A reanalysis of the n 3 , n 4 , and n 6 interacting bands of D 2 CO has been carried out in the region 850-1250 cm 01 using high-resolution Fourier transform spectra recorded at Giessen. As compared to the previous study of these bands (1987, K. Nakagawa, R. H. Schwendeman, and J. W. C. Johns, J. Mo
High-Resolution Analysis of the ν6, ν7, ν8, and ν9Bands of H15N16O3Measured by Fourier Transform Spectroscopy
✍ Scribed by F. Keller; A. Perrin; J.-M. Flaud; J.W.C. Johns; Z. Lu; E.C. Looi
- Publisher
- Elsevier Science
- Year
- 1998
- Tongue
- English
- Weight
- 151 KB
- Volume
- 191
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The analysis of the 6 , 7 , 8 , and 9 bands of H 15 N 16 O 3 located at 646.9641, 578.4719, 743.6166, and 458.2917 cm Ϫ1 , respectively, has been carried out in the 400 -800 cm Ϫ1 region using high-resolution Fourier transform spectra recorded at Ottawa. Using the ground state energy levels calculated from the v ϭ 0 rotational constants of H 15 N 16 O 3 [A. P. Cox, M. C. Ellis, C. J. Attfield, and A. C. Ferris, J. Mol. Struct. 320, 91-106 (1994)], it was possible to assign the A-type 6 and 7 bands and the C-type 8 and 9 bands of H 15 N 16 O 3 up to high J and K a rotational quantum numbers. The v 6 ϭ 1, v 7 ϭ 1, v 8 ϭ 1, and v 9 ϭ 1 experimental energy levels were then introduced in a least-squares fit calculation and precise upper state Hamiltonian constants (band centers and rotational constants) were determined allowing one to reproduce the infrared data to within the experimental uncertainty.
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