Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
11750Sn67   Tin
J(π)=1/2+
T1/2=stable
Abundance: 7.68% 7
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess -90.397782
(0.000483)
-90.240 1.090
BE 995.625 995.467
BE/A 8.510 8.508
<R2ch>1/2 = 4.6302 ± 0.0019 fm [3]
Charge-density Distribution [6]

β2= -0.073
β3= 0.000
β4= 0.002
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-3779.43
β- - decay-1758.18
β+ - decay-2476.74
e-capture-1454.74
1p - decay-9437.04
2p - decay-16891.39
1n - decay-6943.09
2n - decay-16506.55
- - decay-5302.29
β-,n-11647.39
β-,2n-19536.94
β-,d-13499.61
β-,t-14790.21
β--3456.83
β-,n,α-12902.88
EC,p-8974.26
EC,2p-19993.16
EC,α-5795.93
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 314.58 keV
T1/2 = 14.00 d
IT
100%
γ-energies
σ (b)
Capture 2.30
 
μ (nm) Q (b) E* (keV)
-1.3955(10)315
+0.66(5)159
-1.00104(7)0
-0.42(5)315
  
[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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.