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 241<br />
Next, we construct an electrical network E(ρ) on L 2 by, for each edge<br />
e of L 2 , placing an electrical resistor of size ρ(e) at e. Let R = R(Z) be<br />
the effective resistance of this network between 0 and ∞ (which is to say<br />
that R = limn→∞ Rn, where Rn is the resistance between 0 and a composite<br />
vertex obtained by identifying all vertices in ∂B(n)).<br />
Lemma 10.12. We have that P � R(Z) = ∞ � �0 is a rw point � = 1.<br />
Proof. We define the ‘edge-boundary’ ∆eB(n) of B(n) to be the set of edges<br />
e = 〈x, y〉 with x ∈ ∂B(n) and y ∈ ∂B(n + 1). We claim that there exists a<br />
positive constant c and a random integer M such that<br />
(10.13) ρ(e) ≥ c<br />
log n for all e ∈ ∆eB(n) and n ≥ M.<br />
To show this, we argue as follows. Assume that e = 〈x, y〉 is normal, and let<br />
λ1 be the number of edges in the path π(e) on one side of e (this side being<br />
chosen in an arbitrary way), and λ2 for the number on the other side. Since<br />
each new vertex visited by the path is a rw point with probability prw, and<br />
since no vertex appears more than twice in π(e), we have that<br />
P � l(e) > 2k, e is normal � ≤ 2P � λ1 ≥ k, e is normal � ≤ 2(1 − prw) 1<br />
2 (k−1) .<br />
Therefore, for c > 0 and all n ≥ 2,<br />
�<br />
P ρ(e) < c<br />
log n<br />
�<br />
for some e ∈ ∆eB(n)<br />
≤ 4(2n + 1)P<br />
≤ βn 1−α<br />
�<br />
l(e) ><br />
log n<br />
, e is normal<br />
c<br />
where α = α(c) = −(4c) −1 log(1 − prw) and β = β(c, prw) < ∞. We choose c<br />
such that α > 5<br />
2 , whence (10.13) follows by the Borel–Cantelli lemma.<br />
The conclusion of the lemma is a fairly immediate consequence of (10.13),<br />
using the usual argument which follows. From the electrical network E(ρ)<br />
we construct another network with no larger resistance. This we do by identifying<br />
all vertices contained in each ∂B(n). In this new system there are<br />
|∆eB(n)| parallel connections between ∂B(n) and ∂B(n + 1), each of which<br />
has (for n ≥ M) a resistance at least c/ log n. The effective resistance from<br />
the origin to infinity is therefore at least<br />
∞�<br />
n=M<br />
c<br />
|∆eB(n)| log n =<br />
∞�<br />
n=M<br />
c<br />
= ∞,<br />
4(2n + 1)log n<br />
and the proof of the lemma is complete. �<br />
�