conformal radius

In mathematics, the conformal radius is a way to measure the size of a simply connected planar domain D viewed from a point z in it. As opposed to notions using Euclidean distance (say, the radius of the largest inscribed disk with center z), this notion is well-suited to use in complex analysis, in particular in conformal maps and conformal geometry.

A closely related notion is the transfinite diameter or (logarithmic) capacity of a compact simply connected set D, which can be considered as the inverse of the conformal radius of the complement E = Dc viewed from infinity.

Definition

Given a simply connected domain DC, and a point zD, by the Riemann mapping theorem there exists a unique conformal map f : DD onto the unit disk (usually referred to as the uniformizing map) with f(z) = 0 ∈ D and f′(z) ∈ R+. The conformal radius of D from z is then defined as

: \operatorname{rad}(z,D) := \frac{1}{f'(z)}\,.

The simplest example is that the conformal radius of the disk of radius r viewed from its center is also r, shown by the uniformizing map xx/r. See below for more examples.

One reason for the usefulness of this notion is that it behaves well under conformal maps: if φ : DD′ is a conformal bijection and z in D, then \operatorname{rad}(\varphi(z),D') = |\varphi'(z)|\operatorname{rad}(z,D).

The conformal radius can also be expressed as \exp(\xi_x(x)) where \xi_x(y) is the harmonic extension of \log(|x-y|) from \partial D to D.

A special case: the upper-half plane

Let KH be a subset of the upper half-plane such that D := H\K is connected and simply connected, and let zD be a point. (This is a usual scenario, say, in the Schramm–Loewner evolution). By the Riemann mapping theorem, there is a conformal bijection g : DH. Then, for any such map g, a simple computation gives that

: \operatorname{rad}(z,D) = \frac{2\operatorname{Im}(g(z))}

g'(z)
\,.

For example, when K = ∅ and z = i, then g can be the identity map, and we get rad(i, H) = 2. Checking that this agrees with the original definition: the uniformizing map f : HD is

:f(z)=i\frac{z-i}{z+i},

and then the derivative can be easily calculated.

Relation to inradius

That it is a good measure of radius is shown by the following immediate consequence of the Schwarz lemma and the Koebe 1/4 theorem: for zDC,

:\frac{\operatorname{rad}(z,D)}{4} \leq \operatorname{dist} (z,\partial D) \leq \operatorname{rad}(z,D),

where dist(z, ∂D) denotes the Euclidean distance between z and the boundary of D, or in other words, the radius of the largest inscribed disk with center z.

Both inequalities are best possible:

: The upper bound is clearly attained by taking D = D and z = 0.

: The lower bound is attained by the following “slit domain”: D = C\R+ and z = −rR. The square root map φ takes D onto the upper half-plane H, with \varphi(-r) = i\sqrt{r} and derivative |\varphi'(-r)|=\frac{1}{2\sqrt{r}}. The above formula for the upper half-plane gives \operatorname{rad}(i\sqrt{r},\mathbb{H})=2\sqrt{r}, and then the formula for transformation under conformal maps gives rad(−r, D) = 4r, while, of course, dist(−r, ∂D) = r.

Version from infinity: transfinite diameter and logarithmic capacity

{{main|Analytic capacity}}

{{main|Capacity of a set}}

When DC is a connected, simply connected compact set, then its complement E = Dc is a connected, simply connected domain in the Riemann sphere that contains ∞{{citation needed|date=November 2020}}, and one can define

: \operatorname{rad}(\infty,D) := \frac{1}{\operatorname{rad}(\infty,E)} := \lim_{z\to\infty} \frac{f(z)}{z},

where f : C\DE is the unique bijective conformal map with f(∞) = ∞ and that limit being positive real, i.e., the conformal map of the form

:f(z)=c_1z+c_0 + c_{-1}z^{-1} + \cdots, \qquad c_1\in\mathbf{R}_+.

The coefficient c1 = rad(∞, D) equals the transfinite diameter and the (logarithmic) capacity of D; see Chapter 11 of {{harvtxt|Pommerenke|1975}} and {{harvtxt|Kuz′mina|2002}}.

The coefficient c0 is called the conformal center of D. It can be shown to lie in the convex hull of D; moreover,

:D\subseteq \{z: |z-c_0|\leq 2 c_1\}\,,

where the radius 2c1 is sharp for the straight line segment of length 4c1. See pages 12–13 and Chapter 11 of {{harvtxt|Pommerenke|1975}}.

The Fekete, Chebyshev and modified Chebyshev constants

We define three other quantities that are equal to the transfinite diameter even though they are defined from a very different point of view. Let

:d(z_1,\ldots,z_k):=\prod_{1\le i

denote the product of pairwise distances of the points z_1,\ldots,z_k and let us define the following quantity for a compact set DC:

:d_n(D):=\sup_{z_1,\ldots,z_n\in D} d(z_1,\ldots,z_n)^{1\left/\binom n 2\right.}

In other words, d_n(D) is the supremum of the geometric mean of pairwise distances of n points in D. Since D is compact, this supremum is actually attained by a set of points. Any such n-point set is called a Fekete set.

The limit d(D):=\lim_{n\to\infty} d_n(D) exists and it is called the Fekete constant.

Now let \mathcal P_n denote the set of all monic polynomials of degree n in C[x], let \mathcal Q_n denote the set of polynomials in \mathcal P_n with all zeros in D and let us define

:\mu_n(D):=\inf_{p\in\mathcal P_n} \sup_{z\in D} |p(z)| and \tilde{\mu}_n(D):=\inf_{p\in\mathcal Q_n} \sup_{z\in D} |p(z)|

Then the limits

:\mu(D):=\lim_{n\to\infty} \mu_n(D)^{1/n} and \mu(D):=\lim_{n\to\infty} \tilde{\mu}_n(D)^{1/n}

exist and they are called the Chebyshev constant and modified Chebyshev constant, respectively.

Michael Fekete and Gábor Szegő proved that these constants are equal.

Applications

The conformal radius is a very useful tool, e.g., when working with the Schramm–Loewner evolution. A beautiful instance can be found in {{harvtxt|Lawler|Schramm|Werner|2002}}.

References

{{sfn whitelist|CITEREFKuz′mina2002}}

  • {{cite book| last=Ahlfors | first=Lars V. | author-link=Lars Ahlfors | year=1973 | title=Conformal invariants: topics in geometric function theory | url=https://archive.org/details/conformalinvaria00lars | url-access=registration | series=Series in Higher Mathematics | publisher=McGraw-Hill | isbn=978-0-07-000659-1 | mr=0357743 | zbl=0272.30012 }}
  • {{cite book| editor1-last=Horváth | editor1-first=János | year=2005 | title=A Panorama of Hungarian Mathematics in the Twentieth Century, I | series=Bolyai Society Mathematical Studies | publisher=Springer | isbn=3-540-28945-3 }}
  • {{SpringerEOM | last1=Kuz′mina | first1=G. V.|year=2002|title=Conformal radius of a domain}}
  • {{Citation | last1=Lawler | first1=Gregory F. |author-link1=Gregory Lawler| last2=Schramm | first2=Oded | author-link2=Oded Schramm| last3=Werner | first3=Wendelin | author-link3=Wendelin Werner|title= One-arm exponent for critical 2D percolation | url= http://www.math.washington.edu/~ejpecp/viewarticle.php?id=1303&layout=abstract | mr=1887622 | year=2002 | journal= Electronic Journal of Probability | volume=7 | issue=2 | pages=13 pp | zbl=1015.60091| issn=1083-6489 | doi=10.1214/ejp.v7-101| arxiv=math/0108211 }}
  • {{cite book| last=Pommerenke | first= Christian | author-link=Christian Pommerenke | year=1975 | title=Univalent functions | others=With a chapter on quadratic differentials by Gerd Jensen | publisher=Vandenhoeck & Ruprecht | location=Göttingen | zbl=0298.30014 | series=Studia Mathematica/Mathematische Lehrbücher | volume=Band XXV }}

Further reading

  • {{citation | last=Rumely | first=Robert S. | author-link = Robert Rumely | title=Capacity theory on algebraic curves | series=Lecture Notes in Mathematics | volume=1378 | location=Berlin etc. | publisher=Springer-Verlag | year=1989 | isbn=3-540-51410-4 | zbl=0679.14012 }}