Abstract

We report a first-principles evaluation of the exchange-correlation potential (${V}_{\mathrm{XC}}$) at a metal surface. An integral equation relating ${V}_{\mathrm{XC}}$ and the nonlocal electron self-energy (${\ensuremath{\Sigma}}_{\mathrm{XC}}$) is solved numerically for a free-electron metal surface, with use of a static approximation for ${\ensuremath{\Sigma}}_{\mathrm{XC}}$. The strongly inhomogeneous nature of the electron density profile at the surface is treated exactly, i.e., without invoking the usual local-density approximation. Our result for ${V}_{\mathrm{XC}}$ has the correct imagelike asymptotic behavior; it derives implicitly from a nonlocal exchange-correlation energy functional. We study the effect of nonlocality on the position of the effective image plane (${z}_{0}$) from an analysis of the image tail of ${V}_{\mathrm{XC}}$ and also from linear-response theory. The difference in the values of ${z}_{0}$ obtained by both methods for low metallic densities is attributed to electron-overlap effects.

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