TheoremComplete

Harnack's Inequality and Principle

Harnack's inequality provides quantitative control on harmonic functions, bounding the ratio of values at different points. Harnack's principle extends this to monotone sequences.


Statement

Theorem8.13Harnack's inequality

Let uu be harmonic and non-negative on the disk D(z0,R)D(z_0, R). Then for zz with ∣z−z0∣=r<R|z - z_0| = r < R:

R−rR+r u(z0)≤u(z)≤R+rR−r u(z0).\frac{R - r}{R + r}\,u(z_0) \leq u(z) \leq \frac{R + r}{R - r}\,u(z_0).


Proof

Proof

By the Poisson integral formula:

u(z)=12π∫02πPr(θ) u(z0+Reiθ) dθu(z) = \frac{1}{2\pi}\int_0^{2\pi} P_r(\theta)\,u(z_0 + Re^{i\theta})\,d\theta

where Pr(θ)=R2−r2R2−2Rrcos⁡θ+r2P_r(\theta) = \frac{R^2 - r^2}{R^2 - 2Rr\cos\theta + r^2}.

Since R2−2Rrcos⁡θ+r2≤(R+r)2R^2 - 2Rr\cos\theta + r^2 \leq (R+r)^2 and ≥(R−r)2\geq (R-r)^2:

R−rR+r≤Pr(θ)⋅11≤R+rR−r.\frac{R-r}{R+r} \leq P_r(\theta) \cdot \frac{1}{1} \leq \frac{R+r}{R-r}.

More precisely: R2−r2(R+r)2≤Pr(θ)≤R2−r2(R−r)2\frac{R^2-r^2}{(R+r)^2} \leq P_r(\theta) \leq \frac{R^2-r^2}{(R-r)^2}, i.e., R−rR+r≤Pr(θ)≤R+rR−r\frac{R-r}{R+r} \leq P_r(\theta) \leq \frac{R+r}{R-r}.

Since u≥0u \geq 0 on the boundary:

u(z)≤R+rR−r⋅12π∫02πu(z0+Reiθ) dθ=R+rR−r u(z0)u(z) \leq \frac{R+r}{R-r}\cdot\frac{1}{2\pi}\int_0^{2\pi} u(z_0+Re^{i\theta})\,d\theta = \frac{R+r}{R-r}\,u(z_0)

by the mean value property. Similarly for the lower bound. ■\blacksquare

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Harnack's Principle

Theorem8.14Harnack's principle

Let {un}\{u_n\} be a monotone increasing sequence of harmonic functions on a connected domain DD. Then either:

  1. un(z)→+∞u_n(z) \to +\infty for all z∈Dz \in D (uniformly on compact subsets), or
  2. un→uu_n \to u uniformly on compact subsets, where uu is harmonic on DD.
Proof

Let S={z∈D:lim⁡un(z)<∞}S = \{z \in D : \lim u_n(z) < \infty\}. If z0∈Sz_0 \in S, choose a disk D(z0,R)⊂DD(z_0, R) \subset D. For ∣z−z0∣≤R/2|z - z_0| \leq R/2, Harnack's inequality gives:

0≤um(z)−un(z)≤3(um(z0)−un(z0))→00 \leq u_m(z) - u_n(z) \leq 3(u_m(z_0) - u_n(z_0)) \to 0

as m,n→∞m, n \to \infty. So {un}\{u_n\} converges uniformly on D(z0,R/2)D(z_0, R/2), and all points of D(z0,R/2)D(z_0, R/2) belong to SS. Thus SS is open.

Similarly, D∖SD \setminus S is open (if un(z0)→∞u_n(z_0) \to \infty, Harnack gives un(z)≥13un(z0)→∞u_n(z) \geq \frac{1}{3}u_n(z_0) \to \infty on D(z0,R/2)D(z_0, R/2)).

By connectedness, S=∅S = \emptyset or S=DS = D. In the latter case, the limit is harmonic by the theorem that uniform limits of harmonic functions are harmonic. ■\blacksquare

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Applications

ExampleHarnack distance and metric

The Harnack distance on a domain DD is defined by: dH(z1,z2)=log⁡sup⁡{u(z1)/u(z2)}d_H(z_1, z_2) = \log\sup\{u(z_1)/u(z_2)\} where the supremum is over all positive harmonic functions uu on DD. Harnack's inequality gives explicit bounds on this distance in terms of the Euclidean distance and the distance to the boundary.

ExampleConvergence of harmonic series

Consider u(z)=∑n=1∞vn(z)u(z) = \sum_{n=1}^\infty v_n(z) where each vnv_n is harmonic and non-negative. The partial sums form an increasing sequence of harmonic functions. By Harnack's principle, either u≡∞u \equiv \infty or uu is harmonic. If the series converges at one point, it converges everywhere and the sum is harmonic.

RemarkHarnack inequality in higher dimensions

Harnack's inequality generalizes to harmonic functions on Rn\mathbb{R}^n: on a ball B(x0,R)B(x_0, R), (R−r)Rn−2(R+r)n−1u(x0)≤u(x)≤(R+r)Rn−2(R−r)n−1u(x0)\frac{(R-r)R^{n-2}}{(R+r)^{n-1}} u(x_0) \leq u(x) \leq \frac{(R+r)R^{n-2}}{(R-r)^{n-1}} u(x_0). The principle and its consequences extend verbatim.