The effective operator approach is applied to the calculation of both line positions and line intensities of the 13 C 16 O 2 molecule. About 11 000 observed line positions of 13 C 16 O 2 selected from the literature have been used to derive 84 parameters of a reduced effective Hamiltonian globally d
The 3ν1 and ν1 + 3ν3 − ν2 Absorption Bands of 16O3
✍ Scribed by S. Bouazza; A. Barbe; J.J. Plateaux; J.M. Flaud; C. Camypeyret
- Publisher
- Elsevier Science
- Year
- 1993
- Tongue
- English
- Weight
- 240 KB
- Volume
- 160
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
Using a high-pressure (\times) path length sample of ozone it has been possible to record at high resolution ( (0.006 \mathrm{~cm}^{-1}) ) the (3-\mu \mathrm{m}) absorption region of this molecule. A thorough analysis of the spectra has been performed allowing one to assign for the first time the (3 \nu_{1}) band of ({ }^{16} \mathrm{O}{3}). Also, during the course of the analysis it became clear that, in this spectral region, another band almost as strong as (3 \nu{1}) was absorbing: it is the (\nu_{1}+3 \nu_{3}-\nu_{2}) hot band. The ((300)) rotational levels were reproduced together with the ((003),(102)), and (201) ones [J. Mol. Spectrosc. 141, 134-144 ( 1990 )] using a Hamiltonian matrix which takes explicitly into account the Darling-Dennison and the Coriolis interaction terms affecting the levels. The band centers (\nu_{0}\left(3 \nu_{3}\right)=3046.0878), (\nu_{0}\left(\nu_{1}+2 \nu_{3}\right)=3083.7030, \nu_{0}\left(2 \nu_{1}+\nu_{3}\right)=3186.4110), and (\nu_{0}\left(3 \nu_{1}\right)=3289.9297 \mathrm{~cm}^{-1}) were derived as well as precise rotational and coupling constants. Line intensities were also measured for (3 v_{1}) as well as for (\nu_{1}+3 \nu_{3}-\nu_{2}) and were reproduced with suitable transition moment operators. Finally a complete line list of the bands of ({ }^{16} \mathrm{O}_{3}) absorbing around (3 \mu \mathrm{m}) has been generated. C 1993 Academic Press. Inc.
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