Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
5826Fe32   Iron
J(π)=0+
T1/2=stable
Abundance: 0.282% 4
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -62.154467
(0.000492)		 -61.780 1.330
BE 509.950 509.576
BE/A 8.792 8.786
<R2ch>1/2 = 3.7745 ± 0.0014 fm [3]
Charge-density Distribution [6]

β2= 0.173
β3= 0.000
β4= -0.013
β6= -0.003
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-7645.67
β- - decay-2307.87
β+ - decay-7348.94
e-capture-6326.94
1p - decay-11957.34
2p - decay-21451.22
1n - decay-10044.59
2n - decay-17690.65
2β- - decay-1926.24
β-,n-10880.78
β-,2n-22257.23
β-,d-14683.71
β-,t-19623.59
β-,α-9022.81
β-,n,α-17961.59
EC,p-16919.36
EC,2p-30609.40
EC,α-14687.30
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
  
σ (b)
Capture 1.28
 
μ (nm) Q (b) E* (keV)
+0.9(2)811
+0.9(3)811
+0.94(5)811
-0.27(5)811
B(E2)↑ = 0.122 ( 6) e2b2,    β 0  = 0.27 (7)
2

B(E3)↑ = 0.0139 ( 13) e2b3,    β 0  = 0.19 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.