Excited state hyperfine structures in 133Cs using quantum beat spectroscopy

1991 ◽  
Vol 69 (7) ◽  
pp. 808-812 ◽  
Author(s):  
J. Sagle ◽  
W. A. van Wijngaarden

Quantum beats arising from the hyperfine interaction were observed in the fluorescence produced when the 8D3/2, 9D3/2, and 10D3/2 states of 133Cs radiatively decayed to the 6P1/2 state. The period of the beats equals the reciprocal of the magnetic dipole coupling constant a since the 133Cs nucleus has a negligibly small electric quadrupole moment. The results are a = 3.95 ± 0.01, 2.38 ± 0.01, and 1.54 ± 0.02 MHz for the 8D3/2, 9D3/2, and 10D3/2 states, respectively.

1970 ◽  
Vol 151 (2) ◽  
pp. 273-281 ◽  
Author(s):  
H.S. Gertzman ◽  
D. Cline ◽  
H.E. Gove ◽  
P.M.S. Lesser ◽  
J.J. Schwartz

1998 ◽  
Vol 53 (6-7) ◽  
pp. 549-551
Author(s):  
K. Sato ◽  
S. Takeda ◽  
S. Fukuda ◽  
T. Minamisono ◽  
M. Tanigaki ◽  
...  

Abstract In order to determine the electric quadrupole moment of the short-lived β-emitter 41Sc from the quadrupole coupling constant in TiO2 , we measured the field gradient by detecting the Fourier-Transformed-NMR of stable isotope 45Sc doped in TiO2. Also, in order to study the electronic structure of impurities systematically, EFGs were measured for 45Sc, 49Ti and 93Nb in a TiO2 ingle single crystal.


2021 ◽  
Vol 22 (1) ◽  
pp. 19-29
Author(s):  
S.B. Doma ◽  

The binding energy, the root-mean-square radius, the magnetic dipole moment, the electric quadrupole moment, and the moment of inertia of the nucleus 6Li are calculated by applying different models. The translation invariant shell model is applied to calculate the binding energy, the root-mean-square radius, and the magnetic dipole moment by using two- and three-body interactions. Also, the spectra of the nuclei with A = 6 are calculated by using the translation-invariant shell model. Moreover, the ft-value of the allowed transition: 6He(Jπ=0+;T=1)β- → 6Li(Jπ=1+;T'=1) is also calculated. Furthermore, the concept of the single-particle Schrodinger fluid for axially symmetric deformed nuclei is applied to calculate the moment of inertia of 6Li. Also, we calculated the magnetic dipole moment and the electric quadrupole moment of the nucleus 6Li in this case of axially symmetric shape. Moreover, the nuclear superfluidity model is applied to calculate the moment of inertia of 6Li, based on a single-particle deformed anisotropic oscillator potential added to it a spin-orbit term and a term proportional to the square of the orbital angular momentum, as usual in this case. The single-particle wave functions obtained in this case are used to calculate the magnetic dipole moment and the electric quadrupole moment of 6Li.


1983 ◽  
Vol 122 (1) ◽  
pp. 23-26 ◽  
Author(s):  
W.J. Vermeer ◽  
M.T. Esat ◽  
J.A. Kuehner ◽  
R.H. Spear ◽  
A.M. Baxter ◽  
...  

1987 ◽  
Vol 470 (2) ◽  
pp. 415-428 ◽  
Author(s):  
G.J. Gyapong ◽  
R.H. Spear ◽  
M.P. Fewell ◽  
A.M. Baxter ◽  
S.M. Burnett

2019 ◽  
Vol 100 (1) ◽  
Author(s):  
Benquan Lu ◽  
Tingxian Zhang ◽  
Hong Chang ◽  
Jiguang Li ◽  
Yong Wu ◽  
...  

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