Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
179F8   Fluorine
J(π)=5/2+
T1/2=1.07 m
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess 1.951701
(0.000248)		 0.950 3.140
BE 128.220 129.221
BE/A 7.542 7.601
<R2ch>1/2 = 
Charge-density Distribution [6]

β2= 0.061
β3= 0.000
β4= 0.152
β6= 0.035
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-5818.68
β- - decay-14548.71
β+ - decay1738.43
e-capture2760.43
1p - decay-600.30
2p - decay-12727.74
1n - decay-16799.85
2n - decay-30997.71
2β- - decay 
β-,n-30105.72
β-,2n 
β-,d-27990.77
β-,t-44962.47
β-,α-23588.60
β-,n,α-40459.16
EC,p-11021.24
EC,2p-22499.48
EC,α-3598.24
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 3104 keV
T1/2 = 0.019 MeV
IT
0.000063%		p
100%
E = 3857 keV
T1/2 = 0.001 MeV
IT
0.0073%		p
100%
E = 4640 keV
T1/2 = 0.225 MeV
p
100%
E = 5000 keV
T1/2 = 1.530 MeV
p
100%
E = 5488 keV
T1/2 = 0.068 MeV
p
100%
E = 5672 keV
T1/2 = 0.040 MeV
p
100%
E = 5682 keV
T1/2 = 0.001 MeV
p
100%
E = 5820 keV
T1/2 = 0.180 MeV
p
100%
E = 6037 keV
T1/2 = 0.030 MeV
p
100%
E = 6560 keV
T1/2 = 0.200 MeV
p
100%
E = 6697 keV
T1/2 = 0.002 MeV
p
100%
E = 6774 keV
T1/2 = 0.005 MeV
p
100%
E = 7027 keV
T1/2 = 0.004 MeV
p
100%
E = 7448 keV
T1/2 = 0.005 MeV
p
100%
E = 7471 keV
T1/2 = 0.005 MeV
p
100%
E = 7479 keV
T1/2 = 0.795 MeV
p
100%
E = 7546 keV
T1/2 = 0.030 MeV
p
100%
E = 7950 keV
T1/2 = 0.010 MeV
p
100%
E = 8075 keV
T1/2 = -1
p
100%
E = 8436 keV
T1/2 = -1
p
100%
E = 8760 keV
T1/2 = 0.090 MeV
p
100%
E = 8825 keV
T1/2 = -1
p
100%
E = 9450 keV
T1/2 = 0.200 MeV
p
100%
E = 10030 keV
T1/2 = 0.170 MeV
p
100%
E = 10040 keV
T1/2 = 0.280 MeV
p
100%
E = 10220 keV
T1/2 = 0.250 MeV
α
100%
E = 10400 keV
T1/2 = 0.160 MeV
p
100%
E = 10660 keV
T1/2 = 0.090 MeV
p
100%
E = 10910 keV
T1/2 = 0.560 MeV
p
100%
E = 11192.9 keV
T1/2 = 0.003 fs
IT
3.3%
E = 11580 keV
T1/2 = 0.160 MeV
p
100%
E = 12250 keV
T1/2 = 0.300 MeV
p
100%
E = 12355 keV
T1/2 = 0.190 MeV
p
100%
E = 12500 keV
T1/2 = 0.600 MeV
p
100%
E = 13130 keV
T1/2 = 0.520 MeV
p
100%
E = 14000 keV
T1/2 = 0.260 MeV
p
100%
E = 14380 keV
T1/2 = 0.610 MeV
p
100%
E = 14710 keV
T1/2 = 0.470 MeV
p
100%
E = 14809 keV
T1/2 = 0.190 MeV
p
100%
E = 15600 keV
T1/2 = 0.550 MeV
p
100%
E = 17100 keV
T1/2 = 1.500 MeV
p
100%
E = 20900 keV
T1/2 = 0.600 MeV
p
100%
E = 21800 keV
T1/2 = 0.400 MeV
p
100%
E = 22700 keV
T1/2 = 0.600 MeV
p
100%
E = 23800 keV
T1/2 = 0.600 MeV
p
100%
E = 25400 keV
T1/2 = 1.500 MeV
p
100%
E = 27200 keV
T1/2 = 1.500 MeV
p
100%
E = 28900 keV
T1/2 = 2.000 MeV
p
100%
β+ endpoint energies
 
μ (nm) Q (b) E* (keV)
+4.7223(12)0
+4.7213(3)0
0.076(4)0
  
[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.