Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
8236Kr46   Krypton
J(π)=0+
T1/2=stable
Abundance: 11.593% 31
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -80.590318
(0.000877)		 -81.210 2.560
BE 714.274 714.894
BE/A 8.711 8.718
<R2ch>1/2 = 4.1919 ± 0.0025 fm [3]
Charge-density Distribution [6]

β2= 0.129
β3= 0.000
β4= -0.031
β6= 0.006
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-5989.31
β- - decay-4402.48
β+ - decay-4115.08
e-capture-3093.08
1p - decay-9903.67
2p - decay-17408.84
1n - decay-10966.80
2n - decay-18839.61
2β- - decay-4580.20
β-,n-13204.92
β-,2n-24557.42
β-,d-15832.67
β-,t-21097.81
β-,α-9563.06
β-,n,α-17851.68
EC,p-11490.35
EC,2p-22953.89
EC,α-10198.29
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
  
σ (b)
Capture 28.00
 
μ (nm) Q (b) E* (keV)
+1.2(8)1821
+0.80(4)777
B(E2)↑ = 0.2251 ( +67) e2b2,    β 0  = 0.2031 ( +30)
 -612 -28

B(E3)↑ = 0.06 ( 2) e2b3,    β 0  = 0.201 (0)
3

  
[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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.