Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
13050Sn80   Tin
J(π)=0+
T1/2=3.72 m
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -80.132861
(0.002126)		 -80.150 -8.840
BE 1090.287 1090.304
BE/A 8.387 8.387
<R2ch>1/2 = 4.7019 ± 0.0066 fm [3]
Charge-density Distribution [6]

β2= 0.011
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-10300.96
β- - decay2153.44
β+ - decay-11271.04
e-capture-10249.04
1p - decay-14583.97
2p - decay-27468.97
1n - decay-7597.06
2n - decay-12913.44
2β- - decay7220.16
β-,n-3574.79
β-,2n-11645.12
β-,d-9906.50
β-,t-11611.40
β-,α-4784.80
β-,n,α-10152.19
EC,p-23912.90
EC,2p-39808.90
EC,α-21777.80
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 1946.88 keV
T1/2 = 1.70 m
β-
100%
β- endpoint energies
γ-energies
 
μ (nm) Q (b) E* (keV)
-0.381(3)1947
-0.39(12)1947
B(E2)↑ = 0.023 ( 5) e2b2,    β 0  = 0.0344 (37)
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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.