Raman Spectra of Carbon Dioxide and Its Isotopic Variants in the Fermi Resonance Region: Part III. Analysis of Rovibrational Intensities for 12C16O2, 13C16O2, 12C18O2 and 12C16O18O

1982 ◽  
Vol 86 (9) ◽  
pp. 797-805 ◽  
Author(s):  
H. Finsterhölzl
1978 ◽  
Vol 32 (4) ◽  
pp. 401-402 ◽  
Author(s):  
H. W. Klöckner ◽  
H. Finsterhölzl ◽  
K. Srinivasan ◽  
H. W. Schrötter

2004 ◽  
Vol 708 (1-3) ◽  
pp. 189-195 ◽  
Author(s):  
N.A. Atamas ◽  
A.M. Yaremko ◽  
T. Seeger ◽  
A. Leipertz ◽  
A. Bienko ◽  
...  

1952 ◽  
Vol 30 (2) ◽  
pp. 99-110 ◽  
Author(s):  
H. L. Welsh ◽  
P. E. Pashler ◽  
B. P. Stoicheff

Two Raman tubes, one of quartz and one of glass, capable of withstanding pressures up to 75 and 300 atm. respectively, were used to study density effects in the Raman spectrum of carbon dioxide. The components of the ν1 band show changes in frequency and relative intensity with increasing density. An analysis shows that the frequency changes are due to a lowering of the frequency of 2ν2, in Fermi resonance with ν1, with increasing density. The intensity effect, however, is not completely explained by the change in the sharpness of the resonance. In the high pressure gas and in the liquid faint bands corresponding to the Raman inactive frequencies, ν2 and ν3, are observed. The effect of increasing density on the rotational Raman spectrum can be explained in terms of the broadening of anisotropic scattering by intermolecular forces.


1965 ◽  
Vol 16 (2) ◽  
pp. 278-290 ◽  
Author(s):  
G. Amat ◽  
M. Pimbert

1984 ◽  
Vol 15 (4) ◽  
pp. 232-236 ◽  
Author(s):  
Adriano Bigotto ◽  
Gianna Castellani

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