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Brownian motion and harnack inequality for ... - Math.caltech.edu

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260 M. AIZENMAN AND B. SIMON<br />

Thus, (A.2.10) follows from the one-dimensional case (Lemma A.2.7) <strong>and</strong> the<br />

bound<br />

which follows from the monotonicity of S'/~P,'')(X, y) in s.<br />

THEOREM A.2.8.<br />

(A.2.11) <strong>and</strong> let<br />

Let 52 be a rounded convex set in R'. Let P, be given by<br />

Qs(x9 u) = +(x)-1WV'(x9 Y)<br />

PL2 being the integral kernel of the semigroup generated by the Dirichlet Laplacian<br />

in 52. Then (A.2.10) holds <strong>for</strong> any c > 0. Moreover, C, depends onh on Y <strong>and</strong> on the<br />

ratio<br />

sup[ dist(x, aQ)+(x)]/inf[ dist(x, aQ)+(x)].<br />

In particular, the Same C, will work <strong>for</strong> all balls.<br />

Proof: We bound instead<br />

(A.2.12) dist(x,aS2)-1P:(x, y)dist(y, an)<br />

by C, P, I +,)s(x, y) independently of 52 <strong>and</strong> then use Lemma A.2.5. Given x, pick<br />

z E a52 so that dist(z,x) = dist(x, 352) <strong>and</strong> let T be the half-space with z E aT, <strong>and</strong><br />

Cl C T. By translation <strong>and</strong> rotation, we can suppose without loss of generality<br />

that T = {zlzl > 0). Then dist(x, aS2) = xI <strong>and</strong> dist(y, a52) Sy,. Since PR is<br />

monotone in 52, we see that (A.2.12) is bounded by<br />

so Lemma A.2.7 yields the required bound.<br />

Appendix 3. Some Remarks on First Exit Times<br />

Let Cl be an open subset of R' <strong>and</strong> let T be the first hitting time <strong>for</strong> R'\52. The<br />

first fact that we want to note helps explain why Chung-Rau [7] obtain results<br />

which depend only on )QI.<br />

THEOREM A.3. I .<br />

Let f be a monotone non-decreasing function on [O,m). Then

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