Abstract

We have performed an ab initio theoretical investigation of the energetic stability, equilibrium atomic geometry, and scanning tunneling microscope (STM) images of the $\mathrm{Ca}∕\mathrm{Si}(111)$ surface. We have considered the $(3\ifmmode\times\else\texttimes\fi{}1)$, $(3\ifmmode\times\else\texttimes\fi{}2)$, and $(2\ifmmode\times\else\texttimes\fi{}1)$ structural models for Ca coverage of $1∕3$ ML, $1∕6$ ML, and $1∕2$ ML, respectively. Our total energy results indicate that the $(3\ifmmode\times\else\texttimes\fi{}1)$ phase is not expected to occur, even for Ca-rich conditions. In the $(3\ifmmode\times\else\texttimes\fi{}2)$ phase the Ca adatoms lie on the $T4$ sites along the surface trench separated by Si honeycomb chains. Similarly, in the $(2\ifmmode\times\else\texttimes\fi{}1)$ phase the Ca adatoms are adsorbed on the $T4$ sites of the surface trench separated by Si zigzag chains. The equilibrium geometries and electronic charge transfers between Ca adatoms and Si(111) surface for the $(3\ifmmode\times\else\texttimes\fi{}2)$ and $(2\ifmmode\times\else\texttimes\fi{}1)$ phases have been detailed. Our simulated STM images indicate that the higher-lying occupied states are located on the topmost Si atoms along the chains, while the empty states lie on the Ca adatoms, forming bright spots and stripes on the $(3\ifmmode\times\else\texttimes\fi{}2)$ and $(2\ifmmode\times\else\texttimes\fi{}1)$ surfaces. For occupied states, the simulated STM images confirm the experimentally verified $2\ifmmode\times\else\texttimes\fi{}$ modulation along the honeycomb chains in the $\mathrm{Ca}∕\mathrm{Si}(111)\text{\ensuremath{-}}(3\ifmmode\times\else\texttimes\fi{}2)$ surface, induced by attractive interactions between Ca adatoms and the nearest-neighbor Si atoms. Finally we have calculated the electronic band structures for the energetically stable $(3\ifmmode\times\else\texttimes\fi{}2)$ and $(2\ifmmode\times\else\texttimes\fi{}1)$ phases of the $\mathrm{Ca}∕\mathrm{Si}(111)$ surface, and compared (in detail) with the recent experimental findings.

Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.