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Potential energy surface stationary points and dynamics of the F<sup>−</sup>+ CH<sub>3</sub>I double inversion mechanism

35

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51

References

2017

Year

Abstract

Direct dynamics simulations were performed to study the S<sub>N</sub>2 double inversion mechanism S<sub>N</sub>2-DI, with retention of configuration, for the F<sup>-</sup> + CH<sub>3</sub>I reaction. Previous simulations identified a transition state (TS) structure, i.e. TS0, for the S<sub>N</sub>2-DI mechanism, including a reaction path. However, intrinsic reaction coordinate (IRC) calculations from TS0 show it is a proton transfer (PT) TS connected to the F<sup>-</sup>HCH<sub>2</sub>I S<sub>N</sub>2 pre-reaction complex and the FHCH<sub>2</sub>I<sup>-</sup> proton transfer post-reaction complex. Inclusion of TS0 in the S<sub>N</sub>2-DI mechanism would thus involve non-IRC atomistic dynamics. Indeed, trajectories initiated at TS0, with random ensembles of energies as assumed by RRKM theory, preferentially form the S<sub>N</sub>2-DI products and ∼70% follow the proposed S<sub>N</sub>2-DI pathway from TS0 to the products. In addition, the Sudden Vector Projection (SVP) method was used to identify which CH<sub>3</sub>I vibrational mode excitations promote access to TS0 and the S<sub>N</sub>2-DI mechanism. Results of F<sup>-</sup> + CH<sub>3</sub>I simulations, with SVP specified mode excitations, are disappointing. With the CH<sub>3</sub> deformations of CH<sub>3</sub>I excited, the S<sub>N</sub>2 single inversion mechanism is the dominant pathway. If the CH stretch modes are also excited, proton transfer dominates the reaction. S<sub>N</sub>2-DI occurs, but with a very small probability of ∼1%. The reasons behind these results are discussed.

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