Following excitation of the OCS bending overtone 2ν2, with a Q-switched CO2 laser, time-dependent fluorescence from the symmetric stretching fundamental ν1, has been observed for mixtures of OCS with 4He, Ne, Ar, Kr, and Xe. Analysis of the exponential rise and fall of fluorescence provides relaxation rates corresponding to the collisional coupling of the ν1 and ν2 manifolds and the overall vibration–translation/rotation relaxation for collisions of OCS with the various rare gases. For the process 2ν2→ν1, the experimentally derived probabilities per collision are OCS–Ne?1.7×10−4, OCS–Ar 1.2±0.4×10−4, OCS–Kr 0.8±0.2×10−4 and OCS–Xe 1.0±0.2×10−4. For the vibration–translation/rotation relaxation, the probabilities per collision are OCS–Ne 1.4±0.8×10−4, OCS–Ar 0.3±0.3×10−4, OCS–Kr 0.2±0.2 ×10−4, and OCS–Xe 0.1±0.1×10−4. Model calculated probabilities, using a spherically symmetric, short-range repulsive interaction potential, qualitatively agree with these experimental probabilities. If in the case of OCS–4He, only the path 2ν2→ν1 is assumed to couple the bending and stretching (ν1) modes, then the experimental probabilities are 6±2×10−4, for the process 2ν2→ν1 and 10 ± 3×10−4 for the vibration–translation/rotation process. This intermode vibration– vibration probability, however, is unexpectedly large when compared to both the model calculations and the experimental values for the other OCS–rare gas mixtures. A cyclic kinetic path allowing for both 2ν2 and ν2 to couple to ν1 in OCS–4He collisions is suggested by the model calculations and is also consistent with the OCS–4He experimental data. Assuming the complete kinetic cycle results in OCS–4He probabilities with the following ranges: 0–8×10−4 for the process 2ν2→ν1, 0–1×10−4 for the process ν2→ν1 and 5–13×10−4 for the vibration–translation/rotation process, depending on the relative contribution (which cannot be ascertained from these experiments) of the two competing steps filling the ν1 level. The cyclic path kinetics of OCS–4He system exemplifies the general phenomenon of cyclic mechanisms which may be important in promoting rapid vibration–vibration and vibration–translation/rotation energy transfer, particularly for complex or highly excited molecules.
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