A global treatment of reported microwave, millimeter-wave, and Fourier-transform far-infrared (FIR) spectra of the C-13 isotopic species of methanol has been carried out for the first two torsional states ( n t Å 0 below the barrier and n t Å 1 straddling the barrier) of the ground vibrational state
Global Fit of Torsional-Rotational Transitions in the Ground and First Excited Torsional States of Methanol
✍ Scribed by L.H. Xu; J.T. Hougen
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 640 KB
- Volume
- 173
- Category
- Article
- ISSN
- 0022-2852
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✦ Synopsis
Methanol data for (v_{\mathrm{t}}=0) (below the barrier) and (v_{\mathrm{t}}=1) (straddling the barrier) have been treated, using a program based on the formalism of Herbst et al. (J. Mol. Spectrosc. 108, 42-57, 1984). Altogether, 909 microwave lines (mostly assigned a (50 \mathrm{kHz}) measurement uncertainty) and 197 tunable far-infrared lines (mostly assigned 100 or (200 \mathrm{kHz}) uncertainties) in the range (K \leqslant 12, J \leqslant 20) and 5549 Fourier-transform far-infrared lines (assigned an uncertainty of 0.0002 (\mathrm{cm}^{-1}=6 \mathrm{MHz}) ) in the range (K \leqslant 14, J \leqslant 20) have been globally fit to give a unitless weighted standard deviation of 1.032 , using 56 adjustable and 8 fixed parameters. Some difficulties remain in fitting high (K) and (J b)-type tunable far-infrared lines. Although these difficulties may arise from deficiencies in the model, it also seems possible that some measurement problems still remain in the tunable far-infrared data set. Apart from the high (K) and (J) difficulties with this latter data set, a very satisfactory fit has been achieved, leading us to the conclusion that up through the first excited torsional level, a traditional one-dimensional internal rotation model is capable of accurately describing methanol energy levels, without consideration of other large-amplitude-motion effects, such as those arising, for example, when the (\mathrm{OH}) bending vibration carries the molecule to a (C_{3 \mathrm{v}}) configuration and the internal rotation barrier vanishes. 1995 Academic Press, Inc.
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