Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
2210Ne12   Neon
J(π)=0+
T1/2=stable
Abundance: 9.25% 3
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess -8.024714
(0.000018)
-8.230 4.770
BE 177.770 177.976
BE/A 8.080 8.090
<R2ch>1/2 = 2.9525 ± 0.004 fm [3]
Charge-density Distribution [6]

β2= 0.384
β3= 0.000
β4= 0.096
β6= -0.007
Excited States[1]
click on a plot to process it
Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-9666.80
β- - decay-2843.16
β+ - decay-11840.13
e-capture-10818.13
1p - decay-15266.11
2p - decay-26398.88
1n - decay-10364.24
2n - decay-17125.38
- - decay-7624.70
β-,n-13911.34
β-,2n-31017.88
β-,d-14118.45
β-,t-24726.53
β--11322.69
β-,n,α-20472.58
EC,p-23375.66
EC,2p-44367.86
EC,α-23562.82
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
 
σ (b)
Capture 0.05
Scattering 1.71
 
μ (nm) Q (b) E* (keV)
+2.2(6)3357
+0.65(2)1275
-0.19(4)1275
B(E2)↑ = 0.02298 ( 42) e2b2,    β 0  = 0.5616 (51)
2

B(E3)↑ = 0.0009 ( 3) e2b3,    β 0  = 0.331 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.