Export citation

Export citation

Choose format for download:

Download Citation

    Essential role of lattice anharmonicity and coherent contributions in YAgTe2

    Yue Wang1,2, Yinchang Zhao2,*, Jun Ni3,4, and Zhenhong Dai2,5,†

    • *Contact author: y.zhao@ytu.edu.cn
    • †Contact author: zhdai@ytu.edu.cn

    Phys. Rev. B 113, 024309 – Published 16 January, 2026

    DOI: https://doi.org/10.1103/yfwy-wlq2

    Abstract

    The microscopic mechanisms of heat transport in YAgTe2 are explored through advanced first-principles calculations combined with self-consistent phonon theory. The computed normal mode resolved residuals display a characteristic W-shaped profile, indicating significant quartic anharmonicity. Both cubic and quartic anharmonicities are thoroughly considered, including their contributions to phonon frequency renormalization and linewidth broadening. Furthermore, both diagonal and off-diagonal components of the heat flux operator are explicitly evaluated in the calculation of lattice thermal conductivity. The results are in excellent agreement with experimental values near room temperature. Our study identifies the primary cause of the low lattice thermal conductivity in YAgTe2 as strong anharmonicity from the rattling effect of Ag atoms, which leads to substantial three-phonon and four-phonon scattering. Notably, the competition between phonon hardening (described by the loop diagram) and phonon softening (due to the bubble diagram) plays a significant role in influencing particlelike propagation, particularly affecting group velocity and energy conservation. We also confirm that YAgTe2 with space group P4¯21m remains dynamically stable at elevated temperatures. There are minor discrepancies between our high-temperature theoretical predictions and experimental results, which may be attributed to the presence of mixed phases in the experiments, whereas our calculations assume a perfect lattice. A reassessment of the thermoelectric performance shows that, for n-type doping, the maximum ZT of 2.11 is achieved at a carrier concentration of 9×1019cm3 at 700 K, while for p-type doping, the maximum ZT is 1.34 at a carrier concentration of 4×1019cm3 at 700 K. These findings provide valuable insights for guiding future experimental studies.

    Physics Subject Headings (PhySH)

    Authorization Required

    We need you to provide your credentials before accessing this content.

    Supplemental Material (Subscription Required)

    References (Subscription Required)

    Outline

    Information

    Sign In to Your Journals Account

    Filter

    Filter

    Article Lookup

    Enter a citation