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    Silicon spin vacuum: Isotopically enriched silicon-on-insulator28 and silicon28 from ultrahigh fluence ion implantation

    Shao Qi Lim1,2,*, Brett C. Johnson2, Sergey Rubanov3, Nico Klingner4, Bin Gong5, Alexander M. Jakob1, Danielle Holmes6, David N. Jamieson1, Jim S. Williams7 et al.

    Jeffrey C. McCallum1

    • 1Centre for Quantum Computation and Communication Technology, School of Physics, The University of Melbourne, Parkville, Victoria, Australia
    • 2School of Science, RMIT University, Melbourne, Victoria, Australia
    • 3Ian Holmes Imaging Centre, Bio21 Institute, The University of Melbourne, Melbourne, Victoria, Australia
    • 4Helmholtz-Zentrum Dresden-Rossendorf (HZDR), Institute of Ion Beam Physics and Materials Research, Dresden, Germany
    • 5Mark Wainwright Analytical Centre, UNSW Sydney, New South Wales, Australia
    • 6Centre for Quantum Computation and Communication Technology, School of Electrical Engineering and Telecommunications, UNSW Sydney, New South Wales, Australia
    • 7Research School of Physics, The Australian National University, Canberra ACT, Australia

    • *Contact author: qi.lim@rmit.edu.au

    Phys. Rev. Materials 9, 076202 – Published 8 July, 2025

    DOI: https://doi.org/10.1103/787r-9jps

    Abstract

    Isotopically enriched silicon (Si) can greatly enhance qubit coherence times by minimizing naturally occurring Si29 which has a nonzero nuclear spin. Ultrahigh fluence Si28 ion implantation of bulk natural Si substrates was recently demonstrated as an attractive technique to ultrahigh Si28 isotopic purity. In this work, we apply this Si28 enrichment process to produce Si28 and Si28-on-insulator (SOI) samples. Experimentally, we produced a Si28 sample on natural Si substrate with Si29 depleted to 7 ppm (limited by measurement noise floor) that is at least 100 nm thick. This is achieved with an ion energy that results in a sputter yield of less than one and an ultrahigh ion fluence, as supported by our improved computational model that is based on fitting a large number of experiments. Further, our model predicts the Si29 and Si30 depletion in our sample to be less than 1 ppm. In the case of SOI, ion implantation conditions are found to be more stringent than those of bulk natural Si in terms of minimizing threading dislocations upon subsequent solid phase epitaxy annealing. Finally, we do not observe open volume defects in our SOI28 and Si28 samples after SPE annealing (620∘C, 10 min).

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