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Understanding the apparent fractional charge of protons in the aqueous electrochemical double layer.
Chen, Leanne D; Bajdich, Michal; Martirez, J Mark P; Krauter, Caroline M; Gauthier, Joseph A; Carter, Emily A; Luntz, Alan C; Chan, Karen; Nørskov, Jens K.
Afiliación
  • Chen LD; SUNCAT Center for Interface Science and Catalysis, Department of Chemical Engineering, Stanford University, Stanford, CA, 94305, USA.
  • Bajdich M; Division of Chemistry and Chemical Engineering, California Institute of Technology, Pasadena, CA, 91125, USA.
  • Martirez JMP; SUNCAT Center for Interface Science and Catalysis, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA.
  • Krauter CM; Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, NJ, 08544, USA.
  • Gauthier JA; Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, NJ, 08544, USA.
  • Carter EA; Schrödinger GmbH, Dynamostr. 13, D-68165, Mannheim, Germany.
  • Luntz AC; SUNCAT Center for Interface Science and Catalysis, Department of Chemical Engineering, Stanford University, Stanford, CA, 94305, USA.
  • Chan K; School of Engineering and Applied Science, Princeton University, Princeton, NJ, 08544, USA.
  • Nørskov JK; SUNCAT Center for Interface Science and Catalysis, SLAC National Accelerator Laboratory, Menlo Park, CA, 94025, USA.
Nat Commun ; 9(1): 3202, 2018 08 10.
Article en En | MEDLINE | ID: mdl-30097564
ABSTRACT
A detailed atomic-scale description of the electrochemical interface is essential to the understanding of electrochemical energy transformations. In this work, we investigate the charge of solvated protons at the Pt(111) | H2O and Al(111) | H2O interfaces. Using semi-local density-functional theory as well as hybrid functionals and embedded correlated wavefunction methods as higher-level benchmarks, we show that the effective charge of a solvated proton in the electrochemical double layer or outer Helmholtz plane at all levels of theory is fractional, when the solvated proton and solvent band edges are aligned correctly with the Fermi level of the metal (EF). The observed fractional charge in the absence of frontier band misalignment arises from a significant overlap between the proton and the electron density from the metal surface, and results in an energetic difference between protons in bulk solution and those in the outer Helmholtz plane.

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2018 Tipo del documento: Article País de afiliación: Estados Unidos

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2018 Tipo del documento: Article País de afiliación: Estados Unidos