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}
The Perpendicular C–H Stretching Band ν9/ν13and the Torsional Potential of Dimethylacetylene
✍ Scribed by J. Plı́va; A.S. Pine; S. Civiš
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 352 KB
- Volume
- 180
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
The perpendicular band of the fourfold degenerate C-H stretching vibration of dimethylacetylene (2-butyne) occurring in the region 2955-3065 cm 01 has been measured with Doppler-limited resolution at a temperature of Ç195 K on a difference-frequency laser spectrometer, and on a high-resolution Fourier transform instrument at room temperature as well as in a molecular jet at Ç20 K. From a detailed rotational analysis of this complex band, based on an extension of the model of the rotational-torsional interactions described by P. R. Bunker and C. di Lauro (Chem. Phys. 190, 159-169, 1995), accurate spectroscopic constants were determined for the upper CH stretching state, along with values for the first three components of the Fourier expansion for the torsional potential in the ground state, and for six components of this potential in the upper state. Over 700 lines assigned to 37 well-resolved subbands plus 25 additional unresolved line-like Q-branches were fitted with an overall standard deviation of 0.0024 cm 01 . The results yield a value of 6.316 { 0.034 cm 01 for the barrier to internal rotation in the ground state, and 6.643 { 0.006 cm 01 for the C-H stretching state. This value for the ground state barrier is somewhat higher than that recently determined from an analysis of the CH 3 rocking band by P. R.
📜 SIMILAR VOLUMES
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
In an attempt to account for the large-amplitude torsional \(\nu_{9}\) mode of nitric acid, a formalism is set up, based on an internal-axis-method-like approach previously developed for high-barrier tunneling problems. This formalism is applied to the calculation of the tunneling-rotationalvibratio
The ν 1 + ν 3 and the ν 1 + ν 2 + ν 1 4 + ν -1 5 combination bands of 13 C 2 H 2 at 6521.9 and 6535.1 cm -1 , respectively, are studied with diode laser spectroscopy. Line center wavelengths have been determined with 0.00012-nm standard uncertainty up to J = 40 for ν 1 + ν 3 and up to J = 25 for ν 1