Abstract

The SO(X 3 Σ −) product vibrational and rotational state distributions following the title reaction have been studied by laser induced fluorescence on the (B 3 Σ −-X 3 Σ −) transition. The O( 3P) atom was generated by 351 nm photolysis of NO 2. The SO(X 3 Σ −) product is highly vibrationally excited and the vibrational state distribution is inverted at v″=5 with detectable population up to v″=9. The observed vibrational state distribution has been modelled effectively by a Franck-Condon/Golden Rule treatment. The nascent rotational state distribution of v″=4 and 6 can be characterized by rotational temperatures, T R=2288±357 K and T R=2227±297 K, respectively. The rotational state populations are nearly equilibrated with the ambient gas within 10 hard sphere collisions. A surprisal analysis reveals that the observed rotational state distribution is colder than would be predicted on the basis of a purely statistical energy disposal model. The observed SO(X 3 Σ −) internal energy accounts for ≈ 34% of the total energy available to products. The non-statistical energy disposal results are consistent with a direct S atom abstraction mechanism.

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