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With a truly insulating bulk, the potential profile is set by the charge at the sample edges (Ref. 27). AFM would be unable to measure the potential in this limit, because no charge would be able to migrate under the tip in the time scale of the measurement. Our measurements are not in this limit: we have (Formula presented) at (Formula presented) allowing us to operate even on the QH plateaus.
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With a truly insulating bulk, the potential profile is set by the charge at the sample edges (Ref. 27). AFM would be unable to measure the potential in this limit, because no charge would be able to migrate under the tip in the time scale of the measurement. Our measurements are not in this limit: we have (Formula presented) at (Formula presented) allowing us to operate even on the QH plateaus.
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