Sharp stability results for almost conformal maps in even dimensions (original) (raw)

On maps almost conformal at the boundary

Complex Variables, 1997

Repnnts a\a~lable directl) from the pubhsher Photocopying pemmed by l~cznse only @ 1997 OPA (Oieneas Publishers Assouation) Amsterdam B.V Publ~shed under l~cense under the Gordon and Breach Science Publishers imprint.

On absolutely conformal mappings

Publicationes Mathematicae Debrecen, 2010

Let Ω be a domain in R n. It is proved that, if u ∈ C 1 (Ω; R n) and there holds the formula ∇u(x) n = n n/2 | det ∇u(x)| in Ω, then for n ≥ 3 u is a restriction of a Möbius transformation, and for n = 2, u is an analytic function. This extends, partially, the well-known Liouville theorem ([6]), wich states that if u ∈ ACL n (Ω; R n), n ≥ 3, and the condition ∇u(x) n = n n/2 det ∇u(x) is satisfied a.e. in Ω, then u is a restriction of a Möbius transformation.

On the local behaviour of quasi-conformal mappings

Izvestiya: Mathematics, 1995

This paper is devoted to the study of the local behaviour of quasiconformal mappings on the plane and related questions of boundary correspondence in dependence on properties of complex characteristics. The Gardiner-Sullivan symmetries are investigated as well as quasi-circles asymptotically conformal in the sense of Becker and Ponfmerenke.

Cheeger-Gromov convergence in a conformal setting. I

arXiv: Differential Geometry, 2015

For a sequence (Mi,gi,xi)\{(M_i, g_i, x_i)\}(Mi,gi,xi) of pointed Riemannian manifolds with boundary, the sequence (Mi,tildegi,xi)\{(M_i,\tilde g_i,x_i)\}(Mi,tildegi,xi) is its conformal satellite if the metric tildegi\tilde g_itildegi is conformal to gig_igi, that is, tildegi=ufrac4n−2igi\tilde g_i=u^{\frac{4}{n-2}}_ig_itildegi=ufrac4n2igi. Assuming the manifolds (Mi,gi,xi)(M_i,g_i,x_i)(Mi,gi,xi) have uniformly bounded geometry, we show that both sequences have smoothly Cheeger-Gromov convergent subsequences provided the conformal factors uiu_iui are principal eigenfunctions of an appropriate elliptic operator. Part of our result is a Cheeger-Gromov compactness for manifolds with boundary. We use stable versions of classical elliptic estimates and inequalities found in the recently established 'flatzoomer' method.

A note on convex conformal mappings

Proceedings of the American Mathematical Society, 2018

We establish a new characterization for a conformal mapping of the unit disk D to be convex, and identify the mappings onto a half-plane or a parallel strip as extremals. We also show that, with these exceptions, the level sets of λ of the Poincaré metric λ|dw| of a convex domain are strictly convex.

Spectral Notions for Conformal Maps: a Survey

2008

The universal means spectrum of conformal mappings has been studied extensively in recent years. In some situations, sharp results are available, in others, only upper and lower estimates have been obtained so far. We review some of the classical results before discussing the recent work of Hedenmalm and Shimorin on estimates of the universal means spectrum near the origin. It is our ambition to explain how their method works and what its limitations are. We then move on to the recent study of the universal means spectrum of bounded functions near the point two conducted by Baranov and Hedenmalm. A number of open problems related to these topics are pointed out together with some auxilliary results which are interesting in their own right.

On the Conformal Energy of Quasisymmetric and Quasim\"obius Mappings

arXiv (Cornell University), 2023

This article identifies the conformal energy (or mean distortion) of extremal mappings of finite distortion with a given quasisymmetric mapping of the circle as boundary data. The conformal energy of g o : S → S is * Research of both authors supported by the NZ Marsden Fund,

Iterations of holomorphic Collet-Eckmann maps: conformal and invariant measures. Appendix: On non-renormalizable quadratic polynomials

Transactions of the American Mathematical Society, 1998

We prove that for every rational map on the Riemann sphere f : C ¯ → C ¯ f:\overline {\mathbb {C}} \to \overline {\mathbb {C}} , if for every f f -critical point c ∈ J c\in J whose forward trajectory does not contain any other critical point, the growth of | ( f n ) ′ ( f ( c ) ) | |(f^{n})’(f(c))| is at least of order exp ⁡ Q n \exp Q \sqrt n for an appropriate constant Q Q as n → ∞ n\to \infty , then HD ess ⁡ ( J ) = α 0 = HD ⁡ ( J ) \operatorname {HD}_{\operatorname {ess}} (J)=\alpha _{0}=\operatorname {HD} (J) . Here HD ess ⁡ ( J ) \operatorname {HD}_{\operatorname {ess}} (J) is the so-called essential, dynamical or hyperbolic dimension, HD ⁡ ( J ) \operatorname {HD} (J) is Hausdorff dimension of J J and α 0 \alpha _{0} is the minimal exponent for conformal measures on J J . If it is assumed additionally that there are no periodic parabolic points then the Minkowski dimension (other names: box dimension, limit capacity) of J J also coincides with HD ⁡ ( J ) \operatorname {HD}(J)...