The Beijing Municipal Key Laboratory of New Energy Materials and Technologies, School of Materials Science and Engineering , University of Science and Technology Beijing , 100083 Beijing , China.
Department of Materials Science and Engineering , COE, Peking University , Beijing 100871 , China.
ACS Appl Mater Interfaces. 2018 Sep 26;10(38):32201-32211. doi: 10.1021/acsami.8b11300. Epub 2018 Sep 14.
Chalcogenides have been considered as promising thermoelectric materials because of their low cost, nontoxicity, and environmental benignity. In this work, we synthesized a series of CuSTe (0 ≤ x ≤ 1) alloys by a facile, rapid method of mechanical alloying combined with spark plasma sintering process. The CuSTe system provides an excellent vision of the competition between pure phase and phase transformation, entropy-driven solid solution, and enthalpy-driven phase separation. When the Te concentration increases, the CuSTe system changed from the pure monoclinic CuS at x = 0 to monoclinic CuSTe solid solution at 0.02 ≤ x ≤ 0.06 and then transforms to hexagonal CuSTe solid solution at 0.08 ≤ x ≤ 0.1. The phase separation of hexagonal CuTe in the hexagonal CuS matrix occurs at 0.3 ≤ x ≤ 0.7 and finally forms the hexagonal CuTe at x = 1. Owing to the changed band structure and the coexisted CuS and CuTe phases, greatly enhanced power factor was achieved in all CuSTe (0 < x < 1) alloys. Meanwhile, the point defect introduced by the substitution of Te/S atoms strengthened the phonon scattering, resulting in a lowered lattice thermal conductivity in most of these solid solutions. As a consequence, CuSTe exhibits a maximum ZT value of 1.18 at 723 K, which is about 3.7 and 14.8 times as compared to the values of pristine CuS (0.32) and CuTe (0.08), respectively.
硫属化物因其成本低、无毒、环境友好而被认为是很有前途的热电材料。在这项工作中,我们通过机械合金化结合火花等离子烧结工艺,合成了一系列 CuSTe(0 ≤ x ≤ 1)合金。CuSTe 体系提供了一个极好的视角,可以观察到纯相和相变、熵驱动固溶体以及焓驱动相分离之间的竞争。当 Te 浓度增加时,CuSTe 体系从纯单斜 CuS(x = 0)转变为单斜 CuSTe 固溶体(0.02 ≤ x ≤ 0.06),然后转变为六方 CuSTe 固溶体(0.08 ≤ x ≤ 0.1)。六方 CuTe 在六方 CuS 基体中的相分离发生在 0.3 ≤ x ≤ 0.7,最终在 x = 1 时形成六方 CuTe。由于能带结构的变化和共存的 CuS 和 CuTe 相,所有 CuSTe(0 < x < 1)合金的功率因子都得到了极大的提高。同时,Te/S 原子取代引入的点缺陷增强了声子散射,导致大多数这些固溶体的晶格热导率降低。因此,CuSTe 在 723 K 时表现出 1.18 的最大 ZT 值,与原始 CuS(0.32)和 CuTe(0.08)相比,分别提高了 3.7 倍和 14.8 倍。