Abstract

We present the structural evolution of Bi on Au(111) from monolayer to multilayer regimes explored mainly by scanning tunneling microscopy. At the monolayer regime, Bi clusters distribute homogeneously to make an array with $5\phantom{\rule{4pt}{0ex}}\ifmmode\times\else\texttimes\fi{}\phantom{\rule{4pt}{0ex}}5$ periodicity. Further increase of the coverage converts these clusters to the two-dimensional periodic $(\sqrt{37}\ifmmode\times\else\texttimes\fi{}\sqrt{37})\mathrm{R}25.{3}^{\ensuremath{\circ}}$ and $(\mathrm{p}\phantom{\rule{4pt}{0ex}}\ifmmode\times\else\texttimes\fi{}\sqrt{3})$ structures. We propose a model of the $(\sqrt{37}\ifmmode\times\else\texttimes\fi{}\sqrt{37})\mathrm{R}25.{3}^{\ensuremath{\circ}}$ structure based on the STM measurements and density-functional theory calculations. In the multilayer regime, superstructures at first appear with long-range periodicities arising from the moir\'e structures due mainly to the stacking of Bi layers. Then, the thicker films grow whose lattice constants are close to those of the (110) surface of rhombohedral Bi crystal. The Bi(110) films of more than 60 layers grow stably. Thus, this system provides a good stage for further investigation of the peculiar electronic properties of Bi(110).

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.