Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
17271Lu101   Lutetium
J(π)=4-
T1/2=6.70 d
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -56.738135
(0.002771)		 -56.880 -0.310
BE 1389.458 1389.600
BE/A 8.078 8.079
<R2ch>1/2 = 5.3486 ± 0.0302 fm [3]
Charge-density Distribution [6]

β2= 0.287
β3= 0.000
β4= -0.030
β6= -0.022
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay2150.31
β- - decay-335.87
β+ - decay1496.01
e-capture2518.01
1p - decay-4719.11
2p - decay-11519.84
1n - decay-6979.46
2n - decay-15573.70
2β- - decay-5408.09
β-,n-9378.05
β-,2n-16626.85
β-,d-12566.77
β-,t-13603.80
β-,α2418.44
β-,n,α-6643.40
EC,p-4815.70
EC,2p-11207.08
EC,α3827.64
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 41.86 keV
T1/2 = 3.70 m
IT
100%
E = 109.41 keV
T1/2 = 440.00 µs
IT
100%
β+ endpoint energies
γ-energies
 
μ (nm) Q (b) E* (keV)
+0.76(3)42
+3.80(4)0
+2.900(10)0
2.893(15)0
2.25(10)0
+1.98(4)42
  
[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[3] I. Angeli, K.P. Marinova, Atomic Data and Nuclear Data Tables, 2013, vol. 99, pp. 69-95; unpublished update, 2016.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.