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Realisation of topological zero-energy mode in bilayer graphene in zero magnetic field

机译:零磁场下双层石墨烯中拓扑零能量模式的实现

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摘要

Bilayer graphene (BLG) gapped by a vertical electric field represents a valley-symmetry-protected topological insulating state. Emergence of a new topological zero-energy mode has been proposed in BLG at a boundary between regions of inverted band gaps induced by two oppositely polarized vertical electric fields. However, its realisation has been challenged by the enormous difficulty in arranging two pairs of accurately aligned split gates on the top and bottom surfaces of clean BLG. Here we report realisation of the topological zero-energy mode in ballistic BLG, with zero-bias differential conductance close to the ideal value of 4 e 2/h (e is the electron charge and h is Planck’s constant) along a boundary channel between a pair of gate-defined inverted band gaps. This constitutes the bona fide electrical-gate-tuned generation of a valley-symmetry-protected topological boundary conducting channel in BLG in zero magnetic field, which is essential to valleytronics applications of BLG.
机译:垂直电场造成的双层石墨烯(BLG)表示受谷对称性保护的拓扑绝缘状态。在BLG中已经提出了在两个相反极化的垂直电场引起的反向带隙区域之间的边界处的新的拓扑零能量模式的出现。然而,在干净的BLG的顶部和底部表面上布置两对精确对准的分栅时,存在巨大的困难,挑战了其实现。在这里,我们报告了弹道BLG中零拓扑差模电导的实现,零偏微分电导接近理想值4 e 2 / h(e是电子电荷,h是普朗克常数)沿着一对栅极定义的反向带隙之间的边界通道。这构成了在零磁场中在BLG中谷底对称性保护的拓扑边界传导通道的真正电门调谐生成,这对于BLG的Valleytronics应用至关重要。

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