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Observation of Ferromagnetic Phase in the Second Moir\'e Band of Twisted MoTe2

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arxiv 2407.13674 v1 pith:A5TL4DYH submitted 2024-07-18 cond-mat.mes-hall

classification cond-mat.mes-hall
keywords moirphasebandstatestmote2dopingsecondbands
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Flat bands and electron correlation in moir\'e lattices give rise to many exotic phases, including Mott insulators, superconductivity, and topological states. Within the first moir\'e band, integer and fractional quantum anomalous Hall effects have been observed in twisted bilayer MoTe2 (tMoTe2) at one hole doping and fractional doping per moir\'e unit cell, respectively. When the second moir\'e band is fully hole doped, quantum spin Hall insulator has also been reported in tMoTe2 at a certain twist angle. Exotic topological states together with ferromagnetic (FM) states in the high moir\'e band can potentially exist as well. In this study, we report the observation of a FM phase in the second moir\'e band in tMoTe2. The FM phase can be tuned by both the doping level and displacement field. At filling around 2.58 holes per moir\'e unit cell, the FM phase reaches a Curie temperature of 3.5 K. A large displacement field can suppress the FM phase, like the FM phase at the filling of -1. Our results demonstrate the realization of time-reversal symmetry-breaking states in the higher moir\'e bands in tMoTe2.

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  1. A quantum geometric mechanism for chiral domain wall metastability: Application to twisted transition-metal dichalcogenides

    cond-mat.str-el 2026-08 conditional novelty 8.0 of 10

    Chiral domain walls in conjugate Chern bands bind a dipole density set by a geometric coefficient c_G, producing a metastable texture that explains long-lived excitations in twisted MoTe2.

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