quasicircle

{{Short description|Quasiconformal complex image of a circle}}

{{distinguish|Pseudocircle}}

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In mathematics, a quasicircle is a Jordan curve in the complex plane that is the image of a circle under a quasiconformal mapping of the plane onto itself. Originally introduced independently by {{harvtxt|Pfluger|1961}} and {{harvtxt|Tienari|1962}}, in the older literature (in German) they were referred to as quasiconformal curves, a terminology which also applied to arcs.{{harvnb|Lehto|Virtanen|1973}}{{harvnb|Krzyz|1983|p=49}} In complex analysis and geometric function theory, quasicircles play a fundamental role in the description of the universal Teichmüller space, through quasisymmetric homeomorphisms of the circle. Quasicircles also play an important role in complex dynamical systems.

Definitions

A quasicircle is defined as the image of a circle under a quasiconformal mapping of the extended complex plane. It is called a K-quasicircle if the quasiconformal mapping has dilatation K. The definition of quasicircle generalizes the characterization of a Jordan curve as the image of a circle under a homeomorphism of the plane. In particular a quasicircle is a Jordan curve. The interior of a quasicircle is called a quasidisk.{{harvnb|Lehto|1987|p=38}}

As shown in {{harvtxt|Lehto|Virtanen|1973}}, where the older term "quasiconformal curve" is used, if a Jordan curve is the image of a circle under a quasiconformal map in a neighbourhood of the curve, then it is also the image of a circle under a quasiconformal mapping of the extended plane and thus a quasicircle. The same is true for "quasiconformal arcs" which can be defined as quasiconformal images of a circular arc either in an open set or equivalently in the extended plane.{{harvnb|Lehto|Virtanen|1973|pp=97–98}}

Geometric characterizations

{{harvtxt|Ahlfors|1963}} gave a geometric characterization of quasicircles as those Jordan curves for which the absolute value of the cross-ratio of any four points, taken in cyclic order, is bounded below by a positive constant.

Ahlfors also proved that quasicircles can be characterized in terms of a reverse triangle inequality for three points: there should be a constant C such that if two points z1 and z2 are chosen on the curve and z3 lies on the shorter of the resulting arcs, then{{harvnb|Carleson|Gamelin|1993|p=102}}

: |z_1-z_3| + |z_2-z_3| \le C |z_1-z_2|.

This property is also called bounded turning{{harvnb|Lehto|Virtanen|1973|pp=100–102}} or the arc condition.{{harvnb|Krzyz|1983|p=45}}

For Jordan curves in the extended plane passing through ∞, {{harvtxt|Ahlfors|1966}} gave a simpler necessary and sufficient condition to be a quasicircle.{{harvnb|Ahlfors|1966|p=81}}{{harvnb|Krzyz|1983|pp=48–49}} There is a constant C > 0 such that if

z1, z2 are any points on the curve and z3 lies on the segment between them, then

:\displaystyle{\left|z_3 -{z_1+z_2\over 2}\right|\le C |z_1-z_2|.}

These metric characterizations imply that an arc or closed curve is quasiconformal whenever it arises as the image of an interval or the circle under a bi-Lipschitz map f, i.e. satisfying

: C_1|s-t|\le |f(s)-f(t)| \le C_2 |s-t|

for positive constants Ci.{{harvnb|Lehto|Virtanen|1973|pp=104–105}}

Quasicircles and quasisymmetric homeomorphisms

If φ is a quasisymmetric homeomorphism of the circle, then there are conformal maps f of [z| < 1 and g of |z|>1 into disjoint regions such that the complement of the images of f and g is a Jordan curve. The maps f and g extend continuously to the circle |z| = 1 and the sewing equation

: \varphi= g^{-1}\circ f

holds. The image of the circle is a quasicircle.

Conversely, using the Riemann mapping theorem, the conformal maps f and g uniformizing the outside of a quasicircle give rise to a quasisymmetric homeomorphism through the above equation.

The quotient space of the group of quasisymmetric homeomorphisms by the subgroup of Möbius transformations provides a model of universal Teichmüller space. The above correspondence shows that the space of quasicircles can also be taken as a model.{{harvnb|Krzyz|1983|p={{pn|date=September 2023}}}}

Quasiconformal reflection

A quasiconformal reflection in a Jordan curve is an orientation-reversing quasiconformal map of period 2 which switches the inside and the outside of the curve fixing points on the curve. Since the map

:\displaystyle{R_0(z) = {1\over \overline{z}}}

provides such a reflection for the unit circle, any quasicircle admits a quasiconformal reflection. {{harvtxt|Ahlfors|1963}} proved that this property characterizes quasicircles.

Ahlfors noted that this result can be applied to uniformly bounded holomorphic univalent functions f(z) on the unit disk D. Let Ω = f(D). As Carathéodory had proved using his theory of prime ends, f extends continuously to the unit circle if and only if ∂Ω is locally connected, i.e. admits a covering by finitely many compact connected sets of arbitrarily small diameter. The extension to the circle is 1-1 if and only if ∂Ω has no cut points, i.e. points which when removed from ∂Ω yield a disconnected set. Carathéodory's theorem shows that a locally set without cut points is just a Jordan curve and that in precisely this case is the extension of f to the closed unit disk a homeomorphism.{{harvnb|Pommerenke|1975|pp=271–281}} If f extends to a quasiconformal mapping of the extended complex plane then ∂Ω is by definition a quasicircle. Conversely {{harvtxt|Ahlfors|1963}} observed that if ∂Ω is a quasicircle and R1 denotes the quasiconformal reflection in ∂Ω then the assignment

: \displaystyle{f(z)=R_1f R_0(z)}

for |z| > 1 defines a quasiconformal extension of f to the extended complex plane.

Complex dynamical systems

File:Flocke.PNG]]

Quasicircles were known to arise as the Julia sets of rational maps R(z). {{harvtxt|Sullivan|1985}} proved that if the Fatou set of R has two components and the action of R on the Julia set is "hyperbolic", i.e. there are constants c > 0 and A > 1 such that

: |\partial_z R^n(z)| \ge c A^n

on the Julia set, then the Julia set is a quasicircle.

There are many examples:{{harvnb|Carleson|Gamelin|1993|pp=123–126}}{{harvnb|Rohde|1991}}

  • quadratic polynomials R(z) = z2 + c with an attracting fixed point
  • the Douady rabbit (c = –0.122561 + 0.744862i, where c3 + 2 c2 + c + 1 = 0)
  • quadratic polynomials z2 + λz with |λ| < 1
  • the Koch snowflake

Quasi-Fuchsian groups

Quasi-Fuchsian groups are obtained as quasiconformal deformations of Fuchsian groups. By definition their limit sets are quasicircles.{{harvnb|Bers|1961}}{{harvnb|Bowen|1979}}{{harvnb|Mumford|Series|Wright|2002}}{{harvnb|Imayoshi|Taniguchi|1992|p=147}}{{harvnb|Marden|2007|pp=79–80,134}}

Let Γ be a Fuchsian group of the first kind: a discrete subgroup of the Möbius group preserving the unit circle. acting properly discontinuously on the unit disk D and with limit set the unit circle.

Let μ(z) be a measurable function on D with

:\|\mu\|_\infty < 1

such that μ is Γ-invariant, i.e.

:\mu(g(z)){\overline{\partial_{z}g(z)}\over \partial_z g(z)}=\mu(z)

for every g in Γ. (μ is thus a "Beltrami differential" on the Riemann surface D / Γ.)

Extend μ to a function on C by setting μ(z) = 0 off D.

The Beltrami equation

: \partial_{\overline{z}} f (z) =\mu(z)\partial_zf(z)

admits a solution unique up to composition with a Möbius transformation.

It is a quasiconformal homeomorphism of the extended complex plane.

If g is an element of Γ, then f(g(z)) gives another solution of the Beltrami equation, so that

:\alpha(g)=f\circ g \circ f^{-1}

is a Möbius transformation.

The group α(Γ) is a quasi-Fuchsian group with limit set the quasicircle given by the image of the unit circle under f.

Hausdorff dimension

File:Douady rabbit.png is composed of quasicircles with Hausdorff dimension approximately 1.3934{{harvnb|Carleson|Gamelin|1993|p=122}} ]]

It is known that there are quasicircles for which no segment has finite length.{{harvnb|Lehto|Virtanen|1973|p=104}} The Hausdorff dimension of quasicircles was first investigated by {{harvtxt|Gehring|Väisälä|1973}}, who proved that it can take all values in the interval [1,2).{{harvnb|Lehto|1987|p=38}} {{harvtxt|Astala|1993}}, using the new technique of "holomorphic motions" was able to estimate the change in the Hausdorff dimension of any planar set under a quasiconformal map with dilatation K. For quasicircles C, there was a crude estimate for the Hausdorff dimension{{harvnb|Astala|Iwaniec|Martin|2009}}

: d_H(C) \le 1 + k

where

:k={K-1\over K+1}.

On the other hand, the Hausdorff dimension for the Julia sets Jc of the iterates of the rational maps

:R(z) =z^2 +c

had been estimated as result of the work of Rufus Bowen and David Ruelle, who showed that

:1 < d_H(J_c) < 1 + {|c|^2 \over4\log 2} + o(|c|^2).

Since these are quasicircles corresponding to a dilatation

: K=\sqrt{1+t\over 1-t}

where

: t= |1-\sqrt{1-4c}|,

this led {{harvtxt|Becker|Pommerenke|1987}} to show that for k small

:1+ 0.36 k^2\le d_H(C) \le 1 + 37 k^2.

Having improved the lower bound following calculations for the Koch snowflake with Steffen Rohde and Oded Schramm,

{{harvtxt|Astala|1994}} conjectured that

: d_H(C) \le 1 + k^2.

This conjecture was proved by {{harvtxt|Smirnov|2010}}; a complete account of his proof, prior to publication, was already given in {{harvtxt|Astala|Iwaniec|Martin|2009}}.

For a quasi-Fuchsian group {{harvtxt|Bowen|1979}} and {{harvtxt|Sullivan|1982}} showed that the Hausdorff dimension d of the limit set is always greater than 1. When d < 2, the quantity

:\lambda=d(2-d)\,\in (0,1)

is the lowest eigenvalue of the Laplacian of the corresponding hyperbolic 3-manifold.{{harvnb|Astala|Zinsmeister|1994}}{{harvnb|Marden|2007|p=284}}

Notes

{{reflist|2}}

References

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Category:Complex analysis

Category:Dynamical systems

Category:Fractals