A method of measuring electric quadrupole moments of molecules in excited states

1968 ◽  
Vol 14 (6) ◽  
pp. 557-566 ◽  
Author(s):  
M.P. Bogaard ◽  
B.J. Orr
1980 ◽  
Vol 349 (1-2) ◽  
pp. 271-284 ◽  
Author(s):  
G.C. Ball ◽  
O. Häusser ◽  
T.K. Alexander ◽  
W.G. Davies ◽  
J.S. Forster ◽  
...  

1986 ◽  
Vol 458 (1) ◽  
pp. 165-187 ◽  
Author(s):  
G.J. Gyapong ◽  
R.H. Spear ◽  
M.T. Esat ◽  
M.P. Fewell ◽  
A.M. Baxter ◽  
...  

1970 ◽  
Vol 151 (2) ◽  
pp. 282-294 ◽  
Author(s):  
H.S. Gertzman ◽  
D. Cline ◽  
H.E. Gove ◽  
P.M.S. Lesser

1972 ◽  
Vol 190 (3) ◽  
pp. 597-634 ◽  
Author(s):  
P.M.S. Lesser ◽  
D. Cline ◽  
Philip Goode ◽  
R.N. Horoshko

1989 ◽  
Vol 494 (1) ◽  
pp. 102-122 ◽  
Author(s):  
S.M. Burnett ◽  
A.M. Baxter ◽  
G.J. Gyapong ◽  
M.P. Fewell ◽  
R.H. Spear

2017 ◽  
Vol 13 (2) ◽  
pp. 4678-4688
Author(s):  
K. A. Kharroube

We applied two different approaches to investigate the deformation structures of the two nuclei S32 and Ar36 . In the first approach, we considered these nuclei as being deformed and have axes of symmetry. Accordingly, we calculated their moments of inertia by using the concept of the single-particle Schrödinger fluid as functions of the deformation parameter β. In this case we calculated also the electric quadrupole moments of the two nuclei by applying Nilsson model as functions of β. In the second approach, we used a strongly deformed nonaxial single-particle potential, depending on Î² and the nonaxiality parameter γ , to obtain the single-particle energies and wave functions. Accordingly, we calculated the quadrupole moments of S32 and Ar36 by filling the single-particle states corresponding to the ground- and the first excited states of these nuclei. The moments of inertia of S32 and Ar36 are then calculated by applying the nuclear superfluidity model. The obtained results are in good agreement with the corresponding experimental data.


2020 ◽  
Vol 102 (23) ◽  
Author(s):  
Akito Daido ◽  
Atsuo Shitade ◽  
Youichi Yanase

1989 ◽  
Vol 44 (11) ◽  
pp. 1063-1078 ◽  
Author(s):  
H. Krause ◽  
D. H. Sutter

Abstract The rotational Zeeman effect has been observed in methanimine which was produced from ethylenediamine by flash pyrolysis. The observed vibronic ground state expectation values of the molecular g-values, the magnetic susceptibility anisotropies and the molecular electric quadrupole moments are: gaa = -1.27099(22), gbb= -0.18975(7), gcc= -0.03440(8), 2ξaa-ξbb-ξcc = 12.49(19) · 10-6 ergG-2mol-1, 2ξbb-ξcc-ξaa = 5.22(11) · 10-6 ergG-2 mol-1 Qaa = 0.43(17) · 10-26esu cm2, Qbb= 1.08(10) · 10-26 esu cm2, and Qcc= -1.51 (26) . 10-26 esu cm2. With the TZVP ab initio value for the out-off plane electronic second moment as additional input, reliable values can be given also for the individual components of the magnetic susceptibility tensor and for the bulk susceptibility:ξ = (ξaa + ξbb + ξcc)/3=-13.13(88) · 10-6 erg G -2 mol-1. From low-J a-and b-type zero field transitions the spin-rotation coupling constants and the 14N nuclear quadrupole coupling constants could be redetermined with improved accuracy. These data are compared with our new theoretical results.


2018 ◽  
Vol 42 (12) ◽  
pp. 124105
Author(s):  
Xiao-Jun Sun ◽  
Chun-Xing Chen ◽  
Ning Wang ◽  
Hou-Bing Zhou

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