: 7810 keV), (1959Ha13: 7870 keV) and (1970Lu16: 7830 keV). 
J$See also (3/2,5/2) (1970Lu16). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: GE3/2
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-n}(res) (keV)=8325 
E$from E{-n}=8325 keV, which is the average of (1959Ha13: 8350 keV) and (1961Fo07: 8300 keV). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=8848.8 {I6} 
E$from E{-n}=8848.8 keV {I6} (1980Ci03,1981Hi01). See also E{-n}=8840 keV (1959Ha13); E{-x}=12458 keV {I5} (1976Mc11: {+13}C(|a,n)). 
WIDTH$from (1980Ci03,1981Hi01). See also |G=8 keV {I2} (1976Mc11) and |G{-n0}=1.27 keV {I14} (1980Ci03,1981Hi01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$E{-n}(res) (keV)=9065 
E$from E{-n}=9065 keV, which is the aveage of (1959Ha13: 9100 keV) and (1961Fo07: 9030 keV). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=9353 {I6} 
E$from E{-n}=9353 keV {I6} (1981Hi01). See also E{-n}=9340 keV (1959Ha13); E{-x}=12944 keV {I6} (1976Mc11: {+13}C(|a,n)). 
WIDTH$See also |G{-n0}=0.21 keV {I14} (1981Hi01). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=9414.9 {I6} 
E$from E{-n}=9414.9 keV {I6} (1980Ci03,1981Hi01). See also E{-x}=12993 keV {I6} (1976Mc11: {+13}C(|a,n)). 
WIDTH$from (1980Ci03,1981Hi01). See also |G|<3 keV (1976Mc11) and |G{-n0}=0.40 keV {I6} (1980Ci03,1981Hi01). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=10092.5 {I24} 
E$from E{-n}=10092.5 keV {I24} (1981Hi01). 
WIDTH$See also |G{-n0}=0.24 keV {I9} (1981Hi01). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=10725.5 {I15} 
E$from E{-n}=10725.5 keV {I15} (1980Ci03,1981Hi01). 
WIDTH$from (1980Ci03,1981Hi01). See also |G{-n0}=2.07 keV {I16} (1980Ci03,1981Hi01). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=10785 {I3} 
E$from E{-n}=10785 keV {I3} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=0.80 keV {I16} (1981Hi01). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=10960 {I3} 
E$from E{-n}=10960 keV {I3} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=13 keV {I6} (1981Hi01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=11322 {I3} 
E$from E{-n}=11322 keV {I3} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=3.2 keV {I10} (1981Hi01) 


level_energy_unit: KEV
level_spin_parity: (3/2)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=11756 {I3} 
E$from E{-n}=11756 keV {I3} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=11 keV {I3} (1981Hi01). 


level_energy_unit: KEV
level_spin_parity: LE5/2
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=11936 {I3} 
E$from E{-n}=11936 keV {I3} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=7 keV {I1} (1981Hi01). 


level_energy_unit: KEV
level_spin_parity: (7/2+,9/2+)
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=12867 {I4} 
E$from E{-n}=12867 keV {I4} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=2.0 keV {I5} (1981Hi01) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=14136 {I11} 
E$from E{-n}=14136 keV {I11} (1981Hi01). 
WIDTH$See also (J|+1/2)|G{-n0}=8.0 keV {I24} (1981Hi01). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E{-n}(res) (keV)=14853 {I4} 
E$from E{-n}=14853 keV {I4} (1981Hi01). 
WIDTH$from (1981Hi01: Table 1). See also |G=43 keV {I12} (1981Hi01: Table 2), |G{-n0}=1.9 keV {I6} (1981Hi01: Table 1) and (J|+1/2)|G{-n0}=1.0 keV {I3} (1981Hi01: Table 2). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_comment:
$E{-n}(res) (keV)=17300 
E$from E{-n}=17300 keV (1970Bo30). 
WIDTH$|G{-n}|?700 keV (1970Bo30). 
J$from (1970Bo30). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
S$from (2019Ma31). See also S{-average}=0.81 (1970Da14), 0.925 (1972Co15), 0.95 (1974Co04) and S=0.94 {I13} (2005Ts03: analysis). ANC=0.60 fm{+-1} {I4} (2019Ma31), see also (2007Pa10: 0.67 fm{+-1} {I5}). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
E$From E{-|g}=870.725 {I20} (1980Wa24). See also E{-x}(keV)=870.73 {I10} (2015Pa05), 870 {I20} (Bu51), 875 {I12} (1954Sp01), 871 {I4} (1957Br82). 
$T{-1/2}: from |t{-m}=260.2 ps {I29} which is the weighted average of (1960Ka10: 255 ps {I13}), (1963Lo03: 263 ps {I8}), (1964Be15: 258.7 ps {I42}), (1965Mc10: 263 ps {I7}), (1969Go04: 261 ps {I7}). Other values(ps): 250 {I100} (1953Th14), 233 {I26} (1965Al14), 232 {I8} (1967Bi05), 253 {6} (1969Ni09: {+9}Be({+16}O,{+17}O){+8}Be), 421 {I21} (1962Ga15,1962Ga16), 258.7 (1971Do13). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$See E{-x}(keV)=3870 {I40} (Bu51), 3840 {i12} (1954Sp01), 3846 {I5} (1957Br82)/ 
S$See als <0.1 (1970Da14). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$See also E{-x}(keV)=4590 {I20} (Bu51), 4553 {I5} (1957Br82). 
S$using HD parameters; 0.20: using mb parameters (1973Da17). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
E$See also E{-x}(keV)=5060 {I20} (Bu51), 5083 {I10} (1957Br82). 
WIDTH$ See also |G(keV)=67 (1970Vi03), |?70 (1974Co04: average value), |G{-n}=97 keV {I5} (1979An15). 
S$average value: using HD parameters (1973Da17). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$(|G{-n}/|G){-exp}=0.97 {I5} (1993La31: {+16}O(|a,{+3}He){+17}O*(5.697-MeV[7/2-])|)n+{+16}O{-g.s.}[0+]).  


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$S{-1}S{-2}=0.60 
S$1p{-1/2}|)1d{-5/2} neutron transfer configuration (1979Bo36: LOLA). See also (1979Bo36: S{-1}S{-2}=0.49 (I|g normalization(CRC)). 
$See also (2000Ik01: S=0.900 (DWBA), 0.900 (|a)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$S{-1}S{-2}=0.72 
E$Well described as the coupling of a 2s{-1/2} neutron to the {+16}O core (1968Na06). 
L$See also (1976We21,1983Os08). 
S$1p{-1/2}|)2s{-1/2} neutron transfer configuration; extracted using a Coulomb wave Born approximation (1975Se03); and compared with the theoretical value 0.61 (1968Na06: using S{-1}=0.61 for the {+13}C{-g.s.}). See also (1979Bo36: S{-1}S{-2}=0.50 (LOLA), 0.51 (I|g normalization(CRC)). 
$See also (1983Os08: S=0.6138), (2000Ik01: S=0.800 (DWBA), 0.750 (|a)). C{+2}S=0.49; Q(|b{+-})value=-0.804 MeV (1976We21). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$|G{-|g0} (eV)=0.7 {I4} 
E$See also (1978Ho16: 5378 keV). 
S$See also |G{-|g0}=0.06 eV (1978Ho16). 
$E1 transition (1978Ho16). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
$|G{-|g0} (eV)=1.1 {I4} 
E$See also (1978Ho16: 5690 keV). 
S$See also |G{-|g0}=0.4 eV (1978Ho16). 
$E1 transition (1978Ho16). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_uncertain: ?
level_comment:
E$From (1992Zu01: weak resonance at E{-|g}=14.1 MeV {I1}). 
$T=3/2 (1992Zu01). See also 14.0 MeV (1985Ju02) 
${Ia}{-2}=0.0|+0.10 (1985Ju02). 


level_energy_unit: KEV
level_comment:
E$from E{-|g}(res)=15.06 MeV {I5} with |G|?0.45 MeV; a few narrow T=3/2 states and M1 transitions contribute to the measured strength (1992Zu01). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E,WIDTH$from E{-|g}(res)=18.09 MeV {I7}; probably a doublet consisting of (18.101-MeV[J{+|p}=3/2-; T=3/2] (1981Hi01) and very weakly excited state at 18.3-MeV[T=1/2]) (1992Zu01). 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
E,WIDTH$From 19.3-MeV[T=1/2] from E{-|g}(res)=19.28 MeV {I7} (1992Zu01); see also 19.1 MeV (1990Mc06). 


level_energy_unit: KEV
level_comment:
E$from E{-|g}(res)=23.1 MeV {I1} (1992Zu01). 
E$A giant dipole resonance, 6 MeV broad, is centered at 23 MeV (1980Ju01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$See B(E2)|^=2.18 e{+2}fm{+4} {I16} (1987Ma52), and B(C2)|^=2.10 e{+2}fm{+4} {I1} (1978Ki01): deduced from the lifetime measurement of (1971Aj02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$See B(E3)|^=14.1 e{+2}fm{+6} {I39} (1987Ma52), B(E3)|^=31 e{+2}fm{+6} {I6} (1975Ki15), and B(C3)|^=31 e{+2}fm{+6} {I6} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$See B(M2)|^=5|*10{+-2} e{+2}fm{+4} {I2} (1978Ki01); B(E3)|^=93.0 e{+2}fm{+6} {I83} (1987Ma52), B(E3)|^=153 e{+2}fm{+6} {I6} (1975Ki15), and B(C3)|^=153 e{+2}fm{+6} {I6} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$See B(M2)|^=5.4|*10{+-2} e{+2}fm{+4} {I21} (1978Ki01); B(E3)|^=20 e{+2}fm{+6} 12 (1987Ma52), B(E3)|^=98 e{+2}fm{+6} {I8} (1975Ki15), and B(C3)|^=98 e{+2}fm{+6} {I8} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
J$From (1987Ma52). 
$See B(M2)|^<4|*10{+-2} e{+2}fm{+4} (1978Ki01); B(E3)|^=319 e{+2}fm{+6} {I13} 1987Ma52), B(E3)|^=360 e{+2}fm{+6} {I11} (1975Ki15), and B(C3)|^=360 e{+2}fm{+6} {I11} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$See B(M2)|^=6|*10{+-2} e{+2}fm{+4} {I3} (1978Ki01); B(E3)|^=47.9 e{+2}fm{+6} {I43} (1987Ma52), B(E3)|^=45 e{+2}fm{+6} {I12} (1975Ki15), and B(C3)|^=45 e{+2}fm{+6} {I12} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$See B(M2)|^=0.3 e{+2}fm{+4} {I2} (1978Ki01); B(E3)|^=97.0 e{+2}fm{+6} {I65} (1987Ma52), B(E3)|^=270 e{+2}fm{+6} {I32} (1975Ki15), and B(C3)|^=270 e{+2}fm{+6} {I32} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_comment:
$See B(E3)|^=25.3 e{+2}fm{+6} {I51} (1987Ma52), B(E3)|^=17 e{+2}fm{+6} {I10} (1975Ki15), and B(C3)|^=17 e{+2}fm{+6} {I10} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 6970 (1978Ki01). 
J$From (1987Ma52). 
$See B(E2)|^=0.83 e{+2}fm{+4} {I25} and J{+|p}=5/2+ (1987Ma52). Earlier analysis, based in J{+|p}=(1/2-) found B(E3)|^=(147 e{+2}fm{+6} {I34}) (1975Ki15), and B(C3)|^=147 e{+2}fm{+6} {I34} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J,WIDTH$(1987Ma52). 
$Unresolved with 6859 (1978Ki01). 
$See B(E3)|^=75.5 e{+2}fm{+6} {I56} and J{+|p}=(7/2-) (1987Ma52). Earlier analysis based in J{+|p}=(5/2+) from (1978Ki01) found B(C2)|^=1.9 e{+2}fm{+4} {I10} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$See B(E3)|^=11.1 e{+2}fm{+6} {I29} (1987Ma52), and B(E3)|^=22 e{+2}fm{+6} {I25} (1975Ki15). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 7379 (1978Ki01,1987Ma52). 
$See B(E2)|^<0.8 e{+2}fm{+4} (1987Ma52), B(C2)|^=3.6 e{+2}fm{+4} {I10} (1987Ki01), and B(C0)|^=5.5 e{+2} {I10} (1987Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 7378 (1978Ki01,1987Ma52). 
$See B(E3)|^=36.9 e{+2}fm{+6} {I24} (1987Ma52), B(E3)|^=47 e{+2}fm{+6} {I38} (1975Ki15), and B(C3)|^=47 e{+2}fm{+6} {I38} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J,WIDTH$(1987Ma52). 
$See B(E2)|^=4.20 e{+2}fm{+4} {I51} and J{+|p}=7/2+ (1987Ma52), 
$Earlier analysis using J{+|p}=7/2- found E|b(C1)|^=7.8|*10{+-2} e{+2}fm{+2} {I20} (1978Ki01), B(E3)|^=109 e{+2}fm{+6} {I26} (1975Ki15), and B(C3)|^=109 e{+2}fm{+6} {I26} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (11/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$See B(E3)|^=287 e{+2} fm{+6} {I14} and J{+|p}=11/2- (1987Ma52), B(E3)|^=369 e{+2}fm{+6} {I15} (1975Ki15), and B(C3)|^=369 e{+2}fm{+6} {I15} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$Unresolved with 8402, 8467, 8502 (1978Ki01). 
$See B(E2)|^=0.48 e{+2}fm{+4} {I7} (1987Ma52), B(C0)|^=7.6 e{+2} {I14} (1978Ki01), and B(C2)|^=8.3 e{+2}fm{+4} {I26} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 8347, 8467, 8502 (1978Ki01). 
$See B(E2)|^=2.10 e{+2}fm{+4} {I34} (1987Ma52), B(C0)|^=7.6 e{+2} {I14} (1978Ki01), and B(C2)|^=8.3 e{+2}fm{+4} {I26} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 9/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J,WIDTH$(1987Ma52). 
$Unresolved with 8347, 8402, 8502 (1978Ki01). 
$See B(E2)|^=10.1 e{+2}fm{+4} 12 and J{+|p}=9/2+ (1987Ma52) 
$Earlier analysis using J{+|p}=7/2+ found B(C0)|^=7.6 e{+2} {I14} (1978Ki01), and B(C2)|^=8.3 e{+2}fm{+4} {I26} (1978Ki01). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$B(E3)|^ negligible (1975Ki15). 
$Unresolved with 8347, 8402, 8467 (1978Ki01). 
$See B(E3)|^<7 e{+2} fm{+6} (1987Ma52), B(C0)|^=7.6 e{+2} {I14} (1978Ki01), and B(C2)|^=8.3 e{+2}fm{+4} {I26} (1978Ki01). 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E,J,WIDTH$(1987Ma52). 
E$Probably is the level reported in (1965Ba32: 8.884-MeV; |G=8 keV). 
$See B(E3)|^=13.3 e{+2}fm{+6} {I23} (1987Ma52). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 9190 (1987Ma52). 
$See B(E3)|^=2.4 e{+2}fm{+6} {I10} (1987Ma52). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 9180 (1987Ma52). 
$See B(E2)|^=0.48 e{+2}fm{+4} {I16} (1987Ma52). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 11040 (1987Ma52). 
$See B(M2)|^=6.1 |m{-N}{+2}fm{+4} {I19} (1983Ra27). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$See B(M2)|^=6 |m{-N}{+2} fm{+4} {I3} (1983Ra27), and if pure E1, B(E1)|^=1.0|*10{+-2} e{+2}fm{+2} {I4} (1983Ra27). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$See also the triplet 12.96|*10{+3} keV {I5} with |G|?200 keV (1977No06). 
WIDTH$(1987Ma52). 
$Unresolved with 12990 (1987Ma52). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
WIDTH$(1987Ma52). 
$Unresolved with 12940 (1987Ma52). 
$See B(M2)|^=6 |m{-N}{+2}fm{+4} {I3} (1983Ra27), and if pure E1, B(E1)|^=0.4|*10{+-2} e{+2}fm{+2} {I2} (1983Ra27). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
J$(1986Ma48,1987Ma52). 
$See B(M2)|^=46 |m{-N}{+2}fm{+4} {I7} (1983Ra27), and B(E1)|^<0.01 e{+2}fm{+2}, from the estimate of longitudinal component (1983Ra27). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_lifetime_unit: KEV
level_comment:
E,J,WIDTH$(1987Ma52). 
E$See also E{-x}=14750 keV; J{+|p}=9/2- (1983Ra27). 
$See B(M2)|^=27 |m{-N}{+2} fm{+4} {I10} (1983Ra27). 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,WIDTH$(1986Ma48); J{+|p}: (1986Ma48,1987Ma40). 
$See B(M4)|^=177 e{+2}fm{+8} {I17} (1986Ma48). 
J$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). Initially identified in {+17}O(e,e') as (9/2-). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
J$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). Initially identified in {+17}O(e,e') as (7/2-). Also see (7/2-) in {+16}O(p,|p+) and (11/2-) in {+13}C({+6}Li,d). 
$T=(1/2) from (1987Mi25), see comments in (1986Ma48, 1987Ma40, 1987Mi25). Initially reported as T=(3/2) (1986Ma48,1987Ma40) 
E,WIDTH$(1986Ma48); See also E{-x}=17090 keV {I50}; |G: narrow (1977No06). 
$See B(M4)|^=76 e{+2}fm{+8} {I6} (1986Ma48). 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: KEV
level_comment:
E,WIDTH$(1986Ma48); J{+|p}: (1986Ma48,1987Ma40). 
$See B(M4)|^=349 e{+2}fm{+8} {I18} (1986Ma48). 
J$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). Initially identified as 13/2- but later assigned 11/2-. 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,WIDTH$(1986Ma48); J{+|p}: (1986Ma48,1987Ma40). 
$See B(M4)|^=177 e{+2}fm{+8} {I10} (1986Ma48). 
J$From (1987Mi25): See comments, replies and discussion in (1987Mi25) and (1986Ma48, 1987Ma40). Initially identified as 11/2- but later assigned 9/2-. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
$Bremsstrahlung weighted integrated cross section |s=6.01 MeV~*b at Bremsstrahlung endpoint energy E{-brem.}=23.5 MeV; |s=6.71 MeV~*b at E{-brem.}=28 MeV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_comment:
$|s=0.77 MeV~*b at E{-brem.}=23.5 MeV; |s=1.17 MeV~*b at E{-brem.}=28 MeV. These values contain admixtures from the decay of the {+13}C*(3.854 MeV) state. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$wieghted average from (Bu51: 870 keV {I50}), (Wa52: 883 keV {I11}) and (1960Ri05: 878 keV {I6}). See also E{-x}=870 keV {20} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations.) 
L$See (1961Ci02,1962Ta07,1968Pr04,1976Bi03). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$wieghted average from (Bu51: 3030 keV {I60}), (Wa52: 3069 keV {I10}) and (1960Ri05: 3071 keV {I12}). See also E{-x}=3060 keV {30} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reactions calculations.) 
L$See (1968Pr04). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$FWHM=21.52 {I21} 
E$See also E{-x}(keV)=3830 {I40} (Bu51), 3850 {I30} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations), 3856 {I11} (Wa52) and 3866 {I10} (1960Ri05). 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
$FWHM=48.2 {I17} 
E$See also E{-x}(keV)=4560 {I30} (Bu51), 4580 {I20} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations), 4567 {I14} (Wa52) and 4570 {I30} (1960Ri05). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_comment:
$FWHM=93.4 {I26} 
E$See also E{-x}(keV)=5080 {I30} (Bu51), 5070 {I20} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations). 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$FWHM=21.6 {I5} 
E$See also E{-x}(keV)=5310 {I60} (Bu51), 5310 {I20} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations), 5229 {I13} (Wa52), 5245 {I12} (1960Ri05) and (1965El01: 5.23+5.40 MeV unresolved). 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_comment:
$FWHM=21.97 {I14} 
E$See also E{-x}(keV)=5660 {I30} (Bu51), 5760 {I20} (Bu511: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations), 5723 {I14} (Wa52) and 5726 {I8} (1960Ri05). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$FWHM=21.97 {I14} 
E$See also E{-x}(keV)=5758 {I15} (1960Ri05) and (1965El01: 5.71+5.86+5.85 MeV unresolved). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$FWHM=139 {I4} 
E$See also E{-x}(keV)=6210 {I30} (Bu51) and 6240 {I20} (Bu51: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations). 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_comment:
$FWHM=18.8 {I7} 
E$See also E{-x}(keV)=6910 {I30} (Bu51), 6890 {I30} (Bu511: mean energy value of {+19}F(d,|a) and {+16}O(d,p) reaction calculations) and 6869 {I14} (Wa52). 


level_energy_unit: KEV
level_comment:
$FWHM=19.8 {I5} 
$Unresolved E{-x}=7379 (5/2+) and 7382 (5/2-) states. 
E$See also E{-x}(keV)=(7371 {I15}) (Wa52). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
T$From |t=159{++40}{--30} fs and E|g=2184.3{++3}{--2} keV (2020Ci03: |t=159{++40}{--20} fs, 2020Zi03, 2021Ci02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2-
level_lifetime_unit: FS
level_comment:
T$from (2021Ci02: Fig. 21); |t=20 fs {I20} assuming E{-|g}=3842.3 keV {I4} from ENSDF; see also |t<26 fs (1964Al11). 
$No well-defined minimum is found for |h{+2}, but a valley extending from 0-70 fs is seen with a strong dependence on the E{-|g} (2021Ci02). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
S$The relative spectroscopic factor is deduced using the entrance channel optical potential parameters of (2006An14). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1-)
level_comment:
$Found as a broad bump at 3 MeV in |b{+-} delayed |a spectra. Origin unclear, can be several unresolved J|p=1- states or a new broad J|p=1- state in {+18}O 1989Zh04. 


level_energy_unit: KEV
level_comment:
$|s(tot)=131 |mb {I2} 
$Unresolved doublet. J|p assignments are (2-),3- for the 6351 and 6404 keV levels respectively. 


level_energy_unit: KEV
level_comment:
This is the average of several unresolved levels. The main components are at 8.96 and 9.03 MeV. 1985Fo11 


level_energy_unit: KEV
level_spin_parity: 5-
level_lifetime_unit: KEV
level_comment:
J$See discussion in (2019Ya07) and (1984Ra07,2002Cu04). 
$|q{+2}{-|a}=0.02 (if 4+: see 2014Av04); =0.07 (if 5-). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: KEV
level_comment:
J$See discussion in (2019Ya07) and (1984Ra07,2002Cu04). 
$|q{+2}{-|a}=0.56 (if 6+: see 2014Av04,1984Ra07) 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$|q{+2}{-|a}=0.10 (if 2+: see 2014Av04,2006Yi01,2002Cu04); =0.50 (if 5-: see 2014Av04); =0.14 (if 3-: see 2014Av04). 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$|q{-|a}{+2}=0.004 (using |G=8 keV from 1995Ti07) 
J$|G{-|a}/G<0.10 is consistent with the unnatural parity 2{+-} assignment 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$|q{-|a}{+2}=0.08 (using |G=5 keV from 1995Ti07) 
J$|G{-|a}/|G=0.19 is in conflict with the unnatural parity 4- assignment. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: KEV
level_comment:
$|q{-|a}{+2}=0.009 , |G{-2n}/|G<0.26 
J$|G{-|a}/|G=0.48 is in conflict with the unnatural parity 4- assignment. 


level_energy_unit: KEV
level_spin_parity: (6-)
level_lifetime_unit: KEV
level_comment:
$|q{-|a}{+2}=0.05 , |G{-2n}/|G=0.32 {I8} 
J$|G{-|a}/|G=0.46 is in conflict with the unnatural parity 6{+-} assignment. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_comment:
T$Weighted average: 27.2 s {I3} (1965Bo42), 26.76 s {I8} (1967Yu01), 26.5 s {I1} (1968Re04),27.7 s {I1} (1970Al21) 


level_energy_unit: KEV
level_comment:
$Corresponds to two unresolved states. Assuming one of these to be a 3/2- state, the other should have J=7/2 to 13/2. 


level_energy_unit: KEV
level_comment:
$Cross section is too large for the known state at this energy with J|p=3/2+. If this group corresponds to a doublet, the other member should have J=1/2 to 5/2 


level_energy_unit: KEV
level_comment:
$Total cross section to this state is very high implying unresolved states: if there are two states one must have J>13/2 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.25 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.16 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.79 |mb/sr 7 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.37 |mb/sr 4 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.27 |mb/sr 8 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.79 |mb/sr 5 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.18 |mb/sr 8 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.72 |mb/sr 5 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.78 |mb/sr 9 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.82 |mb/sr 5 


level_energy_unit: KEV
level_spin_parity: (9/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=4.27 |mb/sr 14 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.97 |mb/sr 8 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.58 |mb/sr 11 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.61 |mb/sr 7 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.90 |mb/sr 12 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.72 |mb/sr 8 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=4.27 |mb/sr 14 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.66 |mb/sr 7 


level_energy_unit: KEV
level_spin_parity: (11/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=7.23 |mb/sr 19 
$d|s/d|W{-cm}(|q{-lab}=39|')=3.87 |mb/sr 10 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=6.22 |mb/sr 17 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.25 |mb/sr 9 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=5.16 |mb/sr 19 
$d|s/d|W{-cm}(|q{-lab}=39|')=3.05 |mb/sr 10 


level_energy_unit: KEV
level_spin_parity: (13/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=13.8 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.55 |mb/sr 9 


level_energy_unit: KEV
level_spin_parity: (11/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=9.4 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.34 |mb/sr 12 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.95 |mb/sr 15 
$d|s/d|W{-cm}(|q{-lab}=39|')=3.83 |mb/sr 10 


level_energy_unit: KEV
level_spin_parity: (15/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=13.2 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.99 |mb/sr 12 


level_energy_unit: KEV
level_spin_parity: (13/2-)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2- Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=9.64 |mb/sr 24 
$d|s/d|W{-cm}(|q{-lab}=39|')=8.30 |mb/sr 17 


level_energy_unit: KEV
level_spin_parity: (17/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$K|p=3/2+ Cluster Band. 
$d|s/d|W{-cm}(|q{-lab}=20|')=9.7 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=7.26 |mb/sr 15 


level_energy_unit: KEV
level_spin_parity: 9/2+
level_lifetime_unit: FS
level_lifetime_info: ;ERR=GT
level_comment:
T$from |t>400 fs and E{-|g}=2370.6 keV {I+5-3} (2021Ci02). See also |t>400 fs (2020Ci02,2020Ci03), |t>3.5ps (1971Hi06), T{-1/2}>2400 fs in ENSDF. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
T$from |t=140 fs {I+50-40} and E{-|g}=2779.0 keV {I+10-8} (2020Ci02,2020Ci03,2021Ci02). See also |t=117 fs {I26} (1971Hi06) and 70 fs {I26} (1971Br02) which gives the average of |t=92 fs {I19}, T{-1/2}=64 fs 13 in ENSDF. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=0.95 |mb/sr 15 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.7 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.33 |mb/sr 7 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=4.1 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=3.9 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.8 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=0.76 |mb/sr 11 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.2 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.50 |mb/sr 6 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.6 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.5 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.66 |mb/sr 7 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$K|p=0{++}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=1.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.0 |mb/sr 1 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=2.3 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.2 |mb/sr 1 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$K|p=0{++}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=6.3 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=6.7 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.4 |mb/sr 2 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.3 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.7 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.24 |mb/sr 8 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=0.25 |mb/sr 7 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.3 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.13 |mb/sr 5 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=12.3 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=9.7 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=7.2 |mb/sr 2 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.2 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.9 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.5 |mb/sr 1 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=0.7 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.6 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.04 |mb/sr 3 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=3.1 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=3.1 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.5 |mb/sr 2 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=11.8 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=11.8 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.5 |mb/sr 2 


level_energy_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=7.1 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=10.0 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.1 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$K|p=0{++}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=9.5 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=10.2 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=6.8 |mb/sr 3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.6 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.1 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.0 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.0 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.5 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.6 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.4 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.36 |mb/sr 4 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=12.1 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=14.8 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.6 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=0.9 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.0 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.37 |mb/sr 5 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|'): contamination line 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.9 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.4 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=5.5 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=4.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.9 |mb/sr 1 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=1.1 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|'): contamination line 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=1.0 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.7 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.0 |mb/sr 1 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=16.0 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=21.7 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=39|')=11.8 |mb/sr 3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=2.0 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|'): contamination line 
$d|s/d|W{-cm}(|q{-lab}=39|'): contamination line 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.3 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|'): contamination line 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.0 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|'): shielding plate 
$d|s/d|W{-cm}(|q{-lab}=20|')=12.2 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=6.1 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=7.2 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=11.4 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.5 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=13.5 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=13.4 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=7.3 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=3.0 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.2 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.6 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=4.1 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=3.5 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.8 |mb/sr 1 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=6.1 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=20|')=4.5 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=4.0 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.0 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.5 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.3 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=3.2 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=5.3 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=3.7 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=6.6 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=6.8 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=6.1 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=1.3 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=20|')=0.9 |mb/sr 1 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.6 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=23.5 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|')=16.9 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=39|')=16.5 |mb/sr 3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')<0.2 |mb/sr 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.2 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.9 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=6.6 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=4.0 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.8 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=11.4 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|')=8.0 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.9 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=6.3 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=12.2 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.4 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=29.3 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|')=16.4 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=16.9 |mb/sr 3 


level_energy_unit: KEV
level_spin_parity: (5-)
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=16.1 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=20|')=15.7 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=7.5 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=21.1 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=20|')=15.0 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=10.1 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=2.2 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=1.4 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.5 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=2.0 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.1 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|')=1.7 |mb/sr 1 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|'): contamination line 
$d|s/d|W{-cm}(|q{-lab}=20|')=5.5 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=0.3 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=10.2 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=8.2 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.0 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=10.6 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=7.9 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.6 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=3.8 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|'): overlap 
$d|s/d|W{-cm}(|q{-lab}=39|'): overlap 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=18.9 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=20|')=12.8 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=39|')=10.3 |mb/sr 3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=15.0 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=2.0 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=39|'): contamination line 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=15.3 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=9.3 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=2.8 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (8+)
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=16.8 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=21.7 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=39|')=9.2 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=16.9 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=25.2 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=39|')=11.9 |mb/sr 3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=9.5 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=5.4 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=5.7 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=8.1 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=6.0 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=6.1 |mb/sr 2 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=6.2 |mb/sr 2 
$d|s/d|W{-cm}(|q{-lab}=20|')=3.6 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=39|')=3.4 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: (7-)
level_lifetime_unit: KEV
level_comment:
$K|p=0{+-}{-2} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=25.9 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|')=17.6 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=39|')=14.6 |mb/sr 3 


level_energy_unit: KEV
level_spin_parity: (10+)
level_lifetime_unit: KEV
level_comment:
$K|p=0{++}{-4} rotational band. 
$d|s/d|W{-cm}(|q{-lab}=10|')=26.9 |mb/sr 5 
$d|s/d|W{-cm}(|q{-lab}=20|')=28.9 |mb/sr 7 
$d|s/d|W{-cm}(|q{-lab}=39|')=11.8 |mb/sr 3 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$d|s/d|W{-cm}(|q{-lab}=10|')=11.2 |mb/sr 3 
$d|s/d|W{-cm}(|q{-lab}=20|')=7.9 |mb/sr 4 
$d|s/d|W{-cm}(|q{-lab}=39|')=6.4 |mb/sr 2 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
$This level is populated in Branching Ratio (BR)=0.28 {I6} of 1n-knockout reactions at E/A|?700 MeV. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
T$From 1981Al07 
J$From single-particle removal cross section compared to extended Glauber model calculations, weighted by shell model spectroscopic factors (2000Sa47,1989Ca25). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$C{+2}S=0.58 {I14} 
J$3/2+, 5/2+ from L=2, but 5/2+ strength is considered exhausted by the L=2, 5/2+ g.s. 
E$Neutron unbound state corresponding to E{-res}=0.96 MeV {I10} with |G=0.46 MeV {I20}. 


level_energy_unit: KEV
level_spin_parity: (3/2+,7/2-)
level_comment:
$C{+2}S=0.30,0.20 
L$L=2 fit is better than L=3 
S$0.30 {I7} for L=2. {I0}.20 {I5} for L=3 
E$Neutron unbound state corresponding to E{-res}=2.36 MeV {I11} with |G=0.32 MeV {I26}. 
J$Level energy is consistent with J|p=1/2-, 3/2- level observed in {+21}N |b decay. As the L-transfer is indeterminate, the evaluator has assumed it is the same level observed in decay. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_comment:
T$value given in 2020He25 is 290 ps {I+24-22} (stat) {I+24-8} (syst) from RDDM measurement; uncertainties added in quadrature by compiler. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J$ Based on a simple shell model, the authors consider assignments of 5/2+ and 1/2+ depending on whether the neutron configuration in {+21}O is like {+23}Ne or {+19}C, respectively. The g factor was calculated as g{-exp}({+21}O{-g.s.})=0.6036 {I14} and compared to g factors corresponding to both options to support the assignment of J{-|p} = 5/2+ 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$From 2005We06. Other values: 2.25 s {I15} (1989Hu07), 0.91 s {I35} (1982Mu08), and 2.9 s {I15} (1986Du07) 
%B-N$from 1991Re02. Other reference: 1979Ba31. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$3199|g E2 to 0+. 
T$From B(E2)|^=0.0021 {I8} {+197}Au({+22}O,{+22}O') (2000Th11) and adopted |g-ray properties. Other: Also 0.56 ps {I26} from B(E2)|^=0.0015 {I7} in 2000Th11. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From B(E2)|^=0.0021 {I8} (2000Th11) and adopted |g-ray properties. Other: Also 0.56 ps {I26} from B(E2)|^=0.0015 {I7} in 2000Th11. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$From |g-ray energy (2006El05). Other: 3200 keV {I200} (2006Be04) 
$Deformation parameter |b(p,p')=0.26 {I4}, smaller than those for {+20}O and {+18}O. This result indicates a weak neutron contribution to the 2+ state (2006Be04). 
$Deformation parameter |b(d,d')=0.23 {I2} and {+22}O+{+2}H reaction cross section |s(0{++} |) 2{++})=19 mb {I3} (2006El05) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Inclusive two-neutron removal |s{-exp}=146 mb {I33}, with FWHM=309 MeV/c {I36} from associated parallel momentum distribution of the cross section (2018Di09) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
$<r{+2}>{+1/2}({+23}N)=2.95~fm~{I23} (matter radius) (2011Ka36) using Fermi density and 2.97 fm {I11} using harmonic oscillator density; deduced using Glauber model (2011Ka36). Also 3.20 fm {I4} and 3.24 fm {I27} in 2001Oz03. 
J$L=0 from analysis of single neutron removal cross sections in ({+23}O,{+22}O). 
$Configuration: |ns{-1/2} (2007El02 - {+2}H({+22}O,P)) 
T$From 2007Su05. Others: 82~ms~{I+45-28} (1990Mu06), 89~ms~{I76} (2008ReZZ, 1995ReZZ). 
%B-N$From 2007Su05. Others: 31~{I7} (1990Mu06), 28~{I30} (2008ReZZ, 1995ReZZ), and <29 (1991Re02). 


level_energy_unit: KEV
level_spin_parity: (5/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From {+1}H({+24}O,{+23}O). 
J$L=2 (longitudinal momentum distribution - {+1}H({+24}O,{+23}O)). Configuration: |n(0d{-5/2}){+-1} ({+26}Ne,2pnX) - (2007Sc32,2008Fr10). 
$|G: From ({+26}Ne,2pnX) - 2008Ch07. Other: |G=100~keV (2007Sc32 - ({+26}Ne,2pnx)) and (2011Ho05 - ({+26}F,2n{+22}O)) - value should be considered as upper limit - see comments in ({+26}Ne,2pnx). Same research group - 2007Sc32 and 2011Ho05. 


level_energy_unit: KEV
level_comment:
$It is a state in fp shell. Possible configuration: |np{-3/2} with S |? 1.0. Also a smaller probability for |nf{-7/2} with S |? 0.02. (2007El02 - {+2}H({+22}O,p{+23}O)). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J,L$From analysis of single neutron removal cross sections determined from {+22}O |g-ray emission yields and compared to theoretical models based on the Eikonal approximation (2004Co11, 2005Co24). 2002Ka20 propose 1/2+ or 5/2+. 2000Sa47 propose 1/2+ from their work. 
S$C{+2}S from 2005No01 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$C{+2}S=4.1 {I4} 
E$deduced from measured E(resonance)=50 keV {I3} (2014Ts04), and S(n)({+23}O)=2730 keV {I130} (2017Wa10). 
L,J$from longitudinal momentum distribution 
$|s{-1n}(expt)=61 mb {I6} (2014Ts04) 
S$deduced from experimental |s and single-particle |s calculated using distorted wave impulse approximation (DWIA) and eikonal approximation. 


level_energy_unit: KEV
level_comment:
$ It is a state in fp shell. Possible configuration |np{-3/2} with S |? 1.0. Also a smaller probability for |nf{-7/2} state with S |? 0.02. 
$ |s=0.33 mb {I10} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s{-1n}(expt)=74 mb {I11} 
$Determined a FWHM of 115~MeV/c {I13} for the intrinsic {+23}O parallel momentum distribution by fitting the measured values. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2)+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$ from observed neutron-neutron sequential emission of {+22}O fragment -nn coin; first neutron with E(n)|?0.6 MeV from a level at |?7.5 MeV in {+24}O, the second with E(n)<0.1 MeV from a 2.8 MeV level in {+23}O, the latter considered as 45 keV {I2} resonance in {+23}O (2011Ho05) 
$L,|G: assumed value for Breit-Wigner line shape to describe two resonances for simulating the sequential decay of E=600-keV resonance in {+24}O through this state using Monte Carlo simulations. 
$Decays by neutron to {+22}O g.s. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$ This state decays mainly by neutrons. Calculated partial |g-ray width=0.15 meV, corresponding to |g-decay lifetime of 4.5 ps 
E,J$ 5/2+ hole state, 45 keV {I2} (2007Sc32,2008Fr10) above S(n). 
$|G{-decay} from 2008Ch07. 2007Sc32 note the width (100 keV) due to experimental conditions overshadows the Wigner limit by about 3 orders of magnitude and so its lifetime was not determined. However, note their calculated value of total decay width |G{-decay}=5 eV is extremely small. [Measured values in 2007Sc32 and 2008Ch07 should be considered as upper limit due to experimental resolution - email communication with co/corresponding author M. Thoennessen (March 10, 2017)]. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
J$From Adopted Levels 
$ Measured momentum distribution has a Gaussian width=99 MeV/c {I4}. 
$ Measured one-neutron removal cross section=63 mb {I7} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$C{+2}S=6.6 {I9} 
J$From Adopted Levels 
S$For {+12}C({+24}F,p{+23}O) 
$ Measured cross section=6.6 mb {I10} for {+12}C({+24}F,p{+23}O), 6.4 mb {I9} for {+12}C({+25}F,pn{+23}O), and 8.9 mb {I24} for {+12}C({+26}F,p2n{+23}O). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$Inclusive one-neutron removal |s{-exp}=74 mb {I11}, with FWHM=115 MeV/c {I13} from associated parallel momentum distribution of the cross section (2018Di09) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$Measured absorption mean radius: r{-0}{+2}=1.213 fm{+2} {I47} (2006Kh08) in Si({+24}O,X) at GANIL facility 
$Measured mean matter radius=3.19 fm {I13} (2001Oz03) in C({+24}O,X) reaction at GSI facility. 
T$Weighted average of 65 ms {I5} (1999Re16 |g(t) (also reported as 67 ms {I10} in 2001Pe14)), 61 ms {I+32-19} (1990Mu06) and 80 ms {I5} (2015Ca09 - from summed intensity time distribution of 521|g, 1309|g, and 1830|g). 
%B-N$Weighted average of 58 {I12} (1990Mu06) and 40 {I4} (from g.s. feeding of %I|g=39 {I4} (1830|g) and %I|g=21 {I2} (521|g) 2015Ca09). 2015Ca09 report 43 {I4} considering 1305|g (not feeding g.s.) %I|g=18 {I3} instead of 521|g %I|g. 2015Bi05 (evaluation) gives 41 {I4}, considering 1.0(4)% g.s. feeding of 1+ states above 1830 keV level (unknown feeding to the g.s.). Other values: 18 {I6} (1999Re16; also reported as 12 {I6} in 2001Pe14). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MEV
level_comment:
E$Weighted average of 4.75 MeV {I21} ({+24}O,p') and 4.77 MeV {I21} ({+26}F,nX). 
J$From |s(|q) distribution and DWBA analysis (2012Ts03); also in agreement with theoretical predictions (2012Br14, 2012Ha19, 2006Vo14). 
$|b{-2} from (p,p') (2012Ts03) 
$Possible configuration: |n1s{-1/2}{+-1}~#|n0d{-3/2}{+1} 
$No |g rays observed in the work of 2004St08 (also 2004St10), suggesting that this state is unbound to particle emission 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: MEV
level_comment:
E$Weighted average of 5.25 MeV {I22} (2012Ts03) and 5.41 MeV {I21} (2009Ho01). Uncertainty - lower input value. 
J$From |s(|q) distribution and DWBA analysis (2012Ts03); also in agreement with theoretical prediction (2012Br14, 2012Ha19, 2006Vo14) 
$Possible configuration: |n1s{-1/2}{+-1}~#|n0d{-3/2}{+1} 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (-)
level_comment:
E$group of states from decay energy (resonance) of |?3.2 MeV (2012Ts03). 2012Ts03 report only one-neutron decay channel 
J$possible configuration: |n1s{-1/2}{+-1}~#|n(fp){+1} 


level_energy_unit: KEV
level_spin_parity: (+)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$From observed resonance at 715 keV {I110} (stat) {I45} (sys) (({+24}O,2n{+22}O) - 2015Jo14) and S(2n)=6.93 MeV {I17} in AME-2020 (2021Wa16). Other: |? 0.6 MeV (({+26}F,nX) - 2011Ho05). 
J$From Monte-Carlo simulations, both resonances (0.6 MeV in {+24}O and 45 keV in {+23}O) have L=2 (0d{-3/2} neutron decay) (2011Ho05) 
$|G from 2011Ho05 ({+26}F,nX). Other: < 2 MeV (2015Jo14 - ({+24}O,2n{+22}O)). 
$Decays by a two-neutron sequential cascade to {+22}O g.s. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$From decay energy (resonance) of 0.56 MeV {I5} (2012Ts03). Other: 5.1 MeV {I3} (2012La23) 
J$From |s(|q) distribution and DWBA analysis 
$|b{-2}=0.15 {I4} (2012Ts03). |s=2.6 mb {I11} (2012Ts03) 
$Configuration: |n1s{-1/2}{+-1}~#|n0d{-3/2}{+1} 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
E$from decay energy (resonance) of 1.06 MeV {I10} (2012Ts03) 
J$From |s(|q) distribution and DWBA analysis 
$|s=2.2 mb {I12} 
$Configuration: |n1s{-1/2}{+-1}~#|n0d{-3/2}{+1} 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (-)
level_comment:
E$group of states from decay energy (resonance) of |?3.2 MeV (2012Ts03). Other: 6.9 MeV {I3} (2012La23) 
$Configuration: |n1s{-1/2}{+-1}~#|n(fp){+1} 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: MEV
level_comment:
E$From decay energy of 583 keV {I59}: weighted average of measured decay energy, 630 keV {I40} (2009Ho01) and 510 keV {I50} (2015Ro16). 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: MEV
level_comment:
E$From decay energy of 1220 keV {I70}: weighted average (unc - input value) of measured decay energy, 1240 keV {I70} (2009Ho01) and 1200 keV {I70} (2015Ro16). 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (+)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$From observed resonance at |? 0.6 (2011Ho05) deduced from the invariant mass equations in coincidence with another decay at E(n)<0.1 MeV, considered as corresponding to a previously observed decay of a 2.8 MeV, (5/2+) state (45 keV {I2} resonance) in {+23}O to the ground state of {+22}O 
L,T$From Monte-Carlo simulations, both resonances (0.6 MeV in {+24}O and 45 keV in {+23}O) have L=2 (0d{-3/2} neutron decay) and |G=0.1 MeV 
$Decays by a two-neutron sequential cascade to the g.s. of {+22}O. 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From observed resonance at 715 keV {I110} (stat) {I45} (sys) and known S(2n)=6.93 MeV {I17} in AME-2020 (2021Wa16). 
T,L$The resonance energy, width and L-transfer were extracted from the best fit to the three-body decay energy spectrum based on Monte-Carlo simulations. 
$Decays by a two-neutron sequential cascade to {+22}O g.s. via an intermediate state in {+23}O at 45 keV, based on measured energy and angular correlations. Each decay proceeds by emission of an L=2 neutron. Neither a di-neutron nor phase-space models were able to reproduce these correlations (2015Jo14). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$Both energy of the resonance and width in 2013Va18 were extracted from analysis of Breit-Wigner distribution with the assumption of L=2 and expected 0d{-3/2} configuration 
E$g.s. of {+25}O is neutron unbound, {+24}O+n, with measured resonance energy of 725 keV {I+54-29} in 2013Ca18. From their measured value and 770 keV {I+20-10} in 2008Ho03 (Phys. Rev. Lett. 100, 152502), 2013Ca18 gave an average value of 768 keV {I+19-9} as the resonance energy of the g.s. of {+25}O. Corresponding S(n)=-776 keV {I15} in (2012Wa38). As pointed out in 2013Ca18, these measurements are in good agreement with theoretical shell-model calculations based on chiral two- and three-nucleon forces carried out in 2013Ca18, and previous calculations by 2006Br18: Phys. Rev. C 74, 034315, and 2006Vo14: Phys. Rev. C 74, 064314. 
T$reported by 2013Ca18 as average of |G=20 keV {I+60-20} (2013Ca18) and |G=172 keV {I30} (2008Ho03) by using a method by B. Barlow, ArXiv-physics/0401042. Corresponding mean lifetime=|t=4.1|*10{+-21} s {I+9-6} or half-life=2.8|*10{+-21} s {I+6-4} 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E,L$neutron-unbond state with neutron-decay resonant energy=830 keV {I170} from a best-fit to measured decay-energy spectrum (2017Jo12) 
J$from L(n)=2 and theoretical predictions. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_uncertain: ?
level_comment:
E,J,T$measured data are consistent with the inclusion of a 1/2+ state predicted by theoretical calculations, with resonance energy=3.3 MeV and width=1 keV, but are insufficient to confirm the observation of this state (2017Jo12). 
$limit for relative cross section: |s{-1/2+}/|s{-g.s.}=0.25 {I+100-25} (2017Jo12). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$ g.s of {+25}O is neutron unbound with a measured resonance of 749 keV {I10}, FWHM 430 keV at 750 keV, includes both statistical and systematic uncertainties. The measured resonance energy by 2016Ko11 is consistent with 725 keV {I+54-29} (2013Ca18 (Phys Rev C 88, 034313)) and 770 keV {I+20-10} (2008Ho03 (Phys. Rev. Lett. 100, 152502)). 
T$ Measured value of 2016Ko11, including both statistical and systematic uncertainties, is consistent with 20 keV {I+60-20} within 2|s of 2013Ca18 (Phys Rev C 88, 034313) value. 2016Ko11 also note that their measured width is close to the calculated value of 63 keV (2014Vo09 (Phys. Atomic Nuclei 77, 969)). Compiler's note: Measured width |G=88 keV {I6} corresponds to half-life=5.2|*10{+-21} s {I4}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$sum of measured neutron energies of 2.3 MeV, 0.65 MeV and 50 keV in a sequence of three neutrons, and the three-neutron separation energy about 6 MeV (2019Sw04) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
E$ 2016Ko11 deduced g.s of {+26}O as unstable to 2-neutron emission, with an adopted resonance value of 18 keV {I10} (stat) {I4} (syst). from their measurements. 
T$From 2013Ko10. Half-life of 4.5 ps {I+11-15} (stat) {I30} (syst) is deduced at 82% confidence level, suggesting the possibility of two-neutron radioactive decay. Evaluators added the uncertainties in quadrature. Other values: |<4.0 ns, from mean lifetime of |t|<5.7 ns (2013Ca18) at 95% C.L.; <10 fs (2013Th04). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$2016Ko11 propose as the first excited state of {+26}O. 
E$From E{-res}=1280 keV {I+110-80} (2016Ko11 list as 1.28 MeV {I+11-8}). Compiler used E{-res}=1295 keV {I95}, with symmetric uncertainty, to deduce the excited level energy. FWHM 540 keV at 1300 keV. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$From 2013Ko10, resonance energy at approximately 2 MeV. Note that position of this state in Figure 1 of 2013Ko10 is based on predictions from the continuum shell model calculations. 


level_energy_unit: KEV
level_comment:
E$Deduced by evaluator from measured E{-r}=4225 keV {I+227-176} (2013Ca18) and considering E{-r}=18 keV {I10} (stat) {I4} (syst) for g.s. Evaluator used E{-res}=4250 keV {I200}, with symmetric uncertainty, to deduce the excited level energy. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
%2n=100 
E$ 2016Ko11 deduced g.s of {+26}O as unstable to 2-neutron emission, with an adopted resonance value of 18 keV {I10} (stat) {I4} (syst). from their measurements. Considering different modes of decay and assumptions, 2016Ko11 deduced resonance energy values of 22 keV {I+14-11}, 18 keV {I3} (stat), 19 keV {I3} (stat), 17 keV {I3} (stat), 19 keV {I+3-4} and conclude that the resonance energy (g.s.) is model independent. FWHM 110 keV at 20 keV (2016Ko11). 2013Ca18 deduced g.s. of {+26}O as unstable to 2-neutron emission, with measured resonance energy of |<120 keV at 95% C.L. and |<40 keV at 68% C.L. 2015Ko08 extracted an upper limit at 1|s of 53 keV for the ground-state resonance energy of {+26}O from simultaneous and self-consistent fitting of the experimental decay energy and the Jacobi three-body correlation variables. Their earlier value 150 {I+50-150} (2012Lu07) was deduced from fit of the experimental three-body decay spectrum with a Monte Carlo simulation including the decay from the ground state and first excited state. 
T$From 2013Ko10. Half-life of 4.5 ps {I+11-15} (stat) {I30} (syst) is deduced at 82% confidence level, suggesting the possibility of two-neutron radioactive decay. Evaluators added the uncertainties in quadrature. In 2013Ko10, fitting of relative velocity distribution of {+24}O and each of the two neutrons with a Monte Carlo simulation and as function of the half-life parameter, with the consideration whether decay of {+26}O occurs in the reaction target or outside the target. Other values: |<4.0 ns, from mean lifetime of |t|<5.7 ns (2013Ca18) at 95% C.L.; <10 fs (2013Th04). 
$Measured cross section=1.8 mb {I10} (2012Lu07) for population of the {+26}O g.s. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
J$2016Ko11 propose as the first excited state of {+26}O. 
E$From E{-res}=1280 keV {I+110-80} (2016Ko11 list as 1.28 MeV {I+11-8}). Compiler used E{-res}=1295 keV {I95}, with symmetric uncertainty, to deduce the excited level energy. FWHM 540 keV at 1300 keV. 2016Ko11 note that the systematic uncertainty associated with the excited state decay energy is negligible compared to the statistical uncertainty. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_uncertain: ?
level_comment:
E$From 2013Ko10, resonance energy at approximately 2 MeV from Figure 1 in 2013Ko10. Note that position of this state in Figure 1 is based on predictions from the continuum shell model calculations. Possible first excited state. 


level_energy_unit: KEV
level_comment:
E$Deduced by evaluator from measured E{-r}=4225 keV {I+227-176} (2013Ca18) and considering E{-res}=18 keV {I10} (stat) {I4} (syst) for g.s. Evaluator used E{-res}=4250 keV {I200}, with symmetric uncertainty, to deduce the excited level energy. 


level_energy_unit: KEV
level_spin_parity: (3/2+,7/2-)
level_comment:
J$tentatively assigned in 2023Ko15 based on the upper limit of the width compared with theoretical predictions. 
$The decay energy reconstructed from the observed {+24}O and three neutrons is 1.09 MeV {I4}(stat){I2}(syst), with an upper limit of the width of the resonance of 0.18 MeV (68% confidence interval), comparable with the estimated experimental resolution of FWHM=0.22 MeV (2023Ko15) 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$The decay energy reconstructed from the observed {+24}O and four neutrons is 0.46 MeV {I+5-4}(stat){I2}(syst), with an upper limit of the width of the resonance of 0.7 MeV (68% confidence interval) (2023Ko15) 
$2023Ko15 conclude this observed resonance is for the ground state of {+28}O but not an excited state since the latter would have an excitation energy of less than 0.46 MeV which is very much lower then theory suggests (2 MeV or more) 
$The cross-section for single-proton removal from {+29}F populating this resonance is 1.36 mb {I+16-4}(stat){I13}(syst) (2023Ko15) 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_spin_parity: (5/2+)
level_lifetime_unit: MEV
level_comment:
$Analysis of the invariant-mass spectrum is consistent with sequential proton decay via {+12}O(0:0{-1}{++}, 2.2 MeV:2{-1}{++}, 4.8 MeV:2{-2}{++}) with intensities of 40% {I16}, 28% {I18} and 32% {I16}, respectively. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
$E(p+{+14}O){-cm} (keV)=1.28E3 {I4} 
E$The value E{-res}=1.28 MeV {I4} is adopted; excited state energies are calculated using this value. The weighted average of all reported resonance energy values is 1.28 MeV {I2} (external uncertainty); this value compares with the Rajeval technique value (1.29 MeV {I3}) and the Method of Best Representation (see 2014Bi13) value (1.37 MeV {I13}). A critical scrutiny of some of the data may suggest exclusion of some results, such as those from (1978Be26,1978Ke06,2008Mu13), but these have little impact on the values deduced using the weighted average or Rajeval techniques. 
T$The values |G>900 keV (1978Be26) and |G|?1200 keV (2003Pe23) are not considered, and a 20% uncertainty is assigned to |G|?700 keV from 2004Go15. This yields the weighted average |G=660 keV {I20}. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p+{+14}O){-cm} (keV)=2798 {I24} 
E$The value E{-res}=2798 keV {I24} is deduced using the Method of Best Representation; this value is accepted. This compares with the weighted average of all values, E{-res}=2785 keV {I10}, and the value deduced using the Rajeval technique, 2797 keV {I11}. An analysis was carried out in 2016De15 that recommended 2794 keV {I16}. 
T$from the weighted average of all values. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (keV)=6.4E3 {I2} 
E,T$from (2009Mu09,2010Mu12). 
J$3/2- favored from arguments based on the mirror {+15}C nucleus. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
$E(p+{+14}O){-cm} (keV)=1.29E3 {IAP} 
E$The authors give a discussion on the {s}-wave scattering, which highlights a difference between the resonance peak cross section energy (1.29 MeV {I+8}{I-6}) and the maximum of the wavefunction amplitude (1.45 MeV {I+16}{I-1}). This effect also impacts the |G value, which is observed with FWHM|?1.2 MeV. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (keV)=1270 {I14} 
E$This resonance was observed at E{-R}=1270 keV {I10}(stat) {I10}(sys). 
T$The observed width was |G=376 keV {I70}(stat) {I+200-0}(sys). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p+{+14}O){-cm} (keV)=2763 {I13} 
E$This level was deduced from E{-R}=2763 keV {I9}(stat) {I10}(sys) with E{-R}=1270 keV {I10}(stat) {I10}(sys) for the g.s. 
$In 2016De15, the authors note that using the statistical procedure outlined by the Particle Data Group to evaluate all reported energies for this resonance they find E{-R}=2794 keV {I16} and |G=301 keV {I16} for this state. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
$E(p+{+14}O){-cm} (keV)=4757 {I12} 
E$This level was deduced from E{-R}=4757 keV {I6}(stat) {I10}(sys) with E{-R}=1270 keV {I10}(stat) {I10}(sys) for the g.s. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$E(p+{+14}O){-cm} (MeV)=1.5 {I1} 
E$This group of counts is observed in (p{-1}-{+14}O)(p{-2}-{+14}O) correlations from {+16}Ne breakup. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (MeV)=2.80 {I5} 
E$This group is observed in (p{-1}-{+14}O)(p{-2}-{+14}O) correlations from {+16}Ne breakup. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (MeV)=4.9 {I2} 
E$This group is observed in (p{-1}-{+14}O)(p{-2}-{+14}O) correlations from {+16}Ne breakup. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2-)
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (MeV)=6.4 {I2} 
E$This group is observed in (p{-1}-{+14}O)(p{-2}-{+14}O) correlations from {+16}Ne breakup. 
J$3/2- favored from arguments based on the mirror {+15}C nucleus. 


level_energy_unit: KEV
level_spin_parity: (3/2+,5/2+)
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (MeV)=7.8 {I2} 
E$from Q{-2p}({+15}F)=3.2 MeV {I2} group observed in (p{-1}-{+13}N)(p{-2}-{+13}N) correlations. This group is associated with decay via the {+14}O J|p=2+ state at E{-x}=6.59 MeV. Decay to the {+14}O{-g.s.} is weak, with an upper limit of decay via {+14}O{-g.s.}/{+14}O(2+)<0.2. The state corresponds to Q{-1p}({+15}F)=7.8 MeV {I2}. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=GT
level_comment:
$E(p+{+14}O){-cm} (keV)=1.6E3 {I2} 
E$mass excess=16.9 MeV {I2}. 
$The lack of a minimum between the ground and first excited states makes a mass excess determination difficult. Likewise, the lack of an angular momentum barrier for the s{-1/2} state results in a large tail toward higher energies and complicates quantification of the width. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
$E(p+{+14}O){-cm} (keV)=2802 {I25} 
E$mass excess=18.088 MeV {I25}. The value for this resonance energy is sometimes not rigorously deduced; see for example 2005Fo10 who list E{-res}=2.8 MeV with 200 keV uncertainty. This value has been carried over into other analyses. The resonance energy is derivable with 25 keV resolution using the known p and {+14}O mass excesses. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (MeV)=1.37 {I18} 
E$The Q(|b{+-})value is Q=-29.73 MeV {I18} and mass excess=16.67 MeV {I18}. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MEV
level_comment:
$E(p+{+14}O){-cm} (MeV)=2.67 {I10} 
E$The resonance energy is not rigorously discussed in the text; the Q(|b{+-})value to the state is not given. Instead the comment, "the excitation energy of the first excited state is 1.3|+0.1 MeV" is given in the text. The evaluator assumes the mass excess is then |Dm=(16.67+1.30)|+0.10 MeV=17.97|+0.10 MeV, which corresponds to a resonance energy E{-res}=2.67|+0.10 MeV. 
E$In a comparison to the mirror nucleus, the excitation energy is 500 keV higher than the excitation energy of the first excited state in {+15}C. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$From E{-c.m.}=1270 keV {I14} (2016De15) 
${+14}O(0{++})~#p({Is}{-1/2}) (C{+2}S=0.89 {I11}) configuration is assumed 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: KEV
level_comment:
E$From E{-c.m.}=2.81 MeV {I12} 
${+14}O(0{++})~#p({Id}{-5/2}) (C{+2}S=0.75 {I25}) configuration is assumed 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_comment:
E$From E{-c.m.}=4.88 MeV {I21} 
${+14}O(0{++})~#p({Ip}{-1/2}) (C{+2}S=0.0060 {I7}) configuration is assumed 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_lifetime_unit: KEV
level_comment:
E$From E{-c.m.}=5.93 MeV {I10} 
${+14}O(0{++})~#p({If}{-5/2}) (C{+2}S=0.0030 {I15}) + {+14}O(1{+-})~#p({Id}{-5/2}) (C{+2}S=0.70 {I35}) configuration is assumed 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: KEV
level_comment:
E$From E{-c.m.}=6.33 MeV {I13} 
J$From Legendre polynomial fit 
${+14}O(0{++})~#p({Ip}{-3/2}) (C{+2}S=0.0010 {I5}) + {+14}O(1{+-})~#p({Id}{-5/2}) (C{+2}S=0.30 {I15}) configuration is assumed 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: KEV
level_comment:
E$the ground state energy was measured as S{-p}=-534 keV {I5}; this compares with S{-p}=-536 keV {I8} from AME-2012 (2012Wa38). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
E$S{-p}=-527 keV {I7} is deduced, which compares with S{-p}=-536 keV {I8} from (2017Wa10) 
WIDTH$|G=20.6 keV {I57} from a detailed analysis of the 2p correlations, while |G=21.3 keV {I51} is obtained from a more straightforward analysis of the {+17}Ne*(1.76 MeV) invariant mass spectrum. 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: KEV
level_comment:
E$In the present experiment, the ground state is found at E'=518 keV {I9}, which is 13 keV below the value E'=531 keV {I5} that is reported in (2021Wa16). Here we use E'=518 keV {I9} so the g.s. is at zero; (2023Ch22) used E'=531 keV {I5} resulting in a 13 keV energy shift. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: KEV
level_comment:
E$From E'-S{-p}=E{-rel.}(p+{+15}O)+E({+15}O{+*})-S{-p}= 773 keV + 5241 keV -518 keV =5496 keV 
J$Suggested analog of {+16}N{+*}(5.231 MeV: J|p=3{++}). 


level_energy_unit: KEV
level_spin_parity: 0-
level_comment:
S$For the s-wave protons coupled to {+15}O in {+16}F(0,193 keV), |s=8.61 mb {I77} on the hydrogen target and C{+2}S=0.739 {I66}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_comment:
S$For the d-wave protons coupled to {+15}O in {+16}F(424,721 keV), |s=12.30 mb {I76} on the hydrogen target and C{+2}S=1.343 {I83}. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
J,L$The contribution of the {+17}F(g.s., 5/2{++}) to the observed, unresolved angular distribution of g.s.+first excited state was dominated by L=2. 
$ANC{+2}(r{-0}=1.25 fm)=8.2 {I8}. 
$C{+2}S{-exp}(HFB)=1.04 {I10}, ANC{+2}{-HFB}=8.1 {I8}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_comment:
J,L$The contribution of the {+17}F(495 keV, 1/2{++}) (populated with an orbital angular momentum transfer of L=0) to the observed, unresolved angular distribution of g.s.+first excited state could only be distinguished at the most two forward angles around |q{-c.m.}=5|'. 
$ANC{+2}(r{-0}=1.25 fm)=15.5 {I12}. 
$C{+2}S{-exp}(HFB)=0.14 {I1}, ANC{+2}{-HFB}=15.3 {I12}. 
$Since this level was unresolved from the ground state, the given mean spectroscopic factors and ANC{+2} values should be treated as upper limits. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|G(c.m.)=0.8 keV {ILT} 
$This resonance corresponds to two states at 6240 and 6242 keV. The lower member of the doublet (both of which have J|p=3- and mixed isospin) has |G|a=133 eV {I4}, |G{-|g}=0.80 eV {I11}; the higher has |G|a=137 eV {I11}, |G{-|g}=0.73 eV {I11} 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$|G(c.m.)=0.19 keV {I3} 
$This corresponds to a doublet of 3-, mixed isospin states, separated by 2.09 {I4} keV. |w g=2.04 {I45} eV for the lower resonance and 1.16 {I26} eV for the higher one 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_comment:
$|G(c.m.)=0.18 keV {I4} 
$This corresponds to a doublet of 3-, mixed isospin states, separated by 2.09 {I4} keV. |w g=2.04 {I45} eV for the lower resonance and 1.16 {I26} eV for the higher one 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
Branching(0+ -->0+)=0.0770 {I21}, Q(0+ -->0+)=3401.99 keV {I60} 
I|g(660|g)/I|g(1042|g)=0.0171 {I3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_comment:
J$from 1995Ti07. 
$(2J+1)|G{-p}|G{-|g}/|G=0.31 eV {I4}. This compares with (2J+1)|G{-p}|G{-|g}/|G=0.36 eV {I10} (1973Ro03). 


level_energy_unit: KEV
level_comment:
E$ from E{_R}=60 keV {I5} (2010Se13) 
|w|g=3.66|*10{+-9} eV {I+76-64}. Using the Trojan Horse Method, |w|g for the E{-x}=5666 keV state is determined by comparison with |w|g of the E{-x}=5781 keV state. 
An alternate value |w|g=4.21|*10{+-9} eV {I+87-73} is deduced based on assumptions of the effect of electron screening. 


level_energy_unit: KEV
level_comment:
E$ from E{_R}=175 keV {I5} (2010Se13) 
|w|g=1.66|*10{+-3} eV {I10} (weighted average of literature values). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_comment:
$|w|g=1.67 |meV {I12} from activation analysis; uncertainty is statistical + systematic. (|w|g=1.65 |meV |+1.8% (stat) |+7.8% (syst)) and from prompt |g-ray analysis (|w|g=1.70 |meV |+3%(stat) |+7.7%(syst)). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
T$from DDEP evaluation, as quoted by 2012Ha35. However, the DDEP evaluation did not include the measured value of 109.723 min {I11} in 2010Ga04: App Rad & Iso 68, 1561. Value measured in 2012Ha35 is 109.72 min {I19} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MIN
level_comment:
T$from decay curve for 400-keV |g ray (2014Di01). Other: 109 min {I3} (2014Di01,from decay curve of 250-keV |g ray) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_comment:
E$from E(p)(c.m.)=183 keV and S(p)({+18}F)=5607.1 keV {I5} (2012Wa38). E(level)=5786 in Adopted Levels for {+18}F in ENSDF database 
$Resonance strength |w|g=1.67 |meV {I12} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: FS
level_comment:
$E(resonance)(lab)=193 keV 
E$from 2005Fo03 (Phys. Rev. C71, 055801) and 2007Ch25 (Phys. Rev. C75, 035810) 
$|w|g=1.86 meV {I13}, which is the mean of the singles and coincidence values (1.82 meV {I13} and 1.89 meV {I14}, respectively). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4-
level_comment:
$E(resonance)(lab)=518 keV 
$|w|g=13.7 meV {I10}, which is the mean of the singles and coincidence values (14.5 meV {I10} and 12.9 meV {I9}, respectively). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
E$from E{-c.m.}(res)=65.1 keV {I5}. Other: E{-c.m.}(res)=60 keV {I5} (2010Se13: Phys Rev C 82, 032801(R)) 
|w|g=(3.42|+0.60)|*10{+-9} eV. Using the Trojan Horse Method, |w|g for the E{-x}=5666 keV state is determined by comparison with |w|g of the E{-x}=5781 keV state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_comment:
E$from E{-c.m.}(res)=183.35 keV {I25}. Other: E{-c.m.}(res)=175 keV {I5} (2010Se13) 
|w|g=(1.67|+0.07)|*10{+-3} eV (weighted average of literature values). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=?
level_comment:
E$from E{-p}=194.8 keV {I3} and S{-p}=5607.1 keV {I5} (2012Wa38). 
$|w|g=1.68 meV {I3}{-stat} {I12}{-sys}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$|G{-p}=40|+6(stat)|+3(sys) neV. 
$|G{-p} deduced from |w|g=10.0|+1.4(stat)|+0.7(sys) neV and assuming |G{-|a}|?|G=130 eV {I5} (1980Ma26). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
$|G{-p}=39|*10{+-9} eV {I8} (stat.) {I3} (sys.) (2024Ge04). Note that the authors have reported |G{-p}=39|*10{+-9} eV {I9}, where the quadrature sum of statistical and systematic uncertainties are rounded up. 
$|w|g{-(p,|g)}=34|*10{+-12} eV {I7} (stat.) {I3} (sys.) (2024Ge04). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_comment:
E$ possible analog of the 7076-keV level in {+19}Ne, but the widths of the two states are incompatible. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$The 2s{-1/2} and 1d{-5/2} spectroscopic factors of (2J+1)S{-n}: 0.64 {I2} and 0.55 {I3} are deduced, respectively. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$The 2s{-1/2} and 1d{-5/2} spectroscopic factors of (2J+1)S{-n}: 0.67 {I2} and 0.06 {I1} are deduced, respectively. 


level_energy_unit: KEV
level_comment:
$The 2s{-1/2} and 1d{-5/2} spectroscopic factors of (2J+1)S{-n}: 0.75 {I3} and 0.41 {I2} are deduced, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E,T$from Adopted Levels of {+19}F in ENSDF database. 
J$from 2008La13 
$|w|g|<7.8|*10{+-9} eV (90% confidence) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E$from E{-p}=151.2 keV {I3} and S{-p}=7993.600 keV {I1} (2012Wa38). 
$|w|g=164.2 meV {I9}{-stat} {I+121-117}{-sys} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$Analysis of the data gives |w|g(singles)=1.07 meV {I8} and |w|g(coinc.)=1.03 meV {I7}, which yields the mean value of |w|g=1.05 meV {I8}. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$member of a doublet with J|p=5/2+ and 7/2+ from J|p=3+, isospin T=0 parent state at 937 keV in {+18}F. Second member with J|p=7/2+, predicted at 1289 keV from shell-model calculations is not seen in the present work. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
E$member of a doublet with J|p=1/2- and 3/2- from J|p=0-, isospin T=0 parent state at 1081 keV in {+18}F. Second member with J|p=3/2- is not seen in the present work. 
E$other: 1268.3 {I15} from sum of 952.8 and 315.5 gamma rays. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$ANC=0.315 fm{+-1} 
E$Previous measurements by (1970Gr04,1970Sc25) indicated {+19}F{+*}(4556: J{+|p}=3/2-) was populated in this reaction, however the present angular distributions are consistent with the lower {+19}F{+*}(4550: J{+|p}=5/2+) state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$ANC=0.0688 fm{+-1} 
J$The present results are in better agreement with the J{+|p}=5/2+ assignment from (1995Ti05) than J{+|p}=7/2- from (1970Gr04,1970Sc25). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
E$6095 keV in Fig. 2. 
$ANC=0.814 fm{+-1} 
J$J{+|p} is consistent with (1/2-,3/2-); J{+|p}=3/2- is assumed in the analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 7/2-
level_comment:
$ANC=0.00619 fm{+-1} 
J$The state is weakly populated, but the analysis favors J{+|p}=7/2- compared to (5/2+,7/2-) in (1970Sc25). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
E$7120 keV in Fig. 2. 
$ANC=0.0313 fm{+-1} 
J$The angular distribution is inconsistent with J{+|p}=7/2+, which was adopted in (1995Ti07). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: EV
level_comment:
$|G{-|a}=121 eV {I5}. 
S$=90.3 keV {I3} from present thick-target analysis. 
$|w|g=1.57|*10{+-3} meV {I14}(stat){I12}(sys). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
$|G{-|a}=12 eV {I1}. 
$|w|g=2.37 meV {I12}(stat){I18}(sys). 
S$=204.7 keV {I3} from present thick-target analysis. 
T$From weighted average of values deduced from Table 1. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: EV
level_comment:
$|G{-|a}=1.9 keV {I1}. 
S$=317.2 keV {I3} from present thick-target analysis; notice truncation typo in table 1. 
$|w|g=85 meV {I9}(stat){I7}(sys). 
T$From weighted average of values deduced from Table 1. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=AP
level_comment:
E$E{-x}=10426 keV {I10} with |G|?60 keV has previously been reported (1961Ca02,1963Go08,1963Go33), but was not adopted in ENSDF. The state is necessary to fit the Orsay data, but is not necessary to fit the Munich data. 
$Ip{-0}/I|a{-0}|<0.01 


level_energy_unit: KEV
level_comment:
E$E{-x}=10676 keV {I9} has previously been reported (1963Go08,1963Go33), but this state was not adopted in ENSDF. 
$Ip{-0}/I|a{-0}|<0.07 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: S
level_comment:
T$Weighted av: 11.56 s {I5} (1962Ma00), 11.36 s {I7} (1963AaAA), 10.31 s {I7} (1967Yu01), 10.996 s {I20}(1975Al27), 11.08 s {I1}(1976Ge08), 11.063 s {I23} (1978Be61) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_comment:
MOMM1,MOME2$From 2011StZZ 
T$From 1981Wa06, others: 4.27 s {I5} (1963Bu04), 4.34 s {I4} (1965Fo05) 
J$L=2 in (d,|t) 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: NS
level_comment:
T$from 1967Mc05 (Phys. Rev. 154, 1101). Implied units of ps in Table II of 2015Vo12 should be in ns. Note that 1970Wa36 (Phys. Rev. C2, 2235) give a weighted averaged value mean lifetime |t=8.80 ns {I33} from |t=10.10 ns {I72} (1966Me19: Phys. Rev. 152, 1002) and 8.31 ns {I36} (1967Mc05) 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
T$weighted average of mean lifetime |t=60 fs {I35} from 1727|g, and 40 fs {I35} from 1447|g is |t=50 fs {I35}. Other: 49 fs {I42} (1970Wa36) 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: S
level_comment:
J$Also log| {Ift}=4.8 in {+22}F |b{+-} decay to (4)+ state in {+22}Ne at 5523 keV level. Other possibility (3+), log| {Ift}=5.3 to 3+ state at 5641 keV level in {+22}Ne. 
T$from 1974Da02, others: 4.24 s {I8} (1973Gu05), 4.0 s {I4} (1965Va06) 
MOMM1,MOME2$|b-NMR (2010Mi13,2014StZZ). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$log {Ift}=3.8 from 0+ and the angular distribution of 1862.6|g consistent with J|p=1+ assignment (2007Le28-({+14}C,p|g)). Inconsistent with J|p=4+,5+ suggested in (t,{+3}He) (1988Cl04). 


level_energy_unit: KEV
level_spin_parity: 4+,5+
level_comment:
J$Suggested in 1988Cl04-({+3}He,t). No comparable state consistent with the suggested J|p were identified in 2007Le28 ({+14}C,p|g). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: FS
level_comment:
E,J$2007Le28 assumes this state corresponds to a level at 2986 keV of charge exchange reactions. However, 2759.4|g angular distribution rules out E2 decay. 2759.4|g to (3+). 


level_energy_unit: KEV
level_spin_parity: 4+
level_comment:
$Spectroscopic strength 1.48 {I11} (2018Ch36). Compiler gets 1.43 {I14} using (2J{-f}+1)/(2J{-i}+1)S - equation 1 in 2018Ch36. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_comment:
$Spectroscopic strength 0.27 {I8} (2018Ch36). 
E$From {+22}F Adopted Levels in the ENSDF database. Rounded to nearest keV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Spectroscopic strength 0.24 {I6} for l=2 (2018Ch36). For l=0, spin=2 spectroscopic factor and strength are 0.09 {I5} and 0.07 {I5}, respectively. 


level_energy_unit: KEV
level_spin_parity: 3+
level_comment:
$Spectroscopic strength 1.18 {I18} (2018Ch36). For l=2, spin=3 spectroscopic factor and strength both |<0.05. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Spectroscopic strength 0.56 {I9} (2018Ch36). For l=2, spin=2 spectroscopic factor and strength both |<0.05. 


level_energy_unit: KEV
level_comment:
$Spectroscopic strength <0.2 (2018Ch36) (Limit obtained from integrated cross section assuming l=2. 


level_energy_unit: KEV
level_comment:
$Spectroscopic strength <0.3 (2018Ch36) (Limit obtained from integrated cross section assuming l=2. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: S
level_comment:
$<r{+2}>{+1/2}({+23}F)=2.79~fm~{I4} (matter radius) (2001Oz03). 
J$From single neutron removal cross section, core fragment longitudinal momentum distributions and calculations (2004Sa14, 2000Sa47). L=2 and configuration |p d{-5/2} (2004Sa14). 
T$From 1974Go17 ({+23}F |b{+-} decay) - summed yield(t) of 1702-, 1822-, 3431-, and 2734-keV |g rays in four 1.7-sec periods. 
%B-N$From 1995ReZZ and 2008ReZZ 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
J$L=(2) in ({+22}O,{+23}F|g) (2006Mi16) and log| {Ift}=4.3 from 1/2+ parent ({+23}O |b{+-} Decay). Configuration: |pd{-3/2} (({+22}O,{+23}F|g) - 2006Mi16). 


level_energy_unit: KEV
level_comment:
E$|DE dominated by energy calibration extrapolation; neutron unbound state; larger uncertainty is because of extrapolation of calibration. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$From S(n)=7580 {I40} ({+23}F) and x<3.76E3 {I14} [from Q(|b{+-}) ({+23}O=11.34E3 {I13}-S(n)({+23}F) (2017Wa10)]. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
$ (2J+1)C{+2}S=0.73 {I+21-33}, C{+2}=isospin Clebsch-Gordan coefficient. 
L$from observed population strength of the state in |a inelastic scattering, proton transfer in ({+22}O,{+23}F), DWBA comparison. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$ (2J+1)C{+2}S=0.95 {I+29-35}, C{+2}=isospin Clebsch-Gordan coefficient. 
L$from observed population strength of the state in |a inelastic scattering, proton transfer in ({+22}O,{+23}F), DWBA comparison. Configuration: |pd{-3/2} (2006Mi16). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: MS
level_comment:
J Absence of {+24}F |b{+-} feeding from 0+, authors in 2015Ca09 propose 3+ based on {+24}F |b{+-} decay feeding to the 2+ and 4+ states of {+24}Ne at 1981.5 and 3963.1 keV levels, respectively, quoting Ref. [18 - thesis] (not published yet); in 2004Sa14 ({+24}F,{+23}F) 3+ based on one-neutron removal |s, core fragment longitudinal and transverse momentum distributions; also shell model calculations. 
T$Weighted average of 384 ms {I16} (2007Su05 - 1980|g(t) - |g-ray gated) and 340 ms {I80} (1986Du07). Other: 435 ms {I65} (2008ReZZ, 1995ReZZ) - omitted in the weighted averaging as a secondary source and carries less weight for higher uncertainty. Recommended half-life is same as that in 2015Bi05 horizontal evaluation. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$Absence of |b{+-} feeding from 0+ in {+24}O |b{+-} decay. |g from 1+ and |g to (3+). Shell model calculations also indicates 2+. 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$From S(n)=3810 {I100} ({+24}F) and x<7.15|*10{+3} {I21} [from Q(|b{+-}) ({+24}O=10.96|*10{+3} {I19})-S(n)({+24}F) (2021Wa16)]. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_comment:
J$From one-neutron removal |s, core fragment longitudinal and transverse momentum distributions. Glauber model analysis. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: (2+)
level_comment:
E$From |g ray energy. 2017Va24 assume the |g ray as a likely transition from 2{-1}+ to the 3+ g.s. in {+24}F. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: MS
level_comment:
T$Weighted average of 90 ms 9 (2005Pa74) and 70 ms 10 (2001Pe14). Other values : 50 ms 6 (1999Re16) and 59 ms 40 (1991Re02). 
%B-N$From 2005Pa74. Other values: 15 {I10} (1991Re02), 14 {I5} (1999Re16). 
J$From longitudinal and tranverse momentum distributions and cross sections in {+25}C({+12}C,{+13}C) E=43-68 MeV (2004Sa14). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$ 4249 keV {I116} in 2011Fr13, deduced from measured E{-res}= 28 keV {I4} and measured S(n)=4221 keV {I115} (2007Ju03). Assignment assumes the resonance decays to the ground state of {+24}F. 
J$ assignment based on comparison with shell model calculations 
T$ due to experimental resolution, only an upper limit for the width could be extracted. 


level_energy_unit: KEV
level_spin_parity: (3/2-,5/2+)
level_comment:
E$from measured decay energy of 300 {I170} and S(n)=4270 {I100} from 2012Wa38; uncertainty compounded in quadrature by compiler. Note that 2012Sm08 quote 4.66 MeV {I17} by taking S(n)=4360 {I120} from 2009Fi05 (Nucl. Data Sheets 110, 1691) which adopted this value AME-2003 (2003Au03) 
J$from shell-model predictions. 


level_energy_unit: KEV
level_spin_parity: (1/2-)
level_lifetime_unit: KEV
level_comment:
E{-r}=570 {I9}, from E{-r}=49 keV {I9} (2017Va24) + E|g=521 keV {I1} of {+24}F (2015Ca09 - Phys. Rev. C 92, 014327). 2017Va24 measured E|g=510. 
$ Possible configuration: (|p0p{-1/2})(|p0d{-5/2}){+2} 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: MS
level_comment:
J$Log {Ift}=4.9 to 0+, Log {Ift}=4.6 to 2+. J|p=1+ is consistent with the Gallagher-Moszkowski spin-coupling rule for configuration |pd{-5/2}~#|nd{-3/2}. 
T$Weighted average of 7.8 ms {I6} (2013Le03 - Figure 2), and 10.2 ms {I14} (1999Re16). Half-lives were measured from |g(t) measurements. Others: 9.6 ms {I8} (1999Dl01,2001Pe14 - value from the same research group of 1999Re16), 7.7 ms {I2} - 1672.5|g(t) and 7.8 ms {I5} - 1797.1|g(t) growth (due to IT decay) curve fitting (2013Le03). 
%B-N$Average value of 16 {i4} (2013Le03) and 11 {i4} (1999Re16,2001Pe14). Uncertainty - from input value. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$2013Le03 state that the 643.4-keV, 4+ isomer may correspond to the 657 keV {I7}, 2+ level. Further, 2013Le03 state that the energy of the isomer is |?650 {I10} keV. See spin-parity comments. 
J$From shell model calculations in 2013Le03, assuming 643.4|g as a M3 transition to 1+. If this excited level is considered to be the same as 657 keV {I7}, the hypothesis of isomerism of 4+ state would be due to the emission of a very low energy 4+ to 2+ transition (up to 10 keV (to ensure having a long-lived isomer), then followed by 2+ to 1+ transition - noted in 2013Le03. 
T$From 643.4|g(t) (2013Le03). 
%IT$From 2013Le03. May be considered an estimated value, since three decay modes of this isomeric state, i.e. IT, |b{+-}, and |b{+-}n, coupled with same decay product through |b{+-}n decay branch of {+26}F ground state make the measurements a challenge. Reported isomeric ratio R=42 {I8}% in 2013Le03 may also be considered as an estimated value for aforementioned reasons. 
%B-$From 100 - %IT 
%B-N$65 {i18}% of %|b{+-}=18 {i11} |b- branch of 4+ isomeric state (e-mail communication with A. Lepailleur ((1st author of 2013Le03): dated Sept 10, 2015). Note that 2013Le03 do not seem to provide explanation or methodology for the extraction of %|b{+-}n decay mode with a relative value of 65% {I18}. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$Shell model calculations predict 2+ state as the 2nd excited excited state in {+26}F (2004El10 - {+1}H({+27}F,{+26}F|g)). 


level_energy_unit: KEV
level_comment:
E$Deduced by evaluators from E(res)=271 keV {I37}*(Mass({+25}F)+ Mass(n))/Mass({+25}F) + Sn({+26}F)=770 keV {I110} (2012Wa38). 2011Fr13 deduced 1072 keV {I120}, using separation energy obtained from excess mass: 18680 keV 80 (2007Ju03). 
$In the decay spectrum, a broad peak was fitted considering a single resonance. Shell model calculations predict several unbound states. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_comment:
J$2+ state is predicted to be the 2nd excited state in {+26}F in shell model calculations (2004El10). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
%IT$from 2013Le03. May be considered an estimated value, since three decay modes of this isomeric state, i.e. IT, |b{+-}, and |b{+-}n, coupled with same decay product through |b{+-}n decay branch of {+26}F ground state make the measurements a challenge. Reported isomeric ratio R=42 {I8}% in 2013Le03 may also be considered as an estimated value for aforementioned reasons. 
%B-$From 100 - %IT 
%B-N$65 {I18}% of %|b{+-}=18 {I11} |b- branch of 4+ isomeric state (e-mail communication with A. Lepailleur ((1st author of 2013Le03): dated Sept 10, 2015). Note that 2013Le03 do not seem to provide explanation or methodology for the extraction of %|b{+-}n decay mode with a relative value of 65% {I18} 
E$2013Le03 state that the 643.4-keV, 4+ isomer may correspond to the 657 keV {I7}, 2+ level reported in 2012St01 (Phys. Rev. C85, 017303), albeit with a weak confidence. In this scenario, the 657-keV, 4+ isomer will decay via a 2+ state of very low energy (up to 10 keV in consistency with Weisskopf lifetime estimates) and then by the 643.4|g to the 1+ ground state. Further, 2013Le03 state that the energy of the isomer is |?650 {I10} keV 
J$From shell model calculations in 2013Le03, assuming 643.4|g as a M3 transition to 1+. If this excited level is considered to be the same as 657 keV {I7} reported in 2012St01 (Phys. Rev. C85, 017303), the hypothesis of isomerism of 4+ state would be due to the emission of a very low energy 4+ to 2+ transition (up to 10 keV to ensure having a long-lived isomer), then followed by 2+ to 1+ transition - noted in 2013Le03. 
T$From 643.4|g(t) (2013Le03) 


level_energy_unit: KEV
level_comment:
E$Deduced by evaluators from E(res)=271 keV {I37}|*(M({+25}F)+M(n))/ M({+25}F) + Sn({+26}F)=770 keV {I110} (2012Wa38). 2011Fr13 deduced 1072 keV {I120}, using separation energy obtained from excess mass: 18680 keV 80 (2007Ju03). 
$A broad peak in the decay spectrum, fitted considering a single resonance and yield 271 keV {I37} which was assumed to decay to ground state of {+25}F. Shell model calculations predict several unbound states. 


level_energy_unit: KEV
level_spin_parity: 1+
level_comment:
%B-N$Extracted from observed 979.7|g in {+25}Na (granddaughter) and using %I{-|g}=18.1 {I19} (2013Le03). 


level_energy_unit: KEV
level_spin_parity: (4+)
level_lifetime_unit: MS
level_lifetime_info: ;ISO=M
level_comment:
E$2013Le03 propose this isomeric state to be 4+ state predicted from shell model calculations, based on assumed M3 643.4|g transition to 1+. If this excited level is considered to be the same as 657 keV {i7} (2012St01), the hypothesis of isomerism of 4+ state would be due to the emission of a very low energy 4+ to 2+ transition (up to 10 keV to ensure having a long-lived isomer), then followed by 2+ to 1+ transition (2013Le03). 2013Le03 also note that the 4+ state lies at approximately 650 keV {i10}. 
T$From 643.4|g(t) 
%IT$From 2013Le03 
%B-$From 100 - %IT 
%B-N$Deduced by evaluators from %|b{+-}=18 {i11} and listed %|b{+-}n=35 {I18} in Fig. 2. 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: KEV
level_comment:
E$1394 {I134} in 2017Va24. 
E{-r}=323 {I33} 
J$2017Va24 propose 3+ state of 1{-1}{++} - 4{-1}{++} multiplet of the (|p0d{-5/2}){+1}(|n0d{-3/2}){+1} coupling, as 1+, 2+, and 4+ members have already been identified. 


level_energy_unit: KEV
level_spin_parity: (1+,2+,3+)
level_lifetime_unit: KEV
level_comment:
E$2861 {I318} in 2017Va24. 
E{-r}=1790 {I290} in 2017Va24. 
J$From Fig. 6, based on shell model calculations. 


level_energy_unit: KEV
level_comment:
$|G{-0}=10 keV 
E$resonance energy=380 keV 60 from fit of energy spectrum for 26f+n coincidence spectrum with Maxwellian distribution and L=2 Breit-Wigner resonance. Comparisons with shell-model calculations. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: MS
level_comment:
%B-N$From 1999Re16. Other: 90 {I30} (1999Dl01). 
J$From systematics of odd mass fluorine isotopes (2003Au02) 
T$Weighted average of 5.3 ms {I9} (|b-decay time spectrum-1997Ta22), 5.2 ms {I3} (1999Dl01), 6.5 ms {I11} (1999Re16), and 4.9 ms {I2} (1998NoZW). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_comment:
E,J$The shell model calculation predicts a level energy for the 1/2+ excited state at 1100 keV. An excited state closer to this energy can be constructed using the 504|g and 777|g in cascade. However, a state directly feeding the g.s. is more likely (2004El10). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-)
level_uncertain: ?
level_comment:
E,J$From 777 keV + 504 keV |g-rays. Spin/parity assignment from a comparison to other fluorine isotopes, however was not supported by theoretical calculations. The derived octapole deformation parameter |b{-3}=0.7 {I2} do not contradict with the assumption of the existence of a deformed 1/2- state in {+27}F. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-)
level_uncertain: ?
level_comment:
E,J$From 777 keV + 504 keV |g-rays. Spin/parity assignment from a comparison with other fluorine isotopes, however was not supported by theoretical calculations. The derived octapole deformation parameter |b{-3}=0.7 {I2} do not contradict to the assumption of the existence of a deformed 1/2- state in {+27}F. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$ resonance energy=380 keV {I60} from fit of energy spectrum for {+26}F+n coincidence spectrum with Maxwellian distribution and L=2 Breit-Wigner resonance. Comparisons with shell-model calculations. 
$ In CAESAR array for |g rays only two counts were observed in coincidence with {+26}F+n (E|g=780 and 1180 keV). For 100% decay of the 2.50 MeV state to a bound excited state in {+26}F, about 50 counts would be expected in CAESAR, indicating that observed decays feed the ground state of {+26}F. 


level_energy_unit: KEV
level_lifetime_unit: AS
level_lifetime_info: ;ERR=AP
level_comment:
E$From 220 keV {i50} resonance energy. g.s. of {+28}F is neutron unbound. A resonance in the {+27}F+n continuum at 220 keV {i50}, |G{-0}=10 keV, is determined in 2012Ch02 ({+29}Ne,n{+27}F). This resonance energy is referred to be the g.s. of {+28}F in 2012Ch02 and in good agreement with shell model predictions. 
T$Deduced by the evaluator from |G{-0}=10 keV. Other: <40 ns - from a private communication - quoted in 2012Au07 


level_energy_unit: KEV
level_lifetime_unit: AS
level_lifetime_info: ;ERR=AP
level_comment:
E$From 810 keV resonance energy. 
E$This upper resonance energy at 810 keV, |G{-0}=100 keV, is also deduced in the {+27}F+n continuum ({+29}Ne,n{+27}F). It is speculated in 2012Ch02 that contributions from other unresolved resonances may be present, since stronger population of this excited resonance state was not expected. 
T$Deduced by the evaluator from |G{-0}=100 keV (2012Ch02). 


level_energy_unit: KEV
level_lifetime_unit: AS
level_lifetime_info: ;ERR=AP
level_comment:
E$From 220 keV {i50} resonance energy. g.s. of {+28}F is neutron unbound. A resonance in the {+27}F+n continuum at 220 keV {i50}, |G{-0}=10 keV, is determined in 2012Ch02 ({+29}Ne,n{+27}F). This resonance energy is referred to be the g.s. of {+28}F in 2012Ch02 and in good agreement with shell model predictions. 
T$Deduced by the evaluator from |G{-0}=10 keV (2012Ch02). 


level_energy_unit: KEV
level_lifetime_unit: AS
level_lifetime_info: ;ERR=AP
level_comment:
E$From 810 keV resonance energy. This upper resonance energy at 810 keV, |G{-0}=100 keV, is also deduced in the {+27}F+n continuum ({+29}Ne,n{+27}F). It is speculated in 2012Ch02 that contributions from other unresolved resonances may be present, since stronger population of this excited resonance state was not expected. 
T$Deduced by the evaluator from |G{-0}=100 keV (2012Ch02). 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=199 keV {I6} (2020Re06), weighted average of 198 keV {I6} in neutron-removal reaction, and 204 keV {I16} in proton-removal reaction. This resonance was not observed in coincidence with any |g rays 
$One-neutron emission to the {+27}F g.s. 
J$L(n)=1+3, with |?70% L=1 component for 198-keV resonance from transverse momentum distribution and comparison with eikonal-model calculations 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=996 keV {I13}, considered by the authors as different from the 940-keV resonance observed in one-proton removal reaction 
$One-neutron emission to the {+27}F g.s. 
L$72% L=2 and 28% L=0 for 406-keV neutron peak 


level_energy_unit: KEV
level_spin_parity: (1+)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=1321 keV {I30}, from observation of a 406 keV {I28} neutron peak in coincidence with the 915-keV |g ray in {+27}F. This resonance is considered by the authors as different from the 1278-keV resonance in one-proton removal reaction 
$One-neutron emission to the 915, 1/2+ level in {+27}F 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=1880 keV {I80}, considered by the authors the same as the 1840-keV resonance observed in one-proton removal reaction, and also the same as 1869- and 1851-keV resonances observed in two-neutron decay to {+26}F g.s. 
$E(resonance)=1851 keV, with |G=6 keV {I+310-6} from observation of two-neutron decay to the {+26}F g.s. by a 227 keV {I88} neutron peak. 
$|G=10 keV {I+220-10} 
$One-neutron emission to the {+27}F g.s., and two-neutron emission to the {+26}F g.s. 
J$from one-proton removal reaction 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=2115 keV {I81}, from observation of a 1200 keV {I80} neutron peak in coincidence with the 915-keV |g ray in {+27}F in {+27}F 
$One-neutron emission to the 915, 1/2+ level in {+27}F 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=4095 keV {I260}, from observation of a 3180 keV {I260} neutron peak in coincidence with the 915-keV |g ray in {+27}F. Level energy=3896 {I260} 
$One-neutron emission to the 915, 1/2+ level in {+27}F 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=6010 keV {I180}, from observation of a 4390 keV {I170} transition to the {+26}F g.s. 
$This resonance is from Table S2 in the supplementary material, not shown in authors' level-scheme Fig. 1 in the paper and Fig. S1 in the the supplementary material. 


level_energy_unit: KEV
level_spin_parity: (4-)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=199 keV {I6} (2020Re06), weighted average of 198 keV {I6} in neutron-removal ({+29}F,{+28}F) reaction, and 204 keV {I16} in proton-removal ({+29}Ne,{+28}F) reaction. This resonance was not observed in coincidence with any |g rays 
$One-neutron emission to the {+27}F g.s. 


level_energy_unit: KEV
level_spin_parity: (2-)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=940 keV {I20}, considered by the authors as different from the 996-keV resonance observed in one-neutron removal reaction 
$One-neutron emission to the {+27}F g.s. 


level_energy_unit: KEV
level_spin_parity: (1-)
level_lifetime_unit: KEV
level_comment:
$60% neutron branch to the {+27}F g.s., and 40% neutron branch to the 915, 1/2+ state in {+27}F 
$E(resonance)=1280 keV {I30}, decays by one-neutron emission to the {+27}F g.s. Another decay mode is to the 915, 1/2+ state in {+27}F, as observed in 363 keV {I17} neutron peak in coincidence with 915-keV |g ray in {+27}F, defining the resonance at 1278 keV {I21}. This resonance is considered by the authors as different from the 1321-keV resonance in one-neutron removal reaction 
$One-neutron emission to the {+27}F g.s., and also to the 915, 1/2+ level in {+27}F 
$|G=170 keV {I90} for 1280-keV resonance 


level_energy_unit: KEV
level_spin_parity: (3-)
level_lifetime_unit: KEV
level_comment:
$E(resonance)=1840 keV {I30}, considered by the authors the same as the 1880-keV resonance observed in one-neutron removal reaction, and also the same as 1869- and 1851-keV resonances observed in two-neutron decay to {+26}F g.s. 
$E(resonance)=1869 keV, with |G=130 keV {I98} from observation of two-neutron decay to the {+26}F g.s. by a 245 keV {I32} neutron peak. 
$One-neutron emission to the {+27}F g.s., and two-neutron emission to the {+26}F g.s. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=3660 keV {I100}. Also E(resonance)=3648 {I80} from observation of 2024 keV {I52} transition with |G=580 keV {I160} to the {+26}F g.s. 
$One-neutron emission to the {+27}F g.s.; and 2n decay to {+26}F g.s. 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=3725 keV {I370}, from observation of 2810 keV {I360} neutron peak in coincidence with 915-keV |g ray in {+27}F. Level energy=3526 {I370} 
$One-neutron emission to the 915, 1/2+ state in {+27}F 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$E(resonance)=3761 keV {I74}, from observation of a 1480 keV {I43} transition in coincidence with 657-keV |g ray from the first 2+ state in {+26}F 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$weighted average of 2.4 ms {I4} (1999Dl01), 2.6 ms {I4}(1998NoZZ) and 2.4 ms {I8} (2001Pe14,1997Ta22). Other value: 2.9 ms {I8} (1999Re16 - appears to be from the same experiment in 1997Ta22). 
%B-N$From 1999Dl01 
J$systematics: 5/2+ (2003Au02), 3/2+ (1997Mo25) 


level_energy_unit: KEV
level_lifetime_unit: MS
level_comment:
T$from fit to decay curve with function that included decay of parent, exponential growth and decay of daughters (including |bn and |b2n branches) and a constant background (2022Cr03). Reported as 3.4 ms {I4} (stat) {I1} (syst). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$R{-m}{+ex}=3.50 fm {I7} (202Ba27) deduced from |s{+ex}=1396 mb {I28}, with large increase in R{-m}{+ex} relative to {+27}F consistent with two-neutron halo structure. 


level_energy_unit: KEV
level_comment:
${+30}F is most likely particle unstable, since S{-n}=-740 {I730} {I(sy)} and no events were identified in the experimental work of 1999Sa06, 2004Lu19. 


level_energy_unit: KEV
level_comment:
$E{+r}=472 keV {I158} (stat) {I33} (syst) (2024Ka32) 
$|G=477 keV {I+358-177} (stat) (2024Ka32). Authors state that while resonance energy is well described and stable under different fitting conditions, the width is not because of weakly constrained unresolved contributions. 


level_energy_unit: KEV
level_comment:
$Assuming {+31}F g.s. to be particle-bound, the only possible decay mode is |b{+-}, followed by delayed-neutron decays, thus 100% decay mode is assigned, although not observed directly. 
$Theoretical T{-1/2}=1.8 ms, %|b{+-}n=63, %|b{+-}2n=17, %|b{+-}3n=19, %|b{+-}4n=1, %|b{+-}5n=0 (2019Mo01) 
$Theoretical T{-1/2}=4.2 ms, %|b{+-}n=21.4; %|b{+-}2n=25.6; %|b{+-}3n=49.1; %|b{+-}4n=2.9, 3.3; %|b{+-}5n=1.05, 0.65; %|b{+-}6n=0.001; %|b{+-}7n=0.0 (2021Mi17) 
E$the observed {+31}F fragments are assumed to correspond to the g.s. 
J$5/2+ (syst, 2021Ko07). |W{-p}=1/2+ (theory, 2019Mo01) 
T$half-life of {+31}F has not been measured. The value is expected to be greater than the time-of-flight of 260 ns in 1999Sa06. From systematics of half-lives of neighboring fluorine isotopes, the half-life is expected to be <2.5 ms (2.5 ms for {+29}F, 5.0 ms for {+27}F, 8.2 ms for {+26}F and 80 ms for {+25}F; {+30}F and {+28}F are neutron-unbound), from Adopted Level of each nuclide in the ENSDF database. Other: 2 ms (syst,2021Ko07) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$First observation at E({+13}O+2p)=2522 keV {I66}. This corresponds to a mass excess=40215 keV {I69}. 
J$From mirror symmetry with {+15}B. 
$Decays via 3-body {+14}O+2p decay. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=?
level_comment:
E$first observation at E({+13}O+2p)=2522 keV {I66}. This corresponds to a mass excess=40215 keV {I69}. 
J$from mirror symmetry with {+15}B. 
$Decays via 3-body {+13}O+2p decay. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$E({+14}O+2p) (MeV)=1.401 {I20} 
$Decays 100% by 2p decay mode to {+14}O (2008Mu13). 
S$We used S{-2p}=-1401 keV {I20} from (2017Wa10: AME-2016).The weighted average of all measured S{-2p} values is -1413 keV {I17} (external errors) based on -1350 keV {I80} (2008Mu13, 2009Mu09, 2009Mu17, 2010Mu12), -1466 keV {I20} (2014Br19, 2015Br11), -1388 keV {I15} (2014Wa09,2015Ma09), -1463 keV {I45} (1980Bu15), -1399 keV {I24} (1983Wo01) and -1330 keV {I80} (1978Ke06). See also S{-2p}=-1476 keV (2016ChZV). 
$Direct measurements of reaction Q(|b{+-})values to obtain the |DM are given in (1983Wo01: |DM=23.984 MeV {I24}), (1980Bu15: 24.051 MeV {I45}) and (1978Ke06: 23.92 MeV {I8}). In this evaluation we accept |DM=23987 keV {I20} from (2017Wa10: AME-2016). See also (1977Ho13,1978Bu09: 24.4 MeV {I5}) and (1966Ke16, 1978Gu10, 1988Co15, 2013Xu15, 2018Fo04: theory) 
T$The expected width is |?0.8-3.1 keV (2002Gr03, 2015Br11), but the experimental resolution limits observations. In (2014Br19) |G<80 keV was determined from the best fit to the {+14}O+p+p excitation function using a Breit-Wigner line shape. Similarly, in (2014Wa09) a resolution folded Breit-Wigner line shape is fit to the {+14}O+p+p excitation function resulting in |G=82 keV {I15}. Early measurements of {+20}Ne(|a,{+8}He) reported |G=110 keV 40 (1983Wo01) and |G{-exp}=200 keV {I100} (1978Ke06). In (1978Ke06) a detailed discussion on the total decay width is given where proton and diproton penetrabilities are taken into account; the authors suggested a total decay width of 20 keV (ranging between 5-100 keV) and a diproton branching ratio of 10-90% 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E({+14}O+2p) (MeV)=3.17 {I2} 
J$See also 0+ (1997Fo09). 
S$from the weighted average of 3.16 MeV {I2} (2014Br19, 2015Br11) and 3.22 MeV {I5} (2014Wa09, 2015Ma09). See also 3.56 MeV {I21} (1980Bu15) and 3.02 MeV {I11} (1978Ke06). 
T$from (2014Wa09,2015Ma09). See also 200 keV {I200} (2010Mu12) and 150 keV {I50} (2015Br11), which may be influenced by other nearby states. 
$Unusual correlations amongst the {+14}O+2p ejectiles indicate a complex interplay between direct 2p decay and sequential decay via {+15}F*+p (2015Br11). See also (2010Mu12). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E({+14}O+2p) (MeV)=7.59 {I3} 
S$from the weighted average of 7.60 MeV {I4} (2014Br19,2015Br11) and 7.57 MeV {I6} (2014Wa09,2015Ma09). 
T$from (2014Wa09,2015Ma09). See also |<0.5 MeV (2015Br11) and 0.8 MeV {I+8-4} (2009Mu09,2010Mu12). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$Decays 100% by 2p decay mode to {+14}O (2008Mu13). 
S$We used 1401 keV {I20} from (2017Wa10: AME-2016). See also 1350 keV {I80} (2008Mu13,2009Mu09,2009Mu17,2010Mu12), 1466 keV {I20} (2014Br19,2015Br11) and 1476 keV (2016ChZV: |t|?4|*10{+-19} s). 
T$The expected width is |?0.8-3.1 keV (2002Gr03, 2015Br11), but the experimental resolution limits the result. This |G<80 keV was determined from the best fit to the excitation function using a Breit-Wigner line shape (2014Br19). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_comment:
$E({+14}O+2p) (MeV)=3.16 {I2} 
S$From (2014Br19,2015Br11); See also E({+14}O+2p)=3.2 MeV {I2} (2010Mu12) and 3160 keV (2016ChZV). 
T$weighted value of 150 keV {I50} (2015Br11) and 0.2 MeV {I2} (2010Mu12). The width of the state cannot be reproduced in simple models, suggesting that unaccounted for nearby states may influence the observations (2015Br11). 
$Unusual correlations amongst the {+14}O+2p ejectiles indicate a complex interplay between direct 2p decay and sequential decay via {+15}F*+p (2015Br11). See also (2010Mu12). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=LT
level_comment:
$E({+14}O+2p) (MeV)=7.60 {I4} 
S$From (2014Br19,2015Br11). See also E({+14}O+2p)=7.6 MeV {I2} (2009Mu09,2010Mu12) 
$The decay is 24% {I8} to {+15}F(0, 1/2+) and 76% {I8} to {+15}F*(1.3 MeV, 5/2+)) (2009Mu09,2010Mu12). 
T$from |<0.5 MeV (2015Br11). See also |G=0.8 MeV {++8}{--4} (2009Mu09,2010Mu12). 


level_energy_unit: KEV
level_energy_info: ;OFF=X
level_comment:
$Presumably decays 100% by sequential 2p decay mode to {+14}O through the 0, 1/2+; 1290, 5/2+; 3340 and 4840 levels of {+15}F (2008Mu13). 


level_energy_unit: KEV
level_spin_parity: (0+,2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E({+14}O+2p) (MeV)=3.22 {I5} 
E$decays predominantly to {+15}F{-g.s.}(1/2+) by p emission (2015Ma09) 
$Assuming J{+|p}=2+, comparison with {+16}C implies a Thomas-Ehrman shift |D=+70 keV {I46}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$E({+14}O+2p) (MeV)=7.57 {I6} 
$J{+|p}=(2+) in (2014Wa09). Analysis of 3-body correlations in (2015Ma09) confirms J{+|p}=2+. 
E$decays primarily by p emission to {+15}F*(2.8 MeV:5/2+) (2015Ma09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$T{-z}=-2, see (1980Bu15) 
$Q{-0}=-28.785 MeV {I45} (1980Bu15), which implies |DM=24.051 MeV {I45}; analysis of the IMME indicates {Id}=2.5 keV {I37} (1980Bu15; see also (1981SeZR)). 
$See also |DM=24.4 MeV {I5} (1977Ho13,1978Bu09). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: KEV
level_comment:
$E({+14}O+2p) (MeV): We used 1401 keV {I20} from (2017Wa10: AME-2016). See also 1.33 MeV {I8} (1978Ke06) and |?1.4 MeV (1983Wo01). 
T$The weighted value of (1983Wo01: 110 keV {I40}) and (1978Ke06: 200 keV {I100}). Applying penetrability corrections leads to a total decay width for {+16}Ne of 20 keV and a diproton branching ratio of 20%. Consideration of the uncertainties in the mass and width leads to the total decay width of 5-100 keV and the di-proton branching ratio is 10-90% (1978Ke06). 
$Q{-0}=-60.15 MeV {I8} (1978Ke06), which corresponds to |DM=23.92 MeV {I8}; see also Q{-0}=-60.197 MeV {I23} and |DM=23.984 MeV {I24} (1983Wo01). 
$Analysis of the IMME suggests {Id}=8 keV {I5} (1978Ke06); see also {Id}={Ie}=4 keV {I3} (1983Wo01). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: MS
level_comment:
T$weighted average of: 109.3 ms {I6} (1988Bo39), 109 ms {I1} (1971Ha05). Other results can be found in (1967Es02,1967Fi10,1964Mc16) and Hardy, et al., Nucl. Isospin, Proc. 1969 Conf. (Academic Press, 1969) 725. 
|DM=16500.4 keV {I4}: From ISOLTRAP measurement in (2008Ge07). Note: most level energies are taken from (1998Gu10) who measured |DM=16453 keV {I32}. Since other measurements (2002Ch44,2017Br07) tend to support the level energy differences found in (1998Gu10), those relative level energy spacings are preserved in the present evaluation. 


level_energy_unit: KEV
level_spin_parity: (3/2,1/2)-
level_comment:
E$From (1998Gu10), also see E{-x}=1275 keV {I22} from (2002Ch44) Au({+17}Ne,{+17}Ne'). 
J$3/2- is preferred based on comparison with the {+17}N levels (1998Gu10). 
$|G{-2p}/|G <1.6|*10{+-4} (2017Sh29). 


level_energy_unit: KEV
level_spin_parity: (5/2,7/2)-
level_comment:
J$5/2- is preferred based on comparison with the {+17}N levels (1998Gu10). 
E$From average of E{-x}=1764 keV {I12} (1998Gu10) and E{-x}=1745 keV {I7} (2018Ch25). Also see E{-x}=1770 keV {I20} from (2017Br07) {+9}Be({+17}Ne,{+17}Ne'). 


level_energy_unit: KEV
level_spin_parity: 1/2+,(3/2,5/2)+
level_comment:
J$1/2+ is preferred (1998Gu10). 
E$From (1998Gu10), also see E{-x}=1900 keV {I78} from (2002Ch44) Au({+17}Ne,{+17}Ne'). 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2,7/2-
level_comment:
E$From (1998Gu10) {+20}Ne({+3}He,{+6}He). While only one peak has been observed in the region, the group is suggested as a possible doublet (1998Gu10) since relatively poor energy resolution may conceal two groups. An analysis of the angular distributions for the E{-x}|?2623 keV region is consistent with L=3 (J{+|p}=(5/2-,7/2-)), while analysis of the E{-x}|?2765 keV region is consistent with L=2 (J{+|p}=(3/2+,5/2+)). A later analysis of Pb({+17}Ne,{+17}Ne') (2016Ma42) suggests an unresolved doublet with {+17}Ne*(2614 keV {I20}:5/2{++}) and {+17}Ne*(2692 keV {I21}:3/2{+-}). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
E$From (2018Ch25). See also E{-x}=1770 KeV {I20} in (2017Br07). 
$Decays 100% via p+{+16}F{-g.s.} to 2p+{+15}O{-g.s.}. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2)-
level_comment:
J$1/2- is preferred based on comparison with the {+17}N levels (1998Gu10). 
$|DM=16.508 MeV {I23} (1970Me11) 
$|DM=16.453 MeV {I32} (1998Gu10) 


level_energy_unit: KEV
level_spin_parity: 3/2+,5/2,7/2-
level_comment:
E$Possible doublet. Only one peak is observed. However the relatively poor energy resolution may conceal two groups in this region. An analysis of the angular distributions for the E{-x}|?2623 keV region is consistent with L=3 (J{+|p}=(5/2-,7/2-)), while analysis of the E{-x}|?2765 keV region is consistent with L=2 (J{+|p}=(3/2+,5/2+)). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
T$T{-mean}=1.1 ps {I2} (2002Ch44). 
$B(E2)|^=1.24 {i18} (2002Ch44) 
$Decays |?100% via 1p emission to {+16}F{-g.s.} (2002Ch44). 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|s(CH{-2})=4.04 mb {I20}, |s(C)=2.44 mb {I18}, |s(Pb)=11.6 mb {I15}, |s(H)|?0.80 mb {I14}. 
$Analysis of 3-body kinematics suggests decay via {+16}F*(1468:J{+|p}=0-). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$|s(CH{-2})=0.85 mb {I15}, |s(C)=0.81 mb {I15}, |s(Pb)=2.5 mb {I12}, |s(H)|?<0.1 mb. 
$Analysis of 3-body kinematics suggests decay via {+16}F*(1468:J{+|p}=0-). 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|s(CH{-2})=0.97 mb {I51}, |s(C)=1.14 mb {I10}, |s(Pb)=7.68 mb {I74}, |s(H)|?<0.2 mb. 
$Analysis of 3-body kinematics suggests decay via {+16}F*(1892:J{+|p}=2-). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
$|s(CH{-2})=1.40 mb {I53}, |s(C)<0.3 mb, |s(Pb)=0 mb, |s(H)|?0.70 mb {I26}. 
$Analysis of 3-body kinematics suggests decay via {+16}F*(1892:J{+|p}=2-). 


level_energy_unit: KEV
level_spin_parity: (5/2-)
level_comment:
$|s(CH{-2})=1.37 mb {I12}, |s(C)=0.62 mb {I10}, |s(Pb)=0 mb, |s(H)|?0.38 mb {I8}. 
$Analysis of 3-body kinematics suggests 50% decay via {+16}F*(1892:J{+|p}=2-) and 50% decay via {+16}F*(2180:J{+|p}=3-). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$|s(CH{-2})=1.13 mb {I22}, |s(C)=0.46 mb {I19}, |s(Pb)=14.4 mb {I17}, |s(H)|?0.33 mb {I15}. 
$Table 4 lists E{-x}=5141, which is the value reported in (1998Gu10). 
$|s(CH{-2})=2.10 mb {I35}, |s(C)=0.91 mb {I46}, |s(Pb)=0 mb 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$It was shown in (2022Le02) that the {+17}Ne{-g.s.} can be represented by a 3-body model consisting of the {+15}O core and 2 protons. The spectroscopic factor for having both protons in {Is}{+2} configuration was estimated to be C{+2}S= 0.67 {I11}, while that of the {Id}{+2} configuration was estimated to be 1.17 {I16}, resulting in a total spectroscopic factor of 1.8 {I2}. Fractions of 35 {I3}% {Il}=0 and the remaining 65% {Il}=2 were deduced for the motion of the valence protons in {+17}Ne{-g.s.}, which is consistent with shell model interpretation of the magnetic dipole moment measurement of (2005Ge06). 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Neutron pickup orbital: 1{Ip}{-1/2}. 
$ANC{+2}(r{-0}=1.25 fm)=160 {I19}. 
$C{+2}S{-exp}(HFB)=0.72 {I9}, ANC{+2}{-HFB}=179 {I21}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$Neutron pickup orbital: 1{Ip}{-3/2}. 
$ANC{+2}(r{-0}=1.25 fm)=52.3 {I73}. 
$C{+2}S{-exp}(HFB)=0.22 {I3}, ANC{+2}{-HFB}=55 {I8}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_comment:
$ Measured {+2}He (diproton resonance) (two-body) decay=31% {I7} 
$ Measured democratic three-body decay=66% {9} 
$ Virtual sequential decay=3% {I2} 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: KEV
level_comment:
E,J,T$From (2000Bb04) and (1999Ba49). |G=18 keV {I2}(stat) 1(sys). 
$Uncertainties in |G{-|g}: 24|*10{+-3} eV (stat), 30|*10{+-3} eV (syst) 
WIDTHG$from |w|g=33 meV 14(stat) 17(sys) (2009Ch64,2009Ch17) 
WIDTHP$from (2000Bb04). 


level_energy_unit: KEV
level_spin_parity: 1-
level_comment:
E From E{-res}=2.26 MeV {I6}. 
State is visible in the excitation function of {+1}H({+17}F,p{-1}|g), when the spectrum is conditioned exclusively in coincidence with |g-rays from decay of {+17}F*(495 keV). 
The experimental resolution is poor (80 keV) and the resonance width is not obtained from the observed width (|?120 keV {I60}). Values of |G=50 keV {I5} (2001Go01: Phys Rev Lett 86, 43 (2001)) and 58 keV {I2} (2002Ha15: Phys Rev C65, 035803 (2002)) are referenced. 
The authors deduce |G{-P{-0}}|G{-p'}/|G=22.7 keV. 
Using |G=50 and assuming |G{-P{-0}}=|G{-P1} the maximal value is |G{-P{-0}}|G{-p'}/|G=12.5 keV, hence the present results are inconsistent with equal P{-0} and P1 branches. Enhanced P1 is preferred. 
Comments on the astrophysical reaction rate are given using |G|a=3.2 eV {I+50-20} (2002Ha15). A value of |G|a=8 eV {I2} (2003Bl11: Nucl Phys A718, 127c (2003)) is also mentioned. 


level_energy_unit: KEV
level_spin_parity: 3-
level_comment:
$%p{-0}(to g.s.)=89 {I3}; %p'(to first excited state)=11 {I4} 
E$possible doublet. 
J$(2+,3-) in Adopted dataset for {+18}Ne in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: KEV
level_comment:
$%p{-0}(to g.s.)=83 {I3}; %p'(to first excited state)=16 {I7} 
J$(1-,2+) in Adopted dataset for {+18}Ne in ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_comment:
T$this half-life can be compared with the next most precise reported values of T{-1/2}=1.6648 s {I11} (2013Gr03: Phys. Rev. C87, 045502) and 1.669 s {I4} (1975Al27: Phys. Rev. C12, 1690). A weighted average of the three reported values yields T{-1/2}=1.66424 s {I+54-48}, as given by 2015La19 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$C{+2}S(2s{-1/2})=0.22 {I11}(stat) {I3}(syst), C{+2}S(1d{-5/2})=0.88 {I42}(stat) {I11}(syst), ANC(2s{-1/2})=16.0 fm{+-1} {I77}(stat) {I21}(syst), ANC(1d{-5/2})=2.6 fm{+-1} {I12}(stat) {I3}(syst). Note: ANC=22 fm{+-1} {I10}(stat) {I3}(syst) for pure {Il}=0/2s{-1/2}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$C{+2}S(2s{-1/2})=0.41 {I14}(stat) {I6}(syst), C{+2}S(1d{-5/2})=0.76 {I26}(stat) {I11}(syst), ANC(2s{-1/2})=148 fm{+-1} {I52}(stat) {I22}(syst), ANC(1d{-5/2})=3.1 fm{+-1} {I11}(stat) {I5}(syst). Note: ANC=188 fm{+-1} {I66}(stat) {I28}(syst) for pure {Il}=0/2s{-1/2}. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_comment:
$|G{-p}=14.2 keV {i3}(stat) {i11}(syst) 
$C{+2}S=0.78 {I2}(stat) {I6}(syst) from analysis of p+{+17}F spectrum. Note: C{+2}S(2s{-1/2})=0.84 {I10}(stat) {I10}(syst) from analysis of neutron data. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|G{-p}=50 keV {i8}(stat) {i8}(syst) 
$C{+2}S=0.20 {I3}(stat) {I3}(syst) from analysis of p+{+17}F spectrum. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
J$From the {+18}Ne Adopted Levels. The coupled-channels calculation of the present study fits the measured angular distribution very well. However, the L and J{+|p} values are not explicitly mentioned. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
E$From the {+18}Ne Adopted Levels. 
J$The coupled-channels calculation of the present study fits the measured angular distribution well. However, the L value is not explicitly mentioned. 
$|d=1.36 fm: deformation length was deduced from the coupled-channels calculations. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: FS
level_comment:
T$ mean lifetime (|t)=6.9 fs {I15} {I7}, weighted average of two values from two strong transitions. Earlier measurement: 7.6 fs {I+28-21} (2006Ka50, same group as 2008My01) 


level_energy_unit: KEV
level_spin_parity: (1/2-,3/2-)
level_comment:
E from E(c.m.)=1225 keV {I20} 
$The R-matrix fit is nearly equal for Ex=7636 (1/2-) with the above parameters, or with Ex=7644 keV {I18} (from E(c.m.)=1233 keV {I18}) with (3/2-), |G{-p}=1 keV {I1} and |G|a=3 keV {I3}; Ex=7636 (1/2-) is slightly preferred. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2-)
level_lifetime_unit: FS
level_comment:
$|G{-|a}=0.044|*10{+-3} eV {I20} 
|w|g=0.18|*10{+-3} eV {I8} 
J The authors suggest J|p values for the 4143 and 4200 keV levels that are reversed from those in the literature. Prior evaluations had listed the order as 4143 (9/2-) and 4200 (7/2-), apparently based on {+16}O({+6}Li,t) work and {+17}O({+3}He,n|g) work in (1973Da31). The present authors calculated single-particle |a-widths for the states and, based on deduced spectroscopic factors, they favored a reversal of the J values for these states. 


level_energy_unit: KEV
level_comment:
$The 2s{-1/2} and 1d{-5/2} spectroscopic factors of (2J+1)S{-p}: 0.02 {I4} and 0.03 {I7} are deduced, respectively. 


level_energy_unit: KEV
level_spin_parity: 1/2+,3/2+
level_comment:
$|G|a=11.62 keV for J|p=1/2+, 0.44 keV for J|p=3/2+ (2011Ad05). 
$The 2s{-1/2} and 1d{-5/2} spectroscopic factors of (2J+1)S{-p}: 0.92 {I3} and 0.52 {I3} are deduced, respectively. 


level_energy_unit: KEV
level_spin_parity: 1/2-,3/2-
level_comment:
$|G|a=0.27 keV; |G{-p}=2.54|*10{+-38} keV for J|p=1/2- or 1.27|*10{+-38} keV for J|p=3/2- 
$The 1p{-1/2} spectroscopic factor of (2J+1)S{-p}: 0.50 {I2} is deduced. 


level_energy_unit: KEV
level_comment:
E$from E{-res}(p+{+18}F)=678 keV {I5}. 
S$in the text a reference is cited (2002Bb02) which gives |G{-p}=15.2 keV 10, |G|a=23.8 keV {I12} and |G{-p}/|G|a=0.639 {I66}. However in Table I a value |G{-p}=13.5 keV {I7} is given from (2011Ad24); no corresponding |G|a is given in the text; using |G{-p}=13.5 and |G{-p}/|G|a=0.64 {I4} would yield |G|a|?21 keV. 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+)
level_comment:
E$from E{-res}(p+{+18}F)=1468 keV {I26} 
$|G{-p} from J|p=1/2+ (assumed) and (2J+1)S{-p}=0.25 {I5}. 
$|G|a from |G{-p} and |G{-p}/|G|a=1.754 {I14}. 
$%p and %|a deduced by 2012Ad05 from |G{-p}/|G|a=1.754 {I14} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: S
level_comment:
T$from T{-1/2}=17.2832 s {I51} (stat) {I66} (syst) (2014Br06). This value is discrepant with other similarly precise recent measurements of T{-1/2}=17.254 s {I5} (2013Uj01: GANIL |b-ray counter plus 2 EXOGAM HPGe clover detectors), and T{-1/2}=17.262 s {I7} (2012Tr06: TRIUMF SCEPTAR electron-positron array). 2014Br06 give a weighted average of 17.2604 s {I34} by combining their value with eight previous measurements from 1957 to 2013 with reduced |h{+2}=6.3 implying the presence of unaccounted systematic effects 
$From weighted averaged T{-1/2}=17.2604 s {I34}, 2014Br06 deduce Ft=1719.8 {I13} for 1/2+ to 1/2+ |b transition, and Cabibbo-Kobayashi-Maskawa matrix element V{-ud}=0.9712 {I22} 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2+,5/2+)
level_comment:
E$could be the unresolved states of 6282 and 6295 or a single broad state with a width |G|?16 keV (2015Pa46). 
J$see (2011Ad05,2011Ad24,2017To14). 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
E,J$(2011Ad05,2013La01) suggest J{+|p}=3/2- in this region; (2013La01) reported three states at 6416, 6440:J{+|p}=11/2+ and 6459:J{+|p}=(5/2-). 


level_energy_unit: KEV
level_spin_parity: (7/2-)
level_comment:
J$9/2- in ENSDF, but the present decay scheme is more consistent with 7/2- making this the mirror of {+19}F*(3998) 


level_energy_unit: KEV
level_spin_parity: (9/2-)
level_comment:
J$7/2- in ENSDF, but the present decay scheme is more consistent with 9/2- making this the mirror of {+19}F*(4032) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2,3/2)
level_comment:
E$Likely doublet with J{+|p}=11/2+ state reported in (2019Ha08) 
J$If the state is a doublet with a J{+|p}=11/2+ state, then J=1/2 is prefered. If only one state is present, then J|>7/2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3/2-)
level_comment:
J$The authors indicate their observations are consistent with the known 3/2- value, but J|>5/2 is deduced from their best fit. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2-,3/2-)
level_comment:
E$This state is thought to be an unresolved doublet (2021Ri04) consisting of two states: one broad state at E{-x}|?6.008 MeV with |G=124 keV {I25}, and another state at E{-x}|?6.014 MeV. The former state was not observed in (2023Po03). There is also no indication that the observed peak in the spectra of (2023Po03) is broader than a single peak. The angular distribution obtained for this state indicates that only a single state was strongly populated in (2023Po03). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
J$The J{+|p} value is deduced from the present DWBA analysis and the results of (2019Ka15). 
S$ANC=6 fm{+-1/2} (2019Ka15). 


level_energy_unit: KEV
level_spin_parity: 1/2+&7/2+
level_comment:
J$This state is likely a closely spaced doublet consisting of a low and a high spin states (2015Pa46, 2020Ha31) with a significant impact on the interference patterns in the {+18}F(p,|a){+15}O cross section. In the measurement of (2023Po03), this state has been obscured by contaminant states, and is only measured at 4 angles higher than |q{-cm}=20|'. Its angular distribution cannot be described by a single angular momentum transfer but rather by {Il}=0+4 with the 40% {I10} + 60% {I10} proportions. This observation supports the unresolved doublet hypothesis. Angular momenta of {Il}|>4 for the higher energy member of the doublet also fit the data of (2023Po03) well. The J{+|p} value of the high spin member of the doublet was assigned to be (11/2{++}) from observed |g-ray decays (2020Ha31). However, the nearest mirror state in that case would have an energy difference much larger than the average accepted value. So, the authors adopted J{+|p}=1/2{++}+7/2{++} for this doublet to study the maximum effect of this state on the {+18}F(p,|a){+15}O reaction rate. They have also adopted |G{-|a}=11.6 keV (2015Ba51) and ANC=83.5 fm{+-1/2} (2013La01) for the lower spin member of the doublet; and |G{-|a}=2.51 keV and ANC<16 fm{+-1/2} for the higher member of the doublet assuming it has a J{+|p}=7/2{++} assignment. 


level_energy_unit: KEV
level_comment:
E$ This state may corresond to the {+19}Ne*(8.428, (13/2{+-})) state. The tentative J{+|p} value is from (2017To14). 
$|q{+2}{-|a}=0.46 {I12}. This result implies the existance of a strong |a+{+15}O cluster configuration for this state. 


level_energy_unit: KEV
level_comment:
E$ This state may corresond to the {+19}Ne*(8.790, (11/2{++/-})) state. The tentative J{+|p} value is from (2017To14). 
$|q{+2}{-|a}=0.12 {I3}. This result implies the existance of a strong |a+{+15}O cluster configuration for this state. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
$ E(p)(c.m.)=213 keV, |G=0.89 keV {I+135-27} 
$ |G{-p}}=0.011 eV {I+3-2}, |G{-|g1}}<0.06 eV, |G{-|a2}}=0.8 keV {I+13-3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
$ E(p)(c.m.)=323 keV 
$ |G{-p}}=36 eV {I+6-5}, |G{-|g1}}=0.107 eV {I+24-19}, |G{-|a2}}=2.0 keV {I+4-3} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
$ E(p)(c.m.)=460 keV 
$ |G{-p}}=12.1 eV {I17}}, |G{-|g1}}=0.28 eV {I+5-4}, |G{-|a2}}=0.74 keV {I+19-17} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
$ E(p)(c.m.)=634 keV 
$ |G{-p}}=6.53 keV {I+13-10}, |G{-|g1}}=1.27 eV {I+27-25}, |G{-|a2}}=71 eV {I14}} 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: EV
level_lifetime_info: ;ERR=?
level_comment:
WIDTH$from evaluation of earlier data. 
E$from E{-|a}=1113.7 keV {I10}. 
$|w|g=1.8 meV {I4}. Evaluation including earlier data yields |w|g=1.7 meV {I2}. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
WIDTH$evaluation including earlier work yields |G=28 eV {I3}. 
E$from E{-|a}=1314.8 keV {I15}. 
$|w|g=14 meV {I2}. Evaluation including earlier work yields 16.3 meV 16. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_uncertain: ?
level_comment:
$This level is unresolved from {+20}Ne*(5788). Its population in this reaction is assumed to be negligible. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1-
level_lifetime_unit: EV
level_comment:
$The measured partial width, obtained using the ANC analysis technique, compares well with the known width of |G=28 eV {I3} and confirms the validity of the method. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
E$E{-x} is given as E{-x}=11255.4 {I7}(stat) {I+12-6}(syst); level energy listed as 11270 {I5} in Adopted Levels of {+20}Ne in ENSDF database 
T$from Adopted Levels of {+20}Ne in ENSDF database. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_spin_parity: 1-
level_comment:
E$1974Ca22 had observed evidence for a J|p=1- state in this region; the present results indicate E{-p}|?825 keV and E{-x}=13626 for this state. This state is not given in the Adopted Levels of {+20}Ne in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$in Adopted Levels of {+20}Ne in ENSDF database, this state is identified with J|p=0+, however a prior result (1958Is10) had suggested J|p=2+. The angular distribution results in 2015Lo14 confirm the J|p=0+ findings. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|s(-1|')[|mb/sr]=620 {I140}, |s(7|')[|mb/sr]=670 {I150}, |s(16|')[|mb/sr]=160 {I36}, |s(27|')[|mb/sr]=160 {I35} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$|s(-1|')[|mb/sr]=250 {I56}, |s(7|')[|mb/sr]=250 {I57}, |s(16|')[|mb/sr]=58 {I13}, |s(27|')[|mb/sr]=40 {I9} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_comment:
E$4428 in table I of 2015Sw01 is a typographical error 
$|s(-1|')[|mb/sr]=110 {I24}, |s(7|')[|mb/sr]=150 {I33}, |s(16|')[|mb/sr]=120 {I27}, |s(27|')[|mb/sr]=120 {I26} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 0+
level_comment:
$|s(-1|')[|mb/sr]=370 {I82}, |s(7|')[|mb/sr]=186 {I42}, |s(16|')[|mb/sr]=35 {I8}, s(27|')[|mb/sr]=65 {I15} 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_comment:
$|s(-1|')[|mb/sr]=2.2 {I5}, |s(7|')[|mb/sr]=7.3 {I21}, |s(16|')[|mb/sr]=10.0 {I25}, |s(27|')[|mb/sr]=7.7 {I20} 


level_energy_unit: KEV
level_spin_parity: (0+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$|s(-1|')[|mb/sr]=38 {I9}, |s(7|')[|mb/sr]=22 {I5}, |s(16|')[|mb/sr]=7.2 {I16}, |s(27|')[|mb/sr]=7.7 {I17} 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
E$From S(p)=12843 keV (2021Wa16) and E{-c.m.}=323 keV 
$|w|g=3.3{++11}{--9} meV (from |g+{+20}Ne coincidence events) 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
E$isobaric analog state (IAS). The |a decay is forbidden if IAS has pure T=1, however, the IAS is observed to have an |a decay width of 116 eV {I20} from (1976In05: {+16}O(|a,|g)). I|a|?2.77% 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$Weighted average of 7.0 ps {I2} (1977Be30), 7.09 ps {I14} (1978Ro10), and 7.5 ps {I3} (1981Ru01). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
$Relative=2.2 
$Decays by neutrons to g.s. of {+20}Ne 
E,J$This state associated with neutron decay, and identified with previously known 7211, 1/2+ state, and not to 7357, (7/2, 9/2+) level 


level_energy_unit: KEV
level_comment:
$Relative=4.0 
$Probably not a neutron decaying state since seen in all three decay spectra shown in 2010Fr04 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|G(|a)=0.0160 eV for l=0, s=5/2; |G(|a)=0.00045 eV for l=2, s=5/2; |G(n0)=23.0 keV for l=2, s=1/2 
E$From E|a(lab)=1002 {I2} resonance 
$Resonance strength |w|g=7.6 meV {I9} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|G(|a)=0.563 eV for l=1, s=5/2; |G(n1)=1.19 keV for l=1, s=3/2; |G(n1)=140 eV for l=1, s=5/2; |G(n0)=2.34 keV for l=1, s=1/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|G(|a)=0.363 eV for l=1, s=5/2; |G(n1)=320 eV for l=1, s=3/2; |G(n1)=37.7 eV for l=1, s=5/2; |G(n0)=781 eV for l=1, s=1/2 
E$From E|a(lab)=1386 {I2} resonance 
$Resonance strength |w|g=1.2 meV {I2} 


level_energy_unit: KEV
level_spin_parity: 5/2-
level_comment:
$|G(|a)=21.3 eV for l=1, s=5/2; |G(n1)=1.07 keV for l=1, s=3/2; |G(n1)=1.22 keV for l=1, s=5/2; |G(n0)=1.86 keV for l=3, s=1/2 


level_energy_unit: KEV
level_spin_parity: 9/2-
level_comment:
$|G(|a)=0.625 eV for l=3, s=5/2; |G(n1)=222 eV for l=3, s=3/2; and for l=3, s=5/2; |G(n0)=109 eV for l=5, s=1/2 
E$From E|a(lab)=1002 {I2} resonance 
$Resonance strength |w|g=136 meV {I17} 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|G(|a)=217 eV for l=0, s=5/2; |G(|a)=32.4 eV for l=2, s=5/2; |G(n1)=448 eV for l=2, s=3/2; |G(n1)=10.3 keV for l=0, s=5/2; |G(n1)=9.35 eV for l=2, s=5/2; |G(n0)=18.7 keV for l=2, s=1/2 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|G(|a)=131 eV for l=2, s=5/2; |G(n1)=786 eV for l=0, s=3/2; |G(n1)=84.1 eV for l=2, s=3/2; |G(n1)=2.18 keV for l=2, s=5/2; |G(n0)=5.13 keV for l=2, s=1/2 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|G(|a)=31.5 eV for l=0, s=5/2; |G(|a)=768 eV for l=2, s=5/2; |G(n1)=1.03 eV for l=2, s=3/2; |G(n1)=4.43 keV for l=0, s=5/2; |G(n1)=0.0249 eV for l=2, s=5/2; |G(n0)=9.34 keV for l=2, s=1/2 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$|G(|a)=403 eV for l=2, s=5/2; |G(n1)=19.4 eV for l=0, s=3/2; |G(n1)=0.00177 eV for l=2, s=3/2; |G(n1)=1.06 keV for l=2, s=5/2; |G(n0)=881 eV for l=2, s=1/2 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|G(|a)=16.8 keV for l=0, s=5/2; |G(|a)=1.1 keV for l=2, s=5/2; |G(n1)=37.7 eV for l=2, s=3/2; |G(n1)=16.7 keV for l=0, s=5/2; |G(n1)=0.816 eV for l=2, s=5/2; |G(n0)=55.0 keV for l=2, s=1/2 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$|G(|a)=1.83 keV for l=1, s=5/2; |G(n1)=758 eV for l=1, s=3/2; |G(n1)=85.6 eV for l=1, s=5/2; |G(n0)=1.03 keV for l=1, s=1/2 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
$|G(|a)=4.69 keV for l=0, s=5/2; |G(|a)=2.92 keV for l=2, s=5/2; |G(n1)=20.7 eV for l=2, s=3/2; |G(n1)=20.8 keV for l=0, s=5/2; |G(n1)=0.444 eV for l=2, s=5/2; |G(n0)=110 keV for l=2, s=1/2 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_comment:
$Resonance energy (lab)=147.40 keV {I15} 
$g=(2J(res)+1)/((2I{-n}+1)(2I({+20}Ne{-g.s.})+1))=1; not 1/3 as listed in Table II of 2014He25 
$The strength of this resonance is 80% larger than that reported by 1988Wi14. 


level_energy_unit: KEV
level_spin_parity: (7/2,11/2)+
level_uncertain: ?
level_comment:
$|w|g=4.0|*10{+-3} meV {I+31-20}. 
$The lowest data point measured covers three known states. (2013Be11) suggests that the 7.982 MeV level makes the dominant contribution. 


level_energy_unit: KEV
level_comment:
$|w|g=7.51 |meV {I72} (singles), |w|g=8.5 |meV {I11} (coincidence) for 5.6 Torr gas target pressure and |w|g=8.00 |meV {I84} (singles), |w|g=9.4 |meV {I11} (coincidence) for 4.2 Torr gas target pressure 


level_energy_unit: KEV
level_spin_parity: (7/2+)
level_comment:
$|G{-|a}=157|*10{+-4} meV {i59} 
$E{-cm}=472.2 {I15} 
J,L,S$others: L=0, J=5/2+, C{+2}S{-|a}=0.610 {9}, |G{-|a}= 683 |* 10{+-4} meV; L=2, J=3/2+, C{+2}S{-|a}=0.310 {5}, |G{-|a}= 465 |* 10{+-5} meV 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2)+
level_comment:
$|G{-n}=160 eV {I20} for J=3/2 or 120 eV {I10} for J=5/2 
S$for J=3/2, other: 0.120 for J=5/2 
L,S$other: L=3, with C{+2}S=0.145 and |G{-n}=2.9 ev {I2} for J=5/2 and C{+2}S=0.132 and |G{-n}=2.5 eV {I2} for J=7/2. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$|d<r{+2}>({+20}Ne,{+22}Ne)=-0.321 fm{+2} {i4} (stat) {i43} (syst) (2011Ma48,2008Ge07). Absolute {+22}Ne charge radius=2.952 fm {i9} (2008Ge07) deduced with respect to known {+20}Ne charge radius=3.006 fm {i5}. 
J$From optical spectroscopy (1927Ha01); L=0 in ({+6}Li,d), ({+7}Li,t), and (t,p); natural parity. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
E$From |g-ray energy 
J$E2 to 0+; L=2 in ({+6}Li,d), ({+7}Li,t), and (t,p); natural parity. 
MOMM1$Recoil into Vacuum, Differential method (1977Ho01, 2014StZZ) 
MOME2$Coulomb Excitation Reorientation (1981Sp07, 2014StZZ) 
T$From mean lifetime 5.19 ps {I7}: weighted average of mean lifetimes - 5.16 ps {I13} (1984Bh03), 5.1 ps {I2} (1983Ko01), 4.6 ps {I6} (1979Ma13), 5.15 ps {I31} (1979Fo02), 5.2 ps {I3} (1977Ho01), 5.62 ps {I20} (1977Ra01), 4.9 ps {I7} (1977Og03), 5.15 ps {I14} (1977Sc36), 4.9 ps {I4} (1974Ol01), 5.4 ps {I4} (1973An01), 5.5 ps {I10} (1973Si31), 5.9 ps {I11} (1972Sn01), 5.9 ps {I6} (1972Sz05), 3.6 ps {I7} (1970Na07), 4.6 ps {I5} (1969Jo10), 6.1 ps {I5} (1969ScZV), and 3.1 ps {I11} (1960An07). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$L=4 in ({+6}Li,d); natural parity. 
MOMM1$Tilted Foil hyperfine field integral perturbed angular correlation (1984Ba10, 2014StZZ) 
T$From mean lifetime 324 fs {I6}: weighted average of mean lifetimes - 324 fs {I9} (1979Fo02), 311 fs {I17} (1978Fi04), 328 fs {I10} (1978Ek01), 285 fs {I50} (1974Fi16), 360 fs {I50} (1972Br17 - average of measurements with 39 different slowing down materials), 270 fs {I90} (1968Ku05), 400 fs {I110} (1967Wa13), and 390 fs {I80} (1964Es02). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$E2 to 0+; L=2 in ({+6}Li,d), ({+7}Li,t), and L=(2) in (t,p); natural parity. 
T$From (e,e') - 1979Ma13. Other values: <11 fs (1979Al01-({+19}F,p|g)), <30 (|a,p|g)), while 37 fs {I6} (1993Ol05 - (|a,p|g)) is higher compared to other values. 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
J$E1 to 2+, L=1,3 in (t,p); unnatural parity 
T$From mean lifetime 1.1 ps {I2}: weighted average of mean lifetimes - 1.2 ps {I3} (1975Me19), 1.15 ps {I45} (1976Fi02), 1.3 ps {I5} (1979Al01), and 0.9 ps {I4} (1993Ol05). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$Weighted average of data from (e,e'), (|g,|g'), and (|a,p|g) 
J$M1+E2 to 2+, J|p=1+ in (e,e') (1974Ma43); (unnatural parity) 
T$From mean lifetime 1.7 ps {I3}: Weighted average of 1.7 fs {I3} (e,e') (1979Ma13) and 1.8 fs {I7} (|g,|g') (1984Be26). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: FS
level_comment:
J$E2 to 0+; L=2 in (t,p); natural parity 
T$<20 fs in 1976Fi02 - reason for this discrepancy is unknown. 


level_energy_unit: KEV
level_spin_parity: (4)+
level_lifetime_unit: FS
level_comment:
J$L=4 in ({+6}Li,d), (t,p); natural parity; J=3 in {+11}B({+13}C,d) 
T$From mean lifetime 30 fs {I4}: Weighted average of 27 fs {I4} (1979Al01) and 37 fs {I6} (1993Ol05). Uncertainty - lower experimental value. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: FS
level_comment:
E$From (n,|g) 
J$E1 to 2+; L=3 in ({+6}Li,d); natural parity; |g to 4+ 
T$From mean lifetime 46 fs {I16}: Weighted average of 51 fs {I23} (1976Fi02) and 44 fs {I16} (1993Ol05). Uncertainty - lower experimental value. 


level_energy_unit: KEV
level_spin_parity: (6+)
level_lifetime_unit: FS
level_comment:
T$From mean lifetime 70 fs {I6}: Weighted average of 78 fs {I15} (1976Fi02), 70 fs {I10} (1979Al01), and 69 fs {I6} (1993Ol05). Uncertainty - lowest experimental value. 


level_energy_unit: KEV
level_spin_parity: (3)-
level_lifetime_unit: FS
level_comment:
J$L=1 in (d,p), E1 to 2+ (|a,p|g), |g-ray feeding from 4+ state at 8855; natural parity for doublet. Another possibility 1-, as suggested in 1993Ol05 - (|a,p|g), less likely considering |g feeding from 4+. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: AS
level_comment:
E$Other values: 9165 {i3} (1979Be10 - (|g,|g')), 9170 {i4} (1976Fi02 - (|a,p|g)), 9179 {i10} (1974Fl07 - (t,p)) 
J$From (pol |g,|g). 


level_energy_unit: KEV
level_spin_parity: 7-
level_comment:
E$Weighted average of data 11533 {I10} (1994Ma37) and 11520 {I15} (1974Fl07) in (t,p), and 11482 {I20} (|a,p|g). 
J$From (|a,p|g), angular correlation measurements. Natural parity listed in 1990En08 - Table 22.11. 


level_energy_unit: KEV
level_spin_parity: 1
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$Weighted average of data from 11886 {i10} (|a,|g), 11907 {i10} and 11895 {i15} (t,p), and 11880 {i10} ({+4}He,{+4}He'). 
J$1+ in (p,p'), 1- in ({+4}He,{+4}He') and (|a,|g). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_lifetime_unit: FS
level_comment:
T$Weighted average of 227 fs {I7} (1978Ek01), 216 fs {I12} (1978Fi04), and 225 fs {I6} (1979Fo02). Uncertainty: Lowest experimental value. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 6 ps {I2} (1966Li07), 4.1 ps {I4} (1972Sz05), 3.2 ps {I4} (1969Jo10), 4.1 ps {I8} (1972Sn01), 3.7 ps {I3} (1973An01), 3.4 ps {I5} (1977Og03), 3.90 ps {I14} (1977Ra01), 3.58 ps {I9} (1984Bh03). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
T$Other values: 277 fs {I76} (1967Wa13), 187 fs {I62} (1968Ku05), 250 fs {I35} (1972Br17), 198 fs {I35} (1974Fi16). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: FS
level_comment:
J$(3)- in Adopted Levels considering |g feeding from 4+ state. 3,5 in 1976Br06. 
T$Other value: 63 fs {I+38-26} (1976Fi02) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 4460 {I5} (1994Ma37) and 4453 {I5} (1974Fl07). Other value: 4473 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$6330 {I10} from 1994Ma37 may include contribution from 6311 level. Other value: 6349 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 6682 {I10} (1994Ma37) and 6691 {I10} (1974Fl07). Other value: 6696 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 6820 {I10} (1994Ma37) and 6825 {I10} (1974Fl07). Other value: 6823 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 7639 {I10} (1994Ma37) and 7643 {I10} (1974Fl07). Other value: 7633 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 7720 {I10} (1994Ma37) and 7726 {I10} (1974Fl07). Other value: 7720 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 7925 {I10} (1994Ma37) and 7924 {I10} (1974Fl07). Other value: 7913 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8081 {I10} (1994Ma37) and 8085 {I10} (1974Fl07). Other value: 8071 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8129 {I10} (1994Ma37) and 8125 {I10} (1974Fl07). Other value: 8122 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8387 {I10} (1994Ma37) and 8386 {I10} (1974Fl07). Other value: 8368 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8590 {I10} (1994Ma37) and 8593 {I10} (1974Fl07). Other value: 8575 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8743 {I10} (1994Ma37) and 8738 {I10} (1974Fl07). Other value: 8724 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8865 {I10} (1994Ma37) and 8867 {I10} (1974Fl07). Other value: 8890 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 8980 {I10} (1994Ma37) and 8981 {I10} (1974Fl07). Other value: 8970 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 9096 {I10} (1994Ma37) and 9092 {I10} (1974Fl07). Other value: 9069 {I15} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 9181 {I10} (1994Ma37) and 9179 {I10} (1974Fl07). Other value: 9174 {I20} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 9229 {I10} (1994Ma37) and 9225 {I10} (1974Fl07). Other value: 9215 {I20} (1961Si03) 


level_energy_unit: KEV
level_comment:
E$Unweighted average of 9337 {I10} (1994Ma37) and 9329 {I10} (1974Fl07). Other value: 9316 {I15} (1961Si03) 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
E$From 1974Ma43. 1979Ma13 report this as a doublet at 5336 keV. 
T$From total width of 0.38 eV {i7}, deduced in 1979Ma13. 


level_energy_unit: KEV
level_comment:
$B(E2)|^=0.00039 {i15} and B(E2)|^=0.00075 {i40} (1979Ma13) are listed assuming J|p=2+ and 3-, respectively. J|p=1- in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: AS
level_comment:
E$From longitudinal and transverse cross section analysis, 1979Ma13 suggests two states contributing to the cross section. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$Tentative assignment because of complicated level scheme near this level energy (1979Ma13). Assignment J|p=2- at 8540 {i30} (1974Ma43). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$From B(E2)|^=0.0223 {I6} (1977Sc36). Other values: 2.0 ps {I2} from B(E2)|^=0.042 {I4} (1960An07), 2.6 ps {I5} from B(E2)|^=0.033 {I6} (1970Na07), and 3.4 ps {I3} from B(E2)|^=0.025 {I2} (1974Ol01). 
$ |b{-2}=0.370 deduced from |s(|q) of {+22}Ne ions and analyzed by DWBA calculations (2012Bo09). 


level_energy_unit: KEV
level_uncertain: ?
level_comment:
E$Tentative level as it coincides with a possible contaminant from the decay of {+20}Ne to {+16}O + |a. Not adopted. 


level_energy_unit: KEV
level_spin_parity: [3-]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
$|G(|a)=0.224 eV for l=3, s=0; |G(n1)=1.9 keV for l=1, s=2; |G(n1)=45.8 eV for l=1, s=3; |G(n0)=1.7 keV for l=1, s=2 


level_energy_unit: KEV
level_spin_parity: [1-]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$Other value: 10922 (2013Be12) 
$|G(|a)=10.5 eV for l=1, s=0; |G(n1)=6.1 keV for l=1, s=2; |G(n0)=14.1 keV for l=1, s=1; |G(n0)=6.6 keV for l=1, s=2 


level_energy_unit: KEV
level_spin_parity: [2+]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$Other value: 11195 (2013Be12) 
$|G(|a)=13.8 eV for l=2, s=0; |G(n1)=440 eV for l=0, s=2; |G(n0)=4.8 keV for l=0, s=2 


level_energy_unit: KEV
level_spin_parity: [3-]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$Other value: 11268 (2013Be12) 
$|G(|a)=1.6 eV for l=3, s=0; |G(n1)=412 eV for l=1, s=2; |G(n1)=10.2 eV for l=1, s=3; |G(n0)=1.2 keV for l=1, s=2 


level_energy_unit: KEV
level_spin_parity: [1-]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=?
level_comment:
E$Other value: 11432 (2013Be12) 
$|G(|a)=126 eV for l=1, s=0; |G(n1)=25.0 keV for l=1, s=2; |G(n0)=10.2 keV for l=1, s=1; |G(n0)=5.1 keV for l=1, s=2 


level_energy_unit: KEV
level_spin_parity: [4+]
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LE
level_comment:
$|G(|a)=49.9 eV for l=4, s=0; |G(n1)=1.0 keV for l=2, s=2; |G(n1)=1.0 keV for l=2, s=3; |G(n0)=2.5 keV for l=2, s=2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
T$deduced by compiler from B(E2)|_. This value can be compared with 3.60 ps {I5} in {+22}Ne Adopted Levels in the ENSDF database (April 2015 update), and 3.66 ps {I7} in 2016Pr01 (At. Data Nucl. Data Tables 107, 1) evaluation 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$Resonance energy (lab)=662.1 keV 
$|w|g=221 |meV {I21} (stat approach), 225 |meV {I12} (decay scheme) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$Resonance energy (lab)=749.9 keV 
$|w|g=564 |meV {I35} (stat approach), 553 |meV {I34} (decay scheme) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
$Resonance energy (lab)=767.6 keV 
$|w|g=1438 |meV {I86} (stat approach), 1306 |meV {I77} (decay scheme) 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: S
level_comment:
$ |d<r{+2}>({+20}Ne,{+23}Ne)=-0.572 fm{+2} {I34} (2013An02, 2011Ma48) 
$The r.m.s. charge radius <r{+2}>{+1/2}=2.910 fm {I7} (2013An02). 
J$5/2 from LASER spectroscopy (2005Ge06, 2013Ma15), L=2 in (d,p). 
T$From 37.151 s {I56} (wt. ave. of 37.126 s {I30} and 37.276 s {I67} with external uncertainty (2015La19 - also 37.153 s {I28} with statistical uncertainty)), 37.11 s {I6} (from 2007Gr18), 37.24 s {I12} (from 1974Al03), 37.6 s {I1} (1957Pe12), 38.0 s {I3} (1958Nu41), and 37.5 s {I1} (1959Al10) - using the Limitation of Relative Statistical Weight (LWM) method (1985ZiZY). Wt. ave. 37.25 s {I9} with |h{+2}=6.7 and |h{+2}{-crit}=3.0 at 99% C.L. Unweighted ave. 37.43 s {I14}. Other values (outlier - Chauvenet's criterion): 38.7 s {I4} (1967Yu01), 40.2 s {I4} (1950Br78). 
MOMM1$From 2019StZV (in 1994Hi09 -1.0795 {I10} |b-NMR). Others: -1.077 {I4} (2005Ge06 - CFBLS/|b-NMR), -1.08 {I1} (1968Do07), 1.0817 {I9} (2014StZZ). 
MOME2$From 2005Ge06, 2016St14 - CFBLS/|b-NMR. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: PS
level_comment:
J$L=0 in (d,p) 
T$from 1966Fo02 (d,p|g) - p|g(t) coincidence. Other: 208~ps {I110} (d,p|g) (1974Ch35). 


level_energy_unit: KEV
level_energy_info: ;OFF=X;ERR=?
level_comment:
E$From S(n)=5200.65 {I10} ({+23}Ne) and x<3239 {I30} [from Q(|b{+-}) ({+23}F)=8440 {I30}-S(n)({+23}Ne) (2017Wa10)]. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_comment:
E$1975De33 show doublet of 5186 and 5226 in Table I, appears to be a triplet compared to level energies of 5185, 5200, and 5220 in the adopted dataset. Listed energy is the average of these three values. 


level_energy_unit: KEV
level_lifetime_unit: PS
level_comment:
T$From p|g(t) coincidence in 1966Fo02. Other: 208~ps {I110} from mean lifetime of 300~ps {I+150-165} (1974Ch35) by Doppler shift attenuation factor. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$|=1/2 in 1967Ho08 from |g(|q) and correlation measurements for 1/2- and 3/2- from L=1 in (d,p) 1970Ho22. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MIN
level_comment:
T$From 1956Dr11 (|b(t), |g(t)). Other: 3.2 min {I2} (1969Mc12) 
$|D<r{+2}>({+20}Ne,{+24}Ne)=-0.627 {I19} (stat) {I75} (sys) (2011Ma48). 
$<r{+2}>{+1/2}({+24}Ne)=2.9007 fm {I78} (charge radius) (2013An02). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J$From 1968Be55 (|g-ray angular distribution) and also from analysis of |g-ray angular distribution data in 1970Ho17. 
T$Weighted average of 0.62 ps {I+25-20} (1974Wa04) and 0.7 ps {I+2-3} (1969Bh01). Other: <21 ns (1968Be55) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E$From Adopted Levels, rounded value to keV. 
J$From 1970Ho17 (p-|g angular correlation). 
T$Estimated from the resolving time (1970Ho17). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 2.3 ps {I+15-8} (1974Wa04) and 1.1 ps {I+10-4} (1978DoZJ). Other values: >1 ps (1969Bh01), <21 ns (1968Be55). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2(+)
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_comment:
E$From Adopted Levels, rounded value to keV. 
J$2 from 1970Ho17 (p-|g angular correlation measurements). |g to 2+ 
T$Estimated from the resolving time (1970Ho17). 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: MS
level_comment:
MOMM1$Colinear fast beam laser spectroscopy (2005Ge06) 
J$L=0 in {+2}H({+24}Ne,p) 
T$from 1973Go11. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
E$ unusual raising of first 3/2+ state is an indication of migration of neutron magic number from N=20 to N-16 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_comment:
E$assumed that the ground state of {+25}Ne is populated in this decay 
J$from {+25}Ne Adopted Levels in the ENSDF database 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$From beta decay activity (1992Te03 - reported uncertainty {i1} - probably statistical only - evaluator increased to {i2}). Others: 192 ms {i6} (82.5|g(t) - 2004We11); 2007Su05 reports 192 ms {i4} (153|g(t)), 193 ms {i3} (232|g(t)) and 190 ms {i10} (1212|g(t)); 230 ms {i60} (1987DuZU). 
%B-N$from 1992Te03. Other: <0.2% (2004We11) 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$J|p=0+ was originally assigned in {+26}Mg(|p{+-},|p{++}) (1980Na12). 2007Gi06 conclude the measured |s=7 mb {i4} ({+26}Ne,{+26}Ne'|g) - is not consistent with J|p=0+ and comparing with shell model calculation it is assigned as 2+{-2}. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$E1 excited pygmy state detected at energies of |?9 MeV (2008Gi09). This state decays by neutron emission to g.s., 1700, 2000, and 3300 levels in {+25}Ne with branching ratios of 5% {I17-5} to g.s.; 66% {I15} to 1700+2000; and 35% {I9} to 3300 levels, respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (0+)
level_comment:
E$Probably a doublet of 3691 and 3815 keV levels. New 0+ state at 3815.2 keV in Adopted Levels established from {+26}F |b{+-} decay (9.7 ms). 
J$Proposed in 1980Na12 from shell model predictions at 5280 keV. J|p=2+ in Adopted Levels. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$From Adopted Levels. 1999Re16 tentatively assign J|p=0+, as in 1980Na12 from {+26}Mg(|p{+-},|p{++}) studies. 


level_energy_unit: KEV
level_spin_parity: (0+)
level_comment:
E$1999Re16 note a few observed events at about 3750 keV which expected to be the 0+ state. However, without any associated |g transitions, 1999Re16 tentatively assign 0+ state for 3691 keV level. It appears that 3750 could be a doublet of 3691 and 3815 keV levels. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
BE2$From 2007Gi06. Nuclear contribution subtracted. A B(E2)=0.025 {i3} (that includes contribution from nuclear excitation) deduced from total cross section=68 mb {i8} (2007Gi06) is consistent with earlier value of B(E2)=0.0228 {I41} in 1999Pr09. 
T$deduced from B(E2)|^ and adopted 2017.9|g properties. 
$|s=68 mb {i8} (2007Gi06); 74 mb {i13} (1999Pr09) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (2+)
level_comment:
$|s=7 mb {i4} (2007Gi06) 
J$measured |s is not consistent with the J|p=0+, that was proposed in earlier studies. 


level_energy_unit: KEV
level_energy_info: ;ERR=AP;ERR=?
level_comment:
E$From 2008Gi09. E1 excited pygmy state detected at energies of |?9 MeV. This state decays by neutron emission to g.s., 1700, 2000 and 3300 levels in {+25}Ne with branching ratios of 5% {I17-5} to g.s.; 66% {I15} to 1700+2000; 35% {I9} to 3300 levels, respectively. 
L$ From angular distribution measurements 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
J$log| {Ift}=4.4 in {+27}Ne |b{+-} decay to the g.s. (J|p=5/2+) of {+27}Na. J|p({+21}Ne)=3/2+ 
T$from 2006Tr02 (63|g-t). Others: 32 ms {I2} (1992Te03), 22 ms {I6} (2001Pe14,1999Dl01) 
%B-N$from 1992Te03. Others: 3 {I1} (2006Tr02), <3 (2001Pe14,1999Dl01) 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_comment:
J$from (d,p) cross section in inverse kinematics reaction of {+2}H({+26}Ne,{+27}Ne|g) and multipolarity constraints for 765|g, 120|g and 885|g to the g.s. J|p=(3/2+), J|p=(1/2,3/2,5/2)- proposed in 2006Ob01. J|p=(3/2-) is supported by shell model calculation (2006Te04) with a configuration: |np{-3/2} and L=(0,1) from ({+1}H({+28}Ne,{+27}Ne|g)) reaction study. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
J$From comparison of the experimental level energy with the shell model calculation. 
T$The upper limit of T{-1/2} for this state is proposed in 2006Te04 based on the symmetric shape of the 885-keV photopeak. 


level_energy_unit: KEV
level_spin_parity: (1/2,3/2,5/2)-
level_comment:
$C{+2}S=0.6 {I2} 
J$from shell model calculation and multipolarity constraints for 765|g, 120|g, and 885|g to the g.s. J|p=(3/2+). J|p=(1/2,3/2,5/2)- has been proposed in 2006Ob01. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
$|s=21 mb 2 ({+9}Be({+28}Ne,{+27}Ne)), this value may include cross section for the population of a 7/2- isomer (2006Te04) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_lifetime_unit: PS
level_lifetime_info: ;ERR=LT
level_comment:
$C{+2}S=1.07 {I7} 
T$the upper limit of T{-1/2} for this state is proposed in 2006Te04 based on the symmetric shape of the 885-keV photopeak. 
$|s=35 mb 2 ({+9}Be({+28}Ne,{+27}Ne)-2006Te04) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
E$ from 2006Ob01 
J$ From p(765|g)(|q) distributions, best fit for 3/2-, L=1; second best fit is for L=2 giving 3/2+ or 5/2+, but no such state is expected from theoretical predictions 
$ Intruder state 


level_energy_unit: KEV
level_spin_parity: 7/2-
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=LT
level_comment:
E,J$ from 2012Br01. Unbound state to neutron emission 
T$ from Breit-Wigner shape analysis. Width represents 2|s limit. Natural width is 3.5 keV {I10} using Vincent and Fortune method. 
$ Intruder state 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
$|d<r{+2}>({+20}Ne,{+28}Ne)=-0.239 fm{+2} {i35} (stat) {i213} (syst) (2011Ma48). 
T$Average of 21 ms {I1} (2063|g-t) and 19 ms {I1} (863|g-t) in 2006Tr02. Others: 18.4 ms {I5} (2005Tr05), 18 ms {I3} (1999Re16), 20 ms {I3} (1999Dl01), 21 ms {I5} (1997Ta22), 17 ms {I4} (1992Te03) and 16 ms {I9} (1991Re02). 
%B-N$From 2006Tr02 and 2005Tr05. Others: 11 {I3} (1999Re16,1999Dl01), and 22 {I3} (1992Te03). 
%B-2N$From 2006Tr02. Other: 3 {I1} (2005Tr05). 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: PS
level_comment:
J 1304|g E2 to 0+ state. 
T$Using B(E2)|^=0.0132 {I23} (2005Iw02) and the adopted |g-ray properties. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J 4{-1}+ in (({+29}Na,p|g)-2007RoZY), based on comparison of the experimental level scheme with the predicted energies by shell model. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E$In 2007RoZY - ({+29}Na,p|g) - 3904 keV {i7} level is deduced from a single cascade of |g-ray measurements and identified as bound state. In 2012Sm08, 3860 keV {i110} level is deduced from the measured decay energy of 32 keV {i22} in the {+27}Ne+n system and the best fit. Considering S(n)({+28}Ne) and the assumption of decay to the g.s., the state is interpreted as unbound in 2012Sm08. The level energies are statistically consistent and located within/around the neutron separation energy (3820 keV {i120} - 2012Wa38). Evaluator assumes these states are same and may decay by competing |g rays and neutrons. For this to be significant, one expects the |g-decay lifetime to be short compare to the neutron-decay lifetime. Using the M1 strength in Table 6.1 (2007RoZY) and 894|g, a |g-decay lifetime of 4.9 fs is estimated. Considering |G=0.09 eV and J|p=4+ from Table I (2012Sm08) for this state, a neutron-decay lifetime of 7.3 fs is calculated. 
J J|p=4{-2}+, based on comparison of the experimental level scheme with the predicted energies and transition strengths from shell model (2007RoZY). For the 3860 keV level J|p=2+,3+, or 4+ is suggested in 2012Sm08 from shell model calculations. 


level_energy_unit: KEV
level_spin_parity: (2+,3+,4+)
level_comment:
E$Deduced from the measured decay energy of 32 keV {i22} in the {+27}Ne+n system and the best fit. With a neutron separation energy of 3820 keV {i120} and the assumption of decay to the g.s., the state is interpreted as an unbound state in 2012Sm08. 
J$Suggested from shell model calculations. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J 4{-1}+ in 2007RoZY, based on comparison of experimental level scheme with the predicted energies and transition strengths by shell model. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
E From 2007RoZY 
J J|p=4{-2}+, based on comparison of the experimental level scheme with the predicted energies and transition strengths from shell model. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$Excitation |s=23 mb {I2} (2014Mi09) for first 2+ state 
$Deformation length |d=1.33 fm {I6}(stat) {I5}(syst) (2014Mi09) 
$|b{-2}=0.39 {I2}(stat) {I1}(syst) (2014Mi09) 


level_energy_unit: KEV
level_spin_parity: (2+,3+,4+)
level_comment:
E$from measured decay energy of 32 {I22} and S(n)=3820 {I120} from 2012Wa38. Note that 2012Sm08 quote 3.86 MeV {I11} using S(n)=3830 {I110} from 2007Ju03: Phys. Lett. B649, 43 
J$from shell-model predictions. 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$ |s{--1n}(Pb)=252 mb {I45}, Coulomb breakup contribution |s{--1n}(E1)=176 mb {I50}, and |s{--1n}(C)=36 mb {I7} for reaction ({+29}Ne,{+28}Ne(0+){-1}). 
$ Inclusive |s{--1n}(Pb)=379 mb {I14}, Inclusive Coulomb breakup contribution |s{--1n}(E1)=222 mb {I36}, and Inclusive |s{--1n}(C)=74 mb {I2}. 
$ Ground state fraction 66% {I12}, 79% {I26}, and 49% {I9} for |s{--1n}(Pb), |s{--1n}(E1), and |s{--1n}(C), respectively. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 2+
level_comment:
$ |s{--1n}(Pb)=127 mb {I43}, Coulomb breakup contribution |s{--1n}(E1)=46 mb {I49}, and |s{--1n}(C)=38 mb {I7} for reaction ({+29}Ne,{+28}Ne*). 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from |b-decay time spectrum gated on 2063|g. Other value: 18.2 ms {I5} obtained by gating on 863|g (2015Le17). 
%B-N$deduced by 2015Le17 from {+27}Mg |g-ray intensity measurements in {+27}Na |b- decay (1984Gu19 - Nucl. Phys. A 426, 37). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$|s{-exp}=8.4 mb {I8}. The |s{-exp} is deduced by subtracting the cross sections to all excited states from the inclusive |s{-exp}=28 mb {I1}. 


level_energy_unit: KEV
level_spin_parity: 2+
level_comment:
$|s{-exp}=3.6 mb {I3}. J{+|p} deduced from the momentum distibution after the subtraction of the contributions from the feeding states, based on the level scheme. 


level_energy_unit: KEV
level_comment:
$|s{-exp}=2.5 mb {I1}. J{+|p} =(0-,1-,2-,3-) from momentum distribution which favors one neutron removal from 1d{-3/2}. 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_lifetime_unit: MS
level_comment:
%B-N$weighted average of 29 {I7} (2006Tr02,2005Tr05), 27 {I9} (1999Dl01) and 27 {I9} (1999Re16). 
%B-2N$From 2006Tr02, 2005Tr05 
J From systematics. Its intruder configuration predicted to be ~100% 2p2h from shell model calculation. 
T$From 1997Ta22. Others: 15.1 ms {I26} (gated on 72|g-2006Tr02), 16.4 ms {I13} (gated on 1516|g-2006Tr02) 13.8 ms {I5} (2005Tr05,2005Tr13), 15.6 ms {I5} (1998NoZZ), 15 ms {I4} (1999Dl01), 19 ms {I9} (1999Re16), and 200 ms {I100} (1992Te03). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2-)
level_comment:
J Shell model calculation predicts negative-parity 1p1h 3/2- state at 420-keV and a 2p2h state of 1/2+ at 540-keV. 


level_energy_unit: KEV
level_spin_parity: (1/2+,7/2+)
level_comment:
J$From shell model calculation with 2p2h "K=1/2 band" of levels at 540-keV (1/2+) and 850-keV (7/2+). 


level_energy_unit: KEV
level_spin_parity: (1/2+,3/2-)
level_comment:
J The MCSM predicts negative-parity 1p1h 3/2- state at 420-keV and a 2p2h state of 1/2+ at 540-keV. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
$ Dominated by a {+28}Ne(0+{-1})~#2p{-3/2} neutron configuration. 
J$Proposed in 2016Ko05, based on deduced width, 98 MeV/c {I12} (FWHM), of measured inclusive parallel momentum distribution of {+28}Ne residues. Also supported by comparisons of measured inclusive and partial 1n-removal cross sections on C, Pb targets, and spectroscopic information from large-scale shell model calculations. 
$ R{-s}=|s{+exp}{--1n}/|s{+Th}{--1n} = 1.07 {I3} 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$As proposed by 2023Wa18, the experimental partial cross sections measured for {+28}Ne were used to probe the wave function composition of the g.s. The authors state that the large 2p{-3/2} contribution comes from the {+28}Ne 0{++}{-gs} and 2{++} states and from the (0,2){++} states above 2 MeV. The measurements were performed using the momentum distributions of {+28}Ne residues. Based on the measured partial |s{-exp}, 2p{-3/2} spectroscopic factors C{+2}S{-exp} are 1.82 {I7} and 1.16 {I5} using DWIA and eikonal single-particle cross sections, respectively. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$from 2015St14 - |b|g(t). Others: 7.3 ms {I3} (2007Tr08), 7 ms {I2} (2001Pe14,1999Re16,1997Ta22), 7.5 ms {I15} (1999Dl01) is from the same group as 1999Re16 and 1997Ta22, 5.8 ms {I2} (1998NoZZ). 5.8 ms {I2} (1998NoZZ) is a discrepant value - from the 1-page report of 1998NoZZ or other publications the source for this discrepancy is not clear. 
%B-N$from 2015Bi05. Others: 13 {I4} (2007Tr08), 9 {I+17-9} (1999Re16), 9 {I17} (1999Dl01). 
%B-2N$from 2007Tr08, 2015Bi05 
Proton radius: <r{+2}>{+1/2}=2.78 fm {I32} (2014Oz02), deduced from measured total charge-changing cross sections. 


level_energy_unit: KEV
level_spin_parity: (2+)
level_lifetime_unit: PS
level_comment:
E this energy level is the lowest of all the 2{-1}{++} states in the neighboring even-even N=20 isotones and provides evidence for a collective state based on a deformed 2p2h ground state (2010Fa04). 
J expected from the B(E2)|^ measurements. 
T from B(E2)|^=0.0277 {I79}, adopted E|g=794 {I4} and branching ratio. 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$in addition to the comparison of the experimental level energy with the predicted level energy by shell model calculation, the properties of direct two-proton knockout from the 1d{-5/2} level are used to constrain the data for the J|p=(4+) assignment (2010Fa04). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
B(E2)(from |b{-2})=0.046 {i27} (2003Ya05), assuming electromagnetic deformation is the same as for (p,p') scattering. 
$|s=37 mb {I4} (2014Mi09) for the first 2+ state 
$|s=39 mb {I5} (2014Mi09) including possible feeding from higher state; no higher state was reported in 2014Mi09. A 794-1443 cascade was reported in 2010Fa04 and proposed a 2235-keV level. 1443|g was not confirmed in 2014Mi09. 
$Deformation length |d=1.59 fm {I+8-9}(stat) {I7}(syst) (2014Mi09) 
$|b{-2}=0.45 {I+2-3}(stat) {I2}(syst) (2014Mi09) 
$|s=14.4 mb {I14} for the carbon target and 56 {I6} for the lead target (2016Do03). Assumed feeding of 6% {I6} from the higher possible levels was subtracted by authors 
$Deformation length |d{-N}=1.98 fm {I11} (2016Do03) from data with carbon target, which implies deformation parameter |b{-N}=0.53 {I3}, assuming R=1.2|a{+1/3} fm 
$Deformation length |d{-C}=1.87 fm {I25} (2016Do03) from data with lead target, which implies |b{-C}=0.50 {I7} and B(E2)|^=0.0277 {I79}, using |b{-C}=|d{-C}/R, and B(E2)|^=[(3ZeR{+2})/4|p]{+2}|b{-C}{+2}, assuming radius R=1.2|a{+1/3} fm 


level_energy_unit: KEV
level_spin_parity: (4+)
level_comment:
J$in addition to the comparison of the experimental level energy with the predicted level energy by shell model calculation, the properties of direct two-proton knockout from the 1d{-5/2} level are used to constrain the data for the J|p=(4{-1}{++}) assignment (2010Fa04). 


level_energy_unit: KEV
level_spin_parity: 0+
level_comment:
$Inclusive |s{-1n}({+31}Ne,{+30}Ne): 90 mb {I7} (carbon target), 720 mb {I61} (lead target), and 529 mb {I63} (Coulomb breakup). 
$Partial cross section (feeding g.s. of {+30}Ne directly) |s{-1n}({+31}Ne,{+30}Ne*): 33 mb {I15} (carbon target), 518 mb {I103} (lead target), and 448 mb {I108} (Coulomb breakup). 


level_energy_unit: KEV
level_spin_parity: (2+)
level_comment:
J$from the Adopted Levels 
$Partial cross section (feeding excited states of {+30}Ne) |s{-1n}({+31}Ne,{+30}Ne*): 57 mb {I13} (carbon target), 201 mb {I83} (lead target), and 81 mb {I87} (Coulomb breakup). It is assumed that all the populated bound excited states above this level feed the ground state via this 2+ state. 


level_energy_unit: KEV
level_spin_parity: (3/2-)
level_lifetime_unit: MS
level_comment:
$Only the |b{+-} decay has been observed, and particle stability established by 1996Sa34 and 1997Sa14. 
$Theoretical T{-1/2}=15.0 ms, %|b{+-}n=59, %|b{+-}2n=11, %|b{+-}3n=0 (2019Mo01) 
$Theoretical T{-1/2}=7.7 ms, %|b{+-}n=81.5; %|b{+-}2n=9.9, 10.0; %|b{+-}3n=0.68, 0.57; %|b{+-}4n=0.007, 0.003 (2021Mi17) 
J$from comparisons of measured inclusive and partial one-neutron removal cross sections, inclusive parallel momentum distribution of {+30}Ne residues with eikonal-model predictions using C{+2}S(0{++}{-1}; 2p{-3/2})=0.32 {I+21-17} obtained from shell-model calculations considering SDPF-M interactions (2014Na10). From consistency of the measured data with the shell-model calculations, {+31}Ne is identified as deformed and having a significant p-wave halo component. 
$Configuration=|n1/2[330] with |b{-2}=0.2 is favored over the |n3/2[321] with |b{-2}=0.55 in the theoretical calculations (2011Ur01, 2012Ur06) and comparison with measured cross sections for the Coulomb dissociation of {+31}Ne. However, 2011Ur01 point out that 1/2+ configurations such as 1/2[200] with |b{-2}|?0.95 or with oblate |b{-2}|?-0.35 cannot be excluded only from the Coulomb dissociation data. 2012Su09 analyze |s(|q) data in {+12}C({+31}Ne,{+31}Ne') E=240 MeV/nucleon obtained by 2012Ta02 and deduce |b{-2}|?0.4 
T$tentative half-life from |b-decay curve (1998NoZW,1998NoZZ). Further experimental measurements are needed for the half-life measurement. 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_comment:
J$from comparisons of measured inclusive and partial one-neutron removal cross sections, inclusive parallel momentum distribution of {+30}Ne residues with eikonal-model predictions using C{+2}S value noted below. From consistency of the measured data with the shell model calculations, {+31}Ne is identified as deformed and having a significant p-wave halo component. 
$C{+2}S (0{++}{-1}; 2p{-3/2})=0.32 {I+21-17}, obtained from shell model calculations considering SDPF-M interactions (2014Na10). 
$Interaction |s=1435 mb {I22} (2012Ta02). Glauber-type analysis of data and interpretation in terms of low (L=0 or 1) orbital halo structure in {+31}Ne 
$1n-removal |s=90 mb {I7} (2014Na10), 79 mb {I7} (2009Na39) on a carbon target; 720 mb {I61} (2014Na10), 712 mb {I65} (2009Na39), on a Pb target 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: MS
level_comment:
T$weighted average of 4.5 ms {I7} (2022Cr03) and 3.5 ms {I9} (1998NoZW, tentative result). 
$Calculated T{-1/2}=15 ms (2019Mo01), 6.7 ms (2021Mi17) 
$Calculated %|b{+-}n=75, %|b{+-}2n=4, %|b{+-}3n=0 (2019Mo01) 
$Calculated %|b{+-}n=85.2, %|b{+-}2n=3.9, %|b{+-}3n=2.9, %|b{+-}4n=0.015 (2021Mi17) 


level_energy_unit: KEV
level_lifetime_unit: NS
level_lifetime_info: ;ERR=LT
level_uncertain: ?
level_comment:
${+33}Ne g.s. is unbound towards neutron emission, according to non-observation of any events which could be assigned to {+33}Ne in the experimental studies by 2007Ba71, 2002Lu09, and 2002No11 carried out at RIKEN, RIKEN-GANIL-Dubna collaboration, and NSCL-MSU. Most likely this nucleus is unbound towards one-neutron emission, as S(n) is -1060 keV {I780} (syst), and S(2n)=1190 {I660} (syst) (2021Wa16). 
J$predicted values: 3/2- (theory, 2019Mo01), 7/2- (syst, 2021Ko07) 
T$<180 ns estimated from time-of-flight in 2007Ba71. 
$Theoretical T{-1/2}(|b decay)=5.9 ms (2019Mo01), 5.7 ms (2021Mi17) 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: NS
level_lifetime_info: ;ERR=GT
level_comment:
T$limiting value from time-of-flight in 2002No11. Actual half-life is expected to be much longer as suggested by systematics value of 1 ms (systematics, 2003Au02 and 2011AuZY) and calculated value of 5.2 ms (1997Mo25). 
$Calculated %|b{+-}n=1.1, %|b{+-}2n=39.9 (1997Mo25) 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$from E(3p+{+14}O){-rel}=4.85 MeV {I6}. The group is twice as broad as expected and may represent a collection of unresolved J|p=1/2+, 3/2+ and 5/2+ levels. 
J$from expected systematics. 


level_energy_unit: KEV
level_spin_parity: (1/2+)
level_comment:
E$from E(3p+{+14}O){-rel}=4.85 MeV {I6}. The group is twice as broad as expected and may represent a collection of unresolved J|p=1/2+, 3/2+ and 5/2+ levels. 
E$E(3p+{+14}O){-rel}=4.85 MeV {I6} implies S{-p}=-3.45 MeV {I6} using S{-2p}({+14}O)=-1.40 MeV {I2} (2012Wa38). 
J$from expected systematics. 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=LT
level_comment:
$Excitation energies are reported with respect to E{-res}(p+{+17}Ne)=1.25 MeV {I11}, the accepted value in (2012Wa38). 
T$<0.2 MeV (2012Mu05); also see |G=0.48 MeV {I14} (2004Ze05). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
E$from E{-res}=1552 keV {I5} and {+18}Na{-g.s.} with S{-p}=1.25 MeV {I11}. 
T$for |G{-0} to {+17}Ne{-g.s.}; there is a limit of |G<1 keV for decay to {+17}Ne excited states. 


level_energy_unit: KEV
level_spin_parity: 0-
level_lifetime_unit: KEV
level_comment:
E$from E{-res}=1842 keV {I40} and {+18}Na{-g.s.} with S{-p}=1.25 MeV {I11}. 
T$for |G{-0} to {+17}Ne{-g.s.}; there is a limit of |G<10 keV for decay to {+17}Ne excited states. 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: KEV
level_comment:
E$from E{-res}=2030 keV {I20} and {+18}Na{-g.s.} with S{-p}=1.25 MeV {I11}. 
T$for |G{-0} to {+17}Ne{-g.s.}; there is a limit of |G<100 keV for decay to {+17}Ne excited states. 


level_energy_unit: KEV
level_spin_parity: 3-
level_lifetime_unit: KEV
level_comment:
E$from E{-res}=2084 keV {I5} and {+18}Na{-g.s.} with S{-p}=1.25 MeV {I11}. 
T$for |G{-0} to {+17}Ne{-g.s.}; there is a limit of |G<1 keV for decay to {+17}Ne excited states. 


level_energy_unit: KEV
level_spin_parity: (1)-
level_lifetime_unit: MEV
level_lifetime_info: ;ERR=LT
level_comment:
In (2012Mu05) E{-res}(p+{+17}Ne)=1.23 MeV {I15} while (2004Ze05) report 1.27 MeV {I17}. Excitation energies are reported with respect to 1.25 MeV {I11}, the accepted value in (2012Wa38). 
T$<0.2 MeV (2012Mu05); also see |G=0.48 MeV {I14} (2004Ze05). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: MEV
level_comment:
from E{-res}(p+{+17}Ne)=1.55 MeV {I7} (2012Mu05) and {+18}Na{-g.s.}=E{-res}(p+{+17}Ne)=1.25 MeV {I11}. 
T$0.25 MeV {I+25-15} (2012Mu05). 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3-
level_uncertain: ?
level_comment:
from E{-res}(p+{+17}Ne)=2.084 MeV from (2011AsZX) and {+18}Na{-g.s.}=E{-res}(p+{+17}Ne)=1.25 MeV {I11}. This state is not conclusively observed; however in (2012Mu08) including this J|p=3- state at Q(p+{+17}Ne)=2.084 MeV permits a quantitative reproduction of the correlation spectra. 


level_energy_unit: KEV
level_spin_parity: (5/2+)
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
$(2010Mu12) state that |G<40 keV reflects the experimental resolution of the detector system. The actual |G is expected to be <1 eV. 
Decays to {+18}Ne{-g.s.} 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E,J,T,L$from (2003An02). Others: (2005De15,2006Sk09). 
$E{-res}(cm)=1066 keV {I3} (2003An02). 
E$the corresponding level is at 1471.7 keV in the mirror nucleus {+19}O 


level_energy_unit: KEV
level_lifetime_unit: MEV
level_comment:
$Sequential decay via {+18}Ne*(4589) to {+17}F*(495) is suggested. 
E$5809 and 5815 probably correspond to different decay modes of the same state. 


level_energy_unit: KEV
level_spin_parity: 1/2+
level_lifetime_unit: KEV
level_comment:
E,J,T,L$from (2003An02). Others: (2005De15,2006Sk09). 
$E{-res}(cm)=1066 keV {I3} (2003An02). E{-res}(cm)=1076 keV {I6}, |G{-p}=80 keV {I20} (2005De15), and E{-x}=740 keV {I30}, |G=130 keV {I50} (2006Sk09). 
E$corresponding level is at 1471.7 keV in mirror nucleus {+19}O 


level_energy_unit: KEV
level_spin_parity: (5/2,3/2)+
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-0}/|G{-tot}=0.43 {I5} 
$E{-res}(cm)=2780 keV {I30} (2008Pe02), uncertainty of 10 keV is also given in the abstract of (2008Pe02) 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2+)
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-0}/|G{-tot}=0.12 {I4} 
$E{-res}(cm)=3090 keV {I60} (2008Pe02), uncertainty of 50 keV is also given in the abstract of (2008Pe02). 


level_energy_unit: KEV
level_lifetime_unit: KEV
level_lifetime_info: ;ERR=LT
level_comment:
E$From Q{-1p}({+19}Na)=0.328 MeV {I22} group (2010Mu12) which is associated with {+19}Na decay to {+18}Ne{-g.s.} observed in analysis of (p{-1}-{+18}Ne)(p{-2}-{+18}Ne) correlations from {+20}Mg breakup. 
$2010Mu12 state that |G<40 keV reflects the experimental resolution of the detector system. The actual |G is expected to be <1 eV. 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MS
level_comment:
T$Weighted av: 442 ms {I5}(1971Go18),446 ms {I8}(1972Mo08), 448 ms {I4}(1972To08),452 ms {I4}(1989Cl02) 


level_energy_unit: KEV
level_spin_parity: 2+
level_lifetime_unit: MS
level_comment:
MOME2$ from 2009Mi04, deduced using the |b-NMR technique, sign of the quadrupole moment is not given by this method. Value measured relative to Q({+27}Na)(g.s.)=0.0072 {I3} (2000Ke09: Eur Phys J A 8, 31 (2000)) 
$J, t, %|e, %|e|a, T from 'adopted levels, gammas' dataset for {+20}Na in ENSDF database 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$ deduced by 2009Sc23 from B(E2) and B(M1) values. (T{-1/2}=22.2 ps {I+42-51} reported in 2009Sc23 is corrected in the erratum published by 2009Sc23 in Phys Rev C 82, 069902 (2010)) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3+
level_comment:
$Decays 51% to {+19}Ne{-g.s.}({Il}=2) and 49% to {+19}Ne*(0.24 MeV) ({Il}=0), |G{-p0}=0.615|+0.062(stat)|+0.259(sys) eV and |G{-p1}=0.584|+0.066(stat)|+0.036(sys) eV 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1+
level_comment:
$This branch could not be observed in the present measurement due to a high {+20}Na contamination in the beam that obscured the associated part of the spectrum. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
T$Weighted average of 22.55 s {I10} (1974Al03), 22.48 s {I4} (1977Az01) 
J$From magnetic moment. Mirror of {+21}Ne ground state. 
MOMM1,MOME2$From 2011StZZ 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_lifetime_unit: PS
level_comment:
MOMM1,MOME2$From 2011StZZ 
BE2$Weighted average of discrepant values 0.0205 {I14} (2008Sc18) and 0.0137 {I9} (2009Sc28) with external error. 
T$From {+2}H({+20}Ne,n) (1978Ro10). Other values: 10 ps {I2} (1968Ba12), 6.9 ps {I3} (1977Be30). 
J$log| {Ift}=4.79 from 5/2+, {+20}Ne(p,|g) angular correlation. Mirror of 350.7 keV, 5/2+ level in {+21}Ne. 


level_energy_unit: KEV
level_spin_parity: 7/2+
level_lifetime_unit: FS
level_comment:
MOMM1,MOME2$From time differential perturbed angular correlation (TDPAC) measurement (1977Be30) 
J$log| {Ift}=5.11 from 5/2+ and {+24}Mg(|a,p) |a-p{-0} angular correlations. Mirror of 1745.9 keV, 7/2+ level in {+21}Ne. 


level_energy_unit: KEV
level_spin_parity: 1/2-
level_lifetime_unit: FS
level_comment:
J${+24}Mg(|a,p) |a-p{-0} angular correlation, l=1 in {+20}Na(d,n). Mirror of 2788.8 keV 1/2- in {+21}Ne. 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$Weighted average of 31 fs {I10} (1969An14), and 41 fs {I8} (1975An14). Uncertainty increased by evaluator. Other: 8 fs {I2} (1972Du16). 
J$Not 7/2- 


level_energy_unit: KEV
level_lifetime_unit: FS
level_comment:
T$Weighted average of 1.5 fs {I3} (1975Ro08), and 2.7 fs {I8} (1977An17). Other: <0.7 fs (1972Du16). 


level_energy_unit: KEV
level_spin_parity: (3/2+)
level_comment:
S$corresponding to ANC=0.21 {I4}. Other values range from 0.0357 to 0.0423 for different sets of optical potential parameters 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (5/2+)
level_comment:
S$corresponding to ANC=2.78 {I43}. Other values range from 0.409 to 0.492 for different sets of optical potential parameters 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (7/2+)
level_comment:
S$corresponding to ANC=(0.00011 {I3}). Other values range from 0.0328 to 0.0412 for different sets of optical potential parameters 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (1/2+)
level_comment:
S$corresponding to ANC=(6.1|*10{+33} {I8}). Other values range from 0.572 to 0.629 for different sets of optical potential parameters 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
MOME2$From 2009Mi04, deduced using the |b-NMR technique. Value measured relative to Q({+27}Na{-g.s.})=0.0072 {I3} (2000Ke09). Sign of quadrupole moment is not given by this method. 
$J, t, %|e+%|b{++} from Adopted Levels, Gammas. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
J$from Adopted Levels of {+21}Na in ENSDF database 
T$measured as 22.4506 s {I16}(stat) {I29}(syst) by 2017Fi07 from a weighted average of 120 runs, and accounting for systematic uncertainties arising from deadtime and other corrections. Authors give a world averaged value of 22.448 s {I8}, by combining their value, with literature values of 22.422 s {I10} (2015Gr05: Phys. Rev. C91, 032501(R)); 22.48 s {I4} (1975Az01: Phys. Rev. C12, 563); and 22.55 s {I10} (1974Al03: Phys. Rev. C9, 991), where the final uncertainty was inflated by Birge ratio of 1.73. 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 1/2+
level_lifetime_unit: EV
level_comment:
$|G{-|g}=0.17 eV {I3} for R/DC to g.s., mult=M1 
$ANC=-2.80|*10{+17}, with uncertainty 0.14|*10{+17} fm{+-1/2} from a Monte Carlo analysis, and ({I+27.2-2.4})|*10{+17} fm{+-1/2} from variation of the level energy and proton separation energy over 1|s range (2018Ly04) 


level_energy_unit: KEV
level_spin_parity: 3/2-
level_lifetime_unit: EV
level_comment:
$|G{-p}=210 keV {I8} 
$|G{-|g}=0.015 eV {I2} for R/DC to g.s., mult=E1 
$|G{-|g}=-1.1 eV {I1} for R/DC to 332 level, mult=E1 
$|G{-|g}=-0.44 eV {I5} for R/DC to 2425 level, mult=E1 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 5/2+
level_comment:
$|G{-p}=3.93 keV from literature, fixed in the R-matrix fit 
$|G{-|g}=-0.011 eV {I10} (mult=M1) and -0.015 {I11} (mult=E2) for R/DC to g.s. 
$|G{-|g}=-0.18 eV {I5} for R/DC to 332 level, mult=E2 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: 3/2-
level_comment:
$|G{-p}=3500 keV, fixed at Wigner limit 
$|G{-|g}=0.2 eV {I1} for R/DC to g.s., mult=E1 
$|G{-|g}=-20 eV {I8} for R/DC to 332 level, mult=E1 
$|G{-|g}=-6.2 eV {I11} for R/DC to 2425 level, mult=E1 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_comment:
T$From |b(t) measurements. Uncertainty simplified by compiler: 2018Sh27 report half-life value of 22.4615 s {I39} (stat) {I+1-15} (syst). The decay positrons were counted using high-efficiency 4|p proportional gas counter. The final half-life was deduced from the average of the results from 21 separate runs. A global average value of 22.4528 s {I55} reported by 2018Sh27 considering literature values of 22.47 s {I3} (1975Az01 - Phys. Rev. C12, 563), 22.422 s {I10} (2015Gr05 - Phys. Rev. C 91, 032501), and 22.4506 s {I33} (2017Fi07 - Phys. Rev. C 96, 025501) - averaging method not mentioned. A weighted average of 22.4531 s {I55} can be obtained for these values with |h{+2}=4.99 and |h{+2}{-crit}=2.6 at 95% confidence level. Literature values 23.0 s {I2} (1958Ar15 - Nuclear Phys. 6, 196) and 22.55 s {I10} (1974Al03 - Phys. Rev. C9, 991) were not considered as being outlier. 


level_energy_unit: KEV
level_spin_parity: (3/2,5/2,7/2)+
level_comment:
$E{-p} (cm)=5868 keV {I10}, 4257 kev {I10}, 1630 keV {I10}, and 906 keV {I10} (tentative placement later three). 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_comment:
$E{-p} (cm)=5983 keV {I10} and 4356 keV {I10}, 2015Lu12 argue for lower |G{-tot} value compared to literature value of 30 keV {I13} for this resonance. 


level_energy_unit: KEV
level_spin_parity: 5/2+
level_comment:
E$Isobaric Analog State (IAS) of {+21}Mg g.s.. 
$E{-p} (cm)=6537 keV {I10}, 4913 keV {I10}, 2302 keV {I10}, 1564 keV {I10}, and 919 keV {I21}. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: Y
level_comment:
MOMM1$From 2013StZZ, 2014StZZ - Adjusted by tabulator - |b-NMR. Other: +0.185 {i11} - Atomic beam laser spectroscopy (1998Ga44, 2014StZZ). 
T$From 950.3 d {I8}: Weighted average of 957 d {I7} (1961Wy01), 954 d {I4} (1965An07), 950.7 d {I4} (1965An07), 950 d {I4} (1965An07), 950.34 d {I13} (1980Ho17), 950.25 d {I11} (1980RuZX, replaced by 1982RuZV), 950.30 d {I25}, (1982RuZV), 950.1 d {I7} (Updated NIST value in 2014Un01 - earlier value 950.97 d {I15} in 2002Un02). Other values: 946.3 d {I11} (1965An07), 951.71 d {I11} (1982HoZJ, replaced by 1992Un01). 2008Li02 and 2006Li34 report 0.46% {I14} and 1.2% {I14} shorter |b+ half-lives measured in implanted Pd at 15K and 12K, respectively, compared with values measured at room temperatures. However, 2008Ru05 reports no difference at the 0.04% level, measured in implanted Al at 10K and room temperatures. A half-life value of 2.57 y {I13} at room temperature is reported (2008Ru05). 
J$Atomic beam measurement (1949Da14), L=2 in ({+3}He,|a), Unnatural parity (pol d,|a). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: NS
level_comment:
MOMM1$From Time Dependent Perturbed Angular Distribution (1966Su07). +0.523 {i11} in 1989Ra17. 
J$log| {Ift}=3.64 from 0+, L=0+(2) in ({+3}He,p), L=2 in ({+3}He,|a), unnatural parity (pol d,|a). 
T$From 1966Su07. Other value: 266 ns {I10} (1958Te15). 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: FS
level_comment:
J$log| {Ift}=3.46 from 0+, unnatural parity (pol d,|a). 
T$From mean lifetime 19 fs {I6}: weighted average of 29 fs {I5} (1967Wa13) and 16 fs {I3} (1978Bi11). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
MOMM1$From 1976Be06. 
J$L=1 in ({+3}He,|a), L=(1) in ({+3}He,p). |g to 0+. Natural parity (pol d,|a). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: FS
level_comment:
E,J$From angular correlation, linear polarization measurements of 2815|g (|a,n),(|a,n|g) (1973Ma23, 1977Ha11). Natural parity (pol d,|a). 


level_energy_unit: KEV
level_spin_parity: (5+)
level_lifetime_unit: FS
level_comment:
J$Weakly populated in one and two nucleon transfer (indication for high spin), strongly populated in ({+16}O,|a) and consistent with Hauser-Feshbach prediction for spin-parity 7+ (discussion in 1975Sp02); 2995.8|g to 5+; Unnatural parity in (pol d,|a). 
T$From mean lifetime of 103 fs {I48}, weighted average of 55 fs {I20} (1976Ma23), 115 fs {I45} (1973Fr18), and 160 fs {I23} (1977Ev02) using the Limitation of Relative Statistical Weight (LWM) averaging method (1985ZiZY). 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: FS
level_comment:
J$|g to 2+, 3+, 4+, 5+. Possible 3+ discarded based on linear polarization measurement of the 2041|g (1976Ma23). 


level_energy_unit: KEV
level_spin_parity: (3+)
level_lifetime_unit: FS
level_lifetime_info: ;ERR=LT
level_comment:
J$L=2(+0) in ({+3}He,d); Unnatural parity (pol d,|a). 
E$Weighted average of 5317 {I15} (1964Hi05), 5317 {I7} (1971Ga04), and 5322 {I10} (1971Ga22). 


level_energy_unit: KEV
level_comment:
E$Weighted average of 5440 {I7} (1971Ga04), 5436 {I10} (1971Ga22), 5446 {I10} (1964Hi05), 5448 {I10} (1978Ha29). 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
E$Weighted average of 5871 {I10} (1964Hi05), 5858 {I10} (1971Ga04), 5865 {I10} (1971Ga22), 5858 {I10} (1978Ha29). 
J$L=0+2 in ({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
E$Weighted average of 6089 {I10} (1964Hi05), 6088 {I7} (1971Ga04), 6074 {I20} (1971Ga22), 6097 {I10} (1978Ha29). 
J$L=0+2 in ({+3}He,|a) 


level_energy_unit: KEV
level_spin_parity: (0 : 4)+
level_comment:
E$Weighted average of 6190 {I15} (1964Hi05), 6185 {I7} (1971Ga04), 6183 {I10} (1971Ga22), 6196 {I10} (1978Ha29). Possible doublet. 
J$L=2 in ({+3}He,d); (2) in ({+3}He,|a); 


level_energy_unit: KEV
level_comment:
E$Weighted average of 6241 {I15} (1964Hi05), 6247 {I7} (1971Ga04), 6236 {I10} (1971Ga22), 6240 {I10} (1978Ha29). 


level_energy_unit: KEV
level_spin_parity: (0 : 3)-
level_comment:
E$Weighted average of 6329 {I15} (1964Hi05), 6326 {I7} (1971Ga04), 6324 {I10} (1971Ga22), 6339 {I10} (1978Ha29). 
J$L=1 in ({+3}He,d) 


level_energy_unit: KEV
level_comment:
E$Weighted average of 6435 {I10} (1964Hi05), 6437 {I7} (1971Ga04), 6429 {I10} (1971Ga22), 6428 {I10} (1978Ha29). 


level_energy_unit: KEV
level_spin_parity: (1,2)+
level_comment:
E$Weighted average of 6556 {I15} (1964Hi05), 6557 {I7} (1971Ga04), 6543 {I10} (1971Ga22), 6445 {I10} (1978Ha29). 
J$L=0+2 in ({+3}He,d) 


level_energy_unit: KEV
level_comment:
E$Weighted average of 6591 {I15} (1964Hi05), 6582 {I7} (1971Ga04), 6594 {I20} (1971Ga22), 6565 {I15} (1978Ha29). 


level_energy_unit: KEV
level_comment:
E$Weighted average of 6671 {I15} (1964Hi05), 6664 {I7} (1971Ga04), 6674 {I10} (1971Ga22), 6667 {I15} (1978Ha29). 


level_energy_unit: KEV
level_comment:
E$Weighted average of 6752 {I15} (1964Hi05), 6750 {I7} (1971Ga04), 6770 {I20} (1971Ga22), 6780 {I15} (1978Ha29). 


level_energy_unit: KEV
level_spin_parity: 1,2+
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LT
level_comment:
J$|g's to 0+ and 2+. 1982Go11 proposed J|p=1,2 or 3-. J|p=3- is unlikely if |g ray feeding to 0+ is correct. 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
J$L=0 in (p,p),(p,p'). J|p=2+ excluded from non-interference with the Ep=768 keV (resonance state 7471 keV) (1983Go21). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
J$Assignment in 1977Ke04 (p,|g) based on |g feedings to 1-,2-,2+,3+. L=1 in (p,p),(p,p'). 1975Ch15 assigns J|p=1- with a note for doublet. 


level_energy_unit: KEV
level_spin_parity: 0+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 20.3 ps {I7} (1987Ne04), 18.8 ps {I8} (1980Fi07), Other value: 14 ps {I2} (1967KaZW) 


level_energy_unit: KEV
level_spin_parity: 4+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 11 ps {I3} (1967KaZW), 7.5 ps {I12} (1968Bl03), 8.5 ps {I12} (1968Pa11), 11.2 ps {I21} (1972Sn01), 10.2 ps {I5} (1973Ha55), 11.4 ps {I12} (1973Ha55), 9.6 ps {I6} (1977Og03), 10.7 ps {I4} (1977Ra01), 9.8 ps {I3} (1980Fi07), 9.8 ps {I4} (1977Ba77), and 10.0 ps {I5} (1969Jo10). 


level_energy_unit: KEV
level_spin_parity: 5+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 3.3 ps {I11} (1967KaZW), 2.6 ps {I6} (1967Wa13), 2.4 ps {I4} (1968Pa11), 3.5 ps {I4} (1973Ha55), 3.1 ps {I6} (1972Sn01), 3.26 ps {I24} (1973An01), 4.0 ps {I8} (1976Ma23), 4.1 ps {I5} (1977Og03), 3.72 ps {I19} (1977Ra01), 3.5 ps {I5} (1969Jo10), 3.4 ps {I2} (1977Ba77) and 3.0 ps {I10} (1973Ha55). 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: PS
level_comment:
T$Weighted average of 1.2 ps {I3} (1967Wa13), 1.21 ps {I24} (1968Pa11), 1.66 ps {I28} (1976Ma23), 1.66 ps {I21} (1973An01), 1.73 ps {I14} (1977Ra01), and 1.45 ps {I28} (1973Ha55). 


level_energy_unit: KEV
level_spin_parity: 1-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 15.5 ps {I10} (1973An01), 15.3 ps {I7} (1973Ha55), 13.7 ps {I12} (1977Og03), 14.1 ps {I15} (1973Ha55), and 14.7 ps {I6} (1977Ra01), 14.4 ps {I7} (1969Jo10), 15.2 ps {I6} (1976Be06). Other value: 8.3 ps {I14} (1968Bl03). 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: PS
level_comment:
T$Weighted average of 3.1 ps {I7} (1968Bl03), 4.0 ps {I6} (1968Pa11), 6.1 ps {I6} (1973Ha55), and 5.6 ps {I4} (1977Ra01) 


level_energy_unit: KEV
level_energy_info: ;ERR=?
level_spin_parity: (3-)
level_lifetime_unit: FS
level_comment:
T$Weighted average of 444 fs {I110} (1973Ha55) and 485 fs {I105} (1976Ma23). Other: >416 fs (1978Bi11). 


level_energy_unit: KEV
level_spin_parity: 6+
level_lifetime_unit: FS
level_comment:
T$Weighted average of 36 fs {I12} (1969Wa17), 53 fs {I14} (1973Ha55), 90 fs {I17} (1973An01), 55 fs {I28} (1973Ha55) and 76 fs {I14} (1976Ma23) 


level_energy_unit: KEV
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.3|*10{+-3} {I6} 
$Ep=126.3 {I6} (1982Go11). Other: Ep=126.69 {I4} (relative uncertainty) (1992Be35) 
|G from 1992Be35 


level_energy_unit: KEV
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.017 {I3} 
$Ep=270.67 {I4} (relative uncertainty) (1992Be35). Other: Ep=271.7 {I4} (1982Go11). 
|G from 1992Be35 


level_energy_unit: KEV
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.66 {I10} 
$Ep=271.56 {I4} (relative uncertainty) (1992Be35). Other: Ep=271.7 {I6} (1982Go11). 
From Ep=271.56 {I4} (1992Be35) and Sp 
|G from 1992Be35 


level_energy_unit: KEV
level_lifetime_unit: EV
level_lifetime_info: ;ERR=LT
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=0.016 {I3} 
$Ep=290.0 {I4} (1982Go11). Other: Ep=290.50 {I4} (relative uncertainty) (1992Be35) 
|G from 1992Be35 


level_energy_unit: KEV
level_spin_parity: 1+
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=12 {I3} 
J$M1+E2 |g's to 1+ and 2+. J|p=2+ excluded from non-interference with the Ep=768 keV (resonance state 7471 keV) (1983Go21). 
$Ep=701.8 {I5} (1977Be08) 


level_energy_unit: KEV
level_spin_parity: (1,2)-
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=2.9 {I10} 
J$From 1975Ch15 (p,p') and earlier studies. 
$Ep=1089.0 {I10} (1977Be08) 


level_energy_unit: KEV
level_spin_parity: 2-
level_lifetime_unit: KEV
level_comment:
$(2J+1)|G{-p}|G{-|g}/|G=9 {I3} 
$Ep=1237.0 {I21} (1977Ke04) 
J$Assigned in 1977Ke04 on the basis of |g ray feeding. 


level_energy_unit: KEV
level_spin_parity: 3+
level_lifetime_unit: D
level_comment:
T$from exponential fit to activity versus time (2024Po03). 
J$from the Adopted Levels of {+22}Na in the ENSDF database. 


level_energy_unit: KEV
level_spin_parity: 3/2+
level_lifetime_unit: S
level_lifetime_info: ;STABLE
level_comment:
$Matter radius <r{+2}>{+1/2}=2.83 fm {I3} and 2.83 fm {I4} (1998Su07). 
$Charge radius <r{+2}>{+1/2}=2.9936 fm {I21} (2013An02). 
J$3/2 from Atomic beam, optical spectroscopy: 1933Gr03, 1933Jo04, 1934El02, 1934Ra01. Parity from L=2 in {+22}Ne({+3}He,d). 
MOMM1$From 2019StZV - NMR (+2.2174982 {I233} in 2012An18 - ab initio calculation). Other values: +2.2176556 {I6} - NMR (1954Wa37), +2.217522 {I2} - ABMR (1974Be50). 
MOME2$Optical spectroscopy (2008Py02/2006Da14, 2016St14). Other values: +0.1045 {I10} (1999Ke12,2014StZZ), +0.109 {I3} (1992Su01), +0.095 {I15} (1992Vo09), many others in the literature. 


