Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
13054Xe76   Xenon
J(π)=0+
T1/2=stable
Abundance: 4.071% 13
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -89.880462
(0.000009)		 -89.140 -0.090
BE 1096.905 1096.165
BE/A 8.438 8.432
<R2ch>1/2 = 4.7818 ± 0.0049 fm [3]
Charge-density Distribution [6]

β2= -0.125
β3= 0.000
β4= -0.018
β6= -0.007
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-2240.03
β- - decay-2980.68
β+ - decay-3966.34
e-capture-2944.34
1p - decay-8662.32
2p - decay-15464.72
1n - decay-9255.71
2n - decay-16162.78
2β- - decay-2618.66
β-,n-10452.47
β-,2n-20091.46
β-,d-13155.85
β-,t-16508.68
β-,α-4394.02
β-,n,α-11539.44
EC,p-10164.66
EC,2p-19828.20
EC,α-5912.11
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
  
σ (b)
Capture 26.00
 
μ (nm) Q (b) E* (keV)
-1.6(2)2972
-2.05(14)2972
+1.7(2)1205
+0.9(2)1122
+0.62(8)538
+0.76(14)538
+0.67(2)538
B(E2)↑ = 0.634 ( 29) e2b2,    β 0  = 0.1671 (39)
2

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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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