Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
209F11   Fluorine
J(π)=2+
T1/2=11.07 s
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess -0.017463
(0.00003)		 0.200 6.250
BE 154.403 154.185
BE/A 7.720 7.709
<R2ch>1/2 = 
Charge-density Distribution [6]

β2= 0.283
β3= 0.000
β4= 0.159
β6= 0.021
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-8126.27
β- - decay7024.50
β+ - decay-4835.67
e-capture-3813.67
1p - decay-10639.32
2p - decay-27708.63
1n - decay-6601.32
2n - decay-17033.18
2β- - decay-6868.00
β-,n-9840.78
β-,2n-21477.65
β-,d-14026.24
β-,t-16918.93
β-,α2294.67
β-,n,α-13369.23
EC,p-23162.02
EC,2p-39513.62
EC,α-16136.53
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 6627 keV
T1/2 = 0.001 fs
IT
0.45%		n
99.55%
E = 6647.5 keV
T1/2 = 0.002 MeV
IT
0.101%		n
99.899%
E = 6693.4 keV
T1/2 = 0.014 MeV
n
100%
E = 6825 keV
T1/2 = -1
n
100%
E = 6856.7 keV
T1/2 = 0.010 MeV
IT
0.035%		n
99.965%
E = 6967.8 keV
T1/2 = 0.005 MeV
IT
0.048%		n
99.952%
E = 7080 keV
T1/2 = 0.024 MeV
n
100%
E = 7166 keV
T1/2 = 0.008 MeV
IT
0.079%		n
99.921%
E = 7319 keV
T1/2 = 0.033 MeV
IT
0.009%		n
100%
E = 7370 keV
T1/2 = 0.019 MeV
n
100%
E = 7420 keV
T1/2 = 0.010 MeV
n
100%
E = 7495 keV
T1/2 = 0.080 MeV
IT
0.0035%		n
100%
E = 7655 keV
T1/2 = 0.065 MeV
IT
0.006%		n
100%
E = 7734 keV
T1/2 = 0.140 MeV
n
100%
E = 7843 keV
T1/2 = 0.050 MeV
n
100%
E = 7985 keV
T1/2 = 0.014 MeV
n
100%
E = 8113 keV
T1/2 = 0.195 MeV
IT
0.006%		n
100%
E = 8147 keV
T1/2 = 0.015 MeV
n
100%
E = 8421 keV
T1/2 = 0.027 MeV
n
100%
E = 8500 keV
T1/2 = 0.140 MeV
n
100%
E = 8720 keV
T1/2 = 0.030 MeV
n
100%
E = 8770 keV
T1/2 = 0.076 MeV
n
100%
E = 8940 keV
T1/2 = 0.073 MeV
n
100%
E = 9200 keV
T1/2 = -1
n
100%
E = 9520 keV
T1/2 = 0.110 MeV
n
100%
E = 9650 keV
T1/2 = 0.100 MeV
n
100%
E = 9830 keV
T1/2 = 0.033 MeV
n
100%
E = 9850 keV
T1/2 = 0.120 MeV
n
100%
E = 9886 keV
T1/2 = -1
n
100%
E = 9900 keV
T1/2 = 0.030 MeV
n
100%
E = 9929 keV
T1/2 = -1
n
100%
E = 9981 keV
T1/2 = -1
n
100%
E = 10641 keV
T1/2 = 0.070 MeV
n
100%
E = 10990 keV
T1/2 = 0.190 MeV
n
100%
E = 11045 keV
T1/2 = 0.030 MeV
n
100%
E = 11130 keV
T1/2 = 0.025 MeV
n
100%
E = 11244 keV
T1/2 = 0.025 MeV
n
100%
E = 11287 keV
T1/2 = -1
n
100%
β- endpoint energies
γ-energies
 
μ (nm) Q (b) E* (keV)
+2.0935(9)0
+2.09335(9)0
0.056(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.