Single‐Atom and 1 nm Cluster Co‐Modified Thermoelectrics

Y Yezhen Hua (School of Chemistry and Chemical Engineering Nanjing University of Science and Technology Nanjing China) J Ji‐Chang Ren (Nano and Heterogeneous Materials Center School of Materials Science and Engineering Nanjing University of Science and Technology Nanjing China) B Bassem A. Al‐Maythalony (Material Discovery Research Unit Advanced Research Center Royal Scientific Society Amman Jordan) W Wei Zhao P Pengfei Xu H Hao Yang T Tianyu Deng M Molly Meng‐Jung Li (Department of Applied Physics The Hong Kong Polytechnic University Hong Kong China) C Cailing Chen (State Key Laboratory of Inorganic Synthesis and Preparative Chemistry, College of Chemistry, Jilin University, Qianjin Street 2699, Changchun 130012, P. R. China) G Gang Sha X Xiyang Wang (Department of Applied Physics) B Biao Xu

Abstract

ABSTRACT The size‐dependent electronic and phononic configurations of single atoms and nanoclusters enable tailored functionalities. Their synergistic effects also attract attention, yet precise control of anti‐aggregation states during high‐temperature operations poses formidable challenges in multiple fields such as fuel cells and thermoelectrics. Herein, we develop a solution‐processed strategy to precisely incorporate Pt species as isolated atoms (Pt 1 ) and sub‐nanoclusters (Pt n , ∼1 nm) in Bi 2 S 3 . Notably, Pt n of 1 nm size exhibit significant advantages over larger‐size counterparts in tuning electronic structure and optimizing charge transfer. Furthermore, Pt 1 and Pt n scatter 1 Å‐ to 1 nm‐ wavelength phonon that is conventionally underexplored. The 1 nm Pt n exhibits distinct force constant as compared to 3 nm Pt n , leading to ultra‐strong phonon Rayleigh scattering, which in turn significantly reduces thermal conductivity. The optimized Bi 2 S 3 ‐Pt 1 /Pt n composite achieves breakthrough thermoelectric performance, attaining a maximum zT of 1.02 at 773 K and single‐leg conversion efficiency of 1.58%, both setting benchmarks for Bi 2 S 3 systems. This strategy can also be extended to other thermoelectric material systems such as Bi 0.4 Sb 1.6 Te 3 , PbTe, or other fields including solid‐state batteries and solar cells.

Article Details

Volume / Issue Vol. 65, Issue 10
Published March 02, 2026
ISSN 1433-7851
Publisher Wiley

Journal Info

Angewandte Chemie International Edition

Wiley

ISSN: 1433-7851 Physical Sciences

Authors (12)

Y

Yezhen Hua

School of Chemistry and Chemical Engineering Nanjing University of Science and Technology Nanjing China

J

Ji‐Chang Ren

Nano and Heterogeneous Materials Center School of Materials Science and Engineering Nanjing University of Science and Technology Nanjing China

B

Bassem A. Al‐Maythalony

Material Discovery Research Unit Advanced Research Center Royal Scientific Society Amman Jordan

W

Wei Zhao

P

Pengfei Xu

H

Hao Yang

T

Tianyu Deng

M

Molly Meng‐Jung Li

Department of Applied Physics The Hong Kong Polytechnic University Hong Kong China

C

Cailing Chen

State Key Laboratory of Inorganic Synthesis and Preparative Chemistry, College of Chemistry, Jilin University, Qianjin Street 2699, Changchun 130012, P. R. China

G

Gang Sha

X

Xiyang Wang

Department of Applied Physics

B

Biao Xu