Giant Specific Power Generation Capacity of Micro‐Thermoelectric Generators Enabled by High‐Entropy Cocktail Strategy

Z Zhenyang Liu (Department of Chemistry) G Guannan Li J Jianting Dong (School of Physics and Wuhan National High Magnetic Field Center, Huazhong University of Science and Technology 1 , 430074 Wuhan,) X Xianlin Qu S Shipeng Zhou (Chongqing Key Laboratory of Micro&Nano Structure Optoelectronics School of Physical Science and Technology Southwest University Chongqing China) S Shuang Liu (Frontiers Science Center for Transformative Molecules, State Key Laboratory of Polyolefins and Catalysis, School of Chemistry and Chemical Engineering) D Deshun Hong (Department of Applied Physics and Center of Quantum Materials and Devices Chongqing University Chongqing China) J Jia Zhang Z Zhongchang Wang Y Young Sun (Department of Applied Physics, Chongqing University 1 , Chongqing 401331,) Y Yuming Lu (Chongqing Key Laboratory of Micro&Nano Structure Optoelectronics School of Physical Science and Technology Southwest University Chongqing China)

Abstract

ABSTRACT Specific power generation capacity Γ P is a critical performance metric for micro‐thermoelectric generators ( μ ‐TEGs), yet the best reported values are constrained to a few hundred µW cm −2 K −2 . Here, we report a giant Γ P of ∼5000 µW cm −2 K −2 in μ ‐TEGs based on the anomalous Nernst effect (ANE) in medium‐entropy (FeCoNi) 100‐ x Pt x films. Leveraging the high‐entropy cocktail strategy, we have simultaneously achieved a large anomalous Nernst thermopower S xy (>1.4 µV K −1 ) and low resistivity ρ xx (<85 µΩ cm), and suppressed the classical and quantum size effects on both S xy and ρ xx at the optimal composition of x ≈ 50 and film thickness of a few nanometers, enabling the record‐high Γ P . The underlying mechanism arises from cocktail‐driven modulation of energy‐band smearing, density of states, and Berry curvature at the Fermi surface, resulting in an ultrashort carrier mean‐free‐path of ∼3 nm, an ultrahigh carrier density of ∼10 23 cm −3 , and a large anomalous Nernst conductivity above 1.7 A m −1 K −1 . This claim is further supported by first‐principles calculations, which collectively highlight the experimental and theoretical potential of utilizing such materials for high‐performance μ ‐TEG applications.

Article Details

Volume / Issue Vol. 38, Issue 13
Published March 01, 2026
ISSN 0935-9648
Publisher Unknown Publisher

Journal Info

Advanced Materials

Unknown Publisher

ISSN: 0935-9648 Physical Sciences

Authors (11)

Z

Zhenyang Liu

Department of Chemistry

G

Guannan Li

J

Jianting Dong

School of Physics and Wuhan National High Magnetic Field Center, Huazhong University of Science and Technology 1 , 430074 Wuhan,

X

Xianlin Qu

S

Shipeng Zhou

Chongqing Key Laboratory of Micro&Nano Structure Optoelectronics School of Physical Science and Technology Southwest University Chongqing China

S

Shuang Liu

Frontiers Science Center for Transformative Molecules, State Key Laboratory of Polyolefins and Catalysis, School of Chemistry and Chemical Engineering

D

Deshun Hong

Department of Applied Physics and Center of Quantum Materials and Devices Chongqing University Chongqing China

J

Jia Zhang

Z

Zhongchang Wang

Y

Young Sun

Department of Applied Physics, Chongqing University 1 , Chongqing 401331,

Y

Yuming Lu

Chongqing Key Laboratory of Micro&Nano Structure Optoelectronics School of Physical Science and Technology Southwest University Chongqing China