Abstract

The stability and growth of three-dimensional (3D) nanostructures in the Ge on Si system is controlled in part by the strain- and overlayer-thickness-dependent surface energies of the crystal facets involved. Here, we use density functional theory (DFT) with local-density approximation calculations to calculate the strain- and thickness-dependent energy of various Ge(113) and Si(113) surface reconstructions. Results of DFT calculations are compared to Tersoff potential calculations to assess the relative importance of stress-strain effects compared to electronic effects not captured by empirical atomistic potentials. We find that the self-interstitial-based $3\phantom{\rule{0.16em}{0ex}}\ifmmode\times\else\texttimes\fi{}\phantom{\rule{0.16em}{0ex}}2$ adatom-dimer-interstitial and $3\ifmmode\times\else\texttimes\fi{}2$ adatom-interstitial surface reconstructions are stable for Ge overlayer thicknesses from 0 to 4 monolayers and at applied biaxial strains from $\ensuremath{\sim}$$\ensuremath{-}4$$%$ to 0$%$. We leverage calculated surface energies to determine net effective surface energies of various experimentally observed 3D Ge on Si nanostructures.

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