2019
DOI: 10.1021/acscatal.9b01137
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Mechanism of Heterolytic Hydrogen Splitting by Frustrated Lewis Pairs: Comparison of Static and Dynamic Models

Abstract: Free energy surfaces generated via ab initio molecular dynamics simulations for H 2 activation reactions with intramolecular frustrated Lewis pairs (FLPs) point to a concerted (single-step) mechanism of H−H bond cleavage. Statistical analysis carried out for a large number of reaction trajectories reveals notable asynchronicity in the development of donor-H and acceptor-H bonds with the latter being in a more advanced phase. These findings are fully consistent with the results of static quantum chemical calcul… Show more

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Cited by 32 publications
(28 citation statements)
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“…Indeed, this charge‐separated state lies much higher in energy (54.4 kcal mol −1 ) than the neutral donor‐acceptor pair [PMes 3 , B(C 6 F 5 ) 3 ] and undergoes rapid back‐electron transfer (lifetime=237 ps) as determined by transient absorption spectroscopy to regenerate the FLP, [10] thus preventing build‐up of a concentration of radicals large enough to influence the reaction kinetics. This leads to the conclusion that the splitting of dihydrogen by PMes 3 and B(C 6 F 5 ) 3 proceeds via a two‐electron, heterolytic pathway, even when the reaction is performed in ambient light [2e–g] …”
Section: Resultsmentioning
confidence: 99%
“…Indeed, this charge‐separated state lies much higher in energy (54.4 kcal mol −1 ) than the neutral donor‐acceptor pair [PMes 3 , B(C 6 F 5 ) 3 ] and undergoes rapid back‐electron transfer (lifetime=237 ps) as determined by transient absorption spectroscopy to regenerate the FLP, [10] thus preventing build‐up of a concentration of radicals large enough to influence the reaction kinetics. This leads to the conclusion that the splitting of dihydrogen by PMes 3 and B(C 6 F 5 ) 3 proceeds via a two‐electron, heterolytic pathway, even when the reaction is performed in ambient light [2e–g] …”
Section: Resultsmentioning
confidence: 99%
“…The geometries of all species discussed in this work have been optimized at the B3LYP/6‐31G* level of theory [26–27] . The B3LYP hybrid functional have been shown to give accurate geometries and energies for FLP chemistry by previous computational studies, [28–30] and previous benchmark calculations [19,31] revealed that the computed ΔG for FLP reactions are somehow independent on the selected functional (i. e. B97D, M062X) and basis set (i. e. 6‐31G* and 6‐31+G**). Moreover, the adopted computational approach is not to produce accurate Gibbs energies for direct comparison with the experimentally measured quantities, but to provide qualitative trends for predicting FLP′s thermochemistry.…”
Section: Computational Detailsmentioning
confidence: 88%
“… 17 30 In addition, the flexibility and dynamical behavior of FLP systems, including in transition-state (TS) geometries, have been subjected to several molecular dynamics investigations. 31 34 …”
Section: Introductionmentioning
confidence: 99%