铋纳米线的扩散热能及载流子边界散射的作用。掺杂、压力和磁场研究

A. Nikolaeva, T. Huber, L. Konopko
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引用次数: 1

摘要

大块铋和铋锑是固态冷却应用的兴趣。由于量子约束和声子散射,这些材料的复合材料在这些应用中可能比块状材料优越。此外,人们对微型设备和纳米级冷却器的接口也很感兴趣。我们研究了直径在50- 500nm范围内的单双纳米线的热功率。纳米线被制成单链热电材料,单晶,在玻璃包层(一种纤维)。我们观察到,在50 K左右,热功率峰值约为+90 μ v /K。在这个温度范围内,这些值对于任何电导体都是最大的。我们用现象学模型来解释这些效应,其中边界散射对电子比空穴更有效。温度和热功率最大值与磁场和Te掺杂有密切关系。此外,拉伸纤维会产生类似于“负压”的单轴应力[Hicks, LD, et. al., 1993],从而驱动电子拓扑跃迁,类似于Bi-Te的情况[Lin, Y-M, et. al., 2000]。在ETT点附近,我们记录到热功率的非常大的振荡,这与纳米线中的朗道能级有关。我们的工作重点是建立一个数学模型来优化考虑磁场、掺杂和压力的热电优值
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Diffusion Thermopower Of Bismuth Nanowires And The Role Of Carrier's Boundary Scattering. Doping, Pressure and Magnetic Field Studies
Bulk Bi and Bi-Sb are of interest for solid state cooling applications. Composites of these materials may show to be superior to bulk materials in these applications, because of quantum confinement and phonon scattering. Also, there is an interested in miniature devices and nanoscale coolers that interface with them. We have studied the thermopower of single Bi nanowires of diameters in the range 50-500 nm. The nanowires are fabricated as single strands of thermoelectric material, that are monocrystalline, in a glass envelope (a fiber). We observe that the thermopower peaks of around +90 muV/K at around 50 K. These values are the largest for any electrical-conductor in this temperature range. We interpret these effects in terms of a phenomenological model where boundary scattering is more effective for electrons than for holes. The temperature and the value of thermopower maximum depend sensitively with magnetic fields and Te doping. Also, stretching the fibers cause uniaxial stresses similar to that of "negative pressure" [Hicks, LD, et. al., 1993] that drives an electron topological transition, similarly to the case of Bi-Te [Lin, Y-M, et. al., 2000]. Near the ETT point we recorded very large oscillations of the thermopower, that are associated with the Landau levels in the nanowires. Our work focuses in the development a mathematical model to optimize the thermoelectric figure of merit considering magnetic field, doping, and pressure
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