Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
9640Zr56   Zirkonium
J(π)=0+
T1/2=2.00e+19 y
Abundance: 2.8% 9
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -85.44461
(0.001995)		 -83.910 3.380
BE 828.997 827.463
BE/A 8.635 8.619
<R2ch>1/2 = 4.3512 ± 0.0015 fm [3]
Charge-density Distribution [6]

β2= 0.240
β3= 0.000
β4= 0.011
β6= -0.021
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-5002.12
β- - decay162.25
β+ - decay-8125.05
e-capture-7103.05
1p - decay-11522.29
2p - decay-21176.86
1n - decay-7854.35
2n - decay-14316.31
2β- - decay3349.09
β-,n-6730.82
β-,2n-15217.97
β-,d-11309.37
β-,t-13271.69
β-,α-3052.42
β-,n,α-9588.90
EC,p-17611.39
EC,2p-31459.86
EC,α-13097.02
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
  
σ (b)
Capture 0.02
Scattering 6.60
 
μ (nm) Q (b) E* (keV)
+2.9(5)1897
+0.06(14)1750
B(E2)↑ = 0.0314 ( 33) e2b2,    β 0  = 0.0615 (33)
2

B(E3)↑ = 0.202 ( 20) e2b3,    β 0  = 0.284 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.