Vibration-dependent trajectories and their effects on vibrational dephasing |
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Authors: | Q. Ma R.H. Tipping F. Thibault |
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Affiliation: | a NASA/Goddard Institute for Space Studies and Department of Applied Physics and Applied Mathematics, Columbia University, 2880 Broadway, New York, NY 10025, USA b Department of Physics and Astronomy, University of Alabama, Tuscaloosa, AL 35487, USA c Laboratoire de Photophysique Moléculaire, UPR 3361 CNRS, Université Paris-Sud Campus d’Orsay (Bât. 350), 91405 Orsay Cedex, France d Laboratoire de Physique des Atomes, Laser, Molécules et Surfaces (UMR-CNRS 6627) Université de Rennes I, Campus de Beaulieu, F-35042 Rennes Cedex, France e Laboratoire de Physique Moléculaire, UMR CNRS 6624, Université de Franche-Comté, La Bouloie, 25030 Besançon Cedex, France |
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Abstract: | We show that the expression for S1 (i.e., the first term in the expansion of the S matrix) that is essential in calculating vibration-rotation pressure-broadened shifts is not properly given in the usual Robert-Bonamy (RB) formalism. The problem resulted when they considered effects of the vibrational dephasing on S1; they tacitly made an assumption that the trajectories of interest are vibrationally independent. As a result, the current RB expression is an approximate one. Based on a vibration-dependent trajectory model, which is physically sound, we derive the correct expression for S1. We present numerical calculations of the broadening and shifting cross sections and of the line shape parameters for the H2-He pair and find for this molecular system, new results differ significantly from those calculated using the existing formalism. In addition, by comparing with those derived from close coupling calculations, we find that the new results are better than the old ones. Finally, we discuss how important effects from this modification could be for other molecular systems. We conclude that for certain molecular systems where the short-range collisions are the dominant source responsible for the line widths and shifts, and in addition, the isotropic potential has small depth, the present modification is a worthwhile step to be taken in order to refine the current RB formalism. Meanwhile, for other systems it may not be necessary. |
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Keywords: | Vibrational dephasing Trajectory models Pressure broadening and shifting H2-He Raman widths and shifts |
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