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A velocity map imaging study of the photodissociation of the methyl iodide cation

22

Citations

54

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2017

Year

Abstract

The photodissociation dynamics of the methyl iodide cation has been studied using the velocity map imaging technique. A first laser pulse is used to ionize methyl iodide via a (2 + 1) REMPI scheme through the 5pπ → 6p Rydberg state two-photon transition. The produced CH<sub>3</sub>I<sup>+</sup>(X[combining tilde]<sup>2</sup>E<sub>3/2</sub>) ions are subsequently excited at several wavelengths between 242 and 260 nm. The reported translational energy distributions for the methyl and iodine ions present a Boltzmann-type unstructured distribution at low excitation energies as well as a recoiled narrow structure at higher excitation energies highlighting two different dissociation processes. High level ab initio calculations have been performed in order to obtain a deeper understanding of the photodissociation dynamics of the CH<sub>3</sub>I<sup>+</sup> ion. Direct dissociation on a repulsive state from the manifold of states representing the B[combining tilde] excited state leads to CH<sub>3</sub><sup>+</sup>(X[combining tilde]<sup>1</sup>A<sub>1</sub>') + I*(<sup>2</sup>P<sub>1/2</sub>), while the CH<sub>3</sub> + I<sup>+</sup>(<sup>3</sup>P<sub>2</sub>) channel is populated through an avoided crossing outside the Franck-Condon region. In contrast, an indirect process involving the transfer of energy from highly excited electronic states to the ground state of the ion is responsible for the observed Boltzmann-type distributions.

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