Comparison of the structure of grain boundaries in silicon and diamond by molecular-dynamics simulations
Author(s) -
Pawel Keblinski,
Simon R. Phillpot,
D. Wolf,
H. Gleiter
Publication year - 1997
Publication title -
osti oai (u.s. department of energy office of scientific and technical information)
Language(s) - English
Resource type - Reports
DOI - 10.2172/495836
Subject(s) - dangling bond , grain boundary , materials science , molecular dynamics , nanocrystalline material , silicon , diamond , crystallization , diamond cubic , nanocrystal , nanocrystalline silicon , chemical physics , crystallography , graphite , condensed matter physics , amorphous silicon , nanotechnology , crystalline silicon , chemistry , metallurgy , computational chemistry , microstructure , physics , thermodynamics
Molecular-dynamics simulations were used to synthesize nanocrystalline silicon with a grain size of up to 75 {angstrom} by crystallization of randomly misoriented crystalline seeds from the melt. The structures of the highly-constrained interfaces in the nanocrystal were found to be essentially indistinguishable from those of high-energy bicrystalline grain boundaries (GBs) and similar to the structure of amorphous silicon. Despite disorder, these GBs exhibit predominantly four-coordinated (sp{sup 3}-like) atoms and therefore have very few dangling bonds. By contrast, the majority of the atoms in high-energy bicrystalline GBs in diamond are three-coordinated (sp{sup 2}-like). Despite the large fraction of three-coordinated GB carbon atoms, they are rather poorly connected amongst themselves, thus likely preventing any type of graphite-like electrical conduction through the GBs
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