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Brownian Motion and the Dirichlet Problem - UCLA Department of ...

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Theorem 2. If a harmonic function h achieves its maximum or minimum on D,<br />

<strong>the</strong>n it is constant on D.<br />

Pro<strong>of</strong>. Suppose M = maxx∈D h(x) is achieved in D. By (3), h(x) = M impies<br />

h ≡ M in a neighborhood <strong>of</strong> x. Therefore {x ∈ D : h(x) = M} is both open <strong>and</strong><br />

closed, <strong>and</strong> hence h ≡ M on D.<br />

Corollary. Suppose D is bounded, h1 <strong>and</strong> h2 are both harmonic on D, continuous<br />

on <strong>the</strong> closure <strong>of</strong> D, <strong>and</strong> h1 = h2 on ∂D. Then h1 ≡ h2 on D.<br />

Pro<strong>of</strong>. Put h = h1 − h2. Then h is harmonic on D, continuous on <strong>the</strong> closure <strong>of</strong><br />

D, <strong>and</strong> = 0 on ∂D. If h ≡ 0 on D, <strong>the</strong>n it achieves a strictly positive maximum<br />

or strictly negative minimum on D, <strong>and</strong> <strong>the</strong>refore is constant on D, which is a<br />

contradiction.<br />

Examples. Using condition (b) in <strong>the</strong> definition <strong>of</strong> harmonicity, it is easy to check<br />

that<br />

(a) h(x) = x is harmonic on R 1 ,<br />

(b) h(x) = log ||x|| is harmonic on R 2 \{0}, <strong>and</strong><br />

(c) 1/||x|| d−2 is harmonic on R d \{0} if d ≥ 3.<br />

Applications. Take 0 < r1 < r2 <strong>and</strong> D = {x ∈ R d : r1 < ||x|| < r2}. By Theorem<br />

1, letting f(x) = 0 for ||x|| = r1 <strong>and</strong> f(x) = 1 for ||x|| = r2,<br />

h1(x) = P x (X(t) hits ∂B(0, r2) before ∂B(0, r1)) = E x f(X(τD))<br />

is harmonic in D. If X(0) = x is close to ∂D, <strong>the</strong>n <strong>the</strong> process hits ∂D very quickly<br />

with high probability, as can be seen by looking at <strong>the</strong> projection in <strong>the</strong> x direction<br />

<strong>of</strong> X(0), which is a one dimensional <strong>Brownian</strong> motion. (See also Proposition 2<br />

below.) Therefore, h1 is continuous on <strong>the</strong> closure <strong>of</strong> D, <strong>and</strong> h1 = f on ∂D.<br />

On <strong>the</strong> o<strong>the</strong>r h<strong>and</strong>, if a, b are chosen appropriately,<br />

h2(x) =<br />

a log ||x|| + b if d = 2,<br />

a<br />

||x|| d−2 + b if d ≥ 3<br />

has <strong>the</strong> same properties. Therefore, by <strong>the</strong> corollary, h1 ≡ h2 on D. Specifically,<br />

P x (X(t) hits ∂B(0, r2) before ∂B(0, r1))<br />

⎧<br />

⎨<br />

=<br />

⎩<br />

log ||x||−log r1<br />

log r2−log r1<br />

(r2/||x||) d−2 ||x||d−2−r d−2<br />

1<br />

r d−2<br />

2 −rd−2<br />

1<br />

if d = 2,<br />

if d ≥ 3.<br />

Letting σr be <strong>the</strong> hitting time <strong>of</strong> ∂B(0, r), we see that in both cases,<br />

lim<br />

r1→0 P x (σr2 < σr1) = 1, 0 < ||x|| < r2.<br />

Since limr→0 σr = σ0, <strong>the</strong> hitting time <strong>of</strong> 0, P x (σr2 < σ0) = 1, <strong>and</strong> since limr→∞ σr =<br />

∞, it follows that P x (σ0 = ∞) = 1. Therefore, unlike <strong>the</strong> one dimensional case,<br />

<strong>Brownian</strong> motion does not hit points for d ≥ 2:<br />

P x (X(t) = y for some t > 0) = 0<br />

3

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