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    Low-energy gap associated with the anomalous symmetry-breaking states in CsV3Sb5

    Jiahao Hao1,2,*, Xiaoxiang Zhou2,*, Yongkai Li3,4,*, Zhe Liu2, Bingke Ji2, Yaomin Dai2,†, Zhiwei Wang3,4,‡, and Hai-Hu Wen2,§

    • 1State Key Laboratory of Metastable Materials Science and Technology & Hebei Key Laboratory of Microstructural Material Physics, School of Science, Yanshan University, Qinhuangdao 066004, China
    • 2National Laboratory of Solid State Microstructures and Department of Physics, Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China
    • 3Key Laboratory of Advanced Optoelectronic Quantum Architecture and Measurement, Ministry of Education, School of Physics, Beijing Institute of Technology, Beijing 100081, China
    • 4Micronano Center, Beijing Key Lab of Nanophotonics and Ultrafine Optoelectronic Systems, Beijing Institute of Technology, Beijing 100081, China

    • *These authors contributed equally to this work.
    • †Contact author: ymdai@nju.edu.cn
    • ‡Contact author: zhiweiwang@bit.edu.cn
    • §Contact author: hhwen@nju.edu.cn

    Phys. Rev. B 113, 035128 – Published 15 January, 2026

    DOI: https://doi.org/10.1103/z1nj-32tq

    Abstract

    Several anomalous symmetry-breaking states have been reported at temperatures well below the charge-density wave (CDW) transition in CsV3Sb5. Whether these states are concomitant with an electronic structure change remains elusive. Here, we present a study of the optical properties of CsV3Sb5 in the CDW state. In addition to the CDW gap, which opens below TCDW = 91 K, a conspicuous suppression of the optical conductivity develops around 200 cm−1 below T*≃50K, indicating the opening of another low-energy gap well below the CDW transition. A detailed Drude-Lorentz analysis manifests that, similar to the CDW gap, this low-energy gap also opens in the saddle-point bands with V−3d character near the M point. Our experimental results not only reveal a Fermi surface reconstruction coinciding with the emergence of the anomalous symmetry-breaking states, but also underline the importance of the V−3d orbitals in driving these anomalous states in CsV3Sb5.

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