Using Fourier transform spectra recorded at 25 and \(12 \mu \mathrm{m}\), it has been possible to perform the first analysis of the \(3 \nu_{9}-2 \nu_{9}, 3 \nu_{9}-\nu_{5}\) and \(3 \nu_{9}-\nu_{9}\) hot bands of \(\mathrm{HNO}_{3}\) located at \(392.4 \mathrm{~cm}^{-1}\), \(409.8 \mathrm{~cm}^{-1}
Rotational Spectrum of HNO3in the ν5and 2ν9Vibrational States
✍ Scribed by Thomas M. Goyette; Lee C. Oesterling; Douglas T. Petkie; Randy A. Booker; Paul Helminger; Frank C. De Lucia
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 815 KB
- Volume
- 175
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The millimeter/submillimeter transitions of the n 5 -2n 9 interacting bands of HNO 3 have been measured in the symmetric top limit. Torsional splittings in both vibrational bands have been observed. The 2n 9 splitting is due to the torsional motion of H around the NO whereas the n 5 splitting is due to the large mixing with 2n 9 . An analysis is presented in which a Fermi interaction, 2 sets of 2n 9 rotational constants, and one set of n 5 rotational constants are used to account for all of the perturbation and torsional splitting observed in the spectrum. The 860 lines used in this analysis are fit to 91 kHz.
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Torsional splittings in both the \(2 \nu_{9}\) and \(\nu_{5}\) vibrational states have been resolved and observed in the millimeter/submillimeter spectrum of \(\mathrm{HNO}_{3}\). The former splitting is due to the torsional motion of \(\mathrm{H}\) around the \(\mathrm{NO}\) bond in the \(v_{9}\) m
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