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    Classical Hall effect in scanning gate experiments

    A. Baumgartner*, T. Ihn, and K. Ensslin†

    G. Papp‡ and F. Peeters

    K. Maranowski and A. C. Gossard

    • Solid State Physics Laboratory, ETH Zurich, 8093 Zurich, Switzerland

    • Department of Physics, University of Antwerp, Groenenborgerlaan 171, B-2020 Antwerpen, Belgium

    • Materials Department, University of California, Santa Barbara, California 93106, USA

    • *Electronic address: baumgartner@phys.ethz.ch
    • †URL: http://www.nanophys.ethz.ch
    • ‡Permanent address: Department of Theoretical Physics, University of Szeged, Aradi vtk. tere 1, H-6720 Szeged, Hungary, and Institute of Physics, University of West Hungary, Bajcsy Zs. út 5-7, H-9400 Sopron, Hungary.

    Phys. Rev. B 74, 165426 – Published 30 October, 2006

    DOI: https://doi.org/10.1103/PhysRevB.74.165426

    Abstract

    Scanning gate experiments on a two-dimensional electron gas in the regime of the classical Hall effect are presented. The Hall resistance is recorded while tuning the local potential by applying a voltage to the metallic tip of a scanning force microscope. In diffusive samples and at zero magnetic field an intriguing Hall resistance pattern arises that is attributed to tip-induced inhomogeneous current flow. Measurements at small, i.e., nonquantizing, magnetic fields reveal an additional Hall resistance pattern due to the tip-induced inhomogeneous electron density in the Hall cross. Deviations of the measurements on higher-mobility samples from expectations based on symmetry arguments are used to distinguish the diffusive from the mesoscopic transport regime. Finite-element-method modeling for the diffusive regime and trajectory calculations for ballistic electrons allow a concise interpretation of the measurements.

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