Dipole moment and hyperfine properties of the ground state and the C–H excited vibrational state of HCN

1984 ◽  
Vol 80 (9) ◽  
pp. 3989-3991 ◽  
Author(s):  
William L. Ebenstein ◽  
J. S. Muenter
1965 ◽  
Vol 43 (1) ◽  
pp. 144-154 ◽  
Author(s):  
D. H. Phelps ◽  
F. W. Dalby

The ultraviolet spectrum of the OH molecule has been obtained in electric fields up to 64 000 volts per cm. Stark line splittings, broadenings, and field-induced parity-forbidden transitions have been observed. The electric dipole moment of OH in its electronic and vibrational ground state (X2Π) has been determined to be (1.727 ± 0.02) Debyes. The dipole moment in the first excited vibrational state has been found to be about 4% lower.


1981 ◽  
Vol 75 (10) ◽  
pp. 4869-4872 ◽  
Author(s):  
Hiroaki Kuze ◽  
Takayoshi Amano ◽  
Tadao Shimizu

1974 ◽  
Vol 29 (5) ◽  
pp. 797-803 ◽  
Author(s):  
U. Andresen ◽  
H. Dreizier

Abstract The microwave spectrum of methylthiocyanate is reinvestigated on the basis of a molecular model with five degrees of freedom, three for the overall rotation, one for the torsion and one for another vibration. It was possible to fit the splittings of all four measured states (ground state, first excited torsional and vibrational state and second excited vibrational state) with one set of parameters but it was impossible to fit the absolute line frequencies. The value for the potential parameter of the pure torsion V3 is in good agreement with that determined on the basis of the rigid framerigid top (RF-RT) model from the ground state.


1985 ◽  
Vol 40 (9) ◽  
pp. 913-919
Author(s):  
Juan Carlos López ◽  
José L. Alonso

Abstract The rotational transitions of 3,4-dihydro-1,2-pyran in the ground state and six vibrationally excited states have been assigned. The rotational constants for the ground state (A = 5198.1847(24), B = 4747.8716(24) and C = 2710.9161(24) have been derived by fitting μa, μb and μc-type transitions. The dipole moment was determined from Stark displacement measurements to be 1.400(8) D with its principal axis components |μa| =1.240(2), |μb| = 0.588(10) and |μc| = 0.278(8) D. A model calculation to reproduce the ground state rotational constants indicates that the data are consistent with a twisted ring conformation. The average intensity ratio gives vibrational separations between the ground and excited states of the ring-bending and ring-twisting modes of ~ 178 and ~ 277 cm-1 respectively.


2008 ◽  
Vol 128 (4) ◽  
pp. 044304 ◽  
Author(s):  
Lorenzo Lodi ◽  
Roman N. Tolchenov ◽  
Jonathan Tennyson ◽  
A. E. Lynas-Gray ◽  
Sergei V. Shirin ◽  
...  

2006 ◽  
Vol 124 (6) ◽  
pp. 064311 ◽  
Author(s):  
Chikako Oyanagi ◽  
Kiyoshi Yagi ◽  
Tetsuya Taketsugu ◽  
Kimihiko Hirao

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