Related Experiment Video
Updated: Jul 13, 2026

07:50
Electron Channeling Contrast Imaging for Rapid III-V Heteroepitaxial Characterization
Published on: July 17, 2015
Achieving epitaxy between incommensurate materials by quasicrystalline interlayers
K J Franke1, P Gille, K-H Rieder
1Institut für Experimentalphysik, Freie Universität Berlin, Arnimallee 14, 14195 Berlin, Germany.
Physical Review Letters
|August 7, 2007
Summary
Epitaxy, the atomic alignment at interfaces, is redefined for quasicrystals. This new framework uses reciprocal lattice matching to link incommensurate materials, enabling novel interface engineering.
Area of Science:
- Materials Science
- Crystallography
- Surface Science
Background:
- Epitaxy traditionally describes atomic alignment in periodic crystals.
- Quasicrystals, with their unique non-periodic atomic arrangements, present challenges for traditional epitaxy definitions.
Purpose of the Study:
- To generalize the definition of epitaxy to include quasicrystalline materials.
- To explore the real-space structure of interfaces between quasicrystalline and periodic materials.
- To demonstrate the potential of quasicrystals as interlayers for linking incommensurate materials.
Main Methods:
- Defining epitaxy based on reciprocal lattice point matching.
- Analyzing the real-space consequences of this definition for quasiperiodic/periodic interfaces.
- Presenting an experimental realization of such an interface.
Main Results:
- A generalized definition of epitaxy is proposed, applicable to both periodic and quasicrystalline systems.
- Quasicrystals, possessing numerous reciprocal lattice basis vectors, can serve as epitaxial interlayers.
- This facilitates the linking of incommensurate materials through epitaxial interfaces.
Conclusions:
- The study extends the concept of epitaxy to quasicrystalline materials.
- Reciprocal lattice matching provides a universal criterion for epitaxial interfaces.
- Quasicrystals offer new possibilities for designing complex heterostructures and linking incommensurate materials.
Related Concept Videos
Imperfections in Crystal Structure: Point, Line and Plane Defects
A perfect crystal, in theory, has a uniform structure with the same unit cell and lattice points throughout. However, any deviation from this periodic arrangement is known as an imperfection or defect. These defects can be categorized into three types: point, line, and plane defects.Point defects occur when there is a deviation from the ideal due to missing atoms, displaced atoms, or additional atoms. These imperfections might occur due to imperfect packing during crystallization or because of...
Determination of Crystal Structures
In the late 1800s, the revelation that light extended beyond visible wavelengths led to the discovery of X-rays by Wilhelm Roentgen. Recognized as high-energy electromagnetic radiation with short wavelengths, X-rays prompted exploration into their interaction with crystals. Max von Laue proposed in 1912 that the periodic arrangement of atoms, ions, or molecules in crystals would cause them to diffract X-rays, a hypothesis confirmed through experiments with copper sulfate and zinc sulfide...
Metallic Solids
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability. Many...
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability. Many...
Imperfections in Crystal Structure: Stoichiometric Point Defects
Schottky defects arise when some lattice points in a crystal, such as those in NaCl, remain unoccupied, creating lattice vacancies without disturbing the overall electrical neutrality of the crystal. This defect is common in ionic crystals where the positive and negative ions are similar in size, as seen in sodium chloride and cesium chloride. The presence of Schottky defects enables the crystal to conduct electricity to a small extent through an ionic mechanism. Electric fields cause nearby...

