High-temperature quantum valley Hall effect with quantized conductance at zero magnetic field

ORAL

Abstract

Topological edge states offer an excellent platform to study 1D physics and develop functional elements for quantum electronics. Achieving a robust conductance quantization, the hallmark of ballistic transport, is challenging for helical edge states. Previous work from our lab [1-2] has demonstrated that Bernal-stacked bilayer graphene supports the quantum valley Hall effect through electrically defined band inversion, and the resulting topological edge channel, namely the kink states, can perform the operations of a valley valve, waveguide and tunable beam splitter. In this talk, I'll discuss our recent effort to achieve quantized resistance plateaus at zero magnetic field by improving device quality. The resistance plateau is wide in gate sweeps and remains constant as the temperature changes from mK to Kelvins. It changes by only 1% at 12 K and 3% at 46 K, due to the activation of bulk conduction. We demonstrate the operation of a topological switch toggling between conductance 0 and 4e2/h by controlling the existence/absence of the kink states. The excellent ballisticity and maneuverability of the kink states make it a good candidate for developing a quantum interconnect network.

[1] Li. et al., Nat. Nano. 11, 1060 (2016), [2] Li et al., Science 362, 1149 (2018)

* NSF: NSF/DMR-1904986 DOE: DE-SC0022947

Presenters

  • Ke Huang

    Pennsylvania State University

Authors

  • Ke Huang

    Pennsylvania State University

  • Hailong Fu

    Pennsylvania State University

  • Kenji Watanabe

    National Institute for Materials Science, NIMS, Research Center for Electronic and Optical Materials, National Institute for Materials Science, Research Center for Functional Materials, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan, National Institute for Material Science

  • Takashi Taniguchi

    Kyoto Univ, National Institute for Materials Science, Research Center for Materials Nanoarchitectonics, Research Center for Materials Nanoarchitectonics, National Institute for Materials Science, National Institute for Materials Sciences, NIMS, International Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan, National Institute for Material Science, International Center for Materials Nanoarchitectonics, NIMS, Japan, International Center for Materials Nanoarchitectonics, Tsukuba, National Institue for Materials Science, Kyoto University, National Institute of Materials Science, International Center for Materials Nanoarchitectonics and National Institute for Materials Science

  • Jun Zhu

    Penn State University