Role of irreducible occupancy sites on thermoelectric performance of Te-doped BiSbSe3

Q Qi-Zhuang Qu (School of Materials Science and Engineering, Hunan University of Science and Technology 1 , Xiangtan 411201,) Y Yu-Jia Zeng (School of Materials Science and Engineering and Hunan Provincial Key Laboratory of Advanced Materials for New Energy Storage and Conversion, Hunan University of Science and Technology 2 , Xiangtan 411201,) T Tao Li Y Yulou Ouyang (College of Physics and Electronic Engineering, Hengyang Normal University 2 , Hengyang 421002,) G Guo-Feng Xie (School of Materials Science and Engineering, Hunan University of Science and Technology 1 , Xiangtan 411201,) W Wu-Xing Zhou (School of Materials Science and Engineering and Hunan Provincial Key Laboratory of Advanced Materials for New Energy Storage and Conversion, Hunan University of Science and Technology 2 , Xiangtan 411201,)

Abstract

Doping can effectively modulate electron and phonon transport. However, the impact of symmetry-governed irreducible site occupancy remains unclear. In this work, we theoretically investigate the thermoelectric transport properties of Te-doped BiSbSe3 by considering phonon–phonon and electron–phonon scattering. Three irreducible Te-doping sites (S1–S3) are identified via the tree search algorithm. The results show that the three irreducible Te-doped sites have only a slight influence on the bandgap. However, the electron–phonon coupling exhibits site-selective modulation, resulting in up to twofold variations in electrical conductivity and electronic thermal conductivity. Additionally, lattice thermal conductivity decreases by 21%, 41%, and 54% along the c axis when Te atoms are doped at S1, S2, and S3, respectively. Notably, the optical phonon modes contribute over 50% to lattice thermal conductivity along the a axis in both pristine and doped structures, compared to 30% along other axes. Although all doping sites reduce lattice thermal conductivity, only S2 and S3 enhance thermoelectric performance. Specifically, zT values peak at 1.92 (S2) and 2.07 (S3), whereas S1 doping causes a 20%zT reduction due to carrier mobility loss. Our findings suggest that specific crystallographic doping site is essential for optimizing thermoelectric efficiency.

Article Details

Volume / Issue Vol. 138, Issue 9
Published September 07, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (6)

Q

Qi-Zhuang Qu

School of Materials Science and Engineering, Hunan University of Science and Technology 1 , Xiangtan 411201,

Y

Yu-Jia Zeng

School of Materials Science and Engineering and Hunan Provincial Key Laboratory of Advanced Materials for New Energy Storage and Conversion, Hunan University of Science and Technology 2 , Xiangtan 411201,

T

Tao Li

Y

Yulou Ouyang

College of Physics and Electronic Engineering, Hengyang Normal University 2 , Hengyang 421002,

G

Guo-Feng Xie

School of Materials Science and Engineering, Hunan University of Science and Technology 1 , Xiangtan 411201,

W

Wu-Xing Zhou

School of Materials Science and Engineering and Hunan Provincial Key Laboratory of Advanced Materials for New Energy Storage and Conversion, Hunan University of Science and Technology 2 , Xiangtan 411201,