Paudel Tula R, Tsymbal Evgeny Y
Department of Physics and Astronomy & Nebraska Center for Materials and Nanoscience, University of Nebraska, Lincoln, Nebraska 68588-0299, United States.
ACS Omega. 2020 May 22;5(21):12385-12390. doi: 10.1021/acsomega.0c01139. eCollection 2020 Jun 2.
BaTiS 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 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 and the maximum figure of merit ZT = 0.48 for an electron-doped sample and PF = 74 μW K 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 and ZT = 0.77 for the electron-doped sample and PF = 650 μW K and ZT = 0.62 for the hole-doped sample at 800 K. Our results elucidate the promise of BaTiS as a material for the thermoelectric power generator.
BaTiS是一种半导体,其带隙约为0.5 eV,较小,且主要由结构各向异性导致具有很强的输运各向异性;它沿[0001]方向包含分离良好的八面体柱,且晶格热导率低,这使其在热电应用方面颇具吸引力。在此,我们基于第一性原理密度泛函能带结构计算,采用线性化电子和声子玻尔兹曼输运理论,评估了BaTiS作为热电材料的前景。我们发现,对于电子掺杂样品,在室温下,关键热电参数具有相当大的值,例如最大功率因子PF = 928 μW/K,最大品质因数ZT = 0.48;对于空穴掺杂样品,PF = 74 μW/K,ZT = 0.17,且每单位晶胞的掺杂水平为±0.25e。温度升高会使功率因子和品质因数都增加,在800 K时,电子掺杂样品的PF = 3078 μW/K,ZT = 0.77,空穴掺杂样品的PF = 650 μW/K,ZT = 0.62。我们的结果阐明了BaTiS作为热电发电机材料的前景。