(a) Where the errors sit on the cubeMass of the uniform cube by Hamming distance from the center of the worst-case error set: a bump of width ½√n around n/2. By Harper's inequality the error set that expands least is a ball (carmine); r is that ball's radius. It sits just left of n/2 because almost every string lies at distance ≈ n/2 ± √n from the ball's center: a ball holding only an α fraction of the cube must stop cα√n short of the peak — so its radius is already almost n/2. Allowing d extra flips grows it layer by layer; because all the mass is concentrated in an O(√n) band, a few √n layers swallow nearly everything. Blue: inputs with no error within d flips.
dimension n
error rate α
flips d
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(b) Fraction of inputs with a nearby errorThe coverage curve: the fraction of all inputs lying within d bit flips of the worst-case error set, plotted against d in units of √n. It rises from α to essentially 1 over a constant number of √n steps — the “nearby errors” theorem. (Shown is the exact Harper lower bound, discarding at most one partial layer.)
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coverage –
d = –