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Evaluating the Thermoelectric Properties of BaTiS(3) by Density Functional Theory

[Image: see text] BaTiS(3) is a semiconductor with a small bandgap of ∼0.5 eV and strong transport anisotropy caused primarily by structural anisotropy; it contains well-separated octahedral columns along the [0001] direction and low lattice thermal conductivity, appealing for thermoelectric applica...

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Detalles Bibliográficos
Autores principales: Paudel, Tula R., Tsymbal, Evgeny Y.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: American Chemical Society 2020
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7271404/
https://www.ncbi.nlm.nih.gov/pubmed/32548422
http://dx.doi.org/10.1021/acsomega.0c01139
Descripción
Sumario:[Image: see text] BaTiS(3) is a semiconductor with a small bandgap of ∼0.5 eV and strong transport anisotropy caused primarily by structural anisotropy; it contains well-separated octahedral columns along the [0001] direction and low lattice thermal conductivity, appealing for thermoelectric applications. Here, we evaluate the prospect of BaTiS(3) as a thermoelectric material by using the linearized electron and phonon Boltzmann transport theory based on the first-principles density functional band structure calculations. We find sizable values of the key thermoelectric parameters, such as the maximum power factor PF = 928 μW K(–2) and the maximum figure of merit ZT = 0.48 for an electron-doped sample and PF = 74 μW K(–2) and ZT = 0.17 for a hole-doped sample at room temperature, and a small doping level of ±0.25e per unit cell. The increase in temperature yields an increase in both the power factor and the figure of merit, reaching large values of PF = 3078 μW K(–2) and ZT = 0.77 for the electron-doped sample and PF = 650 μW K(–2) and ZT = 0.62 for the hole-doped sample at 800 K. Our results elucidate the promise of BaTiS(3) as a material for the thermoelectric power generator.