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Unconventional superconductivity in twisted bilayer WSe2

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arxiv 2405.14784 v1 pith:GCMZYHQP submitted 2024-05-23 cond-mat.mes-hall cond-mat.str-elcond-mat.supr-con

classification cond-mat.mes-hallcond-mat.str-elcond-mat.supr-con
keywords superconductivitymoirflatmaterialsbandsstrongbandbilayer
verification ladder T0 review T1 audit T2 compute T3 formal
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Moir\'e materials have enabled the realization of flat electron bands and quantum phases that are driven by strong correlations associated with flat bands. Superconductivity has been observed, but solely, in graphene moir\'e materials. The absence of robust superconductivity in moir\'e materials beyond graphene, such as semiconductor moir\'e materials, has remained a mystery and challenged our current understanding of superconductivity in flat bands. Here, we report the observation of robust superconductivity in 3.65-degree twisted bilayer WSe2 which hosts a honeycomb moir\'e lattice. Superconductivity emerges at half-band filling and under small sublattice potential differences, where the moir\'e band is a flat Chern band. The optimal superconducting transition temperature is about 220 mK and constitutes 2% of the effective Fermi temperature; the latter is comparable to the value in high-temperature cuprate superconductors and suggests strong pairing. The superconductor borders on two distinct metals below and above half-band filling; it undergoes a continuous transition to a correlated insulator by tuning the sublattice potential difference. The observed superconductivity on the verge of Coulomb-induced charge localization suggests roots in strong electron correlations.

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Cited by 3 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Charged moir\'e phonons in twisted bilayer graphene

    cond-mat.mes-hall 2026-01 conditional novelty 6.0 of 10

    In doped twisted bilayer graphene, moiré phonons—particularly the phason—become infrared active, with the phason carrying exactly one electron per moiré cell of doping and giving a Drude-like THz response.

  2. Doping-induced Quantum Anomalous Hall Crystals and Topological Domain Walls

    cond-mat.str-el 2024-07 unverdicted novelty 6.0 of 10

    Doping the Kane-Mele-Hubbard model at filling ν=1 induces quantum anomalous Hall crystals with skyrmion spin textures and topological domain walls hosting chiral modes.

  3. Emergent Quantum Valley Hall Insulator from Electron Interactions in Transition-Metal Dichalcogenide Heterobilayers

    cond-mat.mes-hall 2025-12 unverdicted novelty 5.0 of 10

    Long-range electron interactions in MoTe2/WSe2 heterobilayers at filling v=2 generate a robust Quantum Valley Hall Insulator, with competition between s-wave and p±ip-wave states and a Zeeman-field-induced Quantum Ano...

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