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    Holes in silicon are heavier than expected: Transport properties of extremely high mobility electrons and holes in silicon MOSFETs

    J. P. Wendoloski1, J. Hillier1, S. D. Liles1, M. J. Rendell1, Y. Ashlea-Alava1, B. Raes2, R. Li2,*, S. Kubicek2, C. Godfrin2 et al.

    J. Jussot2, S. Beyne2, D. Wan2, Md. M. Rahman3, S. Yianni3,4,†, K. W. Chan3,4, F. E. Hudson3,4, W. H. Lim3,4, K. De Greve2,5, A. S. Dzurak3,4, and A. R. Hamilton1,‡

    • 1School of Physics, University of New South Wales, New South Wales 2052, Australia
    • 2IMEC, Remisebosweg 1, B-3001 Leuven, Belgium
    • 3School of Electrical Engineering and Telecommunications, University of New South Wales, New South Wales 2052, Australia
    • 4Diraq, Sydney, New South Wales, Australia
    • 5Department of Electrical Engineering (ESAT), KU Leuven, Leuven, Belgium

    • *Now at Applied Materials, Inc., Santa Clara, CA 95054, United States of America.
    • †Now at Université Grenoble Alpes, CEA, Grenoble INP, IRIG, PHELIQS.
    • ‡Contact author: alex.hamilton@unsw.edu.au

    Phys. Rev. B 113, 045302 – Published 26 January, 2026

    DOI: https://doi.org/10.1103/g29w-st3q

    Abstract

    The quality of the silicon-oxide interface plays a crucial role in fabricating reproducible silicon spin qubits. In this work we characterize interface quality by performing mobility measurements on silicon Hall bars. We find a peak electron mobility of nearly 40000cm2/Vs in a device with a 21nm oxide layer, and a peak hole mobility of about 2000cm2/Vs in a device with 8nm oxide, the latter being the highest recorded mobility for a p-type silicon MOSFET. Despite the high device quality, we note an order-of-magnitude difference in mobility between electrons and holes. By studying additional n-type and p-type devices with identical oxides, and fitting to transport theory, we show that this mobility discrepancy is due to valence band nonparabolicity. The nonparabolicity endows holes with a density-dependent transverse effective mass ranging from 0.6m0 to 0.7m0, significantly larger than the usually quoted band-edge mass of 0.22m0. Finally, we perform magnetotransport measurements to extract electron momentum and quantum scattering lifetimes.

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