Spring 2019 - Problem 11

harmonic functions, Schwarz reflection principle

Let uC(R)u \in C^\infty\p{\R} be smooth 2π2\pi-periodic. Show that there exists a bounded holomorphic function f+f_+ in the upper half-plane Imz>0\Im{z} > 0 and a bounded holomorphic function ff_- in the lower half-plane Imz<0\Im{z} < 0, such that

u(x)=limε0(f+(x+iε)f(xiε)),xR.u\p{x} = \lim_{\epsilon\to0} \,\p{f_+\p{x + i\epsilon} - f_-\p{x - i\epsilon}}, \quad x \in \R.
Solution.

Since uu is 2π2\pi-periodic, then function u(logzi)u\p{\frac{\log{z}}{i}} is a well-defined smooth function on S1S^1. We may then solve the Dirichlet problem on the disk with boundary data u(logzi)u\p{\frac{\log{z}}{i}} to get a harmonic function v(z)v\p{z} on the disk which is continuous on D\cl{\D}. Since D\D is simply connected, there exists a holomorphic function gg on D\D such that Img=v\Im{g} = v. Then f(z)=g(eiz)f\p{z} = g\p{e^{iz}} is a holomorphic function on the upper half-plane H\H such that for any xRx \in \R,

Imf(x)=Img(eix)=v(eix)=u(x).\Im{f\p{x}} = \Im{g\p{e^{ix}}} = v\p{e^{ix}} = u\p{x}.

Let f+=f2if_+ = \frac{f}{2i}, and by Schwarz reflection, f(z)=f+(z)f_-\p{z} = \conj{f_+\p{\conj{z}}} is a holomorphic function on the lower half-plane. Then

f+(x+iε)f(xiε)=Imf(x+iε)ε0u(x),f_+\p{x + i\epsilon} - f_-\p{x - i\epsilon} = \Im{f\p{x + i\epsilon}} \xrightarrow{\epsilon\to0} u\p{x},

which was what we wanted.