Presolvation Dynamics Preceding the Hydrated Proton Transfer in the Electrical Double Layer

Hydrated proton transfer (PT) mechanisms in a solid-liquid electric double layer (EDL) remain challenging, as the solvation structure is influenced by the operating potential. Under constant potential framework, we combined the fixed-potential method with <i>ab initio</i> molecular dynamics (AIMD) to simulate the PT in the EDL. Near the interface of EDL, negative potential (vs zero-charge potential) promotes the effective diffusion of the excess proton via reducing the proportion of trapping and revisiting processes of PT, but stiffens the hydrogen bond network manifesting as the restriction of water orientation and the elongation of the O···O pairs. At high negative potentials, hydrated hydrogen ions tend to form the Eigen cation (H<sub>2</sub>O)<sub>3</sub>H<sub>3</sub>O<sup>+</sup> during presolvation processes, but this cation exhibits a higher energy barrier for PT than the pentamer (H<sub>2</sub>O)<sub>4</sub>H<sub>3</sub>O<sup>+</sup> with a 4-fold coordinated shell. Further simulations reveal that the stiffening effect and the Eigen cation formation suppress proton conductivity near the electrode surface.

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Publication Details

Journal
The Journal of Physical Chemistry Letters
Published
2025-05-01
DOI
https://doi.org/10.1021/acs.jpclett.5c00721
Citations
3
Primary Topic
Fuel Cells and Related Materials
Type
article
Field-Weighted Citation Impact
2.19

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article

Presolvation Dynamics Preceding the Hydrated Proton Transfer in the Electrical Double Layer

Guoping Gao, Yufei Xue, Lin‐Wang Wang
3 citations
The Journal of Physical Chemistry Letters
Fuel Cells and Related Materials
2.19
article

Presolvation Dynamics Preceding the Hydrated Proton Transfer in the Electrical Double Layer

Guoping Gao, Yufei Xue, Lin‐Wang Wang
article en
3 citations

Abstract

Hydrated proton transfer (PT) mechanisms in a solid-liquid electric double layer (EDL) remain challenging, as the solvation structure is influenced by the operating potential. Under constant potential framework, we combined the fixed-potential method with <i>ab initio</i> molecular dynamics (AIMD) to simulate the PT in the EDL. Near the interface of EDL, negative potential (vs zero-charge potential) promotes the effective diffusion of the excess proton via reducing the proportion of trapping and revisiting processes of PT, but stiffens the hydrogen bond network manifesting as the restriction of water orientation and the elongation of the O···O pairs. At high negative potentials, hydrated hydrogen ions tend to form the Eigen cation (H<sub>2</sub>O)<sub>3</sub>H<sub>3</sub>O<sup>+</sup> during presolvation processes, but this cation exhibits a higher energy barrier for PT than the pentamer (H<sub>2</sub>O)<sub>4</sub>H<sub>3</sub>O<sup>+</sup> with a 4-fold coordinated shell. Further simulations reveal that the stiffening effect and the Eigen cation formation suppress proton conductivity near the electrode surface.

The Journal of Physical Chemistry LettersVol. 16(18)
Chinese Academy of Sciences (CN), Equilibrium Research (GB), Institute of Semiconductors (CN), Xi'an Jiaotong University (CN)
National Natural Science Foundation of China
Openalex Percentile: Top 12%
Fuel Cells and Related Materials
2.19
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Presolvation Dynamics Preceding the Hydrated Proton Transfer in the Electrical Double Layer — Guoping Gao, Yufei Xue, et al. · The Journal of Physical Chemistry Letters (2025) | TGRS Research Map | TGRS