Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
12850Sn78   Tin
J(π)=0+
T1/2=59.07 m
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -83.362021
(0.01766)		 -83.410 -6.340
BE 1077.373 1077.421
BE/A 8.417 8.417
<R2ch>1/2 = 4.6921 ± 0.0054 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-9085.25
β- - decay1268.32
β+ - decay-10238.11
e-capture-9216.11
1p - decay-13752.72
2p - decay-25683.22
1n - decay-7962.09
2n - decay-13489.33
2β- - decay5631.79
β-,n-4733.81
β-,2n-13111.30
β-,d-10482.40
β-,t-12415.37
β-,α-4916.67
β-,n,α-10427.73
EC,p-22160.54
EC,2p-37160.06
EC,α-19586.82
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 2091.5 keV
T1/2 = 6.50 s
IT
100%
β- endpoint energies
γ-energies
 
μ (nm) Q (b) E* (keV)
-2.0(4)2492
(-)0.46(12)1169
-0.1(3)2492
B(E2)↑ = 0.0771 ( 38) e2b2,    β 0  = 0.0636 (16)
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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.