Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
8840Zr48   Zirkonium
J(π)=0+
T1/2=83.40 d
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -83.628329
(0.005444)		 -84.760 0.100
BE 762.611 763.742
BE/A 8.666 8.679
<R2ch>1/2 = 4.2787 ± 0.0025 fm [3]
Charge-density Distribution [6]

β2= -0.011
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-5403.67
β- - decay-7452.31
β+ - decay-351.61
e-capture670.39
1p - decay-7898.99
2p - decay-13683.13
1n - decay-12353.10
2n - decay-21802.28
2β- - decay-10941.72
β-,n-17826.30
β-,2n-30638.02
β-,d-18795.34
β-,t-25404.07
β-,α-12159.72
β-,n,α-21919.97
EC,p-6037.33
EC,2p-15459.35
EC,α-6294.30
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 2887.79 keV
T1/2 = 1.32 µs
IT
100%
γ-energies
 
μ (nm) Q (b) E* (keV)
-1.60(16)2889
-1.81(2)2889
+2.6(7)2140
+0.6(2)1057
+0.44(3)2889
B(E2)↑ = 0.086 ( +11) e2b2,    β 0  = 0.1077 ( +67)
 -92 -54

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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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