Abstract
This paper investigates several dynamically defined dimensions for rational maps f on the Riemann sphere, providing a systematic treatment modeled on the theory for Kleinian groups.¶We begin by defining the radial Julia set Jrad(f), and showing that every rational map satisfies¶\( {\rm H.\,dim}\,J_{{\rm rad}}(f) = \alpha(f) \)¶where \( \alpha(f) \) is the minimal dimension of an f-invariant conformal density on the sphere. A rational map f is geometrically finite if every critical point in the Julia set is preperiodic. In this case we show¶\(\),¶where \( \delta(f) \) is the critical exponent of the Poincare series; and f admits a unique normalized invariant density μ of dimension \( \delta(f) \).¶Now let f be geometrically finite and suppose \( f_n \to f \) algebraically, preserving critical relations. When the convergence is horocyclic for each parabolic point of f, we show fn is geometrically finite for \( n \gg 0 \) and \( J(f_n) \to J(f) \) in the Hausdorff topology. If the convergence is radial, then in addition we show \( {\rm H.\,dim}\,J(f_{n}) \to {\rm H.\,dim}\,J(f) \).¶We give examples of horocyclic but not radial convergence where \( {\rm H.\,dim}\,J(f_{n}) \to 1 > {\rm H.\,dim}\,J(f) = 1/2 + \epsilon \). We also give a simple demonstration of Shishikura's result that there exist \( f_n(z) = z^2 + c_n \) with \( {\rm H.\,dim}\,J(f_{n}) \to 2 \).¶The proofs employ a new method that reduces the study of parabolic points to the case of elementary Kleinian groups.
Highlights
Let f : C → C be a rational map on the Riemann sphere, of degree d ≥ 2
As a bridge between the two subjects, we develop a new technique that reduces the study of parabolic bifurcations of rational maps to the case of Mobius transformations
To summarize the main results, we first introduce various dimensions determined by the dynamics of a rational map f
Summary
Let f : C → C be a rational map on the Riemann sphere, of degree d ≥ 2. To pattern the theory after that of Kleinian groups, we define the radial Julia set of a rational map and a notion of geometric finiteness in the dynamical setting. To summarize the main results, we first introduce various dimensions determined by the dynamics of a rational map f. Our first invariant is its Hausdorff dimension, H. dim J(f ). 2. We can consider the dimension of the radial Julia set Jrad(f ), consisting of those z for which arbitrarily small neighborhoods of z can be expanded. The hyperbolic dimension, hyp-dim(f ) is the supremum of the Hausdorff dimensions of such expanding sets X. 4. An f -invariant density of dimension α > 0 is a finite positive measure μ on C such that μ(f (E)) = |f (x)|α dμ. The critical dimension α(f ) is the minimum possible dimension of an f -invariant density
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