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PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

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252 <strong>Geoffrey</strong> Grimmett<br />

Fig. 11.1. Three stages in the construction of the ‘random Cantor set’ C. At each<br />

stage, a square is replaced by a 3×3 grid of smaller squares, each of which is retained<br />

with probability p.<br />

Theorem 11.3. Let p > 1<br />

9 . The Hausdorff dimension of C, conditioned on<br />

the event {C �= ∅}, equals a.s. log(9p)/ log 3.<br />

Rather than prove this in detail, we motivate the answer. The set C is<br />

covered by Xk squares of side-length ( 1<br />

3 )k . Therefore the δ-dimensional box<br />

measure Hδ(C) satisfies<br />

Hδ(C) ≤ Xk3 −kδ .<br />

Conditional on {C �= ∅}, the random variables Xk satisfy<br />

log Xk<br />

k<br />

→ log µ as k → ∞, a.s.<br />

where µ = 9p is the mean family-size of the branching process. Therefore<br />

which tends to 0 as k → ∞ if<br />

Hδ(C) ≤ (9p) k(1+o(1)) 3 −kδ<br />

δ > log(9p)<br />

log 3 .<br />

It follows that the box dimension of C is (a.s.) no larger than log(9p)/ log3.<br />

Experts may easily show that this bound for the dimension of C is (a.s.)<br />

exact on the event that C �= ∅ (see [130, 184, 312]).<br />

Indeed the exact Hausdorff measure function of C may be ascertained (see<br />

[152]), and is found to be h(t) = td 1 1− (log | log t|) 2 d where d is the Hausdorff<br />

dimension of C.<br />

a.s.

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