We have measured the rotational spectrum of \(\mathrm{H}^{127} \mathrm{I}\) from 0.38 to \(4.58 \mathrm{THz}\left(13-153 \mathrm{~cm}^{-1}\right)\), encompassing the \(R(0)\) through \(R(11)\) rotational lines. using the \(\mathrm{CO}_{2}\) laser difference method for generating coherent far-infrare
The Far Infrared Spectrum of the NO Dimer
โ Scribed by A.R.W. McKellar; J.K.G. Watson
- Publisher
- Elsevier Science
- Year
- 1999
- Tongue
- English
- Weight
- 145 KB
- Volume
- 194
- Category
- Article
- ISSN
- 0022-2852
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โฆ Synopsis
The far-infrared spectrum of the NO dimer in the gas phase has been observed for the first time using a long-path (180 m) cooled (99 K) absorption cell and a Bomem Fourier transform spectrometer. Four weak vibration-rotation bands were detected in the 120 -450 cm ฯช1 region and assigned to intermolecular vibrations of the cis-planar ON-NO complex. The strongest is a type b band at 239.36 cm ฯช1 , which is assigned as the 2 (symmetric bending) fundamental. A second type b band at 134.50 cm ฯช1 , partly obscured by 2 โธ 3/2 4 2 โธ 1/2 transitions of the NO monomer, is assigned as the 3 (intermolecular stretch) fundamental. A third type b band at 351.38 cm ฯช1 can then be assigned as the 2 ฯฉ 3 combination band. Finally, a very weak type a band at 429.14 cm ฯช1 is assigned as the 6 (antisymmetric bending) fundamental. We report here detailed analyses of the 2 and 2 ฯฉ 3 bands, which yielded upper state rotational parameters, centrifugal distortion parameters, and band origins. Somewhat less extensive analyses for 3 and 6 give their rotational parameters and band origins. These results resolve the mystery of the true values of the intermolecular vibrational frequencies of the NO dimer, which turn out to be rather different from previous determinations based on condensed phase spectra.
๐ SIMILAR VOLUMES
TABLE 2 Rotational and 127 I Hyperfine Parameters for DI (in MHz) a Values in parentheses indicate 1 uncertainties of the last digits.
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