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PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

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172 <strong>Geoffrey</strong> Grimmett<br />

Proof of Theorem 5.1. Assume that µ satisfies (5.2), and let f and g be<br />

increasing functions. By adding a constant to the function g, we see that it<br />

suffices to prove (5.3) under the extra hypothesis that g is strictly positive.<br />

We assume this holds. Define positive probability measures µ1 and µ2 on<br />

(ΩE, FE) by µ2 = µ and<br />

g(ω)µ(ω)<br />

µ1(ω) = �<br />

ω ′ g(ω′ )µ(ω ′ )<br />

for ω ∈ ΩE.<br />

Since g is increasing, (5.6) follows from (5.2). By Holley’s inequality,<br />

which is to say that<br />

µ1(f) ≥ µ2(f),<br />

�<br />

ω f(ω)g(ω)µ(ω)<br />

�<br />

ω ′ g(ω′ )µ(ω ′ )<br />

�<br />

≥ f(ω)µ(ω)<br />

as required. �<br />

5.2 Disjoint Occurrence<br />

Van den Berg has suggested a converse to the FKG inequality, namely that,<br />

for some interpretation of the binary operation ◦,<br />

Pp(A ◦ B) ≤ Pp(A)Pp(B) for all increasing events A, B.<br />

The correct interpretation of A◦B turns out to be ‘A and B occur disjointly’.<br />

We explain this statement next.<br />

As usual, E is a finite set, ΩE = {0, 1} E , and so on. For ω ∈ ΩE, let<br />

K(ω) = {e ∈ E : ω(e) = 1},<br />

so that there is a one–one correspondence between configurations ω and sets<br />

K(ω). For increasing events A, B, let<br />

�<br />

A ◦ B =<br />

ω : for some H ⊆ K(ω), we have that ω ′ ∈ A and ω ′′ ∈ B,<br />

where K(ω ′ ) = H and K(ω ′′ ) = K(ω) \ H<br />

and we call A ◦ B the event that A and B occur disjointly.<br />

The canonical example of disjoint occurrence in percolation theory concerns<br />

the existence of disjoint open paths. If A = {u ↔ v} and B = {x ↔ y},<br />

then A ◦ B is the event that are two edge-disjoint paths, one joining u to v,<br />

and the other joining x to y.<br />

ω<br />

�<br />

,

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