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Electrical control of the g-tensor of the first holein a silicon MOS quantum dot

ORAL

Abstract

The spin state of a single hole in a semiconductor device provides a promising platform for a wide range of spin based quantum devices. A primary advantage of using holes, rather than electrons, is the intrinsically strong coupling of hole spins to electric fields. This strong spin-electric coupling allows rapid all-electrical control over the hole spin state, which is advantageous for many spin based devices, such as spin qubits [1-2]. However, due to the complexity of hole spin physics, gaps remain in our understanding of the mechanisms that enable electrical control of hole spins.

 

In this work, we report measurements and simulations of the g-tensor of a single hole that is confined in a silicon planar MOS quantum dot [3]. We show that thermal contraction of the metal gates in this MOS device produces a non-uniform strain profile, resulting in nanometre-scale variations in the hole-spin character. We show that local electric fields can be used to displace the hole relative to the non-uniform strain profile, therefore allowing a new mechanism for electric modulation of the hole g-tensor. Using this mechanism, we demonstrate tuning of the hole g-factor by up to 500%. In addition, we observe a potential sweet spot where dg_(110)/dV = 0, offering a possible configuration to suppress spin decoherence caused by electrical noise [4]. These results open a path towards a previously unexplored technology: engineering of non-uniform strains to optimise spin-based devices

 

[1] - Maurand, R., et al. Nature communications 7.1 (2016): 1-6.

[2] - Hendrickx, Nico W., et al. Nature 591.7851 (2021): 580-585.

[3] - Liles, S. D., et al. arXiv preprint arXiv:2012.04985 (2020).

[4] - Wang, Zhanning, et al. npj Quantum Information 7.1 (2021): 1-8

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Publication: https://arxiv.org/abs/2012.04985

Presenters

  • Scott D Liles

    University of New South Wales

Authors

  • Scott D Liles

    University of New South Wales

  • Frederico Martins

    University of New South Wales

  • Dmitry Miserev

    University of Basel

  • Andrey A Kiselev

    HRL Laboratories, LLC

  • Ian Thorvaldson

    University of New South Wales, Centre of Excellence for Quantum Computation and Communication Technology, School of Physics, University of New South Wales, Sydney, New South Wales 2052, Australia

  • Matthew J Rendell

    University of New South Wales

  • Ikkyeong Jin

    University of New South Wales

  • Fay E Hudson

    University of New South Wales, Centre for Quantum Computation and Communication Technology, School of Electrical Engineering and Telecommunications, UNSW Sydney, New South Wales 2052, Australia.

  • Menno Veldhorst

    Delft University of Technology

  • Kohei M Itoh

    Keio Univ, School of Fundamental Science and Technology, Keio University, Kohoku-ku, Yokohama, Japan., Keio University

  • Oleg P Sushkov

    University of New South Wales

  • Thaddeus D Ladd

    HRL Laboratories, LLC, HRL Laboratories

  • Andrew S Dzurak

    University of New South Wales, Centre for Quantum Computation and Communication Technology, School of Electrical Engineering and Telecommunications, UNSW Sydney, New South Wales 2052, Australia.

  • Alex R Hamilton

    University of New South Wales