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Electron-Hole Crossover in Gate-Controlled Bilayer Graphene Quantum Dots.
Banszerus, L; Rothstein, A; Fabian, T; Möller, S; Icking, E; Trellenkamp, S; Lentz, F; Neumaier, D; Watanabe, K; Taniguchi, T; Libisch, F; Volk, C; Stampfer, C.
Afiliación
  • Banszerus L; JARA-FIT and 2nd Institute of Physics, RWTH Aachen University, 52074 Aachen, Germany, E.U.
  • Rothstein A; Peter Grünberg Institute (PGI-9), Forschungszentrum Jülich, 52425 Jülich, Germany, E.U.
  • Fabian T; JARA-FIT and 2nd Institute of Physics, RWTH Aachen University, 52074 Aachen, Germany, E.U.
  • Möller S; Institute for Theoretical Physics, TU Wien, 1040 Vienna, Austria, E.U.
  • Icking E; JARA-FIT and 2nd Institute of Physics, RWTH Aachen University, 52074 Aachen, Germany, E.U.
  • Trellenkamp S; Peter Grünberg Institute (PGI-9), Forschungszentrum Jülich, 52425 Jülich, Germany, E.U.
  • Lentz F; JARA-FIT and 2nd Institute of Physics, RWTH Aachen University, 52074 Aachen, Germany, E.U.
  • Neumaier D; Peter Grünberg Institute (PGI-9), Forschungszentrum Jülich, 52425 Jülich, Germany, E.U.
  • Watanabe K; Helmholtz Nano Facility, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Taniguchi T; Helmholtz Nano Facility, Forschungszentrum Jülich, 52425 Jülich, Germany.
  • Libisch F; AMO GmbH, Gesellschaft für Angewandte Mikro- und Optoelektronik, 52074 Aachen, Germany, E.U.
  • Volk C; University of Wuppertal, 42285 Wuppertal, Germany, E.U.
  • Stampfer C; Research Center for Functional Materials, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan.
Nano Lett ; 20(10): 7709-7715, 2020 Oct 14.
Article en En | MEDLINE | ID: mdl-32986437
ABSTRACT
Electron and hole Bloch states in bilayer graphene exhibit topological orbital magnetic moments with opposite signs, which allows for tunable valley-polarization in an out-of-plane magnetic field. This property makes electron and hole quantum dots (QDs) in bilayer graphene interesting for valley and spin-valley qubits. Here, we show measurements of the electron-hole crossover in a bilayer graphene QD, demonstrating opposite signs of the magnetic moments associated with the Berry curvature. Using three layers of top gates, we independently control the tunneling barriers while tuning the occupation from the few-hole regime to the few-electron regime, crossing the displacement-field-controlled band gap. The band gap is around 25 meV, while the charging energies of the electron and hole dots are between 3 and 5 meV. The extracted valley g-factor is around 17 and leads to opposite valley polarization for electrons and holes at moderate B-fields. Our measurements agree well with tight-binding calculations for our device.
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Texto completo: 1 Banco de datos: MEDLINE Idioma: En Revista: Nano Lett Año: 2020 Tipo del documento: Article

Texto completo: 1 Banco de datos: MEDLINE Idioma: En Revista: Nano Lett Año: 2020 Tipo del documento: Article