Abstract

We present a systematic study of the atomic and electronic structure of the $\mathrm{Si}(111)\text{\ensuremath{-}}(5\ifmmode\times\else\texttimes\fi{}2)\text{\ensuremath{-}}\mathrm{Au}$ reconstruction using first-principles electronic structure calculations based on the density functional theory. We analyze the structural models proposed by Marks and Plass [Phys. Rev. Lett. 75, 2172 (1995)], those proposed recently by Erwin [ Phys. Rev. Lett. 91, 206101 (2003)], and a completely different structure that was found during our structural optimizations. We study in detail the energetics and the structural and electronic properties of the different models. For the two most stable models, we also calculate the change in the surface energy as a function of the content of silicon adatoms for a realistic range of concentrations. Our model is the energetically most favorable in the range of low adatom concentrations, while Erwin's ``$5\ifmmode\times\else\texttimes\fi{}2$'' model becomes favorable for larger adatom concentrations. The crossing between the surface energies of both structures is found close to $1∕2\phantom{\rule{0.3em}{0ex}}\text{adatom}\phantom{\rule{0.3em}{0ex}}\text{per}\phantom{\rule{0.3em}{0ex}}5\ifmmode\times\else\texttimes\fi{}2\phantom{\rule{0.3em}{0ex}}\text{unit}\phantom{\rule{0.3em}{0ex}}\text{cell}$, i.e., near the maximum adatom coverage observed in the experiments. Both models, our structure and Erwin's ``$5\ifmmode\times\else\texttimes\fi{}2$'' model, seem to provide a good description of many of the available experimental data, particularly of the angle-resolved photoemission measurements.

Highlights

  • The low-energy electronic spectrum of a one-dimensional metal is dominated by collective spin and charge excitations.[1,2,3] This is in contrast with the behavior of typical metals, which can be understood in terms of independentparticle-like excitations usually called quasiparticles

  • We turn our attention to the effect of the different silicon adatom content and the simulated STM images, which we only analyze in detail for the most stable structural models

  • Instead the extra silicon atoms decorate the step edge of the terraces on the surface. These observations seem to have at least two implications: ͑ithe optimal adatom concentration must be certainly lower than one adatom per 5 ϫ 2 cell andiithe structure of the reconstruction must be stable against relatively large changes of the content of adatoms[62] since the density of silicon adatoms can be increased by a factor of 2 without, at least apparently, dramatic structural changes.[36]

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Summary

Introduction

The low-energy electronic spectrum of a one-dimensional metal is dominated by collective spin and charge excitations.[1,2,3] This is in contrast with the behavior of typical metals, which can be understood in terms of independentparticle-like excitations usually called quasiparticles. These predictions are clear and well established. The one-dimensional character of these states is preserved It is in this context that the fabrication of monatomic wires of metal atoms on silicon substrates has attracted much attention in recent years

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