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    High-pressure structures of Bi0.5Sb1.5Te3 at room temperature and in its superconducting states

    C. Halbert1,*, A. Lamichhane2, B. Wang3,†, S. Racioppi4, N. P. Salke2, R. Kumar2, A. H. Manayil Marathamkottil1, H. Farraj1,‡, K. Wang2 et al.

    E. H. T. Poldi2, M. Ahart2, Z. Liu2, D. J. Schulze5, Shaowei Song5, X. Shi5, Zhifeng Ren5, Y. Meng6, G. Konstantin7, R. D. dos Reis8, R. Tartaglia8, L. Z. Deng5, C. W. Chu5, E. Zurek3, and R. J. Hemley1,2,9,10

    • *Contact author: chalbe3@uic.edu
    • †Present address: State Key Laboratory of Metastable Materials Science and Technology & Key Laboratory for Microstructural Material Physics of Hebei Province, School of Science, Yanshan University, Qinhuangdao, Hebei 066004, China.
    • ‡Present address: Deutsches Elektronen-Synchrotron (DESY), 22607 Hamburg, Germany.

    Phys. Rev. Materials 10, 094804 – Published 25 September, 2026

    DOI: https://doi.org/10.1103/ks5f-s1hm

    Abstract

    Post-transition metal and metalloid chalcogenides can have a wide range of unique and valuable properties. Bi0.5Sb1.5Te3 (BST) is part of a family of materials that exhibit multiple functionalities, including thermoelectricity, superconductivity, and electronic topological transitions at high pressure. We have studied the phase transition sequence and equation of state of BST under pressures up to 54 GPa at ambient temperature and 32.5 GPa in the superconducting states using x-ray diffraction. At ambient conditions, BST crystallizes in a hexagonal R3¯m structure and undergoes three structural phase transitions, forming monoclinic C2/m, C2/c, and cubic Im3¯m structures, at 11, 16, and 25 GPa, respectively. Low-temperature diffraction experiments reveal that the superconducting states of BST share the same structures as their room-temperature counterparts. Although the x-ray diffraction clearly indicates that the electronic charge density distribution of the highest-pressure phase has Im3¯m space group symmetry, the symmetry of the underlying atomic lattice depends on the extent of order-disorder of the nuclei. Candidate partially ordered lower symmetry structures of the high-pressure phase are examined in the DFT calculations.

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