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PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

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xk(i, j)<br />

Percolation and Disordered Systems 235<br />

y<br />

B<br />

y ′<br />

Ik(i, j)<br />

Fig. 10.2. A diagram of the region Tk(i, j), with the points Yk(i, j) marked. The<br />

larger box is an enlargement of the box B on the left. In the larger box appear open<br />

paths of the sort required for the corresponding event Eu, where y = yu. Note that<br />

the two smaller boxes within B are joined to the surface of B, and that any two such<br />

connections are joined to one another within B.<br />

Write L(u, v) for the set of vertices lying within euclidean distance √ 3 of<br />

the line segment of R 3 joining u to v. Let a > 0. Define the region<br />

where<br />

Tk(i, j) = Ak(i, j) ∪ Ck(i, j)<br />

Ak(i, j) = B(ak) + L � xk(i, j), Ik(i, j) �<br />

Ck(i, j) = B(ak) + �<br />

L � Ik(i, j), x � .<br />

x∈Ik(i,j)<br />

See Figure 10.2.<br />

Within each Tk(i, j) we construct a set of vertices as follows. In Ak(i, j)<br />

we find vertices y1, y2, . . . , yt such that the following holds. Firstly, there<br />

exists a constant ν such that t ≤ ν3 k for all k. Secondly, each yu lies in<br />

Ak(i, j),<br />

(10.7) yu ∈ L � xk(i, j), Ik(i, j) � , 1<br />

3 ak ≤ δ(yu, yu+1) ≤ 2<br />

3 ak<br />

for 1 ≤ u < t, and furthermore y1 = xk(i, j), and |yt − Ik(i, j)| ≤ 1.<br />

Likewise, for each x ∈ Ik(i, j), we find a similar sequence y1(x), y2(x), . . . ,<br />

yv(x) satisfying (10.7) with xk(i, j) replaced by x, and with y1(x) = yt,<br />

yv(x) = x, and v = v(x) ≤ ν3 k .<br />

The set of all such y given above is denoted Yk(i, j). We now construct<br />

open paths using Yk(i, j) as a form of skeleton. Let 0 < 7b < a. For 1 ≤ u < t,<br />

let Eu = Eu(k, i, j) be the event that<br />

(a) there exist z1 ∈ yu + B(bk) and z2 ∈ yu+1 + B(bk) such that zi ↔<br />

yu + ∂B(ak) for i = 1, 2, and<br />

(b) any two points lying in {yu, yu+1} + B(bk) which are joined to yu +<br />

∂B(ak) are also joined to one another within yu + ∂B(ak).<br />

y<br />

B<br />

y ′

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