Spins in defects in solid state systems provide a versatile platform for quantum information, with applications such as quantum computing, sensing and communication. Defects in silicon carbide (SiC) in particular have been found to combine long-lived, controllable quantum defects with mature growth technology developed by the SiC high power electronics industry.

In any given defect, multiple charge state configurations are possible, but only one of those offers the correct spin properties needed for quantum information. Being able to control the charge state is therefore a pre-requirement to experiments in this system. 

Photoluminescence spectra of silicon carbide point defects under infrared and ultraviolet excitation. Multiple defect emission peaks are labeled for c-axis and basal orientations, showing enhanced optical response and charge-state dynamics under dual-wavelength excitation conditions.

In this study, we demonstrate control over the charge state of divacancies defects in 4H-SiC, where the neutral charge state provides the correct spin state and is optically bright (photoluminescent), enabling spin experiments. Using combinations of near-infrared and near-ultraviolet excitation from two light sources, we are able to convert the defect from this bright to another dark (non-photoluminescent) charge state.

Differential photoluminescence signal versus microwave frequency for implanted and bulk silicon carbide defects. The graph compares infrared-only and combined ultraviolet excitation, highlighting charge-state conversion and spin-dependent optical contrast in defect centers.

We measure enhancements of up to three orders of magnitude in the optical signal depending on the sample, facilitating the realization of any future experimental demonstration. For example, it is typical to implant defects in a sample to obtain spin qubits with a given concentration. Implantation however can locally damage the sample or change its Fermi level, resulting in defects being in the wrong (dark) charge state which cannot be observed. The application of the near-ultraviolet light in this case fully converted this implanted layer of defects, showing a narrow spin signal with millisecond coherence times, even under the illumination.

Charge-state imaging of silicon carbide vacancy defects showing spatial regions labeled I, M, and E with varying defect charge populations. The grayscale map and optical image illustrate controlled charge dynamics and defect-state distribution across the sample surface.

Finally, we demonstrated patterning of the defect charge state over large area of the sample. The charge conversion is persistent at cryogenic temperatures (5 K), therefore defects can locally be changed to either bright or dark, and then measured later. This may provide high-density storage of information.

Overall, these results provide a strong basis for all future quantum experiments using divacancy defects in SiC, as well as the possibility to use the charge state of these defects for alternative applications.

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To learn more about our studies, please refer to:

“Optical charge state control of spin defects in 4H-SiC”, Gary Wolfowicz, Christopher P. Anderson, Andrew L. Yeats, Samuel J. Whiteley, Jens Niklas, Oleg G. Poluektov, F. Joseph Heremans and David D. Awschalom. Nature Communications, 8:1876 (2017).