Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
19081Tl109   Thallium
J(π)=
T1/2=2.60 m
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -24.379
(0.05)		 -24.670 -0.870
BE 1494.560 1494.851
BE/A 7.866 7.868
<R2ch>1/2 = 5.4121 ± 0.0056 fm [3]
Charge-density Distribution [6]

β2= -0.094
β3= 0.000
β4= -0.008
β6= 0.001
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay4910.95
β- - decay-3962.48
β+ - decay5969.14
e-capture6991.14
1p - decay-2041.77
2p - decay-6680.17
1n - decay-7848.12
2n - decay-18185.20
2β- - decay-13779.98
β-,n-14572.10
β-,2n-22706.57
β-,d-15178.26
β-,t-16885.67
β-,α1734.99
β-,n,α-8699.61
EC,p1913.92
EC,2p-1128.03
EC,α11060.54
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 0+x keV
T1/2 = 3.70 m
β+, EC
100%
E = 161.9 keV
T1/2 = 750.00 µs
IT
100%
β+ endpoint energies
γ-energies
 
μ (nm) Q (b) E* (keV)
+0.285(14)0+y
-0.329(9)0+x
+0.254(2)0+x
+0.487(8)0+y
+0.495(4)0+y
  
[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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.