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Layer-engineered quantum anomalous Hall effect in twisted rhombohedral graphene
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Layer-engineered quantum anomalous Hall effect in twisted rhombohedral graphene
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Realizing programmable topological states in quantum anomalous Hall (QAH) insulators requires the ability to design and dynamically tune their topological invariant, the Chern number C. Here, we report a designer QAH platform based on twisted rhombohedral graphene family, in which C becomes a programmable and electrically tunable degree of freedom. By engineering the layer configuration in twisted monolayer-rhombohedral N-layer graphene, denoted as (1+N)L, we realize QAH states with C=N at moire filling v=1, where the layer number N=3,4,5 directly sets the Chern number. Beyond such static layer programming, we demonstrate in-situ electrical control. In a twisted monolayer-trilayer device, the sign of C (chirality) can be switched by electrostatic doping or displacement field. Most strikingly, in twisted Bernal bilayer-rhombohedral tetralayer graphene denoted as (2+4)L, we drive a displacement-field-induced topological phase transition between two distinct QAH states with C=3 and C=4 in a single device. Our work establishes a layer-engineered and electrically tunable platform that transitions topological quantum matter from discovery to design, opening the way toward on-demand engineering of correlated topological states and reconfigurable topological electronics.
Forward citations
Cited by 3 Pith papers
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Flat-Band Stoner Instability and Peierls-Phase Origin of the Transdimensional Anomalous Hall Effect in Rhombohedral Graphite
Microscopic Hartree-Fock theory attributes transdimensional AHE in rhombohedral graphite to Stoner-driven valley polarization modulated by Peierls phase and orbital magnetism.
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Engineering electrically-switchable quantum anomalous Hall states by spin-orbit coupling
Proximity to WSe2 engineers the magnetic energy landscape in tMBG via induced SOC, enabling nonvolatile gate switching of QAH states and gate tuning between |C|=2, |C|=1, and metallic regimes without magnetic reset.
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Tunable high-Chern-number Chern insulators in rhombohedral tetralayer graphene/hBN moir\'e superlattices
New symmetry-broken Chern insulators with C = +3, ±2, ±1 at v = -2.5 or -2.6, plus the known C = -4 at v = -1, were observed in rhombohedral tetralayer graphene/hBN moiré superlattices and shown to be tunable via twis...
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