First-principles quantitative prediction of the lattice thermal conductivity in random semiconductor alloys: the role of force-constant disorder
arXiv:1712.02577 · doi:10.1103/PhysRevB.98.115205
Abstract
The standard theoretical understanding of the lattice thermal conductivity, , of semiconductor alloys assumes that mass disorder is the most important source of phonon scattering. In contrast, we show that the hitherto neglected contribution of force-constant (IFC) disorder is essential to accurately predict the of those polar compounds characterized by a complex atomic-scale structure. We have developed an \emph{ab initio} method based on special quasirandom structures and Green's functions, and including the role of IFC disorder, and applied it in order to calculate the of and alloys. We show that, while for , phonon-alloy scattering is dominated by mass disorder, for , the inclusion of IFC disorder is fundamental to accurately reproduce the experimentally observed . As the presence of a complex atomic-scale structure is common to most III-V and II-VI random semiconductor alloys, we expect our method to be suitable for a wide class of materials.
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