Nucleus[1] Binding energy (MeV) g.s. Radius[3] & Deformation[4]
167N9   Nitrogen
J(π)=2-
T1/2=7.13 s
  Experiment
[2]		 Theory
[4]		 Sh.corr.
[4]
Mass Excess 5.683907
(0.002301)		    
BE 117.981  
BE/A 7.374  
<R2ch>1/2 = 
Charge-density Distribution [6]

β2=
β3=
β4=
β6=
Excited States[1]
click on a plot to process it 		Known and possible Decays[1] Q-values (keV)
roman [2], italic [4]
α - decay-10110.41
β- - decay10420.94
β+ - decay-9032.26
e-capture-8010.26
1p - decay-11478.24
2p - decay-32557.78
1n - decay-2488.83
2n - decay-13322.11
2β- - decay-4996.28
β-,n-5242.96
β-,2n-18466.11
β-,d-10315.17
β-,t-14611.34
β-,α3259.04
β-,n,α-15462.55
EC,p-30563.12
EC,2p-48848.63
EC,α-21818.79
Metastable states and Resonances[1] Radiation energies (keV)[1] Thermal neutrons[1] El.-Magn. properties[5,7,8]
 
E = 3353 keV
T1/2 = 0.015 MeV
n
100%
E = 3523 keV
T1/2 = 0.003 MeV
n
100%
E = 3963 keV
T1/2 = 0.002 MeV
n
100%
E = 4320 keV
T1/2 = 0.020 MeV
n
100%
E = 4391 keV
T1/2 = 0.082 MeV
n
100%
E = 4760 keV
T1/2 = 0.250 MeV
n
100%
E = 4783 keV
T1/2 = 0.059 MeV
n
100%
E = 5054 keV
T1/2 = 0.019 MeV
n
100%
E = 5129 keV
T1/2 = 0.011 MeV
n
100%
E = 5150 keV
T1/2 = 0.011 MeV
n
100%
E = 5230 keV
T1/2 = 0.004 MeV
n
100%
E = 5250 keV
T1/2 = 0.320 MeV
n
100%
E = 5318 keV
T1/2 = 0.260 MeV
n
100%
E = 5521.6 keV
T1/2 = 0.011 MeV
n
100%
E = 5731.7 keV
T1/2 = 0.011 MeV
n
100%
E = 6003 keV
T1/2 = 0.270 MeV
n
100%
E = 6170.7 keV
T1/2 = 0.011 MeV
n
100%
E = 6374 keV
T1/2 = 0.030 MeV
n
100%
E = 6505 keV
T1/2 = 0.034 MeV
n
100%
E = 6840 keV
T1/2 = 0.140 MeV
n
100%
E = 7020 keV
T1/2 = 0.022 MeV
n
100%
E = 7250 keV
T1/2 = 0.017 MeV
n
100%
E = 7572 keV
T1/2 = 0.011 MeV
n
100%
E = 7674 keV
T1/2 = 0.011 MeV
n
100%
E = 7877 keV
T1/2 = 0.100 MeV
n
100%
E = 8048 keV
T1/2 = 0.085 MeV
n
100%
E = 8365 keV
T1/2 = 0.018 MeV
n
100%
E = 8490 keV
T1/2 = 0.050 MeV
n
100%
E = 8720 keV
T1/2 = 0.040 MeV
n
100%
E = 8819 keV
T1/2 = 0.050 MeV
n
100%
E = 9160 keV
T1/2 = 0.100 MeV
n
100%
E = 9340 keV
T1/2 = 0.050 MeV
n
100%
E = 9459 keV
T1/2 = 0.100 MeV
n
100%
E = 10055 keV
T1/2 = 0.030 MeV
n
100%
E = 10370 keV
T1/2 = 0.165 MeV
n
100%
E = 10710 keV
T1/2 = 0.120 MeV
n
100%
E = 11490 keV
T1/2 = -1
n
100%
E = 12090 keV
T1/2 = -1
n
100%
E = 13830 keV
T1/2 = -1
n
100%
E = 14360 keV
T1/2 = 0.180 MeV

100%
β- endpoint energies
γ-energies
 
μ (nm) Q (b) E* (keV)
-1.83(13)397
1.50(8)293
1.60(6)293
1.9859(11)d0
(-)0.018(2)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.