Abstract

We present the results of a comparative study of the equilibrium crystal structure and vibrational properties of the $\mathrm{Na}∕\mathrm{Cu}(111)$ system at coverages up to monolayer saturation. The calculations are performed with interaction potentials from the embedded-atom method. The following ordered structures are considered: $p(3\ifmmode\times\else\texttimes\fi{}3)$, $p(2\ifmmode\times\else\texttimes\fi{}2)$, $(\sqrt{3}\ifmmode\times\else\texttimes\fi{}\sqrt{3})30\ifmmode^\circ\else\textdegree\fi{}$, and $(3∕2\ifmmode\times\else\texttimes\fi{}3∕2)$. The surface relaxation, phonon dispersion, and polarization of vibrational modes for the adsorbate and substrate atoms as well as the local density of states are discussed. It is found that the bond length between an adsorbate and the nearest-neighbor substrate atom slightly increases with increasing coverage. Adsorption of sodium also results in a small rumpling in two upper substrate layers. The mode associated with adatom-substrate stretch vibrations was obtained in our calculation at about $22\phantom{\rule{0.3em}{0ex}}\mathrm{meV}$ for all the structures considered. The strength of this mode decreases with increasing coverage in accordance with the experiment. On the other hand, we find that the frustrated translation mode frequency of sodium on Cu(111) is strongly coverage dependent.

Highlights

  • Adsorption of alkali-metal atoms on metal surfaces causes a drastic change of many properties of metal substrate surfaces

  • It is found that the bond length between an adsorbate and the nearest-neighbor substrate atom slightly increases with increasing coverage

  • We have presented the results of a comparative study of the vibrational and structural properties of the Na/ Cu111͒ systems at coverages up to the monolayer saturation

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Summary

Introduction

Adsorption of alkali-metal atoms on metal surfaces causes a drastic change of many properties of metal substrate surfaces. This adsorption frequently results in the formation of complex crystal structures which involve a certain restructuring of the substrate surface atoms.. This adsorption frequently results in the formation of complex crystal structures which involve a certain restructuring of the substrate surface atoms.1–3 It leads to the modification of the substrate surface electronic states and gives rise to adsorbate- ͑adlayer-͒induced electron states.. As for Na adatoms on the Cu111͒ surface, so far the adsorption structures at coverages below the saturated monolayerMLremain uncertain though adsorbate-induced systems have been studied by different experimental techniques.. Alkali-metal atoms adsorbed on close-packed111͒ metal surfaces generally form hexagonal structures.. To describe the transition from the p3 ϫ 3͒ low-coverage structure to the3 / 2 ϫ 3 / 2͒

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