Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
8636Kr50   Krypton
J(π)=0+
T1/2=stable
Abundance: 17.279% 41
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -83.26566488
(0.00000379)		 -83.430 -0.750
BE 749.235 749.399
BE/A 8.712 8.714
<R2ch>1/2 = 4.1835 ± 0.0021 fm [3]
Charge-density Distribution [6]

β2= 0.000
β3= 0.000
β4= 0.000
β6= 0.000
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-8096.65
β- - decay-518.62
β+ - decay-8655.45
e-capture-7633.45
1p - decay-11979.20
2p - decay-21895.94
1n - decay-9856.63
2n - decay-16968.93
2β- - decay1257.60
β-,n-9169.60
β-,2n-19649.27
β-,d-13961.99
β-,t-18225.40
β-,α-8193.25
β-,n,α-15786.18
EC,p-18141.06
EC,2p-31990.14
EC,α-15587.51
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
  
σ (b)
Capture 0.00
 
μ (nm) Q (b) E* (keV)
+2.2(3)1565
B(E2)↑ = 0.1056 ( 95) e2b2,    β 0  = 0.1347 (60)
2

B(E3)↑ = 0.036 ( 12) e2b3,    β 0  = 0.149 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.