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    Parity Breaking and Sublattice Dichotomy in Monolayer FeSe Superconductor

    Cui Ding1,2,*, Zhipeng Xu3,4,*, Xiaotong Jiao1, Yinqi Hu1, Wenxuan Zhao1, Lexian Yang1,5, Kun Jiang3,4,†, Lili Wang1,5,‡, Jin-Feng Jia2,6,7 et al.

    Jiangping Hu3,8,§ and Qi-Kun Xue1,2,5,6,∥

    • *These authors contributed equally to this work.
    • †Contact author: jiangkun@iphy.ac.cn
    • ‡Contact author: liliwang@tsinghua.edu.cn
    • §Contact author: jphu@iphy.ac.cn
    • ∥Contact author: qkxue@tsinghua.edu.cn

    Phys. Rev. Lett. 136, 066502 – Published 11 February, 2026

    DOI: https://doi.org/10.1103/f3w1-rn6p

    Abstract

    A unit cell represents the smallest repeating structure in solid-state physics and serves as the fundamental building block of a material. In iron-based superconductors, each unit cell contains two iron atoms, which form two sublattices in the two-dimensional iron layers. Under normal circumstances, these sublattices are expected to have identical physical properties due to space inversion symmetry. However, we discover that this sublattice structure can introduce a novel degree of freedom for probing unconventional pairing mechanisms in iron-based superconductors. We observe distinct dual tunneling spectra within the pairing gap energy corresponding to the two sublattices in the monolayer FeSe with atomically homogeneous (1×1) structures on SrTiO3(001) substrates—a phenomenon we term sublattice dichotomy. This dichotomy can be quantitatively explained by a parity-breaking superconducting state, characterized by the coexistence of conventional pairing and interband odd-parity pairing. The interband singlet pairing arises due to the lack of inversion symmetry, which is naturally broken from the interface coupling between the FeSe and TiO2 layer.

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