Computational analysis of I-PCET reveals unique mechanisms in metal-semiconductor-solution systems, highlighting implications for electrocatalysis.
Interfacial proton-coupled electron transfer (I-PCET) in composite metal-semiconductor systems is important for many electrocatalytic processes. Herein, I-PCET at a metal-semiconductor-solution interface is investigated computationally using a Au-TiO2 model system, where the proton transfers from the TiO2 surface to an alcohol acceptor. We studied four possible I-PCET mechanisms that could occur in the system. For each mechanism, the calculated slope of the I-PCET equilibrium constant as a function of applied potential qualitatively agrees with experimental measurements of I-PCET-promoted Bronsted acid catalysis on a Ti-TiO2 composite system, although the dependence of the calculated results on the thickness of the TiO2 slab modeled prevents the unambiguous identification of the I-PCET mechanism. Focusing on one specific I-PCET mechanism, our charge analysis indicates that each proton transfer from the TiO2 surface is coupled to transfer of n ≈ 0.5 electrons from the Au metal to the external circuit. The calculated inverse slope of ∼110 mV is consistent with the Nernstian slope of a 1H+-ne− PCET process. Further analysis shows that the observed slope arises from both electrostatic and capacitive contributions from the interface, together leading to a ∼0.6 eV change in the reaction free energy for deprotonation per 1 V potential change. These analyses reveal unique I-PCET reaction characteristics at electrified metal-semiconductor-solution interfaces and provide fundamental insights into how catalyst material properties influence the potential dependence of these elementary steps.
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Cui et al. (2025) studied this question.
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