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    Identification of the I10 donor in ZnO as a Sn-Li complex with large hyperfine interaction

    Xingyi Wang1, Sai Mu2,3, Yaser Silani4, Jeong Rae Kim5,6, Ethan R. Hansen4, J. K. Nangoi3, Lasse Vines7, Joseph Falson5,6, Chris G. Van de Walle3 et al.

    Kai-Mei C. Fu1,4,8,*

    • *Contact author: kaimeifu@uw.edu

    Phys. Rev. B 114, 225417 – Published 23 October, 2026

    DOI: https://doi.org/10.1103/bmh2-l3cy

    Abstract

    Donor impurities in wide direct band gap semiconductors provide a promising platform for spin-photon quantum technologies by combining a donor spin qubit with optically addressable transitions. In ZnO, the shallow donor with the largest reported binding energy has long been associated with the I10 bound exciton line, but its microscopic origin has remained unresolved. Here we demonstrate the controlled formation and identification of this donor as a Sn-Li complex through a combination of ion implantation, annealing, optical spectroscopy, and first-principles calculations. Resonant two-laser coherent population trapping measurements reveal an electron–Sn119 hyperfine interaction of 392±15MHz, establishing a coupled electron-spin-1/2, nuclear-spin-1/2 system with one of the largest hyperfine couplings reported for shallow donors in semiconductors. Density functional theory calculations show that a nearest-neighbor SnZn−LiZn complex has favorable formation energetics, donor character with the electron localized on Sn, and an extrapolated hyperfine interaction consistent with experiment. The large donor binding energy and excited-state structure indicate enhanced thermal robustness of the optical transition relative to conventional group-III donors, while the strong hyperfine interaction enables fast electron-nuclear spin control and prospects for direct nuclear-spin-photon interfaces. We further observe efficient optically induced nuclear spin polarization, highlighting a path toward nuclear spin initialization. More broadly, our results reveal how a donor-acceptor complex can access previously unexplored regimes of shallow donor physics, extending the design space of donor quantum defects beyond isolated substitutional dopants.

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