Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
13154Xe77   Xenon
J(π)=3/2+
T1/2=stable
Abundance: 21.2324% 30
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -88.413631
(0.00022)		 -88.040 -1.080
BE 1103.510 1103.136
BE/A 8.424 8.421
<R2ch>1/2 = 4.7808 ± 0.0049 fm [3]
Charge-density Distribution [6]

β2= -0.125
β3= 0.000
β4= -0.029
β6= -0.005
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-2556.87
β- - decay-354.72
β+ - decay-1992.88
e-capture-970.88
1p - decay-8766.48
2p - decay-15986.79
1n - decay-6604.47
2n - decay-15860.17
2β- - decay-1729.64
β-,n-9585.15
β-,2n-17056.94
β-,d-12853.24
β-,t-13503.12
β-,α-1854.60
β-,n,α-10998.49
EC,p-8349.72
EC,2p-18362.33
EC,α-4139.09
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 163.93 keV
T1/2 = 11.84 d
IT
100%
γ-energies
σ (b)
Capture 85.00
 
μ (nm) Q (b) E* (keV)
-0.994048(6)164
0.9940(5)164
-0.994(2)d164
+0.691862(4)0
+0.6915(2)d0
+0.72(3)164
-0.114(1)0
  
[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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.