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PDF (double-sided) - Physics Department, UCSB - University of ...

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6.1.2 Scanning Electron Microscopy<br />

Optical microscopes quickly reach their limitations if the feature sizes drop<br />

into the nm range.<br />

Things like step coverage or the quality <strong>of</strong> the insulating<br />

barrier or even surface roughness at more detailed levels cannot be resolved with<br />

an optical microscope. The reason for this is the finite wavelength <strong>of</strong> light. This<br />

finite wavelength gives photons a “size” <strong>of</strong> several hundred nanometers, making it<br />

impossible to resolve features smaller than this size without distortion to the image<br />

due to interference effect. To circumvent this limit, a different type <strong>of</strong> microscope<br />

can be used that is known as an SEM (Scanning Electron Microscope). As the<br />

name suggests, this microscope does not use optical photons to probe the surface,<br />

but a beam <strong>of</strong> electrons that is reflected <strong>of</strong>f the sample. The small size <strong>of</strong> the<br />

electrons allows for magnifications up to 250, 000×, which is sufficient to, for<br />

example, look at the pr<strong>of</strong>ile <strong>of</strong> the 2 nm oxide barrier inside the qubit junction.<br />

The use <strong>of</strong> electrons requires the sample to be conductive so that it can reflect the<br />

electrons efficiently. Commonly, non-conductive samples are therefore first covered<br />

with a thin layer <strong>of</strong> gold. The images generated by the SEM can naturally not<br />

preserve the color <strong>of</strong> the sample.<br />

107

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