Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
23692U144   Uranium
J(π)=0+
T1/2=2.34e+7 y
  Experiment
[2]
Theory
[4]
Sh.corr.
[4]
Mass Excess 42.446515
(0.001792)
42.630 -1.240
BE 1790.409 1790.225
BE/A 7.586 7.586
<R2ch>1/2 = 5.8431 ± 0.0038 fm [3]
Charge-density Distribution [6]

β2= 0.226
β3= 0.000
β4= 0.108
β6= -0.009
Excited States[1]
click on a plot to process it
Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay4572.90
β- - decay-932.89
β+ - decay-3909.47
e-capture-2887.47
1p - decay-7131.38
2p - decay-12745.93
1n - decay-6545.44
2n - decay-11842.91
- - decay-456.27
β-,n-6669.62
β-,2n-13652.72
β-,d-8835.98
β-,t-9423.50
β-4073.68
β-,n,α-1475.61
EC,p-8860.27
EC,2p-16972.71
EC,α867.16
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 2750 keV
T1/2 = 120.00 ns
SF
13%
IT
87%
α
10%
α-energies
γ-energies
σ (b)
Capture 5.11
Fission 0.07
Total 18.70

νn= 2.34
 
B(E2)↑ = 10.96 ( 28) e2b2,    β 0  = 0.2741 (35)
2

B(E3)↑ = 0.53 ( 7) e2b3,    β 0  = 0.081 (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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.