Methods
We employed density functional theory (DFT) calculations combined with the effective screening medium (ESM) technique1 + the reference interaction site method (RISM);2 ESM-RISM formulation3 makes it possible to simulate the electrode (+ reactive ions) and the solution based on quantum mechanics and implicit classical solvation model, respectively. ESM-RISM calculations were performed on the configuration of a vacuum/slab/solvent system as shown in Figure 1, where the DFT slab domain is on the left-hand side, and the RISM solvents, that is, H2O, H3O+, and Cl− treated by the RISM equations, are on the right-hand side. Changing the chemical potential of electron, µe, referenced to the inner potential ΦS at the bulk solution region, we compared the grand potentials Ω for the following reaction R:
H3O+ (1M HCl aq.) + e− (electrode M, M=Pt, Al) ↔︎ 1/2 H2 (gas) + H2O (1M HCl aq.) (R).
Results
ESM-RISM calculations revealed Ω of the left side state of reaction R and that of the right state on Pt(111) electrode. They cross at µe = −5.27 eV, which is equilibrium chemical potential of electron at SHE reaction (= µSHE). This indicates that the electrode potential vs. SHE, E(SHE), is evaluated as E(SHE) = −(µe − µSHE)/e. We also obtained the almost same value of µSHE on Al(111) electrode. On the other hand, Pt(111) and Al(111) is negatively and positively charged at µe = µSHE, respectively. In the presentation, we will compare the potential profile of metal/solution/vacuum region obtained from ESM-RISM and the first-principles molecular dynamics calculation using ESM.4 We further discuss on the difference between µSHE and the absolute SHE obtained by Trasatti.5
References
- M. Otani, O. Sugino, Phys. Rev. B 73, 115407 (2006).
- F. Hirata, P. J. Rossky, Chem. Phys. Lett. 83, 329, (1981).
- S. Nishihara, M. Otani, Phys. Rev. B 96, 115429 (2017).
- M. Otani, I. Hamada, O. Sugino, Y. Morikawa, Y. Okamoto,T. Ikeshoji, J. Phys. Soc. Jpn. 77, 024802 (2008).
- S. Trasatti, Pure Appl. Chem. 58, 955 (1986).