Zhong Jinxuan, Yang Xiaoyu, Lyu Tu, Liang Gege, Zhang Shengnan, Zhang Chaohua, Ao Weiqin, Liu Fusheng, Nan Pengfei, Ge Binghui, Hu Lipeng
College of Materials Science and Engineering, Shenzhen Key Laboratory of Special Functional Materials, Guangdong Research Center for Interfacial Engineering of Functional Materials, Guangdong Provincial Key Laboratory of Deep Earth Sciences and Geothermal Energy Exploitation and Utilization, Institute of Deep Earth Sciences and Green Energy, Shenzhen University, Shenzhen 518060, China.
Information Materials and Intelligent Sensing Laboratory of Anhui Province, Key Laboratory of Structure and Functional Regulation of Hybrid Materials of Ministry of Education, Institutes of Physical Science and Information Technology, Anhui University, Hefei 230601, China.
Sci Bull (Beijing). 2024 Apr 30;69(8):1037-1049. doi: 10.1016/j.scib.2024.02.015. Epub 2024 Feb 12.
In thermoelectrics, doping is essential to augment the figure of merit. Traditional strategy, predominantly heavy doping, aims to optimize carrier concentration and restrain lattice thermal conductivity. However, this tactic can severely hamper carrier transport due to pronounced point defect scattering, particularly in materials with inherently low carrier mean-free-path. Conversely, dilute doping, although minimally affecting carrier mobility, frequently fails to optimize other vital thermoelectric parameters. Herein, we present a more nuanced dilute doping strategy in GeTe, leveraging the multifaceted roles of small-size metal atoms. A mere 4% CuPbSbTe introduction into GeTe swiftly suppresses rhombohedral distortion and optimizes carrier concentration through the aid of Cu interstitials. Additionally, the formation of multiscale microstructures, including zero-dimensional Cu interstitials, one-dimensional dislocations, two-dimensional planar defects, and three-dimensional nanoscale amorphous GeO and CuGeTe precipitates, along with the ensuing lattice softening, contributes to an ultralow lattice thermal conductivity. Intriguingly, dilute CuPbSbTe doping incurs only a marginal decrease in carrier mobility. Subsequent trace Cd doping, employed to alleviate the bipolar effect and align the valence bands, yields an impressive figure-of-merit of 2.03 at 623 K in (GeCdTe)(CuPbSbTe). This leads to a high energy-conversion efficiency of 7.9% and a significant power density of 3.44 W cm at a temperature difference of 500 K. These results underscore the invaluable insights gained into the constructive role of nuanced dilute doping in the concurrent tuning of carrier and phonon transport in GeTe and other thermoelectric materials.
在热电学中,掺杂对于提高优值至关重要。传统策略,主要是重掺杂,旨在优化载流子浓度并抑制晶格热导率。然而,这种策略会因明显的点缺陷散射而严重阻碍载流子传输,特别是在固有载流子平均自由程较低的材料中。相反,稀掺杂虽然对载流子迁移率影响最小,但常常无法优化其他重要的热电参数。在此,我们在GeTe中提出一种更细致入微的稀掺杂策略,利用小尺寸金属原子的多方面作用。仅向GeTe中引入4%的CuPbSbTe就能迅速抑制菱面体畸变,并借助铜间隙原子优化载流子浓度。此外,多尺度微观结构的形成,包括零维铜间隙原子、一维位错、二维平面缺陷和三维纳米级非晶GeO和CuGeTe析出物,以及随之而来的晶格软化,有助于实现超低的晶格热导率。有趣的是,稀CuPbSbTe掺杂仅使载流子迁移率略有下降。随后采用微量Cd掺杂来减轻双极效应并对齐价带,在(GeCdTe)(CuPbSbTe)中于623 K时获得了令人印象深刻的2.03的优值。这在500 K的温差下实现了7.9%的高能量转换效率和3.44 W/cm的显著功率密度。这些结果强调了在GeTe和其他热电材料中,细致入微的稀掺杂在同时调节载流子和声子传输方面所发挥的建设性作用,为我们提供了宝贵的见解。