Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
158O7   Oxygen
J(π)=1/2-
T1/2=2.04 m
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess 2.855605
(0.000491)
   
BE 111.955  
BE/A 7.464  
<R2ch>1/2 = 
Charge-density Distribution [6]

β2=
β3=
β4=
β6=
Excited States[1]
click on a plot to process it
Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-10219.59
β- - decay-13951.17
β+ - decay1732.13
e-capture2754.13
1p - decay-7296.81
2p - decay-14847.40
1n - decay-13223.15
2n - decay-36402.43
- - decay 
β-,n-37180.07
β-,2n 
β-,d-33395.50
β-,t-44008.86
β--23872.90
β-,n,α-46440.67
EC,p-7453.32
EC,2p-28284.55
EC,α-8237.21
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 7556.5 keV
T1/2 = 0.001 MeV
IT
0.0042%
p
99.9958%
E = 8284 keV
T1/2 = 0.004 MeV
IT
0.027%
p
99.973%
E = 8743 keV
T1/2 = 0.032 MeV
IT
0.0015%
p
99.9985%
E = 8922 keV
T1/2 = 0.008 MeV
p
100%
E = 8922 keV
T1/2 = 0.003 MeV
p
100%
E = 8982.1 keV
T1/2 = 0.004 MeV
p
100%
E = 9484 keV
T1/2 = 0.200 MeV
IT
0.0046%
p
100%
E = 9488 keV
T1/2 = 0.010 MeV
IT
0.024%
p
99.976%
E = 9609 keV
T1/2 = 0.009 MeV
IT
0.057%
p
99.943%
E = 9662 keV
T1/2 = 0.002 MeV
p
100%
E = 10290 keV
T1/2 = 0.003 MeV
p
100%
E = 10300 keV
T1/2 = 0.011 MeV
p
100%
E = 10480 keV
T1/2 = 0.025 MeV
IT
0.0014%
p
100%
E = 10506 keV
T1/2 = 0.140 MeV
p
100%
E = 10917 keV
T1/2 = 0.090 MeV
p
100%
E = 10938 keV
T1/2 = 0.099 MeV
IT
0.032%
p
100%
E = 11025 keV
T1/2 = 0.025 MeV
IT
0.0056%
p
100%
E = 11151 keV
T1/2 = 0.010 MeV
p
100%
E = 11218 keV
T1/2 = 0.040 MeV
IT
0.0185%
p
99.9815%
E = 11565 keV
T1/2 = 0.010 MeV
p
100%
E = 11569 keV
T1/2 = 0.020 MeV
IT
0.01%
p
99.99%
E = 11616 keV
T1/2 = 0.080 MeV
p
100%
E = 11719 keV
T1/2 = 0.010 MeV
p
100%
E = 11748 keV
T1/2 = 0.099 MeV
IT
0.01%
p
99.99%
E = 11846 keV
T1/2 = 0.065 MeV
IT
0.0022%
p
99.9978%
E = 11980 keV
T1/2 = 0.020 MeV
p
100%
E = 12129 keV
T1/2 = 0.200 MeV
p
100%
E = 12222 keV
T1/2 = 0.100 MeV
p
100%
E = 12255 keV
T1/2 = 0.135 MeV
p
100%
E = 12471 keV
T1/2 = 0.077 MeV
p
100%
E = 12800 keV
T1/2 = 0.250 MeV
p
100%
E = 12835 keV
T1/2 = 0.016 MeV
p
100%
E = 13008 keV
T1/2 = 0.215 MeV
p
100%
E = 13700 keV
T1/2 = -1
p
100%
E = 13870 keV
T1/2 = 0.150 MeV
p
100%
E = 15100 keV
T1/2 = 1.000 MeV
p
100%
β+ endpoint energies
 
μ (nm) Q (b) E* (keV)
<0.3(2)5241
+0.65(7)5241
0.7189(8)0
0.71951(12)c0
  
[1] National Nuclear Data Center, Evaluated Nuclear Structure Data File, https://www.nndc.bnl.gov/ensdf/.
[2] M. Wang, G. Audi, A.H. Wapstra, F.G. Kondev, M. MacCormick, X. Xu, and B. Pfeiffer, Chinese Physics C, 2012, vol. 36, pp. 1603-2014.
[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.
[4] P. Möller, A.J. Sierk, T. Ichikawa, H. Sagawa, Atomic Data and Nuclear Data Tables, 2016, vol. 109-110, pp. 1-204.
[5] N.J. Stone, https://www-nds.iaea.org/publications/indc/indc-nds-0658/; Atomic Data and Nuclear Data Tables, 2016, vol. 111-112, pp. 1–28.
[6] H. de Vries, C.W. de Jager, C. de Vries, Atomic Data and Nuclear Data Tables, 1987, vol. 36, pp. 495-536.
[7] B. Pritychenko, M. Birch, B. Singh, M. Horoi, Atomic Data and Nuclear Data Tables, 2016, vol. 107, pp. 1–139; 2017, vol. 114, pp. 371–374.
[8] T. Kibedi and R.H. Spear, Atomic Data and Nuclear Data Tables, 2002, vol. 80, pp. 35-82.