1995•Physical review. B, Condensed matterRequires access

Reconstruction of the GaAs (311)Asurface

M. Wassermeier, John L. Sudijono, Matthew D. Johnson, K. T. Leung, Bradford G. Orr, L. Däweritz, K. Ploog

Open publisher page 124 citations

Abstract

We study the reconstruction of the GaAs (311)A surface with reflection high-energy electron-diffraction (RHEED) and scanning tunneling microscopy (STM). The surface observed in situ with RHEED during molecular-beam epitaxy is distinguished by a lateral periodicity of 3.2 nm perpendicular to the [2\ifmmode\bar\else\textasciimacron\fi{}33] direction. This periodicity is confirmed employing in situ STM. High-resolution STM images furthermore reveal a surface reconstruction characterized by a dimerization of the surface As atoms. We show how the reconstruction can be formed, applying a simple electron-counting model. The excellent agreement with the experimental results further support this model, which was already found to explain the reconstructions of the (100) and the (111) surfaces. In order to form a semiconducting surface, the three uppermost layers are involved in the reconstruction process, giving rise to a depth modulation of 0.34 nm.

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What this paper is about

We study the reconstruction of the GaAs (311)A surface with reflection high-energy electron-diffraction (RHEED) and scanning tunneling microscopy (STM). The surface observed in situ with RHEED during molecular-beam epitaxy is distinguished by a lateral periodicity of 3.2 nm perpendicular to the [2\ifmmode\bar\else\textasciimacron\fi{}33] direction. This periodicity is confirmed employing in situ STM. High-resolution STM images furthermore reveal a surface reconstruction characterized by a dimerization of the surface As atoms. We show how the reconstruction can be formed, applying a simple electron-counting model. The excellent agreement with the experimental results further support this model, which was already found to explain the reconstructions of the (100) and the (111) surfaces. In order to form a semiconducting surface, the three uppermost layers are involved in the reconstruction process, giving rise to a depth modulation of 0.34 nm.

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Available abstract

We study the reconstruction of the GaAs (311)A surface with reflection high-energy electron-diffraction (RHEED) and scanning tunneling microscopy (STM). The surface observed in situ with RHEED during molecular-beam epitaxy is distinguished by a lateral periodicity of 3.2 nm perpendicular to the [2\ifmmode\bar\else\textasciimacron\fi{}33] direction. This periodicity is confirmed employing in situ STM. High-resolution STM images furthermore reveal a surface reconstruction characterized by a dimerization of the surface As atoms. We show how the reconstruction can be formed, applying a simple electron-counting model. The excellent agreement with the experimental results further support this model, which was already found to explain the reconstructions of the (100) and the (111) surfaces. In order to form a semiconducting surface, the three uppermost layers are involved in the reconstruction process, giving rise to a depth modulation of 0.34 nm.

Key concepts: Reflection high-energy electron diffraction, Surface reconstruction, Scanning tunneling microscope, Electron diffraction, Reflection (computer programming), Molecular beam epitaxy, Surface (topology), Materials science

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