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PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

PERCOLATION AND DISORDERED SYSTEMS Geoffrey GRIMMETT

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250 <strong>Geoffrey</strong> Grimmett<br />

now make two comparisons, the effect of each of which is to increase all<br />

effective resistances of the network. At the first stage, we replace all finite<br />

edge-resistances l(e) −1 by unit resistances. This cannot decrease any effective<br />

resistance. At the next stage we replace each rw point by<br />

+ with probability π(+; α, β) − p+<br />

ρ (�= +) with probability π(ρ; α, β) − (1 − prw − p+)π(ρ),<br />

in accordance with (10.20) and (10.21) (and where α, β are chosen so that<br />

(10.20), (10.21) hold, and furthermore βc(α, 2) < β < 1). Such replacements<br />

can only increase effective resistance.<br />

In this way we obtain a comparison between the resistance of the network<br />

arising from the above labyrinth and that of the labyrinth L(ω) defined<br />

around (10.19). Indeed, it suffices to prove that the effective resistance between<br />

0 and ∞ (in the infinite equivalence class) of the labyrinth L(ω) is a.s.<br />

finite. By examining the geometry, we claim that this resistance is no greater<br />

(up to a multiplicative constant) than the resistance between the origin and<br />

infinity of the corresponding infinite open percolation cluster of ω. By the<br />

next lemma, the last resistance is a.s. finite, whence the original walk is<br />

a.s. transient (when confined to the almost surely unique infinite equivalence<br />

class).<br />

Lemma 10.22. Let d ≥ 3, 0 < α < 1, and βc(α, 2) < β < 1. Let R be the<br />

effective resistance between the origin and the points at infinity, in the above<br />

bond percolation process ω on L. Then<br />

� � �<br />

R < ∞ �0 belongs to the infinite open cluster = 1.<br />

Pα,β<br />

Presumably the same conclusion is valid under the weaker hypothesis that<br />

β > βc(α, d).<br />

Sketch Proof. Rather than present all the details, here are some notes. The<br />

main techniques used in [163] arise from [164], and principally one uses the<br />

exponential decay noted in Lemma 10.4. That such decay is valid whenever<br />

β > βc(α, d) uses the machinery of [164]. This machinery may be developed in<br />

the present setting (in [164] it is developed only for the hypercubic lattice L d ).<br />

Alternatively, ‘slab arguments’ show (a) and (b) of Lemma 10.4 for sufficiently<br />

large β; certainly the condition β > βc(α, 2) suffices for the conclusion. �<br />

Comments on the Proof of Lemma 10.16. This resembles closely the proof<br />

of the uniqueness of the infinite percolation cluster (Theorem 7.1). We do<br />

not give the details. The notion of ‘trifurcation’ is replaced by that of an<br />

‘encounter zone’. Let R ≥ 1 and B = B(R). A translate x + B is called an<br />

encounter zone if<br />

(a) all points in x + B are rw points, and<br />

(b) in the labyrinth Z d \{x+B}, there are three or more infinite equivalence<br />

classes which are part of the same equivalence class of L d .<br />

Note that different encounter zones may overlap. See [73] for details. �

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