The recent experimental discovery of the fractional quantum spin Hall effect in twisted bilayer MoTe₂ at a twist angle of 2.1 degrees highlights the unique properties of its second moir\'e band. Inspired by this finding, we conduct a comprehensive theoretical investigation of the half-filled second moir\'e band at this angle, utilizing an effective continuum model. Our analysis reveals that the band not only exhibits characteristics akin to the first Landau level, K=∫BZd²k\:tr\:η(k) ≈ 3, but also that its projected Coulomb interaction strikingly mirrors the Haldane pseudopotentials of the first Landau level. They together strongly indicate the potential emergence of a non-Abelian fractional quantum anomalous Hall state at the half-filling under the Coulomb interactions. By performing exact diagonalization calculations, we validate this hypothesis and construct a global phase diagram around this non-Abelian fractional quantum anomalous Hall states. We also introduce a novel metric of 1LL-ness of a band, which quantitatively measures the alignment of the projected Coulomb interaction with the Haldane pseudopotentials in Landau levels. This metric is then compared with the global phase diagram including the non-Abelian fractional quantum anomalous Hall state, revealing its utility in predicting the parameter region of the 1LL-ness. Finally, we discuss the potential implications on experiments.
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Ahn et al. (2024) studied this question.
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