Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
199F10   Fluorine
J(π)=1/2+
T1/2=stable
Abundance: 100% 0
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -1.48744434
(0.00000086)		 -2.190 5.870
BE 147.801 148.504
BE/A 7.779 7.816
<R2ch>1/2 = 2.8976 ± 0.0025 fm [3]
Charge-density Distribution [6]

β2= 0.262
β3= 0.000
β4= 0.180
β6= 0.025
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-4013.78
β- - decay-3239.46
β+ - decay-5842.34
e-capture-4820.34
1p - decay-7993.63
2p - decay-23935.52
1n - decay-10431.86
2n - decay-19581.75
2β- - decay-14416.77
β-,n-14876.33
β-,2n-34130.46
β-,d-16574.81
β-,t-27117.46
β-,α-6767.91
β-,n,α-19991.07
EC,p-21889.65
EC,2p-37096.26
EC,α-13785.52
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 6255 keV
T1/2 = 0.008 MeV
α
100%
E = 6429 keV
T1/2 = 0.280 MeV
α
100%
E = 6989 keV
T1/2 = 0.051 MeV
α
100%
E = 7114 keV
T1/2 = 0.032 MeV
α
100%
E = 7262 keV
T1/2 = 0.006 MeV
α
100%
E = 7364 keV
T1/2 = -1
α
100%
E = 7560 keV
T1/2 = 0.090 MeV
α
100%
E = 7702 keV
T1/2 = 0.030 MeV
α
100%
E = 7900 keV
T1/2 = 0.200 MeV
α
100%
E = 8014 keV
T1/2 = -1
p
100%
E = 8160 keV
T1/2 = 0.050 MeV
α
100%
E = 11350 keV
T1/2 = 0.272 MeV
p
100%
E = 12522 keV
T1/2 = 0.015 MeV
p
100%
E = 12580 keV
T1/2 = 0.285 MeV
p
100%
E = 12860 keV
T1/2 = 0.276 MeV
p
100%
E = 12980 keV
T1/2 = 0.124 MeV
p
100%
E = 13090 keV
T1/2 = 0.285 MeV
p
100%
E = 13360 keV
T1/2 = 0.038 MeV
p
100%
E = 14040 keV
T1/2 = 0.141 MeV
p
100%
E = 14100 keV
T1/2 = 0.084 MeV
p
100%
E = 14330 keV
T1/2 = 0.076 MeV
p
100%
E = 14700 keV
T1/2 = 0.124 MeV
p
100%
E = 14720 keV
T1/2 = 0.257 MeV
α
100%
E = 14920 keV
T1/2 = -1
p
100%
E = 15360 keV
T1/2 = -1
p
100%
E = 15400 keV
T1/2 = -1
p
100%
E = 16200 keV
T1/2 = -1
p
100%
E = 16230 keV
T1/2 = -1
p
100%
E = 17050 keV
T1/2 = 0.331 MeV
p
100%
E = 17160 keV
T1/2 = 0.323 MeV
p
100%
E = 17450 keV
T1/2 = 0.032 MeV
p
100%
E = 17650 keV
T1/2 = 0.095 MeV
p
100%
E = 17930 keV
T1/2 = 0.255 MeV
p
100%
E = 18030 keV
T1/2 = 0.365 MeV
p
100%
E = 19070 keV
T1/2 = 0.560 MeV
p
100%
E = 19830 keV
T1/2 = 0.369 MeV
p
100%
E = 19890 keV
T1/2 = 0.473 MeV
p
100%
E = 20810 keV
T1/2 = 0.412 MeV
p
100%
E = 20930 keV
T1/2 = 0.317 MeV
p
100%
E = 21050 keV
T1/2 = 0.448 MeV
p
100%
  
σ (b)
Capture 0.01
Scattering 3.64
 
μ (nm) Q (b) E* (keV)
0.67(11)1346
3.595(13)197
+3.607(8)197
+2.628868(8)0
-0.0942(9)197
  
[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.