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PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

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Percolation and Disordered Systems 243<br />

We now define bond percolation processes on L2 A and L2B . Assume p+ = 0.<br />

We present the rules for L2 A only; the rules for L2B are analogous. An edge of<br />

L2 1 1 1 1<br />

A joining (m − 2 , n − 2 ) to (m + 2 , n + 2 ) to declared to be open if there is<br />

a NE mirror at (m, n); similarly we declare the edge joining (m − 1 1<br />

2 , n + 2 )<br />

to (m + 1 1<br />

2 , n − 2 ) to be open if there is a NW mirror at (m, n). Edges which<br />

are not open are called closed. This defines percolation models on L2 A and<br />

L2 B in which north-easterly edges (resp. north-westerly edges) are open with<br />

probability pNE = 1<br />

2 (1 − prw) (resp. pNW = 1<br />

2 (1 − prw)). These processes are<br />

subcritical since pNE + pNW = 1 − prw < 1. Therefore, there exists (P-a.s.)<br />

no infinite open path in either L 2 A or L2 B<br />

, and we assume henceforth that no<br />

such infinite open path exists.<br />

Let N(A) (resp. N(B)) be the number of open circuits in L 2 A (resp. L2 B )<br />

which contain the origin in their interiors. Since the above percolation processes<br />

are subcritical, there exists (by Theorem 6.10) a strictly positive constant<br />

α = α(pNW, pNE) such that<br />

(10.14) �<br />

P x lies in an open cluster of L 2 A<br />

�<br />

of diameter at least n ≤ e −αn<br />

for all n,<br />

for any vertex x of L2 A . (By the diameter of a set C of vertices, we mean<br />

max{|y −z| : y, z ∈ C}.) The same conclusion is valid for L2 B . We claim that<br />

(10.15) P � 0 is a rw point, and N(A) = N(B) = 0 � > 0,<br />

and we prove this as follows. Let Λ(k) = [−k, k] 2 , and let Nk(A) (resp.<br />

Nk(B)) be the number of circuits contributing to N(A) (resp. N(B)) which<br />

contain only points lying strictly outside Λ(k). If Nk(A) ≥ 1 then there exists<br />

some vertex (m + 1 1<br />

2 , 2 ) of L2A , with m ≥ k, which belongs to an open circuit<br />

of diameter exceeding m. Using (10.14),<br />

P � Nk(A) ≥ 1 � ≤<br />

∞�<br />

m=k<br />

e −αm < 1<br />

3<br />

for sufficiently large k. We pick k accordingly, whence<br />

P � Nk(A) + Nk(B) ≥ 1 � ≤ 2<br />

3 .<br />

Now, if Nk(A) = Nk(B) = 0, and in addition all points of L2 inside Λ(k) are<br />

rw points, then N(A) = N(B) = 0. These last events have strictly positive<br />

probabilities, and (10.15) follows.<br />

Let J be the event that there exists a rw point x = x(Z) which lies in<br />

the interior of no open circuit of either L 2 A or L2 B<br />

. Since J is invariant with<br />

respect to translations of L 2 , and since P is product measure, we have that<br />

P(J) equals either 0 or 1. Using (10.15), we deduce that P(J) = 1. Therefore<br />

we may find a.s. some such vertex x = x(Z). We claim that x is Z-nonlocalised,<br />

which will imply as claimed that the labyrinth if a.s. non-localised.

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