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COMPLEX GEOMETRY Course notes

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Claim 2.15.3. For every α ∈ N 2 , we have<br />

D α (ρ ɛ ∗ ρ) = ρ ɛ ∗ (D α f)<br />

This result follows similarly applying a change of variables z ↦→ z + ɛ.<br />

Claim 2.15.4. If z ∈ U (ɛ) and f is harmonic on D(z, ɛ), then<br />

(ρ ɛ ∗ f)(z) = f(z).<br />

Proof:<br />

∫<br />

(ρ ɛ ∗ f)(z) = ρ ɛ (ɛ)f(z + ɛ)dVol(ɛ) =<br />

∫ 2π ∫ ɛ<br />

ρ ɛ (r)f(z + rɛ iθ )rdrdθ = 2πf(z)<br />

D(0,z)<br />

0 0<br />

0<br />

∫ ɛ<br />

ρ ɛ (r)rdr = f(z).<br />

Proof of Weyl’s Lemma: Since ɛ −→ ρ ɛ (ɛ − z) has compact support in U, for every z ∈ U (ɛ) ,<br />

h(z) := T ɛ [ρ ɛ (ɛ − z)]<br />

is defined and belongs to A 0 (U (ɛ) ) by Claim 6.2. By Claim 6.4, it suffices to show that for every<br />

f ∈ A 0 c(U (ɛ) ) we have<br />

∫<br />

T [f] = hf,<br />

U (ɛ)<br />

where h is harmonic since<br />

∆h = T ɛ [∆ z ρ ɛ (ɛ − z)] = ∆T ɛ [ρ(ɛ − z)] = 0.<br />

We want to show that T = T h . We have<br />

Hence it suffices to show<br />

∫<br />

T [ρ ɛ ∗ f] = hf.<br />

U (ɛ)<br />

T [f] = T [ρ ɛ ∗ f].<br />

By Claim 6.1, there exists ψ ∈ A 0 such that ∆ψ = f, where ψ is harmonic on V = C − supp(f). Hence<br />

ψ = ρ ɛ ∗ ψ on V ɛ by Claim 6.4. Therefore, O = ψ − ρ ɛ ∗ ρ ∈ A 0 c(U) satisfies<br />

since ∆T = 0, and T (∆ψ) = 0. Hence<br />

∆O = ∆ψ − ρ ɛ ∗ ∆ψ = f − ρ ∗ f<br />

T [f] = T [ρ ∗ f + ∆O] = T [ρ ɛ ∗ f].<br />

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