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PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

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7.4 Percolation in Half-Spaces<br />

Percolation and Disordered Systems 209<br />

In the last section, we almost succeeded in proving that θ(pc) = 0 when<br />

d ≥ 3. The reason for this statement is as follows. Suppose θ(p) > 0 and<br />

η > 0. There is effectively defined in Section 7.3 an event A living in a finite<br />

box B such that<br />

(a) Pp(A) > 1 − ǫ, for some prescribed ǫ > 0,<br />

(b) the fact (a) implies that θ(p + η) > 0.<br />

Suppose that we could prove this with η = 0, and that θ(pc) > 0. Then<br />

Ppc(A) > 1 − ǫ, which implies by continuity that Pp ′(A) > 1 − ǫ for some<br />

p ′ < pc, and therefore θ(p ′ ) > 0 by (b). This would contradict the definition<br />

of pc, whence we deduce by contradiction that θ(pc) = 0.<br />

The fact that η is strictly positive is vital for the construction, since<br />

we need to ‘spend some extra money’ in order to compensate for negative<br />

information acquired earlier in the construction. In a slightly different setting,<br />

no extra money is required.<br />

Let H = {0, 1, . . . } × Z d−1 be a half-space when d ≥ 3, and write pc(H)<br />

for its critical probability. It follows from Theorem 7.8 that pc(H) = pc, since<br />

H contains slabs of all thicknesses. Let<br />

θH(p) = Pp(0 ↔ ∞ in H).<br />

Theorem 7.35. We have that θH(pc) = 0.<br />

The proof is not presented here, but may be found in [48, 49]. It is closely<br />

related to that presented in Section 7.3, but with some crucial differences.<br />

The construction of blocks is slightly more complicated, owing to the lack<br />

of symmetry of H, but there are compensating advantages of working in a<br />

half-space. For amusement, we present in Figure 7.10 two diagrams (relevant<br />

to the argument of [49]) depicting the necessary constructions.<br />

As observed in Section 3.3, such a conclusion for half-spaces has a striking<br />

implication for the conjecture that θ(pc) = 0. If θ(pc) > 0, then there exists<br />

a.s. a unique infinite open cluster in Z d , which is a.s. partitioned into (only)<br />

finite clusters by any division of Z d into two half-spaces.<br />

7.5 Percolation Probability<br />

Although the methods of Chapter 6 were derived primarily in order to study<br />

subcritical percolation, they involve a general inequality of wider use, namely<br />

g ′ �<br />

�<br />

n<br />

π (n) ≥ gπ(n)<br />

− 1<br />

gπ(i)<br />

� n<br />

i=0<br />

where gπ(n) = Pπ(0 ↔ ∂Sn); see equations (3.10) and (3.18) in Section 6.<br />

We argue loosely as follows. Clearly gπ(n) → θ(π) as n → ∞, whence (cross<br />

your fingers here)<br />

θ ′ � �<br />

1<br />

(π) ≥ θ(π) − 1<br />

θ(π)

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