Dynamic Electrochemical Proton Discharge on Metal Electrodes: The Effects of Electronic Nonadiabaticity
ORAL
Abstract
Proton discharge on metal electrodes is a key step in many important electrochemical reactions. This proton-coupled electron transfer is typically a dynamic process, yet it is often treated adiabatically. Nonadiabatic effects arising from proton motion, however, can alter the electron transfer rate and lead to the excitation of coherent electron-hole (e-h) pairs within the metal electrode[1]. These e-h pairs, along with solvent mode excitations, act as additional channels for translational energy transfer, described in the framework of electronic friction.
In this study, we present a comprehensive theoretical investigation of the proton discharge dynamics on metal electrodes, explicitly accounting for energy dissipation into both electronic and phononic excitations. Utilizing the time-dependent Newns-Anderson-Schmickler model, we derive an effective electronic Hamiltonian that incorporates e-h excitations as a perturbation in the slow-motion limit. The proton's motion is coupled to both the solvent modes, modeled as a phonon bath, and the metal's electrons. Through the influence functional path-integral method[2], we derive a quasiclassical Langevin equation and provide a simplified expression for the electronic friction coefficient.
Our numerical simulations[3] reveal a significant shift in the onset of nonadiabatic electron occupation of the proton when electronic friction is considered, with substantial implications for the electron transfer rate.
[1] E. F. Arguelles and O. Sugino, J. Chem. Phys. 160, 144102 (2024).
[2] R. P. Feynman and F. L. Vernon, Ann. Phys. 24, 118 (1963).
[3] E. F. Arguelles and O. Sugino, in preparation.
In this study, we present a comprehensive theoretical investigation of the proton discharge dynamics on metal electrodes, explicitly accounting for energy dissipation into both electronic and phononic excitations. Utilizing the time-dependent Newns-Anderson-Schmickler model, we derive an effective electronic Hamiltonian that incorporates e-h excitations as a perturbation in the slow-motion limit. The proton's motion is coupled to both the solvent modes, modeled as a phonon bath, and the metal's electrons. Through the influence functional path-integral method[2], we derive a quasiclassical Langevin equation and provide a simplified expression for the electronic friction coefficient.
Our numerical simulations[3] reveal a significant shift in the onset of nonadiabatic electron occupation of the proton when electronic friction is considered, with substantial implications for the electron transfer rate.
[1] E. F. Arguelles and O. Sugino, J. Chem. Phys. 160, 144102 (2024).
[2] R. P. Feynman and F. L. Vernon, Ann. Phys. 24, 118 (1963).
[3] E. F. Arguelles and O. Sugino, in preparation.
*Japan New Energy and Industrial Technology Development Organization (NEDO)MEXT as “Program for Promoting Researches on the Supercomputer Fugaku” (Fugaku battery and Fuel Cell Project) (Grant No. JPMXP1020200301, Project Nos. hp220177, hp210173, and hp200131)Japan Digital Transformation Initiative for Green Energy Materials (DX-GEM)JSPS Grants-in-Aid for Scientific Research(Young Scientists) Grant No. 19K15397MEXT Program: Data Creation and Utilization-Type Material Research and Development Project Grant No. JPMXP1122712807
–
Publication: E. F. Arguelles and O. Sugino, J. Chem. Phys. 160, 144102 (2024)
Presenters
-
Elvis F. Arguelles
- Institute for Solid State Physics, The University of Tokyo