Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
17070Yb100   Ytterbium
J(π)=0+
T1/2=stable
Abundance: 2.982% 39
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -60.764729
(0.002059)		 -61.000 -0.100
BE 1378.125 1378.360
BE/A 8.107 8.108
<R2ch>1/2 = 5.2853 ± 0.0056 fm [3]
Charge-density Distribution [6]

β2= 0.287
β3= 0.000
β4= -0.018
β6= -0.019
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay1735.94
β- - decay-3457.66
β+ - decay-1990.47
e-capture-968.47
1p - decay-6778.09
2p - decay-12352.02
1n - decay-8458.93
2n - decay-15325.89
2β- - decay-4510.80
β-,n-10751.89
β-,2n-19839.91
β-,d-12318.95
β-,t-15123.59
β-,α-1301.69
β-,n,α-8332.08
EC,p-7131.12
EC,2p-15282.06
EC,α-119.07
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
  
σ (b)
Capture 11.40
Scattering 5.85
 
μ (nm) Q (b) E* (keV)
-2.18(3)84
+0.674(8)84
B(E2)↑ = 5.721 ( 70) e2b2,    β 0  = 0.3239 (20)
2

B(E3)↑ = 0.11 ( 4) e2b3,    β 0  = 0.068 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.