19O 19N B- DECAY:336 MS:XUNDL-1 2006SU12 200609 19O c Compiled (unevaluated) dataset from 2006Su12: 19O 2c Phys Rev C 74, 024322 (2006). 19O c Compiled by: M. Mitchell and B. Singh (McMaster) August 30, 2006. 19O c {+19}N beam was produced from fragmentation of {+22}Ne beam at 19O 2c 80 MeV/nucleon on a {+9}Be target and separation of fragments 19O 3c using A1200 Fragment Recoil Separator at Michigan. The {+19}N 19O 4c beam were implanted in a scintilaltor, the main impurity was 19O 5c |?0.5% of {+17}C. Measured isotopic half-lives, E|g, I|g, |g|g, 19O 6c delayed neutrons, |gn coin using two HpGe detectors for |g rays and a 19O 7c neutron bar array (16 plastic scintillators) for neutrons. 19O 8c The half-lives were measured from neutron gated |g decay curves. 19O 9c Shell-model calculations 19O cB IB$ Uncertainties assigned by the compilers 19O cB LOGFT$ Deduced by compilers using log| {Ift} code at www.nndc.bnl.gov 19O cL E$From least-squares fit to E|g's (by compilers). 19O cL E$ For neutron decaying states, values deduced by the 19O 2cL compilers using energies (in lab system) of neutron branches as 19O 3cL quoted by 2006Su12 and S(n)(for {+19}O)=3954.9 {I28} (2003Au03) 19N P 0.0 1/2- 336 MS 3 12527 17 19N cP T$From 2006Su12 19N cP QP$from 2003Au03 19O N 1 1 19O cN BR$%|b{+-}n=41.8 {I9} (2006Su12) 19O PN 3 19O L 0 5/2+ 19O B 7.5 LT 8.9 GT 1U 19O cB LOGFT$ for expected first-forbidden unique transition. 19O 2cB 2006Su12 list >6.2 deduced for a non-unique transition 19O S B EAV=6024.7 85 19O L 96.4 3 3/2+ 19O G 96.4 3 47.4 13 19O L 1472.2 6 1/2+ 19O B 1.6 7 6.79 19 19O S B EAV=5283.2 85 19O G 1375.7 5 17.2 5 19O L 3235.7 11 (1/2-,3/2-) 19O B 8.1 3 5.63 2 19O S B EAV=4409.0 85 19O G 3139 1 8.1 3 19O L 3947.6 6 3/2- 19O B 41.0 10 4.76 1 19O S B EAV=4056.4 85 19O G 2475.2 7 15.6 5 19O G 3851 1 22.0 8 19O F G FL=96.4 19O G 3947 1 3.4 2 19O L 4432 4 (1/2-,3/2-) 19O cL E$ 4434 (2006Su12) 19O B 10.4 8 5.24 4 19O S B EAV=3815.6 85 19O L 6403 11 (1/2-,3/2-) 19O cL E$ 6405 (2006Su12) 19O B 4.1 1 5.07 2 19O S B EAV=2842.5 84 19O L 7050 5 (1/2-,3/2-) 19O cL E$ 7053 (2006Su12) 19O B 17.3 4 4.22 2 19O S B EAV=2522.6 92 19O L 8740 14 (1/2-,3/2-) 19O cL E$ 8743 (2006Su12) 19O B 7.6 2 3.85 2 19O cB IB$ 0.9 listed in table IV of 2006Su12 seems a misprint. 19O 2cB 6.7% listed in authors' figure 8 is increased to 7.6 19O 3cB (by compilers) by adding contribution from possible 4514 neutron 19O 4cB branch to the g.s. 19O cB LOGFT$ 4.71 listed in table IV of 2006Su12 corresponds to incorrect 19O 2cB |b feeding 19O S B EAV=1695.2 83 19O L 10573 11 (1/2-,3/2-) 19O B 1.2 1 3.39 4 19O S B EAV=818.8 80 19O 20N B-N DECAY:136MS:XUNDL-2 2006SU12 200609 19O c Compiled (unevaluated) dataset from 2006Su12: 19O 2c Phys Rev C 74, 024322 (2006). 19O c Compiled by: M. Mitchell and B. Singh (McMaster) August 30, 2006. 19O c {+20}N beam was produced from fragmentation of {+22}Ne beam at 19O 2c 80 MeV/nucleon on a {+9}Be target and separation of fragments 19O 3c using A1200 Fragment Recoil Separator at Michigan. The {+20}N 19O 4c beam were implanted in a scintilaltor, the main impurity was 19O 5c |?1.1% of {+18}C. Measured isotopic half-lives, E|g, I|g, |g|g, 19O 6c delayed neutrons, |gn coin using two HpGe detectors for |g rays and a 19O 7c neutron bar array (16 plastic scintillators) for neutrons. 19O 8c The half-lives were measured from neutron gated |g decay curves. 19O cDNIP$Total emission probability =42.9% {i14} 20N P 0.0 2- 136 MS 3 10360 60 20N cP T$ From 2006Su12 20N cP QP$ From 2003Au03 19O N 1 0.429 14 0.429 14 19O cN BR$%|b{+-}n=42.9 {I14} 19O PN 3 19O L 0 5/2+ 19O L 96.4 3 3/2+ 19O DN 1098 1 7.6 7 8860 19O DN 1254 2 5.2 5 9024 19O DN 2071 2 14.9 6 9884 19O G 96.4 3 43.9 19 19O L 1472.0 6 1/2+ 19O DN 1432 2 4.4 5 10587 19O DN 1673 4 4.3 6 10841 19O DN 3269 7 2.5 7 12521 19O DN 3683 5 4.5 5 12957 19O cDNIP$ listed as 4.0 in figure 15 of 2006Su12 19O G 1375.5 5 15.6 7 19O 18O(N,G):E=thermal:XUNDL-3 2007NA26 200711 19O c Compiled (unevaluated) dataset from 2007Na26: 19O 2c Phys Rev C 76, 051301(R) (2007) 19O c Compiled by S. Geraedts and B. Singh (McMaster): Nov 16, 2007 19O c E=thermal. Measured E|g, I|g, |g|g coin using an HPGe detector 19O 2c with Compton-suppression. Enriched target. Experiment performed using 19O 3c JRR-3 reactor at the Japan Atomic Energy Agency. 19O PN 5 19O L 0.0 5/2+ 19O L 96.0 5 3/2+ 19O G 96.0 5 198 30 19O L 1471.0 5 1/2+ 19O G 1375.0 5 100 19O L 3233.3 5 1/2- 19O G 3137.3 5 31 4 19O L 3944.0 5 3/2- 19O cL $ Interpreted as one-hole four-particle state based on strong E1 19O 2cL transition strengths. 19O G 2473.0 5 46 6 19O G 3848.0 5 66 7 19O G 3944 11 LT 19O cG $ |g not observed 19O L 3962.4 5 1/2+ S 19O G 18.4 123 10 S 19O cG $Partial capture cross section=100 |ub {I10} 19O G 729.4 5 36 5 19O cG $Partial capture cross section=32 |ub {I5} 19O G 2491.4 31 4 19O cG $Partial capture cross section=28 |ub {I4} 19O 18O(N,G):XUNDL-4 2008OH05 200805 19O c Compiled (unevaluated) dataset from 2008Oh05: 19O 2c Phys Rev C 77, 051303(R) (2008) 19O c Compiled by S. Geraedts and B. Singh (McMaster); May 29, 2008 19O c E(n)=10-80 keV neutrons produced in the reaction {+7}Li(p,n) reaction 19O 2c using the 3.2 MV Pelletron accelerator at the Tokyo Institute of 19O 3c Technology. Measured E|g, I|g, |g|g-coin using anti-Compton NaI(Tl) 19O 4c spectrometer, time-of-flight method. 19O CL S$LABEL=C{+2}S 19O PN 5 19O L 0 5/2+ 0.57 19O L 96 3/2+ 0.01 19O L 1471 1/2+ 1.0 19O L 3233 1/2- 19O L 3944 3/2- 19O G 2473 26 19O G 3850 37 19O cG $partial cross section<1.0 |mb 19O G 3944 6 LT ? 19O L 4011 S 19O cL E$S(n)+E(n), where S(n)=3959.4 {I28} (2003Au03), E(n)(lab)=52 keV 19O cL $ Total |s=9.8 |mb {I14} 19O G 2540 25 4.6 8 19O cG $Partial cross section=4.6 |mb {I8} 19O G 3920 25 3.6 9 19O cG $Partial cross section=3.6 |mb {I9} 19O F G FL=96 19O G 4010 25 1.6 8 19O cG $Partial cross section=1.6 |mb {I8} 19O F G FL=0 19O 13C(7LI,P):XUNDL-5 2010VO09 201104 19O c Compiled (unevaluated dataset from 2010Vo09 19O c Eur Phys J A 46, 345 (2010) 19O c Compiled by J. Kelley and C.G. Sheu (TUNL), January 31, 2011. 19O c The authors studied resonances in {+19}O with the aim of gaining 19O 2c insight into the rotational bands. 19O c A beam of 44 MeV {+7}Li impinged on a 96.4% enriched 100 |mg/cm{+2} 19O 2c {+13}C target at the Maier-Leibniz Laboratory in Munich. The reaction 19O 3c protons were measured in the Q3D spectrometer at |q=10|', 20|' and 39 19O 4c '; the magnetic filed setting were cycled so that 0|400 fs and E{-|g}=2370.6 keV {I+5-3} (2021Ci02). See also 19O 2cL |t>400 fs (2020Ci02,2020Ci03), |t>3.5ps (1971Hi06), T{-1/2}>2400 fs 19O 3cL in ENSDF. 19O G 2370.6 5 E2 19O cG E$2370.6 keV {I+5-3} (2021Ci02); see also E{-|g}=2371.5 keV {I10} 19O 2cG (2019Zi02), 2370.0 keV {I+5-30} (2020Ci03), 2370.6 keV {I3} (2020Ci02: 19O 3cG private communication, June 2020 indicates that 2370.6 keV {I3} was 19O 4cG deduced along with E{-|g}=2370.6 keV {I+5-3}, which was deduced 19O 5cG using the |a(M) DSAM technique). 19O L 2779.2 107/2+ 97 FS +35-28 19O 2 L FLAG=A 19O cL T$from |t=140 fs {I+50-40} and E{-|g}=2779.0 keV {I+10-8} 19O 2cL (2020Ci02,2020Ci03,2021Ci02). See also |t=117 fs {I26} (1971Hi06) and 19O 3cL 70 fs {I26} (1971Br02) which gives the average of |t=92 fs {I19}, 19O 4cL T{-1/2}=64 fs 13 in ENSDF. 19O G 2779.0 10 M1+E2 0.8 5 19O cG E$2779.0 keV {I+10-8} (2020Ci02,2020Ci03,2021Ci02); see also 19O 2cG E{-|g}=2779 keV {I1} (2019Zi02). 19O L 3066.4 6(3/2+) 19O cL T$Lifetime known to be long (private communication with M. Ciemala, 19O 2cL Aug. 2021). 19O G 1594.5 2 19O cG E$from (2020Ci02 and private communication, Aug. 2021); see also 19O 2cG E{-|g}=1596 keV (2020Ci03). 19O cG RI$weak (2020Ci02). 19O G 2969.7 5 19O cG E$from private communication with M. Ciemala, Aug. 2021; see also 19O 2cG E{-|g}=2968 keV (2020Ci03). 19O L 3153.7 75/2+ 19O G 3057.4 5 19O cG E$from (2020Ci02: private communication, June 2020); see also 19O 2cG E{-|g}=3057 keV (2021Ci02). 19O L 3231 1/2- 19O G 3135 19O cG E$see also (2020Ci02,2021Ci02). 19O L 3940.4 213/2- 19O G 3844 2 19O cG E$from private communication with M. Ciemala, Aug. 2021; see also 19O 2cG E{-|g}=3849 keV (2020Ci02, 2020Ci03, 2021Ci02). 19O cG RI$weak (2020Ci02). 19O G 3945 19O cG E$see also (2020Ci02,2021Ci02). 19O L 4988 4 19O G 4891 4 ? 19O cG E$from private communication with M. Ciemala, Aug. 2021; see also 19O 2cG E{-|g}=4894 keV (2020Ci03). There is a hint for the decay from the 19O 3cG 4990 keV neutron-unbound state (2020Ci03) as quoted in (2016Du02). 19O L 5364.9 14 19O 2 L %IT=13 2 19O G 2585.5 9 100 19O cG E$from private communication with M. Ciemala, Aug. 2021; see also 19O 2cG E{-|g}=2584 keV {I2} (2020Ci03). 19O cG RI$from (2020Ci03). 19O C(19O,19O'):XUNDL-9 2022KA35 202305 19O c Compiled (unevaluated) dataset from 2022Ka35 19O c Phys. Rev. Lett. 129, 142502 (2022) 19O c Compiled by E.A. McCutchan (NNDC,BNL) March 3, 2023 19O c {+19}O secondary beam with E=277 MeV/nucleon produced from 19O 2c fragmentation of primary {+40}Ar beam with E=1 GeV/nucleon at 19O 3c GSI. Fragments were separated with the FRS. Charge changing 19O 4c cross sections were measured with a 4.010 g/cm{+2} C target 19O 5c using the transmission technique employing the multisampling 19O 6c ionization chamber (MUSIC) and position sensitive time projection 19O 7c (TPC) detectors. Deduced root mean square proton (R{-p}) and 19O 8c and matter (R{-m}) radii. 19O L 0.0 19O cL $R{-p}=2.55 fm {I3}, R{-m}=2.71 fm {I3} (2022Ka35)