Intrinsic Ultralow Lattice Thermal Conductivity in the Full-Heusler Compound Ba2AgSb

Shao-Fei Wang, Zhi-Gang Zhang, Bao-Tian Wang, Jun-Rong Zhang, and Fang-Wei Wang
Phys. Rev. Applied 17, 034023 – Published 8 March 2022

Abstract

Full-Heusler thermoelectric materials have intrinsically low lattice thermal conductivity. Our first-principles calculations show that Ba2AgSb is a semiconductor with an indirect band gap of 0.49 eV. The electronic band degeneracy and pockets near the Fermi level facilitate electron transport. The short phonon relaxation time, small group velocity (1.89 km s1), and large phonon scattering space reflect the intense phonon-phonon scattering. The large Grüneisen parameter (1.44) accounts for the strong phonon anharmonicity, thus the low lattice thermal conductivity of 0.5Wm1K1 at 800 K. The isotropic figure of merit with a maximum value of 4.7 at 750 K is comparable to that of reported materials. The distribution of phonon momentum uncovers the important role of Ag in resisting thermal transport. The analysis of symmetry-based phonon-phonon scattering routes reveals the significance of symmetry on phonon scattering. The crystal structure of Ba2AgSb can be used to regulate chemical elements to build high-performance thermoelectric materials. Our calculations provide an effective way to design thermoelectric materials, stimulating the study of full-Heusler materials.

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  • Received 9 May 2021
  • Revised 30 November 2021
  • Accepted 7 February 2022

DOI:https://doi.org/10.1103/PhysRevApplied.17.034023

© 2022 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Shao-Fei Wang1,2,3, Zhi-Gang Zhang4,5, Bao-Tian Wang1,2, Jun-Rong Zhang1,2,3,*, and Fang-Wei Wang2,3,4,5,†

  • 1Institute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049, China
  • 2Spallation Neutron Source Science Center (SNSSC), Dongguan 523803, China
  • 3School of Nuclear Sciences and Technology, University of Chinese Academy of Sciences, Beijing 100049, China
  • 4Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100080, China
  • 5Songshan Lake Materials Laboratory, Dongguan 523808, China

  • *jrzhang@ihep.ac.cn
  • fwwang@iphy.ac.cn

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Vol. 17, Iss. 3 — March 2022

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