Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
9240Zr52   Zirkonium
J(π)=0+
T1/2=stable
Abundance: 17.15% 8
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess -88.45963
(0.001828)
-88.690 0.120
BE 799.727 799.958
BE/A 8.693 8.695
<R2ch>1/2 = 4.3057 ± 0.0013 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-2963.18
β- - decay-2005.85
β+ - decay-4664.61
e-capture-3642.61
1p - decay-9396.75
2p - decay-17088.71
1n - decay-8634.77
2n - decay-15828.67
- - decay-1651.73
β-,n-9892.32
β-,2n-21939.97
β-,d-12821.74
β-,t-18533.01
β--6585.74
β-,n,α-15937.45
EC,p-12096.26
EC,2p-23672.94
EC,α-8275.57
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
 
σ (b)
Capture 0.22
 
μ (nm) Q (b) E* (keV)
1.5(10)1847
-2.0(4)1495
-0.06(10)934
-0.36(2)934
-0.36(4)934
B(E2)↑ = 0.08 ( 39) e2b2,    β 0  = 0.1009 (24)
2

B(E3)↑ = 0.07 ( 2) e2b3,    β 0  = 0.174 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.