Thermoelectric properties of gated phosphorene junctions

磷烯 塞贝克系数 热电效应 凝聚态物理 功勋 材料科学 之字形的 各向异性 热导率 热电材料 电阻率和电导率 物理 光电子学 带隙 热力学 光学 量子力学 复合材料 几何学 数学
作者
K. J. Lamas-Martínez,J. A. Briones-Torres,S. Molina-Valdovinos,I. Rodrı́guez-Vargas
出处
期刊:Physical review [American Physical Society]
卷期号:107 (24) 被引量:9
标识
DOI:10.1103/physrevb.107.245427
摘要

The reduced dimensions of nanostructures offer opportunities to control and improve the performance of thermoelectric devices based on two-dimensional materials. Here, we investigate theoretically the thermoelectric properties of gated phosphorene junctions (GPJs). We focus on the electronic contribution due to the possible ultralow phononic thermal conductivity in GPJs. The effects of nanostructuration, temperature, and phosphorene anisotropy are analyzed. The hybrid matrix method and the Landauer-B\"uttiker formalism are implemented to obtain the transmission coefficient and thermoelectric properties, respectively. We consider electronic transport mediated by holes or equivalently $n\ensuremath{-}p\ensuremath{-}n$ transport, finding that nanostructuration induces a strong anisotropy in all thermoelectric properties. The Seebeck coefficient, figure of merit, and efficiency have a better response in the zigzag direction, whereas, the electronic conductance, power factor and electronic thermal conductance have higher values in the armchair direction. In the case of large chemical potentials, large electrostatic potentials and narrow barriers the temperature generates an increase and broadening in all thermoelectric properties. In the zigzag direction, the figure of merit attains values above the technological limit value $ZT=3$, owing to the significant reduction of the ratio of conductances with respect to the Wiedemann-Franz law and the large values of the Seebeck coefficient. On the contrary, for low chemical potentials, small electrostatic potentials and wide barriers the thermoelectric properties diminish with the temperature. In this case, the figure of merit is dictated essentially by the Seebeck coefficient due to the slight variation of the ratio of conductances with respect to the Wiedemann-Franz law.
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