\(\mathrm{O}_{2}\)-broadening coefficients have been measured for 19 lines ( with \(J\) values ranging from 3 to 46 and \(\mathrm{K}\) up to 11 ) of \(\mathrm{CH}_{3}{ }^{35} \mathrm{Cl}\) in the \(P\) and \(R\) branches of the \(\nu_{3}\) parallel-type band. These lines. located in the spectral ran
Theoretical O2- and N2-Broadening Coefficients of CH3Cl Spectral Lines
β Scribed by J.P. Bouanich; G. Blanquet; J. Walrand
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 467 KB
- Volume
- 161
- Category
- Article
- ISSN
- 0022-2852
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β¦ Synopsis
The intermolecular potential derived by Leavitt from irreducible tensor methods is used in a semiclassical impact theory to calculate the (\mathrm{O}{2^{-}})and (\mathrm{N}{2})-broadening coefficients of the ({ }^{q} P(J, K)) and ({ }^{9} R(J, K)) lines belonging to a parallel band of (\mathrm{CH}{3}{ }^{35} \mathrm{Cl}). To describe the trajectory model, we have used a Lennard-Jones isotropic potential. The parameters of this potential have been calculated for (\mathrm{CH}{3} \mathrm{Cl}, \mathrm{O}{2}), and (\mathrm{N}{2}) by fitting experimental values of second-virial coefficients. By choosing some of the potential parameters among values available in the literature, we have obtained results that are generally in satisfactory agreement with experimental data. Our calculation predicts that for the lines belonging to the same low or medium (J) transitions, the broadening coefficients decrease significantly as (K) increases, especially for (\mathrm{CH}{3} \mathrm{Cl}-\mathrm{N}{2}). ici 1993 Academic Press, Inc.
π SIMILAR VOLUMES
The nitrogen and oxygen broadening coefficients of ozone have been experimentally obtained at two low temperatures (227 and 186 K) in the n 1 / n 3 band, located at 2110 cm 01 . Thirty-five transitions have been chosen to derive the n coefficient defined by a(T ) Γ a(T o )r(T o /T ) n . This is foun
branches of the 5 perpendicular band. These lines with J values ranging from 1 to 23 and K from 0 to 9 (K Υ J) are located in the spectral range 1416 -1573 cm Οͺ1 . The collisional halfwidths are obtained by modeling each spectral line with a Voigt and a Rautian profile. The noncorrelated Rautian mod
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