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Microwave and sub-mmwave study of CH3SiH3 including the perturbation-allowed torsion-vibration difference band (ν12=0,ν6=3)↔(ν12=1,ν6=0)
Authors:I Ozier  A Bauder  N Moazzen-Ahmadi
Institution:a Department of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, BC, Canada V6T 1Z1
b Laboratorium für Physikalische Chemie, Eidgenössische Technische Hochschule, CH-8093 Zürich, Switzerland
c Department of Molecular and Laser Physics, NSRIM, University of Nijmegen, P.O.Box 9010, NL-6500 GL Nijmegen, The Netherlands
d Department of Physics and Astronomy, University of Calgary, 2500 University Drive NW, Calgary, Alta., Canada T2N 1N4
e Department of Physical Sciences, University of Oulu, P.O. Box 3000, FIN-90014, Linnanmaa, Finland
Abstract:The vibration-torsion-rotation Hamiltonian in CH3SiH3 has been investigated using Fourier transform microwave methods and tunable sideband far-infrared spectroscopy. Four different studies have been carried out. First, the Q-branch of the torsion-vibration difference band (ν12=0,ν6=3)↔(ν12=1,ν6=0) has been measured between 17.8 and 26.6 GHz. When three quanta of the torsional mode ν6 are excited in the ground vibrational state (gs) for (σ=−1) torsional sublevels with K=6, these transitions become allowed through resonant Coriolis-like coupling to the lowest lying degenerate mode ν12 with no quanta of ν6 excited. Second, direct l-doubling transitions in the state (v12=1, v6=0) have been observed between 8.3 and 17.5 GHz for both torsional sublevels σ=0 and σ=±1. In the limit that the intervibrational interactions vanish, the σ-splitting between lines of the same J would be difficult to resolve, but frequency differences of more than 1 GHz due to these interactions have been determined. Third, the (J=1←0) spectrum just below 22 GHz has been re-measured with higher resolution for 0?v6?4 in the gs and for (v6=0) in ν12. Finally, the (J=45←44) spectrum near 1 THz has been obtained for 0?v6?2 in the gs. A global data set of 3423 frequencies has been formed by merging the present 123 measurements with the data set used recently in the simultaneous analysis of the ν12 and ν5 bands by Schroderus et al. J. Chem Phys. 115 (2001) 1392]. By refining the (gs/ν12/ν5) Hamiltonian developed in this earlier work in which the torsional motion is grouped with the vibrational degrees of freedom, a good fit to within experimental error has been obtained by varying 45 parameters. A fit of comparable quality has also been obtained using a similar analysis in which the torsional motion is grouped with the rotational degrees of freedom. The values of the molecular constants determined in the two models are compared.
Keywords:Internal rotation  Torsion  Vibration  Methyl silane  Fourier transform microwave  Sub-mmwave  Difference band
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