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    Optical Signatures of −13 Fractional Quantum Anomalous Hall State in Twisted MoTe2

    Haiyang Pan1,2,*, Shunshun Yang1,3,*, Yuzhu Wang2,*, Xiangbin Cai1,2,*, Wei Wang4, Yan Zhao1,2, Kenji Watanabe5, Takashi Taniguchi6, Linlong Zhang3 et al.

    Youwen Liu3, Bo Yang2,†, and Weibo Gao1,2,7,8,‡

    • *These authors contributed equally to this work.
    • †Contact author: yang.bo@ntu.edu.sg
    • ‡Contact author: wbgao@ntu.edu.sg

    Phys. Rev. Lett. 136, 056601 – Published 3 February, 2026

    DOI: https://doi.org/10.1103/f4dj-7sts

    Abstract

    The discovery of fractional charge excitations in new platforms offers crucial insights into strongly correlated quantum phases. While a range of fractional quantum anomalous Hall (FQAH) states have recently been observed in two-dimensional twisted moire systems, the theoretically anticipated filling factor ν=−1/3 FQAH state has remained elusive, with debates centering on its nature of charge density wave or a topological Chern insulator. Here, we report the optical detection of a ν=−1/3 FQAH state in twisted MoTe2 bilayers. Using photoluminescence and reflective magnetic circular dichroism techniques, we identify ferromagnetic states at filling factors ν=−1, −2/3, and −1/3, all tunable by a vertical electric field. The corresponding Curie temperatures are approximately 11, 3.5, and 2.4 K, respectively. The −1/3 state emerges over a narrower electric field range and a lower temperature compared to the integer and other fractional states, indicating a fragile nature that may have led to its absence in previous reports. Notably, the photoluminescence spectra at ν=−1/3 disperse as the out-of-plane magnetic field increases, consistent with a nontrivial topological origin. Theoretical calculations based on the exact diagonalization method further support the interpretation of this topologically nontrivial state.

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