Enhanced thermoelectric properties of the topological phase of monolayer HfC

Abstract Thermoelectric properties of a topological insulator, monolayer HfC, are calculated using first-principles calculation, which accounts for the two contributions from edge and bulk states. By applying strain up to 8% along the a axis, the monolayer HfC shows the topological phase while it is in a non-topological state without strain. The figure of merit, ZT , for the topological phase becomes two-ordered magnitude larger ( ZT ∼ 2) because of larger electric conductivity than that of the non-topological phase due to edge current. The total Seebeck coefficient S , and ZT have maximum values when the chemical potential is located at the highest energy of the edge state. The peak of ZT comes from the fact that the product of divergent S and quickly-decreasing electric conductivity above the highest energy of the edge state. We further optimize S and ZT by changing the sample size and temperature.

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Publication Details

Journal
Chinese Physics B
Published
2025-03-06
DOI
https://doi.org/10.1088/1674-1056/adbd17
Citations
4
Primary Topic
Advanced Thermoelectric Materials and Devices
Type
article
Field-Weighted Citation Impact
2.07
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article

Enhanced thermoelectric properties of the topological phase of monolayer HfC

Baojuan Dong, Huaihong Guo, Wei‐Jiang Gong, Riichiro Saito et al.
4 citations
Chinese Physics B
Advanced Thermoelectric Materials and Devices
2.07
article

Enhanced thermoelectric properties of the topological phase of monolayer HfC

Baojuan Dong, Huaihong Guo, Wei‐Jiang Gong, Riichiro Saito, Nisar Muhammad, Teng Yang, Nguyen Tuan Hung, Wenlong Mu, Zhidong Zhang
article en
4 citations

Abstract

Abstract Thermoelectric properties of a topological insulator, monolayer HfC, are calculated using first-principles calculation, which accounts for the two contributions from edge and bulk states. By applying strain up to 8% along the a axis, the monolayer HfC shows the topological phase while it is in a non-topological state without strain. The figure of merit, ZT , for the topological phase becomes two-ordered magnitude larger ( ZT ∼ 2) because of larger electric conductivity than that of the non-topological phase due to edge current. The total Seebeck coefficient S , and ZT have maximum values when the chemical potential is located at the highest energy of the edge state. The peak of ZT comes from the fact that the product of divergent S and quickly-decreasing electric conductivity above the highest energy of the edge state. We further optimize S and ZT by changing the sample size and temperature.

Chinese Physics BVol. 34(5)
University of Science and Technology of China (CN), Hefei National Center for Physical Sciences at Nanoscale (CN)
Openalex Percentile: Top 14%
Advanced Thermoelectric Materials and Devices
2.07
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