PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT
PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT
PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT
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Percolation and Disordered Systems 269<br />
Lemma 13.20. Let 0 < p < 1 and q ≥ 1. For any non-empty increasing<br />
event A,<br />
d �<br />
log ψp(A)<br />
dp<br />
� ≥ ψp(FA)<br />
p(1 − p)<br />
where<br />
�<br />
�<br />
FA(ω) = inf<br />
e<br />
� ω ′ (e) − ω(e) � : ω ′ ≥ ω, ω ′ ∈ A<br />
Proof. It may be checked that FA1A = 0, and that N + FA is increasing.<br />
Therefore, by the FKG inequality,<br />
�<br />
.<br />
� �<br />
ψp(N1A) − ψp(N)ψp(A) = ψp (N + FA)1A − ψp(N)ψp(A)<br />
≥ ψp(FA)ψp(A).<br />
Now use Theorem 13.19. �<br />
The quantity FA is central to the proof of Theorem 13.17. In the proof,<br />
we shall make use of the following fact. If A is increasing and A ⊆ B1 ∩B2 ∩<br />
· · · ∩ Bm, where the Bi are cylinder events defined on disjoint sets of edges,<br />
then<br />
(13.21) FA ≥<br />
m�<br />
FBi.<br />
i=1<br />
Lemma 13.22. Let q ≥ 1 and 0 < r < s < 1. There exists a function<br />
c = c(r, s, q), satisfying 1 < c < ∞, such that<br />
and for all increasing events A.<br />
ψr(FA ≤ k) ≤ c k ψs(A) for all k ≥ 0<br />
Proof. We sketch this, which is similar to the so called ‘sprinkling lemma’ of<br />
[14]; see also [G, 167].<br />
Let r < s. The measures ψr and ψs may be coupled together in a natural<br />
way. That is, there exists a probability measure µ on Ω2 E = {0, 1}E × {0, 1} E<br />
such that:<br />
(a) the first marginal of µ is ψr,<br />
(b) the second marginal of µ is ψs,<br />
(c) µ puts measure 1 on the set of configurations (π, ω) ∈ Ω 2 E<br />
such that<br />
π ≤ ω.<br />
Furthermore µ may be found such that the following holds. There exists a<br />
positive number β = β(r, s, q) such that, for any fixed ξ ∈ ΩE and subset B<br />
of edges (possibly depending on ξ), we have that<br />
(13.23)<br />
µ � {(π, ω) : ω(e) = 1 for e ∈ B, π = ξ} �<br />
µ � {(π, ω) : π = ξ} � ≥ β|B| .