For donor number density , the mean separation is of order . A donor-state overlap estimate sets this scale comparable with the effective radius:
Relative to the atomic density, this is , about parts per million. If “start to overlap” is defined geometrically by centre separation , the estimate is instead , about parts per million. Thus the geometric estimate is of order –. Real donor wavefunctions have tails, not hard orbit edges, so this does not define a sharp threshold or by itself locate a metal-insulator transition.

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