Abstract

We have determined the unoccupied part of the electronic structure of sodium on Cu(111), employing k-resolved inverse photoemission in the isochromat mode. For Na coverages above 0.15 monolayer, an image-potential surface state is observed 2.3 eV above ${\mathit{E}}_{\mathit{F}}$. For the completed p(2\ifmmode\times\else\texttimes\fi{}2) Na phase at 0.25-monolayer coverage, a pronounced Na ${3\mathrm{p}}_{\mathrm{z}}$\char21{}derived feature occurs 0.4 eV above ${\mathit{E}}_{\mathit{F}}$, which exhibits a nearly-free-electron-like energy dispersion. For wave vectors ${\mathit{k}}_{\mathrm{?}}$\ensuremath{\ge}0.6 A${\mathrm{\r{}}}^{\mathrm{\ensuremath{-}}1}$, the unoccupied part of the Na 3s band appears close to the Fermi level. We compare our results with recent band-structure calculations for free and adsorbed Na monolayers.

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