Tunable Γ−Κ Valley Populations in Hole-Doped Trilayer WSe2

ORAL

Abstract

Semiconducting transition metal dichalcogenides (TMDs) exhibit thickness dependent bandstructures with the monolayers possessing a direct gap at the K points of the Brillouin zone. Beyond the monolayer limit, the TMD bandstructure becomes more complicated with the band extrema locations in few-layer TMDs remaining an open question for the vast majority of TMDs. Here, we address the valence band maxima locations in trilayer WSe2 using magnetotransport measurements in high-mobility, h-BN encapsulated, dual-gated samples. Shubnikov-de Haas oscillations evince holes populating two distinct subbands with effective masses m* = 0.5me belonging to the K valley, and m* = 1.2me belonging to the Γ valley of trilayer WSe2; me is the bare electron mass. At a fixed total hole density, the K and Γ occupations can be tuned by an applied transverse electric field (E), with Γ being the lowest energy state at low E-field and K being the lowest energy state at high E-field. Ab-initio calculations support these findings and explain the shift of the valence band maxima, and the consequent transfer of holes from Γ to K with increasing E-field.

Presenters

  • Hema Movva

    The University of Texas at Austin, Univ of Texas, Austin

Authors

  • Hema Movva

    The University of Texas at Austin, Univ of Texas, Austin

  • Timothy Lovorn

    The University of Texas at Austin

  • Babak Fallahazad

    The University of Texas at Austin

  • Stefano Larentis

    The University of Texas at Austin

  • Kyounghwan Kim

    The University of Texas at Austin

  • 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

  • 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

  • Sanjay Banerjee

    Electrical and Computer Engineering, University of Texas at Austin, Univ of Texas, Austin, The University of Texas at Austin

  • Allan MacDonald

    Physics department, University of Texas at Austin, Physics, University of Texas, Austin, Department of Physics, The University of Texas at Austin, Physics , Univ of Texas, Austin, Univ of Texas at Austin, Physics, The University of Texas at Austin, Department of Physics, Univerisity of Texas at Austin, The University of Texas at Austin, University of Texas

  • Emanuel Tutuc

    The University of Texas at Austin, Department of Electrical and Computer Engineering, The University of Texas at Austin, Univ of Texas, Austin, Electrical and Computer Engineering, The University of Texas at Austin