Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
8838Sr50   Strontium
J(π)=0+
T1/2=stable
Abundance: 82.58% 1
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess -87.921351
(0.001085)
-87.890 -1.160
BE 768.468 768.437
BE/A 8.733 8.732
<R2ch>1/2 = 4.224 ± 0.0018 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-7906.92
β- - decay-3622.56
β+ - decay-6334.39
e-capture-5312.39
1p - decay-10612.56
2p - decay-19233.69
1n - decay-11112.62
2n - decay-19540.75
- - decay-4292.95
β-,n-12974.27
β-,2n-24780.72
β-,d-16533.82
β-,t-21767.84
β--10587.26
β-,n,α-19346.89
EC,p-14500.86
EC,2p-26867.14
EC,α-12563.20
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
 
σ (b)
Capture 0.06
 
μ (nm) Q (b) E* (keV)
+2.3(3)1836
+2.4(2)1836
B(E2)↑ = 0.0903 ( +32) e2b2,    β 0  = 0.1163 ( +20)
 -232 -15

B(E3)↑ = 0.073 ( 3) e2b3,    β 0  = 0.196 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.