Spring 2010 - Problem 4

Jensen's formula, subharmonic functions

Let f(z)f\p{z} be a continuous function on the closed unit disk {zCz1}\set{z \in \C \mid \abs{z} \leq 1} such that f(z)f\p{z} is analytic on the open disk {z<1}\set{\abs{z} < 1} and f(0)0f\p{0} \neq 0.

  1. Prove that if 0<r<10 < r < 1 and if infz=rf(z)>0\inf_{\abs{z}=r}\,\abs{f\p{z}} > 0, then

    12π02πlogf(reiθ)dθlogf(0).\frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{re^{i\theta}}} \,\diff\theta \geq \log\abs{f\p{0}}.
  2. Use (1) to prove that {θ[0,2π]f(eiθ)}=0\abs{\set{\theta \in \br{0, 2\pi} \mid f\p{e^{i\theta}}}} = 0 where again E\abs{E} is the Lebesgue measure of EE.

Solution.
  1. We will prove Jensen's formula: let rr be so that infz=rinff(z)>0\inf_{\abs{z}=r}\, \inf \abs{f\p{z}} > 0. If ErE_r is the set of roots of ff in the open disk B(0,r)B\p{0, r} counting multiplicity, then

    12π02πlogf(reiθ)dθ=logf(0)aErlogar.\frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{re^{i\theta}}} \,\diff\theta = \log\abs{f\p{0}} - \sum_{a \in E_r} \log\frac{\abs{a}}{r}.

    For aDa \in \D, consider the Blaschke product φa ⁣:DD\func{\phi_a}{\D}{\D},

    φa(z)=za1az,\phi_a\p{z} = \frac{z - a}{1 - \conj{a}z},

    which is a holomorphic function on the disk with the property that φa(z)=1\abs{\phi_a\p{z}} = 1 if z=1\abs{z} = 1 or a=1\abs{a} = 1. Thus, if we set

    g(z)=f(z)aErφa/r(z/r),g\p{z} = \frac{f\p{z}}{\prod_{a \in E_r} \phi_{a/r}\p{z/r}},

    then gg is a holomorphic function on D\D which is continuous on the D\cl{\D} that vanishes nowhere on zr\abs{z} \leq r. Indeed, at each root aEra \in E_r of ff, the denominator of gg has a zero at aa with order equal to that of its numerator. Moreover, if z=r\abs{z} = r, then g(z)=f(z)\abs{g\p{z}} = \abs{f\p{z}}, since all the factors in the denominator become 11.

    Hence, logg(z)\log\abs{g\p{z}} is a harmonic function which does not vanish on z=r\abs{z} = r. By the mean value property, we have

    12π02πlogg(reiθ)dθ=logg(0)=logf(0)aErlogar.\frac{1}{2\pi} \int_0^{2\pi} \log\abs{g\p{re^{i\theta}}} \,\diff\theta = \log\abs{g\p{0}} = \log\abs{f\p{0}} - \sum_{a \in E_r} \log\frac{\abs{a}}{r}.

    On the other hand, since reiθ=r\abs{re^{i\theta}} = r,

    12π02πlogg(reiθ)dθ=12π02πlogf(reiθ)dθ,\frac{1}{2\pi} \int_0^{2\pi} \log\abs{g\p{re^{i\theta}}} \,\diff\theta = \frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{re^{i\theta}}} \,\diff\theta,

    which proves Jensen's formula. Observe that logar<0\log\frac{\abs{a}}{r} < 0 for aEra \in E_r, so this gives the inequality

    12π02πlogf(reiθ)dθlogf(0),\frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{re^{i\theta}}} \,\diff\theta \geq \log\abs{f\p{0}},

    which was what we wanted to show.

  2. Since B(0,r)\cl{B\p{0, r}} is compact and ff does not vanish everywhere (since f(0)0f\p{0} \neq 0), it follows that ff can only have finitely many zeroes in B(0,r)\cl{B\p{0, r}}. By writing

    D=n=1B(0,11n),\D = \bigcup_{n=1}^\infty B\p{0, 1 - \frac{1}{n}},

    we see that the zeroes of ff are a countable union of finite sets, so ff has at most countably many zeroes. In particular, we may pick a sequence {rn}n(0,1)\set{r_n}_n \subseteq \p{0, 1} such that rnr_n increases to 11 and infz=rnf(z)>0\inf_{\abs{z}=r_n}\,\abs{f\p{z}} > 0, since countably many zeroes almost removes countably many choices of radii. By Fatou's lemma,

    logf(0)lim supn12π02πlogf(rneiθ)dθ12π02πlogf(eiθ)dθ.\begin{aligned} \log\abs{f\p{0}} \leq \limsup_{n\to\infty} \frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{r_ne^{i\theta}}} \,\diff\theta \leq \frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{e^{i\theta}}} \,\diff\theta. \end{aligned}

    Let E={θ[0,2π]f(eiθ)=0}E = \set{\theta \in \br{0, 2\pi} \mid f\p{e^{i\theta}} = 0}. Since f(0)0f\p{0} \neq 0, we have logf(0)>\log\abs{f\p{0}} > -\infty, so if E>0\abs{E} > 0,

    <logf(0)12π02πlogf(eiθ)dθ=12πElogf(eiθ)dθ+12πEclogf(eiθ)dθ=E2π()+12πEclogf(eiθ)dθ.\begin{aligned} -\infty &< \log\abs{f\p{0}} \\ &\leq \frac{1}{2\pi} \int_0^{2\pi} \log\abs{f\p{e^{i\theta}}} \,\diff\theta \\ &= \frac{1}{2\pi} \int_E \log\abs{f\p{e^{i\theta}}} \,\diff\theta + \frac{1}{2\pi} \int_{E^\comp} \log\abs{f\p{e^{i\theta}}} \,\diff\theta \\ &= \frac{\abs{E}}{2\pi} \cdot \p{-\infty} + \frac{1}{2\pi} \int_{E^\comp} \log\abs{f\p{e^{i\theta}}} \,\diff\theta. \end{aligned}

    The second term is bounded, since ff is continuous on z=1\abs{z} = 1, so the second term is bounded above by some finite number. Thus, if E0\abs{E} \neq 0, then

    <logf(0),-\infty < \log\abs{f\p{0}} \leq -\infty,

    which is impossible. Hence, E=0\abs{E} = 0, as required.