Cargando…
High-level ab initio potential energy surface and dynamics of the F(–) + CH(3)I S(N)2 and proton-transfer reactions
Bimolecular nucleophilic substitution (S(N)2) and proton transfer are fundamental processes in chemistry and F(–) + CH(3)I is an important prototype of these reactions. Here we develop the first full-dimensional ab initio analytical potential energy surface (PES) for the F(–) + CH(3)I system using a...
Autores principales: | , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Royal Society of Chemistry
2017
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC5413972/ https://www.ncbi.nlm.nih.gov/pubmed/28507692 http://dx.doi.org/10.1039/c7sc00033b |
Sumario: | Bimolecular nucleophilic substitution (S(N)2) and proton transfer are fundamental processes in chemistry and F(–) + CH(3)I is an important prototype of these reactions. Here we develop the first full-dimensional ab initio analytical potential energy surface (PES) for the F(–) + CH(3)I system using a permutationally invariant fit of high-level composite energies obtained with the combination of the explicitly-correlated CCSD(T)-F12b method, the aug-cc-pVTZ basis, core electron correlation effects, and a relativistic effective core potential for iodine. The PES accurately describes the S(N)2 channel producing I(–) + CH(3)F via Walden-inversion, front-side attack, and double-inversion pathways as well as the proton-transfer channel leading to HF + CH(2)I(–). The relative energies of the stationary points on the PES agree well with the new explicitly-correlated all-electron CCSD(T)-F12b/QZ-quality benchmark values. Quasiclassical trajectory computations on the PES show that the proton transfer becomes significant at high collision energies and double-inversion as well as front-side attack trajectories can occur. The computed broad angular distributions and hot internal energy distributions indicate the dominance of indirect mechanisms at lower collision energies, which is confirmed by analyzing the integration time and leaving group velocity distributions. Comparison with available crossed-beam experiments shows usually good agreement. |
---|