1. Thermal properties of In2O3 and α-Ga2S3 compounds.
- Author
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Safieddine, Fatima, El Haj Hassan, Fouad, and Kazan, Michel
- Subjects
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BOLTZMANN'S equation , *WIDE gap semiconductors , *THERMOELECTRIC materials , *CRYSTAL orientation , *THERMAL properties , *THERMAL conductivity - Abstract
We investigate the thermal conductivity of In₂O₃ and α-Ga₂S₃ lattices using simulations based on the Boltzmann phonon transport equation (BTE) and first-principles calculations. The study employs a real-space finite displacement method to determine the second- and third-order interatomic force constants (IFCs), which are critical for solving the BTE iteratively. Our findings indicate that In₂O₃ and α-Ga₂S₃ exhibit relatively low thermal conductivities compared to other wide-bandgap semiconductors. At room temperature (300 K), the calculated isotropic thermal conductivity of cubic In₂O₃ is 16.2 Wm−1K⁻1. For monoclinic α-Ga₂S₃, the three principal components of thermal conductivity are 17.0, 20.7, and 15.2 W m⁻1 K⁻1, depending on the crystallographic direction. This low thermal conductivity is primarily attributed to significant phonon scattering via three-phonon processes. Furthermore, we estimate the phonon mean free path (MFP) to be approximately 56 nm for In₂O₃ and between 198 and 231 nm for α-Ga₂S₃, varying with crystal orientation. These findings offer valuable insights into the thermal transport properties of In₂O₃ and α-Ga₂S₃, highlighting their potential for thermoelectric applications while delineating the constraints these properties impose on their use in electronic devices. • In 2 O 3 and α-Ga 2 S 3 have relatively low thermal conductivity. • The low thermal conductivity is due to the high phonon scattering rate via three-phonon processes. • Our predictedvalues of the thermal conductivity for Ga 2 S 3 of the three principal components are 17.0, 20.7, and 15.2 Wm−1K−1. [ABSTRACT FROM AUTHOR]
- Published
- 2024
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