Abstract
We show that the commonly used lowest-order theory of phonon-phonon interactions frequently fails to accurately describe the anharmonic phonon decay rates and thermal conductivity ($\kappa$), even among strongly bonded crystals. Applying a first principles theory that includes both the lowest-order three-phonon and the higher-order four-phonon processes to seventeen zinc blende semiconductors, we find that the lowest-order theory drastically overestimates the measured $\kappa$ for many of these materials, while inclusion of four-phonon scattering gives significantly improved agreement with measurements. We have identified new selection rules on three-phonon processes that help explain many of these failures in terms of anomalously weak anharmonic phonon decay rates predicted by the lowest-order theory competing with four-phonon processes. We also show that zinc blende compounds containing boron (B), carbon (C) or nitrogen (N) atoms have exceptionally weak four-phonon scattering, much weaker than in compounds that do not contain B, C or N atoms. This new understanding helps explain the ultrahigh $\kappa$ in several technologically important materials like cubic boron arsenide, boron phosphide and silicon carbide. At the same time, it not only makes the possibility of achieving high $\kappa$ in materials without B, C or N atoms unlikely, but it also suggests that it may be necessary to include four-phonon processes in many future studies. Our work gives new insights into the nature of anharmonic processes in solids and demonstrates the broad importance of higher-order phonon-phonon interactions in assessing the thermal properties of materials.
Highlights
Phonon-phonon interactions arise from the inherent anharmonicity of the interatomic bonds in solids
We focus on crystals with two different atoms in the unit cell, which encompasses a large number of semiconductors and insulators including the technologically important zinc blende compounds studied in the present work, which have inherently weak anharmonicity of the crystal bonds
Our results indicate that there is very little hope for identifying materials with large contributions to κ coming from the optic phonons, since (a) at moderate-to-high temperatures, fourphonon scattering dominates any frequency region of weak three-phonon scattering for the optic phonons driven by the AAO and AOO#2 selection rules, thereby significantly lowering κ, while (b) at low temperatures, where four-phonon scattering rates can get weaker than their threephonon counterparts, the heat capacity of the optic phonons becomes vanishingly small owing to their high-frequency scale
Summary
Phonon-phonon interactions arise from the inherent anharmonicity of the interatomic bonds in solids. They determine fundamental properties of crystals such as the lattice thermal conductivity (κ) as well as the infrared, Raman, and neutron scattering cross sections [1,2,3]. They impact diverse phenomena including phonon drag [4], phonon bottleneck [5,6], and hydrodynamic thermal transport [7,8].
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