The standard conclusion from the optical flow restriction equation (OFCE, slide 5 of your reference) is that "your movement should be less than a pixel, the less they kill you." Although technically true, you can overcome this in practice by using large, medium-sized windows. This requires you to perform normal statistics, i.e. Not purely the smallest square value as suggested in the slides. Similarly, faster calculations and better results can be achieved by regularizing Tikhonov. This requires setting the setting value (Tikhonov constant). This can be done as a global constant, or allowed to be adjusted for local information in the image (for example, Shi-Tomashi trust, the so-called determinant of the structure tensor).
Note that this does not replace the need for multiscale approaches to deal with large movements. It can slightly expand the range that any single scale can handle.
Implementations, visualizations, and code are available in the tutorial format here, although in Matlab there is no Python.
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