MBE Growth of Custom-Designed III-V Semiconductor Microstructures Scaled to the Physical Limit: Ultrathin-Layer Superlattices and Monolayer Doping

  • Klaus Ploog
Part of the NATO ASI Series book series (NSSB, volume 206)

Abstract

Molecular beam epitaxy (MBE) of custom-designed microstructures has reached a status where monolayer dimensions in artificially layered semi­conductors are being routinely controlled to form a new clls of materials with accurately tailored electrical and optical properties1,2. The unique capabilities of molecular beam epitaxy in terms of spatially resolved ma­terials synthesis has stimulated the inspiration of device engineers to design a whole new generation of electronic and photonic devices based on the concept of band gap engineering3,4. This concept, also called wavefunc­tion or density-of-states engineering5,6, respectively, relies on the ar­bitrary modulation of band-edge potentials in semiconductors through the abrupt change of composition (e.g. GaAs/AlAs, GaSb/InAs, Si/Ge, etc.) or of dopant concentration. The microscopic structuring or engineering of se­miconducting solids to within atomic dimensions is thus achieved by the incorporation of interfaces (consisting of abrupt homo- or heterojunctions) into a crystal in well-defined geometrical and spatial arrangements. The electrical and optical properties are then defined locally, and phenomena related to extremely small dimensions (“quantum size effects”) become more important than the actual chemical properties of the materials involved.

Keywords

Molecular Beam Epitaxy High Electron Mobility Transistor Molecular Beam Epitaxy Growth Super Lattice Molecular Beam Epitaxy System 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer Science+Business Media New York 1989

Authors and Affiliations

  • Klaus Ploog
    • 1
  1. 1.Max-Planck-Institut für FestkörperforschungStuttgart 80FR Germany

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