PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT
PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT
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.