Porous Bi <sub>2</sub> S <sub>3</sub> Bulk With Excellent Thermoelectric Performance by Solid States Replacement and Low Melting‐Point Metal Volatilization

Z Zi‐Yuan Wang (Faculty of Material Science and Engineering and National &amp; Local Joint Engineering Laboratory of Advanced Metal Solidification Forming and Equipment Technology Kunming University of Science and Technology Kunming China) J Jun Guo Y Yi‐Xin Zhang (Faculty of Material Science and Engineering and National &amp; Local Joint Engineering Laboratory of Advanced Metal Solidification Forming and Equipment Technology Kunming University of Science and Technology Kunming China) H Hao Liang (Institute of Carbon Neutrality) X Xing Yang (College of Chemistry, Jilin Province Research Center for Engineering and Technology of Spectral Analytical Instruments, Jilin University, Qianjin Street 2699, Changchun 130012, China) R Rafal E. Dunin‐Borkowski (Ernst Ruska‐Centre for Microscopy and Spectroscopy with Electrons Forschungszentrum Jülich Jülich Germany) F Fengshan Zheng (Spin‐X Institute School of Physics and Optoelectronics State Key Laboratory of Luminescent Materials and Devices Guangdong‐Hong Kong‐Macao Joint Laboratory of Optoelectronic and Magnetic Functional Materials South China University of Technology Guangzhou China) L Lei Jin J Jing Feng Z Zhen‐Hua Ge (Faculty of Material Science and Engineering and National &amp; Local Joint Engineering Laboratory of Advanced Metal Solidification Forming and Equipment Technology Kunming University of Science and Technology Kunming China)

Abstract

Abstract Bismuth sulfide (Bi 2 S 3 ) exhibits potentials in thermoelectric field, due to their environmental friendliness, high Seebeck coefficients, and low thermal conductivity. However, the peak ZT for binary Bi 2 S 3 does not exceed 1.0, inhibiting its practical applications. Starting from the precipitation smelting of bismuth concentrate process, this study constructs multi‐type, multi‐scale in‐situ secondary phases and porous structures through FeCoNi (FCN) medium‐entropy alloy addition, significantly enhancing the ZT value of Bi 2 S 3 ‐based thermoelectric materials. The introduced FCN reacts with pre‐synthesized Bi 2 S 3 nanorod matrix during spark plasma sintering and forms precipitate complex with FCN‐S core and Bi shell microstructures. FCN doping improves the carrier concentration of Bi 2 S 3 and the reduced Bi from Bi 2 S 3 acts as carrier transport channels for mobility optimization. Due to the stacking effect of Bi 2 S 3 nanorods and the volatile nature of metallic Bi, porous Bi 2 S 3 structure is formed, characterized by randomly‐distributed and micro‐to‐nanoscale pores. The coexistence of various lattice defects effectively scatter phonons and suppress the lattice thermal conductivity, thus an excellent peak ZT of 1.1 is achieved at 773 K in a 0.25 wt.% FCN‐doped Bi 2 S 3 sample. This study, drawing on the process of ore smelting, proposes a convenient method for preparing high‐performance chalcogenide thermoelectric materials with porous structures.

Article Details

Volume / Issue Vol. 38, Issue 11
Published February 01, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (10)

Z

Zi‐Yuan Wang

Faculty of Material Science and Engineering and National &amp; Local Joint Engineering Laboratory of Advanced Metal Solidification Forming and Equipment Technology Kunming University of Science and Technology Kunming China

J

Jun Guo

Y

Yi‐Xin Zhang

Faculty of Material Science and Engineering and National &amp; Local Joint Engineering Laboratory of Advanced Metal Solidification Forming and Equipment Technology Kunming University of Science and Technology Kunming China

H

Hao Liang

Institute of Carbon Neutrality

X

Xing Yang

College of Chemistry, Jilin Province Research Center for Engineering and Technology of Spectral Analytical Instruments, Jilin University, Qianjin Street 2699, Changchun 130012, China

R

Rafal E. Dunin‐Borkowski

Ernst Ruska‐Centre for Microscopy and Spectroscopy with Electrons Forschungszentrum Jülich Jülich Germany

F

Fengshan Zheng

Spin‐X Institute School of Physics and Optoelectronics State Key Laboratory of Luminescent Materials and Devices Guangdong‐Hong Kong‐Macao Joint Laboratory of Optoelectronic and Magnetic Functional Materials South China University of Technology Guangzhou China

L

Lei Jin

J

Jing Feng

Z

Zhen‐Hua Ge

Faculty of Material Science and Engineering and National &amp; Local Joint Engineering Laboratory of Advanced Metal Solidification Forming and Equipment Technology Kunming University of Science and Technology Kunming China