放电等离子烧结
拓扑绝缘体
热导率
声子
凝聚态物理
材料科学
拓扑(电路)
电子迁移率
热电效应
热电材料
量子
三元运算
物理
烧结
热力学
组合数学
复合材料
量子力学
计算机科学
程序设计语言
数学
作者
Manisha Samanta,Koushik Pal,Umesh V. Waghmare,Kanishka Biswas
标识
DOI:10.1002/ange.202000343
摘要
Abstract A challenge in thermoelectrics is to achieve intrinsically low thermal conductivity in crystalline solids while maintaining a high carrier mobility ( μ ). Topological quantum materials, such as the topological insulator (TI) or topological crystalline insulator (TCI) can exhibit high μ . Weak topological insulators (WTI) are of interest because of their layered hetero‐structural nature which has a low lattice thermal conductivity ( κ lat ). BiTe, a unique member of the (Bi 2 ) m (Bi 2 Te 3 ) n homologous series ( m : n =1:2), has both the quantum states, TCI and WTI, which is distinct from the conventional strong TI, Bi 2 Te 3 (where m : n =0:1). Herein, we report intrinsically low κ lat of 0.47–0.8 W m −1 K −1 in the 300–650 K range in BiTe resulting from low energy optical phonon branches which originate primarily from the localized vibrations of Bi bilayer. It has high μ ≈516 cm 2 V −1 s −1 and 707 cm 2 V −1 s −1 along parallel and perpendicular to the spark plasma sintering (SPS) directions, respectively, at room temperature.
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