Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
12250Sn72   Tin
J(π)=0+
T1/2=stable
Abundance: 4.63% 3
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess -89.941545
(0.0024)
-90.050 -0.930
BE 1035.525 1035.634
BE/A 8.488 8.489
<R2ch>1/2 = 4.6634 ± 0.0022 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-5664.73
β- - decay-1607.89
β+ - decay-7390.63
e-capture-6368.63
1p - decay-11394.36
2p - decay-20562.19
1n - decay-8815.36
2n - decay-14985.55
- - decay372.97
β-,n-8414.23
β-,2n-17666.13
β-,d-11978.62
β-,t-14826.25
β--5138.16
β-,n,α-11494.64
EC,p-16156.76
EC,2p-28868.08
EC,α-12812.69
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
 
σ (b)
Capture 0.18
 
μ (nm) Q (b) E* (keV)
-0.7(7)2142
-0.1(2)1140
-0.09(4)1140
-0.13(10)1140
B(E2)↑ = 0.1887 ( 45) e2b2,    β 0  = 0.1027 (13)
2

B(E3)↑ = 0.092 ( 10) e2b3,    β 0  = 0.121 (0)
3

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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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