Raman Band Shapes and Molecular Reorientation

1972 ◽  
Vol 57 (4) ◽  
pp. 1795-1796 ◽  
Author(s):  
Stanislav Sýkora
1974 ◽  
Vol 52 (13) ◽  
pp. 1209-1214 ◽  
Author(s):  
S. Sunder ◽  
R. E. D. McClung

The contour of the v2 Raman band of SF6 liquid has been studied over the temperature range 226–315 K. Reorientational and angular momentum correlation times were obtained by comparing the Fourier transforms of the band contours with the reorientational correlation functions calculated using the J diffusion limit of the extended rotational diffusion model. A reanalysis of Hackleman and Hubbard's nuclear relaxation data for liquid SF6, using the correlation times obtained from the Raman studies, yields the value ± 6.2 × 104 s−1 for the asymmetry in the spin–rotation tensor [Formula: see text] for fluorine nuclei in SF6.


1986 ◽  
Vol 17 (1) ◽  
pp. 65-69 ◽  
Author(s):  
Th. Steiger ◽  
K.-W. Brzezinka ◽  
P. Reich

1973 ◽  
Vol 59 (5) ◽  
pp. 2498-2508 ◽  
Author(s):  
R. C. Livingston ◽  
Walter G. Rothschild ◽  
J. J. Rush

2001 ◽  
Vol 15 (28n30) ◽  
pp. 3865-3868 ◽  
Author(s):  
H. MIYAOKA ◽  
T. KUZE ◽  
H. SANO ◽  
H. MORI ◽  
G. MIZUTANI ◽  
...  

We have obtained the Raman spectra of TiCl n (n= 2, 3, and 4). Assignments of the observed Raman bands were made by a normal mode analysis. The force constants were determined from the observed Raman band frequencies. We have found that the Ti-Cl stretching force constant increases as the oxidation number of the Ti species increases.


2021 ◽  
Vol 63 (9) ◽  
pp. 1646-1648
Author(s):  
D. V. Petrov ◽  
I. I. Matrosov ◽  
A. R. Zaripov ◽  
A. S. Tanichev
Keyword(s):  

1964 ◽  
Vol 42 (6) ◽  
pp. 1058-1069 ◽  
Author(s):  
A. D. May ◽  
G. Varghese ◽  
J. C. Stryland ◽  
H. L. Welsh

The frequencies of the Q(J) lines of the fundamental Raman band of compressed hydrogen gas were measured with high spectral resolution for a series of densities from 25 to 400 Amagat units at 300 °K and 85 °K. The frequency shifts are expressed as a power series in the gas density. The linear coefficient at a given temperature has the form aJ = ai + ae(nJ/n), where ai, constant for all the Q lines, can be interpreted in terms of isotropic intermolecular forces, and ae(nJ/n), proportional to the relative population of the initial J level, arises from the inphase coupled oscillation of pairs of molecules. The temperature variation of ai is analyzed on the basis of the Lennard-Jones intermolecular potential and the molecular pair distribution function. The repulsive overlap forces and the attractive dispersion forces give, respectively, positive and negative contributions to ai, which can be characterized by the empirical parameters Krep and Katt. The values of Katt and ae are in good agreement with calculations based on the polarizability model of the dispersion forces. The relation of the results to the Raman frequency shifts in solid hydrogen is discussed.


1996 ◽  
Vol 14 (7-8) ◽  
pp. 727-730
Author(s):  
J.-P. Korb ◽  
L. Malier ◽  
F. Cros

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