April 7 - 11, 2025
Seattle, Washington
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2025 MRS Spring Meeting & Exhibit
SF01.18.05

Excellent Thermoelectric Performance of Bi2MO4Cl (M = Y, La, and Bi) Derived from Ultra-Low Lattice Thermal Conductivity Due to Weak Ionic Bonding

When and Where

Apr 11, 2025
4:30pm - 4:45pm
Summit, Level 3, Room 348

Presenter(s)

Co-Author(s)

Shipeng Bi1,Alexander Squires2,Christopher Savory2,Kieran Spooner2,Dan Han3,David Scanlon2

University College London1,University of Birmingham2,Jilin University3

Abstract

Shipeng Bi1,Alexander Squires2,Christopher Savory2,Kieran Spooner2,Dan Han3,David Scanlon2

University College London1,University of Birmingham2,Jilin University3
Oxides are considered potential candidates for thermoelectric materials due to their high temperature stability in air, low toxicity, and ease of synthesis.1 However, the thermoelectric figure of merit (ZT) of discovered oxides is still significantly lower compared to conventional thermoelectric materials such as Bi2Te3 and PbTe. In this work, we predicted the thermoelectric performance of visible light photocatalysts Bi2MO4Cl (M = Y, La, and Bi)2 by first-principles calculations based on density functional theory (DFT). The results show that Bi3O4Cl and Bi2LaO4Cl exhibit ultra-low average lattice thermal conductivities of less than 0.3 W m-1 K-1 at 1000 K, which is mainly attributed to the presence of heavy atoms, weak ionic bonding, and strong phonon anharmonicity. In addition, the weak ionic bonding significantly inhibits out-of-plane heat transfer, resulting in the lattice thermal conductivity in the out-of-plane direction being the lowest compared to other directions. As a result, the p-type maximum average ZT of Bi3O4Cl reaches 2.2 at 1000 K, which is comparable to that of polycrystalline SnSe,3 and the p-type maximum ZT of Bi2LaO4Cl exceeds 4 in the out-of-plane direction. These results not only illustrate the intrinsic mechanism for the excellent thermoelectric performance of Bi2MO4Cl (M = Y, La, and Bi), but also provide theoretical insights for further experimental exploration.

References
1 K. Brlec, K. B. Spooner, J. M. Skelton and D. O. Scanlon, J. Mater. Chem. A, 2022, 10, 16813-16824.
2 A. Nakada, D. Kato, R. Nelson, H. Takahira, M. Yabuuchi, M. Higashi, H. Suzuki, M. Kirsanova, N. Kakudou, C. Tassel; et al., J. Am. Chem. Soc., 2021, 143, 2491-2499.
3 J. Liu, P. Wang, M. Y. Wang, R. Xu, J. Zhang, J. Z. Liu, D. Li, N. N. Liang, Y. W. Du, G. Chen; et al., Nano Energy, 2018, 53, 683-689.

Keywords

electrical properties | thermal conductivity | thermoelectricity

Symposium Organizers

Yee Kan Koh, National University of Singapore
Zhiting Tian, Cornell University
Tianli Feng, University of Utah
Hyejin Jang, Seoul National University

Session Chairs

Eleonora Isotta
Yanguang Zhou

In this Session