Tuning a Circular p-n Junction in Graphene from Quantum Confinement to Optical Guiding

POSTER

Abstract

The photon-like propagation of the Dirac-electrons in graphene together with the record-high electronic mobility can lead to applications based on ultra-fast electronic response and low dissipation. But the chiral nature of the charge-carriers which is responsible for the high mobility also makes it difficult to control their motion and prevents electronic switching. Here we show how to manipulate the charge-carriers by using a circular p-n junction whose size can be continuously tuned from the nanometer to the micrometer scale. The junction size is controlled with a dual-gate device consisting of a planar back-gate and a point-like top-gate made by decorating an STM tip with an Au nanowire. The nanometer-scale junction is defined by a deep potential well created by the tip-induced charge. It traps the Dirac-electrons in quantum-confined states which are the graphene equivalent of the atomic collapse states predicted to occur at super-critically charged nuclei. As the junction size increases, the transition to the optical regime is signaled by the emergence of whispering-gallery modes1.

1Y. Jiang, et al, Nature Nanotechnology (2017) doi:10.1038/nnano.2017.181

Presenters

  • Yuhang Jiang

    Department of Physics and Astronomy, Rutgers University, Physics, Rutgers

Authors

  • Yuhang Jiang

    Department of Physics and Astronomy, Rutgers University, Physics, Rutgers

  • Jinhao Mao

    Department of Physics and Astronomy, Rutgers University

  • Dean Moldovan

    Departement Fysica, Universiteit Antwerpen

  • Massoud Ramezani Masir

    Department of Physics, University of Texas at Austin, Physics, University of Texas at Austin

  • Guohong Li

    Department of Physics and Astronomy, Rutgers University, Physics and Astronomy, Rutgers Univ, Physics and Astronomy, Rutgers University

  • Kenji Watanabe

    National Institute for Materials Science, NIMS, National Institute for Material Science, Advanced Materials Laboratory, National Institute for Materials Science, National Institute of Materials Science, Research Center for Functional Materials, National Institute for Materials Science, National Institute for Materials Science (NIMS, Advanced Materials Laboratory, NIMS, National Institute for Materials Science, Advanced Materials Laboratory, National Institue for Materials Science, National Institute of Material Science, National Institute for Matericals Science, Advanced Materials Laboratory, National Institute for Materials Science, 1-1 Namiki, Advanced materials laboratory, National institute for Materials Science, NIMS-Japan

  • Takashi Taniguchi

    National Institute for Materials Science, NIMS, National Institute for Material Science, Advanced Materials Laboratory, National Institute for Materials Science, National Institute of Materials Science, Research Center for Functional Materials, National Institute for Materials Science, National Institute for Materials Science (NIMS, Advanced Materials Laboratory, NIMS, National Institute for Materials Science, Advanced Materials Laboratory, National Institue for Materials Science, National Institute of Material Science, National Institute for Matericals Science, Advanced Materials Laboratory, National Institute for Materials Science, 1-1 Namiki, NIMS-Japan

  • François Peeters

    Departement Fysica, Universiteit Antwerpen, Department of Physics, University of Antwerp, University of Antwerp

  • Eva Andrei

    Department of Physics and Astronomy, Rutgers University, Physics and Astronomy, Rutgers Univ, Physics and Astronomy, Rutgers University, Department of Physics and Astronomy, Rutgers the State Univ of NJ New Brunswick