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Gate-controlled topological conducting channels in bilayer graphene

2015/09/30 by Jing Li, J. Li, K. Wang +13 · 6 citations
Materials Science · Physics and Astronomy · #Ballistic conduction #Berry connection and curvature #Bilayer graphene #Condensed matter physics #Electron #Geometric phase #Graphene #Graphene research and applications #Magnetic field #Physics #Point reflection #Position and momentum space #Quantum and electron transport phenomena #Quantum mechanics #Scattering #Topological Materials and Phenomena #Topological insulator #Topology (electrical circuits) #Translational symmetry #cond-mat.mes-hall

paper · pdf · doi:10.1038/nnano.2016.158

published as Nature Nanotechnology, 2016 · 39 pages

openalex publication_date 2016/08/26 · arxiv created 2016/11/01 · arxiv updated 2016/11/03 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

The existence of inequivalent valleys K and K' in the momentum space of two-dimensional hexagonal lattices provides a new electronic degree of freedom, the manipulation of which can potentially lead to new types of electronics, in analogy to the role played by electron spin. In materials with broken inversion symmetry, such as an electrically gated bilayer graphene, the momentum-space Berry curvature Ω carries opposite sign in the K and K' valleys. A sign reversal of Ω along an internal boundary of the sheet gives rise to counter-propagating one-dimensional conducting modes encoded with opposite valley indices. These metallic states are topologically protected against backscattering in the absence of valley-mixing scattering, and thus can carry current ballistically. In bilayer graphene, the reversal of Ω can occur at the domain wall of AB and BA stacked domains, or at the line junction of two oppositely gated regions. The latter approach can provide a scalable platform to implement valleytronic operations such as valves and waveguides, but is technically challenging to realize. Here we fabricate a dual-split-gate structure in bilayer graphene and demonstrate transport evidence of the predicted metallic states. They possess a mean free path of up to a few hundred nanometers in the absence of a magnet field. The application of perpendicular magnetic field suppresses backscattering significantly and enables a 400-nanometer-long junction to exhibit conductance close to the ballistic limit of 4 e2/h at 8 Tesla. Our experiment paves the path to the realization of gate-controlled ballistic valley transport and the development of valleytronic applications in atomically thin materials.

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