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    Pressure-induced structural transitions and dome-shaped superconductivity in the topological insulator PbBi6Te10

    JunYing Hu1, GuangYang Dai2, Liang Ma2,3, JingKai Bi2,*, JianYong Chen2,†, and ZhiWei Men4,‡

    • 1Institute of Physics, Henan Academy of Sciences, Zhengzhou 450046, China
    • 2Institute of Quantum Materials and Physics, Henan Academy of Sciences, Zhengzhou 450046, China
    • 3Key Laboratory of Materials Physics, Ministry of Education, School of Physics, Zhengzhou University, Zhengzhou 450001, China
    • 4Key Laboratory of Physics and Technology for Advanced Batteries of Ministry of Education, College of Physics, Jilin University, Changchun 130012, China

    • *Contact author: bijk@hnas.ac.cn
    • †Contact author: chenjy@hnas.ac.cn
    • ‡Contact author: zwmen@jlu.edu.cn

    Phys. Rev. B 114, 024103 – Published 14 July, 2026

    DOI: https://doi.org/10.1103/rgb8-bsw1

    Abstract

    Topological insulators (TIs) constitute a unique class of quantum materials owing to their topology-protected electron states. While pressure is an effective way to induce superconductivity in TIs, superconductivity often appears after phase transition or structural disorder. Therefore, identifying systems in which superconductivity emerges at relatively low-pressure regions within a well-defined topological structure is desirable. In this work, it was demonstrated that PbBi6Te10 undergoes two structural transitions from R−3m to C2/m and subsequently to disordered Im−3m structure under high pressure. Superconductivity emerged at 0.9 GPa and reached a maximum transition temperature of 8.8 K at 4.2 GPa within the initial structural phase, forming a dome-shaped phase diagram. First-principles calculations revealed that the bands remained topologically nontrivial under 4.0 GPa. These results establish PbBi6Te10 as a platform for exploring the interplay between pressure-induced superconductivity and nontrivial topological states.

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