Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
11950Sn69   Tin
J(π)=1/2+
T1/2=stable
Abundance: 8.59% 4
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -90.065063
(0.000726)		 -90.120 0.640
BE 1011.435 1011.490
BE/A 8.499 8.500
<R2ch>1/2 = 4.6438 ± 0.002 fm [3]
Charge-density Distribution [6]

β2= -0.105
β3= 0.000
β4= -0.008
β6= 0.001
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-4405.57
β- - decay-590.81
β+ - decay-3387.60
e-capture-2365.60
1p - decay-10125.81
2p - decay-18224.60
1n - decay-6483.48
2n - decay-15809.88
2β- - decay-2883.78
β-,n-10140.08
β-,2n-17568.06
β-,d-12802.95
β-,t-13488.83
β-,α-2953.58
β-,n,α-11992.83
EC,p-10652.38
EC,2p-22461.05
EC,α-7507.34
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 89.531 keV
T1/2 = 293.10 d
IT
100%
γ-energies
σ (b)
Capture 2.20
 
μ (nm) Q (b) E* (keV)
-1.40(8)90
+0.682(3)24
+0.633(3)24
-1.04728(7)0
-0.29(3)90
-0.132(1)24
  
[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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.