Liberation of H₂ from (o-C₆H₄Me)₃P—H⁽⁺⁾ + ⁽⁻⁾H—B(p-C₆F₄H)₃ ion-pair: A transition-state in the minimum energy path versus the transient species in Born-Oppenheimer molecular dynamics Available to Purchase

Using Born-Oppenheimer molecular dynamics (BOMD) with density functional theory, transition-state (TS) calculations, and the quantitative energy decomposition analysis (EDA), we examined the mechanism of H₂-liberation from LB—H⁽⁺⁾ + ⁽⁻⁾H—LA ion-pair, 1, in which the Lewis base (LB) is (o-C₆H₄Me)₃P and the Lewis acid (LA) is B(p-C₆F₄H)₃. BOMD simulations indicate that the path of H₂ liberation from the ion-pair 1 goes via the short-lived transient species, LB⋯H₂⋯LA, which are structurally reminiscent of the TS-structure in the minimum-energy-path describing the reversible reaction between H₂ and (o-C₆H₄Me)₃P/B(p-C₆F₄H)₃ frustrated Lewis pair (FLP). With electronic structure calculations performed on graphics processing units, our BOMD data-set covers more than 1 ns of evolution of the ion-pair 1 at temperature T ≈ 400 K. BOMD simulations produced H₂-recombination events with various durations of H₂ remaining fully recombined as a molecule within a LB/LA attractive “pocket”—from very short vibrational-time scale to time scales in the range of a few hundred femtoseconds. With the help of perturbational approach to trajectory-propagation over a saddle-area, we directly examined dynamics of H₂-liberation. Using EDA, we elucidated interactions between the cationic and anionic fragments in the ion-pair 1 and between the molecular fragments in the TS-structure. We have also considered a model that qualitatively takes into account the potential energy characteristics of H—H recombination and H₂-release plus inertia of molecular motion of the (o-C₆H₄Me)₃P/B(p-C₆F₄H)₃ FLP.